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Bierworth, Rick Daniel.
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Design of a rearwheel aftermarket suspension system for manual wheelchairs
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by Rick Daniel Bierworth.
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[Tampa, Fla.] :
b University of South Florida,
2007.
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ABSTRACT: The objective of this study was to design and build an aftermarket suspension for the rear wheels of a manual wheelchair. Suspension for wheelchairs is important because it has been reported that the International Organization for Standards' requirements for vibration loads on wheelchair users (ISO 26311), are not meet by today's standard wheelchairs. Today's wheelchairs need to be able to absorb everyday shock loads, thereby minimizing the energy transmitted to the user. The chosen design is based around the concept of adding shock reduction material between the hub of the wheel, and the axel bolt that connects the wheel to the frame of the chair. The approach taken was to design a suspension system that resides between an oversized wheel bearing, and the axle. To do this, ballrace bearings with an inner diameter of 4" were chosen, and polyurethane rubber was used as the shock absorbing material. ProMechanica, a finite element analysis program, was used to analyze the suspension system. Since the most common camber/tilt for wheelchair wheels is three degrees from the vertical, the anticipated loads were applied to the wheel at this angle. A prototype of the suspension system was constructed to verify that the design would work, but no tests were performed on it. This analysis showed that the suspension system should not fail when subjected to 10 times the static load. This load was considered large enough to encompass the forces that a wheelchair chair wheel is typically subjected to. There is room for further work in the area of weight reduction, and in the use of the suspension system on steeper wheel cambers.
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Thesis (M.S.)University of South Florida, 2007.
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Includes bibliographical references.
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Text (Electronic thesis) in PDF format.
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System requirements: World Wide Web browser and PDF reader.
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Title from PDF of title page.
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Advisor: Stuart Wilkinson, Ph.D.
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Disabled mobility.
Modified wheel.
Shock reduction.
Vibration reduction.
Finite element analysis.
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Dissertations, Academic
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x Mechanical Engineering
Masters.
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t USF Electronic Theses and Dissertations.
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u http://digital.lib.usf.edu/?e14.1964
PAGE 1
Design of a RearWheel AfterMarket Suspension System for Manual Whee lchairs by Rick Daniel Bierworth A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science in Mechanical Engineering College of Mechanical Engineering University of South Florida Major Professor: Stuart Wilkinson, Ph.D. Nathan Crane, Ph.D. Craig Lusk, Ph.D. Date of Approval March 22, 2007 Keywords: Disabled Mobility, Modified Wheel, Shock Reduction, Vibration Reduction, Finite Element Analysis Copyright 2007, Rick Daniel Bierworth
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i Table of Contents List of Figures....................................................................................................................iii List of Nomenclature........................................................................................................vii Abstract............................................................................................................................viii 1. Introduction.....................................................................................................................1 2. Suspension Wheelchair Technology...............................................................................3 2.1 Current Suspension Designs.............................................................................3 2.1.1 Elastomers..........................................................................................5 2.1.2 Steel Springs......................................................................................6 2.1.3 Composite Springs.............................................................................9 3. Structural Failure of Wheelchairs.................................................................................12 3.1 Failure of NonSuspension Wheelchairs........................................................12 3.2 Failure of Suspension Wheelchairs.................................................................14 4. AfterMarket Suspension for Wheelchair.....................................................................19 4.1 Design Process................................................................................................20 4.2 Materials Used................................................................................................25 5. Finite Element Analysis (FEA).....................................................................................28 5.1 Setting Up the FEA Models............................................................................30 5.2 Simulation of the Fork....................................................................................33 5.3 Simulation of the Inner Hub and Pin..............................................................34 5.4 Simulation of the Inner Hub and the 4Â’Â’ Ball Bearings..................................42 5.5 Simulation of the Outer Hub and the Spokes..................................................44 6. FEA Results..................................................................................................................46 6.1 Fork and Bolt Results......................................................................................47 6.2 Inner Hub and Pin Results..............................................................................51 6.3 Inner Hub and Ball Bearing Results...............................................................53 6.4 Outer Hub and the Spokes Results..................................................................56
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ii 7. Prototype.......................................................................................................................58 7.1 Machining and Assembly Process..................................................................58 7.2 Wheelchair Testing Modifications...............................................................59 7.2.1 Wheel Wobble.................................................................................59 7.2.2 Polyurethane Issues..........................................................................61 8. Conclusions...................................................................................................................66 References.........................................................................................................................67 Appendices........................................................................................................................69 Appendix A: Detailed Drawings of the Fork, Inner Hub, and Outer Hub............70 Appendix B: Rubber and Foam Chart From McMasterCarr...............................77 Appendix C: Fork and Bolt Analysis Â– 20 Degree Camber..................................78 Appendix D: Fork and Bolt Analysis Â– 3 Degree Camber...................................89 Appendix E: Inner Hub and Pin Analysis Â– 3 Degrees Camber.........................101 Appendix F: Inner Hub and Pin Analysis Â– 3 Degree Camber Â– With Local Mesh Refinement.................................................................114 Appendix G: Inner Hub and Pin Analysis Â– 20 Degrees Camber.......................128 Appendix H: Inner Hub and Pin Analysis Â– 6 Degrees Camber.........................141 Appendix I: Inner Hub and Ball Bearing Analysis.............................................154 Appendix J: Outer Hub and Spoke Analysis......................................................165
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iii List of Figures Figure 1: NonSuspension Â“Rigid MountÂ” of the Rear Wheels on a Wheelchair..............3 Figure 2: Â“Frog LegsÂ” TM Suspension for Caster Wheels..................................................4 Figure 3: Suspension on an Invacare A6S TM .....................................................................5 Figure 4: Coil Compression Spring Suspension of a Quickie XTR TM ...............................7 Figure 5: Tension Spring Suspension of a Permobil Colours Boing TM ..............................8 Figure 6: Composite Spring Suspension System Mounted on a Rigid Frame Wheelchair................................................................................................9 Figure 7: Failure of the Right Castor Pin of the Permobile Colours Boing TM Chairs.................................................................................................................14 Figure 8: Failure of the Telescoping Tube on the Invacare A6S TM Chair 1 and 3......................................................................................................15 Figure 9: Failure of the Invacare A6S TM Along the Frame of Chair 2............................16 Figure 10: Failure of Quickie XTR TM Chair 1, Where the Mount is Welded to the Frame....................................................................................................16 Figure 11: Failure of the Right Caster Mount on the Quickie XTR TM Chair 3................17 Figure 12: Regular Wheelchair Wheel.............................................................................20 Figure 13: Color Code for Wheel Suspension..................................................................21 Figure 14: Assembly of the Inner Hub, Outer Hub, and BallRace Bearings..................22 Figure 15: Assembly of Needle Roller Bearing and Fork................................................23
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iv Figure 16: Assembly of Fork and 3/8Â’Â’ Pin......................................................................24 Figure 17: Assembly of Bolt and Set Screw.....................................................................24 Figure 18: Urethane Rubber (Green), Which Reduces the Shock Loads and Vibrations That Are Transmitted to the User.................................................25 Figure 19: FreeBody Diagram of the Wheelchair...........................................................32 Figure 20: FEA Model of the Fork and Bolt.....................................................................33 Figure 21: First Model of Interaction Between the Inner Hub and the Pin/Needle Roller Bearing..............................................................................34 Figure 22: The Constraints Applied to the First Model....................................................35 Figure 23: The Contact Areas of the First Model, and the Applied Loads.......................36 Figure 24: Second FEA Model of the Inner Hub..............................................................37 Figure 25: Third (Simplified) Model Â– Inner Hub and Pin Only......................................38 Figure 26: Third Model Translational and Rotational Constraints.................................39 Figure 27: Third Model Contact Areas Between Inner Hub and Pin.............................40 Figure 28: Third Model Transverse Load Applied to the Lower Extension, Which Represents the Rim of the Wheel........................................................41 Figure 29: FEA Model of the Inner Hub, Cut in Half......................................................42 Figure 30: The Load that the BallRace Bearings Transmit to the Inne r Hub is Depicted by the Red Arrows...........................................................................43 Figure 31: FEA Model of the Outer Hub and Spoke Analysis.........................................44 Figure 32: The Model Was Cut in Half and a Symmetric Constraint Was Applied to the Cut Surface..............................................................................45 Figure 33: The Max VonMises Stress of 33,040 psi, for the 3 Degree Camber Fork and Bolt Analysis...................................................................................48
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v Figure 34: Convergence Graphs.......................................................................................50 Figure 35: Closeup of the Max VonMises Stress of 31,455 psi for the Inner Hub and Pin Analysis......................................................................................53 Figure 36: The Max VonMises Stress of 20,380 psi, for the Inner Hub and Ball Bearing Analysis Legend Values Are Set Between 2,040 psi and 18,340 psi.................................................................................................54 Figure 37: Using a Range of 0 to 40,000 psi for the Legend, the Stress Contour Shows that the Inner Hub Experiences Very Little Stress..............................55 Figure 38: The Max VonMises Stress of 37,231 psi, for the Outer Hub Spoke Hole Analysis, is Located at the Top of the Upper Spoke Hole.....................57 Figure 39: Overall VonMises Stress Contour for the Outer Hub Analysis....................57 Figure 40: Inner Hub ReDesign With Hardened Stainless Steel Bushing, a nd a Second CutOut for the Silicone Rubber.....................................................60 Figure 41: Fork ReDesign Needle Roller Bearings are Inserted Int o Either Side of the Fork.......................................................................................................60 Figure 42: The Polyurethane Causes the Fork to Rotate Upward When there is No One in the Wheelchair...............................................................................61 Figure 43: Suspension System with Someone Sitting in the Wheelchair.........................62 Figure 44: ReDesigned Suspension System....................................................................63 Figure 45: Overall Picture of AfterMarket Suspension System......................................64 Figure 46: AfterMarket Suspension System on AuthorÂ’s Wheelchair............................65 Figure 47: Fork DrawingÂ– Isometric View.......................................................................70 Figure 48: Fork DrawingÂ– Front View.............................................................................71 Figure 49: Fork DrawingÂ– Top View...............................................................................71 Figure 50: Inner Hub DrawingÂ– Isometric View..............................................................72
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vi Figure 51: Inner Hub DrawingÂ– Front View....................................................................73 Figure 52: Inner Hub DrawingÂ– Side View......................................................................73 Figure 53: Outer Hub DrawingÂ– Isometric View.............................................................74 Figure 54: Outer Hub DrawingÂ– Front View....................................................................75 Figure 55: Outer Hub DrawingÂ– Side View.....................................................................76 Figure 56: Outer Hub DrawingÂ– Top View......................................................................76 Figure 57: Comparison of Rubber and Foam Chart..........................................................77
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vii List of Nomenclature h Height P Dynamic Load W Static Load m Dynamic Deflection s Static Deflection
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viii Design of a RearWheel AfterMarket Suspension System for Manual Wheelc hairs Rick Daniel Bierworth ABSTRACT The objective of this study was to design and build an aftermarket suspension for the rear wheels of a manual wheelchair. Suspension for wheelchairs is important because it has been reported that the International Organization for StandardsÂ’ require ments for vibration loads on wheelchair users (ISO 26311), are not meet by todayÂ’s standard wheelchairs. TodayÂ’s wheelchairs need to be able to absorb everyday shock loads thereby minimizing the energy transmitted to the user. The chosen design is based around the concept of adding shock reduction material between the hub of the wheel, and the axel bolt that connects the wheel to the frame of the chair. The approach taken was to design a suspension system that resides betw een an oversized wheel bearing, and the axle. To do this, ballrace bearings with an inner diameter of 4 were chosen, and polyurethane rubber was used as the shock absorbing material. ProMechanica, a finite element analysis program, was used to analyze the suspension system. Since the most common camber/tilt for wheelchair wheels i s three degrees from the vertical, the anticipated loads were applied to the wheel at t his angle. A prototype of the suspension system was constructed to verify that the design would work, but no tests were performed on it.
PAGE 10
ix This analysis showed that the suspension system should not fail when subjected to 10 times the static load. This load was considered large enough to encompass the forc es that a wheelchair chair wheel is typically subjected to. There is room for fur ther work in the area of weight reduction, and in the use of the suspension system on steeper wheel cambers.
PAGE 11
1 1. Introduction Up until modern times, wheelchairs were typically made primarily from w ood, but in the 1930Â’s, Everest and Jennings made the first steel wheelchair. After World W ar II, veterans were given this one size fits all (depot) wheelchair, the kind ty pically used by hospitals, airports, and nursing homes today. They were not designed for optimum performance, but were simply meant to allow an individual to be moved from place to place. These generic wheelchairs are not suitable for active wheelc hair users, who need a lightweight, custom fit wheelchair. In the 1970Â’s, wheelchair users starte d to modify their own chairs, and the concept of lightweight, and ultralightweight adjust able wheelchairs was born [1]. Today, over 20 million people use a wheelchair as their primary source of mobility [1]. Wheelchair users that are more active need a chair that is not only lightweight, but is also able to decrease the shock and vibration loads that are transmit ted to the user. Studies have shown that the human body is unable to absorb these repeated shock loads, which cause increased pain, and also increases the chance of secondary spinal cord injury. It has also been reported that the International Organization f or StandardsÂ’ requirements for vibration loads on wheelchair users, (ISO 26311), are not meet by todayÂ’s standard wheelchairs [2]. The same way in which a modern car is designed to absorb a majority of the energy resulting from pot holes, speed bumps and
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2 debris, todayÂ’s wheelchairs need to be able to absorb everyday shock loads, thereby minimizing the energy transmitted to the user.
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3 2. Suspension Wheelchair Technology On nonsuspension wheelchairs, both the rear wheels and the castor wheels of the chair are mounted rigidly to the frame. Figure 1 shows the typical mounting of the re ar wheels of a wheelchair. The shock loads are transmitted directly from the whe el to the frame of the chair. Figure 1: NonSuspension Â“Rigid MountÂ” of the Rear Wheels on a Wheelchair 2.1 Current Suspension Designs Suspension can be added to the rear wheels, the castor wheels, or both. Three common methods used to achieve this include using elastomers, springs, and spring / damper combinations [2]. Â“Frog LegsÂ” TM a product that is currently on the market,
PAGE 14
4 provides aftermarker suspension for the castor wheels by using an elastome r damper to decrease the vibration and shock transmitted from the ground to the wheelchair and user. The elastomer that they use for their suspension is polyurethane with a 60 shoreA durometer. On their website, Â“Frog LegsÂ” TM claims that 80% of a wheelchairÂ’s vibrations come through the front castors [3]. This shows how important castor fork suspension is for the active wheelchair user. Figure 2 below shows a picture of the Â“Frog LegsÂ” TM suspension system, which replaces the factory installed castor wheels by retrofit. The arrow on the left is pointing to the black polyurethane that is used to a bsorb the shock and vibration forces. Figure 2: Â“Frog LegsÂ” TM Suspension for Caster Wheels Suspension is also added to wheelchairs through rearwheel suspension. At the time of this research, no aftermarket suspension was available to the rear wheels of a
PAGE 15
5 manual wheelchair. The suspension chairs available had the suspension incorporated int o their design. Within the category of rear suspension wheelchairs, there are t ypically two design styles: the use of elastomers, and the use steel springs. Composite spri ngs have also been used for wheelchair suspension. 2.1.1 Elastomers A rear suspension wheelchair that uses elastomers as a shock absorber is the Invacare A6S TM which is shown in Figure 3. This system absorbs the shock and damps the system at the same time, effectively replacing a spring and damper w ith a single element. Figure 3: Suspension on an Invacare A6S TM
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6 Low damping elastomers are used for shock absorption because they quickly recover the energy that it took to deform them. They also help to damp out unwanted oscillations. An elastomer is able to behave in this manner due to the arrangement of its molecules. They have long polymer chains that are made up of many carbon atoms. Various other atoms, like hydrogen, nitrogen, chlorine, etc., are then linked to the chai n. The bonds within the chain are very strong, but the bonds connecting all the chains together are considerably weaker. To enable the chains to return to their original pos ition after a load is applied and then removed, the polymer has to be cured, during which strong bonds are made between chains at various points. The curing process can only be done once, therefore, the rubber can not be recycled [4]. When designing with polymers, consideration has to be made as to how they will interact with their surroundings. Polymers are adversely affected by oil, U V radiation, strongly oxidizing environments, and various chemicals. They tend to creep at room temperatures, and to be brittle at low temperatures. However, most polymers res ist water, acids, and alkalis. When carbon black is added to them, polymers obtain protection from UV rays. To add a degree of chemical stability, some of the hyd rogen molecules are replaced with chlorine or fluorine molecules. Polymers also provide excellent electrical resistance [4]. 2.1.2 Steel Springs The Quickie XTR TM shown in Figure 4, uses the kind of Â“rock shockÂ” suspension system that can be seen on most mountain bikes today. It consists of a shock absorber inside a coil compression spring. This system is able to absorb shock, and damp oscillations at the same time. Figure 5 shows the coil spring system of the P ermobil
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7 Colours Boing TM It uses an AArm suspension system that consists of two tension springs. Coil springs are made from typical spring steel. Spring steel is m ade by bending the steel into the desired shape, and then heat treating it to the desired hardness Figure 4: Coil Compression Spring Suspension of a Q uickie XTR TM
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8 Figure 5: Tension Spring Suspension of a Permobil C olours Boing TM
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9 2.1.3 Composite Springs As part of the Capstone Design class at the University of South Florida, the use of composite springs for wheelchair suspension was researched. The design focus ed around the concept of an aftermarket suspension for standard rigid frame wheelchair s. It involved the use of a glass fiber reinforced polymer (GFRP) composite leaf spr ing mounted between the frame and the rear wheels. Normally the axle is hard mounte d to the frame of the chair. With this design, one end of the spring is attached to the f rame of the wheelchair with a mount, and the other end of the spring attached to the axle of the wheels. This results in a cantilevered leaf spring that is able to absorb the s hock loads experienced by the wheels. To damp the oscillations, a rubber strap was wrapped around the frame and the end of the leaf spring. Figure 6 shows the suspension system a dded to an Invacare Terminator TM wheelchair. Figure 6: Composite Spring Suspension System Mounte d on a Rigid Frame W heelchair
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10 When researching the use of composites for springs, the following was uncovered. Composites are made from polymers in the form of thermosetting resins like polyester or epoxy. These polymers, referred to as the matrix, are commonly mi xed with glass fiber, carbon fiber, or Kevlar fiber to produce reinforced polymers (GFRP CFRP, KFRP respectively). PolyesterGFRP is the cheapest composite, while epo xyCFRP and epoxyKFRP are more expensive. To obtain high stiffness and strength, continuous fibers are used, as compared to chopped fibers. The fibers used in the creation of these composites have been through a drawing process that aligns their chains with one another, giving them a strengthtoweight ratio that exceeds steel. The f ibers carry the load, while the polymers act to transmit the loads throughout the fibers, as well a s to protect the fibers from environmental damage. Combining the high stiffness and st rength of glass, carbon, or Kevlar fibers, with the ductility and durability of polyme rs, has created a class of materials that has a strengthtoweight ratio bette r than many types of metals. Factors that affect the performance of composites include: moist ure, fatigue, and heat [4]. Other factors that affect the properties of composites include choice of fiber, choice of matrix/ resin, fiberresin ratio, fiber length, fiber orientation, and la minate thickness. Glass fibers are cheap, but are not as strong as the more expensive ca rbon or Kevlar fibers, which are stronger, stiffer, and have a lower density than glass. Kevlar fibers are also fire retardant and, unlike carbon, allow radio waves to pass through th em. A unique feature about carbon fibers is that they are electrically conductive As for the matrix, polyester has relatively low cost and is the most widely used. Epoxy ma trices provide better properties at elevated temperatures than do polyesters, but they cost more
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11 than polyester. Increasing the fiber to resin ratio, increasing the fiber l ength, and running the fibers in the same direction, all act to increase the strength of the compos ite. Contrary to what one may think, decreasing the laminate thickness increases the strengt h, because the chance of having entrapped air is decreased [4]. Because they are made from oil and do not biodegrade, polymers are seen by many as environmentally unfriendly. However, there is ongoing research into us ing recyclable materials, like sugar and starch, as a basis for the synthesis of polymers [4].
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12 3. Structural Failure of Wheelchairs When redesigning a wheelchair to incorporate suspension, it is important that the structural integrity of the frame is not compromised. It has been reported th at 80% of injuries to people in wheelchairs occur because of engineering factors associ ated with the wheelchair design [5]. Therefore, before engaging in the design of a new kind of suspension for manual wheelchairs, it is important to understand how both suspension and nonsuspension wheelchairs have previously failed when subjected to testing. 3.1 Failure of NonSuspension Wheelchairs A test was done on 3 styles of wheelchairs: depot wheelchairs (DW), lightwei ght wheelchairs (LW), and ultralightweight wheelchairs (UW). The UWs g enerally weigh less than 30 lbs, while the LWs generally weight between 30 and 35 lbs [5]. Depot wheelchairs are the heaviest and cheapest. The chairs were constructed fro m steel, aluminum, titanium, or composite materials. A majority of the UWÂ’s were constr ucted from 6061 (aircraft) aluminum, while some were made from titanium. The DWÂ’s wer e all made from steel, and the LWÂ’s were made from either steel, or composite s [5]. The wheelchairs were subjected to a series of doubledrum test and curbdrop tests. A doubledrum test consists of two metal cylinders that the wheelchair ri des on. These cylinders have slats that are positioned 180 apart, and are supposed to simulate the everyday forces that a wheelchair is subjected to, such as sidewalk crac ks, and door
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13 thresholds. The curbdrop test is supposed to simulate bumping down off a curb, and consists of repeatedly dropping a wheelchair from a height of 5 cm. The doubledrum test is run for 200,000 cycles, and if catastrophic failure has not occurred, the chair is subjected to 6666 cycles of the curbdrop test. To meet ISO requirements, a chair has to survive one complete set of doubledrum and curbdrop tests [2]. After being subjected to a doubledrum test and a curbdrop test, it was found that the UW lasted the longest, and that the DWs had the worst results Some of the modes of failure that took place include: Class 3 Wheelchair frame cracking, caster stem breakage. Chair is dee med unusable at this point Class 2 Repairs that need to be made by a technician, like fixing flat tires or performing wheel alignments. Class 1 Repairs that can be done by the user, like tightening of loose screws and bolts [5]. All of the wheelchairs made from fiberglass experienced failure, and 76% of the chairs that were made from lowstrength steel tubing experienced failure. Howev er, none of the titanium chairs had a class 3 failure. It was found that the UWÂ’s performed the be st overall. These results confirmed the findings from previous tests which stat ed that the UWÂ’s perform better than the LW or DW wheelchairs [5].
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14 3.2 Failure of Suspension Wheelchairs It is obvious that incorporating suspension into manual wheelchairs will create a soother, safer, more comfortable ride for the user. With that in mind, it would also m ake sense that adding suspension to a manual wheelchair should result in more durable, longer lasting wheelchairs. However, three suspension wheelchairs that a re currently on the market, the Quickie XTR TM the Invacare A6S TM and the Permobile Colours Boing TM were subjected to a series of doubledrum and curbdrop tests, and the results showed otherwise [2]. In the study of the Quickie XTR TM Invacare A6S TM and Permobile Colours Boing TM each chair was tested until failure. Three Permobile Colours Boing TM chairs were tested, and all of them experienced fracture of the right caster ste m, as shown in Figure 7. It was suggested that the casters failed because their quick r elease system decreased their strength, and because part of the threaded section of the stem was exposed, resulting in a stress concentration. Figure 7: Failure of the Right Castor Pin of the Pe rmobile Colours Boing TM Chairs
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15 Because the chair was not able to complete the doubledrum test, it was not subject ed to any curbdrop tests [2]. When the three Invacare A6S TM chairs were tasted, all of them completed one cycle of doubledrum and curbdrop tests. The failure in chairs 1 and 3 occurred in the telescoping tube of the suspension system. The failure took place in the heat affe cted zone of a weld, as shown in Figure 8. The failure of the second chair was caused by a stress concentration at a screw hole in the seat part of the frame, as shown in Figu re 9 on the next page [2]. Figure 8: Failure of the Telescoping Tube on the In vacare A6S TM Chair 1 and 3
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16 Figure 9: Failure of the Invacare A6S TM Along the Frame of Chair 2 The three Quickie XTR TM chairs outlasted all the others, with chair 1 lasting 1,000,000 doubledrum cycles and 33,330 curbdrop cycles, before experiencing fracture where the mount was welded to the lower part of the frame, as show in Figure 10. Figure 10: Failure of Quickie XTR TM Chair 1, Where the Mount is Welded to the Frame
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17 Chairs 2 and 3 had similar durability, but failed in different ways. Chair 2 experience d a fracture at a screw hole in the right side of the seat part of the frame, while chair 3 experienced a fracture in the mount for the right caster wheel as shown in Figur e 11. The caster mount for chair three was considered substandard [2]. Figure 11: Failure of the Right Caster Mount on the Quickie XTR TM Chair 3 The results from the suspension wheelchair test were compared with the res ults obtained from a test of four different ultra lightweight wheelchairs (12 whe elchairs total). It was found that the suspension wheelchairs did not show any significant improvement over ultralightweight wheelchairs, in the area of durabilit y. However, the suspension wheelchairs were shown to be more durable than the lightweight wheelchairs. Because the Permobile Colours Boing TM had problems with its castor pins failing, the results for the whole group were unfavorable. When this chair was remove d
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18 from the analysis, the number of cycles for the Quickie XTR TM and the Invacare A6S TM were 911,394, which outlasted the 187,362 cycles of the lightweight wheelchairs. However, they were still below the 1,092,441 cycles for the ultralightwheelchairs [2]. This study of suspension wheelchairs has shown that there is room for improvement in the area of rear suspension for manual wheelchairs. In the next se ction, the design of the aftermarket suspension system that was developed during this t hesis will be discussed.
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19 4. AfterMarket Suspension for Wheelchair There is a need for an aftermarket suspension system for manual wheelcha irs that will allow the users of regular / nonsuspension wheelchairs to add rearwheel suspension to their wheelchairs. During the previous mentioned USF senior design project, af termarket rearwheel suspension was attempted through the addition of leaf spring suspension between the wheels and the frame the chair. However, it was found that wheelchair frames are too diverse to permit a retrofit of one single suspens ion design to all frames. To design a more universal suspension system, this thesis has focused on the design of a wheel that has suspension incorporated into it. This approach will allow the addition of suspension to most wheelchairs by simply buying new wheels. This approac h will also take advantage of the proven durability of ultra lightweight wheelcha irs, allowing the wheelchair user to take a tried and true ultra lightweight whe elchair, and then add suspension wheels to it. The suspension can also be used on other wheelchairs besides ultra lightweight wheelchairs.
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20 4.1 Design Process A typical wheelchair wheel either has a quickrelease pin or a bolt, which pas ses through a set of inner diameter ballrace bearings, and is then inserted into the frame of the chair. For simplicity, a quickrelease pin will be referred to as a bolt for this paper. Figure 12 below shows a typical wheelchair wheel. Figure 12: Regular Wheelchair Wheel The ballrace bearings of a regular wheelchair wheel have a inner diameter, and the quickrelease pin / standard bolt, passes through the middle of the ballrace bearings and is then attached to the frame of the chair. The design for this thesis i s based around the concept of adding shock absorbing material between the spokes of the wheel, and the bolt that connects the wheel to the frame of the chair. The approach taken was to design a suspension system between the inner diameter of the ballrace bearing s, and the bolt. To do this, ballrace bearings with an inner diameter of 4 were chosen. Figure 13
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21 on the following page is a picture of the suspension system designed for this thesis. The green rectangle represents the shock absorbing material that absorbs the sho ck load that would normally be transmitted from the wheel to the frame of the chair. Figure 13: Color Code for Wheel Suspension Red = Outer Hub; Yellow = 4" inner diameter ball be aring; Dark Blue = Inner Hub; Light Blue = Fork; Gold = " quickrelease pin / standard bolt, and 3/8" pin; Green = Urethane
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22 The procedure for constructing the suspension wheel will now be covered. There is no direct contact between the outer hub and the inner hub. They are connected by way of the ballrace bearings being press fitted into the space between the inner and outer hub. The use of a retaining ring was considered, but they were too large for this appl ication. See Figure 14a through 14d below for a description of the assembly process. Figure 14: Assembly of the Inner Hub, Outer Hub, an d BallRace Bearings a. (top left) Inner hub b. (center) Outer hub c. (right) Inner hub is placed inside the outer hub d. (bottom left) The ballrace bearings (yellow) are press fitted between the outer and inner hub, and hold the two together.
PAGE 33
23 Next, a 3/8 inner diameter, 9/16 outer diameter, needle roller bearing is pressed into the 9/16 diameter hole in the inner hub. In Figure 14d, this is the small hole. Then the fork is inserted through the circular and square opening in the inner hub, and aligned so that the 3/8 holes in both sides of the arms of the fork, line up with the 3/8 needle roller bearing. See Figure 15a and 15b below for further description of the ass embly process. Figure 15: Assembly of Needle Roller Bearing and Fo rk a. (left) The needle roller bearing (gray) pressed int o the hole in the inner hub. b. (right) The fork with a hole for bolt that attaches the wheel to the chair and two 3/8 holes for the pin that connects the fork to the inn er hub. The fork is attached to the inner hub with a 3/8 diameter pin that passes through the holes in the fork, and the needle roller bearing. 3/8 washers, not shown, are used between the fork and the inner hub so that they do not bind. Two set screws are used to keep the 3/8 pin from coming out of the fork. Loctite TM can be used to keep the set screws from loosening over time. See Figure 16a and 16b below.
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24 Figure 16: Assembly of Fork and 3/8Â’Â’ Pin a. (left) The fork inserted through the inner hub, and aligned with the needle roller bearing. b. 3/8 inch pin (gold color) that connects the fork to the inner hub Then, a diameter bolt that attaches the wheel to the frame of the wheelchair is inserted into the hole in the fork. No bearings are required at this interface because there is no relative motion between the fork and the bolt during operation. Figures 17a and 17b show the assembly of the outer hub, ballrace bearings, inner hub, fork, pin, and bolt. Figure 17: Assembly of Bolt and Set Screw a. pin/bolt (gold color) that connects the fork to th e wheelchair b. Angled view of suspension system. The end of the p in/bolt that connects the fork/wheel to the chair can be seen.
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25 A block of Urethane rubber is inserted between the bottom of the fork and the flange of the inner hub. Since the fork is fixed in its current position, as the wheel encounters a bump, the Urethane rubber is compressed, and inner hub rotates slightly about the 3/8 diameter pin. See Figure 13 below for a picture of the complete suspension system. Figure 18: Urethane Rubber (Green), Which Reduces th e Shock Loads and Vibrations That Are Transmitted to the User 4.2 Materials Used The materials chosen for the various components are as follows. The fork, inner hub, and outer hub, are made from 6061 T6 Aluminum. This is the same material that most lightweight wheelchairs are made from. It has a yield strength of 40,000 psi, and a modulus of elasticity of 10,000 psi. The 3/8 diameter pin is made from 304 stainless steel. It has a yield strength of 31,200 psi, and a modulus of elasticity of 28,000 psi. The
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26 quickrelease pin / bolt are standard to all wheelchairs, so no special care wa s taken in the selection of these parts. The 4 inner diameter ballrace bearings were purchased from Silverthin Bearing Group They are made from AISI 52100 bearing steel. Two sets of ballrace bearing s, consisting of a radial contact bearing and a fourpoint contact bearing, ar e used for each wheel. A radial contact bearing is mainly used for radial loads, but can also withs tand some axial and moment loads. A fourpoint contact bearing is mainly used for moment loading and reverse axial loading, but can also be used for light radial loading [6]. By using a radial contact bearing and a fourpoint contact bearing on the same wheel the benefits of both types of bearings can be combined. The stress ratings for the ball race bearings were obtained from the Si lverthin website. Both the radial contact and the fourpoint contact bearings are rate d for a static radial load of 1,293 lbs, and a dynamic radial load of 486 lbs. The fourpoint bearing is rated for a static moment of 2,748 lbsinch, and a dynamic moment of 1,035 lbsinch [7]. The 3/8 inner diameter roller needle bearings were bought from McMasterCarr a nd are rated for a dynamic load of 1,300 lbs [8]. As will be shown in section 5.1, the ball race bearing static load rating is greater than the 10 times static load of 1150 lbs that was used for the analysis. However, the dynamic load rating for the ball race bearin gs is below the 10 times static load of 1150lbs. Further research should be done to determine how the dynamic load rating compares to the static load rating. For this thesis, it is assumed that since a factor of safety of 10 is used, the bearings should not fail. See section 5.1 for discussion about what a 10 times static load was used.
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27 Polyurethane was used for the elastomer. Polyurethane has excellent resis tance to oil, abrasion, tearing, and impact. It also has good resistance to weather an d chemicals [8]. Since Â“Frog LegsÂ” TM uses cylinder shaped polyurethane with a 60 shoreA durometer, similar shapes and durometers were tested with the suspension system i n order to find out which shape and durometer provided the most comfortable ride. It was decided that a diameter cylinder of polyurethane, with a durometer of 40 Shore A, was the best combination for the suspension system.
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28 5. Finite Element Analysis (FEA) As with any design, it is necessary to know if the stresses applied to the sys tem are within the material limits listed in section 4.2. Finite element analy sis software was used to perform an elementary analysis of the stresses in this suspension syst em, in order to show that it will not fail. During the process of creating a FEA model, a num ber of assumptions and simplifications are made by the program, and by the user. For the suspension, the following process was used. The real world model is simplified and assumptions were made. The materials used are assumed to be homogeneous, isotr opic, and free of internal defects; and cosmetic features are suppressed so as to r educe the geometric complexity, allowing for faster solve times [9]. To create a mathematical model that represents the part being analyzed, th e FEA program makes various assumptions, such as the linearity of the material, and the natur e of the loading conditions. With these assumptions, mathematical models are create d that describe the change in the variables of interest within the boundaries of the model. T he geometry of the model is then broken up into many elements so that the differential equations created by the mathematical model can be rewritten as a system of simultaneous linear equations to represent the whole model. This network of connected elements is called a mesh [9]. Once these equations are solved, the results obtained represent the variables of interest, such as stress, deformation, etc. However, the accuracy of the res ults need to be
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29 verified by convergence, Â“the process of reducing the local error by using s maller and smaller elements or using elements that can approximate more complex poi nttopoint shapes.Â” One of the differences between FEA programs is the way in which converg ence is achieved. The classical approach is to use helements, which typically limi t the element order to a quadratic formula. To obtain convergence, the mesh has to be refined, or made denser, until the difference between results fall within the desired p ercentage. The advantage to this approach is that first and second order equations solve relatively quickly. The disadvantage is that the mesh has to be refined for each computer run, and the results have to be compared for convergence. The other approach is to use pelements, which can assume higher element edge orders. This allows for better representation of the model. For example, tryin g to represent an arch with only a 2 nd order polynomial is not very accurate if the mesh size is not dense enough. With pelements, this same arch can be represented by only a few elements, each with a polynomial edge order of nine or higher. While a 9 th order polynomial takes longer to solve than a 2 nd order polynomial, no mesh refinement is needed. The order of polynomial used to solve the equations starts at one, and keeps increasing until convergence is reached, or until the max edge order available is reached [10]. To monitor this convergence, Pro/ENGINEER Mechanica uses the results obtained for the maximum Von Mises stress and the total strain energy. The FEA program, Pro/ENGINEER Mechanica, does this automatically. Occasionally convergence is still not reached after solving the 9 th order polynomial, and the mesh needs to be refined. ProMechanica has the capability to do this mesh refinement it self,
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30 and then another analysis can be run using the refined mesh [9]. The advantages to this method are that mesh refinement is usually not needed, and it is generally easie r to use. The disadvantage is that the run times are generally longer. Pro/ENGINEER Mechanica was used for this thesis because it was decided that the ease of use of pelement s was worth the longer solution times. 5.1 Setting Up the FEA Models To create the FEA models for this thesis, the parts were first created in Pro/ENGINEER, a 3D computer modeling software. Features not important to the analysis were suppressed, and then the models were sent to Pro/ENGINEER Mecha nica. In Mechanica, units and material properties were assigned. Then constraints a nd loads that helped to simulate realworld conditions were applied. Since Mechanica automatically Â“weldsÂ” surfaces that are in contact with each other, Â“c ontact regionsÂ” were added to parts like the fork and the bolt. This allowed the two surfaces to separate when a load was applied, like it would in the real world. It is impractical to analyze the whole model at once, because each run time would take a few days, and trouble shooting problems within the model would be very difficult. Therefore, assumptions were made about what were considered critical a reas within the suspension system, and then models were created that focused on these critical ar eas. The system was broken down into four models: 1) the interaction between the fork and the bolt, 2) the inner hub and the 3/8 diameter pin/needle roller bearing, 3) the inner hub and the 4 inner diameter ballrace bearings, 4) and the outer hub and the spokes.
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31 In the real world, the wheel is subjected to a variety of loads, including static dynamic, cyclic, fatigue, and torsion/moment loading. To be reasonably sure t hat failure would not take place, it was decided to analyze the various components at static load, and increase the load until failure took place, or until the load was considered large enoug h to encompass the loads that a wheelchair wheel would be subjected to. When a force of 10 times the static load was used, the stress on the components was still below the yield stress of the aluminum. To check the acceptability of this value, the following calculations were performed. A curb height of 6 (152 mm) was used for the calculation. The maximum allowable deflection for the fork/polyurethane when the wheelchair drops 152 mm, is 34 mm. The corresponding static deflection, the deflection caused by a person sitti ng in the chair, is given by equation 1 below [11]. () mm h m m s 42.3 2 2 = + =d d d Eq.1 The static deflection is then used in equation 2 below to determine the dynamic to stati c load ratio [11]. 48. 10 2 1 1 = + + = s h W Pd Eq.2 Since the shock absorption of the tires and the wheelchair cushion were not considered for the preceding equations, it was decided that a force of 10 times the static loa d would suffice for this analysis. Since the most common camber/tilt for wheelchairs wheels is 3 degrees from t he vertical, the 10 times static load was applied to the wheel at this angle [12]. To ca lculate
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32 the static load, a 200 lb person and a 30 lb chair were assumed. Assuming that this weight acts only on the rear wheels, each wheel experiences half of this lo ad, or 115 lbs. With a 3 degree camber, this comes to 114.8 lbs normal to the rim of the wheel, and 6.0 lbs transverse to the rim. For simplicity, the normal portion of the static load wil l be rounded to 115 lbs. So ten times the static load is 1150 lbs normal to the rim of the wheel, and 60 lbs transverse to the rim of the wheel. See figure 19 below for a free body diagram of a wheelchair with a three degree camber. Figure 19: FreeBody Diagram of the Wheelchair PersonÂ’s Weight 200lbs Chair Weight 30lbs Ground Reaction on Each Rear Wheel (200+30)/2 = 115lbs Assume Front Casters OffGround (Worst Loading Case) Hub Load Components @ 3 Camber Axial = 6lbs Transverse ~ 115lbs
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33 5.2 Simulation of the Fork The first simulation was of the fork and the bolt. First, the 3/8 diameter holes that the 3/8 diameter pin goes through were constrained in all six degrees of freedom. In Figure 20 below, this is shown by the yellow triangles. Then a contact region wa s created between the bolt and the diameter hole in the fork. The contact regions are depicted with two parallel red lines with another line intersecting them, and the yellow balance scale icons. To simulate the static load applied to the bolt from the wheelc hair, the bolt was cut off at the side of the fork, and a force of 10 times the load, 1150 lbs normal to the rim and 60 lbs transverse to the rim, was applied to its crosssection This load is depicted by the red arrows on the end of the gold colored bolt. Figure 20: FEA Model of the Fork and Bolt
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34 5.3 Simulation of the Inner Hub and Pin The second simulation was of the 3/8 diameter pin, the needle roller bearing, and the inner hub. The purpose of this model was to simulate the effect that the needle rolle r bearing and the pin would have on the inner hub. This analysis took the most time, because it was difficult to Figure out how to best constrain the model so as to simula te realworld conditions. A number of models were created, ranging from very sim ple to very complex, until a model was obtained that appeared to adequately model the real world conditions. Three of these models will be discussed in the following pages. Figure 21 shows the first model that was created to simulate the effect the pin would have on the inner hub. In real life, the 9/16 outer diameter needle roller bearing is pressed into the inner hub, and the 3/8 pin is then inserted into the bearing. To simplify the model, a 9/16 diameter pin was used in place of the bearing and pin combination. Figure 21: First Model of Interaction Between the I nner Hub and the Pin/Needle Roller Bearing
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35 Next, the ends of the cylinder were cut off at the surface of the inner hub, as shown in Figure 22 below. This simulates the portion of the pin that is not contained by the fork. The constraints applied to the model are also visible in Figure 22. The outer circular surface of the hub was fixed in all six degrees of freedom, and the ends of the pin were fixed in the zdirection, the plane of their surface. These constraints a re represented by red triangles. Figure 22: The Constraints Applied to the First Mod el
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36 In Figure 23, the two red symbols show that there is a contact region between the pin and the inner hub. To apply a torque load to the wheel, 10 times the static transverse load, 60 lbs, was multiplied by the 12 moment arm that it acted over. The resultant torque of 720 inlbs was then applied to both sides of the cylinder. This load is depicted by the yellow arrows in Figure 23. Figure 23: The Contact Areas of the First Model, an d the Applied Loads This model did not depict real world conditions very well because the zdirection constraints on the pin were causing it to deform in a maner not intended.
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37 The second and most complex model that was created is shown below in Figure 24a, 24b, 24c. Square extension planks were added to the inner hub to simulate the spokes and outer diameter of the wheel. The 10 times static load was applied to these extentions. Figure 24: Second FEA Model of the Inner Hub a. (left) FEA model of the inner hub, with extensions added to simulate the spokes and outer diameter of the wheel, and the 3/8 pin. b. (center) Close up of the inner hub and 3/8 pin model. The fork, urethane, and bolt were added to try to get a better simulation. c. (right) Shows the upward and sideways load (red arr ow at the bottom of the model) that represents the force that the ground exerts on the wheel. Then, 10 times the normal portion of the static load (1150 lbs), and 10 times the transverse portion of the static load (60 lbs) were applied to the bottom and the side of t he lower extension respectively. The red arrow at the bottom of the model in Figure 24c represents the effect of the ground on a tilted wheel.
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38 The bolt was fixed in all six degrees of freedom to represent being attached to the wheelchair. This model had numerous contact areas, and it took about a day and a half for each computer run. About 5 models were run, and each time the results file gave warnings about the contact areas and inaccurate pressure results. Also, the model di d not behave in the manner that it was intended to, so it was decided to try a more simplifie d approach. The third, more simplified model consisted of the inner hub with the extension planks, but the fork, bolt, and urethane were eliminated from the model. This model is very similar to the first model; with the differences being the addition of the e xtension planks, the square cutout, the constraints, and where the load was applied. Figure 25 shows the overall model. Figure 25: Third (Simplified) Model Â– Inner Hub and Pin Only
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39 Figure 26 shows the constraints, depicted by yellow triangles, which were a pplied to the inner hub. To prevent the inner hub from sliding along the pin, the surface of the 9/16 diameter hole in the hub was constrained so that it could not move along its axis. To prevent the inner hub from rotating about the 9/16 diameter hole, the sides of the square cutout were constrained so that they could not move out of the plane of their surface. Figure 26: Third Model Translational and Rotation al Constraints
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40 Figure 27 shows that symbols for the contact areas that were created between t he inner hub and the pin, and that the pin was constrained in all six degrees of freedom. Figure 27: Third Model Contact Areas Between Inne r Hub and Pin Figure 28 shows a force of 10 times the transverse portion of the load (60 lbs), like the load in 24c, applied to the bottom of the lower extension. This represents the torque applied to the pin and hub of a tilted wheel. A normal portion of the static load was not used because none of this load should be transmitted to the 9/16 diameter hole. This load should be transferred from the inner hub to the urethane, where it is damped, and then transmitted to the fork, the bolt, and finally to the frame of the chair.
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41 Figure 28: Third Model Transverse Load Applied to the Lower Extension, Which Represents the Rim of the Wheel
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42 5.4 Simulation of the Inner Hub and the 4 BallRace Bearings The third simulation was of the 4 inner diameter ballrace bearings and the inner hub. A model was created to determine the stress that is created in the inner hub by th e load being transmitted from ground to the ballrace bearings, and then to the inner hub. To simplify the model, the inner hub was cut in half. Then a symmetric constraint, whi ch tells the computer that the right side is a mirror of the left side, was applied to the surface of the cut plane. The symmetric constraint is depicted by the halfway fille d in red box on the left. See Figure 29 below. Figure 29: FEA Model of the Inner Hub, Cut in Half
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43 As shown in Figure 29, the constraint added to the bottom surface of the square cutout constrains the surface in all six degrees of freedom. To simulate the load tr ansmitted from ground to the ballrace bearings, a force of 10 times the normal portion of the sta tic load, 575 lbs on each side of the hub, was applied to the bottom surface of the hub that is in contact with the ballrace bearings. See Figure 30. Figure 30: The Load that the BallRace Bearings Tra nsmit to the Inner Hub is Depicted by the Red Arrows
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44 5.5 Simulation of the Outer Hub and the Spokes The fourth and last simulation was of the outer hub. The purpose of this model was to simulate the effect the spokes have on their corresponding holes in the outer hub. The effect of the ballrace bearings on the outer hub was not analyzed because it w as assumed that the results would be similar to the results obtained from the inner hub. Since it would be very time consuming and difficult to simulate the loads that are appl ied by all the spokes to the outer hub, a model was created to analyze the stress on only one of the spoke holes. The bottom spoke hole was constrained in all six degrees of freedom, while the static load was applied to the top spoke hole. See Figure 31 below. Figure 31: FEA Model of the Outer Hub and Spoke Ana lysis
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45 The model was then cut in half, in order to shorten the computer run time, and a symmetric constraint was applied. See Figure 32 on the following page. Since only one spoke hole was being loaded, it was decided to only use 5 times the normal portion of the static load, 575 lbs. Since half the static load is applied to each side of the outer hub, 278 lbs was applied to the top spoke hole, as shown in Figure 32. Such an extreme loading condition was chosen in order to show that the strength of the spoke holes should be of no concern. Figure 32: The Model Was Cut in Half and a Symmetric Constraint Was Applied to the Cut Surface
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46 6. FEA Results FEA programs create a vast amount of data, and the only way to really examine the results is graphically. ProMechanica has numerous ways of displaying t his data, including displacement animations, stress distributions, mode shapes, etc [9]. With s uch a vast amount of data available, the goals of the project need to be reviewed before proceeding with results interpretation. The goal of this analysis was to pro ve that the suspension system would not fail when subjected to the everyday shock loads that a wheelchair wheel encounters. To prove this, a number of failure modes could have been used. These include the maximum normal stress theory, the maximum shear stres s theory, and the distortion energy (VonMisesHencky) theory [10]. When using the maximum normal stress theory, failure happens when the principal stress equals the failure strength of the material, whether in t ension or compression. This theory can be used for both ductile and brittle materials, but can onl y reasonable predict stress behavior if the principal stresses are simila r in sign and magnitude. The maximum shear stress theory states that failure will oc cur when the maximum shear stress is equal to half the yield strength of the material This theory can only be used for ductile materials because it only predicts failure by yiel ding. The maximum shear stress theory gives a conservative estimate when used t o predict stress. The vonMises theory states that failure occurs when the effective stress i s equal to the yield strength of the material [10].
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47 The vonMises failure theory is very popular because it can describe very complex stress states, and Adams states that this theory Â“provides the best m atch with experimental dataÂ” [10]. For this analysis, the VonMises stress was used to view the results and determine if failure would take place in the models. 6.1 Fork and Bolt Results As stated earlier, a load of 1150 lbs and 60 lbs, which are 10 times the normal and transverse portions of the static load respectively, were applied to the model of the fork and bolt. When the model was run, the results output file stated the following: ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. This was done, but the same warnings were stated again, and the results in the output fil e were exactly the same. The reason for the error was looked into, but an answer coul d not be found. To solve this dilemma, the results of some of the initial analyses were reanalyzed. During the initial stages of the analysis, different cambers were used to determine the maximum allowable camber for the suspension system. This maximum all owable camber will be discussed in section 6.2. The largest camber that could be found was 20 degrees, which is used on specialized sport wheelchairs such as tennis chairs [12]. When 10 times static load was applied to a fork and bolt model with 20 degrees of camber, the
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48 values obtained were 1080 lbs normal to the rim of the wheel, and 390 lbs transverse to the rim. When the analysis was run, the contact area warning was displayed for the f irst two convergence checks, but when a edge order of four was used, which means that a 4 th order polynomial was used to model the mesh elements, the warning did not come up. The analysis continued to run until the model converged with an edge order of seven, and no more contact area warnings. The maximum Von Mises stress obtained for the fork and the bolt when using the 3 degree camber was 33,040 psi, located near the bottom of the diameter hole. In Figure 32 below, the yellow shaded area is where this stress occurs. When the camber of 20 degrees was used, the maximum Von Mises stress was 30,924 psi. Both of these stress results are below the 40,000 psi yield strength for 6061 T6 Aluminum. Figure 33: The Max VonMises Stress of 33,040 psi, for the 3 Degree Camber Fork and Bolt Analysis
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49 The difference in the stress values was considered to be a result of the change i n loading conditions. Because there was not a surprising difference between the two st ress values, it was considered safe to be able to disregard the warning about the conta ct area. As stated earlier in the paper, the bolt/quickrelease pin was not analyzed becaus e they are standard to all wheelchairs and have been proven to be reliable. The process by which ProMechanica determines convergence will now be discussed. The convergence for the 3 degree camber model was set to 10%, which means that the difference between the strain energy for the 6 th order polynomial and the 7 th order polynomial was within 10%. This was considered sufficient because the analysis w as only used to determine how much times the static load the suspension system could withstand. As can be seen from Figure 34a and 34b, the von Mises stress can behave rather erratically, while the strain energy increases in an asymptoti c manner. Due to this behavior, the strain energy is considered a better measure to use when monitori ng convergence [9].
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50 Figure 34: Convergence Graphs a. (top) The strain energy convergence graph for the f ork and pin analysis. b. (bottom) The max vonMises stress convergence graph for the fork and pin analysis.
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51 6.2 Inner Hub and Pin Results A load of 60 lbs, which is 10 times the transverse portion of the static load, was applied to the side of the lower extension of the inner hub in order to simulate the torque load applied to a tilted wheel. When the model was run, the results output file also gave the following warning: ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. The model was rerun using singlepass adaptive convergence with localized mes h refinement, but the same warnings were stated again. Also, the stress res ults in the output file were exactly the same as the stress results in the previous output file. Since using a 20 degree camber caused the warning to go away in the fork and bolt analysis, an analysis using a 20 degree camber was also ran here. However, the warnings s till occurred. This is probably due to the fact that while the magnitude of the load was changed, the loading orientation was still the same. For the case with the for k and bolt, when the 20 degree camber load values were used, the load orientation was changed. I n the previous analysis of the fork and bolt, it was decided that the warning about the contact area could be disregarded. Therefore, the warning will be disregarded here as well.
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52 Regarding the maximum allowable degree of camber, the vonMises stress va lue for the 20 degree camber was 212,618 psi, which exceeds the yield strength of Aluminum. Available angles of camber for wheelchairs include 3, 6, 9, 12, 15, 18, and 20 [12]. A number of analysis were run using the different camber angles in order to f ind the steepest camber that could be used before the inner hub and pin failed. It was found that the maximum camber that could be used was 3 degrees. When a camber of 6 degrees was used, the transverse portion of the 10 times static load was 120 lbs. The resulting vonMises stress for this load was 65,421 psi, which exceeds the 40,000 psi yield strength of the aluminum. For further research, the loading of the model should be analyzed further in order to see if the inner hub and pin are subjected to the full transverse portion of the static load, or if the wheelsÂ’ interaction with the ground lessens some of thi s load. Now getting back to the model at hand, the 3 degree camber model converged after an edge order of 8 was used. Again, the convergence for the model was s et to 10%. The maximum vonMises stress obtained for the inner hub was 31,455 psi, located near the bottom of the 3/8 diameter hole. In Figure 35 below, the yellow shaded area is where this stress occurs. Again, since the yielding strength of 6061 T6 aluminum i s 40,000 psi, this FEA analysis has shown that the 3/8 diameter hole in the inner hub should not experience failure.
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53 Figure 35: Closeup of the Max VonMises Stress of 31,455 psi for the Inner Hub and Pin Analysis 6.3 Inner Hub and Ball Bearing Results As stated earlier, a load of 575 lbs was applied to both of the surfaces of the inner hub that the ballrace bearings are press fitted onto, to give a total load of 1150 lbs. This is 10 times the normal portion of the static load. The model converged after an edge order of 9 was used, which is the maximum edge order available in ProMechanica. Again, the convergence for the model was set to 10%. This model probably required a 9 th order polynomial for convergence because of the sharp edges made by the square cutout, and because the bottom surface of this cutout was constrained in all six degrees of freedom. The maximum vonMises stress obtained for the inner hub was only 20,380 psi, and is located near the edges of the square cutout. Figure 36, shows the default le gend values, 2,040 psi to 18,340 psi. This range of values is better for showing the details of the stress contour, than the true legend values of 0psi to 40,000 psi shown in Figure 37.
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54 Figure 36: The Max VonMises Stress of 20,380 psi, for the Inner Hub and Ball Bearing Analysis Legend Values Are Set Between 2,040 psi and 18,340 psi
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55 Figure 37: Using a Range of 0 to 40,000 psi for the Legend, the Stress Contour Shows that the Inner Hub Experiences Very Little Stress This FEA analysis has shown that the stresses in the inner hub do not even come close to the 40,000 psi yield strength of the aluminum, and failure should not occur. These results confirm that the use of symmetry for this model was appropriate. For further analysis, an optimization study should be done in ProMechanica in order to decrease the size/weight of the inner hub. In an optimization study, a desired g oal is specified (ie. minimum mass) and Mechanica searches for a design that sati sfies the goal based on the constraints applied [9].
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56 6.4 Outer Hub and the Spokes Results As stated earlier, a load of 287 lbs was applied to the top spoke hole of the outer hub model. When the results of the analysis were examined with the thesis committee the suggestion was made that a pieslice model would be more accurate. However, f or this elementary analysis, it was determined that the current analysis would suffice. The 287lbs load simulates 5 times the normal portion of the 10 times static load. The model converged after an edge order of 6 was used. Again, the convergence for the model was set to 10%. The maximum vonMises stress obtained for the inner hub was 37,231 psi, and is located at the top of the upper spoke hole, as shown in Figure 38 below. This FEA analysis has shown that even with a five times static load applied to one spoke hole, the stresses in the outer hub are still under the 40,000 psi yield strength of the aluminum Figure 38 is an over all picture stress contours of the outer hub. For further analy sis, an optimization study should be done on the outer hub as well as the inner hub in order to decrease its size/weight.
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57 Figure 38: The Max VonMises Stress of 37,231 psi, for the Outer Hub Spoke Hole Analysis, is Located at the Top of the Upper Spoke Hole Figure 39: Overall VonMises Stress Contour for th e Outer Hub Analysis
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58 7. Prototype After the FEA results were studied, a prototype was made. Some problems with the design were discovered during the machining and assembly processes, and also whi le installing the suspension system on a wheelchair. This section will go into furt her detail about what problems were detected, and what was done to fix them. 7.1 Machining and Assembly Process During the machining process, it was discovered that the cutout in the inner hub for the polyurethane was not big enough for the fork to be inserted into the inner hub. To fix this, the slot for the polyurethane rubber was increased from wide to 1 wide. Then, the 1 tall fork was able to slide through the 1 rubber slot. In section 6.3, the stress in the inner hub was shown to be very low. Therefore, it was assumed that this modification will not significantly affect the stress distribution of the inne r hub. During the assembly of the prototype, a problem with the ballrace bearings was discovered. The recesses in the inner and outer hubs, for the 4 ballrace bearings, have a press fit of 0.0015 This press fit caused the inner diameter of the ballrace bearings to be slightly expanded, and the outer diameter of the ballrace bearings to be sli ghtly compressed. Because of this extra pressure on the balls, the bearings spun more sluggishly. To address this problem, a press fit of 0.001 should be tried for future assemblies. The use of a thin section retaining ring should also be considered.
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59 7.2 Installation on a Wheelchair When the suspension was installed on a wheelchair, some problems were discovered. This section will discuss these problems, and how they can be fixed. 7.2.1 Wheel Wobble To start with, the fit between the 3/8 dowel pin and the needle roller bearing in the inner hub is too loose because the diameters of the dowel pin and the bearing are not exactly the same. This causes the wheel to wobble about the fork/pin interface. Four nylon washers, two on either side of the needle roller bearing in the inner hub, were supposed to be inserted between the fork and the bearing/web of the inner hub. However, only 3 washers could be inserted. A couple solutions to this wobble problem will now be discussed. One solution would be to have a tighter fit between the two sides of the fork and the web of the inner hub. Instead of a 5/8" gap between the two sides of the fork, the gap could be reduced to 11/16", and washers would still be used. Another solution is to have a hardened steel bushing inserted into the inner hub instead of a needle roller bearin g. Then, two needle roller bearings would be inserted into each side of the fork. Doing this should eliminate the wobble, and still allow the fork to rotate about the small hole in the inner hub. Set screws would be used to keep the dowel pin from sliding out of the fork. See Figure 40 and 41 below.
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60 Figure 40: Inner Hub ReDesign With Hardened Stain less Steel Bushing, and a Second CutOut for the Silicone Rubber Figure 41: Fork ReDesign Needle Roller Bearings are Inserted Into Either Side of the Fork
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61 7.2.2 Polyurethane Issues Another problem that was discovered is that when the polyurethane is inserted into the inner hub, the fork rotates upward with respect to the inner hub, and the bolt is no longer at the center of the wheel. See Figure 42. Figure 42: The Polyurethane Causes the Fork to Rota te Upward When there is No One in the Wheelchair This happens because the polyurethane is oversized so that when the wheelchair user sit s in the chair, the fork/bolt will return to center of the wheel. See Figure 43 below.
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62 Figure 43: Suspension System with Someone Sitting i n the Wheelchair However, when the user gets out of the chair, the wheel becomes uncentered again, and the wheelchair brakes are unable to grip the wheel. In order to keep the bolt at the cent er of the wheel, another cutout should be made in the inner hub and a piece of silicone rubber should be inserted. Figure 40, from a few pages ago, shows this second cutout. A good option for the silicone rubber would be a silicone with a 60 ShoreA durometer. This is stiffer than the 40 ShoreA durometer polyurethane that is used under the fork. The stiffer silicone will be able to keep the bolt centered in the wheel, becaus e it will not be compressed by the force of the polyurethane. The 60 ShoreA Silicone wa s chosen over a 60 ShoreA Polyurethane because the Silicon is orange, and the
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63 polyurethane is black. This will prevent the wheel from being installed upside down. For a picture of the modified suspension system, see Figure 44 below. Figure 44: ReDesigned Suspension System Also of concern is the ability of the polyurethane slip out of place. Figure 42 shows that if the Polyurethane is simply squished between the fork and the inner hub, the only thing preventing it from slipping out is the compression of the cylinder, and the friction between the cylinder, fork, and inner hub. To prevent this from occurring, a collar was made for the Polyurethane. This collar can be seen on the bottom of the
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64 polyurethane in Figure 42. Also, to prevent the Polyurethane from slipping off the back of the fork, the fork should not be rounded at the back. See Figure 44 for a model of a fork that is not rounded at the back. Even though the inner hub was modified, the FEA results from the original model were considered sufficient. This is because the stainless steel bushing is t he same size as the needle roller bearing, and the top cutout will have the same stress contour as the bottom cutout, due to symmetry. Since section 6.3 showed that the bottom cutout was not even close to failure, there is no need to run a new analysis. Figure 46 is an overall picture of the aftermarket suspension system on a wheelchair wheel, and Figure 47 is a picture of the suspension system installed on the authorÂ’s wheelchair. Figure 45: Overall Picture of AfterMarket Suspensi on System
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65 Figure 46: AfterMarket Suspension System on Author Â’s Wheelchair
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66 8. Conclusions This thesis has shown a successful design for an aftermarket suspension syst em for the rear wheels of wheelchair. The analysis showed that the suspension s ystem should not fail when subjected to 10 times the static load, which was considered large enough to encompass the forces that a wheelchair wheel is typically subjecte d to. The modifications that were made to the prototype should be sufficient to eliminate the wobble in the suspension system. There is room for further work in the area of weight reduction, and in the use of the suspension system on steeper wheel cambers. Further study should also be done on the Polyurethane to determine which shape and durometer provides the most shock and vibration reduction. It would also be advisable to perform a doubledrum and a curbdrop test on the suspension system to determine how durable it is. It can be seen where failure takes place, and the sy stem can be strengthened.
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67 References 1. Cooper, Rory. Rehabilitation Engineering Applied to Mobility and Manipulation. Philadelphia PA: Institute of Physics Publishing Bristol and Philadelphia, 1995. Pages 115116, 255256. 2. Kwarciak, Cooper, Ammer, Fitzgerald, Boninger, Cooper. Â“Fatigue Testing of Selected Suspension Manual Wheelchairs Using ANSI/RESNA Standards.Â” Archives of Physical Medicine and Rehabilitation, Volume 86, Issue 1, January 2005, Pages 123129. 3. Frog Legs. Accessed 12707, http://www.froglegsinc.com/ultrasports.php?bl ack. 4. Ashby, Mike, and Johnson, Kara. Materials and Design, The art and science of Material Selection in Product Design. Woburn, MA: ButterworthHeinemann, 2002. Pages 179182. 5. Fitzgerald, Cooper, Boninger, Rentschler. Â“Comparison of Fatigue Life for 3 Types of Manual wheelchairs.Â” Archives of Physical Medicine and Rehabilit ation Volume 82, Issue 10, October 2001, Pages 14841488. 6. Silverthin Selection Guide. Accessed 12707, http://www.silverthin.com/1select.htm. 7. Silverthin Precision Thin Section Bearings. Accessed 12707, http://www.silverthin.com/5sa.htm 8. McMasterCarr Supply Company. Accessed 12707, http://www.mcmaster.com. 9. Toogood, Roger. ProEngineer Wildfire 3.0 Mechanica Tutoril. Edmonton, Alberta: Schroff Development Corporation, 2006. Pages 219.
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68 10. Adams, Vince, and Askenazi, Abraham. Building Better Products With Finite Element Analysis. Sante Fe, NM: OnWord Press, 1998. Pages 5962, 97. 11. Ansel C. Ugural, and Saul K. Fenster. Advanced Strength And Applied Elasticity, 3 rd Ed. Prentice Hall, 1995. Upper Saddle River, NJ. Pages 172175. 12. Wheelchair camber information. Accessed 12707, http://www.spinlife.com/InvacareTopEndTerminatorTitaniumTitanium Wheelchair/spec.cfm?productID=69887.
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69 Appendices
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70 Appendix A: Detailed Drawings of the Fork, Inner Hub, and Outer Hub Figure 47: Fork DrawingÂ– Isometric View
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71 Appendix A: (Continued) Figure 48: Fork DrawingÂ– Front View Figure 49: Fork DrawingÂ– Top View
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72 Appendix A: (Continued) Figure 50: Inner Hub DrawingÂ– Isometric View
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73 Appendix A: (Continued) Figure 51: Inner Hub DrawingÂ– Front View Figure 52: Inner Hub DrawingÂ– Side View
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74 Appendix A: (Continued) Figure 53: Outer Hub DrawingÂ– Isometric View
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75 Appendix A: (Continued) Figure 54: Outer Hub DrawingÂ– Front View
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76 Appendix A: (Continued) Figure 55: Outer Hub DrawingÂ– Side View Figure 56: Outer Hub DrawingÂ– Top View
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77 Appendix B: Rubber and Foam Comparison Chart From McMasterCarr Resistance to: Material Oil Abrasion Tearing Impact Weather Chemicals Electricity Flame BunaN Excellent Good Fair Fair Poor Fair Poor Poor Butyl Poor Good Good Fair Good Not Rated Excellent Poor ECH Excellent Good Fair Fair Good Good Good Poor EPDM Poor Good Poor Fair Excellent Good Fair Poor EVA Good Good Good Excellent Good Good Good Fair Gum Poor Excellent Good Excellent Fair Fair Excellent Poor Hypalon Fair Good Fair Fair Excellent Good Good Good Ionomer Excellent Excellent Excellent Excellent Excellent Excellent Good Good Latex Poor Excellent Excellent Excellent Fair Good Excellent Poor Neoprene Good Good Fair Good Good Fair Fair Good Polyethylene Good Good Excellent Excellent Good Good Fair Fair Polyimide Excellent Poor Poor Poor Poor Excellent Excellent Excellent Polyurethane Excellent Excellent Excellent Excellent Good Good Good Poor Santoprene Fair Good Fair Good Excellent Fair Fair Poor SBR Poor Good Good Excellent Fair Poor Poor Poor Silicone Fair Poor Poor Fair Excellent Fair Good Fair Vinyl Good Fair Fair Good Good Fair Not Rated Poor Viton Excellent Good Poor Poor Good Good Good Excellent Copyright 2006 All rights reserved. Figure 57: Comparison of Rubber and Foam Chart
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78 Appendix C: Fork and Bolt Analysis Â– 20 Degree Camber This is the Â“run statusÂ” output file for the ProMechanica analysis of the For k and Bolt analysis. A camber of 20 degrees was used, 10 times the static load was applied, and t he convergence was set to 10%. Mechanica Structure Version K0141:spg Summary for Design Study "ten_x_static_load_near_fork_1" Thu Jan 25, 2007 16:05:34 Run Settings Memory allocation for block solver: 128.0 Checking the model before creating elements... These checks take into account the fact that AutoGEM will automatically create elements in volumes with material properties, on surfaces with shell properties, and on curves with beam section properties. Generate elements automatically. Checking the model after creating elements... No errors were found in the model. Mechanica Structure Model Summary Principal System of Units: Inch Pound Second (IPS) Length: in Force: lbf Time: sec Temperature: F Model Type: Three Dimensional
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79 Appendix C: (Continued) Points: 265 Edges: 1107 Faces: 1423 Springs: 0 Masses: 0 Beams: 0 Shells: 0 Solids: 582 Elements: 582 Contact Regions: 3 Standard Design Study Description: 10% convergence 1080 lbs normal 390 lbs transverse Static Analysis "ten_x_static_load_near_fork_1": Contact Analysis Convergence Method: MultiplePass Adaptive Plotting Grid: 4 Convergence Loop Log: (16:05:43) >> Pass 1 << Calculating Element Equations (16:05:43)
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80 Appendix C: (Continued) Total Number of Equations: 630 Maximum Edge Order: 1 Solving Equations (16:05:44) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:05:45) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.21210e+00 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:05:54) PostProcessing Solution (16:05:55) Checking Convergence (16:05:55) Elements Not Converged: 582 Edges Not Converged: 1107 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 100.0% Resource Check (16:05:56) Elapsed Time (sec): 22.18 CPU Time (sec): 20.67 Memory Usage (kb): 192486 Wrk Dir Dsk Usage (kb): 5131
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81 Appendix C: (Continued) >> Pass 2 << Calculating Element Equations (16:05:56) Total Number of Equations: 3579 Maximum Edge Order: 2 Solving Equations (16:05:56) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:05:59) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.63034e+00 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:06:16) PostProcessing Solution (16:06:18) Checking Convergence (16:06:18) Elements Not Converged: 359 Edges Not Converged: 824 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 73.9% Resource Check (16:06:18) Elapsed Time (sec): 44.36 CPU Time (sec): 42.59 Memory Usage (kb): 192486 Wrk Dir Dsk Usage (kb): 6155
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82 Appendix C: (Continued) >> Pass 3 << Calculating Element Equations (16:06:18) Total Number of Equations: 11109 Maximum Edge Order: 4 Solving Equations (16:06:18) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:06:33) Load Increment 1 of 1 Load Factor: 1.00000e+00 Contact Area: 1.77322e+00 Calculating Disp and Stress Results (16:07:05) PostProcessing Solution (16:07:07) Checking Convergence (16:07:07) Elements Not Converged: 210 Edges Not Converged: 260 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 32.6% Resource Check (16:07:07) Elapsed Time (sec): 93.42 CPU Time (sec): 91.11 Memory Usage (kb): 193634 Wrk Dir Dsk Usage (kb): 16395 >> Pass 4 << Calculating Element Equations (16:07:07) Total Number of Equations: 22602 Maximum Edge Order: 4 Solving Equations (16:07:09) Load Increment 0 of 1 Load Factor: 0.00000e+00
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83 Appendix C: (Continued) Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:07:36) Load Increment 1 of 1 Load Factor: 1.00000e+00 Contact Area: 1.78534e+00 Calculating Disp and Stress Results (16:09:33) PostProcessing Solution (16:09:34) Checking Convergence (16:09:34) Elements Not Converged: 30 Edges Not Converged: 123 Local Disp/Energy Index: 26.7% Global RMS Stress Index: 15.5% Resource Check (16:09:35) Elapsed Time (sec): 241.36 CPU Time (sec): 236.61 Memory Usage (kb): 197829 Wrk Dir Dsk Usage (kb): 37899 >> Pass 5 << Calculating Element Equations (16:09:35) Total Number of Equations: 36231 Maximum Edge Order: 5 Solving Equations (16:09:41) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:11:08) Load Increment 1 of 1 Load Factor: 1.00000e+00 Contact Area: 1.79261e+00 Calculating Disp and Stress Results (16:14:05)
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84 Appendix C: (Continued) PostProcessing Solution (16:14:07) Checking Convergence (16:14:07) Elements Not Converged: 1 Edges Not Converged: 0 Local Disp/Energy Index: 10.3% Global RMS Stress Index: 8.4% Resource Check (16:14:08) Elapsed Time (sec): 514.59 CPU Time (sec): 458.59 Memory Usage (kb): 205761 Wrk Dir Dsk Usage (kb): 219147 >> Pass 6 << Calculating Element Equations (16:14:08) Total Number of Equations: 45030 Maximum Edge Order: 6 Solving Equations (16:14:15) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:15:51) Load Increment 1 of 1 Load Factor: 1.00000e+00 Contact Area: 1.79752e+00 Calculating Disp and Stress Results (16:19:58) PostProcessing Solution (16:20:25) Checking Convergence (16:20:25) Elements Not Converged: 0 Edges Not Converged: 0 Local Disp/Energy Index: 4.3% Global RMS Stress Index: 4.8%
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85 Appendix C: (Continued) RMS Stress Error Estimates: Load Set Stress Error % of Max Prin Str LoadSet1 1.87e+03 9.6% of 1.95e+04 Resource Check (16:20:29) Elapsed Time (sec): 895.76 CPU Time (sec): 739.63 Memory Usage (kb): 226079 Wrk Dir Dsk Usage (kb): 299019 The analysis converged to within 10% on edge displacement, element strain energy, and global RMS stress. Total Mass of Model: 1.371139e03 Total Cost of Model: 0.000000e+00 Mass Moments of Inertia about WCS Origin: Ixx: 8.64826e04 Ixy: 1.74899e09 Iyy: 1.50782e03 Ixz: 5.27724e06 Iyz: 8.79483e10 Izz: 8.21515e04 Principal MMOI and Principal Axes Relative to WCS Origin: Max Prin Mid Prin Min Prin 1.50782e03 8.65460e04 8.20881e04 WCS X: 2.73079e06 9.92867e01 1.19230e01 WCS Y: 1.00000e+00 2.86660e06 9.67599e07
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86 Appendix C: (Continued) WCS Z: 1.30248e06 1.19230e01 9.92867e01 Center of Mass Location Relative to WCS Origin: ( 4.48315e01, 5.37019e06, 8.40699e04) Mass Moments of Inertia about the Center of Mass: Ixx: 8.64825e04 Ixy: 1.55207e09 Iyy: 1.23223e03 Ixz: 4.76046e06 Iyz: 8.85674e10 Izz: 5.45935e04 Principal MMOI and Principal Axes Relative to COM: Max Prin Mid Prin Min Prin 1.23223e03 8.64896e04 5.45864e04 WCS X: 4.20804e06 9.99889e01 1.49232e02 WCS Y: 1.00000e+00 4.18875e06 1.32397e06 WCS Z: 1.26132e06 1.49232e02 9.99889e01 Constraint Set: ConstraintSet1 Load Set: LoadSet1 Resultant Load on Model: in global X direction: 2.047121e10 in global Y direction: 1.080000e+03 in global Z direction: 3.900000e+02
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87 Appendix C: (Continued) Measures: Name Value Convergence contact_area: 1.797523e+00 0.3% contact_max_pres: 1.944910e+04 11.1% max_beam_bending: 0.000000e+00 0.0% max_beam_tensile: 0.000000e+00 0.0% max_beam_torsion: 0.000000e+00 0.0% max_beam_total: 0.000000e+00 0.0% max_disp_mag: 9.808449e03 1.9% max_disp_x: 9.196215e03 2.0% max_disp_y: 9.797444e03 1.9% max_disp_z: 9.702102e04 0.2% max_prin_mag: 1.945152e+04 11.1% max_rot_mag: 0.000000e+00 0.0% max_rot_x: 0.000000e+00 0.0% max_rot_y: 0.000000e+00 0.0% max_rot_z: 0.000000e+00 0.0% max_stress_prin: 1.665415e+04 2.1% max_stress_vm: 3.092423e+04 4.9% max_stress_xx: 1.397394e+04 1.1% max_stress_xy: 1.755868e+04 4.6% max_stress_xz: 4.280469e+03 0.4% max_stress_yy: 1.495614e+04 3.7% max_stress_yz: 7.995832e+03 22.4% max_stress_zz: 1.558699e+04 0.3% min_stress_prin: 1.945152e+04 11.1% strain_energy: 1.752524e+00 0.2% cntRgn_001cntArea: 9.684937e01 0.0% cntRgn_001maxPres: 4.284050e+03 4.6% cntRgn_002cntArea: 5.836132e01 0.8% cntRgn_002maxPres: 1.944910e+04 11.1% cntRgn_003cntArea: 2.454163e01 0.0%
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88 Appendix C: (Continued) cntRgn_003maxPres: 4.686339e+03 1.3% cntRgn_004cntArea: 9.684937e01 0.0% cntRgn_004maxPres: 4.284050e+03 4.6% cntRgn_005cntArea: 9.684937e01 0.0% cntRgn_005maxPres: 4.284050e+03 4.6% cntRgn_006cntArea: 5.836132e01 0.8% cntRgn_006maxPres: 1.944910e+04 11.1% Analysis "ten_x_static_load_near_fork_1" Completed (16:20:30) Memory and Disk Usage: Machine Type: Windows NT/x86 RAM Allocation for Solver (megabytes): 128.0 Total Elapsed Time (seconds): 898.76 Total CPU Time (seconds): 740.02 Maximum Memory Usage (kilobytes): 226079 Working Directory Disk Usage (kilobytes): 299019 Results Directory Size (kilobytes): 8919 .\ten_x_static_load_near_fork_1 Maximum Data Base Working File Sizes (kilobytes): 20480 .\ten_x_static_load_near_fork_1.tmp\gapel1.bas 198656 .\ten_x_static_load_near_fork_1.tmp\kblk1.bas 69632 .\ten_x_static_load_near_fork_1.tmp\kel1.bas 1024 .\ten_x_static_load_near_fork_1.tmp\l1da1.bas 1024 .\ten_x_static_load_near_fork_1.tmp\l2sq1.bas 8192 .\ten_x_static_load_near_fork_1.tmp\oel1.bas Run Completed Thu Jan 25, 2007 16:20:32
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89 Appendix D: Fork and Bolt Analysis Â– 3 Degree Camber This is the Â“run statusÂ” output file for the ProMechanica analysis of the For k and Bolt analysis. A camber of 3 degrees was used, 10 times the static load was applie d, and the convergence was set to 10%. Mechanica Structure Version K0141:spg Summary for Design Study "ten_times_static_load_near_fork" Thu Jan 25, 2007 15:43:43 Run Settings Memory allocation for block solver: 128.0 Checking the model before creating elements... These checks take into account the fact that AutoGEM will automatically create elements in volumes with material properties, on surfaces with shell properties, and on curves with beam section properties. Generate elements automatically. Checking the model after creating elements... No errors were found in the model. Mechanica Structure Model Summary Principal System of Units: Inch Pound Second (IPS) Length: in Force: lbf Time: sec Temperature: F Model Type: Three Dimensional
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90 Appendix D: (Continued) Points: 265 Edges: 1107 Faces: 1423 Springs: 0 Masses: 0 Beams: 0 Shells: 0 Solids: 582 Elements: 582 Contact Regions: 3 Standard Design Study Description: 10% convergence Static Analysis "ten_times_static_load_near_fork": Contact Analysis Convergence Method: MultiplePass Adaptive Plotting Grid: 4 Convergence Loop Log: (15:43:52) >> Pass 1 << Calculating Element Equations (15:43:53) Total Number of Equations: 630 Maximum Edge Order: 1
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91 Appendix D: (Continued) Solving Equations (15:43:53) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (15:43:54) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.30032e+00 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (15:44:05) PostProcessing Solution (15:44:06) Checking Convergence (15:44:06) Elements Not Converged: 582 Edges Not Converged: 1107 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 100.0% Resource Check (15:44:06) Elapsed Time (sec): 24.23 CPU Time (sec): 21.52 Memory Usage (kb): 193510 Wrk Dir Dsk Usage (kb): 5131 >> Pass 2 << Calculating Element Equations (15:44:06) Total Number of Equations: 3579
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92 Appendix D: (Continued) Maximum Edge Order: 2 Solving Equations (15:44:06) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (15:44:09) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.56700e+00 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (15:44:35) PostProcessing Solution (15:44:37) Checking Convergence (15:44:37) Elements Not Converged: 353 Edges Not Converged: 825 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 74.8% Resource Check (15:44:37) Elapsed Time (sec): 55.17 CPU Time (sec): 51.48 Memory Usage (kb): 193510 Wrk Dir Dsk Usage (kb): 6155 >> Pass 3 << Calculating Element Equations (15:44:37)
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93 Appendix D: (Continued) Total Number of Equations: 11070 Maximum Edge Order: 4 Solving Equations (15:44:37) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (15:44:53) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.67904e+00 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (15:45:41) PostProcessing Solution (15:45:42) Checking Convergence (15:45:42) Elements Not Converged: 209 Edges Not Converged: 245 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 32.9% Resource Check (15:45:42) Elapsed Time (sec): 120.55 CPU Time (sec): 115.38 Memory Usage (kb): 195014 Wrk Dir Dsk Usage (kb): 16395
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94 Appendix D: (Continued) >> Pass 4 << Calculating Element Equations (15:45:42) Total Number of Equations: 22146 Maximum Edge Order: 4 Solving Equations (15:45:44) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (15:46:10) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.70496e+00 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (15:47:43) PostProcessing Solution (15:47:45) Checking Convergence (15:47:45) Elements Not Converged: 29 Edges Not Converged: 111 Local Disp/Energy Index: 24.5% Global RMS Stress Index: 15.4% Resource Check (15:47:45) Elapsed Time (sec): 243.21 CPU Time (sec): 235.76 Memory Usage (kb): 198413 Wrk Dir Dsk Usage (kb): 36875
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95 Appendix D: (Continued) >> Pass 5 << Calculating Element Equations (15:47:45) Total Number of Equations: 35934 Maximum Edge Order: 5 Solving Equations (15:47:49) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (15:48:51) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.71726e+00 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (15:51:42) PostProcessing Solution (15:51:50) Checking Convergence (15:51:50) Elements Not Converged: 1 Edges Not Converged: 0 Local Disp/Energy Index: 10.2% Global RMS Stress Index: 8.7% Resource Check (15:51:52) Elapsed Time (sec): 490.11 CPU Time (sec): 450.92 Memory Usage (kb): 222102 Wrk Dir Dsk Usage (kb): 215051
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96 Appendix D: (Continued) >> Pass 6 << Calculating Element Equations (15:51:53) Total Number of Equations: 44889 Maximum Edge Order: 6 Solving Equations (15:52:10) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (15:53:46) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.72091e+00 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (15:57:57) PostProcessing Solution (15:58:05) Checking Convergence (15:58:05) Elements Not Converged: 0 Edges Not Converged: 0 Local Disp/Energy Index: 4.4% Global RMS Stress Index: 4.9%
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97 Appendix D: (Continued) RMS Stress Error Estimates: Load Set Stress Error % of Max Prin Str LoadSet1 1.99e+03 9.5% of 2.09e+04 Resource Check (15:58:09) Elapsed Time (sec): 866.86 CPU Time (sec): 718.91 Memory Usage (kb): 225934 Wrk Dir Dsk Usage (kb): 293899 The analysis converged to within 10% on edge displacement, element strain energy, and global RMS stress. Total Mass of Model: 1.371139e03 Total Cost of Model: 0.000000e+00 Mass Moments of Inertia about WCS Origin: Ixx: 8.64826e04 Ixy: 1.74899e09 Iyy: 1.50782e03 Ixz: 5.27724e06 Iyz: 8.79483e10 Izz: 8.21515e04 Principal MMOI and Principal Axes Relative to WCS Origin: Max Prin Mid Prin Min Prin 1.50782e03 8.65460e04 8.20881e04 WCS X: 2.73079e06 9.92867e01 1.19230e01 WCS Y: 1.00000e+00 2.86660e06 9.67599e07 WCS Z: 1.30248e06 1.19230e01 9.92867e01
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98 Appendix D: (Continued) Center of Mass Location Relative to WCS Origin: ( 4.48315e01, 5.37019e06, 8.40699e04) Mass Moments of Inertia about the Center of Mass: Ixx: 8.64825e04 Ixy: 1.55207e09 Iyy: 1.23223e03 Ixz: 4.76046e06 Iyz: 8.85674e10 Izz: 5.45935e04 Principal MMOI and Principal Axes Relative to COM: Max Prin Mid Prin Min Prin 1.23223e03 8.64896e04 5.45864e04 WCS X: 4.20804e06 9.99889e01 1.49232e02 WCS Y: 1.00000e+00 4.18875e06 1.32397e06 WCS Z: 1.26132e06 1.49232e02 9.99889e01 Constraint Set: ConstraintSet1 Load Set: LoadSet1 Resultant Load on Model: in global X direction: 1.577994e10 in global Y direction: 1.150000e+03 in global Z direction: 6.000000e+01 Measures: Name Value Convergence contact_area: 1.720907e+00 0.2% contact_max_pres: 2.090662e+04 10.1%
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99 Appendix D: (Continued) max_beam_bending: 0.000000e+00 0.0% max_beam_tensile: 0.000000e+00 0.0% max_beam_torsion: 0.000000e+00 0.0% max_beam_total: 0.000000e+00 0.0% max_disp_mag: 1.306670e02 1.8% max_disp_x: 1.237034e02 1.9% max_disp_y: 1.305403e02 1.8% max_disp_z: 7.257396e04 0.2% max_prin_mag: 2.090933e+04 10.1% max_rot_mag: 0.000000e+00 0.0% max_rot_x: 0.000000e+00 0.0% max_rot_y: 0.000000e+00 0.0% max_rot_z: 0.000000e+00 0.0% max_stress_prin: 1.777704e+04 2.0% max_stress_vm: 3.304002e+04 5.0% max_stress_xx: 1.494734e+04 1.1% max_stress_xy: 1.876216e+04 4.8% max_stress_xz: 3.496715e+03 23.7% max_stress_yy: 1.595143e+04 1.7% max_stress_yz: 8.546310e+03 26.0% max_stress_zz: 1.520768e+04 1.8% min_stress_prin: 2.090933e+04 10.1% strain_energy: 1.905957e+00 0.2% cntRgn_001cntArea: 1.036548e+00 0.0% cntRgn_001maxPres: 4.553970e+03 5.5% cntRgn_002cntArea: 5.613023e01 0.6% cntRgn_002maxPres: 2.090662e+04 10.1% cntRgn_003cntArea: 1.230561e01 0.2% cntRgn_003maxPres: 1.927968e+03 0.1% cntRgn_004cntArea: 1.036548e+00 0.0% cntRgn_004maxPres: 4.553970e+03 5.5% cntRgn_005cntArea: 1.036548e+00 0.0% cntRgn_005maxPres: 4.553970e+03 5.5%
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100 Appendix D: (Continued) cntRgn_006cntArea: 5.613023e01 0.6% cntRgn_006maxPres: 2.090662e+04 10.1% Analysis "ten_times_static_load_near_fork" Completed (15:58:09) Memory and Disk Usage: Machine Type: Windows NT/x86 RAM Allocation for Solver (megabytes): 128.0 Total Elapsed Time (seconds): 867.41 Total CPU Time (seconds): 719.30 Maximum Memory Usage (kilobytes): 225934 Working Directory Disk Usage (kilobytes): 293899 Results Directory Size (kilobytes): 8908 .\ten_times_static_load_near_fork Maximum Data Base Working File Sizes (kilobytes): 19456 .\ten_times_static_load_near_fork.tmp\gapel1.bas 194560 .\ten_times_static_load_near_fork.tmp\kblk1.bas 69632 .\ten_times_static_load_near_fork.tmp\kel1.bas 1024 .\ten_times_static_load_near_fork.tmp\l1da1.bas 1024 .\ten_times_static_load_near_fork.tmp\l2sq1.bas 8192 .\ten_times_static_load_near_fork.tmp\oel1.bas Run Completed Thu Jan 25, 2007 15:58:09
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101 Appendix E: Inner Hub and Pin Analysis Â– 3 Degrees Camber This is the Â“run statusÂ” output file for the ProMechanica analysis of the In ner Hub and Pin analysis. A camber of 3 degrees was used, 10 times the static load was appli ed, and the convergence was set to 10%. This is without local mesh refinement. Mechanica Structure Version K0141:spg Summary for Design Study "ih_and_big_fixed_pin_10_x_two_c" Tue Jan 16, 2007 16:16:21 Run Settings Memory allocation for block solver: 128.0 Checking the model before creating elements... These checks take into account the fact that AutoGEM will automatically create elements in volumes with material properties, on surfaces with shell properties, and on curves with beam section properties. Generate elements automatically. Checking the model after creating elements... No errors were found in the model. Mechanica Structure Model Summary Principal System of Units: Inch Pound Second (IPS) Length: in Force: lbf Time: sec Temperature: F
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102 Appendix E: (Continued) Model Type: Three Dimensional Points: 225 Edges: 961 Faces: 1253 Springs: 0 Masses: 0 Beams: 0 Shells: 0 Solids: 517 Elements: 517 Contact Regions: 2 Standard Design Study Description: I used contact "surfaces" (4 total), instead of contac t "part" (about 12 total) Static Analysis "ih_and_big_fixed_pin_10_x_two_c": Contact Analysis Convergence Method: MultiplePass Adaptive Plotting Grid: 4
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103 Appendix E: (Continued) Convergence Loop Log: (16:16:25) >> Pass 1 << Calculating Element Equations (16:16:25) Total Number of Equations: 607 Maximum Edge Order: 1 Solving Equations (16:16:25) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:16:26) Load Increment 1 of 1 Load Factor: 1.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:16:27) PostProcessing Solution (16:16:28) Checking Convergence (16:16:28) Elements Not Converged: 517 Edges Not Converged: 961 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 100.0% Resource Check (16:16:28) Elapsed Time (sec): 8.62 CPU Time (sec): 6.11 Memory Usage (kb): 185502 Wrk Dir Dsk Usage (kb): 4098 >> Pass 2 << Calculating Element Equations (16:16:28) Total Number of Equations: 3336 Maximum Edge Order: 2 Solving Equations (16:16:28)
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104 Appendix E: (Continued) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:16:29) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.07992e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:16:35) PostProcessing Solution (16:16:36) Checking Convergence (16:16:36) Elements Not Converged: 353 Edges Not Converged: 254 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 87.9% Resource Check (16:16:36) Elapsed Time (sec): 17.26 CPU Time (sec): 14.44 Memory Usage (kb): 186590 Wrk Dir Dsk Usage (kb): 4098 >> Pass 3 << Calculating Element Equations (16:16:36) Total Number of Equations: 9955 Maximum Edge Order: 4
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105 Appendix E: (Continued) Solving Equations (16:16:37) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:16:39) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.57080e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:16:48) PostProcessing Solution (16:16:49) Checking Convergence (16:16:49) Elements Not Converged: 270 Edges Not Converged: 18 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 47.7% Resource Check (16:16:49) Elapsed Time (sec): 29.84 CPU Time (sec): 26.25 Memory Usage (kb): 195934 Wrk Dir Dsk Usage (kb): 10242 >> Pass 4 << Calculating Element Equations (16:16:49) Total Number of Equations: 19819
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106 Appendix E: (Continued) Maximum Edge Order: 5 Solving Equations (16:16:51) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:16:56) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 2.25802e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:17:17) PostProcessing Solution (16:17:18) Checking Convergence (16:17:18) Elements Not Converged: 94 Edges Not Converged: 0 Local Disp/Energy Index: 37.2% Global RMS Stress Index: 25.5% Resource Check (16:17:19) Elapsed Time (sec): 59.63 CPU Time (sec): 54.63 Memory Usage (kb): 197534 Wrk Dir Dsk Usage (kb): 23554
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107 Appendix E: (Continued) >> Pass 5 << Calculating Element Equations (16:17:19) Total Number of Equations: 34342 Maximum Edge Order: 6 Solving Equations (16:17:24) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:17:39) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 3.33794e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:18:38) PostProcessing Solution (16:18:40) Checking Convergence (16:18:40) Elements Not Converged: 17 Edges Not Converged: 0 Local Disp/Energy Index: 17.5% Global RMS Stress Index: 16.0% Resource Check (16:18:41) Elapsed Time (sec): 141.36 CPU Time (sec): 133.28 Memory Usage (kb): 202301 Wrk Dir Dsk Usage (kb): 54274
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108 Appendix E: (Continued) >> Pass 6 << Calculating Element Equations (16:18:41) Total Number of Equations: 53481 Maximum Edge Order: 7 Solving Equations (16:18:53) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:19:38) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 3.43612e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:21:43) PostProcessing Solution (16:21:46) Checking Convergence (16:21:46) Elements Not Converged: 1 Edges Not Converged: 0 Local Disp/Energy Index: 10.0% Global RMS Stress Index: 11.3% Resource Check (16:21:47) Elapsed Time (sec): 328.22 CPU Time (sec): 263.38 Memory Usage (kb): 226922 Wrk Dir Dsk Usage (kb): 296962
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109 Appendix E: (Continued) >> Pass 7 << Calculating Element Equations (16:21:47) Total Number of Equations: 74534 Maximum Edge Order: 8 Solving Equations (16:22:18) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:24:07) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 4.61421e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:32:17) PostProcessing Solution (16:33:15) Checking Convergence (16:33:15) Elements Not Converged: 0 Edges Not Converged: 0 Local Disp/Energy Index: 7.0% Global RMS Stress Index: 8.6%
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110 Appendix E: (Continued) RMS Stress Error Estimates: Load Set Stress Error % of Max Prin Str LoadSet1 3.75e+02 0.8% of 4.61e+04 Resource Check (16:33:27) Elapsed Time (sec): 1027.84 CPU Time (sec): 594.52 Memory Usage (kb): 238822 Wrk Dir Dsk Usage (kb): 498690 The analysis converged to within 10% on edge displacement, element strain energy, and global RMS stress. Total Mass of Model: 1.023137e02 Total Cost of Model: 0.000000e+00 Mass Moments of Inertia about WCS Origin: Ixx: 4.63460e01 Ixy: 2.21914e08 Iyy: 7.85365e03 Ixz: 2.07545e09 Iyz: 4.77616e09 Izz: 4.64919e01 Principal MMOI and Principal Axes Relative to WCS Origin: Max Prin Mid Prin Min Prin 4.64919e01 4.63460e01 7.85365e03 WCS X: 1.42221e06 1.00000e+00 4.87076e08 WCS Y: 1.04497e08 4.87075e08 1.00000e+00 WCS Z: 1.00000e+00 1.42221e06 1.04496e08
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111 Appendix E: (Continued) Center of Mass Location Relative to WCS Origin: ( 5.94321e02, 1.12547e02, 2.40077e07) Mass Moments of Inertia about the Center of Mass: Ixx: 4.63458e01 Ixy: 6.82150e06 Iyy: 7.81751e03 Ixz: 2.22144e09 Iyz: 4.74851e09 Izz: 4.64882e01 Principal MMOI and Principal Axes Relative to COM: Max Prin Mid Prin Min Prin 4.64882e01 4.63458e01 7.81751e03 WCS X: 1.56085e06 1.00000e+00 1.49712e05 WCS Y: 1.03659e08 1.49712e05 1.00000e+00 WCS Z: 1.00000e+00 1.56085e06 1.03892e08 Constraint Set: ConstraintSet1 Load Set: LoadSet1 Resultant Load on Model: in global X direction: 9.346590e11 in global Y direction: 4.433882e10 in global Z direction: 6.000000e+01 Measures: Name Value Convergence contact_area: 4.614214e02 25.5% contact_max_pres: 4.244370e+04 7.6% max_beam_bending: 0.000000e+00 0.0%
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112 Appendix E: (Continued) max_beam_tensile: 0.000000e+00 0.0% max_beam_torsion: 0.000000e+00 0.0% max_beam_total: 0.000000e+00 0.0% max_disp_mag: 7.590963e02 0.7% max_disp_x: 2.286037e03 0.6% max_disp_y: 6.997755e03 0.6% max_disp_z: 7.571832e02 0.7% max_prin_mag: 4.610517e+04 2.6% max_rot_mag: 0.000000e+00 0.0% max_rot_x: 0.000000e+00 0.0% max_rot_y: 0.000000e+00 0.0% max_rot_z: 0.000000e+00 0.0% max_stress_prin: 2.584570e+04 14.0% max_stress_vm: 3.145544e+04 1.6% max_stress_xx: 2.418541e+04 2.4% max_stress_xy: 1.009556e+04 11.7% max_stress_xz: 7.840168e+03 2.1% max_stress_yy: 4.244165e+04 9.2% max_stress_yz: 9.826774e+03 21.6% max_stress_zz: 1.849277e+04 8.1% min_stress_prin: 4.610517e+04 2.6% strain_energy: 2.117846e+00 0.7% cntRgn_009cntArea: 2.945243e02 30.0% cntRgn_009maxPres: 3.565886e+04 1.6% cntRgn_010cntArea: 1.668971e02 17.6% cntRgn_010maxPres: 4.244370e+04 7.6% Analysis "ih_and_big_fixed_pin_10_x_two_c" Completed (16:33:28) 
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113 Appendix E: (Continued) Memory and Disk Usage: Machine Type: Windows NT/x86 RAM Allocation for Solver (megabytes): 128.0 Total Elapsed Time (seconds): 1028.37 Total CPU Time (seconds): 594.88 Maximum Memory Usage (kilobytes): 238822 Working Directory Disk Usage (kilobytes): 498690 Results Directory Size (kilobytes): 10482 .\ih_and_big_fixed_pin_10_x_two_c Maximum Data Base Working File Sizes (kilobytes): 1024 .\ih_and_big_fixed_pin_10_x_two_c.tmp\gapel1.bas 305152 .\ih_and_big_fixed_pin_10_x_two_c.tmp\kblk1.bas 169984 .\ih_and_big_fixed_pin_10_x_two_c.tmp\kel1.bas 2048 .\ih_and_big_fixed_pin_10_x_two_c.tmp\l1da1.bas 1024 .\ih_and_big_fixed_pin_10_x_two_c.tmp\l2sq1.bas 19456 .\ih_and_big_fixed_pin_10_x_two_c.tmp\oel1.bas Run Completed Tue Jan 16, 2007 16:33:28
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114 Appendix F: Inner Hub and Pin Analysis Â– 3 Degree Camber Â– With Local Mesh Refinement This is the Â“run statusÂ” output file for the ProMechanica analysis of the In ner Hub and Pin analysis. A camber of 3 degrees was used, 10 times the static load was appli ed, and the convergence was set to 10%. This is with local mesh refinement (did not help) Mechanica Structure Version K0141:spg Summary for Design Study "ih_bfp_ten_x" Tue Jan 16, 2007 16:46:06 Run Settings Memory allocation for block solver: 128.0 Checking the model before creating elements... These checks take into account the fact that AutoGEM will automatically create elements in volumes with material properties, on surfaces with shell properties, and on curves with beam section properties. Generate elements automatically. Checking the model after creating elements... No errors were found in the model. Mechanica Structure Model Summary Principal System of Units: Inch Pound Second (IPS) Length: in Force: lbf Time: sec Temperature: F 0
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115 Appendix F: (Continued) Model Type: Three Dimensional Points: 225 Edges: 961 Faces: 1253 Springs: 0 Masses: 0 Beams: 0 Shells: 0 Solids: 517 Elements: 517 Contact Regions: 2 Standard Design Study Description: ran with elements from local mech refinment of ih_bfp_ ten_x_two_contact_local_mesh_refin Static Analysis "ih_bfp_ten_x": Contact Analysis Convergence Method: MultiplePass Adaptive Plotting Grid: 4 Convergence Loop Log: (16:46:08)
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116 Appendix F: (Continued) >> Pass 1 << Calculating Element Equations (16:46:08) Total Number of Equations: 607 Maximum Edge Order: 1 Solving Equations (16:46:09) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:46:09) Load Increment 1 of 1 Load Factor: 1.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:46:10) PostProcessing Solution (16:46:11) Checking Convergence (16:46:11) Elements Not Converged: 517 Edges Not Converged: 961 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 100.0% Resource Check (16:46:11) Elapsed Time (sec): 5.88 CPU Time (sec): 4.33 Memory Usage (kb): 185566 Wrk Dir Dsk Usage (kb): 4098 >> Pass 2 << Calculating Element Equations (16:46:11) Total Number of Equations: 3336 Maximum Edge Order: 2 Solving Equations (16:46:11)
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117 Appendix F: (Continued) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:46:12) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.07992e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:46:18) PostProcessing Solution (16:46:19) Checking Convergence (16:46:19) Elements Not Converged: 353 Edges Not Converged: 254 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 87.9% Resource Check (16:46:19) Elapsed Time (sec): 14.30 CPU Time (sec): 12.61 Memory Usage (kb): 186654 Wrk Dir Dsk Usage (kb): 4098
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118 Appendix F: (Continued) >> Pass 3 << Calculating Element Equations (16:46:20) Total Number of Equations: 9955 Maximum Edge Order: 4 Solving Equations (16:46:20) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:46:23) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.57080e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:46:31) PostProcessing Solution (16:46:32) Checking Convergence (16:46:32) Elements Not Converged: 270 Edges Not Converged: 18 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 47.7% Resource Check (16:46:32) Elapsed Time (sec): 27.14 CPU Time (sec): 24.61 Memory Usage (kb): 196338 Wrk Dir Dsk Usage (kb): 10242
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119 Appendix F: (Continued) >> Pass 4 << Calculating Element Equations (16:46:32) Total Number of Equations: 19819 Maximum Edge Order: 5 Solving Equations (16:46:34) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:46:39) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 2.25802e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:46:59) PostProcessing Solution (16:47:01) Checking Convergence (16:47:01) Elements Not Converged: 94 Edges Not Converged: 0 Local Disp/Energy Index: 37.2% Global RMS Stress Index: 25.5% Resource Check (16:47:01)
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120 Appendix F: (Continued) Elapsed Time (sec): 55.87 CPU Time (sec): 52.94 Memory Usage (kb): 197598 Wrk Dir Dsk Usage (kb): 23554 >> Pass 5 << Calculating Element Equations (16:47:01) Total Number of Equations: 34342 Maximum Edge Order: 6 Solving Equations (16:47:06) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:47:20) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 3.33794e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:48:20) PostProcessing Solution (16:48:22) Checking Convergence (16:48:22) Elements Not Converged: 17 Edges Not Converged: 0
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121 Appendix F: (Continued) Local Disp/Energy Index: 17.5% Global RMS Stress Index: 16.0% Resource Check (16:48:22) Elapsed Time (sec): 137.05 CPU Time (sec): 131.58 Memory Usage (kb): 203389 Wrk Dir Dsk Usage (kb): 54274 >> Pass 6 << Calculating Element Equations (16:48:22) Total Number of Equations: 53481 Maximum Edge Order: 7 Solving Equations (16:48:35) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:49:20) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 3.43612e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (16:50:50) PostProcessing Solution (16:50:53)
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122 Appendix F: (Continued) Checking Convergence (16:50:53) Elements Not Converged: 1 Edges Not Converged: 0 Local Disp/Energy Index: 10.0% Global RMS Stress Index: 11.3% Resource Check (16:50:54) Elapsed Time (sec): 289.26 CPU Time (sec): 261.24 Memory Usage (kb): 228842 Wrk Dir Dsk Usage (kb): 296962 >> Pass 7 << Calculating Element Equations (16:50:55) Total Number of Equations: 74534 Maximum Edge Order: 8 Solving Equations (16:51:23) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (16:52:49) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 4.61421e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement.
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123 Appendix F: (Continued) Calculating Disp and Stress Results (16:59:30) PostProcessing Solution (16:59:51) Checking Convergence (16:59:51) Elements Not Converged: 0 Edges Not Converged: 0 Local Disp/Energy Index: 7.0% Global RMS Stress Index: 8.6% RMS Stress Error Estimates: Load Set Stress Error % of Max Prin Str LoadSet1 3.75e+02 0.8% of 4.61e+04 Resource Check (17:00:00) Elapsed Time (sec): 834.93 CPU Time (sec): 586.49 Memory Usage (kb): 239078 Wrk Dir Dsk Usage (kb): 498690 The analysis converged to within 10% on edge displacement, element strain energy, and global RMS stress. Total Mass of Model: 1.023137e02 Total Cost of Model: 0.000000e+00
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124 Appendix F: (Continued) Mass Moments of Inertia about WCS Origin: Ixx: 4.63460e01 Ixy: 2.21914e08 Iyy: 7.85365e03 Ixz: 2.07545e09 Iyz: 4.77616e09 Izz: 4.64919e01 Principal MMOI and Principal Axes Relative to WCS Origin: Max Prin Mid Prin Min Prin 4.64919e01 4.63460e01 7.85365e03 WCS X: 1.42221e06 1.00000e+00 4.87076e08 WCS Y: 1.04497e08 4.87075e08 1.00000e+00 WCS Z: 1.00000e+00 1.42221e06 1.04496e08 Center of Mass Location Relative to WCS Origin: ( 5.94321e02, 1.12547e02, 2.40077e07) Mass Moments of Inertia about the Center of Mass: Ixx: 4.63458e01 Ixy: 6.82150e06 Iyy: 7.81751e03 Ixz: 2.22144e09 Iyz: 4.74851e09 Izz: 4.64882e01 Principal MMOI and Principal Axes Relative to COM: Max Prin Mid Prin Min Prin 4.64882e01 4.63458e01 7.81751e03 WCS X: 1.56085e06 1.00000e+00 1.49712e05 WCS Y: 1.03659e08 1.49712e05 1.00000e+00 WCS Z: 1.00000e+00 1.56085e06 1.03892e08
PAGE 135
125 Appendix F: (Continued) Constraint Set: ConstraintSet1 Load Set: LoadSet1 Resultant Load on Model: in global X direction: 9.346590e11 in global Y direction: 4.433882e10 in global Z direction: 6.000000e+01 Measures: Name Value Convergence contact_area: 4.614214e02 25.5% contact_max_pres: 4.244370e+04 7.6% max_beam_bending: 0.000000e+00 0.0% max_beam_tensile: 0.000000e+00 0.0% max_beam_torsion: 0.000000e+00 0.0% max_beam_total: 0.000000e+00 0.0% max_disp_mag: 7.590963e02 0.7% max_disp_x: 2.286037e03 0.6% max_disp_y: 6.997755e03 0.6% max_disp_z: 7.571832e02 0.7% max_prin_mag: 4.610517e+04 2.6% max_rot_mag: 0.000000e+00 0.0% max_rot_x: 0.000000e+00 0.0% max_rot_y: 0.000000e+00 0.0% max_rot_z: 0.000000e+00 0.0% max_stress_prin: 2.584570e+04 14.0% max_stress_vm: 3.145544e+04 1.6% max_stress_xx: 2.418541e+04 2.4% max_stress_xy: 1.009556e+04 11.7%
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126 Appendix F: (Continued) max_stress_xz: 7.840168e+03 2.1% max_stress_yy: 4.244165e+04 9.2% max_stress_yz: 9.826774e+03 21.6% max_stress_zz: 1.849277e+04 8.1% min_stress_prin: 4.610517e+04 2.6% strain_energy: 2.117846e+00 0.7% cntRgn_009cntArea: 2.945243e02 30.0% cntRgn_009maxPres: 3.565886e+04 1.6% cntRgn_010cntArea: 1.668971e02 17.6% cntRgn_010maxPres: 4.244370e+04 7.6% Analysis "ih_bfp_ten_x" Completed (17:00:00) Memory and Disk Usage: Machine Type: Windows NT/x86 RAM Allocation for Solver (megabytes): 128.0 Total Elapsed Time (seconds): 835.28 Total CPU Time (seconds): 586.77 Maximum Memory Usage (kilobytes): 239078 Working Directory Disk Usage (kilobytes): 498690 Results Directory Size (kilobytes): 10475 .\ih_bfp_ten_x Maximum Data Base Working File Sizes (kilobytes): 1024 .\ih_bfp_ten_x.tmp\gapel1.bas 305152 .\ih_bfp_ten_x.tmp\kblk1.bas 169984 .\ih_bfp_ten_x.tmp\kel1.bas 2048 .\ih_bfp_ten_x.tmp\l1da1.bas
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127 Appendix F: (Continued) 1024 .\ih_bfp_ten_x.tmp\l2sq1.bas 19456 .\ih_bfp_ten_x.tmp\oel1.bas Run Completed Tue Jan 16, 2007 17:00:01
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128 Appendix G: Inner Hub and Pin Analysis Â– 20 Degrees Camber This is the Â“run statusÂ” output file for the ProMechanica analysis of the In ner Hub and Pin analysis. A camber of 20 degrees was used, 10 times the static load was applie d, and the convergence was set to 10%. Mechanica Structure Version K0141:spg Summary for Design Study "tewnty_deg_camber_ten_x_static" Thu Jan 25, 2007 17:35:15 Run Settings Memory allocation for block solver: 128.0 Checking the model before creating elements... These checks take into account the fact that AutoGEM will automatically create elements in volumes with material properties, on surfaces with shell properties, and on curves with beam section properties. Generate elements automatically. Checking the model after creating elements... No errors were found in the model. Mechanica Structure Model Summary Principal System of Units: Inch Pound Second (IPS) Length: in Force: lbf Time: sec Temperature: F Model Type: Three Dimensional
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129 Appendix G: (Continued) Points: 227 Edges: 971 Faces: 1266 Springs: 0 Masses: 0 Beams: 0 Shells: 0 Solids: 522 Elements: 522 Contact Regions: 2 Standard Design Study Description: hub with planks, 390 lb transverse load, fixed pin, 2 con tact areas, xconstraints on square slot, zconstrain t on hole Static Analysis "tewnty_deg_camber_ten_x_static": Contact Analysis Convergence Method: MultiplePass Adaptive Plotting Grid: 4 Convergence Loop Log: (17:35:19)
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130 Appendix G: (Continued) >> Pass 1 << Calculating Element Equations (17:35:19) Total Number of Equations: 612 Maximum Edge Order: 1 Solving Equations (17:35:19) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (17:35:20) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.79502e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (17:35:22) PostProcessing Solution (17:35:23) Checking Convergence (17:35:23) Elements Not Converged: 522 Edges Not Converged: 971 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 100.0% Resource Check (17:35:23) Elapsed Time (sec): 9.61 CPU Time (sec): 7.92 Memory Usage (kb): 185502 Wrk Dir Dsk Usage (kb): 4098
PAGE 141
131 Appendix G: (Continued) >> Pass 2 << Calculating Element Equations (17:35:24) Total Number of Equations: 3369 Maximum Edge Order: 2 Solving Equations (17:35:24) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (17:35:25) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 4.57656e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (17:35:30) PostProcessing Solution (17:35:31) Checking Convergence (17:35:31) Elements Not Converged: 371 Edges Not Converged: 220 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 90.6% Resource Check (17:35:31) Elapsed Time (sec): 17.10 CPU Time (sec): 15.28 Memory Usage (kb): 186590 Wrk Dir Dsk Usage (kb): 4098
PAGE 142
132 Appendix G: (Continued) >> Pass 3 << Calculating Element Equations (17:35:31) Total Number of Equations: 9872 Maximum Edge Order: 4 Solving Equations (17:35:32) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (17:35:34) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 9.78108e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (17:35:47) PostProcessing Solution (17:35:48) Checking Convergence (17:35:48) Elements Not Converged: 259 Edges Not Converged: 27 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 49.6% Resource Check (17:35:48) Elapsed Time (sec): 33.93 CPU Time (sec): 31.58 Memory Usage (kb): 195698 Wrk Dir Dsk Usage (kb): 10242
PAGE 143
133 Appendix G: (Continued) >> Pass 4 << Calculating Element Equations (17:35:48) Total Number of Equations: 19765 Maximum Edge Order: 4 Solving Equations (17:35:49) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (17:35:56) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.47220e01 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (17:36:27) PostProcessing Solution (17:36:30) Checking Convergence (17:36:30) Elements Not Converged: 116 Edges Not Converged: 0 Local Disp/Energy Index: 40.1% Global RMS Stress Index: 28.0% Resource Check (17:36:30) Elapsed Time (sec): 76.14 CPU Time (sec): 71.61 Memory Usage (kb): 197534 Wrk Dir Dsk Usage (kb): 23554
PAGE 144
134 Appendix G: (Continued) >> Pass 5 << Calculating Element Equations (17:36:30) Total Number of Equations: 34664 Maximum Edge Order: 5 Solving Equations (17:36:35) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (17:36:52) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.77811e01 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (17:37:50) PostProcessing Solution (17:37:52) Checking Convergence (17:37:52) Elements Not Converged: 24 Edges Not Converged: 0 Local Disp/Energy Index: 25.3% Global RMS Stress Index: 17.4% Resource Check (17:37:52) Elapsed Time (sec): 158.51 CPU Time (sec): 150.88 Memory Usage (kb): 202371 Wrk Dir Dsk Usage (kb): 55298
PAGE 145
135 Appendix G: (Continued) >> Pass 6 << Calculating Element Equations (17:37:52) Total Number of Equations: 54364 Maximum Edge Order: 6 Solving Equations (17:38:05) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (17:39:07) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.91521e01 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (17:42:51) PostProcessing Solution (17:42:54) Checking Convergence (17:42:54) Elements Not Converged: 1 Edges Not Converged: 0 Local Disp/Energy Index: 11.7% Global RMS Stress Index: 11.5% Resource Check (17:42:55) Elapsed Time (sec): 461.30 CPU Time (sec): 344.20 Memory Usage (kb): 226872 Wrk Dir Dsk Usage (kb): 299010
PAGE 146
136 Appendix G: (Continued) >> Pass 7 << Calculating Element Equations (17:42:55) Total Number of Equations: 76902 Maximum Edge Order: 7 Solving Equations (17:43:25) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (17:45:22) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.96470e01 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (17:52:59) PostProcessing Solution (17:53:26) Checking Convergence (17:53:26) Elements Not Converged: 0 Edges Not Converged: 0 Local Disp/Energy Index: 7.5% Global RMS Stress Index: 8.5%
PAGE 147
137 Appendix G: (Continued) RMS Stress Error Estimates: Load Set Stress Error % of Max Prin Str LoadSet1 2.71e+03 0.9% of 2.89e+05 Resource Check (17:53:36) Elapsed Time (sec): 1102.00 CPU Time (sec): 667.33 Memory Usage (kb): 236762 Wrk Dir Dsk Usage (kb): 518146 The analysis converged to within 10% on edge displacement, element strain energy, and global RMS stress. Total Mass of Model: 1.023144e02 Total Cost of Model: 0.000000e+00 Mass Moments of Inertia about WCS Origin: Ixx: 4.63460e01 Ixy: 3.08734e08 Iyy: 7.85380e03 Ixz: 1.48154e09 Iyz: 2.04349e09 Izz: 4.64919e01 Principal MMOI and Principal Axes Relative to WCS Origin: Max Prin Mid Prin Min Prin 4.64919e01 4.63460e01 7.85380e03 WCS X: 1.01513e06 1.00000e+00 6.77633e08 WCS Y: 4.47083e09 6.77633e08 1.00000e+00 WCS Z: 1.00000e+00 1.01513e06 4.47090e09
PAGE 148
138 Appendix G: (Continued) Center of Mass Location Relative to WCS Origin: ( 5.94376e02, 1.12540e02, 7.60935e07) Mass Moments of Inertia about the Center of Mass: Ixx: 4.63458e01 Ixy: 6.81303e06 Iyy: 7.81765e03 Ixz: 1.01879e09 Iyz: 1.95588e09 Izz: 4.64882e01 Principal MMOI and Principal Axes Relative to COM: Max Prin Mid Prin Min Prin 4.64882e01 4.63458e01 7.81765e03 WCS X: 7.15809e07 1.00000e+00 1.49526e05 WCS Y: 4.28989e09 1.49526e05 1.00000e+00 WCS Z: 1.00000e+00 7.15809e07 4.27919e09 Constraint Set: ConstraintSet1 Load Set: LoadSet1 Resultant Load on Model: in global X direction: 3.176963e09 in global Y direction: 1.278931e09 in global Z direction: 3.900000e+02 Measures: Name Value Convergence contact_area: 1.964696e01 2.5% contact_max_pres: 2.652123e+05 5.4% max_beam_bending: 0.000000e+00 0.0% max_beam_tensile: 0.000000e+00 0.0%
PAGE 149
139 Appendix G: (Continued) max_beam_torsion: 0.000000e+00 0.0% max_beam_total: 0.000000e+00 0.0% max_disp_mag: 4.428371e01 0.7% max_disp_x: 1.710132e02 0.6% max_disp_y: 4.132111e02 0.7% max_disp_z: 4.414927e01 0.7% max_prin_mag: 2.889458e+05 6.3% max_rot_mag: 0.000000e+00 0.0% max_rot_x: 0.000000e+00 0.0% max_rot_y: 0.000000e+00 0.0% max_rot_z: 0.000000e+00 0.0% max_stress_prin: 1.566489e+05 16.3% max_stress_vm: 2.126187e+05 6.5% max_stress_xx: 1.237603e+05 8.8% max_stress_xy: 7.144047e+04 5.5% max_stress_xz: 6.076288e+04 9.4% max_stress_yy: 2.652244e+05 5.5% max_stress_yz: 6.601131e+04 10.8% max_stress_zz: 1.080627e+05 8.2% min_stress_prin: 2.889458e+05 6.3% strain_energy: 8.490668e+01 0.7% cntRgn_007cntArea: 1.168257e01 2.3% cntRgn_007maxPres: 1.928679e+05 6.2% cntRgn_008cntArea: 7.964386e02 2.9% cntRgn_008maxPres: 2.652123e+05 5.4% Analysis "tewnty_deg_camber_ten_x_static" Completed (17:53:36) Memory and Disk Usage: Machine Type: Windows NT/x86 RAM Allocation for Solver (megabytes): 128.0 Total Elapsed Time (seconds): 1102.37
PAGE 150
140 Appendix G: (Continued) Total CPU Time (seconds): 667.69 Maximum Memory Usage (kilobytes): 236762 Working Directory Disk Usage (kilobytes): 518146 Results Directory Size (kilobytes): 11238 .\tewnty_deg_camber_ten_x_static Maximum Data Base Working File Sizes (kilobytes): 1024 .\tewnty_deg_camber_ten_x_static.tmp\gapel1.bas 315392 .\tewnty_deg_camber_ten_x_static.tmp\kblk1.bas 178176 .\tewnty_deg_camber_ten_x_static.tmp\kel1.bas 2048 .\tewnty_deg_camber_ten_x_static.tmp\l1da1.bas 1024 .\tewnty_deg_camber_ten_x_static.tmp\l2sq1.bas 20480 .\tewnty_deg_camber_ten_x_static.tmp\oel1.bas Run Completed Thu Jan 25, 2007 17:53:36
PAGE 151
141 Appendix H: Inner Hub and Pin Analysis Â– 6 Degrees Camber This is the Â“run statusÂ” output file for the ProMechanica analysis of the In ner Hub and Pin analysis. A camber of 6 degrees was used, 10 times the static load was appli ed, and the convergence was set to 10%. Mechanica Structure Version K0141:spg Summary for Design Study "six_deg_camber_ten_x_static" Mon Jan 29, 2007 10:01:26 Run Settings Memory allocation for block solver: 128.0 Checking the model before creating elements... These checks take into account the fact that AutoGEM will automatically create elements in volumes with material properties, on surfaces with shell properties, and on curves with beam section properties. Generate elements automatically. Checking the model after creating elements... No errors were found in the model. Mechanica Structure Model Summary Principal System of Units: Inch Pound Second (IPS) Length: in Force: lbf Time: sec Temperature: F Model Type: Three Dimensional
PAGE 152
142 Appendix H: (Continued) Points: 227 Edges: 971 Faces: 1266 Springs: 0 Masses: 0 Beams: 0 Shells: 0 Solids: 522 Elements: 522 Contact Regions: 2 Standard Design Study Description: hub with planks, 120 lb transverse load, fixed pin, 2 con tact areas, xconstraints on square slot, zconstrain t on hole Static Analysis "six_deg_camber_ten_x_static": Contact Analysis Convergence Method: MultiplePass Adaptive Plotting Grid: 4 Convergence Loop Log: (10:01:28)
PAGE 153
143 Appendix H: (Continued) >> Pass 1 << Calculating Element Equations (10:01:28) Total Number of Equations: 612 Maximum Edge Order: 1 Solving Equations (10:01:29) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (10:01:29) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.79502e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (10:01:32) PostProcessing Solution (10:01:33) Checking Convergence (10:01:33) Elements Not Converged: 522 Edges Not Converged: 971 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 100.0% Resource Check (10:01:33) Elapsed Time (sec): 10.09 CPU Time (sec): 5.91 Memory Usage (kb): 185566 Wrk Dir Dsk Usage (kb): 4098
PAGE 154
144 Appendix H: (Continued) >> Pass 2 << Calculating Element Equations (10:01:33) Total Number of Equations: 3369 Maximum Edge Order: 2 Solving Equations (10:01:33) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (10:01:34) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 4.57656e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (10:01:39) PostProcessing Solution (10:01:40) Checking Convergence (10:01:40) Elements Not Converged: 371 Edges Not Converged: 220 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 90.6% Resource Check (10:01:40) Elapsed Time (sec): 17.25 CPU Time (sec): 12.84 Memory Usage (kb): 187070 Wrk Dir Dsk Usage (kb): 4098
PAGE 155
145 Appendix H: (Continued) >> Pass 3 << Calculating Element Equations (10:01:40) Total Number of Equations: 9872 Maximum Edge Order: 4 Solving Equations (10:01:40) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (10:01:43) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 9.78108e02 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (10:01:55) PostProcessing Solution (10:01:56) Checking Convergence (10:01:56) Elements Not Converged: 259 Edges Not Converged: 27 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 49.6% Resource Check (10:01:56) Elapsed Time (sec): 33.68 CPU Time (sec): 28.35 Memory Usage (kb): 188766 Wrk Dir Dsk Usage (kb): 10242
PAGE 156
146 Appendix H: (Continued) >> Pass 4 << Calculating Element Equations (10:01:56) Total Number of Equations: 19765 Maximum Edge Order: 4 Solving Equations (10:01:57) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (10:02:04) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.47220e01 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (10:02:36) PostProcessing Solution (10:02:37) Checking Convergence (10:02:37) Elements Not Converged: 116 Edges Not Converged: 0 Local Disp/Energy Index: 40.1% Global RMS Stress Index: 28.0% Resource Check (10:02:38) Elapsed Time (sec): 75.07 CPU Time (sec): 66.47 Memory Usage (kb): 197694 Wrk Dir Dsk Usage (kb): 23554
PAGE 157
147 Appendix H: (Continued) >> Pass 5 << Calculating Element Equations (10:02:38) Total Number of Equations: 34664 Maximum Edge Order: 5 Solving Equations (10:02:52) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (10:03:10) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.77811e01 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (10:04:08) PostProcessing Solution (10:04:09) Checking Convergence (10:04:09) Elements Not Converged: 24 Edges Not Converged: 0 Local Disp/Energy Index: 25.3% Global RMS Stress Index: 17.4% Resource Check (10:04:10) Elapsed Time (sec): 167.28 CPU Time (sec): 144.70 Memory Usage (kb): 202754 Wrk Dir Dsk Usage (kb): 55298
PAGE 158
148 Appendix H: (Continued) >> Pass 6 << Calculating Element Equations (10:04:10) Total Number of Equations: 54364 Maximum Edge Order: 6 Solving Equations (10:04:24) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (10:05:12) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.91521e01 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (10:07:57) PostProcessing Solution (10:07:59) Checking Convergence (10:07:59) Elements Not Converged: 1 Edges Not Converged: 0 Local Disp/Energy Index: 11.7% Global RMS Stress Index: 11.5% Resource Check (10:08:00) Elapsed Time (sec): 397.82 CPU Time (sec): 323.83 Memory Usage (kb): 227832 Wrk Dir Dsk Usage (kb): 299010
PAGE 159
149 Appendix H: (Continued) >> Pass 7 << Calculating Element Equations (10:08:01) Total Number of Equations: 76902 Maximum Edge Order: 7 Solving Equations (10:08:45) Load Increment 0 of 1 Load Factor: 0.00000e+00 Contact Area: 0.00000e+00 Calculating Disp and Stress Results (10:10:26) Load Increment 1 of 1 Load Factor: 1.00000e+00 *Contact Area: 1.96470e01 ** Warning: Contact area is small in comparison to size of adjacent element edges for one or more contact regions for all load factors above marked with a "*". If you need pressure results near the contact regions, use singlepass adaptive convergence and select Localized Mesh Refinement. Calculating Disp and Stress Results (10:15:37) PostProcessing Solution (10:16:00) Checking Convergence (10:16:00) Elements Not Converged: 0 Edges Not Converged: 0 Local Disp/Energy Index: 7.5% Global RMS Stress Index: 8.5%
PAGE 160
150 Appendix H: (Continued) RMS Stress Error Estimates: Load Set Stress Error % of Max Prin Str LoadSet1 8.33e+02 0.9% of 8.89e+04 Resource Check (10:16:09) Elapsed Time (sec): 886.63 CPU Time (sec): 626.45 Memory Usage (kb): 239510 Wrk Dir Dsk Usage (kb): 518146 The analysis converged to within 10% on edge displacement, element strain energy, and global RMS stress. Total Mass of Model: 1.023144e02 Total Cost of Model: 0.000000e+00 Mass Moments of Inertia about WCS Origin: Ixx: 4.63460e01 Ixy: 3.08734e08 Iyy: 7.85380e03 Ixz: 1.48154e09 Iyz: 2.04349e09 Izz: 4.64919e01 Principal MMOI and Principal Axes Relative to WCS Origin: Max Prin Mid Prin Min Prin 4.64919e01 4.63460e01 7.85380e03 WCS X: 1.01513e06 1.00000e+00 6.77633e08 WCS Y: 4.47083e09 6.77633e08 1.00000e+00 WCS Z: 1.00000e+00 1.01513e06 4.47090e09
PAGE 161
151 Appendix H: (Continued) Center of Mass Location Relative to WCS Origin: ( 5.94376e02, 1.12540e02, 7.60935e07) Mass Moments of Inertia about the Center of Mass: Ixx: 4.63458e01 Ixy: 6.81303e06 Iyy: 7.81765e03 Ixz: 1.01879e09 Iyz: 1.95588e09 Izz: 4.64882e01 Principal MMOI and Principal Axes Relative to COM: Max Prin Mid Prin Min Prin 4.64882e01 4.63458e01 7.81765e03 WCS X: 7.15809e07 1.00000e+00 1.49526e05 WCS Y: 4.28989e09 1.49526e05 1.00000e+00 WCS Z: 1.00000e+00 7.15809e07 4.27919e09 Constraint Set: ConstraintSet1 Load Set: LoadSet1 Resultant Load on Model: in global X direction: 1.059246e09 in global Y direction: 9.444218e12 in global Z direction: 1.200000e+02 Measures: Name Value Convergence contact_area: 1.964696e01 2.5% contact_max_pres: 8.160378e+04 5.4% max_beam_bending: 0.000000e+00 0.0% max_beam_tensile: 0.000000e+00 0.0%
PAGE 162
152 Appendix H: (Continued) max_beam_torsion: 0.000000e+00 0.0% max_beam_total: 0.000000e+00 0.0% max_disp_mag: 1.362576e01 0.7% max_disp_x: 5.261943e03 0.6% max_disp_y: 1.271419e02 0.7% max_disp_z: 1.358439e01 0.7% max_prin_mag: 8.890640e+04 6.3% max_rot_mag: 0.000000e+00 0.0% max_rot_x: 0.000000e+00 0.0% max_rot_y: 0.000000e+00 0.0% max_rot_z: 0.000000e+00 0.0% max_stress_prin: 4.819966e+04 16.3% max_stress_vm: 6.542112e+04 6.5% max_stress_xx: 3.808010e+04 8.8% max_stress_xy: 2.198168e+04 5.5% max_stress_xz: 1.869627e+04 9.4% max_stress_yy: 8.160752e+04 5.5% max_stress_yz: 2.031117e+04 10.8% max_stress_zz: 3.325007e+04 8.2% min_stress_prin: 8.890640e+04 6.3% strain_energy: 8.038502e+00 0.7% cntRgn_007cntArea: 1.168257e01 2.3% cntRgn_007maxPres: 5.934398e+04 6.2% cntRgn_008cntArea: 7.964386e02 2.9% cntRgn_008maxPres: 8.160378e+04 5.4% Analysis "six_deg_camber_ten_x_static" Completed (10:16:09) Memory and Disk Usage: Machine Type: Windows NT/x86 RAM Allocation for Solver (megabytes): 128.0
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153 Appendix H: (Continued) Total Elapsed Time (seconds): 886.99 Total CPU Time (seconds): 626.78 Maximum Memory Usage (kilobytes): 239510 Working Directory Disk Usage (kilobytes): 518146 Results Directory Size (kilobytes): 10690 .\six_deg_camber_ten_x_static Maximum Data Base Working File Sizes (kilobytes): 1024 .\six_deg_camber_ten_x_static.tmp\gapel1.bas 315392 .\six_deg_camber_ten_x_static.tmp\kblk1.bas 178176 .\six_deg_camber_ten_x_static.tmp\kel1.bas 2048 .\six_deg_camber_ten_x_static.tmp\l1da1.bas 1024 .\six_deg_camber_ten_x_static.tmp\l2sq1.bas 20480 .\six_deg_camber_ten_x_static.tmp\oel1.bas Run Completed Mon Jan 29, 2007 10:16:10
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154 Appendix I: Inner Hub and Ball Bearing Analysis This is the Â“run statusÂ” output file for the ProMechanica analysis of the In ner Hub and Ball Bearing Vertical Symmetry analysis. A camber of 3 degrees was used, 10 times the static load was applied, and the convergence was set to 10%. Mechanica Structure Version K0141:spg Summary for Design Study "IH_and_BB_vert_sym" Fri Mar 23, 2007 16:38:53 Run Settings Memory allocation for block solver: 128.0 Checking the model before creating elements... These checks take into account the fact that AutoGEM will automatically create elements in volumes with material properties, on surfaces with shell properties, and on curves with beam section properties. Generate elements automatically. Checking the model after creating elements... No errors were found in the model. Mechanica Structure Model Summary Principal System of Units: Inch Pound Second (IPS) Length: in Force: lbf Time: sec Temperature: F
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155 Appendix I: (Continued) Model Type: Three Dimensional Points: 187 Edges: 845 Faces: 1125 Springs: 0 Masses: 0 Beams: 0 Shells: 0 Solids: 468 Elements: 468 Standard Design Study Description: 10 times static load bottom of rubber slot fixed vertical symmetry Static Analysis "IH_and_BB_vert_sym": Convergence Method: MultiplePass Adaptive Plotting Grid: 4 Convergence Loop Log: (16:38:57) >> Pass 1 << Calculating Element Equations (16:38:57) Total Number of Equations: 521
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156 Appendix I: (Continued) Maximum Edge Order: 1 Solving Equations (16:38:57) PostProcessing Solution (16:38:57) Calculating Disp and Stress Results (16:38:57) Checking Convergence (16:38:58) Elements Not Converged: 468 Edges Not Converged: 845 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 100.0% Resource Check (16:38:58) Elapsed Time (sec): 6.51 CPU Time (sec): 5.47 Memory Usage (kb): 181350 Wrk Dir Dsk Usage (kb): 2048 >> Pass 2 << Calculating Element Equations (16:38:59) Total Number of Equations: 2979 Maximum Edge Order: 2 Solving Equations (16:38:59) PostProcessing Solution (16:38:59) Calculating Disp and Stress Results (16:38:59) Checking Convergence (16:39:00) Elements Not Converged: 325 Edges Not Converged: 829 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 80.4% Resource Check (16:39:00) Elapsed Time (sec): 8.40 CPU Time (sec): 6.97 Memory Usage (kb): 182430 Wrk Dir Dsk Usage (kb): 2048
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157 Appendix I: (Continued) >> Pass 3 << Calculating Element Equations (16:39:00) Total Number of Equations: 10403 Maximum Edge Order: 4 Solving Equations (16:39:01) PostProcessing Solution (16:39:02) Calculating Disp and Stress Results (16:39:02) Checking Convergence (16:39:03) Elements Not Converged: 189 Edges Not Converged: 713 Local Disp/Energy Index: 84.1% Global RMS Stress Index: 40.0% Resource Check (16:39:03) Elapsed Time (sec): 11.35 CPU Time (sec): 9.63 Memory Usage (kb): 182430 Wrk Dir Dsk Usage (kb): 10240 >> Pass 4 << Calculating Element Equations (16:39:03) Total Number of Equations: 19211 Maximum Edge Order: 5 Solving Equations (16:39:05) PostProcessing Solution (16:39:07) Calculating Disp and Stress Results (16:39:08) Checking Convergence (16:39:09) Elements Not Converged: 41 Edges Not Converged: 1 Local Disp/Energy Index: 46.4% Global RMS Stress Index: 36.2% Resource Check (16:39:09) Elapsed Time (sec): 17.43 CPU Time (sec): 14.72
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158 Appendix I: (Continued) Memory Usage (kb): 184240 Wrk Dir Dsk Usage (kb): 22528 >> Pass 5 << Calculating Element Equations (16:39:09) Total Number of Equations: 30696 Maximum Edge Order: 5 Solving Equations (16:39:14) PostProcessing Solution (16:39:18) Calculating Disp and Stress Results (16:39:20) Checking Convergence (16:39:21) Elements Not Converged: 11 Edges Not Converged: 0 Local Disp/Energy Index: 27.5% Global RMS Stress Index: 23.5% Resource Check (16:39:21) Elapsed Time (sec): 29.44 CPU Time (sec): 25.22 Memory Usage (kb): 192478 Wrk Dir Dsk Usage (kb): 46080 >> Pass 6 << Calculating Element Equations (16:39:21) Total Number of Equations: 42823 Maximum Edge Order: 6 Solving Equations (16:39:30) PostProcessing Solution (16:39:41) Calculating Disp and Stress Results (16:39:44) Checking Convergence (16:39:46) Elements Not Converged: 6 Edges Not Converged: 0 Local Disp/Energy Index: 21.2% Global RMS Stress Index: 21.0%
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159 Appendix I: (Continued) Resource Check (16:39:47) Elapsed Time (sec): 55.01 CPU Time (sec): 45.98 Memory Usage (kb): 197127 Wrk Dir Dsk Usage (kb): 205824 >> Pass 7 << Calculating Element Equations (16:39:47) Total Number of Equations: 53068 Maximum Edge Order: 7 Solving Equations (16:40:02) PostProcessing Solution (16:40:22) Calculating Disp and Stress Results (16:40:27) Checking Convergence (16:40:29) Elements Not Converged: 3 Edges Not Converged: 0 Local Disp/Energy Index: 17.1% Global RMS Stress Index: 17.1% Resource Check (16:40:31) Elapsed Time (sec): 99.15 CPU Time (sec): 81.80 Memory Usage (kb): 201066 Wrk Dir Dsk Usage (kb): 301056 >> Pass 8 << Calculating Element Equations (16:40:31) Total Number of Equations: 61904 Maximum Edge Order: 8 Solving Equations (16:41:09) PostProcessing Solution (16:41:54) Calculating Disp and Stress Results (16:42:08) Checking Convergence (16:42:29) Elements Not Converged: 1
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160 Appendix I: (Continued) Edges Not Converged: 0 Local Disp/Energy Index: 13.0% Global RMS Stress Index: 14.3% Resource Check (16:42:30) Elapsed Time (sec): 218.33 CPU Time (sec): 136.50 Memory Usage (kb): 219446 Wrk Dir Dsk Usage (kb): 412672 >> Pass 9 << Calculating Element Equations (16:42:30) Total Number of Equations: 69053 Maximum Edge Order: 9 Solving Equations (16:43:00) PostProcessing Solution (16:43:58) Calculating Disp and Stress Results (16:44:10) Checking Convergence (16:44:33) Elements Not Converged: 1 Edges Not Converged: 0 Local Disp/Energy Index: 10.4% Global RMS Stress Index: 12.3% RMS Stress Error Estimates: Load Set Stress Error % of Max Prin Str LoadSet1 1.83e+02 0.8% of 2.30e+04 ** Warning: Convergence was not obtained because the maximum polynomial order of 9 was reached. Resource Check (16:44:44) Elapsed Time (sec): 352.38
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161 Appendix I: (Continued) CPU Time (sec): 218.69 Memory Usage (kb): 225768 Wrk Dir Dsk Usage (kb): 509952 The analysis did not converge to within 10% on edge displacement, element strain energy, and global RMS stress. Total Mass of Model: 9.819899e04 Total Cost of Model: 0.000000e+00 Mass Moments of Inertia about WCS Origin: Ixx: 1.68629e03 Ixy: 2.03344e10 Iyy: 1.73531e03 Ixz: 2.83163e06 Iyz: 7.19532e06 Izz: 3.08892e03 Principal MMOI and Principal Axes Relative to WCS Origin: Max Prin Mid Prin Min Prin 3.08897e03 1.73527e03 1.68629e03 WCS X: 2.01870e03 3.11410e04 9.99998e01 WCS Y: 5.31539e03 9.99986e01 3.00676e04 WCS Z: 9.99984e01 5.31477e03 2.02033e03 Center of Mass Location Relative to WCS Origin: (2.30649e02, 5.86321e02, 3.10996e01)
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162 Appendix I: (Continued) Mass Moments of Inertia about the Center of Mass: Ixx: 1.58794e03 Ixy: 1.32778e06 Iyy: 1.63981e03 Ixz: 4.21226e06 Iyz: 1.07106e05 Izz: 3.08503e03 Principal MMOI and Principal Axes Relative to COM: Max Prin Mid Prin Min Prin 3.08512e03 1.63977e03 1.58790e03 WCS X: 2.81996e03 2.50040e02 9.99683e01 WCS Y: 7.41299e03 9.99659e01 2.50243e02 WCS Z: 9.99969e01 7.48121e03 2.63364e03 Constraint Set: ConstraintSet1 Load Set: LoadSet1 Resultant Load on Model: in global X direction: 1.646741e11 in global Y direction: 5.750003e+02 in global Z direction: 6.880718e12 Measures: Name Value Convergence max_beam_bending: 0.000000e+00 0.0% max_beam_tensile: 0.000000e+00 0.0% max_beam_torsion: 0.000000e+00 0.0% max_beam_total: 0.000000e+00 0.0% max_disp_mag: 1.437177e03 0.7%
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163 Appendix I: (Continued) max_disp_x: 5.945448e04 0.4% max_disp_y: 1.345624e03 0.8% max_disp_z: 1.538635e04 0.0% max_prin_mag: 2.295273e+04 6.7% max_rot_mag: 0.000000e+00 0.0% max_rot_x: 0.000000e+00 0.0% max_rot_y: 0.000000e+00 0.0% max_rot_z: 0.000000e+00 0.0% max_stress_prin: 2.028103e+04 15.4% max_stress_vm: 2.038053e+04 16.4% max_stress_xx: 9.037661e+03 7.7% max_stress_xy: 9.476953e+03 16.2% max_stress_xz: 3.849938e+03 14.3% max_stress_yy: 1.616673e+04 9.1% max_stress_yz: 7.891967e+03 8.7% max_stress_zz: 1.577741e+04 7.2% min_stress_prin: 2.295273e+04 6.7% strain_energy: 2.873992e01 0.7% Analysis "IH_and_BB_vert_sym" Completed (16:44:45) Memory and Disk Usage: Machine Type: Windows NT/x86 RAM Allocation for Solver (megabytes): 128.0 Total Elapsed Time (seconds): 352.93 Total CPU Time (seconds): 218.97 Maximum Memory Usage (kilobytes): 225768 Working Directory Disk Usage (kilobytes): 509952
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164 Appendix I: (Continued) Results Directory Size (kilobytes): 12331 .\IH_and_BB_vert_sym Maximum Data Base Working File Sizes (kilobytes): 300032 .\IH_and_BB_vert_sym.tmp\kblk1.bas 188416 .\IH_and_BB_vert_sym.tmp\kel1.bas 21504 .\IH_and_BB_vert_sym.tmp\oel1.bas Run Completed Fri Mar 23, 2007 16:44:45 
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165 Appendix J: Outer Hub and Spoke Analysis This is the Â“run statusÂ” output file for the ProMechanica analysis of the Oute r Hub and Spoke analysis. A camber of 3 degrees was used, 5 times the static load was applie d, and the convergence was set to 10%. Mechanica Structure Version K0141:spg Summary for Design Study "oh_five_x_static" Mon Jan 15, 2007 17:15:32 Run Settings Memory allocation for block solver: 128.0 Checking the model before creating elements... These checks take into account the fact that AutoGEM will automatically create elements in volumes with material properties, on surfaces with shell properties, and on curves with beam section properties. Generate elements automatically. Checking the model after creating elements... No errors were found in the model. Mechanica Structure Model Summary Principal System of Units: Inch Pound Second (IPS) Length: in Force: lbf Time: sec Temperature: F Model Type: Three Dimensional
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166 Appendix J: (Continued) Points: 453 Edges: 1994 Faces: 2559 Springs: 0 Masses: 0 Beams: 0 Shells: 0 Solids: 1036 Elements: 1036 Standard Design Study Description: 287 lbs on top spoke hole bottom spoke hole fixed Static Analysis "oh_five_x_static": Convergence Method: MultiplePass Adaptive Plotting Grid: 4 Convergence Loop Log: (17:15:41) >> Pass 1 << Calculating Element Equations (17:15:41) Total Number of Equations: 1300 Maximum Edge Order: 1 Solving Equations (17:15:41) PostProcessing Solution (17:15:41) Calculating Disp and Stress Results (17:15:41)
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167 Appendix J: (Continued) Checking Convergence (17:15:44) Elements Not Converged: 1036 Edges Not Converged: 1994 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 100.0% Resource Check (17:15:44) Elapsed Time (sec): 13.30 CPU Time (sec): 10.69 Memory Usage (kb): 195558 Wrk Dir Dsk Usage (kb): 8192 >> Pass 2 << Calculating Element Equations (17:15:45) Total Number of Equations: 7164 Maximum Edge Order: 2 Solving Equations (17:15:45) PostProcessing Solution (17:15:45) Calculating Disp and Stress Results (17:15:46) Checking Convergence (17:15:49) Elements Not Converged: 937 Edges Not Converged: 1858 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 93.4% Resource Check (17:15:49) Elapsed Time (sec): 17.91 CPU Time (sec): 13.66 Memory Usage (kb): 195558 Wrk Dir Dsk Usage (kb): 8192 >> Pass 3 << Calculating Element Equations (17:15:49) Total Number of Equations: 26635 Maximum Edge Order: 4
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168 Appendix J: (Continued) Solving Equations (17:15:50) PostProcessing Solution (17:15:53) Calculating Disp and Stress Results (17:15:54) Checking Convergence (17:15:57) Elements Not Converged: 442 Edges Not Converged: 1001 Local Disp/Energy Index: 100.0% Global RMS Stress Index: 17.4% Resource Check (17:15:57) Elapsed Time (sec): 26.32 CPU Time (sec): 19.66 Memory Usage (kb): 197546 Wrk Dir Dsk Usage (kb): 26624 >> Pass 4 << Calculating Element Equations (17:15:58) Total Number of Equations: 46833 Maximum Edge Order: 5 Solving Equations (17:16:03) PostProcessing Solution (17:16:07) Calculating Disp and Stress Results (17:16:10) Checking Convergence (17:16:14) Elements Not Converged: 6 Edges Not Converged: 0 Local Disp/Energy Index: 15.7% Global RMS Stress Index: 7.3% Resource Check (17:16:15) Elapsed Time (sec): 43.63 CPU Time (sec): 31.41 Memory Usage (kb): 201314 Wrk Dir Dsk Usage (kb): 56320
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169 Appendix J: (Continued) >> Pass 5 << Calculating Element Equations (17:16:15) Total Number of Equations: 75896 Maximum Edge Order: 6 Solving Equations (17:16:25) PostProcessing Solution (17:16:39) Calculating Disp and Stress Results (17:16:44) Checking Convergence (17:16:48) Elements Not Converged: 0 Edges Not Converged: 0 Local Disp/Energy Index: 5.9% Global RMS Stress Index: 6.1% RMS Stress Error Estimates: Load Set Stress Error % of Max Prin Str LoadSet1 2.12e+03 5.8% of 3.69e+04 Resource Check (17:16:54) Elapsed Time (sec): 82.37 CPU Time (sec): 62.50 Memory Usage (kb): 230358 Wrk Dir Dsk Usage (kb): 283648 The analysis converged to within 10% on edge displacement, element strain energy, and global RMS stress. Total Mass of Model: 8.107128e04 Total Cost of Model: 0.000000e+00
PAGE 180
170 Appendix J: (Continued) Mass Moments of Inertia about WCS Origin: Ixx: 2.59612e03 Ixy: 1.28562e08 Iyy: 2.59612e03 Ixz: 1.54412e09 Iyz: 1.78294e09 Izz: 4.49841e03 Principal MMOI and Principal Axes Relative to WCS Origin: Max Prin Mid Prin Min Prin 4.49841e03 2.59613e03 2.59611e03 WCS X: 8.11724e07 8.09053e01 5.87735e01 WCS Y: 9.37261e07 5.87735e01 8.09053e01 WCS Z: 1.00000e+00 1.20759e06 2.81216e07 Center of Mass Location Relative to WCS Origin: (4.91346e06, 3.44632e06, 5.73958e01) Mass Moments of Inertia about the Center of Mass: Ixx: 2.32905e03 Ixy: 1.28562e08 Iyy: 2.32904e03 Ixz: 7.42185e10 Iyz: 1.79315e10 Izz: 4.49841e03 Principal MMOI and Principal Axes Relative to COM: Max Prin Mid Prin Min Prin 4.49841e03 2.32906e03 2.32903e03 WCS X: 3.42121e07 8.09053e01 5.87735e01 WCS Y: 8.26556e08 5.87735e01 8.09053e01 WCS Z: 1.00000e+00 2.28215e07 2.67949e07
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171 Appendix J: (Continued) Constraint Set: ConstraintSet1 Load Set: LoadSet1 Resultant Load on Model: in global X direction: 3.711114e10 in global Y direction: 2.870000e+02 in global Z direction: 7.662270e11 Measures: Name Value Convergence max_beam_bending: 0.000000e+00 0.0% max_beam_tensile: 0.000000e+00 0.0% max_beam_torsion: 0.000000e+00 0.0% max_beam_total: 0.000000e+00 0.0% max_disp_mag: 2.280043e02 0.3% max_disp_x: 1.085224e02 0.3% max_disp_y: 2.280042e02 0.3% max_disp_z: 1.281594e03 1.0% max_prin_mag: 3.688925e+04 5.2% max_rot_mag: 0.000000e+00 0.0% max_rot_x: 0.000000e+00 0.0% max_rot_y: 0.000000e+00 0.0% max_rot_z: 0.000000e+00 0.0% max_stress_prin: 3.688925e+04 5.2% max_stress_vm: 3.723139e+04 0.3% max_stress_xx: 3.561172e+04 5.6% max_stress_xy: 1.198523e+04 3.4% max_stress_xz: 8.956634e+03 13.9% max_stress_yy: 2.155031e+04 2.9% max_stress_yz: 3.738425e+03 9.2%
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172 Appendix J: (Continued) max_stress_zz: 1.253873e+04 5.3% min_stress_prin: 2.176151e+04 2.4% strain_energy: 3.205368e+00 0.3% Analysis "oh_five_x_static" Completed (17:16:54) Memory and Disk Usage: Machine Type: Windows NT/x86 RAM Allocation for Solver (megabytes): 128.0 Total Elapsed Time (seconds): 82.95 Total CPU Time (seconds): 62.92 Maximum Memory Usage (kilobytes): 230358 Working Directory Disk Usage (kilobytes): 283648 Results Directory Size (kilobytes): 17814 .\oh_five_x_static Maximum Data Base Working File Sizes (kilobytes): 169984 .\oh_five_x_static.tmp\kblk1.bas 100352 .\oh_five_x_static.tmp\kel1.bas 13312 .\oh_five_x_static.tmp\oel1.bas Run Completed Mon Jan 15, 2007 17:16:54
