56
Copyright by Bennett Alan Ford 2011

Copyright by Bennett Alan Ford 2011 · 2019. 2. 8. · Bennett Alan Ford, M.S.E. The University of Texas at Austin, 2011 Supervisor: James T. O’Connor Photovoltaic vehicles are

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  • Copyright

    by

    Bennett Alan Ford

    2011

  • The Report Committee for Bennett Alan Ford Certifies that this is the approved version of the following report:

    Structural Optimization for a Photovoltaic Vehicle

    APPROVED BY

    SUPERVISING COMMITTEE:

    James T. O’Connor

    John D. Borcherding

    Supervisor:

  • Structural Optimization for a Photovoltaic Vehicle

    by

    Bennett Alan Ford, B.S.

    Report

    Presented to the Faculty of the Graduate School of

    The University of Texas at Austin

    in Partial Fulfillment

    of the Requirements

    for the Degree of

    Master of Science in Engineering

    The University of Texas at Austin

    May 2011

  • Dedication

    This report is dedicated to my wife, Lauren, who has sustained me since the day we met.

  • v

    Acknowledgements

    I would like to thank James O’Connor, John Borcherding, and Steve Nelson for

    their service as educators and mentors at The University of Texas. I would also like to

    thank Ramon Carrasquillo, Make McDermott, and Mark Begert for their roles in

    facilitating my education and career. Most importantly, I want to thank my family for

    their constant support.

  • vi

    Abstract

    Structural Optimization for a Photovoltaic Vehicle

    Bennett Alan Ford, M.S.E.

    The University of Texas at Austin, 2011

    Supervisor: James T. O’Connor

    Photovoltaic vehicles are designed to harness solar energy and use it for self-propulsion.

    In order to collect sufficient energy to propel a passenger, a relatively large photovoltaic

    array is required. Controlling the loads imparted by the array and the body that supports

    it, while protecting the passenger and minimizing vehicle weight, presents a unique set of

    design challenges. Weight considerations and geometric constraints often lead system

    designers toward unconventional structural solutions. This report details analytical and

    experimental processes aimed at proving the concept of integrating aluminum space-

    frame elements with composite panels. Finite element analysis is used to simulate load

    conditions, and results are compared with empirical test data.

  • vii

    Table of Contents

    Background ..............................................................................................................1

    Chassis Design Development ..................................................................................2

    Roll Cage Design Development...............................................................................7

    Validation of Simulation Software ..........................................................................9

    Chassis Simulation Results ....................................................................................14

    Roll Cage Simulation Results ................................................................................19

    Buckling Simulation ..............................................................................................25

    Physical Model Fabrication ...................................................................................27

    Test Gage Placement..............................................................................................29

    Load Testing ..........................................................................................................32

    Comparison of Simulation and Experimental Results ...........................................37

    Conclusion and Further Research ..........................................................................39

    Appendix A Nomenclature ...................................................................................40

    Appendix B Shop Drawings .................................................................................41

    Appendix C CosmosWorks Load Cases ...............................................................44

    References ..............................................................................................................45

    Vita ... .....................................................................................................................46

  • viii

    List of Tables

    Table 1: Theoretical and FEA Results for Stress & Displacement…………….….13

    Table 2: Simulation Results……………………………………………………….14

    Table 3: Roll Cage Properties……………………………………….…………….19

    Table 4: Maximum Stress and Deformation………………………...…………….19

    Table 5: Test Strain Readings vs. Simulation Predictions…………..…………….38

  • ix

    List of Figures

    Figure 1: Initial Chassis Design……………………………………………...…..….5

    Figure 2: Design Concepts with Load Interfaces……………………………...….…5

    Figure 3: Adhesive Dispensing Gun…………………………………………………6

    Figure 4: Load Conditions……………………………………………………..…….7

    Figure 5: Roll Cage Iterations……………………………………………………….8

    Figure 6: Validation Test Tube…………………………………………………...….9

    Figure 7: Von Mises Visualization………………………………...……………….10

    Figure 8: Front Impact Simulation Results…………………..…………………….15

    Figure 9: Side Impact Simulation Results………………………………………….15

    Figure 10: Stress vs. Location……………………………………………………….16

    Figure 11: Displacement vs. Location (front)……………………….………………17

    Figure 12: Displacement vs. Location (side)…………………………………...……18

    Figure 13: CosmosWorks Stress Visualizations……………………………….…….20

    Figure 14: Displacement Visualizations……………………………………….…….21

    Figure 15: Distance Along Low Arc vs. Stress………………………………..…….22

    Figure 16: Distance Along High Arc vs. Displacement……………………….…….23

    Figure 17: Distance Along Low Arc vs. Displacement……………………..……….24

    Figure 18: Buckling Test Results for Chassis Test………………………………….25

    Figure 19: Buckling Loads and Restraints………………………….……………….26

    Figure 20: Pipe Bender………………………………………………………...…….27

    Figure 21: Pipe Bending Setup………………………………….......……………….28

    Figure 22: TIG Welding Process…………………………………………………….28

    Figure 23: Strain Gauge……………………………………………………...……....29

    Figure 24: Sanding Process………………………………………………………….29

    Figure 25: Cleansing Process…………………………………………….………….30

    Figure 26: Aligning a Gage………………………………………………………….30

    Figure 27: Attachment of the Gage………………………………………………….31

    Figure 28: Strain Gage Setting…………………………………………...………….31

  • x

    Figure 29: Compressing Testing Setup……………………………………..……….32

    Figure 30: Data Acquisition Setup…………………………………………….…….33

    Figure 31: Strain Gage Placement……………………………………………..…….33

    Figure 32: Roll Cage at Moment of Failure…………………………………………34

    Figure 33: Load and Displacement vs. Time…………………………...……………35

    Figure 34: Gage Strain vs. Time………………………………………………….….35

    Figure 35: Load and Displacement vs. Time…………………………...……………37

    Figure 36: Strain vs. Time during Compression Testing……………………………38

    Figure 37: Final Chassis and Roll Cage Design……………………….…………….39

  • 1

    Background Photovoltaic (PV) vehicle design, while not directly aimed at producing automobiles with

    immediate commercial potential, is a breeding ground for engineering innovation. The

    extraordinary challenge of building a reliable transportation device, powered only by the

    sun, encourages innovation in material sciences. The primary goals of PV vehicle chassis

    design are to provide safety for the passenger, reduce vehicle weight, maintain structural

    integrity under service loads, and provide mounting locations for system hardware.

    The scope of this report is the design and testing of a structural system consisting of a

    chassis and a roll cage, which act together to carry the design loads of a PV vehicle.

    Testing standards given by the American Solar Challenge Regulations (regulations) were

    chosen to model the stress and deflection experienced when a PV vehicle chassis is

    subjected to collision forces.

    A composite honeycomb sandwich panel was selected as a primary structural material

    due to its ease of assembly, extremely high specific strength, and simple geometry. Thin-

    wall aluminum tube was selected as a roll cage material due to its strength, ductility, and

    suitability for space frame construction. Chassis and roll cage designs were iterated

    multiple times, with improvements integrated based on the results of finite element

    analysis (FEA).

    Roll cage testing, conducted by applying normal compressive loading, was performed

    using a compression tester provided by the Texas Engineering Experiment Station

    (TEES). In order to simulate finite element analysis loading conditions and restraints, a

    steel test jig was fabricated to orient the roll cage properly with respect to the testing

    machine. A custom fabricated horizontal load-spreader beam was used to apply a

    compressive load across the roll hoops. Final test set-up included the strategic placement

    of strain gages.

  • 2

    Chassis Design Development

    Basic geometric parameters were provided by the Solar Motorsports Team (SMT), a

    collegiate PV vehicle design group. SMT also specified that the chassis architecture must

    include two parallel wheels in the front of the chassis and one wheel in the rear. Vehicle

    dynamic considerations dictated that a front tire braking system must be utilized. In order

    to ensure proper braking, 60-70% of the total car weight must be statically transferred to

    the driving surface through the front tires. To verify this weight distribution, the center of

    gravity of all components with considerable weight must be calculated. These

    calculations are made based on geometry-specific equations. One such equation used for

    the batteries, which have a cubic shape, is given in the following Equation 1 (Barber 46):

    〉〈=−−−

    kjiinLincg ,,)(*5.0)(3

    Where L is the length of a side (1)

    Overall chassis weight has significant impact on vehicle dynamics. Newton’s laws of

    motion state that force is a product of mass and acceleration given in Equation 2.

    (2)

    Therefore, lighter materials are desired to allow for rapid vehicle acceleration.

    Two classes of materials are generally used for resisting chassis loads: composites and

    metals. Fiber reinforced composites tend to have very high specific strengths, but their

    properties are typically orthotropic [1] and they tend to be brittle. Metals generally have

    isotropic properties and are typically much stronger than composites, but also tend to

    have lower specific strengths. Additionally, fabrication techniques for metals are

    generally easier to control and test than for composites.

    )sec**

    (

    )sec

    ()()(

    2

    2

    f

    mc

    m

    f

    lbinlb

    g

    inalbmlbF

    ∗=

  • 3

    Several equations are instrumental in evaluating material stress. For example, normal

    stress can be found using Equation 3:

    (3)

    When analyzing stress failure modes, Von Mises Stress theory is suitable and can be

    performed through finite element analysis [2]. The theory states the following in

    Equation 4.

    2 2 2 2 2 23 3 3E xx yy zz xx yy yy zz zz xx xy yz zxσ σ σ σ σ σ σ σ σ σ σ σ σ= + + − − − + + + (4)

    Where σxx, σyy, σzz are planar stress values and σxy, σxz, and σyz are shear values

    The Von Mises stress is compared to the yield and tensile strength of the material to

    determine whether failure will occur. Deflection of the chassis is also a safety concern in

    chassis design. Elastic deflection can be computed by first using Hooke’s Law, shown in

    Equation 5, to calculate the strain [2]:

    (5)

    Once the strain is found, the deflection is calculated through Equation 6, the definition of

    strain [2]:

    (6)

    )()(

    )( 2inAlbF

    psi f=σ

    )()( psiEpsi =ε

    σ

    )()(

    inLinL∆

  • 4

    Both stress and deflection can be estimated by modeling the chassis in three dimensions,

    placing appropriate loading conditions, and simulating it using finite element analysis

    software.

    CosmosWorks is a simulation tool bundled with SolidWorks, a 3D computer drafting

    software package. When a simulation is run using CosmosWorks, a factor of safety is

    indicated with respect to the type of simulation (stress, displacement, strain, etc). Only a

    fraction of the ultimate load capacity of a structural member should be utilized when the

    allowable load is applied. The remainder of the load-carrying capacity of the member is

    kept in reserve to assure safety. The ratio of the ultimate load to the allowable load is

    used to define the factor of safety. The equation for the factor of safety is given in

    Equation 7.

    (7)

    An alternate expression to satisfy the definition of factor of safety is shown in Equation 8.

    )(

    )(.psitressAllowableS

    psiressUltimateStSF = (8)

    The initial chassis design is shown in Figure 1. The stress results calculated in Cosmos

    Works were used to generate plots in Microsoft Excel.

    )()(

    ..f

    f

    lboadAllowableLlbadUltimateLo

    SF =

  • 5

    Figure 1: Initial Chassis Design

    Figure 2: Design Concepts with Load Interfaces

  • 6

    Figure 2 shows all of the chassis designs analyzed. Design geometry for the chassis was

    largely dependent upon fabrication techniques. The construction of the chassis requires

    that the honeycomb composite panels be glued together at all joints. For this process a

    two-part epoxy, 3M Plexus™, was chosen . Plexus™ epoxy has a tensile strength of

    approximately 22 Mpa and lap shear strength of 22 Mpa. In a 23°C ambient environment

    the glue has a 4-6 minute working time and achieves 75% strength in 15 minutes. The

    glue is dispensed from the hand-held gun shown in Figure 3. The glue is applied between

    all joints and also used as a filleting compound along perpendicular joints.

    Figure 3: Adhesive Dispensing Gun

  • 7

    Roll Cage Design Development

    Geometry for the roll cage was partially driven by the geometry of the chassis. The

    design also needed to take into account the size of the driver, the height limitations given

    by the body assembly, and the specifications given by the regulations. The SMT required

    that the roll cage and chassis be large enough to fit a person 74 inches tall with a 36”

    waist.

    Beginning with the three-dimensional SolidWorks model of the preliminary chassis

    design, designs were tested and modified based on FEA simulations. Various load cases,

    were simulated for each design. Figure 4 shows the loading conditions that the roll cage

    must withstand to comply with the regulations.

    Figure 4: Load Conditions

  • 8

    Figure 5: Roll Cage Iterations

    The second and third design iterations focused on reducing the weight of the roll cage.

    With the back and front planes of the roll cage fixed in size by regulations constraints, the

    primary methods available for doing so were to reduce wall thicknesses and optimize

    brace geometries.

  • 9

    Validation of Simulation Software

    In order to check the accuracy of the simulation software with respect to tubular roll

    cages, a solid model of a simple Aluminum 6061 pipe was generated in SolidWorks.

    Figure 6: Validation Test Tube

    The tube was constrained at one end while a normal applied load of 1238 lbf was applied

    to the opposite face. The tube was assigned material properties such as the modulus of

    elasticity, Poisson’s ratio, yield strength, and tensile strength. A solid mesh was

    incorporated into the model with a node element size that was smaller than the pipe

    thickness to ensure that the entire model was meshed. The simulation was run and Von

    Mises Stress and displacement values were recorded.

    In order to directly compare theoretical results to the FEA values, exact model

    dimensions and material specs were incorporated into the theoretical equations. To enable

    calculation of both Von Mises and displacement, several factors were first computed then

    embedded into their respective governing equations. First, the cross-sectional area of the

    pipe was found from Equation 9.

  • 10

    (9)

    Where A = cross sectional area, d0 = outer diameter, di= inner diameter

    Von Mises stress can be found from Equation 10.

    2 2 2 2 2 23 3 3E xx yy zz xx yy yy zz zz xx xy yz zxσ σ σ σ σ σ σ σ σ σ σ σ σ= + + − − − + + + (10)

    The formula above can also be rewritten as shown in Equation 11.

    ( )2 2 2 * * *E L circ rad L circ rad circ L radσ σ σ σ σ σ σ σ σ σ= + + − + + (11)

    Where Lσ = longitudinal stress, circσ = circumferential stress, radσ = radial stress

    Visually, this concept can be seen as:

    Figure 7: Von Mises Visualization

    σ 1 IS LONGITUDINAL STRESS σ 2 IS CIRCUMFERENTIAL STRESS σ 3 IS RADIAL STRESS "a" IS OUTSIDE RADIUS OF SECTION

    "b" IS INSIDE RADIUS OF SECTION

    "L" IS LENGTH OF SECTION

    "r" IS RADIUS AT SELECTED SECTION

    ( ))()(4

    )( 22222 indindinA io −=π

  • 11

    Longitudinal stress:

    (12)

    Asect = section area (in2); F = applied mechanical load (lbf)

    Circumferential stress on internal diameter element:

    (13)

    Pi = internal pressure (psi); Ro = outer radius (in), Ri = inner radius (in)

    Circumferential stress on outer diameter element:

    (14)

    Radial stress on internal diameter element:

    (15)

    Radial stress on external diameter element:

    (16)

    tL A

    F

    sec

    22

    22

    22

    22 )(

    io

    oext

    io

    ioicirc RR

    RPRRRRP

    ID −∗

    −−+

    22

    22

    22

    22 )(

    io

    ioext

    io

    iicirc RR

    RRPRRRP

    OD −+

    −−∗

    irad PID −=σ

    extrad POD −=σ

  • 12

    Displacement equations were adopted from Zienkiewics’ The Finite Element Method.

    Equations 17 through 19 allow for calculation of the generated outside and internal

    diameters as well as the new section length once loading conditions are applied. These

    equations are illustrated below:

    Outside Diameter under load:

    22 2 2 2

    2 2 2 2( )i o i ext o o i

    o oo i o i

    P R R P R R RD RE R R E R R

    υ⎡ ⎤⎛ ⎞∗ ∗ ∗ +

    = + − −⎢ ⎥⎜ ⎟− −⎝ ⎠⎣ ⎦ (17)

    E = modulus of elasticity (psi), υ = Poisson’s ratio (dimensionless)

    Inside Diameter under load:

    (18)

    Section length under load:

    ( ) ( ) tt

    io

    otext

    io

    ititt AE

    lFRRE

    RlPRRE

    RlPlL

    sec

    sec22

    22sec

    22

    22sec

    secsec ∗∗

    +−

    ∗∗∗+

    −∗∗∗

    −=εε

    (19)

    All calculations presented in this section were embedded into a Microsoft Excel

    spreadsheet. Final stress and displacement values from the FEA and theoretical

    computations are presented and compared (in terms of percent difference) in the

    following table:

    ( )2

    22

    22

    22

    22

    ⎥⎦

    ⎤⎢⎣

    −∗∗

    −⎟⎟⎠

    ⎞⎜⎜⎝

    ⎛+

    −+∗

    +=io

    ioext

    io

    ioiiii RRE

    RRPRRRR

    ERPRD ε

  • 13

    Table 1: Theoretical and FEA Results for Stress & Displacement

    VON MISES STRESS (PSI)

    OVERALL DISPLACEMENT (IN)

    FINITE ELEMENT 3720 8.1770E-03 ANALYSIS

    THEORY 3699 8.1101E-03

    PERCENT DIFFERENCE 0.54 0.818

    Clearly the theoretical and simulation values display good agreement. This result

    suggests that the FEA protocol used in the validation test is suitable for roll cage

    simulation.

  • 14

    Chassis Simulation Results

    The stresses and deflections for all four designs in the five regulation-driven loading tests

    are presented in Table 2. Safety factors are also displayed in the table.

    Table 2: Simulation Results

    DESIGN CASE

    Von MisesMAX

    STRESS (psi)

    MAXDEFLECTION

    (inches)

    Safety factor for

    plasticdeformation

    Safety factor for

    failureSMT original 3 g bump 3744 0.05401 3.07 3.60

    5 g front 2803 0.5426 4.10 4.81(First Design) 5 g rear 19610 1.044 0.59 0.69

    5 g side 7500 1.733 1.53 1.803g angular 7845 1.669 1.47 1.72

    Triangle Design 3 g bump 3702 0.0527 3.11 3.645 g front 2943 0.4846 3.91 4.58

    (Second Design) 5 g rear 6896 0.2032 1.67 1.965 g side 3100 0.4014 3.71 4.35

    3g angular 8793 1.625 1.31 1.53Beam Support Design 3 g bump 3711 0.05448 3.10 3.63

    5 g front 2496 0.2928 4.61 5.40(Third Design) 5 g rear 3090 0.1898 3.72 4.37

    5 g side 2253 0.0833 5.10 5.993g angular 8747 1.576 1.31 1.54

    Fillets Focused Design 3 g bump 3720 0.05582 3.09 3.635 g front 1845 0.295 6.23 7.31

    (Fourth Design) 5 g rear 4449 0.1817 2.58 3.035 g side 1675 0.079 6.87 8.05

    3g angular 8743 1.607 1.32 1.54

    CosmosWorks visually displays the results by color-coding areas where the differing

    levels of stress and deflection are experienced. Figures 8 and 9 show these results for the

    front and side CosmosWorks simulations.

  • 15

    Figure 8: Front Impact Simulation Results

    Figure 9: Side Impact Simulation Results

    Several graphs were produced to display directional stress and deflection behavior of the

    designs for the various simulations. Figure 10 displays the stress behavior experienced

  • 16

    during the front impact test while Figures 11 and 12 compare displacement for the front

    and side tests, respectively.

    Figure 10: Stress vs. Location

    Figure 10 compares the stress values experienced laterally across the front panel during

    the front impact test. These results show that the minimum stress occurred along the front

    corners of the chassis where the sides connected to the front.

    0

    500

    1000

    1500

    2000

    2500

    3000

    0 5 10 15 20 25 30

    Stre

    ss (p

    si)

    Displacement along Z-axis (in)

    Original DesignTriangle DesignBeam DesignFinal Design

  • 17

    Figure 11: Displacement vs. Location (front)

    Figure 11 compares the displacement values experienced laterally across the front panel

    during the front impact test. The beam design experienced the lowest total vertical

    displacement with the final design demonstrated the second smallest displacement.

    0.2

    0.25

    0.3

    0.35

    0.4

    0.45

    0.5

    0.55

    0 5 10 15 20 25

    Verti

    cal D

    ispl

    acem

    ent (

    in)

    Distance along Z-axis (in)

    Original Design

    Triangle Design

    Beam Design

    Final Design

  • 18

    Figure 12: Displacement vs. Location (side)

    Figure 12 shows the deflection experienced across the side of the chassis. The deflection

    of the final design is significantly reduced by linking the chassis sidewalls.

    0

    0.2

    0.4

    0.6

    0.8

    1

    1.2

    1.4

    1.6

    1.8

    0 10 20 30 40 50 60 70

    Disp

    lace

    men

    t (in

    )

    Distance Along X-Axis (in)

    Original Design

    Triangle Design

    Beam Design

    Final Design

  • 19

    Roll Cage Simulation Results

    Table 3 indicates the mass properties of the roll cage assembly iterations.

    Table 3: Roll Cage Properties

    Design Volume (in3) Total Length (in) Total Length (ft) Mass (lbm)

    Original Design 105.40 316.87 26.41 10.28

    Second Design 105.14 316.09 26.34 10.26

    Final Design 106.65 320.62 26.72 10.40

    A load of 1500 lb force, which is 3 times the expected weight of the vehicle, was applied

    over the top plane of the car which gave a direct force to the high and low roll hoop arcs.

    Table 4: Maximum Stress and Deformation

    DESIGN CASEVon Mises

    MAX STRESS

    MAXDEFLECTION

    (inches) Safety Factor for

    Plastic Deformation

    Safety factor for

    failure

    Original Design 3g 16100 0.5564 0.71 0.84

    Second Design 3g 18275 0.07531 0.63 0.74

    Final Design 3g 15960 0.04511 0.50 1.13

  • 20

    Figure 13: CosmosWorks Stress Visualizations

  • 21

    Figure 14: Displacement Visualizations

  • 22

    Figure 15: Distance Aong Low Arc vs. Stress

    Figure 15 shows that the average and peak stress differences along the lower arc between

    each of the designs is small. The final design shows the smallest average of each of the

    stress values which was important for choosing among the designs.

    0

    2000

    4000

    6000

    8000

    10000

    12000

    14000

    16000

    18000

    4 9 14 19

    Stre

    ss (p

    si)

    Distance Along Lower Arc (in)

    Original Design

    Second Design

    Final Design

  • 23

    Figure 16: Distance Along High Arc vs. Displacement

    Figure 16 shows the distribution of displacement values experienced at the high arc in

    each of the designs. The final design demonstrates the lowest displacement values.

    0

    0.01

    0.02

    0.03

    0.04

    0.05

    0.06

    0.07

    0.08

    4 6 8 10 12 14 16 18

    Vert

    ical

    Dis

    plac

    emen

    t Exp

    erie

    nced

    (in)

    Distance Along High Arc (in)

    Original Design

    Second Design

    Final Design

  • 24

    Figure 17: Distance Along Low Arc vs. Displacement

    Figure 17 shows the distribution of displacement values experienced at the low arc in

    each of the designs. The final design displays the smallest deflection among the designs.

    0

    0.01

    0.02

    0.03

    0.04

    0.05

    0.06

    4 9 14

    Ver

    tica

    l Dis

    pla

    cem

    ent

    Exp

    erie

    nce

    d (

    in)

    Distance Along Low Arc (in)

    Original Design

    Second Design

    Final Design

  • 25

    Buckling Simulation A section equivalent to the vertical front section of the chassis was utilized for local

    buckling analysis, and a total load of three times the total vehicle and passenger weight

    (1500 lbf) was placed normal to its top surface. The bottom surface of the piece was

    fixed, and buckling analysis was conducted. The resulting deformation visualization,

    including the load and restraint, are shown below:

    Figure 18: Buckling Test Results for Chassis Test

  • 26

    To simulate tube buckling, a test case was set up for the longest tube member on the roll

    cage. CosmosWorks produced a load factor of 1.2658. Figure 19 shows the manner in

    which the loads and restraints were applied to the pipe.

    Figure 19: Buckling Loads and Restraints

  • 27

    Physical Model Fabrication

    Aluminum (6061 T6) with a side wall thickness of 0.113 in was used for the construction

    of the roll cage. A circular saw with a metal cutting blade was used to cut the Aluminum

    pipe. A hydraulic pipe bender was used to create the bends in the front and rear hoops of

    the roll cage, as shown in Figure 20. A 220V Lincoln Electric square wave TIG welder

    was used to weld the individual roll cage components. Pure tungsten electrodes, Argon

    gas, and Aluminum 4043 filler rods were the consumables used in the welding process

    Figure 20: Pipe Bender

    For this particular roll cage design, the front and rear hoops of the roll cage are formed

    from bending straight pieces of aluminum.

  • 28

    Figure 21: Pipe Bending Setup

    The power setting on the welder was AC current mode with a 160 amp maximum power

    setting.

    Figure 22: TIG welding process

    Hydraulic Jack

    Roller

  • 29

    Test Gage Placement

    In order to measure strains during empirical testing, 10 strain gauges were attached to the

    roll cage.

    Figure 23: Strain Gage

    After the gage locations were marked on the tubes, a smooth surface was prepared by

    light sanding.

    Figure 24: Sanding Process

    To cleanse the surface, Methanol was applied swabbed at all gage locations.

  • 30

    Figure 25: Cleansing Process

    Cellophane tape was used to transfer the gages to the tubes. This process is shown in

    Figure 26 and Figure 27.

    Figure 26: Aligning a Gage

  • 31

    Figure 27: Attachment of the Gage

    Finally, the gages are bonded to the tubes using M-Bond AE-10 adhesive. Figure 28

    shows the final setting of a strain gage with wires attached.

    Figure 28: Strain Gage Setting

  • 32

    Load Testing

    The testing apparatus for the roll cage can be seen in Figure 29.

    Figure 29: Compression Testing Setup

    The signal wires were attached to an input device that sends the strain gage readings to

    the monitoring computer. Figure 30 shows how the wiring is attached to the input

    system.

  • 33

    Figure 30: Data Acquisition Setup

    Figure 31: Strain Gage Placement

    3

    4

    5 67

    8

    12

    9

  • 34

    The compression testing machine was set to advance at one half an inch (1/2 in) per

    minute. Figure 32 shows the position of the roll cage in which it was determined that the

    cage had failed. The failure occurred in the lower arc of the specimen while the high arc

    did not appear to undergo measurable permanent deformation. The higher arc is the more

    critical of the two arcs because it protects the driver’s head.

    Figure 32: Roll Cage at Moment of Failure

    The results of compression test recorded by the data acquisition system displayed the

    load and displacement of the compressor in relation to the duration of the experiment

    shown in Figure 33. Additional results, shown in Figure 34, give the strain experienced

    by the tube members of the roll cage with their respective strain gages attached.

  • 35

    Figure 33: Load and Displacement vs. Time

    Figure 34: Gage Strain vs. Time

  • 36

    The roll cage withstood forces reaching nearly 6000 lbs. about 100 seconds into the test,

    after which it began to experience plastic buckling and effective failure. The 6000 lbs.

    withstood by the roll cage is well above the 1500 lb. minimum set forth in the

    regulations.

  • 37

    Comparison of Simulation and Empirical results

    Strain gages placed throughout the physical model during the testing allowed observation

    of exactly what force magnitude the individual roll cage members experienced. This, in

    turn, allows comparison with the FEA simulation Using Figures 35 and 36, it is known

    that 1500 lb force was applied 50 seconds into the test.

    Figure 35: Load and Displacement vs. Time

    50 seconds is when load equals to 1500 lbs

  • 38

    Figure 36: Strain vs. Time during Compression Testing

    Strain values that intersected with the time of experiment of 50 seconds correlate to a

    1500 lb load. These values are listed in Table 5.

    Table 5: Test Strain Readings vs. Simulation Predictions Strain Gages Strain - Physical Test Strain - Computer Model Percent Difference

    1500 lb 1500 lb1 0.1400% 0.1350% 3.70%2 0.0800% 0.0760% 5.26%3 0.0100% 0.0113% 11.50%4 0.0050% 0.0048% 4.17%5 0.0015% 0.0017% 11.76%6 0.1250% 0.1385% 9.75%7 0.1250% 0.1320% 5.30%8 0.0020% 0.0015% 33.33%9 0.0150% 0.0130% 15.38%

    50 seconds is when load equals to 1500 lbs

  • 39

    Conclusion and Further Research

    Figure 37 illustrates the final chassis and roll cage designs. For tubular and composite

    panel elements and assemblies, it has been demonstrated that CosmosWorks can provide

    accurate simulations of stress and deflection behavior. However, further research will be

    required to validate interface connections between space frames and composite panels

    that ensure adequate fatigue life.

    Figure 37: Final Chassis and Roll Cage Design

  • 40

    Appendices

    Appendix A, Nomenclature

    2

    2

    2sec

    ina=Acceleration ( )sec

    A=Area (in )Section Area (in )

    Center of Gravity

    Inside Diameter (in)Outside Diameter (in) Modulus of ElasticityForce ( )

    Critical Force to cause Buckling

    t

    g

    i

    o

    f

    cr

    Ac

    ddEF lb

    F

    ==

    =

    =

    ==

    =

    4

    m

    ( )

    . . Factor of Safety (dimensionless)Moment Area of Inertia (in )Length (in)

    Change in Length (in)Critical Length for Buckling (in)

    m=Mass (lb )Internal Pressure (psi)

    External Pr

    f

    c

    i

    ext

    lb

    F SIL

    LL

    PP

    =

    ==

    ∆ ==

    ==

    xx

    yy

    xy

    essure (psi)Inner Radius (in)Outer Radius (in)

    =Stress (psi)Von Mises Stress (psi)Stress in X-Direction (psi)Stress in Y-Direction (psi)

    Stress in Z-Direction (psi), , Shea

    i

    o

    E

    zz

    yz xz

    RRσσσσ

    σσ σ σ

    =

    =

    ===

    ==

    L

    circ

    rad

    r in respective Plane (psi)

    Longitudinal Stress (psi)Circumference Stress (psi)Radial Stress (psi)

    Strain (dimensionless)Poisson's Ratio (dimensionless)

    σσσευ

    ==

    =

    ==

  • 41

    Appendix B, Shop Drawings

  • 42

  • 43

  • 44

    Appendix C, CosmosWorks Load Cases

    CASE

    575 lb TOT.WEIGHTMULT.

    FACTORFORCE

    lbf

    SURFACE AREA FORCE APPLIED

    (IN2)PRESSURE

    (PSI)3 g bump 3 1725 10.5 164.295 g front 5 2875 183.113 15.705 g rear 5 2875 258.017 11.145 g side 5 2875 89.695 32.05

    3g angular 3 1725 N/A N/A3 g bump 3 1725 10.5 164.295 g front 5 2875 182.504 15.755 g rear 5 2875 270.7 10.625 g side 5 2875 89.693 32.05

    3g angular 3 1725 N/A N/A

    Fillet Focused Study

    APPLICABLEDESIGN(S)

    Original Study

    Triangle studyBeam support study

  • 45

    References

    1. “American Solar Challenge 2005 Regulations.” November, 2003. http://www.americansolarchallenge.org/event/asc2005/tech/asc2005Nov03.pdf (2 June, 2004) 2. Barber, J.R. Intermediate Mechanics of Materials. Boston: McGraw-Hill, 2001. 3. Callister, William D. Fundamentals of Materials Science and Engineering. 5th ed. New York: John Wiley & Sons, 2001. 4. Zienkiewics, O.C. The Finite Element Method. 3rd ed. London: McGraw-Hill, 1979. 5. Vishay Measurements Group, Inc. Student Manual for Strain Gage Technology USA: TD, 1997

  • 46

    Vita

    Bennett Alan Ford was born in Dallas Texas. After graduating from Highland

    Park High School, he entered Texas A&M University. There he developed an interest in

    automotive engineering and photovoltaic energy through involvement in Formula SAE

    and Solar Motorsports projects. He graduated with a Bachelor of Science and moved to

    Austin, where he began working in the photovoltaic energy industry. Bennett enrolled in

    graduate school at the University of Texas in January, 2010.

    Email: [email protected]

    This Report was typed by the author.