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    Stress Concentration Factor Convergence Study of a Flat Plate with an

    Elliptical Hole Under Elastic Loading Conditions

    by

    Dwight Snowberger

    A Project Submitted to the Graduate

    Faculty of Rensselaer Polytechnic Institute

    in Partial Fulfillment of the

    Requirements for the degree of

    MASTER of ENGINEERING in MECHANICAL ENGINEERING

    Approved:

    _________________________________________

    Ernesto Gutierrez-Miravete, Project Adviser

    Rensselaer Polytechnic Institute

    Hartford, ConnecticutDecember 2008

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    CONTENTS

    LIST OF TABLES............................................................................................................. 3

    LIST OF FIGURES ........................................................................................................... 4

    ABSTRACT ...................................................................................................................... 6

    1. Introduction.................................................................................................................. 7

    2. Objectives .................................................................................................................... 8

    3. Methodology................................................................................................................ 9

    3.1 Schematics.....9

    3.2 Stress Concentration Factor Equations for an Elliptical Hole .10

    3.3 Boundary Conditions...11

    3.4 Elements..113.5 FEA Model..12

    4. Results........................................................................................................................ 14

    5. Discussion.................................................................................................................. 18

    6. Conclusion ................................................................................................................. 21

    7. References.................................................................................................................. 22

    8. Appendix A................................................................................................................ 23

    9. Appendix B................................................................................................................ 26

    10. Appendix C................................................................................................................ 32

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    LIST OF TABLES

    Table 1 Stress Concentration Factors for Various Ellipse radii

    Table 2a Plane42 Element Type FEA Model Results/Data

    Table 2b Plane82 Element Type FEA Model Results/Data

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    LIST OF FIGURES

    Figure 1. Flat Plate with an Elliptical Hole

    Figure 2. FEA model Boundary Conditions

    Figure 3. 4-noded Quad Element, (Reference 2)

    Figure 4. 8-noded Quad Element, (Reference 2)

    Figure 5. FEA Model Size Control Labels

    Figure 6 Magnified view of the stress distribution near the tip of the ellipse. (a/b = 1.25,

    b = 0.8, Plane 42 element type shown)

    Figure 7 Ellipse Short Radius, b vs Length of Element at the Right of Ellipse needed to

    obtain an accuracy of +/- 1% from the calculated stress concentration factor

    Figure 8 Ellipse Short Radius, b vs. # of Elements to the Right of the Ellipse needed to

    obtain an accuracy of +/- 1% from the calculated stress concentration factor

    Figure 9 Plane 42 FEA model results with a short radius of b = 0.1

    Figure 10 Plane 42 FEA model results with a short radius of b = 0.2

    Figure 11 Plane 42 FEA model results with a short radius of b = 0.3

    Figure 12 Plane 42 FEA model results with a short radius of b = 0.4

    Figure 13 Plane 42 FEA model results with a short radius of b = 0.5

    Figure 14 Plane 42 FEA model results with a short radius of b = 0.6

    Figure 15 Plane 42 FEA model results with a short radius of b = 0.7

    Figure 16 Plane 42 FEA model results with a short radius of b = 0.8

    Figure 17 Plane 42 FEA model results with a short radius of b = 0.9

    Figure 18 Plane 42 FEA model results with a short radius of b = 1.0

    Figure 19 Plane 82 FEA model results with a short radius of b = 0.1

    Figure 20 Plane 82 FEA model results with a short radius of b = 0.2

    Figure 21 Plane 82 FEA model results with a short radius of b = 0.3

    Figure 22 Plane 82 FEA model results with a short radius of b = 0.4

    Figure 23 Plane 82 FEA model results with a short radius of b = 0.5

    Figure 24 Plane 82 FEA model results with a short radius of b = 0.6

    Figure 25 Plane 82 FEA model results with a short radius of b = 0.7

    Figure 26 Plane 82 FEA model results with a short radius of b = 0.8

    Figure 27 Plane 82 FEA model results with a short radius of b = 0.9

    Figure 28 Plane 82 FEA model results with a short radius of b = 1.0

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    ACKNOWLEDGMENT

    I would like to thank my wife Amanda, and my son Steven for all of their support and

    sacrifice throughout my graduate education experience.

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    ABSTRACT

    A flat plate with an elliptical hole made of steel (E=30e6psi) with dimensions of 10x20

    inches with an elliptical hole of 1 for its long radius and a short radius that varied in

    length from 1 to 0.1 in 0.1 increments, was loaded with a 1000psi pressure load in a

    quartered FEA model created in ANSYS. A comparison was made between the equa-

    tion for a flat plate with a circular hole and an elliptical hole equation with the ellipse

    being a circle from Reference 1. The results were found to be the same, with a stress

    concentration of 2.54 using the elliptical hole equation and 2.50 for the circular hole

    equation. This showed that just the elliptical hole equation could be used to calculate the

    stress concentration for all cases including when the ellipse was a circle.

    Two different finite elements (Plane42 and Plane82 from the ANSYS element li-brary) were used on the model. These elements were used to show that increasing the

    order of the element is one way to improve an FEA model. This was shown by measur-

    ing the length of the element at the tip of the ellipse. The Plane42 (4-noded quad)

    element had the shorter element length with 0.0095 while the Plane82 (8-noded quad)

    had a length of 0.0147. Since the Plane82 element had a longer length than the Plane42

    on the same model it meant that the Plane82 element was better at determining the stress

    concentration factor that is within +/- 1% of the stress concentration as calculated from

    the closed form solution.

    Finally, it was also possible to produce a more accurate FEA model by increasing

    the number of elements in a mesh. To show this, the number of elements used to mesh

    the model were recorded and compared for each ellipse size. The Plane42 model ranged

    from using 7 elements at the ellipse tip for the case of the ellipse being a circle to

    needing 46 elements and an element scaling factor of 32 when the ellipse had a short

    radius of 0.1. The Plane 82 model needed 4 elements with no scaling factor for thecircular hole case to using 38 elements with a scaling factor of 23 when the short radius

    was 0.1. All of the values for the number of elements and element scaling factors were

    recorded for each model only when the model produced a stress concentration that was

    within +/- 1% of the stress concentration as calculated from the closed form solution.

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    1. Introduction

    Changes in geometry such as a circular hole or an elliptical hole cause increases in the

    amount of stress created at these discontinuities. This stress increase is more commonly

    known as the stress concentration factor. This factor is a ratio between the maximum

    stress produced at the discontinuity divided by the nominal stress far away from the hole.

    These factors have been well-studied and documented, with closed form solutions for

    more common geometries available in such texts as Reference 1. For an elliptical hole

    in a flat plate, the stress concentration will be different depending on the narrowness of

    the ellipse.

    FEA programs such as ANSYS can be used to approximate the stress concentration

    factor as calculated using a closed form equation for a given geometry. The accuracy of

    the model can be increased by two ways. One is by increasing the mesh density around

    the discontinuity in order to better capture the increase in stress. The other method is to

    increase the order of the element, such as using an 8-noded quad element vs. a 4-noded

    quad element.

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    2. Objectives

    The objective of this project will be to study the effect an elliptical hole has on the stress

    distribution of a flat plate as the sharpness of the ellipse increases from a circle to a

    narrow crack. It will be shown that as the ellipse sharpness increases, more elements

    will be needed to accurately capture the stress concentration factor to be within 1% of

    the calculated value from Reference (1) for the specific geometry of a flat plate that is

    10x20 inches and a 2-inch long diameter elliptical hole. Two element types will be

    compared, which are the 4-noded quad (ANSYS Plane42) and the 8-noded quad

    (ANSYS Plane82). Finally, the equations for a flat plate with a circular hole and an

    elliptical hole will be compared for the case when the elliptical hole is a circle in order to

    show that the results are similar enough that the elliptical equations can be used for the

    case when the ellipse becomes a circle.

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    3. Methodology

    3.1 Schematics

    This report will focus on the specific geometry of an elliptical hole in a flat plate in

    Figure 1.

    b = short radiusa = long radius

    D = width of the flat plate

    Figure 1 Flat Plate with an Elliptical Hole.

    ba

    1000psi

    2

    D = 10

    20

    1000psi

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    The plates material will be ordinary steel with a Youngs Modulus of 30e6 psi and the

    model will use a pressure load of 1000psi (nominal stress of the model). One important

    point to note, this report is a study of the stress concentration factor under elastic loading

    conditions. The materials modulus does not have any effect on the outcome of the

    results, as long as the stress does not exceed the materials yield point (36,000 psi for

    steel), the maximum stress will always be 1000psi multiplied by the stress concentration

    factor.

    3.2 Stress Concentration Factor Equations for an Elliptical Hole

    Equation (1) (Reference 1) is the stress concentration factor for an elliptical hole in a flat

    plate. Equation (1) is only valid if the a/b ratio is between 0.5 and 10. For this project

    the ratio of a/b varies from 1 to 10.

    (1)

    where:

    a = the long radius of ellipse (1)

    b = the short radius of ellipse (will be varied from 1 to 0.1 in 0.1 increments)D = width of the flat plate (10 inches)

    K = stress concentration factor for an elliptical hole in a flat plate.

    The special case of where b = a for a circular hole, the elliptical hole equation (1) yields

    a stress concentration of 2.54. For the same plate, using the equation for a circular hole

    from Reference (1), the stress concentration is 2.50. This is only a 1.6% difference.

    Therefore, the elliptical hole stress concentration equation (1) will be used for both the

    circular and elliptical hole cases.

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    3.3 Boundary Conditions for FEA model

    Figure 2 shows the boundary conditions for the FEA model. The flat plate from Figure

    1, was modeled as a quarter plate with the left vertical edge constrained in the x direction

    and the bottom edge being constrained in the y direction. The right vertical edge of the

    model will be a free edge and the top edge will be where the pressure load of 1000psi is

    applied.

    Figure 2 FEA model Boundary Conditions

    3.4 Elements

    There will be two element types used in this report. The first element is a 4-noded quad

    element. In ANSYS the name of the element type is Plane42 shown in Figure 3.

    Figure 3. 4-noded Quad Element, (Reference 2)

    1000psi

    Free EdgeEdge constrained, dx = 0

    Edge constrained, dy = 0x

    Load Applied on Edge

    Ellipse

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    The second element to be used is an 8-noded quad element, called the Plane82 in

    ANSYS, shown in Figure 4.

    Figure 4. 8-noded Quad Element, (Reference 2)

    3.5 FEA Model

    The 2-D FEA model in ANSYS (see Appendix A for log file code) was created to

    accurately determine the stress concentration within 1% of the closed form solution of

    equation (1) for an elliptical hole in a flat plate. In order to do this it was necessary to

    set up manual controls for ANSYS to mesh the model and easily capture how many

    elements were used at the point of highest stress, which is at the ellipse tip, to calculate

    the stress concentration factor to be within 1% of the closed form solution calculated by

    equation (1). Figure 5 is a schematic of the FEA models size control limits, which can

    be changed by the user to either increase or decrease the mesh density at the hole and

    around the whole model. These labels are referred to in the FEA model code of Appen-

    dix A.

    Figure 5. FEA Model Size Control Labels

    Each highlighted edge

    of the model will have

    its own size controls.

    Ellipse

    Right Side of Flat PlateLeft Side of Ellipse

    To of Plate

    Right Side of

    Ellipse Tip

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    Additional manual mesh control of the FEA model is achieved by use of the LESIZE

    command in ANSYS. Below is a sample line from the FEA model text file.

    LESIZE,_Y1, , ,10, 3, , , ,1

    This command will generate 10 elements on the line that it is assigned to, and the 3 will

    size those elements based on a scaling factor where the first element will be 3 times

    smaller than the last node in the line. This means that the elements will become gradu-

    ally larger the farther away they are from the hole. The scaling factor command allows

    the user to optimize the number of elements used in a model, since the farther away an

    element is from the elliptical hole, the less its stress is going to change. Because the

    greatest stresses will be produced on the right side of the ellipse tip, smaller elements

    will be needed than at the top of the plate where larger elements can be used.

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    4. Results

    Table 1 shows the stress concentration factor for each of the 10 ellipses used. The first

    column is the a/b ratio, which is the ratio between the long and short radius of the ellipse

    (as seen in Figure 1), the 4 constants C1-C4 needed in equation (1), and the stress

    concentration factor using equation (1). The last two columns of Table 1 are the stress

    concentration factor tolerance, which will be used to determine if the FEA model from

    ANSYS (Appendix A) has an adequate mesh density. This tolerance was chosen as +/-

    1% from the calculated stress concentration (K) in equation (1).

    a/b a b C1 C2 C3 C4 K K+1% K-1%

    10.00 1.00 0.10 21.00 -25.25 32.17 -25.92 17.03 17.20 16.86

    5.00 1.00 0.20 11.00 -12.81 14.50 -10.69 8.93 9.02 8.84

    3.33 1.00 0.30 7.67 -8.67 9.14 -6.14 6.25 6.31 6.19

    2.50 1.00 0.40 6.00 -6.59 6.66 -4.07 4.92 4.96 4.87

    2.00 1.00 0.50 5.00 -5.35 5.28 -2.93 4.12 4.16 4.08

    1.67 1.00 0.60 4.33 -4.52 4.42 -2.24 3.59 3.62 3.55

    1.43 1.00 0.70 3.86 -3.92 3.85 -1.78 3.21 3.24 3.18

    1.25 1.00 0.80 3.50 -3.48 3.44 -1.47 2.93 2.96 2.90

    1.11 1.00 0.90 3.22 -3.13 3.15 -1.24 2.71 2.74 2.68

    1.00 1.00 1.00 3.00 -2.86 2.93 -1.08 2.54 2.56 2.51

    Table 1 Stress Concentration Factors for Various Ellipse radii

    Table 2a and 2b show the results of the FEA models for the Plane 42 and the Plane 82

    elements. This data was recorded for each model only when the maximum stress

    produced at the ellipse tip divided by the nominal stress (1000psi) resulted in a stress

    concentration factor that was within the +/- 1% tolerance from the stress concentration

    calculated by equation (1).

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    This is an explanation of Table 2a and 2bs columns, and Figure 5 gives a graphical

    representation for the naming/location of the edges of the model.

    b = short radius of the ellipse (inch),

    Kroarks = Stress concentration factor calculated using equation (1).

    K+1% and K-1% is the stress concentration factor, Kroarks +/- 1% in order to establish

    a tolerance which will determine if the model has been meshed properlyGnom = Nominal stress in the plate far away from the hole. This will be the 1000psi

    pressure load. (psi),

    Gmax = Maximum stress created at the ellipse tip which is where the highest stresses

    are produced. (psi),

    Kmodel = Stress concentration factor obtained from the FEA model in ANSYS, whichis calculated by dividing Gmax/Gnom.

    Right = Number of elements that were on the bottom edge of the model, which was to

    the right of the ellipse tip.

    Scale = Scaling factor used in the LESIZE command, which scaled the elements,

    Left = Number of elements that were used to generate the mesh on the left vertical edge

    of the model. This is also the side that was constrained to not move in the x-direction.Right Side = Number of elements that were applied to the right vertical edge of the

    model. This was the unconstrained, free edge of the model.

    Top = Number of elements that were applied to the top of model, which was the edge

    that the 1000psi pressure load was applied.

    Element Length on Right of Ellipse = Length of the element that is on the Right Side

    edge of the model at the tip of the ellipse. Figure 6 shows the length dimension of the

    element that was recorded for this column.

    Figure 5. FEA Model Size Controls Labels, re-shown from page 12

    Each edge of themodel will have its

    own size controls.

    Ellipse

    Right SideLeft

    To

    Right

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    Figure 6 Magnified view of the stress distribution at the tip of the ellipse. (a/b = 1.25, b =

    0.8, Plane 42 element type shown)

    Length of element

    y

    x

    Ellipse

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    5. Discussion

    The first objective of this report is to show that the classical solution for a circular hole

    in a flat plate is the same as using the closed form solution for an elliptical hole in a flat

    plate with a short radius of b = a = 1 which is a circular hole. The results of the closed

    form equation (Reference 1) for a flat plate with a circular hole produced a stress con-

    centration of 2.50 and the elliptical hole equation (Reference 1) had a stress

    concentration of 2.54. These results are within 1.6% of each other, which meant just the

    elliptical equations were used to calculate the stress concentration factor for all cases

    including when the ellipse become a circle.

    The second objective was to show that it is possible to improve the results of an

    FEA model by increasing the order of the elements used in the model. Based on the

    results gathered from the FEA models from Tables 2a and 2b, the following figure was

    created.

    Length of Element at the Right of Ellipse vs Ellipse Short Radius

    0

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    1.1

    0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

    b, Ellipse Short Radius (inch)

    LengthofEllementtoRightofEllipse(inch)

    Plane82

    Plane42

    Figure 7 Ellipse Short Radius, b vs Length of Element at the Right of Ellipse needed toobtain an accuracy of +/- 1% from the calculated stress concentration factor

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    Figure 7 shows that as the elliptical hole became narrower a more refined mesh den-

    sity was required. More importantly it shows that the Plane42 element type required the

    most amount of refinement, because the element to the right of the ellipse tip (as shown

    in Figure 6) needed to be smaller in order to capture the stress concentration that was

    within +/- 1% of the actual stress concentration as calculated from closed form solutions.

    In Figure 7, it can be seen that the Plane42 element type always used a smaller length of

    element compared to the Plane82 element. The Plane42 element had a length of 0.0095

    vs. the Plane82s length of 0.0147 when the ellipse had a short radius of 0.1.

    The third objective of this report was to show that an FEA model could increase in

    accuracy by increasing the number of elements used in a model. Figure 8 shows that as

    the ellipse became narrower, more elements were needed at the ellipse tip in order to

    obtain a stress concentration factor that was within +/- 1% of the actual stress concentra-

    tion as calculated from closed form solutions. The figure also shows the Plane82

    element was more efficient at meshing the model since it required less elements in order

    to capture the stress concentration factor within the specified tolerance of +/-

    1%.

    Ellipse Short Radius, b vs. # of Elements to the Right of the Ellipse

    0

    5

    10

    15

    20

    25

    30

    35

    40

    45

    50

    0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

    b, Ellipse Short Radius (inch)

    #ofElementstotheRightoftheEllipse Plane82

    Plane42

    Figure 8 Ellipse Short Radius, b vs. # of Elements to the Right of the Ellipse needed toobtain an accuracy of +/- 1% from the calculated stress concentration factor

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    Finally, this report shows the mesh density needed to calculate the stress concentration

    factor within 1% of the closed form solution. The values needed to generate a mesh

    density that falls within 1% of the closed form solution for the stress concentration factor

    are shown in Tables 2a and 2b. These values are for the specific geometry of an elliptical

    hole in a flat plate with an a/b ratio varying from 1 to 10, a width of 10 and subjected to

    a pressure load of 1000psi, as can be seen in Figure 1, shown below for convenience.

    Figure 1 Flat Plate with an Elliptical Hole.

    ba

    1000psi

    2

    D = 10

    20

    1000psi

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    6. Conclusion

    Discontinuities in a geometry such as an elliptical hole create an increase in the stress

    distribution known as the stress concentration factor. It was shown that the results for

    the stress concentration calculated using the elliptical hole equations when the ellipse

    became a circle were the same. Because of this, the elliptical hole equation was used for

    all cases including the circular hole case.

    It was also shown that the accuracy of an FEA model can be increased by two

    methods. The first method was to increase the order of the element used in the model. It

    was shown that the 4-noded quad element (Plane42) needed smaller elements and more

    of them in order to capture the stress concentration factor to be within +/- 1% of the

    closed form solution for the stress concentration factor for this specific geometry, as

    compared to the 8-noded quad element (Plane82). The second method was to increase

    the number of elements in the model. This was done by showing that as the ellipse

    became narrower, more elements were needed in order to obtain the stress concentration

    factor within 1% of the closed form solution to equation (1) for this specific geometry.

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    7. References

    1 Young, Warren; Budynas, Richard,Roarks Formulas for Stress and Strain

    2 ANSYS Help Menu, ANSYS INC., Release 10.0A1 UP20060105

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    8. Appendix A

    This appendix contains the FEA code used to create all of the ANSYS models for this

    project.

    /CLEAR,START

    /PREP7!

    ET,1,PLANE82

    !

    /REPLOT,RESIZE

    !

    MPTEMP,,,,,,,,

    MPTEMP,1,0

    MPDATA,EX,1,,30e6

    MPDATA,PRXY,1,,.3

    /REPLOT,RESIZE

    CYL4,0,0,1

    FLST,2,1,5,ORDE,1

    FITEM,2,1

    !

    ! ------------------ Ellipse Size ---------------

    !

    ARSCALE,P51X, , ,1,.1,1, ,0,1

    !

    RECTNG,0,5,0,10,

    FLST,2,1,5,ORDE,1

    FITEM,2,2

    FLST,3,1,5,ORDE,1

    FITEM,3,1

    ASBA,P51X,P51X,SEPO,DELETE,DELETE

    !

    FLST,5,1,4,ORDE,1

    FITEM,5,10CM,_Y,LINE

    LSEL, , , ,P51X

    CM,_Y1,LINE

    CMSEL,,_Y

    !

    !--------- Right Side Ellipse (Horizontal) -----------

    !

    LESIZE,_Y1, , ,38, 23, , , ,1

    !

    FLST,5,1,4,ORDE,1

    FITEM,5,9

    CM,_Y,LINE

    LSEL, , , ,P51XCM,_Y1,LINE

    CMSEL,,_Y

    !

    !------------ Ellipse ------------

    !

    LESIZE,_Y1, , ,32,12 , , , ,1

    !

    FLST,5,1,4,ORDE,1

    FITEM,5,13

    CM,_Y,LINE

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    LSEL, , , ,P51X

    CM,_Y1,LINE

    CMSEL,,_Y

    !

    !---------------- Left Side of Ellipse (Vertical) -----------

    !

    LESIZE,_Y1, , ,38, 2, , , ,1

    !FLST,5,1,4,ORDE,1

    FITEM,5,11

    CM,_Y,LINE

    LSEL, , , ,P51X

    CM,_Y1,LINE

    CMSEL,,_Y

    !

    !------------- Right Side of Flat Plate -------------

    !

    LESIZE,_Y1, , ,22, 1, , , ,1

    !

    FLST,5,1,4,ORDE,1

    FITEM,5,12

    CM,_Y,LINE

    LSEL, , , ,P51X

    CM,_Y1,LINE

    CMSEL,,_Y

    !

    !--------------- Top Side of Flat Plate -------------------

    !

    LESIZE,_Y1, , ,11,1 , , , ,1

    !

    MSHKEY,0

    CM,_Y,AREA

    ASEL, , , , 3

    CM,_Y1,AREA

    CHKMSH,'AREA'CMSEL,S,_Y

    !

    AMESH,_Y1

    !

    CMDELE,_Y

    CMDELE,_Y1

    CMDELE,_Y2

    !

    FINISH

    /SOL

    FLST,2,1,4,ORDE,1

    FITEM,2,13

    !/GO

    DL,P51X, ,UX,0

    FLST,2,1,4,ORDE,1

    FITEM,2,10

    !

    /GO

    DL,P51X, ,UY,0

    FLST,2,1,4,ORDE,1

    FITEM,2,12

    /GO

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    !

    ! ---------- Pressure Load (-1000psi) -----------

    !

    SFL,P51X,PRES,-1000,

    /STATUS,SOLU

    SOLVE

    FINISH

    /POST1!

    /DSCALE,ALL,OFF

    /EFACET,1

    PLNSOL, S,EQV, 1,1.0

    !

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    9. Appendix B

    This appendix shows plots of the final FEA models for the Plane42 element type.

    Figure 9 Plane 42 FEA model results with a short radius of b = 0.1

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    Figure 10 Plane 42 FEA model results with a short radius of b = 0.2

    Figure 11 Plane 42 FEA model results with a short radius of b = 0.3

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    Figure 12 Plane 42 FEA model results with a short radius of b = 0.4

    Figure 13 Plane 42 FEA model results with a short radius of b = 0.5

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    Figure 14 Plane 42 FEA model results with a short radius of b = 0.6

    Figure 15 Plane 42 FEA model results with a short radius of b = 0.7

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    Figure 16 Plane 42 FEA model results with a short radius of b = 0.8

    Figure 17 Plane 42 FEA model results with a short radius of b = 0.9

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    Figure 18 Plane 42 FEA model results with a short radius of b = 1.0

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    10. Appendix C

    This appendix shows plots of the final FEA models for the Plane82 element type.

    Figure 19 Plane 82 FEA model results with a short radius of b = 0.1

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    Figure 20 Plane 82 FEA model results with a short radius of b = 0.2

    Figure 21 Plane 82 FEA model results with a short radius of b = 0.3

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    Figure 22 Plane 82 FEA model results with a short radius of b = 0.4

    Figure 23 Plane 82 FEA model results with a short radius of b = 0.5

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    Figure 24 Plane 82 FEA model results with a short radius of b = 0.6

    Figure 25 Plane 82 FEA model results with a short radius of b = 0.7

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    Figure 26 Plane 82 FEA model results with a short radius of b = 0.8

    Figure 27 Plane 82 FEA model results with a short radius of b = 0.9

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    Figure 28 Plane 82 FEA model results with a short radius of b = 1.0