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ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

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K<br />

sh<br />

=<br />

2.<br />

3E<br />

sh<br />

2<br />

( ) 2<br />

1<br />

2<br />

1−ν<br />

( 4)<br />

Rsh<br />

sh<br />

The bulk modulus of the fluid has no effect on the contact stiffness of the shell.<br />

3-2: Analytical Model: Implicit equation for Fmax<br />

With the assumption of a conservative system and by writing the principle of Energy<br />

Conservation before the impact and at the point of maximum contraction:<br />

5<br />

1 2 1 2 1 2 2 1 2 1<br />

2<br />

2<br />

mshVsh + meVe = Ksh∆ xsh + KH ∆ xH + ( msh + me ) Vsh−e + msh ( VshSinα )<br />

2 2 2 5 2 2<br />

(5)<br />

∆ is the deformation due to the membrane and bending of shell, Vsk is the system<br />

xsh<br />

velocity of shell-torus object in the maximum contraction point, and ∆xH is the<br />

Hertzian contact deformation in the shell and torus body together. The impact occurs<br />

in "n" direction and the value ( ) 2<br />

1<br />

msh VshSinα is kinetic energy of the shell in "t"<br />

2<br />

direction during the impact. Using the principle of conservation of momentum:<br />

m V + m V = m + m V (6)<br />

h<br />

( )<br />

sh sh−n e e sh e sh−e− n<br />

Since the impact occurs in "n" direction, in the above equation, Vsk-n is the velocity of<br />

shell in "n" direction before impact, and Vsh-e-n is the common velocity of the two<br />

objects during the impact in "n" direction. By substituting Vsk-n in equation 6 and<br />

solving for Vsh-e-n, we obtain:<br />

xsh<br />

V<br />

sh−e m V Cosα + m V<br />

=<br />

m + m<br />

sh sh e e<br />

sh e<br />

∆ and ∆xH could be obtained from the equation of maximum transferred force<br />

(7)<br />

2<br />

⎛ F 3<br />

max ⎞<br />

x = ⎜<br />

⎟<br />

H<br />

(8)<br />

K H<br />

Fmax<br />

∆ xsh<br />

= And ∆<br />

K sh<br />

⎝ ⎠<br />

By replacing equations 7 and 8 into equation 5 and arranging:<br />

Where<br />

2<br />

max<br />

5<br />

4 F 3<br />

max<br />

sh<br />

2<br />

5<br />

K 3<br />

H<br />

F<br />

∆ U = + (9)<br />

K<br />

∆ U = m V Cos α + m V −<br />

( ) 2<br />

m V Cosα + m V<br />

2 2 2 sh sh e e<br />

sh sh e e<br />

msh + me<br />

Equation 9 is an implicit and approximate representation for the maximum transferred<br />

force which contains both Hertzian contact deformations in shell and torus object and<br />

also membrane and bending effect in the shell. It can be solved analytically for Fmax to<br />

obtain the maximum deformation and maximum acceleration of the fluid filled shell.<br />

∆x<br />

2<br />

3<br />

max max<br />

max ⎟ F ⎛ F ⎞<br />

= ∆x<br />

+ ∆ = + ⎜<br />

sh xH<br />

K sh K H<br />

a<br />

max =<br />

F<br />

m<br />

max<br />

sh<br />

⎝<br />

(11)<br />

⎠<br />

(10)

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