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CONTINUUM MECHANICS for ENGINEERS

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Solution<br />

From Eq 6.7-8 the stress components are<br />

⎛ 2B<br />

D⎞<br />

σr= 2Ar<br />

− + sinθ<br />

3 ⎝ r r ⎠<br />

⎛ 2B<br />

D⎞<br />

σθ= 6Ar<br />

+ + sinθ<br />

3 ⎝ r r ⎠<br />

⎛ 2B<br />

D⎞<br />

τrθ=− 2Ar<br />

− + cosθ<br />

3 ⎝ r r ⎠<br />

The inner and outer radii of the beam are stress-free surfaces leading to<br />

boundary conditions of σ r = τ rθ = 0 at r = a, and at r = b. Also, the applied<br />

<strong>for</strong>ce P may be taken to be the summation of the shear stress acting over the<br />

free end θ = 0<br />

b<br />

τ ∫ rθ<br />

] θ=<br />

0<br />

a<br />

dr =−P<br />

These conditions lead to the three equations from which constants A, B, and<br />

D may be determined<br />

2B<br />

D<br />

2Aa<br />

− + = 0<br />

3<br />

a a<br />

2B<br />

D<br />

2Ab<br />

− + = 0<br />

3<br />

b b<br />

2 2<br />

b a<br />

2 2<br />

Ab a B D 2 2<br />

b<br />

( − ) − ln =<br />

− ( − )+<br />

ab<br />

a P<br />

Solving these three equations in three unknowns, the constants are determined<br />

to be<br />

( )<br />

P<br />

Pa b<br />

Pa + b<br />

A = ; B = − ;<br />

P = −<br />

2N2N N<br />

2 2 2 2<br />

where N = a 2 – b 2 + (a 2 + b 2 ) ln(b/a). Finally, use of these constants in the stress<br />

component equations gives

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