Problem 10-53.  Solution 2.

In torsion, sx = 0, sy = 0, and sz = 0.  By the stress-strain relations ex = 0 and ey = 0.  The strain transformation formulas with q = 30 deg. yield

ex' = excos2q + eysin2q + gxysinqcosq  = gxysqrt(3)/4

ey' = exsin2q + eycos2q - gxysinqcosq   = -gxysqrt(3)/4

With ex' = - ey' = - 45(10-6), the two equations are consistent, and they yield

 gxy = - 45(10-6)(4)/sqrt(3) = -1.0392(10-4)

 txy = Ggxy = -7.794 MPa

Because of the orientation of the (x, y) axes we have

t = trq = - txy = 7.794 MPa

This is the same value as for  t  in Solution 1.  The rest of the solution is the same as before.

Problem 10-53. Solution 3.

Since sz = 0, we can use the stress-strain relations of Plane Stress:

sx' = [E/(1-n2)](ex' + ey')

sy' = [E/(1-n2)](ex' + ey')

With E = 200(103) MPa, n = 0.32, and  ex' = - ey' = - 45(10-6), obtain

sx' = - sy' = - 6.8182 MPa

With sx = 0, sy = 0, and q = 30 deg., the stress transformation formulas yield

sx' = sxcos2q + sysin2q + 2txysinqcosq  = txysqrt(3)/2

sy' = sxsin2q + sycos2q - 2txysinqcosq   = -txysqrt(3)/2

Thus

txy = 2sx'/sqrt(3) = - 7.873 MPa

This differs slightly from the previous solution in which txy = - 7.794 MPa.  The reason for this is that the given values for E, n, and G are slightly inconsistent with a truly isotropic material. With E = 200 GPa, and n = 0.32, the isotropic G would be

Giso = E/2(1 + n) = 75.76 GPa

The given G is 75 GPa.