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.