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Stresses on 40 degree plane; principal stresses

Short answer

On the 40° inclined plane: normal stress 71.28 MPa, shear stress -4.64 MPa. Principal stresses are 71.62 MPa and 8.38 MPa at 35.78° and 125.78°; maximum shear 31.62 MPa with average normal 40.00 MPa.

Determine the normal and shearing stress on the inclined plane at the angle of 40∘40^\circ to the vertical. Also calculate principal stresses and their planes. [Figure: element with 30 MPa30\ \text{MPa} acting vertically on the top and bottom faces, 50 MPa50\ \text{MPa} on the left and right faces, and shear stress 30 MPa30\ \text{MPa}.]

Reading of the figure: both normal stresses are tensile: σx=50\sigma_x = 50 MPa (left/right faces), σy=30\sigma_y = 30 MPa (top/bottom faces), and the shear stress is τxy=30\tau_{xy} = 30 MPa. The plane is at 40∘40^\circ to the vertical, so its normal is at 40∘40^\circ to the xx-axis.

Stresses on the inclined plane (θ=40∘\theta = 40^\circ)

σn=σx+σy2+σx−σy2cos⁡2θ+τxysin⁡2θ=40.00+(10.00)cos⁡80∘+(30.00)sin⁡80∘=71.28 MPaτθ=−σx−σy2sin⁡2θ+τxycos⁡2θ=−(10.00)sin⁡80∘+(30.00)cos⁡80∘=−4.64 MPa\begin{aligned} \sigma_n &= \frac{\sigma_x+\sigma_y}{2} + \frac{\sigma_x-\sigma_y}{2}\cos 2\theta + \tau_{xy}\sin 2\theta \\ &= 40.00 + (10.00)\cos 80^\circ + (30.00)\sin 80^\circ = 71.28\ \text{MPa} \\ \tau_\theta &= -\frac{\sigma_x-\sigma_y}{2}\sin 2\theta + \tau_{xy}\cos 2\theta \\ &= -(10.00)\sin 80^\circ + (30.00)\cos 80^\circ = -4.64\ \text{MPa} \end{aligned}

Resultant stress on the plane =71.282+(−4.64)2=71.43 MPa= \sqrt{71.28^2+(-4.64)^2} = 71.43\ \text{MPa}, inclined at 3.72∘3.72^\circ to the normal of the plane.

Principal stresses

σ1,2=σx+σy2±(σx−σy2)2+τxy2=40.00±(10.00)2+(30.00)2=40.00±31.62\sigma_{1,2} = \frac{\sigma_x+\sigma_y}{2} \pm \sqrt{\left(\frac{\sigma_x-\sigma_y}{2}\right)^2+\tau_{xy}^2} = 40.00 \pm \sqrt{(10.00)^2+(30.00)^2} = 40.00 \pm 31.62

σ1=71.62 MPa\sigma_1 = 71.62\ \text{MPa} and σ2=8.38 MPa\sigma_2 = 8.38\ \text{MPa}.

Principal planes

tan⁡2θp=2τxyσx−σy=2(30.00)20.00⇒2θp=71.57∘\tan 2\theta_p = \frac{2\tau_{xy}}{\sigma_x-\sigma_y} = \frac{2(30.00)}{20.00} \Rightarrow 2\theta_p = 71.57^\circ

So θp=35.78∘\theta_p = 35.78^\circ (normal of the plane carrying σ1\sigma_1) and 125.78∘125.78^\circ (normal of the plane carrying σ2\sigma_2), both measured anticlockwise from the xx-axis. There is no shear stress on these planes.

Maximum shear stress (extra)

τmax=σ1−σ22=(σx−σy2)2+τxy2=31.62 MPa\tau_{max} = \frac{\sigma_1-\sigma_2}{2} = \sqrt{\left(\frac{\sigma_x-\sigma_y}{2}\right)^2+\tau_{xy}^2} = 31.62\ \text{MPa}

It acts on planes at 45∘45^\circ to the principal planes, i.e. at θs=80.78∘\theta_s = 80.78^\circ and 170.78∘170.78^\circ. The normal stress on these planes is σx+σy2=40.00 MPa\frac{\sigma_x+\sigma_y}{2} = 40.00\ \text{MPa}.

Answer: σn=71.28\sigma_n = 71.28, τ=−4.64\tau = -4.64 on the inclined plane; σ1=71.62\sigma_1 = 71.62, σ2=8.38\sigma_2 = 8.38 at θp=35.78∘\theta_p = 35.78^\circ and 125.78∘125.78^\circ; τmax=31.62\tau_{max} = 31.62 with normal stress 40.0040.00 (MPa).

✓ Answer checked by Claude Opus 5.5 (high effort)

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