22-Mec-A7 Advanced Strength of Materials · May 2015
Question 7 of 8: Sizing a Square Bar Under Axial Load and Torque
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Exams, May 2015 — 07-Mec-A7 Advanced Strength of Materials. Open-book, 3 hours. Eight problems of equal value; any five constitute a complete paper. All eight are solved here.
Reference texts. Ugural & Fenster, Advanced Strength and Applied Elasticity (4th ed.); Boresi & Schmidt, Advanced Mechanics of Materials (6th ed.); Hibbeler, Mechanics of Materials (10th ed.); Timoshenko & Goodier, Theory of Elasticity.
Question 7: Sizing a Square Bar Under Axial Load and Torque (20 marks)
Given. Square bar, side b, carrying axial P and torque T; design by Tresca with a factor of safety of 3.
Given data
Yield stress, σY
310 MPa
Axial force, P
195 kN
Torque, T
17 kN·m
Factor of safety, N
3
Square-torsion constant
τmax = T/(0.208 b3)
Find. The minimum side b for (a) axial (normal) P and (b) P applied parallel to the section.
Square-section bar built into a rigid support, loaded by centroidal axial force P and torque T.
Approach. Combine the normal stress from P with the torsional shear from T at the most-stressed point; the Tresca criterion limits the maximum in-plane shear to $\sigma_Y/(2N)$. Solve the resulting nonlinear equation for b.
Allowable shear. The maximum-shear-stress criterion with safety factor 3 gives $$\tau_{\text{allow}}=\frac{\sigma_Y}{2N}=\frac{310}{6}=51.7\ \text{MPa}.$$
(a) Axial + torsion. The axial stress is $\sigma=P/b^2$ and the torsional shear $\tau=T/(0.208b^3)$. The largest shear in the element combining a normal and a shear stress is $\tau_{\max}=\sqrt{(\sigma/2)^2+\tau^2}$, so $$\sqrt{\Big(\frac{P}{2b^2}\Big)^2+\Big(\frac{T}{0.208b^3}\Big)^2}=51.7\ \text{MPa}\ \Rightarrow\ \boxed{b=117\ \text{mm}.}$$ At this size $\sigma=14.3$ MPa and $\tau=51.2$ MPa—torsion dominates.
(b) P applied parallel to the section. Now P is a transverse shear force, not an axial load; its peak (centroidal) shear in a rectangular section is $\tau_P=1.5P/b^2$, acting on the same faces as the torsional shear, so they add: $$\frac{1.5P}{b^2}+\frac{T}{0.208b^3}=51.7\ \text{MPa}\ \Rightarrow\ \boxed{b=133\ \text{mm}.}$$ A larger section is needed because a transverse shear stress superposes directly on the torsional shear rather than combining under a square root.
Check: Part (b) superposes the maximum transverse-shear stress on the maximum torsional shear. Both peak at the mid-point of the side faces parallel to P (the neutral axis for transverse shear, the mid-side for torsion of a square), and on one of those faces they act in the same direction, so the arithmetic sum is the elementary-theory maximum, not an over-estimate. Bending from P is neglected because no member length or eccentricity is given; if a length were supplied, the bending stress at the support would have to be added to part (b).