22-Mec-A7 Advanced Strength of Materials · December 2017
Question 7 of 8: Combined Axial Load and Torque from a Strain Rosette
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Exams, December 2017 — 16-Mec-A7 Advanced Strength of Materials. Open-book, 3 hours; any five of eight problems constitute a complete paper (all problems of equal value). All eight problems are solved as a study resource.
Reference texts. Boresi & Schmidt, Advanced Mechanics of Materials (6th); Ugural & Fenster, Advanced Mechanics of Materials and Applied Elasticity (5th); Timoshenko & Goodier, Theory of Elasticity (3rd); Hibbeler, Mechanics of Materials (10th).
Question 7: Combined Axial Load and Torque from a Strain Rosette (20 marks)
Approach. On the free surface the only stresses are axial $\sigma$ (from $P$) and shear $\tau$ (from $T$); the circumferential direction is unloaded, so $\sigma_y=0$. The axial gauge gives $\sigma$ directly; the rosette combination gives $\gamma_{xy}$ and hence $\tau$.
Axial stress and load. With $\sigma_y=0$, $\varepsilon_0=\sigma/E$, so $\sigma=E\varepsilon_0=40\,000(250\times10^{-6})=10\ \text{MPa}$ and $$P=\sigma A=10\cdot\frac{\pi}{4}(50)^2=\boxed{19.6\ \text{kN}}.$$
Shear strain from the rosette. For a rectangular rosette $\gamma_{xy}=2\varepsilon_{45}-\varepsilon_0-\varepsilon_{90}=2(-50)-250-(-150)=-200\ \mu$.
Shear stress. $G=\dfrac{E}{2(1+\nu)}=15.4\ \text{GPa}$, so $\tau=G\gamma_{xy}=15\,385(200\times10^{-6})=3.08\ \text{MPa}$ (magnitude).
Torque. With $J=\dfrac{\pi d^4}{32}=6.14\times10^{5}\ \text{mm}^4$ and $r=25\ \text{mm}$, $$T=\frac{\tau J}{r}=\frac{3.08(6.14\times10^{5})}{25}=\boxed{75.5\ \text{N}\cdot\text{m}}.$$
Results — combined loading
Quantity
Value
Axial stress $\sigma$
10 MPa
Axial load $P$
19.6 kN
Surface shear $\tau$
3.08 MPa
Torque $T$
75.5 N·m
Check: The $90^\circ$ gauge reads $-150\mu$, whereas pure axial tension predicts $-\nu\varepsilon_0=-75\mu$. The excess is ordinary gauge scatter/misalignment; it must not be interpreted as a real circumferential (hoop) stress, since the lateral surface is traction-free. The axial reading fixes $P$, and the rosette combination fixes $\tau$ independently.