22-Mec-A7 Advanced Strength of Materials · May 2017
Question 1 of 8: Thick-Walled Cylinder – Allowable Internal Pressure
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exams – May 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).
Given. A closed-end thick cylinder loaded by internal pressure ten times the external pressure, sized by the wall radii and the yield strength.
Given data
Symbol
Value
ri
0.10 m (Di/2)
ro
0.16 m (Do/2)
σY
315 MPa
ν
0.29
pi : pe
10 : 1
Find. The largest internal pressure pi the wall can carry at first yield, evaluated separately with the von Mises and Tresca criteria.
Cylinder cross-section: bore radius ri=0.10 m, outer radius ro=0.16 m, internal pressure ten times the external pressure. The critical material point is the bore.
Approach. Evaluate the Lamé stresses at the bore (where they are largest), take the closed-end axial stress as the mean of radial and hoop, then set each yield criterion equal to σY and solve for pi.
Bore stresses from Lamé. With $p_i=10p$ and $p_e=p$, at $r=r_i$ the radial stress is $\sigma_r=-p_i=-10p$ and the hoop stress is $$\sigma_\theta=\frac{p_i(r_i^2+r_o^2)-2p_e r_o^2}{r_o^2-r_i^2}=\frac{10p(0.01+0.0256)-2p(0.0256)}{0.0156}=19.538\,p.$$
Closed-end axial stress. For a capped cylinder the axial stress is the mean of the in-plane stresses, $\sigma_z=\tfrac12(\sigma_r+\sigma_\theta)=\tfrac12(-10p+19.538p)=4.769\,p$, so the ordered principals are $\sigma_\theta \gt \sigma_z \gt \sigma_r$.
Tresca criterion. Yield when $\sigma_\theta-\sigma_r=\sigma_Y$: $(19.538+10)p=29.538\,p=315\Rightarrow p=10.66$, hence $\boxed{p_i=10p=106.6\ \text{MPa}}$.
Von Mises criterion. $\sigma_{vm}=\sqrt{\tfrac12\big[(\sigma_\theta-\sigma_z)^2+(\sigma_z-\sigma_r)^2+(\sigma_r-\sigma_\theta)^2\big]}=25.58\,p=315\Rightarrow p=12.31$, hence $\boxed{p_i=123.1\ \text{MPa}}$.
Compare. Because $\sigma_z$ is exactly the mean of $\sigma_\theta$ and $\sigma_r$, von Mises gives $2/\sqrt3=1.155$ times the Tresca pressure—Tresca is the conservative design value.
Check: The ends are taken as closed (capped), giving $\sigma_z=\tfrac12(\sigma_r+\sigma_\theta)$ from axial equilibrium. Poisson’s ratio is not required by either stress-based yield criterion; it would enter only a deformation calculation. If the ends were open, $\sigma_z=0$ and the von Mises pressure would change slightly, while Tresca (governed by $\sigma_\theta-\sigma_r$) is unchanged.