Question 5 of 8: Stepped Shaft with Distributed Torque
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exams May 2014 – 04-BS-6: Mechanics of Materials
3 hours duration, closed book (one hand-written aid sheet permitted). Any five of the eight
questions constitute a complete paper; all eight are solved below as a complete study resource.
Reference texts: R.C. Hibbeler, Mechanics of Materials, 10th ed.
(Ch. 5 torsion, Ch. 6 shear/moment diagrams & composite beams, Ch. 7 transverse shear,
Ch. 8 combined loadings, Ch. 9 stress transformation, Ch. 12 deflection by integration,
Ch. 13 buckling); F. Beer & E.R. Johnston, Mechanics of Materials; W. Gere &
B. Goodno, Mechanics of Materials (alternates). A wide-flange (W-shape) properties
table printed on the exam's last page supplies the section used in Question 8.
Question 5: Stepped Shaft with Distributed Torque (20 marks)
Stepped shaft, fixed at A: 12 kN·m (CW) at B, 7 kN·m (CCW) at C, 2.5 kN·m/m (CCW) distributed along CD.
Given.
Segment
Length (mm)
Diameter (mm)
AB
1000
80 (solid)
BC
700
60 (solid)
CD
1200
40 (solid)
G = 80 GPa, fy = 250 MPa (shear); TB = 12 kN·m CW;
TC = 7 kN·m CCW; distributed torque t = 2.5 kN·m/m CCW over CD; shaft
fixed at A.
Find. (a) Maximum shear stress and its radial variation. (b) Angle of twist at
D relative to the fixed end A.
Approach. Take CCW as positive. The shaft is fixed only at A (free at D), so
the internal torque at any section equals the sum of every applied torque between that section
and the FREE end D; within CD the distributed torque makes the internal torque vary linearly, so
its contribution to the twist needs an integral rather than a single $TL/GJ$ term.
Internal torque in CD (from D back to C). Measuring ξ from C
($0\le\xi\le1200$ mm), the torque remaining downstream of a cut at ξ is the distributed
torque still ahead of it: $$T_{CD}(\xi) = 2.5\frac{(1200-\xi)}{1000}\ \text{kN}\cdot
\text{m (CCW)}$$ so $T_{CD}$ is maximum right at C, $T_{CD}(0)=2.5(1.2)=+3.0$ kN·m, and
zero at D.
Internal torque in BC and AB (constant).
$$T_{BC} = T_C + T_{CD}(0) = 7+3.0 = +10.0\ \text{kN}\cdot\text{m (CCW)}$$
$$T_{AB} = T_B(\text{CW}) + T_{BC} = -12+10.0 = -2.0\ \text{kN}\cdot\text{m
(i.e. 2.0 kN}\cdot\text{m CW)}$$
(a) Shear stress in every segment ($\tau=T r/J$, $J=\pi d^4/32$).
$$\tau_{AB}=\frac{16(2.0\times10^6)}{\pi(80)^3} = 19.9\ \text{MPa}, \qquad
\tau_{BC}=\frac{16(10.0\times10^6)}{\pi(60)^3} = 235.8\ \text{MPa}$$
$$\tau_{CD,\max}=\frac{16(3.0\times10^6)}{\pi(40)^3} = \boxed{238.7\ \text{MPa}}$$
Even though $T_{BC}>T_{CD}$, the SMALLER 40 mm diameter of segment CD makes it govern (just) over
the 60 mm segment BC ($238.7>235.8$ MPa); both stay below the 250 MPa yield. Shear stress varies
LINEARLY from zero at the shaft centre to this 238.7 MPa maximum at the outer radius of segment
CD, immediately adjacent to C.
(b) Angle of twist at D relative to A. $J_{AB}=\pi(80)^4/32=
4.021\times10^6$ mm4, $J_{BC}=\pi(60)^4/32=1.272\times10^6$ mm4,
$J_{CD}=\pi(40)^4/32=0.2513\times10^6$ mm4.
$$\phi_{AB}=\frac{T_{AB}L_{AB}}{GJ_{AB}} = -0.356^\circ, \qquad
\phi_{BC}=\frac{T_{BC}L_{BC}}{GJ_{BC}} = +3.940^\circ$$
For CD, integrate the linearly varying torque over the segment:
$$\phi_{CD}=\frac{1}{GJ_{CD}}\int_0^{1200} 2.5\frac{(1200-\xi)}{1000}\,d\xi =
+5.129^\circ$$
$$\boxed{\phi_{D/A} = \phi_{AB}+\phi_{BC}+\phi_{CD} = -0.356+3.940+5.129 =
8.71^\circ}\ \text{(net CCW, viewed from D)}$$