Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format: National Exams, May 2014 — 07-Mec-B1 Advanced Machine Design. Open book, 3 hours, 100 marks. Part I (Problems 1–2) compulsory; answer three of the four Part II problems (3–6). All six problems are solved here as a complete study resource.
Reference texts: R. G. Budynas & J. K. Nisbett, Shigley’s Mechanical Engineering Design, 10th ed. (shafts & fatigue §6–7, journal bearings §12, clutches & brakes §16); R. C. Juvinall & K. M. Marshek, Fundamentals of Machine Component Design (lubrication, brakes); R. C. Hibbeler, Mechanics of Materials (beam deflection, impact).
Given. A simply-supported stepped steel shaft (800 mm between bearings) carries $P_1=10$ kN at B and $P_2=20$ kN at D; the central portion is a larger diameter than the two ends.
Given data (from the figure)
Station (from $R_A$)
Position
Feature
A
0 mm
bearing $R_A$; diameter 100 mm begins
B
200 mm
$P_1 = 10$ kN (down)
C
300 mm
step to diameter 125 mm
D
500 mm
$P_2 = 20$ kN (down)
E
700 mm
step back to diameter 100 mm
F
800 mm
bearing $R_F$
Steel modulus $E = 200$ GPa.
Find. (1) the maximum deflection and where it occurs, and (2) the fundamental critical (whirl) speed.
Stepped shaft: 100 mm ends (A–C, E–F), 125 mm centre (C–E); loads at B and D.
Approach. Get the reactions and moment diagram, integrate $M/EI$ twice with the diameter step carried explicitly in $I(x)$ (numeric), then estimate the fundamental critical speed from the load-station static deflections with the Rayleigh formula.
Bending moments. $M_B = 15(200) = 3.0$, $M_C = 3.5$, and the peak $M_D = R_F(300) = 4.5\ \text{kN}\!\cdot\!\text{m}$.
Second moments of area. $I_{100} = \pi(100)^4/64 = 4.909\times10^6\ \text{mm}^4$ for the ends; $I_{125} = \pi(125)^4/64 = 1.198\times10^7\ \text{mm}^4$ for the centre — a $2.44\times$ stiffer core.
Deflection. Double-integrating $M(x)/EI(x)$ with the two steps (at C and E) and $y=0$ at both bearings gives
$$\boxed{\,y_{\max} = 0.152\ \text{mm at }x \approx 356\ \text{mm}\ (\text{between B and D})\,}$$
Critical speed (Rayleigh). Using the static deflections at the load stations, $y_B$ and $y_D$, the fundamental whirl speed is
$$N_{cr} = \frac{60}{2\pi}\sqrt{\frac{g\,(W_1y_B+W_2y_D)}{W_1y_B^2 + W_2y_D^2}} = 2614\ \text{rpm}$$
Assessment. Any practical running speed here (order $10^2$–$10^3$ rpm) is well below $N_{cr}$, so the shaft runs sub-critically with a comfortable whirl margin.