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22-Mec-B1 Advanced Machine Design · May 2018

Question 3 of 6: Double Short-Shoe External Drum Brake

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format: National Exams, 16-Mec-B1 Advanced Machine Design, May 2018. Open book, 3 hours, 100 marks. Part I (Problems 1 & 2) is compulsory; candidates answer only three of the four Part II problems (3–6). All six problems are solved here as a complete study resource.

Reference texts. Budynas & Nisbett, Shigley’s Mechanical Engineering Design (10th ed.) — shaft/fatigue §7, bolted joints §8, journal bearings §12, brakes §16, power screws §8–2; Juvinall & Marshek, Fundamentals of Machine Component Design; Norton, Machine Design: An Integrated Approach.

Question 3: Double Short-Shoe External Drum Brake (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. Two opposed short shoes press on a drum of radius 40 mm and width 60 mm; each shoe pivots on a lever with the actuating force applied at the given $a,b$ offsets.

Given data
Drum radius / width$r=40\ \text{mm}$, $w=60\ \text{mm}$
Lever offsets$a=90\ \text{mm}$, $b=80\ \text{mm}$, $e=30\ \text{mm}$
Contact half-angle$\theta=30^\circ$
Max lining pressure / friction$p_{\max}=1.3\ \text{MPa}$, $\mu=0.3$

Find. Torque capacity $T$, the actuating force $F_a$, and the friction-arm value $c$ that makes the brake self-locking.

O (drum, r=40)shoeshoeO₁O₂F₀a = 90, b = 80 mm (lever)e = 30 mm (O to pivot)θ = 30°, w = 60 mm
Double short-shoe external brake: two shoes at $p_{\max}$ grip the drum; the actuating force acts through the pivot lever with arms $a$ and $b$.

Approach. For a short shoe the pressure is taken uniform at $p_{\max}$ over the projected pad area; the normal force gives the friction torque per shoe, doubled for the two shoes. A moment balance on the self-energizing lever gives $F_a$, and setting $F_a=0$ gives the self-locking condition.

  1. Normal force per shoe. Short-shoe theory uses the projected pad area $A=w\,(2r\sin\tfrac{\theta}{2})$ at uniform $p_{\max}$: $$N=p_{\max}\,w\,(2r\sin\tfrac{\theta}{2})=1.3\times10^{6}\,(0.060)(2\times0.040\sin15^\circ)=1615\ \text{N}.$$
  2. Friction torque (both shoes). Each shoe contributes $\mu N r$; with two shoes at $p_{\max}$, $$T=2\mu N r=2(0.3)(1615)(0.040)=\boxed{38.8\ \text{N}\cdot\text{m}}.$$
  3. Actuating force on the self-energizing shoe. Taking moments of $N$ and the friction force $\mu N$ about the pivot $O_1$, with friction moment arm $c=r-e=40-30=10\ \text{mm}$: $$F_a=\frac{N\,(b-\mu c)}{a}=\frac{1615\,(0.080-0.3\times0.010)}{0.090}=1382\ \text{N}.$$
  4. Self-locking condition. The brake self-locks when the friction moment alone closes the shoe, i.e. $F_a\le0\Rightarrow \mu c\ge b$: $$c\ge\frac{b}{\mu}=\frac{80}{0.3}=\boxed{266.7\ \text{mm}}.$$ The actual friction arm here is only $c=r-e=10\ \text{mm}\ll266.7\ \text{mm}$, so the brake is not self-locking and needs the 1382 N actuating force — a safe, controllable design.
Problem 3 results
QuantityValue
Normal force per shoe$N = 1615\ \text{N}$
Torque per shoe / total$19.4\ \text{N}\cdot\text{m}$ / $T=38.8\ \text{N}\cdot\text{m}$
Actuating force$F_a = 1382\ \text{N}$
Self-locking friction arm$c \ge b/\mu = 266.7\ \text{mm}$ (actual $c=10\ \text{mm}$ → not self-locking)