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22-Mec-B1 Advanced Machine Design · May 2014

Question 5 of 6: Single-Surface Disk Clutch (Uniform Wear)

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).



Problem 5: Single-Surface Disk Clutch (Uniform Wear) (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. A single friction surface, molded lining, sized under the uniform-wear assumption.

Given data
QuantityValue
Torque $T$100 N·m
Speed750 rpm
Max lining pressure $p_{\max}$1.2 MPa
Friction coefficient $\mu$0.25
Diameter ratio $d_i/d_o$0.577
Friction surfaces1

Find. Outside and inside diameters, and the transmitted power.

r_or_ifriction annulus (uniform wear: p·r = const)
Friction annulus. Under uniform wear the pressure is largest at $r_i$ and falls as $p\,r = p_{\max}r_i$.

Approach. Apply the uniform-wear model ($p\,r = \text{const}$, maximum at the inner radius), express torque and axial force in terms of $r_o$ with the fixed ratio, solve for $r_o$, then get the power from $T\omega$.

  1. Uniform-wear law. The pressure varies as $p(r) = p_{\max}\,r_i/r$ (largest at $r_i$). Integrating pressure and friction over the annulus: $$F = 2\pi p_{\max} r_i (r_o - r_i), \qquad T = \pi\mu p_{\max} r_i\,(r_o^2 - r_i^2).$$
  2. Insert the ratio. With $r_i = 0.577\,r_o$, the torque becomes $T = \pi\mu p_{\max}\,(0.577)(1-0.577^2)\,r_o^3 = \pi\mu p_{\max}(0.385)\,r_o^3$.
  3. Solve for the radii. $r_o = \left[\dfrac{100}{\pi(0.25)(1.2\times10^6)(0.385)}\right]^{1/3} = 0.0651\ \text{m}$. Hence $$\boxed{\,d_o \approx 130\ \text{mm},\quad d_i \approx 75\ \text{mm}\,}$$
  4. Axial actuating force. $F = 2\pi(1.2\times10^6)(0.0375)(0.0651-0.0375) = 7.79\ \text{kN}$ (cross-check: $\mu F r_m = 0.25(7790)(0.0513) = 100\ \text{N}\!\cdot\!\text{m}$ ✓).
  5. Power transmitted. $P = T\omega = 100\times\dfrac{2\pi(750)}{60} = 7854\ \text{W} = \boxed{7.85\ \text{kW}}$.

The specified ratio $d_i/d_o = 0.577 \approx 1/\sqrt{3}$ is not arbitrary — it is the value that maximises the torque a uniform-wear clutch of given outer radius can carry, so this design is running at the optimal proportion for its lining.

Problem 5 — Results
QuantityValue
Outside diameter $d_o$130 mm
Inside diameter $d_i$75 mm
Axial actuating force $F$7.79 kN
Power transmitted7.85 kW