Question 3 of 6: Single-surface disk clutch — uniform-wear design and transmitted power (20 marks)
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Exams, December 2019 — 16-Mec-B1 Advanced Machine Design. Three hours, open book, 100 marks. Part I (Problems 1 and 2) is compulsory; the candidate answers three of the four Part II problems (Problems 3–6). Any non-communicating calculator is permitted, all assumptions must be stated, and every tabulated value or equation must be sourced. All six problems are worked here, so the set is complete as a study resource.
Reference texts. Budynas & Nisbett, Shigley's Mechanical Engineering Design, 11th ed. (fatigue and notch sensitivity §6, power screws §8-2, clutches and brakes §16); Norton, Machine Design: An Integrated Approach, 6th ed. (impact loading §3, stress transformation §4, brakes §16); Juvinall & Marshek, Fundamentals of Machine Component Design, 6th ed. (screws, clutches, brakes); Hibbeler, Mechanics of Materials, 10th ed. (beam bending, principal stresses, impact factors); CSA/ISO 14006 Eco-design management systems and ISO 14040 Life-cycle assessment for the green-design criteria.
Question 3: Single-surface disk clutch — uniform-wear design and transmitted power (20 marks)
Given. A single friction face working against a molded lining, with the diameter ratio fixed by the designer.
Given data — Problem 3
Quantity
Symbol
Value
Torque to be transmitted
$T$
120 N·m
Rotational speed
$N$
500 rev/min
Maximum lining pressure
$p_{\max}$
1.5 MPa
Coefficient of friction
$\mu$
0.30
Diameter ratio
$k=d_i/d_o$
0.70
Number of friction surfaces
—
1
Find. The outside and inside diameters of the friction annulus, the required clamping force, and the power transmitted.
Figure 3.1 — Single-surface disk clutch. Left: the friction annulus, 123.9 mm outside by 86.7 mm inside. Right: the uniform-wear pressure distribution, peaking at 1.5 MPa at the bore and falling as 1/r to 1.05 MPa at the outer rim.
Approach. Under the uniform-wear assumption the product $p\,r$ is constant across the annulus, which pins the pressure distribution to $p_{\max}$ at the bore; integrating the friction moment over the annulus then gives torque as an explicit cubic in the outer radius once the ratio $k$ is imposed.
Set up the uniform-wear pressure law. Wear rate is proportional to $p\,v$ and $v\propto r$, so uniform axial wear requires $p\,r=\text{constant}$. The constant is fixed at the inner radius, where the pressure is highest:
$$p(r)\,r = p_{\max}\,r_i \quad\Longrightarrow\quad p(r)=p_{\max}\frac{r_i}{r}$$
This is why a uniform-wear clutch always runs its peak pressure at the bore, and why making $r_i$ too small is self-defeating.
Integrate for the clamping force. With $\mathrm{d}F = p(r)\,2\pi r\,\mathrm{d}r = 2\pi p_{\max} r_i\,\mathrm{d}r$,
$$F=\int_{r_i}^{r_o} 2\pi p_{\max} r_i\,\mathrm{d}r = 2\pi p_{\max} r_i\left(r_o-r_i\right)$$
Integrate for the friction torque. Each ring contributes $\mathrm{d}T=\mu\,r\,\mathrm{d}F$, so for one friction surface
$$T=\int_{r_i}^{r_o}2\pi\mu p_{\max}r_i\,r\,\mathrm{d}r=\pi\mu p_{\max}r_i\left(r_o^{2}-r_i^{2}\right)$$
Impose the diameter ratio and solve for $r_o$. Putting $r_i = k r_o$ with $k=0.7$ turns the torque equation into a cubic in $r_o$ alone:
$$T=\pi\mu p_{\max}k\left(1-k^{2}\right)r_o^{3}$$
$$\pi\times 0.30\times 1.5\times 0.7\times\left(1-0.49\right)=0.5047\ \text{N/mm}^{2}$$
$$r_o=\left(\frac{120\times 10^{3}}{0.5047}\right)^{1/3}=\left(237\,760\right)^{1/3}=61.95\ \text{mm}$$
so that $r_i = 0.7\times 61.95 = 43.37$ mm.
Report the diameters. Doubling the radii,
$$\boxed{d_o = 123.9\ \text{mm},\qquad d_i = 86.7\ \text{mm}}$$
In practice one would specify the next convenient stock lining, say $d_o = 125$ mm with $d_i = 87.5$ mm, which keeps the ratio at 0.70 and adds a small margin.
Clamping force required. Substituting into the force integral,
$$F = 2\pi\times 1.5\times 43.37\times\left(61.95-43.37\right)$$
$$\boxed{F = 7.60\ \text{kN}}$$
A useful cross-check uses the mean radius $r_m=(r_o+r_i)/2 = 52.66$ mm: the uniform-wear torque is exactly $T=\mu F r_m = 0.30\times 7596\times 52.66 = 120.0\ \text{kN}\cdot\text{mm}$, which closes on the specified torque.
Power transmitted. At the stated speed,
$$\omega=\frac{2\pi N}{60}=\frac{2\pi\times 500}{60}=52.36\ \text{rad/s}$$
$$P = T\omega = 120\times 52.36$$
$$\boxed{P = 6.28\ \text{kW}}$$
Sanity-check the lining duty. The mean pressure over the annulus is
$$p_{\text{mean}}=\frac{F}{\pi\left(r_o^{2}-r_i^{2}\right)}=\frac{2p_{\max}r_i}{r_o+r_i}=1.24\ \text{MPa}$$
comfortably below the 1.5 MPa peak at the bore, and the rubbing speed at the mean radius is $v = \omega r_m = 2.76$ m/s — both well inside the normal range for a molded lining.