Given : n = 14 ; 2 \theta=15^{\circ} \text { or } \theta=7.5^{\circ} ; d = 1 m or r = 0.5 m ; m = 2000 kg ; k = 500 mm = 0.5 m ; P = 200 N ; N = 360 r.p.m. ; l = 750 mm ; \mu = 0.25
1. Maximum braking torque
The braking torque will be maximum when OB > OA and the drum rotates anticlockwise as shown in Fig. 19.23. The force P must act upwards and the end of the band attached to A is tight under tension T_{1} and the end of the band attached to B is slack under tension T_{2}.
Taking moments about O,
200 \times 750+T_{1} \times 30=T_{2} \times 120
12 T_{2}-3 T_{1}=15000 …(i)
We know that \frac{T_{1}}{T_{2}}=\left(\frac{1+\mu \tan \theta}{1-\mu \tan \theta}\right)^{n}
=\left(\frac{1+0.25 \tan 7.5^{\circ}}{1-0.25 \tan 7.5^{\circ}}\right)^{14}
=\left(\frac{1+0.25 \times 0.1317}{1-.025 \times 0.1317}\right)^{14}
=(1.068)^{14}=2.512 …(ii)
From equations (i) and (ii),
T_{1}=8440 N , \text { and } T_{2}=3360 N
We know that maximum braking torque,
T_{ B }=\left(T_{1}-T_{2}\right) r=(8440-3360) 0.5=2540 N – m
2. Angular retardation of the drum
Let \alpha = Angular retardation of the drum.
We know that braking torque \left(T_{ B }\right),
2540=I . \alpha=m \cdot k^{2} \cdot \alpha=2000(0.5)^{2} \alpha=500 \alpha
\therefore \alpha=2540 / 500=5.08 rad / s ^{2}
3. Time taken by the system to come to rest
Let t = Required time.
Since the system is to come to rest from the rated speed of 360 r.p.m., therefore
Initial angular speed, \omega_{1}=2 \pi \times 360 / 60=37.7 rad / s
and final angular speed, \omega_{2}=0
We know that \omega_{2}=\omega_{1}-\alpha . t …(– ve sign due to retardation )
\therefore t=\omega_{1} / \alpha=37.7 / 5.08=7.42 s