Given : $d_{1}$ = 1.2 m or $r_{1}$ =0.6 m ; $d_{2}$= 0.5 m or $r_{2}$ =0.25 m; x =4 m; m =0.9 kg/m;
T =2000N; $\mu$ =0.3; $N_{1}$ =200 rpm. ; $N_{2}$ =450 rpm.
We know that velocity of the belt,
$v=\frac{\pi d_{1}N_{1}}{60}=\frac{\pi\times1.2\times 200}{60}$= 12.57 m/s.
and centrifugal tension, $T_{C}$ = m$v^{2}$ =0.9(12.57)$^{2}$ =142N.
Tension in the tight side of the belt,
$T_{1}$ =T- $T_{C}$ =2000-142=1858N.
We know that for an open belt drive,
$\sin\alpha=\frac{(r_{1}-r_{2})}{x}$ =(0.6-0.25)/4 =0.0875 or α = 5.020
Angle of lap on the smaller pulley,
$\theta$ = 1800-2$\alpha$ =1800-(2×5.020) =169.960
=169.96 ×($\pi$/180) =2.967 rad.
$T_{2}$ = Tension in the slack side of the belt,
Let
We know that
$2.3log\frac{(T_{1}}{T_{2})}=\mu\theta$ =0.3×2.967 =0.8901
$log\frac{(T_{1}}{T_{2})}$ =(0.8901/2.3) =0.387 or $\frac{(T_{1}}{T_{2})}$ =2.438 …(Taking antilog of 0.387)
$T_{2}$ = $T_{1}$/2.438 =(1858/2.438) =762N.
Torque on the shaft of larger pulley
We know that torque on the shaft of larger pulley,
$T_{L}$ = ($T_{1}$ –$T_{2}$).$r_{1}$ = (1858-762)0.6 =657.6N.
Torque on the shaft of smaller pulley
We know that torque on the shaft of smaller pulley,
$T_{S}$= ($T_{1}$ –$T_{2}$).$r_{2}$ = (1858-762)0.25 =274N.
Power transmitted:
We know that the power transmitted,
P = ($T_{1}$ + $T_{1}$)ν = (1858-762)12.57 =13780 W
Power lost in friction:
We know that input power,
$P_{1}$ = ($T_{L}$ ×2$\pi N_{1}$) /60 = (657.6×2$\pi$×200)/60 =13780 W =13.78 kW
And output power
$P_{2}$ = ($T_{S}$ ×2$\pi n_{2}$) /60 = (274×$2\pi$×450)/60 =12910 W =12.91 kW
Power lost in friction = $P_{1}$ - $P_{2}$ =13.78-13.91 =0.87 kW
Efficiency of the drive:
We know that efficiency of the drive,
$\eta$ = (output power)/(input power) = 12.91/13.78 =0.937 or 93.7%