Question 3.7: A motor driving a solid circular steel shaft transmits 30 kW...

A motor driving a solid circular steel shaft transmits 30 kW to a gear at B (Fig. 3-34). The allowable shear stress in the steel is 42 MPa.
(a) What is the required diameter d of the shaft if it is operated at 500 rpm?
(b) What is the required diameter d if it is operated at 3000 rpm?

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(a) Motor operating at 500 rpm. Knowing the horsepower and the speed of rotation, we can find the torque T acting on the shaft by using Eq. (3-43) H=2πnT60(550)=2πnT33,000(n=rpm,T=bft,H=hp)H=\frac{2 \pi n T}{60(550)}=\frac{2 \pi n T}{33,000} \quad(n=\mathrm{rpm}, T=\mathrm{b}-\mathrm{ft}, H=\mathrm{hp}) . Solving that equation for T, we get

T=60 P2πn=60(30 kW)2π(500 rpm)=573 NmT=\frac{60  P}{2 \pi n}=\frac{60(30 \mathrm{~kW})}{2 \pi(500 \mathrm{~rpm})}=573 \mathrm{~N} \cdot \mathrm{m}

This torque is transmitted by the shaft from the motor to the gear.
The maximum shear stress in the shaft can be obtained from the modified torsion formula [Eq. (3-14)]:

τmax=16Tπd3\tau_{\max }=\frac{16 T}{\pi d^{3}}

Solving that equation for the diameter d, and also substituting τallow \tau_{\text {allow }} for τmax \tau_{\text {max }}, we get

d3=16Tπτallow =16(573 Nm)π(42MPa)=69.5×106 m3d^{3}=\frac{16 T}{\pi \tau_{\text {allow }}}=\frac{16(573 \mathrm{~N} \cdot \mathrm{m})}{\pi(42 \mathrm{MPa})}=69.5 \times 10^{-6} \mathrm{~m}^{3}

from which

d = 41.1 mm
The diameter of the shaft must be at least this large if the allowable shear stress is not to be exceeded.

(b) Motor operating at 4000 rpm. Following the same procedure as in part (a), we obtain

T=60P2πn=60(30 kW)2π(4000rpm)=71.6 Nmd3=16Tπτallow =16(71.6 Nm)π(42MPa)=8.68×106 m3d=20.6 mm\begin{aligned}T &=\frac{60 \mathrm{P}}{2 \pi n}=\frac{60(30 \mathrm{~kW})}{2 \pi(4000 \mathrm{rpm})}=71.6 \mathrm{~N} \cdot \mathrm{m} \\d^{3} &=\frac{16 T}{\pi \tau_{\text {allow }}}=\frac{16(71.6 \mathrm{~N} \cdot \mathrm{m})}{\pi(42 \mathrm{MPa})}=8.68 \times 10^{-6} \mathrm{~m}^{3} \\d &=20.6 \mathrm{~mm}\end{aligned}

which is less than the diameter found in part (a).
This example illustrates that the higher the speed of rotation, the smaller the required size of the shaft (for the same power and the same allowable stress).

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