The maximum torque that can be safely applied to a shaft of 100 mm diameter if the permissible angle of twist is 1 degree in a length of 3 m and the permissible shear stress is 30 N/mm2. Take G = 0.8 × 105 N/mm2.
4.57 kNm
This problem asks us to find the maximum torque that can be safely applied to a solid circular shaft. The safety is limited by two conditions: the maximum allowable angle of twist and the maximum allowable shear stress. We need to calculate the maximum torque permitted by each condition separately and then choose the smaller value, as that is the torque that satisfies both constraints simultaneously.
The angle of twist formula uses radians. We convert the given angle from degrees to radians:
$\theta \text{ (in radians)} = \theta \text{ (in degrees)} \times \frac{\pi}{180}$
$\theta = 1 \times \frac{\pi}{180} \text{ radians}$
For a solid circular shaft, the polar moment of inertia is given by:
$J = \frac{\pi D^4}{32}$ or $J = \frac{\pi R^4}{2}$
Using $R = 50 \text{ mm}$:
$J = \frac{\pi (50 \text{ mm})^4}{2} = \frac{\pi \times 6,250,000}{2} \text{ mm}^4 = 3,125,000 \pi \text{ mm}^4$
The torsion formula relating torque ($T$), angle of twist ($\theta$), modulus of rigidity ($G$), polar moment of inertia ($J$), and length ($L$) is:
$\frac{T}{J} = \frac{G\theta}{L}$
Rearranging for $T$:
$T_{twist} = \frac{G \theta J}{L}$
Substitute the values:
$T_{twist} = \frac{(0.8 \times 10^5 \text{ N/mm}^2) \times (\frac{\pi}{180} \text{ rad}) \times (3,125,000 \pi \text{ mm}^4)}{3000 \text{ mm}}$
$T_{twist} = \frac{0.8 \times 10^5 \times \pi^2 \times 3,125,000}{180 \times 3000} \text{ N.mm}$
$T_{twist} = \frac{0.8 \times 10^5 \times 9.8696 \times 3,125,000}{540,000} \text{ N.mm}$
$T_{twist} \approx \frac{2,467,400,000,000}{540,000} \text{ N.mm}$
$T_{twist} \approx 4,569,259 \text{ N.mm}$
Converting N.mm to kNm (1 kNm = $10^6$ N.m = $10^9$ N.mm):
$T_{twist} \approx 4,569,259 \times 10^{-9} \text{ kNm} \approx 4.569 \text{ kNm}$
Rounding to two decimal places, $T_{twist} \approx 4.57 \text{ kNm}$.
The torsion formula relating torque ($T$), shear stress ($\tau$), polar moment of inertia ($J$), and radius ($R$) is:
$\frac{T}{J} = \frac{\tau}{R}$
Rearranging for $T$:
$T_{stress} = \frac{\tau_{max} J}{R}$
Substitute the values:
$T_{stress} = \frac{(30 \text{ N/mm}^2) \times (3,125,000 \pi \text{ mm}^4)}{50 \text{ mm}}$
$T_{stress} = \frac{30 \times 3,125,000 \pi}{50} \text{ N.mm}$
$T_{stress} = 0.6 \times 3,125,000 \pi \text{ N.mm}$
$T_{stress} = 1,875,000 \pi \text{ N.mm}$
$T_{stress} \approx 1,875,000 \times 3.14159 \text{ N.mm}$
$T_{stress} \approx 5,890,487.5 \text{ N.mm}$
Converting N.mm to kNm:
$T_{stress} \approx 5,890,487.5 \times 10^{-9} \text{ kNm} \approx 5.890 \text{ kNm}$
Rounding to two decimal places, $T_{stress} \approx 5.89 \text{ kNm}$.
The shaft must satisfy both the angle of twist limit and the shear stress limit. Therefore, the maximum safe torque is the smaller of the two values calculated:
$T_{max} = \min(T_{twist}, T_{stress})$
$T_{max} = \min(4.57 \text{ kNm}, 5.89 \text{ kNm})$
$T_{max} = 4.57 \text{ kNm}$
Thus, the maximum torque that can be safely applied to the shaft is 4.57 kNm.
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