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Torque and power loss in a shaft bearing

Short answer

Using linear velocity profile, surface speed U=1.571 m/s, shear stress τ=μU/c=628 Pa. Resisting torque T=τ·πDL·D/2=1.48 N·m. Power lost P=Tω=46.5 W.

A shaft of diameter 100 mm rotates at 300 rpm inside a stationary sleeve (journal bearing) of length 150 mm. The uniform radial clearance between the shaft and sleeve is 0.2 mm and it is filled with oil of dynamic viscosity 0.08 Pa s. Assuming a linear velocity profile in the oil, find the shear stress on the shaft surface, the resisting torque and the power lost in viscous friction.

Given data

D=0.1 mD = 0.1\ \text{m}, L=0.15 mL = 0.15\ \text{m}, c=0.2 mm=2×10−4 mc = 0.2\ \text{mm} = 2\times10^{-4}\ \text{m}, N=300 rpmN = 300\ \text{rpm}, μ=0.08 Pa s\mu = 0.08\ \text{Pa s}.

Since the clearance is very small compared with the diameter, the oil film can be treated as flat with a linear velocity profile, so du/dy=U/cdu/dy = U/c.

Surface speed of the shaft

U=πDN60=π×0.1×30060=1.571 m/sU = \frac{\pi D N}{60} = \frac{\pi \times 0.1 \times 300}{60} = 1.571\ \text{m/s}

Shear stress

τ=μUc=0.08×1.5712×10−4=628.3 Pa\tau = \mu \frac{U}{c} = 0.08 \times \frac{1.571}{2\times10^{-4}} = 628.3\ \text{Pa}

Resisting torque

Shear area A=πDL=π×0.1×0.15=0.04712 m2A = \pi D L = \pi \times 0.1 \times 0.15 = 0.04712\ \text{m}^2

F=τA=628.3×0.04712=29.61 NT=F×D2=29.61×0.05=1.480 N m\begin{aligned} F &= \tau A = 628.3 \times 0.04712 = 29.61\ \text{N} \\ T &= F \times \frac{D}{2} = 29.61 \times 0.05 = 1.480\ \text{N m} \end{aligned}

Power lost

ω=2πN60=31.42 rad/sP=Tω=1.480×31.42=46.5 W\begin{aligned} \omega &= \frac{2\pi N}{60} = 31.42\ \text{rad/s} \\ P &= T\omega = 1.480 \times 31.42 = 46.5\ \text{W} \end{aligned}

Answer: τ=628 Pa\tau = 628\ \text{Pa}, T=1.48 N mT = 1.48\ \text{N m}, P=46.5 WP = 46.5\ \text{W}

✓ Answer checked by Claude Opus 5.5 (high effort)

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