In a journal bearing diameter of the shaft is 75 mm, L/D = 1, radial clearance = 0.05 mm, minimum film thickness = 0.02 mm, speed of journal= 400 rpm, radial load = 3.5 N, specific gravity of oil is 0.9 and specific heat is 1.75 kJ/kg°C. Calculate the viscosity of suitable oil, temperature rise and power lost in friction.
Given
L = D = 15 mm
C_r=0.05 \mathrm{~mm}
h_0=0.02 \mathrm{~mm}
N^*=\frac{400}{60}=6.67 \mathrm{~rps}
W = 3.5 N
p=\frac{W}{L D}=\frac{3500}{75 \times 75}=0.622 \mathrm{~N} / \mathrm{mm}^2
\frac{h_0}{C_r}=\frac{0.02}{0.05}=0.4
Corresponding to \frac{h_0}{C_r}=0.4,
Sommerfeld number, S = 0.121
CFV = 3.22
FV = 4.33
S=\left(\frac{\mu N^*}{p}\right)\left(\frac{r}{C_r}\right)^2=\left(\frac{\mu \times 6.67}{0.622 \times 10^6}\right)\left(\frac{37.5}{0.05}\right)^2=0.121
\mu=\frac{0.121 \times 0.622 \times 10^6}{6.67} \times\left(\frac{0.05}{37.5}\right)^2=0.02 \mathrm{~N} \cdot \mathrm{s} / \mathrm{m}^2
Temperature rise variable is
\frac{\rho C_p \Delta T}{p}=\frac{\mathrm{CFV}}{\mathrm{FV}} \times 4 \pi=\frac{3.22}{4.33} \times 4 \pi=9.345
Temperature rise is
\Delta T=\frac{9.345 \times p}{\rho C_p}=\frac{9.345 \times 0.622 \times 10^6}{900 \times 1750}=3.69^{\circ} \mathrm{C}=4.0^{\circ} \mathrm{C}
\frac{r}{C_r} f= coefficient of friction variable = CFV = 3.22
f=\frac{3.22 \times 0.05}{37.5}=0.00429
Power loss in friction
H_f=f W \times V=f W\left(\frac{\pi D N}{60,000}\right)=0.00429 \times 3500\left(\frac{\pi \times 75 \times 400}{60,000}\right)=23.59 \mathrm{~W}
Attitude \varepsilon | \frac{h_0}{C_r} | S | \phi | \frac{r}{C_r} f | \frac{Q}{r C_r N^* L} | \frac{Q_s}{Q} | \frac{p}{p_{\max }} |
0 | 1 | 00 | 85 | ∞ | π | 0 | – |
0.1 | 0.9 | 1.33 | 79.5 | 26.4 | 3.37 | 0.15 | 0.54 |
0.2 | 0.8 | 0.63 | 74.02 | 12.8 | 3.59 | 0.28 | 0.529 |
0.4 | 0.6 | 0.264 | 63.10 | 5.79 | 3.99 | 0.497 | 0.484 |
0.6 | 0.4 | 0.121 | 50.58 | 3.22 | 4.33 | 0.680 | 0.415 |