Determine h_0 and e using the following given parameters: \mu = 4 \ μreyn \ , \ N = 30 \ rev/s \ , \ W = 500 \ lbf \ (bearing \ load) \ , \ r = 0.75 \ in \ , c = 0.0015 \ in \ , \ and \ l = 1.5 \ in
Determine h_0 and e using the following given parameters: \mu = 4 \ μreyn \ , \ N = 30 \ rev/s \ , \ W = 500 \ lbf \ (bearing \ load) \ , \ r = 0.75 \ in \ , c = 0.0015 \ in \ , \ and \ l = 1.5 \ in
The nominal bearing pressure (in projected area of the journal) is
P =\frac{W}{2rl}=\frac{500}{2\left(0.75\right) 1.5}= 222 psi
The Sommerfeld number is, from Eq. (12–7),
S =\left(\frac{r}{c} \right)^2where N = N_j = 30 rev/s,
S =\left(\frac{r}{c} \right)^2 \left( \frac{\mu N}{P} \right)=\left(\frac{0.75}{0.0015}\right)^2 \left[ \frac{4\left(10^{−6}\right) 30}{222}\right]= 0.135Also, {l}/{d} = {1.50}/{\left[2\left(0.75\right)\right]} = 1 . Entering Fig. 12–16 with S = 0.135 \ and \ {l}/{d} = 1 gives {h_0}/{c} = 0.42 \ and \ \epsilon = 0.58 . The quantity {h_0}/{c} is called the minimum \ film \ thickness \ variable . Since c = 0.0015 in , the minimum film thickness
h_0 is h_0 = 0.42 \left(0.0015\right) = 0.000 63 in
We can find the angular location \phi of the minimum film thickness from the chart of Fig. 12–17. Entering with S = 0.135 \ and \ {l}/{d} = 1 \ gives \ \phi = 53^{\circ} .
The eccentricity ratio is \epsilon = {e}/{c} = 0.58 . This means the eccentricity e is e = 0.58 \left(0.0015\right) = 0.000 87 in