Flow in a Lubricated Bearing (COMSOL)
Consider the situation in Fig. E8.5.1, in which one inclined plate (surface 3) moves at a velocity V relative to a stationary plate at y=0, the intervening space being occupied by a Newtonian fluid of density 1,000 and viscosity 1.0. All units are mutually consistent (taken as SI by COMSOL unless we specify otherwise). The velocity components of the moving plate are u_{0}=0.05 in the x direction and v_{0}=-0.01 in the y direction. The other three boundary conditions (on surfaces 1, 2 , and 4) are shown in Fig. E8.5.1. The two “ends,” at x=-1.4 and x=1.4, are exposed to a pressure of p=0. In reality, a bearing would have a much smaller mean thickness/length ratio, and would generate higher internal pressures, but the present choice allows the main features to be displayed without “stretching” the y coordinate.
Solve for the streamlines, the pressure distribution, and the variation of pressure along the straight line between midpoints of the opposite “ends”—between points with coordinates (-1.4,0.3) and (1.4,0.1).