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Bearings for Mechanical Drive Turbines  53

                    D = bearing diameter, in
                   W = bearing load, lbf
                   C d = bearing diametral clearance, in

              The problem with sleeve bearings (i.e., all journal bearings excluding
            tilting-pad bearings) is that they support a resultant load with a dis-
            placement that is not directly in line with the resultant load vector but
            is at some angle with rotation from the load vector. This angle can
            approach 90° for light loads and high speed.
              The specific case of a vertically downward gravity load is illustrated
            in Fig. 3.1 for a two-axial groove bearing. This sleeve bearing supports
            the vertically downward load with a displacement that is not directly
            downward but at some angle with rotation from bottom dead center.
            This angle is defined as the attitude angle ψ, as shown in Fig. 3.1.
              Figure 3.2 illustrates the hydrodynamic pressure distribution for a
            high speed, lightly loaded, unstable journal bearing. Note that the
            bearing eccentricity ratio ε= e/c (Fig. 3.1), is very small and the atti-
            tude angle ψ approaches 90°. In this manner, a light Y direction load is
            supported by a  +X displacement. This occurs because the load is so
            light and the resulting pressure profile becomes very small, with little
            change from the maximum film to the minimum film locations. For
            equilibrium, the summation of all vertical components of the hydrody-































            Figure 3.1 Fixed-geometry bearing schematic. (RMT, Wellsville,
            N.Y.)
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