12.2 Derive expressions for the pressure distribution, the load-carrying capac- ity, and the time of approach for a sque

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12.2 Derive expressions for the pressure distribution, the load-carrying capac- ity, and the time of approach for a sque

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12 2 Derive Expressions For The Pressure Distribution The Load Carrying Capac Ity And The Time Of Approach For A Sque 1
12 2 Derive Expressions For The Pressure Distribution The Load Carrying Capac Ity And The Time Of Approach For A Sque 1 (39.11 KiB) Viewed 44 times
12.2 Derive expressions for the pressure distribution, the load-carrying capac- ity, and the time of approach for a squeeze film situation and the following geometry: W Sn h₁ In cylindrical polar coordinates the Reynolds equation for incompressible, isoviscous conditions is expressed in Eq. (12.4). In the present problem axial symmetry is assumed that results in the pressure being a function of radius only. Thus, the preceding Reynolds equation reduces to or (rh³OP)= = -12norw Ər Ər
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