Fluid FlowCONTINUITY EQUATION(b)PressureForceAreaForce(Pressure) (Area)Areapr2F17.2lbfin^{2}p 10 ft2144 in^{2}1 ft^{2}7.78 x 10^{5}lbfPascal’sLawThe pressure of the liquids in each of the previously cited cases has been due to the weight ofthe liquid. Liquid pressures may also result from application of external forces on the liquid.Consider the following examples. Figure 2 represents a container completely filled with liquid.A, B, C, D, and E represent pistons of equal cross-sectional areas fitted into the walls of thevessel. There will be forces acting on the pistons C, D, and E due to the pressures caused bythe different depths of the liquid. Assume that the forces on the pistons due to the pressurecaused by the weight of the liquid are as follows: A = 0 lbf, B = 0 lbf, C = 10 lbf, D = 30 lbf,and E = 25 lbf. Now let an external force of 50 lbf be applied to piston A. This external forcewill cause the pressure at all points in the container to increase by the same amount. Since thepistons all have the same cross-sectional area, the increase in pressure will result in the forceson the pistons all increasing by 50 lbf. So if an external force of 50 lbf is applied to piston A,the force exerted by the fluid on the other pistons will now be as follows: B = 50 lbf, C = 60lbf, D = 80 lbf, and E = 75 lbf.This effect of an external force on a confined fluid was first stated by Pascal in 1653.Pressure applied to a confined fluid is transmitted undiminished throughout theconfining vessel of the system.Rev. 0 Page 7 HT-03

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