Demonstrating Pascal’s Principle
Consider the case in which the incompressible fluid is a liquid contained in a tall cylinder, as in figure :
The cylinder is fitted with a piston on which a container of lead shot rests. The atmosphere , container and shot exert pressure pext on the piston and thus on the liquid. The pressure p at any point P in the liquid is then
Let us add a little more lead shot to the container to increase pext by an amount The quantities rho, g and h in equation are unchanged , so the pressure change at P is
This pressure change is independent of h, so it must hold for all points within the liquid, as Pascal’s principle states.
Pascal’s Principle and the Hydraulic Lever
Figure showsn how pascal’s principle can be made the basis of a hydraulic lever. In operation, let an external force of magnitude Fi be directed downward on the left-hand ( or input) piston, whose surface area is Ai . An incompressible liquid in the device then produces an upward force of magnitude Fo on the right-hand ( or output ) piston, whose surface area is Ao . To keep the system in equilibrium , thre must be a downward force of magnitude Fo on the output piston from an external load ( not shown ) . The force Fi applied on the left and the downward force F0 from the load on the right produce a change p in the pressure of the liquid that is given by
Equation shows that the output force F0 on the load must be greater than the input force Fi if A0 > Ai , as is the case in Figure.
If we move the input piston downward a distance di , the output piston moves upward a distance d0 , such that the same volume V of the incompressible liquid is displaced at both pistons. Then
Which we can write as
This shows that , if A0 > Ai the output piston moves a smaller distance than the input piston moves. We can write the output work as
Which shows that the work W done on the input piston by the applied force is equal to the work W done by the output piston in lifting the load placed on it. The advantage of a hydraulic lever is this :
“ With a hydraulic lever, a given force applied over a given distance can be transformed to a greater force applied over a smaller distance.
The product of force and distance remains unchanged so that the same work is done. However, there is often tremendous advantage in being able to exert the larger force. Most of us, for example , cannot lift an automobile directly but can with a hydraulic jack, even though we have to pump the handle farther than the automobile rises and in a series of small strokes.