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Hydraulic Press: Include Height Differences

Apply hydrostatic pressure changes without misusing Pascal's principle.

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For static liquid of density rho, pressure rises with depth: delta p = rho g h. A pressure change imposed on an enclosed fluid is transmitted, but absolute or gauge pressures at different heights need not be equal. Use gauge pressure and ignore piston weight and friction. Use diagrams and calculations only; never build or operate a press for this activity.

Worked example

With rho = 800 kg/m^3 and g = 10 m/s^2, a point 0.5 m lower has 4,000 Pa more pressure. From 30,000 Pa at the upper face, the lower face has 34,000 Pa.

A lower point is half a meter below an upper point in liquid of density 800 kilograms per cubic meter. With g equal to 10 meters per second squared, gauge pressure rises from 30 to 34 kilopascals.
A lower point is half a meter below an upper point in liquid of density 800 kilograms per cubic meter. With g equal to 10 meters per second squared, gauge pressure rises from 30 to 34 kilopascals.
Question 1 Calculate the pressure increase 800 x 10 x 0.5.
Question 2 What is lower-face gauge pressure for the example?
Question 3 What net fluid force acts on lower area 0.002 m^2?
Question 4 If an extra 2,000 Pa is imposed, with heights fixed, what is the upper pressure?
Question 5 What is the lower pressure after that same change?