Fluid Mechanic's
STATIC PRESSURE OF LIQUIDS, HYDRAULIC PRESSURE, ABSOLUTE AND GAUGE PRESSURE
Introduction
- Fluid has property that it exerts force on all the sides, top and bottom. Pressure exerted by fluid is given as force per unit area which is as follows:
Pressure= Force Applied /Area Exposed
- SI unit of pressure is newton per square metre (N/m2). This is also known as pascal (Pa).
- The values of standard atmospheric pressure are as follows:
- 760 mm of mercury column
- 10.3 m of water column
- 101.3 kN/m2
- 101.3 kPa
- 1 bar
Hydrostatic Law:
- Pressure in a continuously distributed uniform static fluid varies only with vertical distance and is independent of the shape of the container.
- The pressure is the same at all points on a given horizontal plane in the fluid.
- The pressure increases with depth in the fluid.
Pressure head of liquid:
- Consider a fluid of density ρ, having fluid element of area ∆A at a depth distance h from the top surface of liquid (Fig)
Height of fluid element = ∆h
Pressure at top of fluid element = p
Force on the top of fluid element = p ∆A
Weight of fluid element = ∆A. ∆h. ρ g
- Upward force acting at bottom of the fluid element = ̶
- Under equilibrium conditions (downward force = upward force),
- Pressure variation in any static fluid is described by the above basic pressure height relationship.
- This equation describes hydrostatic law and indicates that rate of increase of pressure in a vertical downward direction is equal to the weight density (also known as specific weight) of fluid at that point.
Integrating,
Here h is known as the pressure head and its unit is in metres (m).
Liquid Paradox
- The pressure in a liquid is not a function of shape or size of the container.
- Pressure is only the function of density and height or depth h inside the liquid at which pressure has to be calculated.
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