Pressure Measurement
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Apply the principles of manometer to calculate pressure.
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Differentiate between absolute pressure and gauge pressure.
Piezometer Tube:
The direct proportional relation between gauge pressure and the height h for a fluid of constant density enables the pressure to be simply visualized in terms of the vertical height, \[h = \frac{P}{\rho g}\]
The height h is termed as pressure head corresponding to pressure p. For a liquid without a free surface in a closed pipe, the pressure head \(\displaystyle h = \frac{P}{\rho g}\) at a point corresponds to the vertical height above the point to which a free surface would rise, if a small tube of sufficient length and open to atmosphere is connected to the pipe.
Such a tube is called a piezometer tube, and the height h is the measure of the gauge pressure of the fluid in the pipe. If such a piezometer tube of sufficient length were closed at the top and the space above the liquid surface were a perfect vacuum, the height of the column would then correspond to the absolute pressure of the liquid at the base. This principle is used in the well known mercury barometer to determine the local atmospheric pressure.
Barometer:
Barometer is used to determine the local atmospheric pressure. Mercury is employed in the barometer because its density is sufficiently high for a relative short column to be obtained. and also because it has very small vapour pressure at normal temperature. High density scales down the pressure head(h) to represent same magnitude of pressure in a tube of smaller height.
Manometers:
A manometer is also frequently used to measure the pressure difference, in course of flow, across a restriction in a horizontal pipe.
Inclined Tube Manometer:
For accurate measurement of small pressure differences by an ordinary u-tube manometer, it is essential that the ratio \(\displaystyle \frac{r_{m}}{r_{w}}\) should be close to unity. This is not possible if the working fluid is a gas; also having a manometric liquid of density very close to that of the working liquid and giving at the same time a well defined meniscus at the interface is not always possible. For this purpose, an inclined tube manometer is used.
If the transparent tube of a manometer, instead of being vertical, is set at an angle \(\displaystyle \theta\) to the horizontal, then a pressure difference corresponding to a vertical difference of levels x gives a movement of the meniscus s = x/sin q along the slope.
If \(\displaystyle \theta\) is small, a considerable magnification of the movement of the meniscus may be achieved.
Angles less than 5\(^\circ\) are not usually satisfactory, because it becomes difficult to determine the exact position of the meniscus.
Inverted Tube Manometer:
For the measurement of small pressure differences in liquids, an inverted U-tube manometer is used.