2. Pascalβs Law
β’ β The intensity of pressure at any point in a liquid at rest, is the same in all
directionsβ
Proof: Let us consider a very small wedge shaped element LMN of a liquid.
Let, ππ₯ = πππ‘πππ ππ‘π¦ ππ βππππ§πππ‘ππ ππππ π π’ππ ππ π‘βπ πππππππ‘ ππ ππππ’ππ
ππ¦ = πππ‘πππ ππ‘π¦ ππ π£πππ‘ππππ ππππ π π’ππ ππ π‘βπ πππππππ‘ ππ ππππ’ππ
ππ§
= πππ‘πππ ππ‘π¦ ππ ππππ π π’ππ ππ π‘βπ ππππππππ ππ π‘βπ πππβπ‘ ππππππ π‘ππππππ’πππ ππππ
Ξ± = Angle of the element of the liquid
ππ₯ = πππ‘ππ ππππ π π’ππ ππ π‘βπ π£πππ‘ππππ π πππ πΏπ ππ π‘βπ ππππ’ππ
ππ¦ = πππ‘ππ ππππ π π’ππ ππ π‘βπ βππππ§πππ‘ππ π πππ ππ ππ π‘βπ ππππ’ππ
ππ§ = πππ‘ππ ππππ π π’ππ ππ π‘βπ ππππππππ π πππ πΏπ ππ π‘βπ ππππ’ππ
Now, ππ₯ = ππ₯ x LN β¦β¦(i)
ππ¦ = ππ¦ x MNβ¦β¦β¦β¦.(ii)
ππ§ = ππ§ x LMβ¦β¦β¦β¦β¦(iii)
3. β’ As the element of the liquid is at rest, therefore
the sum of horizontal and vertical components
of the liquid pressures must be equal to zero
β’ Resolving the forces horizontally:
β’ ππ₯ = ππ§ sin Ξ±
β’ ππ₯ x LN = ππ§ x LM sin Ξ±
β’ ππ₯ x LN = ππ§ x LM x
πΏπ
πΏπ
β’ ππ₯ = ππ§ β¦.. (iV)
4. β’ Resolving the forces vertically:
ππ¦ β π = ππ§ cos Ξ± (W= weight of the liquid element)
Since the element is very small, neglecting its weight we have
β’ ππ¦ = ππ§ cos Ξ±
β’ ππ¦. MN = ππ§ LM cos Ξ±
β’ ππ¦. MN = ππ§ LM
MN
LM
β’ ππ¦ = ππ§ β¦β¦..(v)
β’ From (iv) & (v) we get
β’ ππ₯ = ππ¦ = ππ§
5. Pressure Head of a Liquid
β’ A liquid is subjected to pressure due to its own
weight, this pressure increases as the depth of
the liquid increases.
β’ Consider a vessel containing liquid, the liquid
will exert pressure on all sides and bottom of
the vessel.
Now let cylinder be
made to stand in the liquid
6. β’ Let h = height of liquid in the cylinder,
β’ A = area of the cylinder base,
β’ W = specific weight of the liquid,
β’ P = intensity of pressure
Now Total pressure on the base of the cylinder =
weight if liquid in the cylinder
i.e., p A = w x A x h
π =
π€π΄β
π΄
= π€β
π = π€β (β =
π
π€
)
The intensity of pressure in a liquid due to its depth
will vary directly with depth
7. Measurement of Pressure
β’ 1. Manometers
These are defined as the devices used for
measuring the pressure at a point in a fluid by
balancing the column of fluid by the same or
another column of liquid. These are classified as
a) Simple manometers
i. Piezometer
ii. U-tube manometer
iii. Single column manometer
b) Differential manometers
8. β’ Mechanical gauges:
β’ These are the devices in which the pressure is
measured by balancing the fluid column by
spring or dead weight.
β’ These gauges are used for measuring high
pressure and high precision is not required.
β’ Bourdon tube pressure gauge
β’ Bellow pressure gauge
β’ Diaphragm pressure gauge
β’ Dead-weight pressure gauge
9. Simple manometers
β’ 1. Piezometer: A piezometer is the simplest form of
manometer which can be used for measuring moderate
pressures of liquids.
β’ It consists of a glass tube inserted in the wall of a vessel or
of a pipe, containing liquid whose pressure is to be
measured. The tube extends vertically upward to such a
height that liquid can freely rise in it without overflowing.
10. β’ U- tube manometer:
β’ A U-tube manometer consists of a glass tube
bent in U-shape, one end of which is
connected to a point at which pressure is to
be measured and other end remains open to
the atmosphere.