The relationship between pressure and head is used to measure pressure with a manometer (also know as a liquid gauge).
Objective:
The simplest manometer is a tube, open at the top, which is attached to the top of a vessel containing liquid at a pressure (higher than atmospheric) to be measured. An example can be seen in the figure below. This simple device is known as a Piezometer tube. As the tube is open to the atmosphere the pressure measured is relative to atmospheric so is gauge pressure.


This method can only be used for liquids (i.e. not for gases) and only when the liquid height is convenient to measure. It must not be too small or too large and pressure changes must be detectable.
Using a "U"-Tube enables the pressure of both liquids and gases to be measured with the same instrument. The "U" is connected as in the figure below and filled with a fluid called the manometric fluid. The fluid whose pressure is being measured should have a mass density less than that of the manometric fluid and the two fluids should not be able to mix readily - that is, they must be immiscible.

Pressure in a continuous static fluid is the same at any horizontal level so,

For the left hand arm

For the right hand arm

As we are measuring gauge pressure we can
subtract
giving


If the fluid being measured is a gas, the density
will probably be very low in comparison to the density of the
manometric fluid i.e. rman
>> r.
In this case the term
can be neglected,
and the gauge pressure give by

If the "U"-tube manometer is connected to a pressurised vessel at two points the pressure difference between these two points can be measured.

If the manometer is arranged as in the figure above, then

Giving the pressure difference

Again, if the fluid whose pressure difference is
being measured is a gas and
, then the
terms involving
can be neglected, so

The "U"-tube manometer has the disadvantage that the change in height of the liquid in both sides must be read. This can be avoided by making the diameter of one side very large compared to the other. In this case the side with the large area moves very little when the small area side move considerably more.

Assume the manometer is arranged as above to measure
the pressure difference of a gas of (negligible density) and that
pressure difference is
. If the datum
line indicates the level of the manometric fluid when the pressure
difference is zero and the height differences when pressure is
applied is as shown, the volume of liquid transferred from the
left side to the right
And the fall in level of the left side is

We know from the theory of the "U" tube manometer that the height different in the two columns gives the pressure difference so

Clearly if D is very much larger than d then (d/D)2 is very small so

So only one reading need be taken to measure the pressure difference.
If the pressure to be measured is very small then tilting the arm provides a convenient way of obtaining a larger (more easily read) movement of the manometer. The above arrangement with a tilted arm is shown in the figure below.

The pressure difference is still given by the height change of the manometric fluid but by placing the scale along the line of the tilted arm and taking this reading large movements will be observed. The pressure difference is then given by

The sensitivity to pressure change can be increased further by a greater inclination of the manometer arm, alternatively the density of the manometric fluid may be changed.
Care must be taken when attaching the manometer to vessel, no burrs must be present around this joint. Burrs would alter the flow causing local pressure variations to affect the measurement.
Some disadvantages of manometers:
Some advantages of manometers: