This demonstration shows the pressure height gradient in a fluid.
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Possible Incorporated Topics:
 Pressure gradient
 Hydrostatic force
 Newton's Law
Theory:
A sample of the water in a tank has a volume V = A(y_{1}  y_{2}), where A is the top area of the sample, and y_{1} is the position of the top and y_{2} the position of the bottom of the sample. If the water has density r (Greek letter rho), then the weight of the sample is W = rgA(y_{1}  y_{2}). Since the water is not flowing, then the total force on the sample must be zero. There must then be forces other than the weight acting on the sample. These other forces are the pressure on the top of the sample and the pressure on the bottom. If the pressure on the top and on the bottom are P_{1} and P_{2}respectively, then the force on the bottom is F_{1} = P_{1}A and the force on the top is F2 = P_{2}A. Newton's Law give us the following relation.
Figure 1: Forces acting within a tank of water 
P_{2}A  P_{1}A  rgA(y_{1}  y_{2}) = 0
If we take P_{1} to be the pressure at the surface of the water, then it is equal to the atmospheric pressure: P_{1} = P_{atm} and y_{1} = 0
If we make P_{2} to be the pressure at a depth of h below the surface, then:
P_{2} = P and y_{2} = h
The bold equation from above thus gives us the following formula:
P = P_{atm} + rgh
As this fomula shows, P increases with depth, h, in the fluid.
This result can be shown with a pipe filled with water. If the pipe has holes at a few different depths, then the higher pressure at the bottom forces the water out of the hole faster.
Apparatus:
 Clear pipe with three small holes
 Water supply
 Small tub or bucket
 Stand
 Tape
Procedure:

Figure 2: Apparatus 