A rectangular tank is filled to the brim with water. When a hole at its bottom is unplugged, the tank is emptied in time T. If the tank is half-filled with water, it will be emptied in time:
Let the actual Height of the tank be
H and its uniform cross sectional area be A.
Now let us consider that at certain moment the height of water level be
h and the velocity of water emerging through the orifice of cross sectional area a at the bottom of the tank be v.As the surface of water and the orifice are in open atmosphere, then by Bernoulli's theorem we have
v=√2gh
Let dh represents decrease in water level during infinitesimally small time interval dt when the water level is at height h. So the rate of decrease in volume of water will be=
−Adhdt
Again the rate of flow of water at this moment through the orifice is given by v×a=a√2gh.
These two rate must be same by the principle of cotinuity.
Hence a√2gh=−Adhdt
⇒dt=−Aa√2g×h−12dh
If the tank is filled to the brim then height of water level will be H and time required to empty the tank T can be obtained by integrating the above relation.
T=∫T00dt=−Aa√2g⋅∫0Hh−12dh
T=A√2Ha√g
If the tank be half filled with water and the time to empty it be T′ then
T′=A√2Ha√2g
So T′T=1√2
T′=T√2