The flow rate of water out of a valve at the bottom of an open cylindrical tank is given by
where is a constant, , is the valve cross-sectional area, is the gravitational acceleration, and is the vertical height of the water level above the valve.
Let , with .
The water in the tank is drained through the valve starting at .
At , the water level has dropped by cm from its original value. What was the height (in ) of the water level (above the valve) at ?
Take the cross-sectional area of the tank to be , and .
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The flow rate equation can be rewritten as
a d t d y = − C A 2 g y ,
where a is the cross-sectional area of the cylinder.
So, y − 2 1 d y = − a C A 2 g d t
Integrating we get
y = y 0 − a C A t 2 g ,
where y 0 is the initial height of the water level above the valve.
Substituting values we get
y 0 − 0 . 3 ≈ y 0 − 0 . 1 6 9
⟹ y 0 ≈ ( 0 . 3 3 8 0 . 3 + 0 . 2 0 9 ) 2 ≈ 9 4 . 4 cm.