Transfer
The transfer of liquid from one vessel into another
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When two vessels, containing liquid, are connected together by means of an orifice, the liquid will flow from the vessel with a higher level to the vessel with a lower level irrespective of their areas. In such a case the liquid level will fall in one vessel with a corresponding rise in the other. The orifice, through which the flow takes place, is a drowned one and the liquid head causing flow will be the difference between the two liquid levels.
Consider two tanks connected at their bottom by a small orifice as shown in figure.

Let,
- $A_{1}$ = Area of the larger vessel
- $A_{2}$ = Area of the smaller vessel
- $a$ = Area of the orifice
- $H_{1}$ = Initial difference between the liquid levels of the two vessels
- $H_{2}$ = Final difference between the liquid levels of the two vessels
- $T$ = Time, in seconds, required to bring the difference of liquid levels from $H_{1}$ to $H_{2}$
At some instant, let the difference between the two liquid levels be h.
The theoretical velocity, $v = \sqrt {2gh}$
After a small interval of time dt, let the liquid level in the vessel $A_{1}$ fall down by an amount equal to x.
$\therefore$ The volume of liquid that has passed from the tank $A_{1}$ = $A_{1}.x$
and the rise of liquid level in the other tank = $\frac{A_{1}}{A_{2}}x$
If the change of liquid level in the tanks be dh in time dt, then $dh = -(x + \frac{A_{1}}{A_{2}}x)$
(-) negative sign of dh is taken, as the value of h will decrease as the discharge will increase
$\Rightarrow dh = -x(1+\frac{A_{1}}{A_{2}}) = -x(\frac{A_{1}+A_{2}}{A_{2}})$
In time dt, the volume of water that has passed from tank $A_{1}$
= Coefficient of discharge $\times$ Area $\times$ Theoretical Velocity $\times$ Time
Equating equations (1) and (2), $A_{1}.x = C_{d}.a.\sqrt {2gh}\times dt$
$\Rightarrow \frac{-A_{1}.A_{2}.dh}{A_{1}+A_{2}} = C_{d}.a.\sqrt {2gh}\times dt$
$\Rightarrow dt = \frac{-A_{1}.A_{2}.dh}{C_{d}.a.(A_{1}+A_{2})\sqrt {2gh}} = \frac{-A_{1}.A_{2}.h^{-\frac{1}{2}}.dh}{C_{d}.a.(A_{1}+A_{2})\sqrt {2g}}$
Now the total time (T) required to bring the differences of liquid levels from $H_{1}$ to $H_{2}$ may be found out by integrating the above equation between the limits $H_{1}$ and $H_{2}$ i.e.,
$T = \int_{H_{1}}^{H_{2}} \frac{-A_{1}.A_{2}.h^{-\frac{1}{2}}.dh}{C_{d}.a.(A_{1}+A_{2})\sqrt {2g}}$
$\Rightarrow T = \frac{-A_{1}.A_{2}}{C_{d}.a.(A_{1}+A_{2})\sqrt {2g}}\int_{H_{1}}^{H_{2}}h^{-\frac{1}{2}}dh$
$\Rightarrow T = \frac{-2A_{1}.A_{2}(\sqrt H_{2}-\sqrt H_{1})}{C_{d}.a.(A_{1}+A_{2})\sqrt {2g}}$
Taking minus sign out of the bracket as $H_{1}$ is greater than $H_{2}$
$T = \frac{2A_{1}.A_{2}(\sqrt H_{1}-\sqrt H_{2})}{C_{d}.a.(A_{1}+A_{2})\sqrt {2g}}$