Water is filled up to a height h in a beaker of radius R as shown in the figure. The density of water is $\mathrm{\rho }$, the surface tension of water is T and the atmospheric pressure is P₀. Consider a vertical section ABCD of the water column through a diameter of the beaker. The force on water on one side of this section by water on the other side of this section has magnitude:
 

• A

  $\left|2{\mathrm{p}}_0\mathrm{Rh}+{\mathrm{\pi R}}^2\mathrm{\rho gh}-2\mathrm{RT}\right|$

• B

  $\left|2{\mathrm{P}}_0\mathrm{Rh}+{\mathrm{R\rho gh}}^2-2\mathrm{RT}\right|$

• C

  $\left|{\mathrm{P}}_0{\mathrm{\pi R}}^2+{\mathrm{R\rho gh}}^2-2\mathrm{RT}\right|$

• D

  $\left|{\mathrm{P}}_0{\mathrm{\pi R}}^2+{\mathrm{R\rho gh}}^2+2\mathrm{RT}\right|$