A rectangular vessel of dimension (/ x b x h) and mass M contains a liquid of density p. The vessel has an orifice at its bottom at a distance c from the rear wall as shown in the figure.

Force F that must be applied when maximum water stored is $\left[\mathrm{M}+\frac{\mathrm{hcb\rho }}{2}\right]\frac{\mathrm{hg}}{\mathrm{c}}$

The maximum volume of the water that can be stored when the vessel is accelerated is hlb/2.

The maximum volume of the water that can be stored when the vessel is accelerated is hcb/2.

Force F that must be applied when maximum water stored is $\left[\mathrm{M}+\frac{\mathrm{hcb\rho }}{2}\right]\frac{\lg }{\mathrm{c}}$