A cylinder of mass m and density `rho` hanging from a string is lowered into a vessel of cross-section area s containing a liquid of density `sigma (lt rho)` unit it is fully immersed. The increase in pressure at the bottom of the vessel is

A cylinder of mass M and density d_(1) hanging from a string, is lowered into a vessel of cross-sectional area A, containing a liquid of density d_(2) (d_(2) lt d_(1)) until it is fully immersed. The increase in pressure at the bottom of the vessel is

A cylinder of mass M and density d_(1) hanging from a string, is lowered into a vessel of cross-sectional area A, containing a liquid of density d_(2) (d_(2) lt d_(1)) until it is fully immersed. The increase in pressure at the bottom of the vessel is

A block of mass m and density p is hanging from a string . If it is lowered into a vessel of cross-sectional area A containing a liquid of density sigma(lt rho) and gets fully immered, the increase in pressure at the bottom of vessel would be

Two vessels A and B of cross sections as shown contain a liquid up to the same height. As the temperature rises, the liquid pressure at the bottom (neglecting expansion of the vessels ) will :

If a vessel containing a fluid of density rho upto height h is accelerated vertically downwards with accelerations a_(0) . Then the pressure by fluid at the bottom of a vessel is

A metal sphere connected by a string is dipped in a liquid of density rho as shown in figure. The pressure at the bottom of the vessel will be, (p_(0) =atmospheric pressure )

A metal sphere connected by a string is dipped in a liquid of density rho as shown in figure. The pressure at the bottom of the vessel will be, (p_(0) =atmospheric pressure )

A wooden block or mass m and density rho is tied to a string, the other end of the string is fixed to bottom of a tank. The tank is filled with a liquid of density sigma with sigmagtrho . The tension in the string will be