A solid sphere having volume `V` and density `rho` floats at the interface of two immiscible liquids of densityes `rho_(1)` and `rho_(2)` respectively. If `rho_(1) lt rho lt rho_(2)`, then the ratio of volume of the parts of the sphere in upper and lower liquid is

A solid uniform ball having volume V and density rho floats at the interface of two unmixible liquids as shown in Fig. 7(CF).7. The densities of the upper and lower liquids are rho_(1) and rho_(2) respectively, such that rho_(1) lt rho lt rho_(2) . What fractio9n of the volume of the ball will be in the lower liquid.

A solid uniform ball having volume V and density rho floats at the interface of two unmixible liquids as shown in Fig. 7(CF).7. The densities of the upper and lower liquids are rho_(1) and rho_(2) respectively, such that rho_(1) lt rho lt rho_(2) . What fractio9n of the volume of the ball will be in the lower liquid.

A solid uniform ball having volume V and density rho floats at the interface of two unmixible liquids as shown in Fig. 7(CF).7. The densities of the upper and lower liquids are rho_(1) and rho_(2) respectively, such that rho_(1) lt rho lt rho_(2) . What fractio9n of the volume of the ball will be in the lower liquid.

A solid sphere of radius r is floating at the interface of two immiscible liquids of densities rho_(1) and rho_(2)(rho_(2) gt rho_(1)) , half of its volume lying in each. The height of the upper liquid column from the interface of the two liquids is h. The force exerted on the sphere by the upper liquid is (atmospheric pressure = p_(0) and acceleration due to gravity is g):

A solid sphere of radius r is floating at the interface of two immiscible liquids of densities rho_(1) and rho_(2)(rho_(2) gt rho_(1)) , half of its volume lying in each. The height of the upper liquid column from the interface of the two liquids is h. The force exerted on the sphere by the upper liquid is (atmospheric pressure = p_(0) and acceleration due to gravity is g):