Tow liquids of desities `rho_(1)` and `rho_(2)(rho_(2) = 2rho_(1))` are filled up behind a square wall of side 10 m as shown in the figure. Each liquids has a height of 5m. The ratio of the forces due to these liqyuids exeted on upper part MN to that at the lower part NO is (Assume that the liquids are not mixing):

Two liquids of densities rho_(1) and rho_(2)(rho_(2) = 2rho_(1)) are filled up behind a square wall of side 10 m as shown in the figure. Each liquids has a height of 5m. The ratio of the forces due to these liqyuids exeted on upper part MN to that at the lower part NO is (Assume that the liquids are not mixing):

Two liquids of densities rho_1 and rho_2(rho_2 = 3 rho_1) are filled up behind a square wall of side 6 m as shown in figure. Each liquid has a height of 3 m. The ratio of the forces due to these liquids exerted on upper part MN to that at the lower part NO is (Assume that the liquids are not mixing)2

Two liquids of densities rho_1 and rho_2(rho_2 = 3 rho_1) are filled up behind a square wall of side 6 m as shown in figure. Each liquid has a height of 3 m. The ratio of the forces due to these liquids exerted on upper part MN to that at the lower part NO is (Assume that the liquids are not mixing)2

Two liquids of densities rho_1 and rho_2(rho_2 = 3 rho_1) are filled up behind a square wall of side 6 m as shown in figure. Each liquid has a height of 3 m. The ratio of the forces due to these liquids exerted on upper part MN to that at the lower part NO is (Assume that the liquids are not mixing)2

Two liquids of densities p_(1) and p_(2) (p2_= 6 p1 ) are filled up behind a square wall of side 8 m as shown in figure. The liquids have height as shown. The ratio of the forces due to these liquids exerted on upper part MN to that at the lower part NO is (Assume that the liquids are not mixing)

Two liquids of densities p_(1) and p_(2) (p2_= 6 p1 ) are filled up behind a square wall of side 8 m as shown in figure. The liquids have height as shown. The ratio of the forces due to these liquids exerted on upper part MN to that at the lower part NO is (Assume that the liquids are not mixing)

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):