The loss of weight of a solid when immersed in a liquid at `0^(@)C` is `W_(0)` and at `t^(@)C` is `'W'`. If cubical coefficient of expansion of the solid and the liquid are `gamma_(s)` and `gamma_(1)` then `W =`

The loss of weight of a solid when immersed in a liquid at 0^(@)C" is "W_(0) . If alphaandbeta are the volume coefficients of expansion of the solid and the liquid respectively, then the loss of weight at t^(@)C is approximately

The loss of weight of a solid when immersed in a liquid at 0^(0)C is DeltaW_(0) . If alpha and beta are the volume coefficients of expansion of the solid and the liquid respectively, then the loss of weight at t^(@)C is approxumately

Apparent weights of a body immersed in a liquid at the temperature t_(1) is W_(1) and temperature t_(2) is W_(2) . Coefficients of volume expansion of the liquid and the solid are gamma and gamma_(s) respectively. The value of W_(2)-W_(1) will be

A metal ball immersed in water weighs w_(1) at 0^(@)C and w_(2) at 50^(@)C . The coefficient of cubical expansion of metal is less than that of water. Then

A metal ball immersed in water weighs w_(1) at 0^(@)C and w_(2) at 50^(@)C . The coefficient of cubical expansion of metal is less than that of water. Then

A metal sphere immersed in water weighs w_(1) at 0^(@) C and w_(2) at 50^(@) C . The coefficient of cubical expansion of the metal is less than that of water . Then