The volume of the bulb of a mercury thermometer at $0^o C$ is $V_0$and cross section of the capillary is $A_0$. The coefficient of linear expansion of glass is $a_g$ $per ^o C$ and the cubical expansion of mercury $\gamma_m$ $per ^o C$. If the mercury just fills the bulb at $0^o C$, what is the length of mercury column in capillary at $T^o C.$
$\frac{{{V_0}T\left( {{\gamma _m}\, - \,3{a_g}} \right)}}{{{A_0}\left( {1\, + \,2{a_g}T} \right)}}$
$\frac{{{V_0}T\left( {{\gamma _m}\, - \,3{a_g}} \right)}}{{{A_0}\left( {1\, + \,2{a_g}T} \right)}}$
$\frac{{{V_0}T\left( {{\gamma _m}\, + \,2{a_g}} \right)}}{{{A_0}\left( {1\, + \,3{a_g}T} \right)}}$
$\frac{{{V_0}T\left( {{\gamma _m}\, + \,2{a_g}} \right)}}{{{A_0}\left( {1\, + \,3{a_g}T} \right)}}$
A circular disc is shown. On heating, $d_1$ increases by $0.3\%$ , then $d_2$ will
A rod of length $l$ and radius $r$ is held between two rigid walls so that it is not allowed to expand. If its temperature is increased, then the force developed in it is proportional to .........
Give temperature $^oC$, $^oF$ and $K$ when density of water is maximum.
A sphere of diameter $7\,\, cm$ and mass $266.5 \,\,gm$ floats in a bath of a liquid. As the temperature is raised, the sphere just begins to sink at a temperature $35^o C$. If the density of a liquid at $0^o C$ is $1.527 \,\,gm/cc$, then neglecting the expansion of the sphere, the coefficient of cubical expansion of the liquid is$f$ :
An ideal gas is expanding such that ${PT}^{3}=$ constant. The coefficient of volume expansion of the gas is: