We are able to squeeze snow and make balls out of it because of
anomalous behaviour of water
large latent heat of ice
large specific heat of water
low melting point of ice
The apparent coefficient of expansion of a liquid when heated in a copper vessel is $C$ and when heated in a silver vessel is $S$. If $A$ is the linear coefficient of expansion of copper, then the linear coefficient of expansion of silver is
A beaker is completely filled with water at $4°C$. It will overflow if
A non-isotropic solid metal cube has coefficients of linear expansion as:
$5 \times 10^{-5} /^{\circ} \mathrm{C}$ along the $\mathrm{x}$ -axis and $5 \times 10^{-6} /^{\circ} \mathrm{C}$ along the $y$ and the $z-$axis. If the coefficient of volume expansion of the solid is $\mathrm{C} \times 10^{-6} /^{\circ} \mathrm{C}$ then the value of $\mathrm{C}$ is
We would like to make a vessel whose volume does not change with temperature (take a hint from the problem above). We can use brass and iron $\left( {{\beta _{{\text{v brass }}}} = 6 \times {{10}^{ - 5}}/K} \right.$ and $\left. {{\beta _{{\text{viron }}}} = 3.55 \times {{10}^{ - 5}}/K} \right)$ to create a volume of $100\,cc$ . How do you think you can achieve this.
The coefficients of thermal expansion of steel and a metal $X$ are respectively $12 × 10^{-6}$ and $2 × 10^{-6} per^o C$. At $40^o C$, the side of a cube of metal $X$ was measured using a steel vernier callipers. The reading was $100 \,\,mm$.Assuming that the calibration of the vernier was done at $0^o C$, then the actual length of the side of the cube at $0^o C$ will be