1. | \(\dfrac{\Delta\theta_1}{\Delta\theta_2}\) | 2. | \(\dfrac{r_1}{r_2}\) |
3. | \(\dfrac{r_2\Delta\theta_2}{r_1\Delta\theta_1}\) | 4. | \(\dfrac{r_2\Delta\theta_1}{r_1\Delta\theta_2}\) |
1. | \(\left(\dfrac{\Delta I_0}{I_0}\right)\dfrac{1}{\Delta\theta}\) |
2. | \(\dfrac12\left(\dfrac{\Delta I_0}{I_0}\right)\dfrac{1}{\Delta\theta}\) |
3. | \(\dfrac15\left(\dfrac{\Delta I_0}{I_0}\right)\dfrac{1}{\Delta\theta}\) |
4. | \(2\left(\dfrac{\Delta I_0}{I_0}\right)\dfrac{1}{\Delta\theta}\) |
1. | \(P\) to \(Q\). | heat would flow from
2. | \(Q\) to \(P\) . | heat would flow from
3. | \(P\) & \(Q\). | no flow of heat occurs between
4. | \(P\) & \(Q,\) varying with time. | flow of heat may occur back and forth between
1. | \(a\) | 2. | \(b\) |
3. | \(c\) | 4. | \(d\) |
1. | \({\Large\gamma}_L\theta\times{\large p}_0 ~\) |
2. | \({\Large\frac{\theta}{273}}{\large p}_0\) |
3. | \({\dfrac{{\Large\gamma}_L\theta}{273}}{\large p}_0\) |
4. | \(\Big({\Large\gamma}_L\theta+{\Large\frac{\theta}{273}}\Big){\large p}_0 \) |
1. | \(\lambda_m\propto v\) | 2. | \(\lambda_m\propto \dfrac1v\) |
3. | \(\lambda_m\propto v^2 \) | 4. | \(\lambda_m\propto \dfrac1{v^2}\) |
1. | \(0.6\) | 2. | \(0.3\) |
3. | \(0.4\) | 4. | \(0.5\) |