The determination of the value of acceleration due to gravity \((g)\) by simple pendulum method employs the formula,
\(g=4\pi^2\dfrac{L}{T^2}\)
The expression for the relative error in the value of \(g\) is:
| 1. | \(\dfrac{\Delta g}{g}=\dfrac{\Delta L}{L}+2\Big(\dfrac{\Delta T}{T}\Big)\) |
| 2. | \(\dfrac{\Delta g}{g}=4\pi^2\Big[\dfrac{\Delta L}{L}-2\dfrac{\Delta T}{T}\Big]\) |
| 3. | \(\dfrac{\Delta g}{g}=4\pi^2\Big[\dfrac{\Delta L}{L}+2\dfrac{\Delta T}{T}\Big]\) |
| 4. | \(\dfrac{\Delta g}{g}=\dfrac{\Delta L}{L}-2\Big(\dfrac{\Delta T}{T}\Big)\) |
| 1. | The dimensions of \(\beta\) are same as that of force. |
| 2. | The dimensions of \(\alpha^{-1}x\) are same as that of energy. |
| 3. | The dimensions of \(\eta^{-1} \sin \theta\) are same as that of \(\alpha \beta\). |
| 4. | The dimensions of \(\alpha\) same as that of \(\beta\). |
| 1. | \(\dfrac P V\) | 2. | \(\dfrac V P\) |
| 3. | \(PV\) | 4. | \(PV^3\) |
| 1. | \(2.42\times10^{-6} \) rad | 2. | \(2.85\times10^{-6} \) rad |
| 3. | \(2.91\times10^{-4} \) rad | 4. | \(1.75\times10^{-2} \) rad |
| List-I | List-II | ||
| \(\mathrm{(A)}\) | Torque | \(\mathrm{(I)}\) | N-m s-1 |
| \(\mathrm{(B)}\) | Stress | \(\mathrm{(II)}\) | J-kg-1 |
| \(\mathrm{(C)}\) | Latent Heat | \(\mathrm{(III)}\) | N-m |
| \(\mathrm{(D)}\) | Power | \(\mathrm{(IV)}\) | N-m-2 |
| 1. | \(\mathrm{A-III, B-II, C-I, D-IV}\) |
| 2. | \(\mathrm{A-III, B-IV, C-II, D-I}\) |
| 3. | \(\mathrm{A-IV, B-I, C-III, D-II}\) |
| 4. | \(\mathrm{A-II, B-III, C-I, D-IV}\) |
| 1. | \(1\) | 2. | \(2\) |
| 3. | \(3\) | 4. | \(5\) |