The duration of one day is determined by the rotational period of the Earth. If the radius is halved while the mass remains constant, the Earth's moment of inertia \(I\) will change according to:
\[I = k M R^2\]
where \(k\) is a constant, \(M\) is mass, and \(R\) is radius.
Reducing \(R\) by half means:
\[I_{\text{new}} = k M \left(\frac{R}{2}\right)^2 = \frac{1}{4} I_{\text{old}}\]
With a smaller moment of inertia and the same angular momentum (since angular momentum is conserved if no external torques are applied), the Earth would spin faster. The new rotational period \(T_{\text{new}}\) can be estimated by considering the conservation of angular momentum:
\[T_{\text{new}} = \frac{T_{\text{old}}}{2}\]
Given the current period is approximately 24 hours, the new period would be:
\[T_{\text{new}} = \frac{24 \, \text{h}}{2} = 12 \, \text{h}\]
However, because the moment of inertia is reduced by a factor of 4, the day will shorten further, leading to a period of \(6 \, \text{h}\).
| List I | List II |
|---|---|
| (A) The linear momentum of the system remains constant | (IV) The net external force acting on a system of particles is zero |
| (B) The angular momentum of the system remains constant | (III) The external torque acting on a system of particles is zero |
| (C) Inertial frame | (I) The frames relative to which an unaccelerated body appears unaccelerated |
| (D) Non-inertial frame | (II) The frames relative to which an unaccelerated body appears accelerated |
| LIST I | LIST II |
|---|---|
| A. Maxwell's First Equation | I. Modified Ampere's Law |
| B. Maxwell's Second Equation | II. Faraday's Laws of Electromagnetic Induction |
| C. Maxwell's Third Equation | III. Gauss Law in Electrostatics |
| D. Maxwell's Fourth Equation | IV. Gauss Law in Magnetostatics |
| List I | List II |
|---|---|
| (A) (∂S/∂P)T | (I) (∂P/∂T)V |
| (B) (∂T/∂V)S | (II) (∂V/∂S)P |
| (C) (∂T/∂P)S | (III) -(∂V/∂T)P |
| (D) (∂S/∂V)T | (IV) -(∂P/∂S)V |
| List I | List II |
|---|---|
| (A) The linear momentum of the system remains constant | (IV) The net external force acting on a system of particles is zero |
| (B) The angular momentum of the system remains constant | (III) The external torque acting on a system of particles is zero |
| (C) Inertial frame | (I) The frames relative to which an unaccelerated body appears unaccelerated |
| (D) Non-inertial frame | (II) The frames relative to which an unaccelerated body appears accelerated |