Step 1: Given Information
The physical quantity \( \vec{S} \) is defined as:
\[
\vec{S} = \frac{(\vec{E} \times \vec{B})}{\mu_0}
\]
where:
- \( \vec{E} \) is the electric field,
- \( \vec{B} \) is the magnetic field,
- \( \mu_0 \) is the permeability of free space.
We are asked to determine the dimensions of \( \vec{S} \) and match them with the dimensions of one of the given quantities.
Step 2: Determining the Dimensions of \( \vec{S} \)
The dimensions of \( \vec{S} \) depend on the cross product of the electric field \( \vec{E} \) and the magnetic field \( \vec{B} \), and the permeability of free space \( \mu_0 \). We start by analyzing the dimensions of each term:
- The dimensions of the electric field \( \vec{E} \) are given by:
\[
[E] = \frac{M L^2}{T^3 A}
\]
where \( M \) is mass, \( L \) is length, \( T \) is time, and \( A \) is the electric current.
- The dimensions of the magnetic field \( \vec{B} \) are:
\[
[B] = \frac{M}{T^2 A}
\]
- The permeability of free space \( \mu_0 \) has the dimensions:
\[
[\mu_0] = \frac{M}{A^2 T^2}
\]
Now, the cross product \( \vec{E} \times \vec{B} \) results in the dimensions:
\[
[\vec{E} \times \vec{B}] = \left[\frac{M L^2}{T^3 A} \times \frac{M}{T^2 A}\right] = \frac{M^2 L^2}{T^5 A^2}
\]
Dividing by \( \mu_0 \), we get the dimensions of \( \vec{S} \):
\[
[\vec{S}] = \frac{\frac{M^2 L^2}{T^5 A^2}}{\frac{M}{A^2 T^2}} = \frac{M L^2}{T^3 A}
\]
Step 3: Matching the Dimensions
Now, we compare the dimensions of \( \vec{S} \) with the given options. We are asked to find the quantity that has the same dimensions as \( \vec{S} \). The options are:
- (B) \( \frac{\text{Force}}{\text{Length} \times \text{Time}} \)
- (D) \( \frac{\text{Force}}{\text{Length} \times \text{Time}} \)
The dimensions of force \( F \) are:
\[
[F] = \frac{M L}{T^2}
\]
Therefore, the dimensions of \( \frac{\text{Force}}{\text{Length} \times \text{Time}} \) are:
\[
\left[\frac{F}{L T}\right] = \frac{M L}{T^2} \times \frac{1}{L T} = \frac{M}{T^3 A}
\]
This matches the dimensions of \( \vec{S} \). Therefore, both options (B) and (D) are correct.
Final Answer:
The correct options are:
- (B) \( \frac{\text{Force}}{\text{Length} \times \text{Time}} \)
- (D) \( \frac{\text{Force}}{\text{Length} \times \text{Time}} \)
Two concentric circular loops, one of radius $R$ and the other of radius $2 R$, lie in the $x y$-plane with the origin as their common centre, as shown in the figure . The smaller loop carries current $I_{1}$ in the anti-clockwise direction and the larger loop carries current $I_{2}$ in the clock wise direction, with $I_{2}>2 I_{1}, \vec{B}(x, y)$ denotes the magnetic field at a point $(x, y)$ in the $x y$-plane. Which of the following statement (s) is ( are ) correct?
A special metal S conducts electricity without any resistance A closed wire loop, made of S, does not allow any change in flux through itself by inducing a suitable current to generate a compensating flux The induced current in the loop cannot decay due to its zero resistance This current gives rise to a magnetic moment which in turn repels the source of magnetic field or flux Consider such a loop, of radius a, with its centre at the origin A magnetic dipole of moment $m$ is brought along the axis of this loop from infinity to a point at distance $r(>>$ a) from the centre of the loop with its north pole always facing the loop, as shown in the figure below The magnitude of magnetic field of a dipole $m$, at a point on its axis at distance $r$, is $\frac{\mu_{0}}{2 \pi} \frac{ m }{ r ^{3}}$, where $\mu_{0}$ is the permeability of free space The magnitude of the force between two magnetic dipoles with moments, $m _{1}$ and $m _{2}$, separated by a distance $r$ on the common axis, with their north poles facing each other, is $\frac{ km _{1} m _{2}}{ r ^{4}}$, where $k$ is a constant of appropriate dimensions The direction of this force is along the line joining the two dipoles When the dipole $m$ is placed at a distance $r$ from the center of the loop (as shown in the figure), the current induced in the loop will be proportional to