
Step 1: Given Information
Two concentric circular loops are given, one with radius \( R \) and the other with radius \( 2R \). The loops are in the \( xy \)-plane, sharing the origin as their common center.
- The smaller loop carries current \( I_1 \) in the anti-clockwise direction.
- The larger loop carries current \( I_2 \) in the clockwise direction, and we are given that \( I_2 > 2I_1 \).
- We are asked to determine the magnetic field \( \vec{B}(x, y) \) at a point \( (x, y) \) in the \( xy \)-plane.
Step 2: Magnetic Field Due to Circular Current Loop
The magnetic field at a point due to a current-carrying circular loop is given by the Biot-Savart law. The field produced by each loop at any point in the plane of the loop depends on the distance from the point to the center of the loop.
- For a point in the plane of the loop, the magnetic field produced by each loop is perpendicular to the plane of the loop, pointing either upward or downward, depending on the direction of the current.
- The contribution of each loop to the magnetic field at any point depends on the radial distance \( r = \sqrt{x^2 + y^2} \) from the center.
Step 3: Analyzing Statement A
We are asked to verify whether \( \vec{B}(x, y) \) is perpendicular to the \( xy \)-plane at any point in the plane.
- The magnetic field produced by each loop is directed along the axis perpendicular to the plane of the loop, which is the \( z \)-axis in this case.
- Therefore, the magnetic field at any point in the \( xy \)-plane will be along the \( z \)-axis, meaning it will be perpendicular to the \( xy \)-plane.
Hence, statement (A) is correct.
Step 4: Analyzing Statement B
We are asked to verify whether \( |\vec{B}(x, y)| \) depends on \( x \) and \( y \) only through the radial distance \( r = \sqrt{x^2 + y^2} \).
- From the Biot-Savart law and the symmetry of the problem, the magnetic field at any point in the \( xy \)-plane due to both loops will depend only on the radial distance \( r \) from the center of the loops.
- Since the magnetic field produced by each loop is a function of the radial distance \( r \), and because the loops are symmetric about the origin, the field will only depend on \( r \), which is a function of \( x \) and \( y \) as \( r = \sqrt{x^2 + y^2} \).
Hence, statement (B) is correct.
Final Answer:
Both statements (A) and (B) are correct:
- (A) \( \vec{B}(x, y) \) is perpendicular to the \( xy \)-plane at any point in the plane.
- (B) \( |\vec{B}(x, y)| \) depends on \( x \) and \( y \) only through the radial distance \( r = \sqrt{x^2 + y^2} \).
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