A single current-carrying loop of wire carrying current I flows in the anticlockwise direction (seen from the +z direction) and lies in the xy plane. The plot of \(\hat{j}\) component of magnetic field (\(B_y\)) at a distance a (less than radius of the coil) and on the yz plane vs z coordinate looks like:
For magnetic field due to current loops:
• Use the right-hand rule to determine the direction of the field.
• Symmetry plays a critical role in analyzing magnetic field variations.




To solve this problem, we need to determine the behavior of the \(B_y\) component of the magnetic field created by a current loop at a certain point in space.
Given:
Concepts and Analysis:
According to Ampere's Law and Biot-Savart Law, the magnetic field due to a loop of wire has cylindrical symmetry around the axis of the loop (in this case, the \(z\) axis). The magnetic field at a point off the axis can be understood as having three components \((B_x, B_y, B_z)\), but here we only consider the \(B_y\) component.
At any plane parallel to \(xy\), due to the symmetry and direction of the current, it is expected that the \(B_y\) component is non-zero. For positions symmetrically above or below the loop, the vertical component will change direction.
Specifically, the \(B_y\) component at a distance will show a sign change as the position crosses the plane of the loop (\(z=0\)).
Correct Option:
The observed behavior is graphically represented in the correct answer image:

This plot contains matching behavior for \(B_y\), which is zero at the loop center and changes sign as one moves through \(z=0\).
Reasoning Behind Incorrect Options:
