91Ó°ÊÓ

Circular loops are loops which have a consistent circular shape. They are essential in physics, especially when discussing magnetic fields. When a current passes through a circular loop of wire, it generates a magnetic field perpendicular to the plane of the loop. Circular loops are commonly used in experiments and applications to demonstrate how electricity and magnetism interact.
In this context, we have two concentric circular loops, meaning one loop is inside the other, each lying flat on a tabletop. The key aspect for these loops is their size, expressed by their diameter. The inner loop has a diameter of 20.0 cm, while the outer is larger, at 30.0 cm.
The magnetic field generated by a circular loop depends heavily on its size and the current flowing through it. Knowing the radii helps in calculating the magnetic field strength at the center.

The direction of the current plays a crucial role in determining the direction of the magnetic field it produces. In our example, the inner loop carries a clockwise current when seen from above. Current direction is not arbitrary; it is determined by how the electrons move through the conducting path.
Direction of current decides the loop's magnetic field direction due to the magnetic field lines rotating around the wire path. If you invert the current direction, the magnetic field direction also flips.
In the exercise, we're given that the inner loop has this clockwise current, while the calculation for the outer loop suggests that it should carry a current counterclockwise. This opposing direction is necessary to cancel out the magnetic fields at the center of the loops.

The right-hand rule is a mnemonic that helps determine the direction of the magnetic field relative to the direction of current flow. To apply it, you "grab" the loop of wire with your right hand such that your thumb points in the direction of the current flow. Your fingers then curl in the direction of the generated magnetic field lines.
Using this rule, we decide the necessary direction for current in the outer loop. For the inner loop, with clockwise current, the magnetic field at the center goes downward. To cancel this field at the center, the current in the outer loop must create an upward magnetic field.
This upward field is generated when the current in the outer loop is counterclockwise, as the right-hand rule indicates that a counterclockwise current results in an upward field at the loop's center when viewed from above.

The net magnetic field is the sum of all individual magnetic fields present at a certain point. In our case, it's the result of adding the fields from two loops. We're tasked with adjusting these fields to make the net magnetic field at the loops' common center zero.
To achieve this, the magnetic fields produced by each loop must be equal in magnitude but opposite in direction. The inner loop creates a downward magnetic field due to its clockwise current. Thus, the task is to engineer the outer loop's field to be upward and equal in strength.
By adjusting the current magnitude and direction in the outer loop, specifically to -18.1 A in a counterclockwise direction, the net magnetic field at the center can effectively be nulled, as both fields perfectly counterbalance each other.