(I) Ampere’s Circuital Law:
Ampere’s circuital law states that the line integral of the magnetic field \( \vec{B} \) around any closed loop is equal to \( \mu_0 \) times the net current \( I_{\text{enc}} \) enclosed by the loop: \[ \oint \vec{B} \cdot d\vec{l} = \mu_0 I_{\text{enc}} \] Where:
This law is analogous to Gauss’s law in electrostatics and is applicable in highly symmetric situations (e.g., long straight wires, solenoids).
(II) Magnetic Field Outside a Long Solenoid:
As the solenoid becomes longer, the magnetic field lines inside become more uniform and denser, while the field lines outside begin to cancel due to opposite currents in adjacent turns.
In the ideal case of an infinitely long solenoid, the field outside is: \[ B_{\text{outside}} = 0 \]
Reason: The field lines from each turn outside the solenoid point in different directions and tend to cancel each other out due to symmetry. Hence, as length increases, the external field weakens and tends toward zero.
(III) Flexible Loop Becoming Circular in Magnetic Field:
A current-carrying loop placed in an external magnetic field experiences a force that tends to minimize its potential energy. The magnetic pressure acts along the wire, pulling it into a shape that encloses maximum area for minimum perimeter — a circle.
Reason: According to Lenz's law and the tendency to minimize magnetic potential energy, the system favors a configuration with maximum magnetic flux linkage — which occurs when the loop is circular. Thus, a flexible irregular loop deforms into a circle.
Prove that:
\( \tan^{-1}(\sqrt{x}) = \frac{1}{2} \cos^{-1}\left( \frac{1 - x}{1 + x} \right), \quad x \in [0, 1] \)