Mutual inductance \( M \) is a measure of the ability of one current-carrying conductor to induce a current in another conductor.
For a square loop moving away from a long current-carrying conductor, the mutual inductance is given by:
\( M = \mu_0 N \frac{a^2}{2R} \)
where \( a \) is the side length of the square loop,
\( R \) is the distance between the conductor and the loop, and
\( N \) is the number of turns.
As the square loop moves away from the conductor, the distance \( R \) increases, resulting in a decrease in mutual inductance over time.
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly: