For an infinitely long wire bent into a semi-circular shape, we can use the Biot-Savart law to find the magnetic field at the center of the semi-circular loop.
The formula for the magnetic induction along the axis of a semi-circular loop of current is given by: \[ B = \frac{\mu_0 I}{4r} \] Where: - \( \mu_0 \) is the permeability of free space, - \( I \) is the current, - \( r \) is the radius of the semi-circular loop. Given that the radius is 1 m and the magnetic field along the axis is directed along the line passing through the center of the semi-circle, the magnitude of the magnetic induction is \( \frac{\mu_0 I}{4r} \).
Thus, the magnetic induction is \( \frac{\mu_0 I}{4r} \, \text{T} \).
Two point charges M and N having charges +q and -q respectively are placed at a distance apart. Force acting between them is F. If 30% of charge of N is transferred to M, then the force between the charges becomes:
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be: