
To determine the distance \( x \) of point P from wire X, we must analyze the magnetic fields generated by both wires at point P. The magnetic field originating from a straight current-carrying wire at a radial distance \( r \) is quantified by:
\( B = \frac{\mu_0 I}{2\pi r} \)
For wire Y, situated at a distance of 4 cm:
\( B_Y = \frac{\mu_0 \times 4}{2\pi \times 0.04} = \frac{4\pi \times 10^{-7} \times 4}{2\pi \times 0.04} = 10^{-5} \, \text{T} \)
For wire X, located at a distance \( x \):
\( B_X = \frac{\mu_0 \times 5}{2\pi x} = \frac{4\pi \times 10^{-7} \times 5}{2\pi x} = \frac{10^{-6}}{x} \, \text{T} \)
Given that the currents flow in opposite directions, their respective magnetic fields at point P are antiparallel. Consequently, the net magnetic field \( B \) is calculated as:
\( B = |B_X - B_Y| = 3 \times 10^{-5} \, \text{T} \)
Upon substitution of the known values:
\( \left|\frac{10^{-6}}{x} - 10^{-5}\right| = 3 \times 10^{-5} \)
Assuming \( \frac{10^{-6}}{x} \) is greater than \( 10^{-5} \):
\( \frac{10^{-6}}{x} - 10^{-5} = 3 \times 10^{-5} \)
\( \frac{10^{-6}}{x} = 4 \times 10^{-5} \)
\( x = \frac{10^{-6}}{4 \times 10^{-5}} = \frac{1}{4} \times 10^1 = 2.5 \, \text{cm} \)
Consider two arrangements of wires. Find the ratio of magnetic field at the centre of the semi–circular part.