Two identical current carrying coils with same centre are placed with their planes perpendicular to each other. If i = \(\sqrt{2}A\) and radius of coil R = 1 m, then magnetic field at centre C is equal to:
\(\mu_{0}\)
The problem involves two identical current-carrying coils placed with their planes perpendicular to each other. We are required to find the magnetic field at the center, C.
Given data:
To find the magnetic field at the center of each coil, we use the formula for the magnetic field at the center of a circular current loop:
\(B = \frac{\mu_0 i}{2R}\)
Substituting the given values:
\(B_1 = \frac{\mu_0 \cdot \sqrt{2}}{2 \cdot 1} = \frac{\mu_0 \sqrt{2}}{2}\)
Since the fields due to the two coils are perpendicular, we use the Pythagorean theorem to find the resultant magnetic field \(B_r\) at the center:
\(B_r = \sqrt{B_1^2 + B_2^2}\)
Where both \(B_1\) and \(B_2\) are equal.
Substituting, we get:
\(B_r = \sqrt{\left(\frac{\mu_0 \sqrt{2}}{2}\right)^2 + \left(\frac{\mu_0 \sqrt{2}}{2}\right)^2}\)
Calculating further:
\(B_r = \sqrt{\frac{\mu_0^2 \cdot 2}{4} + \frac{\mu_0^2 \cdot 2}{4}}\)
\(B_r = \sqrt{\frac{\mu_0^2 \cdot 4}{4}}\)
\(B_r = \sqrt{\mu_0^2}\)
\(B_r = \mu_0\)
Therefore, the resultant magnetic field at the center is \(\mu_0\), which matches the correct option.
Consider two arrangements of wires. Find the ratio of magnetic field at the centre of the semi–circular part.