To solve the given problem, let's start by analyzing the torque acting on a current-carrying coil in a magnetic field.
When a coil with current \( i \) is placed in a magnetic field \( \vec{B} \), and the plane of the coil is perpendicular to the direction of the magnetic field, the torque \( \tau \) on the coil is given by the formula:
\( \tau = n \cdot i \cdot A \cdot B \cdot \sin(\theta) \)
where:
Given that the magnetic field \( \vec{B} \) is in the plane of the coil, the angle \( \theta = 90^\circ \), hence \( \sin(\theta) = 1 \).
For an equilateral triangle with side \( l \), the area \( A \) is given by:
\( A = \frac{\sqrt{3}}{4} l^2 \)
Substitute the area \( A \) in the torque formula:
\( \tau = i \cdot \left(\frac{\sqrt{3}}{4} l^2\right) \cdot B \)Rearranging to find \( l^2 \), we have:
\( l^2 = \frac{4 \tau}{\sqrt{3} i B} \)
Solving for \( l \), we take the square root:
\( l = \sqrt{\frac{4 \tau}{\sqrt{3} i B}} \)
Simplifying further, we have:
\( l = 2 \left(\frac{\tau}{\sqrt{3} i B}\right)^{1/2} \)
Thus, the option \(2 \left(\frac{\tau}{\sqrt{3} i B}\right)^{1/2}\) is the correct answer, which matches the given correct answer.