To find the radius of the coil, we start with Faraday's law of electromagnetic induction, which states that the induced emf \( \varepsilon \) in a coil is given by the rate of change of magnetic flux \( \Phi \) through the coil:
\(\varepsilon = -\frac{d\Phi}{dt}\)
The magnetic flux \( \Phi \) is given by:
\(\Phi = B \cdot A \cdot \cos(\theta)\)
where \( B = 0.25 \, \text{T} \) is the magnetic field strength, \( A \) is the area of the coil, and \( \theta \) is the angle between the magnetic field and the normal to the coil's plane.
The area \( A \) of the circular coil is:
\( A = \pi r^2 \)
Given that the coil rotates with an angular speed of \( \omega = 6 \, \text{rpm} = \frac{6 \times 2\pi}{60} \, \text{rad/s} = 0.2 \pi \, \text{rad/s}\), the angle \( \theta \) changes with time as \( \theta = \omega t\). After rotation by 30° (\(\theta = 30^\circ = \frac{\pi}{6}\)), and \(\varepsilon = 1.6 \, \text{mV} = 1.6 \times 10^{-3} \, \text{V}\).
Now, find \( \varepsilon \) using the induced emf formula:
\(\varepsilon = \left| \frac{d}{dt}(B \pi r^2 \cos(\omega t)) \right|\)
\(\varepsilon = \left| -B \pi r^2 \omega \sin(\omega t) \right|\)
At \( t \) when \(\theta = \frac{\pi}{6}\),
\(\sin(\omega t) = \sin\left(\frac{\pi}{6}\right) = \frac{1}{2}\)
Substitute the values, we get:
\(1.6 \times 10^{-3} = 0.25 \times \pi \times r^2 \times 0.2\pi \times \frac{1}{2}\)
Solve for \( r^2 \):
\(1.6 \times 10^{-3} = 0.25 \times \pi \times r^2 \times 0.1\pi\)
\(r^2 = \frac{1.6 \times 10^{-3}}{0.025 \times \pi^2}\)
Using \(\pi^2 = 10\) from given:
\(r^2 = \frac{1.6 \times 10^{-3}}{0.025 \times 10}\)
\(r^2 = \frac{1.6 \times 10^{-3}}{0.25}\)
\(r^2 = 6.4 \times 10^{-3}\)
\(r = \sqrt{6.4 \times 10^{-3}} \approx 0.08 \, \text{m} = 8 \, \text{cm}\)
Thus, the radius of the coil is \(8 \, \text{cm}\), fitting the range 8,8.