The magnetic field strength at the center of a tightly wound coil is calculated using the formula for the magnetic field at the center of a circular wire loop:
\[B=\frac{\mu_0 n I}{2R}\]
where:
Substituting the given values into the formula yields:
\[B = \frac{(4\pi \times 10^{-7}) \cdot 100 \cdot 7}{2 \cdot 0.1}\]
Performing the calculation within the parentheses first:
\[B = \frac{(4\pi \times 10^{-7}) \cdot 700}{0.2}\]
Simplifying further:
\[B = \frac{2800\pi \times 10^{-7}}{0.2}\]
\[B = 14000\pi \times 10^{-7}\]
Using the approximation \(\pi \approx 3.1416\):
\[B = 14000 \times 3.1416 \times 10^{-7}\]
\[B \approx 43998.4 \times 10^{-7}\]
Converting the magnetic field to milliTesla (1 T = 1000 mT):
\[B \approx 4.4 \, \text{mT}\]
Consequently, the magnetic field at the coil's center is approximately \(4.4 \, \text{mT}\).
In a uniform magnetic field of \(0.049 T\), a magnetic needle performs \(20\) complete oscillations in \(5\) seconds as shown. The moment of inertia of the needle is \(9.8 \times 10 kg m^2\). If the magnitude of magnetic moment of the needle is \(x \times 10^{-5} Am^2\); then the value of '\(x\)' is
