To determine the magnitude of the magnetic field at the center of a tightly wound coil, we use the formula for the magnetic field at the center of a circular loop of wire:
\[B=\frac{\mu_0 n I}{2R}\]
where:
Substituting the given values into the formula:
\[B = \frac{(4\pi \times 10^{-7}) \cdot 100 \cdot 7}{2 \cdot 0.1}\]
Calculating the expression inside the parentheses first:
\[B = \frac{(4\pi \times 10^{-7}) \cdot 700}{0.2}\]
Further simplifying:
\[B = \frac{2800\pi \times 10^{-7}}{0.2}\]
\[B = 14000\pi \times 10^{-7}\]
Simplifying \(\pi \approx 3.1416\):
\[B = 14000 \times 3.1416 \times 10^{-7}\]
\[B \approx 43998.4 \times 10^{-7}\]
Converting the field into milliTesla (1T = 1000 mT):
\[B \approx 4.4 \, \text{mT}\]
Therefore, the magnitude of the magnetic field at the center of the coil is approximately \(4.4 \, \text{mT}\).
Step 1: Use the formula for the magnetic field at the center of a circular coil. - The magnetic field at the center of a circular coil is given by: \[ B = \frac{\mu_0 N I}{2R} \] where N = 100 (number of turns), I = 7A (current), R = 0.1m (radius), and \(\mu_0 = 4\pi \times 10^{-7} Tm/A\) (permeability of free space). Step 2: Substitute the values into the formula. \[ B = \frac{(4\pi \times 10^{-7}) \cdot 100 \cdot 7}{2 \times 0.1} \] Simplify: \[ B = \frac{28\pi \times 10^{-7}}{0.2} \] \[ B = 4.4 \times 10^{-3} T = \mathbf{4.4mT} \]
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
The current passing through the battery in the given circuit, is:
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :