This question asks for the specific distance on the axis of a circular coil where the magnetic field strength is reduced to one twenty-seventh (1/27th) of its value at the center.
The magnetic field ($B_x$) on the axis of a circular coil with radius $R$, carrying current $I$, at a distance $x$ from the center is given by the formula:
$ B_x = \frac{\mu_0 I R^2}{2 (R^2 + x^2)^{3/2}} $
The magnetic field ($B_0$) at the center of the coil (where $x=0$) is:
$ B_0 = \frac{\mu_0 I}{2R} $
We are given the condition that the magnetic field on the axis is $\frac{1}{27}$th of the field at the center:
$ B_x = \frac{1}{27} B_0 $
Substituting the formulas:
$ \frac{\mu_0 I R^2}{2 (R^2 + x^2)^{3/2}} = \frac{1}{27} \left( \frac{\mu_0 I}{2R} \right) $
Simplify by cancelling common terms ($\mu_0 I / 2$):
$ \frac{R^2}{(R^2 + x^2)^{3/2}} = \frac{1}{27R} $
Rearrange the equation:
$ 27 R^3 = (R^2 + x^2)^{3/2} $
To solve for $x$, raise both sides to the power of $\frac{2}{3}$:
$ (27 R^3)^{2/3} = \left( (R^2 + x^2)^{3/2} \right)^{2/3} $
$ (3^3 R^3)^{2/3} = R^2 + x^2 $
$ 3^2 R^2 = R^2 + x^2 $
$ 9 R^2 = R^2 + x^2 $
Now, isolate $x^2$:
$ x^2 = 9 R^2 - R^2 $
$ x^2 = 8 R^2 $
Finally, take the square root to find $x$:
$ x = \sqrt{8 R^2} $
$ x = \sqrt{8} R $
$ x = 2\sqrt{2} R $
Therefore, the distance from the center on the axis where the magnetic induction is $\frac{1}{27}$th of the value at the center is $2\sqrt{2} R$. This corresponds to Option A.
A uniform time-varying magnetic field exists in a circular region of radius $R$, directed perpendicular into the plane of the paper, increasing at a constant rate $\alpha$. A straight conducting rod of length $2R$ is placed exactly along the diameter of the circular region (passing through the centre). Find the induced emf across the rod.

There is a ring of radius $r$ having linear charge density $\lambda$ and rotating with a uniform angular velocity $\omega$. The magnitude of the magnetic field produced by this ring at its own centre would be
($\mu_0 = \text{permeability of air}$)