Step 1: Understanding the Concept:
This problem involves the formulas for the magnetic field produced by a circular current loop, both at its center and at a point along its axis. We need to establish a relationship between the two.
Step 2: Key Formula or Approach:
Let \(r\) be the radius of the coil.
- The magnetic field at the center of the coil is: \(B_{center} = \frac{\mu_0 I}{2r}\).
- The magnetic field at a distance \(x\) from the center on its axis is: \(B_{axis} = \frac{\mu_0 I r^2}{2(r^2 + x^2)^{3/2}}\).
Step 3: Detailed Explanation:
First, let's relate the given distances to the radius \(r\).
- Diameter of the coil = \(d\).
- Radius of the coil, \(r = d/2\).
- The distance from the center, \(x = \sqrt{2} d = \sqrt{2} (2r) = 2\sqrt{2} r\).
We are given that the field at this distance \(x\) is \(B\). Let's write the expression for \(B\):
\[ B = B_{axis} = \frac{\mu_0 I r^2}{2(r^2 + (2\sqrt{2} r)^2)^{3/2}} \]
Now, simplify the denominator:
\[ r^2 + (2\sqrt{2} r)^2 = r^2 + 8r^2 = 9r^2 \]
So, the expression for B becomes:
\[ B = \frac{\mu_0 I r^2}{2(9r^2)^{3/2}} = \frac{\mu_0 I r^2}{2 \times 9^{3/2} \times (r^2)^{3/2}} = \frac{\mu_0 I r^2}{2 \times (3^2)^{3/2} \times r^3} = \frac{\mu_0 I r^2}{2 \times 3^3 \times r^3} = \frac{\mu_0 I r^2}{2 \times 27 \times r^3} \]
\[ B = \frac{\mu_0 I}{54r} \quad \cdots(1) \]
We need to find the magnetic field at the center, \(B_{center}\):
\[ B_{center} = \frac{\mu_0 I}{2r} \quad \cdots(2) \]
To relate \(B_{center}\) to \(B\), we can express \(\frac{\mu_0 I}{r}\) from equation (1):
\[ \frac{\mu_0 I}{r} = 54B \]
Now substitute this into equation (2):
\[ B_{center} = \frac{1}{2} \left( \frac{\mu_0 I}{r} \right) = \frac{1}{2} (54B) = 27B \]
Step 4: Final Answer:
The magnetic field at the centre of the coil is 27B. Therefore, option (B) is correct.