The question involves understanding magnetic dipole moments and the magnetic field in a circular loop. Let's analyze each step to find the solution.
1. **Magnetic Dipole Moment (m):**
The magnetic dipole moment for a circular loop carrying a current \( I \) and having a radius \( r \) is given by:
m = I \cdot A, where A is the area of the loop. For a circular loop, A = \pi r^2.
2. **Magnetic Field at the Centre (B):**
The magnetic field at the center of the loop is given by:
B = \frac{\mu_0 I}{2r}, where \mu_0 is the permeability of free space.
3. **Relation Between m and B at the Centre:** B = \frac{\mu_0 \cdot m}{2 \pi r^3}. However, since m = I \cdot \pi r^2, we can rearrange to find:
B = \frac{\mu_0 \cdot I}{2r} = \frac{\mu_0 \cdot m}{2 \pi r^3}
4. **Doubling the Dipole Moment:** If the dipole moment \( m \) is doubled while keeping \( I \) constant, it means the area or size of the loop is changed. Let the new dipole moment be m_2 = 2m. We now analyze the change in magnetic field.
5. **New Magnetic Field (B2):** Using the same relation from step 3, the new magnetic field B_2 is proportional to the new dipole moment:
B_2 = \frac{\mu_0 \cdot m_2}{2 \pi r_2^3}
Given m_2 = 2m and realizing that the loop size is such that its new radius r_2 = \sqrt{2} \cdot r, we can substitute and rearrange:
B_2 = \frac{\mu_0 \cdot (2m)}{2 \pi (\sqrt{2}r)^3} = \frac{\mu_0 \cdot m}{\pi 2.828r^3}
6. **Finding the Ratio:** To find the ratio \frac{B_1}{B_2}:
\frac{B_1}{B_2} = \frac{\frac{\mu_0 \cdot m}{2 \pi r^3}}{\frac{\mu_0 \cdot m}{\pi 2.828r^3}}
Simplifying, we find:
\frac{B_1}{B_2} = \sqrt{2}
Hence, the correct answer is \sqrt{2}.
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
