\(√R\)
\(R^{\frac{3}{2}}\)
\(R^{2}\)
Magnetic Flux Linked with Loop B
Step 1: Magnetic Field Due to Loop A
- The magnetic field \( B \) at the center of a circular loop carrying a current \( I \) is given by the formula: \[ B = \frac{\mu_0 I}{2R} \] where:
- \( R \) = radius of loop A,
- \( \mu_0 \) = permeability of free space.
Step 2: Magnetic Flux Linked with Loop B
- The magnetic flux \( \Phi_B \) linked with loop B is given by: \[ \Phi_B = B \times A_B \] where:
- \( A_B = \pi r^2 \) is the area of loop B,
- \( r = \frac{R}{20} \) is the radius of loop B. Thus, \[ \Phi_B = \left( \frac{\mu_0 I}{2R} \right) \times \pi \left( \frac{R}{20} \right)^2 \] Simplifying: \[ \Phi_B = \frac{\mu_0 I \pi R^2}{2R \times 400} = \frac{\mu_0 I \pi R}{800} \] Thus, the magnetic flux linked with loop B is directly proportional to \( R \).
Step 3: Conclusion
The magnetic flux linked with loop B is proportional to \( R \), so the correct answer is: \[ \boxed{(A) \, R} \]
A current-carrying coil is placed in an external uniform magnetic field. The coil is free to turn in the magnetic field. What is the net force acting on the coil? Obtain the orientation of the coil in stable equilibrium. Show that in this orientation the flux of the total field (field produced by the loop + external field) through the coil is maximum.
Simar, Tanvi, and Umara were partners in a firm sharing profits and losses in the ratio of 5 : 6 : 9. On 31st March, 2024, their Balance Sheet was as follows:
Liabilities | Amount (₹) | Assets | Amount (₹) |
Capitals: | Fixed Assets | 25,00,000 | |
Simar | 13,00,000 | Stock | 10,00,000 |
Tanvi | 12,00,000 | Debtors | 8,00,000 |
Umara | 14,00,000 | Cash | 7,00,000 |
General Reserve | 7,00,000 | Profit and Loss A/c | 2,00,000 |
Trade Payables | 6,00,000 | ||
Total | 52,00,000 | Total | 52,00,000 |
Umara died on 30th June, 2024. The partnership deed provided for the following on the death of a partner:
If \(\begin{vmatrix} 2x & 3 \\ x & -8 \\ \end{vmatrix} = 0\), then the value of \(x\) is: