The magnetic field at the center of a semicircular wire carrying current \(I\) and having radius \(R\) is given by:
\(B = \frac{\mu_0 I}{4R}.\)
For the semicircular wires of radii \(R_1\) and \(R_2\):
\(B_{R_1} = \frac{\mu_0 I}{4R_1}, \quad B_{R_2} = \frac{\mu_0 I}{4R_2}.\)
The net magnetic field at the center \(O\) is the sum of the fields due to both semicircular wires:
\(B = B_{R_1} + B_{R_2} = \frac{\mu_0 I}{4R_1} + \frac{\mu_0 I}{4R_2}.\)
Substituting the given values:
\(B = \frac{4\pi \times 10^{-7} \cdot 4}{4 \cdot 2} + \frac{4\pi \times 10^{-7} \cdot 4}{4 \cdot 4}.\)
Simplify:
\(B = \pi \times 10^{-7} + \frac{\pi \times 10^{-7}}{2} = 2\pi \times 10^{-7} + \pi \times 10^{-7} = 3\pi \times 10^{-7} \, \text{T}.\)
Therefore:
\(\alpha = 3.\)
The Correct answer is: 3
Let $ f: \mathbb{R} \to \mathbb{R} $ be a twice differentiable function such that $$ f''(x)\sin\left(\frac{x}{2}\right) + f'(2x - 2y) = (\cos x)\sin(y + 2x) + f(2x - 2y) $$ for all $ x, y \in \mathbb{R} $. If $ f(0) = 1 $, then the value of $ 24f^{(4)}\left(\frac{5\pi}{3}\right) $ is: