A long straight wire of a circular cross-section of radius 'a' is carrying steady current I. The current I is uniformly distributed across this cross-section. What will be the magnetic field in the region $r < a$ and $r > a$? |
$B∝r (r< a)$ and $B ∝ r^{-1} (r > a)$ $B∝r (r> a)$ and $B ∝ r^{-1} (r < a)$ $B=0(r< a)$ and $B ∝ r^{-1} (r > a)$ $B∝r (r< a)$ and $B =0 (r > a)$ |
$B∝r (r< a)$ and $B ∝ r^{-1} (r > a)$ |
The correct answer is Option (1) → $B∝r (r< a)$ and $B ∝ r^{-1} (r > a)$ Given: Long straight wire of radius $a$, carrying steady current $I$, uniformly distributed. Using Ampère’s circuital law: $\oint \mathbf{B} \cdot d\mathbf{l} = μ_0 I_{enc}$ Case 1: For r < a (inside the wire) Current enclosed, $I_{enc} = I \cdot \frac{πr^2}{πa^2} = I \cdot \frac{r^2}{a^2}$ $B(2πr) = μ_0 I_{enc}$ $B = \frac{μ_0 I r}{2π a^2}$ Magnetic field inside the wire: $B = \frac{μ_0 I r}{2π a^2}$ Case 2: For r > a (outside the wire) Current enclosed, $I_{enc} = I$ $B(2πr) = μ_0 I$ $B = \frac{μ_0 I}{2π r}$ Magnetic field outside the wire: $B = \frac{μ_0 I}{2π r}$ Final Answer: For $r < a$: $B = \frac{μ_0 I r}{2π a^2}$ For $r > a$: $B = \frac{μ_0 I}{2π r}$ |