A long straight wire of radius a carries a steady current I. The current is uniformly distributed across its cross section. The ratio of the magnetic field at $\frac{a}{2}$ and $2 a$ from axis of the wire is :
Solution
<p>To find the ratio of the magnetic field at $\frac{a}{2}$ and $2a$ distances from the axis of a long straight wire, we use Ampère's Law, which relates the magnetic field around a current-carrying conductor to the current enclosed by it.</p>
<p>Ampère’s Law is given by:</p>
<p>$\oint \vec{B} \cdot d\vec{l} = \mu_0 I_{\text{enc}}$</p>
<p>where:</p>
<p>$\vec{B}$ is the magnetic field,</p>
<p>$\mu_0$ is the permeability of free space,</p>
<p>$I_{\text{enc}}$ is the enclosed current.</p>
<p>For a point inside the wire (at radius $r=a/2$):</p>
<p>The current enclosed by a radius $r$ is proportional to the area of the cross-section at radius $r$.</p>
<p>The area of the cross-section at radius $r$ is given by:</p>
<p>$\pi \left( \frac{a}{2} \right)^2 = \frac{\pi a^2}{4}$</p>
<p>The total current $I$ is uniformly distributed, thus the current enclosed $I_{\text{enc}}$ at radius $r = \frac{a}{2}$ is:</p>
<p>$$I_{\text{enc}} = I \times \frac{\text{Area enclosed}}{\text{Total area}} = I \times \frac{\frac{\pi a^2}{4}}{\pi a^2} = \frac{I}{4}$$</p>
<p>Applying Ampère’s Law inside the conductor, we get:</p>
<p>$B \cdot 2 \pi \left( \frac{a}{2} \right) = \mu_0 \left( \frac{I}{4} \right)$</p>
<p>So,</p>
<p>$B \cdot \pi a = \frac{\mu_0 I}{4}$</p>
<p>Therefore, the magnetic field inside the wire at $r = \frac{a}{2}$ is:</p>
<p>$B_{\frac{a}{2}} = \frac{\mu_0 I}{4 \pi a}$</p>
<p>For a point outside the wire (at radius $r = 2a$):</p>
<p>The total current enclosed by a radius $r = 2a$ is the entire current $I$.</p>
<p>Applying Ampère’s Law outside the conductor, we get:</p>
<p>$B \cdot 2 \pi (2a) = \mu_0 I$</p>
<p>So,</p>
<p>$B \cdot 4 \pi a = \mu_0 I$</p>
<p>Therefore, the magnetic field outside the wire at $r = 2a$ is:</p>
<p>$B_{2a} = \frac{\mu_0 I}{4 \pi a}$</p>
<p>Hence, the ratio of the magnetic field at $\frac{a}{2}$ and $2a$ is:</p>
<p>$$\frac{B_{\frac{a}{2}}}{B_{2a}} = \frac{\frac{\mu_0 I}{4 \pi a}}{\frac{\mu_0 I}{4 \pi a}} = 1:1$$</p>
<p>So, the correct option is:</p>
<p>Option C: $1:1$</p>
About this question
Subject: Physics · Chapter: Magnetic Effects of Current · Topic: Biot-Savart Law
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