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Consider an infinitely long current carr...

Consider an infinitely long current carrying cylindrical straight wire having radius 'a'. Then the ratio of magnetic field at distance `a/3` and 2a from axis of wire is.

A

`2//3`

B

`1//2`

C

`3//2`

D

2

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To solve the problem of finding the ratio of the magnetic field at distances \( \frac{a}{3} \) and \( 2a \) from the axis of an infinitely long current-carrying cylindrical wire, we can follow these steps: ### Step 1: Understand the Magnetic Field Inside and Outside the Wire For a long straight wire carrying current \( I \): - Inside the wire (for \( r < a \)), the magnetic field \( B \) is given by: \[ B = \frac{\mu_0 I}{2\pi a^2} r \] where \( r \) is the distance from the center of the wire. - Outside the wire (for \( r \geq a \)), the magnetic field \( B \) is given by: \[ B = \frac{\mu_0 I}{2\pi r} \] ### Step 2: Calculate the Magnetic Field at \( r = \frac{a}{3} \) Since \( \frac{a}{3} < a \), we use the formula for the magnetic field inside the wire: \[ B_1 = \frac{\mu_0 I}{2\pi a^2} \left(\frac{a}{3}\right) = \frac{\mu_0 I}{2\pi a^2} \cdot \frac{a}{3} = \frac{\mu_0 I}{6\pi a} \] ### Step 3: Calculate the Magnetic Field at \( r = 2a \) Since \( 2a > a \), we use the formula for the magnetic field outside the wire: \[ B_2 = \frac{\mu_0 I}{2\pi (2a)} = \frac{\mu_0 I}{4\pi a} \] ### Step 4: Find the Ratio of the Magnetic Fields Now, we can find the ratio of \( B_1 \) to \( B_2 \): \[ \text{Ratio} = \frac{B_1}{B_2} = \frac{\frac{\mu_0 I}{6\pi a}}{\frac{\mu_0 I}{4\pi a}} = \frac{1/6}{1/4} = \frac{4}{6} = \frac{2}{3} \] ### Final Answer Thus, the ratio of the magnetic field at a distance \( \frac{a}{3} \) from the axis of the wire to the magnetic field at a distance \( 2a \) is: \[ \frac{B_1}{B_2} = \frac{2}{3} \]
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