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QJEEM24Ph2065: JEE Main 2024 Physics - Class 12 JEEM24Ph2065 Solution: A long straight wire of radius a carries a steady current I.…

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 a2\frac{a}{2} and 2a2 a from axis of the wire is :

Multiple Choice Options

  • A 4:14: 1
  • B 3:43: 4
  • C 1:11: 1
  • D 1:41: 4

Step-by-Step Verified Solution

To find the ratio of the magnetic field at a2\frac{a}{2} and 2a2a 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.

Ampère’s Law is given by:

∮B⃗⋅dl⃗=μ0Ienc\oint \vec{B} \cdot d\vec{l} = \mu_0 I_{\text{enc}}

where:

B⃗\vec{B} is the magnetic field,

μ0\mu_0 is the permeability of free space,

IencI_{\text{enc}} is the enclosed current.

For a point inside the wire (at radius r=a/2r=a/2 ):

The current enclosed by a radius rr is proportional to the area of the cross-section at radius rr .

The area of the cross-section at radius rr is given by:

π(a2)2=πa24\pi \left( \frac{a}{2} \right)^2 = \frac{\pi a^2}{4}

The total current II is uniformly distributed, thus the current enclosed IencI_{\text{enc}} at radius r=a2r = \frac{a}{2} is:

Ienc=I×Area enclosedTotal area=I×πa24πa2=I4I_{\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}

Applying Ampère’s Law inside the conductor, we get:

B⋅2π(a2)=μ0(I4)B \cdot 2 \pi \left( \frac{a}{2} \right) = \mu_0 \left( \frac{I}{4} \right)

So,

B⋅πa=μ0I4B \cdot \pi a = \frac{\mu_0 I}{4}

Therefore, the magnetic field inside the wire at r=a2r = \frac{a}{2} is:

Ba2=μ0I4πaB_{\frac{a}{2}} = \frac{\mu_0 I}{4 \pi a}

For a point outside the wire (at radius r=2ar = 2a ):

The total current enclosed by a radius r=2ar = 2a is the entire current II .

Applying Ampère’s Law outside the conductor, we get:

B⋅2π(2a)=μ0IB \cdot 2 \pi (2a) = \mu_0 I

So,

B⋅4πa=μ0IB \cdot 4 \pi a = \mu_0 I

Therefore, the magnetic field outside the wire at r=2ar = 2a is:

B2a=μ0I4πaB_{2a} = \frac{\mu_0 I}{4 \pi a}

Hence, the ratio of the magnetic field at a2\frac{a}{2} and 2a2a is:

Ba2B2a=μ0I4πaμ0I4πa=1:1\frac{B_{\frac{a}{2}}}{B_{2a}} = \frac{\frac{\mu_0 I}{4 \pi a}}{\frac{\mu_0 I}{4 \pi a}} = 1:1

So, the correct option is:

Option C: 1:11:1

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