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Question: A long straight wire of radius a carries a steady current I. The current is uniformly distributed ov...

A long straight wire of radius a carries a steady current I. The current is uniformly distributed over its cross section. The ratio of the magnetic fields B and B’, at radial distances a2\dfrac{a}{2} and 2a respectively, from the axis of the wire is:
A. 14\dfrac{1}{4}
B.12\dfrac{1}{2}
C. 1
D. 4

Explanation

Solution

As a first step, you could make a rough diagram to understand the given situation. Then you could recall the standard expressions for both the given cases, that is, for the magnetic fields inside and outside respectively. You could then accordingly substitute and take the ratio to find the answer.

Formula used:
Magnetic field:
Inside the wire,
B=μ0Ir2πR2B=\dfrac{{{\mu }_{0}}Ir}{2\pi {{R}^{2}}}
Outside,
B=μ0I2πrB'=\dfrac{{{\mu }_{0}}I}{2\pi r}

Complete Step by step solution:
In the question, we are given a long straight wire of radius a carrying the current I. we are also said that the current is uniformly distributed over the entire cross section. We are asked to find the ratio magnetic field at radial distances a2\dfrac{a}{2} and 2a.

Let B be the magnetic field at radial distance a2\dfrac{a}{2} which would be inside the wire and B’ be the magnetic field at radial distance 2a which would be outside of the wire.

We know that magnetic field at a distance rRr\langle R from the centre of a wire of radius R is given by,
B=μ0Ir2πR2B=\dfrac{{{\mu }_{0}}Ir}{2\pi {{R}^{2}}}
Substituting the given values, we get,
B=μ0I(a2)2πa2B=\dfrac{{{\mu }_{0}}I\left( \dfrac{a}{2} \right)}{2\pi {{a}^{2}}}
B=μ0I4πa\therefore B=\dfrac{{{\mu }_{0}}I}{4\pi a} ………………………………………………….. (1)

Now for the second part let us recall the expression for magnetic field at distance rRr\rangle R outside the wire of radius R will be,
B=μ0I2πrB'=\dfrac{{{\mu }_{0}}I}{2\pi r}

Substituting the given values,
B=μ0I2π(2a)=μ0I4πaB'=\dfrac{{{\mu }_{0}}I}{2\pi \left( 2a \right)}=\dfrac{{{\mu }_{0}}I}{4\pi a}……………………………………………………. (2)

Now, we could take the ratio of (1) and (2) to get,
BB=(μ0I4πa)(μ0I4πa)=1\dfrac{B}{B'}=\dfrac{\left( \dfrac{{{\mu }_{0}}I}{4\pi a} \right)}{\left( \dfrac{{{\mu }_{0}}I}{4\pi a} \right)}=1

Therefore, we found the ratio of magnetic fields at the given distances to be 1.

Hence, option C is found to be the correct answer.

Note:
You may have noticed that we have substituted the values in the respective standard equations for each case. You could easily derive them by using Ampere’s circuital law if you wish. Though by hearting formulae shouldn’t be promoted, if you could remember them, then it would save you time in competitive exams.