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Variation of magnetic field with distanc...

Variation of magnetic field with distance from current carrying conductor is:

A

`B prop a^(2)`

B

`B prop (1)/(a^(2))`

C

`B prop a`

D

`B prop (1)/(a)`

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The correct Answer is:
To determine the variation of the magnetic field with distance from a current-carrying conductor, we can use Ampere's Law. The magnetic field (B) around a long straight conductor carrying a current (I) is given by the formula: \[ B = \frac{\mu_0 I}{2 \pi r} \] where: - \( B \) is the magnetic field, - \( \mu_0 \) is the permeability of free space (approximately \( 4\pi \times 10^{-7} \, \text{T m/A} \)), - \( I \) is the current flowing through the conductor, - \( r \) is the distance from the conductor. ### Step-by-Step Solution: 1. **Identify the Formula**: The formula for the magnetic field around a straight current-carrying conductor is \( B = \frac{\mu_0 I}{2 \pi r} \). 2. **Understand the Variables**: In this formula: - \( \mu_0 \) is a constant (permeability of free space), - \( I \) is the current (which is constant for a given conductor), - \( r \) is the distance from the conductor, which varies. 3. **Analyze the Relationship**: From the formula, we can see that the magnetic field \( B \) is inversely proportional to the distance \( r \). This means that as you move further away from the conductor (increasing \( r \)), the magnetic field \( B \) decreases. 4. **Conclusion**: Therefore, the variation of the magnetic field with distance from a current-carrying conductor is such that it decreases as the distance increases, following the relationship \( B \propto \frac{1}{r} \). ### Final Statement: The variation of the magnetic field with distance from a current-carrying conductor is inversely proportional to the distance from the conductor. ---

To determine the variation of the magnetic field with distance from a current-carrying conductor, we can use Ampere's Law. The magnetic field (B) around a long straight conductor carrying a current (I) is given by the formula: \[ B = \frac{\mu_0 I}{2 \pi r} \] where: - \( B \) is the magnetic field, - \( \mu_0 \) is the permeability of free space (approximately \( 4\pi \times 10^{-7} \, \text{T m/A} \)), - \( I \) is the current flowing through the conductor, ...
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