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A cylindrical conductor of radius 'R' ca...

A cylindrical conductor of radius `'R'` carries a current `'i'`. The value of magnetic field at a point which is `R//4` distance inside from the surface is `10 T`. Find the value of magnetic field at point which is `4R` distance outside from the surface

A

`4/3 T`

B

`8/3 T`

C

`40/3 T`

D

`80/3 T`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem step by step, we will use the formulas for the magnetic field inside and outside a cylindrical conductor. ### Step 1: Understand the problem We have a cylindrical conductor of radius \( R \) carrying a current \( i \). We need to find the magnetic field at a point that is \( 4R \) distance outside from the surface of the conductor, given that the magnetic field at a point \( \frac{R}{4} \) distance inside from the surface is \( 10 \, T \). ### Step 2: Define the distance for the inside point The distance from the center of the cylinder to the point inside the conductor is: \[ r = R - \frac{R}{4} = \frac{3R}{4} \] ### Step 3: Use the formula for the magnetic field inside the cylindrical conductor The magnetic field \( B \) inside a cylindrical conductor is given by the formula: \[ B_{\text{inside}} = \frac{\mu_0}{4\pi} \cdot \frac{2i r}{R^2} \] Substituting \( r = \frac{3R}{4} \): \[ B_{\text{inside}} = \frac{\mu_0}{4\pi} \cdot \frac{2i \cdot \frac{3R}{4}}{R^2} \] This simplifies to: \[ B_{\text{inside}} = \frac{\mu_0 \cdot 3i}{8\pi R} \] ### Step 4: Set the inside magnetic field equal to the given value We know from the problem that: \[ B_{\text{inside}} = 10 \, T \] Thus, we can set up the equation: \[ \frac{\mu_0 \cdot 3i}{8\pi R} = 10 \] ### Step 5: Use the formula for the magnetic field outside the cylindrical conductor The magnetic field \( B \) outside a cylindrical conductor is given by: \[ B_{\text{outside}} = \frac{\mu_0}{4\pi} \cdot \frac{2i}{r} \] For a point \( 4R \) outside the surface, the distance \( r \) from the center of the cylinder is: \[ r = R + 4R = 5R \] Thus, we can write: \[ B_{\text{outside}} = \frac{\mu_0}{4\pi} \cdot \frac{2i}{5R} \] ### Step 6: Relate the two magnetic fields Now we can relate the two magnetic fields using the equations we derived: \[ \frac{B_{\text{inside}}}{B_{\text{outside}}} = \frac{(R - \frac{R}{4})(R + 4R)}{R^2} \] Substituting the values: \[ \frac{10}{B_{\text{outside}}} = \frac{(\frac{3R}{4})(5R)}{R^2} \] This simplifies to: \[ \frac{10}{B_{\text{outside}}} = \frac{15R}{4R^2} = \frac{15}{4R} \] ### Step 7: Solve for \( B_{\text{outside}} \) Rearranging gives: \[ B_{\text{outside}} = \frac{10 \cdot 4R}{15} = \frac{40R}{15} = \frac{8R}{3} \] ### Step 8: Conclusion Thus, the magnetic field at a point which is \( 4R \) distance outside from the surface of the cylindrical conductor is: \[ B_{\text{outside}} = \frac{8}{3} \, T \]
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