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Consider a long cylindrical wire carryin...

Consider a long cylindrical wire carrying current along the axis of wire. The current distributed non-uniformly on cross section. The magnetic field B inside the wire varies with distance `r` from the axis as `B=kr^(4)` where k is a cosntant. The current density `J` varies with distance `r` as `J=cr^(n)` then the value of `n` is (where c is another constant).

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To solve the problem, we need to find the value of \( n \) in the current density \( J = c r^n \) given that the magnetic field \( B \) inside the wire varies with distance \( r \) from the axis as \( B = k r^4 \). ### Step-by-Step Solution: 1. **Understanding the Magnetic Field**: The magnetic field inside the wire is given by: \[ B = k r^4 \] where \( k \) is a constant. 2. **Applying Ampere's Law**: According to Ampere's Law, for a cylindrical wire, we have: \[ \oint B \cdot dl = \mu_0 I \] where \( I \) is the current enclosed by the loop of radius \( r \). 3. **Calculating the Left Side of Ampere's Law**: The left side can be expressed as: \[ B \cdot 2 \pi r \] Substituting the expression for \( B \): \[ (k r^4) \cdot (2 \pi r) = 2 \pi k r^5 \] 4. **Calculating the Right Side of Ampere's Law**: The current \( I \) can be expressed in terms of the current density \( J \): \[ I = \int_0^r J \, dA \] The differential area \( dA \) in cylindrical coordinates is: \[ dA = 2 \pi r \, dr \] Therefore, we have: \[ I = \int_0^r J \cdot 2 \pi r \, dr = \int_0^r (c r^n) \cdot 2 \pi r \, dr = 2 \pi c \int_0^r r^{n+1} \, dr \] 5. **Integrating the Current Density**: The integral can be computed as: \[ \int_0^r r^{n+1} \, dr = \left[ \frac{r^{n+2}}{n+2} \right]_0^r = \frac{r^{n+2}}{n+2} \] Therefore: \[ I = 2 \pi c \cdot \frac{r^{n+2}}{n+2} \] 6. **Equating Both Sides**: Now we equate the left side and the right side of Ampere's Law: \[ 2 \pi k r^5 = \mu_0 \left( 2 \pi c \cdot \frac{r^{n+2}}{n+2} \right) \] 7. **Canceling Common Terms**: We can cancel \( 2 \pi \) from both sides: \[ k r^5 = \frac{\mu_0 c}{n+2} r^{n+2} \] 8. **Comparing Powers of \( r \)**: Now, we can compare the powers of \( r \): \[ 5 = n + 2 \] Solving for \( n \): \[ n = 5 - 2 = 3 \] ### Final Answer: The value of \( n \) is \( 3 \).

To solve the problem, we need to find the value of \( n \) in the current density \( J = c r^n \) given that the magnetic field \( B \) inside the wire varies with distance \( r \) from the axis as \( B = k r^4 \). ### Step-by-Step Solution: 1. **Understanding the Magnetic Field**: The magnetic field inside the wire is given by: \[ B = k r^4 ...
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