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An element dvecl=dxhati (where dx=1cm) i...

An element `dvecl=dxhati` (where `dx=1cm`) is placed at the origin and carries a large current `i=10A`. What is the magnetic field on the Y-axis at a distance of `0.5m`?

A

`2 xx 10^(-8)hat(k)T`

B

`4 xx 10^(-8)hat(k)T`

C

`-2 xx 10^(-8)hat(k)T`

D

`-4 xx 10^(-8)hat(k)T`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we will use the Biot-Savart Law, which describes the magnetic field generated by a current-carrying conductor. The law states: \[ \vec{B} = \frac{\mu_0}{4\pi} \cdot \frac{I \, d\vec{l} \times \vec{r}}{r^3} \] Where: - \( \mu_0 \) is the permeability of free space (\( \mu_0 = 4\pi \times 10^{-7} \, \text{T m/A} \)). - \( I \) is the current (10 A in this case). - \( d\vec{l} \) is the differential length element (given as \( dx \hat{i} \)). - \( \vec{r} \) is the position vector from the current element to the point where we want to find the magnetic field. - \( r \) is the distance from the current element to the point in question. ### Step-by-Step Solution: 1. **Identify the Parameters:** - The current \( I = 10 \, \text{A} \). - The differential length \( d\vec{l} = dx \hat{i} \) where \( dx = 1 \, \text{cm} = 0.01 \, \text{m} \). - The point where we want to find the magnetic field is at a distance \( r = 0.5 \, \text{m} \) along the y-axis. 2. **Determine the Position Vector \( \vec{r} \):** - The position vector \( \vec{r} \) from the current element at the origin to the point on the y-axis is \( \vec{r} = 0.5 \hat{j} \). 3. **Calculate the Cross Product \( d\vec{l} \times \vec{r} \):** - We have \( d\vec{l} = dx \hat{i} \) and \( \vec{r} = 0.5 \hat{j} \). - The cross product \( d\vec{l} \times \vec{r} = (dx \hat{i}) \times (0.5 \hat{j}) = dx \cdot 0.5 (\hat{i} \times \hat{j}) = 0.5 dx \hat{k} \). 4. **Calculate \( r^3 \):** - The distance \( r = 0.5 \, \text{m} \), thus \( r^3 = (0.5)^3 = 0.125 \, \text{m}^3 \). 5. **Substitute into the Biot-Savart Law:** - Now substituting into the formula: \[ \vec{B} = \frac{\mu_0}{4\pi} \cdot \frac{I \cdot 0.5 \cdot dx \hat{k}}{r^3} \] - Substituting the values: \[ \vec{B} = \frac{4\pi \times 10^{-7}}{4\pi} \cdot \frac{10 \cdot 0.5 \cdot 0.01 \hat{k}}{0.125} \] - This simplifies to: \[ \vec{B} = 10^{-7} \cdot \frac{0.05 \hat{k}}{0.125} \] - Calculating the fraction: \[ \frac{0.05}{0.125} = 0.4 \] - Thus, \[ \vec{B} = 10^{-7} \cdot 0.4 \hat{k} = 4 \times 10^{-8} \hat{k} \, \text{T} \] 6. **Final Result:** - The magnetic field at the point on the y-axis at a distance of 0.5 m is: \[ \vec{B} = 4 \times 10^{-8} \hat{k} \, \text{T} \]

To solve the problem, we will use the Biot-Savart Law, which describes the magnetic field generated by a current-carrying conductor. The law states: \[ \vec{B} = \frac{\mu_0}{4\pi} \cdot \frac{I \, d\vec{l} \times \vec{r}}{r^3} \] Where: - \( \mu_0 \) is the permeability of free space (\( \mu_0 = 4\pi \times 10^{-7} \, \text{T m/A} \)). ...
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