Step 1: Biot-Savart Law.
The Biot-Savart Law gives the magnetic field \(d\vec{B}\) produced at a point due to a small current element \(I d\vec{l}\) as:
\[
d\vec{B} = \frac{\mu_0}{4\pi} \frac{I d\vec{l} \times \hat{r}}{r^2},
\]
where:
- \(\mu_0\) is the permeability of free space (\(\mu_0 = 4\pi \times 10^{-7}\ \mathrm{T \cdot m/A}\)),
- \(I\) is the current,
- \(d\vec{l}\) is the vector length of the current element,
- \(\hat{r}\) is the unit vector from the current element to the point where the magnetic field is calculated,
- \(r\) is the distance from the current element to the point.
Step 2: Magnetic Field Due to a Long Straight Conductor.
For an infinitely long, straight conductor carrying a current \(I\), we can integrate the Biot-Savart law along the length of the conductor.
The magnetic field at a distance \(r\) from the conductor is given by:
\[
B = \frac{\mu_0 I}{2\pi r}.
\]
This expression is derived by integrating the Biot-Savart law for an infinite length conductor. The direction of the magnetic field follows the right-hand rule, meaning the magnetic field circulates around the wire in concentric circles.
Final Answer: The magnetic field produced by an infinitely long current-carrying conductor is given by: \[ B = \frac{\mu_0 I}{2\pi r}, \] where \(r\) is the distance from the wire, and the direction is given by the right-hand rule.
The path of scattered \( \alpha \)-particle is:
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