Step 1: Magnetic field due to a long current-carrying wire
The magnetic field at a distance \( r \) from a long, straight current-carrying wire is given by:
\[
B = \frac{\mu_0 I}{2 \pi r}
\]
where:
- \( \mu_0 = 4\pi \times 10^{-7} \) Tm/A is the permeability of free space,
- \( I \) is the current in the wire,
- \( r \) is the perpendicular distance from the wire.
Step 2: Compute the magnetic fields due to both wires
Let wire A carry \( I_A = 2 \) A and wire B carry \( I_B = 6 \) A. The separation between the wires is \( 5 \) m. The point of interest is \( 2 \) m from wire A.
The magnetic field due to wire A at this point is:
\[
B_A = \frac{(4\pi \times 10^{-7}) \times 2}{2\pi \times 2}
\]
\[
= \frac{8\pi \times 10^{-7}}{4\pi}
\]
\[
= 2 \times 10^{-7} \text{ T}
\]
The distance of the point from wire B is:
\[
r_B = 5 - 2 = 3 \text{ m}
\]
The magnetic field due to wire B at this point is:
\[
B_B = \frac{(4\pi \times 10^{-7}) \times 6}{2\pi \times 3}
\]
\[
= \frac{24\pi \times 10^{-7}}{6\pi}
\]
\[
= 4 \times 10^{-7} \text{ T}
\]
Step 3: Determine the net magnetic field
Since both currents are in the same direction, their magnetic fields at the given point will oppose each other (by the right-hand rule).
The resultant magnetic field is:
\[
B_{\text{net}} = B_B - B_A
\]
\[
= (4 \times 10^{-7} - 2 \times 10^{-7}) \text{ T}
\]
\[
= 2 \times 10^{-7} \text{ T}
\]
Thus, the resultant magnetic field at the given point is \( 2 \times 10^{-7} \) T.
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