A 2.0 cm segment of wire, carrying 5.0 A current in positive y-direction lies along the y-axis, as shown in the figure. The magnetic field at a point (3 m, 4 m, 0) due to this segment (part of a circuit) is:
Step 1: Application of the Biot-Savart Law.
The Biot-Savart Law defines the magnetic field generated by a segment of current-carrying wire: \[ dB = \frac{\mu_0}{4\pi} \frac{I \, dl \times \hat{r}}{r^2} \] where:
Step 2: Calculation of \( r \) and \( \hat{r} \).
The distance \( r \) and the unit vector \( \hat{r} \) from the wire segment to the observation point (3 m, 4 m, 0) are calculated as follows: \[ r = \sqrt{3^2 + 4^2} = 5 \, \text{m} \] \[ \hat{r} = \left(\frac{3}{5}, \frac{4}{5}, 0\right) \]
Step 3: Calculation of \( dl \times \hat{r} \) and \( dB \).
The cross product \( dl \times \hat{r} \) is computed using the right-hand rule: \[ dl \times \hat{r} = 0.02 \, \hat{j} \times \left(\frac{3}{5}, \frac{4}{5}, 0\right) = 0.02 \left( 0, 0, -\frac{3}{5} \right) = \left( 0, 0, -0.012 \right) \, \hat{k} \] This indicates that \( dB \) is directed along the negative \( \hat{k} \) axis. The magnitude of \( dB \) is determined to be: \[ dB = \frac{4\pi \times 10^{-7}}{4\pi} \cdot \frac{5 \cdot 0.012}{25} = \frac{10^{-7} \cdot 0.06}{25} = 2.4 \times 10^{-9} \, \text{T} = 0.24 \, \text{nT} \] Considering the direction, the magnetic field is: \[ -0.24 \, \text{nT} \, \hat{k} \] This result corresponds to option (C).