
Application of Biot-Savart and Ampere's Laws
- The magnetic field at the center \( O \) of the circular loop is calculated as: \[ B_{\text{loop}} = \frac{\mu_0 I_{\text{loop}}}{2R} \]. Given \( I_{\text{loop}} = 1.0 A \) and \( R = 10 \) cm (0.1 m), the calculation is: \[ B_{\text{loop}} = \frac{(4\pi \times 10^{-7}) (1)}{2 \times 0.1} \] which results in \[ B_{\text{loop}} = 2 \times 10^{-6} \text{ T} \].
- The magnetic field generated by a long straight wire at a distance \( d = 20 \) cm is given by: \[ B_{\text{wire}} = \frac{\mu_0 I_{\text{wire}}}{2\pi d} \]. Substituting the values: \[ B_{\text{wire}} = \frac{(4\pi \times 10^{-7}) I_{\text{wire}}}{2\pi \times 0.2} \]. This simplifies to: \[ B_{\text{wire}} = \frac{2 \times 10^{-7} I_{\text{wire}}}{0.2} \] and further to \[ B_{\text{wire}} = 10^{-6} I_{\text{wire}} \].
- For the net magnetic field at \( O \) to be zero, the magnitudes of the magnetic fields must be equal: \[ B_{\text{loop}} = B_{\text{wire}} \]. Therefore, \[ 2 \times 10^{-6} = 10^{-6} I_{\text{wire}} \], yielding \( I_{\text{wire}} = 2 A \). Direction of Current in the Wire:
- Applying the Right-Hand Rule, the magnetic field from the circular loop at point \( O \) is directed into the plane.
- To achieve a net magnetic field of zero, the wire must produce a magnetic field directed out of the plane at \( O \).
- This requires the current in the wire to flow in the negative x-direction.
Consequently, the wire requires a current of 2 A, directed along the negative x-axis.