Applying Biot-Savart Law and Ampere’s Law
- The magnetic field at the center \( O \) of the circular loop is given by: \[ B_{\text{loop}} = \frac{\mu_0 I_{\text{loop}}}{2R} \] where \( I_{\text{loop}} = 1.0 A \), \( R = 10 \) cm = 0.1 m.
\[ B_{\text{loop}} = \frac{(4\pi \times 10^{-7}) (1)}{2 \times 0.1} \] \[ B_{\text{loop}} = 2 \times 10^{-6} \text{ T} \] - The magnetic field due to the long straight wire at distance \( d = 20 \) cm is: \[ B_{\text{wire}} = \frac{\mu_0 I_{\text{wire}}}{2\pi d} \] \[ B_{\text{wire}} = \frac{(4\pi \times 10^{-7}) I_{\text{wire}}}{2\pi \times 0.2} \] \[ B_{\text{wire}} = \frac{2 \times 10^{-7} I_{\text{wire}}}{0.2} \] \[ B_{\text{wire}} = 10^{-6} I_{\text{wire}} \] - For net magnetic field at \( O \) to be zero: \[ B_{\text{loop}} = B_{\text{wire}} \] \[ 2 \times 10^{-6} = 10^{-6} I_{\text{wire}} \] \[ I_{\text{wire}} = 2 A \] Direction of Current in the Wire:
- Using the Right-Hand Rule, the circular loop produces a magnetic field into the plane at O.
- To cancel it, the wire must produce a magnetic field out of the plane at O.
- This happens when current in the wire flows in the negative x-direction.
Thus, the required current in the wire is 2 A, flowing in the negative x-direction.
A current-carrying coil is placed in an external uniform magnetic field. The coil is free to turn in the magnetic field. What is the net force acting on the coil? Obtain the orientation of the coil in stable equilibrium. Show that in this orientation the flux of the total field (field produced by the loop + external field) through the coil is maximum.