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Question: Two parallel coaxial circular coils of equal radius 'R' and equal number of turns 'N', carry equal c...

Two parallel coaxial circular coils of equal radius 'R' and equal number of turns 'N', carry equal currents 'I' in the same direction and are separated by a distance '2R'. Find the magnitude and direction of the net magnetic field produced at the midpoint of the line joining their centres.

Answer

The magnitude of the net magnetic field is μ0NI24R\frac{\mu_0 N I \sqrt{2}}{4 R}. The direction is along the axis joining the centers, in the direction determined by the common direction of current in the coils.

Explanation

Solution

The problem asks for the magnitude and direction of the net magnetic field at the midpoint of the line joining the centers of two parallel coaxial circular coils.

1. Setup and Parameters:

  • Radius of each coil = RR
  • Number of turns in each coil = NN
  • Current in each coil = II
  • Currents flow in the same direction.
  • Separation between the coils = 2R2R
  • The point of interest is the midpoint of the line joining their centers.

2. Magnetic Field due to a Single Circular Coil on its Axis: The magnetic field (BB) on the axis of a circular coil of radius RR', NN turns, carrying current II at a distance xx from its center is given by: B=μ0NIR22(R2+x2)3/2B = \frac{\mu_0 N I R'^2}{2(R'^2 + x^2)^{3/2}} In our case, R=RR' = R. So, B=μ0NIR22(R2+x2)3/2B = \frac{\mu_0 N I R^2}{2(R^2 + x^2)^{3/2}}

3. Position of the Midpoint: Let the center of the first coil (Coil 1) be at x=0x=0. Since the coils are separated by a distance 2R2R, the center of the second coil (Coil 2) will be at x=2Rx=2R. The midpoint of the line joining their centers will be at x=0+2R2=Rx = \frac{0 + 2R}{2} = R.

4. Magnetic Field due to Coil 1 at the Midpoint: For Coil 1, the distance from its center (x=0x=0) to the midpoint (x=Rx=R) is x1=Rx_1 = R. The magnetic field B1B_1 due to Coil 1 at the midpoint is: B1=μ0NIR22(R2+R2)3/2B_1 = \frac{\mu_0 N I R^2}{2(R^2 + R^2)^{3/2}} B1=μ0NIR22(2R2)3/2B_1 = \frac{\mu_0 N I R^2}{2(2R^2)^{3/2}} B1=μ0NIR22(23/2)(R2)3/2B_1 = \frac{\mu_0 N I R^2}{2 \cdot (2^{3/2}) \cdot (R^2)^{3/2}} B1=μ0NIR22(22)R3B_1 = \frac{\mu_0 N I R^2}{2 \cdot (2\sqrt{2}) \cdot R^3} B1=μ0NI42RB_1 = \frac{\mu_0 N I}{4\sqrt{2} R}

5. Magnetic Field due to Coil 2 at the Midpoint: For Coil 2, the distance from its center (x=2Rx=2R) to the midpoint (x=Rx=R) is x2=R2R=Rx_2 = |R - 2R| = R. The magnetic field B2B_2 due to Coil 2 at the midpoint is: B2=μ0NIR22(R2+R2)3/2B_2 = \frac{\mu_0 N I R^2}{2(R^2 + R^2)^{3/2}} B2=μ0NI42RB_2 = \frac{\mu_0 N I}{4\sqrt{2} R} (This is the same magnitude as B1B_1 because the distance and coil parameters are identical).

6. Direction of the Magnetic Fields: Since both coils carry current in the same direction, their magnetic fields at the midpoint will also be in the same direction along the axis. For example, if the current in both coils is counter-clockwise when viewed from the right side of the coils, then the magnetic field lines would point from left to right along the axis. Thus, both B1B_1 and B2B_2 will point in the same direction.

7. Net Magnetic Field: Since B1B_1 and B2B_2 are in the same direction, the net magnetic field BnetB_{net} at the midpoint is the sum of their magnitudes: Bnet=B1+B2B_{net} = B_1 + B_2 Bnet=μ0NI42R+μ0NI42RB_{net} = \frac{\mu_0 N I}{4\sqrt{2} R} + \frac{\mu_0 N I}{4\sqrt{2} R} Bnet=2×μ0NI42RB_{net} = 2 \times \frac{\mu_0 N I}{4\sqrt{2} R} Bnet=μ0NI22RB_{net} = \frac{\mu_0 N I}{2\sqrt{2} R}

To rationalize the denominator, multiply the numerator and denominator by 2\sqrt{2}: Bnet=μ0NI2222RB_{net} = \frac{\mu_0 N I \sqrt{2}}{2\sqrt{2} \cdot \sqrt{2} R} Bnet=μ0NI24RB_{net} = \frac{\mu_0 N I \sqrt{2}}{4 R}

Magnitude and Direction: The magnitude of the net magnetic field is μ0NI24R\frac{\mu_0 N I \sqrt{2}}{4 R}. The direction of the net magnetic field is along the axis joining the centers of the coils, in the direction determined by the common direction of current in the coils (e.g., if currents are counter-clockwise when viewed from one side, the field points away from that side).