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3 - N u m e r i c a l   1 0

Problem

Two parallel wires, 10 cm apart, carry currents of 8 A8 \, \mathrm{A} each in opposite directions. What is the magnetic field halfway between them?


Data

  • Current in the first wire: I1=8 AI_1 = 8 \, \mathrm{A},
  • Current in the second wire: I2=8 AI_2 = 8 \, \mathrm{A},
  • Distance halfway between the wires: r=5 cm=5Γ—10βˆ’2 mr = 5 \, \mathrm{cm} = 5 \times 10^{-2} \, \mathrm{m},
  • Permeability of free space: ΞΌ0=4π×10βˆ’7 Wbβ‹…Aβˆ’1β‹…mβˆ’1\mu_0 = 4 \pi \times 10^{-7} \, \mathrm{Wb \cdot A^{-1} \cdot m^{-1}}.

To find:

  • Net magnetic field halfway: Bnet=?B_{\text{net}} = ?.

Prerequisite Concepts

The magnetic field generated by a long straight current-carrying wire at a distance rr is given by:

B=ΞΌ02Ο€β‹…IrB = \frac{\mu_0}{2 \pi} \cdot \frac{I}{r}

Since the currents in the wires are in opposite directions, the magnetic fields generated by each wire will add up midway between them:

Bnet=B1+B2=ΞΌ02Ο€β‹…I1r+ΞΌ02Ο€β‹…I2rB_{\text{net}} = B_1 + B_2 = \frac{\mu_0}{2 \pi} \cdot \frac{I_1}{r} + \frac{\mu_0}{2 \pi} \cdot \frac{I_2}{r}

Simplify:

Bnet=ΞΌ02Ο€rβ‹…(I1+I2)B_{\text{net}} = \frac{\mu_0}{2 \pi r} \cdot (I_1 + I_2)

Solution

  1. Substitute the known values into the formula:
Bnet=4π×10βˆ’72Ο€β‹…5Γ—10βˆ’2β‹…(8+8) B_{\text{net}} = \frac{4 \pi \times 10^{-7}}{2 \pi \cdot 5 \times 10^{-2}} \cdot (8 + 8)
  1. Simplify the denominator:
2Ο€β‹…5Γ—10βˆ’2=Ο€β‹…10βˆ’1. 2 \pi \cdot 5 \times 10^{-2} = \pi \cdot 10^{-1}.
  1. Simplify the numerator:
4π×10βˆ’7Ο€β‹…10βˆ’1=4Γ—10βˆ’710βˆ’1=4Γ—10βˆ’6. \frac{4 \pi \times 10^{-7}}{\pi \cdot 10^{-1}} = \frac{4 \times 10^{-7}}{10^{-1}} = 4 \times 10^{-6}.
  1. Multiply by the sum of currents:
Bnet=4Γ—10βˆ’6β‹…(8+8)=4Γ—10βˆ’6β‹…16=6.4Γ—10βˆ’5 T. B_{\text{net}} = 4 \times 10^{-6} \cdot (8 + 8) = 4 \times 10^{-6} \cdot 16 = 6.4 \times 10^{-5} \, \mathrm{T}.

Answer

The net magnetic field halfway between the wires is:

Bnet=6.4Γ—10βˆ’5 T.B_{\text{net}} = 6.4 \times 10^{-5} \, \mathrm{T}.