Calculating the Magnetic Field Due to a Current — Question 4

Section 29-1 · Physics pages 4658–4659

Question 4 A field null between unequal parallel currents locates their current ratio Two infinitely long wires parallel to +z cross the xy plane at x=0 and x=d. Their positive currents are I1 and I2. A field null is measured at x=alpha d on the segment between them, with 0 < α < 1. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. I1 I2 d x Schematic; labels, not drawing lengths, specify the data. (a) Find I2/I1 and identify the directions of the two fields at the null. (b) If alpha=.300 and I1=1.50 A, find I2. Locate the null if I2 alone is reversed.
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Question 4 - Solution A field null between unequal parallel currents locates their current ratio I1 I2 d x (a) Method and calculation⃗ B1 = µ0I1 2πx ˆy,⃗ B2 = − µ0I2 2π(d −x) ˆy. I1 αd = I2 (1 −α)d ⇒I2/I1 = (1 −α)/α . (b) Interpretation and further calculation I2 = 1.50(0.700/0.300) = 3.50 A . I1 x − I2 x −d = 0 ⇒x = I1d I1 −I2 = −.750d . After reversal, the null lies outside, on the side of the weaker current. Physical check Between opposite currents the fields reinforce, so the null cannot remain between the wires.

Question 4

A field null between unequal parallel currents locates their current ratio

Two infinitely long wires parallel to +z cross the xy plane at x=0 and x=d. Their positive currents are I1 and I2. A field null is measured at x=alpha d on the segment between them, with 0<α<10<\alpha<1. Use vacuum permeability μ0≃4π×10−7Tm/A\mu_0\simeq4\pi\times10^{-7}\,\mathrm{T\,m/A} where numerical values are needed.

Diagram shown in the original SVG worksheet.

  1. Find I2/I1 and identify the directions of the two fields at the null.

  2. If alpha=.300 and I1=1.50 A, find I2. Locate the null if I2 alone is reversed.

Question 4 - Solution

A field null between unequal parallel currents locates their current ratio

Diagram shown in the original SVG worksheet.

(a) Method and calculation

B→1=μ0I12πxŷ,B→2=−μ0I22π(d−x)ŷ.\vec B_1=\frac{\mu_0 I_1}{2\pi x}\hat y,\quad\vec B_2=-\frac{\mu_0 I_2}{2\pi(d-x)}\hat y.I1αd=I2(1−α)d⇒I2/I1=(1−α)/α.\frac{I_1}{\alpha d}=\frac{I_2}{(1-\alpha)d}\Rightarrow\boxed{I_2/I_1=(1-\alpha)/\alpha}.

(b) Interpretation and further calculation

I2=1.50(0.700/0.300)=3.50A.I_2=1.50(0.700/0.300)=\boxed{3.50\,\mathrm A}.I1x−I2x−d=0⇒x=I1dI1−I2=−.750d.\frac{I_1}{x}-\frac{I_2}{x-d}=0\Rightarrow x=\frac{I_1d}{I_1-I_2}=\boxed{-.750d}.After reversal, the null lies outside, on the side of the weaker current.

Physical check

Between opposite currents the fields reinforce, so the null cannot remain between the wires.