Calculating the Magnetic Field Due to a Current — Question 5

Section 29-1 · Physics pages 4660–4661

Question 5 Perpendicular wires produce a vector field that cannot be added as scalars One infinite wire lies along x with current I toward +x; a second lies along y with the same current toward +y. They cross without electrical contact. Consider P = (0, 0, h), with h positive; wire thickness is negligible. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. Iˆx Iyˆy z P perspective sketch Schematic; labels, not drawing lengths, specify the data. (a) Find the total magnetic-field vector and magnitude at P. (b) Choose the magnitude and direction of the y-wire current that makes the total field point along ˆx −2ˆy.
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Question 5 - Solution Perpendicular wires produce a vector field that cannot be added as scalars Iˆx Iyˆy z P perspective sketch (a) Method and calculation⃗ Bx = −µ0I 2πh ˆy,⃗ By = + µ0I 2πh ˆx.⃗ B = µ0I 2πh(ˆx −ˆy), |B| = √ 2µ0I 2πh . (b) Interpretation and further calculation⃗ B = µ0 2πh(Iyˆx −Iˆy) ∥(ˆx −2ˆy). I/Iy = 2 ⇒Iy = I/2 toward + y . Physical check The two fields are perpendicular at P; equal currents give a magnitude larger than either field by a factor of square root of two.

Question 5

Perpendicular wires produce a vector field that cannot be added as scalars

One infinite wire lies along x with current I toward +x; a second lies along y with the same current toward +y. They cross without electrical contact. Consider P=(0,0,h)P=(0,0,h), with h positive; wire thickness is negligible. 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 the total magnetic-field vector and magnitude at P.

  2. Choose the magnitude and direction of the y-wire current that makes the total field point along x̂−2ŷ\hat x-2\hat y.

Question 5 - Solution

Perpendicular wires produce a vector field that cannot be added as scalars

Diagram shown in the original SVG worksheet.

(a) Method and calculation

B→x=−μ0I2πhŷ,B→y=+μ0I2πhx̂.\vec B_x=-\frac{\mu_0 I}{2\pi h}\hat y,\quad\vec B_y=+\frac{\mu_0 I}{2\pi h}\hat x.B→=μ0I2πh(x̂−ŷ),|B|=2μ0I2πh.\vec B=\frac{\mu_0 I}{2\pi h}(\hat x-\hat y),\quad|B|=\boxed{\frac{\sqrt2\mu_0 I}{2\pi h}}.

(b) Interpretation and further calculation

B→=μ02πh(Iyx̂−Iŷ)∥(x̂−2ŷ).\vec B=\frac{\mu_0}{2\pi h}(I_y\hat x-I\hat y)\parallel(\hat x-2\hat y).I/Iy=2⇒Iy=I/2 toward +y.I/I_y=2\Rightarrow\boxed{I_y=I/2\text{ toward }+y}.

Physical check

The two fields are perpendicular at P; equal currents give a magnitude larger than either field by a factor of square root of two.