Calculating the Magnetic Field Due to a Current — Question 6

Section 29-1 · Physics pages 4662–4663

Question 6 A specified error tolerance determines how long a wire must be A segment of total length 2L is observed a distance a from its midpoint. Its field is Bf = B∞L/ √ L2 + a2, where B∞= µ0I/(2πa). Define the relative approximation error using the exact finite field: ϵ = (B∞−Bf)/Bf. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. I P a total length 2L Schematic; labels, not drawing lengths, specify the data. (a) Find the minimum L/a for an error no larger than 1.00 percent. (b) Derive the leading error for L much larger than a and compare its predicted threshold.
Show solutionHide solution
Question 6 - Solution A specified error tolerance determines how long a wire must be I P a total length 2L (a) Method and calculation ϵ = √ 1 + (a/L)2 −1 ≤.0100. L/a ≥[(1.0100)2 −1]−1/2 = 7.05346. (b) Interpretation and further calculation √ 1 + u = 1 + u/2 + O(u2) ⇒ϵ ≃a2/(2L2). ϵ ≤.0100 ⇒L/a ≳ √ 50 = 7.07107. Physical check The definition of relative error matters; normalizing by the infinite-wire estimate gives a slightly different exact threshold.

Question 6

A specified error tolerance determines how long a wire must be

A segment of total length 2L is observed a distance a from its midpoint. Its field is Bf=B∞L/L2+a2B_f=B_\infty L/\sqrt{L^2+a^2}, where B∞=μ0I/(2πa)B_\infty=\mu_0I/(2\pi a). Define the relative approximation error using the exact finite field: ϵ=(B∞−Bf)/Bf\epsilon=(B_\infty-B_f)/B_f. 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 minimum L/a for an error no larger than 1.00 percent.

  2. Derive the leading error for L much larger than a and compare its predicted threshold.

Question 6 - Solution

A specified error tolerance determines how long a wire must be

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ϵ=1+(a/L)2−1≤.0100.\epsilon=\sqrt{1+(a/L)^2}-1\le.0100.L/a≥[(1.0100)2−1]−1/2=7.05346.\boxed{L/a\ge[(1.0100)^2-1]^{-1/2}}=7.05346.

(b) Interpretation and further calculation

1+u=1+u/2+O(u2)⇒ϵ≃a2/(2L2).\sqrt{1+u}=1+u/2+O(u^2)\Rightarrow\epsilon\simeq a^2/(2L^2).ϵ≤.0100⇒L/a≳50=7.07107.\epsilon\le.0100\Rightarrow L/a\gtrsim\sqrt{50}=7.07107.

Physical check

The definition of relative error matters; normalizing by the infinite-wire estimate gives a slightly different exact threshold.