Calculating the Magnetic Field Due to a Current — Question 2

Section 29-1 · Physics pages 4654–4655

Question 2 Oppositely traversed arcs form an annular sector with a nonzero central field A closed wire follows an inner circular arc of radius a counterclockwise through angle phi, a radial connector, an outer arc of radius b clockwise through the same angle, and a second radial connector. Here b > a; all paths lie in the xy plane. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. P a b ϕ Schematic; labels, not drawing lengths, specify the data. (a) Derive the field at the common center, including the radial segments. (b) Find its magnitude and direction for a=.0400 m, b=.100 m, phi=120 degrees and I=2.00 A.
Show solutionHide solution
Question 2 - Solution Oppositely traversed arcs form an annular sector with a nonzero central field P a b ϕ (a) Method and calculation d⃗ℓ∥⃗r ⇒⃗Bradial = 0, Barc = µ0I 4πR ∫ϕ 0 dθ.⃗ B = µ0Iϕ 4π (1 a −1 b ) ˆz . (b) Interpretation and further calculation ϕ = 2π/3, a−1 −b−1 = 25 −10 = 15 m−1.⃗ B = 2π µT ˆz ≃6.28319 µT ˆz. Physical check The smaller-radius arc dominates because each arc field scales as inverse radius; the field vanishes when the radii coincide.

Question 2

Oppositely traversed arcs form an annular sector with a nonzero central field

A closed wire follows an inner circular arc of radius a counterclockwise through angle phi, a radial connector, an outer arc of radius b clockwise through the same angle, and a second radial connector. Here b>ab>a; all paths lie in the xy plane. 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. Derive the field at the common center, including the radial segments.

  2. Find its magnitude and direction for a=.0400 m, b=.100 m, phi=120 degrees and I=2.00 A.

Question 2 - Solution

Oppositely traversed arcs form an annular sector with a nonzero central field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dℓ→∥r→⇒B→radial=0,Barc=μ0I4πR∫0ϕdθ.d\vec\ell\parallel\vec r\Rightarrow\vec B_{\mathrm{radial}}=0,\quad B_{\mathrm{arc}}=\frac{\mu_0 I}{4\pi R}\int_0^\phi d\theta.B→=μ0Iϕ4π(1a−1b)ẑ.\vec B=\boxed{\frac{\mu_0 I\phi}{4\pi}\left(\frac1a-\frac1b\right)\hat z}.

(b) Interpretation and further calculation

ϕ=2π/3,a−1−b−1=25−10=15m−1.\phi=2\pi/3,\quad a^{-1}-b^{-1}=25-10=15\,\mathrm{m^{-1}}.B→=2πμTẑ≃6.28319μTẑ.\vec B=\boxed{2\pi\,\mu\mathrm T\,\hat z}\simeq6.28319\,\mu\mathrm T\,\hat z.

Physical check

The smaller-radius arc dominates because each arc field scales as inverse radius; the field vanishes when the radii coincide.