Ampère's Law — Question 1

Section 29-3 · Physics pages 4692–4693

Question 1 Signed circulation counts enclosed currents rather than nearby currents A closed path is traversed counterclockwise as viewed from +z. Its spanning surface is pierced by 4.00 A and 1.50 A toward +z and 3.00 A toward -z. A further 20.0 A wire passes outside the path. All currents are steady. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. 4 A 1.5 A 3 A 20 A Schematic; labels, not drawing lengths, specify the data. (a) Calculate the circulation of B around the path. (b) Find the circulation for the reversed traversal, and explain whether the outside wire can change B on the path.
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Question 1 - Solution Signed circulation counts enclosed currents rather than nearby currents 4 A 1.5 A 3 A 20 A (a) Method and calculation I C⃗ B · d⃗ℓ= µ0Ienc, Ienc = 4.00 + 1.50 −3.00 = 2.50 A. I C⃗ B · d⃗ℓ= π × 10−6 T m . (b) Interpretation and further calculation d⃗ℓ→−d⃗ℓ⇒ I −C⃗ B · d⃗ℓ= −π × 10−6 T m . I C⃗ Boutside · d⃗ℓ= 0 although⃗Boutside̸ = 0 locally. Physical check Ampère circulation is a signed sum through the surface; it is not a sum of field magnitudes around the boundary.

Question 1

Signed circulation counts enclosed currents rather than nearby currents

A closed path is traversed counterclockwise as viewed from +z. Its spanning surface is pierced by 4.00 A and 1.50 A toward +z and 3.00 A toward -z. A further 20.0 A wire passes outside the path. All currents are steady. 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. Calculate the circulation of B around the path.

  2. Find the circulation for the reversed traversal, and explain whether the outside wire can change B on the path.

Question 1 - Solution

Signed circulation counts enclosed currents rather than nearby currents

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∮CB→⋅dℓ→=μ0Ienc,Ienc=4.00+1.50−3.00=2.50A.\oint_C\vec B\cdot d\vec\ell=\mu_0I_{\mathrm{enc}},\quad I_{\mathrm{enc}}=4.00+1.50-3.00=2.50\,\mathrm A.∮CB→⋅dℓ→=π×10−6Tm.\boxed{\oint_C\vec B\cdot d\vec\ell=\pi\times10^{-6}\,\mathrm{T\,m}}.

(b) Interpretation and further calculation

dℓ→→−dℓ→⇒∮−CB→⋅dℓ→=−π×10−6Tm.d\vec\ell\to-d\vec\ell\Rightarrow\boxed{\oint_{-C}\vec B\cdot d\vec\ell=-\pi\times10^{-6}\,\mathrm{T\,m}}.∮CB→outside⋅dℓ→=0although B→outside≠0 locally.\oint_C\vec B_{\mathrm{outside}}\cdot d\vec\ell=0\quad\text{although }\vec B_{\mathrm{outside}}\ne0\text{ locally}.

Physical check

Ampère circulation is a signed sum through the surface; it is not a sum of field magnitudes around the boundary.