Solenoids and Toroids — Question 2

Section 29-4 · Physics pages 4714–4715

Question 2 Integrating circular turns gives different finite-solenoid fields at the center and end A thin solenoid of radius R and length ell is centered at z=0, with uniform turn density n and current I. Each turn contributes dB = µ0nIR2 dz′/[2(R2 + (z −z′)2)3/2] along +z. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. z ℓ N turns, current I −ℓ/2 +ℓ/2 Schematic; labels, not drawing lengths, specify the data. (a) Integrate to obtain the on-axis field B(z). (b) Find the center and end fields for ell=4R, expressed as multiples of µ0nI, and find their ratio.
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Question 2 - Solution Integrating circular turns gives different finite-solenoid fields at the center and end z ℓ N turns, current I −ℓ/2 +ℓ/2 (a) Method and calculation ∫ R2 du (R2 + u2)3/2 = u √ R2 + u2 , u = z −z′. B(z) = µ0nI 2 [ z + ℓ/2 √ R2 + (z + ℓ/2)2 − z −ℓ/2 √ R2 + (z −ℓ/2)2 ] . (b) Interpretation and further calculation B(0) = µ0nI ℓ/2 √ R2 + ℓ2/4 = 2 √ 5µ0nI. B(ℓ/2) = 2 √ 17µ0nI, Bend/Bcenter = √ 5/17 = .542326 . Physical check Only in the very long limit is the end field one-half of the center field; finite geometry changes both values.

Question 2

Integrating circular turns gives different finite-solenoid fields at the center and end

A thin solenoid of radius R and length ell is centered at z=0, with uniform turn density n and current I. Each turn contributes dB=μ0nIR2dz′/[2(R2+(z−z′)2)3/2]dB=\mu_0nIR^2\,dz\prime/[2(R^2+(z-z\prime)^2)^{3/2}] along +z. 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. Integrate to obtain the on-axis field B(z).

  2. Find the center and end fields for ell=4R, expressed as multiples of μ0nI\mu_0nI, and find their ratio.

Question 2 - Solution

Integrating circular turns gives different finite-solenoid fields at the center and end

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∫R2du(R2+u2)3/2=uR2+u2,u=z−z′.\int\frac{R^2\,du}{(R^2+u^2)^{3/2}}=\frac{u}{\sqrt{R^2+u^2}},\quad u=z-z\prime.B(z)=μ0nI2[z+ℓ/2R2+(z+ℓ/2)2−z−ℓ/2R2+(z−ℓ/2)2].\boxed{B(z)=\frac{\mu_0nI}{2}\left[\frac{z+\ell/2}{\sqrt{R^2+(z+\ell/2)^2}}-\frac{z-\ell/2}{\sqrt{R^2+(z-\ell/2)^2}}\right]}.

(b) Interpretation and further calculation

B(0)=μ0nIℓ/2R2+ℓ2/4=25μ0nI.B(0)=\mu_0nI\frac{\ell/2}{\sqrt{R^2+\ell^2/4}}=\frac2{\sqrt5}\mu_0nI.B(ℓ/2)=217μ0nI,Bend/Bcenter=5/17=.542326.B(\ell/2)=\frac2{\sqrt{17}}\mu_0nI,\quad\boxed{B_{\mathrm{end}}/B_{\mathrm{center}}=\sqrt{5/17}=.542326}.

Physical check

Only in the very long limit is the end field one-half of the center field; finite geometry changes both values.