Crossed Fields: The Hall Effect — Question 6

Section 28-4 · Physics pages 4542–4543

Question 6 Only the field component normal to the Hall strip contributes to its transverse voltage A Hall strip carries current along x. The field of magnitude B lies in the yz plane and makes angle theta with +z. Its measured voltage convention is upper minus lower along y. Assume one carrier type and no transverse conduction. y z⃗ B Bz θ Schematic; labels, not drawing lengths, specify the data. (a) Derive VH(theta) and compare it with the perpendicular-field reading at theta=0. (b) At theta=60.0 degrees, find the density error if the experimenter mistakenly uses the full B in the perpendicular-field formula.
Show solutionHide solution
Question 6 - Solution Only the field component normal to the Hall strip contributes to its transverse voltage y z⃗ B Bz θ (a) Method and calculation⃗ vd ×⃗B = vdByˆz −vdBzˆy, Ey = vdBz. VH(θ) = −IB cos θ nqt = VH(0) cos θ. (b) Interpretation and further calculation ninferred = IB |q|t|VH(θ)| = n | cos θ|. θ = 60.0◦: ninferred = 2n. Physical check The in-plane field can produce a thickness-direction Hall field, but it does not replace Bz in the specified transverse voltage.

Question 6

Only the field component normal to the Hall strip contributes to its transverse voltage

A Hall strip carries current along x. The field of magnitude B lies in the yz plane and makes angle theta with +z. Its measured voltage convention is upper minus lower along y. Assume one carrier type and no transverse conduction.

Diagram shown in the original SVG worksheet.

  1. Derive VH(theta) and compare it with the perpendicular-field reading at theta=0.

  2. At theta=60.0 degrees, find the density error if the experimenter mistakenly uses the full B in the perpendicular-field formula.

Question 6 - Solution

Only the field component normal to the Hall strip contributes to its transverse voltage

Diagram shown in the original SVG worksheet.

(a) Method and calculation

v→d×B→=vdByẑ−vdBzŷ,Ey=vdBz.\vec v_d\times\vec B=v_dB_y\hat z-v_dB_z\hat y,\quad E_y=v_dB_z.VH(θ)=−IBcos⁡θnqt=VH(0)cos⁡θ.V_H(\theta)=-\frac{IB\cos\theta}{nqt}=V_H(0)\cos\theta.

(b) Interpretation and further calculation

ninferred=IB|q|t|VH(θ)|=n|cos⁡θ|.n_{\mathrm{inferred}}=\frac{IB}{|q|t|V_H(\theta)|}=\frac{n}{|\cos\theta|}.θ=60.0∘:ninferred=2n.\theta=60.0^\circ:\quad n_{\mathrm{inferred}}=2n.

Physical check

The in-plane field can produce a thickness-direction Hall field, but it does not replace Bz in the specified transverse voltage.