Crossed Fields: The Hall Effect — Question 1

Section 28-4 · Physics pages 4532–4533

Question 1 The Hall-voltage sign follows the carrier sign only after the contact convention is fixed A strip carries conventional current I along +x in a field Bˆz with B positive. Its width is w along y and thickness t along z. There is one carrier type of signed charge q and density n. Define VH = V (+w/2) −V (−w/2). I U L y x Bˆz w thickness t along z Hall contacts: VH = VU −VL; current points along +x and the shown field along +z. (a) Derive the transverse electric field and signed Hall voltage in steady state. (b) For negative and positive carriers, determine which edge is at higher potential while keeping I and B fixed.
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Question 1 - Solution The Hall-voltage sign follows the carrier sign only after the contact convention is fixed I U L y x Bˆz w thickness t along z (a) Method and calculation Jx = nqvd, Ey −vdB = 0 ⇒Ey = JxB nq . VH = −Eyw = −IB nqt, Jx = I/(wt). (b) Interpretation and further calculation q < 0 ⇒VH > 0 ⇒VU > VL. q > 0 ⇒VH < 0 ⇒VU < VL. Physical check Reversing the voltage-contact order reverses the reported Hall sign without changing the material.

Question 1

The Hall-voltage sign follows the carrier sign only after the contact convention is fixed

A strip carries conventional current I along +x in a field BẑB\hat z with B positive. Its width is w along y and thickness t along z. There is one carrier type of signed charge q and density n. Define VH=V(+w/2)−V(−w/2)V_H=V(+w/2)-V(-w/2).

Diagram shown in the original SVG worksheet.

  1. Derive the transverse electric field and signed Hall voltage in steady state.

  2. For negative and positive carriers, determine which edge is at higher potential while keeping I and B fixed.

Question 1 - Solution

The Hall-voltage sign follows the carrier sign only after the contact convention is fixed

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Jx=nqvd,Ey−vdB=0⇒Ey=JxBnq.J_x=nqv_d,\quad E_y-v_dB=0\Rightarrow E_y=\frac{J_xB}{nq}.VH=−Eyw=−IBnqt,Jx=I/(wt).V_H=-E_yw=-\frac{IB}{nqt},\quad J_x=I/(wt).

(b) Interpretation and further calculation

q<0⇒VH>0⇒VU>VL.q<0\Rightarrow V_H>0\Rightarrow V_U>V_L.q>0⇒VH<0⇒VU<VL.q>0\Rightarrow V_H<0\Rightarrow V_U<V_L.

Physical check

Reversing the voltage-contact order reverses the reported Hall sign without changing the material.