Crossed Fields: The Hall Effect — Question 4

Section 28-4 · Physics pages 4538–4539

Question 4 Combining longitudinal resistance with a Hall measurement separates density and mobility A single-electron-carrier strip has length L=.0200 m, width w=.00500 m and thickness t=.000200 m. At I=.0100 A, its longitudinal voltage is .400 V. With B=.500 T, its upper-minus-lower Hall voltage is +2.00 mV. Use e=1.60 × 10−19 C and σ = neµ. 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) Find conductivity and the signed Hall coefficient RH = Ey/(JxB). (b) Find electron density n and mobility mu.
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Question 4 - Solution Combining longitudinal resistance with a Hall measurement separates density and mobility I U L y x Bˆz w thickness t along z (a) Method and calculation σ = IL Vxwt = 500 S/m. RH = −VHt IB = −8.00 × 10−5 m3/C. (b) Interpretation and further calculation n = 1 e|RH| = 7.8125 × 1022 m−3. µ = σ ne = σ|RH| = .0400 m2/(V s). Physical check A conductivity measurement alone constrains the product of carrier density and mobility, not either separately.

Question 4

Combining longitudinal resistance with a Hall measurement separates density and mobility

A single-electron-carrier strip has length L=.0200 m, width w=.00500 m and thickness t=.000200 m. At I=.0100 A, its longitudinal voltage is .400 V. With B=.500 T, its upper-minus-lower Hall voltage is +2.00 mV. Use e=1.60×10−191.60\times10^{-19} C and σ=neμ\sigma=ne\mu.

Diagram shown in the original SVG worksheet.

  1. Find conductivity and the signed Hall coefficient RH=Ey/(JxB)R_H=E_y/(J_xB).

  2. Find electron density n and mobility mu.

Question 4 - Solution

Combining longitudinal resistance with a Hall measurement separates density and mobility

Diagram shown in the original SVG worksheet.

(a) Method and calculation

σ=ILVxwt=500S/m.\sigma=\frac{IL}{V_xwt}=500\,\mathrm{S/m}.RH=−VHtIB=−8.00×10−5m3/C.R_H=-\frac{V_Ht}{IB}=-8.00\times10^{-5}\,\mathrm{m^3/C}.

(b) Interpretation and further calculation

n=1e|RH|=7.8125×1022m−3.n=\frac1{e|R_H|}=7.8125\times10^{22}\,\mathrm{m^{-3}}.μ=σne=σ|RH|=.0400m2/(Vs).\mu=\frac\sigma{ne}=\sigma|R_H|=.0400\,\mathrm{m^2/(V\,s)}.

Physical check

A conductivity measurement alone constrains the product of carrier density and mobility, not either separately.