Crossed Fields: The Hall Effect — Question 10

Section 28-4 · Physics pages 4550–4551

Question 10 A heating limit changes the thickness scaling of Hall sensitivity A one-carrier strip has resistivity rho, length L, width w and thickness t. Its longitudinal resistance is rho L/(wt). Maximum allowed Joule heating is Pmax. The field B, density n and charge magnitude e are fixed; contacts are ideal. 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 maximum permitted current and the largest Hall-voltage magnitude under the heating limit. (b) If t is halved with all other quantities fixed, compare the new maximum current and maximum Hall voltage with the old values.
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Question 10 - Solution A heating limit changes the thickness scaling of Hall sensitivity I U L y x Bˆz w thickness t along z (a) Method and calculation Imax = √ Pmax R = √ Pmaxwt ρL . |VH|max = BImax net = B ne √ Pmaxw ρLt . (b) Interpretation and further calculation t′ = t/2 ⇒Imax′ = Imax/ √ 2. |VH|max′ = √ 2|VH|max. Physical check At fixed current, halving thickness doubles the voltage; under fixed allowable heating, current must also decrease.

Question 10

A heating limit changes the thickness scaling of Hall sensitivity

A one-carrier strip has resistivity rho, length L, width w and thickness t. Its longitudinal resistance is rho L/(wt). Maximum allowed Joule heating is Pmax. The field B, density n and charge magnitude e are fixed; contacts are ideal.

Diagram shown in the original SVG worksheet.

  1. Derive the maximum permitted current and the largest Hall-voltage magnitude under the heating limit.

  2. If t is halved with all other quantities fixed, compare the new maximum current and maximum Hall voltage with the old values.

Question 10 - Solution

A heating limit changes the thickness scaling of Hall sensitivity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Imax=PmaxR=PmaxwtρL.I_{\max}=\sqrt{\frac{P_{\max}}R}=\sqrt{\frac{P_{\max}wt}{\rho L}}.|VH|max=BImaxnet=BnePmaxwρLt.|V_H|_{\max}=\frac{BI_{\max}}{net}=\frac B{ne}\sqrt{\frac{P_{\max}w}{\rho Lt}}.

(b) Interpretation and further calculation

t′=t/2⇒Imax′=Imax/2.t\prime=t/2\Rightarrow I_{\max}\prime=I_{\max}/\sqrt2.|VH|max′=2|VH|max.|V_H|_{\max}\prime=\sqrt2|V_H|_{\max}.

Physical check

At fixed current, halving thickness doubles the voltage; under fixed allowable heating, current must also decrease.