Crossed Fields: The Hall Effect — Question 7

Section 28-4 · Physics pages 4544–4545

Question 7 Finite voltmeter resistance suppresses a Hall voltage and inflates the inferred density Treat the transverse Hall contacts as an ideal open-circuit voltage VH0 in series with resistance rH. A voltmeter of resistance RV is connected between them. Assume it does not otherwise change the imposed longitudinal current. Hall source rH V RV Schematic; labels, not drawing lengths, specify the data. (a) Find the measured voltage and the density inferred by ignoring the meter loading. (b) Find the minimum RV/rH needed to keep the inferred density no more than one percent above its true value.
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Question 7 - Solution Finite voltmeter resistance suppresses a Hall voltage and inflates the inferred density Hall source rH V RV (a) Method and calculation Vm = VH0 RV rH + RV . ninferred n = |VH0| |Vm| = 1 + rH RV . (b) Interpretation and further calculation ninferred −n n = rH/RV ≤.0100. RV /rH ≥100. Physical check The density error is the inverse of the voltage attenuation, so its exact expression differs from the fractional voltage error.

Question 7

Finite voltmeter resistance suppresses a Hall voltage and inflates the inferred density

Treat the transverse Hall contacts as an ideal open-circuit voltage VH0 in series with resistance rH. A voltmeter of resistance RV is connected between them. Assume it does not otherwise change the imposed longitudinal current.

Diagram shown in the original SVG worksheet.

  1. Find the measured voltage and the density inferred by ignoring the meter loading.

  2. Find the minimum RV/rH needed to keep the inferred density no more than one percent above its true value.

Question 7 - Solution

Finite voltmeter resistance suppresses a Hall voltage and inflates the inferred density

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Vm=VH0RVrH+RV.V_m=V_{H0}\frac{R_V}{r_H+R_V}.ninferredn=|VH0||Vm|=1+rHRV.\frac{n_{\mathrm{inferred}}}n=\frac{|V_{H0}|}{|V_m|}=1+\frac{r_H}{R_V}.

(b) Interpretation and further calculation

ninferred−nn=rH/RV≤.0100.\frac{n_{\mathrm{inferred}}-n}{n}=r_H/R_V\le.0100.RV/rH≥100.R_V/r_H\ge100.

Physical check

The density error is the inverse of the voltage attenuation, so its exact expression differs from the fractional voltage error.