Potential Difference Between Two Points — Question 10

Section 27-5 · Physics pages 4410–4411

Question 10 A divider output tolerance depends on a resistance ratio rather than its total scale A divider has positive nominal R1,R2 and ideal input E. Output is taken across R2 without load. Let k = R2/(R1 + R2). + − E R1 R2 A B M Circuit connections and marked polarities define the model; wire lengths are schematic. (a) Derive the first-order fractional output change caused by small fractional changes epsilon1 and epsilon2 in the two resistors. (b) For R1=R2 and independent hard tolerances of one percent, give the first-order worst-case output error and explain why equal tracking errors cancel exactly.
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Question 10 - Solution A divider output tolerance depends on a resistance ratio rather than its total scale + − E R1 R2 A B M (a) Method and calculation Vo = E R2 R1 + R2 , δ ln Vo = δR2 R2 −δR1 + δR2 R1 + R2 . δVo/Vo ≃(1 −k)(ϵ2 −ϵ1). (b) Interpretation and further calculation k = 1/2 : |δVo|/Vo ≲1 2(.01 + .01) = .0100. Ri′ = (1 + ϵ)Ri ⇒Vo′ = E (1 + ϵ)R2 (1 + ϵ)(R1 + R2) = Vo. Physical check Matched tracking can preserve a voltage ratio even when the total resistance and source current change.

Question 10

A divider output tolerance depends on a resistance ratio rather than its total scale

A divider has positive nominal R1,R2 and ideal input E. Output is taken across R2 without load. Let k=R2/(R1+R2)k=R_2/(R_1+R_2).

Diagram shown in the original SVG worksheet.

  1. Derive the first-order fractional output change caused by small fractional changes epsilon1 and epsilon2 in the two resistors.

  2. For R1=R2 and independent hard tolerances of one percent, give the first-order worst-case output error and explain why equal tracking errors cancel exactly.

Question 10 - Solution

A divider output tolerance depends on a resistance ratio rather than its total scale

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Vo=ER2R1+R2,δln⁡Vo=δR2R2−δR1+δR2R1+R2.V_o=E\frac{R_2}{R_1+R_2},\quad\delta\ln V_o=\frac{\delta R_2}{R_2}-\frac{\delta R_1+\delta R_2}{R_1+R_2}.δVo/Vo≃(1−k)(ϵ2−ϵ1).\delta V_o/V_o\simeq(1-k)(\epsilon_2-\epsilon_1).

(b) Interpretation and further calculation

k=1/2:|δVo|/Vo≲12(.01+.01)=.0100.k=1/2:\quad|\delta V_o|/V_o\lesssim\tfrac12(.01+.01)=.0100.Ri′=(1+ϵ)Ri⇒Vo′=E(1+ϵ)R2(1+ϵ)(R1+R2)=Vo.R_i\prime=(1+\epsilon)R_i\Rightarrow V_o\prime=E\frac{(1+\epsilon)R_2}{(1+\epsilon)(R_1+R_2)}=V_o.

Physical check

Matched tracking can preserve a voltage ratio even when the total resistance and source current change.