Phasors — Question 10

Section 16-10 · Physics pages 2590–2591

Question 10 A nearly closed phasor polygon reveals the direction of an error A collection of phasors sums exactly to zero. One member is Zj = Aeiϕ. All other members remain fixed while that member acquires either a small fractional amplitude error η or a small phase error ϵ. Zj ηZj iϵZj After rotating the reference so Zj is real, amplitude and phase errors point along perpendicular axes. (a) Find the residual phasor to first order for each error separately. (b) Explain how a phase-sensitive residual measurement can distinguish these errors even when their residual magnitudes are equal.
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Question 10 - Solution A nearly closed phasor polygon reveals the direction of an error Zj ηZj iϵZj Method and mathematical working Perturb just one term in a sum that originally closes. Subtract its original value to isolate the residual produced by each kind of small error. δZamplitude = ηZj, δZphase = (eiϵ −1)Zj ≈iϵZj. |δZamplitude| = |η|Aj, |δZphase| ≃|ϵ|Aj, Re[(ηZj)∗(iϵZj)] = Re(iηϵA2 j) = 0. (a) Calculation and conclusion An amplitude change gives ∆Z = ηAeiϕ = ηZj. A phase change gives ∆Z = Zj(eiϵ −1) ≈iϵZj. Their first-order magnitudes are A|η| and A|ϵ|. (b) Interpretation and limits The amplitude-error residual lies along the affected phasor, while the phase-error residual is perpendicular to it. Magnitude alone loses this distinction. Near perfect cancellation the resultant phase can change sharply, so reporting only the phase of a very small residual is numerically fragile. Physical check The amplitude-error residual is parallel to the perturbed vector, while the first-order phase-error residual is perpendicular. Their different directions provide information that residual magnitude alone loses.

Question 10

A nearly closed phasor polygon reveals the direction of an error

A collection of phasors sums exactly to zero. One member is Zj=AeiϕZ_j=Ae^{i\phi}. All other members remain fixed while that member acquires either a small fractional amplitude error η\eta or a small phase error ϵ\epsilon.

Diagram shown in the original SVG worksheet.

  1. Find the residual phasor to first order for each error separately.

  2. Explain how a phase-sensitive residual measurement can distinguish these errors even when their residual magnitudes are equal.

Question 10 - Solution

A nearly closed phasor polygon reveals the direction of an error

Diagram shown in the original SVG worksheet.

Method and mathematical working

Perturb just one term in a sum that originally closes. Subtract its original value to isolate the residual produced by each kind of small error.δZamplitude=ηZj,δZphase=(eiϵ−1)Zj≈iϵZj.|δZamplitude|=|η|Aj,|δZphase|≃|ϵ|Aj,Re⁡[(ηZj)*(iϵZj)]=Re⁡(iηϵAj2)=0.\begin{aligned}\delta Z_{\mathrm{amplitude}}&=\eta Z_j,\\\delta Z_{\mathrm{phase}}&=(e^{i\epsilon}-1)Z_j\approx i\epsilon Z_j.\\[4pt]|\delta Z_{\mathrm{amplitude}}|&=|\eta|A_j,\quad |\delta Z_{\mathrm{phase}}|\simeq|\epsilon|A_j,\\\operatorname{Re}\!\left[(\eta Z_j)^*(i\epsilon Z_j)\right]&=\operatorname{Re}(i\eta\epsilon A_j^2)=0.\end{aligned}

(a) Calculation and conclusion

An amplitude change gives ΔZ=ηAeiϕ=ηZj\Delta Z=\eta Ae^{i\phi}=\eta Z_j. A phase change gives ΔZ=Zj(eiϵ−1)≈iϵZj\Delta Z=Z_j(e^{i\epsilon}-1)\approx i\epsilon Z_j. Their first-order magnitudes are A|η|A|\eta| and A|ϵ|A|\epsilon|.

(b) Interpretation and limits

The amplitude-error residual lies along the affected phasor, while the phase-error residual is perpendicular to it. Magnitude alone loses this distinction. Near perfect cancellation the resultant phase can change sharply, so reporting only the phase of a very small residual is numerically fragile.

Physical check

The amplitude-error residual is parallel to the perturbed vector, while the first-order phase-error residual is perpendicular. Their different directions provide information that residual magnitude alone loses.