Phasors — Question 2

Section 16-10 · Physics pages 2574–2575

Question 2 A regular phasor polygon cancels even when no pair is opposite Three waves of equal amplitude A have phases 0, 2π/3 and 4π/3 at a common reference. Their frequencies and propagation wave numbers are equal. A A A Three equal phasors close an equilateral triangle. (a) Find their sum using complex amplitudes. (b) Generalize to N ≥2 equal amplitudes with phases 2πj/N, j = 0, . . . , N −1. Explain why pairwise cancellation is not necessary.
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Question 2 - Solution A regular phasor polygon cancels even when no pair is opposite A A A Method and mathematical working Use the finite geometric-series identity for equally spaced phase angles. The closed polygon provides the corresponding vector interpretation. N−1 ∑ j=0 e2πij/N = 1 −e2πi 1 −e2πi/N = 0 (N > 1). 1 + e2πi/3 + e4πi/3 = 1 + (−1/2 + i √ 3/2) + (−1/2 −i √ 3/2) = 0. (a) Calculation and conclusion Z = A[1 + e2πi/3 + e4πi/3] = 0. The real parts 1, −1/2, −1/2 and imaginary parts 0, √ 3/2, − √ 3/2 cancel. (b) Interpretation and limits Let q = e2πi/N̸ = 1. Then ∑N−1 j=0 qj = (1 −qN)/(1 −q) = 0. The phasors form a closed regular polygon. For odd N no vector needs a diametrically opposite partner; vector closure is the general cancellation criterion. Physical check The denominator is nonzero for N > 1, and the numerator vanishes exactly. Equal amplitudes and uniform phase spacing are both essential to this cancellation.

Question 2

A regular phasor polygon cancels even when no pair is opposite

Three waves of equal amplitude AA have phases 00, 2π/32\pi/3 and 4π/34\pi/3 at a common reference. Their frequencies and propagation wave numbers are equal.

Diagram shown in the original SVG worksheet.

  1. Find their sum using complex amplitudes.

  2. Generalize to N≥2N\ge2 equal amplitudes with phases 2πj/N2\pi j/N, j=0,…,N−1j=0,\ldots,N-1. Explain why pairwise cancellation is not necessary.

Question 2 - Solution

A regular phasor polygon cancels even when no pair is opposite

Diagram shown in the original SVG worksheet.

Method and mathematical working

Use the finite geometric-series identity for equally spaced phase angles. The closed polygon provides the corresponding vector interpretation.∑j=0N−1e2πij/N=1−e2πi1−e2πi/N=0(N>1).1+e2πi/3+e4πi/3=1+(−1/2+i3/2)+(−1/2−i3/2)=0.\begin{aligned}\sum_{j=0}^{N-1}e^{2\pi i j/N}&=\frac{1-e^{2\pi i}}{1-e^{2\pi i/N}}=0\qquad(N>1).\\[4pt]1+e^{2\pi i/3}+e^{4\pi i/3}&=1+(-1/2+i\sqrt3/2)+(-1/2-i\sqrt3/2)=0.\end{aligned}

(a) Calculation and conclusion

Z=A[1+e2πi/3+e4πi/3]=0Z=A[1+e^{2\pi i/3}+e^{4\pi i/3}]=0. The real parts 1,−1/2,−1/21,-1/2,-1/2 and imaginary parts 0,3/2,−3/20,\sqrt3/2,-\sqrt3/2 cancel.

(b) Interpretation and limits

Let q=e2πi/N≠1q=e^{2\pi i/N}\ne1. Then ∑j=0N−1qj=(1−qN)/(1−q)=0\sum_{j=0}^{N-1}q^j=(1-q^N)/(1-q)=0. The phasors form a closed regular polygon. For odd NN no vector needs a diametrically opposite partner; vector closure is the general cancellation criterion.

Physical check

The denominator is nonzero for N>1N>1, and the numerator vanishes exactly. Equal amplitudes and uniform phase spacing are both essential to this cancellation.