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Physics · Glossary

What is Complex amplitude?

Definition 8.2 University Physics — Year 1 · Chapter 8 — Sinusoidal Steady State and Impedance

To the sinusoid x(t)=Xcos⁡(ωt+φ)x(t) = X\cos(\omega t + \varphi) one associates the complex signal x‾(t)=Xej(ωt+φ)\underline{x}(t) = X\eu^{j(\omega t + \varphi)}, so that x=Re⁡(x‾)x = \Rea(\underline{x}), and the complex amplitude

X‾=Xejφ,x‾(t)=X‾ ejωt,\underline{X} = X\eu^{j\varphi}, \qquad \underline{x}(t) = \underline{X}\,\eu^{j\omega t},

which carries the amplitude X=∣X‾∣X = \abs{\underline{X}} and the phase φ=arg⁡X‾\varphi = \arg\underline{X}. Here jj denotes the imaginary unit, j2=−1j^2 = -1, the letter ii being reserved for currents. Drawn as a vector of length XX at angle φ\varphi, X‾\underline{X} is a phasor (Fresnel vector).

Examples

Example 8.4 (Adding two sinusoids)

3cos⁡ωt+4sin⁡ωt3\cos\omega t + 4\sin\omega t: the complex amplitudes are 33 and 4e−jπ/2=−4j4\eu^{-j\pi/2} = -4j (since sin⁡ωt=cos⁡(ωt−π/2)\sin\omega t = \cos(\omega t - \pi/2)); their sum 3−4j3 - 4j has modulus 55 and argument −0.927 rad-0.927\ \mathrm{rad}: 5cos⁡(ωt−0.927)5\cos(\omega t - 0.927). No trigonometric identity needed.

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