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How does nonlinearity create harmonics and distortion?

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A weakly nonlinear amplifier can be modeled by the power series y = a1x + a2x² + a3x³. Driving it with one tone produces harmonics at 2f and 3f and, when a3 opposes a1, gain compression. Two tones produce intermodulation products at 2f1 − f2 and 2f2 − f1 that fall close to the wanted signal.[1]

What happens with a single tone?

For x = A·cos ωt: the fundamental is (a1A + ¾a3A³), the second harmonic ½a2A² and the third harmonic ¼a3A³. Second-order products grow 2 dB per dB of input and third-order products 3 dB per dB.[1]

What are desensitization and cross-modulation?

A strong blocker reduces the small-signal gain seen by a weak wanted signal (desensitization or blocking) through the a3 term. If the blocker is amplitude-modulated, that modulation transfers to the wanted signal (cross-modulation), which matters in full-duplex systems where the transmitter leaks into the receiver.[1]

Which distortion products matter most?

Frequently asked questions

Do differential circuits cancel even harmonics?

Ideally yes; balance limits the cancellation in practice.

Is a mixer a nonlinear device?

Yes, intentionally: it relies on multiplication, which is a nonlinear (time-varying) operation.

Does the power-series model apply to PAs?

Only approximately; PAs near saturation and with memory effects need more complete behavioral models.

References

Online sources accessed October 21, 2026; printed works cited by edition. See all sources.

  1. “RF Microelectronics, 2nd ed.”. B. Razavi, Prentice Hall. 2012.
  2. “Recommendation ITU-R SM.329: Unwanted emissions in the spurious domain”. ITU-R. current version.