Zacher/Reuter 2024, Abschnitte 3.2 und 5.1.4: Frequenzgang eines P-T1-Glieds

PT1 Frequency Response Amplitude Calculator

A first-order system passes slow sinusoidal signals close to its static gain and increasingly attenuates faster variations.

MINTSI
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Inputs

Half the peak-to-peak range of the steady sinusoidal output. Compare with permitted measurement range or required useful-signal amplitude; startup transient is not included.

Ratio of a very slow or steady output change to input change. Obtain it from two steady states or the first-order model.

Distance from mean to positive peak of the sinusoidal input. Divide a peak-to-peak value by two; do not use RMS amplitude.

First-order time constant from a step test, datasheet or model identification. It sets corner frequency fc=1/(2πT).

Number of complete sinusoidal cycles per second. Obtain it from a signal generator, measurement or expected process excitation; f=0 is the static limiting case.

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Result

Select a target and calculate.

Steady-state sine response: phase shift -32.1°

Three periods of input (orange) and output (green) at steady state. Besides the amplitude attenuation, the output lags by φ = −arctan(ωT) – not part of the calculator's result, but directly readable in the Bode plot.

00.511.522.53-505Âoutxt [s]— output— input
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Calculation

Âout = K·Âin / √[1+(2πfT)²]

A first-order system passes slow sinusoidal signals close to its static gain and increasingly attenuates faster variations.

Understand the inputs
  • Steady output amplitude Âout — Half the peak-to-peak range of the steady sinusoidal output. Compare with permitted measurement range or required useful-signal amplitude; startup transient is not included.
  • Static gain K — Ratio of a very slow or steady output change to input change. Obtain it from two steady states or the first-order model.
  • Input amplitude Âin — Distance from mean to positive peak of the sinusoidal input. Divide a peak-to-peak value by two; do not use RMS amplitude.
  • Time constant T — First-order time constant from a step test, datasheet or model identification. It sets corner frequency fc=1/(2πT).
  • Excitation frequency f — Number of complete sinusoidal cycles per second. Obtain it from a signal generator, measurement or expected process excitation; f=0 is the static limiting case.
Example

K=2, Âin=3, T=0.1 s and f=1 Hz give 2πfT≈0.628 and Âout≈5.081. Without dynamic attenuation, 6 units would be expected.

Assumptions and limits

Linear time-invariant first-order system in sinusoidal steady state, constant parameters and no DC component in the amplitude calculation. Dead time, saturation, additional poles, noise and transient response are excluded.

Technical article

Understand PT1 Frequency Response Amplitude Calculator

This calculator moves the first-order model from time to frequency domain. It shows the amplitude remaining after transients when the input varies sinusoidally, for example a temperature wave, speed fluctuation or smoothed sensor signal.

What does this quantity describe?

A first-order system has proportional static behaviour and one lag. Its frequency response is G(jω)=K/(1+jωT). Magnitude |G(jω)| gives the factor applied to input amplitude at angular frequency ω=2πf. Here j denotes the imaginary unit used in complex frequency calculations.

Formula and variables

Âout = K·Âin / √[1+(2πfT)²]

  • Frequency response: G(jω)=K/(1+jωT)
  • Magnitude: |G(jω)|=K/√[1+(ωT)²]
  • Angular frequency: ω=2πf
  • Output amplitude: Âout=|G(jω)|·Âin
  • Phase: φ(ω)=−arctan(ωT)
Symbol / inputMeaning
Steady output amplitude ÂoutHalf the peak-to-peak range of the steady sinusoidal output. Compare with permitted measurement range or required useful-signal amplitude; startup transient is not included.
Static gain KRatio of a very slow or steady output change to input change. Obtain it from two steady states or the first-order model.
Input amplitude ÂinDistance from mean to positive peak of the sinusoidal input. Divide a peak-to-peak value by two; do not use RMS amplitude.
Time constant TFirst-order time constant from a step test, datasheet or model identification. It sets corner frequency fc=1/(2πT).
Excitation frequency fNumber of complete sinusoidal cycles per second. Obtain it from a signal generator, measurement or expected process excitation; f=0 is the static limiting case.

Choose the inputs correctly

K is static gain from two steady operating points. Âin is peak amplitude relative to mean, half a peak-to-peak value. T comes from a step test or model identification. f is complete cycles per second and comes from the excitation source or measurement.

How to use the calculator

First verify the system is approximately linear and reaches a stationary sinusoid after startup. Evaluate input relative to its mean and determine peak amplitude. Use K and T from the same operating point. Compare output amplitude with measurement range, disturbance limit or required useful signal.

Worked example

For K=2, Âin=3, T=0.1 s and f=1 Hz, ωT≈0.628. Magnitude is 2/√(1+0.628²)≈1.694, giving Âout≈5.081 instead of static value 6.

Understand the result and units

As f→0, Âout approaches K·Âin. At corner frequency fc=1/(2πT), amplitude falls to 70.7% of that static value, corresponding to −3 dB. Above the corner frequency, faster fluctuations are increasingly attenuated. The output also lags the input by φ=−arctan(2πfT) (−45° at the corner frequency, approaching −90° at high frequencies); the chart below the calculator shows this angle. Magnitude and phase over the whole frequency axis are given by the Bode plot calculator, the stability consequences of an additional dead time by the PT1 dead-time phase-margin calculator.

f is entered in hertz; 1 Hz means one cycle per second. T converts internally to seconds, making 2πfT dimensionless. Input and output amplitudes may carry physical units; this general calculator treats them on a consistent normalised scale.

Useful next calculation

If needed, determine T with first-order time identification. The first-order step response shows the same model in the time domain.

Typical applications

Useful for estimating sensor and process smoothing, filter action, periodic disturbance transmission, test design and learning Bode diagrams.

Assumptions, limits and common mistakes

The result covers only the steady sinusoidal component of a linear time-invariant first-order system. Mean value, startup transient, phase shift, dead time, additional poles, nonlinearity and saturation are outside the output. Non-sinusoidal signals require separate frequency components.

Common mistake: Do not enter peak-to-peak height or RMS value as peak amplitude. Do not confuse hertz with angular frequency in rad/s; the calculator applies ω=2πf. Dead time does not change ideal magnitude but does change phase and possible loop stability.

Frequently asked questions

What is “First-order output amplitude under sinusoidal excitation” used for?

Useful for estimating sensor and process smoothing, filter action, periodic disturbance transmission, test design and learning Bode diagrams.

Where do the input values come from?

K is static gain from two steady operating points. Âin is peak amplitude relative to mean, half a peak-to-peak value. T comes from a step test or model identification. f is complete cycles per second and comes from the excitation source or measurement.

What does the result not cover?

The result covers only the steady sinusoidal component of a linear time-invariant first-order system. Mean value, startup transient, phase shift, dead time, additional poles, nonlinearity and saturation are outside the output. Non-sinusoidal signals require separate frequency components.

Sources, method and review

Our method, source hierarchy and automated checks are documented on the methodology page. Read the methodology

Responsible
NormCalc-Redaktion
Last updated
2026-09-20