y=K·Δu·[1−e^(−D·t/T₀)·(cos(ωd·t)+D/√(1−D²)·sin(ωd·t))], ωd=√(1−D²)/T₀
The second-order model describes systems with two coupled storage elements whose output may overshoot the final value depending on damping.
The second-order model describes systems with two coupled storage elements whose output may overshoot the final value depending on damping.
Select a target and calculate.
The second-order model describes systems with two coupled storage elements whose output may overshoot the final value depending on damping.
K=1, Δu=1, D=0.5 and T₀=1 s give y≈1.0746 at t=5 s: the output is still 7.46% above its final value.
Linear time-invariant second-order element initially at rest before an ideal step and underdamped case 0<D<1; dead time, zeros, saturation and additional poles are excluded.
Calculate the time response of an underdamped second-order element from gain, damping, natural time, step height and time.
The second-order model describes systems with two coupled storage elements whose output may overshoot the final value depending on damping. This calculator represents a clearly bounded technical relationship between the displayed quantities. The definition helps put inputs into the same reference state before interpreting the result.
y=K·Δu·[1−e^(−D·t/T₀)·(cos(ωd·t)+D/√(1−D²)·sin(ωd·t))], ωd=√(1−D²)/T₀
| Symbol / input | Meaning |
|---|---|
| Output change y(t) | Instantaneous output change relative to the pre-step state. Add the former output value to obtain an absolute reading. |
| Static gain K | Final output change divided by input step. Determine K from steady readings before and after the test. |
| Input step Δu | Step height, new input minus old input. Together with K it sets the final output value. |
| Damping ratio D | Dimensionless measure of oscillation decay. Obtain D from a step test or model identification; small values mean strong overshoot. This calculator applies for 0<D<1. |
| Natural time T₀ | Reciprocal of undamped natural angular frequency: T₀=1/ω₀. Obtain it from model parameters or measured oscillation period. |
| Time since the step t | Observation time measured from the input step. |
Output change y(t): Instantaneous output change relative to the pre-step state. Add the former output value to obtain an absolute reading. Static gain K: Final output change divided by input step. Determine K from steady readings before and after the test. Input step Δu: Step height, new input minus old input. Together with K it sets the final output value. Damping ratio D: Dimensionless measure of oscillation decay. Obtain D from a step test or model identification; small values mean strong overshoot. This calculator applies for 0<D<1. Natural time T₀: Reciprocal of undamped natural angular frequency: T₀=1/ω₀. Obtain it from model parameters or measured oscillation period. Time since the step t: Observation time measured from the input step.
Select the target quantity, enter the other known values with units, then check the result against the worked example and model limits.
K=1, Δu=1, D=0.5 and T₀=1 s give y≈1.0746 at t=5 s: the output is still 7.46% above its final value.
The second-order model describes systems with two coupled storage elements whose output may overshoot the final value depending on damping. Read the result as a model value for the selected operating point and check units, sign, order of magnitude and application boundary conditions.
Use the displayed units and convert afterwards. Prefixes such as k-, m- and µ- are common sources of mistakes.
PT2 element: damped step response: Such basic calculations support plausibility checks, early component selection and preparation of a complete verification.
Linear time-invariant second-order element initially at rest before an ideal step and underdamped case 0<D<1; dead time, zeros, saturation and additional poles are excluded.
Common mistake: A formally correct result can still be unsuitable when load case, reference state or units do not match the application.
Compare unit and order of magnitude with a second calculation and vary inputs one at a time.
No. The calculator exposes a model; real boundary conditions require separate review.
Only when the calculator converts within the same physical quantity type.