---
title: "Underdamped second order unit step response derivation"
subject: "Control Systems"
chapter: 3
key: "semester_3/control_systems:second-order-step-derivation"
source: https://www.bctengineer.com/q/semester_3/control_systems/second-order-step-derivation
site: BCT Engineering
---

# Underdamped second order unit step response derivation

Control Systems · Chapter 3: System Transfer Function and Responses

- Asked in: 2071 Shrawan, 4 marks
- Video: [unit step response second order system under damped derivation](https://www.youtube.com/watch?v=19eCOPJdNKs) — techgurukula
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_3/control_systems/second-order-step-derivation
- Whole chapter: https://www.bctengineer.com/md/semester_3/control_systems/chapter-3

## Question

For an open loop transfer function with unity feedback G(s) = ωn²/[s(s + 2ξωn)] where ξ < 1, derive an expression for output when unit step input is applied.

## Short answer

For G(s)=ω_n²/[s(s+2ζω_n)] with ζ<1, the unit step response is c(t)=1 – (e^{-ζω_n t}/√(1−ζ²)) sin(ω_d t+θ), where ω_d = ω_n√(1−ζ²) and θ = tan⁻¹(√(1−ζ²)/ζ).

## Answer

For $\xi < 1$ (underdamped) the unit step response is a damped sinusoid that settles at 1.

#### Closed-loop transfer function
$$
\frac{C(s)}{R(s)} = \frac{G}{1+G} = \frac{\omega_n^2}{s^2 + 2\xi\omega_n s + \omega_n^2}
$$
For $\xi < 1$ the poles are complex:
$$
s = -\xi\omega_n \pm j\omega_n\sqrt{1-\xi^2} = -\xi\omega_n \pm j\omega_d, \qquad \omega_d = \omega_n\sqrt{1-\xi^2}
$$

#### Output for a unit step
With $R(s) = 1/s$:
$$
C(s) = \frac{\omega_n^2}{s(s^2 + 2\xi\omega_n s + \omega_n^2)}
$$
Partial fractions:
$$
\begin{aligned}
C(s) &= \frac{1}{s} - \frac{s + 2\xi\omega_n}{s^2 + 2\xi\omega_n s + \omega_n^2} \\
&= \frac{1}{s} - \frac{s + \xi\omega_n}{(s + \xi\omega_n)^2 + \omega_d^2} - \frac{\xi\omega_n}{(s + \xi\omega_n)^2 + \omega_d^2}
\end{aligned}
$$
Using $\mathcal{L}^{-1}\left\{\frac{s+a}{(s+a)^2+\omega^2}\right\} = e^{-at}\cos\omega t$ and $\mathcal{L}^{-1}\left\{\frac{\omega}{(s+a)^2+\omega^2}\right\} = e^{-at}\sin\omega t$:
$$
\begin{aligned}
c(t) &= 1 - e^{-\xi\omega_n t}\cos\omega_d t - \frac{\xi\omega_n}{\omega_d}e^{-\xi\omega_n t}\sin\omega_d t \\
&= 1 - e^{-\xi\omega_n t}\left[\cos\omega_d t + \frac{\xi}{\sqrt{1-\xi^2}}\sin\omega_d t\right]
\end{aligned}
$$
Put $\cos\theta = \xi$ and $\sin\theta = \sqrt{1-\xi^2}$, so that $\cos\omega_d t\,\sin\theta + \sin\omega_d t\,\cos\theta = \sin(\omega_d t + \theta)$:
$$
c(t) = 1 - \frac{e^{-\xi\omega_n t}}{\sqrt{1-\xi^2}}\sin(\omega_d t + \theta), \qquad \theta = \tan^{-1}\frac{\sqrt{1-\xi^2}}{\xi}
$$

The response is a sine wave at $\omega_d$ that decays inside the envelopes $1 \pm e^{-\xi\omega_n t}/\sqrt{1-\xi^2}$ and settles at the final value 1, so the steady state error is zero.

```text
 c(t)
  |    _
  |   / \     _
 1|--/---\---/-\--------- final value
  | /     \_/
  |/
  +------------------------ t
```

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. For unity feedback with G = wn^2/[s(s+2*xi*wn)], C/R is
   A. wn^2/(s^2+2*xi*wn*s)
   B. wn^2/(s^2+2*xi*wn*s+wn^2)
   C. 1/(s^2+2*xi*wn*s+wn^2)
   D. wn^2/(s+2*xi*wn)
   Answer: B. G/(1+G) gives denominator s^2+2*xi*wn*s+wn^2. (Key point: Closed-loop TF)

2. For xi<1, the closed-loop poles are
   A. -xi*wn +/- j*wn*sqrt(1-xi^2)
   B. +/- j*wn
   C. -wn and -xi*wn
   D. -xi*wn +/- wn*sqrt(xi^2-1)
   Answer: A. Complex poles with real part -xi*wn and imaginary part wd = wn*sqrt(1-xi^2). (Key point: Pole location)

3. The unit step response for xi<1 is
   A. 1 - e^(-xi*wn*t)*sin(wd*t)
   B. 1 - e^(-wn*t)*cos(wd*t)
   C. 1 - [e^(-xi*wn*t)/sqrt(1-xi^2)]*sin(wd*t + theta)
   D. 1 + e^(-xi*wn*t)*sin(wd*t)
   Answer: C. Partial fractions and inverse Laplace give this damped sinusoid, with theta = atan(sqrt(1-xi^2)/xi). (Key point: Step response)

4. What is the steady state error for this step response?
   A. Zero, since c(t) settles at 1
   B. Equal to xi
   C. Infinite
   D. 1/wn
   Answer: A. The exponential term decays, so c(t) approaches 1. (Key point: Final value)

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