Delayed Inputs and Convolution
Represent switched forcing and combine an input with an impulse response.
Builds on Laplace Inversion and Initial-Value Problems
The bigger question: Can we turn a changing-time problem into algebra?
On this page
The idea
The step switches on at time . A delayed waveform transforms to . The argument inside must be shifted as well; is generally a different signal.
Visual guide
- Step input
- Response
Method and assumptions
For zero initial data, a linear time-invariant system with impulse response responds to input through convolution: . The Laplace transform of convolution is the product . Each past input contributes a delayed copy of the impulse response.
Worked example: a delayed switch
For and , the transform is . Therefore . It stays zero until the input begins, then approaches one.
Try it yourself.
Choose an answer and explain your reasoning to yourself. Use a hint if you get stuck.
Hint 1 · Find a starting point
A delay shifts the start of the signal to t=a.
Hint 2 · Take the next step
Substitute τ=t−a in the transform integral.
Show the reasoning
Answer: e⁻ᵃˢF(s)
The exponential factor splits as e⁻ᵃˢe⁻ˢτ, giving e⁻ᵃˢF(s).
Before moving on: what would make one of the other answers wrong? Saying why is part of understanding.
Worked example: a ramp through a filter
For , , the impulse response is . Convolution gives . Differentiating confirms .
Interpreting the result
An ordinary step in forcing usually leaves the state continuous while changing its derivative. An impulse can cause a jump instead. Separate the forcing’s discontinuities from the response’s continuity requirements.
Practice
- Transform .
- Write a unit pulse active from to .
- Find the zero-state response of .
Show worked solutions
- .
- .
- Convolution with gives .
Further study
MIT OpenCourseWare: Differential Equations provides a full university course with additional lectures and exercises.
Pause before the next idea.
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