Solving for Impulse Response h(t) Given z'(t) + 4z(t) = 4x(t)

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Discussion Overview

The discussion revolves around finding the impulse response h(t) for the differential equation z'(t) + 4z(t) = 4x(t). Participants explore methods for solving this equation, particularly through the use of Laplace transforms, and address the implications of including the unit step function u(t) in the final expression.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant proposes substituting z(t) with h(t) and x(t) with dirac(t) to reformulate the equation for impulse response.
  • Another participant suggests using Laplace transforms to solve the differential equation, leading to an expression for H(s) and its subsequent partial fraction expansion.
  • A participant expresses confusion about the inclusion of the unit step function u(t) in the final solution, questioning its relevance in the context of signals.
  • One reply emphasizes the necessity of keeping u(t) in the solution to avoid nonzero values before t = 0, when the excitation is applied.

Areas of Agreement / Disagreement

Participants generally agree on the approach of using Laplace transforms, but there is some uncertainty regarding the treatment of the unit step function u(t) in the final expression for h(t). The discussion remains unresolved on the exact formulation of the final solution.

Contextual Notes

There are unresolved aspects regarding the treatment of initial conditions and the implications of including or omitting the unit step function in the solution.

ryukyu
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1. Find the impulse response h(t) given: z'(t) + 4z(t) = 4x(t)




2. The attempt at a solution

I first decided to divide through by 4

(1/4)z'(t) + z(t) = x(t)

since we are looking for impulse response I made the following substitutions:

let z(t) = h(t)

let x(t) = dirac(t)

which yields

(1/4) h'(t) + h(t) = dirac(t)

at which point I don't know how to handle the problem anymore.
 
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I'm assuming you want an explicit solution for h(t)

there are other ways to solve that differential equation, but in signal processing courses you're usually taught to use laplace transforms.

assuming initial conditions are 0
you would get

(1/4)[s*H(s)-h(0)] + H(s) = 1/s
(1/4)[s*H(s)] + H(s) = 1/s
H(s)[s/4 + 1] = 1/s
H(s) = 4/(s*(s+4))
from here, you can use partial fraction expansion, and then take the inverse laplace transform of the fractions separately.
 
Great! This gets me a bit further. Now I am just a bit confused about expressing my answer.

I did the partial fraction expansion and got a=(1/4) and b=(-1/4)

This gave me:

H(s)=(1/4)(1/s) - (1/4)(1/(s+4))

taking the Laplace Inverse

h(t) = (1/4)u(t) - (1/4)e^(-4t)u(t)

While in DiffEq, we ignored the u(t), I'm assuming since it has relevance to signals it should be kept, but I'm not sure.

If so my final solution should be
h(t) = (1/4)u(t)*[1-e^(-4t)] ??
 
ryukyu said:
Great! This gets me a bit further. Now I am just a bit confused about expressing my answer.

I did the partial fraction expansion and got a=(1/4) and b=(-1/4)

This gave me:

H(s)=(1/4)(1/s) - (1/4)(1/(s+4))

taking the Laplace Inverse

h(t) = (1/4)u(t) - (1/4)e^(-4t)u(t)

While in DiffEq, we ignored the u(t), I'm assuming since it has relevance to signals it should be kept, but I'm not sure.

If so my final solution should be
h(t) = (1/4)u(t)*[1-e^(-4t)] ??

You must keep u(t), because if it is omitted your response would have nonzero values before t = 0, when the excitation was applied.
 

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