Match List I with List II List – I List – II f(t) F(S) A. e -at I. \(\rm \frac{s}{s^2+ \omega^2}\) B. te at II. \(\rm \frac{\omega}{s^2+ \omega^2}\) C. sinωt III. \(\rm \frac{1}{(s- a)^2}\) D. cosωt IV. \(\rm \frac{1}{(s+ a)}\) Choose the correct answer from the options given below:
A ‐ IV, B ‐ III, C ‐ II, D ‐ I
This problem requires us to match common time-domain functions \(f(t)\) with their corresponding Laplace transforms \(F(s)\). The Laplace transform is a powerful tool used in engineering and physics to transform differential equations in the time domain \(t\) into algebraic equations in the complex frequency domain \(s\). This makes solving systems much simpler.
To solve this matching problem, we need to know the standard Laplace transforms for the given functions. Here are the relevant formulas:
We also need the frequency shifting property: If \(\mathcal{L}\{f(t)\} = F(s)\), then \(\mathcal{L}\{e^{at}f(t)\} = F(s-a)\).
Let's find the Laplace transform for each function in List I and match it with the correct expression in List II.
Using the standard formula for \(e^{-at}\), we have:
\(\mathcal{L}\{e^{-at}\} = \frac{1}{s - (-a)} = \frac{1}{s+a}\)
This matches expression IV in List II.
So, A – IV.
This function is a product of \(t\) and \(e^{at}\). We can use the frequency shifting property. First, let's find the Laplace transform of \(f(t) = t\). Here, \(n=1\).
\(\mathcal{L}\{t^1\} = \frac{1!}{s^{1+1}} = \frac{1}{s^2}\)
Now, apply the frequency shifting property with \(a\):
\(\mathcal{L}\{e^{at} \cdot t\} = F(s-a)\)
Where \(F(s) = \frac{1}{s^2}\). Replacing \(s\) with \((s-a)\), we get:
\(\mathcal{L}\{te^{at}\} = \frac{1}{(s-a)^2}\)
This matches expression III in List II.
So, B – III.
Using the standard formula for \(\sin(\omega t)\), we have:
\(\mathcal{L}\{\sin(\omega t)\} = \frac{\omega}{s^2 + \omega^2}\)
This matches expression II in List II.
So, C – II.
Using the standard formula for \(\cos(\omega t)\), we have:
\(\mathcal{L}\{\cos(\omega t)\} = \frac{s}{s^2 + \omega^2}\)
This matches expression I in List II.
So, D – I.
Let's put our findings into a table:
| List I \(f(t)\) | Laplace Transform \(\mathcal{L}\{f(t)\}\) | Matching List II \(F(s)\) |
|---|---|---|
| A. \(e^{-at}\) | \(\frac{1}{s+a}\) | IV |
| B. \(te^{at}\) | \(\frac{1}{(s-a)^2}\) | III |
| C. \(\sin(\omega t)\) | \(\frac{\omega}{s^2 + \omega^2}\) | II |
| D. \(\cos(\omega t)\) | \(\frac{s}{s^2 + \omega^2}\) | I |
The correct matching is A – IV, B – III, C – II, D – I.
Let's check the given options:
Option 4 correctly matches our derived Laplace transforms.
| Time Domain \(f(t)\) | Laplace Domain \(F(s) = \mathcal{L}\{f(t)\}\) |
|---|---|
| \(\delta(t)\) (Dirac delta) | \(1\) |
| \(u(t)\) (Unit step) | \(\frac{1}{s}\) |
| \(t^n, n \ge 0\) | \(\frac{n!}{s^{n+1}}\) |
| \(e^{at}\) | \(\frac{1}{s-a}\) |
| \(e^{-at}\) | \(\frac{1}{s+a}\) |
| \(\sin(\omega t)\) | \(\frac{\omega}{s^2 + \omega^2}\) |
| \(\cos(\omega t)\) | \(\frac{s}{s^2 + \omega^2}\) |
| \(\sinh(at)\) | \(\frac{a}{s^2 - a^2}\) |
| \(\cosh(at)\) | \(\frac{s}{s^2 - a^2}\) |
Beyond the basic formulas, understanding the properties of the Laplace transform is crucial for solving more complex problems. Some important properties include:
These properties allow us to find Laplace transforms of more complicated functions by breaking them down or transforming known transforms.
Which of the following is the final value of the impulse response of the system whose transfer function is
(2s + 1)/(s 4 + 8s 3 + 16s 2 + s)
Find the Laplace transform for the following time domain.
y(t) = -2te -t + 4e -t - 4e -2t
The Laplace transform of sin h (at) is
The unilateral Laplace transform of f(t) is \(\frac{1}{s^2+s+1}\). The unilateral Laplace transform of t f(t) is
Laplace transform of the function f(t) denoted by F(s) is given by