Introduction to Laplace Transform

April 11th, 2014 | Posted in Panel Building
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converts differential and integral equations into rather simple algebraic equations. Laplace transform is nothing but a simple operational tool, used to solve linear differential equations with constant coefficients.

The transformation is only applied to general signals and not to sinusoidal signals. Also, it cannot handle steady state conditions. It enables us to study complicated control systems with integrators, differentiators and gains.

On basis of Laplace transformation we analyze LCCODE’s and circuits with several sources, inductors, resistors and capacitors.

For a given function f (t) such that t Introduction to Laplace Transform_symbol1 0, its Laplace transformation is written as F(s) = L {f (t)} and is written as:

Introduction to Laplace Transform_1

From the above equation we conclude that the transformation converges when the limit exists and diverge when it does not. The L notation recognizes that integration always proceeds over t = 0 to t=1 and that the integral involves an integrator Introduction to Laplace Transform_symbol2 dt instead of the usual dt.

Laplace transformation method

Laplace transformation reduces the problem of solving a differential equation to an algebraic problem. Laplace theory is based on Lerch’s cancellation law which is given as follows:

Introduction to Laplace Transform2

In a differential equation, y(t) is an unknown variable depending on time.

Laplace Integral

The Laplace integral of a function g (t) is given as:

Introduction to Laplace Transform3

The integral formulae are derived by illustrating g (t) = 1, g (t) = t and g (t) =

Introduction to Laplace Transform4

By summarizing we get:

Introduction to Laplace Transform5

Some important transformation rules:

Following are some properties of general calculus that can be implemented on the transformation:

  • The sum of two integrals can be combined:

  • Introduction to Laplace Transform6

  • Lerch’s cancellation law is applied on Laplace transformation:

  • Introduction to Laplace Transform7

  • Integration by parts or sometimes called the t-derivative rule:

  • Introduction to Laplace Transform8

  • Constant can be written out of the integral:

  • Introduction to Laplace Transform9

Laplace Transforms of Periodic Functions

At times the non-homogenous term in a linear differential equation is a periodic function. Any function f (t) can be said a t-periodic function if we write it as f (t+T) = f (t) like the period of sine and cosine is Introduction to Laplace Transform_symbol3 radians where period of tangent is Introduction to Laplace Transform_symbol4

For a t-period the function is written as:

Introduction to Laplace Transform_symbol10

Provided that t Introduction to Laplace Transform_symbol1 0

Now the Laplace transform is given as:

Introduction to Laplace Transform10

  • Example 1:

  • Introduction to Laplace Transform11

    Using the definition we have:

    Introduction to Laplace Transform12

    For improper integral to converge we need s > a. Here:

    Introduction to Laplace Transform13

  • Example 2:
  • Let’s have a look at Laplace transform of Sin at and Cos at.

    Using the Euler’s formula we can write:

    Introduction to Laplace Transform14

    By Laplace transform we have:

    Introduction to Laplace Transform15

    By comparing real and imaginary parts we get:

    Introduction to Laplace Transform16


Though the topic of Laplace transform is much wider, we have tried to enclose the basics of it in this article. What is the basic idea and concept of Laplace transform and how it works. We discussed a couple of examples to elaborate it more.

As we move on to the end of these tutorials we will study the most important part in the upcoming one that is Transfer Function. It is the factor on which a control systems depends so stay tuned to us for the tutorial.


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