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GOVT POLYTECHNIC GHANPUR
 Name :
 Pin no :
 Program :
 Course :
 Topic :
E.NANDHA GOPAL
18168-EE-029
EEE
MATHEMATICS
LAPLACE
TRANSFORMATION
Intoduction
 Transformation in mathematical deals with the
conversion of one function to another function that may
not be in the same domain .
 Laplace transform is a powerful transformation tool,
which literally transforms the original differential equation
into an elementary algebraic expression. The latter can
then simply be transformed once again, into the solution
of the original problem.
 This is named after the mathematician and renowned
astronomer “Pierre Simon Laplace” who lived in France.
 The Definition – In this section we give the definition of the Laplace
transform. We will also compute a couple Laplace transforms using
the definition.
 Laplace Transforms – In this section we introduce the way we
usually compute Laplace transforms that avoids needing to use the
definition. We discuss the table of Laplace transforms used in this
material and work a variety of examples illustrating the use of the
table of Laplace transforms.
 Inverse Laplace Transforms – In this section we ask the opposite
question from the previous section. In other words, given a Laplace
transform, what function did we originally have? We again work a
variety of examples illustrating how to use the table of Laplace
transforms to do this as well as some of the manipulation of the
given Laplace transform that is needed in order to use the table.
 Step Functions – In this section we introduce the step or Heaviside
function. We illustrate how to write a piecewise function in terms of
Heaviside functions. We also work a variety of examples showing how to
take Laplace transforms and inverse Laplace transforms that involve
Heaviside functions. We also derive the formulas for taking the Laplace
transform of functions which involve Heaviside functions.
 Solving IVPs' with Laplace Transforms - In this section we will examine
how to use Laplace transforms to solve IVP’s. The examples in this section
are restricted to differential equations that could be solved without using
Laplace transform. The advantage of starting out with this type of
differential equation is that the work tends to be not as involved and we
can always check our answers if we wish to.
 Nonconstant Coefficient IVP’s – In this section we will give a brief
overview of using Laplace transforms to solve some non constant
coefficient IVP’s. We do not work a great many examples in this section.
We only work a couple to illustrate how the process works with Laplace
transforms
 IVP’s with Step Functions – This is the section where the reason for
using Laplace transforms really becomes apparent. We will use
Laplace transforms to solve IVP’s that contain Heaviside (or step)
functions. Without Laplace transforms solving these would involve quite
a bit of work. While we do work one of these examples without Laplace
transforms, we do it only to show what would be involved if we did try to
solve one of the examples without using Laplace transforms
Nandha ppt
Nandha ppt
Nandha ppt

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Nandha ppt

  • 1. GOVT POLYTECHNIC GHANPUR  Name :  Pin no :  Program :  Course :  Topic : E.NANDHA GOPAL 18168-EE-029 EEE MATHEMATICS LAPLACE TRANSFORMATION
  • 2. Intoduction  Transformation in mathematical deals with the conversion of one function to another function that may not be in the same domain .  Laplace transform is a powerful transformation tool, which literally transforms the original differential equation into an elementary algebraic expression. The latter can then simply be transformed once again, into the solution of the original problem.  This is named after the mathematician and renowned astronomer “Pierre Simon Laplace” who lived in France.
  • 3.  The Definition – In this section we give the definition of the Laplace transform. We will also compute a couple Laplace transforms using the definition.  Laplace Transforms – In this section we introduce the way we usually compute Laplace transforms that avoids needing to use the definition. We discuss the table of Laplace transforms used in this material and work a variety of examples illustrating the use of the table of Laplace transforms.  Inverse Laplace Transforms – In this section we ask the opposite question from the previous section. In other words, given a Laplace transform, what function did we originally have? We again work a variety of examples illustrating how to use the table of Laplace transforms to do this as well as some of the manipulation of the given Laplace transform that is needed in order to use the table.
  • 4.  Step Functions – In this section we introduce the step or Heaviside function. We illustrate how to write a piecewise function in terms of Heaviside functions. We also work a variety of examples showing how to take Laplace transforms and inverse Laplace transforms that involve Heaviside functions. We also derive the formulas for taking the Laplace transform of functions which involve Heaviside functions.  Solving IVPs' with Laplace Transforms - In this section we will examine how to use Laplace transforms to solve IVP’s. The examples in this section are restricted to differential equations that could be solved without using Laplace transform. The advantage of starting out with this type of differential equation is that the work tends to be not as involved and we can always check our answers if we wish to.  Nonconstant Coefficient IVP’s – In this section we will give a brief overview of using Laplace transforms to solve some non constant coefficient IVP’s. We do not work a great many examples in this section. We only work a couple to illustrate how the process works with Laplace transforms
  • 5.  IVP’s with Step Functions – This is the section where the reason for using Laplace transforms really becomes apparent. We will use Laplace transforms to solve IVP’s that contain Heaviside (or step) functions. Without Laplace transforms solving these would involve quite a bit of work. While we do work one of these examples without Laplace transforms, we do it only to show what would be involved if we did try to solve one of the examples without using Laplace transforms