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Introduces convolution for analog signals.

In this module we examine convolution for continuous time signals. This willresult in the convolution integral and its properties . These concepts are very important in ElectricalEngineering and will make any engineer's life a lot easier if the time is spent now to truly understand what is going on.

In order to fully understand convolution, you may find it useful to look at the discrete-time convolution as well. Accompanied to this module there is a fully worked out example with mathematics and figures. It will also be helpful to experiment with the Convolution - Continuous time applet available from Johns Hopkins University . These resources offers different approaches to this crucial concept.

Derivation of the convolution integral

The derivation used here closely follows the one discussed in the motivation section above. To begin this, it is necessary to state theassumptions we will be making. In this instance, the only constraints on our system are that it be linear andtime-invariant.

    Brief overview of derivation steps:

  • An impulse input leads to an impulse response output.
  • A shifted impulse input leads to a shifted impulse response output. This is due to the time-invariance of the system.
  • We now scale the impulse input to get a scaled impulse output. This is using the scalar multiplication property oflinearity.
  • We can now "sum up" an infinite number of these scaled impulses to get a sum of an infinite number of scaledimpulse responses. This is using the additivity attribute of linearity.
  • Now we recognize that this infinite sum is nothing more than an integral, so we convert both sides into integrals.
  • Recognizing that the input is the function f t , we also recognize that the output is exactly the convolution integral.

We begin with a system defined by its impulse response, h t .
We then consider a shifted version of the input impulse. Due to the time invariance of the system, we obtain ashifted version of the output impulse response.
Now we use the scaling part of linearity by scaling the system by a value, f , that is constant with respect to the system variable, t .
We can now use the additivity aspect of linearity to add an infinite number of these, one for each possible . Since an infinite sum is exactly an integral, we end up with the integration knownas the Convolution Integral. Using the sampling property , we recognize the left-hand side simply as the input f t .

Convolution integral

As mentioned above, the convolution integral provides an easy mathematical way to express the output of an LTI system basedon an arbitrary signal, x t , and the system's impulse response, h t . The convolution integral is expressed as

y t x h t
Convolution is such an important tool that it is represented by the symbol *, and can be written as
y t x t h t
By making a simple change of variables into the convolution integral, t , we can easily show that convolution is commutative :
x t h t h t x t
which gives an equivivalent form of
y t x t h
For more information on the characteristics of the convolutionintegral, read about the Properties of Convolution .

Implementation of convolution

Taking a closer look at the convolution integral, we find that we are multiplying the input signal by the time-reversedimpulse response and integrating. This will give us the value of the output at one given value of t . If we then shift the time-reversed impulse response by a small amount, we getthe output for another value of t . Repeating this for every possible value of t , yields the total output function. While we would never actually do thiscomputation by hand in this fashion, it does provide us with some insight into what is actually happening. We find that weare essentially reversing the impulse response function and sliding it across the input function, integrating as we go.This method, referred to as the graphical method , provides us with a much simpler way to solve for the outputfor simple (contrived) signals, while improving our intuition for the more complex cases where we rely on computers. Infact Texas Instruments develops Digital Signal Processors which have special instruction sets for computations such as convolution.

Summary

Convolution is a truly important concept, which must be well understood.

y t x h t
y t h x t

Go to?

  • Introduction
  • Convolution - Full example
  • Convolution - Discrete time
  • Properties of convolution

Questions & Answers

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Maira Reply
nanopartical of organic/inorganic / physical chemistry , pdf / thesis / review
Ali
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Maira Reply
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learn
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Giriraj
Preparation and Applications of Nanomaterial for Drug Delivery
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please someone correct me if I'm wrong but I think one can use nanoparticles, specially silver nanoparticles for water treatment.
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Professor
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Damian
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LITNING Reply
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LITNING
scanning tunneling microscope
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Rafiq
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what is simplest way to understand the applications of nano robots used to detect the cancer affected cell of human body.? How this robot is carried to required site of body cell.? what will be the carrier material and how can be detected that correct delivery of drug is done Rafiq
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Any one who tell me about Preparation and application of Nanomaterial for drug Delivery
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what is Nano technology ?
Bob Reply
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Bob
The nanotechnology is as new science, to scale nanometric
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nanotechnology is the study, desing, synthesis, manipulation and application of materials and functional systems through control of matter at nanoscale
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Source:  OpenStax, Information and signal theory. OpenStax CNX. Aug 03, 2006 Download for free at http://legacy.cnx.org/content/col10211/1.19
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