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Fourier Transform I

Part 2: Convolution

Another important notion that we will need in connection with the Fourier Transform is that of convolution. If f and g are both absolutely integrable over the real line, then the convolution of f and g is given by

Definition of convolution

Suppose f is a "random" absolutely integrable function. If g is a nonegative function with integral 1 and support concentrated near 0, then the convolution f * g at x may be thought of as an averaging of the function values of f near x.

  1. Let f be the function given in the worksheet and let hn be the first sequential approximation to the delta function.
    First sequential approximation to the delta function

    Compare the graph of the convolution f * hn with the graph of f for n = 1, 2, 3, and 4.

  2. Now calculate the convolution of f with the delta function and compare that with the graph of f itself.

  3. Alter the the functions hn by shifting the graph of each function one unit to the right. Calculate the convolution of f with the shifted function hn for n = 1, 2, 3, and 4, and compare the graph of this convolution with the graph of f itself.

  4. Calculate the convolution of f with the shifted delta function and compare that with the graph of f itself.

  5. Pick another amount to shift hn and the delta function, and repeat Steps 3 and 4.

  6. Summarize what you have learned about convolution from these experiments.

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