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In words, equation [1] states that y at timet is equal to the integral of x() from minus infinity up to time t. Now, recall thederivative property of the Fourier Transform for a function g(t):

derivative of a function Fourier Transforms properties

Let's rewrite this Fourier property:

rewriting derivative for the fourier transform

We can substitute h(t)=dg(t)/dt [i.e. h(t) is the time derivative of g(t)] into equation [3]:

replacing the integral

Since g(t) is an arbitrary function, h(t) is as well and equation [4] gives a general result:

property of fourier transform

Equation [5] is "mostly" true. The reason it lacks completeness is that we used equation [3] to derive it - and note that the derivative of g(t) removes any constant: that is, the derivative of g(t) is equal to the derivative of the function g(t)+b, for any constant b. Because of this oversite, equation [5] is almost correct. If the total integral of g(t) is 0, then equation [5] directly follows from equation [3], and we have:

fourier transform properties of integration

If the total integral of g(t) is not zero, then there exists some constantc such that the total integral of g(t)-c is zero:

removing the dc constant term

That is,c is the "average value" of the function g(t), which is also often called the "dc term" or the "constant term". Using some math and theFourier Transform of the impulse function, we have the general formula for the Fourier Transform of the integral of a function:

the property of fourier transform for hte integration

The Dirac-Delta impulse function in [7] isexplained here.

The integration property is used and the constant in [8] is utilized on the Fourier Transform pagefor the unit step function, which should help clear things up if the above is not clear.


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