| Heaviside Step Function |
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The Heaviside step function, sometimes called the '''unit step function''' and named in honor of Oliver Heaviside , is a Discontinuous Function whose value is Zero for negative argument and One for positive argument: : The function is used in the mathematics of Control Theory and Signal Processing to represent a signal that switches on at a specified time and stays switched on indefinitely. It is the Cumulative Distribution Function of a Random Variable which is Almost Surely 0. (See Constant Random Variable .) The Heaviside function is the Integral of the Dirac Delta Function . : The value of ''u''(0) is occasionally of disputed value. Some writers give ''u''(0) = 0, some ''u''(0) = 1. ''u''(0) = 1/2 is the most consistent choice used, since it maximizes the Symmetry of the function and becomes completely consistent with the Signum Function . This makes for a more general definition: : : To remove the ambiguity of which value to use for ''u''(0), a subscript specifying which value may be used: : Often an integral representation of the step function is useful: : DISCRETE FORM We can also define an alternative form of the unit step as a function of a discrete variable ''n'': : where ''n'' is an integer. This function is the cumulative summation of the Kronecker Delta : : where : is the Discrete Unit Impulse Function . ANALYTIC APPROXIMATIONS For a Smooth approximation to the step function, one can use the Logistic Function :, where larger ''k'' corresponds to a sharper transition at x=0. SEE ALSO |
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