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Heaviside step function - Wikipedia, the free encyclopedia

Heaviside step function

From Wikipedia, the free encyclopedia

The Heaviside step function, using the half-maximum convention
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The Heaviside step function, using the half-maximum convention

The Heaviside step function, also called unit step function, is a discontinuous function whose value is zero for negative argument and one for positive argument:

H(x) =   \begin{cases} 0,           & x < 0              \\ \frac{1}{2}, & x = 0              \\ 1,           & x > 0   \end{cases}

It seldom matters what value is used for H(0), since H is mostly used as a distribution. Some common choices can be seen below.

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 was named in honor of Oliver Heaviside.

It is the cumulative distribution function of a random variable which is almost surely 0. (See constant random variable.)

The Heaviside function is an antiderivative of the Dirac delta function, H' = δ. This is sometimes written as

H(x) = \int_{-\infty}^x { \delta(t)} \mathrm{d}t

although this expression isn't mathematically correct.

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[edit] Discrete form

We can also define an alternative form of the unit step as a function of a discrete variable n:

H[n]=\begin{cases} 0, & n < 0 \\ 1, & n \ge 0 \end{cases}

where n is an integer.

The discrete-time unit impulse is the first difference of the discrete-time step

\delta[n] = H[n] - H[n-1]\,

This function is the cumulative summation of the Kronecker delta:

H[n] = \sum_{k=-\infty}^{n} \delta[k] \,

where

\delta[k] = \delta_{k,0} \,

is the discrete unit impulse function.

[edit] Analytic approximations

For a smooth approximation to the step function, one can use the logistic function

H(x) \approx \frac{1}{2} + \frac{1}{2}\tanh(kx) = \frac{1}{1+\mathrm{e}^{-2kx}},

where larger k corresponds to a sharper transition at x=0. If we take H(0) = 1/2, equality holds in the limit:

H(x)=\lim_{k \rightarrow \infty}\frac{1}{2}(1+\tanh kx)=\lim_{k \rightarrow \infty}\frac{1}{1+\mathrm{e}^{-2kx}}

There are many other smooth, analytic approximations to the step function. Some might be:

H(x) = \lim_{k \rightarrow \infty} \frac{1}{2} + \frac{1}{\pi}\arctan(kx) \
H(x) = \lim_{k \rightarrow \infty} \frac{1}{2} + \frac{1}{2}\operatorname{erf}(kx) \

[edit] Representations

Often an integral representation of the step function is useful:

H(x)=\lim_{ \epsilon \to 0^+} -{1\over 2\pi \mathrm{i}}\int_{-\infty}^\infty {1 \over \tau+\mathrm{i}\epsilon} \mathrm{e}^{-\mathrm{i} x \tau} \mathrm{d}\tau

[edit] H(0)

The value of the function at 0 can be defined as H(0) = 0, H(0) = 1/2 or H(0) = 1. H(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:

H(x) =   \begin{cases} 0,           & x < 0              \\ \frac{1}{2}, & x = 0              \\ 1,           & x > 0   \end{cases}
H(x) = \frac{1}{2} \left ( 1 + \sgn(x) \right )

To remove the ambiguity of which value to use for H(0), a subscript specifying which value may be used:

H_n(x) =   \begin{cases} 0, & x < 0              \\ n, & x = 0              \\ 1, & x > 0   \end{cases}

[edit] See also

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