Heaviside step distribution
The Heaviside step distribution is defined by (Abramowitz and Stegun Eq. 29.1.3, p. 1020):
Note that other definitions exist at , for example . In the famous Mathematica computer package is unevaluated.
Applications[edit]
Differentiating the Heaviside distribution[edit]
At first glance things are hopeless:
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle {\frac {{\rm {d}}H(x)}{{\rm {d}}x}}=\infty ,~x=0}
however, lets define a less brutal jump in the form of a linear slope such that
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle H_{\epsilon }(x-a)={\frac {1}{\epsilon }}\left(R(x-(a-{\frac {\epsilon }{2}}))-R(x-(a+{\frac {\epsilon }{2}}))\right)}
in the limit this becomes the Heaviside function Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle H(x-a)} . However, lets differentiate first:
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{{\rm d}}{{\rm d}x} H_{\epsilon}(x-a)= \frac{1}{\epsilon}\left( H(x - (a-\frac{\epsilon}{2})) - H (x - (a+\frac{\epsilon}{2}))\right)}
in the limit this is the Dirac delta distribution. Thus
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{{\rm d}}{{\rm d}x} [H(x)]= \delta(x)} .