Difference between revisions of "Rayleigh distribution"
(Importing text file) |
Ulf Rehmann (talk | contribs) m (dead link removed) |
||
Line 11: | Line 11: | ||
<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/r/r077/r077730/r0777307.png" /></td> </tr></table> | <table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/r/r077/r077730/r0777307.png" /></td> </tr></table> | ||
− | when <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/r/r077/r077730/r0777308.png" />; hence, when <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/r/r077/r077730/r0777309.png" /> the Rayleigh distribution coincides with the distribution of the square root of a random variable which has the [[ | + | when <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/r/r077/r077730/r0777308.png" />; hence, when <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/r/r077/r077730/r0777309.png" /> the Rayleigh distribution coincides with the distribution of the square root of a random variable which has the [[Chi-squared distribution| "chi-squared" distribution]] with two degrees of freedom. In other words, a Rayleigh distribution can be interpreted as the distribution of the length of a vector in a plane Cartesian coordinate system, the coordinates of which are independent and have the [[Normal distribution|normal distribution]] with parameters 0 and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/r/r077/r077730/r07773010.png" />. In the three-dimensional space the [[Maxwell distribution|Maxwell distribution]] plays a role analogous to the Rayleigh distribution. |
A Rayleigh distribution is mainly applied in target theory and statistical communication theory. It was first considered by Lord Rayleigh in 1880 as the distribution of the amplitude resulting from the addition of harmonic oscillations. | A Rayleigh distribution is mainly applied in target theory and statistical communication theory. It was first considered by Lord Rayleigh in 1880 as the distribution of the amplitude resulting from the addition of harmonic oscillations. |
Revision as of 11:50, 20 October 2012
A continuous probability distribution with density
depending on a scale parameter . A Rayleigh distribution has positive asymmetry; its unique mode is at the point . All moments of a Rayleigh distribution are finite, the mathematical expectation and variance being and , respectively. The distribution function of a Rayleigh distribution has the form
A Rayleigh distribution is a special case of the distribution with density
when ; hence, when the Rayleigh distribution coincides with the distribution of the square root of a random variable which has the "chi-squared" distribution with two degrees of freedom. In other words, a Rayleigh distribution can be interpreted as the distribution of the length of a vector in a plane Cartesian coordinate system, the coordinates of which are independent and have the normal distribution with parameters 0 and . In the three-dimensional space the Maxwell distribution plays a role analogous to the Rayleigh distribution.
A Rayleigh distribution is mainly applied in target theory and statistical communication theory. It was first considered by Lord Rayleigh in 1880 as the distribution of the amplitude resulting from the addition of harmonic oscillations.
References
[1] | J.W. [Lord Rayleigh] Strutt, "Wave theory of light" , Moscow-Leningrad (1940) (In Russian; translated from English) |
Comments
References
[a1] | A. Papoulis, "Probability, random variables and stochastic processes" , McGraw-Hill (1965) |
Rayleigh distribution. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Rayleigh_distribution&oldid=28549