<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>https://en.formulasearchengine.com/w/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=165.138.236.2</id>
	<title>formulasearchengine - User contributions [en]</title>
	<link rel="self" type="application/atom+xml" href="https://en.formulasearchengine.com/w/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=165.138.236.2"/>
	<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/wiki/Special:Contributions/165.138.236.2"/>
	<updated>2026-07-11T17:44:28Z</updated>
	<subtitle>User contributions</subtitle>
	<generator>MediaWiki 1.47.0-wmf.7</generator>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Regenerative_brake&amp;diff=3835</id>
		<title>Regenerative brake</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Regenerative_brake&amp;diff=3835"/>
		<updated>2014-01-29T18:39:30Z</updated>

		<summary type="html">&lt;p&gt;165.138.236.2: /* Limitations */ edited the location of the 1948 accident to match http://en.wikipedia.org/wiki/List_of_rail_accidents_%281930%E2%80%9349%29&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[mathematics]], for a given complex [[Hermitian matrix]] &amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt; and nonzero [[vector (geometry)|vector]] &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt;, the &#039;&#039;&#039;Rayleigh quotient&#039;&#039;&#039;&amp;lt;ref&amp;gt;Also known as the &#039;&#039;&#039;Rayleigh–Ritz ratio&#039;&#039;&#039;; named after [[Walther Ritz]] and [[Lord Rayleigh]].&amp;lt;/ref&amp;gt; &amp;lt;math&amp;gt;R(M, x)&amp;lt;/math&amp;gt;, is defined as:&amp;lt;ref&amp;gt;Horn, R. A. and C. A. Johnson. 1985. &#039;&#039;Matrix Analysis&#039;&#039;. Cambridge University Press. pp. 176&amp;amp;ndash;180.&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;Parlet B. N. &#039;&#039;The symmetric eigenvalue problem&#039;&#039;, SIAM, Classics in Applied Mathematics,1998&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;R(M,x) := {x^{*} M x \over x^{*} x}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For real matrices and vectors, the condition of being Hermitian reduces to that of being [[Symmetric matrix|symmetric]], and the [[conjugate transpose]] &amp;lt;math&amp;gt;x^{*}&amp;lt;/math&amp;gt; to the usual [[transpose]] &amp;lt;math&amp;gt;x&#039;&amp;lt;/math&amp;gt;. Note that &amp;lt;math&amp;gt;R(M, c x) = R(M,x)&amp;lt;/math&amp;gt; for any [[Real Numbers|real]] scalar &amp;lt;math&amp;gt;c \neq 0 &amp;lt;/math&amp;gt;. Recall that a Hermitian (or real symmetric) matrix has real [[eigenvalues]]. It can be shown that, for a given matrix, the Rayleigh quotient reaches its minimum value &amp;lt;math&amp;gt;\lambda_\min&amp;lt;/math&amp;gt; (the smallest [[eigenvalue]] of &amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt;) when &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; is &amp;lt;math&amp;gt;v_\min&amp;lt;/math&amp;gt; (the corresponding [[eigenvector]]). Similarly, &amp;lt;math&amp;gt;R(M, x) \leq \lambda_\max&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;R(M, v_\max) = \lambda_\max&amp;lt;/math&amp;gt;. The Rayleigh quotient is used in the [[min-max theorem]] to get exact values of all eigenvalues. It is also used in [[eigenvalue algorithm]]s to obtain an eigenvalue approximation from an eigenvector approximation. Specifically, this is the basis for [[Rayleigh quotient iteration]].&lt;br /&gt;
&lt;br /&gt;
The range of the Rayleigh quotient is called a [[numerical range]].&lt;br /&gt;
&lt;br /&gt;
==Special case of covariance matrices==&lt;br /&gt;
An empirical [[covariance matrix]] &#039;&#039;M&#039;&#039; can be represented as the product &#039;&#039;A&#039;&#039;&amp;amp;apos; &#039;&#039;A&#039;&#039; of the [[data matrix (multivariate statistics)|data matrix]] &#039;&#039;A&#039;&#039; pre-multiplied by its transpose &#039;&#039;A&#039;&#039;&amp;amp;apos;. Being a symmetrical real matrix, &#039;&#039;M&#039;&#039; has non-negative eigenvalues, and orthogonal (or othogonalisable) eigenvectors, which can be demonstrated as follows.&lt;br /&gt;
&lt;br /&gt;
Firstly, that the eigenvalues &amp;lt;math&amp;gt;\lambda_i&amp;lt;/math&amp;gt; are non-negative:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;M v_i = A&#039; A v_i = \lambda_i v_i&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Rightarrow v_i&#039; A&#039; A v_i = v_i&#039; \lambda_i v_i&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Rightarrow \left\| A v_i \right\|^2 = \lambda_i \left\| v_i \right\|^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Rightarrow \lambda_i = \frac{\left\| A v_i \right\|^2}{\left\| v_i \right\|^2} \geq 0.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Secondly, that the eigenvectors &amp;lt;math&amp;gt;v_i&amp;lt;/math&amp;gt; are orthogonal to one another:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;M v_i = \lambda _i v_i&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Rightarrow v_j&#039; M v_i = \lambda _i v_j&#039; v_i&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Rightarrow (M v_j )&#039; v_i = \lambda _i v_j&#039; v_i&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Rightarrow \lambda_j v_j &#039; v_i = \lambda _i v_j&#039; v_i&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Rightarrow (\lambda_j - \lambda_i) v_j &#039; v_i = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Rightarrow v_j &#039; v_i = 0&amp;lt;/math&amp;gt; (if the eigenvalues are different – in the case of multiplicity, the basis can be orthogonalized).&lt;br /&gt;
&lt;br /&gt;
To now establish that the Rayleigh quotient is maximised by the eigenvector with the largest eigenvalue, consider decomposing an arbitrary vector &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; on the basis of the eigenvectors &#039;&#039;v&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;i&#039;&#039;&amp;lt;/sub&amp;gt;:&lt;br /&gt;
:&amp;lt;math&amp;gt;x = \sum _{i=1} ^n \alpha _i v_i&amp;lt;/math&amp;gt;,  where  &amp;lt;math&amp;gt; \alpha_i = \frac{x&#039;v_i}{v_i&#039;v_i} = \frac{\langle x,v_i\rangle}{\left\| v_i \right\| ^2}&amp;lt;/math&amp;gt; is the coordinate of x orthogonally projected onto &amp;lt;math&amp;gt;v_i&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
so&lt;br /&gt;
:&amp;lt;math&amp;gt;R(M,x) = \frac{x&#039; A&#039; A x}{x&#039; x}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
can be written&lt;br /&gt;
:&amp;lt;math&amp;gt;R(M,x) = \frac{(\sum _{j=1} ^n \alpha _j v_j)&#039; A&#039; A (\sum _{i=1} ^n \alpha _i v_i)}{(\sum _{j=1} ^n \alpha _j v_j)&#039; (\sum _{i=1} ^n \alpha _i v_i)}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
which, by orthogonality of the eigenvectors, becomes:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;R(M,x) = \frac{\sum _{i=1} ^n \alpha _i ^2 \lambda _i}{\sum _{i=1} ^n \alpha _i ^2} = \sum_{i=1}^n \lambda_i \frac{(x&#039;v_i)^2}{ (x&#039;x)( v_i&#039; v_i)}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The last representation establishes that the Rayleigh quotient is the sum of the squared cosines of the angles formed by the vector &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; and each eigenvector &amp;lt;math&amp;gt;v_i&amp;lt;/math&amp;gt;, weighted by corresponding eigenvalues.&lt;br /&gt;
&lt;br /&gt;
If a vector &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; maximizes &amp;lt;math&amp;gt;R(M,x)&amp;lt;/math&amp;gt;, then any scalar multiple &amp;lt;math&amp;gt;k x&amp;lt;/math&amp;gt; (for &amp;lt;math&amp;gt;k \ne 0&amp;lt;/math&amp;gt;) also maximizes &#039;&#039;R&#039;&#039;, so the problem can be reduced to the [[Lagrange multipliers|Lagrange problem]] of maximizing &amp;lt;math&amp;gt;\sum _{i=1} ^n \alpha _i ^2 \lambda _i&amp;lt;/math&amp;gt; under the constraint that &amp;lt;math&amp;gt;\sum _{i=1} ^n \alpha _i ^2 = 1&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Let &amp;lt;math&amp;gt;\beta_i \overset{\text{def}}= \alpha_i^2&amp;lt;/math&amp;gt;. This then becomes a [[linear program]], which always attains its maximum at one of the corners of the domain. A maximum point will have &amp;lt;math&amp;gt;\alpha _1 = \pm 1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\forall i &amp;gt; 1, \alpha _i = 0&amp;lt;/math&amp;gt; (when the eigenvalues are ordered by decreasing magnitude).&lt;br /&gt;
&lt;br /&gt;
Thus, as advertised, the Rayleigh quotient is maximised by the eigenvector with the largest eigenvalue.&lt;br /&gt;
&lt;br /&gt;
=== Formulation using Lagrange multipliers ===&lt;br /&gt;
Alternatively, this result can be arrived at by the method of [[Lagrange multipliers]]. The problem is to find the [[critical point (mathematics)|critical points]] of the function&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;R(M,x) = x^T M x &amp;lt;/math&amp;gt;, &lt;br /&gt;
subject to the constraint &amp;lt;math&amp;gt;\|x\|^2 = x^Tx = 1.&amp;lt;/math&amp;gt;&lt;br /&gt;
I.e. to find the critical points of &lt;br /&gt;
:&amp;lt;math&amp;gt;\mathcal{L}(x) = x^T M x  -\lambda (x^Tx - 1), &amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\lambda &amp;lt;/math&amp;gt; is a Lagrange multiplier. The stationary points of &amp;lt;math&amp;gt;\mathcal{L}(x)&amp;lt;/math&amp;gt; occur at&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{d\mathcal{L}(x)}{dx} = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\therefore 2x^T M^T  - 2\lambda x^T = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\therefore M x = \lambda x &amp;lt;/math&amp;gt;&lt;br /&gt;
and &amp;lt;math&amp;gt; R(M,x) = \frac{x^T M x}{x^T x} = \lambda \frac{x^Tx}{x^T x} = \lambda.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Therefore, the eigenvectors &amp;lt;math&amp;gt;x_1 \ldots x_n&amp;lt;/math&amp;gt; of &#039;&#039;M&#039;&#039; are the critical points of the Rayleigh Quotient and their corresponding eigenvalues &amp;lt;math&amp;gt;\lambda_1 \ldots \lambda_n&amp;lt;/math&amp;gt; are the stationary values of &#039;&#039;R&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
This property is the basis for [[principal components analysis]] and [[canonical correlation]].&lt;br /&gt;
&lt;br /&gt;
==Use in Sturm&amp;amp;ndash;Liouville theory==&lt;br /&gt;
[[Sturm&amp;amp;ndash;Liouville theory]] concerns the action of the [[linear operator]]&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;L(y) = \frac{1}{w(x)}\left(-\frac{d}{dx}\left[p(x)\frac{dy}{dx}\right] + q(x)y\right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
on the [[inner product space]] defined by&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\langle{y_1,y_2}\rangle = \int_a^b w(x)y_1(x)y_2(x) \, dx&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
of functions satisfying some specified [[boundary conditions]] at &#039;&#039;a&#039;&#039; and &#039;&#039;b&#039;&#039;. In this case the Rayleigh quotient is&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{\langle{y,Ly}\rangle}{\langle{y,y}\rangle} = \frac{\int_a^b{y(x)\left(-\frac{d}{dx}\left[p(x)\frac{dy}{dx}\right] + q(x)y(x)\right)}dx}{\int_a^b{w(x)y(x)^2}dx}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This is sometimes presented in an equivalent form, obtained by separating the integral in the numerator and using [[integration by parts]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{\langle{y,Ly}\rangle}{\langle{y,y}\rangle} = \frac{\int_a^b{y(x)\left(-\frac{d}{dx}\left[p(x)y&#039;(x)\right]\right)}dx + \int_a^b{q(x)y(x)^2} \, dx}{\int_a^b{w(x)y(x)^2} \, dx}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;= \frac{-y(x)\left[p(x)y&#039;(x)\right]|_a^b + \int_a^b{y&#039;(x)\left[p(x)y&#039;(x)\right]} \, dx + \int_a^b{q(x)y(x)^2} \, dx}{\int_a^b{w(x)y(x)^2} \, dx}&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;= \frac{-p(x)y(x)y&#039;(x)|_a^b + \int_a^b\left[p(x)y&#039;(x)^2 + q(x)y(x)^2\right] \, dx}{\int_a^b{w(x)y(x)^2} \, dx}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Generalization==&lt;br /&gt;
For a given pair &amp;lt;math&amp;gt;(A, B)&amp;lt;/math&amp;gt; of matrices, and a given non-zero vector &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt;, the &#039;&#039;&#039;generalized Rayleigh quotient&#039;&#039;&#039; is defined as:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;R(A,B; x) := \frac{x^* A x}{x^* B x}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The Generalized Rayleigh Quotient can be reduced to the Rayleigh Quotient &amp;lt;math&amp;gt;R(D, C^*x)&amp;lt;/math&amp;gt; through the transformation &amp;lt;math&amp;gt;D = C^{-1} A {C^*}^{-1}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;CC^*&amp;lt;/math&amp;gt; is the [[Cholesky decomposition]] of the Hermitian positive-definite matrix &amp;lt;math&amp;gt;B&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Field of values]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Further reading==&lt;br /&gt;
* Shi Yu, Léon-Charles Tranchevent, Bart Moor, Yves Moreau, &#039;&#039;[http://books.google.com/books?id=U6-ubGYgf7QC&amp;amp;dq=&#039;Rayleigh%E2%80%93Ritz+ratio%22+Rayleigh+quotient&amp;amp;source=gbs_navlinks_s Kernel-based Data Fusion for Machine Learning: Methods and Applications in Bioinformatics and Text Mining]&#039;&#039;, Ch. 2, Springer, 2011.&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Rayleigh Quotient}}&lt;br /&gt;
[[Category:Linear algebra]]&lt;/div&gt;</summary>
		<author><name>165.138.236.2</name></author>
	</entry>
</feed>