<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>http://www.sklogwiki.org/SklogWiki/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=129.69.120.36</id>
	<title>SklogWiki - User contributions [en]</title>
	<link rel="self" type="application/atom+xml" href="http://www.sklogwiki.org/SklogWiki/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=129.69.120.36"/>
	<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php/Special:Contributions/129.69.120.36"/>
	<updated>2026-05-01T02:04:00Z</updated>
	<subtitle>User contributions</subtitle>
	<generator>MediaWiki 1.41.0</generator>
	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Rotational_relaxation&amp;diff=19385</id>
		<title>Rotational relaxation</title>
		<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php?title=Rotational_relaxation&amp;diff=19385"/>
		<updated>2016-10-21T06:23:52Z</updated>

		<summary type="html">&lt;p&gt;129.69.120.36: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Rotational relaxation&#039;&#039;&#039; refers to the decay of certain [[autocorrelation]]&lt;br /&gt;
magnitudes related to the orientation of molecules.&lt;br /&gt;
If a molecule has an orientation along a unit vector &amp;lt;math&amp;gt;{\mathbf n}&amp;lt;/math&amp;gt;, its autocorrelation&lt;br /&gt;
will be given by&lt;br /&gt;
:&amp;lt;math&amp;gt;c_1(t)=\langle \mathbf{n}(0)\cdot\mathbf{n}(t) \rangle.&amp;lt;/math&amp;gt;&lt;br /&gt;
From the time decay, or relaxation, of this function, one may extract&lt;br /&gt;
a characteristic relaxation time (either from the long-time exponential decay, or&lt;br /&gt;
from its total integral, see [[autocorrelation]]). This magnitude, which&lt;br /&gt;
is readily computed in a [[Computer simulation techniques |simulation]] is not directly accessible experimentally,&lt;br /&gt;
however. Rather, relaxation times of the second&lt;br /&gt;
[[spherical harmonics|spherical harmonic]] are obtained:&lt;br /&gt;
:&amp;lt;math&amp;gt;c_2(t)=\langle P_2(  \mathbf{n}(0)\cdot\mathbf{n}(t) ) \rangle,&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;P_2(x)&amp;lt;/math&amp;gt; is the second [[Legendre polynomials|Legendre polynomial]].&lt;br /&gt;
&lt;br /&gt;
According to simple [[rotational diffusion]] theory, the relaxation time&lt;br /&gt;
for &amp;lt;math&amp;gt;c_1(t)&amp;lt;/math&amp;gt; would be given by&lt;br /&gt;
&amp;lt;math&amp;gt;\tau_1 = \frac{1}{2D_\mathrm{rot}}&amp;lt;/math&amp;gt;, and the relaxation time for&lt;br /&gt;
&amp;lt;math&amp;gt;c_2(t)&amp;lt;/math&amp;gt; would be &amp;lt;math&amp;gt;\tau_2 = \frac{1}{6D_\mathrm{rot}}&amp;lt;/math&amp;gt;.&lt;br /&gt;
Therefore, &amp;lt;math&amp;gt;\tau_1= 3 \tau_2&amp;lt;/math&amp;gt;. This ratio is actually lower in simulations,&lt;br /&gt;
and closer to &amp;lt;math&amp;gt;2&amp;lt;/math&amp;gt;; the departure from a value of 3 signals rotation&lt;br /&gt;
processes &amp;quot;rougher&amp;quot; than what is assumed in simple [[rotational diffusion]] (Ref 1).&lt;br /&gt;
==Water==&lt;br /&gt;
:&#039;&#039;Main article [[Rotational relaxation of water]]&lt;br /&gt;
Often, molecules are more complex geometrically and can not be described by a single&lt;br /&gt;
orientation. In this case, several vectors should be considered, each with its own&lt;br /&gt;
autocorrelation. E.g., typical choices for [[water]] molecules would be:&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| symbol || explanation || experimental value, and method&lt;br /&gt;
|-  &lt;br /&gt;
| HH   || H-H axis  ||  &amp;lt;math&amp;gt;\tau_2=2.0&amp;lt;/math&amp;gt;ps  (H-H dipolar relaxation NMR)&lt;br /&gt;
|-  &lt;br /&gt;
| OH   || O-H axis  ||  &amp;lt;math&amp;gt;\tau_2=1.95&amp;lt;/math&amp;gt;ps (&amp;lt;sup&amp;gt;17&amp;lt;/sup&amp;gt;O-H dipolar relaxation NMR)&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;\mu&amp;lt;/math&amp;gt; || dipolar axis || not measurable, but related to bulk dielectric relaxation&lt;br /&gt;
|-&lt;br /&gt;
| &amp;lt;math&amp;gt;\perp&amp;lt;/math&amp;gt;   || normal to the molecule plane|| not measurable&lt;br /&gt;
|-&lt;br /&gt;
|}&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Rotational diffusion]]&lt;br /&gt;
*[[Diffusion]]&lt;br /&gt;
*[[Autocorrelation]]&lt;br /&gt;
==References==&lt;br /&gt;
#[http://dx.doi.org/10.1063/1.476482 David van der Spoel, Paul J. van Maaren, and Herman J. C. Berendsen &amp;quot;A systematic study of water models for molecular simulation: Derivation of water models optimized for use with a reaction field&amp;quot;,  J. Chem. Phys. &#039;&#039;&#039;108&#039;&#039;&#039; 10220 (1998)]&lt;br /&gt;
[[Category: Non-equilibrium thermodynamics]]&lt;/div&gt;</summary>
		<author><name>129.69.120.36</name></author>
	</entry>
</feed>