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		<summary type="html">&lt;p&gt;sp&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;The &amp;#039;&amp;#039;&amp;#039;maximum-term method&amp;#039;&amp;#039;&amp;#039; is a consequence of the large numbers encountered in [[statistical mechanics]]. It states that under appropriate conditions the logarithm of a summation is essentially equal to the logarithm of the maximum term in the summation.&lt;br /&gt;
&lt;br /&gt;
These conditions are (see also proof below) that (1) the number of terms in the sum is large and (2) the terms themselves scale exponentially with this number. A typical application is the calculation of a [[thermodynamic potential]] from a [[partition function (statistical mechanics)|partition function]]. These functions often contain terms with factorials &amp;lt;math&amp;gt;n!&amp;lt;/math&amp;gt; which scale as &amp;lt;math&amp;gt;n^{1/2}n^n/e^n&amp;lt;/math&amp;gt; ([[Stirling&amp;#039;s approximation]]).&lt;br /&gt;
&lt;br /&gt;
==Example==&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\lim_{M\rightarrow\infty} \cfrac{\ln\left({\sum_{N=1}^M N!}\right)}{\ln{M!}} = 1 \ &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Proof==&lt;br /&gt;
Consider the sum&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;S = \sum_{N=1}^M T_N \ &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;T_N&amp;lt;/math&amp;gt;&amp;gt;0 for all &amp;#039;&amp;#039;N&amp;#039;&amp;#039;. Since all the terms are positive, the value of &amp;#039;&amp;#039;S&amp;#039;&amp;#039; must be greater than the value of the largest term, &amp;lt;math&amp;gt;T_{\max}&amp;lt;/math&amp;gt;, and less than the product of the number of terms and the value of the largest term. So we have&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;T_{\max} \le S \le M T_{\max}. \ &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Taking logarithm gives&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\ln T_{\max} \le \ln S \le \ln T_{\max}+\ln M. \ &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As frequently happens in statistical mechanics, we assume that &amp;lt;math&amp;gt;T_{\max}&amp;lt;/math&amp;gt; will be &amp;lt;math&amp;gt;O(\ln M!) = O(e^M)&amp;lt;/math&amp;gt;: see [[Big O notation]].&lt;br /&gt;
&lt;br /&gt;
Here we have&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;O(M) \le \ln S \le O(M)+ \ln M \qquad \Rightarrow&lt;br /&gt;
1 \le \frac{\ln S}{O(M)} \le 1 + \frac{\ln M}{O(M)} = 1 + o(1)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For large &amp;#039;&amp;#039;M&amp;#039;&amp;#039;, &amp;lt;math&amp;gt;\ln M&amp;lt;/math&amp;gt; is negligible with respect to &amp;#039;&amp;#039;M&amp;#039;&amp;#039; itself, and so &amp;lt;math&amp;gt;\ln M/O(e^M) \in o(1)&amp;lt;/math&amp;gt;. Then, we can see that ln &amp;#039;&amp;#039;S&amp;#039;&amp;#039; is bounded from above and below by &amp;lt;math&amp;gt;\ln T_{\max}&amp;lt;/math&amp;gt;, and so&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{\ln S}{O(\ln T_{\max})} = 1\ &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*D.A. McQuarrie, Statistical Mechanics. New York: Harper &amp;amp; Row, 1976.&lt;br /&gt;
*T.L. Hill, An Introduction to Statistical Thermodynamics. New York: Dover Publications, 1987&lt;br /&gt;
&lt;br /&gt;
[[Category:Physical chemistry]]&lt;br /&gt;
[[Category:Statistical mechanics]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{statisticalmechanics-stub}}&lt;br /&gt;
{{physical-chemistry-stub}}&lt;/div&gt;</summary>
		<author><name>2603:8000:D300:3650:AD45:E6EE:7A8:8B7C</name></author>
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