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	<updated>2026-05-01T15:28:13Z</updated>
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	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Talk:Percolation_analysis&amp;diff=8956</id>
		<title>Talk:Percolation analysis</title>
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		<updated>2009-09-24T08:09:01Z</updated>

		<summary type="html">&lt;p&gt;147.96.6.43: New page: Muy interesante.  There must be something wrong with the energetic definition of bonds since max(0,exp(u)) = exp(u). Posiblemente b=min(1,exp(-u)) ?  lgmac&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Muy interesante.&lt;br /&gt;
&lt;br /&gt;
There must be something wrong with the energetic definition of bonds&lt;br /&gt;
since max(0,exp(u)) = exp(u). Posiblemente b=min(1,exp(-u)) ?&lt;br /&gt;
&lt;br /&gt;
lgmac&lt;/div&gt;</summary>
		<author><name>147.96.6.43</name></author>
	</entry>
	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=1-dimensional_Ising_model&amp;diff=7840</id>
		<title>1-dimensional Ising model</title>
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		<updated>2009-02-19T17:05:06Z</updated>

		<summary type="html">&lt;p&gt;147.96.6.43: minor index change&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;1-dimensional Ising model&#039;&#039;&#039; is an [[Ising Models| Ising model]] that consists of  a system with &amp;lt;math&amp;gt; N &amp;lt;/math&amp;gt; spins in a row. The energy of the system is given by&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;  U = -J \sum_{i=1}^{N-1} S_{i} S_{i+1} &amp;lt;/math&amp;gt;, &lt;br /&gt;
&lt;br /&gt;
where each variable &amp;lt;math&amp;gt; S_j &amp;lt;/math&amp;gt; can be either -1 or +1.&lt;br /&gt;
&lt;br /&gt;
The [[partition function]] of the system will be:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; Q_N = \sum_{\Omega^N }  \exp \left[ K \sum_{i=1}^{N-1} S_i S_{i+1}  \right]&amp;lt;/math&amp;gt;, &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt; \Omega^N &amp;lt;/math&amp;gt; represents the possible configuration of the N &#039;&#039;spins&#039;&#039; of the system,&lt;br /&gt;
and &amp;lt;math&amp;gt; K = J/k_B T &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; Q_{N} = \sum_{S_1} \sum_{S_2} e^{K S_1S_2} \sum_{S_3} e^{K S_2 S_3} \cdots \sum_{S_{N-1}} e^{K S_{N-2} S_{N-1}}\sum_{S_{N}} e^{K S_{N-1} S_{N} }&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Performing the sum of the possible values of &amp;lt;math&amp;gt; S_{N} &amp;lt;/math&amp;gt; we get:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; Q_{N} = \sum_{S_1} \sum_{S_2} e^{K S_1S_2} \sum_{S_3} e^{K S_2 S_3} \cdots \sum_{S_{N-1}} e^{K S_{N-2} S_{N-1}} \left[ 2 \cosh ( K S_{N-1} ) \right]&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Taking into account that &amp;lt;math&amp;gt; \cosh(K) = \cosh(-K) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; Q_{N} = \sum_{S_1} \sum_{S_2} e^{K S_1S_2} \sum_{S_3} e^{K S_2 S_3} \cdots \sum_{S_{N-1}} e^{K S_{N-2} S_{N-1}} \left[ 2 \cosh ( K ) \right]&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Therefore:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; Q_{N} = \left( 2 \cosh K \right) Q_{N-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; Q_N = 2^{N} \left( \cosh K \right)^{N-1} \approx ( 2 \cosh K )^N &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The [[Helmholtz energy function]] in the [[thermodynamic limit]] will be&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; A = - N k_B T \log \left( 2 \cosh K \right) &amp;lt;/math&amp;gt;&lt;br /&gt;
==References==&lt;br /&gt;
# Rodney J. Baxter  &amp;quot;Exactly Solved Models in Statistical Mechanics&amp;quot;, Academic Press (1982)  ISBN 0120831821 Chapter 2 (freely available [http://tpsrv.anu.edu.au/Members/baxter/book/Exactly.pdf pdf])&lt;br /&gt;
[[Category: Models]]&lt;/div&gt;</summary>
		<author><name>147.96.6.43</name></author>
	</entry>
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