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      <pubDate>2018-02-22 13:09:10 UTC</pubDate>
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         <title>Second Law of Thermodynamics</title>
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         <description><![CDATA[<div>Thermodynamics is a branch of physics which deals with the energy and work of a system. Thermodynamics deals only with the large scale response of a system which we can observe and measure in experiments.</div>]]></description>
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         <pubDate>2018-02-22 13:11:24 UTC</pubDate>
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         <description><![CDATA[<div>There exist a useful thermodynamic variable called entropy (S). A natural process that starts in one equilibrium state and ends in another will go in the direction that causes the entropy of the system plus the environment to increase for an irreversible process and to remain constant for a reversible process</div>]]></description>
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         <description><![CDATA[<div>The second law of thermodynamics is a general principle which places constraints upon the direction of <a href="http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/heatra.html#c1">heat transfer </a>and the attainable efficiency of <a href="http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/heaeng.html#c1">heat engines</a>. In so doing, it goes beyond the limitations imposed by the <a href="http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/firlaw.html#c1">first law of thermodynamics</a>. It's implications may be visualized in terms of the waterfall analogy.</div>]]></description>
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         <pubDate>2018-02-22 13:36:45 UTC</pubDate>
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