<?xml version="1.0" encoding='utf-8'?>
<!DOCTYPE wml PUBLIC "-//WAPFORUM//DTD WML 1.1//EN" "http://www.wapforum.org/DTD/wml_1.1.xml">
<wml>
<card id="card1" title="N-body problem - Page 15 - Wikipedia">
<p>
<a accesskey="1" href="page.php?w=n-body_problem&amp;p=14">1.Previous</a><br />
<a accesskey="3" href="page.php?w=n-body_problem&amp;p=16">3.Next</a>
</p>
<p>for gravitational systems. If  is the total mass and  a characteristic size of the system (for example, the radius containing half the mass of the system), then the critical time for a system to settle down to a dynamic equilibrium is</p>

<p><big> Special cases </big></p>
<p><big> Two-body problem </big></p>
<p>Any discussion of planetary interactive forces has always started historically with the two-body problem. The purpose of this section is to relate the real complexity in calculating any planetary forces. Note in this Section also, several subjects, such</p><p>
<a accesskey="1" href="page.php?w=n-body_problem&amp;p=14">1.Previous</a><br />
<a accesskey="3" href="page.php?w=n-body_problem&amp;p=16">3.Next</a>
</p>

<do type="prev" label="Search">
        <go href="search.wml"/>
</do>

</card>
</wml>
