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	<title>Potential Energy EX 3 - Revision history</title>
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		<title>imported&gt;Patrick at 15:24, 13 August 2011</title>
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		<updated>2011-08-13T15:24:40Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;When released, the block of mass moves down and therefore the gravitational potential energy of the system (Earth-block-spring) decreases. Consequently, the change in gravitational potential energy is negative. While the block slides down some distance &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt;, the spring stretches the same distance. Consequently, the potential energy of the spring increases. The change of the gravitational potential energy can be computed using:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\Delta U = -m g h = -(3)(10) x = -30 x&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
The initial extension of the spring is &amp;lt;math&amp;gt;x_i = 0&amp;lt;/math&amp;gt; and the final extension of the spring is &amp;lt;math&amp;gt;x_f = x&amp;lt;/math&amp;gt;. We can compute the change in potential energy of the spring as follows:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\Delta U = \frac{1}{2} k {x_f}^2 - \frac{1}{2} k {x_i}^2 = \frac{1}{2} k x^2 = 10 x^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
The total potential energy in this case is equal to zero and so&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;math&amp;gt;\Delta U = -30 x + 10 x^2 = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Solving for &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt;, we find &amp;lt;math&amp;gt;x = 3&amp;lt;/math&amp;gt; m.&lt;/div&gt;</summary>
		<author><name>imported&gt;Patrick</name></author>
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