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	<title>Module : Rotational Dynamics - Revision history</title>
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	<updated>2026-04-05T22:01:15Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>https://euler.vaniercollege.qc.ca/gwikis/mechanicsModules/index.php?title=Module_:_Rotational_Dynamics&amp;diff=378&amp;oldid=prev</id>
		<title>Kevin at 00:48, 8 May 2014</title>
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		<updated>2014-05-08T00:48:25Z</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;&amp;#039;&amp;#039;Kreshnik Angoni and Kevin Lenton&amp;#039;&amp;#039;&lt;br /&gt;
&amp;lt;br&amp;gt;&lt;br /&gt;
[http://gauss.vaniercollege.qc.ca/~physics/MechanicsModules/Module%20Worksheets/NYB/MagneticInduction/MagneticInduction.docx Worksheet.docx]&amp;lt;br&amp;gt;&lt;br /&gt;
[http://gauss.vaniercollege.qc.ca/~physics/MechanicsModules/Module%20Worksheets/NYB/MagneticInduction/MagneticInduction.pdf Worksheet.pdf] &amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Other Resources: &amp;lt;br&amp;gt;&lt;br /&gt;
*Haliday &amp;amp; Resnick, Fundamentals of Physics 9.4-11 &lt;br /&gt;
*[http://cnx.org/content/m42155/latest/?collection=col11406/1.7 Openstax]&lt;br /&gt;
* [http://fclass.vaniercollege.qc.ca/~angonik/FOV1-00042F8A/FOV1-0006425E/FOV1-0006425F/LECTURE_11.pdf?FCItemID=S00282F7E Printable version]&lt;br /&gt;
&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===The Moment of Inertia: the rotational equivalent of mass===&lt;br /&gt;
A definition of mass comes from Newton&amp;#039;s second Law: the mass of an object defines how an object will accelerate given a certain linear net force.&amp;lt;br&amp;gt;&lt;br /&gt;
You could say the mass shows you how an object will move. We need an equivalent to describe how an object will &amp;#039;&amp;#039;rotate&amp;#039;&amp;#039;, given a net torques. This equivalent is called the &amp;#039;&amp;#039;The Moment of Intertia&amp;#039;&amp;#039;, given the symbol &amp;#039;&amp;#039;I&amp;#039;&amp;#039;.&amp;lt;br&amp;gt;&lt;br /&gt;
The quantity &amp;#039;&amp;#039;I&amp;#039;&amp;#039; [Units:kg*m2] is called the moment of inertia of the body with respect to the rotation axis. You can tell from the units that the Moment of Inertia is always a mass times radius squared. The exact&lt;br /&gt;
numerical value of I depends on the way that the mass of the body is distributed spatially with respect to &lt;br /&gt;
a particular axis. A quick comparison of expression (22) with K = mv2/2 allows to figure out that, in a &lt;br /&gt;
rotational motion, I is playing the role of the mass for translational motion. So, we can derive that &lt;br /&gt;
&lt;br /&gt;
 The inertia moment is a measure of the resistance a body presents to the change of its rotational &lt;br /&gt;
&lt;br /&gt;
 status of motion or in other terms to its existing angular velocity. &amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
You can get a feel for the moment of inertia by trying to rotate a hammer. If you hold it by the wooden end, and try and spin it (the mass is further away from the pivot i.e. bigger moment of inertia ) it is much more difficult to spin &lt;br /&gt;
than when holding it by the metallic end (more of the mass is closer to the pivot, smaller r, therefore smaller inertia moment). &amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
- Straight from the definition (23) we may see that the same mass &lt;br /&gt;
located at a bigger distance from the axis produces bigger moment &lt;br /&gt;
of inertia. So, one may guess that, for the same mass, the inertia &lt;br /&gt;
moments versus the central axis of symmetry for a ring, a disk, and &lt;br /&gt;
a cylinder (figure 9) are different and Iring &amp;gt;Idisk &amp;gt;Icylinder. &lt;br /&gt;
&amp;lt;br&amp;gt;&lt;br /&gt;
The center of mass CM of the body is a physical concept that &lt;br /&gt;
helps a lot to find I-value for any position of rotation axis. &lt;br /&gt;
&lt;br /&gt;
 &amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Figure 9&lt;/div&gt;</summary>
		<author><name>Kevin</name></author>
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