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	<title>Physics 1</title>
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	<description>Notes, discussion of problems, open questions and other topics related to Physics 1. By Kasper Olsen</description>
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		<title>Physics 1</title>
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		<title>Rotation, Moment of Inertia, Torque and all that..</title>
		<link>http://physics1blog.wordpress.com/2010/11/30/rotation-moment-of-inertia-torque-and-all-that/</link>
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		<pubDate>Mon, 29 Nov 2010 23:00:22 +0000</pubDate>
		<dc:creator>Kasper Olsen</dc:creator>
				<category><![CDATA[Uncategorized]]></category>
		<category><![CDATA[angular momentum]]></category>
		<category><![CDATA[MIT]]></category>
		<category><![CDATA[moment of inertia]]></category>
		<category><![CDATA[rotation]]></category>
		<category><![CDATA[torque]]></category>
		<category><![CDATA[video lecture]]></category>

		<guid isPermaLink="false">http://physics1blog.wordpress.com/?p=234</guid>
		<description><![CDATA[Here are three lectures related to a subject which for good reason has been troubling some students: From rotation of rigid bodies to angular Momentum, moment of Inertia and Torque.  What we usually call &#8220;Impulsmomentsætningen&#8221; (IMS) is in reality just Newton&#8217;s 2. law for rotation, so including Newton&#8217;s 2. law we have the IMS, &#8220;Newton&#8217;s [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=physics1blog.wordpress.com&amp;blog=3726767&amp;post=234&amp;subd=physics1blog&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>Here are three lectures related to a subject which for good reason has been troubling some students: From rotation of rigid bodies to angular Momentum, moment of Inertia and Torque.  What we usually call &#8220;Impulsmomentsætningen&#8221; (IMS) is in reality just Newton&#8217;s 2. law for rotation, so including Newton&#8217;s 2. law</p>
<p><img src='http://s0.wp.com/latex.php?latex=%5CSigma+F+%3D+Ma+%3D+%5Cfrac%7Bdp%7D%7Bdt%7D&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='&#92;Sigma F = Ma = &#92;frac{dp}{dt}' title='&#92;Sigma F = Ma = &#92;frac{dp}{dt}' class='latex' /></p>
<p>we have the IMS, &#8220;Newton&#8217;s 2. law for rotation&#8221;:</p>
<p><img src='http://s0.wp.com/latex.php?latex=%5CSigma+%5Ctau+%3D+I+%5Calpha+%3D+%5Cfrac%7BdL%7D%7Bdt%7D.&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='&#92;Sigma &#92;tau = I &#92;alpha = &#92;frac{dL}{dt}.' title='&#92;Sigma &#92;tau = I &#92;alpha = &#92;frac{dL}{dt}.' class='latex' /></p>
<p>Here <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='p' title='p' class='latex' /> is momentum (also called linear momentum), and <img src='http://s0.wp.com/latex.php?latex=L&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='L' title='L' class='latex' /> is angular momentum, and <img src='http://s0.wp.com/latex.php?latex=I&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='I' title='I' class='latex' /> is the moment of Inertia. Remember that the torque of a force <img src='http://s0.wp.com/latex.php?latex=%5Cvec%7BF%7D&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='&#92;vec{F}' title='&#92;vec{F}' class='latex' /> is <img src='http://s0.wp.com/latex.php?latex=%5Cvec%7B%5Ctau%7D%3D+%5Cvec%7Br%7D%5Ctimes%5Cvec%7BF%7D&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='&#92;vec{&#92;tau}= &#92;vec{r}&#92;times&#92;vec{F}' title='&#92;vec{&#92;tau}= &#92;vec{r}&#92;times&#92;vec{F}' class='latex' />, i.e. a cross-product. In a mechanics problem with rotation, you usually would need both Newton&#8217;s 2&#8242;nd law and IMS to solve it.</p>
<p>Don&#8217;t forget &#8220;rolling without slipping&#8221; of a body with radius R. In this case, you have:</p>
<p><img src='http://s0.wp.com/latex.php?latex=v_%7BCM%7D%3DR%5Comega&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='v_{CM}=R&#92;omega' title='v_{CM}=R&#92;omega' class='latex' />, and <img src='http://s0.wp.com/latex.php?latex=a_%7BCM%7D%3DR%5Calpha&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='a_{CM}=R&#92;alpha' title='a_{CM}=R&#92;alpha' class='latex' />.</p>
<p>The kinetic energy of a body that rolls is,</p>
<p><img src='http://s0.wp.com/latex.php?latex=K+%3D+%5Cfrac%7B1%7D%7B2%7DI_%7BCM%7D%5Comega%5E2%2B%5Cfrac%7B1%7D%7B2%7DMv_%7BCM%7D%5E2&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='K = &#92;frac{1}{2}I_{CM}&#92;omega^2+&#92;frac{1}{2}Mv_{CM}^2' title='K = &#92;frac{1}{2}I_{CM}&#92;omega^2+&#92;frac{1}{2}Mv_{CM}^2' class='latex' />,</p>
<p>the sum of the rotational kinetic energy and the translational kinetic energy.</p>
<p>&#8212; o &#8212;</p>
<span style="text-align:center; display: block;"><a href="http://physics1blog.wordpress.com/2010/11/30/rotation-moment-of-inertia-torque-and-all-that/"><img src="http://img.youtube.com/vi/9A1Zb8109fg/2.jpg" alt="" /></a></span>
<p><strong>Topics covered in this lecture:</strong></p>
<p>Rotation of rigid bodies &#8212; Moment of Inertia &#8212; Parallel axis theorem</p>
<span style="text-align:center; display: block;"><a href="http://physics1blog.wordpress.com/2010/11/30/rotation-moment-of-inertia-torque-and-all-that/"><img src="http://img.youtube.com/vi/ibePFvo22x4/2.jpg" alt="" /></a></span>
<p><strong>Topics covered in this lecture:</strong></p>
<p>Angular momentum &#8212; Torque &#8212; Conservation of angular momentum</p>
<span style="text-align:center; display: block;"><a href="http://physics1blog.wordpress.com/2010/11/30/rotation-moment-of-inertia-torque-and-all-that/"><img src="http://img.youtube.com/vi/EOy1NV21pMY/2.jpg" alt="" /></a></span>
<p><strong>Topics covered in this lecture:</strong></p>
<p>Torque &#8212; Oscillating bodies</p>
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			<media:title type="html">kasperolsen</media:title>
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		<title>Fictitious Force</title>
		<link>http://physics1blog.wordpress.com/2010/10/10/fictitious-force/</link>
		<comments>http://physics1blog.wordpress.com/2010/10/10/fictitious-force/#comments</comments>
		<pubDate>Sun, 10 Oct 2010 20:06:53 +0000</pubDate>
		<dc:creator>Kasper Olsen</dc:creator>
				<category><![CDATA[Uncategorized]]></category>

		<guid isPermaLink="false">http://physics1blog.wordpress.com/?p=330</guid>
		<description><![CDATA[A fictitious force (also called a pseudo force) is an apparent force that acts on all masses in a non-inertial frame of reference, such as a rotating reference frame. So, a fictitious force is one that seems to exist because a frame of reference is accelerated. The forces may be treated algebraically like a real force, but the fictitious forces do [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=physics1blog.wordpress.com&amp;blog=3726767&amp;post=330&amp;subd=physics1blog&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>A <strong>fictitious force</strong> (also called a <strong>pseudo force)</strong><span style="font-size:small;"><span style="font-size:11px;"> </span></span>is an apparent force that acts on all masses in a non-inertial frame of reference, such as a rotating reference frame. So, a fictitious force is one that seems to exist because a frame of reference is accelerated. The forces may be treated algebraically like a real force, but the fictitious forces do not necessarily obey Newton&#8217;s first law.</p>
<p>One example is the <strong>centrifugal force</strong>, another one is the <strong><a href="http://en.wikipedia.org/wiki/Coriolis_force">Coriolis force</a></strong>.</p>
<p><a href="http://en.wikipedia.org/wiki/Fictitious_force">Wikipedia entry</a></p>
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			<media:title type="html">kasperolsen</media:title>
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		<title>Conservation of mechanical energy</title>
		<link>http://physics1blog.wordpress.com/2010/10/03/conservation-of-mechanical-energy-2/</link>
		<comments>http://physics1blog.wordpress.com/2010/10/03/conservation-of-mechanical-energy-2/#comments</comments>
		<pubDate>Sat, 02 Oct 2010 23:00:28 +0000</pubDate>
		<dc:creator>Kasper Olsen</dc:creator>
				<category><![CDATA[Uncategorized]]></category>
		<category><![CDATA[conservation law]]></category>
		<category><![CDATA[experiment]]></category>
		<category><![CDATA[kinetic energy]]></category>
		<category><![CDATA[mechanical energy]]></category>
		<category><![CDATA[MIT]]></category>
		<category><![CDATA[potential energy]]></category>
		<category><![CDATA[video]]></category>

		<guid isPermaLink="false">http://physics1blog.wordpress.com/?p=186</guid>
		<description><![CDATA[Conservation of mechanical energy (potential energy + kinetic energy) discussed in a class given at MIT by Prof. Walter Lewin (course 8.01, Physics I: Classical Mechanics, fall 1999). Motion of car in a loop explained at 23:50, with a (deadly) amusing experiment at 45:40. Topics covered in this lecture: Work &#8211; Conservative forces &#8211; Potential energy &#8211; Kinetic energy &#8211; Mechanical [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=physics1blog.wordpress.com&amp;blog=3726767&amp;post=186&amp;subd=physics1blog&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>Conservation of mechanical energy (potential energy + kinetic energy) discussed in a class given at MIT by Prof. Walter Lewin (course 8.01, <em>Physics I: Classical Mechanics</em>, fall 1999). Motion of car in a loop explained at 23:50, with a (deadly) amusing experiment at 45:40.</p>
<span style="text-align:center; display: block;"><a href="http://physics1blog.wordpress.com/2010/10/03/conservation-of-mechanical-energy-2/"><img src="http://img.youtube.com/vi/CgqBg44azYk/2.jpg" alt="" /></a></span>
<p><strong>Topics covered in this lecture:</strong></p>
<p>Work &#8211; Conservative forces &#8211; Potential energy &#8211; Kinetic energy &#8211; Mechanical energy</p>
<p>(Young and Freedman, chap. 6)</p>
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			<media:title type="html">kasperolsen</media:title>
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		<title>Atwood Machine</title>
		<link>http://physics1blog.wordpress.com/2010/09/30/atwood-machine/</link>
		<comments>http://physics1blog.wordpress.com/2010/09/30/atwood-machine/#comments</comments>
		<pubDate>Thu, 30 Sep 2010 20:26:33 +0000</pubDate>
		<dc:creator>Kasper Olsen</dc:creator>
				<category><![CDATA[Uncategorized]]></category>
		<category><![CDATA[Atwood machine]]></category>
		<category><![CDATA[experiment]]></category>
		<category><![CDATA[mechanics]]></category>
		<category><![CDATA[video]]></category>

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		<description><![CDATA[The Atwood machine was invented in 1784 by, yes Mr. Atwood. Two weights of mass and are connected by a string over a pulley. The acceleration is Here is a demonstration from MIT, USA: Homework: check that the experiment measures an acceleration as given by the equation above.<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=physics1blog.wordpress.com&amp;blog=3726767&amp;post=322&amp;subd=physics1blog&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>The Atwood machine was invented in 1784 by, yes Mr. Atwood. Two weights of mass <img src='http://s0.wp.com/latex.php?latex=M&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='M' title='M' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=m%3CM&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='m&lt;M' title='m&lt;M' class='latex' /> are connected by a string over a pulley. The acceleration is</p>
<p><img src='http://s0.wp.com/latex.php?latex=a+%3D+%5Cfrac%7BM-m%7D%7BM%2BM%7Dg&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='a = &#92;frac{M-m}{M+M}g' title='a = &#92;frac{M-m}{M+M}g' class='latex' /></p>
<p>Here is a demonstration from MIT, USA:</p>
<span style="text-align:center; display: block;"><a href="http://physics1blog.wordpress.com/2010/09/30/atwood-machine/"><img src="http://img.youtube.com/vi/4ovhEkSIqV0/2.jpg" alt="" /></a></span>
<p>Homework: check that the experiment measures an acceleration as given by the equation above.</p>
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			<media:title type="html">kasperolsen</media:title>
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		<title>Circular motion</title>
		<link>http://physics1blog.wordpress.com/2010/09/13/circular-motion/</link>
		<comments>http://physics1blog.wordpress.com/2010/09/13/circular-motion/#comments</comments>
		<pubDate>Mon, 13 Sep 2010 20:40:07 +0000</pubDate>
		<dc:creator>Kasper Olsen</dc:creator>
				<category><![CDATA[Uncategorized]]></category>
		<category><![CDATA[circular motion]]></category>
		<category><![CDATA[MIT]]></category>

		<guid isPermaLink="false">http://physics1blog.wordpress.com/?p=306</guid>
		<description><![CDATA[When an object moves in a circular orbit (of radius ), the acceleration has two components, tangential and radial. The angular speed is defined as , and angular acceleration defined as ( is the angle that measures the movement of the position vector); the two components are then generally: In many cases we work with uniform circular [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=physics1blog.wordpress.com&amp;blog=3726767&amp;post=306&amp;subd=physics1blog&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>When an object moves in a circular orbit (of radius <img src='http://s0.wp.com/latex.php?latex=R&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='R' title='R' class='latex' />), the acceleration has two components, tangential and radial. The angular speed is defined as <img src='http://s0.wp.com/latex.php?latex=%5Comega%3Dd%5Ctheta%2Fdt&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='&#92;omega=d&#92;theta/dt' title='&#92;omega=d&#92;theta/dt' class='latex' />, and angular acceleration defined as <img src='http://s0.wp.com/latex.php?latex=%5Calpha%3Dd%5E2%5Ctheta%2Fdt%5E2&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='&#92;alpha=d^2&#92;theta/dt^2' title='&#92;alpha=d^2&#92;theta/dt^2' class='latex' /> (<img src='http://s0.wp.com/latex.php?latex=%5Ctheta&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='&#92;theta' title='&#92;theta' class='latex' /> is the angle that measures the movement of the position vector); the two components are then generally:</p>
<p><img src='http://s0.wp.com/latex.php?latex=a_%7Btan%7D+%3D+R%5Calpha%2C&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='a_{tan} = R&#92;alpha,' title='a_{tan} = R&#92;alpha,' class='latex' /></p>
<p><img src='http://s0.wp.com/latex.php?latex=a_%7Brad%7D+%3D+R%5Comega%5E2+%3D+%5Cfrac%7Bv%5E2%7D%7BR%7D.&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='a_{rad} = R&#92;omega^2 = &#92;frac{v^2}{R}.' title='a_{rad} = R&#92;omega^2 = &#92;frac{v^2}{R}.' class='latex' /></p>
<p>In many cases we work with <strong>uniform circular motion</strong>, in this case <img src='http://s0.wp.com/latex.php?latex=a_%7Btan%7D%3D0&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='a_{tan}=0' title='a_{tan}=0' class='latex' />.</p>
<span style="text-align:center; display: block;"><a href="http://physics1blog.wordpress.com/2010/09/13/circular-motion/"><img src="http://img.youtube.com/vi/Otmg0-knGtE/2.jpg" alt="" /></a></span>
<p>credit: Prof. Walter Lewin of MIT (course 8.01, Physics I: Classical Mechanics, fall 1999).</p>
<p><strong>Topics covered in this lecture:</strong></p>
<p>Circular Motion &#8211; Centrifuges Moving &#8211; Reference Frames &#8211; Perceived Gravity</p>
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			<media:title type="html">kasperolsen</media:title>
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		<title>How to solve it</title>
		<link>http://physics1blog.wordpress.com/2010/09/12/how-to-solve-it/</link>
		<comments>http://physics1blog.wordpress.com/2010/09/12/how-to-solve-it/#comments</comments>
		<pubDate>Sun, 12 Sep 2010 20:45:03 +0000</pubDate>
		<dc:creator>Kasper Olsen</dc:creator>
				<category><![CDATA[Uncategorized]]></category>
		<category><![CDATA[notes]]></category>
		<category><![CDATA[PDF]]></category>
		<category><![CDATA[Polya]]></category>

		<guid isPermaLink="false">http://physics1blog.wordpress.com/?p=293</guid>
		<description><![CDATA[George Polya (1887-1985) was a Hungarian mathematician. He is famous for work on mathematics education, and for the 4 steps to solve a problem: 1. understand the problem 2. devise a plan 3. carry out the plan 4. look back We can use this method to solve physics problems also. Try it! (It is a good [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=physics1blog.wordpress.com&amp;blog=3726767&amp;post=293&amp;subd=physics1blog&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>George Polya (1887-1985) was a Hungarian mathematician. He is famous for work on mathematics education, and for the <strong>4 steps to solve a problem:</strong></p>
<p><strong>1. understand the problem</strong></p>
<p><strong>2. devise a plan</strong></p>
<p><strong>3. carry out the plan</strong></p>
<p><strong>4. look back</strong></p>
<p>We can use this method to solve physics problems also. Try it! (It is a good idea to make a drawing of the situation in step 1). Single page explaining Polya&#8217;s principles:</p>
<p><a href="http://physics1blog.files.wordpress.com/2010/09/how-to.pdf">how-to</a> [PDF]</p>
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			<media:title type="html">kasperolsen</media:title>
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		<title>Video lectures: 3D Kinematics, projectile motion</title>
		<link>http://physics1blog.wordpress.com/2010/09/06/video-lecture-3d-kinematics-projectile-motion/</link>
		<comments>http://physics1blog.wordpress.com/2010/09/06/video-lecture-3d-kinematics-projectile-motion/#comments</comments>
		<pubDate>Mon, 06 Sep 2010 18:04:44 +0000</pubDate>
		<dc:creator>Kasper Olsen</dc:creator>
				<category><![CDATA[Uncategorized]]></category>
		<category><![CDATA[kinematics]]></category>
		<category><![CDATA[MIT]]></category>
		<category><![CDATA[video lecture]]></category>

		<guid isPermaLink="false">http://physics1blog.wordpress.com/?p=290</guid>
		<description><![CDATA[credit: Prof. Walter Lewin of MIT (course 8.01, Physics I: Classical Mechanics, fall 1999). Topics covered in this lecture: Vectors &#8212; dot product &#8212; cross product &#8212; kinematics &#8212; projectile motion (Young and Freedman, chap. 3)<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=physics1blog.wordpress.com&amp;blog=3726767&amp;post=290&amp;subd=physics1blog&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<span style="text-align:center; display: block;"><a href="http://physics1blog.wordpress.com/2010/09/06/video-lecture-3d-kinematics-projectile-motion/"><img src="http://img.youtube.com/vi/fwNQKjTj-0w/2.jpg" alt="" /></a></span>
<span style="text-align:center; display: block;"><a href="http://physics1blog.wordpress.com/2010/09/06/video-lecture-3d-kinematics-projectile-motion/"><img src="http://img.youtube.com/vi/0OV1E9M9Kkc/2.jpg" alt="" /></a></span>
<p>credit: Prof. Walter Lewin of MIT (course 8.01, Physics I: Classical Mechanics, fall 1999).</p>
<p><strong>Topics covered in this lecture: </strong></p>
<p>Vectors &#8212; dot product &#8212; cross product &#8212; kinematics &#8212; projectile motion</p>
<p>(Young and Freedman, chap. 3)</p>
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			<media:title type="html">kasperolsen</media:title>
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		<title>Interactive simulation: Projectile motion</title>
		<link>http://physics1blog.wordpress.com/2010/09/04/interactive-simulation-projectile-motion/</link>
		<comments>http://physics1blog.wordpress.com/2010/09/04/interactive-simulation-projectile-motion/#comments</comments>
		<pubDate>Sat, 04 Sep 2010 12:15:47 +0000</pubDate>
		<dc:creator>Kasper Olsen</dc:creator>
				<category><![CDATA[Uncategorized]]></category>
		<category><![CDATA[interactive simulation]]></category>
		<category><![CDATA[PhET]]></category>

		<guid isPermaLink="false">http://physics1blog.wordpress.com/?p=267</guid>
		<description><![CDATA[Projectile motion: footballs, humans and pianos &#8211; they all (ideally) move in the same way. Try the interactive simulation by following this link. The equation of motion is just [the simulation is from University of Colorado at Boulder].<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=physics1blog.wordpress.com&amp;blog=3726767&amp;post=267&amp;subd=physics1blog&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p><a href="http://physics1blog.files.wordpress.com/2010/09/projectile-motion-screenshot1.png"><img class="size-full wp-image-270 alignnone" title="Projectile Motion Screenshot" src="http://physics1blog.files.wordpress.com/2010/09/projectile-motion-screenshot1.png?w=490" alt=""   /></a></p>
<p>Projectile motion: footballs, humans and pianos &#8211; they all (ideally) move in the same way. Try the interactive simulation by following <a href="http://phet.colorado.edu/sims/projectile-motion/projectile-motion_en.html">this link</a>. The equation of motion is just</p>
<p><img src='http://s0.wp.com/latex.php?latex=x%3Dx_0%2B%28v_0%5Ccos%5Calpha%29t&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='x=x_0+(v_0&#92;cos&#92;alpha)t' title='x=x_0+(v_0&#92;cos&#92;alpha)t' class='latex' /></p>
<p><img src='http://s0.wp.com/latex.php?latex=y%3Dy_0%2B%28v_0%5Csin%5Calpha%29t-%281%2F2%29g+t%5E2&amp;bg=ffffff&amp;fg=545454&amp;s=0' alt='y=y_0+(v_0&#92;sin&#92;alpha)t-(1/2)g t^2' title='y=y_0+(v_0&#92;sin&#92;alpha)t-(1/2)g t^2' class='latex' /></p>
<p>[the simulation is from University of Colorado at Boulder].</p>
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			<media:title type="html">kasperolsen</media:title>
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			<media:title type="html">Projectile Motion Screenshot</media:title>
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		<title>Equation summaries corrected</title>
		<link>http://physics1blog.wordpress.com/2010/05/23/equation-summaries-corrected/</link>
		<comments>http://physics1blog.wordpress.com/2010/05/23/equation-summaries-corrected/#comments</comments>
		<pubDate>Sun, 23 May 2010 12:02:36 +0000</pubDate>
		<dc:creator>Kasper Olsen</dc:creator>
				<category><![CDATA[Uncategorized]]></category>
		<category><![CDATA[notes]]></category>
		<category><![CDATA[PDF]]></category>

		<guid isPermaLink="false">http://physics1blog.wordpress.com/?p=240</guid>
		<description><![CDATA[Equation summaries for 10020 and 10022 have been corrected to version 1.1: eqsummary10020 [PDF] eqsummary10022 [PDF]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=physics1blog.wordpress.com&amp;blog=3726767&amp;post=240&amp;subd=physics1blog&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>Equation summaries for 10020 and 10022 have been corrected to version 1.1:</p>
<p><a href="http://physics1blog.files.wordpress.com/2010/05/eqsummary100201.pdf">eqsummary10020</a> [PDF]</p>
<p><a href="http://physics1blog.files.wordpress.com/2010/05/eqsummary100221.pdf">eqsummary10022</a> [PDF]</p>
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			<media:title type="html">kasperolsen</media:title>
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		<title>HyperPhysics</title>
		<link>http://physics1blog.wordpress.com/2010/05/11/hyperphysics/</link>
		<comments>http://physics1blog.wordpress.com/2010/05/11/hyperphysics/#comments</comments>
		<pubDate>Tue, 11 May 2010 13:14:29 +0000</pubDate>
		<dc:creator>Kasper Olsen</dc:creator>
				<category><![CDATA[Uncategorized]]></category>
		<category><![CDATA[hyperphysics]]></category>
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		<guid isPermaLink="false">http://physics1blog.wordpress.com/?p=213</guid>
		<description><![CDATA[&#8220;HyperPhysics&#8221; is not science fiction, its science: a nice and simple overview of mechanics, with links to and from different subjects. Try it. HyperPhysics is hosted by the Department of Physics and Astronomy (Georgia State University).<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=physics1blog.wordpress.com&amp;blog=3726767&amp;post=213&amp;subd=physics1blog&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p><a href="http://hyperphysics.phy-astr.gsu.edu/hbase/HFrame.html">&#8220;HyperPhysics&#8221;</a> is not science fiction, its science: a nice and simple overview of mechanics, with links to and from different subjects. Try it.</p>
<p><a href="http://hyperphysics.phy-astr.gsu.edu/hbase/HFrame.html"><img class="alignnone size-full wp-image-216" title="mechconw" src="http://physics1blog.files.wordpress.com/2010/05/mechconw1.gif?w=490&#038;h=327" alt="" width="490" height="327" /></a></p>
<p><em>HyperPhysics is hosted by the Department of Physics and Astronomy (Georgia State University).</em></p>
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			<media:title type="html">kasperolsen</media:title>
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