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	<title>Newtons Laws EX 2 - Revision history</title>
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	<entry>
		<id>https://euler.vaniercollege.qc.ca/gwikis/pwiki/index.php?title=Newtons_Laws_EX_2&amp;diff=293&amp;oldid=prev</id>
		<title>imported&gt;Patrick at 18:17, 30 August 2011</title>
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		<updated>2011-08-30T18:17:34Z</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;First we focus on the mass &amp;lt;math&amp;gt;m_2 = 5&amp;lt;/math&amp;gt; kg. There are four forces acting on this particle: &amp;lt;math&amp;gt;F_G&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;F_N&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;F_f&amp;lt;/math&amp;gt;, and &amp;lt;math&amp;gt;F_T&amp;lt;/math&amp;gt; pointing towards the string pulling the block. The particle moves down the incline and therefore the force of friction points up the incline. Similarly, we list forces on the mass &amp;lt;math&amp;gt;m_1 = 10&amp;lt;/math&amp;gt; kg. The force of tension pulls the block towards the left.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
[[image:N_APP_EX_2_SOLNa.png|TOP]]&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The blocks move at constant velocity and therefore their acceleration is zero. We select the x-axis parallel to the incline and parallel to the horizontal surface as shown in the diagram below.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
[[image:N_APP_EX_2_SOLNb.png|TOP]]&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
We will deal with each particle separately. First we focus on the mass &amp;lt;math&amp;gt;m_2 = 2&amp;lt;/math&amp;gt; kg. The gravitational force points vertically down and therefore it makes a 30° angle with the negative y-axis; consequently, it makes an angle -120° with the positive x-axis.&lt;br /&gt;
&lt;br /&gt;
The components of the forces exerted on &amp;lt;math&amp;gt;m_2&amp;lt;/math&amp;gt; are:&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot; cellpadding=&amp;quot;2&amp;quot; style=&amp;quot;text-align:center&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Forces&lt;br /&gt;
! x-component&lt;br /&gt;
! y-component&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F_G&amp;lt;/math&amp;gt;&lt;br /&gt;
| mg cos(-120°) = 50 cos(-120°) = -25 N&lt;br /&gt;
| 50 sin(-120°) = -43 N&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F_N&amp;lt;/math&amp;gt;&lt;br /&gt;
| 0&lt;br /&gt;
| &amp;lt;math&amp;gt;F_N&amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F_f&amp;lt;/math&amp;gt;&lt;br /&gt;
| &amp;lt;math&amp;gt;F_f&amp;lt;/math&amp;gt;&lt;br /&gt;
| 0&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F_T&amp;lt;/math&amp;gt;&lt;br /&gt;
| &amp;lt;math&amp;gt;F_T&amp;lt;/math&amp;gt;&lt;br /&gt;
| 0&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Note that we used &amp;lt;math&amp;gt;g = 10 m/s^2&amp;lt;/math&amp;gt; in our computations.&lt;br /&gt;
&lt;br /&gt;
First we have to deal with the y-component:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;-43 + F_N = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This yields &amp;lt;math&amp;gt;F_N = 43&amp;lt;/math&amp;gt; N&lt;br /&gt;
&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
Now we can proceed to think about the x-component. Using that the acceleration is 0, we can write:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;F_T + F_f - 25 = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
We cannot solve this equation immediately, and so, we focus on the mass &amp;lt;math&amp;gt;m_1 = 10&amp;lt;/math&amp;gt; kg.&lt;br /&gt;
&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
The components of the forces exerted on &amp;lt;math&amp;gt;m_1&amp;lt;/math&amp;gt; are:&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot; cellpadding=&amp;quot;2&amp;quot; style=&amp;quot;text-align:center&amp;quot;&lt;br /&gt;
|-&lt;br /&gt;
! Forces&lt;br /&gt;
! x-component&lt;br /&gt;
! y-component&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F_G&amp;lt;/math&amp;gt;&lt;br /&gt;
| 0&lt;br /&gt;
| -100 N&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F_N&amp;lt;/math&amp;gt;&lt;br /&gt;
| 0&lt;br /&gt;
| &amp;lt;math&amp;gt;F_N&amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F_f&amp;lt;/math&amp;gt;&lt;br /&gt;
| 15 N&lt;br /&gt;
| 0&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F_T&amp;lt;/math&amp;gt;&lt;br /&gt;
| &amp;lt;math&amp;gt;-F_T&amp;lt;/math&amp;gt;&lt;br /&gt;
| 0&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
First we have to deal with the y-component:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;-100 + F_N = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This yields &amp;lt;math&amp;gt;F_N = 100&amp;lt;/math&amp;gt; N.&lt;br /&gt;
&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
Now we can proceed to think about the x-component, and because acceleration is 0, we can write:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;-F_T + 15 = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
There remains only to solve the following system of two equations:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;F_T + F_f - 25 = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;-F_T + 15 = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Solving for &amp;lt;math&amp;gt;F_T&amp;lt;/math&amp;gt;, we find &amp;lt;math&amp;gt;F_T = 15&amp;lt;/math&amp;gt; N and solving for &amp;lt;math&amp;gt;F_f&amp;lt;/math&amp;gt; we find &amp;lt;math&amp;gt;F_f = 10&amp;lt;/math&amp;gt; N.&lt;/div&gt;</summary>
		<author><name>imported&gt;Patrick</name></author>
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