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	<title>Static Equilibrium EX 4 - Revision history</title>
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	<updated>2026-04-20T21:08:42Z</updated>
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		<title>imported&gt;Patrick: Created page with &#039;The rod is being studied. Three forces act on the rod: the tension in the wire &lt;math&gt;F_T&lt;/math&gt;; the load &lt;math&gt;F_L&lt;/math&gt; and the support at the hinge &lt;math&gt;F&lt;/math&gt;. The wire i…&#039;</title>
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		<updated>2011-07-21T06:33:59Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;#039;The rod is being studied. Three forces act on the rod: the tension in the wire &amp;lt;math&amp;gt;F_T&amp;lt;/math&amp;gt;; the load &amp;lt;math&amp;gt;F_L&amp;lt;/math&amp;gt; and the support at the hinge &amp;lt;math&amp;gt;F&amp;lt;/math&amp;gt;. The wire i…&amp;#039;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;The rod is being studied. Three forces act on the rod: the tension in the wire &amp;lt;math&amp;gt;F_T&amp;lt;/math&amp;gt;; the load &amp;lt;math&amp;gt;F_L&amp;lt;/math&amp;gt; and the support at the hinge &amp;lt;math&amp;gt;F&amp;lt;/math&amp;gt;. The wire is 60 cm long and it appears to be horizontal. It is attached in the middle of the rod. Thus, the wire, the wall and the rod form a right angle triangle with hypotenuse 1 m and one side of 60 cm. From this information, we can compute the angle between the rod and the wall:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\cos{\theta} = {0.6 \over 1} = 0.6&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\theta = 53^{\circ}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The diagram below shows the forces and the lever arm for each of the forces. Note that the load acts 2.00 m from the pivot and the wire pulls at a distance 1 m from the pivot. The torque exerted by the support is equal to zero because it acts at the pivot.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
[[image:Helena_Stat_Equil_Ex_4_SolnA.png|TOP]]&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The rod is in equilibrium and so&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;math&amp;gt;\Sigma F_x = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
 &amp;lt;math&amp;gt;\Sigma F_y = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
 &amp;lt;math&amp;gt;\Sigma \tau = 0&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
We will first compute the torques:&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;
! Force&lt;br /&gt;
! Direction&lt;br /&gt;
! Torque&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F_T&amp;lt;/math&amp;gt;&lt;br /&gt;
| CW&lt;br /&gt;
| &amp;lt;math&amp;gt;\tau = -(1) F_T \sin{143^{\circ}} = -0.6 F_T&amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F_L&amp;lt;/math&amp;gt;&lt;br /&gt;
| CCW&lt;br /&gt;
| &amp;lt;math&amp;gt;\tau = (2)(200)\sin{143^{\circ}} = 240 Nm&amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;\Sigma \tau&amp;lt;/math&amp;gt;&lt;br /&gt;
| &lt;br /&gt;
| 0&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt;&lt;br /&gt;
Solving for &amp;lt;math&amp;gt;F_T&amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
 &amp;lt;math&amp;gt;F_T = {240 \over 0.6} = 400 N&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;br&amp;gt;&lt;br /&gt;
Then we will determine the components of the support at the pivot:&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_T&amp;lt;/math&amp;gt;&lt;br /&gt;
| 400 N&lt;br /&gt;
| 0&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F_L&amp;lt;/math&amp;gt;&lt;br /&gt;
| 0&lt;br /&gt;
| -200 N&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;F&amp;lt;/math&amp;gt;&lt;br /&gt;
| &amp;lt;math&amp;gt;-F_x&amp;lt;/math&amp;gt;&lt;br /&gt;
| &amp;lt;math&amp;gt;F_y&amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
! &amp;lt;math&amp;gt;\Sigma \vec{F}&amp;lt;/math&amp;gt;&lt;br /&gt;
| 0&lt;br /&gt;
| 0&lt;br /&gt;
|}&lt;br /&gt;
&amp;lt;br&amp;gt;&lt;br /&gt;
Solving the two equations we find&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\vec{F} = 400 \hat{i} + 200 \hat{j}&amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>imported&gt;Patrick</name></author>
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