<?xml version="1.0" encoding="UTF-8" ?>
  <resource>
  <id>7678</id>
  <path>/www/nrich/html/content/id/7678/</path>
  <resourceTypeID>1</resourceTypeID>
  <last_published>0000-00-00T00:00:00</last_published>
  <indexXML>&lt;?xml version=&quot;1.0&quot; encoding=&quot;UTF-8&quot;?&gt;
&lt;mdoxml version=&quot;1.0&quot;&gt;
&lt;p style=&quot;text-align: justify;&quot;&gt;A man is holding one end of a board and the another end is on a spool with the outer radius $R$ and the inner radius $r$. A board does not slip on the spool and the spool does not slip on the ground. The man starts to move with the board with a speed $u$. &lt;/p&gt;
&lt;p style=&quot;text-align: center;&quot;&gt;&lt;mdo:image alt=&quot;&quot; src=&quot;spool1.bmp&quot; style=&quot;width: 700px; height: 317px;&quot;&gt;&lt;/mdo:image&gt;&lt;/p&gt;
&lt;p style=&quot;text-align: justify;&quot;&gt;1) How long does it take for the man to reach the spool?&lt;/p&gt;
&lt;p style=&quot;text-align: justify;&quot;&gt;2) Find the distance which must be traveled by the man to reach the spool.&lt;/p&gt;
&lt;p style=&quot;text-align: justify;&quot;&gt;3) Find the distance traveled by the man if $r = R$.&lt;/p&gt;
&lt;p style=&quot;text-align: justify;&quot;&gt;4) Calculate the time and the distance if $l = 298$cm, $R = 101$ cm, $r = 86$ cm, $u = 1$m/s.&lt;/p&gt;

&lt;/mdoxml&gt;</indexXML>
  <solutionXML>&lt;?xml version=&quot;1.0&quot; encoding=&quot;UTF-8&quot;?&gt;
&lt;mdoxml version=&quot;1.0&quot;&gt;&lt;p style=&quot;text-align: center;&quot;&gt;&lt;mdo:image alt=&quot;&quot; src=&quot;spool.bmp&quot; style=&quot;width: 400px; height: 181px;&quot;&gt;&lt;/mdo:image&gt;&lt;/p&gt;
&lt;p&gt;1) Suppose that the spool is rotating with an angular speed $\omega$ about a point A. The spool is a rigid body, this means that the angular speed is the same for all points. Write equations for points B and C:&lt;/p&gt;
&lt;p&gt;$$\omega_C = \frac{v_C}{R},      \omega_B = \frac{v_B}{R + r}$$&lt;/p&gt;
&lt;p&gt;but $\omega_B = \omega_C = \omega$ and $v_B = u$ because the board does not slip on the spool. Thus, $v_C = \frac{R}{R+r}u$. This means that the speed at which the man is approching the spool is $v = u - v_C = u - \frac{R}{R+r}u = \frac{r}{R+r}u$. This means that the time needed for the man to reach the spool is $$t = \frac{l}{v} = \frac{l(R+r)}{ru}$$&lt;/p&gt;
&lt;p&gt; 2) The man will travel $s = ut = \frac{l(R+r)}{r}$.&lt;/p&gt;
&lt;p&gt;3) If $r = R$ then $s = 2l$.&lt;/p&gt;
&lt;p&gt;4) Plug numbers to the equations but do not forget to change units, $t = 6.48$s and $s = 6.48$m.&lt;/p&gt;
&lt;p&gt; &lt;/p&gt;&lt;/mdoxml&gt;</solutionXML>
  <noteXML/>
  <clueXML>&lt;?xml version=&quot;1.0&quot; encoding=&quot;UTF-8&quot;?&gt;
&lt;mdoxml version=&quot;1.0&quot;&gt;
&lt;p&gt;Suppose that a cylinder is rotating about a point A with an angular speed $\omega$ and use the fact that an angular speed is the same for all points of the rigid body. &lt;/p&gt;
&lt;p&gt; &lt;/p&gt;
&lt;p&gt;There is another way of solving this problem. Look at the motion of spool as two seperate motions: the spool moves horizontally as its all mass is at point B and rotates about the point B.&lt;/p&gt;
&lt;p&gt; &lt;/p&gt;
&lt;p&gt;The angular speed is the rate of rotation $\omega = \frac{\delta \Theta}{\delta t}$.&lt;/p&gt;

&lt;/mdoxml&gt;</clueXML>
  <canonXML>&lt;?xml version=&quot;1.0&quot; encoding=&quot;UTF-8&quot;?&gt;
&lt;mdoxml version=&quot;1.0&quot;&gt;
&lt;p style=&quot;text-align: center;&quot;&gt;&lt;mdo:image alt=&quot;&quot; src=&quot;spool.bmp&quot; style=&quot;width: 400px; height: 181px;&quot;&gt;&lt;/mdo:image&gt;&lt;/p&gt;
&lt;p&gt;1) Suppose that the spool is rotating with an angular speed $\omega$ about a point A. The spool is a rigid body, this means that the angular speed is the same for all points. Write equations for points B and C:&lt;/p&gt;
&lt;p&gt;$$\omega_C = \frac{v_C}{R},      \omega_B = \frac{v_B}{R + r}$$&lt;/p&gt;
&lt;p&gt;but $\omega_B = \omega_C = \omega$ and $v_B = u$ because the board does not slip on the spool. Thus, $v_C = \frac{R}{R+r}u$. This means that the speed at which the man is approching the spool is $v = u - v_C = u - \frac{R}{R+r}u = \frac{r}{R+r}u$. This means that the time needed for the man to reach the spool is $$t = \frac{l}{v} = \frac{l(R+r)}{ru}$$&lt;/p&gt;
&lt;p&gt; 2) The man will travel $s = ut = \frac{l(R+r)}{r}$.&lt;/p&gt;
&lt;p&gt;3) If $r = R$ then $s = 2l$.&lt;/p&gt;
&lt;p&gt;4) Plug numbers to the equations but do not forget to change units, $t = 6.48$s and $s = 6.48$m.&lt;/p&gt;
&lt;p&gt; &lt;/p&gt;

&lt;/mdoxml&gt;</canonXML>
  <end_user_role>2</end_user_role>
  <difficulty>4</difficulty>
  <keystage1>0</keystage1>
  <keystage2>0</keystage2>
  <keystage3>1</keystage3>
  <keystage4>1</keystage4>
  <keystage4plus>1</keystage4plus>
  <title>Board and spool</title>
  <description>

</description>
</resource>