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<record version="1" id="288">
 <title>cylindrical coordinate motion example of generalized coordinates</title>
 <name>CylindricalCoordinateMotionExampleOfGeneralizedCoordinates</name>
 <created>2008-07-18 20:25:21</created>
 <modified>2008-07-18 20:25:21</modified>
 <type>Example</type>
<parent id="286">generalized coordinates  for free motion</parent>
 <creator id="1" name="bloftin"/>
 <modifier id="1" name="bloftin"/>
 <author id="1" name="bloftin"/>
 <classification>
	<category scheme="msc" code="45.20.-d"/>
 </classification>
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 <content>As an example let us get the equations in cylindrical coordinates

$$
 x=r\cos\phi, \,\,\,\,\,\, y=r\sin\phi, \,\,\,\,\,\, z=z,
$$

$$
T=\frac{m}{2} \left[\dot{r}^{2}+r^2\dot{\phi}^{2}+\dot{z}^{2} \right].
$$

$$
\frac{\partial T}{\dot{r}}=m\dot{r},
$$

$$
\frac{T}{\partial r}=m r\dot{\phi}^{2},
$$

$$
\frac{\partial T}{\partial\dot{\phi}}=mr^{2}\dot{\phi},
$$
$$
\frac{\partial T}{\partial \dot{z}}=m\dot{z}.
$$

$$
\delta_{r}W=m \left[\ddot{r} - r\dot{\phi}^{2} \right] \delta r=R\delta r,
$$

$$
\delta_{\phi}W=m\frac{d}{dt} \left(r^{2}\dot{\phi}\right)\delta\phi=\Phi r\delta\phi,
$$

$$
\delta_z W= m \ddot{z} \delta z = Z \delta z;
$$

or 

$$m \left[ \frac{d^{2}r}{dt^{2}}-r \left(\frac{d\phi}{dt}\right)^{2}\right]=R,$$

$$
\frac{m}{r}\frac{d}{dt}\left(r^{2}\frac{d\phi}{dt}\right)=\Phi,
$$
$$
m\frac{d^{2}z}{dt^{2}}=Z.
$$</content>
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