Solving Kinetic Energy with Rotation Around Y Axis

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The discussion focuses on calculating the kinetic energy of a rod rotating around the y-axis. The user initially describes their understanding of kinetic energy in the xy-plane and expresses confusion about incorporating rotation around the y-axis. They derive the position and velocity components for the center of mass, including a translation component in the z-direction. The user questions the correctness of their approach to the kinetic energy formula, particularly regarding the rotation component. Ultimately, they confirm that they have resolved the problem independently.
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Homework Statement


The rod of length 2a swings and it rotates \dot{\phi}[/tex]. Find kinetic energy.<br /> <h2>The Attempt at a Solution</h2><br /> <br /> I know how to find kinetic energy if we have rotation just in xy plane, but I&#039;m having a problem to understand how to do it with rotation around y axis.<br /> <br /> If we have rotation in xy plane:<br /> x_{cm}=asin(\theta)<br /> y_{cm}=acos(\theta)<br /> \dot{x}_{cm}=acos(\theta)\dot{\theta}<br /> \dot{y}_{cm}=-asin(\theta)\dot{\theta}<br /> E_{kin}=\frac{1}{2}m(\dot{x}_{cm}^2+\dot{y}_{cm}^2)+\frac{1}{2}m\cdot\frac{1}{12}(2a)^2\dot{\theta}^2<br /> E_{kin}=\frac{2}{3}m\dot{\theta}^2<br /> <br /> For rotation around y, I assume that we have translation component in z direction, and rotation component.<br /> z_{cm}=asin(\theta)sin(\phi)<br /> Is this correct? (look at the picture)<br /> \dot{z}_{cm}=a(cos(\theta)sin(\phi)\dot{\theta}+cos(\phi)sin(\theta)\dot{\phi})<br /> E_{z}=\frac{1}{2}m\dot{z}_{cm}^2+\frac{1}{2}I_{cm}\dot{\phi}^2.<br /> Rotation part of E_{z} bothers me, maybe I have to multiply it by (lsin(\theta))^2.
 

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Is this ok:

E=\frac{1}{2}(\dot{x}_{cm}^2+\dot{y}_{cm}^2+\dot{z}_{cm}^2)+\frac{1}{2}I_{cm}(\dot{\theta}^2+\dot{\phi}^2)

?
 
Last edited:
I have successfully solved the problem by my self, so no need for an answer.
 

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