Intermediate Mechanics:Central Force Motion

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{{Start Hierarchy|link=Course Wikis|title=Course Wikis}}
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{{Hierarchy Item|link=Physics Course Wikis|title=Physics Course Wikis}}
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{{Hierarchy Item|link=Intermediate Mechanics|title=Intermediate Mechanics}}
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Second coolest equation ever (T&M 8.21):
 
Second coolest equation ever (T&M 8.21):
  
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<math>u = \frac{1}{r}</math>
 
<math>u = \frac{1}{r}</math>
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==Central Force Orbits==
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<math>
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\frac{\alpha}{r} = 1 + \epsilon \cos \theta
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</math>
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<math>
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\epsilon = \sqrt{1 + \frac{2 E L^2}{m K^2}}
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</math>
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{| border="1" cellpadding="5" cellspacing="0"
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|+'''Central Force Motion Orbits'''
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!<math>\epsilon</math> value
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!Orbit Type
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!Energy Value
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|-
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|<math>\epsilon = 0 </math>
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| Circle
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|
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|-
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|<math>0 < \epsilon < 1 </math>
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| Ellipse
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|<math>E < 0 </math>
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|-
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|<math>\epsilon = 1 </math>
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| Parabola
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|<math>E = 0 </math>
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|-
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|<math>\epsilon > 1 </math>
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| Hyperbola
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|<math>E > 0 </math>
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|}

Latest revision as of 22:06, 13 March 2006

Course Wikis > Physics Course Wikis > Intermediate Mechanics

Second coolest equation ever (T&M 8.21):

\frac{\partial u}{\partial \dot{\theta}} + u = -\frac{\mu r^2}{l^2}F(r)

u = \frac{1}{r}

Central Force Orbits


\frac{\alpha}{r} = 1 + \epsilon \cos \theta


\epsilon = \sqrt{1 + \frac{2 E L^2}{m K^2}}

Central Force Motion Orbits
ε value Orbit Type Energy Value
ε = 0 Circle
0 < ε < 1 Ellipse E < 0
ε = 1 Parabola E = 0
ε > 1 Hyperbola E > 0
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