"Classical field theory and classical mechanics"의 두 판 사이의 차이

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<h5>books</h5>
 
<h5>books</h5>
  
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*   <br>
 
*  Classical mechanics [[2610572/attachments/1142452|Classical_Mechanics.djvu]]V.I. Arnold<br>
 
*  Classical mechanics [[2610572/attachments/1142452|Classical_Mechanics.djvu]]V.I. Arnold<br>
* [http://library.nu/docs/1U9OCRM7QY/Electrodynamics%20and%20Classical%20Theory%20of%20Fields%20and%20Particles Electrodynamics and Classical Theory of Fields and Particles]<br>
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* [[Emmy Noether’s Wonderful Theorem]]<br>
 
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*   <br>[http://library.nu/docs/1U9OCRM7QY/Electrodynamics%20and%20Classical%20Theory%20of%20Fields%20and%20Particles Electrodynamics and Classical Theory of Fields and Particles]<br>
* [[2010년 books and articles]]
 
  
 
 
 
 

2012년 8월 14일 (화) 13:39 판

introduction
  • can be formulated using classical fields and Lagrangian density
  • change the coordinates and fields accordingly
  • require the invariance of action integral over arbitrary region
  • this invariance consists of two parts : Euler-Lagrange equation and the equation of continuity
  • three important conserved quantity
    • energy
    • momentum
    • angular momentum

 

 

notation
  • dynamical variables \(q_{k}, \dot{q}_k\) for \(k=1,\cdots, N\)
  • \(T\) kinetic energy
  • \(V\) potential energy
  • We have Lagrangian \(L=T-V\)
  • Define the Hamiltonian
  • \(H =\sum_{k=1}^{N} p_{k}\dot{q}_{k}-L\)
  • \(p\dot q\) is twice of kinetic energy
  • Thus the Hamiltonian represents \(H=T+V\) the total energy of the system

 

 

Lagrangian formalism

 

 

canonically conjugate momentum
  • canonically conjugate momenta
    \(p_{k}=\frac{\partial L}{\partial \dot{q}_k}\)
  • instead of \(q_{k}, \dot{q}_k\), one can use \(q_{k}, p_{k}\) as dynamical variables

 

 

 

Hamiltonian mechanics

 

 

 

Poisson bracket

For \(f(p_i,q_i,t), g(p_i,q_i,t)\) , we define the Poisson bracket

\(\{f,g\} = \sum_{i=1}^{N} \left[ \frac{\partial f}{\partial q_{i}} \frac{\partial g}{\partial p_{i}} - \frac{\partial f}{\partial p_{i}} \frac{\partial g}{\partial q_{i}} \right]\)

In quantization we have correspondence

\(\{f,g\} = \frac{1}{i}[u,v]\)

 

 

phase space

 

 

하위페이지

 

 

 

links and webpages

 

question and answers(Math Overflow)

 

 

 

history

 

 

related items

 

 

encyclopedia

 

 

books

 

 

expositions
  • Benci V. Fortunato D., Solitary waves in classical field theory, in Nonlinear Analysis and Applications to Physical Sciences