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

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4번째 줄: 4번째 줄:
 
* change the coordinates and fields accordingly
 
* change the coordinates and fields accordingly
 
* require the invariance of action integral over arbitrary region
 
* require the invariance of action integral over arbitrary region
 +
* this invariance consists of two parts : Euler-Lagrange equation and the equation of continuity
  
 
 
 
 
20번째 줄: 21번째 줄:
  
 
*  current density <math>J_{\mu}</math> satisfies<br><math>\partial^{\mu} J_{\mu}=0</math><br>
 
*  current density <math>J_{\mu}</math> satisfies<br><math>\partial^{\mu} J_{\mu}=0</math><br>
*  conserved quantity<br><math>G:=\int_V J_0(x) \,d^3 x</math><br>  <br>
+
we get a conserved quantity<br><math>G:=\int_V J_0(x) \,d^3 x</math><br>
 +
* Lagrangian can be used to express the current density explicity
 +
 
 +
 
  
 
 
 
 

2010년 3월 3일 (수) 18:44 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

 

 

Euler-Lagrange equation
  • if field satisfies the equation of motion, EL is satisfied

 

 

equation of continuity
  • current density \(J_{\mu}\) satisfies
    \(\partial^{\mu} J_{\mu}=0\)
  • we get a conserved quantity
    \(G:=\int_V J_0(x) \,d^3 x\)
  • Lagrangian can be used to express the current density explicity

 

 

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