"Special relativity"의 두 판 사이의 차이

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imported>Pythagoras0
imported>Pythagoras0
6번째 줄: 6번째 줄:
 
** four momentum $(m,mv_1,mv_2,mv_3)$
 
** four momentum $(m,mv_1,mv_2,mv_3)$
 
** electromagnetic field
 
** electromagnetic field
 
 
  
 
   
 
   
101번째 줄: 99번째 줄:
 
* http://gigapedia.com/items/45025/relativity-demystified---a-self-teaching-guide--2005-12
 
* http://gigapedia.com/items/45025/relativity-demystified---a-self-teaching-guide--2005-12
  
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==expositions==
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* [http://webs.morningside.edu/slaven/Physics/gr/ General relativity:a very weird world]
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==articles==
 
==articles==

2014년 1월 5일 (일) 02:05 판

four-vector

  • can be transformed by Lorentz transformation
  • examples
    • space-time $(ct,x,y,z)$
    • four momentum $(m,mv_1,mv_2,mv_3)$
    • electromagnetic field


review of Maxwell's equation



Lorentz transformation and Maxwell's equation

\[E_{tt}-E_{zz}=0\]


Vacuum field equation and gravitational field equation

  • gravitational potentail satisfies the following equation (Poisson's equation)

\[\nabla^2 \phi = - 4 \pi G \rho\]

  • \(\rho\) is the matter density
  • in relativity theory, the metric plays the role of gravitational potential



energy-momentum tensor

  • also called as stress-energy tensor
  • describe the densities and flows of energy and momentum
  • all forms of mass-energy can be sources of gravitational fields
  • the stress-energy tensor \(T_{\mu \nu}\) acts as a source of the gravitational field




relativistic Vacuum field equation

relativistic matter field equation

\[R_{\mu \nu} - {1 \over 2}g_{\mu \nu}\,R + g_{\mu \nu} \Lambda = {8 \pi G \over c^4} T_{\mu \nu}\]




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