Special relativity
imported>Pythagoras0님의 2014년 1월 5일 (일) 01:05 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
- http://en.wikipedia.org/wiki/Lorentz_transformation
- one-dimensional example
\[E_{tt}-E_{zz}=0\]
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
\[R_{\mu \nu} - {1 \over 2}g_{\mu \nu}\,R + g_{\mu \nu} \Lambda = {8 \pi G \over c^4} T_{\mu \nu}\]
하위페이지
encyclopedia
- http://en.wikipedia.org/wiki/Newton's_law_of_universal_gravitation
- http://en.wikipedia.org/wiki/Einstein_field_equations
- http://en.wikipedia.org/wiki/Solutions_of_the_Einstein_field_equations
- http://en.wikipedia.org/wiki/Lorentz_covariant
- http://en.wikipedia.org/wiki/Four-vector
books
expositions
articles
- On the electrodynamics of moving bodies
- A. Einstein, 1905
blogs and webpage
- Introduction to Differential Geometry and General Relativity
- Lecture Notes by Stefan Waner