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Group ResearchRelativistic Motions around a Black Hole
2010 KIAS-SNU Physics Winter CampDate : February 7, 2010Talk : 주부경, 조창우, 김은찬, 서윤지, 고성문, 노대호
Table
• What is space-time ?
• How a particle moves?
- As a geometry
• The black-hole
• ?
What is space-time ?Space + Time (additional dim)
성기오빠!한화리조트
215호에서 만나
215호? 알았어 !!
< 2134ft, N37, E128 >
한화리조트 215호
< t, 2134ft, N37, E128 >
Additional Dimension
t = t성기 연아 t t성기 연아≠
How a particle moves?As a Geometry
Action - Euclidian Space
2 2 2
2 2 2
ds dx dy dz
dx dy dz dtdt dt dt
= + +
⎛ ⎞ ⎛ ⎞ ⎛ ⎞= + +⎜ ⎟ ⎜ ⎟ ⎜ ⎟⎝ ⎠ ⎝ ⎠ ⎝ ⎠
∫ ∫
∫
Action - Euclidian Space
• Euler – Lagrange Equation
0d L Ldt xx
•
⎛ ⎞∂ ∂− =⎜ ⎟
⎜ ⎟ ∂∂⎝ ⎠
0v•
→ =
Action – In special relativity
2 2 2 2 2 2d dt dx dy dz dSτ− = − + + + =
2d dS dx dxμ νμντ τ η= = − = −∫ ∫ ∫
1 0 0 00 1 0 00 0 1 00 0 0 1
μνη
−⎛ ⎞⎜ ⎟⎜ ⎟=⎜ ⎟⎜ ⎟⎝ ⎠
dx dx d Ldd d
μ ν
μνη σ σσ σ
→ − =∫ ∫
Action - In special relativity
• Euler – Lagrange Equation
0d L Ld xx
μμσ •
⎛ ⎞∂ ∂⎜ ⎟ − =⎜ ⎟ ∂∂⎝ ⎠
⇒
Action – In general relativity
2d dS g dx dxμ νμντ τ= = − = −∫ ∫ ∫
( )?gμν =dx dxg d Ldd d
μ ν
μν σ σσ σ
→ − =∫ ∫
The black holeExtremely curved space-time
Schwarzschild metric
22 2 2 2 2 2 2
2
2
2(1 ) ( sin )21
GM drds c dt r d dGMc rc r
θ θ ϕ= − − + + +−
Q=0, S=0, Massive
Constant of motion
2
2 2 2
2 2 22
2 3
2(1 )( )
( )
1 ( ) ( ) ( )
1 1 ( )2 2 2
ttt
t rtt rr
M dte u g ur d
dl u g u rd
u u g u g u g u
e dr M l Mlm d r r r
φφφ
φφφ
ξτ
φητ
ετ
= − ⋅ = − = −
= ⋅ = =
⋅ = − = + +
−→ = = − + −
Radial motion
2
2 2
0, 1
10 ( )2
1 ( ) ( )t rtt rr
l e
dr Md r
u u g u g u
τ
= =
= −
⋅ = − = +
Near the horizon
12(1 )
2 2(1 )
dt Md rdr M Mdr dt
d ddt r r
τ
τ τ
−= −
= = − −
2dr Md rτ
= −
Event horizon
Eddington-Finkelstein coordinates
2 lo g 12
rt r MM
υ= − − −
2 2 2 2 2 22(1 ) 2 ( sin )Mds d d dr r d dr
υ υ θ θ φ= − − + + +
22(1 ) 2 0M d d drr
υ υ− − + =
( )const ingoing radial light raysυ =
2(1 ) 2 0M d drr
υ− − + =
2( 2 log 1)2rr M constM
υ − + − =
•
1/23/2 1/2
* 1/2
2 ( 2 ) 12 [ ( ) 2( ) log ]3 2 2 ( 2 ) 1
r r r Mt t MM M r M
+= + − − +
−
22 2 2 2 2 2 2
2(1 ) ( sin )
(1 )
M drds dt r d dMrr
θ θ ϕ= − − + + +−
Reissner–Nordström metric
Q≠0, S=0, Massive
Eddington again…
2~2
2~ ~2 2
~ ~
2
22
~
ln( )
1
(1 ) 2 (1 ) 0
1 , ( ) ( )
111
Mt t M r Mr M
h f
ds h d t hd t dr h dr
t r const d t drM dr dtdt dr Mr M dr fr
r
d t hdr hdtdr f
= + − −−
≡ −
= − − + + + =
+ = → = −
→ = − = − = −− −
+=
−
=
We need elevator
Black Hole
Reference
• Wikipedia– Key Word
Black hole, Action Principle, General Relativity, Metric, Lagrangian, etc
• Google– Key Word
Black hole & charged, space-time
• Book– Gravity (J.B.Hartle)– Introducing Einstein`s Relativity (Ray D’Inverno)