Metric tensor in General Relativity
by
Halo Anwar Abdulkhalaq
May, 2016
University of Sulaimani
School of Science education
Physics department
Overview
• Introduction
• Euclidian Metric
• Minkowski Metric
• Metric in General relativity
1- General form
2- Schwarzschild Metric
3- Some more Metrics
• Use for Einstein field equations
• Summary
Introduction
• Metric tensor (Metric) is an important quantity in General
relativity.
• Sometimes it is thought of as alternative of Newton’s
gravitational potential .
• It is in fact the geometrical representation of space or space-
time.
• Metric is considered to be basic block of Einstein's equations
of field.
• It can be calculated from the line element (the distance
between two points in space or space-time).
Euclidian Metric
• To understand metric it is useful to start with simplest line
element.
• Distance between two points in two or three dimension in
space is called Euclidian geometry:
And in 3-D:
• The metric components of the above line element are (1,1,1),
they are the coefficients of the coordinates (dx, dy, dz).
222
yxs 
222
dydxds 

2222
dzdydxds 
Minkowski Metric
• This is the combination between Euclidean 3-D space with
time.
• The line element here represents the distance between two
events:
• This can be written in general form as:
• Hence:
,
• Here conventional units have been used, where (c=1) and
Einstein summation convention been applied.
22222
dzdydxdtds 
232221202
)()()()( dxdxdxdxds 

 dxdxds 2
3,2,1,0
• So the Minkowski metric is (-1,1,1,1).
• And it can be written as a 4x4 matrix:













1000
0100
0010
0001

Metric in General relativity
1. General form:
,
In matrix notation:
In flat geometry:

 dxdxgds 2
3,2,1,0













33323130
23222120
13121110
03020100
gggg
gggg
gggg
gggg
g
 g
2- Schwarzschild Metric:
• It is written as:
• It is actually driven from spherical coordinate
line element.
• The metric components are:
222222122
sin)
2
1()
2
1(  drdrdr
r
M
dt
r
M
ds  






















22
2
1
sin000
000
00)
2
1(0
000)
2
1(
r
r
r
M
r
M
g
3- Some more Metrics:
• Eddington-Finkelstein
• Kruskal-Szekeres
• Friedman-Robertson-Walker
Einstein field equations
• Field equations are set of equations relate geometry to
matter.
• According to these equations gravity is geometry.
• They are as follow:
where is Einstein tensor given by:
• To solve these equations we need to follow this pattern:
 GTG 8
G
 RgRG
2
1



 GRgds 2
• The ricci tensor is written in terms of the
spacetime connection:
• The spacetime connection is directly written in
terms of the metric tensor:











  ,,R
)(
2
1
,,, 

 gggg 
Summary
• Metric tensor is key factor in Einstein's theory of general
relativity.
• It can be calculated from line element.
• By having metric tensor the spacetime connection can be
calculated.
• From spacetime connection Ricci tensor and Ricci scalar are
determined.
• Finally, from Ricci tensor and scalar Einstein tensor will be
evaluated which is final step of solving field equations.
References
• T. Clifton, P.G. Ferreira, A. Padilla, and C. Skordis. Modied gravity and
cosmology. Phys.Rept., 513:1, 2012.
• S.M.Carroll. Spacetime and Geometry: An Introduction to General Rel-
ativity. Chicago, Addison Wesley, 2004.
• C.W. Misner, K.S. Throne, and J.A. Wheeler. Gravitation. Freeman,1973.
• H. Stephani. Relativity: An Introduction to Special and General Relativity.
3id edition, 2004.
• B.F.Schutz. A First Course in General Relativity. Cambridge University Press,
2nd edition, 2009.
• http://gfm.cii.fc.ul.pt/events/lecture_series/general_relativity/gfm-
general_relativity-lecture4.pdf
Thanks for your attendance
and
Happy to hear your questions

Metric tensor in general relativity

  • 1.
    Metric tensor inGeneral Relativity by Halo Anwar Abdulkhalaq May, 2016 University of Sulaimani School of Science education Physics department
  • 2.
    Overview • Introduction • EuclidianMetric • Minkowski Metric • Metric in General relativity 1- General form 2- Schwarzschild Metric 3- Some more Metrics • Use for Einstein field equations • Summary
  • 3.
    Introduction • Metric tensor(Metric) is an important quantity in General relativity. • Sometimes it is thought of as alternative of Newton’s gravitational potential . • It is in fact the geometrical representation of space or space- time. • Metric is considered to be basic block of Einstein's equations of field. • It can be calculated from the line element (the distance between two points in space or space-time).
  • 4.
    Euclidian Metric • Tounderstand metric it is useful to start with simplest line element. • Distance between two points in two or three dimension in space is called Euclidian geometry: And in 3-D: • The metric components of the above line element are (1,1,1), they are the coefficients of the coordinates (dx, dy, dz). 222 yxs  222 dydxds   2222 dzdydxds 
  • 5.
    Minkowski Metric • Thisis the combination between Euclidean 3-D space with time. • The line element here represents the distance between two events: • This can be written in general form as: • Hence: , • Here conventional units have been used, where (c=1) and Einstein summation convention been applied. 22222 dzdydxdtds  232221202 )()()()( dxdxdxdxds    dxdxds 2 3,2,1,0
  • 6.
    • So theMinkowski metric is (-1,1,1,1). • And it can be written as a 4x4 matrix:              1000 0100 0010 0001 
  • 7.
    Metric in Generalrelativity 1. General form: , In matrix notation: In flat geometry:   dxdxgds 2 3,2,1,0              33323130 23222120 13121110 03020100 gggg gggg gggg gggg g  g
  • 8.
    2- Schwarzschild Metric: •It is written as: • It is actually driven from spherical coordinate line element. • The metric components are: 222222122 sin) 2 1() 2 1(  drdrdr r M dt r M ds                         22 2 1 sin000 000 00) 2 1(0 000) 2 1( r r r M r M g
  • 9.
    3- Some moreMetrics: • Eddington-Finkelstein • Kruskal-Szekeres • Friedman-Robertson-Walker
  • 10.
    Einstein field equations •Field equations are set of equations relate geometry to matter. • According to these equations gravity is geometry. • They are as follow: where is Einstein tensor given by: • To solve these equations we need to follow this pattern:  GTG 8 G  RgRG 2 1     GRgds 2
  • 11.
    • The riccitensor is written in terms of the spacetime connection: • The spacetime connection is directly written in terms of the metric tensor:              ,,R )( 2 1 ,,,    gggg 
  • 12.
    Summary • Metric tensoris key factor in Einstein's theory of general relativity. • It can be calculated from line element. • By having metric tensor the spacetime connection can be calculated. • From spacetime connection Ricci tensor and Ricci scalar are determined. • Finally, from Ricci tensor and scalar Einstein tensor will be evaluated which is final step of solving field equations.
  • 13.
    References • T. Clifton,P.G. Ferreira, A. Padilla, and C. Skordis. Modied gravity and cosmology. Phys.Rept., 513:1, 2012. • S.M.Carroll. Spacetime and Geometry: An Introduction to General Rel- ativity. Chicago, Addison Wesley, 2004. • C.W. Misner, K.S. Throne, and J.A. Wheeler. Gravitation. Freeman,1973. • H. Stephani. Relativity: An Introduction to Special and General Relativity. 3id edition, 2004. • B.F.Schutz. A First Course in General Relativity. Cambridge University Press, 2nd edition, 2009. • http://gfm.cii.fc.ul.pt/events/lecture_series/general_relativity/gfm- general_relativity-lecture4.pdf
  • 14.
    Thanks for yourattendance and Happy to hear your questions