This is exercises about chapter 7, Exercises of Relativity Theory

This is exercises about chapter seven

Typology: Exercises

2025/2026

Uploaded on 04/05/2026

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bg1
7
.
2
since
Gabed
is
like
a
rank- 4
covariant
tensor
;
the
usual
term
:
OnLand-F
....
by
1
.
2
Ambared
=
Ombabed -
Tid
......
-
W
.
Tencased
w
(
-
1)
San
(X)
=
*
God(x)
=
g
=
jg
gabgb"
=
Sa
Fj
=
]
59
Omg
=
Omg)
from
symmetric
matix
,
Ombulg
=
g
Jugga
=>
amFg
=
E
Fggagan
Gabed
=
Fg
Eabed
(scalar
density
of
reight
-
1)
=>
ImWand
=
(Gng) and
=
Eg
g
mSpz
and
Tem
=
Egamgab
-
Wanda
=
FgUmig
&
and
=
o
,
Im
Eg
=
0
while
F
=
T
but
E-e
.
is
antisymmetro
that
is
to
say
:
-
We
+
Temladed
e
:
and
So
Pubravad
=
Ounhabod
+
0
=
0
#
pf3
pf4
pf5
pf8

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since (^) Gabed (^) is like arank- 4 covarianttensor^ ; the (^) usual (^) term : OnLand-F.... by

1.^2

Ambared = Ombabed - Tid (^) ......^ -^ W^. Tencased w (

San (X)^ = * God(x)

g

jg gabgb" = Sa Fj = ] (^59) Omg = Omg)

from

symmetric

matix

, Ombulg = g Jugga =>^ amFg = (^) E Fggagan

Gabed =

Fg Eabed (scalar^ density of (^) reight -

=> ImWand = (Gng) and = Eg g mSpz and (^) Tem = Egamgab

  • Wanda = FgUmig (^) &

and =o

Im Eg

ile (^) F = (^) T but E-e (^). is (^) antisymmetro that (^) is to say :

  • We^ +^ Temladed e: and So (^) Pubravad =^ Ounhabod + 0 = 0

do the^ same^ again to gabed & m (^) gabed = Om gabed (^) de Le Tem gabed 1

(^) 1)

= (^0) + 0 =

n.^8 Is" = ede-exdr-vido"-visited where (^) v = U (t, r) ,

X =^ x^ (t, v)

gr =^ ev ,

gov =^

  • et

,^900

= -^

= -Using

K =^ le-^ e-VErsint)^ by n^.^48 UK^ = (^0) ,

E

check (^) X=^ t, v , 0 , %^ que into^ -

t

: =^ et Vr^ V

r =^ &rv = (^) (

= V'(t

, v) I levi) =^ te't.^ V, +^ = so (^) eq : (evi-ev+ ev^ = 0 v (^) : = (^) tetYr-te *^ +r- rErso z =^ ej eg--ei)

  • [vir-eid, -ro-remo 0 : E =^ Er 25000^ = (^) VSMG 2010

28 :v)^ -^ v'snoooo U = E

· E^ = -vsm % ef :^ ful-vism20^ %)^ =>

here (^) comes T =^ E v'(t, v) ↑= -red si Tee =^ +e^

v'(t, v) No = in =^ Ex(t,^ v)^ I Ti =^ T

  • (^) X T =^ -re To% = (^) cot (^) O

2oX* +^ taX"^

wa +^ Wa = (^50) W =^ - Wha - is^ antisymmetric so (^) it has^3 independant components in (^) 3D (^3) constaus from Wab =^ rotations (^3) ta :^ translations Translations :^ T1.^ X")^ =^ Ex I^ translation about (^) X) T2. Y14^ = by [ 11 y) Ts.^ **

= Gz &^

  • (^1) z) Rotations RI :x()^ = y7z
  • z2y rotation^ about X)

R

: <

= (^) z(2x - XGz [^ -y) R3" (^) y(4) = x by

  • y2x ( (^) - z) let X

X (^) , ... Xo be^ constants so Xa^

= X , 0x + Xa

Gy

+ x30z +

xy(y8z

  • zzy) +^ x5(z7x^ -X(z) + Xo(X(y - y(x) comput [ *** ) , <153] (^2). (^) [Ti

Tjj

= 0 for

is j^ = (^1).^2. 3

[Ri (^) , Rj J

WijkRk =>^ [R, RuJ = Ry = Y(x) [Rn (^) , Rs =^ Ri^ =^ **

& ERs , R,^ FRc = (15)

3 - (^) [Ri

, Tjj

=jaTk = [R,Tz] =^ Ts^ =^ **

S

[Rz

, i1)^

= (^) - T3 =^ -^ T()

[Rc , is]

= T

= (^) ** [Rs

, T2]^

= - T

= -^ *

I [Ps^ , T1]

= Tz = (^) **

/[m

, , Ts]^

= - Tz =^ -^ ** lothers = (^8)

Y" = 2x

** (^) = (^) y8z - zby

M = by

(b) =^ z7x^ = x7z T() = 0z (0) =^ X^ Jy

  • y2x