AstroNuclPhysics ® Nuclear Physics - Astrophysics - Cosmology - Philosophy | Gravity, black holes and physics |
Chapter 2
GENERAL THEORY OF
RELATIVITY
- PHYSICS OF GRAVITY
2.1. Acceleration and gravity from the point
of view of special theory of relativity
2.2. Versatility - a basic property and the key to understanding
the nature of gravity
2.3. The local principle of
equivalence and its consequences
2.4. Physical
laws in curved spacetime
2.5. Einstein's
equations of the gravitational field
2.6. Deviation
and focus of geodesics
2.7. Gravitational
waves
2.8. Specific
properties of gravitational energy
2.9.Geometrodynamic system of units
2.10. Experimental
verification of the theory of relativity and gravity
2.2. Universality - the basic property and the key to understanding the nature of gravity
Law of
free fall, inertia and gravitational mass
In §1.2 " Newton's law of gravitation " we have shown that the combination of the laws
of classical mechanics with the law of general gravity results in
a remarkable property of universal gravity on the motion of
bodies . regardless of their mass (which
disappears from the equation of motion - it will be shortenes) . Thus,
Galilei already had the basic key to understanding the nature of
gravity in its law of free fall, according to which all bodies
fall to the ground with the same acceleration regardless of their
composition and weight. This specific property of gravity, now
called universality, has long remained virtually unnoticed. Only
Albert Einstein understood that it is the universality
of gravitational action that is the most important property of
gravity, and he drew the appropriate physical consequences from
it and thus built his general
theory of relativity as the physics of gravity and the
properties of space-time.
^{ }The weight of a body manifests itself in
physical phenomena in essentially three ways, and we can
distinguish three types of mass accordingly :
According to Newton's
law of action and reaction, in Newton's theory of gravity, the active and passive gravity are the same . Here so far we notice only the
inertial and passive gravitational masses; we will consider the
gravitational field as given (already"finished") (the question of excitation of the gravitational field
will be discussed in §2.5 " Einstein's
equations of the gravitational field ") .
^{ }The
material test particle will move in the gravitational field
according to the equation
d ^{2
}r m _{s} ------ = m _{t} . grad j . dt ^{2} |
(2.4) |
In other words, the universality of gravitational action here says that for each body the inertial and gravitional mass are the same: m _{s} = m _{t} (more precisely, these masses are proportional and the unit proportionality constants, ie the equality of both masses, is achieved by a suitable choice of units) . The masses in equation (2.4) are then truncated and the motion in the gravitational field is given by the equation d^{2}r/dt^{2} = grad j , which in accordance with the criterion of universality does not contain any individual characteristics of the moving body.
Experience and accurate measurements (see below) show that the inertia and gravity are indeed the same for all bodies. Such equality does not follow from Newton's theory, from its point of view it is a remarkable coincidence that cannot be explained or justified in any way. In Newton's theory, gravity describes a completely different property of bodies than inertial mass. Gravitational mass expresses the ability of a given body to gravitationally attract to other material objects, while the inertial mass characterizes the "resistance" of a given body against to mechanical acceleration with respect to an inertial system. Only Einstein's general theory of relativity, based on the properties of spacetime, explains this equality of inertia and gravity in a completely natural way.
Composing inertial and
gravitational forces
The fact that gravitational and inertial forces have the same
physical nature and can be composed together can
be clearly illustrated by a simple imaginary experiment (which can be realized in practice without any problems)
. We will prepare a railway wagon with a
perfectly flat floor and ceiling, with closed doors and windows.
With the help of a locomotive, we will run it on a straight
smooth track at a constant speed (for example, 80 km / h). We
place a heavy billiard ball on the carriage surface and release a
balloon filled with hydrogen or helium. As long as the wagon is
moving at a constant speed, the ball will lie in a certain place
on the floor and the balloon will float above it in a certain
place on the ceiling. When the wagon starts to brake,
it begins to move forward on the floor due to
the inertia of the ball . Surprisingly, we see that the balloon
began to move in the opposite direction across the ceiling, backwards
against the movement of the wagon. However, this is not because
the law of inertia does not apply to the balloon. The reason is
that the inertial forces created by braking combined
with the gravitational forces from the Earth - a
"sloping" gravitational field was created, as if the
wagon were tilted forward. In this resulting (changed)
gravitational field, the balloon is lightened, according to
standard Archimedes' law, not vertically upwards, but in
a somewhat oblique direction, and begins to move backwards. If we
performed this experiment in a vacuum, of course, the balloon
would move in the same direction as the sphere (and he did not float to the ceiling, but he was rolling
on the floor ...) .
Gravity
and kinematics of motion
Thus, in a gravitational field, all bodies move with the same
acceleration, regardless of their composition and mass. Different
bodies thrown from the same point with the same (vector) velocity
will move along exactly the same trajectories. This versatility,
as noted by Einstein, is strikingly similar to the universality of kinematics . We will shed light on this key
aspect of gravity in the imaginary experiment according to
Fig.2.3. Imagine for a moment that there is no gravity and freely
through space (engine off) moves rocket, in whos cabin one
observer performs mechanical experiments; the second observer it
watches from the outside through the transparent wall of the
cabin._{
}
^{ }If the indoor experimenter places, for
example, a lead ball and a feather motionless next to each other
at a certain "height" above the cabin floor, the two
bodies will always "hang" next to each other at rest
relative to the rocket floor; the same will be seen by the
outside observer. However, if the engines start and the rocket
starts to move with constant acceleration, the situation will
change. The inner observer will feel the "weight" and
will see that all the bodies fall to the cabin floor. If he
doesn't know about the rocket engines running, he says:
"There's a force field in my cabin in which all the bodies
fall with the same acceleration." The feather and the lead
ball hit the cabin floor exactly at the same time, although their
composition and weight are very different. He remembers Galileo's
law of free fall and says: "This force field is a
gravitational field. Probably my rocket is
on the surface (or leaning
against the surface - the situation in Fig. 2.4) of a planet that
is the source of the gravitational field that I observe."
Fig.2.3. An imaginary experiment showing the
"imitation" of a gravitational field in an accelerated
frame of reference.
a) In the cabin of a rocket moving freely in
space without gravity, Newton's law of inertia applies.
b) After turning on the rocket engines, the
experimenter will feel heavy inside the cabin and all bodies
(metal ball and feather) will fall to the floor with the same
acceleration - from the point of view of the internal observer,
there is a gravitational field in the cabin.
c) From the point of view of an external
observer, however, there is no "real" gravitational
field in the cabin, the equally accelerated movements of all
bodies relative to the floor and walls of the cabin are a
kinematic effect in the non-inertial frame of reference.
Note: In this
imaginary experiment, of course, we assume that there is a vacuum
in the free space and inside the cabin (the spacesuit is not
drawn); the same in Fig.2.4.
However, the outside observer laughs at him because he has a different explanation: "There is no gravitational field inside the cabin! The inside observer feels the weight because it is accelerated with the cabin by the force of rocket engines. The lead ball and feather remain in place but the floor began to move against them with acceleration. That the ball and the feather collide with the floor at the same time is from a kinematic point of view evident . No gravity, but a non-inertial frame of reference in which an apparent field of inertial forces acts. "
We can imagine the opposite situation (Fig.2.4), when the rocket cabin is supported by a longer rod on the surface of a planet. The experimenter inside the cabin will again observe that all bodies fall to the floor with the same acceleration and may consider this a consequence of the presence of a gravitational field with universal effects. However, if he recalls a dispute with an outside observer in the previous case, he may submit also other justification: "My rocket is in free space without gravity, but the rocket engines are turned on, that the entire racket uniformly accelerating. The heaviness which I feel is the inertial resistance of my body weight against acceleration, falling bodies with the same acceleration is kinematic effect in non-inertial system. "
Compared to the previous case, however, there is a certain difference, which is still insignificant, but will play an important role in the next. The second explanation will be physically equivalent to the first explanation only locally , within a sufficiently small cabin. The gravitational field around the planet is inhomogeneous - its intensity decreases with height above the surface and the direction is always to the center of the planet. Therefore, if the cabin were too large, the inside observer would find that bodies at a higher height above the floor fall with slightly less acceleration than bodies closer to the floor, and the direction of fall of bodies in one corner of the cabin is somewhat different from the direction of fall in the opposite corner of the cabin. This behavior would no longer be explained by the accelerated movement of the cabin without gravity. Under the term "locally" will be understood in the following "in a sufficiently small region of spacetime, where the given gravitational field can be considered homogeneous".
Fig.2.4.
An imaginary experiment showing the local
indistinguishability of inertial and gravitational
forces. a) An observer inside a cabin supported by a fixed rod against the surface of a gravitational planet will observe a gravitational field with universal effects, in which both the lead ball and the light feather will fall with the same acceleration and fall to the floor at the same time. However, he could explain the same with the rocket engines running and the accelerated movement of the cabin; however, the outside observer will not agree. b) After removing the support rod, the cab with all objects inside will fall freely, there will be a state of weightlessness. The outside observer, of course, explains this by a free fall in a gravitational field, while the inner observer can equally consider his cabin to be inertial without gravity. |
If we remove the
supporting rod in Fig.2.4, the rocket will start to fall to the
surface of the planet in a free fall. Because all bodies,
regardless of their composition and weight, fall in the
gravitational field with the same acceleration, their mutual
acceleration in the cabin will be zero - a state of
weightlessness will be created. A feather and a lead bullet still
remain "hanging" side by side at the same height above
the floor booths y. The inner experimenter declares:
"My cabin is an inertial system that moves freely in space
without gravity." However, an outside observer (connected to
the planet) has a different explanation: "The rocket's cabin
and all its bodies inside fall freely in the planet's
gravitational field. and with the cab, so that they shall be at
peace with their floors and walls . " A cabin falling freely
in a gravitational field is inertial to the inner observer, but
again only locally inertial, because the gravitational field is
inhomogeneous and thus inertiality is achieved in different
places by different accelerations of free fall *).
*) All the above conclusions
will also apply to (the fate of the inner observer far more
favorable!) Variant, where instead of free fall to the surface,
we choose the orbital motion of the 1st cosmic velocity around
the planet. Such a state of weightlessness, caused by the
universal compensation of gravitational and centrifugal forces,
was immediately tested by all astronauts.
Which of the two observers described in the imaginary experiments is right? Internal or external? Whatever will perform any local (within the cab) mechanical experiments, it is possible to completely equally explain how the presence of the gravitational field, or by the action of inertial forces in a non-inertial frame of reference. In such a non-inertial frame of reference (eg in the cabin of an accelerating rocket) we observe a field of "inertial forces", which for the external observer is of purely kinematic origin (and therefore "apparent"), but for the internal observer it is a real field having all the properties of the gravitational field - a universal effect on all events. Conversely, a real (ie, excited by some matter, eg around a planet or star) gravitational field has locally the same properties as an inertial force field in a non-inertial system.
Equivalence principle - the
universality of gravity
Inertia and gravity are therefore in a sense, two pages of the
same coin: what one observer considers as inertia, for another
observer is gravity, and vice versa. Gravitational
and inertial forces cannot be distinguished from
each other by any local experiment (there is no "local indicator"
for them). We can thus express the
so-called principle of equivalence :
Theorem 2.1 (principle of equivalence) |
The motion of bodies in a gravitational field is locally equivalent to the motion in a non-inertial frame of reference without gravity. |
The principle of
equivalence can also be formulated as : The trajectory of a body when moving in a gravitational field depends exclusively on its initial position and velocity, not on its structure, composition or other properties. |
The consequence of the
principle of equivalence is the indistinguishability between gravitational and
inertial phenomena: acceleration and gravity are manifested in
the same way, so the theory of accelerating systems (which is a general theory of relativity in the narrower
sense) is also a
theory of gravity. The fact of the equivalence of inertial and
gravitational mass, which for a long time was considered a
coincidence, was elevated by Einstein to the basic law of gravity and the basis
of his general theory of relativity.
Comment:
Sometimes differentiate two or three levels of the
equivalence principle ^{ }:
- Weak equivalence principle- the
gravitational action of bodies does not depend on their mass and
composition, the gravitational and inertial mass of bodies is
equivalent (it is mutually proportional,
with a suitable choice of units it is identical) .
- Strong principle of equivalence applies
not only to mechanical but also to electromagnetic processes. The
mass corresponding to the energy of the electromagnetic field (as well as other interactions) should
also have gravitational effects , see below.
^{ }At the beginning of the construction of GTR, A.
Einstein proceeded from the weak principle of equivalence, and
then gradually switched to its extension to electromagnetic
processes. The current GTR is based on the strong principle
of equivalence .
^{ }The principle of equivalence
expresses the effect of the "already finished"
gravitational field on material objects. V 2.5 "Einstein's
equation of the gravitational field "we generalize it to the universality of
excitation of the gravitational field by all
matter-energy, regardless of its composition and nature. This
completes the general theory of relativity as the physics of
gravity and (curved) spacetime.
An important question
arises as to whether the universality of gravitational action is
limited to mechanical phenomena or applies to all physical processes. An indirect
indication in favor of the second possibility is already given by
the fact that bodies of very different
composition
fall in a gravitational field with the same
acceleration
. This finding of Galileo was verified by experiments by Eötvös
(at the beginning of our century) with an accuracy of 10 ^{-8} , Dicke et al. (r.1963) with an accuracy
of 10 ^{-11} [220] and Braginský et al. (r.1977) with
an accuracy of 10 ^{-12} [31]. Bodies of different
composition have different representations of electrons, protons
and neutrons, different proportions of mass, eg of
electromagnetic origin .Thus, if we measure the same
inertial and gravitational mass for bodies of different
composition, we can say that the gravitational field has the same
effect on protons, neutrons, electrons and on the electromagnetic
field itself. The effect of the gravitational field on light,
resp. on electromagnetic waves, was also directly experimentally
verified - gravitational spectral shift ( §2.4 " Physical
laws in curved spacetime
", passage " Gravitational frequency shift " ) and curvature of light rays in
the gravitational field ( §4.3 " Schwarzschild
static black holes ",
passage " Deflection
of particles and light in the Schwarzschild field " ) .
^{ }The inertial mass of atoms
is given mainly by the following components :
a) The rest mass of protons and neutrons; b)
Rest mass of electrons; c) The binding potential
energy of protons and neutrons in the atomic nucleus caused by
strong nuclear interactions; d) Potential
electrostatic energy of electrons and electrostatic energy of the
nucleus; e) Kinetic energy of electrons, protons
and neutrons; f) Effects related to vacuum
polarization (formation of virtual particle-antiparticle pairs); g)
Energy of weak interactions between nucleons in nuclei; h)
Gravitational energy.
^{ }The contributions of strong, electromagnetic, weak
and gravitational interactions to the mass of an object are in
the ratio:
- for an atom about 1:10 ^{-2} : 10 ^{-12} : 10 ^{-40} ; - for macroscopic bodies about 1: 10 ^{-2} : 10 ^{-12} : 10 ^{-29} ; - for a star with
the mass of the Sun 1: 10 ^{-2} : 10 ^{-12} : 10 ^{-16} .
^{ }Verified by Eötvös, Dicke and Braginsky
measurements (with an accuracy of 10 ^{-12}) equality of inertial and gravitational mass for
platinum (78 protons and electrons, 117 neutrons) and aluminum
(13 protons and electrons, 14 neutrons) shows in a more detailed
analysis that the principle of equivalence is verified for the
rest mass of protons and neutrons with an accuracy of 10 ^{-11} and for an electron
mass of about 10 ^{-8} . For the mass related to the nuclear binding energy of
nucleons, the kinetic energy of nucleons in the nucleus (related
to the Pauli principle) and the electrostatic energy of the
nucleus, the verification of the principle of equivalence with an
accuracy of ~ 10 ^{-9} to 10 ^{-10} applies . The potential an kinetic energy of electrons,
accuracy is 10 ^{-6} to 10 ^{-7} .
Antimatter:
gravitates or antigravitates
?^{
}
The basic pillar of Einstein's GTR
principle of equivalence says that the action
of gravity does not depend on the composition and structure of
matter . The gravitational interaction between matter
and antimatter should be identical . An object
made of antimatter will thus fall in the gravitational field of
the Earth with the same acceleration as a body made of matter (here on the surface of the Earth its fall will take
place with a known value of the gravitational acceleration of
9.81 m/s ^{2}
) . The law of free fall and the principle
of equivalence are very accurately verified for ordinary
matter^{ } composed of atoms consisting of
electrons, protons and neutrons. Logically, we conclude that it
also applies to individual elementary particles - ordinary
(electrons, protons, neutrons), and probably also exotic
(neutrinos, mesons, hyperons, ...). However, direct experimental
verification of gravitational properties of individual isolated
particles is very difficult (if not
impossible) , because these particles move
at high speeds and show electromagnetic and strong interactions
with the environment, much stronger than gravitational (discussed in the section " Antiparticles -
antiatoms - antimatter - antisworlds ", paragraph"
Artificial production of antimatter "in the book" Nuclear physics and physics
of ionizing radiation ") .
But as is the case with antiparticles (positrons,
antiprotons, antineutrons), "antiatoms"
composed of them and in general in antimatter
*)? We know from experiments on accelerators that particles and
antiparticles have the same inertial mass . But
will antimatter gravitate or antigravity
? The analysis of the probabilities of short-term existence of
virtual electron-positron, proton-antiproton and other particle
pairs ("vacuum polarization") shows that the results of
Eötvös, Dicke and Bragin measurements confirm the validity of
the principle of equivalence for common antiparticles (such as
positron and antiproton) with accuracy 10 ^{-5} to 10 ^{-6} . So certainly for antimatter can not expect
"antigravity" - no " falling
up "! Antimatter will normally gravitate
- it is not yet precisely measured whether with the same or
slightly different gravitational constant than ordinary matter
..? ..
*) On the issue of antimatter see §1.5,
passage " Antiparticles -
antiatomy - antimatter - antisworlds " in the book " Nuclear physics and
physics of ionizing radiation ".
^{ }Experimental uncertainties about the gravitational
properties of antiparticles and antimatter leave some room for hypotheses
with a slightly different gravitational force of
antimatter from ordinary matter.
In some alternative or generalized theories of
gravity, other fields and interactions are introduced (eg in Kaluza-Klein's 5-dimensional unitary
theory of gravity + electromagnetism - §B.2, part " 5-dimensional
gravity-electromagnetism
") , which in the quantum approach can
be related to intermediate quantum-particles. In
addition to the standard "tensor" graviton
with spin 2, there is a "vector" gravifoton with
spin 1 and also a " graviscalar " with spin 0.
These contributions can be a source of violation of the
equivalence principle. The consequence would be that the
gravitational potential between two static mass objects m _{1} and m _{2} at a distance r
would have an anomalous course :
V (r) = - G . ^{m} 1 ^{. }^{m} 2 /_{r }. (1+ F . e^{- }^{r
/ d }) ,
where in addition to the standard Newtonian gravitational
potential G.m _{1} .m _{2} / r, the Yukawa potential e ^{- }^{r
/ d} with range d also appears . F is
the scaling constant of this complementary interaction, which
could hypothetically differ slightly "+/-" for matter
and antimatter..?..
^{ }It can therefore be said that the
principle of equivalence is with relatively high accuracy^{ }proven for strong and electromagnetic
interactions. With weak interaction, the contribution to the
total mass of the body is relatively very small (of the order of
about 10 ^{-12} ), the accuracy of these
experiments is not sufficient to completely reliable verification
of the equivalence principle, however some indications in favor
of its validity for weak interactions, exist here[105]. Regarding
the principle of equivalence for the gravitational interaction,
these experiments do not provide any information on the
gravitational properties of gravitational energy (ie whether
gravitational energy contributes equally to inertial and
gravitational mass), because its share in the total mass of
conventional macroscopic bodies is negligible ( ~ 10^{-30} ). However, with increasing weight and
compactness, the relative contribution of gravitational energy to
the total mass of the body increases. For large planets like
Jupiter it is already 10 ^{-8} , for the Sun 10 ^{-6} ; for massive compact formations
such as white dwarfs or neutron stars is the width you
much higher. Comparison of real astronomically observed
trajectories of such bodies with orbits predicted by celestial
mechanics, or relativistic astrophysics, confirm the validity of
the equivalence principle for gravitational energy, so far not
with very high accuracy ...
Cosmic verification of the
law of free fall
The current space technology makes it possible, at least
in principle, to verify the principle of equivalence in direct
relation to Galileo's experiments with free fall. Instead of a
short track from the legendary Leaning Tower of Pisa, however, a
very long "free fall" would be used to orbit the
spacecraft around Earth many times over. In principle, the
principle of such an arrangement can be seen from Figure 2.3a
above. In the cabin of a satellite orbiting freely in a
gravitational field around the Earth, two test specimens of
different compositions are freely placed in a weightless state.
If the principle of equivalence applies, both bodies will orbit
in the same geodetic path, their mutual position will not
change even after a large number of cycles. For accurate
verification, of course, the arrangement could not be as trivial
as in Fig. 2.3a, where an asymmetric gravitational attraction
between the test specimens, objects in the cabin and with its
walls would be manifested. The arrangement would have to be
exactly symmetrical - concentric or coaxial, the position of the
test specimens would be evaluated not visually, but by electronic
sensing.
^{ }An experiment of this kind
was designed in 1972 by experts from the University of Stanford
under the leadership of P.W.Worden under the name STEP
( Satellite Test Equivalence Principle ). Using
precision technology and sensitive methods of sensing the
position of test specimens, the principle of equivalence could be
verified in this way with an accuracy of up to 10 ^{-18}. So far, only a
model of the device has been created, the actual experiment in
orbit will hopefully be carried out after 2000.
^{ }The most accurate verification of the
validity of the principle of equivalence for all kinds of
interactions and in the widest possible range of physical
situations is very important, because the whole
general theory of relativity as the physics of space-time and
gravitation, is based on the very exact validity of the principle
of equivalence for all physical phenomena (ie
absolute universality of gravitational interaction) . The slightest reliably detected
deviation would shake this theory in the very foundations ..!..
Gravity -
the only absolutely universal force
Gravity acts on all bodies, but also on energy - on all fields,
because the physical field has energy and thus also mass that can
"gravitate". So gravity is the only universal force that acts on absolutely everything in
this world!
^{ }The universality of gravitational action
is a basic property that distinguishes gravity from all other
types of forces in nature. The fields of gravitational and
inertial forces are equivalent for all physical processes, the
same physical laws apply to them and are therefore completely indistinguishable from each other locally . From the point
of view of the general theory of relativity, it can be said that
the inertial and gravitational forces have the same^{ }the (common) physical nature; in
the following paragraphs we will see that this common essence is
the geometric properties of
spacetime .
^{ }The versatility of gravity allowed us to convert gravity to
kinematics. Kinematics is an expression of the geometric
properties of space and time. Thus, we can expect in advance that
if gravity changes the kinematics, it will also change the
geometric properties of space and time. The statement about the universal
action of gravity on all physical phenomena, expressed in
Einstein's principle of equivalence, thus has far-reaching
consequences and is the basis of Einstein's general theory of
relativity.
General theory
of relativity and the essence of gravity
The question of whether the general theory of relativity explains
the essence of gravity cannot be answered other than: yes and no ! The general theory of relativity
converted gravitational action into inertial motion - it combined
gravity and inertia, identifying them with the geometric
properties of spacetime. It converts the laws that govern gravity
into the laws that govern space-time. Thus, unifying
relationships between previously separated phenomena were
discovered. To the question of the cause of
gravitational action, the general theory of relativity answers
with curved spacetime, but does it not explain why bodies in their vicinity curve spacetime?
The general theory of relativity shows how
, but not why.
The only complete answer (but from the opposite side) could
perhaps be given by a consistent unitary
field theory - see the individual chapters of Appendix B
" Unitary field theory ". To the deepest foundation of all "why?"
and "what's next?" but we probably
won't get it anyway ..?..
2.1. Acceleration and gravity from the point of view of special theory of relativity | 2.3. Local principle of equivalence |
Gravity, black holes and space-time physics : | ||
Gravity in physics | General theory of relativity | Geometry and topology |
Black holes | Relativistic cosmology | Unitary field theory |
Anthropic principle or cosmic God | ||
Nuclear physics and physics of ionizing radiation | ||
AstroNuclPhysics ® Nuclear Physics - Astrophysics - Cosmology - Philosophy |