AstroNuclPhysics ® Nuclear Physics - Astrophysics - Cosmology - Philosophy | Gravity, black holes and physics |
Chapter 1
GRAVITATION AND ITS PLACE IN PHYSICS
1.1. Historical development of knowledge
about gravity
1.2. Newton's law of gravitation
1.3. Mechanical LeSage hypothesis of the
nature of gravity;
1.4. Analogy between gravity and
electrostatics
1.5. Electromagnetic field. Maxwell's equations.
1.6. Four-dimensional spacetime and
special theory of relativity
1.5. Electromagnetic field. Maxwell's equations.
In the previous §1.4 we
saw that the analogy between Newton's gravistatics and Coulomb's
electrostatics is very tight. However, the electrostatic field is
a special case of the general electromagnetic field that prevails in the
vicinity of moving electric charges. It is therefore useful to
note the properties of the electromagnetic field and to try to
find possible analogies with the general "gravidynamic"
field around moving bodies. Electrodynamics is the most perfect and
successful theory of classical physics, which retains its full
validity even in modern relativistic physics. It can be said that
electrodynamics is one of the
cornerstones of all physics and has played a key role in shaping both
the special and general theory of relativity.
Note:The historical development of
knowledge about electricity and magnetism is briefly outlined in
§1.1 in the passage " Electrodynamics,
atomic physics, theory of relativity, quantum physics ". The relativistic view of the relationship
between electric and magnetic fields is briefly discussed below
in the section " Relativistic Electromagnetism ", and in more detail in the references cited
therein.
In an electromagnetic field, a total force ( Lorentz force ) acts on a test particle with a charge q moving at a velocity v
F =
q . E + q .
(1/c) [ v ´ B ] , electric force magnetic force |
(1.30) |
where E is the intensity of the electric field and B is the intensity of the magnetic field for historical reasons called magnetic induction, " x " means the vector product. In field theory, the distribution of electric charges is expressed by the charge density r (x, y, z, t), which is generally a function of place and time, so that the total charge contained in the spatial region V is Q = _{V }òòò r dV. The motion of electric charges is described by the current density j (x, y, z, t) º r . v , where v is the instantaneous velocity of charges at that point (x, y, z); electric current flowing through a given surface S then I = _{S }òò j dS. The law of conservation of electric charge then states that the change in charge contained in each given spatial area V must be equal to the amount of charge that passes through the closed surface S = ¶ V surrounding this area:
(1.31a) |
Using Gauss's theorem, the well-known equation of continuity follows
div j + ¶r / ¶ t = 0 , | (1.31b) |
expressing the law of conservation of electric charge in differential form.
Act excitation electric field by electric charges, i.e. fundamental Coulomb's law (1.22a) §1.4 above can be expressed in the form of Gaussian sentences electrostatics (obr.1.3a)
(1.32a) |
where the differential equation derives from
div E = 4 p r . | (1.32b) |
Fig.1.3. Excitation of electric and magnetic fields by electric
charges and currents.
a ) The total
electric charge Q contained in the space inside any closed
surface S is given by the
Gauss sentences flux of the electric field E over the closed surface S .
b ) circulation of the vector magnetic field B
around the closed curve C
is proportional to the total electric current I flowing
through the surface S bounded
by the curve C .
c ) The
electromagnetic field excited by a system of moving electric
charges is given by the distribution of charges and currents
,retarded, always by the time
required by the field to overcome the distance r - r
'from the individual places dV'
of the system to the examined place r .
Strong electric fields under many millions of
volts can be generated in nature and in electronic applications.
For interest, we can give a small discussion, what is the
strongest electric field that can be achieved? :
What is the strongest
electric field can be? ^{ }
In classical (non-quantum) physics, the electric field in a
vacuum can be arbitrarily strong, almost to infinity (in a material environment, however, this is limited by
the electrical strength of the dielectric) .
From the point of view of quantum electrodynamics ,
however, even in vacuum there is a fundamental limitation caused
by the existence of mutual antiparticles of
electron and positron : it is not possible to
create an electric field with an intensity stronger than E _{e} - _{e} += m _{e }^{2} c ^{3} / eh = 1.32 .
10 ^{16} V / cm, where m _{e} is the rest mass of the electron or positron. When this
intensity is exceeded, the potential gradient is higher than the
threshold energy 2m _{e} c ^{2} and a pair of electrons and positrons
is formed, which automatically reduces the intensity of the
electric field. Such a strong electric field has not yet been
created, with conventional electronics this is not possible;
strong impulses from extremely powerful lasers could be a certain
possibility in the future ...
At the end of §1.6, in the passage " Nonlinear electrodynamics", a purely theoretical model of classical
relativistic nonlinear electrodynamics will be discussed.
The magnetic field is excited by moving electric charges, ie electric current , according to the Biot-Savart-Laplace law
d B = (1 / c). I. [d l ´ r ] / r ^{3} , | (1.33a) |
where d 1 is the element of the length of the conductor through which the stationary electric current I flows and r is the polar vector directed from this current element to the examined point. Ampere's law follows from Biot-Savart 's law
(1.33b) |
according to which the curve integral (circulation) of the magnetic induction vector along any closed curve C is proportional to the total current flowing through the surface S , which this curve surrounds (Fig. 1.3b).
The integral on the left side of Ampere's law depends only on the curve C = ¶ S, so for equation (1.33b) to be generally valid, the area integral on the right side must be the same for all surfaces S having the curve C behind the contour . Using Gauss sentences can be easily shown that this is only fulfilled if div j = 0, i.e. when it is the stationary electric current that does not cause changes in the distribution of electric charge in the vicinity of the curve C . For general non-stationary currents, it is therefore necessary to generalize Equation (1.33b) to be compatible with the continuity equation. Substituting in the equation of continuity (1.31b), which also applies to non-stationary currents, for r from equation (1.32b), we get
div [ j + (1/4 p) ¶ E / ¶ t] = 0.
This vector is found, j + ^{1}/_{4 }_{p} ¶ E / ¶ T whose divergence is always equal to zero, and that in the stationary case, coincides with a normal density "conductive" stream j . The expression j_{Maxw} = (1/4 p) ¶ E / ¶ t is called the Maxwell displacement current and can exist even in a vacuum without the presence of real electric charges. Maxwell proposed in the case of a non-stationary field in equation (1.33b) to replace the current density j with the vector j + (1/4 p) ¶ E / ¶ t , or stated the hypothesis that the displacement current has the same magnetic effects as the normal "conductive" current of real electric charges :
(1.34a) |
The magnetic field is thus excited by the total effective current
I_{ef} = nn j dS + nn (1/4p) ¶E/¶t dS . conductive current Maxwell displacement current |
(1.35) |
Maxwell's hypothesis proved to be very correct and fully corresponds to all experiences with electromagnetic phenomena. Maxwell displacement current is, for example, the current that "exceeds" the insulating layer of capacitors and causes their "conductivity" for alternating currents. If we have a planar capacitor with a plate surface S , then between the intensity of the homogeneous electric field in the gap and the charge of the capacitor q, the relation E = 4 p q / S holds , so that the instantaneous current flowing through the capacitor I = ¶ q / ¶ t = S. (1 / 4 p) ¶ E / ¶ t = S. j _{Maxw} is given by Maxwell current.
The displacement current, which - although not formed by the motion of real electric charges - has normal magnetic effects, finds its analogy in the gravitational field, where even in a vacuum without real material bodies there is effective Isaacson energy and gravitational wave momentum , which has gravitational effects (curvature spacetime) like any other matter (see §2.7-2.8).
By converting the integral along the curve C using the Stokes theorem to the integral over the surface S surrounded by this curve, we obtain the equation of excitation of the magnetic field by an electric current (conductive and sliding) in a differential form
rot B = (4 p / c) j + (1 / c) ¶ E / ¶ t. | (1.34.b) |
From this equation it is clear that the magnetic field can be created not only by the movement (current) of electric charges, but also by a time-varying electric field .
Another basic law of electromagnetism is the knowledge that magnetic field lines are continuous and closed curves . In other words, the magnetic field is source-free , there are no magnetic "charges" (monopolies) *) from which magnetic field lines originate or enter (unlike electric charges, where electric field lines begin and end). Therefore, exactly as many magnetic field lines must enter from the closed surface S as enter them, ie the magnetic flux from the closed surface is equal to zero:
(1.36a) |
By converting the area integral to the volume integral using the Gauss theorem, we get the equation
div B = 0 , | (1.36b) |
which is a mathematical
expression of the principle of continuity of magnetic field lines
in differential form.
---------------------------
*) We leave here Dirac's hypothesis about the existence of
magnetic monopoles based on the idea of symmetry of electrodynamics equations.
Experiments trying to find magnetic monopoles have not yet
yielded any convincing results. However, magnetic monopolies are
considered in modern quantum unitary field theories, which is
related to their significance for the cosmology of the very early
universe (Chapter 5, §5.5).
The generation of an electric field by a time-varying magnetic field is expressed by Faraday's law of electromagnetic induction
(1.37a) |
whereby the electromotive force ( voltage ) U s ?n_{C} E dl induced along a closed curve C is proportional to the speed with which a change in magnetic flux F s nn_{S}B dS by surface S enveloped by the curve C . In the integral on the right side it does not matter the choice of the surface S surrounded by the given curve C , because the magnetic field is source-free (div B = 0). By converting the curve integral on the left side using the Stokes theorem to the area integral we get the law of electromagnetic induction expressed in differential form :
rot E = - (1 / c) ¶ B / ¶ t. | (1.37b) |
Maxwell's
equations
The outlined application of the mathematical
apparatus of differential and integral calculus to the
empirically determined laws of electromagnetism (ie to the
knowledge of Coulomb, Ampere, Faraday, Biot, Savart, etc.) and
their generalization was performed by J.C. Maxwell, who arrived at a
complete system of basic equations of the electromagnetic field
and summarized the individual findings into a comprehensive
theory. These Maxwell's equations (1.31b) to (1.37b), which we
gradually derived above, can be clearly summarized in
differential form as follows :
Maxwell's equations of the electromagnetic field |
(1.38) | |
(1.39) | |
(1.40) | |
(1.41) |
These equations
determine the electric and magnetic fields E
and B excited
by a given distribution of charges and currents r and j . The
first pair of Maxwell's equations describes the
generation of electric and magnetic fields by material sources,
ie the density of electric charge r and current j
protruding on the right side, the second pair expresses other internal
properties of the field. It can be seen from equations (1.38) and
(1.40), that the electric E
and magnetic B
fields can mutually generate
each other with their
time variability --> electrodynamics
.
The
Lagrangian for the electromagnetic field^{ }
We derived the Maxwell equation of the electromagnetic field here
physically - inductively from Coulomb's,
Biot-Savart's, Ampere's, Faraday's law. In theoretical physics,
the laws of motion and field equations are often derived in a
deductive manner using the variational principle of least
action [165]. The classical physical system is described by the integral of the action S
S = ò L (q _{1} , q _{2} , ... q _{n} ,, q ^{.}_{ 1} , q ^{.}_{ 2} , ......... q ^{.}_{ N} ) d t .... |
where L is the so-called Lagrange function - Lagrangian
, describing all dynamic characteristics q_{i} of a given system and their time derivatives q^{.}_{i} , n is the
number of degrees of freedom. The variational principle of the smallest
action d S = 0 then leads
to Lagrange's equations , from which the equations of motion or field
equations of the studied system follow
(for more details, see §2.5 in the section " Variational Derivation of
Gravitational Field Equations
") .
For the electromagnetic field, the Lagrangian has the form:
L = 1/8 p ( E ^{2} - B ^{2} ) + j . A - r . j . | (1.42) |
Maxwell's equations (1.38-41) can be derived from the variational principle of the smallest action with Lagrangian (1.42).
Electromagnetic field in the
material environment - electrodynamics of the continuum
In our theoretical analysis, we consider the
electromagnetic field mainly in vacuum , which
is the basic natural environment for fundamental physics. For the
sake of completeness, we will briefly outline here how the
electromagnetic field behaves in material environments
(the material " continuum "). The interaction
of electric and magnetic fields with atoms and molecules of
matter leads to their electric polarization and magnetization,
which is reflected in the vectors of electric and magnetic field
intensity. The way in which the electrical polarization and
magnetization of atoms and molecules of the material environment
arise and how it is reflected in the intensities of the resulting
electric and magnetic field is clearly shown in §1.1, passage
" Electromagnetic and Optical
Properties of Substances
" monograph " Nuclear Physics and Ionizing
Radiation Physics ".
To quantify this influence of the material environment on
electric and magnetic field intensities, two new vectors are
introduced: electric field induction D
and magnetic field intensity H (historically confusing terminology is discussed below
in the note " Intensity < -^{ } > induction in electromagnetism
?) The following are related to
the basic electrical quantities E and B
in a vacuum:
D = e . E , B = m . H , |
where e is the electrical permittivity of the
substance (also called dielectric constant)
describing the attenuation of the electric
field due to the polarization of the substance, m is the magnetic permeability
indicating the amplifying or attenuating effect of magnetization
of the substance on the magnetic field.
Maxwell's equations of the electromagnetic field in a material
environment (electrically non-conductive) can then be written in the same form (1.38-41) as in a
vacuum, in which, however, "vacuum" intensities E
and B are replaced by "substance"
vectors D and H at appropriate
places :^{ }
(1.38´-41´) |
where the relationships between E
and D = E / e , B
and H = B / m contain the material
coefficients of electrical permittivity e and magnetic
permeability m . They also include possibly inhomogeneities and
nonlinearities of polarization and magnetization - in some
material environments and at high field intensities nonlinear
electrodynamics can manifest itself (theoretical possibility of nonlinear electrodynamics
even in vacuum for extremely strong electromagnetic field is
discussed at the end of the following §1.6
"Four-dimensional spacetime and special theory of
relativity", passage "Nonlinear electrodynamics ").
The laws of continuum electrodynamics ,
summarized in Maxwell's equations (1.38´-41´), describe all
electromagnetic phenomena occurring in material
environments (see the already
mentioned passage" Electromagnetic and optical properties of
substances "). Due to the interaction of electric and magnetic fields
with atoms and molecules of matter, time changes in fields (see " Retarded potentials " below) and electromagnetic waves in matter
environments propagate at a rate c´ lower
than in vacuum : c´ = 1 /Ö(e.m) <c = 1 / Ö ( e _{o} . M _{o} ) = 2,998.10 ^{8} m / s @ 300,000 km / s (for light this leads to known optical phenomena of
refraction of light rays during the transition between substances
with different "optical densities" - different
refractive index caused by different velocities c ´) .
Terminological note:
Intensity of
<-> induction in electromagnetism?^{ }
The term intensity in science (even in ordinary expression) characterizes
the degree of power , mightines, yield of an
event, a phenomenon - here the power of the field
. The intensity of the electric field E really
expresses an
electric force acting in this field on a particle with a
unit electric charge (in suitable units) . The "intensity" of the magnetic field B
should analogously express the magnetic Lorentz force (the second term in (1.30) ) acting in
this field on a unit-charged particle, when perpendicular to the
unit velocity. However, the quantity B ,
describing the actually acting magnetic force, is called in
magnetism not intensity, but magnetic induction
! And the "intensity" of the magnetic field is called
the derived quantity H (= B / m )
"corrected" for the magnetic permeability of the
material environment. At the same time, it is in electrostaticselectric
induction D (= E / e ) derived quantity
characterizing the electric field minus the effect of dielectric
polarization. So it's the opposite ...
^{ }This unfortunate "intersection"
of the names " intensity-induction " arose
during the historical development of the science
of electricity and magnetism, when magnetism was explained by fluid
theory , analogous to electrostatics. And unfortunately it
has already remained so ... In our treatises, therefore, we will
often understand the vector B (conventionally
called magnetic induction) by " magnetic field
strength " .
Note: The word
" induction"here he
characterizes the electrical and magnetic changes in substances
caused by their insertion into electromagnetic fields. Do not
confuse with electromagnetic induction (1.37) ..! ..
Properties
of Maxwell's equations
Let's briefly note some general properties of the system of
Maxwell's equations (in vacuum). First of all, from the 1st pair
of Maxwell's equations we get (by applying the operation
"div" on equation (1.38), the operation " ¶ / ¶ t" on equation (1.39) and
their sum m) the continuity equation div j + ¶r / ¶ t = 0 The distribution and movement of
electric charges cannot therefore be entered completely
arbitrarily; in order for Maxwell's equations to be satisfiable,
the continuity equation must be satisfied. In other words, the
electric charges around them excite the electric and magnetic
fields so that they maintain themselves - the continuity equation
is a consequence of the field
equations .
^{ }Equations (1.39) and (1.41) do
not contain time derivatives and therefore have the character of
boundary conditions; the remaining two equations (1.38) and
(1.40), which can be (using the "div" operation on both
sides) adjusted to the form
¶ / ¶ t (div E - 4 pr ) = - 4 p (div j + ¶r / ¶ t ) = 0, (continuity equation)
^{¶} / _{¶ }_{t} div B = -c div rot E º 0,
then they guarantee that if these initial conditions div E = 4 pr and div B = 0 are satisfied at some time t = 0, they remain satisfied at all times.
Field potentials
In field theory, in addition to the intensity
vectors of a given field, it is advantageous to introduce field potentials , which are quantities whose derivatives
(differential forms) indicate the respective intensities. In
electrostatics, the intensity of the electric field E can be expressed as a gradient of the electric potential j ( E = - grad j ),
which identically satisfies the equation rot
E = 0. In magnetism, the equation div B = 0 holds, so there must be a quantity
(vector field) A , such that B = rot A . From the second pair Maxwelequations, it follows that the
vectors E and B in the case of a general electromagnetic
field can be expressed by quantities j and A in the form
E = - grad j - (1 / c) ¶ A / ¶ t, | (1.43a) |
B = rot A . | (1.43b) |
By introducing such an electric
potential j and a magnetic vector potential A , the last two Maxwell's
equations are fulfilled identically.
Since the field intensities depend only on the derivatives of the
potentials, these potentials are not determined unambiguously;
different values of the potentials may correspond to the given
fields E and B. E.g. to A can be attributed to an
arbitrary constant vector, and j arbitrary
constant without changing intensities E
and B . In
general, the magnetic field B = rot
A does not
change, if we add to A
a gradient of any
function f ( rot grad f º 0);
in order not to change the electric field E (1.43a), it is also necessary to
add the term - (1 / c) to the potential j . ¶ f / ¶ t. If we perform
the so-called calibration transformation of potentials
A ® A '= A + grad f, j ® j ' = j - (1 / c) ¶ f / ¶ t , | (1.44) |
where f ( r , t) is an arbitrary scalar function of place and time, the corresponding electromagnetic field does not change ( E ® E '= E , B ® B ' = B ). This certain "freedom" in choosing potentials allows you to select the shape of the potential (to carry out their "calibration") so that it was possible best for the specific problem.
The retarded potentials
Maxwell's equations (1.38) and (1.39), expressed by substituting
z (1.43a, b) with the potentials, generally have a rather complex
form
These equations are greatly simplified if the so-called Lorentz calibration condition is prescribed for potentials :
grad A + (1 / c) ¶j / ¶ t = 0 | (1.45) |
(this condition can be satisfied by the transformation (1.44) with the function f satisfying the equation D f - (1 / c ^{2} ). ¶ ^{2} f / ¶ t ^{2} = div A + (1 / c). ¶j / ¶ t ). During this calibration, the Maxwell's equations, expressed by means of potentials, take on a separated and symmetrical form of the d'Alembert equations
(1.46a) (1.46b) |
where o º ¶ ^{2}/¶x ^{2} + ¶^{2}/¶y ^{2} + ¶ ^{2}/¶z ^{2} - (1 / c ^{2} ) ¶ ^{2} / ¶ t ^{2} is d'Alembert's differential operator. In mathematical physics, it turns out that the general solution of these equations has the form *)
(1.47a, b) |
where r = (x, y, z) is the position vector of the
point at which we determine the potentials, r '= (x', y ', z') is the position
vector of the volume element dV '= dx'dy'dz' when integrating the
charge density and current, j
_{o} and A _{o}
describe the external field acting on the system (or integration
constants). Equations (1.47a, b) show that at a given place r
and at a given time t , the field is given not by the
instantaneous distribution of charge and current in the whole
space, but by the distribution retarded (delayed in the past) always by
time | r - r '| / c, which is needed to
overcome the distance R = |r - r '| at speed c
from individual points (x ', y', z ') of the source system to the
examined place (x, y, z) - see Fig.1.3c. Solution (1.47) is
therefore called retarded potentials . The change (disturbance) in
the electromagnetic field (caused, for example, by a change in
the distribution of charges) therefore propagates
at a final
speed equal to the speed of light c.
*) Note: In the previous §1.4 and in the first
half of this §1.5 we marked area and volume integrals triple
integrals: òò _{S}
f (...) dS and òòò
_{V} f (...) dV. In the following, however,
for brevity we will use only one integration sign: ò _{S} f (...) dS and ò _{V}f (...) dV indicating the surface
S and the volume V .
Relativistic electromagnetism
In classical electrodynamics, electric and magnetic fields are
separate fields, interconnected only by the laws of excitation
and induction, summarized in Maxwell's
equations . In
the special theory of relativity (discussed in the following §1.6 "Four- dimensional
spacetime and special theory of relativity ") , created by A. Einstein on the basis of a
careful analysis of electromagnetism, however, we will see that
the division of electromagnetic forces into separate electrical
and magnetic ones is not fundamental, but may depend on the frame
of reference. Simply put, what appears to the observer in one
frame of reference with the rest distribution of electric charges
as a purely electric force will appear to the moving observer in
another frame of reference as a magnetic force, resp. combination
of electric and magnetic forces. In other words, the magnetic
field can be considered a relativistic
manifestationelectric field. If we have a system of
static electric charges in one frame of reference, only the
electric field will act here, we will not observe any magnetic
field. However, a moving observer in another frame of reference,
looking at the same system of charges, will see a current of charges , exciting a magnetic field - creating a
magnetic field associated with the movement of charges - with an
electric current - according to Biot-Savart-Laplace's law. The
magnetic field appears as a "relativistic product" in Lorentz coordinate transformations in the presence of a quiescent
electric field. However, all these connections are based on the
relationship between electric and magnetic fields, expressed in
Maxwell's equations
^{ }This relativistic combination of
electric and magnetic forces will be analyzed in more detail in
§1.6, part "Four- dimensional electrodynamics ", where the electric and
magnetic fields will be combined into a 4- tensor
of the 2nd
order electromagnetic field . We will see that by changing
the inertial frame of reference, its electrical
and magnetic components are mixed - similarly to the special theory of
relativity, it mixes spatial and temporal coordinates in
space-time. This is the theoretical basis of relativistic electromagnetism .
Electromagnetic
waves
The general laws of wave
propagation in nature are discussed in §2.7, passage " Wave
propagation - a general natural phenomenon ". Here we show the origin and properties of waves
in an electromagnetic field.
^{ }If we write Maxwell's equations (1.38) and
(1.40) for the space domain, where j = 0 and r = 0,
then by their partial derivation according to time and
substituting from the remaining two Maxwell's equations we get d'Alembert's equations
D E - (1 / c ^{2} ) ¶ ^{2 }E / ¶ t ^{2} = 0, D B - (1 / c ^{2} ) ¶ ^{2 }B / ¶ t ^{2} = 0 | (1.48) |
analogous to equations (1.46) for potentials, but without the presence of electric charges. Since these equations have non-zero solutions, the electromagnetic field can also exist independently , without direct connection to electric charges and currents. If we look for particular solutions that depend on only one coordinate, eg on x , and at time t , equation (1.48) is simplified to
¶ ^{2 }E / ¶ x ^{2} - (1 / c ^{2} ) ¶ ^{2 }E / ¶ t ^{2} = 0 (and analogously for B )
and the solution will be every function of the shape
E = E (x, t - x / c), B = B (x, t - x / c).
The same value of the field E and B as in the point o coordinate x _{o}
at the time t _{o} will be in all places whose
coordinates and time satisfy the equation x -
x _{o} = c.
(T - t _{o}
). It is thus a wave
propagating in the direction of the X axis at the phase velocity c .
From Maxwell's equations follows the existence of electromagnetic
waves that
propagate at a speed equal to the speed
of light (from a general-physical
point of view, the speed of light is discussed in §1.1, passage
" Speed of light ") .
This finding led Maxwell to believe that light is probably an electromagnetic
wave of very short wavelength. In this way, Maxwell managed to
unify into a comprehensive theory not only electrical and
magnetic phenomena, but also to include optical
phenomena .
Note:^{ }The origin and properties of
various types of electromagnetic radiation (radio waves, infrared
radiation, visible light, UV and X-rays, g radiation ) are discussed
in more detail, for example, in §1.1 " Atoms and atomic nuclei " , section " Electromagnetic
fields and radiation "treatise " Nuclear
Physics and Physics of Ionizing Radiation " .
In a plane wave propagating in the direction of the X axis, all quantities are functions only t-x/c. If E = E (tx / c), then from Maxwell's equations (1.38) and (1.40) for r = 0, j = 0, it follows ¶ B / ¶ t = - rot E = ( n ° / c) ´ (d E / d (tx / c)) = n ° ´ ¶ E / ¶ t, so the relationship between electric and magnetic field in an electromagnetic wave is
B = n ° ´ E , | (1.49) |
where n ° is the unit vector in the direction of wave propagation (" x " indicates the vector product). That is, the vectors of electric and magnetic fields E and B are always perpendicular to each other and also to vector n ° direction of propagation - electromagnetic waves are transverse . Since B = rot A , only the vector potential A is sufficient for the description of the plane wave , by which the fields E and B are determined by the relations
B = (1/c) (A^{.} ´ n°) , B = (1/c) [(A^{.} ´ n°) ´ n°] | (1.49 ') |
(the dot A is the time derivative: A ^{.} o ¶ A / ¶ T). The simplest case of an electromagnetic wave is a monochromatic wave, in which the field is a simple harmonic function of time at each given point: A (t) _{r = const. }= A _{o} (r) .cos ( w t + a ), a = a (r), where w = 2 p .f = 2 p / T is the circular frequency of the wave, a is a constant phase shift. Size l = 2 p c / w then represents the wavelength , ie the distance that the wave travels in one period T (the distance of the two nearest places with the same phase). In a planar monochromatic wave, the field will be a harmonic function of the argument tx / c
A = A _{o} cos [ w . (T - x / c) + a ],
where A _{o} nor a does not depend on t nor x . By introducing a wave vector
k = ^{def} ( w / c). n ° | (1.50) |
a plane wave can be expressed in form
A ( r , t) = A _{o} cos ( w t - k . R + a ) | (1.51) |
valid for any direction of wave propagation (analogously for B and E ). This term for a monochromatic plane wave is often written in a complex form
A = Re [ Â _{o} . e ^{i ( k . r - }^{w }^{t)} ] , | (1.51 ') |
where Â _{a} = A . e ^{i }^{a} is a constant complex vector; the fields E and B can be expressed similarly .
During rotation of the coordinate system by an angle J along the direction of propagation n° plane electromagnetic waves in the wave field will be transformed by law Â ® Â '= e ^{i }^{J} . Â ; the electromagnetic wave is invariant due to the rotation of an angle of 360° around the direction of propagation. The symmetry properties of plane waves with respect to rotation around the direction of propagation are important in quantum physics, where they determine the spin of the respective particles created by quantization of a given field. At the classical level, spin is defined as
s = 360 ° / (angle of symmetry of a plane wave with respect to rotation about the direction of propagation) ;
the spin of the electromagnetic field (electromagnetic waves and their quantum - photons) is therefore equal to s = 1 .
In electrostatics, it can be shown by simple considerations (about the work needed to place the charges in a given configuration) that the electrostatic energy of a system of N charged bodies
e _{e} = (1/2) _{a = 1} S ^{N} q _{a} . j _{a} = (1/2) ò r . j dV = (1/8 p ) ò E ^{2} dV
can be expressed by the integral of the intensity of their common electric field, so that the electric field can be attributed to the energy distributed with the density W _{e} = (1/8 p ) E ^{2} in space. Similar considerations of labor required to produce the electric currents in the system of electrical circuits (against induced electromotive forces generated increase of the magnetic field), show that the energy of system this conductors
e _{m} = (1/2) _{a = 1} S ^{N} I _{a} . F _{a} = (1/2) o A . j dV = (1/8 p ) ò B ^{2} dV
is given by the volume integral of the induction vector B of the excited magnetic field and can be considered as the energy of this magnetic field distributed in space with density D _{m} = (1/8 p ) B ^{2} . The energy density in the electromagnetic field is then equal to the sum of the densities corresponding to the electric and magnetic components:
W _{elmag} = (1/8 p ) (E ^{2} + B ^{2} ) . | (1.52) |
It is clear that such an assignment of energy to the field is purely formal under Coulomb, Ampere, and Faraday's law, because it is just another description of the interaction energy in the idea of the instantaneous force action of charges and currents at a distance. However, the physical justification is given by the fact that the commotion in the electromagnetic field propagates at a finite speed . This final rate of propagation of changes in the field leads to the conclusion (repeat, see the argument in the introduction §2.8) that the electromagnetic field itself must actually contain energy (and momentum) that can flow from one place to another and do work on electric charges and currents - changing to other forms of energy. The electromagnetic field is therefore not just a space in which electric and magnetic forces act, but is a separate physical reality - a specific form of matter .
By scalar multiplication of Maxwell's equation (1.38) by the field E and equation (1.40) by the field B and their addition we get the equation after adjustment
¶ [(E ^{2} + B ^{2} ) / 8] / ¶ t = - div [(c / 4 p ). ( E ´ B )] - j . E . | (1.53) |
Integration over some chosen spatial area V after the application of the Gauss theorem then gives
(1.54) |
The left side represents the change in the energy of the electromagnetic field e _{elmag} contained within the region V per unit time. The first integral on the right indicates the work that electric forces do with charges per unit time, or the change in kinetic energy e _{kin }of charges per unit time (magnetic forces with charges do no work and therefore do not change their kinetic energy). Equation (1.54) thus expresses the law of conservation of energy in the electromagnetic field: the electromagnetic energy contained in the spatial region V decreases on the one hand by mechanical work performed by electric forces with charges inside the region V , on the other hand by energy transmitted (radiated) by the field from the area V through the bounding surface S = ¶ V to the outer space. Equation (1.54) can also be written in the form
(1.54 ') |
whereby a decrease in total energy of the electromagnetic field and the charged particles in the volume V per unit time is equal to the flux vector (c / 4 p ). ( E x B ) surface S surrounding region V . Therefore vector
P = (c / 4 p ). ( E ´ B ) | (1.55) |
called the Poynting vector represents the
energy passing through a unit of area per unit of time, or it is a vector of the flux density of
electromagnetic energy in space. When integrating in (1.54) over
the whole space, when the bounding surface S is infinitely spaced and the
field on it is equal to zero, it expresses equation (1.54), resp.
(1.54 '), simply the law of conservation of the sum of the total
energy of the electromagnetic field and the kinetic energy of all
charges.
Similarly, it can be shown that the electromagnetic field has momentum p given by the integral^{ }
p = ò (1/4 p c). ( E ´ B ) dV, | (1.56) |
so the momentum of the
volume unit of the electromagnetic field is equal to P / c ^{2} .
The energy current
in a plane electromagnetic wave is equal to (1.49)^{ }
P = (c / 4 p ) ( E x B ) = (c / 4 p ) E ^{2} . n ° = (c / 4 p ) B ^{2} . n °, | (1.57) |
which with respect to (1.52) is related to the energy density W _{elmag} by the relation P = c. W _{elmag} . n °, from which it can also be seen that the field propagates in the wave at the speed of light.
Let us have a system of moving electric charges concentrated in some limited spatial area (Fig.1.4). If we place the origin of coordinates somewhere in the system of charges, then the study of the field at large distances R >> L, where L is the characteristic dimension of the system will place all of the source system at about the same distance R as the origin of the coordinates. Distances |R - r | of the individual points r 'of the source from the investigated distant point R is approximately equal to | R - r '| @ R - R °. r ', where R ° is a unit vector pointing from the origin O to the investigated point, so that the retarded potential can be written in the form
j ( R , t) = (1 / R). n r ( r ', t - R / c + R °. r ' / c) dV ', A ( R , t) = (1 / R). ò j ( r ', t - R / c + R °. r ' / c) dV '.
The retardation time
thus consists of two different parts. The first part R / c
determines the external retardation, ie the time required for the
changes in the electromagnetic field to exceed the distance from
the origin of the coordinates, or from the source system, to the
distant observation point. The second part is equal to - R °. r '/ c characterizes the internal
retardation, ie the time of propagation of the disturbance in the
field within the source system.
If the charge distribution in the system changes slowly enough,
internal retardation can be neglected. For this, it is sufficient
that the characteristic time T, during which the charge
distribution changes appreciably, satisfies the condition T
>> L / c. Since cT is the wavelength l electromagnetic waves
emitted by the system, the condition of negligibility of internal
retardation can also be written in the form L << l , ie the dimensions of the system must be
small in comparison with the length of the emitted waves. The
characteristic time T changes in the distribution of charges is
related to the average velocity v of
charges rounds
following equation: T » L / V, so that neglecting
retardation it is necessary to apply v«c, i.e. the speed of motion of
charges must be small compared to the speed of light. If internal
retardation is neglected, the potentials are equal at
great distances from the source system
j ( R , t) = (1 / R). n r ( r ', t - R / c) dV', A ( R , t) = (1 / R). ò j ( r ', t - R / c) dV'.
At these distances large in comparison with both the dimensions of the source system and the length of the radiated waves - in the wave zone - it is possible to consider the variable field component as a plane wave within small areas of space. It is therefore sufficient to determine the vector potential A = (1 / cR) here. ò r . v dV '= (1 / cR) _{a = 1 }S ^{N} q _{a }v _{a} = (1 / cR) (d / dt) _{a = 1 }S ^{N} q _{a }r ' _{a} , i.e.
A ( R , t) = (1 / cR). d ^{. }(tR / c), | (1.58) |
where d º S q _{a }r _{a} is the electric dipole moment of the system as it was at time tR / c. The electric and magnetic fields are then equal to (1.49)
E (R , t) = (1 / c ^{2} R) [( d ^{..} ´ R °) ´ R °], B (R , t) = (1 / c ^{2} R) ( d ^{..} ´ R °) , | (1.59) |
where the dipole moment d is again taken at the moment tR / c (dots above d mean the derivative according to time) .
The flow of electromagnetic energy in the wave zone, ie the intensity of electromagnetic radiation, is expressed by the Poynting vector according to (1.57)
P = (c/4p) (E´B) = (1/4pc^{3}R^{2}) (d^{..}´R°)^{2} = (d^{..}^{ 2}/4pc^{3}R^{2}) sin^{2}J . R° , | (1.60) |
where J is the angle between the directions of the vectors d ^{..} and R (if we use polar coordinates - Fig.1.4b). The angular distribution of the intensity of the electric dipole radiation is given by the coefficient sin ^{2} J , the corresponding directional diagram is in Fig.1.4c. The total energy radiated by the system per unit time (ie radiated power) I = dE / dt is then given by the flow of energy over the entire spherical surface R = const. :
(1.61) |
If the source system consists of only one accelerating force q, is d ^{..} = q. r ^{..} = q. a , and the radiated power is equal to
I º dE / dt = (2.q ^{2} / 3c ^{3} ). a ^{2} . | (1.61 ') |
This radiation law was derived in 1899 by the Irish physicist J. Larmor. In addition, in the system of SI units, the coefficient k = 1 / (4 pe _{o} ) present in Coulomb's law is present.
Fig.1.4. Electromagnetic field of an island system of moving
electric charges.
a ) The field excited
by a system of moving electric charges is given not by an
instantaneous but by a retarded distribution and movement of the
charges.
b ) At a great
distance from the source system (in the wave zone), the variable
component of the field is given by the second time derivative of
the dipole moment of the system d ^{..}
and has the character of electromagnetic waves carrying the
kinetic energy of the source into space.
c ) Directional diagram of
electric dipole radiation.
Relationships (1.58) to (1.61) for the field and radiation of the island system of electric charges in the wave zone were obtained in the first order approximation in the ratio L / l (higher order members were neglected), which led to the application of only the dipole moment of the system. In the general case, however, it is necessary to take into account other members in the development of the potential according to powers L / l , which leads to the fact that the total intensity of electromagnetic radiation of a system of moving charges is given by time derivatives of individual multipole moments of charge distribution. In addition to the dipole moment is usually the most radiation involved the quadrupole moment K _{b} = o r . (X3 _{and} x _{b} - d _{ab} .r ^{2} ) dV and possibly magnetic dipole moment m = (1 / 2c) ò r . ( r ´ v ) dV, which contribute to radiation according to a known relationship (see eg [166])
(1.62) |
If the properties of the source system are such that d ^{..} = 0 (this is the case, for example, in a system composed of bodies with the same specific charge q / m), dipole radiation does not occur. In such cases, only radiation caused by other members in the development of the potential according to powers of L / l , ie radiation of higher multipoles, is applied.
Electrodynamics thus comes to the general conclusion that with each
accelerated (uneven) movement of electric charges, electromagnetic
waves are emitted , which carry part of their kinetic
energy into space *). In §2.7 we will see that the general
theory of relativity arrives at essentially the same conclusion -
the emission of gravitational waves during the accelerated motion
of gravitational bodies, although the properties of gravitational
waves differ from the properties of electromagnetic waves in some
respects.
*) This phenomenon plays an important role in atomic
physics for the structure of the atomic shell and the formation
of radiation during its deexcitation (see §1.1 " Atoms
and atomic nuclei " of the
book "Nuclear Physics and Physics of Ionizing
Radiation"). Furthermore, in
nuclear physics and physics of ionizing radiation. Particularly
fast-flying electrons are sharply braked
when interacting with the material environment , so that
according to the relation (1.61´) they emit relatively intense
electromagnetic radiation - so-called braking radiation
. Braking radiation finds significant use in the excitation of X-rays
by the impact of electrically accelerated electrons on
the anode in X-rays tubes - see §3.2 " X-ray diagnostics ", or in the excitation of hard g- radiation
by the impact of high-energy electrons from betatron or
linear accelerator (see §1.5 "Elementary particles").
, the " Charged Particle Accelerators " section of the same publication) on a suitable
target.
We investigated the variable electromagnetic fields excited by a system of moving charges in the wave zone, ie at sufficiently large distances from the source system, and we calculated the radiated energy using the Poynting vector. Analysis of the electromagnetic field at short distances then shows that a small variable component of the electric field with a phase different from the main variable component is generated inside and near the source system . In the third order approximation, this term is equal
E _{re} = (2 / 3c ^{3} ) d ^{...} .
In the source system, therefore, each charge q will be acted upon by a certain additional force "reaction" f _{re} = q. E _{re} acting per unit time of work f _{re} . in so that the total work done in this field, all based hub system and _{re} = (2 / 3c ^{3} ) d ^{...} S q _{and }the _{a} = (2 / 3c ^{3} ) d ^{...} . d ., which when averaged over time (over several periods T) gives
A _{re} = - (2 / 3c ^{3} ) d ^{..}^{ 2} .
It can be seen that this
additional field component causes a corresponding braking of the charge
movements in the source by the back reaction of the
emitted waves, in full energy agreement with the formula (1.61)
obtained by the analysis of the field in the far wave zone. Such
an analysis is of great importance for gravitational waves, where
the calculation of energy in the wave zone is not nearly as clear
and unambiguous as in electrodynamics - we will see this in §2.8
" Specific properties of
gravitational energy ".
Equation of motion m. v = q. E
+ (q / c). ( v x B ) charged
particles in the electromagnetic field under the influence of the
Lorentz force (1.30) is therefore necessary to supplement the braking action^{ } electromagnetic radiation:
m. v = q. E + (q / c) ( v ´ B ) + (2q ^{2} / 3c ^{3} ) v ^{..} ; | (1.63) |
this
equation is applicable when the velocity is small compared to the
speed of light and the braking force is significantly smaller
than the Lorentz force acting on the charge of the external field
E and B .
^{ }Further details on the properties of the
electromagnetic field and their applications can be found in the
relevant literature; from review momographies we can mention eg
[235], [264], [206].
Electromagnetic fields have been considered as a manifestation of
certain types of ether motion *). Some (electrically charged)
bodies set this ether in motion, which propagates in it at a
finite speed and is passed on to other bodies. However, such an
ether would have to have very unusual physical properties. In
order for electromagnetic waves to propagate in it, which are
transverse, it would have to have some properties of a solid
body. And the mechanical model of the ether is no longer
compatible with the experimentally determined constant of the
speed of light in all inertial systems. Attempts to reconcile
this fact with the ether model did not lead to success (for example, the assumption of "entrainment of the
ether" by the movement of the Earth failed to confront the
observed aberration of light from the constellations) . Therefore, the idea of ??ether
wasabandoned and it was realized that the
carrier of the electromagnetic field is the space
itself . A. Einstein then completed this concept in a special theory of relativity by concluding
that the stability
of the speed of light is a reflection of the connection between
space and time. Electromagnetism thus played an important
heuristic role in revealing the deeper and more general laws of
nature - the laws of relativistic
physics .
*) E
t h e r :^{ }
19th century physics she took it for granted that every wave
could propagate only in the flexible material (matter) medium
whose oscillating motion created it. It is difficult to imagine
sea waves without water or sound without air (or other flexible
acoustic environment of gaseous, liquid or solid phase - see the
well-known elementary experiment with an alarm clock or a bell
under the recipient of the pump). When it was discovered that
light and other electromagnetic waves propagate not only in air
and other optical media environments, but also in a vacuum
, a problem arose in the environment or medium
in which electromagnetic waves propagate. Thus was born the idea
of ether (Latin aether , in analogy to
a volatile organic solvent called ether) - universal all
- pervading "substances", filling all space and
penetrating all matter (just as water penetrates the meshes of a
fishing net towed behind a boat). This ether creates an
environment for the propagation of light, heat and other
electromagnetic waves; it is also a carrier of gravity. Since the
ether did not manifest itself in any other physical and chemical
phenomena, it was judged to be translucent, unweightable,
perfectly permeable without friction, and had no chemical
properties. A substance with such conflicting properties was
practically undetectable experimentally.
One could only study how the penetration of ether affects the speed
of lightunder different configurations of the state of
motion of the light source and the observer. Maxwell himself has
already designed an experiment using the motion of the Earth:
light moving with the ether in the same direction as the Earth
orbits the Sun must have a slightly different speed than light
that propagates perpendicular to this motion or in the opposite
direction. be about 10 ^{-7} . Maxwell did not see the result of this experiment; up
to 8 years after his death, in 1887, A. Michelson and E. Morley
made this measurement by interfering with the rays of
monochromatic light reflected by two mirrors in the horizontal
and vertical directions, while the whole interference device on
the floating plate could be rotated. The result was that no
difference was measured in the speed of light in both
directions, seemed unexpected and paradoxical at the time.
However, the negative result of this experiment was confirmed by
other measurements. No ad hoc hypotheses, such as ether
entrainment (the ether is drawn along with the earth's surface,
so its position relative to the interferometer) has not been
confirmed. In contrast, the negative result of Michesson's and
Morley's experiment was explained by the Lorentz contraction
hypothesis , according to which the dimensions of all
bodies in the direction of their velocity v are shortened
in the ratio 1 / Ö (1-v ^{2} / c ^{2} ). Einstein then gave a definitive and universal
explanation in his special theory of relativity,
according to which the speed of light (in vacuum) is the same in
all moving conditions and in all directions. The idea of ??the
ether was thus definitively abandoned , replaced
by the properties of empty space itself, connected with time into
a single space-time continuum . Nevertheless, in
the field of radio applications of electromagnetic waves, the
terms " transmit to ether " or " receive
from ether " are often used .
Nonlinear electrodynamics
?
At all the intensities we observe in nature and in the
laboratory, the electric and magnetic fields in the vacuum appear
to us to be linear - the principle of
superposition applies exactly to the values of
intensities E and B , as well
as to potentials .
At the end of the following §1.6 "Four-Dimensional
Spacetime and
Special Theory of Relativity", passage " Nonlinear Electrodynamics ", the possibilities of how an extremely strong
electromagnetic field could behave in a non-linear
manner even in a vacuum will be discussed .
1.4. Analogy between
gravity and electrostatics |
1.6. Four-dimensional
spacetime and special theory of relativity |
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