As is well–known from affine geometry,1 there are spaces with the allowable systems of orthogonal coordinates having the common origin, an identical unit volume and the same orientation. Such is our real 3d–space. Why? Because our real space could be created only owing to long ranged attractive forces, e.g., by the forces of gravitation. An empty space, i.e., the space without any matter, can have any dimension–from zero up to ‘n’. The mathematical space is the empty.
The main goal of this article is to find connection between the spaces of different dimensions i (from zero up to ‘n’) and the long–range attractive forces that create these spaces and have (forces) its dimension j (from zero up to ‘m’). By the dimension of long–range attraction forces Fis meant the value of the exponent j in the denominator of the formula
,
where
and
are interacting masses (kg);
is a coefficient;the distance between these masses (m);
.
Our problem should not be confused with problem that P. Ehrenfest was solving 100 years ago.2–5 He made attempt to link the dimension of space with fundamental laws of physics but he did not concern the problems connected with the creature of spaces under influence of long–ranged interaction forces.
Call any space containing matter real space. Any real space has to contain the sources of long–range interactions, in our case of the attraction between masses. The existence of these sources is defined by divergence the vector of interaction a between masses. For example, for our 3–D real space the divergence of awill have the following form if ais only the function of the coordinate
(spherical coordinate system):
(1)
(2)
where index “3” in (1) indicates that the above formulae refer to 3D–
space;
is a surface element (in our case of the spherical surface);the unit vector perpendicular to
;Vvolume
the interaction force between masses
and
;
the constant of gravitation (
);Ethe vector of gravitation field intensity (
), as
If
, then we can write down (1) as
. (3)
Since
in spherical system of coordinate
we have after integration (3):
(4)
If we would use another formula instead,
e.g.,
(5)
then we have
(6)
It means that
depends on “
’, it means, in turn, that the law of energy conservation is broken. Indeed, if
(see (1)), then
and
. It means that the gravitation source at this point of space is not observed. The analogous picture takes place at other points of our space. In fact, it means as well that there is no any real space, since the interaction (5) cannot maintain its existence.
Now take such a law instead (5):
(7)
then instead (6) we have
(8)
and
if
and, consequently,
tends to zero. It means that our space collapses into a point, i.e., we obtain a black hole.
Here we should make an important remark. As seen, studying the above case, we have used the sphere of dimension 3. It means that we have been studying an isotropic space. If the space investigated had a fractional dimension, e.g., 2.9, then we had to take for our investigations not a sphere but an ellipsoid. Consequently, we cannot take the relation for the element of the ellipsoid surface as
, since in this case
should be a function of the angles
and
. In this work we have been studying only isotropic spaces.
Now we can put a question: how will things be going for spaces of other dimensions–from zero to
? To answer this question, first of all write down expressions for volumes and surfaces of different ranks. We begin to study spaces whose dimensions , i.e.
, 0,1,2.
If
, then we consider a circumference and a space inside it (we we call this space a flat sphere). Therefore we have:
(9)
(10)
here the coefficient kin
units.
If
, then we can write down (9) as
(11)
Since
in polar system of coordinate
, we have after integration in (11):
. (12)
If we would have another formula instead , e.g.,
(13)
Then we would have
(14)
It means that
depends on “r’, it means, in turn, that the law of energy conservation is broken. Indeed, if
(see (9)), then
and
. It means that the gravitation source at this point of space is not observed. The analogous picture takes place at other points of this space. In fact, it means as well that there is no any real 2D–space. Since the interaction (13) cannot maintain its existence.
Now take such a law instead (10):
(15)
Then instead (14) we have
, (16)
and
, if
, i.e., the flat sphere collapses into point and we have black hole but in 2D–space. Below the Greek letters
and
will be replaced by Greek letter
with index
, since we shall study spaces with
.
If
, a straight–line segment will be as if an analogue of the above flat sphere and a pair of points will be as if analogue of the above circumference bounding the above flat one. At this case we have:
(17)
(18)
Here the coefficient kis in
units. At last, if, then the space is a point here and its,
i.e. we have uncertainty. Now we shall study the spaces having the dimensions from
up to
If
, then we have:6
(19)
(20)
Where index “4” in (19–20) indicates that these formulae refer to 4D–space;
is the element of 3D–surface;
component of unit vector perpendicular to each point of this 3D–surface;
4–D volume;
interaction force between masses
and
in 4D–space;
constant of gravitation in 4D–space (
); E vector of gravitation field intensity
(
), as.
If
, then we can write down (19) as
(21)
Since
in a spherical system of coordinate
then we have after integration (21):
(22)
If we would have another formula instead F=km1m2R(4)/, e.g.
,
(23)
Then we would have
( 24)
It means that
depends on “
dq&ruo;, it means, in turn, that the law of energy conservation is broken. Indeed, if
(see (19), then
and
. The analogous picture takes place at other points of our space. In fact, it means as well that there is no any real space, since the interaction (23) cannot maintain its existence.
Now take such a law instead (23):
(25)
Then instead (24) we have
(26)
And
if
and, consequently
,tend to zero. It means that our space collapses into a point, i.e., we obtain a black hole.
In principle, we get a similar picture for the cases . Show it for the case
.
(27)
(28)
where index “n” in (27–28) indicates that these formulae refer to nD–space;
is the element of nD–surface;
a component of unit vector perpendicular to each point of this (n–1)D–surface;
nD–volume;
the interaction force between of masses
and
in nD–space;the constant of gravitation in nD–space (
); E the vector of gravitation field intensity (
), as; gamma function.
If
, then we can write down (27) as
(29)
Since
in a spherical system of coordinate
we have after integration (29):
(30)
If we would have another formula instead, e.g.,
(31)
Then we would have
(32)
It means that
depends on
it means, in turn, that the law of energy conservation is broken. Indeed, if
(see (27), then
and
. It means that the gravitation source at this point of space is not observed. The analogous picture takes place at other points of this space. In fact, it means as well that there is no any real space since the interaction (31) cannot maintain its existence.
Now take such a law instead (31):
(33)
Then instead (24) we have
(34)
And
if
and, consequently,
tend to zero. It means that our space collapses to point, i.e., we obtain a black hole.
Now we can assume that vacuum is a
space where the interaction law between masses has the rank
. There are fluctuations of the number
in the interaction one and the rank of the interaction may become less than the dimension
of the space. As a result, there occurs the Big Bang. Thus we have shown that long–raged interaction forces of the dimensionscan form real isotropic Euclidean spaces if and only if, when the dimensionsof these spaces equals
. Then we can affirm, using the method of mathematical induction, that long–raged interaction forces of the dimensions
can form a real isotropic Euclidean space of the rank
.
This is a theorem which we name “Theorem on spaces and long–ranged interaction forces forming these spaces” or, more shortly, “Theorem on spaces and forces forming them”.