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Valentin Tzvetanov Penev
Ludmil Lubomirov Konstantinov
Central Laboratory of Mineralogy and
Crystallography
Bulgarian Academy of Sciences
Acad. Georgi Bonchev Str., bl. 107,
1113 Sofia, BULGARIA
Fax: (+359 2) 9797 056; Phone:
(+359 2) 97 97 055
E-mail: vpenev@interbgc.com,
vpenev@bas.bg, v_penev@mail.bg
Web site: http://www.clmc.bas.bg
ABSTRACT
The space and the coordinate system, necessary to construct entirely mathematical representations of the complex chemical objects, are introduced. It is proved that using the method proposed in [1] one can construct entirely mathematical and unique representations of arbitrary complex chemical objects. It is shown that using this method an exactly defined "chemical charge" is in fact ascribed to each point of the ordinary three-dimensional physical space.
KEYWORDS: geometrization, theoretical chemistry, foundations of chemistry, mathematical models
INTRODUCTION
In the previous papers [2, 3, 4]:
The main goals of this paper are:
to demonstrate the method for construction of such representations.
DEFINING THE SPACES AND COORDINATE SYSTEMS
Prior to construction entirely mathematical representations of complex chemical objects we shall recall some definitions formulated in [1, 4]:
DEFINITION A. By the term structure of a given complex object in a specified energy state we denote such a unity of a particular composition and a particular construction, which characterizes uniquely this complex object in this energy state.
DEFINITION B. By the term composition of a given complex object in a specified energy state we denote such a set of relatively independent particular parts (e.g. simple chemical objects), which characterizes uniquely this complex object in this energy state.
DEFINITION C. By the term construction of a given complex object in a specified energy state we denote such a particular mutual disposition in the three-dimensional physical space VE(3) of relatively independent parts (e.g. simple chemical objects), composing this complex object, which characterizes uniquely the object in this energy state.
According to thermodynamics in the definitions A, B and C, energy state of a particular object means the quantity of the internal energy of this object considered as a thermodynamic system (TDS).
DEFINITION I. By the term simple chemical object we denote each chemical object composed of a unique atomic kernel and the corresponding electron shell.
DEFINITION II. By the term complex chemical object we denote each chemical object composed of more than one simple chemical object.
DEFINITION "A&IA". By the term atom we denote each electrically neutral simple chemical object, and by the term monatomic ion (or ionised atom) we denote each simple chemical object, which is electrically charged either really or formally. In other words, an atom is each simple chemical object, which oxidation state is equal to zero, and a monatomic ion is each simple chemical object which oxidation state is different from zero.
From these definitions it becomes clear that each complex chemical object is a specific chemical structure built of a countable set of simple chemical objects. That is why in order to construct an entirely mathematical spatial representation of an arbitrarily chosen complex chemical object one should:
Construct such a mathematical space that allows each chemical structure to be represented entirely mathematically and uniquely as a unity of two qualities - chemical composition (i.e. chemical species of each of the building this structure simple chemical objects) and construction (i.e. mutual disposition of the building this structure simple chemical objects in the ordinary physical space VE(3));
Choose in this space such a coordinate system with respect to which each chemical structure can be represented entirely mathematically and uniquely as a unity of the two above-mentioned qualities.
So, the necessary space VS(6) is built as a Cartesian product of the ordinary 3 dimensional physical space VE(3) and the Mendeleev's space VM(3), introduced for the first time in [1, 4], i.e.: VS(6) = VM(3) x VE(3). We shall further refer to VS(6) as space of chemical structures.
Let us build in VS(6) such a 6 dimensional coordinate system KS(6)=(OS,z,r,j;u,v,w), which is a Cartesian product of the Mendeleev's coordinate system KM(3)=(OM;z,r,j), introduced firstly in [1, 4], and such a 3 dimensional coordinate system KE(3)=(OE;u,v,w) in the ordinary physical space VE(3), in the origin OE of which there is no simple chemical objects. In other words, let KS(6) = KM(3) x KE(3), where: the projection of the 6 dimensional point OS onto the 3 dimensional Mendeleev's space VM(3) coincides with its natural zero-point1, i.e. with the 3 dimensional point OM which, by definition [1, 4] is the origin of the coordinate system KM(3); the projection of the point OS onto the ordinary 3 dimensional physical space VE(3) coincides with the origin OE of the coordinate system KE(3). We shall refer further to KS(6) as coordinate system of chemical structures.
From the definition of VS(6) and KS(6) as Cartesian products and from the qualitative meaning of VM(3), KM(3), VE(3) and KE(3) one can conclude that:
Here, we shall pay a special attention to the requirement that no simple chemical objects should be present at the origin OE of the coordinate system KE(3). This limitation on the choice of points in VE(3) for origin of the coordinate system KE(3) is in fact a requirement for a conceptual correlation between the origins of the coordinate systems KM(3) and KE(3). Namely the observation of this requirement guarantees the necessary conceptual correlation between the spaces VM(3) and VE(3). It is easy to see that if the requirement for a conceptual correlation between the origins of KM(3) and KE(3) is not fulfilled, the corresponding 6 dimensional point OS (OS = OM x OE) will not play the role of origin of the 6 dimensional coordinate system KS(6), i.e. of a point which coordinates are (0,0,0;0,0,0) with respect to KS(6). Indeed, let us choose as origin, OE, of the coordinate system KE(3) such a point in VE(3) in which there is some, simple, chemical object. Then, the second triad of coordinates of the corresponding 6 dimensional point OS, with respect to KE(3) will by definition be equal to zero (because the projection of OS onto VE(3) coincides with the point OE chosen by definition as origin of the coordinate system KE(3)). At the same time according to the third conclusion, the first triad of coordinates of the corresponding 6 dimensional point OS will not be equal to zero, because in the corresponding position of VE(3), represented by OE, there will be some species of simple chemical object. But according to [1, 4] the presence of a simple chemical object of any species is always represented in VM(3) by a point with non-zero coordinates with respect to KM(3)).
It becomes clear that not any point of the 3 dimensional physical space can be chosen as origin of the coordinate system KE(3) due to the necessity of a conceptual correlation between the spaces VM(3) and VE(3) manifested as a requirement for conceptual correlation between the origins of the coordinate systems KM(3) and KE(3). However, the question arises: is there at least one point in VE(3) which fulfils the imposed requirement and thus to be chosen as the origin of KE(3)? It is easy to see that at each moment of time the set of points in VE(3), in which there are simple chemical objects is countable (discrete), whereas the set of points, in which there are no simple chemical objects is always continuous. In other words, at each moment of time the set of points in VE(3) which fulfils the imposed requirement (and, consequently, able to be chosen as the origin of KE(3)) is a continuum, whereas the set of points which does not fulfil it (and, consequently, not able to be chosen as the origin of KE(3)) is always countable (discrete). Or, from the viewpoint of the requirement for a conceptual correlation between the spaces VM(3) and VE(3), at each moment of time the 3 dimensional physical space VE(3) can, in fact, be considered as an empty continuum with point-like "holes", i.e. as a continuum in which only an countable set of points is occupied by simple chemical objects. By this we illustrated in fact that at each moment of time in the ordinary physical space VE(3) there is a whole continuum of coordinate systems fulfilling the requirement for conceptual correlation.
MATHEMATICAL REPRESENTATION OF THE CHEMICAL STRUCTURES
With respect to the so defined coordinate system KS(6) in VS(6) one can easily construct an entirely mathematical and unique representation of an arbitrary complex chemical object. For this purpose it is sufficient to prove the following statement:
THEOREM "CS". Each chemical structure can be represented entirely mathematically and uniquely with respect to KS(6) in VS(6) through the corresponding unique, discrete and noninvertible function, which domain is the ordinary 3 dimensional physical space VE(3) and it range (codomain) is the Mendeleev's space VM(3).
This theorem can be easily proved using the method
of demonstration via constructing. Indeed, let us consider an arbitrarily chosen
chemical structure with known stoichiometric formula. Then, the sought unique
discrete function representing the considered chemical structure is obtained
merely by replacing in the stoichiometric formula of this structure the symbols
of the simple chemical objects by the coordinates of the corresponding species
of these objects in the Mendeleev's space VM(3) by using any of the
two generalized mathematical models
or
, developed in
[1, 4].
It should be accentuated on the fact that all unique and discrete functions used to represent entirely mathematically the various chemical structures are noninvertible. To come round to the validity of this statement it is sufficient to remind that there are chemical structures which composition includes several (more than one) simple chemical objects of one and the same chemical species. In such structures, to the various points of the ordinary physical space VE(3) one can juxtapose one and the same point of the Mendeleev's space VM(3) that represent the species of the same chemical simple chemical objects.
The following can be drawn from this theorem:
1) At each moment of time any set of arbitrarily chosen chemical objects (both simple and complex) is represented entirely mathematically, uniquely and spatially (with respect to KS(6) in VS(6)) through establishing the corresponding noninvertible image2 of the ordinary physical space VE(3) onto Mendeleev's space VM(3). The image itself is constructed using the following two rules:
Rule I: To each point
of VE(3), in which some simple chemical object exists, one juxtaposes
the mathematical image in VM(3) of this species of simple
chemical objects obtained by any of the generalized spatial mathematical
models
or
.
Rule II: To each point of VE(3) in which there is no simple chemical object at all one juxtaposes the natural zero-point of VM(3).
The qualitative meaning of these two rules is as follows: they define a unique procedure for attributing an exactly specified chemical charge to each point of the ordinary 3 dimensional physical space VE(3). By the term chemical charge of a point of VE(3) we mean the species of the corresponding simple chemical object, occupying this point at a given moment of time.
2) From a mathematical point of view chemistry deals with the description and investigation of one exactly defined subset of the set of all functions - the subset of these unique discrete and noninvertible functions, which describes the possible chemical objects.
3) The definition and classification of the structures of various complex chemical objects are in fact determination and classification of these types of unique discrete and noninvertible functions which have chemical meaning in VS(6) (i.e. which are mathematical images of complex chemical objects).
4) From the Theorem "CS" follows also that:
COROLLARY "PC". All complex chemical objects of periodic construction can be represented entirely mathematically and uniquely with respect to KS(6) in VS(6) through the corresponding periodic unique discrete and noninvertible functions.
Therefore, it becomes clear that crystal chemistry deals with description and investigation of one exactly specified subset from the set of all unique discrete and noninvertible functions - the subset of the periodic unique discrete and noninvertible functions, describing the chemical objects with periodic construction.
REFERENCES
[1] Penev V. Tz. Geometrization of the fundamentals of chemistry. 1997, Riva Publ. House, Sofia, 224 pp. (in Bulgarian with an extended summary in English) (Full text and summary are available through the official site of the project "Geometrization of the language of chemistry" – http://www.clmc.bas.bg/staff/V_Penev/gcl/)
[2] Penev, V., L. Konstantinov, M. Marinov. 1999. Geometrization of the language of chemistry. Formulation of the problem. - Compt. rend. Acad. bulg. Sci., 52, 1-2, 49-52.
[3] Penev, V., L. Konstantinov, M. Marinov. 2000. The problem of geometrization of the language of chemistry. – Academic Open Internet Journal, Volume 2 (2000), Part 2: Chemistry – http://www.acadjournal.com/2000/v2/part2/p2/
[4] Penev, V., L. Konstantinov, M. Marinov. 2000. Logical structure of the fundamentals of chemistry, conceptual schemes of its geometrization and spatial mathematical models of the sets of different species of simple chemical objects. - Academic Open Internet Journal, Volume 2 (2000), Part 2: Chemistry – http://www.acadjournal.com/2000/v2/part2/p3/
NOTES
1 The Mendeleev's space VM(3) has by definition a natural zero-point OM, which qualitative meaning is the absence of any protons, neutrons and electrons. Namely this natural zero-point OM is chosen as origin of the Mendeleev's coordinate system KM(3).
2 In mathematics the notions function, mapping and image are synonymous.