The system describing an interaction between electrons and clusters of phonons in a crystalline lattice can be given as a result of parametric coupling of (1) and (6):

………… (7)

Where is the n th coupling coefficient along the chain <1, F₁is the energy of the heat vibrations of the lattice.

The system (7) describes the interaction process between electrons and clusters of phonons in the crystalline lattice. The solutions of (7) represent a sophisticated energy distribution along the lattice. Since the system (7) represents in fact one of the quantum recurrence forms 3 the general solution of (7) will look like follows:

……… (8)

The first members in (8) represent the Fourier sequences and the second members - sums of nonequidistant harmonics formed as a result of dispersion in a lattice 3. Phases reflect the individual parameters of the crystalline lattice (admixtures, plastic deformations, vacancies, dislocations, anisotropy etc). Within the framework of the proposed electric current model solutions (8) any electrical or ionic current can carry information about the properties of the crystalline lattice or plasma, or ionic solution where the current flows. In connection with this it's worth mentioning about an original experiment carried out by an australian researcher Bevan.L.Reid 4 in which he showed that an ionic current passing between the two vessels with sodium chloride solutions proved to be able to carry information for the crystal growth patterns from one vessel to another.

Computer study of the system (7) solutions shows an intermittency process typical for the recurrence mode similar to the Fermi-Pasta-Ulam recurrence 5. As it has been shown 5 that the recurrence phenomenon possesses a «memory» for the initial conditions and redisplays their configuration during the period of recurrence.

The coupled system (7) can simulate a physical functioning of a simple electric transformer for example an ingnition coil. As a first step of applying the computer model for a desciption of this electrical device the system's boundary conditions were chosen to simulate two coils of an electric transformer for example, an ingnition coil. For that purpose the boundary conditions of the first (electron) equation of (7) corresponded to the open ends of the chain and for the second (phonon) equation for half fixed ends (the beginning of the chain had fixed ends but the end had open ones). The solutions in this case show that despite an equal number of points in both difference-differential equations in (7) the amplitude in the electron chain was by an order larger than that in the phonon chain. It allows to speak out in favor of a quantum mechanical basis for the describing the physics of a simple electric transformer. The transformer mode of the system (7) is shown in Figure 14, Figure 15, Figure 16, Figure 17.

The results of the transformer mode simulation within the proposed model suggest a quantum mechanical basis for the description of its physical functioning. That is an exchange of energy between the two electron and phonon quantum recurrences (8) in accordance with the general properties of the resonant interaction between the recurrences 6. According to the model the most essential parameter is the rate of interaction between the recurrences along the whole chain (coefficients in (7)) which can be changed by inserting into the system an another crystalline lattice of a core whose parameters differ from the lattice that under consideration in the model. In fact, it adds another couple of equations like (7) into the model. Using different material for the core can result in regrouping of the energy in the electric current between electron and phonon components. For example such material as ferrite possessing with ferroelectric properties and a high electric resistance can cause an increasing the energy of the phonon part of the electric current in a transformer, whereas such conductive ferromagnetics as iron, steel and their alloys can be effective for icreasing the electron part of the energy especially at low frequencies.

Next step of the computer simulation was to visualize the general dynamics of the interaction between electron and phonon amplitudes described by the equations (7) in case of the open ends mode of the boundary conditions for both chains in (7).

Computer solutions of the electric current model (7) given in Figure 18, Figure 19, Figure 20, Figure 21 manifest a periodical repumping of the electron and phonon energy in a crystalline lattice between sums of equidistant and nonequidistant harmonics (8). For a model (7) with a large number of «atoms» (n=1000) there were observed much longer orders of spatial periodicity in solutions and their periods were multiple to the lattice parameter b. According to the model an electric current in a crystalline lattice of a conductor can appear as a result of increasing energy of the phonon component in (8) due to starting of the intrinsic selfparametric processes. The crucial parameter that brings the system (7) into a selfparametric excitation mode proved to be the the values of the coupling coefficients reflecting the rate of interaction between electron and phonon amplitudes along the chain. This mode demonstrates an exponential encreasing of the amplitudes (7) with time and space. A physical interpretation of it is a sharp increasing of the heat vibrations in the lattice. Figure 22, Figure 23 show the selfparametric mode in the system (7) when .Worth mentioning that the selfparametric excitation mode can arise in a closed dynamic system and the energy for increasing oscillations is extracted from the system itself. This phenomenon is well known in radioelectronics as a consequence of the Mathieu equation's physical realisation in a form of parametric electric generators having specific properties 7. In particular an exponential growth of the generator's current could be restricted only by switching non linear resistors for example filament lamps into the generator's ciruit.

The solutions of the system (7) (Figure 22, Figure 23) suggest an another property of the electric current: to concentrate energy of electrons and phonons in the part of a crystalline lattice that has different parameters to compare with the main part of it and that result in changing the values of the interaction coefficients . For example combining two types of a conducting wire: a copper and a tungsten one will lead to a considerable heating in the tungsten part to compare with the copper one because the other type of the tungsten's cystalline lattice causes a development of the selfparametric mode in its part for the electron and phonon components (Figure 22, Figure 23) of the current.