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European Journal of Applied Sciences – Vol. 12, No. 5

Publication Date: October 25, 2024

DOI:10.14738/aivp.125.17511.

Blanovsky, A. (2024). Classical Field Theory-based Design of Green Energy Systems. European Journal of Applied Sciences, Vol -

12(5). 01-08.

Services for Science and Education – United Kingdom

Classical Field Theory-based Design of Green Energy Systems

Anatoly Blanovsky

Westside Environmental Technology, Los Angeles, CA 90046

ABSTRACT

Novel technologies are often traced back to fundamental science. Green energy,

particularly fission-, gamma- and photo-electric (PE) cells, are no exception. Based

on the fundamentally sound Lorentz Theory, this article aims to explain how

implementation of blackbody-cavity PE cells can greatly increase efficiency of the

integrated conventional thermal and photovoltaic systems. Long before quantum

mechanics, Lorentz suggested that some disturbances, like waves, travel with

particles through a certain medium - motionless ether. The waves are described

by the Klein-Gordon equation and dispersion relation 2=c2k2+c

2. In

hydromechanics, they are known as non-propagating waves and a boundary

frequency c is called the cutoff frequency. The group velocity approaches zero

and waves are not propagating if their frequency is below the cutoff frequency c.

Their group and phase velocity are related by vu=c2, in the infinite k limit v=u=c

and the group velocity maximum are c. A quantum object is considered as a

vibrating particle or material body with a rest mass m moving in resonance with

wave characterized by the cutoff or Compton frequency c =mc2/

 .

Keywords: Lorentz theory, blackbody-cavity, photoelectric, solar, fission - electric cell,

CIGS cylindrical photovoltaic, carbon nano-tube cathode.

INTRODUCTION

The goal of this research article is to offer an innovative approach to current nuclear and solar

power systems that would greatly increase their energy output and efficiency. The proposed

blackbody cavity design compensates for the loss of energy inherently incurred by solar

receivers due to radiation from the absorbing surface. Electron emission in a cavity can be

achieved through three common mechanisms: photoelectric (PE), thermionic (TE) and field

emission.

The most heavily deployed solar power technologies are photovoltaic (PV) panels and

concentrated solar power (CSP) systems. A proposed modification of CSP, flat or CIGS

cylindrical PV modules combines solar photoelectric (PE) and thermal systems to efficiently

convert solar radiation to electricity and thermal energy (to be stored and/or converted to

electricity). Mo, Pt, Al, Ni, or Ag based thin films back contact material for CIGS solar cells can

serve as the PE anode. An inverter such as hybrid PE solar panel and thyratron changes the

energy from direct current (DC) to alternating current (AC), which is typically used in

buildings.

CLASSICAL FIELD THEORY

The two fundamental wave types in the quantum medium are the longitudinal and transverse

waves. Classical physics provides the accurate field values (group velocity and intensity of

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European Journal of Applied Sciences (EJAS) Vol. 12, Issue 5, October-2024

transverse waves) into Maxwell's field equations, and characterizes antiparticles as

longitudinal waves with negative group velocity in Newtonian mechanics. The pairs such as

electron-positrons described by the four Klein-Gordon equations are balanced by the energy

2mc2 at the distance d=e2/(4πε2mc2)=1.4*10-15m. Originally, the energy mc2 was introduced

to stabilize the charged particles by compensating the Coulomb interactions.

Analogy between the acoustic and quantum waves naturally appears when we consider waves

on a discrete string of atoms. The frequency of the oscillation should be computed in terms of

the mass of the atom M and the string elastic constant a. Here a is the distance between two

neighboring atoms. The length of the string of N atoms is L=Na, the material density =M/a

and the characteristic speed c=(a/)

1/2. It can be shown that deviation of the nth atom from

the equilibrium position is zn=Ane

i(t+kna), where n is integer. The internal energy density

2

3

2 m

k

c

u

=

and discrete set of k is connected with medium structure.

Then the number of oscillators or traveling wave states between k and dk in the polar

coordinates is

( )

dN k dk 2

3

2

4

=

and their energy is

ck, we have kc=1016m-1 and

( )

4

3

2

3 m

k

c

u

 

= 1037 N/m2. For wavelengths shorter than mean distance between the atoms

(cutoff wave number kc=N/L=/a), propagation becomes impossible.

As kc=108 cm-1 and c=3×105 cm/s, the cutoff frequency of the material oscillations

c=ckm1013s

-1. If the cutoff frequencies of vacuum oscillations νc is ~1024s

-1, it leads to

restriction on its characteristic size >2c/νc=10-16m. For ideal quantum fluid or radiation,

pressure of energy density is P=u/3.

In 1923, de Broglie suggested that real wave pilots the particle in a vacuum. At that time, the

idea was not accepted as conflicting relativity. Instead of a systematic effect analysis, the

constancy of light velocity was postulated to justify the result of the Michelson or Sagnac

experiment on open paths, in which the Earth appears not to rotate around the Sun.

Mathematically, it was based on the Lorentz transformation that preserves a wave equation in

moving frame instead of time. As an algebraic expressions - Lorentz transformation is equally

applies to any wave motion, the variable values of light velocity were used in Einstein original

manuscript. Moreover, field equations of general relativity do not lead to attraction between

material bodies [1-4].

Photoelectric Solar and Radioisotope Systems

In the photoelectric (PE) modules, spacing between transparent or cavity-type anode and

cathode allows for greatly improved fundamental properties compared to, photovoltaic (PV)

modules. Particularly, a combined photoelectric, photovoltaic and blackbody-cavity thermal

solar module converts incident sunlight to both electricity and high-temperature thermal

energy. This greatly increases thermal insulation and efficiency of the concentrated solar

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Blanovsky, A. (2024). Classical Field Theory-based Design of Green Energy Systems. European Journal of Applied Sciences, Vol - 12(5). 01-08.

URL: http://dx.doi.org/10.14738/aivp.125.17511

power (CSP) systems, green buildings and radioisotope thermal generators (RTG). Even

under one sun illumination, PE cathode/gate directional selectivity has the potential to raise

receiver efficiency levels to those of concentration systems.

Figure 1: PE panele with in-plane gate and CNT electrodes.

A principal loss mechanism for solar receivers in solar-thermal systems is radiation from the

absorbing surface. By the first law of thermodynamics and Planck's law of blackbody

radiation, the absorption efficiency of solar absorber is given as

η = Ejn-Eout/Ein =1-σT4/DNI*C.

Here Ein is the absorber input solar power, Eout is power loss due to thermal radiation from

the absorber, σ is Stefan-Boltzmann constant, T is the temperature of the absorber, DNI is

direct normal irradiance of sunlight, and C is concentration ratio of the absorber.

Figure 2: Photoelectric blackbody-cavity CSP plants and PE-cavity converters

The surfaces with high solar absorption and low thermal emission could efficiently convert

solar radiation into electricity and useful heat. Ni pigmented anodized Al is one of the typical

examples of spectral selective surfaces for efficient photo/thermal conversion of solar energy.

Here the metal particles are much smaller than the wavelengths of the electromagnetic

radiation

In a typical absorber of a parabolic trough solar receiver with a concentration ratio of 70 and

an operating temperature of about 400oC, about 17% of solar energy input would be lost via

thermal radiation. The radiation loss can be reduced by using the photoelectric/photovoltaic

blackbody-cavity receiver.

In the blackbody-cavity receiver, the maximum enhancement factor for absorption with

respect to a single pass absorption is limited to 4n2 with n being the refractive index of the

absorbing layer. The discharge geometry with Al, thoriated tungsten, phosphorus-doped

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European Journal of Applied Sciences (EJAS) Vol. 12, Issue 5, October-2024

polycrystalline diamond, graphene or GaAs photo-cathodes activated by cesium and oxygen

surrounded by the Al anode is one of the several possible configurations. Unlike the single- junction Shockley-Queisser limit as a function of band gap, the efficiency of photoelectric solar

power improves monotonically as the electrode work functions shrink. The preliminary

analyses of the CSP with thermal energy storage (TES) show that the PE/PV blackbody cavity

and solar thermal system efficiencies are around 55% and absorber/cathode temperature can

be high up to 900◦C under 10 suns.

Unlike conventional PV module, the concentrated PV or PE receiver must be continuously

aligned with DNI (direct normal irradiance) for continuous power generation. In green

buildings, hybrid photoelectric/thermal systems produce electricity and hot water

simultaneously. The plasma-enhanced photoelectric PE power module can also serve as a

thyratron [5, 6].

The ratio between DNI and global normal irradiance (GNI) can be used to partly identify

atmospheric conditions. The solar radiation striking the earth is close to collimated, thus a PE

cell facing the sun absorbs direct sunlight at near normal incidence but emits IR radiation in

all directions. The PE x-ray or gamma ray radioisotope generator model is very similar to an

ideal PE solar power device.

Figure 3: DNI for a month on an inclined surface of the southern orientation of the cylindrical

PE/PV solar module and radioisotope photoelectric generator.

The cylindrical PE/PV module can generate higher electric power than the conventional CIGS

PV module. Cylindrical panels demonstrated positive proof of their durability against wind of

50 m/s through the field test. As compared with other conventional heat engines, a

thermionic energy converter (TEC) offers remarkable advantages due to its compactness,

high power density, silent operation, and long operational lifespan. Also, nano-grating

comparable with the de Broglie wavelength of the electron can change the electronic and

electron emission properties of materials. Studies on the influence of nano-grating structures

on the properties of materials have shown that this process may lead to effects similar to

those created by doping with donors.

The resistivity values measured in Si-based nano-grating layers, for example, were

approximately 10−2 Ohm cm, similar to those of Si semiconductors doped with phosphorus

impurities having a volume concentration of 1018 cm−3 .

It is almost independent of initial resistivity of samples: 5000 Ohm cm, 8.5-11.5 Ohm cm, 12-

14 Ohm cm.