The Light during Gravitational Super-Compressibility

doi:10.4236/jmp.2013.44066

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Journal of Modern Physics, 2013, 4, 468-473

http://dx.doi.org/10.4236/jmp.2013.44066 Published Online April 2013 (http://www.scirp.org/journal/jmp)

The Light during Gravitational Super-Compressibility

Kholmurad Khasanov

Gas and Wave Dynamics Department, M. V. Lomonosov Moscow State University, Moscow, Russia

Email: [email protected]

Received January 20, 2013; revised February 21, 2013; accepted February 28, 2013

which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

ABSTRACT

The interaction of electromagnetic and gravitational fields and gravitational super-compressibility were investigated ex-

perimentally. Dynamic emitter provides conditions for the generation of eigenfunctions with eigenvalues for the various

fields, including: acoustic, gravitational and electromagnetic. We observe the gravitational waves in gas flowing from

the dynamic emitter and their interaction with electromagnetic waves. The gravitational field energy was decreasing when

electromagnetic field was emitted through the excitation of condensed medium. The direction of maximum change of

the emitted energy of excited medium was strongly opposed to gravity vector at that point. The frequency of radiation

against the gravity vector in given point of space exceeded radiation frequency of same source in opposite direction.

Keywords: Gravitational Super-Compressibility; Interaction of Electric and Gravitational Fields; Light Frequency

Increasing against Gravity Vector

1. Introduction

The light of high energy emitted during super-compres-

sibility of supersonic spiraled jets was discussed in [1-4].

High energy field density is detected in gas flowing from

the dynamic emitter (nozzle with a central cone). This

dynamic emitter is resonator of acoustic, gravitational

and electromagnetic waves [3]. The phenomenon of su-

per-compressibility in under-expanded submerged jet on

output of the dynamic emitter results to the arising of

super-compressed and gravitational waves. These waves

structures form the stable boundary layers and emit high

energy radiation, as summarized in [5-7].

In our experiments vapor jets form channels of station-

ary boundary layers with progressing strong compression

and condensation of gas due to gravitational super-com-

pressibility. These phenomena are accompanied with

emission of high energy radiation from the X-ray to in-

frared spectrum and in short radio waves regions [8-10].

We detect at first in [11,12] anti-gravitational directed

quanta of high energy that emitted from the excited

condensed medium against gravity vector in given point.

The interaction of electric and gravitational fields and

gravitational super-compressibility were investigated ex-

perimentally. In present, paper experimental results are

given about shifting emission spectra of the excited gas

or condensed medium depending on gravitational field.

Spiraled supersonic jets and incandescent nichrome and

wolfram wires and red-hot steel rod in gravitation field

were investigated. Separation in space of photons by en-

ergy levels were visualized and detected. The phenome-

non of gravitational super-compressibility in under-ex-

panded submerged jet on output of the dynamic emitter

results to the arising of stationary gravitational waves

and is one of case of the separation of light by energy

levels.

Alternating super-accelerations arise through the exci-

tation of gas and condensed media. The excited state of

the medium and instability of the field generate gravitons

and gravitational waves. This field is found in the gravi-

ton-photon interaction that provides light emission.

The results of measurement of the changing of energy

and frequency of light during gravitational super-com-

pressibility, when light is emitted by the excited gas and

condensed medium, are presented in this work. It occurs

so that frequency of radiation against the gravity vector

in given point of space exceeds radiation frequency of

same source in opposite direction.

On the other hand weight of substance is varied at the

photon-graviton interaction including when the substance

is heating or cooling [11,12].

The distortion of the phase structure of the fields

through excitation of the medium leads to the processes

of compensating of phase structure changing.

KH. KHASANOV 469

Phenomena of separation in space of photons by en-

ergy levels were visualized and detected.

Alternate super-accelerations of interacting particles in

excited medium generate quadruple waves with two po-

larization directions.

2. Experimental Part

2.1. Separation of Light from the Inclined

Supersonic Jet

Separation of light on the energy levels in gas and con-

densed media is found, when emission spectra are vary-

ing in gravitation field depending on the direction of light

emission in reference to vector of gravity. In our experi-

ments the length of the wave structure was equal to 10

diameters of outlet of the nozzle approximately.

The jet with such spiral configuration presents a new

type of gravitational waves.

Light emission in fragments of spiral structures of the

jet flowing from nozzle with a conic central body was

found. In case of the inclined nozzle the light emission

with different colors is detected. The bottom and top

sides of the jet flowing from the nozzle with central cone

are differently glowing (see Figure 1).

2.2. The Increasing of Light Frequency Emitted

against Gravity Vector

The increasing of the frequency of light in incandescent

nichrome and wolfram wires is found. One can see in

Figure 2 the increasing of frequency of light on top side

of wire. Here gravity vector is perpendicular to wire.

In Figure 2, frequency of radiation from top side di-

rected against the gravity vector exceeds radiation fre-

quency of the wire in the opposite direction. Violet re-

gion of glowing is disposed on outside surface, on top

line of the wire. Yellow region of glowing is disposed

also on outside surface, on bottom line of the wire. And

the sides of the wire are glowing with the same fre-

quency.

In Figure 3, there are presented the visualization of in-

candescent nichrome wire with blue filter and with the

same camera. Here top part of glowing space above the

wire extends bottom part more than on 60%.

2.3. Thermal Field of Horizontal Aglow Rod

along Gravity Vector

The distribution of the energy levels of glowing above

and below the red-hot steel rod, disposed horizontally

was measured. The red-hot steel rod was disposed hori-

zontally on 2 m from the lab floor. Temperature in dif-

ferent levels under and over the rod was measured (see

Figure 4). No convection was detected.

The direct current in the red-hot rod was 100 A, volt-

age was less than 1 V. Diameter of rod in Figure 4 is 3

Figure 1. Separation of light emitted from the inclined su-

personic jet. The bottom and top sides of the jet flowing

from the dynamic emitter of gravitational waves with cen-

tral cone are differently glowing. Top side of jet is violet

with more energy and bottom one is green. In Figure 1,

there are no outside electromagnetic sources to excite the jet.

The pressure in pre-chamber is 4 atm.

Figure 2. Horizontal spanned incandescent nichrome wire

in air has different color on top (violet) and bottom (yellow)

sides. Different glowing colors in space are varying along

the gravity vector. The diameter of investigated nichrome

wire is 1 mm. The length of spanned wire here is 20 mm.

Camera SONY Digital Handycam DCR-TRV147E PAL

Digital 8 with 560× digital zoom was used for the visualiza-

tion.

mm and its length is 200 mm. Temperature of the air

around the rod was measured on the distances from 50

cm below rod to 60 cm over the rod. During direct cur-

rent the temperature remains at same level in given point

of space over or under the rod. The charts in Figure 4

describe similar cases with the wire illustrated in Figures

2 and 3.

Temperature field under and over the rod at the same

distances are different. In Figure 4, appropriate tempera-

ture for –50 cm (50 cm under the rod) is equal 298 K and

KH. KHASANOV

470

appropriate temperature for +50 cm (50 cm over the rod)

is equal 433 K. Appropriate colors of glowing also are

different.

The presented temperature distribution confirms light

separation on energy levels along the gravity vector.

In Figures 2-4, there are presented the results of inter-

action of electromagnetic wave with the background gra-

vitation field.

2.4. Spectral Measurements for Incandescent

Wolfram Horizontal Wire in Lamp

Spectral mtasurements for incandescent wolfram spiral

wire disposed in glass lamp is measured. Automated sys-

tem for measuring the spectra (see Figure 5) of lamp with

spiral wolfram wire in gravitation field has been imple-

mented on the basis of monochromator MDR-12, which

ensures accuracy with dispersion 2.4 nm/mm.

Figure 3. Horizontal spanned incandescent nichrome wire

in air with another focusing of camera. The lens of camera

is equipped with blue light filter. The diameter of investi-

gated nichrome wire is 1 mm. The length of spanned wire

here is 20 mm. Camera SONY Digital Handycam is the

same as in Figure 2.

When the width of input slit is less than 30 microns it

was possible to achieve a spectral resolution of set up to

1 Å. This corresponds to measurements with defined

accuracy of the photon energy of 0.3 - 0.4 MeV in the

blue and green regions of the spectrum (450 - 550 nm).

The measurements were performed with constant step of

wavelengths Δλ = 0.1 - 1 nm up to 170 - 1700 points on

the spectral interval, averaged over 3 - 15 measurements

at each point. Digital instruments included in the meas-

urement system for the amplification and measurement

of the signals allowed to increase the dynamic range of

the installation of up to 5 orders of magnitude. Noise and

crosstalk limits the dynamic range of the spectrum for a

single (but not of the spectra) at the level of 10−2 - 10−3 of

270

320

370

420

470

520

570

-50-40-30-20-10010 2030 40 50 60

Dis tance from agl ow rod, cm

Temperature, K

Temperature

Temperat ure trend

Figure 4. Temperature field distribution above and below

red-hot steel rod disposed horizontally.

Figure 5. Experimental setup provided spectral measurements and estimate temperature distribution of incandescent wire in

lamp in the automatic mode.

KH. KHASANOV 471

signal intensity at the maximum. Digital power supply

Motech LPS-303 allows us to set the current J and volt-

age V in the lamp within, respectively, from microam-

pere to 2 amperes and from 10 millivolts to 20 volts. J

and V were measured with accuracy 0.1%. The voltage

across the lamp recorded digital multimeter APPA-101

(7). Multimeter APPA 207 (5) provides detection of tem-

perature on the housing with thermocouples. The radia-

tion from the wire in lamp is focused with collimator (13)

on the entrance slit (14) of the diffraction grating mono-

chromator MDR-12 (15). The diameter of the collimating

lens is 72 mm and the distance from the lens to the wire

determines the solid angle in which the radiation is fo-

cused on the slit.

Determine spectral content of the light passes through

the exit slit (16) on the photomultiplier FEU-100 (17),

high voltage (1200 V) of which is supported by the

power supply (18). While working on a direct current

signal from the photomultiplier goes through a matching

circuit (30), goes to the DC amplifier (DCA) (19) and fed

to a digital voltmeter ARRA-207 (20) to control the out-

put. The sensitivity of the input stage of DCA ranges

from 50 to 1000 nA.

Digital signal with a voltmeter goes to the COM port

(21) of computer (24) and recorded. Control pulses to the

control unit (22) of the monochromator stepper motor

come with the interface card. The couplings (23) com-

municated with a personal computer (24) via a second

COM port (25). Voltage of the board (23) implemented

via block (26). Experimental setup allows us to investi-

gate the electroluminescence spectra of wire in constant

current mode. Then the lamp through the ammeter MA-

11/5 (6) to control current value is connected to a uni-

versal DC power supply (4), with which you can set the

desired voltage through the wire. The voltage across the

wire recorded with digital multimeter APPA-101 (7).

The figure also shows the following interface devices:

the monitor (28) and a printer (29), used in the process of

measuring and analyzing the results.

Setup allows the spectra in the automatic mode. The

spectra were plotted as chart: “wavelength-intensity” in

arbitrary units (see Figures 7 and 8).

In Figures 6 and 7, the emission spectra of horizontal

spiral wolfram wire are presented for various voltage and

electrical current applied to the wire. Measurement error

for wavelength is no more than 0.1 nm. The diameter of

investigated spiral wolfram wire in Figures 6-9 is less

than 1 mm. The length of wire in lamp is 2 cm.

In Figures 6 and 7, temperature difference ΔT between

“top” and “bottom” of wolfram wire for same current and

voltage is presented. In Figure 8, the uneven along the

spectrum character of intensity increasing is obvious. Gen-

eration of short-wavelength component (450 nm) of the

spectrum is observed in case of more power of heating.

Figure 6. Emission spectra shifting due to frequencies dif-

ference from “top” and from “bottom” of the spiral.

Figure 7. Emission spectra shifting due to frequencies dif-

ference from “top” and from “bottom” of wolfram spiral in

case of more power of heating.

In Figure 8, the power of heating, resistance and cur-

rent of spiral wire in lamp versus the voltage on it are

presented. Power was received as the product of voltage

and current, measured with voltage at the same time.

Measurements show that presented interaction has re-

sonance nature (see Figure 9).

In Figures 8 and 9, there are presented the results of in-

teraction of electromagnetic waves with the background

gravitation field.

We observe the gravitational waves in gas flowing

from the dynamic emitter and their interaction with elec-

tromagnetic waves. The background gravitation field was

identified when light was emitted by the excited con-

densed medium. The direction of maximum change of

the eigenvalues of excited medium was strongly opposed

to gravity vector at that point. The frequency of radiation

against the gravity vector in given point of space exceeds

KH. KHASANOV

472

Figure 8. Power of heating, resistance and current of incandescent spiral wolfram wire in lamp versus voltage on it.

Figure 9. Temperature difference (Ttop − Tbottom > 0) between the top and bottom lines of the horizontal wire in the lamp and

convenient spectral shifting (λtop − λbottom < 0) versus voltage on the wire.

radiation frequency of same source in opposite direction.

It is result of interaction of background gravitation field

with electromagnetic field.

3. Conclusions

The interaction of electromagnetic and gravitational fields

and gravitational super-compressibility were investigated

experimentally.

 Dynamic emitter provides conditions for the genera-

tion of eigenfunctions with eigenvalues for the vari-

ous fields, including: acoustic, gravitational and elec-

tromagnetic waves.

 Gravitational super-compressibility of continuous me-

dia provides high energy light emission.

 The gravitational field energy was decreasing when

electromagnetic field was emitted through the excita-

tion of condensed medium.

 The direction of electromagnetic field gradient was

constant with respect to gravity vector at given point

of the found alternate background gravitation field.

 The frequency of radiation against the gravity vector

in given point exceeds radiation frequency of the same

source in the opposite direction.

 Uneven along the spectrum character of intensity in-

creasing is found. Generation of short-wavelength

component (450 nm) of the spectrum is observed in

case of more power of heating.

 Measurements show that presented electromagnetic

and gravitational interactions have resonance nature.

4. Acknowledgements

Author gratefully acknowledges for the long-term sup-

port and consulting to V. A. Sadovnichiy, academician of

RAS and R. I. Nigmatulin, academician of RAS.

Author deeply appreciates to A. E. Yunovich from M.

V. Lomonosov Moscow State University Semiconductor

KH. KHASANOV 473

Physics Department for kindly provided equipment for

spectral measurements.

REFERENCES

[1] Kh. Khasanov, “Double Spiraled Supersonic Jet,” Fluid

Dynamics, Vol. 46, No. 3, 2011, pp. 433-436.

doi:10.1134/S0015462811030094

[2] Kh. Khasanov, “Bi-Spiral Switched Supersonic Jet Flow

Escaping from a Circular Nozzle: Interaction with Metal

and Polymer Screens, Infrared Radiation Phenomenon,”

International Conference: Fluxes and Structures in Fluids.

Physics of Geospheres, Moscow, 24-27 June 2009, pp.

206-210.

[3] Kh. Khasanov and S. V. Petukhov, “Dynamic Emitter,”

PF Patent No. 2058196, 1996.

[4] Kh. Khasanov, “Super-Compressibility Phenomenon,” Jour-

nal of Modern Physics, Vol. 4, No. 2, 2013, pp. 200-207.

[5] Kh. Khasanov, “Radiation of Bi-Spiral Switched Super-

sonic Jet Flow Escaping from an Annular Nozzle,” In:

Fluxes and Structures in Fluids, Physics of Geospheres,

Moscow, 24-27 June 2009, 2010, Abstracts.

[6] Kh. Khasanov, “Visualization of Bi-Spiral Twisted Su-

personic Gas Flow,” The 8th Pacific Symposium of Flow

Visualization and Image Processing, Moscow, 21-25 Au-

gust 2011, p. 51.

[7] Kh. Khasanov, “Visualization of Super-Compressibility

in Supersonic Spiral-Twisted Jets,” Physics Letters A, Vol.

376, No. 5, 2012, pp. 748-753.

doi:10.1016/j.physleta.2011.12.018

[8] Kh. Khasanov, A. I. Klimov, A. S. Pashchina, I. Moralev

and M. Sidorenko, “Interaction of Supersonic Jet with

Capacity Coupled HF Discharge,” The 11th International

Workshop on Magneto-Plasma Aerodynamics, Moscow,

10-12 April 2012, pp. 95-96.

[9] Kh. Khasanov, “High-Energy Radiation of Continuous

Medium as It Interacts with Sub-Millimeter Fields of

Outer Space,” The 11th International Workshop on Mag-

neto-Plasma Aerodynamics, Moscow, 10-12 April 2012,

pp. 96-97.

[10] Kh. Khasanov, “Emission of High Energy during Super-

Compressibility of Supersonic Jets,” Open Journal of

Fluid Dynamics (OJFD), Vol. 2, 2012, pp. 172-179.

[11] Kh. Khasanov, “Phenomena Taking Place at the Atomic

Level under Certain Perturbation,” 56th International

Symposium on Molecular Spectroscopy, Ohio State Uni-

versity, Columbus, 11-15 June 2001, p. 125.

[12] Kh. Khasanov, “Quantum Antigravitation of Vapor-Air

Jet,” 56th Meeting of International Symposium on Mole-

cular Spectroscopy, Ohio State University, Columbus,

11-15 June 2001, p. 199.