METHOD AND APPARATUS FOR DECOMPOSING CARBON DIOXIDE GAS

Abstract

A method of producing carbon-oxygen structures by the Decomposition of Carbon Dioxide Gas at low pressure, from 14.7 to 100 psi, using laser irradiation in the mid-infrared spectrum, from 2.3 to 3.3 microns.

Claims

1. A method of decomposing carbon dioxide gas comprising: evacuating air from a reaction container; combining carbon dioxide gas and water vapor gas molecules in said reaction container; directing a mid-infrared laser beam having a wavelength of 2.3 to 3.3 microns into said reaction container to photo-dissociate the carbon dioxide gas into carbon, oxygen and carbon-oxygen activated species; and recombining the activated species to form solid carbon-oxygen structures; whereby carbon dioxide gas is decomposed.

2. The method of decomposing carbon dioxide gas in accordance with claim 1 including the step of pressuring said reaction container holding said carbon dioxide with a pressure of less that 100 psi.

3. The method of decomposing carbon dioxide gas in accordance with claim 1 including the step of pressuring said reaction container holding said carbon dioxide with a pressure of from 14.7 to 100 psi.

4. The method of decomposing carbon dioxide gas in accordance with claim 1 including the step of directing an Er: YAG laser beam with a wavelength of 2.94 m into said reaction container.

5. The method of decomposing carbon dioxide gas in accordance with claim 1 including the step of directing an HF laser beam with a wavelength of 2.7 microns into said reaction container.

6. The method of decomposing carbon dioxide gas in accordance with claim 1 including the step of combining said carbon dioxide gas with said water vapor gas molecules to form a weakly bonded carbon dioxide-water which is assisted by the polar surface of the reaction container.

7. The method of decomposing carbon dioxide gas in accordance with claim 1 including the step of combining said carbon dioxide gas with said water vapor gas molecules to form a weakly bonded carbonic acid which is assisted by the polar surface of the reaction container.

8. The method of decomposing carbon dioxide gas in accordance with claim 1 in which said reaction container is a glass container.

9. The method of decomposing carbon dioxide gas in accordance with claim 3 in which the carbon dioxide gas is dissociated into carbon, oxygen and carbon-oxygen activated species is by reaction of said mid-infrared light and said water vapor gas mediating molecules.

10. The method of decomposing carbon dioxide gas in accordance with claim 1 including the step of pressuring said reaction container holding said carbon dioxide with a pressure of about 15 psi.

11. A method of decomposing carbon dioxide gas comprising: combining carbon dioxide gas and water vapor gas molecules under pressure of between 14.7 to 100 psi in a reaction container having the air evacuated therefrom; directing a laser beam having a wavelength of 2.3 to 3.3 microns into said reaction container to photo-dissociate the carbon dioxide gas into carbon, and oxygen; and capturing heat released by said reaction; whereby carbon dioxide gas is decomposed.

12. The method of decomposing carbon dioxide gas in accordance with claim 11 including the step of directing an Er: YAG laser beam with a wavelength of 2.94 m into said reaction container.

13. The method of decomposing carbon dioxide gas in accordance with claim 11 including the step of directing an HF laser beam with a wavelength of 2.7 microns into said reaction container.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0010] The accompanying drawings, which are included to provide further understanding of the invention, are incorporated in and constitute a part of the specification and illustrate an embodiment of the invention and together with the description serve to explain the principles of the invention.

[0011] In the drawings:

[0012] FIG. 1 is a schematic diagram of the laser controlled decomposition apparatus in accordance with the present invention;

[0013] FIG. 2 is a schematic diagram of the laser controlled decomposition process in accordance with the present invention;

[0014] FIG. 3 shows the absorption spectrum of water in the region from 0.1 to 600 um;

[0015] FIG. 4 shows the emission spectra of flash light during irradiation;

[0016] FIG. 5 shows the emission spectra of black-body light at 3300K; and

[0017] FIG. 6 is an EDS spectrum of the area of glass irradiated by a laser in he presence of CO.sub.2.

DETAILED DESCRIPTION OF AN EXEMPLARY EMBODIMENT

[0018] This invention is directed to providing a method for decomposing carbon dioxide producing carbon particles and carbon-oxygen structures. The method includes flooding the carbon dioxide gas into a reaction vessel (i.e. glass vessel) and activating the gas with water vapor prior to shooting mid-infrared light through the reaction vessel. This causes a photo-excitation of the OH activated bonds that induces the photo-decomposition or photo-dissociation of carbon dioxide gas producing carbon and carbon-oxygen species and emitting high energy. The apparatus includes a reaction vessel, a means for feeding carbon dioxide and water vapor into the reaction vessel, and an Er:YAG laser or an HF laser which irradiates mid-infrared light through the reaction vessel.

[0019] An object of the invention is to provide a practical, low risk, and environmentally safe way to remove carbon dioxide from exhausts or combustion gases of petroleum and coal based products.

[0020] Another object is to provide a method for releasing carbon dioxide using a laser and water vapor as activating specie to ensure effectiveness of the process.

[0021] Another object is to provide a method for releasing carbon dioxide in low pressure conditions, employing laser and water vapor as activating specie to ensure effectiveness of the process and reduced associated complications.

[0022] Another object is to provide a method for producing energy exploiting the photo-dissociation of carbon dioxide by a laser.

[0023] The present invention is a method of decomposing CO.sub.2 gas at low pressure (from 14.7 to 100 psi). A pulsed or continues wave laser having a wavelength of 2.3 to 3.3 microns, such as an Er: YAG laser with a wavelength of 2.94 m or HF laser at 2.7 m is used to stimulate the OH bonds contained in the gas system. The decomposition of CO.sub.2 by laser radiation, when combined with water vapor inside a laboratory vessel, is the method used to activate the carbon-oxygen atoms. When this transformation occurs, an instantaneous flash of light, measured as black body, is observed and the temperature is increased to an estimated value of 3300K. When a glass vessel is used, contemporary to the flash of light, the silica of the glass is melted and the carbon dioxide produces both carbon particles and carbon-oxygen structures.

[0024] The present invention relates to the decomposition of carbon dioxide via mid-infrared irradiation that involves the photo-excitation of a carbon dioxide-water vapor complex with a formation of an activated species and release of energy, followed by reaction with carbon dioxide. The carbon dioxide-water vapor complex can be provided by flowing carbon dioxide gas in liquid water using conventional techniques. In certain embodiments, it is preferable for the carbon dioxide-vapor mixture to also supply only carbon dioxide gas to achieve higher concentration of carbon dioxide necessary for major amounts of carbon and carbon-oxygen product formation. Moreover, the carbon dioxide decomposition process is environmentally friendly and does not require any additional energy supply to facilitate carbon and carbon-oxygen structures formation.

[0025] In a certain embodiment, liquid water is introduced at room temperature into the reaction vessel before the introduction of carbon dioxide (molar ratio carbon dioxide/water 1:1, 2:1), but the carbon dioxide-water complex is not formed or, at least, present in a very low concentration in accordance with the following Equation: (see On the surprising kinetic stability of carbonic acid (H2CO3) by T. Loerting, C. Tautermann, R. T. Kroemer, I. Kohl, A. Hallbrucker, E. Mayer and K. R. Liedl in Angew. Chem. Int. Ed. (2000), vol. 39 (5), pp. 892-894; Aqueous carbonic acid (H2CO3) by T. Loerting and J. Bernard in Chem Phys Chem (2010), vol. 11, pp. 2305-2309).

H2CO3+nH2O===CO2+(n+1)H2O

[0026] Moreover, the heat gained from the released energy is dissipated from the water, producing vapor. The pressure of the reaction mixture (carbon dioxide and vapor) within the reaction vessel prior to the radiation may also vary. In certain embodiments, the pressure of carbon dioxide gas is 100 psi or less. In particular embodiments the pressure is about 15 psi, or about 100 psi.

[0027] FIG. 1 is a schematic diagram of a typical embodiment of a laser controlled decomposition apparatus for a laser controlled decomposition process. It shows a schematic of one embodiment of a laser controlled decomposition system 10 for the laser controlled decomposition process 20 illustrated in FIG. 2.

[0028] An Er:YAG laser 11 operating at 2.94 microns launches mid-infrared light 12 into the reaction chamber 13 through the glass wall of the chamber (vessel). Air inside the chamber is evacuated by a conventional vacuum pump 14 via a 3-way stopcock 15 before carbon dioxide gas and water vapor 16 are inserted into the vessel 13. Carbon dioxide 17 is inserted in the reaction chamber via the same 3-way stopcock inlet 15 using conventional techniques in order to have sufficiently high pressure to ensure efficient decomposition by mid-infrared light 12. The reaction chamber is a standard vessel designed to handle gases at relatively high pressure. Optimal photo-decomposition is obtained by utilizing a glass vessel to favor the formation of carbon dioxide-water vapor complex and to increase the efficacy of the mid-infrared light 12 within the CO2 ambient. The use of an Er:YAG laser at 2.94 microns is not a requirement to achieve photo-decomposition of the carbon dioxide gas; UV-wavelength laser beams or far UV-wavelengths are, in fact, used in the photolysis of carbon dioxide. However, the high energy obtained by photo-excitation of carbon dioxide-water complex, and the formation of activated species will increase the effectiveness of the process. Similarly, there is no restriction to mid-infrared light at 2.94 microns, but photons of sufficient energy are provided at 2.94 microns to excitate the OH bonds. Other laser beams such as a HF laser beam with a wavelength of 2.7 microns may be appropriate for the process.

[0029] FIG. 2 shows a flow diagram of the process 20 of laser controlled decomposition (LCD) of carbon dioxide that requires the evacuation 21 of air from the reaction chamber 13 and the placing 22 of about 15 psi of the mixture carbon dioxide gas-water vapor within the LCD reaction chamber. The placing 23 of additional carbon dioxide gas at pressure ranging from 15 to 100 psi into the LCD reaction chamber enables the formation of important amounts of carbon and carbon-oxygen structures after the complexation 24 of carbon dioxide and vapor has occurred. Launching 25 of mid-Infrared (m-IR) photons of m-IR light 12 from Er:YAG laser 11 or another low energy photon source into LCD reaction chamber 13 in an either pulsed or continuous wave mode enables the photo-excitation 26 of the carbon dioxide-water vapor complex into activated species and releasing of energy (heat). The activated species enable a spontaneous reacting 27 with carbon dioxide to form carbon and carbon-oxygen structures. The relevant energy produced in the photo-excitation 26 can assist the reacting 27 between the activated species and CO2 favoring the thermal decomposition 28 of CO2 into carbon and oxygen. Details of this process are described below.

[0030] This process relies in the hydration of carbon dioxide gas and on the absorption properties of hydrated carbon dioxide intermediates (carbon dioxide-vapor complex and carbonic acid) in the m-IR region of the electromagnetic spectrum. Carbonic acid and its isomeric weakly bond carbon dioxide-water complex have been shown to be formed in gas phase, see Carbonic acid in the gas phase and its astrophysical relevance, by W. Hage, K. R. Liedl, A. Hallbrucker, in Science (1998), vol 279, pp. 1332-1335; Structure and internal rotation of H2OCO2, HDOCO2, and D2OCO2 van der Waals complexes, by K. I. Peterson and W. Klemperer, in J. Chem. Phys. (1984), vol. 80, pp. 2439-2445.

[0031] FIG. 3 shows the absorption spectrum of water in the region from 0.1 to 600 m, Potential applications of Erbium:YAG laser in periodontics by I. Ishikawa, A. Aoki and A. A. Takasaki in J. Periodont. Res. (2004), vol. 39, pp. 275-285. The strongest absorption is observed at about 3.00 m where the OH bonds are easily excited by the m-IR photons of an Er:YAG laser operating at 2.94 m with releasing of energy. The great amount of heat produced (estimated temperature around 3300 K) enables the thermal dissociation of CO.sub.2 into carbon and oxygen. Thermal dissociation of CO.sub.2 has shown that, for each total pressure, exists a critical temperature (typically below 700 C.) above which the decomposition products of carbon and oxygen, see The thermal decomposition of carbon dioxide by M. H. Lietzke and C. Mullins in J. inorg. nucl. Chem. (1981), vol. 43, pp. 1769-1771.

[0032] An example of LCD process used to induce decomposition of CO.sub.2 gas is given by:

(I) Interaction of Water Vapor with CO.sub.2 Produces

CO.sub.2g+H.sub.2O.sub.g.fwdarw.CO.sub.2H.sub.2O complex, (2)

(II) Photo-Activation of the CO.sub.2H.sub.2O Complex According to the Reaction

CO.sub.2H.sub.2O+h.fwdarw.CO.sub.2H.sub.2O+energy (3)

(III) Activated Complex Reactions with CO.sub.2 and Thermal Decomposition of CO.sub.2 Produce

##STR00001##

The resulting product C.sub.mO.sub.n is mixed with ablated glass and form a white deposit like cotton candy. The mixture is slightly soluble in water.

[0033] The following examples depict the various methods of the invention. These examples are intended to illustrate, not limit, the present invention.

EXAMPLE 1

[0034] The apparatus used in this example is schematically described in FIG. 1. It is constructed in glass so that the laser beam is applied through the apparatus. Carbon dioxide at 14 psi was firstly flowed in liquid water and then the mixture carbon dioxide-water vapor was introduced into the evacuated apparatus, and waited for 15-30 minutes before the irradiation with a 2.94 microns Er:YAG laser beam at 100 mJ. As a result, bright flashes of light with local and confined melting of the glass apparatus were observed as well as the production of very small amounts of carbon and carbon-oxygen particles. The melting of glass was due to the release of energy during the decomposition of the carbon dioxide-water vapor complex. SEM images taken of the confined melted glass indicated an increase of temperature during the irradiation of the carbon dioxide-water vapor complex. An EDS spectrum of the glass reactor wall after laser irradiation indicated the production of carbon and carbon-oxygen structures. For comparison, carbon dioxide at pressure of 14 psi without water vapor was irradiated with the same above laser beam (at 100 mJ and 135 mJ). As a result, no flashes of light were observed as well as the local melting of glass.

EXAMPLE 2

[0035] The procedure of Example 1 was repeated, except that an irradiation beam at 80 mJ, 135 mJ and 200 mJ were used instead of 100 mJ. As a result, it was confirmed that for all the irradiation conditions carbon and carbon-oxygen structures were produced, as well as the local melting of the glass wall of the vessel.

EXAMPLE 3

[0036] The procedure of Example 2 was repeated, except that the apparatus was first washed with a mixture sulfuric acid (99%)/hydrogen peroxide (30%) 3:1, rinsed 4 times with Milli Q water and dried in an oven at 80 C. Also in this case, it was confirmed that the decomposition of carbon dioxide occurred with release of energy and formation of carbon and carbon-oxygen structures.

[0037] FIG. 4 shows the emission spectra of the flash light during laser irradiation. The peak at 630 nm is the guide laser. The spectra get a little noisy at high wavelengths, but that is to be expected since the spectrometer is not as sensitive in that range and in the emission spectrum of black-body light at 3300 K. Overall, the spectra of flash light roughly like blackbody spectra, but don't fit perfectly. The best fit temperature is about 3300 K. The spectra (from 320 to 800 nm) were taken with a USB2000 spectroradiometer (Ocean Optics Inc. Dundein, Fla.) coupled with a 1000 um diameter fiber optic cable. The integration time was 300 msec. The spectra had the baseline stripped and were then were corrected for the spectral sensitivity of the detector, but not calibrated in absolute units. So the values are given in relative watts.

[0038] During testing SEM images of the Pyrex reactor wall after laser irradiation showed evidence of the transformation of the glass silica due to the temperature rise and an EDS spectrum of the area of glass irradiated by laser in the presence of CO.sub.2 and vapor. A micro-photo detail showed the material formed inside the glass vessel during the laser irradiation of CO.sub.2 at a pressure of 100 psi. Another micro-photo detail showed the carbon particles formed inside the glass vessel during the laser irradiation of CO.sub.2. Melted silica was also visible (white brilliant points) in the micro-photos. An SEM image showed the carbon-oxygen structures on the vertical surface of the glass vessel during the Er:YAG laser irradiation of CO2.

[0039] It should be clear at this time that a method and apparatus for producing carbon-oxygen structures by the Decomposition of Carbon Dioxide Gas has been provided. However the present invention is not to be considered limited to the forms shown which are to be considered illustrative rather than restrictive.