Cold plasma ozone generator

Abstract

The present invention provides a cold plasma ozone generator, comprising: an inlet gas port; at least one in-electrode, said in-electrode having a plurality of holes substantially at a perimeter of the same; said plurality of perimeter holes are in fluid communication with said inlet gas port, said plurality of perimeter holes configured to allow said dry gas to pass therethrough; at least one out-electrode, said out-electrode having at least one hole at the center of the same, said at least one hole configured to allow gas to pass therethrough; said in-electrode and said out-electrode configured to maintain said high voltage AC therebetween; at least one spacer between said in-electrode and said out-electrode, said spacer configured to maintain a constant-width gap between said in-electrode and said out-electrode; an outlet port.

Claims

1. A cold plasma ozone generator to generate ozone from oxygen in a gas, said cold plasma ozone generator comprising: an inlet gas port; at least one in-electrode, said in-electrode having a plurality of holes proximate a perimeter of the in-electrode; said plurality of perimeter holes are in fluid communication with said inlet gas port, said plurality of perimeter holes configured to allow gas to pass therethrough; at least one out-electrode, said out-electrode having at least one hole at the center of the out-electrode, said at least one hole configured to allow gas to pass therethrough; said in-electrode and said out-electrode configured to maintain AC voltage therebetween; at least one spacer between said in-electrode and said out-electrode, said spacer configured to maintain a constant-width gap between said in-electrode and said out-electrode, said constant-width gap configured to allow said gas to pass through said plurality of perimeter holes in said in-electrode and then radially inward from the perimeter of the gap to said at least one hole in said out-electrode; and an outlet port in fluid communication with said at least one hole in said out-electrode.

2. The cold plasma ozone generator of claim 1, wherein a thickness of said gap is in a range between about 0.1 mm and about 0.5 mm.

3. The cold plasma ozone generator of claim 2, wherein thickness of said gap is about 0.3 mm.

4. The cold plasma ozone generator of claim 1, wherein said gas is configured to flow radially inward from said plurality of perimeter holes to said at least one central hole to allow said gas to contact substantially all of an area in said gap between said electrodes so as to maximize an amount of ozone produced from said gas.

5. The cold plasma ozone generator of claim 1, wherein said AC voltage is about 1800 volts.

6. The cold plasma ozone generator of claim 1, wherein a frequency of said AC voltage is between about 7 kHz and about 30 kHz.

7. The cold plasma ozone generator of claim 6, wherein a frequency of said AC voltage AC is about 8 kHz.

8. The cold plasma ozone generator of claim 1, wherein an amount of ozone generated is controllable by adjustment of a frequency of said AC voltage AC.

9. The cold plasma ozone generator of claim 1, wherein a coating of ceramic dielectric material is bonded to at least one of said electrodes.

10. The cold plasma ozone generator of claim 9, wherein said ceramic dielectric coating is on a side of said at least one electrode facing said gap.

11. The cold plasma ozone generator of claim 9, wherein total thickness of said ceramic dielectric coating is about 75 to about 125 pm.

12. The cold plasma ozone generator of claim 9, wherein said ceramic dielectric coating is produced by means of a screen printing technique, followed by curing in an oven.

13. The cold plasma ozone generator of claim 1, wherein said gas is selected from a group consisting of oxygen, air, and any combination thereof.

14. The cold plasma ozone generator of claim 13, wherein said air is dry air.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) FIG. 1a is a perspective view of an embodiment of a cold plasma ozone generator of the present invention;

(2) FIG. 1b is a side elevation cross-sectional view of the embodiment of FIG. 1a;

(3) FIG. 1c is an exploded perspective view of the cold plasma ozone generator of FIG. 1a;

(4) FIG. 1d is a perspective view of another embodiment of a cold plasma ozone generator of the present invention;

(5) FIG. 1e is a side cross-sectional view of the embodiment of FIG. 1d;

(6) FIG. 1f shows an exploded view of the embodiment of an ozone generating cell of FIG. 1d;

(7) FIG. 1g shows the outside of the outlet enclosure of the embodiment of an ozone generating cell of FIG. 1d;

(8) FIG. 1h shows the inside of the outlet enclosure of the embodiment of an ozone generating cell of FIG. 1d;

(9) FIG. 2 shows the gas flow inside an ozone generator cell;

(10) FIG. 3a-c illustrates an embodiment of a screen-printing process for laying down the precursor layers to form a dielectric coating on a stainless steel electrode;

(11) FIG. 4a illustrates the amount of power needed to generate, from an oxygen feed, a concentration of ozone in the exit gas from the ozone generator;

(12) FIG. 4b illustrates the amount of power needed to generate, from a dry air feed, a concentration of ozone in the exit gas from the ozone generator;

(13) FIG. 5a-b illustrates the effect of oxygen flow rate on ozone generation for an oxygen input gas; and

(14) FIG. 6a-b illustrates the effect of air flow rate on ozone generation for an input gas of dry air.

DETAILED DESCRIPTION OF THE INVENTION

(15) The following description is provided, alongside all chapters of the present invention, so as to enable any person skilled in the art to make use of said invention and sets forth the best modes contemplated by the inventor of carrying out this invention. Various modifications, however, will remain apparent to those skilled in the art, since the generic principles of the present invention have been defined specifically to provide a means and method for efficiently generating ozone in a flat plate type dielectric barrier discharge (DBD) plasma reactor.

(16) The term ‘facility’ hereinafter refers to a portion of an edifice, an edifice or a limited number of edifices supplied with water from a single source. Typically, the source is a pipe connected to a municipal water supply system. Non-limiting examples of a facility include a house, a business, a school, and an apartment building.

(17) The term ‘about’ hereinafter refers to a range of plus or minus 25% around the nominal value. If a range of values is given, the extreme limits of the range therefore become (75% of the minimum of the range) to (125% of the maximum of the range).

(18) The present invention is an improved flat plate type dielectric barrier discharge (DBD) plasma reactor.

(19) The improved flat plate DBD cell for generating ozone has a generally convergent radial gas flow; the net gas flow direction through the plasma gap is from the outer edges of the cell inward towards an exit port in the approximate center of the cell. This eliminates parasitic arcing at the perimeter, greatly increases the life of the perimeter seal, and provides a homogenous gas flow which increases ozone output.

(20) Prior art flat plate DBD cells are prone to arcing outside of the cell, which becomes more likely as the ambient humidity increases. Arcing outside the cell produces ozone outside of the cell, which is extremely undesirable because this ozone ends up inside the electronics cabinet and in the ambient air.

(21) In the improved flat plate DBD cell of the present invention, external arcing is eliminated due to the long electrical path, to the isolation provided by the enclosures of the electrodes and by a design that makes it unnecessary to use wires to connect the electrodes to the power supply circuit. In some embodiments, the electrodes are assembled on the PCB and the lines connecting the electrodes to the power supply are inside the PCB and isolated from the environment so no external arcing can occur. In other embodiments, the electrodes are connected to the power supply by connectors inside the electrodes themselves, again eliminating wires and preventing eternal arcing.

(22) The cell design allows both electrodes to be operated at high voltage, therefore, instead of one electrode being essentially at ground with the full voltage applied to the other electrode, each electrode has at a voltage difference from ground of approximately half the total voltage difference between the electrodes, reducing the effective voltage difference with respect to ground by half and increasing the safety of the device.

(23) Most prior art ozone cell construction requires that one electrode be at ground potential. The present invention has no permanent ground electrode, it has a “floating ground” and is designed to be able to operate either with one electrode grounded and the other at 1.8 KV or preferably with both electrodes at 0.9 KV (generally 180 degrees out of phase from each other). Operating both electrodes at high voltage effectively halves the voltage difference with respect to ground in any portion of the cell, which together with the generous radii of all external surfaces eliminates problems of corona, arcing and ozone formation on the outside of the cell.

(24) This greatly increases the service life of the electrodes because both electrodes have equal electric and mechanical stresses, as opposed to prior art ozone generators where one electrode is always ground potential and substantially unstressed, while the other undergoes both electrical and mechanical stresses and thus will be ruined faster than the ground electrode.

(25) This greatly increases safety, makes mounting and weather protection less critical and UL and other safety approval less difficult, and allows the use of less expensive and more commonly available high-voltage transformers such as the midpoint ground type of neon-sign transformer. The plasma cell of the present invention ignites easily at all temperatures without requiring a special starting circuit.

(26) The high voltage necessary to drive the corona discharge is produced by a power supply which includes a transformer capable of transforming low DC voltage to a high AC voltage. In prior art ozone generators, the voltage is usually between 5 and 25 kilovolts. Minimizing the voltage at which an ozone generator operates is of very great importance, for this not only minimizes the high-voltage stress on all components for longer life, but is also safer, minimizes arcing and external corona, and decreases the cost of the transformer. At a fixed voltage, the quantity of ozone generated is roughly proportional to the continuous wave AC frequency or the pulse repetition rate until an upper frequency limit is reached. The practical upper limit for efficient ozone generation usually lies between 600 and 2500 Hz, and depends on corona cell geometry, properties of the dielectric used and cooling efficiency.

(27) In the present invention the corona is operated at a relatively low voltage, about 1800 volts and at a relatively high frequency, on the order of 8 kHz, at which the corona is stable and homogeneous and the average output power and therefore the amount of ozone generated is controlled by adjusting the frequency (between about 7 kHz and about 30 kHz) rather than the voltage.

(28) This high frequency cold plasma ozone generator offers a very compact design due to smaller transformers and corona cells needed to operate it. As the corona is occurring up to 8,000 times per second, there is no need for a large air gap and a high voltage.

(29) This high frequency cold plasma ozone generator is very energy efficient and compact in size allowing for a very flexible platform to either use multiple cells for redundancy or other configuration changes.

(30) Typically, trade-offs in design parameters of a corona cell for an ozone generator include the width of the discharge gap (the distance between the faces of the electrodes) and the voltage necessary to achieve an appropriate voltage gradient between the electrodes. Generally, the wider the discharge gap, the greater the voltage must be and the greater the current necessary to sustain that higher voltage. Higher voltages in ozone generators can be problematic, causing a significant amounts of the power supplied to the ozone generator to be dissipated as heat, which can destroy some or all of the ozone which is formed. Thus, to obtain an optimum net yield of ozone from the ozone formation reaction, it is advantageous to have a narrower gap between the electrodes, thereby lowering the voltage needed to achieve the necessary potential for the reaction. Of course, with lower voltages, lower currents can be employed and so less power will be dissipated into heat. The net effect, then, of a narrower discharge gap is a more efficient ozone generator, with more ozone obtainable from the system since, by utilizing lower voltages and, therefore, lower currents, to achieve the ozone formation reaction, less heat dissipation occurs and less of the ozone produced through the ozone formation reaction is destroyed by heat after formation.

(31) Unlike prior art ozone generators that require air or water to cool the electrodes, the present invention does not require any kind of electrode cooling since, because the voltage is small (1700-1800 V) and the gap is very narrow (200-400 micron), the amount of power dissipated as heat is small enough that, under normal operating conditions, the electrodes will not heat significantly

(32) This invention is a very high efficiency cold plasma ozone generator, with a very high ozone yield of about 90 gram O.sub.3/kWh when dry air used as the feed gas and 267 gram O.sub.3/kWh when oxygen used as the feed gas.

(33) The cold plasma ozone generator can operate with a feed gas of dry air, a feed gas of oxygen and any combination thereof.

(34) In the present invention, both electrodes are coated with ceramic non-porous dielectric material.

(35) The dielectric layer prevents the desired controlled silent discharge from changing into a glow or arc discharge that would damage or even destroy the electrodes due to high currents. Therefore, the electrodes of the present invention have very long life. In addition, ensuring a silent discharge evenly distributed across the surface of the electrodes results in an optimum yield of ozone, which leads to a higher efficiency ozone generator.

(36) The discharge utilizing non-porous dielectric barrier was more uniform and synthesized ozone with higher energy efficiency than the discharge utilizing smooth-surface dielectric barrier.

(37) The non-porous dielectric discharge of the present invention uses less than 30% of the power delivered by the prior art rough-surface dielectric discharge in order to achieve the same level of ozone yield.

(38) FIG. 1a is a perspective view of the embodiment. This view illustrates the enclosures (6) for the electrodes, the PCB electrode with its conductive pad (4), the two 90 degree ozone resistant fittings forming the inlet gas port (10) and the outlet gas plus ozone port (20), and the screws (9) that fasten an electrode enclosure (6), a PCB electrode (4) and a PCB spacer (11) to the main high voltage AC power supply PCB (3). The conductive electrodes with a non-porous ceramic dielectric coating and the sealing components are not visible in this view.

(39) FIG. 1b is a side cross-sectional view of the embodiment of FIG. 1a

(40) The electrodes (1, 2) are preferably plates of stainless steel coated with ceramic dielectric material, and are preferably of the same size and shape and have the same non-porous ceramic dielectric coating. They can be generally circular, oval or elliptical, it can form a rounded rectangle, and any combination thereof, as long as all conductive edges are rounded to reduce non-linear high voltage field effects which can lead to parasitic corona and arcing.

(41) The in-electrode (1) has a plurality of holes in the perimeter, so that gas from the inlet fitting (10) flows downward and outward to the perimeter of the in-electrode, through the perimeter holes, and then radially inward from the perimeter of the gap to its center.

(42) The out-electrode (2) has at least one hole, and preferably a single hole, in the center, so that gas flows directly from the out-electrode to the outlet gas port (20).

(43) The PCB spacer (11) design provides accurate spacing and accurate parallelism between the in- and out-electrodes (1, 2), resulting an accurate, and uniform plasma gap between the generally flat central portions of the faces of the in-electrode (1) and the out-electrode (2).

(44) The thickness of the plasma gap is dependent on the thickness of the non-porous ceramic dielectric coating, thickness of the main PCB (3), PCB spacer (11), PCB electrode (4) and on the geometry of the in- and out-electrodes (1, 2). In a preferred embodiment, the gap is about 0.3 mm. It can range from about 0.1 mm to about 0.5 mm.

(45) Since the cell is sealed, the gas cannot leak from the cell. The electrodes are sealed externally by enclosure O-ring (5), forming a perimeter seal with the main PCB (3) and the PCB electrode (4). Preferably, the O-ring (5) is made of non-conductive ozone-resistant material such as silicone, PVDF or PTFE, while the plasma gap is sealed by a Teflon O-ring (8) that seals the gaps and prevents ozone from leaking and damaging the PCB's. Another important seal is the electrode O-ring (7) which prevents ozone from escaping from the cell and damaging other components like electrode enclosure (6) and the PCB's.

(46) This sealing technology provides secure hermetic sealing that prevents leaks of both feed gas and ozone. Therefore, this design enables use of less-expensive non ozone-resistant material for the electrode enclosures (6), PCB spacer (11), and the PCB electrode (4). This also allows the option of assembling the cold plasma reactor on the main high voltage AC power supply PCB (3).

(47) FIG. 1c is an exploded perspective view of the cold plasma ozone generator of FIG. 1a. This view illustrates that the assembly and the maintenance of this electrode is very simple. These components are preferably held in their assembled position by 3 screws (11) from each side.

(48) Unlike prior art ozone generators, the cell is an integral part of the high voltage AC power supply PCB (3), rather than being separate from it. This allows the lines that provide high voltage to the electrodes to be internal connections within the main PCB (3), rather than being external wired connections. This increases the safety of the ozone generator, makes approval for safety (such as UL approval) less difficult, and reduces both assembly time and the cost of assembly.

(49) FIGS. 1d-h show another embodiment of the cold plasma ozone generator of the present invention. Part numbers are different between the embodiment of FIGS. 1a-c and the embodiment of FIGS. 1d-h.

(50) FIG. 1d is a perspective view of the embodiment. This view illustrates the enclosures (4, 5) for the electrodes (3, 2, not shown), the two 90 degree ozone resistant fittings forming the inlet gas port (8) and the outlet gas plus ozone port (18), and the screws (10) that fasten together the electrode enclosures (4, 5) and the electrode spacer (1). Also shown is the spring mechanism (25) which ensures good contact between the electrodes and the PCB

(51) FIG. 1e is a side cross-sectional view of the embodiment of FIG. 1d

(52) The in-electrode (2) and the out-electrode (3) are preferably plates of stainless steel coated with ceramic dielectric material, and are preferably of the same size and shape and have the same thickness of the same type of non-porous ceramic dielectric coating. They can be generally circular, oval or elliptical, it can form a rounded rectangle, and any combination thereof, as long as all conductive edges are rounded to reduce non-linear high voltage field effects which can lead to parasitic corona and arcing.

(53) In less-preferred embodiments, at least one of the following can be true: at least one of the in-electrode and the out-electrode lacks a non-porous ceramic dielectric coating, the in-electrode and the out-electrode have different thicknesses of non-porous ceramic dielectric coating, and the in-electrode and the out-electrode have different types of non-porous ceramic dielectric coating,

(54) The electrode spacer (1) design provides accurate spacing and accurate parallelism between the in- and out-electrodes (2, 3), resulting an accurate, and uniform plasma gap between the generally flat central portions of the faces of the in-electrode (2) and the out-electrode (3).

(55) The thickness of the plasma gap is dependent on the thickness of the non-porous ceramic dielectric coating, which is on the sides of the in-electrode and the out-electrode that face each other, so that the surface of each non-porous ceramic dielectric coating forms one face of the gap; on the thickness of the electrode spacer (1); and on the geometry of the in- and out-electrodes (2, 3). In a preferred embodiment, the gap is about 0.3 mm. It can range from about 0.1 mm to about 0.5 mm.

(56) Since the cell is sealed, the gas cannot leak from the cell. The electrodes are sealed externally by the enclosure O-rings (7), forming a perimeter seal with the enclosures (4, 5), the electrode spacer (1) and the in- (2) and out- (3) electrodes. Preferably, the O-rings (7) are made of non-conductive ozone-resistant material such as silicone, PVDF or PTFE, while the out-electrode O-ring (6) which prevents ozone from escaping from the cell and damaging other components can be made of non-conductive ozone-resistant material such as silicone, PVDF or PTFE, or can be made of Teflon.

(57) This sealing technology provides secure hermetic sealing that prevents leaks of both feed gas and ozone. Therefore, this design enables use of less-expensive non ozone-resistant material for the electrode enclosures.

(58) In this embodiment, the PCB's and the electrodes are separately replaceable, thereby reducing the cost of repairs.

(59) FIG. 1f shows an exploded view of the embodiment of an ozone generating cell of FIG. 1d.

(60) The inlet gas port (8) is at the top, with the screws (10) below the inlet gas port (8) and the inlet enclosure (4) is between the screws (10) and the upper enclosure O-ring (7). Below the upper enclosure O-ring (7) is the in-electrode (2).

(61) The in-electrode (2) has a plurality of holes (21) in the perimeter, so that gas from the inlet fitting (8) flows downward and outward to the perimeter of the in-electrode, through the perimeter holes, and then radially inward from the perimeter of the gap to its center.

(62) Below the in-electrode (2) is the spacer (1), and below the spacer is the out-electrode (3). In this embodiment, the out-electrode (3) has a single hole (31) in the center, through which gas can leave the gap and enter the outlet gas port (18).

(63) Below the out-electrode (3) is the out electrode O-ring (6), and below this, the lower enclosure O-ring (7), the outlet enclosure (5), which comprises voltage connectors to ensure that there is a good electrical connection between the voltage contacts on the PCB and the in- (2) and out- (3) electrodes, so that the high voltage is efficiently transferred from the PCB to the electrodes (2, 3).

(64) Below the outlet enclosure (5) is the outlet gas port (18).

(65) FIG. 1g-h shows the outside (FIG. 1g) and inside (FIG. 1h) of the outlet enclosure (5), showing the strengthening ribs (51) on the interior of the outlet enclosure (5). The ribs both stiffen and lighten the outlet enclosure (5).

(66) FIG. 2 shows the gas flow inside a cold plasma ozone generator cell. The gas feed, which is typically atmospheric air, but can be air enriched with oxygen or pure oxygen, enters through the inlet gas port (9) and passes to the center of the upper surface of the in-electrode (1). The flow then passes radially across the upper surface of the in-electrode (1) to the perimeter of in-electrode (1) (represented by black arrows) and enters the plasma gap through the holes in the perimeter of the in-electrode (1).

(67) The gas then flows radially inward (white arrows) from the perimeter to the center of the in- (1) and out- (2) electrodes. The gas then exits from the plasma gap via the single hole in the center of the out-electrode (2) and exits the cold plasma ozone generator through the corresponding ozone outlet fitting (10).

(68) The electrodes (1, 2) are kept at a high voltage supplied by an AC power supply (3). Since the voltage across the electrodes is uniform and the spacing between the electrodes is uniform, there will be a uniform plasma in the plasma gap. As the air flows through the plasma gap, it is subjected to repeated micro discharges, which convert some of the oxygen molecules in the air into ozone molecules. Therefore, the air flowing out of the cold plasma ozone generator will be ozone enriched.

(69) The radial flow ensures that the air contacts substantially all of the area in the plasma gap between the electrodes (1, 2) and that the air spends sufficient time between the electrodes so as to maximize the amount of ozone in the exit gas.

(70) This results in a very reliable and efficient cold plasma ozone generator with a high and stable yield ozone. Typically, the yield is about 90 gram O.sub.3/kWh when dry air used as the feed gas and 267 gram O.sub.3/kWh when oxygen is used as the feed gas.

(71) Non-Porous Ceramic Dielectric Coating on Electrodes

(72) In some embodiments of the system of the present invention, the non-porous ceramic dielectric coating on the electrodes is a multilayer thick-film coating. This non-porous ceramic dielectric coating can be produced using a screen-printing technique, as shown in FIG. 3a-c. FIG. 3a shows the beginning of the process of laying down one layer; FIG. 3b shows an intermediate stage in the process of laying down the layer, and FIG. 3c shows the end of the process of laying down the layer. In this embodiment, the electrode (120) is firmly held by a substrate (110) so it does not slip during processing. A mesh screen (160) is held by a frame (130) at a distance above the electrode (110), the distance small enough that pressure from a squeegee (140) can cause the mesh screen (160) to come into contact with the electrode (120). On the upper side of the screen is a precursor for a dielectric, in the form of a paste (150). On the lower side of the screen (160) and adhering to the screen (160) is a layer of emulsion (170); the holes (175) in the emulsion (170) allow the paste (150) to pass through the emulsion (170) and come into contact with the electrode (120).

(73) At the beginning of the process, the paste dielectric precursor (150) forms a layer on top of the mesh screen (160).

(74) In order to form the image on the electrode (120), the squeegee (140) is pressed down onto the mesh screen (160), bringing the portion of the emulsion (170) directly under the squeegee (140) into contact with the electrode (120). As shown in FIG. 3b, the squeegee (140) is them moved across the upper surface of the electrode (120), pressing paste (150) through the holes (175) in the emulsion (170) and onto the electrode (120). The squeegee also presses the paste (150) ahead of itself.

(75) At the end of the process of laying down the layer (FIG. 3c), the squeegee (140) has crossed entirely over the electrode (120), and has forced paste (150) through all the holes (175) in the emulsion (170). A stop (180) prevents unnecessary loss of paste, which can be reused for another electrode or another layer. The mesh screen (160) can now be removed and the paste precursor (150) processed into a non-porous ceramic dielectric coating.

(76) The dielectric precursor layer is then cured, transforming it into a non-porous ceramic dielectric coating. In the curing process, the paste-coated electrode is placed in a drying oven at about 150 degrees C. for a few minutes (<10 minutes) to dry the paste and vaporize elements such as solvents and adhesion promoters. The electrode is then placed in an oven and heated, at a predetermined rate, to about 900 degrees C. The oven temperature is held at about 900 degrees C. for about 15 minutes, after which the electrode is cooled at a predetermined rate.

(77) In a typical embodiment of the coated electrodes of the present invention, the above process, of screen printing a precursor layer, drying in a drying oven and then heating to about 900 degrees C. is repeated 3-5 times, each time producing a ceramic dielectric layer about 20 μm to about 25 μm thick so that the total thickness of the non-porous ceramic dielectric coating is about 75 μm to about 125 μm. In this manner, the non-porous ceramic dielectric coating can be produced without cracks.

(78) In this process, the high temperature combustion process causes the first layer of the non-porous ceramic dielectric coating to migrate a few μm into the surface of the stainless steel electrode, thereby improving the adhesion of the non-porous ceramic dielectric coating to the electrode.

(79) In preferred embodiments, the non-porous ceramic dielectric coating material has about the same coefficient of expansion as the stainless steel of the electrode, so that the non-porous ceramic dielectric coating will not crack or spall during heating or cooling of the electrode during use.

(80) In general, the above-described process will not produce a completely homogenous non-porous ceramic dielectric coating nor a non-porous ceramic dielectric coating of completely uniform thickness. However, the uniformity will be sufficient to prevent formation of air pockets, and the non-porous ceramic dielectric coating will be flat enough and homogeneous enough to prevent arcing or breakdown that can reduce the reliability and lifetime of the electrodes.

Example 1

(81) FIG. 4a-b illustrates the amount of power needed to generate a concentration of ozone in the exit gas from the cold plasma ozone generator. FIG. 4a illustrates the yield if the input gas (the feed gas) is oxygen, while FIG. 4b illustrates the yield if the input gas (the feed gas) is dry air. For both oxygen input gas and dry air input gas, the yield decreases as the concentration of ozone in the exit gas increases. In other words, the amount of power needed to generate a concentration of ozone increases faster than the amount of ozone. Therefore, for the cold plasma ozone generator of the present invention, it is preferable to generate a somewhat smaller concentration of ozone in the exit gas in order to minimize the power requirements of the cold plasma ozone generator.

Example 2

(82) FIG. 5a-b illustrates the effect of oxygen flow rate on ozone generation for an oxygen input gas. The test was performed at 25 degrees C., using an Air Sep Onyx Plus Oxygen Concentrator to generate the input gas. The ozone in the output was measured using an Ozone Analyzer BMT 964. As the oxygen flow rate through the cold plasma ozone generator increased, the amount of ozone generated also increased (FIG. 5a), but the concentration of ozone in the exit gas decreased (FIG. 5b), since the amount of ozone generated increased more slowly than the flow rate.

Example 3

(83) FIG. 6a-b illustrates the effect of air flow rate on ozone generation for an input gas of dry air. The test was performed at 25 degrees C., using a silica gel air dryer to remove water from the input gas. The ozone in the output was measured using an Ozone Analyzer BMT 964. As the air flow rate through the cold plasma ozone generator increased, the amount of ozone generated also increased (FIG. 6a), but the concentration of ozone in the exit gas decreased (FIG. 6b), since the amount of ozone generated increased more slowly than the flow rate.

(84) For both an oxygen input gas and an air input gas, the ozone concentration changed approximately linearly with flow rate. However, although the ozone output increased approximately linearly with flow rate for the air input, it only increased sub-linearly with flow rate for the oxygen input gas.

(85) In the foregoing description, embodiments of the invention, including preferred embodiments, have been presented for the purpose of illustration and description. They are not intended to be exhaustive or to limit the invention to the precise form disclosed. Obvious modifications or variations are possible in light of the above teachings. The embodiments were chosen and described to provide the best illustration of the principals of the invention and its practical application, and to enable one of ordinary skill in the art to utilize the invention in various embodiments and with various modifications as are suited to the particular use contemplated. All such modifications and variations are within the scope of the invention as determined by the appended claims when interpreted in accordance with the breadth they are fairly, legally, and equitably entitled.