Patent Application
20180020508
Not Applicable
The disclosure concerns a method for heating materials by application of radio frequency (“RF”) energy, also known as electromagnetic energy. In particular, the disclosure concerns an advantageous method for RF heating of materials with a low or zero electric dissipation factor, magnetic dissipation factor, and electrical conductivity, such as petroleum ore. For example, the disclosure enables efficient, low-cost heating of bituminous ore, oil sands, oil shale, tar sands, or heavy oil.
Bituminous ore, oil sands, tar sands, and heavy oil are typically found as naturally occurring mixtures of sand or clay and dense and viscous petroleum. Recently, due to depletion of the world's oil reserves, higher oil prices, and increases in demand, efforts have been made to extract and refine these types of petroleum ore as an alternative petroleum source. Because of the extremely high viscocity of bituminous ore, oil sands, oil shale, tar sands, and heavy oil, however, the drilling and refinement methods used in extracting standard crude oil are typically not available. Therefore, bituminous ore, oil sands, oil shale, tar sands, and heavy oil are typically extracted by strip mining, or in situ techniques are used to reduce the viscocity of viscocity by injecting steam or solvents in a well so that the material can be pumped. Under either approach, however, the material extracted from these deposits can be a viscous, solid or semisolid form that does not easily flow at normal oil pipeline temperatures, making it difficult to transport to market and expensive to process into gasoline, diesel fuel, and other products. Typically, the material is prepared for transport by adding hot water and caustic soda (NaOH) to the sand, which produces a slurry that can be piped to the extraction plant, where it is agitated and crude bitumen oil froth is skimmed from the top. In addition, the material is typically processed with heat to separate oil sands, oil shale, tar sands, or heavy oil into more viscous bitumen crude oil, and to distill, crack, or refine the bitumen crude oil into usable petroleum products.
The conventional methods of heating bituminous ore, oil sands, tar sands, and heavy oil suffer from numerous drawbacks. For example, the conventional methods typically utilize large amounts of water, and also large amounts of energy. Moreover, using conventional methods, it has been difficult to achieve uniform and rapid heating, which has limited successful processing of bituminous ore, oil sands, oil shale, tar sands, and heavy oil. It can be desirable, both for environmental reasons and efficiency/cost reasons to reduce or eliminate the amount of water used in processing bituminous ore, oil sands, oil shale, tar sands, and heavy oil, and also provide a method of heating that is efficient and environmentally friendly, which is suitable for post-excavation processing of the bitumen, oil sands, oil shale, tar sands, and heavy oil.
One potential alternative heating method is RF heating. “RF” is most broadly defined here to include any portion of the electromagnetic spectrum having a longer wavelength than visible light. Wikipedia provides a definition of “radio frequency” as comprehending the range of from 3 Hz to 300 GHz, and defines the following sub ranges of frequencies:
“RF heating,” then, is most broadly defined here as the heating of a material, substance, or mixture by exposure to RF energy. For example, microwave ovens are a well-known example of RF heating.
The nature and suitability of RF heating depends on several factors. In general, most materials accept electromagnetic waves, but the degree to which RF heating occurs varies widely. RF heating is dependent on the frequency of the electromagnetic energy, intensity of the electromagnetic energy, proximity to the source of the electromagnetic energy, conductivity of the material to be heated, and whether the material to be heated is magnetic or non-magnetic. Pure hydrocarbon molecules are substantially nonconductive, of low dielectric loss factor and nearly zero magnetic moment. Thus, pure hydrocarbon molecules themselves are only fair susceptors for RF heating, e.g. they may heat only slowly in the presence of RF fields. For example, the dissipation factor D of aviation gasoline may be 0.0001 and distilled water 0.157 at 3 GHz, such that RF fields apply heat 1570 times faster to the water in emulsion to oil. (“Dielectric materials and Applications”, A. R. Von Hippel Editor, John Wiley and Sons, New York, N.Y., 1954).
Thus far, RF heating has not been a suitable replacement for conventional processing methods of petroleum ore such as bituminous ore, oil sands, tar sands, and heavy oil. Dry petroleum ore itself does not heat well when exposed to RF energy. Dry petroleum ore possesses low dielectric dissipation factors (ε″), low (or zero) magnetic dissipation factors (μ″), and low or zero conductivity. Moreover, while water may provide some susceptance at temperatures below 212° F. (100° C.), it is generally unsuitable as a susceptor at higher temperatures, and may be an undesirable additive to petroleum ore, for environmental, cost, and efficiency reasons.
An aspect of the present invention is a method for RF heating of materials with a low or zero dielectric dissipation factor, magnetic dissipation factor, and electrical conductivity. For example, the present invention may be used for RF heating of petroleum ore, such as bituminous ore, oil sands, tar sands, oil shale, or heavy oil. An exemplary embodiment of the present method comprises first mixing about 10% to about 99% by volume of a substance such as petroleum ore with about 1% to about 50% by volume of a substance comprising susceptor particles. The mixture is then subjected to a radio frequency in a manner which creates heating of the susceptor particles. The radio frequency can be applied for a sufficient time to allow the susceptor particles to heat the surrounding substance through conduction, so that the average temperature of the mixture can be greater than about 212° F. (100° C.). After the mixture has achieved the desired temperature, the radio frequency can be discontinued, and substantially all of the susceptor particles can optionally be removed, resulting in a heated substance that can be substantially free of the susceptor particles used in the RF heating process.
Other aspects of the invention will be apparent from this disclosure.
The subject matter of this disclosure will now be described more fully, and one or more embodiments of the invention are shown. This invention may, however, be embodied in many different forms and should not be construed as limited to the embodiments set forth herein. Rather, these embodiments are examples of the invention, which has the full scope indicated by the language of the claims.
In an exemplary method, a method for heating a petroleum ore such as bituminous ore, oil sands, tar sands, oil shale, or heavy oil using RF energy is provided.
The presently disclosed method can be utilized to either heat a petroleum ore that has been extracted from the earth, prior to distillation, cracking, or separation processing, or can be used as part of a distillation, cracking, or separation process. The petroleum ore can comprise, for example, bituminous ore, oil sands, tar sands, oil shale, or heavy oil that has been extracted via strip-mining or drilling. If the extracted petroleum ore is a solid or includes solids with a volume greater than about 1 cubic centimeter, the petroleum ore can be crushed, ground, or milled to a slurry, powder, or small-particulate state prior to RF heating. The petroleum ore can comprise water, but alternatively contains less than 10%, less than 5%, or less than 1% by volume of water. Most preferably, the petroleum ore can be substantially free of added water.
The petroleum ore used in the present method is typically non-magnetic or low-magnetic, and non-conductive or low-conductive. Therefore, the petroleum ore alone is not generally suitable for RF heating. For example, exemplary petroleum ore when dry, e.g. free from water, may have a dielectric dissipation factor (ε″) less than about 0.01, 0.001, or 0.0001 at 3000 MHz. Exemplary petroleum ore may also have a negligible magnetic dissipation factor (μ″), and the exemplary petroleum ore may also have an electrical conductivity of less than 0.01, 0.001, or 0.0001 S·m−1 at 20° C. The presently disclosed methods, however, are not limited to petroleum products with any specific magnetic or conductive properties, and can be useful to RF heat substances with a higher dielectric dissipation factors (ε″), magnetic dissipation factor (μ″), or electrical conductivity. The presently disclosed methods are also not limited to petroleum ore, but are widely applicable to RF heating of any substance that has dielectric dissipation factor (ε″) less than about 0.05, 0.01, or 0.001 at 3000 MHz. It is also applicable to RF heating of any substance that has have a negligible magnetic dissipation factor (μ″), or an electrical conductivity of less than 0.01 S˜m−1, 1×10−4 S·m−1, or 1×10−6 S·m−1 at 20° C.
The presently disclosed method utilizes one or more susceptor materials in conjunction with the petroleum ore to provide improved RF heating. A “susceptor” is herein defined as any material which absorbs electromagnetic energy and transforms it to heat. Susceptors have been suggested for applications such as microwave food packing, thin-films, thermosetting adhesives, RF-absorbing polymers, and heat-shrinkable tubing. Examples of susceptor materials are disclosed in U.S. Pat. Nos. 5,378,879; 6,649,888; 6,045,648; 6,348,679; and 4,892,782, which are incorporated by reference herein.
In the presently disclosed method, the one or more susceptors are for example in the form of susceptor particles. The susceptor particles can be provided as a powder, granular substance, flakes, fibers, beads, chips, colloidal suspension, or in any other suitable form whereby the average volume of the susceptor particles can be less than about 10 cubic mm. For example, the average volume of the susceptor particles can be less than about 5 cubic mm, 1 cubic mm, or 0.5 cubic mm. Alternatively, the average volume of the susceptor particles can be less than about 0.1 cubic mm, 0.01 cubic mm, or 0.001 cubic mm. For example, the susceptor particles can be nanoparticles with an average particle volume from 1×10−9 cubic mm to 1×10−6 cubic mm, 1×10−7 cubic mm, or 1×10−8 cubic mm.
Depending on the preferred RF heating mode, the susceptor particles can comprise conductive particles, magnetic particles, or polar material particles. Exemplary conductive particles include metal, powdered iron (pentacarbonyl E iron), iron oxide, or powdered graphite. Exemplary magnetic materials include ferromagnetic materials include iron, nickel, cobalt, iron alloys, nickel alloys, cobalt alloys, and steel, or ferromagnetic materials such as magnetite, nickel-zinc ferrite, manganese-zinc ferrite, and copper-zinc ferrite. Exemplary polar materials include butyl rubber (such as ground tires), barium titanate powder, aluminum oxide powder, or PVC flour.
Preferably, a mixing or dispersion step is provided, whereby a composition comprising the susceptor particles is mixed or dispersed in the petroleum ore. The mixing step can occur after the petroleum ore has been crushed, ground, or milled, or in conjunction with the crushing, grinding, or milling of the petroleum ore. The mixing step can be conducted using any suitable method or apparatus that disperses the susceptor particles in a substantially uniform manner. For example, a sand mill, cement mixer, continuous soil mixer, or similar equipment can be used.
An advantageous capability of the presently disclosed methods can be the fact that large amounts of susceptor particles can optionally be used without negatively affecting the chemical or material properties of the processed petroleum ore. Therefore, a composition comprising susceptor particles can for example be mixed with the petroleum ore in amount from about 1% to about 50% by volume of the total mixture. Alternatively, the composition comprising susceptor particles comprises from about 1% to about 25% by volume of the total mixture, or about 1% to about 10% by volume of the total mixture.
After the susceptor particle composition has been mixed in the petroleum ore, the mixture can be heated using RF energy. An RF source can be provided which applies RF energy to cause the susceptor particles to generate heat. The heat generated by the susceptor particles causes the overall mixture to heat by conduction. The preferred RF frequency, power, and source proximity vary in different embodiments depending on the properties of the petroleum ore, the susceptor particle selected, and the desired mode of RF heating.
In one exemplary embodiment, RF energy can be applied in a manner that causes the susceptor particles to heat by induction. Induction heating involves applying an RF field to electrically conducting materials to create electromagnetic induction. An eddy current is created when an electrically conducting material is exposed to a changing magnetic field due to relative motion of the field source and conductor; or due to variations of the field with time. This can cause a circulating flow or current of electrons within the conductor. These circulating eddies of current create electromagnets with magnetic fields that opposes the change of the magnetic field according to Lenz's law. These eddy currents generate heat. The degree of heat generated in turn, depends on the strength of the RF field, the electrical conductivity of the heated material, and the change rate of the RF field. There can be also a relationship between the frequency of the RF field and the depth to which it penetrate the material; in general, higher RF frequencies generate a higher heat rate.
Induction RF heating can be for example carried out using conductive susceptor particles. Exemplary susceptors for induction RF heating include powdered metal, powdered iron (pentacarbonyl E iron), iron oxide, or powdered graphite. The RF source used for induction RF heating can be for example a loop antenna or magnetic near-field applicator suitable for generation of a magnetic field. The RF source typically comprises an electromagnet through which a high-frequency alternating current (AC) is passed. For example, the RF source can comprise an induction heating coil, a chamber or container containing a loop antenna, or a magnetic near-field applicator. The exemplary RF frequency for induction RF heating can be from about 50 Hz to about 3 GHz. Alternatively, the RF frequency can be from about 10 kHz to about 10 MHz, 10 MHz to about 100 MHZ, or 100 MHz to about 2.5 GHz. The power of the RF energy, as radiated from the RF source, can be for example from about 100 KW to about 2.5 MW, alternatively from about 500 KW to about 1 MW, and alternatively, about 1 MW to about 2.5 MW.
In another exemplary embodiment, RF energy can be applied in a manner that causes the susceptor particles to heat by magnetic moment heating, also known as hysteresis heating. Magnetic moment heating is a form of induction RF heating, whereby heat is generated by a magnetic material. Applying a magnetic field to a magnetic material induces electron spin realignment, which results in heat generation. Magnetic materials are easier to induction heat than non-magnetic materials, because magnetic materials resist the rapidly changing magnetic fields of the RF source. The electron spin realignment of the magnetic material produces hysteresis heating in addition to eddy current heating. A metal which offers high resistance has high magnetic permeability from 100 to 500; non-magnetic materials have a permeability of 1. One advantage of magnetic moment heating can be that it can be self-regulating. Magnetic moment heating only occurs at temperatures below the Curie point of the magnetic material, the temperature at which the magnetic material loses its magnetic properties.
Magnetic moment RF heating can be performed using magnetic susceptor particles. Exemplary susceptors for magnetic moment RF heating include ferromagnetic materials or ferromagnetic materials. Exemplary ferromagnetic materials include iron, nickel, cobalt, iron alloys, nickel alloys, cobalt alloys, and steel. Exemplary ferromagnetic materials include magnetite, nickel-zinc ferrite, manganese-zinc ferrite, and copper-zinc ferrite. In certain embodiments, the RF source used for magnetic moment RF heating can be the same as that used for induction heating—a loop antenna or magnetic near-field applicator suitable for generation of a magnetic field, such as an induction heating coil, a chamber or container containing a loop antenna, or a magnetic near-field applicator. The exemplary RF frequency for magnetic moment RF heating can be from about 100 kHz to about 3 GHz. Alternatively, the RF frequency can be from about 10 kHz to about 10 MHz, 10 MHz to about 100 MHZ, or 100 MHz to about 2.5 GHz. The power of the RF energy, as radiated from the RF source, can be for example from about 100 KW to about 2.5 MW, alternatively from about 500 KW to about 1 MW, and alternatively, about 1 MW to about 2.5 MW.
In a further exemplary embodiment, the RF energy source and susceptor particles selected can result in dielectric heating. Dielectric heating involves the heating of electrically insulating materials by dielectric loss. Voltage across a dielectric material causes energy to be dissipated as the molecules attempt to line up with the continuously changing electric field.
Dielectric RF heating can be for example performed using polar, non-conductive susceptor particles. Exemplary susceptors for dielectric heating include butyl rubber (such as ground tires), barium titanate, aluminum oxide, or PVC. Water can also be used as a dielectric RF susceptor, but due to environmental, cost, and processing concerns, in certain embodiments it may be desirable to limit or even exclude water in processing of petroleum ore. Dielectric RF heating typically utilizes higher RF frequencies than those used for induction RF heating. At frequencies above 100 MHz an electromagnetic wave can be launched from a small dimension emitter and conveyed through space. The material to be heated can therefore be placed in the path of the waves, without a need for electrical contacts. For example, domestic microwave ovens principally operate through dielectric heating, whereby the RF frequency applied is about 2.45 GHz. The RF source used for dielectric RF heating can be for example a dipole antenna or electric near field applicator. An exemplary RF frequency for dielectric RF heating can be from about 100 MHz to about 3GHz. Alternatively, the RF frequency can be from about 500 MHz to about 3 GHz. Alternatively, the RF frequency can be from about 2 GHz to about 3 GHz. The power of the RF energy, as radiated from the RF source, can be for example from about 100 KW to about 2.5 MW, alternatively from about 500 KW to about 1 MW, and alternatively, about 1 MW to about 2.5 MW.
The reflection of incident RF energy such as an incident electromagnetic wave can reduce the effectiveness of RF heating. It may be desirable for the RF fields or electromagnetic waves to enter the materials and susceptors to dissipate. Thus, in one embodiment the susceptor particles can have the property of equal permeability and permeability, e.g. μr=ε4 to eliminate wave reflections at an air-susceptor interfaces. This can be explained as follows: wave reflections occur according to the change in characteristic impedance at the material interfaces: mathematically r=(Z1−Z2)/(Z1+Z2) where r is the reflection coefficient and Z1 and Z1 are the characteristic or wave impedances of the individual materials 1 and 2. Whenever Z1=Z2 zero reflection occurs. As the characteristic wave impedance of a material is Z=120π(√μr/εr), whenever μr=εr, Z=120π=377 ohms. In turn, there would be no wave reflection for that material at an air interface, as air is also Z=377 ohms. An example of a isoimpedance magnetodielectric (μr≡εr) susceptor material, without reflection to air, is light nickel zinc ferrite which can have μr=εr=14. As background, other than refractive properties, nonconductive materials of μr≡□r may be invisible in the electromagnetic spectrum where this occurs. With sufficient conductivity, μr ≡εr susceptor materials have excellent RF heating properties for high speed and efficiency.
The susceptor particles may be proportioned in the hydrocarbon ore to obtain μr≡εr from the mixture overall, for reduced reflections at air interface and increased heating speed. The logarithmic mixing formula log εm′=θ1 log ε1′+θ2 log ε2′ may be used to adjust the permittivity of the mixture overall by the volume ratios e of the components and the permittivities E of components, 1 and 2. In the case of semiconducting susceptor particles the size, shape, and distribution of particles may however affect the material polarizability and some empiricism may be required. The paper “The Properties Of A Dielectric Containing Semiconducting Particles Of Various Shapes”, R. W. Sillars, Journal of The Institution Of Electrical Engineers (Great Britain), Vol. 80, April 1937, No. 484 may also be consulted.
In another embodiment of the present invention, pentacarbonyl E iron powder is advantageous as a magnetic (H) field susceptor. In the pentacarbonyl, E iron powder embodiment, iron susceptor powder particles in the 2 to 8 micron range are utilized. A specific manufacture is type EW (mechanically hard CIP grade, silicated 97.0% Fe, 3 um avg. particle size) by BASF Corporation, Ludwigshafen, Germany (www.inorganics.BASF.com). This powder may also be produced by GAF Corporation at times in the United States. Irrespective of manufacture, sufficiently small bare iron particles (EQ) are washed in 75 percent phosphoric acid (“Ospho” by Marine Enterprises Inc.) to provide an insulative oxide outer finish, FePO4. The iron powder susceptors have a low conductivity together in bulk and small particle size such that RF magnetic fields are penetrative. The susceptor powder particles must be small relative the radio frequency skin depth, e.g. particle diameter d<√(λ/πσμc) where wavelength is the wavelength in air, σ is conductivity of iron, p is the permeability of the iron, and c is the speed of light.
The susceptor particles need not be solids, and in another embodiment liquid water may be used. The water can be mixed with or suspended in emulsion with the petroleum ore. The dissipation factor of pure, distilled water is provided as
In yet another embodiment, the RF energy source used can be far-field RF energy, and the susceptor particles selected act as mini-dipole antennas that generate heat. One property of a dipole antenna is that it can convert RF waves to electrical current. The material of the dipole antenna, therefore, can be selected such that it resistively heats under an electrical current. Mini-dipole RF heating can be preferably performed using carbon fiber, carbon fiber floc, or carbon fiber cloth (e.g., carbon fiber squares) susceptors. Carbon fibers or carbon fiber floc preferably are less than 5 cm long and less than 0.5 MW.
In each of the presently exemplary embodiments, RF energy can be applied for a sufficient time to allow the heated susceptor particles to heat the surrounding hydrocarbon oil, ore, or sand. For example, RF energy can be applied for sufficient time so that the average temperature of the mixture can be greater than about 212° F. (100° C.). Alternatively, RF energy can be applied until the average temperature of the mixture is, for example, greater than 300° F. (150° C.), or 400° F. (200° C.). Alternatively, RF energy can be applied until the average temperature of the mixture is, for example, greater than 700° F. (400° C.). In a variation on the exemplary embodiment the RF energy can be applied as part of a distillation or cracking process, whereby the mixture can be heated above the pyrolysis temperature of the hydrocarbon in order to break complex molecules such as kerogens or heavy hydrocarbons into simpler molecules (e.g. light hydrocarbons). It is presently believed that the suitable length of time for application of RF energy in the presently disclosed embodiments can be preferably from about 15 seconds, 30 seconds, or 1 minute to about 10 minutes, 30 minutes, or 1 hour. After the hydrocarbon/susceptor mixture has achieved the desired average temperature, exposure of the mixture to the radio frequency can be discontinued. For example, the RF source can be turned off or halted, or the mixture can be removed from the RF source.
In certain embodiments, the present disclosure also contemplates the ability to remove the susceptor particles after the hydrocarbon/susceptor mixture has achieved the desired average temperature.
If the susceptor particles are left in the mixture, in certain embodiments this may undesirably alter the chemical and material properties of primary substance. One alternative is to use a low volume fraction of susceptor, if any. For example, U.S. Pat. No. 5,378,879 describes the use of permanent susceptors in finished articles, such as heat-shrinkable tubing, thermosetting adhesives, and gels, and states that articles loaded with particle percentages above 15% are generally not preferred, and in fact, are achievable in the context of that patent only by using susceptors having relatively lower aspect ratios. The present disclosure provides the alternative of removing the susceptors after RF heating. By providing the option of removing the susceptors after RF heating, the present disclosure can reduce or eliminate undesirable altering of the chemical or material properties of the petroleum ore, while allowing a large volume fraction of susceptors to be used. The susceptor particle composition can thus function as a temporary heating substance, as opposed to a permanent additive.
Removal of the susceptor particle composition can vary depending on the type of susceptor particles used and the consistency, viscocity, or average particle size of the mixture. If necessary or desirable, removal of the susceptor particles can be performed in conjunction with an additional mixing step. If a magnetic or conductive susceptor particle is used, substantially all of the susceptor particles can be removed with one or more magnets, such as quiescent or direct-current magnets. In the case of a polar dielectric susceptor, substantially all of the susceptor particles can be removed through flotation or centrifuging. Carbon fiber, carbon floc, or carbon fiber cloth susceptors can be removed through flotation, centrifuging, or filtering. For example, removal of the susceptor particles can be performed either while the petroleum ore/susceptor mixture is still being RF heated, or within a sufficient time after RF heating has been stopped so that the temperature of the petroleum ore decreases by no more than 30%, and alternatively, no more than 10%. For example, it is exemplary that the petroleum ore maintain an average temperature of greater than 200° F. (93° C.) during any removal of the susceptor particles, alternatively an average temperature of greater than 200° F. (93° C.).
Another advantage of the exemplary embodiments of the present disclosure can be that the susceptor particles can optionally be reused after they are removed from a heated mixture.
Alternatively, in certain instances it may be appropriate to leave some or all of the susceptor particles in some or all of the material of the mixture after processing. For example, if the particles are elemental carbon, which is non-hazardous and inexpensive, it may be useful to leave the particles in the mixture after heating, to avoid the cost of removal. For another example, a petroleum ore with added susceptor material can be pyrolyzed to drive off useful lighter fractions of petroleum, which are collected in vapor form essentially free of the susceptor material, while the bottoms remaining after pyrolysis may contain the susceptor and be used or disposed of without removing the susceptor.
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The following examples illustrate several of the exemplary embodiments of the present disclosure. The examples are provided as small-scale laboratory confirmation examples. However, one of ordinary skill in the art will appreciate, based on the foregoing detailed description, how to conduct the following exemplary methods on an industrial scale.
A sample of ¼ cup of Athabasca oil sand was obtained at an average temperature of 72° F. (22° C.). The sample was contained in a Pyrex glass container. A GE DE68-0307A microwave oven was used to heat the sample at 1 KW at 2450 MHz for 30 seconds (100% power for the microwave oven). The resulting average temperature after heating was 125° F. (51° C.).
A sample of ¼ cup of Athabasca oil sand was obtained at an average temperature of 72° F. (22° C.). The sample was contained in a Pyrex glass container. 1 Tablespoon of nickel zinc ferrite nanopowder (PPT #FP350 CAS 1309-31-1) at an average temperature of 72° F. (22° C.) was added to the Athabasca oil sand and uniformly mixed. A GE DE68-0307A microwave oven was used to heat the mixture at 1 KW at 2450 MHz for 30 seconds (100% power for the microwave oven). The resulting average temperature of the mixture after heating was 196° F. (91° C.).
A sample of ¼ cup of Athabasca oil sand is obtained at an average temperature of 72° F. (22° C.). The sample is contained in a Pyrex glass container. 1 Tablespoon of powdered pentacarbonyl E iron at an average temperature of 72° F. (22° C.) is added to the Athabasca oil sand and uniformly mixed. A GE DE68-0307A microwave oven is used to heat the mixture at 1 KW at 2450 MHz for 30 seconds (100% power for the microwave oven). The resulting average temperature of the mixture after heating will be greater than the resulting average temperature achieved using the method of Example 1.
A sample of ¼ cup of Athabasca oil sand is obtained at an average temperature of 72° F. (22° C.). The sample is contained in a Pyrex glass container. 1 Tablespoon of butyl rubber (such as ground tire rubber) at an average temperature of 72° F. (22° C.) is added to the Athabasca oil sand and uniformly mixed. A GE DE68-0307A microwave oven is used to heat the mixture at 1 KW at 2450 MHz for 30 seconds (100% power for the microwave oven). The resulting average temperature of the mixture after heating will be greater than the resulting average temperature achieved using the method of Example 1.
This specification is related to McAndrews, Held & Malloy attorney docket numbers: 20476US0120480US0120481US0120483US0120484US0120485US0120486US0120487US0120496US01 filed on or about the same date as this specification, each of which is incorporated by reference herein.
| Number | Date | Country | |
|---|---|---|---|
| Parent | 14705182 | May 2015 | US |
| Child | 15715247 | US | |
| Parent | 12395995 | Mar 2009 | US |
| Child | 14705182 | US |
