This invention relates to a new method for gas storage. Particularly, it refers to a method for gas storage in the form of nanobubbles or nano gas layers on the solid-liquid surface.
The storage of high purified gas can be used in a lot of fields, especially the storage of hydrogen which is very significant in utilization of hydrogen energy. But recently human being faces a flinty challenge from energy, resource and environmental crisis. This is caused by traditional energy sources, such as petroleum and coal, which become less and less, and greenhouse effects and acid rain produced by conflagrant productions of petroleum and coal, CO2 and SO2. So, human being needs clear and new energy sources. Hydrogen energy attracts much attention from a wide audience of scientists due to reproduction and abundant resources. More importantly, hydrogen does not cause the environmental pollution and is a very ideal and clear energy source. The storage of hydrogen is the key of utilization and also the scabrous problem. Many countries are paying great money trying to resolve this problem. In 2003, the United States financed US$1200 millions to develop hydrogen producing and storage. There are two important indexes to quantify the hydrogen storage, volume density (kgH2/m3) and mass percentage (wt %). Volume density defines the hydrogen mass of storage per volume in this system. Mass percentage defines the ratio of hydrogen mass and system mass. Of course, there are also other parameters such as the reversibility of charging and releasing of the hydrogen, the charging speed of the hydrogen, and so on. The purpose is to store more hydrogen as possible in a smaller volume and a smaller mass storage system under environmental temperature and lower pressure. The authoritative standard is the one released by U.S. Department of Energy (DOE). For fuel cell vehicles, the main standard to quantify the storage of hydrogen is the volume density should reach 62 kg/m3, mass fraction of 6.5% (Hynek, S.; Fuller, W.; Bentley, J. Hydrogen storage by carbon sorption. Int. J. Hydrogen Energy 1997, 22, 601-610). Besides, the reversibility of charging and releasing of hydrogen is a very important index. All in all, the aim is to store more hydrogen as possible in a smaller volume and a smaller mass storage system under environmental temperature and lower pressure, and the fast speed of charging and releasing of hydrogen and the lifetime are also standard.
Traditional storage of hydrogen has two ways. One way is using steel bottle with high pressure to store hydrogen. But in this case, although the pressure of steel bottle inside reaches 150 atm, the mass of hydrogen is less than 1 percent of the bottle and it is also very dangerous to explode. Another way is to store liquid hydrogen. i.e., the temperature of gas hydrogen is decreased to −253° C. and hydrogen becomes liquid to store. But in this method the storage box must be very large and has perfect adiabatic performance to prevent liquid hydrogen from evaporation. Therefore, storing hydrogen under high pressure needs large vessel and good materials, but has low energy density and safety to use. Although energy density of the liquid hydrogen is high, it costs energy and money, and is difficult to operate and use.
Recently, several new methods were developed, mainly by developing new materials of hydrogen storage by which hydrogen can be absorbed physically/chemically or reacted chemically. So far, the materials for hydrogen storage are sorted into three types: liquid organic compounds, alloy materials and nonmetal materials. All those materials have advantages and disadvantages.
The storage of hydrogen by liquid organic compound is that hydrogen is happened addition reaction with unsaturated organic compound by chemical catalysis reaction, for example, benzene reacts with toluene to produce cyclohexane, and so on. This method has high density of hydrogen storage of about 7% but the process of absorption and release of hydrogen is complex and also causes a lot of problems, such as the recycle of organic compounds is very difficult.
As for alloy compound for hydrogen storage, developed materials are lanthanon and titanic alloy materials. The volume density of those materials for hydrogen storage is very high, but the mass density is only 2%, and the materials are very expensive and incidental materials poisoning decreases the storage ability. Although some light alloy materials have large mass fraction of hydrogen storage, the speed of absorption and release of hydrogen is low and the process of hydrogen storage is not reversible completely.
Inorganic nonmetal materials for hydrogen storage have a lot of types, such as glass microsphere and carbon based materials. It is found that carbon based materials are very nice hydrogen absorbents. They include activated carbon, carbon nanotube, carbon nanofibers and layers graphite, and so on. Among them, the mass fraction of absorbing hydrogen of traditional activated carbon is less than 1% under low temperature. However, for superactivated carbon with surface areas of 3000 m2/g, volumes of micro-hole of 1.5 Ml/g, mass fraction of absorbing hydrogen can reach to 5% under the special condition of low temperature and high pressure. U.S. Pat. No. 6,290,753 disclosed a carbon material for hydrogen storage via cone microstructures. Under the condition of temperature of 22-527° C. and the pressure of 0.3-10 atm, the mass fraction of hydrogen storage can exceed 15%. During couple of years research on carbon nanotubes and carbon nanofibers used for hydrogen storage became hot topics. There have been many patents and documentations related to carbon nanotubes. For example, U.S. Pat. No. 6,517,800 disclosed a method of hydrogen storage via carbon nanotubes with single wall in which the storage amount is about 4.24% using this material under normal temperature and pressure of 100-120 atm. Dillon obtained mass fraction of hydrogen storage is about 5-10% using single wall carbon nanotubes under normal temperature and pressure of about 40 kPa (Dillon, A. C.; Jones, K. M.; Bekkedahl, T. A.; Kiang, C. H.; Bethune, D. S.; Heben, M. J. Storage of hydrogen in single-walled carbon nanotubes. Nature 1997, 386, 377-379.) Ye et al also obtained the mass fraction of hydrogen absorption of 8.25% using single wall carbon nanotubes with 98% purity under the temperature of −193° C. and pressure above 4 MPa. Results from different researchers are different and they debates. It is reported that the highest mass fraction of hydrogen storage in carbon nanotubes is 67%, and the lowest fraction is only 0.1% (Hirscher, M.; Becher, M.; Haluska, M.; Zeppelin, F.; Chen, X.; Dettlaff-Weglikowska, U.; Roth, S. Are carbon nanostructures an efficient hydrogen storage medium? Journal of Alloys and Compounds 2003, 356-357, 433-437.) Carbon nanofibers also do not go on wheels. For example, Chambers et al got the mass fraction of hydrogen storage of 67% under the condition of 12 MPa, 25° C. But nobody can repeat this result until now (Rodriguez, N. M.; Chambers, A.; Baker, R. T. K. Catalytic engineering of carbon nanostructures. Langmuir 1995, 11, 3862-3866). In summary, carbon materials for hydrogen storage still exist a lot of problems, such as low speed of absorption and release of hydrogen, i.e., it needs 5 h to reach the largest volume for carbon nanotubes, 12 h for carbon nanofibers. Also, the stability of absorbed volume is bad, 8 cycles of absorption and release make the absorption volume decrease 30%, and since the strong dependence on pressure and temperature, carbon nanomaterials for hydrogen storage must be done under high pressure or low temperature, technique of preparation is very complex.
The object of this invention is to overcome the disadvantage of the prior art and provides a new method for gas storage, particularly a new method for hydrogen storage. This method has perfect repeatability, can perform under the normal temperature and pressure easily, does not bring contaminations, and the density of hydrogen storage per surface area is high and the speed of filling and releasing of hydrogen is fast.
The research in the lab found that gases can be stably absorbed on solid-liquid surface with high density in the form of nanobubbles or gas nanolayers. But this can not be explained by macroscopic theory. If the gas molecules inside the bubbles aggregate as macroscopic gas, the pressure of nanobubbles with the radii of 10 nm may be 144 atm which will cause them disappear instantly. But if the gas in nanobubbles exists in a new state with high density, the nanobubbles might stably exist on solid-liquid surface. The applicants of this invention obtained by molecular dynamics simulation that the density of hydrogen nanobubbles is about 420 times higher than that of hydrogen gas density in macroscopic scale, and is about 53 percents of density of liquid hydrogen (70 kg/m3). This is also supported by the conclusion of reduced density layer on hydrophobic interface reported by other groups. They detected a layer by neutron scattering or X ray with the reduced density of 0.65-0.95 g/cm3 which is presumed as gas layer, but no direct evidence (Steitz R. et al. Nanobubbles and their precursor layer at the interface of water against a hydrophobic substrate. Langmuir 2003, 19, 2409-2414; Schwendel D. et al. Interaction of water with self-Assembled monolayers: neutron reflectivity measurements of the water density in the interface region. Langmuir 2003, 19, 2284-2293.). Based on the finding that flat and smooth surface can absorb nanobubbles or gas nanolayer with high coverage and density, this invention is provides a new method for gas storage, particularly a method for hydrogen storage. This invention can be achieved via the following technical solutions:
This invention further provides an integrative method of producing and storing hydrogen. The feature is that hydrogen is produced by electrochemical approach in electrolyte solution, and the conductive and flat solid surface is used as cathode to absorb nanoscale hydrogen bubbles or gas layers. It is performed by following technical solutions:
2H++2e−→H2 (acidic solution)
2H2O+2e−→H2+2OH− (salt and base solution)
The HOPG aforesaid in this invention is a new conductive high purity carbon with layer structures, and is the highest level of graphite (ZYA level).
In this invention, the AFM used for observation is NanoScope IIIa SPM system (Digital Instruments, Inc.) with O-ring, liquid cell, “E” scanner and normal NP tip with the spring constant of 0.58 N/m. the tip should be cleaned by water, ethanol and acetone respectively. Imaging is performed under the normal temperature and pressure.
As for the nanobubbles formed on the cathode surface, the volume of single nanobubble should be obtained firstly when calculating the amount of gas storage. Therefore, this invention presents the model of nanobubbles absorbed on interface as shown in
The volume of single nanobubble:
Average volume of several nanobubbles on certain areas:
Wherein, Vapparent is average volume of many nanobubbles on the graphite within certain areas. Hmean is average height of nanobubbles produced on the graphite surface within certain areas. Smean is average area of a nanobubble contacting with the graphite.
Firstly, hydrogen nanobubbles are observed and images are saved. Then average area Smean and average height Hmean are obtained by “particle analysis” in off-line of AFM software. According to the model shown in
Hydrogen stored on surface of cathode can be released by many methods, such as draining of the water covering the nanobubbles, mechanical disturbance, ultrasonic disturbance or heating etc can make the hydrogen release.
Obviously, in order to store more hydrogen, we hope that surface area of the solid used as substrates is as large as possible. For example, solid can be disposed by layers or hydrogen is absorbed on materials with large surface areas such as porous materials and carbon nanotubes, by which storage of hydrogen can be increased sharply.
In this invention the volume of nanobubbles and output of the hydrogen can be controlled by changing the voltage and time in the electrochemical reaction. Hydrogen nanobubbles are very stable, they can exist more than ten hours without disturbance, and their morphology has no obvious changes during the experimental time. This invention has prefect repeatability, can perform under the normal temperature and pressure easily, does not cause pollution, and of the hydrogen is released easily. Moreover, the device is low cost, easily to produce, transport and operate with high safety and long lifetime. This method can achieve high density of hydrogen storage fast speed of filling and releasing of hydrogen. The method of hydrogen storage provided by this invention has large potential application value in the utilization of hydrogen source, especially in automobile fuel battery, storage battery and other fields.
The Following is the embodiments to further illustrate this invention, but is not intended to limit the invention.
Wherein, the AFM used in the embodiments is NanoScope IIIa SPM system (Digital Instruments, Inc.) with O-ring, liquid cell, “E” scanner and normal NP tip with the spring constant of 0.58 N/m. the tip should be cleaned by water, ethanol and acetone, respectively. The Water is Millipore water with high purity. The Electrolytes are GR grade which were purchased from Chinese Chemical Reagent Co. The electrochemical workstation used is bought from Shanghai Cheng Hua Instruments Company. The HOPG is purchased from Mikromasch Company.
As shown in
After loading electrodes to liquid cell, software to control electrochemical reactions is started and corresponding parameters can be set, power is switched on. In situ observation can be performed by AFM after loading a voltage and in reaction time on cathode surface, images are saved. The parameters of AFM are drive frequency of 7.2 KHz, drive amplitude of 280 mV, scan rate of 2 Hz, scan size of 12 μm×12 μm, setpoint is ascertained by force curve.
According to the cyclic voltammetric (CV) curves of electrolyzing water (see
It is found in the lab that reaction is very stable when the concentration of sulfuric acid solution is about 0.001˜1.0 mol/L and the voltage is about −1.2 V˜2.5 V. Under this condition, a lot of bubbles can be formed after 5 s-30 s.
Then average area Smean and average height Hmean are obtained by “particle analysis” in off-line process of atomic force microscopy software. According to the model equation 2 shown in
According to the calculation provided by U.S. Department of Energy, assuming graphite and absorbed hydrogen as a unit, weight fraction of hydrogen=mass of hydrogen/(mass of graphite+mass of hydrogen). In order to the comparison with the standard of hydrogen storage set by U.S. Department of Energy, we chose a typical image of hydrogen nanobubbles with high coverage (89%). As for image of hydrogen nanobubbles shown in
Under the normal temperature and pressure, hydrogen can be released by draining of the water covering the nanobubbles through the drainpipe of liquid cell. As shown in
The least voltage and time of producing hydrogen nanobubbles might be different in the different electrolytes. As for the same electrolyte, the size and number of nanobubbles are dominated by reaction voltage and time. For example, generally, the higher the voltage is applied, the smaller and the more nanobubbles are produced; the longer the reaction time, the more and the larger nanoubbles. Normally, the reaction time can not exceed 120 s because that too much time make bubbles merge each other, become larger and escape or broken, then the number of bubbles decreases. Of course, if further postpone the reaction time, bubbles may be formed on graphite surface again.
The device and operation are same as those in embodiment 1. But potassium hydroxide solution of 0.001-10 mol/L is chosen as the electrolyte, the range of voltage loaded is −0.5 V-−2.0 V, the reaction time is at least 0.01 s. Under this condition, the range of height of nanobubbles is 2-100 nm.
The size of nanobubbles formed in the solution of sodium nitrate, potassium nitrate and barium sulphate etc. with concentration of 0.001-10 mol/L are same as that in the solution of sulfuric acid and potassium hydroxide. Here, we do not illustrate more embodiments about that.
Nitrogen nanobubbles are obtained on different solid surfaces by the exchanging of ethanol and water.
In this invention the exchange of ethanol and water is a method that nanobubbes can be formed on solid surface by replacing gas-saturated ethanol solution in the container with gas-saturated water. Using this method excessive gases can be separated out because of the different solubility between water and ethanol to the same gas. That excessive gas can be absorbed on the surface and form nanobubbles.
In this invention water and ethanol is degassed in vacuum pump firstly, then press nitrogen with high pressure into water and ethanol, and water and ethanol are kept in nitrogen saturated state. Nitrogen-saturated ethanol solution is poured into liquid cell quickly, then the solution is replaced by nitrogen-saturated water. The AFM is used to observe. As shown in
Nano gas layer is obtained on graphite surface by the exchanging of ethanol and water
The experimental process is the same as in embodiment 3. As shown in
The formation of nitrogen and hydrogen nanobubbles (gas layers) on graphite surface in water
In this invention, the calculation method is molecular dynamics simulation (software Gromacs of version 3.2.1).
Firstly, force field parameters used are given. Covalent bonds of double atoms (N2 and H2) in a molecule are defined by harmonic oscillator potential:
V(r)=½k(r−b)2,
k and b are force constant of harmonic oscillator potential and standard bond length, respectively.
Interactions between molecules can be expressed by Lennard-Jones potential:
φ=4ξ[(σ/r)12−(σ/r)6],
σ and ξ are length dimension and energy scale, respectively. As for force field parameters, we adopt Universal Force Field parameters shown in the follows:
We adopt SPC water model.
Simulation process and results are shown in the follows:
Number | Date | Country | Kind |
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200510111758.3 | Dec 2005 | CN | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/CN2006/003046 | 11/13/2006 | WO | 00 | 6/20/2008 |