This invention relates to a method to manufacture microtanks and a system to store compressed gas such as hydrogen with high safety.
There are numbers of hydrogen storage methods. These include liquid hydrogen at low temperature, compressed gaseous hydrogen in gas-cylinders, metal hydrides and chemical hydrides and physical-chemical absorbed hydrogen in carbon nanotubes. Some of these methods have moved from laboratory stage into prototype vehicles. Each of these options has advantages and disadvantages. Compressed gaseous and liquid hydrogen storage is most mature technology and commercially available.
Extensive active research and development efforts have been made to overcome technical barriers for hydrogen storage. The major barriers for hydrogen storage are low H2 gravimetric and volumetric storage capacity, difficulty in storing and releasing H2, high materials and system costs and safety.
In US Patent “Hydrogen supply method” (U.S. Pat. No. 4,211,537, Jul. 8, 1980), Teitel proposed storage of high-pressure hydrogen in glass microspheres as a solution to the problems inherent in hydrogen storage and transport. Hollow glass microspheres for storage of hydrogen gas onboard a vehicle involve charging, filling, and discharging. First, the hollow glass spheres are filled with H2 at high pressure (350-700 bars) and high temperature (300° C.) by permeation in a high-pressure vessel. Next, the micro spheres are cooled down to room temperature and transferred to the low-pressure vehicle tank. Finally, the micro spheres are heated to 200-300° C. for controlled release of H2 to run the vehicle. The microspheres generally have a diameter ranged from 5 microns to about 500 microns. The wall of the microspheres is generally from 1% to 10 % that of the microsphere diameter. Glass microspheres have the potential to be inherently safe as they store H2 at a relatively low pressure onboard and are also suitable for conformable tanks. This allows for low container cost. It is demonstrated that storage density of hydrogen reaches to 5.4 wt. %. Theoretical calculations indicated that hydrogen storage capacity with over 40 wt % and liquid hydrogen density in super-high-strength microspheres is achievable. However, there are two technical challenges associated with the hollow microsphere hydrogen storage for practical applications: One is manufacture of high strength hollow microspheres; the other one is how to heat microspheres to promptly release stored hydrogen.
Shelby disclosed a technique to overcome the hydrogen release problem of hollow glass microspheres in US Patent “Glass membrane for controlled diffusion of gases” (U.S. Pat. No. 6,231,642, May 15, 2001). They found the stored hydrogen in glass microsphere could be instantly released upon irradiated by infrared (IR) light. The response time is less than 1 second compared to conventional furnace heating method where 10′s minutes need for hydrogen release. The out-gassing of H2 was enhanced by absorption of light in Fe3O4 or NiO doped glasses. The H2 release rate is proportional to lamp intensity above a threshold. The rapid response is essential for the microsphere storage when H2 gas is required to be supplied on demand. However, it was found that only a portion of the hydrogen was released by photo-induction, possibly suggesting that this phenomenon occurred in the near surface of the glass. This partially release of hydrogen will be a main technical barrier prohibiting hollow glass microspheres from as hydrogen storage media.
It is an objective of present invention to disclose high strength holey fiber structures as compressed gas storage media with large storage capacity.
Another object of the present invention is that holey fibers function as light waveguides to deliver lights to heat up fibers for release of stored gas with instant response and controllable gas supply rate.
It is a further object of present invention that an new storage system for compressed gas provide safe, inexpensive and convenient solution to applications such as onboard fuel supply for on ground automobile vehicles, aircraft, spacecraft, and fuel cells for portable electronic devices.
According to the invention, capped holey fibers are used to form microtanks. Holey fibers have shell and hollow or porous structures. Characteristic structures of holey fibers provide properties of high mechanical strength and large gas filling capacity and desired gas permeability. Diameters of holey fibers are ranged from 60 microns to 2000 microns. The thickness of shell is ranged from 1 micron to tens microns. The thickness of wall of porous structure is typically smaller than one micron. The aspect ration of porous structure is greater than 5. The materials of holey fibers have high tensile strength with value no less than 4 GPa. Preferably, synthetic fused silica is used as holey fiber materials.
Another embodiment of present invention is that plurality of microtanks are assembled in groups and aligned with same direction. Further, the grouped microtanks are packed in a vessel and aligned at same directions. In this manner, lights can be coupled into following groups and transmitted through.
Present invention also disclosed a method to fill, store and release of compressed gas in invented microtanks. Compressed gas is induced into microtanks by permeation in a vessel at elevated temperature and high pressure. The compressed gas is stored in plurality of microtanks at ambient temperature. The gas is released at controllable rate by illumination of lights on ends of microtanks.
A better understanding of the invention will obtained by reference to the detailed description below, in conjunction with the following drawings, in which:
Optical fibers produced with synthetic fused silica have remarkable strength. Based on the Si-O bond strength, the fiber has a theoretical strength of ˜2000 kpsi or 14 GPa, which is stronger than steel. In practice the observed strength is considerably lower (typically 700 kpsi or 5.5 GPa) due to the presence of small flaws in the bulk and on the surface of the silica.
The proof tensile strength of microstructured holey fiber is about 4.5 GPa, which is slightly lower than the one of standard silica fibers. This is partially because of lower fiber drawing temperature that is necessary to avoid collapse of glass walls of hollow fibers. This high tensile strength allows us to make super-strength-holey fibers.
In the case of simple spherical symmetry, a stretching stress is given by
σ=RbP/2ΔRb=PAb/2
where P is the gas pressure, in a thin-walled shell with a radius of Rb, a thickness of ΔRb and a aspect ratio Ab(Ab=/RbΔRb). The created stretching stress, σ, should be lower than the stress of destruction, σι, of the shell materials. This formula indicated that larger stress of destruction of shell materials is required if a geometry with larger aspect ration is used. On the other hand, it is preferred to use a geometry with larger aspect ratio for higher storage capacity. Mechanical strength and storage capacity require contrarily a aspect ration for a geometry of a vessel.
In accordance with the invention, referring to
A cross section view of holey fiber 10 is shown in
The porous layer 12 is composed of microtubes 13. The cross section shape of microtubes 13 can be a round circle, ellipse, rectangle, square, or polyhedron or their combinations. The cross section view of circle microtubes 13 is shown in
Porosity of the holey fibers 10, ν, the ration of holes area to wall area, is given by formula
ν≅(A+2B/(B+2))/(A+2)
Porosity of holey fibers can exceed over ˜95% when aspect ratio A and B were properly selected to simultaneously achieve high mechanical strength of holey fibers and high storage capacity.
Stored hydrogen in cylinder microtanks will be diffused out through thin walls of fibers. The stored amount of hydrogen, A, after time, t, can be expressed as
A =A
Oexp(−t/τ)
where AO is initial stored hydrogen, τ is a characteristic time. τ is related to the radius of hollow core, R, the thickness of porous layer, ΔR, the thickness of shell, ΔRs, and wall materials permeability parameters K, by formula:
The capability of filling shells and storing hydrogen is based on the fact that for the majority of materials the gas permeabilities rapidly increased with temperature according to formula:
K=K
0 exp(−Ek/kT)
where k is the Boltzman constant and Ek is the activation energy. For the fused silica, the parameter k is ranged between 0.007 and 0.1×10−10cm2atm−1s−1. Obviously, the storage time and release time of stored hydrogen can be controlled by geometry of microtanks, temperature or materials properties. The k value of metal material is at least three orders lower than the one of silica glass materials. A very thin metal film 18, as shown in
Both ends 21 of holey fibers are capped to form closure microtanks 20. The capped end of holey fibers is shown in
The hydrogen storage system is shown in