System and process for gas recovery

Chemistry of inorganic compounds – Modifying or removing component of normally gaseous mixture

Reexamination Certificate

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C423S215500, C423S219000, C423S220000, C423S235000, C423S262000

Reexamination Certificate

active

06517791

ABSTRACT:

FIELD OF THE INVENTION
The present invention relates to the recovery of gases, and more particularly to the recovery of helium gas in the cold spray forming process.
BACKGROUND OF THE INVENTION
Helium is the gas of choice for cold spray forming (CSF) process. However, the use of helium is economically prohibitive without sufficient helium recovery.
Generally, high velocities are necessary to accelerate the CSF powder towards the work piece. At 5 mole % nitrogen in helium, the sonic velocity will drop 8%. If the nitrogen concentration increases to 20 mole %, then the sonic velocity will reduce 33%. If a heavier impurity such as carbon dioxide reaches 20 mole % with the balance helium, then the sonic velocity will be reduced 43%. High gas velocities possible with pure helium are a desirable physical property regardless of the specific CSF application.
TABLE 1
Sonic Velocity as a Function of Gas
Composition
Carbon
Sonic
Helium
Nitrogen
Water
Dioxide
Velocity
Mole %
Mole %
Mole %
Mole %
Temp. (F.)
(Ft/sec)
100
0
0
0
100
3958
95
5
0
0
100
3467
90
10
0
0
100
3120
85
15
0
0
100
2859
80
20
0
0
100
2653
95
0
5
0
100
3645
95
0
0
5
100
3225
90
0
0
10
100
2788
85
0
0
15
100
2489
80
0
0
20
100
2267
CSF is a newly developed technology that as of this writing has not been made commercial. CSF can be compared to thermal spraying (TS) with a primary difference being the nozzle gas temperature. TS uses particle velocity combined with thermal heat to form a coating on a work piece. A description of both processes will show a problem associated with TS that is solved with CSF and why helium was not used before and is the gas of choice for CSF.
FIG. 1
shows a schematic of the equipment enclosure for CSF and TS. One TS application is plasma spray. Passing gas through an electric arc inside nozzle
14
forms the plasma. Thus, for TS, nozzle
14
, must be water cooled or contain refractory to permit high temperatures. The expected life for nozzle
14
is usually less than 100 hours. Gas and powder pass through nozzle
14
to form spray pattern
16
. Typical nozzle gases could be a mixture of argon and hydrogen. In spray pattern
16
the hydrogen will combust to add additional heat to the powder. The powder will partially or completely melt in spray pattern
16
before hitting work piece
18
and forming a coating on work piece
18
. Care must be taken that work piece
18
does not become too hot or the coating applied too thick. If the coating is too hot or applied too thick, then the coating will crack upon cooling. Care must also be taken in selecting the powder particle size. If the particle size is too small, then losses from vaporization will be economically prohibitive. Spray pattern
16
uses gas velocity and density to accelerate the particle at work piece
18
. High temperatures present in spray pattern
16
decrease gas density which minimizes the impact of gas velocity on particle velocity. TS particle velocities of up to 200 m/s could be expected. Helium can provide higher gas velocities but the density would be substantially lower.
TS may require that a separate fluid be used to cool work piece
18
. The separate fluid could be liquid carbon dioxide or water. Air is also passed through enclosure
12
through gas inlet
22
. A high volume of air passes over work piece
18
and removes excess powder that did not adhere as the coating. The air and powder exhaust from enclosure
12
through gas discharge port
20
. If helium were used in nozzle
14
, then using air to sweep work piece
18
would make helium recovery and purification difficult and expensive.
CSF differs from TS in that at ambient temperatures the powder can be accelerated with helium to about 1000 to about 1200 m/s in nozzle
14
to work piece
18
. CSF temperatures in nozzle
14
, typically less than about 400° F., allows the use of particulate less than 20 micron in size and containing volatile alloying elements. The high velocities capable with helium give the particles sufficient energy to fuse into a coating when striking work piece
18
. The resulting coating does not cause work piece
18
substrate to change as could happen if it was exposed to TS temperatures. Helium is also passed through inlet
22
to sweep over work piece
18
and remove excess powder. The helium and powder discharge from enclosure
12
through vent
20
to helium recovery and purification equipment. In CSF, helium ultimately serves two functions. One, it accelerates the coating powder, supplying kinetic energy. Two, it serves as a clean sweeping gas to clean the work piece of extraneous particles.
No known helium recovery system is believed to exist for CSF. The absence of helium recovery systems for CSF is not surprising because current CSF processes are lab scale and use small quantities of helium. However, other processes that use larger volumes of helium have helium recovery systems.
U.S. Pat. No. 5,377,491 discloses a coolant gas recovery process for a fiber optic cooling tube that uses a vacuum pump/compressor to remove cooling gas from the cooling tube, remove particulate and contaminants and then return the coolant gas to the fiber optic cooling tube. Purification equipment such as pressure swing adsorption, dryer and membrane are discussed with respect to removing water and oxygen, with the maximum quantity of oxygen in the range of 1 to 50 mole percent, and the cooling tube required to cool gas at 0 to 150 psig.
U.S. Pat. No. 4,845,334 discloses a plasma furnace gas recovery system where the gas exits the furnace at high temperature (~700 C) and low pressure (<2 psig). The discharge gas is cooled and then followed by particulate removal equipment. The particulate free gas is then compressed, filtered again and then dried. The dry, compressed helium is then recycled back to the furnace at pressure using gas flows and pressures of 150 SCFM and 100 psig via an oil flooded screw machine.
U.S. Pat. No. 5,158,625 discloses a process for removing helium from a metal hardening (quenching) chamber, purifying the helium and compressing the helium. The quenching chamber was described as 10 M
3
with helium at 2.5 bar absolute (875 SCF of helium). Helium and impurities may be recovered from the hardening furnace through a vacuum pump. Down stream of the vacuum pump the helium plus impurities would be compressed and stored in one receiver. Once all of the desired helium from the hardening furnace was removed, then helium with impurities was passed through a membrane, dryer, PSA or catalytic oxidation of hydrogen to remove oxygen and water from the process. The purified helium is then compressed again and stored at pressure in another receiver until the next hardening cycle starts. The above process uses higher than atmospheric pressures in the quenching chamber to increase the helium density and thus improve the heat transfer capability.
The prior art does not teach or suggest the recovery and purification system comprised of three continuous loops involving the strategic placement of the purification equipment. Further, each loop has its own separate function. In addition to purification and recovery, the current invention is capable of pressurizing the helium to achieve the requisite sonic velocity.
OBJECTS OF THE INVENTION
It is therefore an object of the invention to provide a cost effective helium recovery system that will provide acceptable helium purity (>80 mole %), volume and pressure at the CSF nozzle and for the cleansing sweep across the work piece.
It is another object of this invention to provide for a helium recovery system that will remove contaminants such as oxygen, nitrogen, water, carbon dioxide and particulate from the helium.
SUMMARY OF THE INVENTION
This invention is directed to a three-stage process for recovering and purifying a gas. The steps comprises a) introducing a gas from a chamber to a particulate removing apparatus to form a particulate-free gas, and recycling a first portion of the particulate-free gas to the chamber; b) passing a second portion of the particulate-free gas to a first compressor prior to pass

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