KR101796482B1 - Diaphragmless shock tube - Google Patents
Diaphragmless shock tube Download PDFInfo
- Publication number
- KR101796482B1 KR101796482B1 KR1020160021635A KR20160021635A KR101796482B1 KR 101796482 B1 KR101796482 B1 KR 101796482B1 KR 1020160021635 A KR1020160021635 A KR 1020160021635A KR 20160021635 A KR20160021635 A KR 20160021635A KR 101796482 B1 KR101796482 B1 KR 101796482B1
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- South Korea
- Prior art keywords
- pressure chamber
- chamber
- shock wave
- high pressure
- low
- Prior art date
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B01—PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
- B01J—CHEMICAL OR PHYSICAL PROCESSES, e.g. CATALYSIS OR COLLOID CHEMISTRY; THEIR RELEVANT APPARATUS
- B01J3/00—Processes of utilising sub-atmospheric or super-atmospheric pressure to effect chemical or physical change of matter; Apparatus therefor
- B01J3/06—Processes using ultra-high pressure, e.g. for the formation of diamonds; Apparatus therefor, e.g. moulds or dies
- B01J3/08—Application of shock waves for chemical reactions or for modifying the crystal structure of substances
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B01—PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
- B01J—CHEMICAL OR PHYSICAL PROCESSES, e.g. CATALYSIS OR COLLOID CHEMISTRY; THEIR RELEVANT APPARATUS
- B01J19/00—Chemical, physical or physico-chemical processes in general; Their relevant apparatus
- B01J19/08—Processes employing the direct application of electric or wave energy, or particle radiation; Apparatus therefor
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B01—PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
- B01L—CHEMICAL OR PHYSICAL LABORATORY APPARATUS FOR GENERAL USE
- B01L99/00—Subject matter not provided for in other groups of this subclass
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F16—ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
- F16L—PIPES; JOINTS OR FITTINGS FOR PIPES; SUPPORTS FOR PIPES, CABLES OR PROTECTIVE TUBING; MEANS FOR THERMAL INSULATION IN GENERAL
- F16L55/00—Devices or appurtenances for use in, or in connection with, pipes or pipe systems
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- Chemical & Material Sciences (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Health & Medical Sciences (AREA)
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- Organic Chemistry (AREA)
- Clinical Laboratory Science (AREA)
- Mechanical Engineering (AREA)
- General Health & Medical Sciences (AREA)
- Toxicology (AREA)
- Crystallography & Structural Chemistry (AREA)
- Measuring Fluid Pressure (AREA)
- Pipe Accessories (AREA)
Abstract
With regard to the seam-free shock wave tube,
A high pressure chamber having a leak chamber connection hole at one side thereof; A low pressure chamber having one end inserted into the interior of the high pressure chamber; A leak chamber installed at one side of the high pressure chamber; And an opening / closing rubber fixedly installed on one side of the inside of the high-pressure chamber
It is possible to carry out the repetitive shock wave experiment easily while reducing the time and manpower required for the experiment preparation such as the diaphragm replacement and the like without generating debris or debris in the shock wave generation process.
Description
The present invention relates to a seam-free shock wave tube, and more particularly, to a seam-free shock wave tube capable of opening a low-pressure chamber through an opening / closing rubber that expands or shrinks according to a pressure of a gas filled in a leak chamber, so that debris or debris And to perform repetitive experiments without replacement of the diaphragm.
Fig. 1 is a schematic view of a general shock wave tube, and Fig. 2 is an example of a membrane of a diaphragm.
Generally, as shown in FIG. 1, the
The shock wave tube (10) is an apparatus that obtains shock waves in a low pressure tube through an instantaneous flow generated by a diaphragm (13).
The
The shock wave generated by the membrane of the
When these waves propagate inside the tube and are reflected at the closed end of the tube or the open end of the pipe, a very complex flow occurs.
On the other hand, since the shock wave obtained by the shock wave tube is accompanied by an instantaneous pressure and a temperature rise and propagates at a very high speed, there is a demand in recent years for an industrial demand which utilizes such a characteristic.
In the engineering applications of the shockwave tube, the strength (pressure rise) and propagation speed of the shock wave are mainly determined by the pressure ratio of the high-pressure chamber and the low-pressure chamber and the thickness of the material of the diaphragm. Therefore, So that it can be easily obtained.
The diaphragm material is made of cellophane or synthetic vinyl which is very thin to generate a weak shock wave when the working pressure ratio of the shock wave tube is low, and copper plate or iron plate may be used to generate a very strong shock wave.
As shown in Fig. 2, the diaphragm of such a diaphragm has a form such as a natural diaphragm due to a pressure difference between a high pressure plate and a low pressure plate of a shock wave tube and a forced diaphragm due to a needle or the like from the outside.
Fig. 2 (a) shows the state of the natural wave film, and Fig. 2 (b) shows the wave film by the declination.
The most important problems encountered in the application of most shockwave tubes are the problem of reproducibility of the shock wave tube process and contamination by debris or debris generated during the wave process.
FIG. 3 is a view showing debris or debris generated in the process of rupturing.
Generally, even if the pressure ratio of the shock wave tube is the same, the details of the wave propagation process will vary depending on the experiment, and it is very difficult to precisely control the wave propagation process.
In addition, debris such as debris from faults is generated, which is an important technical problem to be solved in the engineering application of the shock wave tube.
Therefore, it is troublesome to carry out new experiment after cleaning up such pollutants. Moreover, since the diaphragm can not be regenerated after the membrane, it is necessary to replace it with a new diaphragm material every time. It is becoming a limiting factor.
The following Patent Document 1 discloses an improved shock tube structure.
Disclosure of the Invention The present invention has been made to solve the problems of the prior art described above, and its object is to prevent generation of debris or debris in the shock wave generation process by generating shock waves without breaking the diaphragm, Time and manpower
So that the repetitive shock wave test can be performed more easily while reducing the cost of the shock absorber.
In order to accomplish the above object, according to the present invention, there is provided a seam-free shockwave pipe comprising: a high-pressure chamber having a leak chamber connection hole at one side; A low pressure chamber having one end inserted into the interior of the high pressure chamber; A leak chamber installed at one side of the high pressure chamber; And an opening / closing rubber fixedly installed on one side of the interior of the high-pressure chamber.
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The unseparated shockwave tube according to the present invention is characterized in that a recessed portion is provided on the leakage chamber side of the opening / closing rubber.
The non-diaphragm shockwave pipe according to the present invention is characterized in that an induction member is provided at the concave portion of the opening / closing rubber.
The seawater-free shockwave tube according to the present invention is characterized in that the induction slope portion is provided at the tip of the low-pressure chamber.
According to the seawater-free shock wave tube according to the present invention, the shock wave can be generated more accurately, and the shock wave is propagated to the low-pressure chamber, so that no debris or debris is generated by the wave membrane.
Therefore, according to the seawater-free shock wave tube according to the present invention, since it is not necessary to replace the diaphragm, the time required for preparing the experiment can be greatly reduced.
Further, according to the seawater-free shock wave tube according to the present invention, it is possible to repeatedly perform the shock wave test by reusing the high-pressure chamber and the low-pressure chamber.
In addition, according to the non-segregated shockwave pipe according to the present invention, it is possible to reduce the flow generated in the process of flowing the gas of the high-pressure chamber into the low-pressure chamber and to improve the reproducibility of the shock wave generated in the low- do.
1 is a structural view of a general shock wave tube,
Fig. 2 is an example of a membrane of a diaphragm,
FIG. 3 is a view showing debris or debris generated in the process of membrane breaking,
FIG. 4 is a schematic view of a seawall-free shock wave tube according to a preferred embodiment of the present invention,
5 is a detailed view of the main part of the seawater-free shock wave tube according to the preferred embodiment
6 is a sectional view taken along line AA in Fig. 5,
FIG. 7 is a schematic view of a non-segregated shockwave tube according to another embodiment of the present invention. FIG.
FIG. 8 is a longitudinal sectional view of the main part of a seawall-free shock wave tube according to another embodiment; FIG.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will now be described more fully hereinafter with reference to the accompanying drawings, in which preferred embodiments of the present invention are shown.
In the following, the terms "upward", "downward", "forward" and "rearward" and other directional terms are defined with reference to the states shown in the drawings.
FIG. 4 is a configuration diagram of a non-diaphragm shock wave tube according to a preferred embodiment of the present invention, FIG. 5 is a detailed view of a principal portion of a non-diaphragm shock wave tube according to the present preferred embodiment, and FIG. 6 is a sectional view taken along line A-A of FIG.
A seawater-free
The high-
A leak
The low-
The
The distal end portion of the
The
The
The
The opening /
The opening /
The pressureless pressure Ps of the gas filled in the
The high pressure gas filled in the
Therefore, the opening /
If the diaphragm of the
When the pressure inside the
As described above, according to the preferred embodiment of the present invention, the
Therefore, when the shock wave is propagated to the low-
In addition, since it is not necessary to replace the diaphragm, the time required for preparing the experiment can be greatly reduced, and the high-
FIG. 7 is a configuration diagram of a non-diaphragm shock wave tube according to another embodiment of the present invention, and FIG. 8 is a longitudinal sectional view of a principal part of a non-diaphragm shock wave tube according to another embodiment of the present invention.
7 and 8, the
The
The guiding
Further, the flow of the
In addition, the
The
Although the present invention has been described in detail with reference to the above embodiments, it is needless to say that the present invention is not limited to the above-described embodiments, and various modifications may be made without departing from the spirit of the present invention.
100: No-seawater shock wave tube
110: high pressure chamber
120: Low pressure chamber
130: leak chamber
140: Opening and closing rubber
150:
Claims (6)
A low pressure chamber (120) having one end inserted into the high pressure chamber (110);
A leak chamber 130 installed at one side of the high pressure chamber 110;
And an opening / closing rubber (140) fixedly installed on one side of the inside of the high pressure chamber (110)
Wherein the opening / closing rubber (140) is provided with a recessed portion (141) on the side of the leak chamber (130).
Wherein an induction member (150) is provided on a concave portion (141) of the opening / closing rubber (140).
A low pressure chamber (120) having one end inserted into the high pressure chamber (110);
A leak chamber 130 installed at one side of the high pressure chamber 110;
And an opening / closing rubber (140) fixedly installed on one side of the inside of the high pressure chamber (110)
Characterized in that the induction slope part (121) is provided at the tip end of the low-pressure chamber (120).
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
KR1020160021635A KR101796482B1 (en) | 2016-02-24 | 2016-02-24 | Diaphragmless shock tube |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
KR1020160021635A KR101796482B1 (en) | 2016-02-24 | 2016-02-24 | Diaphragmless shock tube |
Publications (2)
Publication Number | Publication Date |
---|---|
KR20170099506A KR20170099506A (en) | 2017-09-01 |
KR101796482B1 true KR101796482B1 (en) | 2017-12-01 |
Family
ID=59923912
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
KR1020160021635A KR101796482B1 (en) | 2016-02-24 | 2016-02-24 | Diaphragmless shock tube |
Country Status (1)
Country | Link |
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KR (1) | KR101796482B1 (en) |
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2016
- 2016-02-24 KR KR1020160021635A patent/KR101796482B1/en active IP Right Grant
Non-Patent Citations (1)
Title |
---|
Geophysical Reseach Letters, 2014, vol. 41, no. 2, pp. 414~421* |
Also Published As
Publication number | Publication date |
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KR20170099506A (en) | 2017-09-01 |
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