JPS6360828B2 - - Google Patents
Info
- Publication number
- JPS6360828B2 JPS6360828B2 JP59195391A JP19539184A JPS6360828B2 JP S6360828 B2 JPS6360828 B2 JP S6360828B2 JP 59195391 A JP59195391 A JP 59195391A JP 19539184 A JP19539184 A JP 19539184A JP S6360828 B2 JPS6360828 B2 JP S6360828B2
- Authority
- JP
- Japan
- Prior art keywords
- airflow
- control tube
- tube
- ejector
- jet
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
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Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B05—SPRAYING OR ATOMISING IN GENERAL; APPLYING FLUENT MATERIALS TO SURFACES, IN GENERAL
- B05B—SPRAYING APPARATUS; ATOMISING APPARATUS; NOZZLES
- B05B7/00—Spraying apparatus for discharge of liquids or other fluent materials from two or more sources, e.g. of liquid and air, of powder and gas
- B05B7/16—Spraying apparatus for discharge of liquids or other fluent materials from two or more sources, e.g. of liquid and air, of powder and gas incorporating means for heating or cooling the material to be sprayed
- B05B7/22—Spraying apparatus for discharge of liquids or other fluent materials from two or more sources, e.g. of liquid and air, of powder and gas incorporating means for heating or cooling the material to be sprayed electrically, magnetically or electromagnetically, e.g. by arc
- B05B7/222—Spraying apparatus for discharge of liquids or other fluent materials from two or more sources, e.g. of liquid and air, of powder and gas incorporating means for heating or cooling the material to be sprayed electrically, magnetically or electromagnetically, e.g. by arc using an arc
- B05B7/224—Spraying apparatus for discharge of liquids or other fluent materials from two or more sources, e.g. of liquid and air, of powder and gas incorporating means for heating or cooling the material to be sprayed electrically, magnetically or electromagnetically, e.g. by arc using an arc the material having originally the shape of a wire, rod or the like
-
- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C4/00—Coating by spraying the coating material in the molten state, e.g. by flame, plasma or electric discharge
- C23C4/12—Coating by spraying the coating material in the molten state, e.g. by flame, plasma or electric discharge characterised by the method of spraying
- C23C4/131—Wire arc spraying
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Chemical & Material Sciences (AREA)
- Plasma & Fusion (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Materials Engineering (AREA)
- Mechanical Engineering (AREA)
- Metallurgy (AREA)
- Organic Chemistry (AREA)
- Electromagnetism (AREA)
- Nozzles (AREA)
- Coating By Spraying Or Casting (AREA)
Description
【発明の詳細な説明】
従来の溶射方法は、「溶融ないし半溶融金属を
吹き付ける方法」と天動説的に見掛け上の定義に
則した手断の溶射機を用いており、その溶射機か
ら吹き付けられた金属粒子の各箇は、被射体へ付
着直後に冷却と同時に収縮を生じる。この収縮作
用の累積度が頗る大きく、僅かに0.1m/m厚さ
にの平面皮膜が歪なく得られない現実が、創始以
来70余年間続いており、従つて、質的問題が多
く、用途の制約がある。[Detailed Description of the Invention] The conventional thermal spraying method uses a hand-cut thermal spraying machine that conforms to the apparent geocentric definition of ``a method of spraying molten or semi-molten metal.'' Immediately after the metal particles adhere to the object, they cool and simultaneously shrink. The cumulative effect of this shrinkage is so large that it has been difficult to obtain a flat film with a thickness of only 0.1 m/m without distortion for more than 70 years since its creation. There are restrictions.
上記見掛け説とは別に、地動説的に全く逆説的
に、固体金属粒子を吹き付けて、歪なく、質的に
も秀れた各種金属成形物を得る方法を発明し、実
用化を計つているものが、特許第673182号と特許
第1068648号並に特許願昭56―181936号及び昭56
―174889号とで、この新溶射機の性能を更に向上
を計ろうとする方法の発明である。 Apart from the above-mentioned apparent theory, he invented a method of spraying solid metal particles to obtain various metal moldings with excellent quality and no distortion, and is planning to put it into practical use. Patent No. 673182 and Patent No. 1068648 as well as patent application No. 181936 and Patent No. 181936.
- No. 174889, is an invention of a method to further improve the performance of this new thermal spraying machine.
即ち、ニツケルなどの高融点金属の場合、限ら
れた吹き付け用空気量で、亜鉛や真鍮などと同じ
ように、溶射粒子を、大気温度程度まで冷却を行
なうことが困難なため、少し細い溶射材料線を用
いなければならない制約があつた。その後冷却法
について検討の結果、想像外の物象が重複して存
在することと、その対策も判明した。 In other words, in the case of high-melting point metals such as nickel, it is difficult to cool the sprayed particles to about atmospheric temperature with a limited amount of air, as with zinc and brass, so it is difficult to cool the sprayed particles to about atmospheric temperature with a limited amount of air. There was a constraint that I had to use lines. After examining the cooling method, it was discovered that unexpected phenomena overlapped, and countermeasures were also taken.
各種の金属溶射機に亜鉛線を用いて、各機毎に
剛体金属面の一点へ集中溶射を行なうと、期せず
して富士山形の厚い溶射皮膜(成形物)が得られ
る。この溶射物は決して珍しいものではないが各
種の物象を現している。第1図は、これら成形物
の四半裁物断面を2種で説明する。図中Aは、前
記特許の溶射機を用いたもので、歪がなく被射体
54へ付着状態のもの。Bは従来の各種溶射機を
用いたものを表し、激しい歪力で形が崩れ、被射
体から自然的に剥離した状態を表している。 When a zinc wire is used in various metal spraying machines and each machine performs concentrated spraying on one point on a rigid metal surface, a thick sprayed coating (molded product) in the shape of Mt. Fuji is unexpectedly obtained. This thermal spray material is by no means rare, but it exhibits various phenomena. FIG. 1 illustrates two types of quarter cross sections of these molded products. A in the figure shows a spraying machine using the patented thermal spraying machine, which is adhered to the target object 54 without distortion. B represents a state in which various types of conventional thermal spraying machines were used, and the shape was distorted due to severe strain and the material was naturally peeled off from the object being irradiated.
気体の膨張力を利用する吹き付け用気体(空
気)は、噴出時は爆発的で頗る高速度であるが、
常時膨張性が働いており、その一つが末広がり現
象である。この末広がり角に比例した速度と密度
(気圧)の急低減であり、諸能力が零の真空に近
い状態となる。 The blowing gas (air) that utilizes the expansion power of gas is explosive and extremely high velocity when ejected.
Expansive properties are always at work, one of which is the spreading phenomenon. There is a sudden decrease in speed and density (atmospheric pressure) proportional to the divergence angle, resulting in a state close to a vacuum where various capacities are zero.
この気体に比べて金属粒子は巨大な質量であり
初速時に与えられた方向へ銃弾状に、高速度に飛
行する性質が強く、その現れが富士山形で、砂時
計の落下砂の堆積状態に類似しており、傾斜面部
への粒子の結合状態は異状に悪くてもろい点など
より推察すると気流軸心部の粒子分布密度は将に
砂時計並で、初速以後気流の影響が見られない。 Compared to this gas, metal particles have a huge mass and have a strong tendency to fly at high speed in a bullet-like direction in a given direction at the time of initial velocity.The appearance of this is the shape of Mt. Fuji, which is similar to the accumulation of falling sand in an hourglass. Judging from the fact that the bonding state of the particles to the inclined surface is unusually poor and brittle, the particle distribution density at the center of the airflow axis is approximately the same as that of an hourglass, and no influence of the airflow is seen after the initial velocity.
気流速度が急減するに対し、粒子の速度は速
く、気流の軸心圏を群団状に通り抜けて行き、粒
子のもつ残り熱で逆に加温せられるに対し、外周
圏の温度は低く、量的には軸心圏の6〜7倍であ
る。従つて、末広がり現象の制御作用だけでもか
なりの冷却効果を増す筈である。この熱分布状態
を第2図の濃淡で表しており、また、この濃淡
は、粒子の分布度合にも相当していることは、第
1図の富士山形成形物に相当しているからであ
る。 While the airflow speed decreases rapidly, the speed of the particles is high and they pass through the axial center of the airflow in a group, and are heated by the residual heat of the particles, whereas the temperature of the outer circumference is low. In terms of quantity, it is 6 to 7 times larger than the axis. Therefore, the effect of controlling the divergence phenomenon alone should add considerably to the cooling effect. This heat distribution state is represented by the shading in Figure 2, and this shading also corresponds to the degree of distribution of particles, since it corresponds to the Mt. Fuji formation in Figure 1. .
上記の好ましくない冷却作用の改良を計る方法
の要領が第3図の通りで、噴射気流の外周に末広
がりを抑制するための制御管を設ける必要性を前
記したとおりに用いると共に、この制御管をこれ
以外の多重利用で、二重のエジエクター装置とし
て、大量大気の利用と〈かくはん〉と気流の高密
度化等、総合冷却作用が得られ、溶射量及び質的
に史上最高位の溶射機が得られるようになつた。 The outline of the method for improving the above-mentioned undesirable cooling effect is shown in Figure 3.The necessity of providing a control pipe on the outer periphery of the jet air flow to suppress the divergence is as described above, and this control pipe is used as described above. With multiple uses other than this, as a dual ejector device, a comprehensive cooling effect can be obtained by utilizing a large amount of air, stirring, and increasing the density of airflow, resulting in the highest thermal spraying machine ever in terms of spray amount and quality. Now I can get it.
その成果の過程を次の通り詳述する。第1図の
成形物A・B及び第2図の熱分布より勘案して第
3図状で、内部抵抗の低い末広がりの制御管を試
用した例について説明する。 The process of achieving this result is detailed below. In consideration of the molded products A and B in FIG. 1 and the heat distribution in FIG. 2, an example will be described in which a control tube with a wide end and a low internal resistance is used on a trial basis in the third diagram.
この制御管50の一端を、経験の深い独自形式
の環状噴射口18で成る溶射筒1とで図状に結合
を計つている。図中4の圧縮空気供給管より送り
込まれた圧縮空気は、直結する高気圧気圏31を
経て環状噴射口18より噴出し、噴射気流の合流
点20を頂点とする円すい形体60を形成し、底
辺は開放状で、溶射筒1の中心部を通じて矢印6
6部よりエジエクター作用で、大量の大気が吸入
せられており、この大気は合流点20より噴射気
流に吸収せられて、増量気流となり、高圧・高速
度狭角度気流を形成して、制御管50の軸心よ
り、前方の管外へ放射する。吹き付け用噴射気流
の最も強烈な集合部20の気流が一直線に管内を
突き抜けようとするとき、その気流の外周部から
末広がり現象を示すと共に、恰も無数の突起を持
つかの如き振舞いで、自体に接する気体を誘導と
混合並に〈かく乱〉及び熱交換等気体特有の性癖
は、第2のエジエクター作用の場を現出し、制御
管50の内壁との間に、大容量の真空圏を生じる
ため、多数の通気孔51より、大気が波動状に巻
き込まれ、大気と噴射気流との乱流となり〈共鳴
音〉を発することもあり、軸気流の強い進行惰性
力と大量大気とが管内で押し合い柔み合う形で進
行し、環状の熱分布53は崩れ比較的高密度の低
温度(大気温度に近接した)気流となつて管内を
突き抜ける。尚、制御管50の先端部を図状より
長くすると管内の気体密度をある程度まで向上
と、気体温度の低下が計れる。 One end of this control pipe 50 is connected in a diagrammatic manner to the thermal spray tube 1, which is composed of an annular injection port 18 of a unique type with extensive experience. The compressed air sent from the compressed air supply pipe 4 in the figure is ejected from the annular injection port 18 after passing through the directly connected high-pressure atmosphere 31, forming a conical body 60 whose apex is the confluence point 20 of the injection airflow, and whose base is It is open and the arrow 6 passes through the center of the spray tube 1.
A large amount of air is inhaled from section 6 by the ejector action, and this air is absorbed by the jet airflow from the confluence point 20 and becomes an increased airflow, forming a high-pressure, high-velocity, narrow-angle airflow, and then passing through the control pipe. From the axis of 50, it radiates out of the tube in front. When the airflow at the most intense gathering part 20 of the jet airflow tries to penetrate the inside of the pipe in a straight line, the airflow shows a phenomenon of spreading out from the outer periphery and behaves as if it has countless protrusions, and the airflow itself The characteristics peculiar to gases, such as induction, mixing, disturbance, and heat exchange of the gases in contact with the gases, create a field of second ejector action, and create a large-capacity vacuum zone between the control tube 50 and the inner wall of the control tube 50. , the air is drawn into the wave form from the numerous vents 51, and the air and the jet air flow become turbulent, sometimes producing a "resonant sound", and the strong advancing inertia of the axial air flow and the large amount of air push against each other inside the pipe. The air flows in a flexible manner, and the annular heat distribution 53 collapses, forming a relatively high-density, low-temperature (close to atmospheric temperature) airflow that penetrates the inside of the pipe. Note that if the tip of the control tube 50 is made longer than the figure, the gas density within the tube can be improved to a certain extent and the gas temperature can be lowered.
噴射口18が作動しているとき、円すい形体6
0の内側(低気圧気流圏)19へ大気の流入を遮
断すると該部は高度の真空圏を形成する。また該
部へ大気と共に砂を供給すると、その砂は高速度
で前方へ飛散し、所謂サンドブラスト装置作用を
発揮し、鉄鋼・ガラス面を梨地面状に傷付け、米
粒大の砂粒は銃弾状はガラスを貫通する威力を発
揮する。砂の代りにスチールグリツトを用いる
と、砂の作つた傷面より深いが、皮膜を絶対に作
らない。しかし、金属の溶体を上記同様に供給す
ると、紙を始めとする殆んどの微細粗面の固体面
に、金属の皮膜を作る。 When the injection port 18 is activated, the conical body 6
When the inflow of the atmosphere is blocked to the inside of 0 (low pressure atmosphere) 19, this area forms a high vacuum sphere. In addition, when sand is supplied to the area together with the atmosphere, the sand scatters forward at high speed, exerting the effect of a so-called sandblasting device, causing scratches on steel and glass surfaces in the form of a pear-like surface. Demonstrates the power to penetrate. When steel grit is used instead of sand, the scratches are deeper than those created by sand, but never form a film. However, when a metal solution is supplied in the same manner as described above, a metal film is formed on most finely rough solid surfaces including paper.
この現象は直ちに理解が困難なようである。 This phenomenon seems difficult to understand immediately.
持論の説明不足か?対照的な旧説が再燃してい
た時期のためか?これを空論として誰にも顧られ
なかつたが、前記特許の実験溶射機が、一流企業
間に普及し、この現象を既成事実として製品で立
証し、かつ高度な製品を開発しているが、更に高
度化のため、冷却不足で不便を感じている、高融
点金属・合金のニツケル及び高ニツケル.クロー
ム鋼など、高級実用材の利用問題を解消要求のた
めの発明で、紙面だけでは信じ足りないであろう
この現象を理解するために、次の条件を念頭に置
く必要がある。 Am I not explaining my theory enough? Was it because of the period when contrasting old theories were being rekindled? No one thought of this as an empty theory, but the experimental thermal spraying machine of the patent mentioned above has become popular among leading companies, and they have proven this phenomenon as a fait accompli with their products and are developing advanced products. Nickel and high-nickel high melting point metals and alloys are becoming more sophisticated and are experiencing inconvenience due to insufficient cooling. This invention was created to solve the problem of using high-grade practical materials such as chrome steel, and in order to understand this phenomenon, which may be difficult to believe on paper alone, it is necessary to keep the following conditions in mind.
多くの粉体を集録する「粉体物性図説」中にも
該当するものが無く、硬質物体に触れて粉砕され
る一般的粉体と異り、金属の高温溶融体が、激動
する高圧気体中で裂砕せられると、体積比表面積
が頗る大きな樹枝状粉体となり、その瞬間に冷却
と固体化の要因となる。特に高圧気体は高密度で
液体に近い冷却力を持ち、激動状態はその能力を
助長する。この粉体の形態は、飛散中の火山弾及
び、強烈に発生した波の瞬間を高速度カメラが捉
えたものに相当しているが、その粉体の構造と振
舞いから〈雪の断片状〉と、説明が最も理解され
易い。即ち、単独で吹き付けができる点と、絡み
合い性が強く、その集団に加わる圧力に応じて固
まり或は剛体化する性質が共通するからである。 There is no corresponding item in the "Illustrated Illustration of Powder Properties" which collects many powders, and unlike general powders that are crushed by contact with hard objects, high-temperature molten metals are immersed in turbulent high-pressure gas. When crushed, it becomes a large dendritic powder with a large volumetric surface area, which instantly causes cooling and solidification. In particular, high-pressure gas has a high density and a cooling power close to that of a liquid, and turbulent conditions enhance this ability. The shape of this powder corresponds to that captured by a high-speed camera at the moment of a flying volcanic bomb or a powerful wave, but due to the structure and behavior of the powder, it resembles a snow fragment. The explanation is the easiest to understand. That is, they have in common the ability to be sprayed individually, their strong intertwining properties, and the ability to solidify or become rigid in response to pressure applied to the group.
このような性状の粉体が、円すい形噴射気体の
頂点で20部から銃弾状に噴射せられ、その前方
部の気流は熱的には大気に稀釈せられ、断面積的
には約3分の1に縮少した管50内へ数倍化した
混合気流が充満状態で乱流する部分を通過するこ
とは、時間的にも温度的にも充分な冷却が行なわ
れた粉体となり、被射物体と常時均しい温度で溶
射作業の継続ができることは、溶射皮膜に歪の発
生がなく、安易に〓能率的に高融点金属の良質金
属皮膜が得られるようになつたのである。従つ
て、1000℃以下の融点金属は、倍倍的に溶射能力
が増大と無制限厚さの成形物が得られることは、
質・量共に史上最高を誇れるダブル.エジエクタ
ー方式の低温化金属溶射方法。 Powder with such properties is injected like a bullet from 20 parts at the apex of the conical jet gas, and the air flow in the front part is thermally diluted into the atmosphere and has a cross-sectional area of about 3 minutes. When the mixed airflow, which has been reduced to 1, passes through the turbulent part in a full state, the powder is sufficiently cooled both in terms of time and temperature, and is not exposed to heat. Being able to continue thermal spraying at a constant temperature equal to that of the projectile means that there is no distortion in the sprayed coating, and it has become possible to easily and efficiently obtain high-quality metal coatings of high-melting point metals. Therefore, for metals with a melting point below 1000℃, the thermal spraying ability can be doubled and molded products of unlimited thickness can be obtained.
A double that boasts the highest quality and quantity ever. Ejector method low temperature metal spraying method.
第1図は、電気溶線式溶射機の噴射気流の噴流
角度と、噴射金属粒子の堆積状態を縦断面図で表
し、第2図は、第1図の気流が被射体面上に到着
時点の気流軸中の熱分布を、色彩濃度で表す。第
3図は本発明溶射機の作動状態で表す縦断面図。
1は溶射筒、2はラツパ形壁体、4は圧縮空気
送気管、5は環状噴射口体、7は導線管、8は溶
射用線、9は導電端子、10は皿状抱金、12は
送線ロール、18は環状噴射口、19は低気圧気
流圏、20は噴射気流の合流点、21は吹き付け
気流、23はアーク、27はケース、31は高気
圧気圏(圧縮空気圏)、40は複数の微小噴射口、
50は末広がり制御管、51は末広がり制御管に
穿たれた複数箇の大気通気口兼透視孔、52は金
属の溶体、53は従来機の吹き付け気流、54は
被射体、55は本溶射機の堆積物、60は円すい
形噴射気流、66は大気通気路、Aは低温化溶射
幾の溶射堆積物、Bは縦来機の熱間溶射堆積物、
Cは熱分布。
Figure 1 shows the jet angle of the jet air stream of an electric wire thermal spray machine and the deposition state of the sprayed metal particles in a longitudinal cross-sectional view, and Figure 2 shows the state of the air stream at the time of arrival on the surface of the object to be sprayed. The heat distribution in the airflow axis is expressed by color density. FIG. 3 is a longitudinal sectional view showing the thermal spraying machine of the present invention in an operating state. 1 is a thermal spray tube, 2 is a lapper-shaped wall body, 4 is a compressed air supply pipe, 5 is an annular injection port body, 7 is a conductor tube, 8 is a thermal spray wire, 9 is a conductive terminal, 10 is a plate-shaped holder, 12 is a feed roll, 18 is an annular jet nozzle, 19 is a low-pressure atomosphere, 20 is a confluence of jet airflows, 21 is a blowing airflow, 23 is an arc, 27 is a case, 31 is a high-pressure atomosphere (compressed airsphere), 40 has multiple micro-injection orifices,
50 is a control tube that spreads out at the end, 51 is a plurality of atmospheric vents and see-through holes bored in the control tube that spreads out at the end, 52 is a metal solution, 53 is a blowing air stream of a conventional machine, 54 is an object to be irradiated, and 55 is this thermal spraying machine. , 60 is a conical jet air flow, 66 is an atmospheric ventilation passage, A is a thermal spray deposit from a low-temperature spray jet, B is a hot spray deposit from a previous machine,
C is heat distribution.
Claims (1)
端方向に、大小複数箇の貫通孔をもち、内部軸心
に設けた環状噴射口から他端に向けた噴射気流が
形成する円すい形体の内側真空部圏部内へ、底辺
方向から大気と共に送り込む金属溶体を、該圏先
端の噴射気体合流部で、樹枝状に裂砕と冷却によ
る固体化並に加速を計ると共に、前記円すい形体
の外側と末広がり制御管の内壁間に生じる真空圏
へ流入する大量大気と噴射気流とで成る高密度で
低温度の混合気流で、その固体化金属粒子の冷却
度を更に高めつつ、前方の末広がり制御管他端よ
り放射を計ることを特徴とするダブル.エジエク
ター方式の低温化金属溶射方法。 2 溶射筒の前端部に設けた軸方向螺子へ、透視
窓及び通気孔を複数箇設けた任意長さと太さの末
広がり制御管を互換性に、溶射筒頭部へ螺合構成
を特徴とする特許請求の範囲第1項記載のダブ
ル.エジエクター方式の低温化金属溶射方法。 3 円すい形噴射気流の内側竝に外側と末広がり
制御管の内壁間とに生じるエジエクター作用によ
る吸気大気とで吹き付け気流の温度低下を計るこ
とを特徴とする特許請求の範囲第1項と第2項記
載のダブル.エジエクター方式の低温化金属溶射
方法。[Scope of Claims] 1. A plurality of large and small through holes are provided at one end of the airflow control tube that surrounds the jet airflow, and a jet airflow is formed from an annular injection port provided at the internal axis toward the other end. The metal solution, which is fed into the inner vacuum sphere of the conical shape from the bottom direction together with the atmosphere, is splintered into dendritic shapes and solidified by cooling at the injection gas confluence section at the tip of the sphere, as well as being accelerated. A high-density, low-temperature mixed airflow consisting of a large amount of air flowing into the vacuum space created between the outside of the shape and the inner wall of the control tube that spreads outward, and the jet airflow, further increases the degree of cooling of the solidified metal particles and cools the solidified metal particles. A double type characterized by measuring radiation from the other end of the control tube that spreads out at the end. Ejector method low temperature metal spraying method. 2. A diverging control tube of arbitrary length and thickness with multiple viewing windows and ventilation holes is compatible with the axial screw provided at the front end of the thermal spraying tube and is screwed onto the head of the thermal spraying tube. The double according to claim 1. Ejector method low temperature metal spraying method. 3. Claims 1 and 2, characterized in that the temperature of the blown air stream is reduced by the intake atmosphere due to the ejector action that occurs between the inner wall of the conical injection air stream and the inner wall of the control tube that spreads outward. Double as stated. Ejector method low temperature metal spraying method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59195391A JPS6173871A (en) | 1984-09-17 | 1984-09-17 | Method for spraying thermally metal at lower temperature by double ejector type |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59195391A JPS6173871A (en) | 1984-09-17 | 1984-09-17 | Method for spraying thermally metal at lower temperature by double ejector type |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6173871A JPS6173871A (en) | 1986-04-16 |
| JPS6360828B2 true JPS6360828B2 (en) | 1988-11-25 |
Family
ID=16340368
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59195391A Granted JPS6173871A (en) | 1984-09-17 | 1984-09-17 | Method for spraying thermally metal at lower temperature by double ejector type |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6173871A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE112020004771T5 (en) | 2019-10-03 | 2022-06-15 | AGC Inc. | LAMINATED GLASS |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6490597A (en) * | 1987-09-30 | 1989-04-07 | Ryoichi Kasagi | Manufacture of electromagnetic wave absorption film and its applied article |
| JP2799718B2 (en) * | 1988-12-23 | 1998-09-21 | 御芳 中川 | Arc spraying method and apparatus |
| ATE192510T1 (en) * | 1996-06-28 | 2000-05-15 | Metalspray International Lc | METHOD AND DEVICE FOR THERMAL SPRAYING |
| JP4268193B2 (en) * | 2006-09-01 | 2009-05-27 | 株式会社神戸製鋼所 | Acceleration nozzle |
-
1984
- 1984-09-17 JP JP59195391A patent/JPS6173871A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE112020004771T5 (en) | 2019-10-03 | 2022-06-15 | AGC Inc. | LAMINATED GLASS |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6173871A (en) | 1986-04-16 |
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