TW201233449A - Plasma spraying device - Google Patents

Plasma spraying device Download PDF

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Publication number
TW201233449A
TW201233449A TW100145036A TW100145036A TW201233449A TW 201233449 A TW201233449 A TW 201233449A TW 100145036 A TW100145036 A TW 100145036A TW 100145036 A TW100145036 A TW 100145036A TW 201233449 A TW201233449 A TW 201233449A
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Taiwan
Prior art keywords
gas
wire
primary
plasma
nozzle
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TW100145036A
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Chinese (zh)
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TWI650182B (en
Inventor
Masanobu Sugimoto
Kenichi Yamada
Masanobu Irie
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Fuji Eng
Yamada Corrosion Prot Co Ltd
West Nippon Expressway Company Ltd
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Publication of TW201233449A publication Critical patent/TW201233449A/en
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    • HELECTRICITY
    • H05ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05HPLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
    • H05H1/00Generating plasma; Handling plasma
    • H05H1/24Generating plasma
    • H05H1/26Plasma torches
    • H05H1/32Plasma torches using an arc
    • H05H1/42Plasma torches using an arc with provisions for introducing materials into the plasma, e.g. powder, liquid
    • CCHEMISTRY; METALLURGY
    • C23COATING 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
    • C23CCOATING 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
    • C23C4/00Coating by spraying the coating material in the molten state, e.g. by flame, plasma or electric discharge
    • C23C4/12Coating by spraying the coating material in the molten state, e.g. by flame, plasma or electric discharge characterised by the method of spraying
    • C23C4/134Plasma spraying

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  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Plasma & Fusion (AREA)
  • Chemical & Material Sciences (AREA)
  • Mechanical Engineering (AREA)
  • Materials Engineering (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Nozzles (AREA)
  • Coating By Spraying Or Casting (AREA)
  • Plasma Technology (AREA)

Abstract

The subject of this invention is to provide a plasma spray device capable of reducing the surface oxidation of particles becoming molten droplets to form the spray coating film with less oxide. The solution of this invention comprises: a primary gas passage (11), forming a primary gas nozzle (10) at the outer periphery of a cathode (40) and covering the front end part of the cathode (40); a secondary gas nozzle (20) disposed outside the primary gas nozzle (10) and forming a secondary gas passage (21); and a tertiary gas nozzle (30) forming a tertiary gas passage (31) between the primary gas nozzle (10) and the secondary gas nozzle (20). The tertiary gas passage (31) receives the thermal jet of plasma flame (F) at the outer periphery part of the plasma flame (F) to become a tertiary gas of high temperature gas jet.

Description

201233449 六、發明說明: 【發明所屬之技術領域】 本發明係關於,將電漿電弧移至電傳導性之金屬絲 發生電漿火焰,一邊使金屬絲熔滴一邊進行噴射之電槳 塗裝置。 【先前技術】 第7圖係傳統電漿噴塗裝置之槪念剖面圖。如第7 所示,傳統電漿噴塗裝置90,係具備:形成一次氣體 路91a之一次氣體噴嘴91 ;配置於一次氣體噴嘴91之 側,形成二次氣體通路92a之二次氣體噴嘴92 ;配置 一次氣體噴嘴91之噴嘴口 91b及二次氣體噴嘴92之噴 口 92a之大致中心軸上的陰極93;電源裝置94;以及 二次氣體噴嘴92之噴嘴口 92a附近供應噴塗用之電傳 性金屬絲W的金屬絲導引孔95。 金屬絲W,係從金屬絲導引孔95朝向噴嘴口 92a 中心軸而供應給斜前方。並且,從一次氣體通路9 1 a噴 之一次氣體,被發生在介由二次氣體噴嘴92間接連結 電源裝置94之陽極側的金屬絲W、及連結於電源裝置 之陰極側的陰極93之間的電弧電漿化而成爲電漿火焰 ,並以熔滴D來噴射金屬絲W。該熔滴D,被從二次氣 通路92 a朝二次氣體噴嘴92之前方噴射的二次氣體進 步微細化,再加速地被噴射於被處理物τ上’而形成噴 被膜S。 來 噴 圖 通 外 於 嘴 對 導 之 出 於 94 F 體 塗 -5- 201233449 並且,如上所示之傳統電漿噴塗裝置90時,一次氣 體,係使用氮氣體或氬氣體等惰性氣體,二次氣體,係使 用壓縮空氣、氮氣體、碳酸氣體等之氣體(例如,參照專 利文獻1)。然而,實際運用時,二次氣體方面,因爲氮 氣體及碳酸氣體等之運轉成本較高,而利用低成本之壓縮 空氣。在電漿噴塗裝置90,以該二次氣體之壓縮空氣來 圍繞被電漿化之一次氣體,可以使電漿化之一次氣體的噴 射變細,而且,可以實現一次氣體之高速化。 [專利文獻1]日本特開平9-30897〇號公報 【發明內容】 然而,在傳統之電漿噴塗裝置90,係利用二次氣體 之噴射來使熔融之金屬絲W的熔滴D變細,而且,爲了 對各熔滴D賦予充份之速度,噴塗皮膜S中之金屬材料 ,因爲熔融時之二次氣體之壓縮空氣的急速混入,而於電 漿火焰F之外周部發生擾動。所以,成爲熔滴D之粒子 的表面氧化,而使噴塗皮膜S中含有金屬材料之氧化物。 所以,本發明之目的,係在提供一種以降低成爲熔滴 之粒子表面的氧化,來形成氧化物較少之噴塗皮膜的電漿 噴塗裝置。 本發明之電漿噴塗裝置,係具備:陰極;於該陰極之 外周形成一次氣體通路並覆蓋陰極之前端部的一次氣體噴 嘴;配置於該一次氣體噴嘴之外側並形成二次氣體通路之201233449 VI. Description of the Invention: [Technical Field] The present invention relates to an electric paddle coating device that moves a plasma arc to a conductive wire to generate a plasma flame while ejecting the wire while spraying . [Prior Art] Fig. 7 is a cross-sectional view of a conventional plasma spraying device. As shown in Fig. 7, the conventional plasma spraying device 90 includes a primary gas nozzle 91 that forms the primary gas passage 91a, and a secondary gas nozzle 92 that is disposed on the side of the primary gas nozzle 91 to form the secondary gas passage 92a. The nozzle 93 of the primary gas nozzle 91 and the cathode 93 on the substantially central axis of the nozzle 92a of the secondary gas nozzle 92; the power supply device 94; and the vicinity of the nozzle opening 92a of the secondary gas nozzle 92 supply the electroconductive wire for spraying Wire guide hole 95 of W. The wire W is supplied obliquely forward from the wire guiding hole 95 toward the central axis of the nozzle opening 92a. Further, the primary gas sprayed from the primary gas passage 9 1 a is caused to be indirectly connected between the wire W on the anode side of the power supply device 94 via the secondary gas nozzle 92 and the cathode 93 connected to the cathode side of the power supply device. The arc is plasmated to become a plasma flame, and the wire W is sprayed by the droplet D. The droplet D is further refined by the secondary gas injected from the secondary gas passage 92a toward the front of the secondary gas nozzle 92, and is accelerated to be sprayed onto the workpiece τ to form the spray film S. When the conventional plasma spraying device 90 shown above is used as the above-mentioned conventional plasma spraying device 90, the primary gas is an inert gas such as nitrogen gas or argon gas, twice. As the gas, a gas such as compressed air, a nitrogen gas, or a carbonic acid gas is used (for example, refer to Patent Document 1). However, in actual use, in terms of secondary gas, low-cost compressed air is utilized because of the high operating cost of nitrogen gas and carbonic acid gas. In the plasma spraying apparatus 90, the primary gas to be pulverized is surrounded by the compressed air of the secondary gas, whereby the primary gas of the plasma can be sprayed, and the speed of the primary gas can be increased. [Patent Document 1] Japanese Laid-Open Patent Publication No. Hei 9-30897-A No. JP-A No. Hei 9-30897-A. SUMMARY OF THE INVENTION However, in the conventional plasma spraying apparatus 90, the droplet D of the molten metal wire W is thinned by the spraying of the secondary gas. Further, in order to impart a sufficient speed to each of the droplets D, the metal material in the spray coating S is disturbed in the outer periphery of the plasma flame F because the compressed air of the secondary gas at the time of melting rapidly enters. Therefore, the surface of the particles of the droplet D is oxidized, and the sprayed coating S contains an oxide of a metal material. Accordingly, it is an object of the present invention to provide a plasma spraying apparatus which forms a sprayed film having less oxide by reducing oxidation of the surface of the particles which become droplets. A plasma spraying apparatus according to the present invention includes: a cathode; a primary gas nozzle that forms a primary gas passage on the outer periphery of the cathode and covers an end portion of the cathode; and is disposed outside the primary gas nozzle to form a secondary gas passage

S -6- 201233449 二次氣體噴嘴;以及對該二次氣體噴嘴之噴嘴口附近供應 噴塗用之金屬絲的金屬絲通路,利用由金屬絲通路所供應 之金屬絲的前端、與陰極之間所產生的電弧,一次氣體噴 嘴所噴射之一次氣體被電漿化,並形成由一次氣體噴嘴所 噴射之電漿火焰使金屬絲之前端成爲熔滴,再以電漿火焰 及二次氣體噴嘴所噴射之二次氣體將該溶摘噴射至被處理 物上之電漿噴塗裝置,且,在一次氣體噴嘴及二次氣體噴 嘴之間,於電漿火焰之外周部則具備有:形成有用以噴射 使其受取電漿火焰之熱而成爲高溫之氣體噴射爲目的之三 次氣體之三次氣體通路的三次氣體噴嘴。 依據本發明之電漿噴塗裝置,在從配置於一次氣體通 路及二次氣體通路之間之三次氣體通路所噴射之三次氣體 流之內側,受取電漿火焰之熱而形成高溫之氣體噴射。藉 由該高溫之氣體噴射,於外側噴射之二次氣體之急速混入 時,抑制從電漿火焰之外周部所發生的擾動,因爲防止電 漿火焰之擴散,故可減少成爲熔滴之粒子表面的氧化。 此處,三次氣體可以使用壓縮空氣及碳酸氣體等,然 而,三次氣體以使用氬氣體及氮氣體等惰性氣體爲佳。三 次氣體使用惰性氣體時,防止二次氣體之急速混入而從電 漿火焰之外周部所發生之擾動,並且.,在電漿火焰之外周 部,形成受取電漿火焰之熱而成爲高溫之惰性氣體噴射。 藉此,熔滴之粒子,因爲在高溫之惰性氣體噴射中被微細 化、加速,而可避免二次氣體所導致的氧化。 並且,在本發明之電漿噴塗裝置,即使一次氣體使用 201233449 壓縮空氣時,也可形成氧化較少之噴塗皮 用壓縮空氣時,一次氣體大約含有20% 體被電漿化之狀態下,熔融金屬之氧化作 使用壓縮空氣作爲一次氣體,應可減少噴 然而,在傳統之電漿噴塗裝置,因爲二次 而使電漿火焰受到擾動時,熔滴之氧化會 次氣體使用壓縮空氣時,會導致皮膜品質 面,本發明之電漿噴塗裝置時,係利用三 焰之外周部形成受取電漿火焰之熱而成爲 ,因爲可以防止二次氣體之急速混入而使 動,即使一次氣體使用壓縮空氣時,也可 噴塗皮膜。 (1)藉由具有:於一次氣體噴嘴及 間,形成有用以噴射以在電漿火焰之外周 之熱而成爲高溫之氣體噴射爲目的之三次 通路的三次氣體噴嘴,故可防止電漿火焰 爲熔滴之粒子表面的氧化,而可形成氧化 膜。 (2 )三次氣體使用惰性氣體時,於 部形成受取電漿火焰之熱而成爲高溫之惰 爲熔滴之粒子在高溫之惰性氣體噴射中被 而避免二次氣體所導致之氧化,故可形成 塗皮膜。 (3) —次氣體使用壓縮空氣時,三 膜。一次氣體使 之氧,然而,氣 用當然減少,故 塗皮膜之氧化。 氣體之急速混入 過度進行,故一 的降低。另一方 次氣體於電漿火 高溫之氣體噴射 電漿火焰受到擾 形成氧化較少之 二次氣體噴嘴之 部受取電漿火焰 氣體之三次氣體 之擴散,減少成 物較少之噴塗皮 電漿火焰之外周 性氣體噴射,因 微細化、加速, 氧化物更.少之噴 次氣體也會於電 -8 -S -6- 201233449 secondary gas nozzle; and a wire passage for supplying a wire for spraying near the nozzle opening of the secondary gas nozzle, using a tip end of the wire supplied from the wire passage and the cathode The generated arc, the primary gas injected by the primary gas nozzle is plasmad, and a plasma flame sprayed by the primary gas nozzle is formed to make the front end of the wire become a droplet, and then sprayed by the plasma flame and the secondary gas nozzle. The secondary gas is sprayed onto the plasma spraying device on the workpiece, and between the primary gas nozzle and the secondary gas nozzle, the peripheral portion of the plasma flame is provided with: It is a tertiary gas nozzle that takes the heat of the plasma flame and becomes the tertiary gas passage of the tertiary gas for the purpose of high-temperature gas injection. According to the plasma spraying apparatus of the present invention, the heat of the plasma flame is received from the inside of the three gas streams ejected from the three gas passages disposed between the primary gas passage and the secondary gas passage to form a high-temperature gas injection. By the high-temperature gas injection, when the secondary gas injected on the outside is rapidly mixed, the disturbance occurring from the outer periphery of the plasma flame is suppressed, and since the diffusion of the plasma flame is prevented, the particle surface to be the droplet can be reduced. Oxidation. Here, as the tertiary gas, compressed air, carbonic acid gas or the like can be used. However, it is preferable to use an inert gas such as argon gas or nitrogen gas for the tertiary gas. When the inert gas is used for the tertiary gas, the rapid intrusion of the secondary gas is prevented, and the disturbance occurs from the outer periphery of the plasma flame, and, in the outer periphery of the plasma flame, the heat of the plasma flame is formed to become the inertia of the high temperature. Gas injection. Thereby, the particles of the droplet can be prevented from being oxidized by the secondary gas because they are refined and accelerated in the inert gas injection at a high temperature. Further, in the plasma spraying apparatus of the present invention, even when the primary gas uses 201233449 compressed air, it is possible to form a compressed air for the sprayed skin which is less oxidized, and the primary gas contains about 20% of the body to be pulverized and melted. The oxidation of metal as a primary gas should reduce the spray. However, in the conventional plasma spraying device, when the plasma flame is disturbed by the second time, the oxidation of the droplet will use compressed air when the gas is used. In the plasma spraying apparatus of the present invention, the plasma spraying device of the present invention is formed by using the heat of the plasma flame in the peripheral portion of the three flames, because the secondary gas can be prevented from rapidly entering and moving, even if the primary gas uses compressed air. The film can also be sprayed. (1) By having a tertiary gas nozzle for injecting a three-passage for the purpose of jetting a gas which is heated to a high temperature in the outer periphery of the plasma flame, it is possible to prevent the plasma flame from being The surface of the droplets is oxidized to form an oxide film. (2) When the inert gas is used for the tertiary gas, the heat generated by the plasma flame is formed in the portion to become a high temperature. The particles which are droplets are prevented from being oxidized by the secondary gas in the high-temperature inert gas injection, so that it can be formed. Coating the film. (3) - Three membranes when compressed air is used for secondary gas. The primary gas makes oxygen, however, the gas is of course reduced, so the oxidation of the coating film. The rapid mixing of the gas is excessively carried out, so that it is lowered. The other gas is irritated by the gas jet plasma flame at the high temperature of the plasma fire to form the third gas nozzle which is less oxidized, and is diffused by the three gases of the plasma flame gas, thereby reducing the spray plasma flame of the product. Excessive gas injection, due to miniaturization, acceleration, oxides, and less, the gas will also be in the electricity -

S 201233449 漿火焰之外周部形成受取電漿火焰之熱而成爲高溫之氣體 噴射,進而防止二次氣體之急速混入所造成之電漿火焰的 擾動,故可形成氧化較少之噴塗皮膜。 【實施方式】 第1圖係本發明之實施方式之電漿噴塗裝置的槪略構 成圖,第2圖係第1圖之電漿火矩之主要部位的詳細縱剖 面圖,第3圖係第2圖之A箭頭方向圖,第4圖係第1 圖之電漿火矩的動作說明圖。 第1圖中,本發明之實施方式之電漿噴塗裝置1,係 具有:將因電漿火焰而成爲熔滴之金屬絲W噴射於被處 理物上之電漿噴塗火矩2;對電漿噴塗火矩2供應一次氣 體及二次氣體之氣體供應源3;對電漿噴塗火矩2供應動 作電力之電源4 ;供金屬絲W捲繞之金屬絲捲軸5 ;用以 矯正從金屬絲捲軸5被拉出之金屬絲W之捲曲習性的金 屬絲矯正機6 ;以及以金屬絲步進管8對電漿噴塗火矩2 供應金屬絲W之金屬絲供應機構7。 如第2圖所示,電漿噴塗火矩2,係具備:形成一次 氣體通路11之一次氣體噴嘴10;配置於一次氣體噴嘴10 之外側,形成二次氣體通路21之二次氣體噴嘴20;配置 於一次氣體噴嘴10及二次氣體噴嘴20之間,形成三次氣 體通路31之三次氣體噴嘴30:配置於一次氣體噴嘴1〇 之噴嘴口 12及二次氣體噴嘴20之噴嘴口 22之大致中心 軸上的陰極40;以及對二次氣體噴嘴20之噴嘴口 22附 -9 - 201233449 近供應噴塗用金屬絲W之金屬絲通路5 0。 一次氣體噴嘴10,係以覆蓋陰極40之前端部的方 來形成,並且,於陰極40之外周,形成一次氣體通路 。供應給該一次氣體通路11之一次氣體,係以發生電 火焰而使金屬絲之前端成爲熔滴爲目的之氣體,爲氮氣 及氬氣體等惰性氣體。或者,該一次氣體也可使用壓縮 氣。由一次氣體通路11所供應之一次氣體,以繞過陰 4〇外周的方式被供應,由一次氣體噴嘴10之噴嘴口 朝二次氣體噴嘴20之前方噴射。 三次氣體噴嘴30,係以包圍一次氣體噴嘴1〇之外 的方式來形成,並且,於一次氣體噴嘴10之外周,形 三次氣體通路31。三次氣體,係以於一次氣體所發生 電漿火焰外周部形成受取電漿火焰之熱而成爲高溫之氣 噴射爲目的之氣體,爲壓縮空氣及碳酸氣體等氣體。二 氣體噴嘴20,係以包圍三次氣體噴嘴30之外側的方式 形成,並且,於三次氣體噴嘴30之外周,形成二次氣 流路2 1。二次氣體,係以從外側對一次氣體所形成之 漿火焰之噴射以急速混入之方式進行噴射,使熔滴成爲 細之物並使熔滴具有充份之速度來噴射於被處理物上爲 的之氣體,係壓縮空氣及碳酸氣體等氣體。 一次氣體,因爲係以氣體流量變化來適度改變電漿 陷之溫度、速度及發生電壓,故其流量以在50〜120 ( 分)之範圍爲佳。並且,一次氣體之流量爲50 ( L/分 以下時,電漿火焰之速度較慢,將導致噴塗皮膜品質的 式 11 漿 體 空 極 12 側 成 之 體 次 來 體 電 更 g 火 L/ ) 降S 201233449 The outer peripheral part of the slurry flame forms a gas which is subjected to the heat of the plasma flame and becomes a high temperature, thereby preventing the disturbance of the plasma flame caused by the rapid mixing of the secondary gas, so that a spray film having less oxidation can be formed. [Embodiment] Fig. 1 is a schematic structural view of a plasma spraying apparatus according to an embodiment of the present invention, and Fig. 2 is a detailed longitudinal sectional view of a main part of a plasma flame moment of Fig. 1, and Fig. 3 is a Fig. 2 is a diagram showing the arrow direction of Fig. 4, and Fig. 4 is an explanatory diagram of the operation of the plasma flame moment of Fig. 1. In the first embodiment, a plasma spraying apparatus 1 according to an embodiment of the present invention has a plasma spraying torch 2 for spraying a wire W which becomes a droplet due to a plasma flame onto a workpiece; Spraying the fire moment 2 to supply the gas supply source 3 of the primary gas and the secondary gas; the power supply 4 for supplying the operating power to the plasma spraying torch 2; the wire reel 5 for winding the wire W; for correcting the wire reel A wire straightening machine 6 for the crimping habit of the drawn wire W; and a wire supplying mechanism 7 for supplying the wire W to the plasma spraying torch 2 by the wire stepping tube 8. As shown in Fig. 2, the plasma spraying torch 2 includes a primary gas nozzle 10 forming a primary gas passage 11, and a secondary gas nozzle 20 disposed outside the primary gas nozzle 10 to form a secondary gas passage 21; The tertiary gas nozzle 30 disposed between the primary gas nozzle 10 and the secondary gas nozzle 20 to form the tertiary gas passage 31 is disposed at substantially the center of the nozzle opening 12 of the primary gas nozzle 1 and the nozzle opening 22 of the secondary gas nozzle 20. The cathode 40 on the shaft; and the nozzle opening 22 of the secondary gas nozzle 20 are attached to the wire passage 50 of the coating wire W. The primary gas nozzle 10 is formed to cover the front end of the cathode 40, and a primary gas passage is formed on the outer circumference of the cathode 40. The primary gas supplied to the primary gas passage 11 is an inert gas such as nitrogen gas or argon gas for the purpose of generating an electric flame and causing the front end of the wire to be a droplet. Alternatively, compressed gas may be used as the primary gas. The primary gas supplied from the primary gas passage 11 is supplied so as to bypass the outer circumference of the cathode, and is ejected from the nozzle opening of the primary gas nozzle 10 toward the front of the secondary gas nozzle 20. The tertiary gas nozzle 30 is formed to surround the primary gas nozzle 1 ,, and the gas passage 31 is formed three times outside the primary gas nozzle 10. The tertiary gas is a gas for the purpose of gas injection in which the heat of the plasma flame is generated in the outer peripheral portion of the plasma flame and is a high-temperature gas injection, and is a gas such as compressed air or carbonic acid gas. The two gas nozzles 20 are formed to surround the outer side of the tertiary gas nozzle 30, and a secondary gas flow path 21 is formed on the outer periphery of the tertiary gas nozzle 30. The secondary gas is sprayed in such a manner that the jet flame formed by the primary gas is rapidly mixed in from the outside, so that the droplet becomes fine and the droplet has a sufficient speed to be ejected onto the workpiece. The gas is a gas such as compressed air or carbonic acid gas. The primary gas is preferably in the range of 50 to 120 (minutes) because the temperature, velocity, and voltage of the plasma are moderately changed by the change in the gas flow rate. Moreover, when the flow rate of the primary gas is 50 (L/min or less, the speed of the plasma flame is slow, which will result in the quality of the sprayed film, and the shape of the slurry on the side of the slurry 12 is the second generation of the body. drop

S -10- 201233449 ' 低。另一方面,一次氣體之流量超過120( L/分)時,電 漿火焰之速度太快,溫度降低而導致噴塗皮膜品質的降低 〇 二次氣體,如前面所述,係以從外側對一次氣體所形 成之電漿火焰之噴射以急速混入之方式進行噴射,來使熔 滴細化且賦予熔滴充份之速度爲目的,故其流量以250〜 5 00 ( L/分)爲佳。並且,二次氣體之流量在250 ( L/分) 以下時,熔滴細化不足,或者,賦予熔滴充份之速度的效 果減少,將導致噴塗皮膜品質的降低。另一方面,二次氣 體之流量超過500 ( L/分)時,熔滴過細且熔滴過度冷卻 ,將導致噴塗皮膜品質的降低。 三次氣體,如前面所述,爲了於一次氣體所發生之電 漿火焰的外周部形成受取電漿火焰之熱而成爲高溫之氣體 噴射,故體積比應爲一次氣體之流量的20〜50 %之範圍 ,並且,爲了抑制二次氣體噴射所導致之電漿火焰的擾動 及氣體擴散,體積比以二次氣體之流量的5〜10%之範圍 爲佳。而且,爲了有效發揮抑制二次氣體噴射所導致之電 漿火焰之擾動及氣體擴散的效果,使三次氣體之流量,隨 著二次氣體流量之增減而連動變化,故以二次氣體之流量 較少時,三次氣體之流量也較少,二次氣體之流量較多時 ,三次氣體之流量也較多之方式爲佳。 並且,三次氣體之流量,在一次氣體之流量未達20 %、或二次氣體之流量未達5%時,因爲三次氣體之噴射 - 抑制電漿火焰之擾動及氣體擴散的效果較少,不易得到提 -11 - 201233449 升噴塗皮膜品質之效果。另一方面,三次氣體之流量,超 過一次氣體之流量的50%、或超過二次氣體之流量的1〇 %時,因爲發生較強之三次氣體的噴射,形成於其內側之 受取電漿火焰之熱而成爲高溫之氣體噴射不足,就無法充 份發揮抑制電漿火焰之擾動及氣體擴散的效果,而難以獲 得提升噴塗皮膜品質的效果。 金屬絲通路50,係由:具有形成於二次氣體噴嘴20 之噴嘴口 2 2附近之金屬絲出口 5 1 b的一次金屬絲通路 5 1 a ;及對該一次金屬絲通路5 1 a以特定傾斜角Θ供應金屬 絲W之二次金屬絲通路5 2 a ;所構成。金屬絲通路5 0, 係以一次金屬絲通路5 1 a及二次金屬絲通路5 2 a,對金屬 絲W賦予不超過彈性限度之範圍的彎曲。 如第3圖所示,一次金屬絲通路51a,係具有電漿火 焰之伸展方向較長之略呈長方形的剖面形狀,係以使配置 於二次氣體噴嘴20外側之一次金屬絲導引構件5 1貫通成 直線狀之方式來形成。同樣的,二次金屬絲通路52a,也 具有電漿火焰之伸展方向較長之略呈長方形的剖面形狀, 係以使配置於離開一次金屬絲通路5 1 a之位置的二次金屬 絲導引構件52貫通成直線狀之方式來形成。 一次金屬絲通路51a之長邊方向的寬度a,設定成金 贐絲W之直徑d之1 0 %以上且9 5 %以下之範圍的大小。 此外,一次金屬絲通路5 1 a之短邊方向的寬度b,則設定 成金屬絲W之直徑d之3 %以上且未達1 〇 %之範圍的大 小。並且,本實施方式之金屬絲W的直徑d爲1.6mm ’S -10- 201233449 ' Low. On the other hand, when the flow rate of the primary gas exceeds 120 (L/min), the speed of the plasma flame is too fast, and the temperature is lowered to cause a decrease in the quality of the sprayed coating. The secondary gas, as described above, is once from the outside. The jet of the plasma flame formed by the gas is sprayed in such a manner as to be rapidly mixed, so that the droplet is refined and the speed of the droplet is sufficient, so that the flow rate is preferably 250 to 500 (L/min). Further, when the flow rate of the secondary gas is 250 (L/min) or less, the droplet refinement is insufficient, or the effect of imparting the speed of the droplet filling is reduced, resulting in deterioration of the quality of the spray coating. On the other hand, when the flow rate of the secondary gas exceeds 500 (L/min), the droplets are too fine and the droplets are excessively cooled, resulting in deterioration of the quality of the spray coating. The tertiary gas, as described above, is formed into a high-temperature gas jet in order to form a high-temperature gas jet in the outer peripheral portion of the plasma flame generated by the primary gas, so that the volume ratio should be 20 to 50% of the flow rate of the primary gas. In addition, in order to suppress the disturbance of the plasma flame and the gas diffusion caused by the secondary gas injection, the volume ratio is preferably in the range of 5 to 10% of the flow rate of the secondary gas. Further, in order to effectively exert the effect of suppressing the disturbance of the plasma flame and the gas diffusion caused by the secondary gas injection, the flow rate of the tertiary gas is changed in conjunction with the increase or decrease of the flow rate of the secondary gas, so that the flow rate of the secondary gas When there are few, the flow rate of the tertiary gas is also small, and when the flow rate of the secondary gas is large, the flow rate of the tertiary gas is also large. Moreover, the flow rate of the tertiary gas is less than 20% of the flow rate of the primary gas, or the flow rate of the secondary gas is less than 5%, because the injection of the tertiary gas - the effect of suppressing the disturbance of the plasma flame and the gas diffusion is less, and it is not easy Get the effect of -11 - 201233449 liter spray film quality. On the other hand, when the flow rate of the tertiary gas exceeds 50% of the flow rate of the primary gas or exceeds 1% of the flow rate of the secondary gas, the plasma gas is formed on the inner side due to the injection of the stronger tertiary gas. When the heat is high and the gas is injected at a high temperature, the effect of suppressing the disturbance of the plasma flame and the gas diffusion cannot be sufficiently exerted, and it is difficult to obtain an effect of improving the quality of the sprayed film. The wire passage 50 is composed of a primary wire passage 5 1 a having a wire outlet 5 1 b formed in the vicinity of the nozzle opening 2 2 of the secondary gas nozzle 20; and specific to the primary wire passage 5 1 a The inclination angle Θ is supplied by the secondary wire passage 5 2 a of the wire W. The wire passage 50 is a primary wire passage 5 1 a and a secondary wire passage 5 2 a, and the wire W is bent to a range not exceeding the elastic limit. As shown in Fig. 3, the primary wire passage 51a has a slightly rectangular cross-sectional shape in which the plasma flame extends in a long direction, so that the primary wire guiding member 5 disposed outside the secondary gas nozzle 20 is provided. 1 is formed in a straight line. Similarly, the secondary wire passage 52a also has a slightly rectangular cross-sectional shape in which the plasma flame extends in a long direction, so as to guide the secondary wire disposed at a position away from the primary wire passage 51a. The member 52 is formed to penetrate in a straight line. The width a of the primary wire passage 51a in the longitudinal direction is set to a range of 10% or more and 95% or less of the diameter d of the wire W. Further, the width b of the primary wire passage 5 1 a in the short-side direction is set to be smaller than the diameter d of the wire W by 3% or more and less than 1 〇 %. Further, the diameter d of the wire W of the present embodiment is 1.6 mm'

S -12- 201233449 ' 長邊方向之寬度a設定成比金屬絲W之直徑d大0.2〜 1 . 5mm程度的大小,短邊方向之寬度b則設定成比金屬絲 W之直徑d大0 . 〇 5〜0 · 1 5 mm程度的大小。二次金屬絲通 路52a方面,也是相同的設定。 並且,一次金屬絲通路5 1 a及二次金屬絲通路5 2 a所 具有之大致呈長方形的剖面形狀,除了長方形剖面形狀以 外,也包含在長方形剖面形狀之角部不接觸金屬絲W之 外面的範圍實施C面倒角及R面倒角等之加工的形狀。 然而,本實施方式之金屬絲W,一次金屬絲通路5 1 a及二 次金屬絲通路52a內之長邊方向之平面或短邊方向之平面 的任一平面,只承受到垂直方向之力。 而且,二次金屬絲通路52a之相對於一次金屬絲通路 5 1 a之傾斜角Θ,係一次金屬絲通路5 1 a之中心線及二次 金屬絲通路52a之中心線所夾之角。本實施方式時,傾斜 角Θ設定在1〜5°程度。並且,二次金屬絲導引構件52, 係配設於與一次金屬絲通路5 1 a及二次金屬絲通路52a隔 著間隙c之位置。本實施方式時,間隙c設定成3〜1 0mm 程度。 如上所示之本實施方式之電漿噴塗火矩2時,與一次 金屬絲通路5 1 a及二次金屬絲通路52a係隔著間隙c來進 行配置,而分別依直線狀之一次金屬絲通路5 1 a及二次金 屬絲通路52a形成爲擬似大曲線狀的金屬絲通路50,對 . 金屬絲W賦予不超過彈性範圍之範圍的彎曲。並且,一 次金屬絲通路5 1 a及二次金屬絲通路52a ’也可以分別爲 -13- 201233449 曲線狀》 電源4之陽極側,係連結於一次金屬絲導引構件5 1 ,並且,間接連結於通過該一次金屬絲導引構件5 1之一 次金屬絲通路5 1 a內的金屬絲W。另一方面,電源4之陰 極側,則連結於陰極40。並且,電源4之陽極側,有時 也直接連結於金屬絲W。 上述構成之電漿噴塗裝置1,被捲繞於金屬絲捲軸5 之金屬絲W由金屬絲供應機構7對電漿噴塗火矩2送出 時,由金屬絲矯正機6進行金屬絲W之強捲曲習性的矯 正,使其伸展成緩和之曲線狀。並且,金屬絲W介由金 屬絲步進管8被供應給金屬絲通路5 0。在金屬絲通路5 0 ,金屬絲W,只有在一次金屬絲通路5 1 a及二次金屬絲通 路52a內之長邊方向之平面或短邊方向之平面的其中平面 承受到垂直方向之力,如第4圖所示,賦予朝電漿火焰F 之伸長方向之不超過彈性限度之範圍的彎曲。 此處,一次金屬絲通路51a及二次金屬絲通路52a, 因爲具有於電漿火焰F之伸展方向較長之大致呈長方形的 剖面形狀,捲曲習性朝電漿火焰F之伸展方向舒展。尤其 是,本實施方式時,短邊方向之寬度b,因爲設定成比金 屬絲W之直徑d大3%以上且未達10%之範圍的大小, 故不會朝相對於電漿火焰F之伸展方向的直角方向舒展。 所以,金屬絲W之前端部分,相對於電漿火焰F之伸展 方向,即使發生若干位置偏移,也可防止其朝相對於電獎 火焰F之伸長方向的直角方向偏移,而位於電漿火焰FtS -12- 201233449 'The width a of the longitudinal direction is set to be larger than the diameter d of the wire W by 0.2 to 1. The width of the short side direction is set to be larger than the diameter d of the wire W by 0 to 5 mm. 〇5~0 · 1 5 mm size. The same is true for the secondary wire passage 52a. Further, the primary wire passage 5 1 a and the secondary wire passage 5 2 a have a substantially rectangular cross-sectional shape, and the rectangular cross-sectional shape is not included in the corner portion of the rectangular cross-sectional shape and does not contact the outer surface of the wire W. The range of processing such as C-face chamfering and R-face chamfering is performed in the range. However, in the wire W of the present embodiment, any plane in the plane of the longitudinal direction or the plane of the short side direction in the primary wire passage 5 1 a and the secondary wire passage 52a receives only the force in the vertical direction. Further, the inclination angle Θ of the secondary wire passage 52a with respect to the primary wire passage 5 1 a is the angle between the center line of the primary wire passage 5 1 a and the center line of the secondary wire passage 52a. In the present embodiment, the tilt angle Θ is set to about 1 to 5 degrees. Further, the secondary wire guiding member 52 is disposed at a position spaced apart from the primary wire passage 51a and the secondary wire passage 52a by a gap c therebetween. In the present embodiment, the gap c is set to about 3 to 10 mm. When the plasma spray flame 2 of the present embodiment as described above is disposed, the primary wire passage 5 1 a and the secondary wire passage 52 a are disposed with a gap c interposed therebetween, and the primary wire passages are linearly arranged. The 5 1 a and secondary wire passages 52 a are formed into a wire passage 50 which is shaped like a large curve, and the wire W is given a bending which does not exceed the range of the elastic range. Further, the primary wire passage 5 1 a and the secondary wire passage 52a ' may be the anode side of the power supply 4 of the curve -13 - 201233449, respectively, and are connected to the primary wire guiding member 5 1 and indirectly connected. The wire W passing through the primary wire passage 5 1 a of the primary wire guiding member 51 is passed. On the other hand, the cathode side of the power source 4 is connected to the cathode 40. Further, the anode side of the power source 4 may be directly connected to the wire W. In the plasma spraying apparatus 1 of the above configuration, when the wire W wound around the wire reel 5 is fed by the wire supplying mechanism 7 to the plasma spraying torch 2, the wire straightening machine 6 performs strong crimping of the wire W. The correction of habits causes it to stretch into a gentle curve. Further, the wire W is supplied to the wire passage 50 via the metal wire stepping tube 8. In the wire passage 50 and the wire W, only the plane in the longitudinal direction of the primary wire passage 5 1 a and the secondary wire passage 52a or the plane in the short side direction receives the force in the vertical direction. As shown in Fig. 4, the bending in the range in which the direction of elongation of the plasma flame F does not exceed the elastic limit is given. Here, the primary wire passage 51a and the secondary wire passage 52a have a substantially rectangular cross-sectional shape in which the direction in which the plasma flame F extends is long, and the curling behavior is stretched toward the extending direction of the plasma flame F. In particular, in the present embodiment, the width b in the short-side direction is set to be larger than the diameter d of the wire W by 3% or more and less than 10%, so that it does not face the plasma flame F. Stretch in the direction of the right angle of the stretch. Therefore, the front end portion of the wire W, relative to the direction in which the plasma flame F is stretched, can be prevented from being displaced in a direction perpendicular to the direction of elongation of the electric prize flame F even when a certain positional shift occurs, and is located in the plasma. Flame Ft

S -14 - 201233449 軸線上。 第5圖,係金屬絲通路之剖面形狀及金屬絲所受取之 力的方向。第5圖中,大致長方形剖面A,係長方形剖面 形狀,大致長方形剖面B,對長方形剖面形狀之角部在未 接觸金屬絲W之外面的範圍實施C面倒角加工的形狀, 大致長方形剖面C,係對長方形剖面形狀之角部在未接觸 金屬絲W之外面的範圍實施R面倒角加工的形狀。該大 致呈長方形之剖面形狀時,金屬絲W不論是接觸到長邊 方向之平面或接觸到短邊方向之平面,都只承受到相對於 各平面之垂直方向的力。 金屬絲W,因爲無法由金屬絲矯正機構7完全矯正成 直線狀,而有捲曲習性殘留。並且,金屬絲步進管8,因 爲作業時之電漿噴塗火矩2的處理,產生各種狀態之彎曲 形狀的變化,而無法有一定之形狀。是以,形狀不一定之 殘留著捲曲習性的金屬絲W在金屬絲步進管8內被傳送 的話,配合金屬絲步進管8之形狀的彎曲及扭轉力作用於 金屬絲W。藉由該彎曲及扭轉之力,金屬絲W在彈性限 度內與彈簧同樣地自由彎曲,而以力之方向呈現安定的位 置,在金屬絲步進管8內蛇行而被傳送。 此時,在上述之大致呈長方形之剖面形狀,金屬絲W 接觸到短邊方向之平面時,承受到相對於該短邊方向之平 面的垂直方向,亦即,電漿火焰F之伸展方向(以下,稱 爲「'X方向」)之力,捲曲習性朝電漿火焰F之伸展方向 舒展。並且,只接觸到該短邊方向之平面而承受到相對於 -15- 201233449 電漿火焰F之伸展方向的直角方向(以下,稱爲rY方向 」)之力時,金屬絲W,在短邊方向之寬度b的間隙份內 自由移動,雖然接觸到長邊方向之平面,此時,因爲相對 於長邊方向之平面的垂直方向(Y方向)之力的作用,而 使金屬絲W之位置處於安定。尤其是,承受到扭轉之力 時,X方向及Y方向之力分散成短邊方向及長邊方向之力 ,力以垂直方向作用於各面,產生抑制金屬絲W之扭轉 的作用,故金屬絲W之位置處於安定。 另一方面,圓形剖面及橢圓剖面時,金屬絲W接觸 圓形剖面及橢圓剖面之曲面的話,只會承受到相對於該曲 面之垂直方向的力,金屬絲w可沿著曲面自由地移動。 尤其是,承受到扭轉之力時,因爲金屬絲W沿著曲面自 由旋轉,而不抑制金屬絲W之扭轉。所以,金屬絲W所 承受之力的方向不一定,故金屬絲w之位置處於不安定 〇 是以,本實施方式之電漿噴塗裝置1時,金屬絲 W 之前端部分,可以對電漿火焰F之中心部安定地供應金屬 絲W。並且,一次氣體通路1 1所噴出之一次氣體识,被 介由一次金屬絲導引構件5 1間接地連結於電源4之陽極 側的金屬絲W、及連結於電源4之陰極側之陰極40之間 所產生電弧電漿化而成爲電漿火焰F’並以熔滴D來噴射 金屬絲W。該熔滴D,因爲從二次氣體通路21被朝二次 氣體噴嘴20之前方噴射之二次氣體而更微細化,並更加 速地噴射於被處理物T上,而形成噴塗皮膜S。S -14 - 201233449 on the axis. Figure 5 is the cross-sectional shape of the wire passage and the direction of the force the wire is subjected to. In Fig. 5, the substantially rectangular cross section A has a rectangular cross-sectional shape, a substantially rectangular cross-section B, and a C-side chamfered shape in a corner portion of the rectangular cross-sectional shape that does not contact the outer surface of the wire W, and has a substantially rectangular cross-section C. The shape of the corner portion of the rectangular cross-sectional shape is subjected to R-face chamfering in a range where the outer surface of the wire W is not in contact with the surface. In the case of the substantially rectangular cross-sectional shape, the wire W receives only the force in the vertical direction with respect to each plane regardless of whether it is in contact with the plane of the long side direction or the plane of the short side direction. The wire W cannot be completely corrected in a straight line by the wire correcting mechanism 7, and has a curling habit. Further, the wire stepping tube 8 does not have a constant shape due to the treatment of the plasma spray flame 2 during the operation, resulting in a change in the shape of the bend in various states. Therefore, if the wire W having a curling property which does not necessarily have a shape is conveyed in the wire stepping tube 8, the bending and torsion force in accordance with the shape of the wire stepping tube 8 acts on the wire W. By the bending and torsion forces, the wire W is freely bent in the same manner as the spring within the elastic limit, and is in a stable position in the direction of the force, and is snaked in the wire stepping tube 8 to be conveyed. At this time, in the substantially rectangular cross-sectional shape described above, when the wire W contacts the plane in the short-side direction, it receives the vertical direction with respect to the plane of the short-side direction, that is, the direction in which the plasma flame F is stretched ( Hereinafter, the force called "'X direction"), the curling habit stretches toward the stretching direction of the plasma flame F. Further, when only the plane in the short-side direction is received and the force in the direction perpendicular to the direction of extension of the plasma flame F of -15-201233449 (hereinafter referred to as rY direction) is received, the wire W is on the short side. The gap portion of the width b of the direction is freely moved, and although it is in contact with the plane in the longitudinal direction, at this time, the position of the wire W is caused by the force in the vertical direction (Y direction) with respect to the plane of the longitudinal direction. In stability. In particular, when the force of the torsion is applied, the forces in the X direction and the Y direction are dispersed into the forces in the short side direction and the long side direction, and the force acts on the respective surfaces in the vertical direction, thereby suppressing the twist of the wire W, so the metal The position of the wire W is stable. On the other hand, in the case of a circular cross section and an elliptical cross section, when the wire W contacts the curved surface of the circular cross section and the elliptical cross section, only the force in the vertical direction with respect to the curved surface is received, and the wire w can freely move along the curved surface. . In particular, when the force of the twist is applied, the wire W is freely rotated along the curved surface without suppressing the twist of the wire W. Therefore, the direction of the force of the wire W is not necessarily the same, so the position of the wire w is unstable. Therefore, in the plasma spraying device 1 of the present embodiment, the front end portion of the wire W can be used for the plasma flame. The center of the F is supplied with the wire W in a stable manner. Further, the primary gas generated by the primary gas passage 11 is indirectly connected to the anode W side of the power source 4 via the primary wire guiding member 51, and the cathode 40 connected to the cathode side of the power source 4. The arc generated between them is plasmated to become a plasma flame F' and the wire W is sprayed by the droplet D. The droplet D is made finer by the secondary gas injected from the secondary gas passage 21 toward the front of the secondary gas nozzle 20, and is more rapidly ejected onto the workpiece T to form the spray coating S.

S -16- 201233449 此時’在本實施方式之電漿噴塗裝置1,在從配置於 一次氣體通路11及二次氣體通路21之間的三次氣體通路 31所噴射之三次氣體流的內側,形成受取電漿火焰F之 熱而成爲高溫之氣體噴射G。藉由該高溫之氣體噴射G, 可以抑制於其外側所噴射之二次氣體之急速混入而於電漿 火焰F之外周部所發生的擾動,而防止電漿火焰F之氣體 擴散,減低成爲溶滴D之粒子之表面的氧化。藉此,可 以形成被處理物T上氧化較少之噴塗皮膜S。 此外,是以,在本實施方式之電漿噴塗裝置1,因爲 利用三次氣體於電漿火焰F之外周部形成受取電漿火焰F 之熱而成爲高溫之氣體噴射,來防止二次氣體之急速混入 所導致之電漿火焰F的擾動,即使一次氣體使用壓縮空氣 時,也可形成氧化較少之噴塗皮膜S。 並且,三次氣體使用惰性氣體之氮氣體及氬氣體等時 ,如上面所述,不但可以防止二次氣體之急速混入所導致 之電漿火焰F之外周部所發生的擾動,而且,於電漿火焰 F之外周部形成受取電漿火焰F之熱而成爲高溫之惰性氣 體噴射。藉此,熔滴D之粒子,在防止粒子之成分變化 的狀態下,被高溫之惰性氣體噴射微細化,並被加速,故 可避免二次氣體所導致的氧化。藉此,可以形成氧化較少 之噴塗皮膜72。 並且,本實施方式時,使一次金屬絲通路51a及二次 金屬絲通路52a之雙方具有電漿火焰之伸展方向較長之大 致呈長方形之剖面形狀,然而,也可以爲只有其中一方具 -17- 201233449 有電漿火焰之伸展方向較長之大致呈長方形之剖面形狀。 此時,利用具有電漿火焰之伸展方向較長之大致呈長方形 之剖面形狀的一次金屬絲通路或二次金屬絲通路,使金屬 絲W之捲曲習性朝電漿火焰F之伸展方向舒展,可將金 屬絲W之前端部分供應給電漿火焰F之中心部。 [實施例] 在三次氣體使用壓縮空氣及惰性氣體之氮氣體、及不 使用三次氣體時,實施比較試驗。在本實施例,噴塗材料 係使用鋁系合金,測定噴塗皮膜之自然電位作爲噴塗皮膜 之氧化程度的指標,來確認三次氣體之效果。並且,在運 轉成本之降低手法上,一次氣體、二次氣體、及三次氣體 之全部氣體皆使用便宜之壓縮空氣來製作噴塗皮膜,測定 噴塗皮膜之自然電位,來確認3次氣體之效果。第6圖, 係自然電位測定方法的說明圖。 第6圖所示之自然電位之測定,係利用飽和KC1之鹽 橋於試驗片(試驗TP)之噴塗皮膜表面創造5w%NaCl之 環境,比對電極使用飽和氯化銀電極,以檢驗機測定自然 電位。並且,爲了使電位之測定數値呈現安定,以測定開 始之600秒後的電位作爲測定値。試驗結果,彙整如表1 所示,表1之各條件之皮膜的自然電位測定結果如表2所 示。S -16-201233449 At this time, the plasma spraying apparatus 1 of the present embodiment is formed inside the three-phase gas flow injected from the tertiary gas passage 31 disposed between the primary gas passage 11 and the secondary gas passage 21. The gas jet G is heated to a high temperature by the heat of the plasma flame F. By the high-temperature gas injection G, it is possible to suppress the disturbance of the secondary gas injected on the outer side and the disturbance occurring in the outer portion of the plasma flame F, thereby preventing the gas diffusion of the plasma flame F and reducing the dissolution. Oxidation of the surface of the particles of D. Thereby, the spray coating film S having less oxidation on the workpiece T can be formed. Further, in the plasma spraying apparatus 1 of the present embodiment, since the heat of the plasma flame F is formed in the peripheral portion of the plasma flame F by the tertiary gas to be a high-temperature gas injection, the rapidity of the secondary gas is prevented. The disturbance of the plasma flame F caused by the mixing is formed, and even if the primary gas uses compressed air, the sprayed film S having less oxidation can be formed. Further, when the nitrogen gas of the inert gas and the argon gas are used for the tertiary gas, as described above, not only the disturbance occurring in the peripheral portion of the plasma flame F caused by the rapid mixing of the secondary gas but also the plasma can be prevented. The outer peripheral portion of the flame F forms an inert gas jet which is subjected to the heat of the plasma flame F to become a high temperature. As a result, the particles of the droplet D are prevented from being oxidized by the secondary gas in a state where the particles of the droplets are prevented from being changed by the high-temperature inert gas. Thereby, the spray coating 72 having less oxidation can be formed. Further, in the present embodiment, both of the primary wire passage 51a and the secondary wire passage 52a have a substantially rectangular cross-sectional shape in which the direction in which the plasma flame extends is long. However, only one of them may have -17 - 201233449 There is a roughly rectangular cross-sectional shape in which the plasma flame extends in a long direction. At this time, the primary wire passage or the secondary wire passage having a substantially rectangular cross-sectional shape in which the plasma flame extends in a long direction is used to stretch the curling habit of the wire W toward the stretching direction of the plasma flame F. The front end portion of the wire W is supplied to the center portion of the plasma flame F. [Examples] A comparative test was carried out when a nitrogen gas of compressed air and an inert gas was used for three times of gas, and when three gases were not used. In the present embodiment, an aluminum-based alloy was used as the coating material, and the natural potential of the sprayed coating was measured as an index of the degree of oxidation of the sprayed coating to confirm the effect of the tertiary gas. Further, in the method of reducing the operating cost, all of the primary gas, the secondary gas, and the tertiary gas are sprayed with inexpensive compressed air, and the natural potential of the sprayed coating is measured to confirm the effect of the third gas. Fig. 6 is an explanatory diagram of a method for measuring a natural potential. The measurement of the natural potential shown in Fig. 6 is carried out by using a salt bridge of saturated KC1 to create a 5w% NaCl environment on the surface of the sprayed film of the test piece (test TP), and using a saturated silver chloride electrode for the comparison electrode. Natural potential. Further, in order to stabilize the measured number of potentials, the potential after 600 seconds from the start was measured as the measurement enthalpy. The test results are summarized as shown in Table 1. The results of the measurement of the natural potential of the film of each condition of Table 1 are shown in Table 2.

S -18 - 201233449 [表i] 三次氣體之條件 皮膜之電位 三次氣體使用氮氣體時 -1150(-1196 〜-1106)mV 三次氣體使用壓縮空氣時 -1063(-1080 〜-1032)mV 一次、二次、三次氣體皆使用壓縮空氣時 -1052(-1069 〜-1020)mV 傳統之未利用三次氣體時 -997(-1019 〜-980)mV 具代表性之噴塗條件 一次氣體流量:氮氣體=70(1/分) 二次氣體流量:壓縮空氣=400(1/分) 三次氣體流量:壓縮空氣及氮氣體=30(1/分) 皮膜厚度:1〇〇(±20)μιη 發生電壓:130(±5)(V) 發生電流:60(±1)(A) 噴塗用金屬絲之材質:5%鎂、95%鋁合金材(質量比) -19- 201233449 [表2] 表2 各條件之皮膜的自然電位測定結果 次 體 種 類 一次 氣體 流量 ΐ k, 體 種 類 二次 氣體 流量 1 M. 體 種 類 三次 氣體 侖量 皮膜 之 電位 皮膜 之 平均 電位 備註 1-1 氮 70 空 氣 400 氮 30 -1194 -1150 氮之二次氣體 的遮蔽效果 120 500 25 -1142 70 400 20 -1196 下限 70 400 35 -1106 上限 100 250 22 -1114 1-2 氮 100 空 氣 500 氮 20 -1005 範圍 外 二次之未達5% 70 400 40 -921 /jcjcrsi 範圍 外 超過一次之50% 50 250 35 -894 範圍 外 超過上限値 2-1 氮 70 空 氣 400 空 氣 30 -1080 -1063 空氣之三次氣體 的混入效果 120 500 40 -1074 70 400 20 -1065 下限 70 400 35 -1032 上限 100 250 22 -1062 2-2 氮 100 空 氣 500 空 氣 20 -924 範圍 外 二次之未達5% 70 400 40 -876 範圍 外 超過一次之50% 50 250 35 -894 範圍 外 超過上限値 3 空 氣 70 空 氣 400 空 氣 30 -1069 -1052 3氣體全部爲空氣 時,三次氣體之 混入效果 120 500 40 -1063 70 400 20 -1052 下限 70 400 35 -1055 上限 100 250 22 -1020 4 氮 70 空 氣 400 Ant. 挑 0 -984 -997 傳統之無二次氣體 120 500 0 -997 100 400 0 -1019 70 500 0 -1005 100 250 0 -980 -20- 201233449 .如表1所示,未使用三次氣體時及使用壓縮空氣作爲 三次氣體時,使用壓縮空氣作爲三次氣體,呈現約60mV 之低電位。此外,使用惰性氣體之氮氣體作爲三次氣體時 ,呈現約150mV之低値。並且,全部氣體使用便宜之壓 縮空氣時,呈現約5 OmV之低値。由此可確認到,利用三 次氣體,可以減少噴塗皮膜內部之氧化6 本發明之電漿噴塗裝置,對於以在鋼構造物之表面形 成防鏽用噴塗皮膜爲目的之裝置係有用的。 【圖式簡單說明】 第1圖係本發明之實施方式之電漿噴塗裝置的槪略構 成圖。 第2圖係第1圖之電漿噴塗火矩之主要部位的詳細縱 剖面圖。 第3圖係第2圖之A箭頭方向圖》 第4圖係第1圖之電漿噴塗火矩的動作說明圖。 第5圖係金屬絲通路之剖面形狀及金屬絲所受取之力 的方向說明圖。 第6圖係自然電位測定方法的說明圖。 第7圖係傳統電漿噴塗裝置的槪念剖面圖。 【主要元件符號說明】 1 :電漿噴塗裝置 2 :電漿噴塗火矩 -21 - 201233449 3 :氣體供應源 4 :電源 5 :金屬絲捲軸 6 :金屬絲矯正機 7 =金屬絲供應機構 1 〇 :—次氣體噴嘴 11: 一次氣體通路 1 2 :噴嘴口 20 :二次氣體噴嘴 21 :二次氣體通路 22 :噴嘴口 30 :三次氣體噴嘴 31 :三次氣體通路 40 :陰極 5 0 :金屬絲通路 5 1 : —次金屬絲導.引構件 5 1 a —次金屬絲通路 52 :二次金屬絲導引構件 5 2 a :二次金屬絲通路S -18 - 201233449 [Table i] The potential of the film of the three gas conditions is three times when the gas is used for nitrogen gas -1150 (-1196 ~1106) mV. When the compressed gas is used for three times, the gas is -1063 (-1080 ~-1032) mV, When the compressed air is used for the secondary and tertiary gases -1052 (-1069 ~ -1020) mV. The traditional three-gas is not used -997 (-1019 ~-980) mV. Typical spraying conditions. Primary gas flow: nitrogen gas = 70 (1/min) Secondary gas flow: compressed air = 400 (1/min) Three gas flow: compressed air and nitrogen gas = 30 (1/min) Film thickness: 1 〇〇 (±20) μιη Voltage generation: 130(±5)(V) Current generation: 60(±1)(A) Material of spray wire: 5% magnesium, 95% aluminum alloy (mass ratio) -19- 201233449 [Table 2] Table 2 The natural potential measurement result of the film of the condition is the primary gas flow rate ΐ k, the volume of the secondary gas flow of the body type 1 M. The average potential of the potential film of the three-dimensional gas tensor film of the body type Remarks 1-1 Nitrogen 70 Air 400 Nitrogen 30 - 1194 -1150 The shielding effect of nitrogen secondary gas 120 500 25 -1142 70 400 20 -1196 70 400 35 -1106 Upper limit 100 250 22 -1114 1-2 Nitrogen 100 Air 500 Nitrogen 20 -1005 Out of range less than 5% 70 400 40 -921 /jcjcrsi More than 50% outside the range 50 250 35 -894 Outside the range exceeds the upper limit 値 2-1 Nitrogen 70 Air 400 Air 30 -1080 -1063 Mixing effect of three gases of air 120 500 40 -1074 70 400 20 -1065 Lower limit 70 400 35 -1032 Upper limit 100 250 22 -1062 2-2 Nitrogen 100 Air 500 Air 20 -924 Out of range less than 5% 70 400 40 -876 Out of range 50% 50 250 35 -894 Out of range exceeds upper limit 値3 Air 70 Air 400 Air 30 -1069 -1052 3 When all the gases are air, the mixing effect of the three gases is 120 500 40 -1063 70 400 20 -1052 Lower limit 70 400 35 -1055 Upper limit 100 250 22 -1020 4 Nitrogen 70 Air 400 Ant. Pick 0 -984 -997 Secondary gas 120 500 0 -997 100 400 0 -1019 70 500 0 -1005 100 250 0 -980 -20- 201233449 . As shown in Table 1, when three gases are not used and compressed air is used as the tertiary gas, compression is used. air For the three gases, presenting a low potential of about 60mV. Further, when a nitrogen gas of an inert gas was used as the tertiary gas, a low enthalpy of about 150 mV was exhibited. Also, when all of the gas uses a cheap compressed air, it exhibits a low enthalpy of about 5 OmV. As a result, it has been confirmed that the plasma spraying apparatus of the present invention can be reduced by the use of the tertiary gas. 6 The plasma spraying apparatus of the present invention is useful for forming a coating film for preventing rust on the surface of a steel structure. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic view showing the structure of a plasma spraying apparatus according to an embodiment of the present invention. Fig. 2 is a detailed longitudinal sectional view showing the main part of the plasma spray flame of Fig. 1. Fig. 3 is a diagram showing the direction of the arrow A of Fig. 2, and Fig. 4 is an explanatory diagram of the operation of the plasma spraying torch of Fig. 1. Fig. 5 is a cross-sectional view of the cross-sectional shape of the wire passage and the direction of the force to which the wire is taken. Fig. 6 is an explanatory diagram of a method for measuring a natural potential. Figure 7 is a cross-sectional view of a conventional plasma spraying device. [Main component symbol description] 1 : Plasma spraying device 2 : Plasma spraying fire moment - 21 - 201233449 3 : Gas supply source 4 : Power supply 5 : Wire reel 6 : Wire straightening machine 7 = Wire supply mechanism 1 〇 : - Secondary gas nozzle 11 : Primary gas passage 1 2 : Nozzle opening 20 : Secondary gas nozzle 21 : Secondary gas passage 22 : Nozzle opening 30 : Third gas nozzle 31 : Third gas passage 40 : Cathode 5 0 : Wire passage 5 1 : - secondary wire guide. lead member 5 1 a - secondary wire passage 52 : secondary wire guiding member 5 2 a : secondary wire passage

S -22-S -22-

Claims (1)

201233449 七、申請專利範圍: 1. 一種電漿噴塗裝置,其係具備:陰極;於該陰極 之外周形成一次氣體通路並覆蓋前述陰極之前端部的一次 氣體噴嘴;配置於該一次氣體噴嘴之外側並形成二次氣體 通路之二次氣體噴嘴;以及對該二次氣體噴嘴之噴嘴口附 近供應噴塗用金屬絲之金屬絲通路;且,藉由在前述金屬 絲通路所供應之前述金屬絲的前端與前述陰極之間所發生 之電弧,使由前述一次氣體噴嘴所噴射之一次氣體電漿化 ,而形成由前述一次氣體噴嘴所噴射之電漿火焰’使前述 金屬絲之前端成爲熔滴,藉由前述電漿火焰及前述二次氣 體噴嘴所噴射之二次氣體,將該熔滴噴射於被處理物上之 電漿噴塗裝置,其特徵爲: 在前述一次氣體噴嘴與前述二次氣體噴嘴之間’具備 於前述電漿火焰之外周部形成有可承受前述電漿火焰之熱 並噴射高溫氣體噴射用的三次氣體之三次氣體通路的三次 氣體噴嘴。 2. 如申請專利範圍第1項記載之電漿噴塗裝置,其 中 前述三次氣體之流量,其體積比係前述一次氣體之流 量的20〜50%且爲前述二次氣體之流量的5〜10%。 3. 如申請專利範圍第1項記載之電漿噴塗裝置,其 中 前述三次氣體,係壓縮空氣或碳酸氣體。 - 4.如申請專利範圍第2項記載之電漿噴塗裝置,其 -23- 201233449 中 前述三次氣體,係壓縮空氣或碳酸氣體。 5. 如申請專利範圍第1項記.載之電漿噴塗裝置,其 中 前述三次氣體,係惰性氣體。 6. 如申請專利範圍第2項記載之電漿噴塗裝置,其 中 前述三次氣體,係惰性氣體。 7. 如申請專利範圍第至6項之任一項記載之電漿 噴塗裝置,其中 前述一次氣體,係壓縮空氣。 S -24-201233449 VII. Patent application scope: 1. A plasma spraying device, comprising: a cathode; forming a gas passage outside the cathode and covering a primary gas nozzle at a front end of the cathode; and being disposed outside the primary gas nozzle And forming a secondary gas nozzle of the secondary gas passage; and a wire passage for supplying the coating wire to the vicinity of the nozzle opening of the secondary gas nozzle; and the front end of the wire supplied by the wire passage And an arc generated between the cathode and the cathode, wherein the primary gas injected by the primary gas nozzle is plasma-formed to form a plasma flame injected by the primary gas nozzle to make the front end of the wire become a droplet. a plasma spraying device for spraying the droplet onto the object to be treated by the plasma flame and the secondary gas injected from the secondary gas nozzle, wherein: the primary gas nozzle and the secondary gas nozzle Between the outer portion of the plasma flame is formed with a heat that can withstand the plasma flame and sprays a high-temperature gas spray Three gas nozzles for three gas passages of three gases. 2. The plasma spraying device according to claim 1, wherein the volume of the tertiary gas is 20 to 50% of the flow rate of the primary gas and 5 to 10% of the flow rate of the secondary gas. . 3. The plasma spraying apparatus according to claim 1, wherein the third gas is compressed air or carbonic acid gas. - 4. The plasma spraying device of claim 2, wherein the third gas in -23-201233449 is compressed air or carbonic acid gas. 5. The plasma spraying apparatus of claim 1, wherein the third gas is an inert gas. 6. The plasma spraying apparatus according to claim 2, wherein the third gas is an inert gas. 7. The plasma spraying apparatus according to any one of the preceding claims, wherein the primary gas is compressed air. S -24-
TW100145036A 2010-12-10 2011-12-07 Plasma spraying device TWI650182B (en)

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