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JP3280994B2 - Atmospheric pressure glow plasma reaction method in tube - Google Patents
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JP3280994B2 - Atmospheric pressure glow plasma reaction method in tube - Google Patents

Atmospheric pressure glow plasma reaction method in tube

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Publication number
JP3280994B2
JP3280994B2 JP40946090A JP40946090A JP3280994B2 JP 3280994 B2 JP3280994 B2 JP 3280994B2 JP 40946090 A JP40946090 A JP 40946090A JP 40946090 A JP40946090 A JP 40946090A JP 3280994 B2 JP3280994 B2 JP 3280994B2
Authority
JP
Japan
Prior art keywords
tube
atmospheric pressure
discharge
insulator
gas
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 - Fee Related
Application number
JP40946090A
Other languages
Japanese (ja)
Other versions
JPH05202481A (en
Inventor
益弘 小駒
幸子 岡崎
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Japan Science and Technology Agency
Original Assignee
Japan Science and Technology Corp
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Filing date
Publication date
Application filed by Japan Science and Technology Corp filed Critical Japan Science and Technology Corp
Priority to JP40946090A priority Critical patent/JP3280994B2/en
Publication of JPH05202481A publication Critical patent/JPH05202481A/en
Application granted granted Critical
Publication of JP3280994B2 publication Critical patent/JP3280994B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Chemical Vapour Deposition (AREA)
  • Drying Of Semiconductors (AREA)
  • Plasma Technology (AREA)

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】この発明は、管内大気圧グロープ
ラズマ反応方法に関するものである。さらに詳しくは、
この発明は、円筒管等の絶縁体管の内面や内部の静止、
移動または流通物を大気圧下で処理あるいは反応させる
ことのできる管内大気圧グロープラズマ反応方法に関す
るものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an in-tube atmospheric pressure glow plasma reaction method. For more information,
The present invention relates to stationary inner and inner surfaces of an insulator tube such as a cylindrical tube,
The present invention relates to an in-tube atmospheric pressure glow plasma reaction method capable of treating or reacting a moving or flowing material under atmospheric pressure.

【0002】[0002]

【従来の技術とその課題】従来より、プラスチック、ガ
ラス、セラミックス等の絶縁体管の内面への膜付け、ま
たは親水・疎水化等の表面処理は、薬品処理あるいは低
圧プラズマ処理により行われてきている。しかしなが
ら、従来法による表面処理においては、一般的に、危険
な薬品を使用してきており、またその処理も大変面倒で
あるという欠点があった。この中でも低圧プラズマ処理
は良好な表面処理を実現するという利点を有するもの
の、通常、数Torr以下の低圧下で行わなければならない
という問題がある。これは、管内の圧力を上昇させてい
くと100Torr 前後から放電が一点に集中し始め、大気圧
付近では火花放電に移行し、管内面または管内部に設置
された物体等への均一な処理が不可能となるからであ
る。このため、低圧プラズマ処理では、真空排気システ
ムを必要とし、これによって装置が大がかりなものとな
り、コストが高くなるという欠点がある。
2. Description of the Related Art Conventionally, film formation on an inner surface of an insulating tube made of plastic, glass, ceramics, or the like, or surface treatment such as hydrophilicity / hydrophobicity has been performed by chemical treatment or low-pressure plasma treatment. I have. However, the surface treatment by the conventional method has a drawback in that dangerous chemicals are generally used, and the treatment is very troublesome. Among them, the low-pressure plasma treatment has an advantage of realizing a good surface treatment, but usually has a problem that it must be performed under a low pressure of several Torr or less. This is because when the pressure inside the tube is increased, the discharge starts to concentrate at about 100 Torr, and at around atmospheric pressure, it shifts to spark discharge, and uniform treatment of the inside surface of the tube or the objects installed inside the tube is performed. It is impossible. For this reason, low-pressure plasma processing requires a vacuum evacuation system, which has the disadvantage of requiring a large-scale apparatus and increasing costs.

【0003】また、低圧プラズマ処理では、反応性ガス
等の気体を導入するために、長尺のプラスチック細管や
管壁に多数の小孔を形成したポーラス状細管を使用する
ため、このような細管の管路や管壁を透過してくる空気
により内圧が上昇し、充分な放電処理を行うことは実質
的に不可能でもあった。一方、この発明の発明者らは、
Heを主体とした希ガスを希釈ガスとして用い、反応性
ガスを大希釈し、全圧を大気圧近辺に保持して、拡散し
たグロー放電を発生させる大気圧プラズマ反応方法をす
でに提案してもいる。この方法では、大気圧下に拡散し
た安定なグロー放電を発生させることができるため、真
空排気システムを省略することができ、処理装置のコス
トを極めて低減させることを可能としている。
[0003] In the low-pressure plasma treatment, a long plastic thin tube or a porous thin tube having a large number of small holes formed in a tube wall is used to introduce a gas such as a reactive gas. The internal pressure rises due to the air passing through the pipe and the pipe wall, and it has been substantially impossible to perform a sufficient discharge treatment. On the other hand, the inventors of the present invention
Even if an atmospheric pressure plasma reaction method for generating a diffused glow discharge by using a rare gas mainly composed of He as a diluent gas, greatly diluting a reactive gas, and maintaining the total pressure near the atmospheric pressure has already been proposed. I have. In this method, since a stable glow discharge diffused under the atmospheric pressure can be generated, the evacuation system can be omitted, and the cost of the processing apparatus can be extremely reduced.

【0004】しかしながら、この大気圧プラズマ反応方
法においては、放電電極を平行平板電極としているた
め、平らな面を有する試料への処理が主体となってお
り、円筒管等の絶縁体管内面の処理、また、管内部を流
通する気体の反応生成物を効果的に得るためには種々の
改良を必要としていた。ところで、従来の低圧プラズマ
処理におけるガラス等からなる円筒管に対する放電形式
としては、たとえば図7〜図9に示したような容量結合
型または誘導結合型が広く知られている。
However, in this atmospheric pressure plasma reaction method, since the discharge electrode is a parallel plate electrode, processing on a sample having a flat surface is mainly performed, and processing on the inner surface of an insulator tube such as a cylindrical tube is performed. In addition, various improvements have been required in order to effectively obtain a gaseous reaction product flowing through the inside of the tube. By the way, as a discharge type for a cylindrical tube made of glass or the like in the conventional low-pressure plasma processing, for example, a capacitive coupling type or an inductive coupling type as shown in FIGS. 7 to 9 is widely known.

【0005】図7に示した容量結合型の放電形式におい
ては、一対のリング状電極(ア)(イ)を円筒管(ウ)
の外周に対向配置している。図8に示した放電形式も容
量結合型であり、円筒管(ウ)の外周に曲板状電極
(エ)を配設している。また、図9に示した誘導結合型
の放電形式の場合には、コイル型電極(オ)を円筒管
(ウ)の外周部に配設している。
In the discharge type of capacitive coupling shown in FIG. 7, a pair of ring-shaped electrodes (a) and (b) are connected to a cylindrical tube (c).
Are arranged to face each other on the outer periphery. The discharge type shown in FIG. 8 is also a capacitive coupling type, in which a curved plate-shaped electrode (d) is arranged on the outer periphery of a cylindrical tube (c). In the case of the inductively coupled discharge type shown in FIG. 9, the coil-type electrode (e) is disposed on the outer periphery of the cylindrical tube (c).

【0006】これらの放電形式をこの発明者らが提案し
ている大気圧下でのプラズマ反応方法に応用することが
考えられもするが、しかしながらその応用は実質的には
不可能であるのが実情であった。すなわち、図7に示し
たリング状電極(ア)(イ)を用いた放電形式の場合に
は、たとえHeで希釈した混合ガス(カ)を用いても大
気圧下での放電は困難であり、しかも放電に広がりがな
く局所的となり、円筒管(ウ)内部での放電処理には不
適当である。
It is conceivable to apply these discharge types to the plasma reaction method under atmospheric pressure proposed by the present inventors, however, it is practically impossible to apply them. It was a fact. That is, in the case of the discharge type using the ring-shaped electrodes (A) and (A) shown in FIG. 7, it is difficult to discharge under atmospheric pressure even if a mixed gas (F) diluted with He is used. In addition, the discharge does not spread and becomes local, which is unsuitable for the discharge treatment inside the cylindrical tube (c).

【0007】一方、図8に示した曲板状の電極(エ)を
用いた放電形式の場合には、電極(エ)の軸方向の長さ
を変えることで管軸方向へ放電を拡散させることができ
るが、大気圧下He混合ガス(カ)中での放電可能な電
極間距離は高々20mmであり、直径が20mm以上の大口
径管の場合には放電を発生させることができない。しか
も径方向の放電密度にばらつきが多いという問題もあ
る。
On the other hand, in the case of a discharge type using a curved plate-like electrode (D) shown in FIG. 8, the discharge is diffused in the tube axis direction by changing the axial length of the electrode (D). However, the distance between electrodes capable of discharging in a He mixed gas (f) at atmospheric pressure is at most 20 mm, and a large-diameter tube having a diameter of 20 mm or more cannot generate discharge. In addition, there is also a problem that the discharge density in the radial direction varies widely.

【0008】また、図9に示したコイル型電極(オ)を
用いた放電形式の場合には、大気圧グロー放電の必要条
件であるパルス状放電とならないため、放電が本質的に
局部的となり、しかも高温アークになりやすく、低温プ
ラズマには不適当である。この発明は、以上の通りの事
情に鑑みてなされたものであり、従来の絶縁性管内部で
のプラズマ処理の欠点を解消し、円筒管等の絶縁体管の
内面や内部の静止、移動または流通物を大気圧下で処理
あるいは反応させることのできる、新しい管内大気圧グ
ロープラズマ反応方法を提供することを目的としてい
る。
Further, in the case of the discharge type using the coil-type electrode (E) shown in FIG. 9, since the pulse-like discharge which is a necessary condition of the atmospheric pressure glow discharge does not occur, the discharge becomes essentially local. In addition, a high-temperature arc easily occurs, which is not suitable for low-temperature plasma. The present invention has been made in view of the above circumstances, and solves the drawbacks of the conventional plasma treatment inside an insulating tube, and makes the inner surface or the inside of an insulating tube such as a cylindrical tube stationary, moving or moving. An object of the present invention is to provide a new in-pipe atmospheric pressure glow plasma reaction method capable of treating or reacting a flow product under atmospheric pressure.

【0009】[0009]

【課題を解決するための手段】この出願の発明は、上記
の課題を解決するものとして、第1には、外周部に一対
箔状の平行電極対をスパイラル状に張り付け周設され
ており、絶縁体管の一端部から反応性ガスと希ガスとの
混合ガスを導入し、大気圧下で絶縁体管内部にグロー放
電プラズマを発生させ、管内面、または管内部の静止
体、移動体あるいは流通物をグロープラズマ処理するこ
とを特徴とする管内大気圧グロープラズマ反応方法を提
供する。また、この出願の発明は、第2には、絶縁体管
の外周部に一対の箔状の平行電極対がスパイラル状に張
り付け周設されており、絶縁体管の一端部から反応性ガ
スと希ガスとの混合ガスを導入して大気圧下で絶縁体管
内部にグロー放電プラズマを発生させ、絶縁体管内部に
おいてグロープラズマ処理を可能としたことを特徴とす
る管内大気圧グロープラズマ反応用装置を提供する。
According to the invention of the present application, as a solution to the above-mentioned problem, first , a pair of foil-shaped parallel electrode pairs are spirally attached to an outer peripheral portion. , A mixed gas of a reactive gas and a rare gas is introduced from one end of the insulator tube, and a glow discharge plasma is generated inside the insulator tube at atmospheric pressure, and a stationary or moving body inside the tube or inside the tube. Alternatively, there is provided an in-tube atmospheric pressure glow plasma reaction method characterized by performing glow plasma treatment on a flowing material. In addition, the invention of this application secondly provides an insulator tube
A pair of foil-shaped parallel electrode pairs are spirally stretched around
Reactive gas is supplied from one end of the insulator tube.
Insulation tube under atmospheric pressure by introducing a mixed gas of
Glow discharge plasma is generated inside, and inside the insulator tube
In which glow plasma processing is possible.
And an apparatus for glow plasma reaction in a tube.

【0010】たとえば図1に示したように、この発明の
方法においては、円筒管等の絶縁体管(1)の外周部に
一対のスパイラル状の平行電極対を設け、一方を高圧電
極(2)とし、他方をアース電極(3)とする。絶縁体
管(1)の材質としては特に制限はなく、たとえばガラ
ス、ビニルチューブ等の汎用プラスチックの他、PTF
T,FEP,PET,PPS,PEEK,ABS,シリ
コンチューブ等の工業用汎用プラスチック材料、セラミ
ックス等の任意のものとすることができる。また、絶縁
体管(1)の太さについても格別の限定はなく、直径1
0cmを越える大口径管や0.1mm φ以下の極細管などの任
意のものとすることができる。その断面形状も図1に例
示した円形の他、多角形などとすることもできる。
For example, as shown in FIG. 1, in the method of the present invention, a pair of spiral parallel electrodes is provided on the outer peripheral portion of an insulating tube (1) such as a cylindrical tube, and one of the spiral parallel electrode pairs is provided. ) And the other is a ground electrode (3). The material of the insulator tube (1) is not particularly limited. For example, in addition to general-purpose plastics such as glass and vinyl tubes, PTF
T, FEP, PET, PPS, PEEK, ABS, general-purpose industrial plastic materials such as silicon tubes, ceramics, and any other materials. There is no particular limitation on the thickness of the insulator tube (1).
An arbitrary one such as a large-diameter tube exceeding 0 cm or an ultrafine tube having a diameter of 0.1 mm or less can be used. The cross-sectional shape may be a polygon other than the circle illustrated in FIG.

【0011】スパイラル状平行電極対(2)(3)とし
ては、たとえばこの図1に示したように、箔状の電極を
用い、これを絶縁体管(1)の外周面に張り付けること
ができる。電極対(2)(3)の材質としては、銅、
銀、ニッケル、アルミニウム、ステンレス、カーボン等
の種々の導電性材料を任意に用いることができる。この
ようなスパイラル状平行電極対(2)(3)の電極間距
離(1)としては、0.1mmからおよそ30mmまで
とすることができる。好ましくは5mmから20mmで
ある。また、図1に例示したような箔状の電極対の場合
には、その幅(m)を0.1mmから30mmまでとす
ることができ、絶縁体管(1)の直径に対応させること
ができる。さらに、外部沿面放電を防止するために、た
とえば図2に示したように、エポキシまたはシリコン接
着剤等の絶縁性接着剤(4)で外周面全面をカバーする
こともできる。
As the spiral parallel electrode pairs (2) and (3), for example, as shown in FIG. 1, a foil-like electrode is used, which is attached to the outer peripheral surface of the insulator tube (1). kill at. The material of the electrode pair (2) and (3) is copper,
Various conductive materials such as silver, nickel, aluminum, stainless steel, and carbon can be arbitrarily used. The distance (1) between the electrodes of such a spiral parallel electrode pair (2) (3) can be from 0.1 mm to about 30 mm. Preferably it is 5 mm to 20 mm. In the case of a foil-shaped electrode pair as exemplified in FIG. 1, the width (m) can be set to 0.1 mm to 30 mm, and can correspond to the diameter of the insulator tube (1). it can. Further, in order to prevent external creeping discharge, as shown in FIG. 2, for example, an insulating adhesive (4) such as an epoxy or silicone adhesive can be used to cover the entire outer peripheral surface.

【0012】このようなスパイラル状平行電極(2)
(3)に接続する電源(5)についても特に制限はな
く、数kHz の低周波から数10kHz あるいは13.56MHzま
での高周波とすることができる。また、絶縁性管(1)
の一端部から導入する混合ガス(6)の反応性ガスとし
ては、酸素、アンモニア等の無機モノマーやC2 4
3 6 等のフッ化エチレン系、CF4 ,C2 6 等の
フッ素パラフィン炭化水素、またはフッ素原子を含む側
鎖のついた鎖状炭化水素、あるいはフッ素化芳香族炭化
水素などの官能基を有する、もしくは有さない炭化水素
等の任意の有機モノマーを用いることができる。このよ
うな反応性ガスをHeを主体とする希釈ガスで大希釈
し、混合ガス(6)とする。グロー放電の安定化のため
にはHeの混合割合が大きいほど好ましいが、必要に応
じてAr,N2 等の不活性ガスを混入することもでき
る。たとえばHeに対するArの混合割合を90%程度
とすることができる。これにより、高価なHeの使用量
を低減させ、コストを安価とすることが可能となる。い
ずれの場合も混合ガス(6)の全圧は1気圧付近とす
る。
Such a spiral parallel electrode (2)
There is no particular limitation on the power supply (5) connected to (3), and a low frequency of several kHz to a high frequency of several tens of kHz or 13.56 MHz can be used. Insulating tube (1)
As a reactive gas of the mixed gas (6) introduced from one end of the gas, an inorganic monomer such as oxygen or ammonia, C 2 F 4 ,
Functionality such as fluorinated ethylenes such as C 3 F 6 , fluorinated paraffin hydrocarbons such as CF 4 and C 2 F 6 , or chain hydrocarbons with side chains containing fluorine atoms, or fluorinated aromatic hydrocarbons Any organic monomer, such as a hydrocarbon, with or without groups can be used. Such a reactive gas is greatly diluted with a diluent gas mainly composed of He to obtain a mixed gas (6). For stabilization of the glow discharge, it is preferable that the mixing ratio of He is large, but an inert gas such as Ar or N 2 can be mixed if necessary. For example, the mixing ratio of Ar to He can be about 90%. This makes it possible to reduce the amount of expensive He used and reduce the cost. In any case, the total pressure of the mixed gas (6) is set at around 1 atm.

【0013】一方、発生するグロー放電は、電極対
(2)(3)の対極となる電極が管軸方向および円周方
向に少しずつずれていくため、絶縁体管(1)の内面に
密着した形で、管軸方向に沿って広がり、放電密度も平
均化される。このように拡散するグロー放電プラズマに
より種々の表面処理や、薄膜形成、合成、分解等の任意
の化学反応を生起させることができ、その効率を著しく
向上させることができる。
On the other hand, the glow discharge generated is such that the electrodes, which are the counter electrodes of the electrode pairs (2) and (3), are slightly displaced in the tube axis direction and the circumferential direction, so that they adhere to the inner surface of the insulator tube (1). In this way, it spreads along the tube axis direction, and the discharge density is also averaged. Various chemical treatments such as various surface treatments, thin film formation, synthesis, and decomposition can be caused by the glow discharge plasma thus diffused, and the efficiency can be significantly improved.

【0014】処理または反応の対象としては、絶縁体管
(1)の内面の他、絶縁体管(1)内部に設置される物
体または管内を浮遊あるいは振動して運ばれる粉体等の
移動体表面、気体等の流通物、一部に気相を残した液体
表面などの任意のものとすることができる。表面処理す
ることのできる表面についても、特に制限はなく、未処
理面をはじめとして、セルロース、生体材料等で形成さ
れた、または表面処理された表面の任意のものとするこ
とができる。
The object to be treated or reacted is, in addition to the inner surface of the insulator tube (1), an object placed inside the insulator tube (1) or a moving body such as a powder which is carried by floating or vibrating in the tube. Any material such as a surface, a flowable substance such as a gas, a liquid surface partially leaving a gas phase, or the like can be used. The surface that can be surface-treated is also not particularly limited, and may be any surface, such as an untreated surface, or a surface that has been formed of cellulose, a biomaterial, or has been surface-treated.

【0015】[0015]

【実施例】以下実施例を示し、この発明の管内大気圧グ
ロープラズマ反応方法についてさらに詳しく説明する。 実施例1 図3に示したように、外径10mm,厚さ1mmのパイレッ
クス製ガラス管(7)の内側に円周に沿って厚さ190 μ
m,長さ240mm のポリイミドフィルム(8)(カプトン
H/Dupon 製)を管軸方向に一様にかつ一重になるよう
に張り付けた。また、ガラス管(7)の外側にポリイミ
ドフィルム(8)の左端より2cmの位置から18cmまで
の位置に一対のスパイラル状銅箔電極(9)(10)を
配設した。ガラス管(7)の一端部より管内に1気圧
(約760Torr )のHeとO2 との混合ガス(O2 が10
%)を総流量2000ml/min で導入するとともに、ガラス
管(7)の外周面に配設した銅箔電極(9)(10)に
高周波高電圧を周波数3kHz,3mAで印加し、放電を発
生させた。
The present invention will be described in more detail with reference to the following examples. Example 1 As shown in FIG. 3, a 190 μm thick pipe having a thickness of 190 μm was formed inside a Pyrex glass tube (7) having an outer diameter of 10 mm and a thickness of 1 mm.
A polyimide film (8) (manufactured by Kapton H / Dupon) having a length of 240 mm and a length of 240 mm was attached uniformly and unitarily in the tube axis direction. In addition, a pair of spiral copper foil electrodes (9) and (10) were disposed outside the glass tube (7) at positions from 2 cm to 18 cm from the left end of the polyimide film (8). Mixed gas (O 2 and He and O 2 at 1 atm into the tube from one end of the glass tube (7) (approximately 760 Torr) is 10
%) Is introduced at a total flow rate of 2000 ml / min, and a high-frequency high voltage is applied at a frequency of 3 kHz and 3 mA to the copper foil electrodes (9) and (10) disposed on the outer peripheral surface of the glass tube (7) to generate discharge. I let it.

【0016】銅箔電極(9)(10)の16cmにわたっ
て青白いHe放電発光が観察された。放電後、ガラス管
(7)の内側に張り付けたポリイミドフィルム(8)を
抜き取り、放電前後のフィルム(8)内表面の親・疎水
性の変化を水滴の接触角で評価した。その結果を示した
ものが表1である。
A pale He discharge emission was observed over 16 cm of the copper foil electrodes (9) and (10). After the discharge, the polyimide film (8) attached to the inside of the glass tube (7) was extracted, and the change in hydrophilicity / hydrophobicity of the inner surface of the film (8) before and after the discharge was evaluated by the contact angle of a water droplet. Table 1 shows the results.

【0017】[0017]

【表1】 [Table 1]

【0018】放電前のフィルム(8)の接触角は70度
であった。表1からも明らかなように、電極(9)(1
0)直下のフィルム(8)内表面の親水性が放電後に上
昇した。また、放電領域前後、特に下流域においては相
当長距離にわたって放電により親水化されることが確認
された。このような表面処理効果は、ポリイミドフィル
ム(8)をガラス管(7)の内径より小さい幅で切断
し、短冊状にしてガラス管(7)内に挿入した時にも確
認された。
The contact angle of the film (8) before discharging was 70 degrees. As is clear from Table 1, the electrodes (9) (1
0) The hydrophilicity of the inner surface of the film (8) immediately below increased after discharge. In addition, it was confirmed that before and after the discharge region, particularly in the downstream region, the region was hydrophilized by the discharge over a considerably long distance. Such a surface treatment effect was also confirmed when the polyimide film (8) was cut into a width smaller than the inner diameter of the glass tube (7), cut into a strip, and inserted into the glass tube (7).

【0019】実施例2 実施例1と同様に、図3に示したような装置を組み立
て、HeとC2 4 (テトラフルオロエチレン,TF
E)との混合気体を1気圧下で、He流量2000ml/min
,TFE流量4ml/min で導入し、電極(9)(1
0)間に3kHz ,2〜4.5mA ので印加し、放電を発生さ
せた。ポリイミドフィルム(8)内表面に透明な膜が形
成した。
Example 2 In the same manner as in Example 1, an apparatus as shown in FIG. 3 was assembled, and He and C 2 F 4 (tetrafluoroethylene, TF
E) mixed gas at 1 atm, He flow rate 2000ml / min
And TFE at a flow rate of 4 ml / min.
During 0), a voltage was applied at 3 kHz and 2 to 4.5 mA to generate a discharge. A transparent film was formed on the inner surface of the polyimide film (8).

【0020】図4は、この堆積膜のESCA(X線光電
子分光)測定によるフッ素と炭素の原子密度比を放電電
流との関係で示した相関図である。また、図5は、放電
電流と成膜速度との関係を示した相関図である。これら
の図4および図5からも明らかなように、基板として用
いたポリイミドフィルム(8)上に充分な速度でポリテ
トラフルオロエチレン(PTFE)類似膜が生成したこ
とが確認された。このプラズマ重合膜の水滴接触角を測
定したところ、およそ110 度から115 度であった。テフ
ロンにも匹敵する強い疎水性を示した。
FIG. 4 is a correlation diagram showing the relationship between the atom density ratio of fluorine and carbon measured by ESCA (X-ray photoelectron spectroscopy) of the deposited film in relation to the discharge current. FIG. 5 is a correlation diagram showing the relationship between the discharge current and the film forming speed. As is clear from FIGS. 4 and 5, it was confirmed that a polytetrafluoroethylene (PTFE) -like film was formed at a sufficient speed on the polyimide film (8) used as the substrate. The measured contact angle of water droplets on the plasma polymerized film was about 110 ° to 115 °. It showed strong hydrophobicity comparable to Teflon.

【0021】実施例3 実施例1と同様な装置中に、モデル排ガスとしてのNH
3 とNO2 を、各々、HeおよびArで大希釈し、以下
の条件で循環ポンプを通して放電領域に還流した。 混合気体流量: NH3 (NO2 ) 1ml/min He 1000ml/min Ar 1000ml/min 圧力 : 大気圧 放電周波数 : 13.56MHz 出力 : 100 W 放電領域を通過した気体の一部を取り出し、ガスクロマ
トグラフィで分析した。
Example 3 In a device similar to that of Example 1, NH as a model exhaust gas was used.
3 and NO 2 were each largely diluted with He and Ar, and refluxed to the discharge region through a circulation pump under the following conditions. Mixed gas flow rate: NH 3 (NO 2 ) 1 ml / min He 1000 ml / min Ar 1000 ml / min Pressure: Atmospheric pressure Discharge frequency: 13.56 MHz Output: 100 W A part of the gas that passed through the discharge area was taken out and analyzed by gas chromatography. did.

【0022】図6は、放電時間に対するNH3 およびN
2 の分解率を示した相関図である。この図6からも明
らかなように、NH3 およびNO2 が短時間に分解する
ことが確認された。特にNH3 は1分以内に完全に分解
した。生成物としてはNH3 の場合には、N2 とH2
他に、N2 4 が検出された。NO2 の場合の生成物
は、N2 とO2 とであった。
FIG. 6 shows NH 3 and N versus discharge time.
FIG. 4 is a correlation diagram showing the decomposition rate of O 2 . As is clear from FIG. 6, it was confirmed that NH 3 and NO 2 were decomposed in a short time. In particular, NH 3 was completely decomposed within 1 minute. In the case of NH 3 as a product, N 2 H 4 was detected in addition to N 2 and H 2 . The products in the case of NO 2 were N 2 and O 2 .

【0023】このような分解反応は、希釈ガスのHeお
よびArが、放電により高い励起状態の準安定原子に上
げられ、このエネルギーが試料気体に転移して生ずるも
のと考えられる。もちろんこの発明は、以上の例によっ
て限定されるものではない。電極の形態および材質、導
入する反応性気体および希ガスの種類、印加電力とその
周波数等の細部については様々な態様が可能であること
はいうまでもない。
It is considered that such a decomposition reaction occurs when He and Ar of the diluent gas are raised to metastable atoms in a highly excited state by electric discharge, and this energy is transferred to the sample gas. Of course, the present invention is not limited by the above examples. It goes without saying that various aspects are possible with respect to details such as the form and material of the electrode, the types of the reactive gas and the rare gas to be introduced, the applied power and the frequency thereof.

【0024】[0024]

【発明の効果】以上詳しく説明した通り、この発明によ
って、ガラス、プラスチック、セラミックス等からなる
円筒管等の絶縁体管の内面、または内部の静止、移動あ
るいは流通物へのプラズマ処理を大気圧下で行うことが
可能となる。
As described above in detail, according to the present invention, the plasma treatment of the inner surface of an insulating tube such as a cylindrical tube made of glass, plastic, ceramics, or the like, or the stationary, moving, or circulating material is performed under atmospheric pressure. It is possible to do with.

【図面の簡単な説明】[Brief description of the drawings]

【図1】この発明の管内大気圧グロープラズマ反応方法
に用いることのできる装置を例示した斜視図である。
FIG. 1 is a perspective view illustrating an apparatus that can be used for the in-tube atmospheric pressure glow plasma reaction method of the present invention.

【図2】装置の別の例を示した側面図である。FIG. 2 is a side view showing another example of the device.

【図3】(a)(b)は、各々、円筒管内面でのポリイ
ミドフィルムの親水化処理に用いた装置を示した横断面
図および縦断面図である。
FIGS. 3A and 3B are a cross-sectional view and a vertical cross-sectional view, respectively, showing an apparatus used for hydrophilizing a polyimide film on the inner surface of a cylindrical tube.

【図4】放電電流とプラズマ重合膜のESCA測定によ
るフッ素と炭素の原子密度比ととの関係を示した相関図
である。
FIG. 4 is a correlation diagram showing a relationship between a discharge current and an atomic density ratio between fluorine and carbon by ESCA measurement of a plasma polymerized film.

【図5】成膜速度と放電電流との関係を示した相関図で
ある。
FIG. 5 is a correlation diagram showing a relationship between a deposition rate and a discharge current.

【図6】放電時間に対するNH3 およびNO2 の分解率
を示した相関図である。
FIG. 6 is a correlation diagram showing a decomposition rate of NH 3 and NO 2 with respect to a discharge time.

【図7】従来の絶縁体円筒管への放電形式を示した斜視
図である。
FIG. 7 is a perspective view showing a conventional type of discharge to an insulator cylindrical tube.

【図8】従来の絶縁体円筒管への放電形式を示した斜視
図である。
FIG. 8 is a perspective view showing a conventional type of discharge to an insulator cylindrical tube.

【図9】従来の絶縁体円筒管への放電形式を示した斜視
図である。
FIG. 9 is a perspective view showing a conventional discharge type to an insulator cylindrical tube.

【符号の説明】[Explanation of symbols]

1 絶縁体管 2 高圧電極 3 アース電極 4 絶縁性接着剤 5 電源 6 混合ガス 7 ガラス管 8 ポリイミドフィルム 9,10 スパイラル状銅箔電極 DESCRIPTION OF SYMBOLS 1 Insulator tube 2 High voltage electrode 3 Earth electrode 4 Insulating adhesive 5 Power supply 6 Mixed gas 7 Glass tube 8 Polyimide film 9,10 Spiral copper foil electrode

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 外周部に一対の箔状の平行電極対をスパ
イラル状に張り付け周設した絶縁体管の一端部から反応
性ガスと希ガスとの混合ガスを導入し、大気圧下で絶縁
体管内部にグロー放電プラズマを発生させて、管内面、
または管内部の静止体、移動体あるいは流通物をグロー
プラズマ処理することを特徴とする管内大気圧グロープ
ラズマ反応方法。
1. A pair of foil-shaped parallel electrode pairs are formed on an outer peripheral portion by a spa
A mixed gas of a reactive gas and a rare gas is introduced from one end of an insulator tube attached in a peripheral shape, and a glow discharge plasma is generated inside the insulator tube under atmospheric pressure.
Alternatively, an in-pipe atmospheric pressure glow plasma reaction method, wherein glow plasma processing is performed on a stationary body, a moving body, or a flowing material inside the pipe.
【請求項2】 絶縁体管の外周部に一対の箔状の平行電
極対がスパイラル状に張り付け周設されており、絶縁体
管の一端部から反応性ガスと希ガスとの混合ガスを導入
して大気圧下で絶縁体管内部にグロー放電プラズマを発
生させ、絶縁体管内部においてグロープラズマ処理を可
能としたことを特徴とする管内大気圧グロープラズマ反
応用装置。
2. A pair of foil-shaped parallel electric wires are provided on the outer peripheral portion of the insulator tube.
The pole pairs are spirally attached and installed around the insulator.
Introduce mixed gas of reactive gas and rare gas from one end of tube
Glow discharge plasma inside the insulator tube under atmospheric pressure
Glow plasma treatment inside the insulator tube.
Atmospheric pressure glow plasma reaction tube
Applied equipment.
JP40946090A 1990-12-28 1990-12-28 Atmospheric pressure glow plasma reaction method in tube Expired - Fee Related JP3280994B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP40946090A JP3280994B2 (en) 1990-12-28 1990-12-28 Atmospheric pressure glow plasma reaction method in tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP40946090A JP3280994B2 (en) 1990-12-28 1990-12-28 Atmospheric pressure glow plasma reaction method in tube

Publications (2)

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JP3280994B2 true JP3280994B2 (en) 2002-05-13

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US7387081B2 (en) 2003-01-23 2008-06-17 3M Innovative Properties Company Plasma reactor including helical electrodes
CN100577716C (en) * 2004-09-08 2010-01-06 爱沃特株式会社 Fluororesin tubular film inner peripheral surface treatment method, fluororesin tubular film, fluororesin tubular film inner peripheral surface treatment device, PFA tubular film inner peripheral surface treatment method, PFA tubular film, PFA tubular film The inner peripheral surface treatment device and roller
JP5082459B2 (en) * 2006-01-20 2012-11-28 東京エレクトロン株式会社 Plasma processing apparatus and top plate manufacturing method
WO2011092186A1 (en) * 2010-01-26 2011-08-04 Leibniz-Institut Für Plasmaforschung Und Technologie E. V. Device and method for generating an electrical discharge in hollow bodies
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