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JPH0341207B2 - - Google Patents
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JPH0341207B2 - - Google Patents

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Publication number
JPH0341207B2
JPH0341207B2 JP20578483A JP20578483A JPH0341207B2 JP H0341207 B2 JPH0341207 B2 JP H0341207B2 JP 20578483 A JP20578483 A JP 20578483A JP 20578483 A JP20578483 A JP 20578483A JP H0341207 B2 JPH0341207 B2 JP H0341207B2
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JP
Japan
Prior art keywords
membrane
liquid
microwave
container
separation
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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JP20578483A
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Japanese (ja)
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JPS6099313A (en
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Priority to JP20578483A priority Critical patent/JPS6099313A/en
Publication of JPS6099313A publication Critical patent/JPS6099313A/en
Publication of JPH0341207B2 publication Critical patent/JPH0341207B2/ja
Granted legal-status Critical Current

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  • Separation Using Semi-Permeable Membranes (AREA)
  • Organic Low-Molecular-Weight Compounds And Preparation Thereof (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

(技術分野) 本発明は相溶性のある液体混合物の膜による分
離において、液・膜界面に高周波を印加する方法
に関するものである。 (従来技術とその問題点) 一般に相溶性のある液体混合物の各々の成分を
分離するには困難が伴なう。従来最も一般的に行
なわれている工業的分離方法は蒸留である。しか
し蒸留法は成分間の沸点差が大きく共沸混合物を
形成せず、且つ熱に対して安定な系でないと適用
できない。 又適用できる場合でも、蒸留には大量の熱エネ
ルギが必要であり、よりエネルギ消費の少ない分
離方法が求められている。 これに応え得る可能性を有する分離方法が膜分
離法である。このような観点から、従来より液体
混合物の膜分離は種々試みられてきた。 これらのうち、比較的普遍的な方法は、逆浸透
法および浸透気化法である。逆浸透法は海水の淡
水化等に実用化されている方法で、溶質である塩
(イオン)は不透過性で理想的には溶媒のみを透
過する半透膜を用い、溶液/透過液間に生ずる浸
透圧以上の圧力を溶液側に加えて、溶媒を透過さ
せ、分離する方法である。 この原理は液体混合物についても適用できるは
ずで、液体混合物の分離に逆浸透を適用した試み
も多い。しかし相溶性のある液体混合物では分子
サイズ、化学的性質等類似している場合が多いた
め、必らずしも分離性はよくない。又溶液/透過
液間の浸透圧を無視できず、濃縮限界が存在す
る。通常の操作圧では10〜15%程度が限界とな
り、液体混合物への逆浸透の適用は、特殊な場合
を除いて現状では有用でない。 浸透気化法は膜の片面を分離さるべき液体混合
物に接触させ、他の一面を減圧とするか、キヤリ
アガスと接触させた系よりなる。 原理的にはこの系における成分の分離は成分液
体の膜への溶解度の差、膜内の拡散速度の差に基
づいて行なわれるため逆浸透のような限界はない
と考えられ、液体混合物の分離には有望とみられ
ている。 しかし上述の分離過程からもわかるように、化
学的・物理的性質の類似した液体の組合せの場合
には、膜の材質、構成などに工夫が必要であり、
現在までに浸透気化法を実用した例はほとんどな
い。 これらの普遍的方法とは異なつた膜分離法が最
近発表された。その概要は第1図に示すような構
成で、高周波振動を利用して、エタノール水溶液
から、エタノールを分離することができるといわ
れている。 第1図について説明すると、1は分離されるべ
きエタノール水溶液、2は炭酸カリウム又は乳酸
カリウム水溶液、3は透過したエタノール、4は
多孔芯テフロン膜、5はテフロン膜の表面をラジ
カル化処理して導電性をもたせたラジカル化テフ
ロン膜、6はフツ化ビニリデン膜である。 第1図において、ラジカル化テフロン膜5に電
極7,7′を通じて100〜1000KHzの高周波電流を
かけて、フツ化ビニリデン膜6の表面にマイクロ
波振動を起こさせ、このマイクロ波振動エネルギ
によつて会合したエタノール分子の中心に水を抱
いた構造のエタノール包接化合物と、その周囲の
水との間の給合が切れ、エタノール包接化合物の
みを膜4,5,6を経て液2中に取出し、更にテ
フロン膜10を経て透過液3として取出すといわ
れている。電極8,9間には直流電圧を印加する
ことによつて透過を促進することができるとい
う。 しかしこの方法に関する具体的記載は見当ら
ず、関連技術と思われる特開昭58−95502〜95520
号公報にも実施例の記述はなく、構成内容不明で
ある。 (発明の構成) 本発明は液体混合物の膜による分離において、
液・膜界面に容易に且つ効率よく高周波を印加す
る方法を提供するものである。即ちマイクロ波は
波長がcmからmmのオーダーとなるため、いわゆる
電波としての性質を有し、通常の電線によつては
伝播し得ず、又通常の電極によつては電場を印加
できない。従つてこれを膜・液界面に印加するた
めには、特殊な導波路を設け、印加空間の形状、
膜の配置を工夫しなければならない。本発明は導
波路と別個に設けた印加空間内で膜・液界面にマ
イクロ波を印加しつゝ膜分離を行なう方法を提供
するものである。 以下第2図に示す本発明の一実施例について説
明する。21はマイクロ波の伝播空間として働ら
く導体に囲まれた空間、24はマイクロ波の発信
機、23は導波管である。24で発信されたマイ
クロ波はアンテナ22を経て、導波管内を進行
し、開口部27からマイクロ波伝播空間21内に
放射される。25は誘電体よりなる容器でマイク
ロ波伝播空間21の内部に設置され、その内部に
は中空状のポリ四フツ化エチレン多孔膜チユーブ
26を配置する。分離すべき液体混合物は貯槽1
1よりポンプ12によりポリ四フツ化エチレン多
孔膜チユーブ26内を通つて再び貯槽11へと循
環される。キヤリヤーガスとして用いられる窒素
ガスは配管13を経て容器25内に送入され、ポ
リ四フツ化エチレン多孔膜チユーブ26の外面と
接触しつゝ進行した後、コールドトラツプ14へ
と導かれる。ポリ四フツ化エチレン多孔膜チユー
ブ26を透過してくる透過物はキヤリヤーガスと
共に容器25マイクロイ波伝播空間21の外部に
運び出され、コールドトラツプ14においてキヤ
リヤーガスから分離される。上例では膜としてポ
リ四フツ化エチレン多孔膜チユーブを用いたがマ
イクロ波帯域における誘電正接の小さい、即ち損
失の小さい材質から成る膜なら、ポリ四フツ化エ
チレンでなくてもよく、特に誘電正接約300×
10-4以下の材料は膜材料として適している。 多孔体でない膜を使用する場合にはキヤリヤー
ガスを用いる代りに減圧としてもよい。又キヤリ
ヤーガスは分離されるべき液体混合物の各成分と
反応しない不活性ガスならば窒素ガスに限定され
るものではない。 このような構成の系において、上述の如くマイ
クロ波をマイクロ波伝播空間21内に放射する
と、容器25及び膜26は誘電体より成るためマ
イクロ波をほとんど吸収しないが、液体混合物に
は吸収され、液体成分を活性化する。従つてこの
状態では、液体成分の活性化の差異によつて、特
定成分が他の成分に比べて膜を透過する割合が大
きくなり、透過速度、分離の効率が向上する。 液体中でのマイクロ波の吸収による減衰のた
め、液・膜界面附近での吸収が大きく内部に向か
うに従つてマイクロ波は減衰してゆく。膜分離に
おいては実質的に分離に有効なのは、液・膜界面
の限られた範囲であるから、上述のような構成
で、液・膜界面で最大の吸収を示すというのはマ
イクロ波の利用効率の面で有利である。 尚上述の説明よりわかるように、マイクロ波の
進行路上に薄い液・膜界面層を設けることはマイ
クロ波の利用効率を改善するうえに更に有効であ
る。 これは例えば微細な径を有する中空糸状の膜を
多数本束状にして中空糸の内部又は外部の一方に
分離すべき液体を流し、他の部分にキヤリヤーガ
スを流したり、或はこれを減圧とする方法、又は
平面状の膜を層状に積層し、膜の片面に液体を流
し、他の片面にキヤリヤーガスを流したり、或は
減圧とすることにより実現できる。これらの例を
以下に説明する。 第3図は第2図の容器25の内部を液体の進行
方向に直角な面の概念的な断面図を示す。容器2
5内に微細径の中空状膜31を充てんしたもの
で、下半分は省略してある。このような構成にお
いて中空状膜の内部に分離すべき液体を流し、外
部にキヤリヤーガスを流すか又は減圧にする。又
内部と外部とを逆にしてもよい。 第4図は両端を密封して袋状とした膜41をの
り巻状にして容器25内に配置したものの断面図
で、膜の片面側の空間42にキヤリヤーガスを流
すか減圧とし、他の面側の空間43に分離すべき
液体を流すものである。この場合も、空間42と
43とを逆に用いてもよい。 又図には示さないが、のり巻状にせず平面状の
まま空間を残しつゝ積層し、交互にキヤリヤーガ
ス又は減圧の部分と液体を流す部分とを設けるこ
ともできる。 以下に本法による液体分離の実施例を述べる。 実施例 1 第2図に示す構成の装置を用い、膜として孔径
0.1μm、膜厚0.5mm、管径15mm、長さ19cmのポリ
四フツ化エチレン多孔膜チユーブを用い、周波数
2.45GHzのマイクロ波を照射して、被分離液約4
%エタノール水溶液を14ml/minの流速で循環さ
せ、窒素ガスを1ml/minの流速で流した。容器
としては長さ30cm、内径2.2cmのガラス管を使用
した。 比較例 1 マイクロ波は照射しない他は、実施例1と同じ
条件で液体分離を行なつた。 前記実施例1及び比較例1より得られた結果を
まとめて次表に示す。
(Technical Field) The present invention relates to a method of applying high frequency waves to a liquid/membrane interface in separating compatible liquid mixtures using a membrane. (Prior Art and its Problems) Generally, it is difficult to separate the components of a liquid mixture that are compatible with each other. The most commonly used industrial separation method is distillation. However, the distillation method cannot be applied unless the system has a large boiling point difference between the components, does not form an azeotrope, and is stable against heat. Furthermore, even when applicable, distillation requires a large amount of thermal energy, and there is a need for a separation method that consumes less energy. A separation method that has the potential to meet this demand is membrane separation. From this point of view, various attempts have been made to membrane separation of liquid mixtures. Among these, the relatively common methods are reverse osmosis and pervaporation. Reverse osmosis is a method that has been put to practical use in desalination of seawater, etc., and uses a semipermeable membrane that is impermeable to salts (ions), which are solutes, and ideally allows only the solvent to pass through. In this method, a pressure higher than the osmotic pressure generated in the solution is applied to the solution side to allow the solvent to permeate and separate the solution. This principle should also be applicable to liquid mixtures, and there have been many attempts to apply reverse osmosis to the separation of liquid mixtures. However, since compatible liquid mixtures often have similar molecular sizes, chemical properties, etc., separation is not always good. Furthermore, the osmotic pressure between the solution and the permeate cannot be ignored, and there is a concentration limit. At normal operating pressures, the limit is about 10-15%, and the application of reverse osmosis to liquid mixtures is currently not useful except in special cases. The pervaporation process consists of a system in which one side of the membrane is in contact with the liquid mixture to be separated and the other side is under reduced pressure or in contact with a carrier gas. In principle, separation of components in this system is performed based on differences in solubility of component liquids in the membrane and differences in diffusion rates within the membrane, so it is thought that there is no limit like reverse osmosis, and separation of liquid mixtures is possible. is seen as promising. However, as can be seen from the separation process described above, in the case of a combination of liquids with similar chemical and physical properties, it is necessary to devise the material and structure of the membrane.
To date, there are almost no examples of practical use of the pervaporation method. A membrane separation method different from these universal methods has recently been announced. Its outline is shown in Figure 1, and it is said that ethanol can be separated from an aqueous ethanol solution using high-frequency vibrations. To explain Figure 1, 1 is the ethanol aqueous solution to be separated, 2 is the potassium carbonate or potassium lactate aqueous solution, 3 is the permeated ethanol, 4 is the porous core Teflon membrane, and 5 is the surface of the Teflon membrane subjected to radicalization treatment. The radicalized Teflon film 6 is a vinylidene fluoride film having conductivity. In FIG. 1, a high frequency current of 100 to 1000 KHz is applied to the radicalized Teflon film 5 through electrodes 7 and 7' to cause microwave vibrations on the surface of the vinylidene fluoride film 6, and the microwave vibration energy is applied to the surface of the vinylidene fluoride film 6. The supply between the ethanol clathrate compound, which has a structure in which water is held in the center of the associated ethanol molecules, and the surrounding water is cut off, and only the ethanol clathrate compound passes through the membranes 4, 5, and 6 into the liquid 2. It is said that the permeated liquid 3 is taken out through the Teflon membrane 10. It is said that permeation can be promoted by applying a DC voltage between electrodes 8 and 9. However, there is no specific description of this method, and Japanese Patent Application Laid-open No. 58-95502 to 95520, which are considered to be related techniques,
There is no description of an embodiment in the publication, and the contents of the structure are unknown. (Structure of the Invention) The present invention provides a method for separating a liquid mixture using a membrane.
The present invention provides a method for easily and efficiently applying high frequency waves to a liquid/film interface. That is, since microwaves have wavelengths on the order of cm to mm, they have the properties of so-called radio waves, and cannot be propagated using ordinary electric wires, nor can an electric field be applied using ordinary electrodes. Therefore, in order to apply this to the membrane/liquid interface, a special waveguide is provided, and the shape of the application space,
The arrangement of the membrane must be devised. The present invention provides a method for performing membrane separation while applying microwaves to a membrane/liquid interface in an application space provided separately from a waveguide. An embodiment of the present invention shown in FIG. 2 will be described below. 21 is a space surrounded by a conductor that serves as a microwave propagation space, 24 is a microwave transmitter, and 23 is a waveguide. The microwave emitted at 24 passes through the antenna 22, travels within the waveguide, and is radiated into the microwave propagation space 21 from the opening 27. A container 25 made of a dielectric material is installed inside the microwave propagation space 21, and a hollow polytetrafluoroethylene porous membrane tube 26 is arranged inside the container. The liquid mixture to be separated is stored in tank 1.
1, the polytetrafluoroethylene porous membrane tube 26 is circulated again to the storage tank 11 by the pump 12. Nitrogen gas used as a carrier gas is introduced into the container 25 through the pipe 13 and, after contacting the outer surface of the polytetrafluoroethylene porous membrane tube 26, is guided to the cold trap 14. The permeate passing through the polytetrafluoroethylene porous membrane tube 26 is carried out of the container 25 and the microwave propagation space 21 together with the carrier gas, and is separated from the carrier gas in the cold trap 14. In the above example, a polytetrafluoroethylene porous membrane tube was used as the membrane, but if the membrane is made of a material with a small dielectric loss tangent in the microwave band, that is, a small loss, it does not need to be polytetrafluoroethylene. Approximately 300×
Materials below 10 -4 are suitable as membrane materials. When a non-porous membrane is used, reduced pressure may be used instead of using a carrier gas. Further, the carrier gas is not limited to nitrogen gas as long as it is an inert gas that does not react with the components of the liquid mixture to be separated. In a system with such a configuration, when microwaves are emitted into the microwave propagation space 21 as described above, the container 25 and the membrane 26 are made of dielectric material and therefore hardly absorb the microwaves, but they are absorbed by the liquid mixture. Activates liquid ingredients. Therefore, in this state, due to the difference in activation of the liquid components, a specific component permeates through the membrane at a higher rate than other components, improving the permeation rate and separation efficiency. Because microwaves are attenuated by absorption in the liquid, the absorption is large near the liquid-membrane interface, and the microwaves are attenuated as they move toward the inside. In membrane separation, what is actually effective for separation is the limited range of the liquid/membrane interface, so in the configuration described above, the maximum absorption at the liquid/membrane interface is due to microwave utilization efficiency. It is advantageous in terms of As can be seen from the above explanation, providing a thin liquid/film interface layer on the path of the microwave is more effective in improving the microwave utilization efficiency. This can be done, for example, by bundling a large number of hollow fiber-like membranes with minute diameters, flowing the liquid to be separated into one of the inside or outside of the hollow fibers, and flowing a carrier gas into the other part, or by reducing the pressure. This can be achieved by stacking planar membranes in layers, by flowing a liquid on one side of the membrane and a carrier gas on the other side, or by applying reduced pressure. Examples of these are described below. FIG. 3 shows a conceptual cross-sectional view of the inside of the container 25 shown in FIG. 2 in a plane perpendicular to the direction in which the liquid travels. container 2
5 is filled with a hollow membrane 31 of minute diameter, and the lower half is omitted. In such a configuration, the liquid to be separated is passed inside the hollow membrane, and a carrier gas is passed or a reduced pressure is applied to the outside. Also, the inside and outside may be reversed. FIG. 4 is a cross-sectional view of a bag-shaped membrane 41 with both ends sealed and placed in a rolled-up container 25, in which a carrier gas is flowed or depressurized into the space 42 on one side of the membrane, and the other side is The liquid to be separated flows into the side space 43. In this case as well, the spaces 42 and 43 may be used in reverse. Although not shown in the figure, it is also possible to stack them without forming them into a spiral shape, leaving a space in a planar shape, and alternately providing carrier gas or reduced pressure sections and sections through which liquid flows. Examples of liquid separation using this method will be described below. Example 1 Using an apparatus with the configuration shown in Figure 2, the pore size of the membrane was
Using a polytetrafluoroethylene porous membrane tube of 0.1 μm, membrane thickness 0.5 mm, tube diameter 15 mm, and length 19 cm,
By irradiating 2.45GHz microwave, the liquid to be separated is approximately 4
% ethanol aqueous solution was circulated at a flow rate of 14 ml/min, and nitrogen gas was flowed at a flow rate of 1 ml/min. A glass tube with a length of 30 cm and an inner diameter of 2.2 cm was used as the container. Comparative Example 1 Liquid separation was carried out under the same conditions as in Example 1, except that microwave irradiation was not performed. The results obtained from Example 1 and Comparative Example 1 are summarized in the following table.

【表】 実施例 2 第2図に示す構成の装置を用い、容器25を第
3図に示す構成で行なつた。使用した容器は実施
例1と同じで、周波数2.45GHzのマイクロ波を照
射して膜として孔径10.1μm、膜厚0.5mm、管径1
mm、長さ19cmのポリ四フツ化エチレン多孔膜チユ
ーブ28本を束ね、周波数2.45GHzのマイクロ波を
照射して、膜内部に被分離液約4%エタノール水
溶液を14ml/minの流速で循環させ、窒素ガスを
1ml/minの流速で流した。 比較例 2 マイクロ波は照射しない他は、実施例2と同じ
条件で液体分離を行なつた。 前記実施例2及び比較例2より得られた結果を
まとめて次表に示す。
[Table] Example 2 Using an apparatus having the configuration shown in FIG. 2, a test was carried out with the container 25 having the configuration shown in FIG. 3. The container used was the same as in Example 1, and was irradiated with microwaves with a frequency of 2.45 GHz to form a membrane with a pore diameter of 10.1 μm, a film thickness of 0.5 mm, and a tube diameter of 1.
28 polytetrafluoroethylene porous membrane tubes with a length of 19 cm and a length of 19 cm are bundled together and irradiated with microwaves at a frequency of 2.45 GHz to circulate an approximately 4% ethanol aqueous solution of the liquid to be separated inside the membrane at a flow rate of 14 ml/min. , nitrogen gas was flowed at a flow rate of 1 ml/min. Comparative Example 2 Liquid separation was carried out under the same conditions as in Example 2, except that microwave irradiation was not performed. The results obtained from Example 2 and Comparative Example 2 are summarized in the following table.

【表】 (発明の効果) 本発明によれば従来の如き複雑な膜構造は不要
となり、既に技術的に実績のあるマイクロ波発信
機を用いて、液・膜界面近傍に効率よくマイクロ
波を供給できるので、高周波を用いた液体分離の
効率を向上させることができ、且つ操作性が向上
する。
[Table] (Effects of the invention) According to the present invention, there is no need for a complicated membrane structure as in the past, and a microwave transmitter that has already been technically proven is used to efficiently transmit microwaves near the liquid/membrane interface. Since the liquid can be supplied, the efficiency of liquid separation using high frequency can be improved, and the operability can be improved.

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

第1図は従来の液体混合物の膜分離法を示す説
明図、第2図は本発明の実施例を示す図、第3図
は第2図の容器25の内部の液体の進行方向に直
角な面の概念的な断面図、第4図は第2図の容器
25の内部に両端を密封して袋状とした膜をのり
巻状に配置した断面図である。 1……エタノール水溶液、2……炭酸カリウム
又は乳酸カリウム水溶液、3……透過したエタノ
ール、4……多孔芯テフロン膜、5……ラジカル
化テフロン膜、6……フツ化ビニリデン膜、7,
7′,8,9……電極、10……テフロン膜、2
1……マイクロ波の伝播空間として働く導体に囲
まれた空間、22……アンテナ、23……導波
管、24……マイクロ波発信機、25……誘電体
よりなる容器、26……ポリ四フツ化エチレン多
孔膜チユーブ、27……開口部、11……貯槽、
12……ポンプ、13……配管、14……コール
ドトラツプ、31……微細孔の中空状膜、41…
…両側を密封して袋状とした膜、42……膜の片
面側の空間、43……他の両側の空間。
FIG. 1 is an explanatory diagram showing a conventional membrane separation method for liquid mixtures, FIG. 2 is a diagram showing an embodiment of the present invention, and FIG. FIG. 4 is a conceptual cross-sectional view of the surface of the container 25 shown in FIG. 2, in which a bag-shaped membrane with both ends sealed is arranged in a roll. 1... Ethanol aqueous solution, 2... Potassium carbonate or potassium lactate aqueous solution, 3... Permeated ethanol, 4... Porous core Teflon membrane, 5... Radicalized Teflon membrane, 6... Vinylidene fluoride membrane, 7.
7', 8, 9... Electrode, 10... Teflon membrane, 2
DESCRIPTION OF SYMBOLS 1...A space surrounded by a conductor that acts as a microwave propagation space, 22...Antenna, 23...Waveguide, 24...Microwave transmitter, 25...Container made of dielectric material, 26...Polymer Tetrafluoroethylene porous membrane tube, 27...opening, 11...storage tank,
12...Pump, 13...Piping, 14...Cold trap, 31...Hollow membrane with micropores, 41...
...a bag-shaped membrane with both sides sealed, 42...a space on one side of the membrane, 43...a space on the other both sides.

Claims (1)

【特許請求の範囲】 1 液体混合物から高周波電磁場の存在下で膜を
用いて前記液体成分を分離する方法において、マ
イクロ波発振源から放射されるマイクロ波を伝播
する導波経路内に誘電体からなる容器を設け、容
器の内部を高分子膜で区画し、該膜の片面に分離
すべき液体混合物を接触させ、他の面には該膜を
透過してくる成分を誘導し捕捉するためのキヤリ
ヤーガス或は減圧の雰囲気を形成することを特徴
とする液体の膜分離方法。 2 マイクロ波導波経路内の容器内を区画する高
分子膜が複数の微細径中空糸状膜を集束した構造
であることを特徴とする特許請求範囲第1項記載
の液体の膜分離方法。
[Claims] 1. A method for separating liquid components from a liquid mixture using a membrane in the presence of a high-frequency electromagnetic field, in which a dielectric material is disposed in a waveguide path for propagating microwaves emitted from a microwave oscillation source. The inside of the container is partitioned with a polymer membrane, one side of the membrane is brought into contact with the liquid mixture to be separated, and the other side is provided with a membrane for guiding and trapping the components passing through the membrane. A method for membrane separation of liquids characterized by forming a carrier gas or a reduced pressure atmosphere. 2. The liquid membrane separation method according to claim 1, wherein the polymer membrane that partitions the inside of the container in the microwave waveguide path has a structure in which a plurality of fine diameter hollow fiber membranes are bundled.
JP20578483A 1983-11-04 1983-11-04 Process for separating liquid using membrane Granted JPS6099313A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20578483A JPS6099313A (en) 1983-11-04 1983-11-04 Process for separating liquid using membrane

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20578483A JPS6099313A (en) 1983-11-04 1983-11-04 Process for separating liquid using membrane

Publications (2)

Publication Number Publication Date
JPS6099313A JPS6099313A (en) 1985-06-03
JPH0341207B2 true JPH0341207B2 (en) 1991-06-21

Family

ID=16512614

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20578483A Granted JPS6099313A (en) 1983-11-04 1983-11-04 Process for separating liquid using membrane

Country Status (1)

Country Link
JP (1) JPS6099313A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5025844B2 (en) * 2000-06-02 2012-09-12 日産化学工業株式会社 Membrane permeation control method by microwave
KR100722398B1 (en) 2005-12-26 2007-05-28 주식회사 포스코 Core temperature measuring device
JP6395321B2 (en) 2015-10-26 2018-09-26 株式会社ニフコ Grommet

Also Published As

Publication number Publication date
JPS6099313A (en) 1985-06-03

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