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JPH0341205B2 - - Google Patents
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JPH0341205B2 - - Google Patents

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Publication number
JPH0341205B2
JPH0341205B2 JP58205782A JP20578283A JPH0341205B2 JP H0341205 B2 JPH0341205 B2 JP H0341205B2 JP 58205782 A JP58205782 A JP 58205782A JP 20578283 A JP20578283 A JP 20578283A JP H0341205 B2 JPH0341205 B2 JP H0341205B2
Authority
JP
Japan
Prior art keywords
membrane
liquid
microwave
separation
microwaves
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 - Lifetime
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JP58205782A
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Japanese (ja)
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JPS6099311A (en
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Priority to JP20578283A priority Critical patent/JPS6099311A/en
Publication of JPS6099311A publication Critical patent/JPS6099311A/en
Publication of JPH0341205B2 publication Critical patent/JPH0341205B2/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を、液・膜界
面にマイクロ波を印加して分離する膜分離方法に
使用する分離装置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。 実際の分離は、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。原理
的には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・物理的性質のい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。 これは、新聞発表があつたのみで詳細は不明で
あるが、第1図に示すような構成により、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アル化テフ
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
との間の結合が切れ、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許公開公報特開昭58−
95502〜95520号公報にも実施例の記述はなく、構
成内容は不明である。 (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マイクロ波を印
加することの可能な液体分離装置を提供するもの
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。本発明はマイクロ波
を膜分離に適用するに適した導波路、印加空間、
膜の配置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。 61は同軸ケーブル状構造体、62,63は
夫々中心導体および外導体で、これにマイクロ波
発信機64よりマイクロ波を印加すれば該構造体
内をマイクロ波が伝播し得る。 65はポリ四フツ化エチレン多孔体チユーブで
ある。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の材料からなる膜ならばポ
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。 本実施例では上記チユーブを中心導体62を中
心として同軸状に配置してある。66は気密性を
保つための端末構造物である。分離されるべき液
体混合物は貯槽51よりポンプ52によつてポリ
四フツ化エチレン多孔体チユーブ65の内部を通
り、再び貯槽51へと循環される。55は窒素ガ
スボンベで、キヤリヤーガスとして用いる窒素ガ
スは本例ではコールドトラツプ54によつて水分
を除いた後、同軸ケーブル状構造体61内に送入
され、外部導体63とポリ四フツ化エチレン多孔
体チユーブ65との間の空間を通過し、コールド
トラツプ54へと導かれる。キヤリヤーガスとし
ては分離されるべき液体混合物の各成分と反応し
ない不活性ガスであれば窒素ガスに限定されるも
のではない。又膜として多孔体を使用しない場合
はキヤリヤーガスを用いる代りに、減圧としても
よい。 このような構成の系においてマイクロ波を供給
した場合、マイクロ波は構造体61の長さ方向に
伝播し、これに伴なう電場は中心導体面と外部導
体面に直交する面内にある。このためマイクロ波
の進行方向に平行に置かれた膜による損失は殆ん
どなく、これに接した分離されるべき液体の進行
方向に平行な面内には表面電流がマイクロ波の波
長とほぼ等しい周期であらわれる。液体が完全な
導体と見なせる場合は、この表面電流のロスは非
常に小さいが、通常の液体ではこの部分での吸収
が起こる。マイクロ波はこの他液体の誘電緩和に
よる損失があるが、これも表面で大きく、深部へ
行くに従つて減少する。このように吸収が起るの
は、表面近傍の領域であるので、膜による液体分
離という目的にとつては、膜・液界面附近での吸
収は大きいが分離にとつては有効でない液体深部
での吸収は小さく、マイクロ波のエネルギを有効
に膜分離に利用できる。このような状況からわか
るように膜として微細な径の中空糸を用いて、こ
れらを多数本束状にしてマイクロ波の進行方向に
平行に配置して、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にすれば、液−膜接
触界面が多くなるので、マイクロ波の利用効率が
よくなる。 以下に本法による液体分離の実施例を述べる。 実施例 1 膜として孔径0.1μm、膜厚0.5mm、管径15mm、
長さ17cmのポリ四フツ化エチレン多孔膜チユーブ
を用い、周波数500MHz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7ml/minの
流速で循環させ、窒素ガスを0.5/minの流速
で流した。 実施例 2 周波数5GHzのマイクロ波を用いる以外は、実
施例1と同じ条件で液体分離を行なつた。 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、2及び比較例1より得られた結
果をまとめて下表に示す。
(Technical Field) The present invention relates to a separation device used in a membrane separation method in which compatible liquid mixtures are separated by applying microwaves to the liquid/membrane interface. (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. The actual separation is based on the difference in the solubility of the component liquids in the membrane,
This is done based on differences in diffusion rates within the membrane. In principle, it does not seem to have the same limitations as reverse osmosis, and it appears to be promising for separating liquid mixtures. 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 consider the material and structure of the membrane. There are very few examples. A membrane separation method different from these universal methods has recently been announced. This was only announced in the press and the details are unknown, but it is said that with the configuration shown in Figure 1, 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 radialized 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 the electrodes 7 and 7' to cause microwave vibrations on the surface of the vinylidene fluoride film 6, and the energy of the microwave vibrations causes the particles to bind together. The bond between the ethanol clathrate compound, which has a structure in which water is held in the center of the ethanol molecule, and the surrounding water is broken, and only the ethanol clathrate compound is extracted into the liquid 2 through the membranes 4, 5, and 6. It is said that the permeate is further taken out as a permeate 3 through a 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 the patent publication publication JP-A-58-1989, which is considered to be a related technology, has not been found.
No. 95502 to No. 95520 also contain no description of an embodiment, 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 liquid separation device that can easily and efficiently apply microwaves to a liquid/membrane 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 must be provided, and the shape of the application space and the arrangement of the membranes must be devised. The present invention provides a waveguide, an application space, and a waveguide suitable for applying microwaves to membrane separation.
Provides membrane placement. An embodiment of the present invention shown in FIG. 2 will be described below. 61 is a coaxial cable-like structure, and 62 and 63 are a center conductor and an outer conductor, respectively. When a microwave is applied to this from a microwave transmitter 64, the microwave can propagate within the structure. 65 is a polytetrafluoroethylene porous tube. Polytetrafluoroethylene may not be used as a membrane if it is made of a material with a small dielectric loss tangent in the microwave band, that is, a material with low loss.In particular, a material with a dielectric loss tangent of about 300×10 -4 or less is suitable as a membrane material. . In this embodiment, the tubes are arranged coaxially with the center conductor 62 as the center. 66 is a terminal structure for maintaining airtightness. The liquid mixture to be separated is circulated from the storage tank 51 through the inside of the polytetrafluoroethylene porous tube 65 by the pump 52 and back to the storage tank 51. Reference numeral 55 denotes a nitrogen gas cylinder. In this example, the nitrogen gas used as a carrier gas is fed into the coaxial cable-like structure 61 after moisture is removed by the cold trap 54, and is connected to the outer conductor 63 and the polytetrafluoroethylene porous structure. It passes through the space between the body tube 65 and is guided to the cold trap 54. 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. Further, when a porous body is not used as the membrane, reduced pressure may be used instead of using a carrier gas. When microwaves are supplied in a system having such a configuration, the microwaves propagate in the length direction of the structure 61, and the accompanying electric field is in a plane orthogonal to the central conductor surface and the outer conductor surface. For this reason, there is almost no loss due to the membrane placed parallel to the direction of microwave propagation, and the surface current in the plane parallel to the direction of propagation of the liquid to be separated that is in contact with it is almost the same as the wavelength of the microwave. Appears at equal intervals. If the liquid could be considered a perfect conductor, this surface current loss would be extremely small, but in normal liquids, absorption occurs in this area. Microwaves also suffer losses due to dielectric relaxation of the liquid, which is also large at the surface and decreases as it goes deeper. Since absorption occurs in the region near the surface, for the purpose of liquid separation using a membrane, absorption is large near the membrane/liquid interface, but it is not effective for separation deep inside the liquid. absorption is small, and microwave energy can be effectively used for membrane separation. As can be seen from this situation, hollow fibers with a fine diameter are used as membranes, and a large number of them are bundled and arranged parallel to the direction of propagation of the microwave, and separated either inside or outside the hollow fiber. By flowing the liquid to be treated and flowing a carrier gas to other parts, or by reducing the pressure, the number of liquid-film contact interfaces increases, and the efficiency of using microwaves is improved. Examples of liquid separation using this method will be described below. Example 1 The membrane has a pore diameter of 0.1 μm, a membrane thickness of 0.5 mm, a tube diameter of 15 mm,
Using a polytetrafluoroethylene porous membrane tube with a length of 17 cm, irradiation with microwaves at a frequency of 500 MHz circulates an approximately 4% ethanol aqueous solution to be separated at a flow rate of 7 ml/min, and nitrogen gas at a flow rate of 0.5/min. It was washed away. Example 2 Liquid separation was carried out under the same conditions as in Example 1 except that microwaves with a frequency of 5 GHz were used. 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 Examples 1 and 2 and Comparative Example 1 are summarized in the table below.

【表】 次に他の実施例について説明する。第3図にお
いて、21はマイクロ波の伝播空間として働く導
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51より
ポンプ52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51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53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54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、マイクロ波伝播空間21の外部に運び出
され、コールドトラツプ54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4図は第3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5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。 以下にこの方式による液体分離の実施例を述べ
る。 実施例 3 第3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 2 マイクロ波は照射しない他は、実施例3と同じ
条件で液体分離を行なつた。 前記実施例3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] Next, other examples will be described. In FIG. 3, 21 is a space surrounded by conductors that acts as a microwave propagation space, 24 is a microwave transmitter,
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 circulated from the storage tank 51 through the polytetrafluoroethylene porous membrane tube 26 by the pump 52 and back to the storage tank 51. Nitrogen gas used as a carrier gas is introduced into the container 25 through the pipe 53 and, after contacting the outer surface of the polytetrafluoroethylene porous membrane tube 26, is guided to the cold trap 54. Polytetrafluoroethylene porous membrane tube 26
The permeate 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 54. 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. Materials with a density of about 300×10 -4 or less 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 and the liquid Activate 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 a limited range of the liquid/membrane interface, so with the above configuration, the liquid/membrane interface is effective.
Showing maximum absorption at the membrane interface is advantageous in terms of microwave utilization efficiency. 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. 4 shows a conceptual cross-sectional view of the interior of the container 25 shown in FIG. 3 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. 5 shows a membrane 41 sealed at both ends in a bag-like shape and placed in a container 25 in the form of a roll. 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 flat shape, and alternately providing carrier gas or reduced pressure areas and areas through which liquid flows. An example of liquid separation using this method will be described below. Example 3 Using an apparatus with the configuration shown in Figure 3, 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 2 Liquid separation was carried out under the same conditions as in Example 3, except that microwave irradiation was not performed. The results obtained from Example 3 and Comparative Example 2 are summarized in the following table.

【表】 実施例 4 第3図に示す構成の装置を用い、容器25を第
4図に示す構成で行なつた。使用した容器は実施
例3と同じで、膜として孔径0.1μm、膜厚0.5mm、
管径1mm、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 3 マイクロ波は照射しない他は、実施例4と同じ
条件で液体分離を行なつた。 前記実施例4及び比較例3より得られた結果を
まとめて次表に示す。
[Table] Example 4 Using an apparatus having the structure shown in FIG. 3, a test was carried out using the container 25 having the structure shown in FIG. The container used was the same as in Example 3, and the membrane had a pore diameter of 0.1 μm, a film thickness of 0.5 mm,
Twenty-eight polytetrafluoroethylene porous membrane tubes with a tube diameter of 1 mm and a length of 19 cm are bundled together and irradiated with microwaves at a frequency of 2.45 GHz to inject an approximately 4% ethanol aqueous solution of the liquid to be separated into the membrane at a flow rate of 14 ml/min. It was circulated and nitrogen gas was passed at a flow rate of 1 ml/min. Comparative Example 3 Liquid separation was carried out under the same conditions as in Example 4, except that microwave irradiation was not performed. The results obtained from Example 4 and Comparative Example 3 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、既に技術的にい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、マイクロ波を用いた液
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 micro-waves near the liquid/membrane interface. Since waves can be supplied, the efficiency of liquid separation using microwaves can be improved, and the operability can be improved.

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

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図は本発明の一実施例についての説明
図、第3図は他の実施例についての説明図、第4
図は第3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5図は第3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、31……微細径
の中空状膜、41……両端を密封して袋状とした
膜、42……膜の片面側の空間、43……他の面
側の空間、51……貯槽、52……ポンプ、53
……配管、54……コールドトラツプ、55……
窒素ガスボンベ、61……同軸ケーブル状構造
体、62……中心導体、63……外部導体、64
……マイクロ波発信機、65……ポリ四フツ化エ
チレン多孔体チユーブ、66……端末構造物。
Figure 1 is an explanatory diagram showing a conventional membrane separation method for liquid mixtures, Figure 2 is an explanatory diagram of one embodiment of the present invention, Figure 3 is an explanatory diagram of another embodiment, and Figure 4 is an explanatory diagram of another embodiment.
The figure is a conceptual cross-sectional view of a plane perpendicular to the direction of liquid movement inside the container 25 of FIG. 3, and FIG. 5 shows a bag-shaped membrane with both ends sealed inside the container 25 of FIG. It is a sectional view arranged in a spiral shape. 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, 31... Hollow membrane with a fine diameter, 41... Membrane sealed at both ends to form a bag shape, 42... Space on one side of the membrane, 43... ...Space on the other surface side, 51...Storage tank, 52...Pump, 53
...Piping, 54...Cold trap, 55...
Nitrogen gas cylinder, 61... Coaxial cable-like structure, 62... Center conductor, 63... Outer conductor, 64
... Microwave transmitter, 65 ... Polytetrafluoroethylene porous tube, 66 ... Terminal structure.

Claims (1)

【特許請求の範囲】[Claims] 1 マイクロ波電磁場を印加する部分と、該電磁
場内に液相と気相とを区画する如く設けた膜と、
該膜を通して気相側に透過してくる液相成分を冷
却する部分とからなる装置であつて、前記マイク
ロ波電磁場を印加する部分が、同軸状に設けられ
た外部導体と中心(内部)導体とから構成され、
前記二つの導体の間にマイクロ波電磁場を印加す
るものであるか又は、マイロク波を放射する部分
と放射されたマイクロ波の伝播空間として働く導
体に囲まれた空間とを有するものであることを特
徴とする液体分離装置。
1. A part to which a microwave electromagnetic field is applied, a membrane provided within the electromagnetic field to partition a liquid phase and a gas phase,
A device that includes a part that cools the liquid phase component that permeates through the membrane to the gas phase side, and the part that applies the microwave electromagnetic field has an outer conductor and a center (inner) conductor that are coaxially provided. It consists of
A microwave electromagnetic field is applied between the two conductors, or a microwave-emitting part and a space surrounded by the conductor serve as a propagation space for the emitted microwaves. Characteristic liquid separation equipment.
JP20578283A 1983-11-04 1983-11-04 Liquid separating apparatus Granted JPS6099311A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20578283A JPS6099311A (en) 1983-11-04 1983-11-04 Liquid separating apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20578283A JPS6099311A (en) 1983-11-04 1983-11-04 Liquid separating apparatus

Publications (2)

Publication Number Publication Date
JPS6099311A JPS6099311A (en) 1985-06-03
JPH0341205B2 true JPH0341205B2 (en) 1991-06-21

Family

ID=16512579

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20578283A Granted JPS6099311A (en) 1983-11-04 1983-11-04 Liquid separating apparatus

Country Status (1)

Country Link
JP (1) JPS6099311A (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5895503A (en) * 1981-11-25 1983-06-07 Nitto Electric Ind Co Ltd Solution separating pipe
JPS5895518A (en) * 1981-11-27 1983-06-07 Nitto Electric Ind Co Ltd Solution separating device

Also Published As

Publication number Publication date
JPS6099311A (en) 1985-06-03

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