JPS6125403B2 - - Google Patents
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- Publication number
- JPS6125403B2 JPS6125403B2 JP11972777A JP11972777A JPS6125403B2 JP S6125403 B2 JPS6125403 B2 JP S6125403B2 JP 11972777 A JP11972777 A JP 11972777A JP 11972777 A JP11972777 A JP 11972777A JP S6125403 B2 JPS6125403 B2 JP S6125403B2
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- JP
- Japan
- Prior art keywords
- liquid
- solid
- pressure
- phase
- pressure container
- Prior art date
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- Expired
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- 239000007788 liquid Substances 0.000 claims description 63
- 239000007787 solid Substances 0.000 claims description 33
- 238000000034 method Methods 0.000 claims description 25
- 238000000926 separation method Methods 0.000 claims description 17
- 238000007906 compression Methods 0.000 claims description 16
- 230000006835 compression Effects 0.000 claims description 16
- 239000007791 liquid phase Substances 0.000 claims description 15
- 239000007790 solid phase Substances 0.000 claims description 15
- 239000013078 crystal Substances 0.000 claims description 11
- 239000012452 mother liquor Substances 0.000 claims description 10
- 239000000463 material Substances 0.000 claims description 7
- 239000000155 melt Substances 0.000 claims description 7
- 238000000605 extraction Methods 0.000 claims 1
- 238000002844 melting Methods 0.000 description 14
- 230000008018 melting Effects 0.000 description 14
- 230000007423 decrease Effects 0.000 description 9
- 239000000126 substance Substances 0.000 description 9
- 239000000203 mixture Substances 0.000 description 8
- 230000009466 transformation Effects 0.000 description 7
- 239000012535 impurity Substances 0.000 description 6
- 230000000694 effects Effects 0.000 description 4
- IWDCLRJOBJJRNH-UHFFFAOYSA-N p-cresol Chemical compound CC1=CC=C(O)C=C1 IWDCLRJOBJJRNH-UHFFFAOYSA-N 0.000 description 4
- UHOVQNZJYSORNB-UHFFFAOYSA-N Benzene Chemical compound C1=CC=CC=C1 UHOVQNZJYSORNB-UHFFFAOYSA-N 0.000 description 3
- 230000005496 eutectics Effects 0.000 description 3
- 238000010438 heat treatment Methods 0.000 description 3
- AUHZEENZYGFFBQ-UHFFFAOYSA-N mesitylene Substances CC1=CC(C)=CC(C)=C1 AUHZEENZYGFFBQ-UHFFFAOYSA-N 0.000 description 3
- 125000001827 mesitylenyl group Chemical group [H]C1=C(C(*)=C(C([H])=C1C([H])([H])[H])C([H])([H])[H])C([H])([H])[H] 0.000 description 3
- 238000003825 pressing Methods 0.000 description 3
- GWHJZXXIDMPWGX-UHFFFAOYSA-N 1,2,4-trimethylbenzene Chemical compound CC1=CC=C(C)C(C)=C1 GWHJZXXIDMPWGX-UHFFFAOYSA-N 0.000 description 2
- 238000002425 crystallisation Methods 0.000 description 2
- 230000008025 crystallization Effects 0.000 description 2
- 239000000374 eutectic mixture Substances 0.000 description 2
- 238000009413 insulation Methods 0.000 description 2
- RLSSMJSEOOYNOY-UHFFFAOYSA-N m-cresol Chemical compound CC1=CC=CC(O)=C1 RLSSMJSEOOYNOY-UHFFFAOYSA-N 0.000 description 2
- KXGFMDJXCMQABM-UHFFFAOYSA-N 2-methoxy-6-methylphenol Chemical compound [CH]OC1=CC=CC([CH])=C1O KXGFMDJXCMQABM-UHFFFAOYSA-N 0.000 description 1
- 229910000831 Steel Inorganic materials 0.000 description 1
- 230000002411 adverse Effects 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 238000005056 compaction Methods 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 238000011109 contamination Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 230000006837 decompression Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000007599 discharging Methods 0.000 description 1
- 229920001971 elastomer Polymers 0.000 description 1
- 238000001914 filtration Methods 0.000 description 1
- 239000010419 fine particle Substances 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 239000011259 mixed solution Substances 0.000 description 1
- 238000002156 mixing Methods 0.000 description 1
- 239000011368 organic material Substances 0.000 description 1
- 239000012071 phase Substances 0.000 description 1
- 238000010587 phase diagram Methods 0.000 description 1
- 229920001568 phenolic resin Polymers 0.000 description 1
- 239000005011 phenolic resin Substances 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 238000011084 recovery Methods 0.000 description 1
- 238000004062 sedimentation Methods 0.000 description 1
- 239000006104 solid solution Substances 0.000 description 1
- 239000000243 solution Substances 0.000 description 1
- 239000002904 solvent Substances 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 239000011550 stock solution Substances 0.000 description 1
- 229920003002 synthetic resin Polymers 0.000 description 1
- 239000000057 synthetic resin Substances 0.000 description 1
Landscapes
- Organic Low-Molecular-Weight Compounds And Preparation Thereof (AREA)
Description
【発明の詳細な説明】
本発明は高圧力下に共存する固液から固体成分
を高純度に分離する方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for separating solid components from coexisting solid and liquid under high pressure with high purity.
かねてより本発明者らは、高圧力下における物
質分離法の研究を展開してきたが、高圧力下での
晶析操作によつて得られた固液共存状態から、高
純度且つ効果的に固体を分離してこれを精製する
方法については、幾つかの問題があることを知つ
た。 The present inventors have been conducting research on methods for separating substances under high pressure for some time, and have found that solid-liquid coexistence states obtained through crystallization operations under high pressure can be used to effectively separate solids with high purity. I learned that there are several problems with the method of separating and purifying this.
例えば第1図は2成分単純共晶系混合物の固液
状態図で、線1は純成分x1の固液変態を示し、線
2はx1及びx2の共晶成分の固液変態を示す。そし
てA,A′,A″の各点は、特定成分x1の固相と、
成分x1,x2からなる混合母液の共存点であり、以
下この図に基づいて問題点の所在を明らかにす
る。 For example, Figure 1 is a solid-liquid phase diagram of a two-component simple eutectic mixture, where line 1 shows the solid-liquid transformation of pure component x 1 , and line 2 shows the solid-liquid transformation of the eutectic components x 1 and x 2 . show. And each point A, A′, A″ is a solid phase of specific component x 1 ,
This is the coexistence point of the mixed mother liquor consisting of components x 1 and x 2 , and the location of the problem will be clarified below based on this figure.
今仮に、A′点或はその近傍において晶析操作
が完了し、A′点において固液が完全に1次分離
されたとする。分離された固体は、いずれは大気
圧中に取出すことが必要であるが、最初の減圧に
よつて純成分x1の変態線1上のB′点に達する。こ
の過程では固体が膨張し、膨張熱による若干の冷
却はあるが、特に重大な影響はないので便宜上説
明を省略する。引続き減圧していくと、変態線1
に沿つて降圧しながらE点に向うと共に、結晶が
順次融解し始める。この段階では結晶の融解によ
る潜熱と、融解した液相の膨張に伴なう内部エネ
ルギーの増加の為、温度は急激に降下する。E点
で全量が融解すると、後は液体の膨張に伴なう因
子のみで徐々に降温する。尚、Tmは大気圧下に
おける純成分x1の融点である。 Suppose now that the crystallization operation is completed at or near point A', and the solid-liquid is completely primary separated at point A'. The separated solid must eventually be taken out to atmospheric pressure, but by the initial pressure reduction it reaches point B' on the transformation line 1 of pure component x 1 . In this process, the solid expands, and although there is some cooling due to the heat of expansion, there is no particularly significant effect, so the explanation will be omitted for the sake of convenience. As the pressure continues to decrease, the transformation line 1
As the pressure decreases along the direction toward point E, the crystals begin to melt one after another. At this stage, the temperature drops rapidly due to latent heat due to melting of the crystal and increase in internal energy due to expansion of the molten liquid phase. When the entire amount melts at point E, the temperature gradually decreases only due to the expansion of the liquid. Note that Tm is the melting point of pure component x 1 under atmospheric pressure.
これに対しA点やA″点で固液の分離が行なわ
れたときには、この固相を大気圧中に解放しても
全量融解することはない。例えばA点から減圧を
開始したとすると、B点に至つて融解が開始され
以下前と同様に融解と共に降圧・降温するが、す
ぐに融点Tmに到達するので、融解の進行が停止
する。もしA点における固液分離が不十分である
と、結晶の一部は降圧と共に一部融解する効果が
潜熱として表われ降温量が大きくなり、C点に至
り、更に降圧・降温するが、不純物が混入してい
る為融点Tmより低い温度に達した時点で融解の
進行が停止する。A点における固液分離が更に不
十分であると、純成分x1の固液変態線1に達する
ことなく、一部融解をしながら融点Tmより低い
D点に至つて融解が停止する。この様にA点から
出発するときは固相の全部を融解させることがで
きず、しかも製品の純度は極めて低いものにな
る。又A″から出発する場合にこの傾向が更に顕
著になることについては、格別の説明を要する迄
もなく自明である。 On the other hand, when solid-liquid separation is performed at point A or A'', even if this solid phase is released into atmospheric pressure, the entire amount will not melt.For example, if pressure reduction is started from point A, Melting begins when it reaches point B, and the pressure and temperature decrease as it melts as before, but the melting point Tm is quickly reached, so the progress of melting stops.If solid-liquid separation at point A is insufficient Then, as the pressure decreases, part of the crystal melts, which appears as latent heat, and the amount of temperature decrease increases, reaching point C, and the pressure and temperature decrease further, but due to the inclusion of impurities, the temperature becomes lower than the melting point Tm. When the solid-liquid separation at point A is insufficient, the solid-liquid transformation line 1 of pure component Melting stops when reaching point D. In this way, when starting from point A, it is not possible to melt all of the solid phase, and the purity of the product is extremely low. Also, when starting from point A'' It is self-evident that there is no need for special explanation that this tendency becomes even more pronounced.
一般に減圧に伴なう温度の低下は、現象として
は様々な形態をとり得るが、断熱的に減圧する場
合の温度降下量は非常に大きく、多くの有機物質
を固体から液体に融解するときの温度降下量は、
70〜150℃にも及ぶ。従つて前記説明において、
高純度の特定成分結晶を減圧操作のみで全量融解
させる為には、例えばB′点−E点間が70〜150℃
の温度差を有している場合でなければならない。
又多くの有機物質における変態圧力の温度依存性
(線1の勾配)は、30〜60Kg/cmであるから、B′点
−E点間の温度差が100℃であるとすると、B′点
−E点間の圧力差は3000〜6000Kg/cm2でなければ
ならない。しかも実際に固液分離を行なうときの
圧力は、これよりも更に数百〜数千気圧高くなる
ことが多く、結局減圧操作のみによつて固体の全
量を融解する為には、A′点を極めて高い圧力に
しなければならない。 In general, the temperature drop that accompanies depressurization can take various forms, but the amount of temperature drop when depressurizing adiabatically is extremely large, and is similar to that when many organic substances are melted from solid to liquid. The amount of temperature drop is
The temperature ranges from 70 to 150℃. Therefore, in the above explanation,
In order to melt the entire amount of high-purity specific component crystals only by reducing pressure, for example, the temperature between point B' and point E must be 70 to 150℃.
It must be the case that there is a temperature difference of
Also, the temperature dependence of transformation pressure (slope of line 1) in many organic materials is 30 to 60 kg/cm, so if the temperature difference between point B' and point E is 100°C, point B' -The pressure difference between points E must be between 3000 and 6000 Kg/ cm2 . Moreover, the pressure when actually performing solid-liquid separation is often several hundred to several thousand atmospheres higher than this, and in the end, in order to melt the entire amount of solid only by depressurizing operation, it is necessary to reach point A′. The pressure must be extremely high.
しかるにこの様な高圧力操作を行なう為には、
特別の高圧力装置が必要になり、汎用性とい点で
問題がある。そこでそれ程の高圧力操作を行なわ
ず、減圧過的中に高圧力容器内で加熱融解させる
ことも考えられる。しかしその為には高圧力容器
内に熱交換器を置いたり高圧容器装置の加熱装置
が必要になつたりするが、前者の場合には固液分
離作業例えば圧搾分離が困難になるし、特に後者
の場合は厚肉の鋼製容器を加熱することになるの
で熱効率及び時間効率が悪くなる。又いずれの場
合にしても設備費が高騰するし、融解液排出後次
回の操作を行なう前に高圧容器を再冷却する必要
が生じ、一層非能率的である。この他該特定成分
と同一の物質或は適当な溶媒を加熱して高圧力容
器に注入して固体の融解乃溶融解を促進する方法
も考えられないではない。しかし熱的損失はかな
り大きいものであり、根本的な解決策とは言い難
い。 However, in order to perform such high pressure operation,
This requires a special high-pressure device, which poses a problem in terms of versatility. Therefore, it may be possible to heat and melt the material in a high-pressure container during depressurization without performing such a high-pressure operation. However, this requires a heat exchanger placed inside the high-pressure vessel or a heating device for the high-pressure vessel, but in the former case, solid-liquid separation, such as compression separation, becomes difficult, and the latter is especially difficult. In this case, a thick steel container must be heated, resulting in poor thermal efficiency and time efficiency. In either case, equipment costs increase, and the high-pressure vessel must be re-cooled after discharging the melt before the next operation, making it even more inefficient. In addition, it is not impossible to consider a method in which the same substance as the specific component or a suitable solvent is heated and injected into a high-pressure container to promote melting or melting of the solid. However, the thermal loss is quite large, so it is difficult to call this a fundamental solution.
本発明はこの様な考察に立つてなされたもので
あり、高圧力下に存在する固液混合物から、固体
を高純度且つ効果的に取出す方法を提供しようと
するものである。即ち本発明の構成は、少なくと
も1成分又はそれ以上の特定成分の結晶と、該特
定成分と他成分との混合母液とが、高圧力下にお
いて固液共存状態にあるときに、この特定成分を
固体のまま分離精製する方法であつて、まず高圧
力下に存在する固液共存物を圧搾することによつ
て液体のみを高圧容器外に放出し、高圧容器内の
圧力を下げることによつて高圧容器内に残されて
いる結晶状特定成分の一部を融解して固液共存状
態とし、該固液共存物を圧搾することによつて液
体のみを高圧容器外に放出し、残された固体は高
圧容器を開放することによつて系外に取出すこと
を要旨とするものである。 The present invention has been made based on such considerations, and it is an object of the present invention to provide a method for efficiently extracting solids with high purity from a solid-liquid mixture existing under high pressure. That is, the structure of the present invention is such that when crystals of at least one or more specific components and a mixed mother liquor of the specific component and other components are in a solid-liquid coexistence state under high pressure, this specific component is This is a method of separating and purifying the solid as it is. First, by squeezing the solid-liquid coexistence that exists under high pressure, only the liquid is released outside the high-pressure container, and then by lowering the pressure inside the high-pressure container. A part of the crystalline specific component left in the high-pressure container is melted to form a solid-liquid coexistence state, and by squeezing the solid-liquid coexistence, only the liquid is released outside the high-pressure container, and the remaining The idea is to remove the solids from the system by opening the high-pressure container.
まず高圧力下における固液共存状態の形成方法
であるが、その手段は本発明を制限するものでは
ない。しかし一般的には、常圧下全量液相又は大
部分液相である2成分又はそれ以上の成分からな
る混合物を適当な温度で加圧することによつて得
られたものが好ましい。又この加圧中の温度制御
も任意であり、要は高圧下において前記混合物が
固液共存状態を呈するものである限り全て本発明
の方法が適用できる。 First, there is a method for forming a solid-liquid coexistence state under high pressure, but this method does not limit the present invention. However, in general, it is preferable to use a mixture obtained by pressurizing a mixture of two or more components, which are entirely in liquid phase or mostly in liquid phase, at an appropriate temperature under normal pressure. Further, temperature control during this pressurization is also optional, and the method of the present invention can be applied to any method as long as the mixture exhibits a solid-liquid coexistence state under high pressure.
本発明の第1工程は、前記固液混合物から固液
を1次分離することによつて行なわれる。この1
次分離は勿論高圧容器(高圧配管その他を含む、
以下同じ)中で行なわれ、具体的には過、圧
搾、沈降、等の各分離手段が例示できる。この工
程では固液を完全に分離する必要はなく、任意の
手段による粗分離でも差支えないが、前記考察か
らも理解できる様に固液の分離が完全である程、
以後の工程を理論的に展開させることが容易にな
るので、圧搾法によつて可及的十分な固液分離を
行なうことが推奨される。もつとも圧搾法には限
界があるので、本発明の場合においても第1図A
−C、A−Dの如き経緯で降圧・降温が進行する
ことは当然である。尚第2図は本発明の実施に使
用される装置の一例で、高圧容器3の内面には、
必要に応じて断熱層5が形成され、上下には油圧
駆動のピストン1,2が装着されている。6,
7,8は圧搾液抜取用のパイプで、夫々には逆止
バルブ6a,7a,8aが配設される。尚ピスト
ン2については、高圧容器3に固定される下プラ
グに代えてもよい。又4は固液共存物であつて、
もちろん高圧下に保持されている。従つて本工程
の圧搾を行なうにあたつては、ピストン1及び/
又は2を作動して固液共存物4の圧搾を行なう
が、分離された液はパイプ6,7,8を通つて系
外に排出される。 The first step of the present invention is carried out by first separating solid-liquid from the solid-liquid mixture. This one
Of course, the next separation is a high-pressure vessel (including high-pressure piping, etc.)
The same applies hereinafter), and specific examples include filtration, compression, sedimentation, and the like. In this step, it is not necessary to completely separate the solid-liquid, and rough separation by any means is acceptable, but as can be understood from the above discussion, the more complete the solid-liquid separation is, the more
It is recommended to perform as much solid-liquid separation as possible by the squeezing method, as this makes it easier to develop the subsequent steps theoretically. However, since there are limits to the compression method, even in the case of the present invention, Fig. 1A
It is natural that the pressure and temperature decrease proceed as shown in -C and A-D. FIG. 2 shows an example of the apparatus used to carry out the present invention, and the inner surface of the high-pressure container 3 is
A heat insulating layer 5 is formed as required, and hydraulically driven pistons 1 and 2 are mounted on the upper and lower sides. 6,
Reference numerals 7 and 8 are pipes for extracting compressed liquid, and check valves 6a, 7a, and 8a are provided respectively. Note that the piston 2 may be replaced with a lower plug fixed to the high pressure container 3. Further, 4 is a solid-liquid coexistence substance,
Of course, it is held under high pressure. Therefore, when performing the compression in this step, the piston 1 and/or
or 2 is operated to compress the solid-liquid coexistence material 4, and the separated liquid is discharged to the outside of the system through pipes 6, 7, and 8.
次に本発明の第2工程として、高圧容器内が減
圧される。このときの到達圧力は第1図の説明か
ら容易に理解できる様に1で示された固液平衡圧
力以下の圧力であり、下限は大気中に至る。その
結果特定成分の結晶は一部融解され、固体表面に
付着し、或は結晶間の隙間に巻込まれていた液体
不純物は融解液によつて洗浄除去されると共に、
残された固体は自からの融解液に覆われた状態に
なつて汚染から防止されるので、高純度の固体が
得られる。 Next, as the second step of the present invention, the pressure inside the high-pressure container is reduced. As can be easily understood from the explanation of FIG. 1, the ultimate pressure at this time is below the solid-liquid equilibrium pressure indicated by 1, and the lower limit reaches the atmosphere. As a result, the crystals of the specific component are partially melted, and the liquid impurities that have adhered to the solid surface or are caught in the gaps between the crystals are washed away by the melt, and
The remaining solid is covered with its own melt and is protected from contamination, resulting in a highly pure solid.
本工程の実施態様については種々考えられ、特
許請求の範囲に記載したものはその一例に過ぎな
いが、代表的な方法は、圧力を連続的又は段階的
に除々に減じ、生じた融解液を逐次分離する方法
である。従つて高圧容器内における圧力降下は瞬
間的に行なわれるのではなく且つ融解液はその都
度固液共存系より排除されるので、融解液の膨張
熱による降温効果が少ない。しかもこの融解液は
不純液を伴なつてその都度除去されているから不
純液の除去効果が極めて高く、特定成分結晶の不
純物による融点降下も少ない。この様な次第であ
るから、逐次減圧の任意の段階で少なくとも1回
の圧搾を行なつて固液分離を十分に行なうことが
推奨される。この圧搾によつて液相の除去を十分
に行なうと、金属やセラミツク等の粉末成形(メ
カニカルプレスやラバープレス等)における如く
特定物質の多結晶微粒子が圧搾され、巨大なブロ
ツク状固晶が得られる。 Various embodiments of this process can be considered, and the one described in the claims is just one example, but a typical method is to gradually reduce the pressure continuously or stepwise and remove the resulting melt. This is a method of sequential separation. Therefore, the pressure drop in the high-pressure container does not occur instantaneously, and the molten liquid is removed from the solid-liquid coexistence system each time, so that the temperature-lowering effect due to the heat of expansion of the molten liquid is small. Moreover, since this melt is removed each time along with the impurity liquid, the effect of removing the impurity liquid is extremely high, and the melting point drop due to impurities in the specific component crystals is also small. Because of this, it is recommended to perform compression at least once at any stage of sequential pressure reduction to sufficiently perform solid-liquid separation. When the liquid phase is sufficiently removed by this compression, the polycrystalline fine particles of the specific substance are compressed, as in the case of powder compaction of metals, ceramics, etc. (mechanical press, rubber press, etc.), and huge block-shaped solid crystals are obtained. It will be done.
一般にこの様な圧搾は、高圧域で行なう程固相
の回収効率が高まり、低圧域である程固相の純度
が高まりしかも大気圧に開放したときの固相ブロ
ツクが強固になる。従つて段階的又は連続的減圧
の過程における圧搾は数多く行なうことが望まし
く、段階的減圧の都度又は連続的減圧に連動して
圧搾すれば更に望ましい効果が得られる。 In general, the higher the pressure range is used for such compression, the higher the recovery efficiency of the solid phase, and the lower the pressure range, the higher the purity of the solid phase, and the stronger the solid phase block when released to atmospheric pressure. Therefore, it is desirable to perform many compressions in the process of stepwise or continuous pressure reduction, and more desirable effects can be obtained if compression is performed each time stepwise or in conjunction with continuous pressure reduction.
ここに言う圧搾の程度は、固液共存相における
平均的圧力と排出液相の圧力との差で表わされる
べきであり、多くの場合は数十乃至数百気圧、時
には1000気圧以上の圧力によつて良好な結果が得
られる。 The degree of squeezing referred to here should be expressed as the difference between the average pressure in the solid-liquid coexistence phase and the pressure in the discharged liquid phase, and in most cases the pressure is tens to hundreds of atmospheres, sometimes over 1000 atmospheres. Therefore, good results can be obtained.
以上の如くして得られたブロツク状固体は、最
終的に大気圧又はその近傍の圧力に迄減圧され、
その後高圧容器を開放して取出されるが、取出し
直前に再び圧搾して固液を分離したり、取出し後
の自然融解液や積極的加熱による一部融解後の圧
搾分離を行なえば更に高純度の固体を得ることが
できる。特に大気圧への減圧後の圧搾は、断熱層
背面、ピストンと容器の間隙等に圧縮された淀み
部分の母液の圧力が開放されるので、この淀み部
分に残置していた液相を分離除去するうえで効果
的である。もつともこの不純液相は、高圧容器か
ら固体を取出す前にガス体で流出せしめることも
可能であるから、前記圧搾は必ずしも不可欠の工
程ではない。このような、ガス体による分離は、
すでに圧搾によつて固体がブロツク状となつてい
る時点では、前記淀み部分の残置母液の分離及び
ブロツク表面の融解母液の除去に効果的である。
更にこの時ブロツク状固相を圧搾することによつ
て、減圧による融解量を最少に押えられる。ガス
体は、なるべく混合物の成分と反応しないもので
あることが好ましい。通常、数気圧、時には10気
圧以上のガス体を上方から流し又は、残置母液と
置換する。残置母液を真空置換することは格別な
事ではない。 The block-shaped solid obtained as described above is finally depressurized to atmospheric pressure or a pressure close to it, and
After that, the high-pressure container is opened and taken out, but the purity can be further improved by squeezing again just before taking out to separate the solid and liquid, or by pressing and separating the natural melt after taking out or after partially melting by active heating. can be obtained as a solid. In particular, during compression after decompression to atmospheric pressure, the pressure of the mother liquor in the stagnation area compressed at the back of the insulation layer, the gap between the piston and the container, etc. is released, so the liquid phase remaining in this stagnation area is separated and removed. It is effective in doing so. However, this squeezing is not necessarily an essential step, since this impure liquid phase can also be forced out as a gas before the solid is removed from the high-pressure vessel. This kind of separation by gas is
At the time when the solid has already become a block by compression, it is effective to separate the mother liquor remaining in the stagnation portion and to remove the molten mother liquor on the surface of the block.
Furthermore, by squeezing the block solid phase at this time, the amount of melting due to reduced pressure can be minimized. It is preferable that the gas is one that does not react with the components of the mixture. Usually, a gas of several atmospheres, sometimes 10 atmospheres or more, is flowed from above or replaced with the remaining mother liquor. There is nothing special about replacing the remaining mother liquor in a vacuum.
又上記の減圧や圧搾による固液分離或は固体の
取出し操作は、高圧容器と内部被処理物の間の熱
交換を断つた状態で処理することによつて一層効
果あらしめることができる。即ち減圧によつて内
部被処理物の温度が低下すると、高圧容器との間
に温度差が生じるが、その結果高圧容器側からの
熱の流入が生じると、高純度の固相が必要以上に
融解するし、高圧容器自体の温度が低下して次サ
イクルに悪影響を与えることもある。これに対し
断熱層を形成しておくと、固相の融解は外部条件
の影響から遮断され、工業的には実質上圧力管理
のみで操業を制御することが可能になり、高圧容
器内の均一性、条件伝播の均一性という圧力操作
の利点を有意義に享受することができる。尚この
様な断熱層としては、例えばフエノール樹脂等の
如き合成樹脂が小熱容量物質として推奨される
が、当然ながら断熱層の存否及び材質は本発明を
制限するものではない。 Further, the above solid-liquid separation or solid removal operation by reducing pressure or squeezing can be made more effective by performing the treatment in a state where heat exchange between the high-pressure container and the internal object to be treated is cut off. In other words, when the temperature of the internal processed material decreases due to depressurization, a temperature difference occurs between it and the high-pressure container, but as a result, when heat flows in from the high-pressure container side, the high-purity solid phase becomes more concentrated than necessary. It will melt, and the temperature of the high-pressure vessel itself may drop, adversely affecting the next cycle. On the other hand, if a heat insulating layer is formed, the melting of the solid phase will be blocked from the influence of external conditions, making it possible to virtually control the operation only by pressure management, and ensuring uniformity within the high-pressure vessel. The advantages of pressure manipulation such as uniformity and uniformity of condition propagation can be meaningfully enjoyed. As such a heat insulating layer, a synthetic resin such as phenolic resin is recommended as a material with a low heat capacity, but the presence or absence of the heat insulating layer and the material thereof are not intended to limit the present invention.
尚仮に、残存する固相を全量加熱融解させよう
とすると、例えば固相が50Kgのベンゼンである。
場合には、潜熱が30cal/gであるから、全部で
1500Kcal/50Kg必要であり、2KWのヒーターで
加熱しても理論的に75分間加熱しなければなら
ず、熱の流出温度勾配による熱伝導等を考慮すれ
ば更に長時間の加熱が必要になる。これに対し固
体をそのまま放出するとすればわずか1分程度も
あれば十分であり、その生産性に与える影響は頗
る大きい。 If one were to heat and melt the entire amount of the remaining solid phase, the solid phase would be, for example, 50 kg of benzene.
In this case, the latent heat is 30 cal/g, so the total
1500Kcal/50Kg is required, and even if heated with a 2KW heater, it would theoretically have to be heated for 75 minutes, and if heat conduction due to the heat outflow temperature gradient is taken into account, a longer heating time will be required. On the other hand, if the solid is to be discharged as it is, only about one minute is sufficient, and the impact on productivity is significant.
又更に、ブロツク状で取出された固体の表面
が、不純物を多量に含む液で、濡れている場合、
ブロツク状固体表面を熱風等で融解するだけで容
易に滴下分離しうる。以上の説明は、便宜上2成
分単純共晶系混合物の例を主として説明したが、
この方法は、多成分共晶系であつてもよく、又固
溶体系の混合物でもよい。又、特定成分は特定の
1物質に限らず、2物質の共晶体や分子間化合物
であつてもよい。要は、高圧下における固化又は
融解にともなつて、特定成分以外の成分が液相中
に濃縮又は稀釈される全ての混合物に適用できる
のである。 Furthermore, if the surface of the solid taken out in the form of a block is wet with a liquid containing a large amount of impurities,
Drop separation can be easily achieved by simply melting the block-shaped solid surface with hot air or the like. The above explanation mainly focused on the example of a two-component simple eutectic mixture for convenience.
This method may be a multi-component eutectic system or a mixture of solid solution systems. Further, the specific component is not limited to one specific substance, but may be a eutectic or an intermolecular compound of two substances. In short, it can be applied to all mixtures in which components other than specific components are concentrated or diluted in the liquid phase as they solidify or melt under high pressure.
以下本発明の実施例を説明する。 Examples of the present invention will be described below.
実施例 1
メシチレン(mp−44.8℃)に約10%のプソイ
ドクメン(mp−43.9℃)の混入した原液を加圧
して固液共存状態を得た。−13℃、1500気圧で母
液を圧搾分離し、1000気圧に下げてから更に母液
を圧搾分離した。次いで大気圧に戻し、約30秒後
にメシチレンの固体を回収した。この量は1000気
圧の下で分離したときの固体量の約50%であつた
が、その純度は99.9%を越えており、大気圧下で
分離除去されたメシチレンの液体は純度99.5%で
あつた。Example 1 A stock solution containing about 10% pseudocumene (mp-43.9°C) mixed with mesitylene (mp-44.8°C) was pressurized to obtain a solid-liquid coexistence state. The mother liquor was separated by pressing at -13°C and 1500 atm, and after the pressure was lowered to 1000 atm, the mother liquor was further separated by pressing. The pressure was then returned to atmospheric pressure, and solid mesitylene was collected after about 30 seconds. This amount was about 50% of the solid amount when separated under 1000 atmospheres, but its purity exceeded 99.9%, and the mesitylene liquid separated and removed under atmospheric pressure had a purity of 99.5%. Ta.
実施例 2
m−クレゾールとp−クレゾールの混合液(混
合比20:80)を40℃で2000気圧にして固液共存状
態とした。これを圧搾して固液分離し、残つた固
体を大気圧に戻すと30℃の固液共存物となつた。
これをただちに圧搾分離し、残つた固体(p−ク
レゾール)を高圧容器外に取出すと、2000気圧、
40℃の時点における圧搾による理論収量の80%で
あり、到達純度は99.5%であつた。Example 2 A mixed solution of m-cresol and p-cresol (mixing ratio 20:80) was heated to 2000 atm at 40°C to create a solid-liquid coexistence state. This was squeezed to separate solid and liquid, and when the remaining solid was returned to atmospheric pressure, it became a solid-liquid coexistence at 30°C.
When this is immediately compressed and separated and the remaining solid (p-cresol) is taken out of the high-pressure container, the pressure is 2000 atm.
The yield was 80% of the theoretical yield by compression at 40°C, and the purity achieved was 99.5%.
本発明は以上の如く構成されているので、高圧
下に存在する固液共存物から、固体物質を高純度
且つ好収率で取出すことが可能になつた。 Since the present invention is configured as described above, it has become possible to extract a solid substance with high purity and good yield from a solid-liquid coexistence material existing under high pressure.
第1図は固液共存物の分離を説明する為の固液
変態図、第2図は本発明の実施に利用される高圧
容器を概念的に示す断面図である。
1,2……ピストン、3……高圧容器、5……
断熱層。
FIG. 1 is a solid-liquid transformation diagram for explaining the separation of solid-liquid coexisting substances, and FIG. 2 is a cross-sectional view conceptually showing a high-pressure vessel used for carrying out the present invention. 1, 2... Piston, 3... High pressure vessel, 5...
insulation layer.
Claims (1)
の結晶と、該特定成分と他成分との混合母液と
が、高圧力下において固液共存状態にあるとき
に、この特定成分を分離精製する方法であつて、
まず高圧力下に存在する固液共存物を圧搾するこ
とによつて液体のみを高圧容器外に放出し、高圧
容器内の圧力を下げることによつて高圧容器内に
残されている結晶状特定成分の一部を融解して固
液共存状態とし、該固液共存物を圧搾することに
よつて液体のみを高圧容器外に放出し、残された
固体は高圧容器を開放することによつて系外に取
出すことを特徴とする固液分離法。 2 高圧容器外への最初の液体の放出後、高圧容
器内の圧力を下げるに当たり、圧力を連続的又は
段階的に徐々に減じて固体の一部を融解し、融解
液を逐次分離する特許請求の範囲第1項記載の方
法。 3 融解液の分離にあたつては、任意の段階で少
なくとも1回の圧搾を行なつて液相を分離する特
許請求の範囲第2項記載の方法。 4 少なくとも、高圧容器外への最初の液体の放
出以後の工程は、断熱層を設けた容器内で行なう
特許請求の範囲第1〜3項のいずれかに記載の方
法。 5 高圧容器から取出された固体を加熱し、一部
融解除去する特許請求の範囲第1〜4項のいずれ
かに記載の方法。 6 融解液の分離にあたつては、少なくとも1回
圧搾を行なつて液相を分離した後の固相を、該圧
搾前の処理圧より低い圧力に下げ、その表面にガ
ス体を流すことによつて液相を分離する特許請求
の範囲第1〜5項のいずれかに記載の方法。 7 融解液の分離にあたつては、少なくとも1回
圧搾を行なつて液相を分離した後の固相を、該圧
搾前の処理圧より低い圧力に下げ、次いで再び固
相に圧搾を加えつつその表面にガス体を流すこと
によつて液相を分離する特許請求の範囲第1〜5
項のいずれかに記載の方法。[Claims] 1. When crystals of at least one or more specific components and a mixed mother liquor of the specific component and other components are in a solid-liquid coexistence state under high pressure, A method of separating and purifying,
First, by squeezing the solid-liquid coexistence material existing under high pressure, only the liquid is released outside the high-pressure container, and by lowering the pressure inside the high-pressure container, the crystals remaining in the high-pressure container are isolated. A part of the components is melted to form a solid-liquid coexistence state, and only the liquid is released outside the high-pressure container by squeezing the solid-liquid coexistence, and the remaining solid is released by opening the high-pressure container. A solid-liquid separation method characterized by extraction from the system. 2. After the initial discharge of liquid outside the high-pressure container, the pressure within the high-pressure container is gradually reduced in a continuous or stepwise manner to melt a portion of the solid and successively separate the melted liquid. The method described in item 1. 3. The method according to claim 2, wherein in separating the molten liquid, compression is performed at least once at any stage to separate the liquid phase. 4. The method according to any one of claims 1 to 3, wherein at least the steps after the first discharge of liquid to the outside of the high-pressure container are performed in a container provided with a heat insulating layer. 5. The method according to any one of claims 1 to 4, wherein the solid taken out from the high-pressure container is heated and partially melted and removed. 6. When separating the molten liquid, the solid phase after the liquid phase has been separated by compression at least once is lowered to a pressure lower than the processing pressure before the compression, and a gaseous body is caused to flow on the surface of the solid phase. The method according to any one of claims 1 to 5, wherein the liquid phase is separated by. 7. When separating the melt, the solid phase is compressed at least once to separate the liquid phase, and then the pressure is lowered to lower than the processing pressure before the compression, and then the solid phase is compressed again. Claims 1 to 5, in which the liquid phase is separated by flowing a gaseous body over the surface of the liquid phase.
The method described in any of the paragraphs.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11972777A JPS5452677A (en) | 1977-10-04 | 1977-10-04 | Solid-liquid separating method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11972777A JPS5452677A (en) | 1977-10-04 | 1977-10-04 | Solid-liquid separating method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5452677A JPS5452677A (en) | 1979-04-25 |
| JPS6125403B2 true JPS6125403B2 (en) | 1986-06-16 |
Family
ID=14768620
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP11972777A Granted JPS5452677A (en) | 1977-10-04 | 1977-10-04 | Solid-liquid separating method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5452677A (en) |
-
1977
- 1977-10-04 JP JP11972777A patent/JPS5452677A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5452677A (en) | 1979-04-25 |
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