JPH03170592A - Working fluid - Google Patents
Working fluidInfo
- Publication number
- JPH03170592A JPH03170592A JP1311163A JP31116389A JPH03170592A JP H03170592 A JPH03170592 A JP H03170592A JP 1311163 A JP1311163 A JP 1311163A JP 31116389 A JP31116389 A JP 31116389A JP H03170592 A JPH03170592 A JP H03170592A
- Authority
- JP
- Japan
- Prior art keywords
- vapor
- working fluid
- liquid equilibrium
- weight
- line
- 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.)
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- 239000012530 fluid Substances 0.000 title claims abstract description 20
- RWRIWBAIICGTTQ-UHFFFAOYSA-N difluoromethane Chemical compound FCF RWRIWBAIICGTTQ-UHFFFAOYSA-N 0.000 claims abstract description 16
- NPNPZTNLOVBDOC-UHFFFAOYSA-N 1,1-difluoroethane Chemical compound CC(F)F NPNPZTNLOVBDOC-UHFFFAOYSA-N 0.000 claims abstract description 11
- UJPMYEOUBPIPHQ-UHFFFAOYSA-N 1,1,1-trifluoroethane Chemical compound CC(F)(F)F UJPMYEOUBPIPHQ-UHFFFAOYSA-N 0.000 claims abstract description 7
- 239000007788 liquid Substances 0.000 description 20
- 239000000203 mixture Substances 0.000 description 18
- 229920006395 saturated elastomer Polymers 0.000 description 15
- CBENFWSGALASAD-UHFFFAOYSA-N Ozone Chemical compound [O-][O+]=O CBENFWSGALASAD-UHFFFAOYSA-N 0.000 description 7
- 230000000694 effects Effects 0.000 description 6
- 238000001704 evaporation Methods 0.000 description 3
- 230000008020 evaporation Effects 0.000 description 3
- 230000005494 condensation Effects 0.000 description 2
- 238000009833 condensation Methods 0.000 description 2
- NBVXSUQYWXRMNV-UHFFFAOYSA-N fluoromethane Chemical compound FC NBVXSUQYWXRMNV-UHFFFAOYSA-N 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- 239000012808 vapor phase Substances 0.000 description 2
- 238000010792 warming Methods 0.000 description 2
- ZAMOUSCENKQFHK-UHFFFAOYSA-N Chlorine atom Chemical compound [Cl] ZAMOUSCENKQFHK-UHFFFAOYSA-N 0.000 description 1
- OTMSDBZUPAUEDD-UHFFFAOYSA-N Ethane Chemical class CC OTMSDBZUPAUEDD-UHFFFAOYSA-N 0.000 description 1
- 238000004378 air conditioning Methods 0.000 description 1
- 238000009835 boiling Methods 0.000 description 1
- 229910052801 chlorine Inorganic materials 0.000 description 1
- 239000000460 chlorine Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 150000008282 halocarbons Chemical class 0.000 description 1
- 230000001105 regulatory effect Effects 0.000 description 1
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明(よ エアコン・冷凍機等のヒートポンブ装置に
使用される作動流体に関すも
従来の技術
従来 エアコン・冷凍機等のヒートボンプ装置において
1よ 作動流体としてフロン類(以下R○○またはR○
○○と記す)と呼ばれるハロゲン化炭化水素が知られて
おり、利用温度としては凝縮温度および/または蒸発温
度が略O〜略50℃の範囲において通常使用されも 中
でもクロロジフルオロメタン(CHCIF*、R22)
は家庭用エアコン、ビル用エアコンや大型冷凍機等の作
動流体として幅広く用いられていも
発明が解決しようとする課題
しかしなが転 近年フロンによる戊層圏オゾン層破壊が
地球規模の環境問題となっており、或層圏オゾン破壊能
力が犬であるフロン類(以下、特定フロンと記す)につ
いてC戴 すでに国際条約によって使用量及び生産量
の規制がなされ さらに将来的には特定フロンの使用・
生産を廃止しようという動きがあも さて、R22はオ
ゾン破壊係数(トリクロロフルオロメタン(CCl*l
”)の底層圏オゾン破壊能力を1としたときの成層圏オ
ゾン破壊能九 以下ODPと記す)が0. 05と微少
であり、特定フロンではないものの将来的に使用量の増
大が予想され 冷凍・空調機器が広く普及した現&
R22の使用量及び生産量の増大が人類の生活環境に与
える影響も大きくなるものと予想されている。従って、
戊層圏オゾン破壊能力が小であるものQ 若干の破壊能
力があるとされるR22の代替となる作動流体の早期開
発も強く要望されている。[Detailed Description of the Invention] Industrial Application Fields of the Invention The present invention relates to working fluids used in heat pump devices such as air conditioners and refrigerators. as fluorocarbons (hereinafter referred to as R○○ or R○
Halogenated hydrocarbons known as R22)
Although it is widely used as a working fluid in home air conditioners, building air conditioners, and large refrigerators, the problem that the invention attempts to solve continues to change. The use and production of fluorocarbons (hereinafter referred to as specified fluorocarbons), which have a certain level of stratospheric ozone depletion ability, has already been regulated by international treaties.
Now, there is a movement to abolish production of R22.
The stratospheric ozone depletion potential 9 (hereinafter referred to as ODP) is as small as 0.05, and although it is not a specified fluorocarbon, its usage is expected to increase in the future. Nowadays, air conditioning equipment has become widespread and
It is expected that an increase in the amount of R22 used and produced will have a greater impact on the living environment of humankind. Therefore,
There is also a strong demand for the early development of a working fluid that can replace R22, which has a low ability to destroy stratospheric ozone.
本発明(よ 上述の問題に鑑みて試されたもので、戊層
圏オゾン層に及ぼす影響がほとんどなli< R22
の代替となる作動流体を提供するものであも課題を解決
するための手段
本発明は上述の課題を解決するた吹 少なくとL ジフ
ルオロメタン(CHI!F2)とトリフルオロエタン(
C2H * F − )とジフルオ口エタン(CaH
4F2)の三種のフロン類を含へ ジフルオロメタン0
〜略60重量米 トリフルオロエタン0〜略80重量米
ジフルオロエタン略20〜略65重量%の組戊範囲で
あることを特徴とするものであり、特に ジフルオロメ
タンO〜略50重量米トリフルオロエタン0〜略80重
量米 ジフルオロエタン略20〜略65重量%の組戊範
囲が望ましいものであも
作用
本発明(よ 上述の組合せによって、作動流体を、オゾ
ン破壊能力のほとんどなし\ 分子構造中に塩素を含ま
ないフロン類であるジフルオロメタン(ODP=0)、
トリフルオロエタン(○D P = 0)およびジフ
ルオロエタン(○DP=O)の混合物となすことにより
、戊層圏オゾン層に及ぼす影響をR22よりもさらに小
さく、ほ−とんどなくすることを可能とするものである
。又 本発明は上述の組戊範囲とすることによって、エ
アコン・冷凍機等のヒートポンプ装置の利用温度である
略0〜略50℃においてR22と同程度の蒸気圧を有し
R22の代替として現行機器で使用可能な作動流体を提
供することを可能とするものであも 従って上述の組合
せおよび組戒範囲における○DPも0と予想さ11..
R22の代替として極めて有望な作動流体となるもので
あa またかかる混合物は非共沸混合物となり、凝縮過
程および蒸発過程において温度勾配をもった△ 熱源流
体との温度差を近接させたロレンツサイクルを構或する
ことにより、R22よりも高い或績係数を期待できるも
のである。The present invention was tested in view of the above-mentioned problems, and has little effect on the stratospheric ozone layer.
SUMMARY OF THE INVENTION The present invention provides an alternative working fluid for solving the above-mentioned problems.
C2H*F − ) and difluoroethane (CaH
Contains three types of fluorocarbons (4F2) Difluoromethane 0
It is characterized by a composition range of about 60% by weight, trifluoroethane 0 to about 80% by weight, difluoroethane about 20% to about 65% by weight, particularly difluoromethane O to about 50% by weight trifluoroethane 0. A composition range of about 20 to about 65% by weight of difluoroethane is desirable. Difluoromethane (ODP=0), which is a fluorocarbon that does not contain
By forming a mixture of trifluoroethane (○DP=0) and difluoroethane (○DP=O), the effect on the stratospheric ozone layer is even smaller than that of R22, and it is possible to almost eliminate it. That is. Moreover, by adopting the above-mentioned assembly range, the present invention has a vapor pressure comparable to that of R22 at a temperature of about 0 to about 50 degrees Celsius, which is the usage temperature of heat pump devices such as air conditioners and refrigerators, and can be used as a substitute for R22 in current equipment. Therefore, it is expected that ○DP in the above combinations and combination ranges will also be 0. ..
It is a very promising working fluid as an alternative to R22.a Also, such a mixture becomes a non-azeotropic mixture, and has a temperature gradient in the condensation process and evaporation process. With this structure, a higher performance coefficient than R22 can be expected.
また一般に 戒層圏オゾン破壊能力があるフロン類(ヨ
その○DPの値の大きさにつれて地球温暖化の効果
も大きい傾向がある八 本発明による作動流体はODP
がOであるフロン類のみの三種以上から或る混合物によ
って構戊されているた敗地球温暖化の効果はR22と同
程度あるいはR22未満と推定され 最近世界的問題と
なっている地球温暖化への寄与を小とすることをも可能
とするものであも
実施例
以下、本発明による作動流体の実施例について、図を用
いて説明する。Additionally, in general, fluorocarbons (fluorocarbons), which have the ability to deplete stratospheric ozone, tend to have a greater global warming effect as their DP value increases.
The effect of global warming created by a certain mixture of three or more types of fluorocarbons, in which O is O, is estimated to be the same as or less than R22, and has recently become a worldwide problem. Embodiments Hereinafter, embodiments of the working fluid according to the present invention will be described with reference to the drawings.
図は ジフルオロメタン(R32)、 l,1,1−1
リフルオ口エタン(R143a)、 1. 1ジフル
オロエタン(R152a)の三種のフロン類の混合物に
よって構或される作動流体α定温度・一定圧力における
平衡状態を三角座標を用いて示したものである。本三角
座標においては三角形の各頂点に 上側頂点を基点とし
て反時計回りに沸点の低い順に単一物質を配置しており
、座標平面上のある点における各或分の組戒比(重量比
)(ヨ 点と三角形の各辺との距離の比で表される。The diagram shows difluoromethane (R32), l,1,1-1
Refluorinated ethane (R143a), 1. The equilibrium state of a working fluid α composed of a mixture of three types of fluorocarbons, 1 difluoroethane (R152a), at constant temperature and constant pressure is shown using triangular coordinates. In this triangular coordinate system, single substances are placed at each vertex of the triangle in a counterclockwise order starting from the upper vertex in descending order of boiling point, and the composition ratio (weight ratio) of each portion at a certain point on the coordinate plane is (Yo) It is expressed as the ratio of the distance between the point and each side of the triangle.
またこのとき、点と三角形の辺との距離Cヨ辺に相対す
る側にある三角座標の頂点に記された物質の組戊比に対
応ずも 図においてt Ct 温度0℃・圧力4.
0 4 4 kg/cm”Gにおける混合物の気液平
衡線であり、この温度・圧力はR22の飽和状態に相当
する。気液平衡線(R22 0℃相当)lの上側の線
は飽和気相線 気液平衡線(R22 0℃相当)1の
下側の線は飽和液相線を表わし この画線で挟まれた範
囲においては気液平衡状態となる。また2ζよ 温度5
0℃・圧力18. 782kg/cm2Gにおける混
合物の気液平衡線であり、この温度・圧力もR22の飽
和状態に相当すも 図からわかるよう4,:,R32、
R143a及びR152aがそれぞれ0〜略60重量%
. 0〜略80重量勉 略20〜略65重量%となるよ
うな組威範囲(よ 略0〜略50℃の利用温度において
R22とほぼ同等の蒸気圧を有するため望ましシチ
さらに R32、R143a及びRl52aがそれぞれ
0〜略50重量%. O〜略80重量勉 略20〜略6
5重量%となるような組戊範囲(よ O℃と50℃の間
のすべての利用温度においてR22とほぼ同等の蒸気圧
を有するため特に望ましい。Also, at this time, the distance C between the point and the side of the triangle does not correspond to the composition ratio of the substance written at the vertex of the triangular coordinates on the side opposite the side.
This is the vapor-liquid equilibrium line of the mixture at 0 4 4 kg/cm"G, and this temperature and pressure correspond to the saturated state of R22. The upper line of the vapor-liquid equilibrium line (corresponding to R22 0°C) is the saturated vapor phase. The line below the line Vapor-liquid equilibrium line (R22, equivalent to 0°C) 1 represents the saturated liquidus line, and the area between these lines is in a vapor-liquid equilibrium state.
0℃・Pressure 18. This is the vapor-liquid equilibrium line of the mixture at 782 kg/cm2G, and this temperature and pressure also correspond to the saturated state of R22.As can be seen from the figure, 4:, R32,
R143a and R152a are each 0 to approximately 60% by weight
.. 0 to approximately 80% by weight, and a composition range of approximately 20 to approximately 65% by weight.
Further, R32, R143a and Rl52a each contain 0 to about 50% by weight. O ~ Approximately 80 weight studies Approximately 20 ~ Approximately 6
5% by weight is particularly desirable since it has a vapor pressure approximately equal to that of R22 at all operating temperatures between 0°C and 50°C.
図中の点A1〜点F1における作動流体の組或を表に示
す。点A1〜点C+は気液平衡線(R2250℃相当)
2の飽和気相線上に 点D1〜点E1は気液平衡線(R
22 50℃相当)2の飽和液相線上にあり、共に気
液平衡線(R22 0℃相当)1の飽和気相線及び気
液平衡線(R22 0℃相当)1の飽和液相線の画線
で挟まれた範囲にあることから、温度O℃・圧力4.
044kg/cm2G(R22の飽和状態に相当)に
おいては気液平衡状態となる。また 点F1は気液平衡
線(R22 0℃相当)lの飽和液相線上にあると共
に気液平衡線(R22 50℃相当)2の飽和気相線
及び気液平衡線(R22 50℃相当)2の飽和液相
線の画線で挟まれた範囲にあることか板温度50℃・圧
力18. 782kg/cm2G(R22の飽和状態
に相当)においては気液平衡状態となる。従って、第1
表に示された組或を有する作動庵体(よ 0℃・50℃
におけるR22の飽和蒸気圧の条件下で飽和状態あるい
は気液平衡状態を実現し 略O〜略50℃の利用温度に
おいて、同温度におけるR22の飽和蒸気圧で操作する
ことにより、R22とほぼ等しい凝縮温度・蒸発温度を
得ることが可能となるものであも
ここで(上 気液平衡線(R22 0℃相当)lある
いは気液平衡線(R22 50℃相当)2上の点につ
いてのみ説明した力丈 点A+〜点F1の内側にある点
、すなわ板 温度O℃・圧力4.044kg/cm2G
及び温度50℃・圧力18.782kg/cm2G(両
者ともR22の飽和状態に相当)において気液平衡状態
となる組戒を有する作動流体についても同様に操作する
ことにより、略O〜略50℃の利用温度においてR22
とほぼ等しい凝縮温度・蒸発温度を得ることが可能とな
るものである。The working fluid combinations at points A1 to F1 in the figure are shown in the table. Points A1 to C+ are vapor-liquid equilibrium lines (equivalent to R2250°C)
On the saturated vapor phase line of 2, points D1 to E1 are on the vapor-liquid equilibrium line (R
22 is on the saturated liquidus line of 2 (equivalent to 50°C), and both are on the saturated vapor line of vapor-liquid equilibrium line (R22 equivalent to 0°C) 1 and the saturated liquidus line of vapor-liquid equilibrium line (R22 equivalent to 0°C) 1. Since it is within the range between the lines, the temperature is 0°C and the pressure is 4.
At 044 kg/cm2G (corresponding to the saturated state of R22), a gas-liquid equilibrium state is reached. In addition, point F1 is on the saturated liquidus line of the vapor-liquid equilibrium line (R22, equivalent to 0°C) 1, and the saturated vapor line and vapor-liquid equilibrium line (R22, equivalent to 50°C) of the vapor-liquid equilibrium line (R22, equivalent to 50°C) 2. The plate temperature is 50℃ and the pressure is 18. At 782 kg/cm2G (corresponding to the saturated state of R22), a gas-liquid equilibrium state is reached. Therefore, the first
Actuating body with the composition shown in the table (at 0°C and 50°C)
Achieving a saturated state or a vapor-liquid equilibrium state under the saturated vapor pressure of R22 in Although it is possible to obtain the temperature and evaporation temperature, here we explain only the points on the vapor-liquid equilibrium line (R22, equivalent to 0°C) 1 or the vapor-liquid equilibrium line (R22, equivalent to 50°C) 2. Length Point inside point A+ to point F1, strap plate Temperature 0℃, pressure 4.044kg/cm2G
By performing the same operation for a working fluid that has a gas-liquid equilibrium state at a temperature of 50°C and a pressure of 18.782 kg/cm2G (both correspond to the saturated state of R22), it is possible to R22 at usage temperature
This makes it possible to obtain condensation and evaporation temperatures that are approximately equal to .
本実施例においては作動流体は三種のフロン類の混合物
によって構或されている力支 構造異性体を含めて四種
以上のフロンの混合物によって作動流体を構戊すること
も勿論可能である。特に上述の組合せおよび組或範囲に
おける○DPも0と予想さh R22の代替として極
めて有望な作動流体となるものであも またかかる混合
物は非共沸混合物となり、凝縮過程および蒸発過程にお
いて温度勾配をもったべ 熱源流体との温度差を近接さ
せたロレンツサイクルを構戊することにより、R22よ
りも高い戊績係数を期待できるものであも
発明の効果
以上の説明から明らかなように 本発明(飄 作動流体
を、分子構造中に塩素を含まないフロン類のみの三種以
上から或る混合物となし その組戒範囲を特定したこと
により、
(1)底層圏オゾン層に及ぼす影響をR22よりもさら
に小さく、ほとんどなしとする作動流体の選択の幅を拡
大することが可能であも
(2)機器の利用温度においてR22と同程度の蒸気圧
を有L R22の代替として現行機器で使用可能であ
る。In this embodiment, the working fluid is composed of a mixture of three types of fluorocarbons.Of course, the working fluid can also be composed of a mixture of four or more types of fluorocarbons, including structural isomers. In particular, in the above-mentioned combinations and ranges, ○DP is also expected to be 0, making it a very promising working fluid as an alternative to R22. Although it is possible to expect a higher performance coefficient than R22 by constructing a Lorenz cycle in which the temperature difference between the heat source fluid and the heat source fluid is close to each other, the present invention (飄 The working fluid is a mixture of three or more types of fluorocarbons that do not contain chlorine in their molecular structure.By specifying the range of the combination, (1) the effect on the bottom ozone layer is greater than that of R22. Although it is possible to expand the range of selection of working fluids that are small and almost non-existent, (2) it has a vapor pressure similar to that of R22 at the operating temperature of the equipment, and can be used in current equipment as an alternative to R22. .
(3)非共沸混合物の温度勾配の性質を利用して、R2
2よりも高い戒績係数を期待できる等の効果を有するも
のである。(3) Taking advantage of the temperature gradient properties of non-azeotropic mixtures, R2
This has the effect that a higher precept coefficient can be expected than 2.
図は 三種のフロン類の混合物によって構或さl・・・
気液平衡線(R22 0℃相当)、2・気液平衡線(
R22 50℃相当)。The figure shows a structure made of a mixture of three types of fluorocarbons...
Vapor-liquid equilibrium line (R22 0℃ equivalent), 2. Vapor-liquid equilibrium line (
R22 equivalent to 50°C).
Claims (2)
エタン80重量%以下、ジフルオロエタン20〜65重
量%以下の少なくとも三種のフロン類を含む作動流体。(1) A working fluid containing at least three types of fluorocarbons: 60% by weight or less of difluoromethane, 80% by weight or less of trifluoroethane, and 20 to 65% by weight of difluoroethane.
エタン80重量%以下、ジフルオロエタン20〜65重
量%以下であることを特徴とする作動流体。(2) A working fluid characterized by containing 50% by weight or less of difluoromethane, 80% by weight or less of trifluoroethane, and 20 to 65% by weight of difluoroethane.
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1311163A JPH03170592A (en) | 1989-11-30 | 1989-11-30 | Working fluid |
KR1019900019595A KR930010515B1 (en) | 1989-11-30 | 1990-11-30 | Working fluid |
US08/125,146 US5433879A (en) | 1989-11-30 | 1993-09-23 | Working fluid containing difluoroethane |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1311163A JPH03170592A (en) | 1989-11-30 | 1989-11-30 | Working fluid |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH03170592A true JPH03170592A (en) | 1991-07-24 |
Family
ID=18013851
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1311163A Pending JPH03170592A (en) | 1989-11-30 | 1989-11-30 | Working fluid |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH03170592A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5232618A (en) * | 1991-09-30 | 1993-08-03 | E. I. Du Pont De Nemours And Company | Substantially constant boiling compositions of difluoromethane and trifluoroethane or perfluoroethane |
US5645754A (en) * | 1993-03-02 | 1997-07-08 | E. I. Du Pont De Nemours And Company | Compositions including a hexafluoroprpoane and dimethyl ether for heat transfer |
-
1989
- 1989-11-30 JP JP1311163A patent/JPH03170592A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5232618A (en) * | 1991-09-30 | 1993-08-03 | E. I. Du Pont De Nemours And Company | Substantially constant boiling compositions of difluoromethane and trifluoroethane or perfluoroethane |
US5788877A (en) * | 1991-09-30 | 1998-08-04 | E. I. Du Pont De Nemours And Company | Substantially constant boiling compositions of difluoromethane and trifluoroethane |
US5645754A (en) * | 1993-03-02 | 1997-07-08 | E. I. Du Pont De Nemours And Company | Compositions including a hexafluoroprpoane and dimethyl ether for heat transfer |
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