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JPS603147B2 - Refrigeration equipment - Google Patents
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JPS603147B2 - Refrigeration equipment - Google Patents

Refrigeration equipment

Info

Publication number
JPS603147B2
JPS603147B2 JP5871380A JP5871380A JPS603147B2 JP S603147 B2 JPS603147 B2 JP S603147B2 JP 5871380 A JP5871380 A JP 5871380A JP 5871380 A JP5871380 A JP 5871380A JP S603147 B2 JPS603147 B2 JP S603147B2
Authority
JP
Japan
Prior art keywords
passage
condenser
refrigerant
soot
flow rate
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
Application number
JP5871380A
Other languages
Japanese (ja)
Other versions
JPS56157770A (en
Inventor
晃 渥美
研作 小国
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP5871380A priority Critical patent/JPS603147B2/en
Publication of JPS56157770A publication Critical patent/JPS56157770A/en
Publication of JPS603147B2 publication Critical patent/JPS603147B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は空気調和機、チラーュニット等の冷凍装置に係
り、特に冷凍装置の凝縮器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a refrigeration system such as an air conditioner or a chiller unit, and particularly relates to a condenser of a refrigeration system.

第1図に従来の冷凍装置用凝縮器を示す。FIG. 1 shows a conventional condenser for refrigeration equipment.

この凝縮器は図示されていない圧縮機、減圧装置、蒸発
器等と共に冷凍装置が形成される。第1図において、1
は凝縮器、2はガス側へッダ、3は液側へッダ、4aは
複数本の通路のうち最上段速路の入口パイプ、5aは出
口パイプ、4nは複数本の通路のうち最下段通路の入口
パイプ、5nは出口パイプである。圧縮機(図示せず)
を出た袷煤はガス側へツダ2にて各冷煤通路に分流され
、凝縮器1内で凝縮し、過冷却液となって液側へッダ3
にて合流され、減圧装置(図示せず)へ流れる。上記構
造の凝縮器1の各通路に高低差がある場合、具体的には
図示のように最上段通蕗パイプ5aと最下段通路パイプ
5nの間に日(m)の高低差がある場合に、この高低差
別こ起因して各通路への冷煤流量が不均一となり凝縮器
1が有効に使用されないために結果的に凝縮圧力の上昇
、冷房能力の低下をまねし、てし、た。以下、この現象
について説明する。第2図は、冷媒通路の長さと冷媒圧
力の関係で、各通路に均一に冷媒が流れたとした場合の
説明図である。第2図では代表例として鮫上段通路と最
下段通路について示した。最上段遜路4a−5a(実線
)、最下段通路4n一5n(破線)とも、冷媒流量が同
一であるから冷煤圧力は凝縮器1内で管摩擦により@点
から■点へと同機に低下していく。
This condenser forms a refrigeration system together with a compressor, a pressure reducing device, an evaporator, etc. (not shown). In Figure 1, 1
is a condenser, 2 is a gas side header, 3 is a liquid side header, 4a is an inlet pipe of the highest speed passage among multiple passages, 5a is an outlet pipe, 4n is the highest of multiple passages. The inlet pipe of the lower passage, 5n is the outlet pipe. Compressor (not shown)
The soot that exits the gas side is diverted to each cold soot passage at the header 2, condenses in the condenser 1, becomes supercooled liquid, and is sent to the liquid side header 3.
and flows to a pressure reducing device (not shown). When there is a height difference between each passage of the condenser 1 having the above structure, specifically, when there is a height difference of days (m) between the uppermost passage pipe 5a and the lowermost passage pipe 5n as shown in the figure, Due to this difference in height, the flow rate of cold soot to each passage becomes uneven, and the condenser 1 is not used effectively, resulting in an increase in condensing pressure and a decrease in cooling capacity. This phenomenon will be explained below. FIG. 2 is an explanatory diagram when it is assumed that the refrigerant flows uniformly through each passage due to the relationship between the length of the refrigerant passage and the refrigerant pressure. FIG. 2 shows the shark upper passage and the lowermost passage as representative examples. Since the refrigerant flow rate is the same in both the top passage 4a-5a (solid line) and the bottom passage 4n-5n (broken line), the cold soot pressure changes from the @ point to the ■ point in the condenser 1 due to pipe friction. It continues to decline.

出口パイプ5a,5n部での圧力は■点で示され同じで
あるが、第1図に示す液へツダ3内の■部こ着目すると
、液へツドH×y(ここでyは液袷嬢の密度k9′で)
に相当する分だけ投下段通路の圧力が高くなり、第2図
で示す@点となる。この結果、ガス側へツダ2と液側へ
ッダ3の■」点の間の圧力差は液へツドによる分だけ各
通路で差が生じ、従って最上段通路の冷媒流量が多くな
るという不均一が生じる。第3図は前詑原因にて冷煤流
量の不均一が生じた場合の袷嬢通路長さと圧力の関係を
示すものであり、また第4図は、各通路の流量を示した
ものである。第3図で、最上段通路(実線)では、冷煤
流量が多いために凝縮器1内での管摩擦による圧力降下
が大きく■−■の様になり、液側へッグ3の■ではHy
だけ圧力が上昇し■点となる。一方、穣下段通路(破線
)では、冷嬢流量が少なく凝縮器1内での管摩擦による
圧力降下は小さく第3図で■−■点の様になる。この場
合、各通路への冷煤流量は、第4図に示す様に最上段が
最も多く、高さの低い通路ほど少なくなる。凝縮器内の
冷媒流量が少なくなると液冷煤が滞留しやすくなること
から、最下段通路内には液冷煤が滞留し、伝熱面積が有
効に利用できなくなる。この結果、凝縮圧力が上昇し「
冷房能力、成績係数の低下をまねく。本発明の目的は、
従来の欠陥を除去し、凝縮器の伝熱面積を有効に使用す
ることを目的とする。
The pressures at the outlet pipes 5a and 5n are indicated by points ``■'' and are the same, but if we focus on the ``■'' part in the liquid chamber 3 shown in FIG. (with the density of the lady k9')
The pressure in the drop stage passage increases by an amount corresponding to , and becomes the @ point shown in FIG. As a result, the pressure difference between the gas side header 2 and the liquid side header 3 at point 2 is different in each passage by the amount due to the liquid header, and therefore there is a problem that the refrigerant flow rate in the uppermost passage increases. Uniformity occurs. Figure 3 shows the relationship between the length of the slip passage and the pressure when the cold soot flow rate is uneven due to the previous cause, and Figure 4 shows the flow rate of each passage. . In Fig. 3, in the uppermost passage (solid line), the pressure drop due to pipe friction in the condenser 1 is large due to the large flow rate of cold soot, as shown by -■, and in the liquid side passage 3, the pressure drop is large. Hy
The pressure increases by the amount of time and reaches point ■. On the other hand, in the lower passageway (broken line), the flow rate of the refrigerant is small, and the pressure drop due to pipe friction in the condenser 1 is small, as shown by points ■-■ in FIG. In this case, as shown in FIG. 4, the flow rate of cold soot to each passage is highest in the uppermost stage, and decreases as the height of the passage decreases. When the refrigerant flow rate in the condenser decreases, liquid-cooled soot tends to accumulate, so liquid-cooled soot accumulates in the lowest passage, making it impossible to effectively utilize the heat transfer area. As a result, the condensation pressure increases and
This will lead to a decrease in cooling capacity and coefficient of performance. The purpose of the present invention is to
The purpose is to eliminate the deficiencies of the conventional technology and effectively use the heat transfer area of the condenser.

本発明の構成は、複数の冷媒通路を有する凝縮器におい
て、各通路長さを高位直に向うに従って順次長く形成し
たことを特徴とする。本発明の−実施例を第5図にもと
づき説明する。
The structure of the present invention is characterized in that, in a condenser having a plurality of refrigerant passages, the length of each passage is formed to be sequentially longer toward the higher level. An embodiment of the present invention will be described based on FIG.

図は凝縮器を示し、この凝縮器10は上部に位簿する冷
煤通路程通路長さが長く形成されている。上記構成の凝
縮器10では、ガス側へツダ12から袷煤通路の各入口
管4a,4b・・・・・・4nを経て各冷煤通路11a
,11b・・・・・・11nを流速する冷煤流量は凝縮
器出口の液側へツダ13にかかる液へッドH′により、
第6図に示すように最上段の通路11aが最も多く、下
方の冷煤通路11n程少ない。
The figure shows a condenser, and the condenser 10 is formed so that the cold soot passage located at the top has a longer passage length. In the condenser 10 having the above configuration, each cold soot passage 11a passes from the tube 12 to the gas side through each inlet pipe 4a, 4b...4n of the soot passage.
, 11b...11n, the flow rate of the cold soot is determined by the liquid head H' applied to the head 13 on the liquid side of the condenser outlet.
As shown in FIG. 6, the uppermost passage 11a has the largest number of passages, and the lower cold soot passages 11n have fewer passages.

この袷煤流量は通路長さ、熱交換量等にも影響される。
以上を考慮して各冷媒通路の長さを適当に選択する。即
ち、上部に位層する冷嬢遍路11a程長さを長く形成す
ることにより第7図に示すように各冷煤通路の凝縮器出
口側の冷煤温度が等しくなるような凝縮器が設計できる
。以上説明したように本発明によれば、複数の冷嬢通路
を有する凝縮器において、それぞれの凝縮器出口での冷
媒温度が等しくなり、凝縮器全体を有効に使用できる。
従って凝縮圧力の上昇、冷房能力あるいは暖房能力の不
足や成績係数の低下を防止することが可能となる。
The soot flow rate is also affected by the passage length, heat exchange amount, etc.
Considering the above, the length of each refrigerant passage is appropriately selected. That is, by forming the upper reijo pilgrimage 11a to be longer, it is possible to design a condenser in which the cold soot temperature on the condenser outlet side of each cold soot passage becomes equal, as shown in Fig. 7. . As explained above, according to the present invention, in a condenser having a plurality of cooling passages, the refrigerant temperature at each condenser outlet becomes equal, and the entire condenser can be used effectively.
Therefore, it is possible to prevent an increase in condensing pressure, a lack of cooling capacity or heating capacity, and a decrease in the coefficient of performance.

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

第1図は従来の凝縮器の構造図、第2図、第3図、第4
図は従来技術の作用説明図、第5図は本発明の一実施例
を示す凝縮器の構造図、第6図、第7図は第5図の凝縮
器の作用説明図である。 4a,4b,4n…・・・冷煤通路の入口管、5a,5
b,5n・・…・冷嬢通路の出口管、10・・・・・・
凝縮器、11a,11b,11n・・・・・・冷媒通路
、12・…・・ガス側へッダ、13・・・・・・液側へ
ッダ。 多‘図弟Z図 髪ヲ風 第4四 髪″ヲ皮l 務ら側 孫ワ図
Figure 1 is a structural diagram of a conventional condenser, Figures 2, 3, and 4.
FIG. 5 is a structural diagram of a condenser showing an embodiment of the present invention, and FIGS. 6 and 7 are explanatory diagrams of the operation of the condenser shown in FIG. 5. 4a, 4b, 4n...Inlet pipe of cold soot passage, 5a, 5
b, 5n...Exit pipe of cold treatment passage, 10...
Condenser, 11a, 11b, 11n...refrigerant passage, 12...gas side header, 13...liquid side header. Ta'tu younger brother Z figure wo style 4th hair ``wo skin l Tsutomu et al side grandson wa figure

Claims (1)

【特許請求の範囲】[Claims] 1 圧縮機、凝縮器、減圧装置、蒸発器を順次配管接続
して冷媒回路を形成し、上記凝縮器の冷媒通路を複数本
形成し、それぞれの冷媒通路長さを該通路が高位置に向
うに従って順次長くしたことを特徴とする冷凍装置。
1 A compressor, a condenser, a pressure reducing device, and an evaporator are sequentially connected via piping to form a refrigerant circuit, and a plurality of refrigerant passages for the condenser are formed, and the length of each refrigerant passage is set so that the passage points toward a higher position. A refrigeration device characterized in that the length is sequentially increased according to the following.
JP5871380A 1980-05-06 1980-05-06 Refrigeration equipment Expired JPS603147B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5871380A JPS603147B2 (en) 1980-05-06 1980-05-06 Refrigeration equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5871380A JPS603147B2 (en) 1980-05-06 1980-05-06 Refrigeration equipment

Publications (2)

Publication Number Publication Date
JPS56157770A JPS56157770A (en) 1981-12-05
JPS603147B2 true JPS603147B2 (en) 1985-01-25

Family

ID=13092128

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5871380A Expired JPS603147B2 (en) 1980-05-06 1980-05-06 Refrigeration equipment

Country Status (1)

Country Link
JP (1) JPS603147B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6215064U (en) * 1985-07-12 1987-01-29

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0548032Y2 (en) * 1988-09-02 1993-12-20
JPH0532971U (en) * 1991-09-27 1993-04-30 三菱重工業株式会社 Condenser
JP2000154991A (en) * 1998-11-20 2000-06-06 Kimura Kohki Co Ltd Heat exchange coil for low water volume fan coil unit
WO2019159371A1 (en) * 2018-02-19 2019-08-22 日揮株式会社 Natural gas liquefier
US12000633B2 (en) 2019-01-21 2024-06-04 Mitsubishi Electric Corporation Outdoor unit and air-conditioning apparatus

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6215064U (en) * 1985-07-12 1987-01-29

Also Published As

Publication number Publication date
JPS56157770A (en) 1981-12-05

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