JPH1123165A - Air-cooled condenser - Google Patents
Air-cooled condenserInfo
- Publication number
- JPH1123165A JPH1123165A JP17967097A JP17967097A JPH1123165A JP H1123165 A JPH1123165 A JP H1123165A JP 17967097 A JP17967097 A JP 17967097A JP 17967097 A JP17967097 A JP 17967097A JP H1123165 A JPH1123165 A JP H1123165A
- Authority
- JP
- Japan
- Prior art keywords
- heat transfer
- steam
- air
- condensation
- outlet
- 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.)
- Withdrawn
Links
- 230000003247 decreasing effect Effects 0.000 claims abstract 2
- 230000005494 condensation Effects 0.000 abstract description 25
- 238000009833 condensation Methods 0.000 abstract description 25
- 230000007423 decrease Effects 0.000 abstract description 6
- 238000001816 cooling Methods 0.000 abstract description 2
- 238000010438 heat treatment Methods 0.000 abstract 6
- 230000005540 biological transmission Effects 0.000 abstract 1
- 239000003570 air Substances 0.000 description 17
- 238000010586 diagram Methods 0.000 description 6
- 238000009825 accumulation Methods 0.000 description 3
- 238000011144 upstream manufacturing Methods 0.000 description 2
- 239000012080 ambient air Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
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- Heat-Exchange Devices With Radiators And Conduit Assemblies (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は火力発電プラント、
等に用いられ、伝熱管内に蒸気を流し、空気で冷却して
蒸気を凝縮させる空冷コンデンサに関し、凝縮性能を向
上させたものである。TECHNICAL FIELD The present invention relates to a thermal power plant,
The present invention relates to an air-cooled condenser that is used for the purpose of flowing steam in a heat transfer tube, cooling the air, and condensing the steam.
【0002】[0002]
【従来の技術】図3に火力発電プラントに用いられる従
来の空冷コンデンサの構成を示す。水平に配置された複
数の伝熱管3が入口室2、出口室4に接続されて、管群
を構成している。管群上部には送風機ダクト9があり、
送風機ダクト9内部には送風機固定具10で固定された
送風機7が設置されている。送風機7は送風機固定具1
0に取付けられた電動機8で駆動される。2. Description of the Related Art FIG. 3 shows a configuration of a conventional air-cooled condenser used in a thermal power plant. A plurality of heat transfer tubes 3 arranged horizontally are connected to the inlet chamber 2 and the outlet chamber 4 to form a tube group. There is a blower duct 9 at the top of the tube bank,
A blower 7 fixed by a blower fixture 10 is installed inside the blower duct 9. Blower 7 is blower fixture 1
0 is driven by a motor 8 attached to the motor.
【0003】蒸気は入口管1から入口室2へ流入し、複
数の伝熱管3へ分配される。蒸気より温度が低い周囲の
空気が、送風機7により最下段の伝熱管3の下方から管
群内周囲へ吸い込まれ、管群内を下から上へ通過して送
風機7を通り、上方へ排気される。蒸気は伝熱管3内を
流れながら管外周囲を流れる空気で冷却されて凝縮し、
出口室4で複数の伝熱管3で凝縮した液が合流して、出
口管5から流出する。蒸気中に含まれている空気などの
不凝縮ガス20は、出口室4に設けられたベント管6か
ら排出される。ベント管6は図示していない真空ポンプ
に接続されている。[0003] Steam flows into the inlet chamber 2 from the inlet pipe 1 and is distributed to the plurality of heat transfer tubes 3. Ambient air having a temperature lower than that of the steam is sucked by the blower 7 from below the lowermost heat transfer tube 3 into the inside of the tube group, passes through the tube group from bottom to top, passes through the blower 7, and is exhausted upward. You. The steam is cooled by air flowing around the outside of the tube while flowing inside the heat transfer tube 3 and condensed.
The liquids condensed in the plurality of heat transfer tubes 3 in the outlet chamber 4 merge and flow out of the outlet tube 5. Non-condensable gas 20 such as air contained in the steam is discharged from a vent pipe 6 provided in the outlet chamber 4. The vent pipe 6 is connected to a vacuum pump (not shown).
【0004】このような構成の空冷コンデンサにおいて
は、複数の伝熱管3はそれぞれ共通の入口室2と出口室
4に接続されているので、各伝熱管3の入口圧力と出口
圧力がそれぞれ同じになるように蒸気の数量が決まる。
すなわち、各伝熱管3内の流れの圧力損失は同一であ
る。In the air-cooled condenser having such a configuration, since the plurality of heat transfer tubes 3 are connected to the common inlet chamber 2 and outlet chamber 4, respectively, the inlet pressure and the outlet pressure of each heat transfer tube 3 are the same. The quantity of steam is decided so that it becomes.
That is, the pressure loss of the flow in each heat transfer tube 3 is the same.
【0005】一方、空気は最下段の伝熱管3の下方から
流入し、下部の伝熱管3で加熱されて温度が上昇しなが
ら上方へ流れるので、上方の伝熱管3ほど蒸気と空気の
温度差が小さくなる。従って、各伝熱管3の凝縮能力
は、蒸気と空気の温度差が最も大きい最下段が最大で、
上方へいくにつれて低下する。On the other hand, the air flows in from below the lowermost heat transfer tube 3 and is heated by the lower heat transfer tube 3 and flows upward while the temperature rises. Becomes smaller. Therefore, the condensation capacity of each heat transfer tube 3 is largest at the lowest stage where the temperature difference between steam and air is largest,
It decreases as going upward.
【0006】伝熱管3内の流れの圧力損失は流入する蒸
気流量が多いほど大きいので、凝縮能力に見合うだけの
蒸気量が各伝熱管3へ流入すると、下方の伝熱管3ほど
圧力損失が大きくなり、圧力バランスがとれない。その
ため、圧力バランス上,下方の伝熱管3は途中で凝縮が
完了し、図3に示すように、凝縮液は管の底の部分を流
れながら出口室4へ流出し、凝縮完了位置から伝熱管3
出口までの管内上方には不凝縮ガス20が滞溜する状態
となる。[0006] Since the pressure loss of the flow in the heat transfer tube 3 increases as the flow rate of the steam flowing in increases, the amount of steam sufficient to condense into the heat transfer tubes 3 increases the pressure loss of the lower heat transfer tube 3. And the pressure cannot be balanced. For this reason, the heat transfer tubes 3 above and below the pressure balance are completely condensed on the way, and as shown in FIG. 3, the condensate flows out to the outlet chamber 4 while flowing through the bottom of the tubes. 3
The non-condensable gas 20 stays in the upper part of the pipe up to the outlet.
【0007】図4は上記に説明の伝熱管3の長手方向位
置での各伝熱管での凝縮完了位置との関係を示す図であ
り、図示のように圧力バランス上、凝縮能力の大きい下
方の伝熱管3ほど管の上流側で凝縮完了となっている。
このような状態にあっては、伝熱管3内の不凝縮ガス2
0が滞溜した部分は凝縮は起こらないので、この部分の
伝熱面は無効であり、全体として有効な伝熱面積が不足
して、凝縮量不足を引き起こす。FIG. 4 is a diagram showing the relationship between the position of the heat transfer tube 3 described above and the position where the condensation is completed in each heat transfer tube at the longitudinal position. As shown in FIG. Condensation of the heat transfer tube 3 is completed on the upstream side of the tube.
In such a state, the non-condensable gas 2 in the heat transfer tube 3
Since condensation does not occur in the portion where 0 has accumulated, the heat transfer surface of this portion is ineffective, and the effective heat transfer area is insufficient as a whole, resulting in an insufficient amount of condensation.
【0008】[0008]
【発明が解決しようとする課題】前述のように従来の空
冷コンデンサにおいては、空気が最下段の伝熱管側から
流入し、上方へ流れ、下方から上方の伝熱管を順次通っ
て伝熱管を冷却し、空気は加熱され、従って空気は上方
に行くほど温度が高くなり、上方の伝熱管ほど蒸気と空
気の温度差が小さくなる。そのため、各上下の伝熱管の
凝縮能力は、蒸気と空気の温度差が最も大きい最下段が
最大で上方にゆくにつれて低下し、各伝熱管での凝縮完
了位置は下段の伝熱管ほど蒸気流れの上流側となり、そ
の管内の凝縮完了位置より下流側では凝縮液が伝熱管底
面を流れ、管内上部空間には不凝縮ガスが滞溜し、この
部分の伝熱面は無効となり、全体として有効伝熱面積が
不足し、凝縮量不足の事態が生じていた。As described above, in the conventional air-cooled condenser, air flows in from the lowermost heat transfer tube side, flows upward, and cools the heat transfer tubes sequentially from the bottom through the upper heat transfer tubes. However, the air is heated, so that the temperature of the air rises as it goes upward, and the temperature difference between the steam and the air becomes smaller as the heat transfer tubes rise. Therefore, the condensation capacity of the upper and lower heat transfer tubes decreases as the lowest stage, where the temperature difference between steam and air is the largest, goes up at the maximum. On the upstream side, the condensate flows on the bottom surface of the heat transfer tube downstream of the condensation completion position in the tube, non-condensable gas accumulates in the upper space inside the tube, the heat transfer surface in this part becomes invalid, and the effective transfer The heat area was insufficient, and the amount of condensation was insufficient.
【0009】そこで本発明は空冷コンデンサの上下に配
置された伝熱管の蒸気流入量を上下段で各々変化させ、
各伝熱管で蒸気の入口側から出口側までの圧力損失が等
しくなるようにし、各伝熱管内に不凝縮ガスの滞溜をな
くし、伝熱面積を有効に作用させるような空冷コンデン
サを提供し、凝縮量不足が生じないようにすることを課
題としてなされたものである。Therefore, the present invention changes the steam inflow of the heat transfer tubes arranged above and below the air-cooled condenser in the upper and lower stages, respectively.
Provide an air-cooled condenser that equalizes the pressure loss from the inlet side to the outlet side of steam in each heat transfer tube, eliminates the accumulation of non-condensable gas in each heat transfer tube, and effectively acts the heat transfer area. The object of the present invention is to prevent the shortage of the amount of condensation from occurring.
【0010】[0010]
【課題を解決するための手段】本発明は前述の課題を解
決するために、次の(1),(2)の手段を提供する。The present invention provides the following means (1) and (2) in order to solve the above-mentioned problems.
【0011】(1)内部に蒸気を導く伝熱管を複数段上
下に配置し、同伝熱管周囲に空気を流して同伝熱管内の
蒸気を冷却して凝縮させる空冷コンデンサにおいて、前
記各伝熱管の蒸気入口部にオリフィスを設けると共に、
同オリフィスは上段にゆくほど順次狭くすることを特徴
とする空冷コンデンサ。(1) In an air-cooled condenser in which a plurality of heat transfer tubes for guiding steam are arranged inside and below the heat transfer tubes, air flows around the heat transfer tubes to cool and condense the steam in the heat transfer tubes. And an orifice at the steam inlet
The orifice is an air-cooled condenser characterized in that the orifice is gradually narrowed toward the top.
【0012】(2)内部に蒸気を導く伝熱管を複数段上
下に配置し、同伝熱管周囲に空気を流して同伝熱管内の
蒸気を冷却して凝縮させる空冷コンデンサにおいて、前
記伝熱管の径は上段にゆくほど順次小さくすることを特
徴とする空冷コンデンサ。(2) In an air-cooled condenser in which a plurality of heat transfer tubes for guiding steam inside are arranged vertically and air flows around the heat transfer tubes to cool and condense the steam in the heat transfer tubes. An air-cooled condenser characterized in that the diameter gradually decreases as it goes up.
【0013】本発明の(1)においては、伝熱管の蒸気
入口部にはオリフィスが設けてあり、各段のオリフィス
の絞り程度は伝熱管の蒸気出口で丁度凝縮が完了するよ
うな蒸気流入量となるように設定する。即ち、伝熱管の
出口で丁度凝縮が完了したときの伝熱管入口から出口ま
での圧力損失が全ての伝熱管で等しくなるようにオリフ
ィスの絞り程度を各段ごとに変化させる。従って、この
ような各オリフィスで圧力損失を付加することにより、
各伝熱管への凝縮能力に見合う量の蒸気が流入した状態
で圧力損失がバランスするので、各伝熱管内では従来の
ように、入口、出口の途中で凝縮が完了してその後流側
で不凝縮ガスが滞溜するようなことがなく、全ての伝熱
管の伝熱面が有効に作用して凝縮量不足となることがな
い。In (1) of the present invention, an orifice is provided at the steam inlet of the heat transfer tube, and the degree of throttle of the orifice at each stage is such that the steam inflow at which the condensation is completed at the steam outlet of the heat transfer tube is completed. Set so that That is, the degree of restriction of the orifice is changed for each stage so that the pressure loss from the inlet to the outlet of the heat transfer tube when condensation has just completed at the outlet of the heat transfer tube is equal in all the heat transfer tubes. Therefore, by adding pressure loss at each such orifice,
Since the pressure loss is balanced when a sufficient amount of steam flows into each heat transfer tube, the condensation is completed in the middle of the inlet and outlet in each heat transfer tube, and then the flow There is no accumulation of condensed gas, and the heat transfer surfaces of all the heat transfer tubes work effectively, and the amount of condensate does not become insufficient.
【0014】本発明の(2)においては、各伝熱管の内
径は、伝熱管出口で丁度凝縮が完了したときの伝熱管入
口から出口までの圧力損失が全ての伝熱管で等しくなる
ように各段ごとに順次下から上へゆく程小さく設定す
る。伝熱管の内径をこのように適切に設定することによ
り、各伝熱管へ凝縮能力に見合う量の蒸気が流入した状
態で圧力損失がバランスするので、上記(1)と同様に
伝熱管内に不凝縮ガスが滞溜することがなく、全ての伝
熱面積が有効に作用して、凝縮量不足が生じない。In (2) of the present invention, the inner diameter of each heat transfer tube is set so that the pressure loss from the inlet to the outlet of the heat transfer tube when condensation is completed at the outlet of the heat transfer tube is equal in all the heat transfer tubes. The smaller the value is, the lower the setting goes from bottom to top. By appropriately setting the inner diameter of the heat transfer tubes in this manner, the pressure loss is balanced in a state where the amount of steam flowing into each heat transfer tube matches the condensing capacity. There is no accumulation of condensed gas, all the heat transfer areas work effectively, and there is no shortage of condensed gas.
【0015】[0015]
【発明の実施の形態】以下、本発明の実施の形態につい
て図面に基づいて具体的に説明する。図1は本発明の実
施第1形態に係る空冷コンデンサの構成図である。図に
おいて、符号1乃至10は図3に示す従来の構成と同一
機能を有するので省略し、そのまま引用して説明する
が、本発明の特徴部分は符号11で示す部分であり、以
下に詳しく説明する。Embodiments of the present invention will be specifically described below with reference to the drawings. FIG. 1 is a configuration diagram of the air-cooled condenser according to the first embodiment of the present invention. In the figure, reference numerals 1 to 10 have the same functions as those of the conventional configuration shown in FIG. 3 and thus are omitted and will be referred to as they are. I do.
【0016】図1において、11はオリフィスであり、
最下段の伝熱管3(A)にはオリフィスは設けず、
(B),(C),(D)と、上段にゆくに従ってその絞
り程度を狭くしている。空気は最下段の伝熱管3(A)
から(B),(C),(D)と順次上方へ流れるので、
上方の伝熱管程周囲の空気は加熱されており、蒸気と空
気の温度差が小さくなる。従って凝縮能力は下段程大き
く、上段にゆくに従って小さくなる。In FIG. 1, reference numeral 11 denotes an orifice;
No orifice is provided in the bottom heat transfer tube 3 (A),
(B), (C), and (D), the degree of aperture is narrowed toward the top. Air is the bottom heat transfer tube 3 (A)
From (B), (C), (D) to flow upward sequentially,
The air around the upper heat transfer tube is heated, and the temperature difference between steam and air becomes smaller. Accordingly, the condensing capacity is higher in the lower stage and decreases in the upper stage.
【0017】オリフィス11の絞りの程度は、伝熱管3
の出口で丁度凝縮完了したときの伝熱管3入口から出口
までの圧力損失が全ての伝熱管3で等しくなるように絞
り程度を各段ごとに変えてある。The degree of restriction of the orifice 11 depends on the heat transfer tube 3
The degree of throttling is changed for each stage so that the pressure loss from the inlet to the outlet of the heat transfer tube 3 when condensation is completed at the outlet of the heat transfer tube 3 becomes equal in all the heat transfer tubes 3.
【0018】従って、最下段の伝熱管3(A)では蒸気
が入口側より流入し、周囲の空気を加熱して管内下流側
に流れるに従って凝縮して出口側で凝縮が完了するよう
な蒸気流入量となるように径を設定してある。伝熱管3
の上段(B),(C),(D)にゆくに従って凝縮能力
が低下してゆくのでオリフィス11もその分蒸気流入量
を制限するように順次オリフィス11を絞り、各伝熱管
3の(B),(C),(D)においては入口側より流入
した蒸気が出口側において凝縮が完了するような蒸気流
入量としている。Accordingly, in the lowermost heat transfer tube 3 (A), steam flows in from the inlet side, heats the surrounding air, condenses as it flows downstream in the tube, and completes the condensation at the outlet side. The diameter is set so as to be the amount. Heat transfer tube 3
As the condensation capacity decreases as going to the upper stages (B), (C), and (D), the orifice 11 also sequentially narrows the orifice 11 so as to limit the steam inflow amount by that amount. ), (C) and (D), the steam inflow amount is such that the steam flowing from the inlet side is completely condensed at the outlet side.
【0019】従って、本実施の第1形態においては、こ
のようなオリフィスの圧力損失を付加することにより、
各伝熱管3へ凝縮能力に見合う量の蒸気が流入した状態
で圧力損失がバランスするので、伝熱管3内に不凝縮ガ
スが滞溜することはなく、全ての伝熱面が有効に作用し
て、凝縮量不足は生じない。上記以外の構成、作用は従
来例と同じであるので説明は省略する。Therefore, in the first embodiment, by adding such pressure loss of the orifice,
Since the pressure loss is balanced in a state where the amount of steam corresponding to the condensing capacity flows into each heat transfer tube 3, non-condensable gas does not accumulate in the heat transfer tube 3, and all the heat transfer surfaces function effectively. Thus, there is no shortage of condensation. The configuration and operation other than those described above are the same as those of the conventional example, and thus description thereof is omitted.
【0020】図2は本発明の実施の第2形態に係る空冷
コンデンサの構成図である。図において符号1,2,4
乃至10は実施の第1形態と同一機能を有するので説明
は省略するが、本実施の第2形態の特徴部分は符号31
乃至34で示す伝熱管であり、次に説明する。FIG. 2 is a configuration diagram of an air-cooled condenser according to a second embodiment of the present invention. In the figure, reference numerals 1, 2, 4
10 to 10 have the same functions as those of the first embodiment, and a description thereof will not be repeated.
Heat transfer tubes denoted by reference numerals 34 to 34 will be described below.
【0021】図2において、伝熱管31,32,33,
34はそれぞれ内径が異なっており、31が最も大き
く、32,33,34と上段にゆくに従って上方の伝熱
管ほど管内径を小さくしている。伝熱管内径が小さいほ
ど同一流量での圧力損失は大きい。伝熱管31,32,
33,34の内径は、伝熱管の出口で丁度凝縮が完了し
たときの伝熱管入口から出口までの圧力損失となるよう
に設定し、この圧力損失が全ての伝熱管で等しくなるよ
うに、各段ごとに変えてある。In FIG. 2, heat transfer tubes 31, 32, 33,
Numerals 34 have different inner diameters, 31 being the largest, and 32, 33, 34, with the upper heat transfer tubes having smaller diameters as they go upward. The smaller the inner diameter of the heat transfer tube, the greater the pressure loss at the same flow rate. Heat transfer tubes 31, 32,
The inner diameter of each of the pipes 33 and 34 is set so that the pressure loss from the inlet to the outlet of the heat transfer pipe when the condensation is completed at the outlet of the heat transfer pipe is equalized. It is changed for each stage.
【0022】上記構成の実施の第2形態においては、伝
熱管の内径をこのように適切に選定することにより、各
伝熱管31,32,33,34へ凝縮能力に見合う量の
蒸気が流入した状態で圧力損失がバランスするので、伝
熱管内に不凝縮ガスが滞溜することはなく、全ての伝熱
面が有効に作用して、凝縮量不足は生じない。なお、上
記以外の構成、作用は実施の第1形態と同じであるので
説明は省略する。In the second embodiment of the above configuration, by appropriately selecting the inner diameter of the heat transfer tubes in this manner, the amount of steam flowing into each of the heat transfer tubes 31, 32, 33, and 34 matches the condensing capacity. Since the pressure loss is balanced in the state, the non-condensable gas does not accumulate in the heat transfer tube, all the heat transfer surfaces work effectively, and the condensed amount does not become insufficient. Note that the configuration and operation other than those described above are the same as those of the first embodiment, and a description thereof will be omitted.
【0023】[0023]
【発明の効果】本発明の(1)は内部に蒸気を導く伝熱
管を複数段上下に配置し、同伝熱管周囲に空気を流して
同伝熱管内の蒸気を冷却して凝縮させる空冷コンデンサ
において、前記各伝熱管の蒸気入口部にオリフィスを設
けると共に、同オリフィスは上段にゆくほど順次狭くす
ることを特徴としている。このような空冷コンデンサの
オリフィスで各伝熱管に圧力損失を付加することによ
り、各伝熱管へは凝縮能力に見合う蒸気量が流入した状
態で圧力損失がバランスし、各伝熱管内に不凝縮ガスが
滞溜することがなく、全ての伝熱面が有効に作用し、凝
縮不足が生じなくなる。According to the first aspect of the present invention, an air-cooled condenser is provided in which a plurality of heat transfer tubes for guiding steam are arranged inside and below, and air flows around the heat transfer tubes to cool and condense the steam in the heat transfer tubes. Wherein an orifice is provided at a steam inlet of each of the heat transfer tubes, and the orifice is gradually narrowed toward an upper stage. By adding a pressure loss to each heat transfer tube with the orifice of such an air-cooled condenser, the pressure loss balances with the amount of steam flowing into each heat transfer tube in a manner commensurate with the condensation capacity. Does not accumulate, all the heat transfer surfaces function effectively, and insufficient condensation does not occur.
【0024】本発明の(2)は、更に、空冷コンデンサ
において、各伝熱管の径は上段にゆくほど順次小さくす
ることを特徴としている。このように各伝熱管の内径
を、伝熱管の出口で丁度凝縮が完了したときの伝熱管入
口から出口までの圧力損失が全ての伝熱管で等しくなる
ように選定することにより、各伝熱管には凝縮能力に見
合う蒸気量が流入した状態で圧力損失がバランスし、上
記(1)と同様の効果を奏することができる。Further, (2) of the present invention is characterized in that, in the air-cooled condenser, the diameter of each heat transfer tube is gradually reduced as going upward. In this way, by selecting the inner diameter of each heat transfer tube so that the pressure loss from the heat transfer tube inlet to the outlet when the condensation is completed at the outlet of the heat transfer tube is equal for all the heat transfer tubes, The pressure loss is balanced in a state where the amount of steam corresponding to the condensing capacity flows, and the same effect as the above (1) can be obtained.
【図1】本発明の実施の第1形態に係る空冷コンデンサ
の構成図である。FIG. 1 is a configuration diagram of an air-cooled condenser according to a first embodiment of the present invention.
【図2】本発明の実施の第2形態に係る空冷コンデンサ
の構成図である。FIG. 2 is a configuration diagram of an air-cooled condenser according to a second embodiment of the present invention.
【図3】従来の空冷コンデンサの構成図である。FIG. 3 is a configuration diagram of a conventional air-cooled condenser.
【図4】従来の空冷コンデンサでの各段の伝熱管の凝縮
完了位置を示す図である。FIG. 4 is a view showing a position where condensation of a heat transfer tube in each stage is completed in a conventional air-cooled condenser.
【符号の説明】 1 入口管 2 入口室 3 伝熱管 4 出口室 5 出口管 6 ベント管 7 送風機 8 電動機 9 送風機ダクト 11 オリフィス 31〜34 伝熱管[Description of Signs] 1 inlet pipe 2 inlet chamber 3 heat transfer pipe 4 outlet chamber 5 outlet pipe 6 vent pipe 7 blower 8 motor 9 blower duct 11 orifice 31 to 34 heat transfer pipe
Claims (2)
配置し、同伝熱管周囲に空気を流して同伝熱管内の蒸気
を冷却して凝縮させる空冷コンデンサにおいて、前記各
伝熱管の蒸気入口部にオリフィスを設けると共に、同オ
リフィスは上段にゆくほど順次狭くすることを特徴とす
る空冷コンデンサ。1. An air-cooled condenser, in which a plurality of heat transfer tubes for introducing steam into the inside of the heat transfer tube are arranged vertically and air flows around the heat transfer tubes to cool and condense the steam in the heat transfer tubes. An air-cooled condenser characterized in that an orifice is provided at the steam inlet and the orifice is gradually narrowed toward the top.
配置し、同伝熱管周囲に空気を流して同伝熱管内の蒸気
を冷却して凝縮させる空冷コンデンサにおいて、前記伝
熱管の径は上段にゆくほど順次小さくすることを特徴と
する空冷コンデンサ。2. An air-cooled condenser, in which a plurality of heat transfer tubes for guiding steam inside are arranged vertically and air flows around the heat transfer tubes to cool and condense the steam in the heat transfer tubes. Is an air-cooled condenser characterized by decreasing in size as it goes up.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17967097A JPH1123165A (en) | 1997-07-04 | 1997-07-04 | Air-cooled condenser |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17967097A JPH1123165A (en) | 1997-07-04 | 1997-07-04 | Air-cooled condenser |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH1123165A true JPH1123165A (en) | 1999-01-26 |
Family
ID=16069827
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17967097A Withdrawn JPH1123165A (en) | 1997-07-04 | 1997-07-04 | Air-cooled condenser |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH1123165A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2015124945A (en) * | 2013-12-26 | 2015-07-06 | 三菱重工業株式会社 | Air cooler and air cooling method |
| CN112683077A (en) * | 2020-12-25 | 2021-04-20 | 山西德望节能科技有限公司 | Energy-saving natural convection air cooling tower |
-
1997
- 1997-07-04 JP JP17967097A patent/JPH1123165A/en not_active Withdrawn
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2015124945A (en) * | 2013-12-26 | 2015-07-06 | 三菱重工業株式会社 | Air cooler and air cooling method |
| CN112683077A (en) * | 2020-12-25 | 2021-04-20 | 山西德望节能科技有限公司 | Energy-saving natural convection air cooling tower |
| CN112683077B (en) * | 2020-12-25 | 2022-10-25 | 山西德望节能科技有限公司 | Energy-saving natural convection air cooling tower |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| A300 | Withdrawal of application because of no request for examination |
Free format text: JAPANESE INTERMEDIATE CODE: A300 Effective date: 20040907 |