JPH0449024B2 - - Google Patents
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- Publication number
- JPH0449024B2 JPH0449024B2 JP59052974A JP5297484A JPH0449024B2 JP H0449024 B2 JPH0449024 B2 JP H0449024B2 JP 59052974 A JP59052974 A JP 59052974A JP 5297484 A JP5297484 A JP 5297484A JP H0449024 B2 JPH0449024 B2 JP H0449024B2
- Authority
- JP
- Japan
- Prior art keywords
- heat storage
- cooling
- shell
- cold heat
- spherical shell
- 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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- Compression-Type Refrigeration Machines With Reversible Cycles (AREA)
Description
本発明は冷房、冷凍装置に係わり、更に詳しく
は、潜熱蓄熱装置を付加して冷房、冷凍負荷をま
かなうようにした装置の改良に関する。
従来から、熱利用装置に蓄熱装置を付加する技
術が種々提案されている。これは安い深夜電力を
利用して、熱量を貯えておき、必要な時に負荷の
要求に応じて放熱するので、熱の供給と需要との
間の時間的なズレを調整し、省エネルギーに寄与
する。
そして、冷房、冷凍の分野でも当然の事ながら
このような考え方の多数が提案されている。例え
ば実公昭46−443号公報にみられる。即ち蒸発器
と冷却器の間に於けるブライン循環系に冷熱蓄熱
槽を付加し、この冷熱蓄熱槽内に、冷熱媒体をシ
エル内に収容して成る冷熱蓄熱体の多数を収容し
た技術が提案されている。この従来技術に於ける
冷熱媒体を収容せるシエルを観ると、即ち冷熱媒
体をみると、この冷熱媒体はシエル内に密に充填
されている。従つてシエル内の空間に最大限冷熱
媒体を収容することとなるから、蓄熱容量を大き
くとれる利点を有するものの、液相から固相への
変化時に於ける冷熱媒体の体積膨張の為の対策に
何等の工夫が施されていない。故に繰返し使用に
伴なうシエルの破損、耐久性の考慮がなく実用す
る上ではシエルの材質検討等幾つかの解決課題を
有している。
そこで、この冷熱媒体に関し、それをシエル内
に充填する時に、冷熱媒体の体積膨張を100%吸
収できるようにシエル内に予め比較的大きな空間
をつくつて充填する技術が考慮される。例えば特
開昭53−55547にみられる。この従来技術にれば、
冷熱媒体の体積膨張時、この膨張量を上記空間が
吸収することとなる為、この体積膨張を原因とす
るシエルの破損がない。所が、このように体積膨
張量全部を吸収する為に必要な空間を当初から十
分残す為に冷熱媒体の収容量がその十分必要な分
だけ少なくなり、蓄熱容量が小となる。これは冷
熱蓄熱槽内に収容される冷熱媒体の数が多数であ
ることから無視できない点である。
本発明は述上の点に鑑み成されたもので、その
要旨とする所は、蒸発器、圧縮機、凝縮器、膨張
弁を備え、上記蒸発器と冷却器の間をブライン循
環系によつて接続し、このブライン循環系に冷熱
蓄熱槽を付設し、上記冷熱蓄熱槽内には、冷熱媒
体を球状シエル内に収容して成る蓄熱体の多数が
収容され、上記冷熱媒体は液相から固相に変わる
時に固化の潜熱として冷熱を蓄熱し、固相から液
相に変わる時に先に蓄熱した冷熱を放熱する性質
を有し、而も液相から固相へ変化した時に、その
体積が膨張する性質を有し、上記冷熱媒体の液相
時には上記球状シエル内に空間が残るように設定
された冷房、冷凍装置に於いて、上記冷熱媒体が
液相時に残る上記球状シエル内の空間の容積は、
上記冷熱媒体が液相から固相へ変化した時の冷熱
媒体の体積膨張量の全てを吸収できるように定め
られていず、体積膨張量の一部のみを吸収する大
きさに定められていると共に、上記体積膨張量全
部の内の残りの体積膨張量を上記球状シエルの同
心円的な膨張によつて吸収できるように上記球状
シエルを上記冷熱媒体の体積膨張に応じて同心円
的に膨らむ材質によつて形成し、而も球状シエル
の同心円的な膨らみの範囲は、球状シエルの材質
の弾性限界内に設定されている事を特徴とする冷
房、冷凍装置であつて、その目的とする所は、冷
熱媒体の体積膨張時には、その膨張量をシエル内
に僅かに残した空間と、シエルの同心円的な膨張
により吸収可能とする事により冷熱媒体の体積膨
張量を十分吸収でき実用的に実施可能とすると共
にシエルの耐久性を図り、同時に可及的に多くの
潜熱蓄熱の為の冷熱媒体をシエル内に収容可能と
し、限られた大きさの冷熱蓄熱槽に多くの冷熱蓄
熱容量を確保するにある。
次に添付図面に従い本発明の実施例を詳細に説
明する。第1図に於いて、蒸発器1で発生する冷
媒蒸気は圧縮機2で圧縮されて高圧の過熱蒸気と
なり、凝縮器3で冷却水に熱を奪われて液体とな
る。この高圧の液を膨張弁4で減圧し、低圧低温
の冷媒を蒸発器1で蒸発させて、凝固点の低いブ
ラインから蒸発熱をとつて、それを冷却し、この
ブラインをブライン循環系5を介して冷却器6に
送り冷房、冷凍の用に供する。そして、上記ブラ
イン循環系5に冷熱を蓄熱し、放熱する蓄熱槽7
を付設する。この例では蒸発器1を中にして、そ
の上流と下流を管8で接続し、管8の中間に蓄熱
槽7を配した例を示してある。そして、上記管8
と並列にバイパス管9を設ける。上記管8とブラ
イン循環系5の接続箇所及び管9とブライン循環
系5の接続箇所には各々三方向制御弁10,1
1,12,13を配設し、又ブライン循環系5中
に蒸発器循環用ポンプ14、放冷用ポンプ15を
配置する。上記蓄熱槽7内には、第2図で示す如
き球状蓄熱体16の多数が収容されている。この
球状蓄熱体16は、凝固温度で液相から固相に変
わる時に、固化の潜熱として冷熱を蓄熱し、固相
から液相に変わる時に先に蓄熱した冷熱を放出す
る冷熱媒体17を球状のシエル18内に充填した
ものである。
上記球状蓄熱体16の個々の大きさは、直径20
mm〜200mmの範囲、例えば65mm程度であるが、こ
の事は冷房、冷凍装置の条件、蓄放熱運転条件等
によつて必要な蓄熱槽全体の蓄、放熱量が決定さ
れるから、その必要蓄、放熱量を確保するに十分
な伝熱面積を確保することを基準として定めれば
よい。望ましくは同時に、蓄熱槽7の一定容積中
に収容する数が多くなればなるほど、即ち個々の
球状蓄熱体16の直径が小さくなればなるほど製
作費が高くなるから、上記の条件を満すと同時
に、この製作上の条件を満すようにして加工する
とよい。更に、この球状蓄熱体16を蓄熱槽7中
に収容するにあたつては、図示せざるも例えば、
蓄熱槽7の一方の入口又は出口と、他方の入口又
は出口付近に、多数の流通孔の形成された板を装
設し、上記板と板の間に球状蓄熱体16を収容す
るとよい。このようにすることによつて、蓄熱槽
7中にブラインが出入りする際に、上記板によつ
てブラインが分散して蓄熱槽7中に出入し、多数
収容されている球状蓄熱体16に平均に接触せし
められる。更にブラインの蓄熱槽7内に於ける移
動速度は極くゆつくりとしたもので、例えば1時
間当り5m3のブラインの移動量が確保されるよう
に速度を設定する等装置の条件に応じて定める。
さて、冷熱媒体17については、本例に於いて
は共融混合体を用いる。即ち、塩類等の熱媒体の
水溶液は一定の濃度で最低の凝固温度が得られる
が、その最も低温度が得られるときの濃度の溶液
を用いるものである。この共融濃度の共融混合体
によれば、最も低温度で、塩類等の熱媒体と水が
あたかも単一の物質のように凝固する。従つて融
解−凝固のサイクルに対して確実に且つ安定して
動作する。この時凝固の潜熱として冷熱媒体17
が熱を蓄熱する。
このような共融混合体の数例を次に示す。
The present invention relates to air conditioning and refrigeration equipment, and more particularly, to an improvement of the equipment in which a latent heat storage device is added to cover the cooling and refrigeration loads. Conventionally, various techniques for adding a heat storage device to a heat utilization device have been proposed. This uses cheap late-night electricity to store heat and dissipate it when needed according to the demands of the load, thereby adjusting the time lag between heat supply and demand and contributing to energy savings. . Naturally, many such ideas have been proposed in the field of air conditioning and refrigeration. For example, this can be seen in Utility Model Publication No. 46-443. That is, a technology has been proposed in which a cold heat storage tank is added to the brine circulation system between the evaporator and the cooler, and a large number of cold heat storage bodies each containing a cold medium stored in a shell are housed in this cold heat storage tank. has been done. Looking at the shell that accommodates the cooling medium in this prior art, that is, looking at the cooling medium, the cooling medium is densely packed within the shell. Therefore, since the space inside the shell accommodates as much of the cooling medium as possible, it has the advantage of increasing heat storage capacity, but it is difficult to prevent the volumetric expansion of the cooling medium when it changes from liquid phase to solid phase. No improvements have been made. Therefore, there are several problems to be solved in practical use, such as damage to the shell due to repeated use and consideration of the material of the shell, without consideration of durability. Therefore, regarding this cooling medium, a technique is being considered in which, when filling the shell with the cooling medium, a relatively large space is created in advance in the shell so that 100% of the volumetric expansion of the cooling medium can be absorbed. For example, it can be seen in JP-A-53-55547. According to this conventional technology,
When the cooling medium expands in volume, the space absorbs the amount of expansion, so there is no damage to the shell due to this volumetric expansion. However, in order to leave enough space from the beginning to absorb the entire amount of volumetric expansion, the capacity of the cooling medium is reduced by the amount necessary, and the heat storage capacity is reduced. This is a point that cannot be ignored since the number of cold/heat media accommodated in the cold heat storage tank is large. The present invention has been made in view of the above points, and its gist is that it is provided with an evaporator, a compressor, a condenser, and an expansion valve, and that a brine circulation system is used between the evaporator and the cooler. A cold heat storage tank is attached to this brine circulation system, and a large number of heat storage bodies each containing a cold heat medium in a spherical shell are housed in the cold heat storage tank, and the cold heat medium is transferred from a liquid phase to a cold heat storage tank. It has the property of storing cold heat as the latent heat of solidification when changing from a solid phase to a liquid phase, and dissipating the previously stored cold heat when changing from a solid phase to a liquid phase, and when changing from a liquid phase to a solid phase, its volume increases. In a cooling or freezing device that has the property of expanding and is set so that a space remains in the spherical shell when the cooling medium is in a liquid phase, the space in the spherical shell that remains when the cooling medium is in a liquid phase is The volume is
The size is not determined to absorb all of the volumetric expansion of the cooling and heating medium when the cooling and heating medium changes from a liquid phase to a solid phase, but is determined to absorb only a part of the volumetric expansion. , the spherical shell is made of a material that expands concentrically in response to the volumetric expansion of the cooling medium so that the remaining volumetric expansion of the total volumetric expansion can be absorbed by the concentric expansion of the spherical shell. A cooling and freezing device characterized in that the range of the concentric bulge of the spherical shell is set within the elastic limit of the material of the spherical shell, and its purpose is to: When the volumetric expansion of the cooling and heating medium occurs, the volumetric expansion of the cooling and heating medium can be absorbed by the small amount of space left inside the shell and the concentric expansion of the shell. At the same time, the durability of the shell is improved, and at the same time, as much cooling medium for latent heat storage as possible can be accommodated within the shell, and a large amount of cold heat storage capacity is secured in the limited size cold heat storage tank. be. Next, embodiments of the present invention will be described in detail with reference to the accompanying drawings. In FIG. 1, refrigerant vapor generated in an evaporator 1 is compressed by a compressor 2 to become high-pressure superheated vapor, and in a condenser 3, heat is removed by cooling water and becomes a liquid. This high-pressure liquid is depressurized by an expansion valve 4, the low-pressure low-temperature refrigerant is evaporated by an evaporator 1, the heat of evaporation is removed from the brine with a low freezing point, and the brine is cooled. and sent to a cooler 6 for cooling and freezing. A heat storage tank 7 stores cold heat in the brine circulation system 5 and radiates the heat.
Attached. In this example, an evaporator 1 is placed inside, its upstream and downstream sides are connected by a pipe 8, and a heat storage tank 7 is arranged in the middle of the pipe 8. And the pipe 8
A bypass pipe 9 is provided in parallel with the above. Three-way control valves 10 and 1 are provided at the connection points between the pipe 8 and the brine circulation system 5 and the connection points between the pipe 9 and the brine circulation system 5, respectively.
1, 12, and 13, and an evaporator circulation pump 14 and a cooling pump 15 are also arranged in the brine circulation system 5. Inside the heat storage tank 7, a large number of spherical heat storage bodies 16 as shown in FIG. 2 are accommodated. This spherical heat storage body 16 stores cold heat as the latent heat of solidification when changing from a liquid phase to a solid phase at the solidification temperature, and uses a spherical cooling medium 17 to release the previously stored cold heat when changing from a solid phase to a liquid phase. It is filled in the shell 18. The individual size of the spherical heat storage bodies 16 is 20 mm in diameter.
mm to 200 mm, for example about 65 mm, but this is because the required storage and heat radiation amount of the entire heat storage tank is determined by the conditions of the cooling and refrigeration equipment, heat storage and radiation operation conditions, etc. , it may be determined based on ensuring a sufficient heat transfer area to ensure the amount of heat dissipation. Preferably, at the same time, the above conditions are satisfied, since the larger the number of spherical heat storage elements 16 accommodated in a certain volume of the heat storage tank 7, that is, the smaller the diameter of each spherical heat storage element 16, the higher the manufacturing cost. , it is preferable to process it so as to satisfy this manufacturing condition. Furthermore, when accommodating this spherical heat storage body 16 in the heat storage tank 7, there are other steps not shown, such as,
It is preferable that plates with a large number of communication holes are installed near one inlet or outlet and the other inlet or outlet of the heat storage tank 7, and the spherical heat storage body 16 is housed between the plates. By doing this, when the brine goes in and out of the heat storage tank 7, the brine is dispersed by the plates, goes in and out of the heat storage tank 7, and is averaged over the spherical heat storage bodies 16 that are accommodated in large numbers. be brought into contact with. Furthermore, the moving speed of the brine in the heat storage tank 7 is extremely slow, and the speed is set to ensure a moving amount of brine of 5 m 3 per hour, for example, depending on the conditions of the equipment. stipulate. Now, regarding the cooling medium 17, a eutectic mixture is used in this example. That is, an aqueous solution of a heat medium such as a salt can obtain the lowest solidification temperature at a certain concentration, and a solution having a concentration that provides the lowest temperature is used. According to the eutectic mixture with this eutectic concentration, the heat medium such as salts and water solidify as if they were a single substance at the lowest temperature. Therefore, it operates reliably and stably in the melting-solidification cycle. At this time, as the latent heat of solidification, the cooling medium 17
stores heat. Some examples of such eutectic mixtures are shown below.
【表】
上記の共融濃度は重量濃度である。
このような例の共融混合体の冷熱媒体によれば
凝固、融解時に凝固、融解熱が50〜72Kcal/Kg
程生ずるものである。
これらの冷熱媒体17には、勿論過冷却防止と
しての炭酸カルシウム等の発核剤や、ポリアクリ
ル酸ソーダ等の結晶水分離防止剤、並びにヨウ化
銀等の結晶加速剤が添加される。即ち、過冷却防
止に関しては、発核剤を使用しない場合、本来の
凝固点を大幅(10〜20℃)に下回ることが多い
が、従来用いられている熱媒体各に対応する種々
の発核剤を用いると最大でも2℃程度に抑えるこ
とができ動作が安定する。又結晶水の分離防止剤
については、多くの水和塩の融点は包晶点である
が、この場合融点において均一融解がおこらな
い。即ち元の結晶と異なる組成(結晶水が小さ
い)の結晶と、これと平衡する組成の融液との二
相に分離する。この為にゲル化剤としての粘土を
微量加えることが有効である。
そして、特にこの発明では、冷熱媒体17が、
液相の時に、シエル18内に冷熱媒体17の非占
有の空間19、が形成するようにシエル18の大
きさを定めるものである。しかし単に空間を形成
するだけでなく同時に冷熱媒体の凝固による体積
膨張時の膨張量を、上記空間19とシエル18の
同心円的な膨張の双方によつて、吸収するように
空間19の大きさを定めるものである。
そして冷熱媒体が固相から液相に変わつた時に
は、シエル18も収縮するがシエル18は当初設
定した大きさの空間19を残して収縮を止める。
例えば冷熱媒体17が強固した時、液体の時の体
積1.08倍、即ち8%膨張したとすると、空間19
で5.5%、シエル18の膨張で2.5%その膨張量を
吸収するように空間19の大きさを定めるもので
ある。換言すれば冷熱媒体17を、中空成型法、
真空成型法等で加工した球状シエル18内に注入
等により充填する際は、当然のように冷熱媒体1
7は液体であるが、その液体の冷熱媒体17を充
填する際に、空間19として上記の例では5.5%
相当を残して充填するものである。
球状シエル18自体は固い球穀であるが、薄肉
に形成されるので、凝固冷熱媒体の膨張時の内圧
によつて、冷熱媒体の膨張に応じて膨張し、冷熱
媒体が液相に変化した時には当初の空間を残して
自然に原状に復するものであり、例えば軟化点90
℃以上の合成樹脂中でも他の耐力性、耐熱性、加
工性をも考慮すると高密度ポリプロピレン、高密
度ポリエチレンが好適である。
上述したように球状シエル18は膨張し、収縮
するものであるが、球状シエルの同心円的な膨ら
みの範囲は球状シエルの材質の弾性限界内に設定
される。これにより繰り返しの膨張、収縮に耐え
て常に球状シエル18を球形に保つ。
次にこの実施例の各動作を第4図〜第8図に従
い説明する。
第4図に示した運転例は蓄熱動作のみである。
この場合は、蒸発器1によつて蒸発熱をとられ
ることによつて冷却されたブラインを矢示20で
示す如くポンプ14によつて蒸発器と冷熱蓄熱槽
7間にのみ循環させる。これにより蓄熱槽7内に
多数の球状蓄熱体16とブラインが接触すること
により、球状蓄熱体16が冷却されて共融点に於
いて凝固する。凝固時に固化の潜熱としての冷熱
が球状蓄熱体16の冷熱媒体17中に蓄熱され
る。
第5図に示した運転例は、蓄熱しながら圧縮機
2を駆動して冷房、冷凍運転している場合であ
る。即ち、矢示21で示すようにブラインをポン
プ15によつて冷却器6に循環させながら冷房、
冷凍の負荷に応じつつ、ポンプ14によつて冷熱
蓄熱槽7へも循環させ蓄熱する例である。この例
の場合、冷却器6を出たブラインはバイパス管9
を経由して再び冷却器6に戻される。従つて戻り
量の程度に応じてブラインの温度が調節され、冷
房、冷凍結合が調節される。
第6図に示した運転例は、蓄熱槽の放熱動作の
みで冷房、冷凍運転している例である。即ち、矢
示22で示すように冷房、冷凍サイクル系の圧縮
機2の運転を停止して、ブラインをポンプ15に
より冷熱蓄熱槽7と冷却器6の間に循環させるも
のである。冷却器6を経由した後のブラインが冷
熱蓄熱槽7に流入すると、その熱が冷熱蓄熱槽7
の球状蓄熱体16に伝えられ、共融点に至ると冷
熱媒体17が融解し、先に蓄熱した冷熱を融解の
潜熱としてブラインに放出する。従つてブライン
が冷却されて、冷房、冷凍負荷に応ずる。この例
の場合は冷却器6を出たブラインの一部はバイパ
ス管9を経由して再び冷却器6に戻され、ブライ
ンの温度を調節する。第7図、第8図に示した例
は、矢示23,24で示すように蓄熱槽の放熱動
作と、圧縮機2の駆動動作の双方で、冷房、冷凍
運転している例である。但し第7図の例は、冷却
器6を出たブラインの一部はバイパス管9を経由
して再び冷却器6に戻される。
上記の種々の冷房、冷凍運転、蓄熱、放熱運転
を可能にする為に三方向制御弁10,11,1
2,13及びポンプ14,15が従来周知の制御
方法により場合ごとに、それぞれに応じて切換動
作、発停動作せしめられる。
そして、通常上記の冷熱蓄熱槽7による冷熱の
蓄熱は、料金の安い深夜に圧縮機を駆動して行な
われ、負荷需要の多い時に放熱される。この為
に、第3図に例示する如く、冷房、冷凍負荷の要
求パターンでAが示されていて、例えば蓄熱装置
を有さない場合には、最大負荷時の略14〜15時刻
頃には圧縮機の容量が100KW程度必要であつた
とした場合、蓄熱装置を有すると安い深夜電力の
使用できる他の時間帯に圧縮機を駆動して蓄熱a
し、それを冷房、冷凍必要時間帯に放熱bするこ
ができるから、例えば圧縮器の容量を50KWの如
くに小容量化でき、省エネルギーに資する。
さて、上記蓄熱、放熱の過程に於いて、本発明
に用いる球状蓄熱体16中の冷熱媒体17は、共
融濃度の共融混合体なので、凝固点降下を格段と
可能ならしめ、その降下した凝固、融解温度に於
いて相変化する時の潜熱を効果的に蓄熱し、放熱
するものである。又上記の融解−凝固動作は、あ
たかも単一の物質のように行なわれるので動作が
安定し、実用的となる。
而して、シエル18内に液相の冷熱媒体17を
封入する際に、シエル18内に空間19が存する
ように定めて封入するだけでなく、冷熱媒体17
の液相から固相への変化による冷熱媒体17の体
積膨張時には、その膨張量を上記空間19と冷熱
媒体17の体積膨張に応ずるシエル18の同心円
的な膨張により吸収するようにしたので、冷熱媒
体の凝固時の体積膨張に応ずることができると共
に、可及的に冷熱媒体を多く充填できるので、一
つ一つの球状蓄熱体の蓄熱量を大とすることがで
き、蓄熱槽の全体の蓄熱容量をより大にすること
ができるものである。
更に、球状潜熱蓄熱体16なので、これらを密
に収容しても、球状潜熱蓄熱体16同志の接触は
点接触であるから温水の流動に大きな抵抗を与え
ず、望ましい流動、通過を確保できる。故に、密
に充填可能だから、熱交換量を増大できる。且
つ、これら球状潜熱蓄熱体群を蓄熱槽中に保持し
且つ温水の分散流入を可能ならしめる為の温水分
散板が必要最低限でよく、加工がし易い。
更に蓄熱槽中への球状蓄熱体の充填も、並べる
ことなく単に投入すれば自づと規則正しく整列す
るので充填も容易である。
以上詳述した如くこの発明によれば、潜熱蓄熱
の為の冷熱媒体が液相から固相へ変化する時、体
積膨張するが、この体積膨張量を、当初シエル内
に残した空間で吸収すると共に、空間だけではな
く、シエルの同心円的な膨らみにより吸収するの
で、実用的な実施に十分適う。而も球状シエルの
同心円的な膨らみの範囲は球状シエルの材質の限
界内に設定されている。故にシエル破損もなく、
耐久性に富む。特に上記空間の大きさは、空間自
体全部で上記の冷熱媒体の体積膨張を吸収する大
きさに定めていないので、即ち体積膨張の一部は
シエルの同心円的な膨らみで吸収するから、その
分だけより多くの潜熱蓄熱の為の冷熱媒体を収容
できる。故に1つ1つの潜熱蓄熱体の蓄熱容量が
大となると共に、蓄熱槽の限られた大きさのスペ
ース内の蓄熱容量が大きくとれる。加えてシエル
の膨らみは同心円的に実施されるから、シエルに
局部的なストレスがかからず、この意味でも耐久
性に富む等実用上各種の利点を呈するものであ
る。[Table] The above eutectic concentrations are weight concentrations. According to the cooling medium of the eutectic mixture in this example, the heat of solidification and fusion during solidification and melting is 50 to 72 Kcal/Kg.
It is something that occurs. Of course, a nucleating agent such as calcium carbonate to prevent supercooling, an agent for preventing separation of crystal water such as sodium polyacrylate, and a crystal accelerator such as silver iodide are added to the cooling medium 17. In other words, in order to prevent supercooling, if a nucleating agent is not used, the freezing point will often fall significantly (10 to 20°C) below the original freezing point. By using this, the temperature can be suppressed to around 2°C at maximum and the operation becomes stable. Regarding agents for preventing separation of crystal water, the melting point of many hydrated salts is the peritectic point, but in this case uniform melting does not occur at the melting point. That is, the crystal separates into two phases: a crystal with a composition different from that of the original crystal (low water of crystallization) and a melt with a composition in equilibrium with this crystal. For this purpose, it is effective to add a small amount of clay as a gelling agent. In particular, in this invention, the cooling medium 17 is
The size of the shell 18 is determined so that a space 19 not occupied by the cooling medium 17 is formed within the shell 18 when it is in the liquid phase. However, the size of the space 19 is designed not only to simply form a space, but also to absorb the volumetric expansion due to solidification of the cooling medium through both the space 19 and the concentric expansion of the shell 18. It is determined. When the cooling medium changes from a solid phase to a liquid phase, the shell 18 also contracts, but the shell 18 stops contracting, leaving a space 19 of the initially set size.
For example, if the cooling medium 17 becomes solid and expands by 1.08 times its volume when it is a liquid, that is, by 8%, then the space 19
The size of the space 19 is determined so as to absorb the expansion amount of 5.5% by the expansion of the shell 18 and 2.5% by the expansion of the shell 18. In other words, the cooling/heating medium 17 is formed by hollow molding,
When filling the spherical shell 18 processed by vacuum forming method etc. by injection etc., it is natural that the cooling medium 1
7 is a liquid, but when filling the liquid cooling/heating medium 17, the space 19 is 5.5% in the above example.
Fill it with a considerable amount remaining. The spherical shell 18 itself is a hard ball, but because it is formed with a thin wall, it expands according to the expansion of the cooling medium due to the internal pressure when the solidified cooling medium expands, and when the cooling medium changes to a liquid phase. It naturally returns to its original state while leaving the original space, for example, a softening point of 90
Among the synthetic resins having a temperature of ℃ or higher, high-density polypropylene and high-density polyethylene are preferable in consideration of other stress resistance, heat resistance, and processability. As described above, the spherical shell 18 expands and contracts, and the range of concentric expansion of the spherical shell is set within the elastic limit of the material of the spherical shell. This allows the spherical shell 18 to always maintain its spherical shape by withstanding repeated expansion and contraction. Next, each operation of this embodiment will be explained with reference to FIGS. 4 to 8. The operation example shown in FIG. 4 is only a heat storage operation. In this case, the brine cooled by removing the heat of evaporation by the evaporator 1 is circulated only between the evaporator and the cold heat storage tank 7 by the pump 14 as shown by the arrow 20. As a result, the brine comes into contact with a large number of spherical heat storage bodies 16 in the heat storage tank 7, whereby the spherical heat storage bodies 16 are cooled and solidified at the eutectic point. During solidification, cold heat as latent heat of solidification is stored in the cold heat medium 17 of the spherical heat storage body 16. The operation example shown in FIG. 5 is a case where the compressor 2 is driven to perform cooling and freezing operations while storing heat. That is, as shown by the arrow 21, the brine is circulated through the cooler 6 by the pump 15 while cooling.
This is an example in which heat is stored by circulating it also to the cold heat storage tank 7 by the pump 14 according to the refrigeration load. In this example, the brine leaving the cooler 6 is transferred to the bypass pipe 9
The water is returned to the cooler 6 via the. Therefore, the temperature of the brine is adjusted according to the degree of the return amount, and the cooling and freezing combinations are adjusted. The operation example shown in FIG. 6 is an example in which cooling and freezing operations are performed only by the heat dissipation operation of the heat storage tank. That is, as shown by the arrow 22, the operation of the compressor 2 of the cooling and refrigeration cycle system is stopped, and the brine is circulated between the cold heat storage tank 7 and the cooler 6 by the pump 15. When the brine that has passed through the cooler 6 flows into the cold heat storage tank 7, the heat is transferred to the cold heat storage tank 7.
When it reaches the eutectic point, the cold heat medium 17 melts and releases the previously stored cold heat to the brine as latent heat of melting. Therefore, the brine is cooled to meet the cooling and refrigeration load. In this example, a portion of the brine leaving the cooler 6 is returned to the cooler 6 via the bypass pipe 9 to adjust the temperature of the brine. The example shown in FIGS. 7 and 8 is an example in which cooling and freezing operations are performed by both the heat dissipation operation of the heat storage tank and the driving operation of the compressor 2, as shown by arrows 23 and 24. However, in the example shown in FIG. 7, a portion of the brine leaving the cooler 6 is returned to the cooler 6 via the bypass pipe 9. Three-way control valves 10, 11, 1 are used to enable the above-mentioned various cooling, freezing, heat storage, and heat radiation operations.
2 and 13 and pumps 14 and 15 are switched and started/stopped depending on the case by a conventionally known control method. Normally, the storage of cold heat in the cold heat storage tank 7 is carried out by driving the compressor late at night when the charges are low, and the heat is radiated when the load demand is high. For this reason, as illustrated in Fig. 3, A is shown in the request pattern for cooling and refrigeration loads, and for example, when a heat storage device is not provided, at around 14 to 15 hours at the maximum load, Assuming that the compressor capacity is about 100KW, having a heat storage device will allow you to drive the compressor during other times when cheap late-night electricity is available and store heat.
However, since the heat can be radiated during the time period when cooling and freezing are required, the capacity of the compressor can be reduced to, for example, 50KW, contributing to energy conservation. Now, in the process of heat storage and heat dissipation, since the cold medium 17 in the spherical heat storage body 16 used in the present invention is a eutectic mixture with a eutectic concentration, it is possible to significantly lower the freezing point, and the lowered solidification , which effectively stores and radiates latent heat during phase change at the melting temperature. Furthermore, the above-mentioned melting-solidification operation is performed as if it were a single substance, so the operation is stable and practical. Therefore, when enclosing the liquid-phase cooling medium 17 in the shell 18, not only is the space 19 defined and sealed in the shell 18, but also the cooling medium 17 is sealed.
When the volume of the cooling medium 17 expands due to the change from the liquid phase to the solid phase, the amount of expansion is absorbed by the space 19 and the concentric expansion of the shell 18 corresponding to the volumetric expansion of the cooling medium 17. In addition to being able to respond to the volumetric expansion of the medium during solidification, it is also possible to fill as much of the cooling medium as possible, so the amount of heat stored in each spherical heat storage element can be increased, and the heat storage capacity of the entire heat storage tank can be increased. It is possible to increase the capacity. Furthermore, since the spherical latent heat storage bodies 16 are used, even if they are packed closely together, the contact between the spherical latent heat storage bodies 16 is point contact, so there is no large resistance to the flow of hot water, and desired flow and passage can be ensured. Therefore, since it can be densely packed, the amount of heat exchange can be increased. In addition, the number of hot water dispersion plates for holding these spherical latent heat storage bodies in the heat storage tank and enabling the distributed inflow of hot water is required and is easy to process. Furthermore, it is easy to fill the heat storage tank with the spherical heat storage bodies because they are simply placed in the heat storage tank without being lined up, and the spherical heat storage bodies are automatically arranged in a regular manner. As detailed above, according to the present invention, when the cooling medium for storing latent heat changes from a liquid phase to a solid phase, it expands in volume, but this volumetric expansion is absorbed by the space initially left in the shell. At the same time, it is absorbed not only by the space but also by the concentric bulges of the shell, so it is sufficiently suitable for practical implementation. Moreover, the range of the concentric bulge of the spherical shell is set within the limits of the material of the spherical shell. Therefore, there is no damage to the shell,
Highly durable. In particular, the size of the space is not set to a size that allows the space itself to absorb the volumetric expansion of the cooling medium, i.e., part of the volumetric expansion is absorbed by the concentric bulges of the shell. It can only accommodate more cooling medium for latent heat storage. Therefore, the heat storage capacity of each latent heat storage body becomes large, and the heat storage capacity within the limited space of the heat storage tank can be increased. In addition, since the shell is bulged concentrically, no local stress is applied to the shell, and in this sense, it has various practical advantages such as being highly durable.
添付図面は本発明の実施例を示し、第1図は配
管系統図、第2図は球状蓄熱体の例図、第3図は
蓄熱運転のパターン例図、第4図〜第8図は各々
動作例図であり、図中1は蒸発器、2は圧縮機、
3は凝縮機、4は膨張弁、5はブライン循環系、
6は冷却器、7は冷熱蓄熱槽、16は球状蓄熱
体、17は冷熱媒体、18は球状シエル、19は
空間である。
The attached drawings show embodiments of the present invention, in which Fig. 1 is a piping system diagram, Fig. 2 is an example of a spherical heat storage body, Fig. 3 is an example of a heat storage operation pattern, and Figs. 4 to 8 are each This is an operation example diagram, in which 1 is an evaporator, 2 is a compressor,
3 is a condenser, 4 is an expansion valve, 5 is a brine circulation system,
6 is a cooler, 7 is a cold heat storage tank, 16 is a spherical heat storage body, 17 is a cold medium, 18 is a spherical shell, and 19 is a space.
Claims (1)
備え、上記蒸発器1と冷却器6の間をブライン循
環系5によつて接続し、このブライン循環系5に
冷熱蓄熱槽7を付設し、上記冷熱蓄熱槽7内に
は、冷熱媒体17を球状シエル18内に収容して
成る蓄熱体16の多数が収容され、上記冷熱媒体
17は液相から固相に変わる時に固化の潜熱とし
て冷熱を蓄熱し、固相から液相に変わる時に先に
蓄熱した冷熱を放熱する性質を有し、而も液相か
ら固相へ変化した時に、その体積が膨張する性質
を有し、上記冷熱媒体17の液相時には上記球状
シエル18内に空間が残るように設定された冷
房、冷凍装置に於いて、上記冷熱媒体17が液相
時に残る上記球状シエル18内の空間の容積は、
上記冷熱媒体が液相から固相へ変化した時の冷熱
媒体の体積膨張量の全てを吸収できるように定め
られていず、体積膨張量の一部のみを吸収する大
きさに定められていると共に、上記体積膨張量全
部の内の残りの体積膨張量を上記球状シエル18
の同心円的な膨張によつて吸収できるように上記
球状シエル18を上記冷熱媒体の体積膨張に応じ
て同心円的に膨らむ材質によつて形成し、而も球
状シエル18の同心円的な膨らみの範囲は、球状
シエル18の材質の弾性限界内に設定されている
事を特徴とする冷房、冷凍装置。1 Equipped with an evaporator 1, a compressor 2, a condenser 3, and an expansion valve 4, the evaporator 1 and the cooler 6 are connected by a brine circulation system 5, and a cold heat storage tank 7 is connected to the brine circulation system 5. A large number of heat storage bodies 16 each having a cold heat medium 17 housed in a spherical shell 18 are housed in the cold heat storage tank 7, and the cold heat medium 17 solidifies when changing from a liquid phase to a solid phase. It has the property of storing cold heat as latent heat and dissipating the previously stored cold heat when changing from the solid phase to the liquid phase, and also has the property of expanding its volume when changing from the liquid phase to the solid phase. In a cooling or freezing device that is set so that a space remains in the spherical shell 18 when the cooling medium 17 is in the liquid phase, the volume of the space in the spherical shell 18 that remains when the cooling medium 17 is in the liquid phase is:
The size is not determined to absorb all of the volumetric expansion of the cooling and heating medium when the cooling and heating medium changes from a liquid phase to a solid phase, but is determined to absorb only a part of the volumetric expansion. , the remaining amount of volumetric expansion out of the total amount of volumetric expansion is determined by the amount of volumetric expansion of the spherical shell 18.
The spherical shell 18 is made of a material that expands concentrically in accordance with the volumetric expansion of the cooling medium, and the range of the concentric expansion of the spherical shell 18 is , a cooling and freezing device characterized by being set within the elastic limit of the material of the spherical shell 18.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5297484A JPS60196558A (en) | 1984-03-19 | 1984-03-19 | Air conditioning, refrigeration equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5297484A JPS60196558A (en) | 1984-03-19 | 1984-03-19 | Air conditioning, refrigeration equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60196558A JPS60196558A (en) | 1985-10-05 |
| JPH0449024B2 true JPH0449024B2 (en) | 1992-08-10 |
Family
ID=12929864
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5297484A Granted JPS60196558A (en) | 1984-03-19 | 1984-03-19 | Air conditioning, refrigeration equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60196558A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2009281642A (en) * | 2008-05-21 | 2009-12-03 | Daikin Ind Ltd | Heat source device of air conditioning system |
| JP6451212B2 (en) * | 2014-10-30 | 2019-01-16 | 株式会社デンソー | Cooling system |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5355547A (en) * | 1976-10-29 | 1978-05-20 | Agency Of Ind Science & Technol | Heat accumulator |
-
1984
- 1984-03-19 JP JP5297484A patent/JPS60196558A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60196558A (en) | 1985-10-05 |
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