JP4087176B2 - Transparent ice manufacturing apparatus and transparent ice manufacturing method - Google Patents
Transparent ice manufacturing apparatus and transparent ice manufacturing method Download PDFInfo
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Description
【0001】
【発明の属する技術分野】
本発明は家庭用冷蔵庫における透明氷を製造する透明氷製造装置、及び透明氷製造方法に関する。
【0002】
【従来の技術】
従来、家庭用冷蔵庫における透明氷の製氷は、製氷皿に給水後、製氷皿を振動させて、凍結に伴い発生した気泡が氷の中に混入するのを防いだり、製氷する前に空気などの溶存ガスを脱気した水を用いて製氷する方法が採られていた。
【0003】
また、業務用製氷庫では、水を凍結させるための製氷皿を下に向けて噴水上に給水し、製氷皿の側面から徐々に凍らせていく方法が採られていた。更に天然の氷筍に倣って単結晶氷の育成方法などがあった。
【0004】
【発明が解決しようとする課題】
透明氷を製氷する場合の大きな課題は、凍結時に発生する気泡を如何に氷の中に取り込まれないようにするかである。また、硬度の高い井戸水やミネラル水などに存在する硬度イオン成分そのものの析出や硬度イオン成分などの不純物が核となって発生する気泡を防ぐことである。
【0005】
一般の水道水には、硬度イオン成分が15〜30ppm、溶存ガスが20ppm程度含まれている。水が結晶化して氷となる場合には、水が結晶化する速度と結晶化した氷から不純物を排出しようとする速度の兼ね合いによって、透明氷になったり、不透明氷になったりする。
【0006】
特に、溶存空気による不透明氷の生成には、水中における空気の拡散が大きく関わっており、氷と水の界面移動速度が速い場合に、溶存空気が氷内に閉じこめられる。しかし、界面移動速度が遅い場合には、氷内に入り込めない空気分子が、界面近傍の水内に溜まり、空気分子濃度の過剰な領域が形成される。このような過剰空気分子量は、氷の成長とともに次第に多くなり、ある限界を越えると巨視的な空気の泡となり、最終的に進行してきた氷内に閉じこめられる。
【0007】
製氷皿に物理的に振動を与えて、水が結晶化する際に発生した気泡が氷内に閉じ込まれるのを防ぐ方法は、ある程度の透明度はあるが、発生した気泡が小さい場合には、氷と水の界面から気泡が離れず氷内に閉じ込まれるという課題があった。
【0008】
また、結晶化する前に予め脱気してガス成分を除去する方法は、透明氷を作成する上で有効であるが、装置が大がかりになり大幅なコストアップに繋がるだけでなく、製氷に時間がかかると脱気水に再び空気が溶け込み、結晶化するときに気泡が発生して、透明度の高い氷は得られない課題があった。
【0009】
更に、容器のない平坦な部分に水滴を落下させて透明度の高い単結晶氷を製氷する方法があるが、家庭用冷蔵庫や業務用冷凍庫では容器内に製氷する必要があり、氷筍のようにならない課題があった。
【0010】
このように、透明度の高い氷を得ることは困難であるという課題がある。
【0011】
本発明は、上記課題を考慮し、透明度の高い氷を得ることが出来る透明氷製造装置、及び透明氷製造方法を提供することを目的とするものである。
【0012】
【課題を解決するための手段】
上述した課題を解決するために、第1の本発明は、冷凍空間と、
前記冷凍空間に配置され、上部より底部の方が低温に保たれた容器と、
前記容器に給水する給水手段とを備え、
5μm/s以下の製氷速度で製氷し、
前記給水手段は、前記容器の液層部分のうち大気に接する部分が製氷の完了まで凍結しないよう、前記容器の上部より間欠的に給水する透明氷製造装置である。
【0013】
また、第2の本発明は、前記容器の液層部分の厚さは、実質上気泡が形成されない厚さ以下である第1の本発明の透明氷製造装置である。
【0014】
また、第3の本発明は、前記製氷速度は2μm/s以上の速度である第1または2の本発明の透明氷製造装置である。
【0016】
また、第4の本発明は、前記給水手段は、現在給水した水の表面が凍結する前に次回の給水を行い、製氷される氷が所定の厚さになるまで前記給水を繰り返し、
前記給水を停止した際、前記容器内の液層部が凍結するまでは前記容器内の前記液層部の大気に接する部分が凍結しない第1の本発明の透明氷製造装置である。
【0017】
また、第5の本発明は、前記給水手段が給水する間隔は、前記容器内の液層部全体が過冷却にならないような間隔である第1または4の本発明の透明氷製造装置である。
【0018】
また、第6の本発明は、前記容器の側面温度は底面温度より高い第1〜5の本発明のいずれかの透明氷製造装置である。
【0019】
また、第7の本発明は、冷凍空間と、前記冷凍空間に配置され、上部より底部の方が低温に保たれた容器と、前記容器に給水する給水手段とを備えた透明氷製造装置を用いて透明氷を製造する透明氷製造方法であって、
5μm/s以下の製氷速度で製氷し、
前記容器の液層部分のうち大気に接する部分が製氷の完了まで凍結しないよう、前記給水手段により前記容器の上部より間欠的に給水する透明氷製造方法である。
【0020】
【発明の実施の形態】
以下に、本発明の実施の形態の構成をその動作とともに図面を参照して説明する。
【0021】
従来の透明氷の製氷では、水道水や井戸水などに含まれる硬度イオン成分や溶存空気などを如何にして氷の中に入ることなく透明にするかがポイントであるが、本実施の形態は、溶存空気(0℃、1気圧で、約40ppm存在する)を氷の中に取り込まれないようにすると共に液層中で気泡核を発生させないようにして効率よく脱気すると同時に、硬度イオン成分などの不純物を除去することなく、粒界などの氷の中に閉じ込めて、透明な氷を製氷するものである。
【0022】
まず、図示していない給水手段により間欠給水すると気泡の発生を効率よく抑制できるメカニズムについて説明する。
【0023】
図1は、製氷容器1に入れた水が、一部は凍結して氷3となり、一部は水2のまま残っている様子を示す。図1では示していないが、製氷容器1の底部を低温に保つために、冷風を多く当てたり、冷却板を配置し、また製氷容器1の上部を高温に保つためにヒータもしくは断熱材を配置して、製氷容器1の底部温度を例えば−10℃、上部温度を0℃になるようにする。そして、給水手段は、製氷容器1の上部より間欠給水している。
【0024】
製氷速度が非常に速いと氷と水との固液界面で気泡が発生し、白濁の原因となるが、製氷速度が5μm/s以下にすると氷3に取り込まれずに水に押し出された溶存空気4は、気泡とならずに水3の中に溶け込み、更に大気中に放出される。
【0025】
図2に示すように、固液界面の水側には氷から押し出された空気分子が、直ちに液層全体に拡散するのではなく、過剰に存在する領域ができる。製氷速度が速いと、過剰領域の溶存空気分子が限界濃度を超えて気泡核を形成し、周辺に存在する空気分子が流れ込んで一気に気泡となるが、凍結速度が5μm/s以下であると、過剰領域の溶存空気濃度が限界濃度以下となって気泡が発生しない。
【0026】
以下に、気泡核を発生しない理由について説明する。過剰領域で、何らかの原因で溶存空気分子が集合して、直径bの小さな気泡核を形成したとする。気泡が出来る瞬間に水は界面を形成し、初発分子は内部エネルギーを放出して一気に膨張し、気泡内部圧力Pは、静水圧+表面張力とバランスするところまで低下するので次の数1が成立する。
【0027】
【数1】
P=Po + Λ
ここで、Po:静水圧(大気圧+水の重さ≒1気圧)
Λ=4γ/b (γ:表面張力 71dyn/cm)
直径b、表面積sの気泡核が出来た直後に、周囲から微量の分子δnモルが追加流入され、気泡内圧力はPに維持されたままで、分子数が、δnモル増加した分、気泡径が僅かδbだけ大きくなったとした場合、系のエネルギーの変化量δGは、以下のようにして求めることが出来る。
【0028】
すなわち、流入分子のエネルギ解放量及び水の表面エネルギー増加量は次の数2で表される。
【0029】
【数2】
流入分子のエネルギー解放量=−(δn)RT{ln(Ψ/P)}
水の表面エネルギー増加量 =(δs)γ
気泡内の状態方程式は、PV=nRT、気泡の容積はV=πb/6、気泡の表面積はs=πbであり、それぞれの変分は、次の数3で表される。
【0030】
【数3】
δn=(δV)P/RT=(δb)πbP/2RT
δs=2πb(δb)
従って、系のエネルギーの変化量δGは、次の数4となる。
【0031】
【数4】
δG=−(δb)π(b/2)PIn(Ψ/P)+2πbγ(δb)
δG/δb=π(b/2)[−PIn(Ψ/P)+4γ/b]
気泡が成長するためには、気泡径の増大に伴ってエネルギーが減少することである。すなわち、数5が成立することである。
【0032】
【数5】
δG/δb≦0
従って、次の数6が成立する。
【0033】
【数6】
PIn(Ψ/P)≧4γ/b=Λ
気泡内部の最小圧力Ψminは数7のようになる。
【0034】
【数7】
Ψmin=Pexp{Λ/P}
図3に、気泡径bと気泡内の圧力Ψminの関係を示す。図3は、何らかの原因(溶存シリカや硬度イオン成分など)で、気泡径1μm程度の気泡が発生するためには、気泡内圧力を7.9気圧程度にするための過剰空気分子が必要であることを示す。
【0035】
即ち、飽和空気分子濃度(約1気圧)の約8倍の空気分子濃度が必要である。しかし、一度気泡核が発生すると、気泡核内に空気分子が流れ込み一気に気泡内圧力を下げてしまい、安定な気泡として液層内に存在することを意味している。
【0036】
従って、気泡による白濁化を防止するためには、製氷速度が、出来る限り遅い方がよいが、あまり遅いと夏場のように欲しいときに製氷ができない問題を生じる。そこで、検討した結果、製氷速度が、2〜5μm/sなら、体積が10mlの透明氷を1〜2時間で製氷できることを見出した。
【0037】
すなわち、図6に製氷速度と透明度との関係を示す。図6は、製氷開始から所定の時間経過後に製氷された氷の厚みを計測し、その計測された氷の厚みを所定の時間でわり算することによって製氷速度を求めた。そして、製氷された氷の透明度を計測し、製氷速度と製氷された氷の透明度との関係をグラフに示したものである。図6からは、製氷速度が5μm/s以下である場合には製氷された氷の透明度は90%以上であることがわかる。
【0038】
また、製氷された氷を目視し、どの程度の透明感が得られるかを試験してみた。その結果、次のことが判明した。すなわち、透明度が90%以上の氷を目視した場合にはすぐれた透明感が得られた。これに対して、製氷された氷の透明度が90%より低下していくと、急激に目視による透明感が低下していくことがわかった。
【0039】
従って、製氷速度が5μm/s以下である場合には透明感のある氷を製氷することが出来ると言える。
【0040】
図1に示すように、氷3から押し出された溶存空気が水2の中に過剰な空気として存在するが、一回の給水量がたとえば0.2〜1ml程度とすると水2の厚さは0.1〜0.5mm程度と非常に薄く、過剰な空気は水2から更に大気へと放出され、気泡が発生するために必要な過剰空気濃度(飽和空気濃度に対して約8倍)には達しない。
【0041】
すなわち、水2の厚さが厚い場合、空気が水2の中を移動する場合に時間を要するので、水2の空気濃度がかなり上昇し気泡が発生する場合がある。これに対して水2の厚さを0.1〜0.5mm程度と非常に薄くすると、空気が気泡になる前に大気中に放出される。
【0042】
しかし、一回の給水量がこのように少ないと、給水した水全体が過冷却に成りやすくなるので、水2の全体が過冷却となる前に、次の給水を行うことで、固液界面近傍の水2は過冷却のままに保ちつつ、水2の上部は給水した水によって温度が上昇し、水2全体が過冷却となって一瞬にシャーベット状の氷になることを防止している。
【0043】
また、間欠的に給水することによって、常に液層の上部に大気と接する液層面が存在するので過剰空気分子は、気泡核に成らずに液層を伝って大気中に放出される。気泡によって白濁化する主な要因に製氷セル内の水の上部が凍結して過剰空気分子が大気中に放出されないことがあるが、本実施の形態によって、上部の一部は常に液層即ち水であるので、過剰空気分子が氷内に閉じ込められることはない。
【0044】
次に、気泡による白濁化の他に硬度イオン成分の析出による白濁化があるが、水道水や井戸水に含まれる硬度イオン成分などの不純物の析出を防止して透明氷を製氷する方法について説明する。一般に、水道水には、水(H2O)から発生する水素イオン(H+)と水酸イオン(OH-)の他に、溶存空気(O2、N2、CO2など)やCO2の溶解で発生する炭酸水素イオン(HCO3 -)、更にナトリウムイオン(Na+)、カリウムイオン(K+)、カルシウムイオン(Ca2+)、マグネシウムイオン(Mg2+)、塩素イオン(Cl-)、硝酸イオン(NO3 -)、硫酸イオン(SO4 2-)、次亜塩素イオン(OCl-)、ケイ酸イオン(SiO4 4-)など多数存在する。
【0045】
純氷はH2Oの水素結合のみからなり不純物を含まない純度の高い結晶であるが、前述の如く水道水には多くの不純物が存在し、カチオンや一部のアニオンは特別な水処理をしない限り除去できず、水が凍結することによって未凍結水の中に排出されて濃縮され、沈殿物となって凝集すると氷の中に析出物として白濁化する。
【0046】
そこで、一回の給水量を例えば0.2〜1ml程度として、製氷速度を2〜5μm/sの範囲にすると、不純物イオンを未凍結水中に押し出すことなく、一部はイオンの状態で、また一部は析出するが氷の中に閉じ込められて、透明度が90%以上の氷が製氷できることを見出した。即ち、氷の中に不純物が存在しても例えば大きさが1μm以下で且つ凝集しなければ、光の透過率は減少するが、目視できず透明な氷となる。
【0047】
また、図4に示すように製氷容器1の側面温度が、底面温度より少し高いと、不純物は製氷容器側面方向に広く拡散するので、水道水や井戸水に不純物が含まれていても、透明氷が製氷できる。
【0048】
これまでの製氷では、製氷セル内の水を6方向から冷やすことによって凍結させていたため、不純物は氷の中心方向に拡散して氷の中心で析出して透明度を下げていたが、本発明では、ほとんどの不純物は氷の表面方向に拡散するので析出しても目立たなくなり、透明度の高い氷が得られる。
【0049】
図5に、使用する水の硬度と透明度の関係を示す。本発明によると硬度が80ぐらいまで、透明度が90%である氷が得られることが分かる。
【0050】
以上説明したように、本実施の形態によれば、次のような効果を得ることができる。
【0051】
すなわち、家庭用冷蔵庫を用いて製氷した場合、透明度が90%以上の氷を製氷しようとすると4時間以上必要としていたものが、本発明では給水から離氷までの時間は、1〜2時間となり、大幅な時間短縮が可能となった。また、硬度が80ぐらいまで、90%以上の透明度を確保できるので、特別な地域を除き、透明な氷が家庭で手軽に出来るようになった。
【0052】
【発明の効果】
以上説明したところから明らかなように、本発明は、透明度の高い氷を得ることが出来る透明氷製造装置、及び透明氷製造方法を提供することが出来る。
【図面の簡単な説明】
【図1】本発明の実施の形態における製氷容器内での製氷の様子を示す断面図
【図2】本発明の実施の形態における空気分子濃度の変化を示すグラフを示す図
【図3】本発明の実施の形態における気泡径と気泡内圧力の関係を示すグラフを示す図
【図4】本発明の実施の形態における不純物の拡散を示す断面図
【図5】本発明の実施の形態における硬度と透明度の関係を示すグラフを示す図
【図6】本発明の実施の形態における製氷速度と透明度との関係を示す図
【符号の説明】
1 製氷容器
2 水
3 氷
4 押し出された溶存空気
5 大気中に放出された溶存空気
41 不純物拡散方向[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a transparent ice manufacturing apparatus and a transparent ice manufacturing method for manufacturing transparent ice in a household refrigerator.
[0002]
[Prior art]
Conventionally, ice making of transparent ice in household refrigerators is performed by shaking the ice tray after supplying water to the ice tray to prevent air bubbles generated by freezing from mixing into the ice, and before making ice The method of making ice using the water which deaerated dissolved gas was taken.
[0003]
Moreover, in the commercial ice store, the ice tray for freezing water was turned downward and water was supplied onto the fountain, and gradually frozen from the side of the ice tray. In addition, there was a method of growing single crystal ice following natural ice cubes.
[0004]
[Problems to be solved by the invention]
A major problem in making clear ice is how to prevent bubbles generated during freezing from being taken into the ice. Another object of the present invention is to prevent precipitation of the hardness ion component itself existing in the well water and mineral water having high hardness and bubbles generated by impurities such as the hardness ion component as a nucleus.
[0005]
General tap water contains about 15 to 30 ppm of hardness ion components and about 20 ppm of dissolved gas. When water crystallizes into ice, it becomes transparent ice or opaque ice depending on the balance between the speed at which water crystallizes and the speed at which impurities are discharged from the crystallized ice.
[0006]
In particular, the generation of opaque ice by dissolved air is greatly related to the diffusion of air in water, and the dissolved air is confined in the ice when the interface movement speed of ice and water is high. However, when the interface moving speed is slow, air molecules that cannot enter ice accumulate in the water in the vicinity of the interface, and a region having an excessive air molecule concentration is formed. Such excess air molecular weight gradually increases with the growth of ice, and when it exceeds a certain limit, it becomes a macroscopic air bubble and is confined in the ice which has finally progressed.
[0007]
The method of preventing the bubbles generated when water crystallizes by physically vibrating the ice tray is somewhat transparent, but if the generated bubbles are small, There was a problem that air bubbles were not separated from the interface between ice and water and were closed in the ice.
[0008]
In addition, the method of degassing and removing the gas component in advance before crystallization is effective for producing transparent ice, but it not only leads to a significant increase in cost due to the large scale of the apparatus, but also the time for ice making. When this occurs, air is dissolved again in the degassed water, and bubbles are generated during crystallization, resulting in a problem that ice with high transparency cannot be obtained.
[0009]
Furthermore, there is a method of making single crystal ice with high transparency by dropping water droplets on a flat part without a container, but it is necessary to make ice in the container in a domestic refrigerator or commercial freezer, There was a problem that was not possible.
[0010]
Thus, there is a problem that it is difficult to obtain ice with high transparency.
[0011]
In view of the above problems, an object of the present invention is to provide a transparent ice manufacturing apparatus and a transparent ice manufacturing method capable of obtaining ice with high transparency.
[0012]
[Means for Solving the Problems]
In order to solve the above-described problem, the first aspect of the present invention includes a frozen space,
A container disposed in the frozen space, the bottom being kept at a lower temperature than the top; and
Water supply means for supplying water to the container,
Ice making at an ice making speed of 5 μm / s or less,
The water supply means, such that the portion in contact with the atmosphere of the liquid layer portion of the container is not binding frozen until the completion of ice making is intermittently feed water to permeable Akirakori manufacturing apparatus from the top of the container.
[0013]
Moreover, 2nd this invention is the transparent ice manufacturing apparatus of 1st this invention whose thickness of the liquid layer part of the said container is below the thickness in which a bubble is not formed substantially.
[0014]
The third aspect of the present invention is the transparent ice manufacturing apparatus according to the first or second aspect of the present invention, wherein the ice making speed is 2 μm / s or more.
[0016]
In addition, according to a fourth aspect of the present invention, the water supply means performs the next water supply before the surface of the currently supplied water freezes, and repeats the water supply until the ice to be made has a predetermined thickness,
The transparent ice manufacturing apparatus according to the first aspect of the present invention is such that when the water supply is stopped, a portion of the liquid layer portion in the container that is in contact with the atmosphere does not freeze until the liquid layer portion in the container is frozen.
[0017]
In addition, the fifth aspect of the present invention is the transparent ice manufacturing apparatus according to the first or fourth aspect of the present invention, wherein the interval at which the water supply means supplies water is such that the entire liquid layer in the container is not overcooled. .
[0018]
The sixth aspect of the present invention is the transparent ice manufacturing apparatus according to any one of the first to fifth aspects of the present invention, wherein the side surface temperature of the container is higher than the bottom surface temperature.
[0019]
The seventh aspect of the present invention is a transparent ice manufacturing apparatus comprising: a refrigerated space; a container disposed in the refrigerated space, the bottom portion being kept at a lower temperature than the top; and a water supply means for supplying water to the container. A method for producing transparent ice using transparent ice,
Ice making at an ice making speed of 5 μm / s or less,
It said that portion in contact with the atmosphere of the liquid layer portion of the container is not frozen until the completion of the ice, which is permeable Akirakori manufacturing process intermittently supply water from the top of the container by the water supply means.
[0020]
DETAILED DESCRIPTION OF THE INVENTION
The configuration of the embodiment of the present invention will be described below with reference to the drawings together with the operation thereof.
[0021]
In the conventional ice making of transparent ice, the point is how to make the hardness ion component or dissolved air contained in tap water or well water transparent without entering into the ice, but this embodiment is Dissolve air (existing at about 40 ppm at 0 ° C and 1 atm) is not desorbed into ice and does not generate bubble nuclei in the liquid layer. Without removing the impurities, it is confined in ice such as grain boundaries to produce transparent ice.
[0022]
First, a mechanism that can efficiently suppress the generation of bubbles when water is intermittently supplied by a water supply means (not shown) will be described.
[0023]
FIG. 1 shows a state in which a part of the water put in the
[0024]
If the ice-making speed is very high, bubbles are generated at the solid-liquid interface between ice and water, causing white turbidity. However, if the ice-making speed is 5 μm / s or less, the dissolved air is not taken into the ice 3 and is pushed out into the water. 4 does not become bubbles but dissolves in water 3 and is released into the atmosphere.
[0025]
As shown in FIG. 2, air molecules pushed out from ice do not immediately diffuse into the entire liquid layer, but an excessively existing area is formed on the water side of the solid-liquid interface. When the ice making speed is fast, the dissolved air molecules in the excess region exceed the limit concentration to form bubble nuclei, and the air molecules existing in the vicinity flow into bubbles at a stretch, but the freezing speed is 5 μm / s or less. Bubbles are not generated because the dissolved air concentration in the excess region is below the limit concentration.
[0026]
The reason why bubble nuclei are not generated will be described below. It is assumed that dissolved air molecules gather for some reason in the excess region to form a bubble nucleus having a small diameter b. At the moment when bubbles are formed, water forms an interface, the initial molecule releases internal energy and expands at once, and the internal pressure P of the bubbles decreases to a point where it balances with hydrostatic pressure + surface tension, so the following
[0027]
[Expression 1]
P = Po + Λ
Where Po: hydrostatic pressure (atmospheric pressure + water weight ≈ 1 atm)
Λ = 4γ / b (γ: surface tension 71 dyn / cm)
Immediately after a bubble nucleus having a diameter b and a surface area s is formed, a small amount of molecule δn mol is additionally flown from the surroundings, the bubble pressure is maintained at P, and the number of molecules is increased by δn mol. Assuming that δb is increased by a small amount, the amount of change δG in the system energy can be obtained as follows.
[0028]
That is, the energy release amount of the inflowing molecules and the surface energy increase amount of the water are expressed by the following formula 2.
[0029]
[Expression 2]
Energy release amount of inflowing molecule = − (δn) RT {ln (Ψ / P)}
Increase in surface energy of water = (δs) γ
The equation of state inside the bubble is PV = nRT, the volume of the bubble is V = πb / 6, the surface area of the bubble is s = πb, and each variation is expressed by the following equation (3).
[0030]
[Equation 3]
δn = (δV) P / RT = (δb) πbP / 2RT
δs = 2πb (δb)
Therefore, the change amount δG of the energy of the system is expressed by the following formula 4.
[0031]
[Expression 4]
δG = − (δb) π (b / 2) PIn (Ψ / P) + 2πbγ (δb)
δG / δb = π (b / 2) [−PIn (Ψ / P) + 4γ / b]
In order for bubbles to grow, the energy decreases as the bubble diameter increases. That is,
[0032]
[Equation 5]
δG / δb ≦ 0
Therefore, the following formula 6 is established.
[0033]
[Formula 6]
PIn (Ψ / P) ≧ 4γ / b = Λ
The minimum pressure Ψmin inside the bubble is as shown in Equation 7.
[0034]
[Expression 7]
Ψmin = Pexp {Λ / P}
FIG. 3 shows the relationship between the bubble diameter b and the pressure Ψmin in the bubble. FIG. 3 shows that in order to generate bubbles with a bubble diameter of about 1 μm for some reason (dissolved silica, hardness ion component, etc.), excess air molecules are required to make the pressure inside the bubble about 7.9 atm. It shows that.
[0035]
That is, an air molecule concentration of about 8 times the saturated air molecule concentration (about 1 atm) is required. However, once bubble nuclei are generated, air molecules flow into the bubble nuclei, reducing the pressure inside the bubbles at once, meaning that they are present as stable bubbles in the liquid layer.
[0036]
Therefore, in order to prevent white turbidity due to bubbles, the ice making speed is preferably as slow as possible. However, if it is too slow, there is a problem that ice making cannot be performed when desired in summer. As a result, it was found that if the ice making speed is 2 to 5 μm / s, clear ice having a volume of 10 ml can be made in 1 to 2 hours.
[0037]
That is, FIG. 6 shows the relationship between ice making speed and transparency. In FIG. 6, the ice making speed was obtained by measuring the thickness of ice made after a predetermined time elapsed from the start of ice making, and dividing the measured ice thickness by a predetermined time. Then, the transparency of the ice made is measured, and the relationship between the ice making speed and the transparency of the ice made is shown in a graph. From FIG. 6, it can be seen that when the ice making speed is 5 μm / s or less, the transparency of the ice made is 90% or more.
[0038]
In addition, the ice produced was visually observed to test how much transparency was obtained. As a result, the following was found. That is, when the ice having a transparency of 90% or more was visually observed, excellent transparency was obtained. On the other hand, it was found that when the transparency of the ice made was lowered from 90%, the visual transparency suddenly decreased.
[0039]
Therefore, it can be said that transparent ice can be made when the ice making speed is 5 μm / s or less.
[0040]
As shown in FIG. 1, the dissolved air pushed out from the ice 3 exists as excess air in the water 2, but if the amount of water supplied at one time is, for example, about 0.2 to 1 ml, the thickness of the water 2 is It is very thin, about 0.1 to 0.5 mm, and excess air is further released from the water 2 to the atmosphere, resulting in the excess air concentration (about 8 times the saturated air concentration) required for generating bubbles. Does not reach.
[0041]
That is, when the thickness of the water 2 is thick, it takes time for the air to move in the water 2, so that the air concentration of the water 2 may increase considerably and bubbles may be generated. On the other hand, if the thickness of the water 2 is very thin, about 0.1 to 0.5 mm, the air is released into the atmosphere before it becomes bubbles.
[0042]
However, if the amount of water supplied at one time is so small, the whole supplied water is likely to be supercooled. Therefore, by performing the next water supply before the whole water 2 is supercooled, the solid-liquid interface While the water 2 in the vicinity is kept supercooled, the temperature of the upper part of the water 2 is increased by the supplied water, and the whole water 2 is prevented from being supercooled and becoming sherbet-like ice instantly. .
[0043]
Further, by intermittently supplying water, there is always a liquid layer surface in contact with the atmosphere above the liquid layer, so excess air molecules are released into the atmosphere through the liquid layer without forming bubble nuclei. The main cause of white turbidity due to air bubbles is that the upper part of the water in the ice making cell freezes and excess air molecules are not released into the atmosphere. However, according to this embodiment, a part of the upper part is always a liquid layer or water. Therefore, excess air molecules are not trapped in ice.
[0044]
Next, in addition to white turbidity due to bubbles, there is white turbidity due to precipitation of hardness ion components. A method for making transparent ice by preventing precipitation of impurities such as hardness ion components contained in tap water and well water will be described. . In general, tap water includes hydrogen ions (H + ) and hydroxide ions (OH − ) generated from water (H 2 O), dissolved air (O 2 , N 2 , CO 2 etc.) and CO 2 Hydrogen carbonate ions (HCO 3 − ) generated by dissolution of sodium chloride, sodium ions (Na + ), potassium ions (K + ), calcium ions (Ca 2+ ), magnesium ions (Mg 2+ ), chloride ions (Cl −) ), Nitrate ions (NO 3 − ), sulfate ions (SO 4 2− ), hypochlorite ions (OCl − ), and silicate ions (SiO 4 4− ).
[0045]
Pure ice is a high-purity crystal consisting only of hydrogen bonds of H 2 O and containing no impurities, but as mentioned above, there are many impurities in tap water, and cations and some anions are treated with special water treatment. Unless it is removed, the water is frozen and discharged into unfrozen water and concentrated. When it becomes a precipitate and aggregates, it becomes cloudy as a precipitate in ice.
[0046]
Therefore, if the amount of water supplied at one time is, for example, about 0.2 to 1 ml, and the ice making speed is in the range of 2 to 5 μm / s, the impurity ions are not pushed out into the unfrozen water, some are in the state of ions, It was found that some of the precipitates were trapped in ice but could be made into ice having a transparency of 90% or more. That is, even if impurities exist in ice, for example, if the size is 1 μm or less and the particles do not aggregate, the light transmittance is reduced, but the ice cannot be visually observed and becomes transparent ice.
[0047]
Further, as shown in FIG. 4, when the side surface temperature of the
[0048]
In the past ice making, the water in the ice making cell was frozen by cooling from 6 directions, so the impurities diffused toward the center of the ice and precipitated at the center of the ice, lowering the transparency. Most impurities diffuse in the direction of the surface of the ice, so even if they are deposited, they become inconspicuous and ice with high transparency can be obtained.
[0049]
FIG. 5 shows the relationship between the hardness of the water used and the transparency. According to the present invention, it can be seen that ice having a hardness of about 80 and a transparency of 90% can be obtained.
[0050]
As described above, according to the present embodiment, the following effects can be obtained.
[0051]
In other words, when making ice using a household refrigerator, it took 4 hours or more to make ice with a transparency of 90% or more. In the present invention, the time from water supply to deicing is 1 to 2 hours. It was possible to save a lot of time. In addition, transparency of 90% or more can be secured up to a hardness of about 80, so transparent ice can be easily made at home except in special areas.
[0052]
【The invention's effect】
As is apparent from the above description, the present invention can provide a transparent ice manufacturing apparatus and a transparent ice manufacturing method capable of obtaining ice with high transparency.
[Brief description of the drawings]
FIG. 1 is a cross-sectional view showing a state of ice making in an ice making container in an embodiment of the present invention. FIG. 2 is a graph showing a change in air molecule concentration in the embodiment of the present invention. The figure which shows the graph which shows the relationship between the bubble diameter and bubble internal pressure in embodiment of invention. FIG. 4 is sectional drawing which shows the spreading | diffusion of the impurity in embodiment of this invention. FIG. 5 Hardness in embodiment of this invention FIG. 6 is a graph showing the relationship between the transparency and the transparency. FIG. 6 is a diagram showing the relationship between the ice making speed and the transparency in the embodiment of the present invention.
1 Ice making container 2 Water 3 Ice 4 Extruded dissolved
Claims (7)
前記冷凍空間に配置され、上部より底部の方が低温に保たれた容器と、
前記容器に給水する給水手段とを備え、
5μm/s以下の製氷速度で製氷し、
前記給水手段は、前記容器の液層部分のうち大気に接する部分が製氷の完了まで凍結しないよう、前記容器の上部より間欠的に給水する透明氷製造装置。Frozen space,
A container disposed in the frozen space, the bottom being kept at a lower temperature than the top; and
Water supply means for supplying water to the container,
Ice making at an ice making speed of 5 μm / s or less,
The water supply means, such that the portion in contact with the atmosphere of the liquid layer portion of the container is not binding frozen until the completion of ice making, intermittently feed water to permeable Akirakori manufacturing apparatus from the top of the container.
前記給水を停止した際、前記容器内の液層部が凍結するまでは前記容器内の前記液層部の大気に接する部分が凍結しない請求項1記載の透明氷製造装置。The water supply means performs the next water supply before the surface of the currently supplied water freezes, and repeats the water supply until the ice to be made has a predetermined thickness,
The water supply and when stopped, until the liquid layer portion of the container is frozen transparent ice production apparatus according to claim 1, wherein the portion in contact with the atmosphere of the liquid layer portion of the container should not be frozen.
5μm/s以下の製氷速度で製氷し、
前記容器の液層部分のうち大気に接する部分が製氷の完了まで凍結しないよう、前記給水手段により前記容器の上部より間欠的に給水する透明氷製造方法。Transparent ice for producing transparent ice using a transparent ice production apparatus comprising a freezing space, a container disposed in the freezing space, the bottom of which is kept at a lower temperature than the top, and water supply means for supplying water to the container A manufacturing method,
Ice making at an ice making speed of 5 μm / s or less,
Said that portion in contact with the atmosphere of the liquid layer portion of the container is not frozen until the completion of the ice making, Toru Akirakori manufacturing method intermittently supply water from the top of the container by the water supply means.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2002215713A JP4087176B2 (en) | 2002-07-24 | 2002-07-24 | Transparent ice manufacturing apparatus and transparent ice manufacturing method |
| US10/447,878 US6935124B2 (en) | 2002-05-30 | 2003-05-29 | Clear ice making apparatus, clear ice making method and refrigerator |
| EP03012435A EP1367345A3 (en) | 2002-05-30 | 2003-05-30 | Clear ice making apparatus, clear ice making method and refrigerator |
| CN03138144.8A CN1275013C (en) | 2002-05-30 | 2003-05-30 | Equipment for making clear ice cake, method for making clear ice cake and rfrigerator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2002215713A JP4087176B2 (en) | 2002-07-24 | 2002-07-24 | Transparent ice manufacturing apparatus and transparent ice manufacturing method |
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| Publication Number | Publication Date |
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| JP2004060899A JP2004060899A (en) | 2004-02-26 |
| JP2004060899A5 JP2004060899A5 (en) | 2005-10-13 |
| JP4087176B2 true JP4087176B2 (en) | 2008-05-21 |
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| AT512684B1 (en) * | 2012-03-30 | 2014-03-15 | Ibs Inst Fuer Brandschutztechnik Und Sicherheitsforschung Ges M B H | Method for producing ice balls |
| JP6982869B2 (en) * | 2015-11-10 | 2021-12-17 | 江藤酸素株式会社 | Hydrogen-containing ice and its manufacturing method |
| KR101952299B1 (en) * | 2015-11-18 | 2019-02-26 | 삼성전자주식회사 | System and Method for producing clear ice |
| EP3862699B1 (en) * | 2018-10-02 | 2025-08-27 | LG Electronics Inc. | Refrigerator |
| CN112789461B (en) * | 2018-10-02 | 2023-07-14 | Lg电子株式会社 | refrigerator |
| US12085325B2 (en) | 2021-09-08 | 2024-09-10 | Electrolux Home Products, Inc. | Ice maker for a refrigerator and method for producing clear ice |
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