JPH0131121B2 - - Google Patents
Info
- Publication number
- JPH0131121B2 JPH0131121B2 JP56072243A JP7224381A JPH0131121B2 JP H0131121 B2 JPH0131121 B2 JP H0131121B2 JP 56072243 A JP56072243 A JP 56072243A JP 7224381 A JP7224381 A JP 7224381A JP H0131121 B2 JPH0131121 B2 JP H0131121B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- ice
- water
- winding
- spiral
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B7/00—Measuring arrangements characterised by the use of electric or magnetic techniques
- G01B7/02—Measuring arrangements characterised by the use of electric or magnetic techniques for measuring length, width or thickness
- G01B7/06—Measuring arrangements characterised by the use of electric or magnetic techniques for measuring length, width or thickness for measuring thickness
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
Description
【発明の詳細な説明】
本発明は結氷厚さの検出装置に於ける電極構造
に係り、電極棒を取り囲む結氷面が電極棒の存在
に影響されることがなく、結氷厚さに対応する信
号を出すことが出来るようにした結氷厚検出装置
の電極構造に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electrode structure in an ice thickness detection device, in which the ice surface surrounding the electrode rod is not affected by the presence of the electrode rod, and a signal corresponding to the ice thickness can be detected. The present invention relates to an electrode structure of an ice thickness detection device that is capable of detecting ice formation.
従来、例えばアイスバンクと称せられる水の冷
却装置に於ては、その冷却面に成長する結氷厚さ
が最適になるように制御する検出装置がある。電
気的には、結氷時の氷の電気導電度は殆ど零に近
くなるので、これと被冷却水との差異を検出する
ことによつて行うことが出来るものであるが、こ
れに用いられる電極棒は結氷の成長時及び融氷時
の何れに於ても結氷面に常に追従性を持たせなけ
ればならないものである。然し例えば、鋼材のよ
うな熱伝導の良好な素材で構成された電極棒の場
合には、結氷時に冷却面が低温度に冷却されて、
電極棒は結氷面よりの冷却で冷却水側が早期に冷
却されて氷で覆われ、融氷時には電極棒を通して
被冷却水側より結氷側に熱が伝導され、早期に電
極棒を囲む部分が融氷する。このように電極棒を
囲む結氷面が冷却面上の平均結氷面に追従するこ
とが出来ず、結氷面の正しい検出が不可能となる
ものである。 BACKGROUND ART Conventionally, for example, in a water cooling device called an ice bank, there is a detection device that controls the thickness of ice that grows on the cooling surface to be optimal. Electrically, the electrical conductivity of ice when it freezes is almost zero, so this can be done by detecting the difference between this and the water to be cooled, but the electrodes used for this The rod must always have the ability to follow the ice surface both when the ice is growing and when it is melting. However, for example, in the case of an electrode rod made of a material with good thermal conductivity, such as steel, the cooling surface is cooled to a low temperature when it freezes.
As the electrode rod is cooled from the frozen surface, the cooling water side is quickly cooled and covered with ice, and when the ice melts, heat is conducted from the cooled water side to the frozen side through the electrode rod, and the area surrounding the electrode rod quickly melts. Ice. In this way, the frozen surface surrounding the electrode rod cannot follow the average frozen surface on the cooling surface, making it impossible to accurately detect the frozen surface.
本発明は此の点に鑑み行われたもので、熱伝導
率が氷のそれよりも小さな値を有し、電気絶縁性
のある巻心棒の外周に金属細線を螺旋状に巻装し
て電極棒となし、冷却面に垂直に取りつけるよう
にしたものである。 The present invention has been made in view of this point, and has a thermal conductivity smaller than that of ice, and is an electrically insulating mandrel. It is a rod and is attached perpendicularly to the cooling surface.
銅材を電極とした場合は、その熱の伝導率が大
きいためこのような電極が不適当であることは前
述の通りであるが、これを本発明のようにするこ
とにより、電極棒の軸方向の熱伝導は金属細線の
巻線ピツチと前記巻心棒の軸方向の熱伝導の和と
なり、その値は見掛け上、小ならしめることが出
来る訳である。前記銅線に比較し、熱伝導の小さ
いステンレス線の如きものを使用することによ
り、電極を囲む結氷面の追従性を更に優れたもの
にすることが出来るものである。 As mentioned above, when a copper material is used as an electrode, such an electrode is inappropriate due to its high thermal conductivity. However, by making this as in the present invention, the axis of the electrode rod The heat conduction in the direction is the sum of the winding pitch of the thin metal wire and the heat conduction in the axial direction of the winding core, and its value can be made small in appearance. By using a material such as stainless steel wire, which has a lower thermal conductivity than the copper wire, it is possible to improve the ability to follow the frozen surface surrounding the electrode.
更に前記巻心棒に2本の金属細線を並列、等間
隔の二重螺旋状に巻装した電極棒とすることによ
り、2電極間の結氷部分を除いた被冷却水を通し
て電極線に流れる電流を測定することにより、結
氷厚に対して優れた比例特性を持たせることが出
来るものである。 Furthermore, by forming an electrode rod in which two thin metal wires are wound in a double helical manner in parallel and at equal intervals around the core, the current flowing through the electrode wire can be passed through the cooled water excluding the frozen part between the two electrodes. By measuring this, it is possible to have excellent proportionality characteristics with respect to ice thickness.
これを図について説明する。第1図は冷却管面
上の電極棒取付の場合の略図で、イは従来のもの
の場合、ロは本発明によるものゝ場合、第2図イ
は螺旋状に金属細線を巻装した電極棒、ロは二重
螺旋状に金属細線を巻装した電極棒の説明図の一
例である。第1図、第2図に於て、1は冷却管、
2は巻心棒で、その熱伝導率は氷のそれよりも小
さな値を有し、電気的に絶縁性のある材質、3は
熱伝導率の比較的小さなステンレスのような金属
細線で、前記巻心棒2に前記細線3を相互に接触
しない程度の巻線ピツチで巻装した電極棒、3
1,32は2本の金属細線を並列、等間隔の二重
螺旋状に巻装したものでこの電極保持器4を冷却
管1にバンドで締付けられるものとする。5は電
極の導線、6は導線の芯線、7は単極の出力の端
子、71,72は独立2電極の出力端子、8は被
冷却水、9は結氷成長過程の結氷面、10は融氷
過程の結氷面、、2′は従来の電極棒、11は従来
の電極に於ける早期結氷状態、12はその早期融
氷状態、13は螺旋状電極に対する他の電極とし
ての接地側電極14は調節器を示す。 This will be explained with reference to the diagram. Figure 1 is a schematic diagram of the case of mounting an electrode rod on the surface of a cooling pipe, where A is a conventional type, B is a type according to the present invention, and Figure 2 A is an electrode rod wound spirally with a thin metal wire. , B are examples of explanatory diagrams of an electrode rod wrapped with a thin metal wire in a double spiral. In Figures 1 and 2, 1 is a cooling pipe;
2 is a winding core made of an electrically insulating material whose thermal conductivity is smaller than that of ice; 3 is a thin metal wire such as stainless steel with a relatively low thermal conductivity; An electrode rod, 3, in which the thin wire 3 is wound around a mandrel 2 with a winding pitch such that the wires do not touch each other.
Reference numerals 1 and 32 are two thin metal wires wound in parallel and at equal intervals in a double spiral shape, and the electrode holder 4 can be fastened to the cooling pipe 1 with a band. 5 is an electrode conductor, 6 is a core wire of the conductor, 7 is a single-pole output terminal, 71 and 72 are independent two-electrode output terminals, 8 is water to be cooled, 9 is a frozen surface in the process of freezing, and 10 is a melting surface. The freezing surface of the ice process, 2' is the conventional electrode rod, 11 is the early freezing state of the conventional electrode, 12 is its early melting state, 13 is the ground side electrode 14 as the other electrode for the spiral electrode. indicates a regulator.
先づ、冷却管1内の冷媒の蒸発潜熱で冷却が行
われるものとすれば、被冷却水8中に置かれる冷
却管1面上に結氷が行われる。第1図イのように
従来の電極の場合には電極2′を通して冷却が早
期に行われ、遂には結氷面が電極棒2′の先端に
達する以前に結氷で覆われ11に示すような形状
を呈することになり、融氷時には早期融氷のため
に12のような形状を呈することになる。従つて
被冷却水8を通して電極棒2′に流れる電流は結
氷面によつて増減するものゝ、その電流値は結氷
面に対し常に対応することが出来ず、このために
電極を通して流れる出力電流は結氷及び結氷時に
対して履歴現象を起こし調整器14の結氷厚の制
御が出来なくなるものである。 First, if cooling is performed using the latent heat of vaporization of the refrigerant in the cooling pipe 1, ice will form on the surface of the cooling pipe 1 placed in the water to be cooled 8. In the case of a conventional electrode as shown in FIG. When the ice melts, it will take on a shape like 12 due to early ice melting. Therefore, the current flowing through the cooled water 8 to the electrode rod 2' increases or decreases depending on the frozen surface, but the current value cannot always correspond to the frozen surface, and for this reason, the output current flowing through the electrode is A hysteresis phenomenon occurs when freezing occurs, and the regulator 14 becomes unable to control the thickness of the ice.
本発明に於ては巻心棒2の熱伝導率は氷のそれ
よりは小さく、電気絶縁性を有する巻心棒の外周
に金属細線を螺旋状に巻装して電極棒を構成して
いるので、螺旋状に巻装されている金属細線を通
しての熱伝導は外周方向で行われることになり電
極の軸心方向の熱の移動は金属細線の巻線ピツチ
と巻心棒自体の熱伝導との和となり、見掛上は電
極の軸心にそつての熱の移動が阻止されたことに
なり、第1図イに示したような早期結氷状態11
や、早期融氷状態12のような現象の生ずること
がなくなるものである。 In the present invention, the thermal conductivity of the winding core 2 is lower than that of ice, and the electrode rod is constructed by winding a thin metal wire spirally around the outer periphery of the winding core, which has electrical insulation properties. Heat conduction through the spirally wound metal wire occurs in the direction of the outer periphery, and the heat transfer in the axial direction of the electrode is the sum of the winding pitch of the metal wire and the heat conduction of the winding core itself. , the movement of heat along the axis of the electrode is apparently blocked, resulting in an early freezing state 11 as shown in Figure 1A.
This eliminates the occurrence of phenomena such as ice melting and early ice melting state 12.
即ち電極3を囲む結氷は冷却管1の結氷と同一
結氷面となり、接地電極13との間の被冷却水8
を通して流れる電流値は常に結氷面に対応した電
流が流れることになる。この電流値で冷却管を流
れる冷媒量を制御し、結氷面の厚みの制御を確実
に行わせることが出来るものである。 In other words, the ice surrounding the electrode 3 forms the same surface as the ice in the cooling pipe 1, and the cooled water 8 between it and the ground electrode 13
The current value flowing through the ice cap will always correspond to the frozen surface. This current value can be used to control the amount of refrigerant flowing through the cooling pipe, thereby making it possible to reliably control the thickness of the frozen surface.
次に第2図ロに示すように2本の金属細線3
1,32を並列、等間隔の二重螺旋状に巻装した
電極では2電極31,32間の金属細線は互いに
近接した2本の平行線間の被冷却水を通して電流
が流れることになり、結氷により電極となる金属
細線の長さが短縮されるので、それに対応する電
流は減少することになり、結氷厚さと電極間電流
との間の比例関係は著しく優れたものになるもの
である。 Next, as shown in Figure 2B, two thin metal wires 3
In the case where electrodes 1 and 32 are wound in parallel in a double helical pattern with equal spacing, current flows through the cooled water between the thin metal wires between the two electrodes 31 and 32, which are close to each other. Since the length of the thin metal wire serving as the electrode is shortened due to freezing, the corresponding current decreases, and the proportional relationship between the thickness of the ice and the current between the electrodes becomes extremely excellent.
勿論電極棒の見掛け上の熱伝導を適当な値にす
ることは、前述のような巻心棒の表面上に半導体
や他の金属の蒸着、其の他類似の方法によつても
可能であり、思想的にはこのようなものも本発明
に含まれるものである。 Of course, it is also possible to set the apparent heat conduction of the electrode rod to an appropriate value by vapor depositing a semiconductor or other metal on the surface of the core rod as described above, or by other similar methods. Conceptually, such things are also included in the present invention.
本発明は以上のような構造の結氷厚検出電極と
したために、結氷管面の結氷厚に対し、電極を取
り囲む結氷面が結氷の成長時及び融氷時の何れに
も常に追従し、極めて簡単な構造を有する螺旋状
金属細線による電極棒によつて高度の制御精度及
び出力特性が得られるものである。 Since the present invention has an ice thickness detection electrode having the above-described structure, the ice surface surrounding the electrode always follows the ice thickness on the ice tube surface both during the growth and melting of the ice, which is extremely simple. A high degree of control accuracy and output characteristics can be obtained by using an electrode rod made of a spiral metal wire having a similar structure.
第1図は結氷厚検出用電極の取付略図でイは従
来の電極の場合、ロは本考案による電極の場合、
第2図イ,ロは電極の詳細図の一例、
1……冷却管、2……巻心棒、3……単極金属
細線、4……電極保持器、5……電極導線、6…
…導線の芯線、7……単極出力端子、8……被冷
却水、9……結氷成長過程の結氷面、10……融
氷過程の結氷面、2′……従来の電極棒、11…
…従来の早期結氷状態、12……従来の早期融氷
状態、13……接地側電極、14……調節器、3
1,32……螺旋状金属細線、71,72……2
電極出力端子。
Figure 1 is a schematic diagram of the installation of the electrode for detecting ice thickness, where A is the conventional electrode, B is the electrode according to the present invention,
Figure 2 A and B are examples of detailed diagrams of electrodes. 1...Cooling pipe, 2...Winding rod, 3...Monopolar thin metal wire, 4...Electrode holder, 5...Electrode conductor wire, 6...
... Core wire of conductor, 7 ... Unipolar output terminal, 8 ... Water to be cooled, 9 ... Frozen surface in the process of freezing and growth, 10 ... Frozen surface in the process of melting, 2' ... Conventional electrode rod, 11 …
... Conventional early freezing state, 12 ... Conventional early ice melting state, 13 ... Ground side electrode, 14 ... Adjuster, 3
1, 32... spiral metal thin wire, 71, 72... 2
Electrode output terminal.
Claims (1)
成長する結氷厚検出装置の電極に於て、熱伝導率
が氷のそれよりは小さな値を有し、電気的絶縁性
を有する巻心棒の外周に金属細線を螺旋状に巻装
して電極棒となし、結氷部分を除いた被冷却水部
分を通して水中にある他の電極と螺旋状電極との
間に流れる電流で結氷厚検出を行うことを特徴と
する結氷厚検出装置の電極構造。 2 前記他の電極が前記螺旋状電極に対して並
行、等間隔に金属細線を前記巻心棒に二重螺旋状
に巻装したものである特許請求の範囲第1項記載
の結氷厚検出装置の電極構造。[Claims] 1. In an electrode of an ice thickness detection device that grows on a cooling surface due to the difference in electrical conductivity between ice and water, the thermal conductivity has a smaller value than that of ice, and the electrical conductivity is smaller than that of ice. The electrode rod is made by winding a thin metal wire in a spiral around the outer periphery of a winding core, which has electrically insulating properties, and the water flows between the spiral electrode and other electrodes in the water through the cooled water portion excluding the frozen portion. An electrode structure of an ice thickness detection device characterized by detecting ice thickness using electric current. 2. The ice formation thickness detecting device according to claim 1, wherein the other electrode is formed by winding fine metal wires around the core in a double helical shape parallel to and at equal intervals with respect to the spiral electrode. Electrode structure.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7224381A JPS57187602A (en) | 1981-05-15 | 1981-05-15 | Construction of electrode for ice thickness detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7224381A JPS57187602A (en) | 1981-05-15 | 1981-05-15 | Construction of electrode for ice thickness detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57187602A JPS57187602A (en) | 1982-11-18 |
| JPH0131121B2 true JPH0131121B2 (en) | 1989-06-23 |
Family
ID=13483650
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7224381A Granted JPS57187602A (en) | 1981-05-15 | 1981-05-15 | Construction of electrode for ice thickness detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57187602A (en) |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62209303A (en) * | 1986-03-11 | 1987-09-14 | Mayekawa Mfg Co Ltd | Freezing thickness detector |
| JPS62186008U (en) * | 1986-05-16 | 1987-11-26 | ||
| JPH0522807Y2 (en) * | 1986-07-14 | 1993-06-11 | ||
| CN105737729A (en) * | 2016-03-02 | 2016-07-06 | 杭州源牌环境设备有限公司 | Ice thickness measurement device used for ice storage coil pipe |
| CN107388700B (en) * | 2017-01-20 | 2020-08-21 | 芯海科技(深圳)股份有限公司 | Refrigerator frost sensor |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5910563Y2 (en) * | 1978-11-08 | 1984-04-03 | 株式会社前川製作所 | Structure of ice thickness detection electrode |
-
1981
- 1981-05-15 JP JP7224381A patent/JPS57187602A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57187602A (en) | 1982-11-18 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5936157A (en) | Thermosensitive flow rate detecting element and flow rate sensor using same | |
| KR910000829B1 (en) | Elongate electrical heaters | |
| EP0431109A1 (en) | Temperature sensor probe for improving time response | |
| US2510986A (en) | Electrically heated pitot tube | |
| US2149448A (en) | Resistance element | |
| JPH0131121B2 (en) | ||
| CN118794553B (en) | Platinum sheet thermal resistance heat flow sensor and preparation method thereof | |
| WO2007053991A1 (en) | Analog linetype constant temp fire detecting cable | |
| CN118794554B (en) | Platinum sheet heat flow sensor with long effective test time and preparation and use method thereof | |
| EP0282780B1 (en) | Method for measuring heat transfer coefficient and sensor including heat transfer element and thermal insulation element | |
| US3497443A (en) | Internal anode for the cathodic rust protection of pipelines | |
| US4338479A (en) | Surface thermocouple assembly and method of making same | |
| JPS5910563Y2 (en) | Structure of ice thickness detection electrode | |
| US3761857A (en) | Resistance wire temperature sensor and method of making same | |
| CN212115714U (en) | Constant temperature heating wire body containing PTC thermal sensitive performance | |
| JP2831659B2 (en) | Heating wire and snow melting wire using it | |
| US1983862A (en) | Soil warming device and method of manufacturing same | |
| KR920002071B1 (en) | Heating sensor manufacturing method using liquid state measure | |
| JP2653451B2 (en) | Method for determining insulation thickness of superconducting conductor | |
| JPH0577737U (en) | Thin film resistance thermometer | |
| US20250258192A1 (en) | Measuring equipment comprising a heating device | |
| JPS6357724B2 (en) | ||
| US3253181A (en) | Grid electrode for an electric discharge tube | |
| CN100430967C (en) | Linear temperature sensing element equipped with fused insulating layer and pressure-sensitive rubber layer | |
| JPH0222661Y2 (en) |