JPH0145195B2 - - Google Patents
Info
- Publication number
- JPH0145195B2 JPH0145195B2 JP12327084A JP12327084A JPH0145195B2 JP H0145195 B2 JPH0145195 B2 JP H0145195B2 JP 12327084 A JP12327084 A JP 12327084A JP 12327084 A JP12327084 A JP 12327084A JP H0145195 B2 JPH0145195 B2 JP H0145195B2
- Authority
- JP
- Japan
- Prior art keywords
- lining
- heating tube
- steel pipe
- current heating
- long
- 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
- 238000010438 heat treatment Methods 0.000 claims description 34
- 229910000831 Steel Inorganic materials 0.000 claims description 29
- 239000010959 steel Substances 0.000 claims description 29
- 239000004020 conductor Substances 0.000 claims description 13
- 230000005291 magnetic effect Effects 0.000 claims description 12
- 230000005294 ferromagnetic effect Effects 0.000 claims description 9
- 229910052751 metal Inorganic materials 0.000 claims description 7
- 239000002184 metal Substances 0.000 claims description 7
- 238000000034 method Methods 0.000 claims description 7
- HCHKCACWOHOZIP-UHFFFAOYSA-N Zinc Chemical compound [Zn] HCHKCACWOHOZIP-UHFFFAOYSA-N 0.000 claims description 5
- 239000011701 zinc Substances 0.000 claims description 5
- 229910052725 zinc Inorganic materials 0.000 claims description 5
- 229910001369 Brass Inorganic materials 0.000 claims description 3
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 claims description 3
- 229910052782 aluminium Inorganic materials 0.000 claims description 3
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 claims description 3
- 239000010951 brass Substances 0.000 claims description 3
- 229910052802 copper Inorganic materials 0.000 claims description 3
- 239000010949 copper Substances 0.000 claims description 3
- 229910000906 Bronze Inorganic materials 0.000 claims description 2
- 229910000963 austenitic stainless steel Inorganic materials 0.000 claims description 2
- 239000010974 bronze Substances 0.000 claims description 2
- KUNSUQLRTQLHQQ-UHFFFAOYSA-N copper tin Chemical compound [Cu].[Sn] KUNSUQLRTQLHQQ-UHFFFAOYSA-N 0.000 claims description 2
- 238000001514 detection method Methods 0.000 claims description 2
- 230000015556 catabolic process Effects 0.000 claims 1
- 239000011133 lead Substances 0.000 claims 1
- 238000003466 welding Methods 0.000 description 4
- 230000007423 decrease Effects 0.000 description 3
- 230000020169 heat generation Effects 0.000 description 3
- 239000004568 cement Substances 0.000 description 2
- 238000009413 insulation Methods 0.000 description 2
- 239000012212 insulator Substances 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 230000007797 corrosion Effects 0.000 description 1
- 238000005260 corrosion Methods 0.000 description 1
- 230000002500 effect on skin Effects 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 239000003302 ferromagnetic material Substances 0.000 description 1
- 230000006698 induction Effects 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 239000000155 melt Substances 0.000 description 1
- 239000000615 nonconductor Substances 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
Landscapes
- Resistance Heating (AREA)
Description
【発明の詳細な説明】
本発明は1つの交流電源より給電される、好ま
しくはその長さが数Km以上の長距離表皮電流発熱
管内に使用される絶縁電線の縁絶不良、短絡、断
線等の故障位置を交流電源の位置より容易かつ正
確に発見することに関する。DETAILED DESCRIPTION OF THE INVENTION The present invention is intended to prevent poor insulation, short circuits, disconnections, etc. of insulated wires used in long-distance skin current heating tubes, preferably several kilometers in length or more, which are powered by one AC power supply. The present invention relates to finding the location of a fault more easily and accurately than the location of an AC power source.
ここにいう表皮電流発熱管とは原理的に2種類
の回路のものを含む。その第1は第1図に示すよ
うな強磁性発熱鋼管1に絶縁電線又はケーブル2
を通し交流電源4に対しこれらが直列になるよう
に電線3によつて結線されたものである。 The skin current heating tube referred to here includes, in principle, two types of circuits. The first is a ferromagnetic heat-generating steel pipe 1 and an insulated wire or cable 2 as shown in Figure 1.
These are connected in series to an AC power source 4 through an electric wire 3.
その第2は、第2図に示すように強磁性発熱鋼
管1に絶縁電線2を通し、この絶縁電線を1次回
路とし前記鋼管1が2次回路となるようにその両
端部をできるだけ小さいインピーダンス3′で結
んだ誘導型表皮電流発熱管と呼ばれるものであ
る。 The second method is to pass an insulated wire 2 through a ferromagnetic heat-generating steel tube 1 as shown in FIG. It is called an induced type skin current heating tube connected at 3'.
そしてこれらの強磁性管1は、その内表面にの
み電流iが流れ管外表面に流出しないようにそれ
ら管の肉厚が、それを通る交流の表皮の深さの2
倍以上の厚さを持つている。 These ferromagnetic tubes 1 are designed such that the wall thickness of these tubes is 2 times the skin depth of the alternating current passing through them, so that the current i flows only on the inner surface and does not flow out to the outer surface of the tube.
It is more than twice as thick.
尚第1の種類の表皮電流発熱管は特公昭40−
12128号(米国特許第3293407号)に開示され、第
2の種類の表皮電流発熱管は特公昭46−588号
(米国特許第3515837号)に開示されている。 The first type of skin current heating tube was published in the 1970s.
No. 12128 (US Pat. No. 3,293,407), and a second type of skin current heating tube is disclosed in Japanese Patent Publication No. 46-588 (US Pat. No. 3,515,837).
近時このような表皮電流発熱管は、長距離パイ
プラインの加熱保温に用いられ、その長さが数10
Km以上、100Km以上に達するものが実施されてい
る。しかし1つの交流電源より供給される表皮電
流発熱管の長さは10〜20Km程度まであり、しかも
陸上パイプラインが主であつた。 Recently, such skin current heating tubes have been used to heat and insulate long-distance pipelines, and their lengths are several tens of meters long.
Km or more, and those reaching 100 Km or more have been implemented. However, the length of skin current heating tubes supplied by one AC power source is about 10 to 20 km, and land pipelines were the main method.
一方第1図又は第2図に示す表皮電流発熱管に
おいて絶縁電線2に例えば短絡又は断線5が発生
した場合、故障5の電源4よりの位置の発見のた
めに例えばパルスレーダー法が用いられた。 On the other hand, when a short circuit or disconnection 5 occurs in the insulated wire 2 in the skin current heating tube shown in FIG. 1 or FIG. .
しかしこのパルスレーダー法は特願昭58−
213758号「故障区画発見回路を有する表皮電流発
熱管」にも明記した如く、発熱鋼管1が強磁性体
であるため、電圧パルスの減衰が早く、電源より
数Km以遠の故障位置5の発見は困難であつた。 However, this pulse radar method was applied for in 1983.
As stated in No. 213758 "Skin current heating tube with fault section detection circuit", since the heating steel tube 1 is made of ferromagnetic material, the voltage pulse attenuates quickly, making it difficult to detect the fault location 5 located several kilometers away from the power source. It was difficult.
本発明は表皮電流発熱管のもつ特性を損ずるこ
となく、20Km以上までの故障位置5の発見を可能
にしようとするものである。 The present invention is intended to make it possible to discover the fault location 5 up to 20 km or more without impairing the characteristics of the skin current heating tube.
第3図は本発明表皮電流発熱管の断面図である
が、第1又は2図の公知例の強磁性発熱鋼管1と
相違して、1の内面に非磁性金属導体層6をも
つ。 FIG. 3 is a sectional view of the skin current heating tube of the present invention, which, unlike the known ferromagnetic heating steel tube 1 shown in FIGS. 1 and 2, has a non-magnetic metal conductor layer 6 on its inner surface.
第1又は2図の公知の表皮電流発熱管において
は通常電線2の発熱量は全体の10〜30%程度で残
余は鋼管1の内表面において発生される。そして
望ましいことは発熱はできるだけ鋼管1の内表皮
において多く発生させる方が望ましい。それは、
電線2における発熱は絶縁層7を通過して被加熱
物8へ流れるが、通常プラスチツクスである電線
2の絶縁物は電気の絶縁物であると同時に熱絶縁
物であるから、電線の発熱の割合が多いほど導体
2の温度が上昇する。これに反し、鋼管1の内表
皮における発熱は、溶接9などを通して被加熱物
8に流れるが、この部分の熱抵抗は極めて小さ
く、従つて被加熱物8に対する鋼管1の温度上昇
は1℃以下にしかならない。従つて発熱は電線2
よりも、鋼管1の内表皮部分にできるだけ多くな
るように設計した方が、耐熱性の高い絶縁物7を
使用する必要を生ぜしめず、経済性が高くなる。
その目的のためには第1又は2図では電線2に流
れる電流はそのままの大きさで鋼管2に流れるか
ら、鋼管2の内表皮部分の抵抗を電線2のそれよ
り大きくした方が良い。表皮電流発熱管では単に
電流iの管外流出を防止するだけでなく、その表
皮作用を大きくし、この部分の抵抗を高くするた
めに強磁性鋼管を利用している。 In the known skin current heating tube shown in FIGS. 1 and 2, the amount of heat generated by the electric wire 2 is usually about 10 to 30% of the total, and the remainder is generated on the inner surface of the steel tube 1. It is desirable to generate as much heat as possible in the inner skin of the steel pipe 1. it is,
The heat generated in the wire 2 flows through the insulating layer 7 to the object to be heated 8, but since the insulation of the wire 2, which is usually plastic, is both an electrical insulator and a thermal insulator, the heat generated in the wire is reduced. The higher the ratio, the higher the temperature of the conductor 2. On the other hand, the heat generated in the inner skin of the steel pipe 1 flows to the object to be heated 8 through the weld 9, etc., but the thermal resistance of this part is extremely small, and therefore the temperature rise of the steel pipe 1 relative to the object to be heated 8 is less than 1°C. It only becomes. Therefore, the heat is generated by wire 2
It is more economical to design the inner skin portion of the steel pipe 1 to have as much as possible, since there is no need to use the highly heat-resistant insulator 7.
For this purpose, it is better to make the resistance of the inner skin of the steel pipe 2 larger than that of the wire 2, since the current flowing through the wire 2 in FIG. 1 or 2 flows through the steel pipe 2 with the same magnitude. In the skin current heating tube, a ferromagnetic steel tube is used not only to prevent the current i from flowing out of the tube, but also to increase the skin action and increase the resistance of this part.
しかし万一電線2に5のような故障が発生した
時、パルスレーダー法で故障点を発見しようとし
ても、そのパルスの巾は、時間で表わしたとき、
マイクロ秒のオーダーであるから、表皮効果のた
めに等価抵抗が大きくなり、表皮電流発熱管では
非磁性管の場合に比べてパルスの減衰は極めて大
きく、パルスの発生場所即ち測定点から故障点ま
での距離はせいぜい数Kmまでである。 However, in the unlikely event that a fault like that in 5 occurs in wire 2, even if you try to find the fault point using the pulse radar method, the width of the pulse, expressed in time, will be
Since it is on the order of microseconds, the equivalent resistance becomes large due to the skin effect, and the attenuation of the pulse in a skin current heating tube is extremely large compared to that in a non-magnetic tube. The distance is at most several kilometers.
本発明はこの測定可能距離を増大するために行
われた。 The present invention was made to increase this measurable distance.
本発明では発熱管として使用される場合その電
源周波数が10〜100Hzの範囲即ち通常の商用周波
数であるのに対し、パルスレーダー法ではMHzの
オーダであることに着目した。通常このような発
熱管1の電流iの流れる範囲を示す表皮の厚さ
(又は深さ)S(cm)はρを導体の抵抗率(Ωcm)、
μを比透磁率、fを電源の周波数(Hz)としたと
き
であることは良く知られており、鋼管の場合で
ρ1=18×10-6Ωcm、μ=1000、f=60Hz
としたとき(1)式のSは
S1=0.087cm=0.87mm (2)
であるのに対し、例えば非磁性材料の亜鉛の場合
で、μ=1、ρ2=6×10-6、f=1MHzとしたと
きは
S2=0.0123cm=0.123mm (3)
と(2)式の場合の14%程度しかない。 In the present invention, we focused on the fact that when used as a heating tube, the power frequency is in the range of 10 to 100 Hz, that is, a normal commercial frequency, whereas in the pulse radar method, it is on the order of MHz. Normally, the thickness (or depth) S (cm) of the skin, which indicates the range through which the current i flows in the heating tube 1, is expressed as ρ, the resistivity of the conductor (Ωcm),
When μ is the relative magnetic permeability and f is the frequency of the power supply (Hz) It is well known that in the case of steel pipes, S in equation (1) is S 1 = 0.087cm = 0.87mm ( 2) On the other hand, for example, in the case of zinc, a non-magnetic material, when μ=1, ρ 2 =6×10 -6 and f=1MHz, S 2 =0.0123cm=0.123mm (3) It is only about 14% of the case of equation (2).
そこで本発明は強磁性鋼管1の内表面に非磁性
導体6を1〜1000ミクロン、好ましくは3〜500
ミクロン、更に好ましくは10〜300ミクロンの程
度に内張りすることを要旨とする。 Therefore, the present invention provides a non-magnetic conductor 6 on the inner surface of the ferromagnetic steel pipe 1 with a thickness of 1 to 1000 microns, preferably 3 to 500 microns.
The gist is to form an inner lining of about 10 to 300 microns, more preferably about 10 to 300 microns.
前記非磁性導体6として使用しうる材質として
は、亜鉛の他アルミニウム、銅、真ちゆう、オー
ステナイト系ステンレス、青銅等を例示すること
ができる。 Examples of materials that can be used for the non-magnetic conductor 6 include aluminum, copper, brass, austenitic stainless steel, bronze, etc. in addition to zinc.
この内張りによる鋼管の円周方向内表面幅1
cm、鋼管長さ1cm当りの抵抗の減少は、まず内張
りのない場合の抵抗をr1とすると(2)式を利用して
r1=ρ/S1=18×10-6/0.087=2.069×10-4Ω (4)
であるのに対し、内張りの抵抗r2は(3)式を利用し
て
r2=ρ2/S2=6×10-6/0.0123=4.88×10-4Ω (5)
であるから合成抵抗rは
r=r1r2/r1+r2=1.453×10-4Ω (6)
となつて、内張りのない場合の約70%に減少す
る。 The inner surface width in the circumferential direction of the steel pipe due to this lining 1
cm, the decrease in resistance per 1 cm of steel pipe length can be calculated using equation (2), where the resistance without lining is r 1 = ρ/S 1 = 18×10 -6 /0.087 = 2.069 ×10 -4 Ω (4) On the other hand, the resistance r 2 of the lining can be calculated using equation (3): r 2 = ρ 2 /S 2 = 6 × 10 -6 /0.0123 = 4.88 × 10 -4 Ω (5), so the combined resistance r is r=r 1 r 2 /r 1 +r 2 =1.453×10 -4 Ω (6), which is reduced to about 70% of the case without lining.
したがつて以上の場合で内張りのないとき、電
線2の発熱が20%、発熱管1の発熱が80%であつ
たとすると、内張りのために発熱は電流i一定と
すると
20+80×0.7=76(%)
となり、76%に減少することになり、この点では
経済性が悪くなる。しかし、同時に発熱管単位長
当りの電圧は電流iを一定とすると、76%と低く
なり、電線の定格又は電源電圧を一定とすると、
それに応じて単一電源による給電距離は長くなる
という利点がある。以上では理解を容易にするた
めに、内張りの存在による鋼管の表皮の深さへの
影響などを無視しているが、近似的な傾向として
は正しい。 Therefore, in the above case, when there is no lining, if the heat generation of electric wire 2 is 20% and the heat generation of heating tube 1 is 80%, then the heat generation due to the lining is 20 + 80 × 0.7 = 76 (assuming that the current i is constant) %), which would decrease to 76%, making it uneconomical in this respect. However, at the same time, the voltage per unit length of the heating tube is as low as 76% when the current i is constant, and when the wire rating or power supply voltage is constant,
There is an advantage that the power supply distance by a single power supply becomes correspondingly longer. In order to make it easier to understand, the above explanation ignores the influence of the presence of a lining on the depth of the skin of the steel pipe, but the approximate trend is correct.
以上で説明したように内張りの存在によつて発
熱管としての経済性は多少影響を受けるが、亜鉛
のような非磁性内張りによつてパルスレーダーに
よる故障点発見可能距離は20〜40Kmと飛躍的に増
大することが、計算と実験によつて確かめられ
た。 As explained above, the presence of the lining affects the economic efficiency of the tube as a heat generating tube to some extent, but the non-magnetic lining such as zinc allows the distance at which a pulse radar can detect a failure point to be dramatically increased to 20 to 40 km. It was confirmed through calculations and experiments that the
なお例えば発熱鋼管として25Aの鋼管を利用し
た場合、その内径は27.6mmであるから、内張り厚
さを前記の0.123mmとすると有効内径は27.354mm
となるだけで、実用上内径が小さくなつたことに
はならない。 For example, if a 25A steel pipe is used as a heat-generating steel pipe, its inner diameter is 27.6mm, so if the lining thickness is 0.123mm, the effective inner diameter is 27.354mm.
This does not mean that the inner diameter has become smaller in practical terms.
そして既に銅、アルミニウムなどの非磁性導体
を利用する電力ケーブル、同軸ケーブルなどで確
認されている如くパルスレーダー法による故障点
発見可能距離は桁違いに増加する。 As has already been confirmed in power cables, coaxial cables, etc. that use non-magnetic conductors such as copper and aluminum, the distance over which fault points can be found using the pulse radar method increases by an order of magnitude.
又発熱管として以上に述べた経済性の低下をで
きるだけ防止するには、単一電源による発熱管の
長さに縦つて内張りの厚さを変更することも考え
ねばならない。 In addition, in order to prevent as much as possible the above-mentioned decline in economical efficiency of the heating tube, consideration must be given to changing the thickness of the lining along the length of the heating tube powered by a single power source.
さらに内張りの非磁性金属導体層は一種類に限
定される必要はなく、2層以上であつてもよい。
たとえば耐蝕性などの要求があれば、一層は亜鉛
層、もう1層は真ちゆう層の2層とすることも可
能である。 Further, the number of nonmagnetic metal conductor layers forming the lining is not limited to one type, and may be two or more layers.
For example, if there is a requirement for corrosion resistance, it is possible to use two layers, one layer being a zinc layer and the other being a brass layer.
第3図で9は発熱管1と被加熱物8間を固定
し、さらには熱伝達を良くするための溶接又は伝
熱セメントを意味するが溶接の場合、内張りが亜
鉛等の鋼より低温で溶解するものではその一部が
損傷されるかもしれないが、溶接は通常断続的に
行われ、溶接のための加熱時間が短時間であるか
ら損傷部はほんの部分的なものであり、上記本発
明の効果に影響を与える程度には至らない。 In Fig. 3, 9 means welding or heat transfer cement to fix the heat generating tube 1 and the heated object 8 and to improve heat transfer. If the material melts, a part of it may be damaged, but since welding is usually done intermittently and the heating time for welding is short, the damage is only a partial part, and this is not the case in the above book. It does not reach the extent that it affects the effectiveness of the invention.
第1図は公知の直列型表皮電流発熱管、第2図
は公知の誘導型表皮電流発熱管の各縦断面略図
で、1は強磁性発熱鋼管、2は1に通される絶縁
電線又はケーブル、3は接続電線、3′は強磁性
発熱鋼管の両端を接続する低インピーダンスの導
体、4は電源、5は故障点を示す。
第3図は本発明に従つて改良された表皮電流発
熱管の横断面で6は鋼管1の内張り、7は電線2
の絶縁物層、8は被加熱物で例えば加熱を必要と
するパイプライン本管の管壁の一部を示してい
る。9は発熱鋼管1と被加熱物8間を固定しさら
に熱伝達を良くするための溶接又は伝熱セメント
等を示している。
Fig. 1 is a schematic vertical cross-sectional view of a known series-type skin current heating tube, and Fig. 2 is a schematic vertical cross-sectional view of a known induction type skin current heating tube, where 1 is a ferromagnetic heating steel tube, and 2 is an insulated wire or cable passed through 1. , 3 is a connecting wire, 3' is a low impedance conductor connecting both ends of the ferromagnetic heat generating steel pipe, 4 is a power source, and 5 is a failure point. FIG. 3 is a cross section of a skin current heating tube improved according to the present invention, where 6 is the lining of the steel pipe 1, and 7 is the electric wire 2.
The insulating layer 8 indicates an object to be heated, for example, a part of the pipe wall of a pipeline main pipe that requires heating. Reference numeral 9 indicates welding, heat transfer cement, or the like for fixing the heat generating steel pipe 1 and the object to be heated 8 and further improving heat transfer.
Claims (1)
絶縁電線と鋼管を交流電源に対して直列になるよ
うに結線するか、この絶縁電線を1次回路とし、
鋼管が2次回路となるように構成し、かつ鋼管の
肉厚が、鋼管に流れる交流電流の表皮の深さのほ
ぼ2倍以上になるようにしたいわゆる表皮電流発
熱管において、前記絶縁電線が断線又は絶縁破壊
のような故障発生のとき、所定位置より故障点ま
でをレーダーパルス法によつて発見を可能にする
肉厚の非磁性金属導体層を前記鋼管の内表面に内
張りとして少くとも一層もつことを特徴とする内
張りのある長距離表皮電流発熱管。 2 前記内張りである非磁性金属導体層の厚さが
1〜1000ミクロンであることを特徴とする特許請
求範囲第1項記載の内張りのある長距離表皮電流
発熱管。 3 前記内張りである非磁性金属導体層の厚さが
5〜500ミクロンであることを特徴とする特許請
求範囲第2項記載の内張りのある長距離表皮電流
発熱管。 4 前記内張りである非磁性金属導体層の厚さが
10〜300ミクロンであることを特徴とする特許請
求範囲第3項記載の内張りのある長距離表皮電流
発熱管。 5 前記内張りである非磁性金属導体層が亜鉛、
アルミニウム、銅、鉛、真ちゆう、オーステナイ
ト系ステンレス、青銅の内の少なくとも一種から
できていることを特徴とする第1〜5項のいずれ
かに記載の内張りのある長距離表皮電流発熱管。[Claims] 1. Pass an insulated wire through a ferromagnetic steel pipe, connect the insulated wire and the steel pipe in series with an AC power supply, or use the insulated wire as a primary circuit,
In a so-called skin current heating tube configured such that a steel pipe serves as a secondary circuit, and the wall thickness of the steel pipe is approximately twice or more the depth of the skin of an alternating current flowing through the steel pipe, the insulated wire is The inner surface of the steel pipe is lined with at least a thick non-magnetic metal conductor layer that enables detection from a predetermined position to the failure point by the radar pulse method in the event of a failure such as a disconnection or dielectric breakdown. A long-distance skin current heating tube with an inner lining, which is characterized by having a long distance. 2. The long-distance skin current heating tube with a lining as claimed in claim 1, wherein the non-magnetic metal conductor layer serving as the lining has a thickness of 1 to 1000 microns. 3. The long-distance skin current heating tube with a lining as claimed in claim 2, wherein the non-magnetic metal conductor layer serving as the lining has a thickness of 5 to 500 microns. 4 The thickness of the non-magnetic metal conductor layer that is the lining is
The long-distance skin current heating tube with lining as claimed in claim 3, characterized in that the lining is 10 to 300 microns. 5 The non-magnetic metal conductor layer serving as the lining is made of zinc,
6. The lined long-distance skin current heating tube according to any one of items 1 to 5, characterized in that it is made of at least one of aluminum, copper, lead, brass, austenitic stainless steel, and bronze.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12327084A JPS614192A (en) | 1984-06-15 | 1984-06-15 | Lined long distance skin current heating tube |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12327084A JPS614192A (en) | 1984-06-15 | 1984-06-15 | Lined long distance skin current heating tube |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS614192A JPS614192A (en) | 1986-01-10 |
| JPH0145195B2 true JPH0145195B2 (en) | 1989-10-02 |
Family
ID=14856403
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12327084A Granted JPS614192A (en) | 1984-06-15 | 1984-06-15 | Lined long distance skin current heating tube |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS614192A (en) |
-
1984
- 1984-06-15 JP JP12327084A patent/JPS614192A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS614192A (en) | 1986-01-10 |
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