JPS5947712A - Electromagnet device - Google Patents

Electromagnet device

Info

Publication number
JPS5947712A
JPS5947712A JP15756082A JP15756082A JPS5947712A JP S5947712 A JPS5947712 A JP S5947712A JP 15756082 A JP15756082 A JP 15756082A JP 15756082 A JP15756082 A JP 15756082A JP S5947712 A JPS5947712 A JP S5947712A
Authority
JP
Japan
Prior art keywords
iron core
coil
fixed
core
fixed iron
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.)
Pending
Application number
JP15756082A
Other languages
Japanese (ja)
Inventor
Yukio Kishikawa
岸川 幸生
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura Electric Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP15756082A priority Critical patent/JPS5947712A/en
Publication of JPS5947712A publication Critical patent/JPS5947712A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F7/00Magnets
    • H01F7/06Electromagnets; Actuators including electromagnets
    • H01F7/08Electromagnets; Actuators including electromagnets with armatures

Abstract

PURPOSE:To attempt to save energy consumed by an electromagnet device by eliminating its noise and holding its apparent power and power consumption while in operation to the minimum through such an arrangement wherein an AC power source is impressed on a series circuit, and No.1 and No.2 fixed iron cores are magnetically insulated from each other, but they are mechanically interconnected, and No.1 and No.2 movable iron core are also magnetically insulated from each other, but they are also mechanically interconnected. CONSTITUTION:A fixed iron core 1a is wrapped around by a coil 2a, and a movable iron core 3a is arranged opposingly to the fixed iron core 1a. The yoke 16a of the fixed iron core 1a is magnetically insulated by a gap or a nonmagnetic body 14 and it makes a pair with a yoke 16b of another fixed iron core 1b, and under this condition, the fixed iron cores 1a and 1b are mechanically interconnected securely by rivets, etc. while they are magnetically insulated from each other. On the one hand, a movable iron core 3b is arranged opposingly to the fixed iron core 1b, this movable iron core 3b is magnetically insulated from the movable iron core 3a by a gap or a nonmagnetic body 15, and the movable iron cores 3a and 3b are mechanically interconnected securely by rivets, etc. while they are magnetically insulated from each other.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は烏、磁石の改良に関するものである。[Detailed description of the invention] [Technical field of invention] The present invention relates to improvements in crows and magnets.

〔発明の技術的背景〕[Technical background of the invention]

第1図は、従来の電磁石の一例葡示すものである。図に
おいて、1はU字形の固定鉄心で、この固定鉄心1には
コイル2が巻回されている。
FIG. 1 shows an example of a conventional electromagnet. In the figure, reference numeral 1 denotes a U-shaped fixed iron core, and a coil 2 is wound around this fixed iron core 1.

また、固定鉄心1と対向し1つ所定の空隙lを。Also, a predetermined gap l is provided opposite the fixed iron core 1.

隔てて、可動鉄心3が配置されている。A movable iron core 3 is arranged apart from each other.

かかる構成の電磁石は、コイル2に通電すると固定鉄心
1は磁化されて可動鉄心3を吸引し、逆にコイル2への
通電を断つと固定鉄心−1は磁力を失って可動鉄心3は
元の位置に戻る。
In an electromagnet with such a configuration, when the coil 2 is energized, the fixed core 1 is magnetized and attracts the movable core 3, and conversely, when the coil 2 is de-energized, the fixed core 1 loses its magnetic force and the movable core 3 returns to its original state. Return to position.

第2図は、上記コイル2への通電により、可動鉄心3が
固定鉄心1に吸引される電磁吸引力と空隙lとの関係を
示した特性曲線図であシ、縦軸は吸引力を、また横軸は
空隙lを夫々示している。
FIG. 2 is a characteristic curve diagram showing the relationship between the electromagnetic attraction force by which the movable iron core 3 is attracted to the fixed iron core 1 by energizing the coil 2 and the gap l, where the vertical axis represents the attraction force; Further, the horizontal axis indicates the void l.

第3図は、上記電磁石MGの電気的等価回路を示すもの
であシ、図においてa、bは電源に接続する入力端子で
ある。電磁石MGは、一般にリアクタンスωLと抵抗R
が直列接続されたものとなシ、リアクタンスωLと空隙
!との関係は第4図に示す特性曲線のようになる。
FIG. 3 shows an electrical equivalent circuit of the electromagnet MG, in which a and b are input terminals connected to a power source. Electromagnet MG generally has reactance ωL and resistance R.
are connected in series, reactance ωL and air gap! The relationship with is as shown in the characteristic curve shown in FIG.

第5図は、可動鉄心3が固定鉄心Jに吸引された後の、
可動鉄心3に作用する吸引力を示すものであり、図中A
で示される吸引カフ時性曲線はくまとりコイル4で囲1
れた磁極部5aで発生する吸引力を、またBで示される
吸引力!時性曲線はくまとりコイル4て囲まれない磁極
部5bで発生する吸引力を夫々示す。まだ、吸引力特性
曲線Aと吸引力特性量ill B ’c合せた総合吸引
力を吸引力!Fケ性曲糾Cで示す。すなわち、吸引力!
時性曲線Cで示す吸引力でもって、負荷反抗力りに抗し
て’i=J動鉄心3が固定鉄心ノに吸引保持されるもの
である。
FIG. 5 shows the state after the movable core 3 is attracted to the fixed core J.
This shows the suction force acting on the movable iron core 3, and A in the figure
The suction cuff time curve shown in is surrounded by the dark coil 4 and 1
The attraction force generated in the magnetic pole portion 5a, which is also the attraction force indicated by B! The temporal curves each indicate the attractive force generated in the magnetic pole portion 5b that is not surrounded by the bearded coil 4. Still, the total suction power that is the sum of the suction force characteristic curve A and the suction force characteristic quantity ill B 'c is the suction force! It is shown as Fke characteristic curve C. In other words, suction power!
With the suction force shown by the temporal curve C, the 'i=J moving iron core 3 is suctioned and held by the fixed iron core against the load reaction force.

〔背景技術の問題点〕[Problems with background technology]

熟年ら、以上のような従来の電磁石において、くまとり
コイル4が断線した場合には吸引力時性曲線Bで示され
る吸引力が発生しなくなり、また磁極面上にゴミ等の異
物がはさまったような場合には吸引力特性曲線Bで示さ
れる吸引力が極端に小さくなり、いずれの場合も電磁石
よシ騒音が発生することがある。すなわち、総合吸引力
Cが時間の経過とともに負荷反抗勾りより大きくなった
シ小さくなったシする為、可動鉄心3が固定鉄心1に接
離を繰シ返し、この際に騒音が発生するものである。
In the conventional electromagnet as described above, when the bear coil 4 is disconnected, the attractive force shown by the attractive force time curve B is no longer generated, and foreign objects such as dust are caught on the magnetic pole surface. In such cases, the suction force shown by the suction force characteristic curve B becomes extremely small, and in either case, electromagnet noise may occur. In other words, as the overall suction force C becomes larger or smaller than the load resistance gradient over time, the movable core 3 repeatedly approaches and separates from the fixed core 1, and noise is generated at this time. It is.

〔発明の目的〕[Purpose of the invention]

本発明は上記のような事情に鑑みて成されたもので、そ
の目的は騒音の発生をなくすると共に動作中の皮相電力
および消費電力を小さく抑えて省エネルギー化を図るこ
とが可能な電磁石装置を提供することにある。
The present invention was made in view of the above circumstances, and its purpose is to provide an electromagnetic device that can eliminate noise generation and reduce apparent power and power consumption during operation to save energy. It is about providing.

〔発明の概要〕[Summary of the invention]

上記目的を達成するために本発明では、固定鉄心に巻回
されたコイル通電することにより ’OT動鉄心を磁気
吸引する電磁石において、直流端子側に第1のコイルを
接続した交直変換機器の交流端子側に第2のコイルを直
列接続した直列回路に交流電源を印加するように構成し
、上記第1のコイルを巻回した第1の固定鉄心と上記第
2のコイルを巻回した第2の固定鉄心とを磁気絶縁する
と共に機械的に連結し、且つ上記第1、第2の固定鉄心
に夫々対向する第1.第2の可動鉄心をも磁気絶縁する
と共に機械的に連結するようにしたことを特徴とする。
In order to achieve the above object, the present invention provides an electromagnet that magnetically attracts an OT moving iron core by energizing a coil wound around a fixed iron core. It is configured to apply AC power to a series circuit in which a second coil is connected in series on the terminal side, and includes a first fixed iron core around which the first coil is wound and a second fixed iron core around which the second coil is wound. The first fixed core is magnetically insulated and mechanically connected to the fixed core, and is opposed to the first and second fixed cores, respectively. It is characterized in that the second movable iron core is also magnetically insulated and mechanically connected.

〔発明の実施例〕[Embodiments of the invention]

以下本発明を図面に示す一実施例について説明する。第
6図は、本発明による市、磁石装置の枯成例を示すもの
である。図においで、1aはU字形の同定鉄心で、この
固定鉄心1aにはコイル2aが巻回されている。また、
固定鉄心1aと対向し且つ所定の空隙lを隔ててuJ動
鉄心3aが配置される。上記固定鉄心1aの、コイル2
aが巻回されていない継鉄部161Lは、空隙もしくは
非磁性体14にてイ1d気絶縁が施されて、他の固定鉄
・し1bのコイル2bが巻回されていない継鉄部16b
と一対奮なした状態で、上記各固定鉄心1aと1bが図
示しないリベット等により機械的に、しかも固定鉄心1
aと)bが磁気絶縁された状態で強固に連結される〇一
方、上記側の固定鉄心1bと対向し且つ所定の空1)i
! / ’に隔てて可動鉄心3bが配置4されるが、こ
のd」動鉄心3bも可動鉄心3aと空隙もしくは非磁性
体15にて磁気絶縁が施されて、図示しないリベット等
によシ機械的に、しかも可動鉄心3aと3bが磁気絶縁
された状態で強固に連結される。なお、可動鉄心3bと
固定鉄心1a、および可動鉄心3aと固定鉄心1bとが
それぞれ磁気絶縁されるように、空隙もしくは非磁性体
14.15が設置される。さらに、上記コイル2aの一
端は電源の接続端子aとなシ、他端は交1N変換機器1
3の交流入力11111の一端に接続され、且つ交直変
換機器13の他端が電源の接続端子すとなる。そして、
交直変換機器13の直流出力側には、上記コイル2bが
接続される。なお、本電磁石の電気的等価回路を示すと
第7図のようになる。MGaは交流励磁の、MGbは直
流励磁の電磁石である。
An embodiment of the present invention shown in the drawings will be described below. FIG. 6 shows an example of a dry magnet device according to the present invention. In the figure, 1a is a U-shaped identification core, and a coil 2a is wound around this fixed core 1a. Also,
A uJ dynamic core 3a is arranged opposite to the fixed core 1a and separated by a predetermined gap l. Coil 2 of the fixed iron core 1a
The yoke part 161L where a is not wound is insulated by air gap or non-magnetic material 14, and the yoke part 16b where the coil 2b of the other fixed iron 1b is not wound.
In this state, each of the fixed cores 1a and 1b is mechanically fixed with rivets (not shown), and the fixed core 1
a and ) b are firmly connected in a magnetically insulated state. On the other hand, a predetermined space 1) i facing the fixed iron core 1b on the above side
! A movable iron core 3b is placed 4 apart from the movable iron core 3b, and this moving iron core 3b is also magnetically insulated from the movable iron core 3a by an air gap or a non-magnetic material 15, and is mechanically insulated by a rivet or the like (not shown). Furthermore, the movable cores 3a and 3b are firmly connected in a magnetically insulated state. Note that air gaps or non-magnetic bodies 14, 15 are installed so that the movable iron core 3b and the fixed iron core 1a and the movable iron core 3a and the fixed iron core 1b are magnetically insulated. Further, one end of the coil 2a is connected to the power supply connection terminal a, and the other end is connected to the AC 1N converter 1.
3, and the other end of the AC/DC converter device 13 serves as a power supply connection terminal. and,
The coil 2b is connected to the DC output side of the AC/DC conversion device 13. The electrical equivalent circuit of this electromagnet is shown in FIG. MGa is an AC-excited electromagnet, and MGb is a DC-excited electromagnet.

かかる構成の電磁石装置において、電源端子aとbに交
流電圧を印加する場合、コイル21Lと固定鉄心1aと
可動鉄心3aとからなる電磁石MGiのりアクタンスω
Liは、第4図に示すように空隙lが大きいときは小さ
く、空隙lが/hさいときは大きく力る。ところが、コ
イル2bと固定鉄心1bとn」動鉄心3bとからなる″
[h磁石、〜iGhのリアクタンスωLb(りI’、 
、空隙eによって変化することはない1.このため、市
、源端子aとbに印加さtまた父所1;、圧sr’、 
tt:f−、空隙lが大きいときd、コイル21]にそ
のほとんどが電力11されることになり、空隙lが小さ
いときはコイル2aにも印加さtすることになる。
In an electromagnet device having such a configuration, when an alternating current voltage is applied to power supply terminals a and b, the actance of the electromagnet MGi consisting of the coil 21L, fixed iron core 1a, and movable iron core 3a is
As shown in FIG. 4, when the gap l is large, the force is small, and when the gap l is /h small, the force is large. However, it consists of a coil 2b, a fixed iron core 1b, and a moving iron core 3b.
[h magnet, ~iGh reactance ωLb(riI',
, does not change due to the gap e1. For this, the pressure sr' applied to the source terminals a and b is also the source 1;
tt:f-, when the air gap l is large, d, most of the electric power 11 is applied to the coil 21], and when the air gap l is small, the electric power 11 is also applied to the coil 2a.

このことを数式を用いて詳述すると、電磁石■Gaのイ
ンぎ一グンスをZ $1 、’Fl¥、磁石MGbのイ
ンピーダンスf ”7. bとすると、コイル2bに印
加されるtti圧E2b+−,3二 にて表わされる。
To explain this in detail using a mathematical formula, if the force of the electromagnet ■Ga is Z $1,'Fl\, and the impedance of the magnet MGb is f''7.b, then the tti pressure applied to the coil 2b is E2b+- , 32.

上記したようKZbはtlは一定であるが、Z2は空隙
eによって変化する。空隙lが大きいとき、インピーダ
ンスZ8がZbに比べて伽七?兄できるほど小さいとす
ると、可動鉄心3 a 、 、? b f固定鉄心Ja
+2bに吸引する吸引力は、雷、磁石1vNG1.が大
部分発生することになる。ところが、吸引が完了すると
空隙lが小さくなるからインピ〜・グンスz8も大きく
なり、吸引保持力けMGbとMGaがそれぞれ分担する
ことになる。しかし、インピーダンス(Za+Zb )
は吸引開始前よりも大きくなっているので、吸引完了後
は回路に流れる笥、流が小さくなり、したがって皮相電
力および消費電力が少なくなる。
As described above, in KZb, tl is constant, but Z2 changes depending on the gap e. When the air gap l is large, is the impedance Z8 a little smaller than Zb? Assuming it is small enough to be a big brother, the movable core 3a, ,? b f fixed core Ja
The attraction force that attracts +2b is lightning, magnet 1vNG1. will occur for the most part. However, when the suction is completed, the gap 1 becomes smaller, so that the impedance z8 also becomes larger, and the suction holding force MGb and MGa share their respective roles. However, the impedance (Za+Zb)
is larger than before the start of suction, so after suction is completed, the amount of current flowing through the circuit becomes smaller, and therefore the apparent power and power consumption are reduced.

吸引完了後における回動鉄心、9 a 、 3 bに作
用する吸引力を示すと第8図のようになる。図において
、゛電磁石MGaによυ発生する吸引力を示すのが吸引
力特性曲線E、同じりMGbによシ発生する吸引力全示
すのが吸引力特性曲線F1これらを合わせた吸引力を示
すのが吸引力特性曲線Gであり、負荷反抗力りに抗して
可動鉄心Ja+Jbが固定鉄心7a+Jbに吸引保持さ
れているのが判る。
FIG. 8 shows the suction force acting on the rotating iron cores 9a and 3b after suction is completed. In the figure, the attraction force characteristic curve E shows the attraction force generated by the electromagnet MGa, and the attraction force characteristic curve F1 shows the total attraction force generated by the electromagnet MGb. This is the attraction force characteristic curve G, and it can be seen that the movable core Ja+Jb is attracted and held by the fixed core 7a+Jb against the load reaction force.

一方、電磁石MG bは直流磁励されるため、吸引力特
性曲線Fで示されるように吸引力は脈動することがなく
、負荷反抗力りよシも大きな吸引力を発生する場合は、
電磁石MGbは騒音音発生じない。
On the other hand, since the electromagnet MG b is magnetically excited with direct current, the attraction force does not pulsate as shown by the attraction force characteristic curve F, and when it generates an attraction force that is larger than the load reaction force,
Electromagnet MGb does not generate noise.

以上のように電磁石MGbとMGaを上手にバランスよ
く設計すれば、吸引後の省エネルギーを図ることができ
、しかも直流励磁によシ無騒音とすることができる。
As described above, if the electromagnets MGb and MGa are designed in a well-balanced manner, it is possible to save energy after attraction, and moreover, it is possible to achieve noiseless DC excitation.

上述したように本電磁石装置は、互いに磁気的に絶縁さ
れた電磁石MGa、MGbを機械的に連結し、その一方
の電磁石MGai交流励磁するとともに、この電磁石M
G、と電気的に直列接続された他方の電磁石MGbt”
直流励磁するように構成し、電磁石の投入動作時は電源
電圧の大部公金直流励磁のコイルに印加し、吸引後は上
記2種類の電磁石MGa+ MGbの吸引力で吸引保持
するとともに、夫々のインピーダンスZB y Zbの
ベクトル和によって制限される回路電流を小さくし得る
ので、吸引後の省エネルギー化を図ることができ、しか
も直流励磁による吸引力が作用するので、電磁石は無騒
音とすることができ、極めて信頼性の高いものが得られ
る。
As described above, this electromagnet device mechanically connects electromagnets MGa and MGb that are magnetically insulated from each other, and excites one of the electromagnets MGai with alternating current, and this electromagnet M
G, and the other electromagnet MGbt electrically connected in series.
It is configured to be DC excited, and when the electromagnet is turned on, the power supply voltage is applied to the DC excitation coil, and after attraction, it is attracted and held by the attraction force of the two types of electromagnets MGa + MGb, and the respective impedances are Since the circuit current limited by the vector sum of ZB y Zb can be reduced, it is possible to save energy after attraction, and since the attraction force due to DC excitation is applied, the electromagnet can be made noiseless. An extremely reliable product can be obtained.

〔発明の@米〕[Invention @rice]

以上説明したように本発明によれは、騒音の発生をなく
すると共に動作中の皮相電力および消費電力を小さく抑
えて省エネルギー化を図ることが可能な信頼性の高い′
出磁石装買が得供できる。
As explained above, the present invention provides a highly reliable system that can eliminate noise generation and reduce apparent power consumption and power consumption during operation to save energy.
You can get good deals on magnet equipment.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来の電磁石の一例を示す図、第2図は交流励
磁される電磁石における固定鉄心と可動鉄心との間の空
隙□吸引力特性曲線す図、第3図は交流励磁される’4
. Ti1石の隼気的等価回路を示す構成図、第4図は
父流励(144される電磁石における固定鉄心と可動鉄
心との間の空隙−リアクタンス特性を示す特性図、第5
図および第8図社従来の市、磁石および本発明のTi磁
石の吸引完了後の可動鉄心と固定1決心に作用4する吸
引力特性を示す図、第6図は本発明の一実施例を示す構
成図、第7図は氷見1、す4り電磁石の山気的等価回路
を示す構成図である。 1 + 1 a 、 1 b−−−固定鉄心、2.2a
+2b−−s”’:’1イル、3.3a、3b・・・n
J動鉄心、4−(まとりコイル、5a+5b・・・磁極
部、A w B re、E、F、G・・・吸引力特性曲
線、D・・・負荷反抗力、ノ3・・・交直変換機器、1
4.15・・・空隙もしくは非磁性体、16g、16b
・・・継鉄部、MG 、MGa、MGb・・・電磁石、
a、b・・・入力端子、!・・・空隙。 出願人代理人  弁理士 鈴 江 武 彦第1図 第2図 ’z*l (mm) 第1図 第5図 六 □電気角(&) 第6図 第7図 第8図 電気内(腐) 1
Figure 1 is a diagram showing an example of a conventional electromagnet, Figure 2 is a diagram showing the gap between the fixed core and the movable core in an electromagnet that is excited by AC, and the attraction force characteristic curve. 4
.. Figure 4 is a configuration diagram showing the hyalonic equivalent circuit of a Ti1 stone.
Figures 8 and 8 are diagrams showing the attraction force characteristics that act on the movable core and fixed 1 after completion of attraction of the conventional city magnet and the Ti magnet of the present invention, and Figure 6 shows an example of the present invention. FIG. 7 is a block diagram showing a typical equivalent circuit of the Himi 1 and Suri electromagnets. 1 + 1 a, 1 b---fixed core, 2.2a
+2b--s"':'1il, 3.3a, 3b...n
J moving iron core, 4-(cross coil, 5a+5b... magnetic pole part, A w B re, E, F, G... attractive force characteristic curve, D... load reaction force, No. 3... alternating or directing Conversion equipment, 1
4.15... air gap or non-magnetic material, 16g, 16b
...Yoke, MG, MGa, MGb...Electromagnet,
a, b...input terminals,! ...Void. Applicant's representative Patent attorney Takehiko Suzue Figure 1 Figure 2 'z*l (mm) Figure 1 Figure 5 6 Electrical angle (&) Figure 6 Figure 7 Figure 8 Electrical angle (&) 1

Claims (1)

【特許請求の範囲】[Claims] 固定鉄心に巻回されたコイルに通電、することによ、!
l) FIJ動鉄心”c (iH気吸引する電磁石にお
いて、直流端子側に第1のコイルを接続した文面変換機
器の交流端子側に第2のコイルを直列接続した直列回路
に交流電源全印加するように構成し、前記第1のコイル
を巻回した第1の固定鉄心と「)IJ記第2のコイルを
巻回した第2の固定鉄心とを718気絶縁すると共に機
械的に連結し、且つ前記4ル1゜第2の固定鉄心に夫々
対向する第1.第2の可動鉄心をも磁気絶縁すると共に
機械的に連結するようにしたことを特徴とする電磁石装
置。
By energizing the coil wound around the fixed core,!
l) FIJ moving iron core "c" (In an electromagnet that attracts iH air, full AC power is applied to a series circuit in which the first coil is connected to the DC terminal side and the second coil is connected in series to the AC terminal side of the text conversion device. The first fixed iron core around which the first coil is wound and the second fixed iron core around which the second coil is wound are insulated by 718 degrees and mechanically connected, An electromagnet device characterized in that the first and second movable cores, which respectively face the second fixed core, are also magnetically insulated and mechanically connected.
JP15756082A 1982-09-10 1982-09-10 Electromagnet device Pending JPS5947712A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15756082A JPS5947712A (en) 1982-09-10 1982-09-10 Electromagnet device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15756082A JPS5947712A (en) 1982-09-10 1982-09-10 Electromagnet device

Publications (1)

Publication Number Publication Date
JPS5947712A true JPS5947712A (en) 1984-03-17

Family

ID=15652343

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15756082A Pending JPS5947712A (en) 1982-09-10 1982-09-10 Electromagnet device

Country Status (1)

Country Link
JP (1) JPS5947712A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5945361A (en) * 1989-05-18 1999-08-31 Nippon Pillar Packing Co., Ltd. Heat-resistant expansive member

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5945361A (en) * 1989-05-18 1999-08-31 Nippon Pillar Packing Co., Ltd. Heat-resistant expansive member

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