JPH0319064B2 - - Google Patents

Info

Publication number
JPH0319064B2
JPH0319064B2 JP58116401A JP11640183A JPH0319064B2 JP H0319064 B2 JPH0319064 B2 JP H0319064B2 JP 58116401 A JP58116401 A JP 58116401A JP 11640183 A JP11640183 A JP 11640183A JP H0319064 B2 JPH0319064 B2 JP H0319064B2
Authority
JP
Japan
Prior art keywords
mold
cover
electrode plate
convex
attached
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
Application number
JP58116401A
Other languages
Japanese (ja)
Other versions
JPS608066A (en
Inventor
Hiroaki Usui
Isao Morikuni
Hiroshi Ishigaki
Masanobu Myazaki
Masaru Yokoyama
Yasunori Myamoto
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.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works 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 Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP58116401A priority Critical patent/JPS608066A/en
Publication of JPS608066A publication Critical patent/JPS608066A/en
Publication of JPH0319064B2 publication Critical patent/JPH0319064B2/ja
Granted legal-status Critical Current

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  • Finished Plywoods (AREA)
  • Manufacture Of Wood Veneers (AREA)
  • Laminated Bodies (AREA)

Description

【発明の詳細な説明】 〔技術分野〕 この発明はフリツチの製造装置に関するもので
ある。 〔背景技術〕 一般に、フリツチの製造装置は、凸状のわん曲
型面をもつ上型と、凹状のわん曲型面をもつ下型
を備えており、上型と下型との間に、複数枚の素
材単板(木質単板等)を接着剤を介して積層した
積層体を入れて加圧圧締することによりフリツチ
を製造するようになつている。しかしながら、こ
のようにしてフリツチを製造する場合には、接着
剤の硬化がなかなか進まないため、第1図に示す
ように、上型1の型面上に高周波電極板2を取付
けるとともに下型3の型面上にも高周波電極板4
を取付け、素材単板積層体5に対して圧締時に高
周波誘電加熱を施すことが考えだされ、一部です
でに実施されている。ところが、このようにして
高周波誘電加熱を施すと、高周波電極板2,4が
図示のように曲率型であるため高周波電界6に密
なところと疎なところが生じ、電界の密な部分の
温度上昇が大きく疎なところの温度上昇は小さく
なる。高周波誘電加熱は、高温による材の変質防
止等のため、高温部の温度を基準にして行われ
る。そのため、温度上昇の小さいところでは接着
不良が生じるという問題が生じていた。 〔発明の目的〕 この発明は、このような温度差の解消を目的と
するものである。 〔発明の開示〕 この発明は、凸状もしくは凹状のうちの一方の
わん曲型面をもつ上型と、凸状もしくは凹状のう
ちの他方のわん曲型面をもつ下型と、上型および
下型の型面上にそれぞれ形成される高周波電極板
と、凸状の型の高周波電極板の上に取付けられる
ところの中央部が厚く端部が薄いカバーと、凹状
の型の高周波電極板の上に取付けられるところの
中央部が薄く端部が厚いカバーを備え、上記の型
とその型面上に取付けられるカバーとで目標とす
る型面形状が形成され、かつそのカバーがフリツ
チ化の対象となる素材単板積層体よりも比誘電率
および誘電正接のともに小さい材料で構成されて
いることを特徴とするフリツチの製造装置をその
要旨とするものである。 すなわち、上記のような構造にすることによ
り、温度差の解消を実現しうるのである。 つぎに、この発明を詳しく説明する。 第1図に示すような大きくわん曲している電極
板を用いて高周波誘電加熱を施すと、高周波電界
は第1図に細線6で示すように放射状に生じ、電
界強度分布が不均一になる。この電界強度分布を
均一にするためには、上型7を平型にし(第2
図)平板状の電極板8を取付け、さらにその電極
板8に、第1図の上型1の凸状わん曲部と同形状
であつて圧締対象の素材単板積層体5と同じ誘電
特性をもつわん曲型9を取付けるとともに、下型
10および電極板11も上記と同様に構成し、さ
らに電極板11上に素材単板積層体5と同じ誘電
特性をもつわん曲型12を取付け、高周波誘電加
熱を施すことが考えられる。通常、上記わん曲型
9,12は素材単板積層体5と同じ材質の素材で
構成される。このようにすれば、平型である上電
極板8と下電極板11の間の部分(積層体5と型
9,12)は、全て同じ誘電特性(通常は材質も
同じ)となり、平行平板電極の間に素材単板積層
体を入れて高周波誘電加熱することと同じことに
なる。したがつて、高周波電界強度分布は第2図
に細線6で示すように均一となる。しかしなが
ら、このようにすると、素材単板積層体5が加熱
されると同時に、わん曲型9,12も同様に加熱
されるため、これを繰返し使用すると、非常な高
温になり、わん曲型9,12が劣化、変形する。
わん曲型9,12の発熱を抑制するためには、発
熱は次式で求められるため、 P=5/9fεtanδE2×10-10 (W/m3) f:周波数(Hz) ε:比誘電率 tanδ:誘電正接 E:電界強度(V/m) わん曲型9,12の構成材料として、比誘電率
εおよび誘電正接tanδの小さい材料を用いればよ
い。すなわち、比誘電率ε、誘電正接tanδの小さ
い材料を用い、わん曲型9,12とアドミツタン
ス(Y=G+jωC、G=ωεtanδ(A)/(d)、C=ε
(A)/(d))の等しい型に構成すれば、目的を達成し
うる。しかしながら、実際に、わん曲型9,12
全体を単一材料で構成して上記の条件を満たすこ
とは困難である。そこで、積層体5に比べて比誘
電率、誘電正接の小さい材料を用い、中央部が厚
く端部が薄い上型カバーと、中央部が薄く端部が
厚い下型カバーとをつくり、第3図に示すよう
に、凸状部のわん曲度の小さい上型14に電極板
15を介して上型カバー16を取付けるととも
に、凹状部のわん曲度の小さい下型17に電極板
18を介して下型カバー19を取付け、高周波誘
電加熱を施すようにすれば上記の条件を容易に満
たしうるようになる。ここで、上型14、下型1
7のわん曲度は、それぞれカバー16,19で被
覆されたのちの型面形状が目的とする型面形状に
なるように設定される。 つぎに、具体的に上型および下型カバー16,
19の形状およびそれが取付けられる上型14、
下型17の型面形状の設定について第4図を参照
して説明する。 (Step1) 電界強度分布均一化のための条件は、第4図に
おいて、横方向(y一定)で電位差がないことで
あり、 V1=Vy1/d ……(1) V2=Vy2/d ……(2) となる。 (Step2) 上記(1)、(2)式の条件を満たすようにカバー1
6,19の厚みを決定する。 Γ型形状がSin型(対称型)の場合 y1=A(1−sinx/2lπ) ……(3) y2=Asinx/2lπ ……(4) また、カバー16,19と素材単板積層体のア
ドミツタンスYは次式のようになる。 Y=G+jωC=(σ+jωε)ΔS/d ……(5) Y1=(σ1+jωε1)ΔS/d1 ……(6) Y2=(σ2+jωε2)ΔS/d2 ……(7) ここで、流れる電流量は一定であるので VY=V1Y1=V2Y2 ……(8) (8)式に(5)、(6)式を代入して V/V1=Y1/Y=σ1+jωε1/σ+jωε・
d/d1=σ1σ+ω2ε1ε+jω(σε1−σ1ε)/σ2
+ω2ε2・d2/d1……(9) (1)、(9)より d/y1=|V/V1|=√(σ1σ+ω2ε
1ε)2+ω2(σε1−σ1ε)2/σ2+ω2ε2・d/d1 d1=√(σ1σ+ω2ε1ε)2+ω2(σ
ε1−σ1ε)2/σ2+ω2ε2・y1 また、同様に、 d2=√(σ2σ+ω2ε2ε)2+ω2(σ
ε2−σ2ε)2/σ2+ω2ε2・y2 (Step3) つぎに、上記のようにして求められたカバー1
6,19の値を基準にし、カバー16,19で被
覆されたのちの型面形状が目標とするSin型とな
るような上型14、下型17のわん曲度を求め
る。 このわん曲度は、Sin型のある点からその点に
おけるカバー16または19の厚みd1の円を描
き、それらの円の隣接円との接線を結んだものと
なる。(x−a)2+(y−b)2=r2において(x1
y1)座標における接線の方程式は、 (x1−a)(x−a)+(y1−b)(y−b
)=r2 x=a+r2(x1−a)±r(y1−b)√(x1
−a)2+(y1−b)2−r2/(x1−a)2+(y1−b)2
y=b+r2(y1−b)〓r(x1−a)√(x1
−a)2+(y1−b)2−r2/(x1−a)2+(y1−b)2
となる。 このようにして実際に求めたSin型の縮尺3/5の
図を第5図に示す。この場合、素材単板(アガチ
ス単板)積層体のε=17.3、tanδ=1.12であり、
カバー16,19はポリエステル製で、ε=
3.60、tanδ=0.03に設定した。なお、14は上
型、17は下型である。 つぎに、フリツチ製造の具体例について説明す
る。 第3図に示すフリツチの製造装置を用い、つぎ
のようにしてフリツチをつくつた。すなわち、含
水率20〜40%のアガチス脱染色単板(ε=15.5、
tanδ=1.25)を100枚積層し、カバーとしてポリ
エステルシート(ε=3.6、tanδ=0.03)を用い
て高周波誘電加熱成形を行ないフリツチを製造し
た。この際、型形状が正弦波半波長状で、端部角
度が26.6゜の型を用いた。また、カバーの最大厚
みは8.4mmに設定した。高周波誘電加熱による温
度上昇は、従来までのカバーを用いない方法で
は、全体を常温から70℃まで加熱する場合、温度
のばらつきは±20℃程度あつたがカバーを用いる
ことにより温度ばらつきが±8℃以下となり、温
度ばらつきに起因する部分的な接着不良を解消す
ることができた。 〔発明の効果〕 以上のように、この発明のフリツチの製造装置
は、凸状もしくは凹状のうちの一方のわん曲型面
をもつ上型と、凸状もしくは凹状のうちの他方の
わん曲型面をもつ下型と、上型および下型の型面
上にそれぞれ形成される高周波電極板と、凸状の
型の高周波電極板の上に取付けられるところの中
央部が厚く端部が薄いカバーと、凹状の型の高周
波電極板の上に取付けられるところの中央部が薄
く端部が厚いカバーを備え、上記の型とその型面
上に取付けられるカバーとで目標とする型面形状
が形成され、かつそのカバーがフリツチ化の対象
となる素材単板積層体よりも比誘電率および誘電
正接のともに小さい材料で構成されているため、
高周波誘電加熱時の素材単板積層体の温度ばらつ
きを解消しうるようになる。そのため、フリツチ
な部分的な接着不良の発生を防止しうるようにな
る。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to a fritch manufacturing apparatus. [Background Art] In general, a fritsch manufacturing device includes an upper mold having a convex curved surface and a lower mold having a concave curved surface, and between the upper mold and the lower mold, Fritches are manufactured by inserting a laminate in which a plurality of material veneers (wooden veneers, etc.) are laminated with an adhesive and then pressing them together. However, when manufacturing fritches in this way, the curing of the adhesive does not progress easily, so as shown in FIG. A high frequency electrode plate 4 is also placed on the mold surface.
It has been devised to apply high-frequency dielectric heating to the laminated veneer material 5 during pressing, and has already been carried out in some cases. However, when high-frequency dielectric heating is applied in this way, since the high-frequency electrode plates 2 and 4 are curved as shown, the high-frequency electric field 6 has areas where it is dense and areas where it is sparse, and the temperature rises in the areas where the electric field is dense. The temperature rise will be small where the temperature is large and sparse. High-frequency dielectric heating is performed based on the temperature of the high-temperature part in order to prevent deterioration of the material due to high temperatures. Therefore, there has been a problem that poor adhesion occurs in areas where the temperature rise is small. [Object of the Invention] The purpose of the present invention is to eliminate such a temperature difference. [Disclosure of the Invention] The present invention comprises an upper mold having a curved surface that is one of convex or concave, a lower mold having the other curved surface of convex or concave, and the upper mold and A high-frequency electrode plate formed on the mold surface of the lower mold, a cover that is thick in the center and thin at the ends and is attached to the convex high-frequency electrode plate, and a cover that is attached to the convex high-frequency electrode plate, and a concave high-frequency electrode plate. A cover that is attached to the top is thin in the center and thick at the ends, and the target die surface shape is formed by the above mold and the cover attached to the mold surface, and the cover is the object of fritching. The gist of this invention is an apparatus for producing a fritsch characterized by being made of a material having a smaller dielectric constant and dielectric loss tangent than the material laminate of single plates. That is, by adopting the above structure, it is possible to eliminate the temperature difference. Next, this invention will be explained in detail. When high-frequency dielectric heating is performed using a highly curved electrode plate as shown in Figure 1, a high-frequency electric field is generated radially as shown by thin lines 6 in Figure 1, and the electric field intensity distribution becomes non-uniform. . In order to make this electric field intensity distribution uniform, the upper mold 7 should be made flat (second
Figure) A flat electrode plate 8 is attached, and the electrode plate 8 has the same shape as the convex curved part of the upper mold 1 in Figure 1 and the same dielectric material as the material veneer laminate 5 to be pressed. In addition to attaching the curved shape 9 having the characteristics, the lower mold 10 and the electrode plate 11 are configured in the same manner as above, and furthermore, the curved shape 12 having the same dielectric characteristics as the material veneer laminate 5 is attached on the electrode plate 11. , it is possible to apply high-frequency dielectric heating. Usually, the curved shapes 9 and 12 are made of the same material as the material veneer laminate 5. In this way, the portion between the flat upper electrode plate 8 and the lower electrode plate 11 (laminated body 5 and molds 9, 12) will all have the same dielectric properties (usually the same material), and will become parallel flat plates. This is the same as placing a laminate of material veneers between electrodes and subjecting them to high-frequency dielectric heating. Therefore, the high frequency electric field strength distribution becomes uniform as shown by the thin line 6 in FIG. However, in this case, the curved molds 9 and 12 are also heated at the same time as the material veneer laminate 5 is heated, so if this is used repeatedly, the temperature will become extremely high, and the curved molds 9 and 12 will be heated. , 12 deteriorate and deform.
In order to suppress the heat generation of the curved shapes 9 and 12, the heat generation is calculated by the following formula, so P=5/9fεtanδE 2 ×10 -10 (W/m 3 ) f: Frequency (Hz) ε: Specific dielectric Rate tan δ: Dielectric loss tangent E: Electric field strength (V/m) As the constituent material of the curved shapes 9 and 12, a material with a small relative permittivity ε and a small dielectric loss tangent tan δ may be used. That is, using a material with a small dielectric constant ε and a small dielectric loss tangent tan δ, the curved shapes 9 and 12 and the admittance (Y=G+jωC, G=ωεtanδ(A)/(d), C=ε
The purpose can be achieved by configuring it into an equal type (A)/(d)). However, in reality, the curved shape 9, 12
It is difficult to satisfy the above conditions by constructing the entire device from a single material. Therefore, we used a material with a smaller dielectric constant and dielectric loss tangent than the laminate 5 to make an upper mold cover that is thick in the center and thin at the ends, and a lower mold cover that is thin in the center and thick at the ends. As shown in the figure, an upper mold cover 16 is attached to the upper mold 14 whose convex portion has a small degree of curvature through an electrode plate 15, and an electrode plate 18 is attached to the lower mold 17 whose concave portion has a small degree of curvature. The above conditions can be easily met by attaching the lower die cover 19 and applying high frequency dielectric heating. Here, upper mold 14, lower mold 1
The degree of curvature of No. 7 is set so that the shape of the mold surface after being covered with the covers 16 and 19 becomes the desired shape of the mold surface. Next, specifically, the upper mold cover 16 and the lower mold cover 16,
19 shape and the upper mold 14 to which it is attached,
Setting the mold surface shape of the lower mold 17 will be explained with reference to FIG. 4. (Step 1) In Fig. 4, the conditions for making the electric field intensity distribution uniform are that there is no potential difference in the lateral direction (y constant), and V 1 = Vy 1 /d...(1) V 2 = Vy 2 /d...(2) becomes. (Step 2) Cover 1 to satisfy the conditions of equations (1) and (2) above.
6. Determine the thickness of 19. When the Γ shape is a sin type (symmetrical type) y 1 = A (1-sinx/2lπ) ...(3) y 2 = Asinx/2lπ ...(4) In addition, the covers 16 and 19 and the laminated veneer of the material The admittance Y of the body is expressed as follows. Y=G+jωC=(σ+jωε)ΔS/d...(5) Y 1 =(σ 1 +jωε 1 )ΔS/d 1 ...(6) Y 2 =(σ 2 +jωε 2 )ΔS/d 2 ...(7 ) Here, since the amount of current flowing is constant, VY=V 1 Y 1 = V 2 Y 2 ...(8) Substituting equations (5) and (6) into equation (8), we get V/V 1 = Y 1 /Y=σ 1 +jωε 1 /σ+jωε・
d/d 11 σ+ω 2 ε 1 ε+jω(σε 1 −σ 1 ε)/σ 2
2 ε 2・d 2 /d 1 ...(9) From (1) and (9) d/y 1 = |V/V 1 |=√(σ 1 σ+ω 2 ε
1 ε) 22 (σε 1 −σ 1 ε) 222 ε 2・d/d 1 d 1 =√(σ 1 σ+ω 2 ε 1 ε) 22
ε 1 −σ 1 ε) 222 ε 2y 1Similarly, d 2 =√(σ 2 σ+ω 2 ε 2 ε) 22
ε 2 −σ 2 ε) 222 ε 2・y 2 (Step 3) Next, cover 1 obtained as above
Based on the values of 6 and 19, the degree of curvature of the upper mold 14 and the lower mold 17 is determined so that the mold surface shape after being covered with the covers 16 and 19 becomes the target sin shape. This degree of curvature is obtained by drawing a circle having a thickness d 1 of the cover 16 or 19 at that point from a certain point of the Sin type, and connecting the tangents of these circles with the adjacent circles. (x-a) 2 + (y-b) 2 = r 2 (x 1 ,
The equation of the tangent at the y 1 ) coordinate is (x 1 -a) (x-a) + (y 1 -b) (y-b
)=r 2 x=a+r 2 (x 1 −a)±r(y 1 −b)√(x 1
-a) 2 + (y 1 - b) 2 -r 2 / (x 1 - a) 2 + (y 1 - b) 2
y=b+r 2 (y 1 −b) 〓r(x 1 −a)√(x 1
-a) 2 + (y 1 - b) 2 -r 2 / (x 1 - a) 2 + (y 1 - b) 2
becomes. A 3/5 scale diagram of the Sin type actually obtained in this way is shown in Figure 5. In this case, the material veneer (Agathis veneer) laminate has ε = 17.3 and tan δ = 1.12,
The covers 16 and 19 are made of polyester, and ε=
3.60, tan δ = 0.03. Note that 14 is an upper mold, and 17 is a lower mold. Next, a specific example of flitch manufacturing will be explained. A flitch was manufactured using the flitch manufacturing apparatus shown in FIG. 3 in the following manner. That is, agathis destained veneer with a moisture content of 20-40% (ε = 15.5,
A fritchi was manufactured by laminating 100 sheets of polyester sheet (tan δ = 1.25) and performing high-frequency dielectric heating molding using a polyester sheet (ε = 3.6, tan δ = 0.03) as a cover. At this time, a mold with a sinusoidal half-wavelength shape and an end angle of 26.6° was used. Additionally, the maximum thickness of the cover was set to 8.4mm. Regarding the temperature rise caused by high-frequency dielectric heating, when heating the whole body from room temperature to 70℃ using the conventional method without using a cover, the temperature variation was about ±20℃, but by using a cover, the temperature variation was ±8℃. ℃ or less, and we were able to eliminate the partial adhesion failure caused by temperature variations. [Effects of the Invention] As described above, the fritch manufacturing apparatus of the present invention has an upper mold having a curved surface that is either convex or concave, and a curved surface that is the other curved surface that is convex or concave. A lower mold with a surface, a high-frequency electrode plate formed on the mold surfaces of the upper mold and lower mold, respectively, and a cover that is thick in the center and thin at the ends, which is attached to the high-frequency electrode plate of the convex mold. and a cover that is thin in the center and thick at the ends, which is attached to the high-frequency electrode plate of the concave mold, and the target mold surface shape is formed by the above mold and the cover attached to the mold surface. and the cover is made of a material that has a smaller relative dielectric constant and dielectric loss tangent than the material laminate of single plates to be fritched.
It becomes possible to eliminate temperature variations in the laminate of veneers of material during high-frequency dielectric heating. Therefore, occurrence of partial adhesion failure due to frizz can be prevented.

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

第1図は従来例の説明図、第2図はこの発明の
原理説明図、第3図はこの発明の一実施例の説明
図、第4図はカバー形状および型面形状の設計説
明図、第5図はそれによつて設計された具体例の
説明図である。 14……上型、15,18……電極板、16…
…上型カバー、17……下型、19……下型カバ
ー。
Fig. 1 is an explanatory diagram of a conventional example, Fig. 2 is an explanatory diagram of the principle of the present invention, Fig. 3 is an explanatory diagram of an embodiment of the present invention, Fig. 4 is an explanatory diagram of the design of the cover shape and mold surface shape, FIG. 5 is an explanatory diagram of a specific example designed accordingly. 14... Upper mold, 15, 18... Electrode plate, 16...
...Upper die cover, 17...Lower die, 19...Lower die cover.

Claims (1)

【特許請求の範囲】[Claims] 1 凸状もしくは凹状のうちの一方のわん曲型面
をもつ上型と、凸状もしくは凹状のうちの他方の
わん曲型面をもつ下型と、上型および下型の型面
上にそれぞれ形成される高周波電極板と、凸状の
型の高周波電極板の上に取付けられるところの中
央部が厚く端部が薄いカバーと、凹状の型の高周
波電極板の上に取付けられるところの中央部が薄
く端部が厚いカバーを備え、上記の型とその型面
上に取付けられるカバーとで目標とする型面形状
が形成され、かつそのカバーがフリツチ化の対象
となる素材単板積層体よりも比誘電率および誘電
正接のともに小さい材料で構成されていることを
特徴とするフリツチの製造装置。
1. An upper mold with a curved surface of one of convex or concave shapes, a lower mold with a curved surface of the other of convex or concave shapes, and molds on the mold surfaces of the upper mold and the lower mold, respectively. A high-frequency electrode plate to be formed, a cover that is thick at the center and thin at the ends to be attached to the convex-shaped high-frequency electrode plate, and a center part to be attached to the concave-shaped high-frequency electrode plate. The mold has a cover that is thin and thick at the ends, the target mold surface shape is formed by the above mold and a cover attached to the mold surface, and the cover is made of a laminate of material veneer that is to be fritched. A manufacturing device for a fritsch, characterized in that it is made of a material having a small dielectric constant and a small dielectric loss tangent.
JP58116401A 1983-06-27 1983-06-27 Production unit for flitch Granted JPS608066A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58116401A JPS608066A (en) 1983-06-27 1983-06-27 Production unit for flitch

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58116401A JPS608066A (en) 1983-06-27 1983-06-27 Production unit for flitch

Publications (2)

Publication Number Publication Date
JPS608066A JPS608066A (en) 1985-01-16
JPH0319064B2 true JPH0319064B2 (en) 1991-03-14

Family

ID=14686129

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58116401A Granted JPS608066A (en) 1983-06-27 1983-06-27 Production unit for flitch

Country Status (1)

Country Link
JP (1) JPS608066A (en)

Also Published As

Publication number Publication date
JPS608066A (en) 1985-01-16

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