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JPS5925938B2 - microwave heating furnace - Google Patents
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JPS5925938B2 - microwave heating furnace - Google Patents

microwave heating furnace

Info

Publication number
JPS5925938B2
JPS5925938B2 JP2471079A JP2471079A JPS5925938B2 JP S5925938 B2 JPS5925938 B2 JP S5925938B2 JP 2471079 A JP2471079 A JP 2471079A JP 2471079 A JP2471079 A JP 2471079A JP S5925938 B2 JPS5925938 B2 JP S5925938B2
Authority
JP
Japan
Prior art keywords
container
microwave
heating furnace
microwave heating
inner container
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
Application number
JP2471079A
Other languages
Japanese (ja)
Other versions
JPS55118587A (en
Inventor
進 前田
正和 滝
憲治 吉沢
芳文 美濃和
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP2471079A priority Critical patent/JPS5925938B2/en
Publication of JPS55118587A publication Critical patent/JPS55118587A/en
Publication of JPS5925938B2 publication Critical patent/JPS5925938B2/en
Expired legal-status Critical Current

Links

Landscapes

  • Constitution Of High-Frequency Heating (AREA)
  • Vertical, Hearth, Or Arc Furnaces (AREA)
  • Furnace Details (AREA)

Description

【発明の詳細な説明】 この発明はマイクロ波で物質を加熱するマイクロ波加熱
炉に関し、特に高温加熱を効率よく達成するための改良
に関するたとえば、陶器などの焼物を作るのに用いる先
行技術にかかるマイクロ波加熱炉として&A第1図に示
すものがある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a microwave heating furnace that heats substances using microwaves, and in particular relates to improvements for efficiently achieving high temperature heating, for example, related to prior art used for making pottery such as pottery. There is a microwave heating furnace shown in Fig. 1 of &A.

図において、マイクロ波発生装置1は導波管2を介して
マイクロ波オープン3に結合される。マイクロ波オープ
ン3の中には、被加熱物4が配置される。そして、この
被加熱物4は、まず内側容器5によつて囲繞される。こ
の内側容器5は、マイクロ波発熱する物質たとえば酸化
亜鉛を主成分とする金属酸化物で構成される。内側容器
5は中間容器6により囲繞される。この中間容器6はマ
イクロ波損失の小さい耐火断熱体たとえばJIS規格A
類7種で構成される。次に動作について説明する。
In the figure, a microwave generator 1 is coupled to a microwave open 3 via a waveguide 2 . A heated object 4 is placed inside the microwave opener 3 . The object to be heated 4 is first surrounded by the inner container 5. The inner container 5 is made of a material that generates heat by microwaves, such as a metal oxide whose main component is zinc oxide. The inner container 5 is surrounded by an intermediate container 6. This intermediate container 6 is made of a fireproof insulating material with low microwave loss, such as JIS standard A.
It consists of 7 species. Next, the operation will be explained.

マイクロ波発生装置1で発生されたマイクロ波は、導波
管2によつてマイクロ波オープン3に導かれる。このと
き、マイクロ波オープン3内には、各種のモードの共振
電磁界が形成される。この共振電磁界&ち中間容器6を
透過して内側容器5を均一にマイクロ波加熱する。この
マイクロ波加熱により高温度となつた内側容器5の内部
は、均一な熱輻射場が形成され、被加熱物4は均一に加
熱されることになる。つぎに、熱平衡状態における熱効
率について考察する。中間容器6が外径2γ、■0.2
〔M〕の球体、内側容器5が外径2を0=0.1〔M〕
の球体であつて、その外周面が中間容器5の内周面に密
着している形状に構成されている場合の内側容器5の温
度をθ。
Microwaves generated by a microwave generator 1 are guided to a microwave open 3 by a waveguide 2. At this time, resonant electromagnetic fields of various modes are formed within the microwave opener 3. This resonant electromagnetic field is transmitted through the intermediate container 6 to uniformly heat the inner container 5 with microwaves. A uniform heat radiation field is formed inside the inner container 5, which has reached a high temperature due to this microwave heating, and the object to be heated 4 is heated uniformly. Next, consider thermal efficiency in a state of thermal equilibrium. The intermediate container 6 has an outer diameter of 2γ, ■0.2
The sphere of [M], the inner container 5 has an outer diameter 2 of 0 = 0.1 [M]
The temperature of the inner container 5 is θ when the inner container 5 is a spherical body whose outer peripheral surface is in close contact with the inner peripheral surface of the intermediate container 5.

〔℃〕、中間容器6の表面温度をθ、〔℃〕、その周
囲温度をθ。Cc〕、中間容器6の表面積をACM2〕
、その表面から放散される熱量をQCKca/H〕とす
ると、中間容器6の表面温度θ1は、ただしhは熱輻射
を考慮した総括熱伝達係数で、対流による熱伝達係数を
Hcとすると、ここに.、εは中間容器6の熱輻射率で
ある。
[°C], the surface temperature of the intermediate container 6 is θ, [°C], and its ambient temperature is θ. Cc], the surface area of the intermediate container 6 is ACM2]
, the amount of heat dissipated from its surface is QCKca/H], then the surface temperature θ1 of the intermediate container 6 is, where h is the overall heat transfer coefficient considering thermal radiation, and the heat transfer coefficient due to convection is Hc. To. , ε is the thermal emissivity of the intermediate container 6.

つぎに内側容器5の表面温度θ。へただし、kは中間容
器6の熱伝導率〔Kcal/MHdeg〕である。
Next, the surface temperature θ of the inner container 5. where k is the thermal conductivity [Kcal/MHdeg] of the intermediate container 6.

従つて、θoを高くするには、θ1を高く、このために
は総括熱伝達係数hを小さく、このためには中間容器6
の熱輻射率εを小さくすればよいことが判る。中間容器
6は前記のような耐火断熱材で構成されているので、ε
の値は0.8〜0.9程度であり、特にεの小さい物質
は見出されていない。
Therefore, in order to increase θo, θ1 is increased, and for this purpose, the overall heat transfer coefficient h is decreased, and for this purpose, the intermediate vessel 6 is
It can be seen that it is sufficient to reduce the thermal emissivity ε of . Since the intermediate container 6 is made of the above-mentioned fireproof heat insulating material, ε
The value of is about 0.8 to 0.9, and no substance with a particularly small ε has been found.

つぎに具体的な事例について、上記算式に基いて内側容
器5の表面温度θ。
Next, regarding a specific example, the surface temperature θ of the inner container 5 is determined based on the above formula.

を試算した結果を説明する。今、Q二429〔Kcal
/H〕、即ち電力に換算するとP=Q/0.86=50
00の ,Hc=5〔Kcal/M2Hdegl,k=
0.5〔Kcal/M2Hdeg〕 ,ε=0.9,θ
o=20〔℃〕とすると、θo+870〔゜C〕 ,θ
1+190〔゜C〕となる。
We will explain the results of the trial calculation. Now, Q2429 [Kcal
/H], that is, converted to electric power, P=Q/0.86=50
00, Hc=5 [Kcal/M2Hdegl, k=
0.5 [Kcal/M2Hdeg], ε=0.9, θ
If o=20 [°C], θo+870 [°C], θ
It becomes 1+190 [°C].

この例では、内側容器5の温度は陶器などの焼成には低
く、焼成に必要な1200〔℃〕まで昇温させるにはマ
イクロ波人力は700〔w〕を要し、経済的でない。
In this example, the temperature of the inner container 5 is low for firing pottery, etc., and 700 [W] of microwave power is required to raise the temperature to 1200 [° C.] required for firing, which is not economical.

この発明は以上のような考察に基いてなされたもので、
同じマイクロ波入力時において、内側容器をより高温度
に加熱することのできるマイクロ波加熱炉を提供するこ
とを目的とするもので、中間容器6を熱輻射率εの小さ
い物質で形成した外側容器内に収め、この外側容器に設
けた開口部からマイクロ波を照射する構成としたもので
ある。
This invention was made based on the above considerations.
The purpose of this furnace is to provide a microwave heating furnace that can heat the inner container to a higher temperature when the same microwave is input. The container is placed inside the outer container, and microwaves are irradiated through an opening provided in the outer container.

以下、この発明の一実施例を図について説明する。第2
図はこの発明の一実施例の断面図、第3図は第2図一線
における断面図で、中間容器6は熱輻射率εが小さい物
質、たとえば銅材で形成され、表面が研磨されている外
側容器7の中に設置される。なお8はマイクロ波が人射
できるように設けられた開口である。次に、この発明の
動作について説明する。
An embodiment of the present invention will be described below with reference to the drawings. Second
The figure is a sectional view of an embodiment of the present invention, and FIG. 3 is a sectional view taken along the line in FIG. It is placed inside the outer container 7. Note that 8 is an opening provided so that microwaves can be emitted to the person. Next, the operation of this invention will be explained.

今、マイクロ波周波数が2450MHz1外側容器7の
形状が円筒であり、その外側容器内の誘電率が1である
とすると、外側容器7の直径が0.0717〔M〕以上
であると容器内に各種モードの共振電磁界が発生し、こ
の共振電磁界は、中間容器6を透過して内側容器5を均
一にマイクロ波加熱する。つぎに、この実施例における
熱平衡状態における内側容器5の温度θ。を試算した結
果を説明する。内側容器5、および中間容器6は前記試
算例と同じ球体とし、また外側容器7も、計算の便宜上
内径0.2〔M〕の銅製の球体と考え、その熱輻射率ε
−0.05、外側容器6の表面から放散する熱量が電力
に換算して500〔W〕であるとすると、外側容器7の
表面温度θ2キ510〔℃〕 ,θ1+510〔゜C〕
,θo−1200〔℃〕となり、同じマイクロ波人射
電力においてθ。
Now, assuming that the microwave frequency is 2450 MHz, the shape of the outer container 7 is cylindrical, and the dielectric constant inside the outer container is 1, if the diameter of the outer container 7 is 0.0717 [M] or more, Resonant electromagnetic fields of various modes are generated, and this resonant electromagnetic field passes through the intermediate container 6 and uniformly microwaves the inner container 5. Next, the temperature θ of the inner container 5 in the thermal equilibrium state in this example. We will explain the results of the trial calculation. The inner container 5 and the intermediate container 6 are the same spheres as in the above calculation example, and the outer container 7 is also assumed to be a copper sphere with an inner diameter of 0.2 [M] for convenience of calculation, and its thermal emissivity ε
-0.05, and assuming that the amount of heat dissipated from the surface of the outer container 6 is 500 [W] in terms of electric power, the surface temperature of the outer container 7 is θ2 + 510 [°C], θ1 + 510 [°C]
, θo-1200 [°C], and θ at the same microwave radiation power.

は約330〔゜C〕高温度に加熱されることになる。な
お第4図はマイタロ波電力P(W)と内側容器の温度θ
o (℃)との関係を先行技術と本発明について比較し
た特性図で、図中特性Aは先行技術による内側容器の温
度を、特性Bはこの発明に係るものの温度を示している
。なお、上記実施例では外側容器7として銅製の円筒を
用いたものを示したが、熱輻射率εが小さい黄銅、アル
ミニウム、ステンレス鋼、金などの金属またはこれらの
金属でメツキしたものでもよい以上のように、この発明
によれば、被加熱物を収容するマイクロ波発熱する物質
からなる内側容器と、この内側容器を収容するマイクロ
波損失の小さい耐火断熱材からなる中間容器と、この中
間容器を収容する熱輻射率が小さい物質からなり、内部
にマイクロ波が人射し得る開口が設けられている外側容
器と、上記開口から内部にマイクロ波を照射するマイク
ロ波照射装置とを備えたもので、内側容器をより高温度
に加熱することのできるマイクロ波加熱炉が得られる。
will be heated to a high temperature of approximately 330°C. In addition, Fig. 4 shows the miterro wave power P (W) and the temperature θ of the inner container.
o (°C) in the prior art and the present invention. In the figure, characteristic A indicates the temperature of the inner container according to the prior art, and characteristic B indicates the temperature according to the present invention. In the above embodiment, a cylinder made of copper is used as the outer container 7, but metals such as brass, aluminum, stainless steel, gold, etc., which have a small thermal emissivity ε, or materials plated with these metals may also be used. According to the present invention, an inner container made of a substance that generates microwave heat and contains an object to be heated, an intermediate container made of a fireproof heat insulating material with low microwave loss and which contains the inner container, and this intermediate container. An outer container made of a material with a low thermal emissivity that houses the container, and equipped with an opening that allows microwaves to be radiated into the interior, and a microwave irradiation device that irradiates the inside with microwaves from the opening. Thus, a microwave heating furnace capable of heating the inner container to a higher temperature is obtained.

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

第1図は先行技術に係るマイクロ波加熱炉の断面図、第
2図はこの発明の一実施例の断面図、第3図は第2図−
における断面図、第4図は先行技術とこの発明に係る加
熱炉の内側容器の温度を比較した特性図である。 図において、1はマイクロ波発生装置、2は導波管、3
はマイクロ波オーブン、4は被加熱物、5は内側容器、
6は中間容器、7は外側容器、8は開口である。
FIG. 1 is a sectional view of a microwave heating furnace according to the prior art, FIG. 2 is a sectional view of an embodiment of the present invention, and FIG. 3 is a sectional view of a microwave heating furnace according to the prior art.
FIG. 4 is a characteristic diagram comparing the temperature of the inner container of the heating furnace according to the prior art and the present invention. In the figure, 1 is a microwave generator, 2 is a waveguide, and 3 is a microwave generator.
is a microwave oven, 4 is an object to be heated, 5 is an inner container,
6 is an intermediate container, 7 is an outer container, and 8 is an opening.

Claims (1)

【特許請求の範囲】 1 マイクロ波発熱する物質よりなり内部に被加熱物を
収容しうるように構成された内側容器、マイクロ波損失
の小さい耐火断熱性を有する中間容器、熱輻射率の小さ
い物質よりなり上記中間容器を収容するとともに当該中
間容器をとおしてその内部に収容された内側容器にマイ
クロ波を照射するための開口が設けられている外側容器
、およびこの外側容器の開口からマイクロ波を照射する
マイクロ波照射装置を備えたマイクロ波加熱炉。 2 外側容器を表面が熱輻射率の小さい金属で覆われて
いる構成とした特許請求の範囲第1項に記載のマイクロ
波加熱炉。 3 外側容器を形成する物質もしくはその表面を覆う金
属が、銅、アルミニウム、ステンレス鋼又は金である特
許請求の範囲第1項又は第2項に記載のマイクロ波加熱
炉。
[Scope of Claims] 1. An inner container made of a substance that generates heat by microwaves and configured to accommodate an object to be heated, an intermediate container having fireproof and heat-insulating properties with low microwave loss, and a material with low thermal emissivity. an outer container that accommodates the intermediate container and is provided with an opening for irradiating microwaves through the intermediate container to an inner container accommodated therein, and radiating microwaves from the opening of the outer container. A microwave heating furnace equipped with a microwave irradiation device. 2. The microwave heating furnace according to claim 1, wherein the outer container has a surface covered with a metal having a low thermal emissivity. 3. The microwave heating furnace according to claim 1 or 2, wherein the material forming the outer container or the metal covering the surface thereof is copper, aluminum, stainless steel, or gold.
JP2471079A 1979-03-02 1979-03-02 microwave heating furnace Expired JPS5925938B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2471079A JPS5925938B2 (en) 1979-03-02 1979-03-02 microwave heating furnace

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2471079A JPS5925938B2 (en) 1979-03-02 1979-03-02 microwave heating furnace

Publications (2)

Publication Number Publication Date
JPS55118587A JPS55118587A (en) 1980-09-11
JPS5925938B2 true JPS5925938B2 (en) 1984-06-22

Family

ID=12145720

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2471079A Expired JPS5925938B2 (en) 1979-03-02 1979-03-02 microwave heating furnace

Country Status (1)

Country Link
JP (1) JPS5925938B2 (en)

Also Published As

Publication number Publication date
JPS55118587A (en) 1980-09-11

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