JPH0240515A - Light source for infrared-ray spectroscope - Google Patents

Light source for infrared-ray spectroscope

Info

Publication number
JPH0240515A
JPH0240515A JP19097788A JP19097788A JPH0240515A JP H0240515 A JPH0240515 A JP H0240515A JP 19097788 A JP19097788 A JP 19097788A JP 19097788 A JP19097788 A JP 19097788A JP H0240515 A JPH0240515 A JP H0240515A
Authority
JP
Japan
Prior art keywords
light source
core
infrared
heating element
fourier transform
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
JP19097788A
Other languages
Japanese (ja)
Inventor
Katsuhiko Ichimura
市村 克彦
Masanao Nishida
西田 正直
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.)
Shimadzu Corp
Original Assignee
Shimadzu 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 Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP19097788A priority Critical patent/JPH0240515A/en
Publication of JPH0240515A publication Critical patent/JPH0240515A/en
Pending legal-status Critical Current

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  • Spectrometry And Color Measurement (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 (イ)産業上の利用分野 本発明は、赤外分光装置に関し、特に、汎用性のフーリ
エ変換赤外分光光度測定袋f(FT−IR)又は赤外干
渉分光光度測定装置に関する。また、本発明は、赤外分
光光度計に使用される光源用の黒体炉即ち空洞放射体に
関し、特に、汎用性に優れるフーリエ変換赤外分光光度
計又は赤外干渉分光光度計の光源用の出口面積の大きい
黒体炉に関する。
Detailed Description of the Invention (a) Industrial Application Field The present invention relates to an infrared spectrometer, particularly a versatile Fourier transform infrared spectrophotometry bag f (FT-IR) or an infrared interference spectrophotometer. Concerning a measuring device. The present invention also relates to a blackbody furnace, that is, a cavity radiator, for a light source used in an infrared spectrophotometer, and in particular, for a light source of a Fourier transform infrared spectrophotometer or an infrared interference spectrophotometer, which is highly versatile. Regarding a blackbody furnace with a large exit area.

(ロ)従来の技術 フーリエ変換赤外分光光度計は、全反射吸収測定法、拡
散反射測定法、高感度反射測定法、光音響分光法、赤外
発光法、微量微少試料測定法及びガスクロマトグラフィ
法又は高速液体クロマトグラフィ法と組み合わせるなど
、種々の測定の用途に使用されている。
(b) Conventional technology Fourier transform infrared spectrophotometers include total reflection absorption measurement method, diffuse reflection measurement method, high-sensitivity reflectance measurement method, photoacoustic spectroscopy, infrared emission method, trace amount micro sample measurement method, and gas chromatography. It is used for various measurement applications, such as in combination with high-performance liquid chromatography methods or high-performance liquid chromatography methods.

しかし、従来のフーリエ変換赤外分光光度計の光源には
、ニクロム線、炭化ケイ素棒を使用するグローバー光源
、ジルコニウム酸化物に、イツトリウム、トリウム、エ
ルビウム等の稀土類酸化物を配合した・ネルンスト光源
及び高圧水銀灯等が使用されている。
However, the light sources for conventional Fourier transform infrared spectrophotometers include a nichrome wire, a Grover light source that uses a silicon carbide rod, and a Nernst light source that combines zirconium oxide with rare earth oxides such as yttrium, thorium, and erbium. and high-pressure mercury lamps are used.

(ハ)発明が解決しようとする問題点 しかし、従来のフーリエ変換赤外分光光度計に使用され
るこれらの光源は、温度が高くできないために、輝度が
低く、しかもヒータの特性吸収が出るなどの点で、その
ような多くの用途に使用できず、問題とされている。
(c) Problems to be solved by the invention However, these light sources used in conventional Fourier transform infrared spectrophotometers have low brightness because the temperature cannot be raised, and there is also absorption due to the characteristics of the heater. Therefore, it cannot be used for many such purposes and is considered a problem.

そこで、アルミナ、ジルコニア、マグネシア等の高融点
セラミック材料の棒状体の周囲に、螺旋状の溝を形成し
、この清に沿って白金等の金属線を巻き、その端部に開
口する円筒円錐状の空洞を、その内部軸方向に形成した
小形の黒体炉が提案されている(例えば、米国特許第4
,499,382号明細書)。
Therefore, a spiral groove is formed around a rod-shaped body of a high melting point ceramic material such as alumina, zirconia, or magnesia, and a metal wire such as platinum is wound along this groove, and a cylindrical-conical shape with an opening at the end is formed. A small blackbody furnace has been proposed in which a cavity is formed in the direction of its internal axis (for example, U.S. Pat.
, 499, 382).

しかし、このような小形の黒体炉は、高い輝度が期待で
きるものの、かえって、試料室の大きさが制限されるた
めに、汎用のフーリエ変換赤外分光光度計の光源として
使用することができず問題である。
However, although such a small blackbody furnace can be expected to produce high brightness, it cannot be used as a light source for a general-purpose Fourier transform infrared spectrophotometer because the size of the sample chamber is limited. This is a problem.

本発明は、従来のフーリエ変換赤外分光光度計の光源の
輝度及びその汎用性等に係る問題点を解決することを目
的としている。
The present invention aims to solve problems related to the brightness of the light source of the conventional Fourier transform infrared spectrophotometer and its versatility.

(二〉問題点を解決するための手段 本発明は、汎用フーリエ変換赤外分光光度計が使用され
る全波数域に互って、安定してしかも高い放射率で、赤
外部の光源として使用できる黒体炉を備える汎用フーリ
エ変換赤外分光光度計等の赤外分光装置を提供すること
を目的としている。
(2) Means for Solving the Problems The present invention enables a general-purpose Fourier transform infrared spectrophotometer to be used as an infrared light source with stable and high emissivity over the entire wavenumber range in which it is used. The purpose of the present invention is to provide an infrared spectrometer such as a general-purpose Fourier transform infrared spectrophotometer equipped with a blackbody furnace that can be used.

即ち、本発明は、開口する円錐状の凹部がその一端に形
成されている円柱状の炉心が、その側面が螺旋状に一つ
の帯状の抵抗加熱用の発熱体によって巻かれており、前
記発熱体の外側が断熱層で囲繞されて、黒体炉に形成さ
れていることを特徴とする赤外分光装置用光源にある。
That is, in the present invention, a cylindrical reactor core having an open conical recess formed at one end is wound around its side surface in a spiral manner by a band-shaped resistance heating heating element, and the heating element A light source for an infrared spectrometer is characterized in that the outside of the body is surrounded by a heat insulating layer and formed into a blackbody furnace.

本発明において、黒体炉の炉心は、アルミナ、ジルコニ
ア又はマグネシア等の高融点のセラミック材料又はその
他界外線放射体で形成されるのが、高い輝度が得られる
ので好ましい1本発明においては、炉心を加熱するため
に、ニクロム、クローム−A1、Cr −F e −A
 I、炭化ケイ素、白金、白金−ロジウム等の抵抗加熱
材料製の帯状の発熱体が使用される。しかし、帯状の炭
化ケイ素発熱体は、空気中で安定して、しかも容易に高
温を得ることができるので好ましい。帯状の発熱体は、
炉心外面に接して螺旋状に巻き付けられる。この場合、
帯状の発熱体を二重螺旋状に炉心に巻き付けると、炉心
の放射面と反対側の端部に、接続端子が配置でき、しか
も、加熱密度を大きくできるので好ましい1本発明にお
いては、帯状の発熱体の熱が外部に逃散しないように、
断熱材で覆われるのが好ましい。
In the present invention, the core of the blackbody reactor is preferably formed of a ceramic material with a high melting point such as alumina, zirconia, or magnesia, or other external radiation emitters, since high brightness can be obtained. To heat nichrome, chromium-A1, Cr-Fe-A
A strip-shaped heating element made of a resistance heating material such as I, silicon carbide, platinum, or platinum-rhodium is used. However, a band-shaped silicon carbide heating element is preferable because it is stable in the air and can easily reach a high temperature. The band-shaped heating element is
It is wound spirally in contact with the outer surface of the core. in this case,
In the present invention, it is preferable to wrap the band-shaped heating element around the reactor core in a double helical manner, since the connecting terminal can be arranged at the end opposite to the radiation surface of the core, and the heating density can be increased. To prevent heat from the heating element from escaping to the outside,
Preferably covered with insulation.

本発明において、炉心には、空洞放射ができるように、
その端部に開口して空洞が形成される。
In the present invention, the reactor core includes:
A cavity is formed by opening at the end.

この場合、端部に形成される空洞が、窪んだ円錐状に形
成されると、放射束が平行に形成されるの。
In this case, if the cavity formed at the end is formed in the shape of a concave cone, the radiant beams will be formed in parallel.

で好ましい、この空洞は、高放射率の放射束度が容易に
得られるように、空洞の深さ及び空洞の開口部の半径の
大きさを適宜選択して形成したり又は空洞内面を黒化す
るのが好ましい0本発明における黒体炉は、放射強度が
炉心の温度により決まるので、炉心に温度センサを設け
て、放射強度が一定となるように、炉心の温度制御を行
えるように炉心を形成するのが好ましい。
This cavity is preferably formed by appropriately selecting the depth of the cavity and the radius of the opening of the cavity, or by blackening the inner surface of the cavity so that a high emissivity and radiant flux can be easily obtained. In the blackbody reactor according to the present invention, the radiation intensity is determined by the temperature of the core, so a temperature sensor is provided in the core to control the temperature of the core so that the radiation intensity is constant. It is preferable to form.

(ホ)作用 本発明においては、柱状の一端に円錐状の凹部が形成さ
れ、その側面に螺旋状に一つの帯状の抵抗加熱用の発熱
体を巻き付けて黒体炉の炉心を形成して、フーリエ変換
赤外分光光度測定装置の光源としたので、全波数域に互
って、均一な高い放射率を有し、輝度が高い大きな発光
体を、フーリエ変換赤外分光光度測定装置用の光源とす
ることができる。このため試料室が大きい汎用のフーリ
エ変換赤外分光光度用の光源として利用できる。
(E) Function In the present invention, a conical recess is formed at one end of the columnar shape, and a belt-shaped heating element for resistance heating is wound spirally around the side surface of the conical recess to form the core of the blackbody furnace. Since the light source for the Fourier transform infrared spectrophotometer was used as the light source for the Fourier transform infrared spectrophotometer, a large luminous body with high brightness and uniform high emissivity across the entire wavenumber range was used as the light source for the Fourier transform infrared spectrophotometer. It can be done. Therefore, it can be used as a light source for general-purpose Fourier transform infrared spectroscopy with a large sample chamber.

(へ)実施例 以下、添付図面を参照して、本発明の実施の態様につい
て説明するが、本発明は、以下の説明及び例示によって
、何等の制限を受けるものではない。
(F) EXAMPLES Hereinafter, embodiments of the present invention will be described with reference to the accompanying drawings, but the present invention is not limited in any way by the following explanations and examples.

第1図は、本発明の一実施例における光源の黒体炉部に
ついての概略の部分側断面図である。
FIG. 1 is a schematic partial side sectional view of a blackbody furnace portion of a light source in an embodiment of the present invention.

本例において、黒体炉1は、炉心2としてアルミナ製の
円柱体が設けられている、この炉心2の放射側端部3に
は、円錐状の穴4が形成されており、この穴4の大きさ
は直径的4msである。炉JC12の側面7の周囲には
、二重螺旋状に、帯状の炭化ケイ素製の発熱体5が巻き
付けられている。
In this example, the blackbody reactor 1 has a cylindrical body made of alumina as the core 2. A conical hole 4 is formed in the radiation side end 3 of the core 2. is 4 ms in diameter. A band-shaped heating element 5 made of silicon carbide is wound around the side surface 7 of the furnace JC 12 in a double spiral.

本例に使用される帯状の炭化ケイ素発熱体5は、炉心2
の外形によって決定されるが、例えば、炉IC12の外
径が10輪輪、穴4の径が6−−の場合、帯状炭化ケイ
素発熱体の螺旋体は、外径25mm以下、長さ70m+
e以下である。帯状の炭化ケイ素発熱体5は、電気的絶
縁をはかるために、それらの間に充填される電気絶縁用
の耐熱性のセメント6によって、炉心2の側面7に固定
されている。この帯状の炭化ケイ素発熱体5の両端部8
及び9には、端子10及び11が夫々設けられており、
この端子10及び11には導線12及び13が電気的に
接続している。
The band-shaped silicon carbide heating element 5 used in this example is
For example, if the outer diameter of the furnace IC 12 is 10 rings and the diameter of the hole 4 is 6--, the spiral body of the band-shaped silicon carbide heating element has an outer diameter of 25 mm or less and a length of 70 m+.
It is less than or equal to e. The band-shaped silicon carbide heating elements 5 are fixed to the side surface 7 of the core 2 by heat-resistant cement 6 for electrical insulation filled between them for electrical insulation. Both ends 8 of this band-shaped silicon carbide heating element 5
and 9 are provided with terminals 10 and 11, respectively,
Conductive wires 12 and 13 are electrically connected to the terminals 10 and 11.

本例においては、黒体炉1からの熱の損失を防ぐために
、帯状の炭化ケイ素発熱体5を囲んで、円筒状の断熱材
14が設けられている。
In this example, in order to prevent heat loss from the blackbody furnace 1, a cylindrical heat insulating material 14 is provided surrounding the band-shaped silicon carbide heating element 5.

本例の黒体炉は、以上のように構成されているので、ス
イッチ(図示されていない。)を入れて、炭化ケイ素発
熱体5に電気を通して発熱させ、炉心2を加熱すると、
炉心2は加熱されて高温となり放射側3の穴の面から、
赤外部の波数全域に互って高い均一な放射率を有しそし
て輝度の大きい赤外線を放射することができる。
The blackbody furnace of this example is configured as described above, so when a switch (not shown) is turned on and electricity is passed through the silicon carbide heating element 5 to generate heat, the reactor core 2 is heated.
The reactor core 2 is heated to a high temperature, and from the surface of the hole on the radiation side 3,
It has a high uniform emissivity over the entire range of infrared wavenumbers and can emit infrared rays with high brightness.

本例の黒体炉1は、冷却コイル等を備える容器(図示さ
れていない。)に収容して、赤外分光光度計の光源とし
て使用された。
The blackbody furnace 1 of this example was housed in a container (not shown) equipped with a cooling coil and the like, and was used as a light source for an infrared spectrophotometer.

このように、本例の黒体炉1を光源とするフーリエ変換
赤外分光光度測定装置を、全反射吸収測定法、拡散反射
測定法、高感度反射測定法、光音響分光法、発光測定法
及び微量微少試料測定法等の測定に使用して良好な結果
が得られた。また、本例の黒体炉1をガスクロマトグラ
フィ分離装置又は高速液体クロマトグラフィ分離装置と
組み合わせても、同様に、良好な結果が得られた。
In this way, the Fourier transform infrared spectrophotometer using the blackbody furnace 1 of this example as a light source can be used with total internal reflection absorption measurement, diffuse reflectance measurement, high-sensitivity reflectance measurement, photoacoustic spectroscopy, and luminescence measurement. Good results were obtained when used in measurements such as the micro sample measurement method and the micro sample measurement method. Similarly, good results were also obtained when the blackbody furnace 1 of this example was combined with a gas chromatography separation device or a high-performance liquid chromatography separation device.

本例にお・いては、発熱体5と炉心2を直接接触させて
いるが、熱の伝導を良好にするために、従来の黒体炉と
同様に、耐熱性のセメントで、炉心2と発熱体5の間を
固着させることができる。また、同様に、炉心2の温度
を一定に保つために、炉心2内に温度センサを設けて、
温度コントロール可能にすることができる。炉心2の穴
4の内面に黒化処理を施して、吸収率を大きく形成する
と、必要な反射の回数が少なくなり、開口部の大きさを
比較的大きくできるなど、赤外線放射率を向上させるこ
とができる。
In this example, the heating element 5 and the reactor core 2 are in direct contact, but in order to improve heat conduction, heat-resistant cement is used to connect the reactor core 2 with heat-resistant cement, as in conventional blackbody reactors. The space between the heating elements 5 can be fixed. Similarly, in order to keep the temperature of the reactor core 2 constant, a temperature sensor is provided inside the reactor core 2,
Temperature control can be made possible. By blackening the inner surface of the hole 4 in the core 2 to increase the absorption rate, the number of necessary reflections will be reduced and the size of the opening can be made relatively large, thereby improving the infrared emissivity. Can be done.

本例は、炉心をアルミナ製としたが、他の高融点のジル
コニア、マグネシアその他界外線放射体により同様に形
成することができる。
In this example, the core is made of alumina, but it can be similarly made of other high melting point zirconia, magnesia, or other external radiation emitters.

(ト)発明の効果 本発明においては、柱状のセラミック体の一端に、円錐
状の凹部を形成し、その側面に螺旋状に、帯状の抵抗加
熱用の発熱体を巻き付けて黒体炉の炉心を形成して赤外
分光光度測定装置の光源としたので、本発明の光源は、
従来の赤外分光光度測定装置の光源と比較して、輝度が
高い大きな光源とすることができ、しかも、赤外部の使
用される波数域に互って高い放射率で光量の変動が小さ
な光源となり、精度の高いフーリエ変換赤外分光光度測
定を行うことができる。
(g) Effects of the invention In the present invention, a conical recess is formed at one end of a columnar ceramic body, and a band-shaped resistance heating heating element is wound spirally around the side surface of the conical recess to form the core of a blackbody furnace. The light source of the present invention has the following properties:
Compared to the light source of conventional infrared spectrophotometer measurement equipment, it can be a large light source with high brightness, and also has a high emissivity in the infrared wavenumber range used and has small fluctuations in light intensity. Therefore, highly accurate Fourier transform infrared spectrophotometry can be performed.

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

第1図は、本発明の一実施例における光源の黒体炉部に
ついての概略の部分側断面図である。 図中の符号について、1は黒体炉、2は炉心、3は放射
側端部、4は穴、5は帯状の炭化ケイ素発熱体、6は耐
熱性セメント、7は炉心の側面、8及び9は抵抗発熱体
の端部、10及び11は端子、12及び13は導線、1
4は断熱材である。
FIG. 1 is a schematic partial side sectional view of a blackbody furnace portion of a light source in an embodiment of the present invention. Regarding the symbols in the figure, 1 is the black body furnace, 2 is the core, 3 is the radiation side end, 4 is the hole, 5 is the band-shaped silicon carbide heating element, 6 is the heat-resistant cement, 7 is the side of the core, 8 and 9 is the end of the resistance heating element, 10 and 11 are terminals, 12 and 13 are conductive wires, 1
4 is a heat insulating material.

Claims (1)

【特許請求の範囲】[Claims] 開口する円錐状の凹部がその一端に形成されている円柱
状の炉心が、その側面が螺旋状に一つの帯状の抵抗加熱
用の発熱体によつて巻かれており、前記発熱体の外側が
断熱層で囲繞されて、黒体炉に形成されていることを特
徴とする赤外分光装置用光源。
A cylindrical reactor core is formed with an open conical recess at one end, and the side surface of the core is spirally wrapped around a band-shaped heating element for resistance heating. A light source for an infrared spectrometer, characterized in that it is surrounded by a heat insulating layer and formed in a blackbody furnace.
JP19097788A 1988-07-30 1988-07-30 Light source for infrared-ray spectroscope Pending JPH0240515A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19097788A JPH0240515A (en) 1988-07-30 1988-07-30 Light source for infrared-ray spectroscope

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19097788A JPH0240515A (en) 1988-07-30 1988-07-30 Light source for infrared-ray spectroscope

Publications (1)

Publication Number Publication Date
JPH0240515A true JPH0240515A (en) 1990-02-09

Family

ID=16266817

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19097788A Pending JPH0240515A (en) 1988-07-30 1988-07-30 Light source for infrared-ray spectroscope

Country Status (1)

Country Link
JP (1) JPH0240515A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5479025A (en) * 1994-11-18 1995-12-26 Hughes Aircraft Company Boresight thermal reference source

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5479025A (en) * 1994-11-18 1995-12-26 Hughes Aircraft Company Boresight thermal reference source
EP0713075A1 (en) * 1994-11-18 1996-05-22 Hughes Aircraft Company Boresight thermal reference source

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