JPH0534277A - Ultraviolet absorption detector - Google Patents
Ultraviolet absorption detectorInfo
- Publication number
- JPH0534277A JPH0534277A JP3596391A JP3596391A JPH0534277A JP H0534277 A JPH0534277 A JP H0534277A JP 3596391 A JP3596391 A JP 3596391A JP 3596391 A JP3596391 A JP 3596391A JP H0534277 A JPH0534277 A JP H0534277A
- Authority
- JP
- Japan
- Prior art keywords
- light
- mirror
- slit
- reflected
- comparison
- 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
Links
Landscapes
- Spectrometry And Color Measurement (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
- Photometry And Measurement Of Optical Pulse Characteristics (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、紫外線吸収検出器に関
し、更に詳しくは、高速液体クロマトグラフ等の検出器
として使用されフロ―セル内を流れる試料に紫外線を照
射し該紫外線の減少量から前記試料中の被測定成分を検
出する紫外線吸収検出器に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an ultraviolet absorption detector, and more specifically, it is used as a detector for a high performance liquid chromatograph or the like, and a sample flowing in a flow cell is irradiated with ultraviolet rays to determine the decrease amount of the ultraviolet rays. The present invention relates to an ultraviolet absorption detector that detects a component to be measured in the sample.
【0002】[0002]
【従来の技術】第2図は、紫外線吸収検出器の一般的な
構成説明図であり、図中、1は光源、2,4,6は凹面
鏡、3は入射スリット、5は回折格子、7はハ―フミラ
―、8,11は出射スリット、9はフロ―セル、10は
サンプル光センサ―、12は比較光センサ―である。こ
のような構成からなる従来の紫外線吸収検出器におい
て、光源1から照射された光は凹面鏡2で反射されて入
射スリット3に集光される。また、入射スリット3を通
った光は、凹面鏡4で反射されて平行光となり回折格子
5によって種々の波長の光に分光される。2. Description of the Related Art FIG. 2 is a diagram for explaining the general structure of an ultraviolet absorption detector. Is a harf mirror, 8 and 11 are exit slits, 9 is a flow cell, 10 is a sample photosensor, and 12 is a comparative photosensor. In the conventional ultraviolet absorption detector having such a configuration, the light emitted from the light source 1 is reflected by the concave mirror 2 and focused on the entrance slit 3. Further, the light that has passed through the entrance slit 3 is reflected by the concave mirror 4 and becomes parallel light, which is split into lights of various wavelengths by the diffraction grating 5.
【0003】このようにして分光された凹面鏡6に入射
した平行光のうち特定波長の光は、凹面鏡6の焦点付近
に配設されている出射スリット8とフロ―セル9を通
り、サンプル光センサ―10で検出される。また、凹面
鏡6に入射した平行光の一部は、ハ―フミラ―7で反射
されてのち出射スリット11を通り、比較光センサ―1
2で検出される。Of the parallel light that is incident on the concave mirror 6 in this way, light of a specific wavelength passes through the exit slit 8 and the flow cell 9 arranged near the focal point of the concave mirror 6, and passes through the sample optical sensor. -10 is detected. Also, a part of the parallel light incident on the concave mirror 6 is reflected by the half mirror 7 and then passes through the exit slit 11, and then the comparative optical sensor-1.
Detected in 2.
【0004】一方、フロ―セル9の中には試料が流され
ており、該試料の成分濃度に応じてサンプルの光強度が
変化する。このため、A,I,Io をそれぞれ吸光度,
サンプル光出力,比較光出力とするとき、下式(1)に
示すランベルト・ベアの法則に従って吸光度Aの変化が
出力されるようになっている。 A=lLog(Io /I)…………………(1)On the other hand, a sample is flown into the flow cell 9, and the light intensity of the sample changes according to the component concentration of the sample. Therefore, A, I, and I o are the absorbance,
When the sample light output and the comparison light output are used, the change in the absorbance A is output according to the Lambert-Beer law shown in the following equation (1). A = lLog (I o / I) …………………… (1)
【0005】因みに、サンプル光出力Iが0.1%変化
すると、吸光度Aは下式(2)に示すように −4.4
×10-4だけ変化するようになる。 ΔA=Log(Io /I)−Log{Io /(0.999I)} =Log(0.999) =−4.4×10-4…………………………(2)Incidentally, when the sample light output I changes by 0.1%, the absorbance A becomes -4.4 as shown in the following equation (2).
It changes by × 10 -4 . ΔA = Log (I o / I ) -Log {I o /(0.999I)} = Log (0.999) = -4.4 × 10 -4 .............................. (2)
【0006】[0006]
【発明が解決しようとする課題】然しながら、上記従来
例においては、光学系のゼロ点校正や波長校正は回折格
子5の角度を僅かに移動させてサンプル光側の出力だけ
を監視するようになっていた。このため、サンプル光側
と比較光側では観測している波長が異なり、検出器の出
力に悪影響を及ぼすという欠点があった。本発明は、か
かる従来例の欠点に鑑みてなされたものであり、その目
的は、サンプル光側と比較光側での波長のズレがなく出
力が安定している紫外線吸収検出器を提供することにあ
る。However, in the above-mentioned conventional example, in the zero point calibration and the wavelength calibration of the optical system, the angle of the diffraction grating 5 is slightly moved to monitor only the output on the sample light side. Was there. Therefore, there is a drawback in that the observed wavelength is different between the sample light side and the comparison light side, which adversely affects the output of the detector. The present invention has been made in view of the drawbacks of the conventional example, and an object thereof is to provide an ultraviolet absorption detector in which the output is stable without a wavelength shift between the sample light side and the comparison light side. It is in.
【0007】[0007]
【課題を解決するための手段】本発明は、光源から照射
された光が第1凹面鏡で反射されて入射スリットに集光
され、該入射スリットを通った光が第2凹面鏡を通って
平行光となり回折格子によって種々の波長の光に分光さ
れて後、第3凹面鏡に入射して平行となった光のうち特
定波長の光を、第3凹面鏡の焦点付近に配設されている
出射スリットとフロ―セルを通し、光センサ―で検出し
てフロ―セル内を流れる試料中の被測定成分を検出する
紫外線吸収検出器において、第3凹面鏡と出射スリット
との間にハ―フミラ―を配設すると共に、該ハ―フミラ
―を回転させるモ―タを設けることによって前記課題を
解決したものである。SUMMARY OF THE INVENTION According to the present invention, light emitted from a light source is reflected by a first concave mirror and condensed on an entrance slit, and light passing through the entrance slit passes through a second concave mirror to form parallel light. After being split into light of various wavelengths by the diffraction grating, the light of a specific wavelength among the light that is incident on the third concave mirror and becomes parallel is output to the exit slit arranged near the focal point of the third concave mirror. In the ultraviolet absorption detector that detects the component to be measured in the sample that flows through the flow cell through the flow cell and is detected by the optical sensor, place a half mirror between the third concave mirror and the output slit. The above problem is solved by providing a motor for rotating the half mirror while being installed.
【0008】[0008]
【作用】本発明は次のように作用する。即ち、光学系の
ゼロ校正や波長校正において、先ず、回折格子を微小な
角度動かし、その時のサンプル光側のゼロ校正や波長校
正を行なう。次に、ビ―ムスプリッタ―を微小な角度動
かし、その時の比較光側の出力値を監視して比較光側の
ゼロ校正や波長校正を行なう。このようにサンプル光側
と比較光側の両方でゼロ校正や波長校正を行なうことに
より、両者の波長のズレはなくなる。The present invention operates as follows. That is, in zero calibration and wavelength calibration of the optical system, first, the diffraction grating is moved by a small angle, and zero calibration and wavelength calibration on the sample light side at that time are performed. Next, the beam splitter is moved by a slight angle, and the output value on the comparison light side at that time is monitored to perform zero calibration or wavelength calibration on the comparison light side. By thus performing the zero calibration and the wavelength calibration on both the sample light side and the comparison light side, the wavelength shift between the two is eliminated.
【0009】[0009]
【実施例】以下、本発明について図を用いて詳細に説明
する。図1は本発明実施例を説明するための構成説明図
であり、図中、図2と同一記号は同一意味を持たせて使
用しここでの重複説明は省略する。また、13´は回折
格子5を回転させるための第1モ―タ、14はビ―ムス
プリッタ7を回転させるための第2モ―タである。The present invention will be described in detail below with reference to the drawings. FIG. 1 is a configuration explanatory view for explaining an embodiment of the present invention. In the figure, the same symbols as those in FIG. 2 are used with the same meanings, and duplicate explanations are omitted here. Further, 13 'is a first motor for rotating the diffraction grating 5, and 14 is a second motor for rotating the beam splitter 7.
【0010】このような構成からなる本発明の実施例に
おいて、光源1から照射された光は凹面鏡2で反射され
て入射スリット3に集光される。また、入射スリット3
を通った光は、凹面鏡4を通って平行光となり回折格子
5によって種々の波長の光に分光される。このようにし
て分光され凹面鏡6に入射した平行光のうち特定波長の
光は、その焦点に集光する。In the embodiment of the present invention having such a structure, the light emitted from the light source 1 is reflected by the concave mirror 2 and focused on the entrance slit 3. In addition, the entrance slit 3
The light that has passed through becomes a parallel light through the concave mirror 4 and is split into lights of various wavelengths by the diffraction grating 5. The light of a specific wavelength of the parallel light thus split and incident on the concave mirror 6 is condensed at its focal point.
【0011】ここで、凹面鏡6は第1図に示すように第
1球面6a(凹面鏡6の中央部分)と第2球面6b(凹
面鏡6の端部分)の2つの曲面を有しており、第1球面
6aの焦点と第2球面6bの焦点は異なっている。この
ため、第1球面6aで反射された光は、その焦点付近に
配設されている出射スリット8を通過して限定されたバ
ンド幅の光となってフロ―セル9を通り、サンプル光セ
ンサ―10で検出される。Here, the concave mirror 6 has two curved surfaces of a first spherical surface 6a (a central portion of the concave mirror 6) and a second spherical surface 6b (an end portion of the concave mirror 6) as shown in FIG. The focus of the first spherical surface 6a and the focus of the second spherical surface 6b are different. Therefore, the light reflected by the first spherical surface 6a passes through the exit slit 8 disposed near the focal point of the first spherical surface 6a, becomes light of a limited band width, passes through the flow cell 9, and passes through the sample optical sensor. -10 is detected.
【0012】また、第2球面6bで反射された光は、そ
の焦点付近に配設されている比較光用出射スリット11
を通り、限定されたバンド幅の光となってフロ―セル9
を通過し比較光センサ―12で検出される。このように
して、サンプル光センサ―10で検出された検出信号
(I)と比較光センサ―12で検出された検出信号(I
o )に基いて前記第(1)式に示したような演算が行わ
れ、フロ―セル9内を流れる流体の紫外線吸光度が検出
されるようになっている。The light reflected by the second spherical surface 6b is
Exit slit 11 for comparison light, which is arranged near the focal point of
The light with a limited bandwidth passes through the frothel 9
And is detected by the comparative optical sensor-12. in this way
Then, the detection signal detected by the sample optical sensor-10
(I) and the detection signal (I
o), The calculation as shown in the equation (1) is performed.
And the UV absorbance of the fluid flowing in the flow cell 9 is detected.
It is supposed to be done.
【0013】即ち、光学系のゼロ校正や波長校正におい
て、先ず、回折格子5を微小な角度動かし、その時のサ
ンプル光側のゼロ校正や波長校正を行なう。次に、ビ―
ムスプリッタ―を微小な角度動かし、その時の比較光側
の出力値を監視して比較光側のゼロ校正や波長校正を行
なう。このようにサンプル光側と比較光側の両方でゼロ
校正や波長校正を行なうことにより、両者の波長のズレ
はなくなる。That is, in zero calibration and wavelength calibration of the optical system, first, the diffraction grating 5 is moved by a minute angle, and zero calibration and wavelength calibration on the sample light side at that time are performed. Next, bee
The splitter is moved by a small angle and the output value on the comparison light side at that time is monitored to perform zero calibration or wavelength calibration on the comparison light side. In this way, by performing the zero calibration and the wavelength calibration on both the sample light side and the comparison light side, the wavelength shift between the two is eliminated.
【0014】尚、本発明は第1図の実施例に限定される
ことなく種々の変形が可能であり、例えば次のやの
ようにしても良いものとする。紫外線吸収検出器だけ
でなく赤外線その他の光学系検出器に用いる。凹面鏡
の主軸を上下方向に平行でなく、焦点距離をずらすよう
にする。The present invention is not limited to the embodiment shown in FIG. 1, and various modifications are possible. For example, the following may be adopted. Used not only for UV absorption detectors, but also for infrared and other optical system detectors. The principal axis of the concave mirror is not parallel to the vertical direction, but the focal length is shifted.
【0015】[0015]
【発明の効果】以上詳しく説明したような本発明によれ
ば、サンプル光側と比較光側での波長のズレがなく出力
が安定している紫外線吸収検出器が実現する。According to the present invention as described in detail above, an ultraviolet absorption detector having a stable output with no wavelength shift between the sample light side and the comparison light side can be realized.
【図1】本発明実施例の構成説明図である。FIG. 1 is a structural explanatory view of an embodiment of the present invention.
【図2】従来例の構成説明図である。 1 光源 2,4,6 凹面鏡 3 入射スリット 5 回折格子 7 ハ―フミラ― 8,11 出射スリット 9 フロ―セル 10 サンプル光センサ― 12 比較光センサ― 13,14 モ―タFIG. 2 is an explanatory diagram of a configuration of a conventional example. 1 Light Source 2, 4, 6 Concave Mirror 3 Entrance Slit 5 Diffraction Grating 7 Haar Miller 8, 11 Exit Slit 9 Flow Cell 10 Sample Optical Sensor-12 Comparative Optical Sensor-13, 14 Motor
Claims (1)
されて入射スリットに集光され、該入射スリットを通っ
た光が第2凹面鏡を通って平行光となり回折格子によっ
て種々の波長の光に分光されて後、第3凹面鏡に入射し
て平行となった光のうち特定波長の光を、前記第3凹面
鏡の焦点付近に配設されている出射スリットとフロ―セ
ルを通し、光センサ―で検出して前記フロ―セル内を流
れる試料中の被測定成分を検出する紫外線吸収検出器に
おいて、前記第3凹面鏡と出射スリットとの間にハ―フ
ミラ―を配設すると共に、該ハ―フミラ―を回転させる
モ―タを設けたことを特徴とする紫外線吸収検出器。Claim: What is claimed is: 1. Light emitted from a light source is reflected by a first concave mirror and condensed on an incident slit, and light passing through the incident slit passes through a second concave mirror to become parallel light and diffracted. The light of a specific wavelength, of the light that has been split into light of various wavelengths by the grating and then entered the third concave mirror and becomes parallel, is output from the output slit and the flow slit arranged near the focal point of the third concave mirror. -In the ultraviolet absorption detector which detects the component to be measured in the sample flowing through the flow cell by passing through the cell and detecting with an optical sensor, a half mirror is provided between the third concave mirror and the exit slit. An ultraviolet absorption detector characterized by being provided with a motor for rotating the half mirror.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3596391A JPH0534277A (en) | 1991-03-01 | 1991-03-01 | Ultraviolet absorption detector |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3596391A JPH0534277A (en) | 1991-03-01 | 1991-03-01 | Ultraviolet absorption detector |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0534277A true JPH0534277A (en) | 1993-02-09 |
Family
ID=12456613
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3596391A Pending JPH0534277A (en) | 1991-03-01 | 1991-03-01 | Ultraviolet absorption detector |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0534277A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5822063A (en) * | 1996-04-18 | 1998-10-13 | Toyota Jidosha Kabushiki Kaisha | Apparatus for measuring magneto-optical effect |
-
1991
- 1991-03-01 JP JP3596391A patent/JPH0534277A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5822063A (en) * | 1996-04-18 | 1998-10-13 | Toyota Jidosha Kabushiki Kaisha | Apparatus for measuring magneto-optical effect |
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