JP3147976B2 - Qualitative analysis of amorphous samples - Google Patents

Qualitative analysis of amorphous samples

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Publication number
JP3147976B2
JP3147976B2 JP07258692A JP7258692A JP3147976B2 JP 3147976 B2 JP3147976 B2 JP 3147976B2 JP 07258692 A JP07258692 A JP 07258692A JP 7258692 A JP7258692 A JP 7258692A JP 3147976 B2 JP3147976 B2 JP 3147976B2
Authority
JP
Japan
Prior art keywords
sample
ray
crystalline
profile
diffraction
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 - Fee Related
Application number
JP07258692A
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Japanese (ja)
Other versions
JPH05232049A (en
Inventor
秀信 石田
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
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Shimadzu Corp
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Publication date
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Priority to JP07258692A priority Critical patent/JP3147976B2/en
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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は結晶部分と非結晶部分と
が混合したような試料の非結晶部分のX線回折装置によ
る定性分析法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a qualitative analysis method for an amorphous portion of a sample, such as a mixture of a crystalline portion and an amorphous portion, using an X-ray diffractometer.

【0002】[0002]

【従来の技術】従来X線回折法は、結晶性試料の定性分
析に利用されてきた。これは結晶性試料はX線回折像に
幾つかの明瞭な回折線を現し、この回折線群が試料の結
晶構造を示しているので、回折線から試料物質の同定が
できることによる。これに対して非結晶質のX線回折パ
ターンは広い角度範囲にわたってX線強度がなだらかに
分布する散乱パターンを示すだけで、特別な回折線が現
れないため、試料同定には利用されていなかった。
2. Description of the Related Art Conventionally, X-ray diffraction has been used for qualitative analysis of crystalline samples. This is because the crystalline sample shows several distinct diffraction lines in the X-ray diffraction image, and since the group of diffraction lines indicates the crystal structure of the sample, the sample substance can be identified from the diffraction lines. Only shows the X-ray intensity scattered pattern distributed gently across the X-ray diffraction pattern is a wide angular range of amorphous contrast, since the special diffraction line does not appear, it has not been utilized for sample identification .

【0003】[0003]

【発明が解決しようとする課題】X線回折装置を用いて
非結晶或は結晶部分と非結晶部分が混合している試料の
非結晶物質の定性分析を行う方法を提供する。
SUMMARY OF THE INVENTION The present invention provides a method for qualitatively analyzing an amorphous substance of a sample which is amorphous or a mixture of a crystalline part and an amorphous part using an X-ray diffractometer.

【0004】[0004]

【課題を解決するための手段】各種非結晶物質のX線回
折装置によるX線の散乱特性のプロファイルデータを記
憶させておき、被測定試料のX線回折装置によるX線散
乱パターンのデータから試料の結晶部分による回折線の
ピークを除いた散乱X線のプロファイルを求め、予め記
憶させてある各種物質の散乱特性のプロファイルとの一
致度の最も良い物質を索出するようにした。
Means for Solving the Problems Profile data of X-ray scattering characteristics of various non-crystalline substances by an X-ray diffractometer are stored, and a sample is measured from data of an X-ray scattering pattern of the sample to be measured by the X-ray diffractometer. The scattered X-ray profile excluding the peak of the diffraction line due to the crystal part was obtained, and a substance having the highest degree of coincidence with the previously stored scattering characteristic profiles of various substances was searched for.

【0005】[0005]

【作用】非結晶性試料でも各物質固有のX線散乱パター
ンを示す。この散乱パターンはなだらかな形をしている
ので、結晶質の回折線のピークとは容易に区別できる。
従って結晶質と非結晶質とが混合している試料であつて
も、非結晶質だけの散乱パターンを測定することができ
る。上述したように非結晶質の散乱パターンは物質に固
有な形があり、その形が予め記憶させてあるので、試料
の散乱パターンをこれと比較することで、試料の非結晶
部分の定性ができる。本発明は結晶質の回折像と非結晶
質の散乱像とを識別すると云うことに主旨があるのでは
なく、本発明が結晶部分を含まない非結晶質だけの試料
の定性にも適用できるものであることは云うまでもな
い。
The X-ray scattering pattern peculiar to each substance is exhibited even in an amorphous sample. Since this scattering pattern has a gentle shape, it can be easily distinguished from the peak of a crystalline diffraction line.
Therefore, even if the sample is a mixture of crystalline and non-crystalline materials, the scattering pattern of only the non-crystalline materials can be measured. As described above, the amorphous scattering pattern has a shape unique to a substance, and the shape is stored in advance. By comparing the scattering pattern of the sample with the shape, the qualitative determination of the amorphous portion of the sample can be performed. . The present invention is not intended to distinguish between a crystalline diffraction image and a non-crystalline scattering image, and the present invention can be applied to the qualitative determination of a non-crystalline sample that does not include a crystalline portion. Needless to say,

【0006】[0006]

【実施例】図1に本発明の一実施例の概要をフローチャ
ートにして示す。予め非結晶質の標準試料についてX線
回折装置によって散乱X線強度の角度分布を測定し、デ
ータ処理装置のデータファイルに格納しておく(イ)。
その後実際の試料について散乱X線強度の角度分布を測
定し、得られたデータをメモリに格納する(ロ)。その
後測定結果についてデータ処理を行う。データ処理は測
定結果のデータから試料中の結晶成分による回折線ピー
クを除き(ハ)、回折線ピークを除くことで平坦化され
た測定データのプロフアイルとデータフアイル各種標準
物質の散乱X線強度の角度分布のプロファイルとの近似
度を順次算出し(ニ)、近似度の最も高い標準物質を索
出(ホ)して表示する。上の説明は試料中の非結晶成分
についてのみの分析についてであるが、結晶性の成分と
非結晶性成分の混合している試料の場合、回折X線のピ
ークによって公知各種の方法で結晶成分の同定も行うこ
とは云うまでもない。
FIG. 1 is a flowchart showing an outline of an embodiment of the present invention. The angular distribution of the scattered X-ray intensity of an amorphous standard sample is measured in advance by an X-ray diffractometer and stored in a data file of a data processor (A).
Thereafter, the angular distribution of the scattered X-ray intensity is measured for the actual sample, and the obtained data is stored in the memory (b). Thereafter, data processing is performed on the measurement result. The data processing removes the diffraction line peak due to the crystal component in the sample from the data of the measurement result (c), and the profile of the measurement data flattened by removing the diffraction line peak and the scattering X-ray intensity of the data file various standard substances The degree of approximation to the profile of the angle distribution is sequentially calculated (d), and the standard substance having the highest degree of approximation is searched out (e) and displayed. The above explanation is about the analysis of only the non-crystalline component in the sample. However, in the case of the sample in which the crystalline component and the non-crystalline component are mixed, the crystal component is obtained by various methods known by the diffraction X-ray peak. It is needless to say that the identification is also performed.

【0007】上記(ハ)(ニ)の処理の一例を説明す
る。メモリに格納された測定データは平滑化処理を行っ
て散乱X線の滑らかなプロファイルのデータにする。こ
のデータはX線の散乱角の小さい側から大きい側へX線
回折装置の角度送りの一ステップ毎に採取されたもので
ある。図2に示すようにこのデータを散乱角の小さい側
から順に隣合うデータ間の差を求めこの差が基準値を超
えたときの散乱角aを回折X線ピークの開始点、差が大
きい側から基準値より下へ下がった時の散乱角bを回折
X線ピークの終点とする。このようにして求められた各
回折線ピークの開始点,終点より夫々所定点数だけ当該
ピークから遠ざかった測定点A,Bにおける測定値を直
線で結んで、これを回折X線のピークを除いた散乱X線
強度のプロファイルの一部とする。
An example of the above processes (c) and (d) will be described. The measurement data stored in the memory is subjected to a smoothing process to obtain data of a smooth scattered X-ray profile. This data is collected at every step of the angle feed of the X-ray diffractometer from the side where the X-ray scattering angle is small to the side where it is large. As shown in FIG. 2, a difference between adjacent data is determined in order from the side having the smallest scattering angle, and the scattering angle a when this difference exceeds a reference value is determined as the starting point of the diffraction X-ray peak and the side having the larger difference. The scattering angle b when the value falls below the reference value from is set as the end point of the diffraction X-ray peak. The measurement values at the measurement points A and B, which were obtained from the start point and the end point of each diffraction line peak by a predetermined number of points away from the peaks, were connected by straight lines, and the peaks of the diffraction X-rays were excluded. A part of the scattered X-ray intensity profile.

【0008】このようにして回折X線ピークを除いた散
乱X線のプロファイルを図3Aに示す。図3Bはデータ
ファイルに格納されている標準物質の一つの散乱X線の
プロファイルである。これらのデータのサンプリング点
を左から1,2,…i…nとする。両方のプロファイル
の近似度の算出の一例は次のようにして行われる。サン
プリング点1,2,…i…nに対する被測定試料のX線
強度をIui,標準試料のX線強度をIsiとする。ま
ずKi=Iui/Isiを求めKiの平均 K=ΣKi/n を求める。一致度Eは E=1−|(ΣIui−KΣIsi)|/ΣIui 或は対数を導入して logK=Σ(logIui−logIsi)/n E=1−Σ|(logIui−logKIsi)|/ΣlogIui としてもよい。
FIG. 3A shows a scattered X-ray profile excluding the diffraction X-ray peak. FIG. 3B is a scattered X-ray profile of one of the standard materials stored in the data file. The sampling points of these data are 1, 2,..., I. An example of the calculation of the degree of approximation of both profiles is performed as follows. It is assumed that the X-ray intensity of the sample to be measured with respect to the sampling points 1, 2,. First, Ki = Iui / Isi is determined, and the average of Ki, K = ΣKi / n, is determined. The degree of coincidence E can be expressed as E = 1− | (ΣIui−KΣIsi) | / ΣIui or logarithm, and logK = Σ (logIui−logIsi) / n E = 1−Σ | (logIui−logKIsi) | / ΣlogIui Good.

【0009】或は最小自乗法を用いて次のように一致度
を決めてもよい。測定データに定数Kを掛けて標準試料
のデータから引いたときの差の自乗和が最小になるよう
にKを決める。即ち自乗和 S=Σ(Iui−KIsi)2 …(1) を最小にするKを求める。上式をKで微分して0とお
く。即ち −2Σ(Iui−KIsi)Isi=0 上式から ΣIuiIsi=KΣIsi2 従って K=ΣIuiIsi/ΣIsi2 …(2) Kをこのように決めて自乗和Sを求め、一番小さいSを
与える標準試料を索出すれば、これが被測定試料の非結
晶質の物質名である。上記自乗和Sは(1) 式に(2) 式を
入れて整理すると、 S=ΣIui2 −(ΣIuiIsi)2 /ΣIsi2 …(3) (3) 式右辺第1項は標準試料だけに関する値で予め計算
してデータファイルに格納しておくことができる。従っ
てデータ処理の過程では(3) 式右辺第2項について、Σ
IuiIsiおよびΣIsi2 を計算して(3) 式に代入
してSを求めればよい。
Alternatively, the degree of coincidence may be determined using the least squares method as follows. K is determined so that the sum of squares of the difference when the measured data is multiplied by a constant K and subtracted from the data of the standard sample is minimized. That is, K that minimizes the sum of squares S = Σ (Iui−KIsi) 2 (1) is obtained. The above equation is differentiated by K and set to 0. That is, −2Σ (Iui−KIsi) Isi = 0 From the above equation, ΣIuiIsi = KΣIsi 2, and thus K = ΣIuiIsi / ΣIsi 2 . Is the name of the non-crystalline substance of the sample to be measured. The above sum of squares S can be rearranged by putting equation (2) into equation (1): S = ΣIui 2 − (ΣIuiIsi) 2 / ΣIsi 2 (3) (3) Can be calculated in advance and stored in a data file. Therefore, in the process of data processing, for the second term on the right side of equation (3), Σ
The IuiIsi and ShigumaIsi 2 calculated (3) may be obtained an S substituted into equation.

【0010】[0010]

【発明の効果】本発明によれば、非結晶質試料の同定を
X線回折装置を使って行うことができる。元来X線回折
装置を使えば結晶質の定性分析ができるので、本発明方
法の導入により結晶質試料も非結晶試料も両者が混合し
たような試料も全て同じ装置で分析できることになる。
According to the present invention, an amorphous sample can be identified using an X-ray diffractometer. Since an X-ray diffractometer can be used to perform a qualitative analysis of a crystalline material, the introduction of the method of the present invention makes it possible to analyze both a crystalline sample, an amorphous sample, and a sample in which both are mixed by the same device.

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

【図1】本発明方法の一実施例を説明するフローチャー
FIG. 1 is a flowchart illustrating an embodiment of the method of the present invention.

【図2】X線回折装置による散乱X線強度の角度分布を
示すプロファイルの一例
FIG. 2 is an example of a profile showing an angular distribution of scattered X-ray intensity by an X-ray diffractometer.

【図3】試料の非結晶成分による散乱X線(A)と標準
試料の散乱X線のプロファイル
FIG. 3 is a profile of scattered X-rays (A) due to an amorphous component of a sample and scattered X-rays of a standard sample.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 各種非結晶質の標準試料のX線回折装置
によるX線散乱特性のプロファイルを記憶しておき、被
測定試料のX線回折装置による散乱X線のプロファイル
を測定し、被測定試料が結晶質を含んでいる場合は、
料中の結晶成分による回折X線ピークを除去して、予め
記憶させてある各種標準試料のX線散乱特性のプロファ
イルとの一致度を求め、試料物質の非結晶成分を一致度
の最も大なる標準試料物質と同定することを特徴とする
非結晶性試料の定性分析法。
1. A profile of X-ray scattering characteristics of various non-crystalline standard samples by an X-ray diffractometer is stored, and a profile of a sample to be measured is scattered by the X-ray diffractometer, and the profile of the X-ray is measured. If the sample contains crystalline material, the diffraction X-ray peaks due to the crystal components in the sample are removed, and the degree of coincidence with the X-ray scattering characteristics profiles of various standard samples stored in advance is obtained, and the sample substance is obtained. A qualitative analysis method for a non-crystalline sample, characterized by identifying the non-crystalline component of (1) as a standard sample substance having the highest degree of coincidence.
JP07258692A 1992-02-20 1992-02-20 Qualitative analysis of amorphous samples Expired - Fee Related JP3147976B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP07258692A JP3147976B2 (en) 1992-02-20 1992-02-20 Qualitative analysis of amorphous samples

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP07258692A JP3147976B2 (en) 1992-02-20 1992-02-20 Qualitative analysis of amorphous samples

Publications (2)

Publication Number Publication Date
JPH05232049A JPH05232049A (en) 1993-09-07
JP3147976B2 true JP3147976B2 (en) 2001-03-19

Family

ID=13493639

Family Applications (1)

Application Number Title Priority Date Filing Date
JP07258692A Expired - Fee Related JP3147976B2 (en) 1992-02-20 1992-02-20 Qualitative analysis of amorphous samples

Country Status (1)

Country Link
JP (1) JP3147976B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110793988B (en) * 2019-11-21 2022-03-15 山东建筑大学 Method for representing amorphous-crystal transformation dynamic characteristics by high-energy X-ray

Also Published As

Publication number Publication date
JPH05232049A (en) 1993-09-07

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