The present invention claims priority under 35 U.S.C. § 119 to Japanese Application No. 2021-095294, filed on Jun. 7, 2021, the entire contents of which being incorporated herein by reference.
The present disclosure relates to a degree-of-crystallinity measurement apparatus, a degree-of-crystallinity measurement method, and an information storage medium, and more particularly, to measurement of a degree of crystallinity using X-ray diffraction.
Polymers include crystalline polymers and amorphous polymers. However, even in a crystalline polymer, the crystalline polymer does not have an entirely crystalline structure and includes a crystalline portion and an amorphous portion as a mixture. A proportion of a weight of the crystalline portion with respect to an overall weight of the crystalline polymer is referred to as “degree of crystallinity.” The degree of crystallinity is important information in understanding properties of the crystalline polymer, such as a mechanical property and a chemical property.
In various methods of measuring the degree of crystallinity, a method using X-ray diffraction has great practical advantages in that a sample of any size may be used, and in that the method can be executed without destroying the sample, for example.
In the method using the X-ray diffraction, a degree of crystallinity of a target substance corresponds to a value obtained by dividing an integrated intensity of a scattering pattern (which is, in this case in particular, a diffraction pattern) from the crystalline portion of the target substance by a sum of integrated intensities of scattering patterns from the crystalline portion and the amorphous portion (that is, an integrated intensity of a scattering pattern of the entire target substance).
Accordingly, in order to determine the degree of crystallinity, it is required to accurately identify at least the scattering pattern (diffraction pattern) from the crystalline portion. However, the diffraction pattern from the crystalline portion, which is weak in diffraction intensity in a high-angle region, is buried in scattering patterns from the amorphous portion and other substances and is difficult to identify. Further, when the crystalline polymer is mixed with other mixed substances such as a filler, and especially with an amorphous mixed substance such as glass fiber, it becomes more difficult to separate the scattering pattern from those mixed substances.
According to at least one embodiment of the present disclosure, there is provided a degree-of-crystallinity measurement apparatus, including: a measured pattern acquisition unit configured to acquire a measured X-ray scattering pattern of a sample containing a target substance and another known mixed substance; a known pattern acquisition unit configured to acquire a known X-ray scattering pattern of the other known mixed substance; a crystalline pattern acquisition unit configured to at least partially acquire, based on the measured X-ray scattering pattern of the sample, an X-ray diffraction pattern of a crystalline portion included in the target substance; a crystalline integrated intensity calculation unit configured to calculate an integrated intensity for the acquired X-ray diffraction pattern of the crystalline portion; a target substance integrated intensity calculation unit configured to calculate an integrated intensity for an X-ray scattering pattern of the target substance based on the measured X-ray scattering pattern of the sample and the known X-ray scattering pattern; and a degree-of-crystallinity calculation unit configured to calculate a degree of crystallinity of the target substance based on the integrated intensity for the X-ray diffraction pattern of the crystalline portion and the integrated intensity for the X-ray scattering pattern of the target substance.
Further, according to at least one embodiment of the present disclosure, there is provided a degree-of-crystallinity measurement method, including: a measured pattern acquisition step of acquiring a measured X-ray scattering pattern of a sample containing a target substance and another known mixed substance; a known pattern acquisition step of acquiring a known X-ray scattering pattern of the other known mixed substance; a crystalline pattern acquisition step of at least partially acquiring, based on the measured X-ray scattering pattern of the sample, an X-ray diffraction pattern of a crystalline portion included in the target substance; a crystalline integrated intensity calculation step of calculating an integrated intensity for the acquired X-ray diffraction pattern of the crystalline portion; a target substance integrated intensity calculation step of calculating an integrated intensity for an X-ray scattering pattern of the target substance based on the measured X-ray scattering pattern of the sample and the known X-ray scattering pattern; and a degree-of-crystallinity calculation step of calculating a degree of crystallinity of the target substance based on the integrated intensity for the X-ray diffraction pattern of the crystalline portion and the integrated intensity for the X-ray scattering pattern of the target substance.
Further, according to at least one embodiment of the present disclosure, there is provided a non-transitory computer-readable information storage medium storing a program for causing a computer to execute: a measured pattern acquisition step of acquiring a measured X-ray scattering pattern of a sample containing a target substance and another known mixed substance; a known pattern acquisition step of acquiring a known X-ray scattering pattern of the other mixed substance; a crystalline pattern acquisition step of at least partially acquiring, based on the measured X-ray scattering pattern of the sample, an X-ray diffraction pattern of a crystalline portion included in the target substance; a crystalline integrated intensity calculation step of calculating an integrated intensity for the acquired X-ray diffraction pattern of the crystalline portion; a target substance integrated intensity calculation step of calculating an integrated intensity for an X-ray scattering pattern of the target substance based on the measured X-ray scattering pattern of the sample and the known X-ray scattering pattern; and a degree-of-crystallinity calculation step of calculating a degree of crystallinity of the target substance based on the integrated intensity for the X-ray diffraction pattern of the crystalline portion and the integrated intensity for the X-ray scattering pattern of the target substance.
A description is given below in detail of an embodiment of the present disclosure, based on the drawings.
(Apparatus Configuration)
The X-ray diffractometer 12 performs X-ray diffractometry. Specifically, the X-ray diffractometer 12 allows an X-ray of a known wavelength to enter a sample and measures an intensity of a scattered X-ray. Data of the X-ray intensity for each value of a diffraction angle 2θ is output as a measured pattern from the X-ray diffractometer 12 to the arithmetic device 14. The measured pattern output to the arithmetic device 14 may be a measured pattern subjected to correction with a Lorentz-polarization factor (Lp correction). The X-ray diffractometer 12 can measure the intensity of the scattered X-ray at each diffraction angle from a minimum angle 2θL that is as small as about 100 to a maximum angle 2θH that is as large as about 120°. In the present application, a profile of the X-ray intensity measured by the X-ray diffractometer 12 (data indicating a change in X-ray intensity with respect to a change in diffraction angle) is referred to as “X-ray scattering pattern.” The X-ray scattering pattern is in particular an “X-ray diffraction pattern” when the sample is crystalline.
In this embodiment, as the sample serving as a measurement target of the X-ray scattering pattern, a target substance such as a polymer in a powdery form or having fluidity, which may be in a crystalline state in part and in an amorphous state in the remainder, mixed with one or a plurality of other known substances (mixed substances) such as fillers in powdery forms, for example, may be used. When the sample is produced, types and a weight ratio of a plurality of substances forming the sample are known. A chemical formula and a chemical formula weight of each substance are also known. Further, an X-ray scattering pattern of the mixed substances is also known. In the following description, a measurement target substance is in a bulk solid form. When such a measurement target substance is synthesized, the polymer in powdery form or having fluidity, and a plurality of other known substances in a powdery form, such as fillers, are mixed. Such a mixture is subjected to forming and heating processing to produce a resin material of a product, which is the sample. As a matter of course, the present invention is applicable not only to a sample in a bulk solid form, but also to a sample in a powdery form.
The arithmetic device 14 is formed of, for example, a publicly known computer system, and includes a CPU and a memory. The storage unit 16 formed of a computer-readable information storage medium such as a solid state disk (SSD) or a hard drive disk (HDD) is connected to the arithmetic device 14. The storage unit 16 stores a degree-of-crystallinity measurement program in an embodiment of the present disclosure, and the apparatus and the method according to an embodiment of the present invention are implemented by the arithmetic device 14 executing the program. The storage unit 16 further stores chemical formula information of each substance included in the sample (a chemical formula, a chemical formula weight, and an electron number of each atom contained in the substance), and the weight ratio of the substances. The X-ray scattering patterns and other such information of the above-mentioned mixed substances are also stored.
The display unit 18 is a display device which displays a result of calculation by the arithmetic device 14. For example, the display unit 18 displays a degree of crystallinity of the target substance as a numerical value or a graph.
(Outline of Sample Measurement and Degree-of-Crystallinity Calculation)
As described above, the sample may include a plurality of mixed substances, but it is assumed here that the sample includes one type of mixed substance, and
The mixed substance may be amorphous, crystalline, or a mixture thereof. When the mixed substance is crystalline, the X-ray scattering pattern of the mixed substance is a diffraction pattern. Further, when the sample contains a plurality of mixed substances, data similar to that described above may be stored for each of the substances in the storage unit 16. Alternatively, the plurality of mixed substances having predetermined weight fractions as a whole may be regarded as one mixed substance, and data similar to that described above may be stored for the one mixed substance in the storage unit 16.
In a first embodiment of the present disclosure to be described later, a value obtained by dividing an integrated intensity (with the correction with the Lorentz-polarization factor (Lp correction)) with an interval of integration from 2θL to 2θM in the crystalline pattern y1C shown in
Further, in a second embodiment of the present disclosure to be described later, the crystalline pattern y1C shown in
In this embodiment, for the sample as the measurement target per se, or for another sample having the same composition, the X-ray scattering pattern is measured in advance over the angle range from 2θL to 2θH as shown in
(Theoretical Background: Degree of Crystallinity)
Now, the theoretical background of the degree-of-crystallinity calculation by the arithmetic device 14 will be described. For the analysis in the arithmetic device 14, a relatively new quantitative analysis approach invented by the inventor of the present invention is applied, and the degree of crystallinity of the target substance is formulated to indicate weight fractions of the crystalline portion and an amorphous portion. Further, the above-mentioned new quantitative analysis approach is applied to calculate the scale factor SCk described above. The above-mentioned quantitative analysis approach is also described in, for example, J. Appl. Cryst. (2016). 49, 1508-1516, Japanese Patent No. 6231726, Japanese Patent Translation Publication No. 2017/149913, and the like.
The following equation (1) is a relational expression of an integrated intensity Yk derived from each substance, which is derived by the above-mentioned new quantitative analysis approach, in which “k” is an ordinal number indicating the substance.
Here, Yk is expressed by the following equation (2), in which y(2θ)k is an X-ray scattering pattern of the k-th substance, and G(2θ) is an Lp correction factor. An interval of integration is the entire interval of integration from 2θL, which is about 10°, to 2θH, which is about 120°, for example.
Yk=∫y(2θ)kG(2θ)d(2θ) (2)
Further, a reciprocal of ak is given by the following equation (3). In the equation, NA is the number of atoms contained in a chemical formula of the k-th substance, nki is an electron number of the i-th atom contained in the chemical formula of the k-th substance, and Mk is a chemical formula weight of the k-th substance contained in the sample.
The equation (1) can also be expressed as the following equation (4).
When a weight ratio between the crystalline portion and the amorphous portion of the target substance is defined as the degree of crystallinity, the degree of crystallinity DOC of the k-th substance is expressed by the following equation (5). In the equation, WkC is a weight of the crystalline portion in the k-th substance, WkA is a weight of the amorphous portion in the k-th substance, wkc is a weight fraction of the crystalline portion in the k-th substance, and wkA is a weight fraction of the amorphous portion in the k-th substance.
When a weight fraction of the k-th substance in the sample is represented by wk, wk is expressed by the following equation (6).
wk=wkC+wkA (6)
It is assumed here that k=1 and that the 1st substance is a target for calculating the degree of crystallinity, that is, the target substance. When the equation (6) is substituted into the equation (5), and the equation (4) is further substituted, the following equation (7) is obtained for the degree of crystallinity DOC of the 1st substance. In the equation, Y1c is an integrated intensity with the Lp correction of the X-ray diffraction pattern y1C derived from a crystalline portion of the 1st substance (see an equation (19)), and Y1A is an integrated intensity with the Lp correction of an X-ray diffraction pattern derived from an amorphous portion of the 1st substance. In any case, an interval of integration is the entire range from 2θL to 2θH, for example.
In accordance with the equation (7), when an integrated intensity Y1 with the Lp correction of the X-ray scattering pattern of the entire target substance and an integrated intensity Y1C with the Lp correction of the X-ray diffraction pattern of the crystalline portion in the target substance are known, the degree of crystallinity DOC can be determined.
(Theoretical Background: Background Intensity)
As described above, the X-ray scattering pattern contains the background intensity. When the entire X-ray scattering pattern of the k-th substance is represented by y(2θ)kBP, the background intensity is represented by y(2θ)BG, and a component derived from only the k-th substance is represented by y(2θ)k, the following equation (8) is established.
y(2θ)kBP=Y(2θ)k+y(2θ)BG (8)
Here, integrated intensities of y(2θ)kBP, y(2θ)k, and y(2θ)BG are expressed by an equation (9) to an equation (11), respectively. These equations hold over a suitable and common interval of integration.
YkBP=∫y(2θ)kBPG(2θ)d(2θ) (9)
Yk=∫y(2θ)kG(2θ)d(2θ) (10)
Bk=∫y(2θ)BGG(2θ)d(2θ) (11)
From the expression (8), YkBP, Yk, and Bk have a relationship of the following equation (12).
YkBP=Yk+Bk (12)
When a background ratio Rk of the k-th substance is defined by the following equation (13), the equation (12) can be rewritten as an equation (14).
Rk=Bk/Yk (13)
YkBP=(1+Rk)Yk (14)
In other words, with the equation (14), an integrated intensity YkBP with the background and an integrated intensity Yk without the background can be mutually converted using the background ratio Rk.
(Theoretical Background: Calculation of Degree of Crystallinity DOC (Part 1))
In accordance with the DD method, a calculated integrated intensity YkBP_calc of the k-th substance is given by the following equation (15).
The integrated intensity YkBP of the k-th substance is considered as being obtained by prorating an observed integrated intensity YBP_obs of the entire sample by a ratio of the calculated integrated intensity YkBP_calc, and hence the following equation (16) is established.
In the equation, YBP_calc is given by the following equation (17), and D is given by an equation (18) after the next.
YBP_calc=Y1BP_calc+Y2BP_calc+ . . . +YKBP_calc (17)
D=Σk′=1K(1+Rk′)wk,ak∝−1 (1δ)
In other words, the integrated intensity Y1BP of the 1st substance serving as the target substance can be calculated based on the observed integrated intensity YBP_obs of the entire sample, and Rk, wk, and ak of every substance in the sample. All of those items of information can be grasped at the time of preparing the sample. Further, Y1BP can be transformed to Y1 using the equation (14). Still further, the integrated intensity Y1C of the crystalline portion of the target substance can be calculated by the following equation (19). Through substitution of the thus-acquired Y1 and Y1C into the equation (7), the degree of crystallinity DOC can be obtained.
Y1C=∫y(2θ)1CG(2θ)d(2θ) (19)
(Theoretical Background: Calculation of Degree of Crystallinity DOC (Part 2))
The degree of crystallinity DOC of the equation (7), which is derived on the basis of the new quantitative analysis approach, is based on the premise that an interval of integration in calculating the integrated intensities Y1C and Y1 is the entire range. In order to calculate those values, it is required to accurately identify the X-ray scattering pattern from the crystalline portion included in the target substance. However, the diffraction pattern y1C from the crystalline portion, which has weak diffraction intensity in a high-angle region, is buried in scattering patterns from the amorphous portion and other substances, and is difficult to identify. This leads to underestimation of Y1C and the degree of crystallinity DOC.
Thus, in order to calculate a more likely approximate value of the degree of crystallinity DOC, it is considered to limit the interval of integration in calculating the integrated intensities Y1C and Y1.
An X-ray scattering pattern y(2θ)BP with the background of the entire sample is expressed by the following equation (20). In the equation, y(2θ)1BP is an X-ray scattering pattern with the background of the 1st substance (target substance), y(2θ)kBP is an X-ray scattering pattern with the background of the k-th substance (mixed substance), and SCk is a scale factor.
y(2θ)BP=y(2θ)1BP+Σk′=2KSck′y(2θ)k′BP_obs (20)
Here, when y(2θ)kBP is known for the mixed substance, the following equation (21) is established for k=2 to K based on the equation (20) and the equation (16). Then, the scale factor SCk can be obtained from the equation (21).
When the thus-obtained scale factor SCk is used, for any given interval of integration (2θX to 2θY) as in the following equation (22), an integrated intensity YXPBP (=y1BP) of the target substance can be determined by the following equation (22).
YXYBP=Y1BP=∫2θ
Over the interval of integration (2θX to 2θY), an integrated intensity YC-XY (=Y1C) of the crystalline portion of the target substance can also be determined by the following equation (23).
YC-XY=Y1C∫2θ
Through substitution of those values into the equation (7), the degree of crystallinity DOC of the target substance can be determined approximately.
Now, accuracy of the degree of crystallinity obtained by limiting the interval of integration as described above is evaluated.
In accordance with the above notation, the equation (7) can be expressed as the following equation (24).
Further, when a degree of crystallinity in a case in which the interval of integration is limited to 2θL to 2θM is notated as DOCM, DOCM can be defined as the following equation (25).
An error ΔDOCM between the degree of crystallinity DOC of the equation (24) and the degree of crystallinity DOCM of the equation (25) can be expressed as the following equation (26).
ΔDOCM=DOCM−DOC (26)
The equation (26) can be transformed to the following equation (27).
Here, the following equation (28), which is a parenthesized value in the right-hand side of the equation (27), is about 0.11 in accordance with consideration by the inventor.
Further, the portion of the following equation (29) in the right-hand side of the equation (27) is about 0.5 when 2θM is around 70° in accordance with consideration by the inventor.
Thus, when the degree of crystallinity is about 40%, ΔDOCM can be estimated to be about 0.0088. This means that, as long as other errors are small, even when the interval of integration is limited, the following equation (30) is established, that is, DOCM is a good approximate value of DOC.
DOCM≈DOC (30)
(Theoretical Background: Calculation of Degree of Crystallinity DOC (Part 3))
DOCM is a good approximate value of DOC, but when the X-ray scattering pattern of the sample is measured up to 2θT, which is an angle higher than 2θM, DOC can be brought even closer to a true value.
First, an initial value DOCT is defined as expressed by the following equation (31).
An error ΔDOCT between the degree of crystallinity DOC of the equation (24) and the degree of crystallinity DOCT of the equation (31) can be expressed as the following equation (32).
ΔDOCT=DOCT−DOC (32)
ΔDOCT can be transformed to the following equation (33).
Here, the following equation (34) is obtained based on the equation (30), and the equation (33) can be transformed to an equation (35).
DOC, DOCT, and ΔDOCT have a relationship of an equation (36), and hence a recurrence formula of an equation (37) is obtained using the equation (35).
In the equation (37), DOCT is substituted as an initial value of DOC on the right-hand side to calculate DOC on the left-hand side. Then, the thus-obtained DOC is substituted again into DOC on the right-hand side. This can be repeated to obtain a degree of crystallinity DOC that is close to the true value.
Now, the first embodiment will be described. The first embodiment corresponds to “Calculation of Degree of Crystallinity DOC (Part 2)” described above.
In the first embodiment, the scale factor SCk is first calculated in accordance with a flowchart of
Next, the arithmetic device 14 reads the known pattern yxBP-obs (see FIG. 3) of the mixed substance from the storage unit 16 (Step S101). Here, one type of mixed substance is used, and “k” for the mixed substance is 2.
Further, the arithmetic device 14 reads, for each of the substances (the target substance and the mixed substance) forming the sample, the chemical formula, the chemical formula weight Mk, and the electron number nki, the weight fraction wk, and the background ratio Rk of each atom contained in the chemical formula of the substance from the storage unit 16 (Step S102).
After that, the arithmetic device 14 calculates a scale factor SC2 in accordance with the equation (21) and stores the calculated scale factor SC2 in the storage unit 16 (Step S103).
Next, the arithmetic device 14 calculates the degree of crystallinity DOCM in accordance with a flowchart of
Next, the arithmetic device 14 reads the known pattern yxBP_obs (
The arithmetic device 14 calculates the target substance pattern y1BP (see
Further, the arithmetic device 14 extracts diffraction lines from an angle range from 2θL to 2θM of the target substance pattern y1BP obtained in Step S203, to thereby extract a crystalline pattern y1C (see
After that, the arithmetic device 14 calculates an integrated intensity YLM (Step S205). Specifically, the arithmetic device 14 calculates YLMBP based on the equation (22). Further, the arithmetic device 14 reads a background ratio R1 (calculated over an interval of integration from 2θL to 2θM) stored in advance in the storage unit 16 and converts YLMBP into YLM using the equation (14). The X-ray scattering pattern y1BP of the target substance also contains a background intensity indicated by the broken line in
Further, the arithmetic device 14 integrates the crystalline pattern y1C obtained in Step S204 over the angle range from 2θL to 2θM and with the Lp correction to acquire an integrated intensity YC-LM (Step S206). Then, YC-LM obtained in Step S206 is divided by YLM obtained in Step S205 to obtain the degree of crystallinity DOCM (Step S207). With the processing described above, a likely value of the degree of crystallinity can be obtained for the target substance.
Now, the second embodiment will be described. The second embodiment corresponds to “Calculation of Degree of Crystallinity DOC (Part 3)” described above.
In the second embodiment, the arithmetic device 14 first calculates the scale factor SCk in accordance with the flowchart of
Next, the arithmetic device 14 calculates the degree of crystallinity DOC in accordance with a flowchart of
In Step S307, the arithmetic device 14 calculates an integrated intensity YMT. Specifically, the arithmetic device 14 calculates YMTBP based on the equation (22). Further, the arithmetic device 14 reads a background ratio R1 (calculated over an interval of integration from 2θM to 2θT) stored in advance in the storage unit 16, and converts YMTBP into YMT using the equation (14).
Next, the arithmetic device 14 substitutes the values obtained in Step S305 to Step S307 into the equation (31) to calculate the initial value DOCT (Step S308). Then, the arithmetic device 14 substitutes the values obtained in Step S305, Step S307, and Step S308 into the right-hand side of the recurrence formula (37) to obtain DOC on the left-hand side. This calculation is repeated a predetermined number of times, or until a value of DOC converges to obtain the final DOC (Step S309). With the processing described above, a more likely value of the degree of crystallinity can be obtained for the target substance.
The present disclosure is not limited to the embodiments described above. Various modifications can be made within the spirit of the present disclosure, and such modifications are also encompassed in the scope of the present disclosure.
Number | Date | Country | Kind |
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2021-095294 | Jun 2021 | JP | national |
Number | Name | Date | Kind |
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20180364183 | Toraya et al. | Dec 2018 | A1 |
20210020272 | Godwin | Jan 2021 | A1 |
Number | Date | Country |
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2017149913 | Sep 2017 | WO |
Entry |
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Rutland, “X-ray Determination of Crystallinity and Diffuse Disorder Scattering”; Acta Cryst. vol. 14, Jan. 11, 1961; pp. 1180-1185. |
Toraya, “A new method for quantitative phase analysis using X-ray powder diffraction: direct derivation of weight fractions from observed integrated intensities and chemical compositions of individual phases”, Journal of Applied Crystallography, vol. 49, Jun. 28, 2016; pp. 1508-1516. |
Number | Date | Country | |
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20220390392 A1 | Dec 2022 | US |