Rapid quantification of components in solid mixtures of chemicals via time-domain NMR spectroscopy
10697911 ยท 2020-06-30
Inventors
Cpc classification
G01N24/084
PHYSICS
G01R33/4625
PHYSICS
International classification
Abstract
There is described a method for determining the relative quantities of the expected components in a multi-component mixture of solids. The proposed quantification method makes use of a time domain nuclear magnetic resonance (TD-NMR) spectrometer and requires that, for each of the expected components in the mixture, a T1 saturation recovery curve (SRCi) is measured and recorded. The saturation recovery curve for the mixture sample (SRCmix) is determined from a measurement of the sample with the spectrometer. The relative amounts of the expected components present in the mixture sample are determined by fitting a linear combination of the component SRCs (SRCi) to the SRCmix. The resulting value of each weighting coefficient in the fit provides the relative proportion of the corresponding component in the overall sample.
Claims
1. A method of determining the relative quantities of a plurality of expected components in a sample using a time-domain nuclear magnetic resonance (TD-NMR) spectrometer, the method comprising: a) obtaining a component saturation recovery curve (SRC) for each of the components; b) measuring the sample using a TD-NMR spectrometer and obtaining a mixture saturation recovery curve (SRC.sub.mix) therefrom; and c) fitting to the SRC.sub.mix a linear combination of the component SRCs, each scaled by a weighting coefficient, the respective weighting coefficients being indicative of the relative quantities of the plurality of expected components in the sample.
2. The method of claim 1 wherein obtaining a component saturation recovery curve (SRC) for each of the components comprises measuring the component using the TD-NMR spectrometer.
3. The method of claim 1, wherein fitting to the SRC.sub.mix a linear combination of the component SRCs comprises identifying the weighting coefficients that minimize a representative value of a difference vector between the SRC.sub.mix and the linear combination of the component SRCs.
4. The method of claim 3, wherein minimizing the representative value of the difference vector comprises minimizing the variance between the SRC.sub.mix and the linear combination of the component SRCs.
5. The method of claim 1, wherein fitting to the SRC.sub.mix a linear combination of the component SRCs comprises normalizing the SRC.sub.mix and the component SRCs.
6. The method of claim 5, wherein the normalizing reflects operational parameters of the TD-NMR spectrometer.
7. The method of claim 5, wherein the normalizing reflects a molecular weight and/or a number of protons of each sample component.
8. The method of claim 3, wherein identifying the weighting coefficients comprises minimizing a representative value of
9. The method of claim 1, wherein obtaining a component saturation recovery curve (SRC) comprises obtaining one of a .sup.1H, a .sup.13C, a .sup.19F and a .sup.31P T.sub.i saturation recovery curve, and obtaining a mixture saturation recovery curve (SRC.sub.mix) comprises obtaining the one of a .sup.1H, a .sup.13C, a .sup.19F and a .sup.31P T.sub.i saturation recovery curve.
10. The method of claim 1, wherein obtaining a component SRC for each of the components comprises obtaining an SRC for at least one active pharmaceutical ingredient and at least one excipient component of a pharmaceutical formulation.
11. The method of claim 1, wherein obtaining a component SRC for each of the components comprises obtaining an SRC for at least two polymorphs, solvates or hydrates of a compound.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1) Further features and advantages of the present disclosure will become apparent from the following detailed description, taken in combination with the appended drawings, in which:
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DETAILED DESCRIPTION
(12) Shown in
(13) Time-domain NMR (TD-NMR) can be used to measure bulk relaxation in solid materials, and omits Fourier transformation of the acquired free induction decay (FID) to the frequency domain. For the method described herein, high spectral resolution in the frequency domain is not needed, so the result may be obtained without sophisticated and expensive technology, such as ultra-homogeneous, high-field magnets (e.g., 9.4 T with better than parts-per-million (ppm) homogeneity over sample volumes on the milliliter scale).
(14) Advantageously, TD-NMR spectroscopic instruments can be provided as tabletop instruments. As such, they occupy less space and are less costly to purchase and operate as compared to their high-resolution ssNMR counterparts. This is why TD-NMR spectroscopic instruments are popular in industrial settings, for example in quality control processes. Moreover, in the TD-NMR approach, only the first few points (e.g., about 6-8) of the FID are acquired and averaged, resulting in a considerably reduced amount of time required to conduct the relaxation measurement.
(15) Another significant benefit of using a TD-NMR instrument is the capability of analyzing very heterogeneous samples, e.g., pharmaceutical formulations in tablet, capsule, gel, or paste form, as well as rubbers, polymers, and soils. By contrast with conventional high-resolution ssNMR analysis, there is no requirement on sample texture or homogeneity, and magic-angle spinning is not necessary. A large variety of solids can be introduced into the sample chamber 16.
(16) In the present invention, FID intensities are used to construct the corresponding saturation recovery curves (SRCs) from which quantification can be performed. Notably, the SRC of a given sample embodies a composite of the different SRCs of its components. Such a curve would typically display multi-exponential behavior due to the variety of T.sub.1 relaxation times of its components. However, even pure materials can exhibit multiple relaxation rates and give rise to SRCs with multi-exponential behavior. The multi-exponential behavior of the SRC of pure materials complicates their identification and quantification in the time-domain.
(17) There have been attempts to use the Inverse Laplace Transform (ILT) to decompose bulk relaxation curves measured by TD-NMR into their individual contributions. Indeed, the ILT can be used to extract exponential components from a multi-exponential graph such as the T.sub.1 or T.sub.2 relaxation curve of a mixture. Moreover, from the resulting relaxation time distribution plot the components may be quantified relative to each other using ILT. For a full determination of the relaxation time profile from a saturation recovery experiment for a mixture of N components, each component i containing some number M.sub.i of distinctly relaxing spins, would be fit to
I(t)=I.sub.0.sub.i=1.sup.Np.sub.i(.sub.j=1.sup.M.sup.
where t is time, I.sub.0 is the overall intensity, p.sub.i is a weighting factor specifying the relative signal contribution of the i.sup.th component, and (T.sub.1).sub.ij represents the time constants characteristic of each subpopulation of distinctly relaxing spins in that component. The f.sub.ij are fixed, compound-specific properties reflecting the fractional contributions of its subpopulations to the signal. Thus, fitting the profile observed from a multi-component mixture to equation (a) entails searching for the optimum values of M.sub.total time constants (T.sub.1,ij) (where (M.sub.total=.sub.i=1.sup.NM.sub.j)N), of N weighting factors (p.sub.i), and of one overall intensity (I.sub.0).
(18) However, the ILT methodology described above often results in misleading and inaccurate fits when a variety of solutions (i.e., optimum or near-optimum parameter sets) may yield a similar quality of fit. For example, even in fitting to the profile of a pure compound as a single polymorph (N=1), it can be difficult to determine multi-exponential behavior (M>1) for similarly relaxing subcomponents. Therefore, ILT fails to quantify components in an unambiguous and reliable way. However, clear and consistent quantification methods for TD-NMR instruments are needed in order to take advantage of the many benefits these instruments offer.
(19) Unlike prior approaches, the present invention uses .sup.1H and .sup.19F T.sub.1 saturation recovery curves (SRCs) obtained using a TD-NMR instrument, such as a Bruker Minispec mq20 benchtop instrument, not by extracting relaxation parameters, but rather as a fingerprint in which specific details of the recovery, such as time constants and/or possible multiexponentiality, remain unknown and unquantified. For the analysis of a given mixture, the SRCs for the relevant pure components, as well as for the mixture itself are measured. The relative amounts of the mixture components are obtained from a fit of the mixture SRC with a linear combination of normalized and weighted SRCs of the pure components. The method that uses SRCs to quantify mixture components will occasionally be called QSRC hereinafter.
(20) The QSRC method circumvents the problems associated with quantifying components in mixtures using full relaxation profiles by replacing the complexity of an individual-component relaxation with a measured SRC as a fingerprint, I.sub.i(t), for each substance present in a mixture. In this case, equation (a) simplifies to:
I(t)=I.sub.0.sub.i=1.sup.np.sub.iI.sub.i(t)(b)
Thus, no time constant needs to be retrieved from the data, even though the time profile observed from a sample reflects a composite of several relaxation times, including even multi-exponential sets for individual components. Here, unlike in prior approaches in which the T.sub.1,ij values needed to be characterized, only critical p.sub.i values are explicit in the equation and thus need to be obtained. In the method described herein, the T.sub.1,ij values remain uncharacterized, but are implicitly represented by premeasured SRCs of the expected components.
(21) The QSRC method described herein is depicted in the flowchart of
(22) Following identification of the probable sample components, the operational parameters of the instrument (number of scans per recovery increment, number of points on the SRCs, time profile of points, etc.) are set (step 120). Once the TD-NMR instrument is ready, each one of the pure compounds from the list identified in step 110 is individually measured using the TD-NMR instrument (step 130) and the corresponding reference SRC is stored, such as in the memory of a host computer of the TD-NMR instrument. Steps 130 and 140 are then repeated for each of the probable sample components so as to construct a set of reference SRCs. The set of reference SRCs may also be constructed in advance and stored in a database, to be accessed later during the sample analysis procedure.
(23) In step 150, the mixture known to comprise the components in unknown concentrations is then measured using the TD-NMR instrument. The SRCs of each of the components and the mixture are then normalized (step 170). In an exemplary embodiment, normalization includes various scaling factors applied to the SRCs based on the parameters of data acquisition by the instrument and component chemical properties, notably the molecular weight and number of protons of the mixture components. Once all SRCs are scaled appropriately, a fitting process is used to find the coefficients of normalized reference SRCs that provide the best fit to the mixture SRC (step 190). The fitting parameters c represent the concentrations of the components identified in step 110.
(24) The accuracy of the QSRC method of the present invention is demonstrated below in the .sup.1H and .sup.19F SRC data measured on several model systems. Since the method is based on differences in SRCs, .sup.1H and .sup.19F model systems containing components with different T.sub.1 ratios are investigated. .sup.1H SRC data on numerous physical binary blends of ibuprofen and indomethacin, and of ibuprofen and itraconazole, illustrate how well the method based on .sup.1H SRC data reproduces the prepared blend compositions. To establish how well the QSRC method works for observing .sup.19F, .sup.19F SRCs of several binary physical blends of 2-trifluoromethyl cinnamic acid and 6-trifluoromethyl uracil and of 2-trifluoromethyl cinnamic acid and fluoxetine HCl were analyzed.
EXPERIMENTAL DETAILS
(25) Experiments were performed on different mixtures of model compounds 15 shown in
(26) Samples
(27) As shown in
(28) TABLE-US-00001 TABLE 1 Compositions of the binary blends of ibuprofen and indomethacin. Blend Name Bl-1 Bl-2 Bl-3 Bl-4 Bl-5 Bl-6 Bl-7 m (Ibu) [mg] 205.456 126.202 120.092 90.466 60.506 29.64 15.086 m (Indo) [mg] 203.712 124.196 180.674 210.024 240.898 270.514 285.38 m % Ibu 50.2 50.4 39.9 30.1 20.1 9.9 5.0
(29) TABLE-US-00002 TABLE 2 Compositions of the binary blends of ibuprofen and itraconazole. Bl-1 Bl-2 Bl-3 Bl-4 Bl-5 Bl-6 Bl-7 m (Ibu) [mg] 163.080 151.184 116.426 85.502 55.968 32.982 16.084 m (Itra) [mg] 140.432 151.318 184.652 215.060 244.778 268.402 285.846 m % Ibu 53.7 50.0 41.4 30.0 20.1 10.1 5.3
(30) TABLE-US-00003 TABLE 3 Compositions of the binary blends of 2-trifluoromethyl cinnamic acid and 6-trifluoromethyl uracil. Blend Name Bl-1 Bl-2 Bl-3 Bl-4 Bl-5 m (6TFMU) 2621.571 1496.472 495.511 301.410 153.316 [mg] m 405.647 1413.120 2525.890 2673.836 2885.314 (2TFMCA) [mg] m % 86.6 51.4 16.1 10.1 5.5 6TFMU
(31) TABLE-US-00004 TABLE 4 Compositions of the binary blends of 2-trifluoromethyl cinnamic acid and fluoxetine HCl. Blend Name Bl-1 Bl-2 Bl-3 m (FXT HCl) [mg] 967.262 631.693 115.667 m (2TFMCA) [mg] 502.741 2390.760 945.501 m % FXT HCl 65.8 20.9 10.9
Time-Domain NMR
(32) All experiments were conducted on a commercial Mq20 bench-top TD-NMR spectrometer from BRUKER BioSpin Corp., Billerica, Mass., at a magnetic field of 0.47 Tesla (19.95 MHz .sup.1H Larmor frequency) generated by a permanent magnet with 25 mm gap size. The magnetic field of the permanent magnet was kept constant by controlling the magnet temperature at 400.001 C. The instrument was equipped with a .sup.1H probe exhibiting a 6.7 s receiver dead-time, accommodating 10 mm glass tubes as sample holders, and a .sup.19F probe possessing a 21.1 s receiver dead-time accommodating 18 mm glass tubes as sample holders. The probe for .sup.1H measurements is a variable temperature probe and all .sup.1H detected experiments were performed at 20 C., temperature-controlled with a Julabo chiller unit. The probe for .sup.19F measurements does not allow for temperature control and all .sup.19F observed experiments were performed at the temperature of the sample orifice which is approximately 40 C., close to the magnet temperature. T.sub.1 saturation recovery curves were measured by using a standard pulse program with a 50 ms saturation pulse train, followed by an exponentially incremented recovery delay, and a 90 read out pulse. The recycle delay was 0.1 s for all experiments. Typical 90 pulse lengths were about 2.8 s for .sup.1H and 4.5 for .sup.19F. The number of recovery delay increments was varied in order to study respective effects on the analysis. The longest recovery delay used in the experiments was adjusted for each experiment to allow the relevant model compounds to reach full recovery.
(33) Values of all parameters listed above are those that were used during the experiments. The method described herein can be performed without being limited to these values; other parameters with which TD-NMR instruments are known to be operable may also be used.
(34) QSRC Method
(35) The QSRC method is based on the expression of a given SRC collected for a physical mixture of solids, SRC.sub.mix, as a linear combination (i.e., weighted average) of the SRCs of the individual components, SRC.sub.i. With the right coefficients (i.e., proportions) that need to be determined, the SRCs of the individual components can be summed up to the SRC.sub.mix with a minimum error.
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(37) In equation (1), each of the SRCs is a vector having points consisting of the respective signal intensities, I, at the n recovery times:
SRC={I.sub.1,I.sub.2,I.sub.3, . . . ,I.sub.n}(2)
(38) As such, the summing of SRCs (e.g., the linear combination shown in equation (1)) may be performed on a point-by-point basis. Furthermore, c.sub.i, N, and b are, respectively, the fraction of component i in the mixture, the number of components in the mixture, and an arbitrary offset. The arbitrary offset b is usually small and results from experimental imperfections.
I.sub.mix,=5.0 s=0.5I.sub.1,=5.0 s+0.5I.sub.2,=5.0 s(3)
(39) For illustration purposes, the recovery points in
(40) According to an exemplary embodiment of the invention, the reference SRCs are appropriately scaled and normalized. This is done in order for the approach of using a linear combination of SRCs to be generally applicable to quantifying the components in a mixture.
(41) Generally, the intensity of a signal measured by an NMR instrument is dependent upon three key parameters: the number of scans acquired, the sample mass (equivalent to the number of moles of the observed nucleus), and the characteristic electronic properties and receiver gain settings of the instrument. In the proposed quantification method, the reference SRCs (20a, 20b) are rendered independent of the sample masses, number of scans, and instrument characteristics and receiver gain settings. This normalization has clear advantages and is discussed below. This normalization is performed by dividing a given reference SRC (20a, 20b) by the product of the mass (m.sub.molecule) of the corresponding reference molecule, the number of scans (ns) acquired per recovery increment, and the signal intensity (S.sub.0) observed for a given receiver gain setting per scan and per mole of the observed nuclei, as shown in equation (4):
(42)
(43) Equation (4) can be simplified and its utility significantly enhanced when combined with two other expressions. First, the intensities of SRC data points for >5 T.sub.1 is given by:
I.sub.5T1=nNnsS.sub.0(5)
where nN is the number of moles of the observed nuclei. Second, the mass of a given reference molecule can be expressed as a function of the number of moles of the observed nuclei per moles of reference molecule, NN (e.g., NN=18 for a .sup.1H SRC of ibuprofen):
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(45) Here, n.sub.molecule and M are the number of moles of reference molecules and the molecular mass of the reference molecule, respectively. Combining equations (4)-(6) yields the normalized reference SRC as:
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(47) In effect, every intensity along a given reference SRC is divided by the product of the intensity of the same SRC at >5T.sub.1 (last recovery point collected, also the maximum value of the SRC) and the molecular mass of the respective reference molecule, and multiplied by the number of moles of observed nuclei per moles of reference molecules.
(48) After normalization, the normalized reference SRCs can be utilized in the linear combination of reference SRCs with the weighting coefficients, c.sub.i.sup.norm, and the arbitrary offset, b.sup.norm as fitting parameters. The parameters of the linear combination which minimize the difference between the linear combination and the mixture SRC should be found, as formalized in equation (8).
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Since the bracketed expression in equation (8) represents a vector, a scalar value of this vector is minimized, as explained further below in conjunction with
(50) The normalization as described in equation (7) has noteworthy advantages. It makes it entirely unnecessary to determine any sample masses, and uncertainties about the size and position of the active space in the sample tubes are completely circumvented. Moreover, the normalization allows for the use of SRCs acquired with different numbers of scans and receiver gain settings in the same analysis.
(51) Results
(52) QSRC MethodProof Of Concept on .sup.1H SRC Data
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for ibuprofen and indomethacin are:
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respectively. The normalization reduces the arbitrary intensities of the reference SRCs significantly, resulting in plateaus below 0.1, more specifically plateaus of 0.08725 and 0.044719, for ibuprofen and indomethacin respectively (25a, 25b). Accordingly, in order to facilitate an easier and faster minimization procedure, the intensity of the raw blend Bl-1 SRC was scaled to a similar plateau level (e.g., 1.0). All intensities of that blend SRC.sub.mix 32 were divided by the intensity of its last point, resulting in the normalized blend SRC 35 (square points) reaching a plateau at 1.0. The normalized SRCs 25a, 25b from
(58) The actual values obtained for the fitting parameters, c.sub.ibuprofen.sup.norm, c.sub.indomethacin.sup.norm, and b.sup.norm are 7.69, 7.49, and 0.0036, respectively. The results of the QSRC analysis for blend Bl-1 are also displayed in
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respectively.
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(61) From the data in
(62) The QSRC analysis is predictive, as evidenced in
(63) TABLE-US-00005 TABLE 5 .sup.1H QSRC results for the ibuprofen/indomethacin binary blends. Blend Name Bl-1 Bl-2 Bl-3 Bl-4 Bl-5 Bl-6 Bl-7 m % Ibu (prep) 50.2 50.4 39.9 30.1 20.1 9.9 5.0 m % Ibu (fit) 50.6 50.1 40.3 30.8 20.2 9.3 4.6 rms 0.0082 0.01 0.0081 0.0097 0.0116 0.0135 0.0120
QSRC MethodEffect of Signal-To-Noise and Number of Recovery Points
(64) The number of delay points collected along the SRCs and the signal to noise ratio (SNR) of the SRCs play an important role in the accuracy of the QSRC analysis. The effects of both parameters were explored utilizing the ibuprofen/indomethacin blends 1-7 from Table 1. SRCs of ibuprofen, indomethacin, and all 7 blends were collected with varying number of scans per recovery increment and number of recovery points, and the data analyzed with the QSRC method. Table 6 summarizes the various experimental conditions used. The results of the analyses are displayed in
(65) TABLE-US-00006 TABLE 6 .sup.1H QSRC results for the ibuprofen/indomethacin blends utilizing SRCs collected with different experimental conditions. Condition Number of Number of Exp Name scans points time R.sup.2 slope intercept 4sc_50p 4 50 8 0.9995 1.012 0.304 32sc_50p 32 50 0.9984 1.001 0.196 4sc_30p 4 30 0.9994 1.047 0.236 32sc_30p 32 30 0.9980 1.005 0.480 4sc_10p 4 10 0.9906 0.975 1.484 32sc_10p 32 10 0.9978 0.990 0.419
(66) The data in Table 6 and
(67) QSRC MethodEffect of T.sub.1 Differences
(68) The QSRC method utilizes the differences in the shapes of reference and mixture SRCs to quantify the components in the mixtures. Smaller differences in the T.sub.1 relaxation times of the components will lead to correspondingly smaller differences in SRCs and at the limit of equal relaxation times, the QSRC approach will fail. In order to estimate the impact of the T.sub.1 differences on the validity of the QSRC method, a model system with components possessing significantly more similar .sup.1H T.sub.1 relaxation times than the ibuprofen/indomethacin model system was analyzed. Ibuprofen and itraconazole have .sup.1H T.sub.1 relaxation times of approximately 626 ms and 720 ms, respectively (estimated from mono-exponential fits of saturation recovery data), hence the T.sub.1s only differ by about 13%. A series of seven binary blends of ibuprofen and itraconazole with varying mass percentages of ibuprofen were prepared and analyzed with the QSRC method. The blend compositions are given above in Table 2.
(69) If SRCs of two different compounds are very close, the QSRC method is still capable of differentiating these compounds; however, the number of scans per increment should be high enough, as discussed below.
(70) TABLE-US-00007 TABLE 7 .sup.1H QSRC results for the ibuprofen/itraconazole blends utilizing SRCs collected with different experimental conditions. Condition Number of Number of Exp Name scans points time R2 slope intercept 4sc_50p 4 50 0.8836 0.774 24.8 32sc_50p 32 50 0.9868 0.928 1.905 64sc_50p 64 50 0.9716 0.927 3.27 128sc_50p 128 50 0.9968 1.011 0.066 64sc_30p 64 30 0.9913 1.027 0.047
(71) When only four scans per recovery increment are collected, the QSRC analysis fails. Increasing the number of scans per increment to 32 and 64 significantly improves the accuracy of the analysis and prepared blend compositions are reproduced within approximately 5%. Finally, utilizing 128 scans per increment yields a very good correlation, comparable to the one observed for the ibuprofen/indomethacin system. The results for the ibuprofen/itraconazole model system from Table 7 show that a notably higher SNR of the SRCs is required to achieve the same accuracy in the QSRC analysis as compared to the ibuprofen/indomethacin system. This is due to the similar .sup.1H T.sub.1 relaxation times of ibuprofen and itraconazole.
(72) QSRC MethodApplication to .sup.19F SRCs
(73) In order to explore the applicability of the QSRC method to .sup.19F SRCs, two model systems containing .sup.19F were analyzed. The systems are 2-trifluoromethyl cinnamic acid/6-trifluoromethyl uracil (2TFMCA/6TFMU) and 2-trifluoromethyl cinnamic acid/fluoxetine HCl (2TFMCA/FXT). The 2TFMCA/6TFMU model system represents the situation in which the T.sub.1 relaxation times of the references differ significantly (slightly more than a factor of two). On the other hand, for the 2TFMCA/FXT model system the reference .sup.19F T.sub.1s only differ by about 12%. Several binary blends of the two .sup.19F model systems were prepared and analyzed with the QSRC method. Tables 3 and 4 list the compositions of the blends. The SRCs for the both model systems were collected with fifty logarithmically distributed recovery time points and covering a total delay range from 2-40000 ms. However, the SRCs for the 2TFMCA/6TFMU and the 2TFMCA/FXT model systems were collected with 32 and 128 scans per recovery experiment, respectively.
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(75) In general, the experiment times to collect the .sup.19F SRCs with sufficient SNR for QSRC analysis are longer than the corresponding experiment times necessary utilizing .sup.1H SRCs. The signal intensity that is acquired per scan will drop by going from observing .sup.1H to observing .sup.19F simply based on the fact that there are generally a lot fewer fluorine atoms present in a given molecule than hydrogen atoms. In fact, the .sup.19F model system compounds used in this study only contain one fluorine atom each.
(76) The QSRC analysis could be applied to nuclei other than .sup.1H and .sup.19F. For example, mineral or soil samples analysis could benefit from conducting the QSRC analysis based on .sup.13C and .sup.31P SRCs. Other NMR-active nuclei, such as .sup.35Cl, may also be used.
(77) The QSRC method described above reliably determines coefficients that represent the relative mass percentages of components in a solid mixture. The method is advantageous in various ways. Firstly, the method takes advantage of the high sensitivity of observing protons or fluorine directly. In addition, it utilizes the time-efficient way of collecting high-quality relaxation data on a low-field TD-NMR benchtop instrument. In the TD NMR approach, the collection of a complete FID and subsequent Fourier Transformation are omitted, rather only the first few points of the FID are collected and averaged to produce the intensity of a recovery point in a relaxation experiment. The resulting intensity can subsequently be used to measure NMR relaxation of the bulk of the material. The utilization of TD-NMR benchtop instruments is beneficial with respect to other aspects as well. These instruments exhibit a small footprint and can easily be placed directly on lab benchtops without any special electrical and safety requirements. TD-NMR spectrometers also do not require cryogenic cooling. This enables the use of TD-NMR instruments in very diverse laboratory environments, such as industrial production sites. Finally, the simplicity of the sample preparation for analysis in a TD NMR benchtop instrument as well as the option for automation cannot be overstated. These final benefits are especially important in high-throughput environments like the pharmaceutical industry or the production of fine chemicals.
(78) The described analysis of SRC data may be used to quantify the drug loading of a given API in a pharmaceutical formulation. A formulation is a mixture of the desired and potentially undesired API forms, along with a specific combination of pharmaceutical excipients. To obtain the drug loading, the excipients are treated as one pure component, even though more than one excipient may be present in the formulation, and the API forms (including polymorphs, solvates and hydrates of each API) are treated as the remaining components. Quantifying API forms is relevant if there are at least two forms present in the sample (e.g., various polymorphs, solvate and non-solvate, etc.). The drug-loading analysis requires the collection of one SRC of a blend of excipients with the respective concentrations as present in the actual formulation (placebo SRC). The proton number and molecular mass of the excipients is weighted according to the relative mass percentages of the excipients. The qSRC analysis can then be conducted as proposed above.
(79) An example would be a hypothetical formulation containing two excipients A and B with a relative molar ratio of the two excipients of 20% A and 80% B. Assuming further that excipient A has a molecular mass of 100 and a proton number 6, and excipient B has a molecular mass of 200 and a proton number 10, the weighted average molecular mass for the excipients would be 20+160=180, and the corresponding weighted proton number would be 1.2+8=9.2. An SRC of an excipient placebo blend of 20% A and 80% B by mole would be collected and treated in the qSRC analysis as one pure excipient component with a molecular mass of 180 and proton number 9.2. The respective qSRC fitting result would yield weighting coefficients representing the individual mass percentages for each API form (polymorph, hydrate, solvate) and for each API, but only one mass percentage for the combined excipients. The ratio of API to excipient concentrations would reveal the drug loading of the formulation.
(80) While preferred embodiments have been described above and illustrated in the accompanying drawings, it will be evident to those skilled in the art that modifications may be made without departing from this disclosure. Such modifications are considered as possible variants comprised in the scope of the disclosure.