Ryota
Nakajima
*a,
Hiromi
Sawada
b,
Shinichiro
Hayashi
b,
Akishi
Nara
b and
Mitsunari
Hattori
b
aJapan Agency for Marine-Earth Science and Technology (JAMSTEC), 2-15 Natsushima, Yokosuka, Kanagawa 237-0061, Japan. E-mail: nakajimar@jamstec.go.jp
bThermo Fisher Scientific K.K., 3-9 Moriya, Yokohama, Kanagawa 221-0022, Japan
First published on 10th February 2025
The (semi-) automation of microplastic analysis would dramatically accelerate the otherwise time-consuming and labor-intensive process, enabling more efficient identification of global microplastic distribution. Numerous methods have been proposed for the automated analysis of small microplastics (approximately less than 100 μm) on filters using micro-FTIR (Fourier Transform Infrared Spectroscopy). However, the development of automated analysis technology for relatively larger microplastics (e.g., >500 μm), which can be handled with forceps, has progressed relatively slowly. In this study, we developed a device that enables semi-automated analysis of such large microplastics. This device modifies the reflection measurement accessory of FTIR for microplastic analysis and integrates it with an image recognition camera and a motorized stage. This system allows for the final output of the number, size, and polymer type of microplastics placed on a sample plate into a Microsoft Excel file in a single procedure. The accuracy rate of identifying degraded microplastics (comprising eight types of polymers) collected from environmental sources, including the ocean, using this device was over 98% when compared to the commonly used ATR (Attenuated Total Reflection)-FTIR method. Furthermore, the time required for analysis—from the placement of the sample and size measurement to material identification—was, on average, 6.6 times faster than conventional methods. The current MARS system can reliably and automatically identify environmentally degraded microplastics with a minimum size threshold of 400 μm, and it offers significant advantages in terms of reduced data collection time and high throughput for the processing of large microplastics.
Environmental significanceMicroplastic analysis is time-consuming and labor-intensive, requiring manual handling and lengthy procedures for identifying quantity, size, and polymer types. Efficient microplastic analysis is crucial for monitoring environmental impacts, predicting trends, and evaluating mitigation measures. Microplastics pose threats to ecosystems and health, carrying toxic pollutants and disrupting organisms' biological systems. The study developed a semi-automated device using reflectance-FTIR spectroscopy integrated for large microplastics, achieving 98% accuracy and reducing analysis time by 6.6 times compared to a conventional method. This advancement addresses the inefficiencies in microplastic analysis, enabling faster and more reliable data collection critical for environmental monitoring and policy-making. |
One of the biggest obstacles in microplastic study is the effort and time required for the analysis. In case of microplastics that can be collected with standard manta/neuston nets from the surface water in aquatic environments, it is not uncommon for it to take several days to over 10 days to determine the quantity, polymer type, and size of microplastics from a single sample.6 These three items are acknowledged as essential factors to understand the fate and impact of microplastics.7 However, the effort, time, and human labor required to obtain these factors make rapid assessment of microplastics significantly challenging. In evaluating existing microplastic analysis procedures, we identified the need for a (semi-) automated instrument that allows rapid and efficient analysis of microplastics to determine their quantity, size, and polymer type.
Chemical analyses of microplastics to determine their polymer types are among the most labor-intensive and time-consuming processes. These chemical analyses include spectroscopy methods such as Fourier Transform Infrared Spectroscopy (FTIR) and Raman, as well as pyrolysis, with FTIR probably being the most widely used method.8–12 For FTIR analysis, either FTIR with a single-reflection diamond Attenuated Total Reflection (ATR) or micro-FTIR is commonly used, depending mainly on particle size.13 Generally, ATR-FTIR is employed for the analysis of microplastics that can be recognized with the naked eye and picked up with forceps or a sampling needle, with the suitable size of analyzed particles being larger than 500 μm,14–16 and the technically lowest size limit being around 100 μm.17 Micro-FTIR is generally used for smaller particles.18 In this study, we focus on larger microplastics (>500 μm–5 mm)17 that can be feasibly analyzed using ATR-FTIR.
In the ATR method, the sample particle is pressed against the prism to ensure close contact for analysis, making it well-suited for analyzing thick or irregularly shaped samples.7,19 Yet, it takes a long time to analyze a large number of particles because each microplastic-like particle must be manually placed onto the ATR prism one by one and measured.13 Since ATR analysis involves pressing the particle against the prism, it frequently destroys deteriorated microplastics due to the applied pressure. For this reason, the measurement of the size of all microplastic-like particles is carried out ‘before’ ATR analysis, resulting in measuring the size of particles that are not actually plastic, which again leads to a loss of time.
Reflectance-FTIR spectroscopy can be a solution to these problems, as it is a non-contact method that is non-destructive and allows high throughput of samples.20 Reflectance-FTIR spectroscopy is commonly used in micro-FTIR for analyzing small microplastics on a metal mesh filter, but is generally not used for larger microplastic analysis, simply because they are too big to be measured by micro-FTIR. To date, in conventional FTIR (not micro-FTIR), there has not been a device available that uses the reflectance method to measure microplastics. By combining reflectance-FTIR with a motorized stage and an image capturing camera, it would be possible to analyze the polymer types and size of a large number of microplastic-like particles in less time. In this paper, we report a new semi-automated analysis device that combines reflectance-FTIR spectroscopy with imaging capabilities for rapid measurements of larger microplastics that can be recognized with the naked eye and handled with forceps. (Semi-) automated analytical technologies of microplastic that would significantly accelerate the otherwise labor-intensive and time-consuming process have been actively developed in recent years, particularly for small microplastics (<500 μm).21–34 However, the development of (semi-) automated analytical technologies for larger microplastics has been relatively limited.35–38
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Fig. 1 Overview of the newly developed semi-automated analytical system of microplastics (Microplastic Analyzer using Reflectance-FTIR Semi-automatically, MARS). The system consists of (a) an imaging unit, (b) a measuring unit, and (c) an analysis unit. The details of each unit are described in Fig. 2–4. |
The sample plate with particles is placed on a motorized XY stage (Finesys Co., Ltd) (Fig. 2b). This motorized stage has space designed to fit the sample plate precisely. The stage can move 100 mm in both the X and Y directions, with a minimum movement of 0.001 mm and a repeat positioning accuracy of ±0.001 mm (Finesys Co., Ltd).
At the start of the measurement, the system recognizes particles on the sample plate (Fig. S1†). When the MARS system software, FT-IR scanner, is launched and “Start Measurement” is clicked, the sample plate is photographed using a coaxial epi-illumination microscope (MML06-HR65DV1-5M, Moritex Corp.) (Fig. 2a and b). The motorized stage moves the sample plate, allowing the microscope to capture images of the designated area of the sample plate. The area captured in one capture is 14 mm × 20 mm, so 15 images are required to capture the entire sample plate (3 horizontally and 5 vertically). The area to be captured on the sample plate can be changed arbitrarily. The multiple images are then automatically merged to create a single image of the designated area of the sample plate (Fig. 2c). Particles on the sample plate appear black in the images captured by the coaxial epi-illumination microscope camera, while the background appears white. Then, the images are converted to grayscale and subsequently binarized using Otsu's thresholding, allowing for particle recognition39 (Fig. 2d). Then, the contours of particles are detected using the ‘FindContours’ function from OpenCV (an open-source image processing library) and detected particles are each assigned a number (Fig. 2d). After recognizing the coordinates of all the particles on the sample plate, each particle is individually photographed by the coaxial epi-illumination microscope. In order to measure the size of detected particles, the centroid position and coordinates of the corners (short and long sides) of each particle were obtained using ‘BoxPoints’ and ‘MinAreaRect’ from OpenCV. Here the long side and the short side refer to the sides of the rotated bounding rectangle of the particle (Fig. 2e). The size measurement includes (1) the short side and long side of each particle, (2) the aspect ratio of the long side to the short side, and (3) the area of the particle.
The acquisition of infrared spectra was performed using a FTIR spectrometer with a liquid nitrogen-cooled mercury cadmium telluride (MCT) detector (Thermo Fisher Scientific, Nicolet iS10) (Fig. 3a). The wavelength range covered was 4500–650 cm−1. We modified an external reflectance accessory (Thermo Fisher Scientific, ConservatIR) compatible with the sample compartment of the Nicolet iS10 for the analysis of microplastics (Fig. 3a and b). The extended reflection optics for FTIR, which illuminates and receives the reflected spectra, is positioned directly beneath the sample plate using mirrors, enabling the measurement of particles on the plate (Fig. 3b). The extended reflection optics emits infrared light with a diameter of 1.25 mm through a mirror, and the reflected spectra from the sample and the underlying sample plate (a stainless-steel metal plate) are received by the detector.
A CCD camera integrated into the extended reflection optics provides a visible image of the illuminated area (Fig. 3b and c). An adjustment dial on the upper side of the extended reflection optics allows for the adjustment of the Z-axis, enabling the focusing of the particle image during measurement (Fig. 3b). The field of view of this CCD camera has a diameter of ca. 1 mm. In other words, to avoid capturing mixed spectra, only one particle or part of a particle should be within this 1 mm diameter range. Therefore, sample particles on the sample plate must be spaced at least 1 mm apart.
The acquisition of infrared spectra for the particles uses OMNIC, Thermo Fisher Scientific's analysis software, linked with the MARS system software, FTIR scanner. The number of scans can be adjusted in OMNIC, and 16 scans with a resolution of 4 cm−1 were performed in this study. Before performing FTIR measurements on the particles on the sample plate, a background measurement is automatically conducted. The background is obtained by measuring the infrared reflectance spectrum of a reference mirror mounted on the motorized XY stage.
For the development of this analysis unit, a new library for the identification of degraded plastics was created specifically for reflectance measurements. Details of this library are described later. This degraded plastics identification library, combined with Thermo Fisher's conventional material library, is used to identify the materials of both plastic and non-plastic particles.
When the MARS system software is launched and the analysis starts, a folder with a user-defined name is created in a designated location (Fig. 4a) that consists of the generated data including the summary Excel file (Fig. 4b), microscope images for size measurement (Fig. 4c) and CCD camera images for FTIR measurement (Fig. 4d) of each particle, and spectral files (.SPA) of each measured particle (Fig. 4e). The measurement results of all particles on a single sample plate, including size and material identification results, are output to a single Excel file (Fig. 4b).
The polymer types of all environmental microplastics were initially identified using an ATR-FTIR spectrometer (Thermo Fisher Scientific, Nicolet iS5). Samples were placed on the ATR crystal and compressed using the instrument clamp to ensure proper optical contact. During this process, minimal force was applied to avoid damaging the particles, and if significant damage occurred, the affected particles were excluded from subsequent reflectance measurements. Spectra were collected at a resolution of 4 cm−1 by averaging 16 scans per sample. Background measurements in air were taken every 60 minutes throughout the measurement process. Each obtained spectrum was then compared against several spectral database libraries, including both synthetic polymers and non-synthetic materials in OMNIC 9 software (Thermo Fisher Scientific). For subsequent analyses, 100 microplastic particles representing eight different polymer types (PE, PP, PS, PVC, EVA, PUR, PA, PET) were prepared.
Reflectance spectra for 100 particles each of the eight known polymer types were examined using the reflectance FTIR spectrometer. The spectral features of plastic particles from each polymer type were visually observed, and characteristics including (1) spectra with strong specular reflection (differentiated peak shape), (2) diffuse reflection spectra (low peak distortion, i.e., absence of specular reflection), (3) spectra with a mix of specular and diffuse reflection, and (4) highly saturated spectra (where peak shapes are nearly unobservable) were visually identified (Fig. S2†). Finally, 100 spectra for each polymer type were visually classified into one of the aforementioned patterns. From each class, 2 to 3 representative spectra were randomly selected and averaged to generate a representative spectrum for that class. The spectra were smoothed using the Savitzky–Golay filter to reduce the impact of water vapor. Next, to determine whether the representative spectra of each class were suitable for identifying the types of polymers, we conducted discriminant analysis using TQ Analyst software (Thermo Fisher Scientific). Discriminant analysis evaluates samples by calculating the distance between the class center and the sample spectra. For discriminant analysis, the spectrum was normalized using the standard normal variate (SNV) to correct the vertical axis of the spectrum. The Mahalanobis distance was used to measure the distance from the center of each class to the spectra. The Mahalanobis distance indicates how well a sample matches a given class, and a smaller value signifies a higher likelihood that the sample belongs to that class. The distance to the next class represents the discriminant measure, with a higher distance ratio indicating a clearer discrimination.
Initially, the time required for analysis using the conventional ATR-FTIR method was measured. The analysis included the following tasks: arranging sample particles, photographing and measuring sizes of particles, identifying materials with ATR-FTIR, and entering data into an Excel sheet. Each task's time was measured with a stopwatch. Arranging samples involved transferring the 25 microplastics to a numbered well plate with forceps. Photographing and measuring sizes involved capturing images of the microplastics on the well plate with a microscope (Olympus, SZX16) and a connected camera (Olympus, DP74) and measuring sizes with image analysis software (Olympus, cellSens Dimension 2.1). Material identification with ATR-FTIR involved measuring each microplastic one by one and determining their polymer types with the same setting described above. Finally, data entry involved recording the sizes and materials of the microplastics in an Excel sheet. After completing this series of tasks, the time required to measure the same 25 microplastics (four sets) using MARS was measured. This included placing the 25 microplastics on the MARS sample plate, clicking the start button, and obtaining size and material results output to an Excel sheet. The time required for the initial setup (i.e., starting up the computer and optimizing the alignment) was not considered for both ATR-FTIR and MARS. The difference in microplastic analysis time between the conventional method and the MARS method was analyzed using a t-test. A p-value of 0.05 or less was considered statistically significant.
One of the issues with measuring microplastics using the ATR method is that the microplastics are often damaged because the sample is pressed against the prism during measurement.13 After ATR measurement, the microplastics may crack or crumble into smaller pieces, making subsequent recovery difficult and limiting their further use (e.g., for weight measurement). Therefore, in this study, to overcome the issues associated with ATR, a non-contact reflection method was employed for measuring large microplastics.
In conventional FTIR, the transmission method is also known as a non-contact technique. However, in the transmission method, it is necessary for the sample thickness to be less than approximately 10 μm to allow the infrared light to pass through.8 Since it is not feasible to section microplastics, the transmission method is unsuitable for analyzing larger microplastic samples. Therefore, we consider that the use of the reflection method is suitable for the rapid and non-destructive measurement of large microplastics. Although a reflection measurement method using standard FTIR has existed, to the best of our knowledge, it had never been used for the analysis of larger microplastics. Although Thermo Fisher Scientific had developed an external reflection measurement accessory, ConservatIR, that could be attached to a conventional FTIR spectrometer, it was only capable of measuring objects positioned laterally (at 90° relative to gravity) or upwards (at 180° relative to gravity) from the FTIR. Therefore, we modified the reflection detector to face downward and enhanced it with a mirror to focus on and measure small objectives.
In contrast, the corresponding reflectance FTIR spectra displayed highly variable baselines due to distorted band shapes. These distortions are believed to be caused by the thickness and shape of the sample particles, which are thought to result in phenomena such as reflections from the sample surface (anomalous dispersion of the refractive index), absorption within the sample, and diffuse reflection.20
Despite these limitations, the reflectance FTIR spectra still contained the necessary chemical information for polymer identification. The comparison of reflectance and ATR-FTIR spectra identified the general regions of interest for polymer absorption bands, including the CH stretching region (3000–2800 cm−1), the CH bending region (1470–1365 cm−1), the carbonyl stretching region (1820–1680 cm−1), and the NH stretching region of PA (3500–3300 cm−1).20,46 Particularly, the range in the near-infrared region around 4400–4100 cm−1, which includes a combination of CH stretching and CH bending vibration and where spectral saturation and specular reflection are minimal, resulted in the large Mahalanobis distance ratio between the designated class and the nearest class (Table 1).
Actual class | Calculated class | Distance | Next class | Next distance | Mahalanobis ratio |
---|---|---|---|---|---|
PE-1 | PE | 1.0 | EVA | 1.78 | 1.7 |
PE-2 | PE | 0.4 | EVA | 2.33 | 5.9 |
PE-3 | PE | 0.5 | EVA | 2.1 | 4.7 |
PE-4 | PE | 0.6 | EVA | 2.1 | 3.4 |
EVA-1 | EVA | 0.5 | PE | 1.8 | 3.6 |
EVA-2 | EVA | 1.0 | PE | 2.3 | 2.3 |
EVA-3 | EVA | 1.0 | PA | 2.4 | 2.4 |
EVA-4 | EVA | 0.7 | PE | 1.4 | 1.9 |
PP-1 | PP | 0.6 | PVC | 3.6 | 5.6 |
PP-2 | PP | 0.8 | PVC | 3.3 | 4.4 |
PP-3 | PP | 1.0 | PVC | 3.7 | 3.6 |
PP-4 | PP | 1.0 | PVC | 4.1 | 4.1 |
PVC-1 | PVC | 0.9 | EVA | 3.2 | 3.4 |
PVC-2 | PVC | 1.0 | EVA | 3.9 | 3.8 |
PVC-3 | PVC | 1.0 | EVA | 4.1 | 4.3 |
PUR-1 | PUR | 0.9 | PS | 3.5 | 3.9 |
PUR-2 | PUR | 0.9 | PS | 3.3 | 3.7 |
PA-1 | PA | 1.0 | EVA | 3.5 | 3.4 |
PA-2 | PA | 1.0 | EVA | 2.7 | 2.7 |
PA-3 | PA | 1.0 | EVA | 3.2 | 3.2 |
PS-1 | PS | 0.1 | PUR | 3.2 | 36.0 |
PS-2 | PS | 0.1 | PUR | 3.3 | 36.3 |
PET-1 | PET | 0.6 | PP | 4.2 | 7.1 |
PET-2 | PET | 0.6 | PS | 4.2 | 7.2 |
The results of the discriminant analysis indicated that all eight polymer types were classified into their respective classes (Table 1). The distances were relatively large, demonstrating the ability to distinguish specific types of polymers. The number of target spectra and the number of successfully identified spectra for each type of polymer are listed in Table 2. The results of the library search indicated that more than 98% of the spectra were recognized as the same polymer types identified with ATR-FTIR. These findings suggest that, although the reflectance FTIR spectra may appear complex, they are capable of extracting sufficient chemical information to enable the identification of polymers even in degraded plastics collected from the environment, using multivariate statistics.
Polymer type | Number of target spectra | Success rate (%) |
---|---|---|
PE | 100 | 97 |
PP | 100 | 97 |
PS | 100 | 98 |
PET | 100 | 100 |
PVC | 100 | 95 |
PUR | 100 | 100 |
EVA | 100 | 100 |
PA | 100 | 100 |
Overall | 98.4 ± 1.9 |
Particle no. | 100 μm | 200 μm | 300 μm | 400 μm | 500 μm | |||||
---|---|---|---|---|---|---|---|---|---|---|
Diameter (μm) | Identified material | Diameter (μm) | Identified material | Diameter (μm) | Identified material | Diameter (μm) | Identified material | Diameter (μm) | Identified material | |
1 | 94.5 | Acrylic resin | 250 | Acrylic resin | 303 | PE | 375.5 | PE | 498 | PE |
2 | 103.5 | Acrylic resin | 241 | Acrylic resin | 385 | PE | 399.5 | PE | 480 | PE |
3 | 97 | Acrylic resin | 264 | Acrylic resin | 331 | Acrylic resin | 382 | PE | 566.5 | PE |
4 | 117.5 | Acrylic resin | 180 | Acrylic resin | 264 | Acrylic resin | 398 | PE | 505 | PE |
5 | 96.5 | Acrylic resin | 193.5 | Acrylic resin | 305.5 | PE | 466 | PE | 478.5 | PE |
6 | 101.5 | Acrylic resin | 211 | Acrylic resin | 305.5 | Acrylic resin | 395.5 | PE | 636.5 | PE |
7 | 138.5 | Acrylic resin | 197.5 | Acrylic resin | 357.5 | PE | 459 | PE | 597 | PE |
8 | 83 | Acrylic resin | 236.5 | Acrylic resin | 347.5 | PE | 424.5 | PE | 513 | PE |
9 | 93.5 | Acrylic resin | 201.5 | Acrylic resin | 271.5 | PE | 408.5 | PE | 687 | PE |
10 | 120.5 | Acrylic resin | 219 | Acrylic resin | 283 | PE | 405 | PE | 588 | PE |
11 | 174.5 | Acrylic resin | 218 | PE | 304 | PE | 363 | PE | 579 | PE |
12 | 113 | Acrylic resin | 211.5 | Acrylic resin | 332 | PE | 426.5 | PE | 461 | PE |
13 | 100 | Acrylic resin | 248 | Acrylic resin | 255 | Acrylic resin | 439 | PE | 579.5 | PE |
14 | 109.5 | Acrylic resin | 208 | Acrylic resin | 310.5 | PE | 500.5 | PE | 579 | PE |
15 | 106 | Acrylic resin | 248.5 | Acrylic resin | 315 | PE | 400.5 | PE | 639 | PE |
16 | 88 | Acrylic resin | 264 | Acrylic resin | 298 | PE | 404 | PE | 497 | PE |
17 | 111 | Acrylic resin | 221.5 | Acrylic resin | 307.5 | PE | 531 | PE | 543.5 | PE |
18 | 98 | Acrylic resin | 271.5 | PE | 287.5 | Acrylic resin | 444 | PE | 540 | PE |
19 | 122.5 | Acrylic resin | 208 | Acrylic resin | 333.5 | PE | 424.5 | PE | 560.5 | PE |
20 | 82 | Acrylic resin | 280 | PE | 319 | PE | 367 | PE | 670.5 | PE |
21 | 82 | Acrylic resin | 246.5 | Acrylic resin | 266.5 | PE | 514 | PE | 482 | PE |
22 | 103.5 | Acrylic resin | 247 | Acrylic resin | 295.5 | Acrylic resin | 467.5 | PE | 694 | PE |
23 | 139.5 | Acrylic resin | 336 | PE | 380.5 | PE | 498 | PE | 558.5 | PE |
24 | 128 | Acrylic resin | 303 | Acrylic resin | 308 | PE | 650 | PE | 748 | PE |
25 | 86 | Acrylic resin | 173.5 | Acrylic resin | 388 | PE | 443 | PE | 516 | PE |
107.6 ± 21.4 | 0% | 235.2 ± 38.3 | 16% | 314.2 ± 36.4 | 76% | 439.4 ± 63.4 | 100% | 567.9 ± 76.4 | 100% |
The decrease in accuracy for smaller particles may be attributed to multiple factors related to the physical properties of the particles and the limitations of the MARS detection system. As particle size decreases, the surface area-to-volume ratio increases, which amplifies the effects of surface phenomena such as distortion and diffuse reflection. Smaller particles, due to their increased curvature and surface irregularities, tend to scatter light more diffusely. This diffuse scattering reduces the intensity of the reflected spectral data and alters its path, potentially making it difficult for the detector to capture sufficient and accurate signals required for material identification. It is also possible that, for particles <400 μm, spectral information from optical systems other than the resin is being reflected, which may lead to a decrease in library search accuracy. To address these challenges, further technological advancements in the MARS system should be considered. For instance, the use of a Cassegrain mirror to focus infrared light specifically on the target area at high magnification could enhance detector sensitivity. Such improvements could play a pivotal role in improving the system's ability to accurately identify smaller particles.
Even for the experienced technician, analyzing 25 particles using the conventional method took 108 min, meaning that analyzing 1000 particles would take 72 h—a task that would require nine days at eight hours of work per day. In contrast, using MARS, analyzing 1000 particles would take only 14.9 h. Although it is currently physically impossible to place 1000 particles on a single sample plate, even if the sample is divided and measured multiple times, the task could still be completed within two 8 hours workdays. This substantial reduction in microplastic analysis time suggests that the utilization of MARS will enable the analysis of larger quantities of samples within a limited timeframe.
Furthermore, while the experienced technician completed the analysis significantly faster than the novice technician using conventional methods (p < 0.0001), no significant difference was observed between experienced and novice technicians when using MARS (p = 0.310). This indicates that, unlike conventional methods where experienced technicians are naturally faster, MARS requires minimal manual intervention beyond placing the sample particles on the sample plate. Once the particles are on the plate, the system automatically determines the size and material, and then outputs an Excel sheet that summarizes the data, eliminating the speed differential due to technician experience. This means that anyone, regardless of their level of experience, can obtain results at the same speed using MARS.
In conventional ATR-FTIR methods, the standard approach is to analyze all particles that resemble microplastics. However, there is a possibility that microplastic particles that do not visually appear as microplastics may have been overlooked, which may introduce investigator bias. In contrast, MARS allows for the simultaneous placement and analysis of both microplastic-like particles and visually non-microplastic particles on the sample plate and completes the analysis within a short time. Therefore, investigator bias is expected to be reduced compared to conventional methods.
Additionally, the current model of MARS relies on a relatively small spectral library encompassing only eight polymer types, which limits its accuracy in identifying less common polymers or emerging synthetic materials. To enable broader applications and improve its utility, continuous updates and expansion of the spectral library will be essential. These developments will ensure the system remains adaptable to the growing diversity of polymers encountered in environmental samples.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4va00400k |
This journal is © The Royal Society of Chemistry 2025 |