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Article

Iron Oxide and Hydroxide Speciation in Emissions of Brake Wear Particles from Different Friction Materials Using an X-ray Absorption Fine Structure

by
Hiroyuki Hagino
1,*,
Ayumi Iwata
2,3 and
Tomoaki Okuda
2
1
Japan Automobile Research Institute (JARI), 2530 Karima, Tsukuba 305-0822, Ibaraki, Japan
2
Faculty of Science and Technology, Keio University, 3-14-1, Hiyoshi, Yokohama 223-8522, Kanagawa, Japan
3
Meteorological Research Institute Japan Meteorological Agency, 1-1 Nagamine, Tsukuba 305-0052, Ibaraki, Japan
*
Author to whom correspondence should be addressed.
Atmosphere 2024, 15(1), 49; https://doi.org/10.3390/atmos15010049
Submission received: 8 December 2023 / Revised: 27 December 2023 / Accepted: 27 December 2023 / Published: 30 December 2023
(This article belongs to the Special Issue Study of Brake Wear Particle Emission)
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Abstract

:
Iron (Fe), the main component of non-exhaust particulates, is known to have variable health effects that depend on the chemical species of iron. This study characterized the possible contribution of iron oxides and hydroxides to airborne brake wear particles under realistic vehicle driving and braking conditions with different brake pad friction materials. We found significant differences in wear factors and PM10 and PM2.5 emissions between non-asbestos organic (NAO) and European performance (ECE) brake pads. Iron was the dominant contributor to PM10 and PM2.5 brake wear particles for both NAO and ECE. The iron concentration ratio in the particle mass (PM) was comparable to the disc-to-pads ratio measured by wear mass. The fact that magnetite, which is of interest with respect to health effects, was less abundant in NAO than in ECE suggested that tribo-oxidations occurred in NAO. Metallic iron is generated not only from abrasive wear but also from tribo-chemical reduction with magnetite as the starting material. We found that there were differences in PM emissions between brake friction materials, and that the phase transformations of iron differed between friction materials. These differences were apparent in the distribution of iron oxides and hydroxides. Heat, tribo-oxidation, and tribo-reduction are intricately involved in these reactions.

1. Introduction

Exposure of humans to particulate matter due to air pollution is associated with a range of respiratory, cardiovascular, and neurological problems that are known to cause increased morbidity and mortality worldwide [1]. Particulate matter is known to be a complex mixture of organic and inorganic components emitted from a variety of primary sources and subject to various types and degrees of secondary reprocessing and environmental weathering. Exhaust particles consisting of carbonaceous compounds are a major source of air pollution from particulate matter in urban areas, but as emission controls reduce combustion-derived exhaust particles [2], the proportion of non-exhaust particles in particulate matter likely to be inhaled by humans in urban areas and near road traffic will increase. The most abundant element in non-exhaust particulates is generally known to be iron (Fe). Its presence in wear products from vehicle braking systems and in engine emissions from combustion and/or wear suggests that urban traffic is an important source of Fe in particulate matter in urban areas [3]. Identification of the source of Fe in urban areas has revealed that the wear of Fe on brake pads containing steel fibers or Fe powder and grey cast iron discs are sources of metallic Fe (Fe (0)) [4,5,6,7,8]. Magnetite (Fe3O4, Fe (II, III)) nanoparticles with a particle size of less than 100 nm are thought to be introduced into urban air from vehicle exhaust emissions, engine wear, and braking system wear [4,6,7]. The oxides and hydroxides of Fe (e.g., metallic iron (α-Fe, Fe (0)); divalent iron (Fe (II)); and trivalent iron (Fe (III)) may play an important role in the development of neurodegeneration and Alzheimer’s disease, e.g., [9]. It is therefore important to be able to distinguish iron oxides and hydroxides in order to identify the contribution of sources of non-exhaust particles in urban areas by iron speciation, as well as the potential impact of iron particles on human health.
Braking systems for motor vehicles are known to be an important source of iron in non-exhaust particulates in urban areas, and they vary according to the type of vehicle as well as national and regional markets. Brake pads in the basic brake system of a modern car are available in a wide range of compositions of friction material, which includes the gray cast iron brake disc. The two most important categories are low-steel (low metallic) pads (also called European performance “ECE”), developed and produced primarily for the European market, and non-asbestos organic (NAO) pads, designed primarily for the North American and Asian markets [10]. These two types of pads can be distinguished, inter alia, by the percentage of metal components in them. Low-steel (low-metallic) pads contain a significant percentage of iron, whereas NAO pads are usually iron-free.
Brake disc and pad wear products include brake wear particles and the subsequent formation of friction layers. Brake wear particles and gases are released from surfaces of pads and discs [4]. The brake wear particles adhere to the friction surface of the brake pad and form a friction layer. This layer is critical to the ability of each brake pad to function as a source of friction. Iron oxide has proven to be the main component of the friction layer [11]. For example, dynamometer tests have been performed with ECE brake materials at different temperatures from 25 to 700 °C. At temperatures above 400 °C, the formation of magnetite (Fe3O4, Fe (II, III)) and maghemite (γ-Fe2O3, Fe (III)) has been detected, and above 600 °C, the formation of hematite (α-Fe2O3, Fe (III)) has been detected. Lepidocrocite (γ-Fe(O)OH, Fe (II)) formation has been detected only at 400 °C [12]. In contrast, pin-on-disc tests of NAO brake materials with maximum contact temperatures below 50 °C have been performed, and magnetite (Fe3O4, Fe (II, III)), a product of tribo-oxidation of cast iron discs, has been reported to be the principal mineral formed on the friction layer [13]. Because different magnetite (Fe3O4, Fe (II, III)) formation temperatures have been reported, the friction phenomena are complex, and the mechanism of formation of the friction layer is not yet fully understood, even though the wear particle structures present on the brake pad surface are very important in terms of brake wear particle emissions [4]. There is very limited knowledge of iron speciation of airborne brake wear particles from various brake friction materials of relevance to air quality and human health. Tests have been conducted under braking conditions, such as the Worldwide-harmonized Light Vehicle Test Procedure (WLTP) brake cycle [14].
The goal of this study was therefore to characterize the possible contribution of iron oxides and hydroxides to airborne brake wear particles under realistic vehicle driving and braking conditions with different friction materials. Chemical forms of iron were identified using the X-ray absorption fine structure (XAFS) method [15,16] in order to allow bulk measurements in any solid or liquid state, regardless of the sample phase, to avoid the influence of iron magnetism [7] and to reduce the cumbersome analytical operations that contribute to measurement errors.

2. Materials and Methods

2.1. Brake Dynamometer Test and Airborne Brake Wear Particle Measurement

Brake wear particles were measured and collected in accordance with a previous study [17] and the JASO C 470 test protocol [18]. A single passenger car front brake wheel was used for driving and brake control in accord with the WLTP brake driving profile [14] using an electric inertia dynamometer. The test brake assembly was a commercially available genuine brake assembly; it consisted of a cast iron ventilated disc, floating caliper, and brake pads made of NAO material or ECE materials, and the elements it contained were measured by wavelength-dispersive X-ray fluorescence analysis (ZSX Primus II, Rigaku, Corp.,Tokyo, Japan). Disc temperature was measured by locating a thermocouple 10 mm radially outward from the center of the friction pad and disc at a depth of 1.0 ± 0.1 mm from the disc surface.
Two pad types were tested with individual conventional gray cast iron brake discs of the same type. The NAO and ECE tests were conducted on cast iron discs of each material, and the WLTP brake cycle was repeated three times after bedding in accord with the JASO C470 test protocol [18]. The test vehicle mass was 1240 kg, and the brake force front/rear distribution was 80%, with a tire dynamic load radius of 298 mm, an inertia of 38.3 kg-m2, and a nominal front wheel load-to-disc mass (WLn-f/DM) ratio [19] of 79.6. Because the Global Technical Regulation (GTR24) test method was not defined at the time of this experiment [19], the sampling of brake wear particles was based on the JASO C 470 test method, which consists of an enclosure with the brake assembly inserted downstream of the air supplied through an HEPA filter, and a constant flow sampling tunnel (1 m3/min, 20 °C standard) [18].
Different test operating conditions (e.g., temperature, cooling profile, velocity profile, energy index, and time at the tribological interface) can dramatically alter the distribution of chemical species and the oxidation state in the metal. It is important to provide the reader with such comparisons because they highlight the differences in operating conditions that must be considered when comparing similar results to those obtained under the future UN GTR24 [19]. However, the results of this study are not strictly comparable with those of the GTR24 because of the control of the brake temperature by cooling air, the measurement of the disc temperature at a depth of 1 mm, and the lack of strict feedback control of the speed and braking torque (Nm) in the experiments carried out in this study.
During the emissions tests, the number of speeding violations ranged from 36 to 42 for NAO and 41 to 45 for ECE. The fact that they did not exceed 475 for the full WLTP brake cycle meant they were within the tolerance. For the purposes of the Kinetic Energy Dissipation Quality Test, the total nominal specific brake friction work of the braking event is defined as Trip #10 of the WLTP brake cycle (5555 ± 278 J/kg) over the entire WLTP brake cycle (15,983 ± 799 J/kg). In this study, the total value of brake friction work was 4675 ± 624 J/kg at Trip #10 and 16,034 ± 1788 J/kg over the entire WLTP brake cycle for NAO, and 4563 ± 193 J/kg at Trip #10 and 13,853 ± 387 J/kg over the entire WLTP brake cycle for ECE. The reason that these did not satisfy the tolerance was that the dynamometer at the time of the tests did not have strict feedback control of the braking torque. For the brake temperature tolerances, the mean disc temperature, the initial brake temperature (IBT), and the final brake temperature (FBT) for trip#10 were 64 ± 6 °C, 64 ± 5 °C, and 89 ± 6 °C, respectively, for NAO, and 68 ± 3 °C, 61 ± 3 °C, and 94 ± 3 °C, respectively, for ECE. The IBT and FBT were both lower than the brake temperature tolerance of the UN GTR24 [19].
Sampling of PM10 and PM2.5 was carried out with a low-pressure impactor (LPI) (LP-20, Tokyo Dylec Corp., Tokyo, Japan) according to the methods previously reported [17] on a Teflon filter (Filter A: Fluoropore FP-500-100, 47 φ for PM10 and PM2.5, 80 φ for LPI, Sumitomo Electric Fine Polymer Corp., Osaka, Japan; Filter B: Teflo, 47 φ for PM10 and PM2.5, Pall Corp., New York, USA) or a quartz filter (Pallflex, 2500QAT-UP, 47 φ for PM10 and PM2.5, Pall Corp., New York, USA) by aspirating from a sampling nozzle equipped with isokinetic sampling nozzles. Filter masses before and after the test were weighed on an electronic balance to determine the emissions of PM10 and PM2.5. A cyclone particle collector (a sanitary stainless steel cyclone with an electropolished interior, Clean Valve Co. Ltd., Okayama, Japan) was installed at the end of the constant flow sampling tunnel to collect PM10 powdered brake wear particles. The diameters of the particles collected by the cyclone were at least 100 nm, which is the same geometry used in previous studies with a PM10 impactor (HV-1000-PM10, Shibata Scientific Technology Ltd., Tokyo, Japan) attached to the cyclone inlet [20,21]. The cyclone sampling method for particulate matter in this study has also been suggested as a method that can be used to assess health effects, e.g., [22] because it is a technique that collects particles in the air as a powder. Organic and elemental carbon (OC, EC) collected on the quartz filters were measured by a thermal–optical carbon analyzer (model 2001, Desert Research Institute) using the IMPROVE protocol [23]. Total metals, including water-soluble and insoluble fractions, were measured via energy-dispersive X-ray fluorescence (XRF) (Epsilon 5, Malvern PANalytical, Malvern, UK) [24].

2.2. X-ray Absorption Fine Structure Analysis

To identify the iron speciation in the brake wear particles and to quantify their contribution, we mainly used the X-ray absorption near edge structure (XANES) to study the valence state of absorbed atoms measured at the Kyushu Synchrotron Radiation Research Center (SAGA-LS) using beamlines 11 and 15 [15,16]. We ensured the quality of the continuous spectra through XAFS measurements using synchrotron radiation [16]. The analytical method is described in brief here.
Speciation of each metal compound was performed by a linear combination fitting method using metal reference compounds (Fe, FeO, Fe3O4, Fe2O3(α,γ) and Fe(O)OH). Each reference compound was mixed well with boron nitride in a mortar for 20 min, and then pressed into pellets similar to the aerosol samples. A total of six PM10 powder samples (NAO and ECE) and four PM2.5 filter samples were subjected to XAFS separation of the chemical forms of iron. XAFS spectra were measured in transmission geometry in the energy region 6781–7858 eV near the Fe K-edge for each of the six standard and all of the analyzed samples (I0, He 50%: N2 50%; I1, N2 85%: Ar 15%). The measurement parameters were set to 0.36 eV/step (1 s/step) only in the XANES region from 7081 to 7172 eV for all samples, and to 1.91 to 9.90 eV/step (1 s/step) for the remaining regions (12.6 min in total). We weighed the two PM10 powder samples and the Fe(O)OH reference sample to be analyzed, other than the SAGA-LS–owned reference sample, and each powder was mixed using a pestle and mortar for 20 min, after which time the powder was pressed at 50 kN into a pellet mold 13 mm in diameter and placed in plastic bags for measurement. Four filter samples were also placed in a plastic bag and measured in the same way.
For the XAFS spectrum analysis, normalization of the experimental data and the linear fitting calculation using the least-squares method for valence ratio were performed using Athena software (ver. 0.9.26) [25]. The detailed procedures have been described in a previous study [15,16]. The R factors, which are generally used for the evaluation of fitting results, fell in the range of 0.002–0.06 for iron speciation in the linear combination fitting analysis.

3. Results and Discussion

3.1. Characterization of Brake Wear Particles

3.1.1. Brake Pad and Disc Wear

The amounts of disc and brake pad wear (i.e., mass loss [19,26]) can provide information that facilitates evaluation of the reasonableness of the particulate matter measurements in this study, compared to previous studies that measured brake wear particles. Such measurements are known to be highly variable. For the measurements of mass loss [26] in this study, the WLTP brake cycle was repeated three times after bedding to allow sufficiently accurate measurement of the wear mass, and the mass difference between the pad and disc before and after the test was measured. The mass loss of the NAO pads was 0.92 g for the pads (inner), 0.65 g for the pads (outer), and 0.75 g for the discs, for a total of 2.32 g. Brake wear particles are known to result from wear of discs as well as brake pads. Disc wear accounted for 32% of the total wear. Mass loss as a wear factor was determined by dividing the total mass loss of the friction partner (mg) by the total test distance (km) of the three tests. Mass loss was 4.02 mg/km per brake for the NAO pads in Figure 1. Mass loss for the ECE pads was 1.31 g for the pads (inner), 0.87 g for the pads (outer), and 3.19 g for the discs, for a total of 5.37 g. Disc wear accounted for 59% of the total wear. Mass loss as a wear factor was 9.31 mg/km per brake with ECE pads (Figure 1). A comparison of these results to the benchmarks of a previous interlaboratory study (ILS) [8] revealed that higher emissions were observed in that study than in this study (6.5 mg/km per brake with NAO pads and 21 mg/km per brake with ECE pads) [26,27]. NAO was developed to optimize comfort (reduction of noise and rim contamination), and this study (Figure 1) as well as previous studies have shown higher emissions with ECE than with NAO [26]. However, this comparison is based on different brake assemblies and masses of test vehicles, and in this study, we found higher wear factors with ECE in only some pairings of NAOs and ECEs with discs. Further systematic studies will be needed to clarify whether there are significant differences in wear factors between NAO and ECE pads.

3.1.2. Brake Wear Particle Emissions

Emissions of brake wear particles (average of n = 3) were 1.43 ± 0.29 (3.73 ± 0.19) mg/km per brake for PM10 and 0.59 ± 0.08 (1.31 ± 0.08) mg/km per brake for PM2.5 with NAO (ECE). The PM10-to-mass loss ratio [26] was 35% for the NAO pairing and 40% for the ECE pairing. In contrast to this result, a comparison of the results of previous studies by the authors, both using the same friction material (PV565 unique identification code based on brake friction registration by the National Sanitation Foundation), showed that the PM10-to-mass loss ratio of Vehicle II in the literature [17] was 29%, comparable to the ratio of 35% for the NAO pairing of this study, although the test vehicle (mass 1240 kg, tire dynamic rolling radius 298 mm, 80% front–rear brake distribution), braking system, and driving conditions (JC08) were very different [17]. However, these results showed a slightly lower detection than those of the interlaboratory study [26], which reported the average PM10-to-mass loss ratio for disc brake systems to be 35–49%. The fact that the average PM10-to-mass loss ratio for disc brake systems in the interlaboratory study [26] fell in the range 35–49% suggested that the brake systems used in this study lost weight for other reasons, such as adhesion to the calipers or scrub remaining on the pad surface during adhesive wear. It is therefore reasonable to assume that the PM10-to-mass loss ratio was not 100%, and that the ratio varied as a function of the friction material, disc material and structure, and caliper structure.
In this study, we measured the emissions of brake wear particle masses according to their aerodynamic particle diameters measured with an LPI. Figure 2 shows the results. Generally, the height of each particle size interval is affected by the width of that interval. The result is a distortion of the shape of the fraction. We therefore used a histogram for the vertical axis, in which the particle mass of each fraction was divided by the width of that fraction (dM/dlogDp), and the particle size distribution was normalized by the particle size intervals [28]. However, because in this study the height of each particle size fraction was expressed as the emission factor of the particle mass measured in each fraction, the vertical axis of the graph was used as dM. The emissions were distributed in a mode diameter range of 1–5 μm throughout the WLTP brake cycle. The ratio of emissions of nanoparticles (PM0.12 based on LPI specifications) to PM11 was 0.05% (0.0006 mg/km) for NAO and 0.06% (0.0015 mg/km) for ECE. For the brakes investigated in this study, the contributions of nanoparticles to the overall PM emissions were small. The implication is that even cyclones with low collection efficiencies for particles smaller than 0.1 nm generally collected all of the PM10 in this study.

3.1.3. Chemical Characterization

The brake wear particle emissions test required in GTR24 addresses only physical quantities such as particle mass (PM10 and PM2.5) and number of particles (total particle numbers and solid particle numbers) [19]. The composition of brake wear particles can provide important information on air quality implications, mechanisms of toxicity, and mechanisms of brake wear. Figure 3a–f show the elemental contents of the pad friction surface, PM10, and PM2.5 in NAO and ECE. Because the aim of this study was Fe speciation, this discussion will focus on Fe in Figure 3a–f. Each of the NAO and ECE brake pads contained some iron (Figure 3a,d, respectively). Although NAOs are typically iron-free [10], they may contain iron as a lubricant (as iron sulfide) and/or as an abrasive (iron oxide, chromium oxide) [e.g, 5]. The NAO used in this study contained less iron than the ECE, because this NAO was developed and produced for both the European and Asian markets. There are various types of NAOs, and the brake pads used in this study were NAOs according to the manufacturer. The contribution of Fe tends to increase from the pad (Figure 3a,d) to brake wear particles (Figure 3b,c,e,f), and it is most abundant in PM10 and PM2.5 for both NAO and ECE. The friction material counterpart, the cast iron disc, is composed mainly of iron and tiny amounts of additive metals. When the disc was ground by the pad, wear particles that contributed to the brake wear particles (PM10 and PM2.5) were emitted. These results supported the findings of previous studies [17,29].
The PM originating from disc wear (PMdisc) and pad wear (PMpad) can be distinguished from the PMx, where x equals 2.5 or 10, by solving the following simultaneous Equations (1) and (2), which express the PM and Fe mass balance:
PMdisc + PMpad = PMx,
[Fe]disc × PMdisc + [Fe]pad × PMpad = [Fe]PMx × PMx.
Here,
PMx is the PM10 or PM2.5 emissions,
[Fe]disc is the Fe mass concentration (%) in the disc fixed at 100%, and
[Fe]pad is the Fe mass concentration (%) in the pad.
The result for [Fe]pad was 5.8% and 8.3% for NAO and ECE, respectively. By solving Equations (1) and (2), we determined the contribution of the disc to the PMx (Fdisc [%]) from Equation (3):
Fdisc = PMdisc/PMx × 100 = ([Fe]PMx − [Fe]pad)/([Fe]disc − [Fe]pad) × 100.
A limitation of the analysis using Equations (1)–(3) should be mentioned. The Fe contained in NAO and ECE may be transferred to a disc, but there has been no study of whether it can be transferred to materials other than cast iron discs. Further large-scale investigations with many types of pads and discs of different materials would be required to address this question.
From the elemental analysis of collected PM10 and PM2.5, we determined the Fe content of PMx in the NAO (ECE) to be 26.1% (59.0%) for PM10 and 27.8% (58.9%) for PM2.5. We could therefore estimate the mass fraction of PMx originating from the disc (F disc = PMdisc/PMx) (%) to be 22% (55%) in the NAO (ECE) for PM10 and 23% (55%) in the NAO (ECE) for PM2.5. The percentages contributed by the disc to PM10 and PM2.5 were generally consistent with and not contradictory to the results of the elemental analysis. The disc wear rates measured from mass loss in this study accounted for 32% of total wear for the NAO pairing and 59% for the ECE pairing, respectively. Although not all of the disc wear particles and debris deposited on the ground are emitted as PM10 or PM2.5, the Fe concentrations in the PM measured in this study suggested that the iron concentration ratios for particle mass were comparable to the disc-to-pads ratio measured by wear mass.

3.2. Iron Speciation

3.2.1. XAFS Spectra for Reference Materials

For quantitative speciation of iron oxides and hydroxides, XAFS spectra were measured for a total of six chemical species: metallic Fe (α-Fe, Fe (0)) as the reference material for iron; two Fe(III) iron oxides with different crystal structures: hematite (α-Fe2O3, Fe (III)) and maghemite (γ-Fe2O3, Fe (III)); the iron oxide magnetite (Fe3O4, Fe (II, III)) with co-existing divalent and trivalent iron oxides; the divalent iron oxide wüstite (FeO, Fe (II)); and the trivalent iron hydroxide goethite (α-Fe(O)OH, Fe (III)). The results are shown in Figure 4a–d.
The position of the absorption edge with the largest peak differed for each chemical species, but peaks were obtained in approximately the same energy region for the three species of metallic Fe (α-Fe, Fe (0)), magnetite (Fe3O4, Fe (II, III)), and goethite (α-Fe(O)OH, Fe (III)). The absorption edges of hematite (α-Fe2O3, Fe (III)) and maghemite (γ-Fe2O3, Fe (III)) were also detected at similar positions for the iron oxide species hematite (α-Fe2O3, Fe (III)) and maghemite (γ-Fe2O3, Fe (III)), but the highest peaks were shifted by about 1 eV. The fact that the spectrum of hematite (α-Fe2O3, Fe (III)) had a unique peak at about 7125–7130 eV suggested that the crystal structure could be distinguished. The same trivalent iron was also used as the crystal structure of hematite (α-Fe2O3, Fe (III)). The positions of the peaks differed between hematite (α-Fe2O3, Fe (III)) and goethite (α-Fe(O)OH, Fe (III)), even if they contained the same trivalent iron. It is therefore possible to distinguish chemical species with the same valence but different chemical states using this method. The clear differences between the XAFS spectra of each chemical species indicated that the present method was effective for identification of iron chemical species.

3.2.2. XAFS Spectra for Brake Wear Particles

Figure 4b shows the XAFS spectra of PM10 powder samples of NAO and ECE brake wear particles. The fact that the shapes of the XAFS spectra of NAO and ECE were very different implied that the amounts of Fe in the two brake friction materials differed. Figure 4c,d show the XAFS spectra of the PM10 powder and PM2.5 filter samples of NAO and of ECE, respectively. The ECE PM10 powder and filter samples yielded similar spectra that largely overlapped, whereas the NAO PM10 powder and filter samples yielded spectra with slightly different shapes. These results suggested that the separation of the chemical form of iron in brake wear particles was not affected by the collection method, the analytical form of the sample (powder and filter samples), or the particle size (PM10, PM2.5).

3.2.3. Iron Speciation

One goal of this research was to characterize and quantify the possible contributions of iron oxides and hydroxides to airborne brake wear particles under realistic vehicle driving and braking conditions with different friction materials. A number of hetero-iron compounds other than iron oxides and hydroxides have been detected in brake wear particles [11,12,13]. This study focused exclusively on iron oxides and hydroxides, which have been detected in atmospheric observations [3,6] and discussed in terms of health effects, e.g., [9]. The iron oxides and hydroxides discussed in this study may therefore be an overestimation.
Figure 5 shows the results of our quantitative evaluation of the phase composition of brake wear particles from emission measurements made on NAO and ECE.
When we compared NAO (Figure 5a–c) and ECE (Figure 5d–f), we observed a higher proportion of the Fe (III) iron oxide Fe2O3 (sum of hematite (α-Fe2O3, Fe (III)), maghemite (γ-Fe2O3, Fe (III))), and goethite (α-Fe(O)OH, Fe (III)) in NAO. Conversely, we observed a higher proportion of zero-valence metallic Fe (α-Fe, Fe (0)), divalent iron oxide wüstite (FeO, Fe (II)), and mixed divalent and trivalent iron oxide magnetite (Fe3O4, Fe (II, III)) in ECE. A comparison of the PM2.5 filter samples obtained from the same brake as the NAO showed a common trend in that Fe2O3 (sum of hematite (α-Fe2O3, Fe (III)) and maghemite (γ-Fe2O3, Fe (III))) accounted for about 45% in both cases. The remaining chemical species were present in the 10% range on average, although there were some differences. In the PM10 sample of NAO, the proportions of metallic Fe (α-Fe, Fe (0)), wüstite (FeO, Fe (II)), Fe2O3 (sum of hematite (α-Fe2O3, Fe (III)), and maghemite (γ-Fe2O3, Fe (III))) were similar, whereas magnetite (Fe3O4, Fe (II, III)) was less abundant, and goethite (α-Fe(O)OH, Fe (III)) was detected more frequently. We thus observed that in the particles generated from this type of brake, there was a tendency for a large amount of magnetite (Fe3O4, Fe (II, III)) to be contained in small particles with diameters less than 2.5 µm and a large amount of goethite (α-Fe(O)OH, Fe (III)) to be present in the coarse particles with diameters of 2.5 µm or more.
Next, a comparison of the composition of PM10 and PM2.5 in the filter samples obtained from ECE showed that in both cases, wüstite (FeO, Fe (II)) accounted for more than 40% of the iron; Fe2O3 (sum of hematite (α-Fe2O3, Fe (III)) and maghemite (γ-Fe2O3, Fe (III))) accounted for about 16%; goethite (α-Fe(O)OH, Fe (III)) was not detected; and we observed a low proportion of trivalent iron. For other chemical species, metallic Fe (α-Fe, Fe (0)) was observed at around 17%, and magnetite (Fe3O4, Fe (II, III)) was present at around 25% for both PM10 and PM2.5. When PM2.5 filter samples (different filters collected) of ECE were compared, there were some differences, but no significant overall differences in trends were observed for magnetite (Fe3O4, Fe (II, III)) for both PM10 and PM2.5.
A previous study [6] has reported that the PM10 of brake wear particles collected from a brake dynamometer using ECE contains about 20.2% magnetite (Fe3O4, Fe (II, III)), 1.6% metallic iron (Fe (0)), and 54.6% hematite (α-Fe2O3) (Fe (III)). The differences between the literature and this study for small percentages of metallic iron (Fe (0)) may be due to differences in the friction material of the ECE pads or to differences in the braking conditions, but the details are unknown. However, the distributions of the chemical forms of iron quantified in this study could be used as source profiles and to apportion sources in atmospheric studies, and could thereby facilitate further research.

3.2.4. Phase Transformation

One important aspect of the above results (Figure 5) regarding the difference between NAO and ECE is that goethite (α-Fe(O)OH, Fe (III)) was not detected in ECE and contributed less to NAO PM2.5 than to NAO PM10. There are reports of no goethite being detected when ECE brakes and cast iron discs are used [7] and results of a little goethite being detected at low brake temperatures [8]. These reports support the almost complete absence of goethite in ECE in this study. On the other hand, a mixture of hydroxides, including goethite (α-Fe(O)OH), have also been detected on the disc and pad surface as the main corrosion products of gray cast iron [30].
This study considered the phase transformation of iron oxides and hydroxides, because the ECE and NAO were collected at roughly the same time, about one week apart, and not under conditions wherein iron would be prone to corrosion in an excessively humidified atmosphere. The phase transformation of iron oxides and hydroxides (FexOyHz) with temperature typically occurs at 675 °C for hematite (α-Fe2O3, Fe (III)), <600 °C for maghemite (γ-Fe2O3, Fe (III)), 575–586 °C for magnetite (Fe3O4, Fe (II, III)), <575 °C for wüstite (FeO, Fe (II)), and <200 °C for goethite (α-Fe(O)OH, Fe (III)) [31,32], although there are some differences that depend on the particle size. The temporal profiles of the disc temperatures shown in Figure 6 indicated that the difference between ECE brake temperatures (<140 °C) and NAO brake temperatures (<120 °C) was only about 20 °C at most. The maximum brake disc temperature recorded using a brake assembly during an interlaboratory event varied over a wide range of 150–190 °C [33]. We consider the maximum temperature of 120 °C for NAO and 140 °C for ECE in this study to be the maximum brake temperatures among the eight laboratories. Depending on the roughness of the pad surface, the real contact area may be much smaller than the apparent contact area, and the flash temperature of the real contact parts could exceed 1100 °C [34,35,36,37,38]. It is therefore difficult to fully explain the mechanism based on only the bulk temperature. The formation of brake wear particles is known to be caused by a very complex mechanochemical process that includes multiple compounds in the friction material [4].
We considered that the phase transformation from goethite (α-Fe(O)OH, Fe (III)) to iron oxides Fe2O3 (hematite (α-Fe2O3, Fe (III)) and maghemite (γ-Fe2O3, Fe (III))) in the ECE brake in this study was due to a tribological reaction involving hydrothermal transformation [32] related to the above-mentioned differences in brake temperature and disc surface microstructure friction material. Because the Fe-O phase transformation diagram indicates that FeO can exist stably at 700 °C, we hypothesized that goethite (α-Fe(O)OH, Fe (III)) underwent a phase transformation to FeO via the formation of hematite (α-Fe2O3, Fe (III)), maghemite (γ-Fe2O3, Fe (III)), and magnetite (Fe3O4, Fe (II, III)) by dehydrogenation. We suggest that the dehydrogenative phase transformation from goethite (α-Fe(O)OH, Fe (III)) to wüstite (FeO, Fe (II)) therefore resulted in a higher proportion of wüstite (FeO, Fe (II)) compared to NAO in the ECE brake. Even if the mechanism of corrosion and hydroxide formation on the pad and iron surface due to moisture generated from organic matter in NAO was the main mechanism, and hydroxide formation due to phase transition was a minor mechanism, the difference in observed iron oxides from NAO and ECE brake pads at a similar level of Fe content was a step toward meeting our goal.

3.2.5. Tribo-Reduction

One other feature of the results in Figure 5 is the difference between NAO and ECE; metallic Fe (α-Fe, Fe (0)) contributed less to ECE than to NAO. It is commonly assumed that metallic iron (α-Fe, Fe (0)) is generated only by abrasive wear of brake pads and cast iron discs [4,5]. We should note that metallic Fe is also produced by a tribo-chemical reduction with magnetite (Fe3O4, Fe (II, III)) as the starting material [39]. The following two reduction processes are required to produce metallic iron (α-Fe, Fe (0)) [39]. The reduction proceeds from magnetite (Fe3O4, Fe (II, III)) to wüstite (FeO, Fe (II)) as follows:
Fe3O4 + CO → 3Fe + CO2↑
Fe3O4 + H2 → 3FeO + H2O↑.
The reduction then proceeds from wüstite (FeO, Fe (II)) to metallic iron (α-Fe, Fe (0)) as follows:
FeO + CO → Fe + CO2↑
FeO + H2 → Fe + H2O↑.
Reduction gases such as carbon monoxide (CO) and hydrogen (H2) are generated by the decomposition of phenolic resin, which is a binder in brake pads [35,36,40,41,42], and the reduction can proceed as described in Equations (4)–(7) [39].
Tribological interfaces typically experience oxidative environments and conditions because the gases that should be involved in the reported reactions [39] do not remain near the pad and disc for long periods of time. Furthermore, the evidence for the process of tribo-reduction in the case of the aforementioned disc/pad interface is supported by the very limited experimental literature cited above [39]. The majority of the metallic iron in brake wear dust is clearly contributed by direct wear of the friction pair. This is also consistent with the finding of higher amounts of metallic iron in PM samples for ECE pad pairings compared to NAO pad pairings; ECE friction materials are typically characterized by a higher wear factor against cast iron discs compared to NAO friction materials [10]. In addition, NAO usually contains more organic resins than ECE. As a result, tribo-reduction processes are rarely observed at the disc–pad interface. It is reasonable to assume that the majority of the metallic iron (α-Fe, Fe (0)) observed in this study was contributed largely by direct wear of the friction pair.

3.2.6. Tribo-Oxidations

The amount of magnetite (Fe3O4, Fe (II, III)) in brake wear particles was higher in ECE than in NAO (Figure 5). Because of the small fraction of Fe (α-Fe, Fe (0)) and wüstite (FeO, Fe (II)) in NAO, the formation of Fe (α-Fe, Fe (0)) and wüstite (FeO, Fe (II)) from magnetite (Fe3O4, Fe (II, III)) by the tribo-reduction process in Equations (4)–(7) [39], which requires phenolic resin to be present on the pad and disc surfaces, does not occur. Under NAO paired-pad conditions, the main iron oxides are hematite (α-Fe2O3, Fe (III)) and maghemite (γ-Fe2O3, Fe (III)), which are produced mainly from the tribo-oxidation of the cast iron disc, in agreement with other results from the literature [43,44], which predict a highly oxidative environment for this type of NAO pad tribological system. The formation of magnetite (Fe3O4, Fe (II, III)) with a flash temperature (e.g., phase transformation temperature) of >586 °C [31,32] would be less favored than the formation of hematite (α-Fe2O3, Fe (III)) and maghemite (γ-Fe2O3, Fe (III)) [31,32]. In contrast, iron oxides (hematite (α-Fe2O3, Fe (III)) and maghemite (γ-Fe2O3, Fe (III))) are produced by a mechanism involving a reaction of the brake wear particles on the surface of the pad and disc with the outer atmosphere. However, at the time of the experiment, it was not possible to determine the detailed mechanisms responsible for the formation of the main iron oxide (hematite (α-Fe2O3, Fe (III)) and maghemite (γ-Fe2O3, Fe (III))) from the NAO, and the smaller percentages of magnetite (Fe3O4, Fe (II, III)) in NAO rather than ECE. Further experiments will be required to identify these mechanisms.

4. Conclusions

In this study, we characterized the possible contribution of iron oxides and hydroxides to airborne brake wear particles under realistic vehicle driving and braking conditions with different friction materials. The conclusions of this study were as follows:
  • Significant differences between wear factors and PM10 emissions were observed between NAO and ECE brake pads. Mass losses as wear factors were found to be 4.02 mg/km per brake for the NAO pads and 9.31 mg/km per brake for the ECE pads. Emissions of brake wear particles were 1.43 ± 0.29 mg/km per brake for PM10 with NAO and 3.73 ± 0.19 mg/km per brake for PM10 with ECE.
  • The dominant contribution to PM10 and PM2.5 brake wear particles was Fe for both NAO and ECE. The iron concentration ratio in the particle mass was comparable to the disc-to-pads ratio measured by wear mass.
  • Differences in the consistency of iron oxides and hydroxides were observed between NAO and ECE brake pads.
  • The hydroxide goethite (α-Fe(O)OH, Fe (III)) was detected only in the NAO pad. It is difficult to fully explain the mechanism based on only the bulk temperature, but a high goethite (α-Fe(O)OH, Fe (III)) contribution to the NOA brake was suggested because of the phase transformation from goethite (α-Fe(O)OH, Fe (III)) to iron oxides (hematite (α-Fe2O3, Fe (III)) and maghemite (γ-Fe2O3, Fe (III))) in this study.
  • Metallic iron (α-Fe, Fe (0)) was generated not only from abrasive wear but also from the tribo-chemical reduction with magnetite (Fe3O4, Fe (II, III)) as the starting material.
  • Magnetite (Fe3O4, Fe (II, III)), which is of interest from the point of view of health effects, was less abundant in NAO than in ECE. The implication is that magnetite (Fe3O4, Fe (II, III)) is less likely to form in NAO because of the tribo-oxidations that occur in NAO.
The quantification of iron speciation in this study could serve as an example of source identification in atmospheric observations of brake wear particles, and could contribute to further research.

Author Contributions

Conceptualization, H.H.; methodology, H.H.; formal analysis, H.H., A.I. and T.O.; investigation, H.H., A.I. and T.O.; resources, H.H. and T.O.; data curation, H.H., A.I. and T.O.; writing—original draft preparation, H.H; writing—review and editing, H.H., A.I. and T.O.; visualization, H.H.; supervision, H.H., A.I. and T.O.; project administration, H.H.; funding acquisition, H.H., A.I. and T.O. All authors have read and agreed to the published version of the manuscript.

Funding

This work was partially supported by the Japan Society for the Promotion of Science (JSPS) KAKENHI (grant numbers JP 22K03895, 20K20614) and JST CREST (grant number JPMJCR19H3).

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

The brake emission data presented in this study are available upon reasonable request from the corresponding author. The data are not publicly available due to a confidentiality agreement with the part providers.

Acknowledgments

The authors would like to thank the co-workers who supported the set-up and operation of the dynamometer and the measurements. Hiroyuki Setoyama of the Kyushu Synchrotron Radiation Research Centre (SAGA-LS) helped with the acquisition and analysis of the XAFS spectra. The experiments using synchrotron radiation were performed at the beamlines BL11 and BL15 of the SAGA Light Source with the proposal Nos. 1809080F and 1809081F (for BL11), and also 22050540F and 2210101F (for BL15). The author would also like to thank the reviewers who provided numerous helpful suggestions to improve the quality of the paper.

Conflicts of Interest

The authors declare no conflicts of interest.

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Figure 1. Comparison of NAO and ECE pads paired with conventional gray cast iron ventilated discs in wear factors for the front brake axle.
Figure 1. Comparison of NAO and ECE pads paired with conventional gray cast iron ventilated discs in wear factors for the front brake axle.
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Figure 2. Emissions of brake wear particle masses of the front brake axles versus particle mass sizes of NAO and ECE paired with a conventional gray cast iron ventilated disc.
Figure 2. Emissions of brake wear particle masses of the front brake axles versus particle mass sizes of NAO and ECE paired with a conventional gray cast iron ventilated disc.
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Figure 3. Elemental components of the pad friction surface, PM10, and PM2.5 in NAO and ECE paired with discs. The components unaccounted for in the PM10 and PM2.5 samples include elements such as oxygen and other elements not measurable by XRF analysis of the filter samples.
Figure 3. Elemental components of the pad friction surface, PM10, and PM2.5 in NAO and ECE paired with discs. The components unaccounted for in the PM10 and PM2.5 samples include elements such as oxygen and other elements not measurable by XRF analysis of the filter samples.
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Figure 4. XAFS spectra of (a) standard samples, (b) NAO and ECE for powdered PM10 samples, (c) NAO for powdered PM10 and filtered PM2.5 samples, and (d) ECE for powdered PM10 and filtered PM2.5 samples.
Figure 4. XAFS spectra of (a) standard samples, (b) NAO and ECE for powdered PM10 samples, (c) NAO for powdered PM10 and filtered PM2.5 samples, and (d) ECE for powdered PM10 and filtered PM2.5 samples.
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Figure 5. Iron speciation of (a) NAO of powdered PM10 samples, (b) NAO of powdered PM2.5 samples (Filter A), (c) NAO of powdered PM2.5 samples (Filter B), (d) powdered PM10 samples, (e) ECE of powdered PM2.5 samples (Filter A), and (f) ECE of powdered PM2.5 samples (Filter B).
Figure 5. Iron speciation of (a) NAO of powdered PM10 samples, (b) NAO of powdered PM2.5 samples (Filter A), (c) NAO of powdered PM2.5 samples (Filter B), (d) powdered PM10 samples, (e) ECE of powdered PM2.5 samples (Filter A), and (f) ECE of powdered PM2.5 samples (Filter B).
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Figure 6. Temporal profiles of brake temperatures for NAO and ECE paired with conventional gray cast iron ventilated discs for the front brake axle.
Figure 6. Temporal profiles of brake temperatures for NAO and ECE paired with conventional gray cast iron ventilated discs for the front brake axle.
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Hagino, H.; Iwata, A.; Okuda, T. Iron Oxide and Hydroxide Speciation in Emissions of Brake Wear Particles from Different Friction Materials Using an X-ray Absorption Fine Structure. Atmosphere 2024, 15, 49. https://doi.org/10.3390/atmos15010049

AMA Style

Hagino H, Iwata A, Okuda T. Iron Oxide and Hydroxide Speciation in Emissions of Brake Wear Particles from Different Friction Materials Using an X-ray Absorption Fine Structure. Atmosphere. 2024; 15(1):49. https://doi.org/10.3390/atmos15010049

Chicago/Turabian Style

Hagino, Hiroyuki, Ayumi Iwata, and Tomoaki Okuda. 2024. "Iron Oxide and Hydroxide Speciation in Emissions of Brake Wear Particles from Different Friction Materials Using an X-ray Absorption Fine Structure" Atmosphere 15, no. 1: 49. https://doi.org/10.3390/atmos15010049

APA Style

Hagino, H., Iwata, A., & Okuda, T. (2024). Iron Oxide and Hydroxide Speciation in Emissions of Brake Wear Particles from Different Friction Materials Using an X-ray Absorption Fine Structure. Atmosphere, 15(1), 49. https://doi.org/10.3390/atmos15010049

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