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Mass reconstruction methods for PM2.5: a review

Judith C. Chow, Douglas H. Lowenthal, L.-W. Antony Chen and 2 more (opens in a new tab)

Air Quality, Atmosphere & Health · 2015

doi:10.1007/s11869-015-0338-3 (opens in a new tab)

Abstract

Electronic supplementary material. The online version of this article (doi:10.1007/s11869-015-0338-3) contains supplementary material, which is available to authorized users.

Full text

From PubMed Central, U.S. National Library of Medicine, as current on Oct 27, 2026. Paragraph numbers are ours, so an answer can point at one.

Introduction

Particles with aerodynamic diameters <2.5 μm (PM2.5) and 10 μm (PM10) mass concentrations are regulated by the National Ambient Air Quality Standards (NAAQS; Bachmann; Chow et al. ) in the USA, with variations being adopted in other countries (Cao et al. ). For compliance monitoring, ambient particles are collected over 24-h durations onto filters that are weighed before and after sampling (Chow; Watson and Chow ). Chemically speciated PM is needed to better understand pollution sources, atmospheric processing (e.g., transport and transformation), temporal and spatial variations and long-term trends, as well as adverse health and environmental consequences. PM2.5 mass and chemical components (i.e., ions, elements, and carbon) have been acquired in the National Park Service (NPS) Interagency Monitoring of Protected Visual Environments (IMPROVE) non-urban network, and the US Environmental Protection Agency (EPA) urban Chemical Speciation Network (CSN; Solomon et al.; USEPA ) on an every-third- or sixth-day schedule since 1987/1988 and 1999/2000, respectively. Measurement protocols for the US PM2.5 networks are documented by Chow et al. and Solomon et al.. Sampling and chemical analysis methods vary in these and other long-term networks and in special studies from the USA and elsewhere (e.g., Dabek-Zlotorzynska et al.; Zhang et al. ).

Chow and Watson summarize different PM chemical analysis methods. The major PM components measured to explain gravimetric mass include: (1) anions (e.g., chloride (Cl−), nitrate (NO3 −), and sulfate (SO4 =)) and cations (e.g., water-soluble sodium (Na+), potassium (K+), and ammonium (NH4 +)); (2) elements, including metals (up to 51 elements from sodium (Na) to uranium (U)); and (3) organic carbon (OC) and elemental carbon (EC) and their carbon fractions. To accommodate chemical speciation, at least two types of sampling substrates (i.e., Teflon-membrane and quartz-fiber filters) are needed (Chow ). IMPROVE and CSN use three parallel channels, in which mass by gravimetry and elements by X-ray fluorescence (XRF; Watson et al. ) are measured on Teflon-membrane filters; ions by ion chromatography (IC; Chow and Watson ) are measured on nylon-membrane filters preceded by a sodium carbonate (Na2CO3) denuder (Ashbaugh and Eldred ) to remove nitric acid (HNO3); and OC and EC by thermal/optical carbon analysis (Chow et al.,, ) are measured on quartz-fiber filters. PM components include carbon (C), hydrogen (H), nitrogen (N), sulfur (S), oxygen (O), and a wide variety of other elements. Owing to practical analytical limitations (Chow and Watson ), most networks do not measure H and O associated with OC, geological minerals, and liquid water—with the exception of the IMPROVE network, where H was quantified from 1988 to 2010 (Nejedly et al. ). As a result, the sum of the measured species is often lower than the gravimetric mass. Watson specifies a percent mass explained of 100 ± 20 % for source apportionment models, and this is a reasonably good criteria for mass reconstruction.

PM mass reconstruction (also called mass closure or material balance) applies multipliers to several of the measured species to estimate unmeasured components. Mass reconstruction is used to: (1) identify and correct potential measurement errors as part of data validation efforts (Chow et al.; Malm et al.; Watson et al. ); (2) understand temporal and spatial variations of chemical composition (Hand et al.; Malm et al. ); and (3) estimate source contributions to PM and light extinction (Chow and Watson; Watson ). Mass reconstruction attempts to achieve closure between gravimetric mass and the sum of major components with assumptions to account for unmeasured species, but without double counting. For example, when SO4 = is included, elemental S is omitted; inclusion of elemental chlorine (Cl) excludes water-soluble Cl−; and the same applies for elemental potassium (K) and water-soluble potassium (K+) (Chow et al. ). Although this review focuses on PM2.5, a similar approach is applicable for PM10. As PM2.5 is part of PM10, mass reconstruction should be conducted for both PM2.5 and PMcoarse (i.e., PM10–2.5) when PM10 speciation is available (e.g., Chow et al. ).

Various approaches have been taken for PM mass reconstruction (e.g., Frank; Hand et al.; Malm et al. )—the widely used 11 equations are documented in “Commonly applied reconstructed mass equations.” Applications of these equations to past studies (summarized in the supplemental material) are enumerated in “Applications of mass reconstruction equations to special studies.” To provide a perspective on the fraction of mass explained, examples of mass reconstruction applications for the long-term US IMPROVE network are given in “Evaluation of mass reconstruction through analysis of large data sets.” Various regression techniques have been used to derive multipliers for major PM components and to examine the adequacy of using the IMPROVE equations for mass reconstruction. Major factors that bias mass reconstruction (e.g., the use of an OC multiplier to estimate organic matter (OM), carbon sampling and analysis artifact, ammonium and nitrate volatilization, and particle-bound water on Teflon-membrane filters) are discussed in “Major factors influencing mass reconstruction.” This review examined hundreds of prior studies and intends to: (1) track the evolution and approaches for mass reconstruction; (2) discuss the adequacy of each approach; and (3) address major PM sampling and analysis issues that influence mass reconstruction.

Commonly applied reconstructed mass equations

Table 1 summarizes 11 PM mass reconstruction methods (i.e., Eqs. 1 to 11, sequence in chronological order of publication) that have been applied to data acquired since the late 1970s. Some variations from other studies are referenced. Reconstructed mass (RM) is expressed as the sum of its seven representative chemical components, including: (1) inorganic ions; (2) OM or OC; (3) EC, also referred to as “black carbon” (BC), “soot,” or light absorbing carbon (LAC); (4) geological minerals (or materials), often referred to as “dust,” “soil,” or “crustal material;” (5) salt (sea salt near oceans and inland seas, but also deriving from wintertime de-icing material and desert playas); (6) trace elements (other elements that are not accounted for as minerals, as from fly ash); and (7) “others,” or “remaining mass,” representing other unaccounted or unidentified components. As such, RM equations take the following form:

Each of these components can derive from a variety of sources, though they are often dominated by a few sources. Minerals, for example, do not include OM that might be associated with engine exhaust or bioaerosols deposited onto roadways or agricultural soils. These would be included in the OM fraction. Similarly, some fugitive dust sources include salts, but these would be accounted for in the salt fraction; sulfates and nitrates that react with salt (Hoffman et al. ) would be accounted for in the inorganic ion fraction. The background and assumptions related to these RM components are described in the following subsections.

Inorganic ions

In addition to commonly measured anions and cations by IC, automated colorimetric (AC), atomic absorption spectroscopy (AAS), and inductively coupled plasma-atomic emissions spectroscopy (ICP-AES) have also been applied for ionic speciation (Chow and Watson ). Depending on the measurements available, the following methods are used to determine their mass contributions:In the absence of NH4 + measurement, SO4 = and NO3 − are assumed to be neutralized to ammonium sulfate ((NH4)2SO4) and ammonium nitrate (NH4NO3), with the NH4 + fraction accounted for by stoichiometric multipliers: 1.375SO4 = and 1.29NO3 −, respectively (i.e., Eqs. 1, 10, and 11 in Table 1). An ion balance based on molar equivalence between the measured anions and cations should be applied to verify the extent of neutralization (Chow et al. ).SO4 =, NO3 −, and NH4 + are summed without weighting factors (i.e., Eqs. 2, 3, 5, 6, and 8). This does not account for H when SO4 = is incompletely neutralized by NH4 + as in sulfuric acid (H2SO4), ammonium bisulfate (NH4HSO4), or letovicite ((NH4)3H(SO4)2).When only S is measured, it is assumed to be neutralized (NH4)2SO4 (i.e., 4.125S in Eqs. 7 and 9) and summed with either NO3 − (Landis et al. ) or NH4NO3 (1.29NO3 − in Eqs. 7 and 9). If NO3 − is not measured, NH4NO3 is assumed to be negligible (Malm et al., Eq. 4). This assumption is valid only when the NO3 − concentration is low, as it is for some non-urban, eastern US IMPROVE sites but not for others (Pitchford et al. ). Abundant NO3 − has been found in several urban areas, especially during fall and winter (Green et al. ).

In the absence of NH4 + measurement, SO4 = and NO3 − are assumed to be neutralized to ammonium sulfate ((NH4)2SO4) and ammonium nitrate (NH4NO3), with the NH4 + fraction accounted for by stoichiometric multipliers: 1.375SO4 = and 1.29NO3 −, respectively (i.e., Eqs. 1, 10, and 11 in Table 1). An ion balance based on molar equivalence between the measured anions and cations should be applied to verify the extent of neutralization (Chow et al. ).

SO4 =, NO3 −, and NH4 + are summed without weighting factors (i.e., Eqs. 2, 3, 5, 6, and 8). This does not account for H when SO4 = is incompletely neutralized by NH4 + as in sulfuric acid (H2SO4), ammonium bisulfate (NH4HSO4), or letovicite ((NH4)3H(SO4)2).

When only S is measured, it is assumed to be neutralized (NH4)2SO4 (i.e., 4.125S in Eqs. 7 and 9) and summed with either NO3 − (Landis et al. ) or NH4NO3 (1.29NO3 − in Eqs. 7 and 9). If NO3 − is not measured, NH4NO3 is assumed to be negligible (Malm et al., Eq. 4). This assumption is valid only when the NO3 − concentration is low, as it is for some non-urban, eastern US IMPROVE sites but not for others (Pitchford et al. ). Abundant NO3 − has been found in several urban areas, especially during fall and winter (Green et al. ).

Assuming 1.29NO3 − for NH4NO3 may not be valid when HNO3 reacts with suspended dust to form calcium nitrate (Ca(NO3)2) or when it reacts with sodium chloride (NaCl) from a marine intrusion or suspension from an alkaline playa to form sodium nitrate (NaNO3) (Hoffman et al. ). Lee et al. noted the presence of PM2.5 Ca(NO3)2 at several IMPROVE sites owing to a coarse particle NO3 − tail that extended below 2.5 μm. Harrison et al. applied Eq. 7 for PM2.5 ions and added NaNO3 for PM10–2.5. Several studies used front filter NO3 − (i.e., non-volatilized NO3 − from Teflon-membrane or quartz-fiber filters), as volatilized NO3 − is not part of the gravimetric mass (Chow et al. ). Ma et al. estimated NH4NO3 as 2.857 N, with N measured by an elemental analyzer, which is commonly applied to fuel assays. The presence of ammonium chloride (NH4Cl) in PM2.5 was noted by Kelly et al. for Utah’s Salt Lake valley; by Pant et al. in New Delhi, India, where there is abundant trash burning; and by Levin et al. for biomass burning samples.

Elemental S has been commonly measured by XRF or proton-induced X-ray emission (PIXE) analyses (Watson et al. ). Based on molecular weight, 3S can be used to estimate SO4 =, assuming that all S is water-soluble SO4 =. This is not the case when: (1) S is associated with insoluble organic compounds such as mercaptans; (2) S is not completely water-soluble, as is the case for minerals such as gypsum (CaSO4·2H2O) and pyrite (FeS2); or (3) S consists of sulfur dioxide (SO2) adsorbed onto soot or other particles (Watson ).

For coastal environments, non-sea-salt sulfate (i.e., nssSO4 = = SO4 = − 0.252Na+, based on SO4 =/Na+ molar ratio in sea water) can be estimated (Sciare et al. ). Summed nssSO4 = + NO3 − + NH4 + has been applied to estimate contributions from inorganic ions (Cheung et al.; Maenhaut et al.; Mkoma et al.; Querol et al.; Terzi et al. ). Zhang et al. also included K+ (a marker for biomass burning) as an additional inorganic ion.

Since NH4 + is not quantified in the IMPROVE network, (NH4)2SO4 is estimated by 4.125S (Eq. 7). Due to variations between SO4 = (by IC) and S (by XRF) ratios, Hand et al. used 1.375SO4 = (Eq. 10). Both the original (Eq. 7) and the revised (Eq. 10) IMPROVE equations have been the foundation for reconstructing light extinction in the USA under the Regional Haze Rule (now termed the Clean Air Visibility Rule; Pitchford et al.; USEPA; Watson ).

Organic mass/organic carbon (OM/OC)

To account for the unmeasured H, O, N, and S in organic compounds, a conversion factor (or multiplier) is used to transform OC to OM, i.e.,

The f multipliers of 1.4 and 1.8 in Table 1 are not site or time specific. Depending on the extent of OM oxidation and secondary organic aerosol (SOA) formation, values for f vary from 1.2 for fresh aerosol in urban areas (Chow et al., ) to 2.6 for aged aerosol (Countess et al.; Robinson et al.,; Roy et al.; Turpin and Lim ). For example, benzo(a)pyrene (C20H12), an indicator of incomplete fuel combustion found in engine exhaust (Lowenthal et al. ) has an f = 1.05; whereas cellulose (C6H10O5)n, a major component of unburned biological material, has an f = 2.25 (Cerqueira et al.; Puxbaum and Tenze-Kunit; Sanchez-Ochoa et al. ).

The origins for f = 1.2–1.5 result from circular reasoning with limited measurements. Macias et al. (, Eq. 1) used 1.5 based on an assumed organic composition proportional to CH2O0.25. Solomon et al. (, Eq. 2) used 1.4, citing Gray et al., who used both 1.2 and 1.4 for studies in California’s South Coast Air Basin (SoCAB). The f = 1.2 originated from Countess et al., based on the analysis of ambient carboxylic acid (C16: (C + H + O)/C = 1.3), polynuclear aromatic ((C + H)/C = 1.08), and aliphatic compounds ((C + H)/C = 1.17) (van Vaeck and van Cauwenberghe ) in Denver, CO. Ma et al. used 1.4 but cited Countess et al.. As noted by Andrews et al. and Watson, the 1.4 derives from Grosjean and Friedlander, based on two Los Angeles total suspended particle (TSP) samples. The ratios of C to the sum of C, H, N, and O was 0.66 for oxygenated organics and 0.86 for aliphatics; the inverses are 1.5 and 1.2, respectively. Gray et al. referred to White and Roberts, who used f = 1.4 to construct a chemical light extinction budget based on Grosjean and Friedlander. Harrison et al. used 1.4 for urban background sites in Birmingham, UK, and 1.3 for roadside sites in London, UK, citing Russell.

Chow et al. (;, Eqs. 3 and 5, respectively) used 1.4, citing Solomon et al.. Andrews et al. (, Eq. 6) also used 1.4, citing both White and Roberts and Grosjean and Friedlander. Maenhaut et al. (, Eq. 8) used 1.4 for samples from Melpitz, Germany, citing Turpin et al.. DeBell et al. (, Eq. 9) and Hand et al. (, Eq. 10) increased the f from 1.4 to 1.8 for the revised IMPROVE equation (Eq. 10) based on non-urban aerosols (e.g., El-Zanan et al. ) and regression analysis by Malm and Hand. The average regression coefficient was 1.7 for OC across all IMPROVE sites for years 1988–2003. This is similar to the f = 1.8 used by Maenhaut et al. for samples from K-puszta, an EUSAAR station in Hungary, and by Mkoma et al. for a rural site in East Africa.

Several studies (e.g., Mkoma et al.; Ni et al.; Remoundaki et al.; Terzi et al.; Vecchi et al.; Viana et al. ) used an f multiplier of 1.6, whereas f = 1.7 was reported by others (e.g., Guinot et al.; Putaud et al.; Rees et al. ). The value of the f multiplier under different situations remains the subject of current research. Biomass burning (especially during the smoldering phase) may require a higher f multiplier as it contains many oxygenated organic compounds (Chen et al.; Chow et al. ), such as levoglucosan (C6H10O5), a wood smoke marker (Simoneit et al. ) with the same chemical formula but a structure that differs from cellulose. For laboratory-generated vegetative burning, Levin et al. reported f = 1.55, consistent with a finding of f = ∼1.5 by Reid et al.. Aiken et al. reported f = 1.55–1.7 for primary biomass combustion emissions in Mexico City, lower than 1.9–2.1 found by Polidori et al. in Pittsburgh, PA, during winter and 2.2–2.6 suggested by Turpin and Lim.

Elemental carbon

The RM equation in Table 1 contain EC without any multiplier. Since OC and EC are operationally defined, absolute OC and EC concentrations and the ratio of OC to EC vary by carbon analysis method (Watson et al. ).

Geological minerals

Geological “minerals” might better represent geological “material,” as only assumed oxides of mineral elements (e.g., aluminum (Al), silicon (Si), calcium (Ca), K, titanium (Ti), and iron (Fe)) are included to calculate geological mass. These elements have been measured by XRF, PIXE (e.g., Maenhaut et al. ), and, in some cases, instrumental neutron activation analysis (INAA; Maenhaut et al.; Siddique and Waheed ) or ICP-mass spectrometry (ICP-MS). Most researchers use one of the five soil formulae listed in Table 1. Macias et al. (, Eq. 1) expressed minerals as the sum of the oxides of Al, Si, Ca, K, and Fe assuming the common oxide forms of Al2O3, SiO2, CaO, K2O, and Fe2O3, respectively (Pettijohn ). Several studies eliminated the 1.2 K (Eq. 2), except for Andrews et al. (, Eq. 6), Kleindienst et al., and Ni et al., which also included 1.67Ti. A higher value (1.95Ca) was used by Terzi et al. and Remoundaki et al. to account for both CaO and CaCO3.

The IMPROVE “soil” formula (Malm et al., Eq. 4), applied in Eqs. 7–10, follows Macias et al. (, Eq. 1) with the following modifications: (1) iron oxides are equally divided between Fe2O3 and FeO; (2) K in soil is estimated as 0.6Fe, based on the composition of coarse particles (Cahill et al. ), because some PM2.5 K is emitted by biomass burning; and (3) titanium dioxide (TiO2) is included. All of the initial element coefficients are then multiplied by 1.16 to account for unmeasured O, therefore:

The IMPROVE “soil” formula (Eq. C) has been applied in several other studies (e.g., Chan et al.; Pant et al. ). Rogula-Kozlowska et al. applied Eq. C but supplemented with 2.4K based on the stoichiometric concentration of K2O. Due to the uncertainties associated with Al by XRF (McDade ), Simon et al. (, Eq. 11) eliminated Al and used 3.48Si, based on the Al to Si ratio (0.46) in IMPROVE samples. Landis et al. also eliminated Al but used 3.79Si, citing uncertainties in quantifying Al by energy-dispersive XRF. Hueglin et al. estimated Si in Eq. 1 as 3.41Al (Mason ) and also included 1.66Mg.

Single crustal elements have also been used to estimate the geological mineral contribution to PM mass. Si is the most abundant element (10–20 %) in the earth’s crust besides O (Chow et al.; Houck et al. ). Countess et al. used 3.5Si, and Ma et al. used 4.807Si (assuming 20.8 % Si in soil; Scheff and Valiozis ). Using Al as a soil marker (Duce et al. ), Ho et al. used 13.77Al, Hsu et al. used 12.5Al, and Zhang et al. used 14.29Al. Besides 4.3Ca (from gypsum), Harrison et al. used the sum of 9Fe for background and 3.5Fe to 5.5Fe for roadside sites, assuming 11–29 % of Fe in fugitive dust. Putaud et al. summed non-sea-salt (nss)K+, nssCa++, and gravimetric analyses of water insoluble species as residues (600 °C for 8 h) to estimate minerals. Since geological minerals are not a major component of PM2.5, variations in the assumptions regarding metal oxides or multipliers do not contribute to large variations in RM.

Salt

Chow et al. (, Eq. 5) and Rogula-Kozlowska et al. used the sum of Na+ and Cl− to track summertime transport of marine aerosol in California. Others (e.g., Maenhaut et al., Eq. 8,; Mkoma et al.; Viana et al. ) used Cl + 1.4486Na, based on the ratio of the sum of all elements (except Cl) to Na in sea water (Riley and Chester ). Ohta and Okita used 3.27Na+, and others (e.g., Chan et al.; Chow et al.; Ho et al.; Siddique and Waheed; Yan et al. ) used 2.54Na+, whereas Harrison et al. and Joseph et al. used 1.65Cl− to represent salt content.

PM2.5 Na is a conservative marker for salt (Lowenthal and Kumar; White ), but it suffers self-absorption interferences by XRF (Dzubay and Nelson; Formenti et al.; Watson et al. ). Therefore, 1.8Cl−, based on the abundance of Cl− in sea water (White ), is used in the revised IMPROVE equation (Eq. 10). This approach is reasonable when: (1) there is no depletion of Cl− in salt aerosols from reaction with H2SO4 or HNO3; (2) hydrochloride acid (HCl) is retained on the nylon-membrane filter, i.e., the preceding Na2CO3 denuder to remove HNO3 (Channel 2 of the IMPROVE sampler) does not remove any HCl; and (3) HCl only originated from reactions of acids with salt particles. In any case, 1.8Cl− is a lower limit to estimate salt, assuming that Cl− is measured accurately by IC (Chow and Watson ). With advances in chromatographic techniques, the Cl− signal in the chromatogram no longer overlaps the deionized distilled water dip and can be determined quantitatively. As Cl may be depleted under vacuum by XRF analysis, Cl− is a logical choice to estimate salt concentration. More water-soluble species in salt sources (e.g., sea water; Pytkowicz and Kester ) could be measured to reduce the uncertainty.

Depletion of Cl− occurs as H2SO4 or HNO3 reacts with sea salt, which exchanges Cl− for SO4 = or NO3 −, respectively. This will increase the sea salt mass as SO4 = (MW = 96) and NO3 − (MW = 62) are heavier than Cl− (MW = 35) (Bardouki et al. ). For coastal samples from Canada, Yao and Zhang hypothesized Cl− replacement with di-nitrogen pentoxide (N2O5), instead of HNO3, and that SO4 = may be associated with Cl− depletion under acidic conditions. Sciare et al. defined sea salt (ss) as the sum of Na+, Cl−, ssCa++, ssK+, water-soluble magnesium (Mg++), and ssSO4 =; Zhang et al. substituted ssMg++ for Mg++, whereas Hsu et al. used the sum of Na+, Cl−, and Mg++.

Trace elements

Minor or trace elements, excluding geological species, can be added to the RM. Macias et al. (, Eq. 1) summed the trace elements in the form of CuO, ZnO, and PbO. Other studies (i.e., Eqs. 3, 5, 6, and 8) summed remaining elements by XRF, excluding S and the geological elements, with the exception of Solomon et al. (, Eq. 2), who also included Na+ and Mg++. Trace elements are more pronounced in coarse particles or at sampling sites near industrial facilities contaminated with toxic metals (Chow et al. ) when some elements are not accounted for by the mineral formulae in Table 1. More complicated trace element oxides (TEOs; sum of oxides for vanadium (V), manganese (Mn), nickel (Ni), copper (Cu), zinc (Zn), arsenic (As), lead (Pb), selenium (Se), strontium (Sr), phosphorus (P), chromium (Cr), and K) were used by Landis et al. and Zhang et al., but this component accounted for a small fraction (0.5–1.6 %) of PM2.5 mass. Therefore, summing the remaining elements may be sufficient.

Others

The remaining mass may be attributed to measurement errors, improper multiplier(s), missing source(s), and/or particle-bound water (e.g., Frank; Malm et al. ). This component could represent negative mass if RM overestimates gravimetric mass.

Non-crustal K was estimated as “Others” by Maenhaut et al., Simon et al., and Yan et al. based on either K − 0.6Fe (Eq. 8) or 1.2 × (K − 0.6Fe) (Eq. 11), respectively. Organic acids (sum of acetate, fomite, methane sulfonate, pyruvate, and oxalate) were added to RM by Putaud et al..

Applications of mass reconstruction equations to special studies

Supplemental Table S-1 summarizes previous studies which give rise to the 11 RM equations in Table 1. Only a subset of equations (i.e., Eqs. 1, 2, 3, 5, and 8) are applied in these short-term special studies. Concerns over visibility degradation in the southwestern USA prompted the establishment of the Western Fine Particle Network that measured size segregated mass and elements during 1977–1981 (Flocchini et al. ). As part of the Denver Winter Haze Study and Project VISTTA, Countess et al. and Macias et al. started using RM to determine sources of haze-causing aerosol in uban Denver and non-urban Grand Canyon areas, respectively. Equation 1 was developed by Macias et al. for PM samples at two remote desert sites near Page, AZ. SO4 = was not completely neutralized based on the molar ratio of NH4 + to SO4 = (1.65 instead of 2.0). RM accounted for 75–93 % of PM2.5 and 50–69 % of PM15–2.5. Low PM15–2.5 RMs were attributed to the absence of carbon measurements.

For nine sites in the SoCAB (Solomon et al., Eq. 2), RM accounted for 86–94 % (averaging 92 %) of annual PM10. Average measured NH4 + concentrations were 17 % lower than those estimated from (NH4)2SO4 and NH4NO3, consistent with sulfates being slightly acidic or some of the nitrates being present as NaNO3. In another SoCAB study (Chow et al., Eq. 3), RM accounted for 70–80 % of PM2.5 and 80–85 % of PM10 at nine sites during summer; unexplained mass was 5 % lower at six sites during fall. Chow et al. measured OC on tandem quartz-fiber filter packs (i.e., OC on quartz-fiber front filter as OCQF, followed by a quartz-fiber backup filter as OCQBQ) to estimate adsorption of volatile organic compounds (VOCs; Chow et al.; Subramanian et al.; Turpin et al. ), but large variations were found in OCQBQ. Average OC field blanks (OCFB) are commonly subtracted from OCQF (Chow et al.; Watson et al. ). In such cases, RM uses blank subtracted values.

In central California (Chow et al., Eq. 5), RM accounted for >90 % of PM2.5 and PM10 at ten sites. At PM concentrations <30 μg/m3, the RM often exceeded the measured PM mass. This was in part attributed to OCQF that was not blank-corrected as OCQBQ > OCQF in 168 out of 584 (29 %) samples during ozone episodes. Uncorrected OCQF may be affected by a combination of positive (adsorption) and negative (volatilization) biases (Chow et al.; Watson et al. ).

In Melpitz, Germany, RM accounted for 86 % of PM2 and 116 % of PM10–2 (Maenhaut et al., Eq. 8). OC was overestimated owing to adsorption of VOCs on quartz-fiber filters, as PM mass was 21 % higher from the quartz-fiber than the collocated Nuclepore-membrane filters. Water associated with hygroscopic species was not accounted for by gravimetry. Considering that the sum of inorganic ions accounted for 34 % of the PM10–2, the associated water at 50 % filter equilibration RH could have accounted for the overestimation of PM10–2 mass.

Evaluation of mass reconstruction through analysis of large data sets

Several studies have evaluated RM in the IMPROVE network (see Eqs. 4, 6, 7, and 9–11 in Table 1), the largest and most consistently acquired chemical speciation data set in the world. Malm et al. (, Eq. 4) first applied the IMPROVE “soil” formula (Eq. ) to 36 sites, and RM accounted for 75–80 % of PM2.5, consistent with an OM underestimation using 1.4OC. Andrews et al. (, Eq. 6) reported low RM (58–67 % of PM2.1) among four different types of samplers at Great Smoky Mountains National Park. Replacing SO4 = with (NH4)2SO4 increased RM by 6 %. The corresponding IMPROVE samples yielded RM as 83 % of measured mass. Andrews et al. attributed the mass deficit to: (1) underestimation of geological minerals; (2) water retention on the Teflon-membrane filter deposit; and (3) underestimation of OM. However, the mineral contribution was too small to account for the deficit. The RM deficiency was reduced to 15–23 % after estimating water content; hygroscopic organics may result in additional particle-bound water (Saxena and Hildemann ). In addition to the low OM (1.4OC) estimate, subtracting OCQBQ over-corrected for organic vapor adsorption (Andrews et al. ).

Lowenthal and Kumar applied Eq. 7 to 59 IMPROVE sites from 1988 to 1999. RM averaged 88 %, ranging 61–98 % of PM2.5. Incorporating Na, Cl, and trace elements increased RM by 30 % at the coastal Point Reyes site but had a small effect (∼3 %) at other sites. RM accounted for a larger fraction during winter than summer at 51 of 59 sites.

At ∼40 % RH (i.e., IMPROVE filter equilibration conditions for gravimetric analysis), (NH4)2SO4 and NH4NO3 (Eq. 7) absorb about 0.3 and 0.2 g of water/g of dry compound, respectively, assuming supersaturated (NH4)2SO4 (Chan et al.; Tang and Munkelwitz ). The addition of water would increase RM by 11 % in summer and 12 % in winter. A more hygroscopic form of SO4 = or H2SO4 is needed during summer to account for the observed seasonal differences. However, this assumption cannot be tested without measured NH4 + or H+ and would not explain the discrepancies when SO4 = levels are low.

Using 2.1OC (Turpin and Lim ) increased RM by 14 % in summer and 16 % in winter (which overestimated measured PM2.5). A lower f may be applicable in winter due to lower photochemical activity (i.e., less unmeasured O in OM). For IMPROVE sites, monthly median OCQBQ (acquired at ∼5 % of IMPROVE sites) was used for blank subtraction, assuming VOCs adsorbed on both QF and QBQ became saturated (Watson et al. ). During 1990–1999, monthly median OCQBQ in summer were 0.155 μg/m3 (∼3 % of PM2.5) higher than winter. Gaseous organic adsorption and seasonal effects in the OC multiplier, evaluated by Lowenthal and Kumar, narrowed the seasonal RM deficit.

PM2.5 sampling methods in both the IMPROVE network and CSN result in artifacts for RM (DeBell et al., Eq. 9; Hand et al., Eq. 10). Malm et al. addressed the uncertainties in PM2.5 gravimetric and speciation measurements. PM2.5 ions (e.g., Cl−, NO3 −, and SO4 =) are measured on a nylon-membrane filter after a denuder to remove HNO3, which captures both non-volatilized and volatilized NO3 −. Particulate NH4NO3 exists in equilibrium with gaseous HNO3 and ammonia (NH3) (Hering and Cass ) depending on temperature, pressure, and RH. During sampling, NO3 − can evaporate as HNO3 due to the pressure drop across the filter and be re-absorbed as volatilized NO3 −. However, volatilized NO3 − is not part of the gravimetric mass, resulting in a negative artifact, which is most prominent during summer. The uptake of water by sulfates, nitrates, and organics during weighing (at ∼40 % RH) counterbalances NO3 − volatilization from the Teflon-membrane filter (Chow et al. ).

Blank subtraction is applied to OCQF for IMPROVE samples but not for CSN samples (Chow et al.; Watson et al. ). For the period prior to 2007/2008, carbon analysis followed the STN_TOT protocol in CSN (thermal/optical transmittance; Peterson and Richards ) and the IMPROVE_TOR protocol in IMPROVE (thermal/optical reflectance; Chow et al. ). Although total carbon (TC = OC + EC) is comparable, STN_TOT reports higher OC and lower EC than the IMPROVE_A_TOR protocol (Chow et al. ). Malm et al. used collocated measurements in order to relate CSN to IMPROVE carbon concentrations using ordinary least squares (OLS; unweighted) regression:where “Other” is the sum of EC, geological minerals, and salt (DeBell et al., Eq. 9). The two regression coefficients, a1 and a2, should equal unity if SO4 = and NO3 − are present as (NH4)2SO4 and NH4NO3, respectively. Equation D assumes no water uptake at weighing equilibration conditions and no NH4NO3 evaporation during sampling. a3 is the OC multiplier (f) and a4 = 1 if the weighting factors for geological minerals and salt are correct. For 168 IMPROVE sites during 1988–2008, average a1, a2, a3, and a4 values were 1.12, 0.75, 1.60, and 1.06, respectively. This implies a 12 % contribution from water mass associated with (NH4)2SO4 during weighing, a net loss of 25 % NH4NO3 during sampling, and an OC multiplier of 1.6 with 6 % more EC, geological minerals, and salt. A higher a3 for OC was found during summer (f = 1.7) than winter (f = 1.42), with a lower a2 during summer showing more NH4NO3 evaporation, as expected.

Different regression analyses were conducted for 708 IMPROVE samples at the urban Fresno Supersite (Watson et al. ) from 2004 to 2010, as shown in Table 2. Ordinary weighted least squares (OWLS) regression takes into account the measurement uncertainty of the independent variable (i.e., PM2.5), while effective variance (EV) regression takes into account the uncertainties of both the independent and dependent variables and should provide the most realistic results. Table 2 shows that average PM2.5 NO3 − (3.9 ± 4.9 μg/m3) and OC (3.2 ± 2.5 μg/m3) were the major components, with 1.33 ± 1.26 μg/m3 for SO4 =. The average EC, geological minerals, and salt concentrations were 0.93, 1.42, and 0.27 μg/m3, respectively. Without accounting for measurement uncertainties, a large OLS a1 of 1.61 for SO4 = yields an increment (1.61–1.00 = 0.61) five times higher than the 0.12 increment (i.e., regression coefficient of 1.12) from Malm et al.—this is inconsistent with 30–40 % RH weighing conditions. The 8 % NO3 − volatilization (i.e., a2 = 0.92) and an OC multiplier (a3) of 1.67 in Table 2 seem reasonable for typical ion concentrations. The geological mineral mass is overestimated (a4 = 0.59) by the IMPROVE “soil” formula (Eq. C).

Table 2 shows a1 < 1 (0.90–0.93) by OWLS and EV regression methods, implying SO4 = is somewhat acidic in Fresno, which is probably not the case. NH3 is abundant in this agricultural region (e.g., Chow et al.,, ). The a2 of 0.85–0.88 is slightly lower than 0.92 in OLS, but it is consistent with NO3 − volatilization. The a3 is 2–4 % higher in OWLS (1.74) and EV (1.71) than OLS (1.67), but a4 (0.78) is ∼30 % higher than OLS (0.59). The high a1 and low a4 in the OLS regression are not realistic. However, the regressions in all cases are statistically significant and the squared multiple correlations (r 2) are 0.98 or 0.99. Hand et al. and Malm et al. provide insights into sampling and analytical artifacts in long-term PM2.5 networks. However, the example illustrated for Fresno indicates limitations on generalizing from a single dataset and one statistical approach.

Simon et al. (, Eq. 11) employed data screening procedures to eliminate suspect or physically unreasonable concentrations. Data sets with correlation coefficients (r) among explanatory variables greater than the absolute value of 0.85 were eliminated; whereas EC was removed due to correlations with OC. However, the effects of collinearity fell along a continuum, and selecting the level of correlation that can be tolerated is subjective. OLS regression was found to produce more bias in regression coefficients than OWLS or EV. Overall, the estimated median OC multipliers (a3) at the 50th percentile were lower for winter (f = 1.39) and fall (f = 1.59) and comparable between spring (f = 1.83) and summer (f = 1.81). The lowest median a3 (f = 1.29) was estimated at western sites during winter. Simon et al. concluded that more realistic and unbiased estimates of the OC multiplier were obtained using an “error in variables” regression and eliminating EC.

Major factors influencing mass reconstruction

The key factors affecting RM are examined for: (1) the OC multiplier (f); (2) sampling artifacts; (3) carbon analysis methods; (4) ammonium and nitrate volatilization; and (5) water uptake on Teflon-membrane filter deposits at different equilibration RHs.

Measurement of the OC multiplier (f) to estimate OM

Several aerosol extraction (a combination of water, organic solvents, and/or solid-phase extraction) and analytical methods (e.g., elemental analysis, Fourier-transform infrared (FTIR) spectroscopy, quadrupole-aerosol mass spectrometer (Q-AMS), etc.) have been applied to estimate the f multiplier (i.e., the OM/OC ratio). As shown in Table 3, the results from these direct measurements are variable with f = 1.27–2.2. Aircraft sampling with FTIR often yielded f = ∼1.3–1.4 (Gilardoni et al.; Maria et al.; Russell ) with a higher f multiplier (1.6–1.8) found by Takahama et al.. Lower f values (∼1.4) were also found for personal and indoor sampling (Reff et al. ), for ship emissions (∼1.6 by Gilardoni et al. ), and for urban areas (∼1.6 by Day et al.; Hawkins and Russell; Ruthenburg et al. ). Higher f values (∼2.0 to 2.2) were typically found for aged aerosols sampled in remote areas (e.g., Gilardoni et al.; Takahama et al. ).

Weighing samples before and after solvent extraction (Japar et al. ) resulted in f = 1.4 for diesel exhaust samples. In Pittsburgh, PA, Polidori et al. found that f increased with increasing polarity with f higher in summer (June and July) and winter (December and January) than in spring (March) and fall (October and November). High summer and winter values (f = 2.08–2.11) were attributed to biomass burning and residential wood combustion (RWC), respectively. Accounting for both solvent extractable and non-extractable material, the annual average f was estimated to be 2.05 ± 0.18.

Based on AMS measurements and multivariate analyses (e.g., principle component analysis (PCA), regression analysis, and positive matrix factorization (PMF)), Zhang et al. and Aiken et al reported average f = 1.7–1.8 with f = 1.2–1.3 for hydrocarbon-like organic aerosols (HOAs) and f = 1.9–2.5 for oxygenated OA (OOA). Aiken et al. also reported f = 1.6–1.7 for biomass burning OA (BBOA). Based on a series of field studies, Philip et al. parameterize OM/OC from AMS measurements using f = 1.3 for primary organic aerosol and f = 2.1 for OOA. The OM/OC ratio is determined as 1.3(f POA) + 2.1(1–f POA), where f POA is the primary organic aerosol (POA) fraction of the AMS data, a proxy for combustion emissions (derived from ambient NO2 measurements). The OM/OC ratios ranged from 1.7 to 2.1.

The f multiplier is expected to be higher in rural than in urban areas due to oxidation and/or addition of SOA during transport. However, the results in Table 3 do not show systematic variations. Organic compounds vary by location, season, and time of day. Site-specific f values need to be measured.

Sampling and analysis artifacts

Different approaches to sampling and analysis introduce uncertainties and systematic biases, including carbon sampling artifacts, thermally evolved carbon analysis methods, ammonium and nitrate volatilization, and particle-bound water on Teflon-membrane filters. The following subsections address these measurement uncertainties.

Carbon sampling artifacts and carbon analysis by thermal evolution

As noted, PM2.5 sampling onto quartz-fiber filters is accompanied by positive (e.g., VOC adsorption) and negative (e.g., volatilization during and after sample collection) OC artifacts (Chow et al.; Putaud et al.; Turpin et al.; Watson et al. ). Positive artifacts (e.g., estimated by field blank (OCFB), backup filter (OCQBQ), preceding organic denuders, and regression analyses) often exceed negative artifacts (ten Brink; Watson et al. ). OC artifacts may bias EC values by as much as ∼50 %, especially by TOT, as light attenuation due to charring of the adsorbed organics within the filter has greater influence than charring of the surface particle deposit in TOR (Chen et al.; Chow et al. ).

In a review of carbon comparison studies, Watson et al. found EC differed by up to a factor of seven (Schmidt et al. ) among 19 thermal evolution methods. Table 4 summarizes the three most widely applied thermal/optical carbon analysis protocols (i.e., IMPROVE_A_TOR, STN_TOT, and EUSAAR_2_TOT). The US long-term networks (e.g., IMPROVE and CSN) apply the IMPROVE_A_TOR protocol (USEPA ). The European Union EUSAAR-2 protocol (Cavalli et al.; Panteliadis et al. ) is similar to the IMPROVE_A temperature protocol with variations in selected temperature plateaus and shorter (70–180 s) residence times. Higher OC values in TOT can result in lower OM/OC ratios and might bias RM.

Ammonium and nitrate volatilization

Compared with total particulate NO3 −, Chow et al. found volatilized NO3 − losses ranging from <10 % during cold months to >80 % during warm months (from the front quartz-fiber filter) for urban and non-urban sites. The amount of NH4NO3 volatilization from the Teflon-membrane filter can be estimated by a thermodynamic model (Hering and Cass; Mozurkewich ), but this is only possible when gaseous HNO3 and NH3, total particle NO3 −, temperature, and RH are known (Chow et al.; Stelson et al. ). Volatilized NO3 − is not considered in the USEPA’s PM2.5 Federal Reference Method (FRM) for compliance monitoring. However, for evaluating light extinction or health effects, it is necessary to account for NO3 − volatilization during sampling.

Yu et al. noted that gaseous HNO3 interacts with nylon filters and retains HNO3 that volatilized from NH4NO3. However, losses of NH4 + (i.e., gaseous NH3) from nylon filters after a Na2CO3 denuder for the selected six IMPROVE sites ranged from 10 to 28 % (monthly average) during summer. Yu et al found that, for individual samples, the NH4 + losses spread between 1 and 65 %. NH4 + volatilization is enhanced by increasing temperature and RH, and with the fraction of total NHx (sum of NH3 and NH4 +) present as NH3 (Chen et al. ).

Losses of NH4 + after sampling need to be investigated. Non-volatilized NH4 + can be acquired on Teflon-membrane or quartz-fiber filters without preceding denuders. Ideally, both non-volatilized and volatilized NH4 + should be acquired on a parallel channel, using a preceding citric acid denuder to remove NH3, followed by a quartz-fiber filter with a citric acid impregnated cellulose-fiber backup filter (e.g., Chow; Chow et al. ).

Particle-bound water on the Teflon-membrane filter

The influence of particle-bound and particle-adsorbed water on PM has been explored in several studies (e.g., Frank; Malm et al.; Malm and Day; Perrino et al.; Rees et al.; Temesi et al. ). Water associated with PM was estimated by Harrison et al. by applying 1.29 to the sum of (NH4)2SO4 and NH4NO3 concentrations and in others (e.g., Murillo et al.; Siddique and Waheed ) by multiplying 0.32 to the sum of NH4 + and SO4 =.

Hygroscopic salts (e.g., (NH4)2SO4, NH4NO3, and NaCl) absorb water as a function of RH (Chan et al.; Tang and Munkelwitz ). At the deliquescence RH (DRH; ∼80 %), dry (NH4)2SO4 particles start to absorb water and the amount rises with increasing RH. The hydrated particle retains water below the DRH until it re-crystallizes at the efflorescence RH (ERH) of ∼30–40 %, the hysteresis effect (e.g., Han and Martin ). Acidic H2SO4 absorbs and desorbs water continuously with changes in RH, without exhibiting deliquescence or efflorescence. The DRH and ERH of pure NH4NO3 are 62 and 32 %, respectively. Tang et al. found that sea salt begins to deliquesce at low RH in the presence of Mg++ and Ca++, but that most of the material deliquesces between 70 and 74 %, the DRH of NaCl. Day et al. and Malm et al. found little evidence for deliquescence or efflorescence in ambient aerosols at the IMPROVE sites.

At RH >80 %, water may constitute more than 50 % of PM2.5 mass (Chen et al.; McMurry ). If particles were hydrated during sample collection, the sample filters may retain water for weighing (equilibration of RH 30–40 %; USEPA ), unless they were dried below ERH between sample collection and weighing. Based on theoretical thermaldynamic modeling of salt mixtures, Pilinis et al. found that aerosol may contain up to 30 % water for RH = ∼20–50 %. McInnes et al. observed that water associated with sea salt particles contributed 26 % of the mass at 40 % RH. Speer et al. measured changes in PM2.5 mass as a function of RH in a humidity-controlled chamber (increased from 4 to 94 % in 5 % increments and then decreased similarly to 12 %) using a beta attenuation monitor (BAM) on Teflon-membrane filters. For samples collected at Research Triangle Park, NC, Speer et al observed hysteresis in most cases.

The water-soluble organic carbon (WSOC) portion of OM can enhance or inhibit water absorption by inorganic salts (Facchini et al.; Mircea et al.; Saxena et al.; Saxena and Hildemann ). At Great Smoky Mountains National Park during the summer of 2006, Lowenthal et al. reported the water uptake as 5 % PM2.5 WSOC at 45 % RH and 33 % at 80 % RH. Based on thermodynamic modeling (Chen et al.; Clegg et al.; Tang and Munkelwitz ), ∼80 % of the measured water can be associated with SO4 = and NO3 −. Speer et al. attributed the ∼20 % “residual water” to organics; the amount of water per unit mass of organics was ∼50 % of that associated with (NH4)2SO4 (per unit mass) at 60–80 % RH. Conversely, Engelhart et al. determined that water growth of aerosols in Crete, Greece, was consistent with thermodynamic modeling based on inorganic constituents alone. Water mass on the Teflon-membrane filter can be determined by weighing the filter under equilibrium conditions (30–40 % RH), drying the filter completely in a desiccator, and then rapidly re-weighing.

Recent advances in thermodynamic models have incorporated some organic compounds to estimate the associated water activity (Clegg et al.,; Clegg and Seinfeld ). However, most of the organic species have not been identified, and their thermodynamic properties are uncertain (Saxena and Hildemann; Sempéré and Kawamura ). While thermodynamic modeling may provide insights on particle-bound water, the most straightforward means is through direct gravimetric analysis over a range of RHs.

Summary and conclusions

As PM2.5 mass concentration has been regulated in NAAQS to protect public health and welfare, it is important to understand the particle composition in order to: (1) examine the causes of elevated concentrations; (2) attribute ambient concentrations to air pollution sources; (3) relate toxic components to public health and ecosystems; and (4) associate particle scattering and absorption properties with visibility impairment, the Earth’s radiation balance, and climate change. With advances in sampling and analysis techniques, the demand for characterizing the chemical, physical, and optical properties of atmospheric aerosol is increasing worldwide. The validity of mass and chemical measurements needs to be examined prior to or in conjunction with air-quality modeling to develop pollution control strategies and reduce human exposure to hazardous pollutants.

Mass reconstruction is a simple and useful tool for validating the consistencies and addressing uncertainties among mass and chemical measurements. The reconstruction of measured mass was started by Countess et al. and Macias et al. as PM chemical speciation for ions, carbon, and elements became available. The 11 reconstructed mass (RM) equations examined here provide history and insight into the evolution of RM. Major PM components include: (1) major inorganic ions (e.g., SO4 =, NO3 −, and NH4 +); (2) OC and its multiplier (f) to estimate OM, (3) EC, (4) geological minerals (based on estimated metal oxides), (5) salt, (6) trace elements (excluding double counting of ions and crustal components in geological minerals), and (7) others (as remaining mass including particle-bound water). The remaining mass can be negative when RM overestimates the gravimetric mass.

For inorganic ions, either the sum of (NH4)2SO4 and NH4NO3 (calculated by their respective stoichiometric multiplier as 1.375SO4 and 1.29NO3 −) or the sum of SO4 =, NO3 −, and NH4 + is most commonly applied. For coastal environments, variations account for non-sea salt SO4 = (nssSO4), CaSO4, Na(NO3)2, and NH4Cl. The assumption that SO4 = is completely neutralized as (NH4)2SO4 overestimates SO4 = mass when non-neutralized (acidic) sulfates are present. Summing of SO4 =, NO3 −, and NH4 + will not account for H associated with partially neutralized SO4 = (e.g., NH4HSO4). Ion balances should be applied to ensure the molar equivalence between the measured anions and cations and to justify the degree of neutralization. NH4 + measurements should be included in routine monitoring networks and special studies, preferably on a quartz-fiber filter or with preceding citric acid denuder and citric acid impregnated backup filter that can capture both non-volatilized and volatilized NH4 +, respectively.

PM2.5 NH4NO3 may evaporate from Teflon-membrane and quartz-fiber filters during warm, non-winter periods, but its contribution to RM is expected to be highest during winter when low temperatures and high RH favor the particle phase. Ammonium and nitrate volatilization during sampling does not affect mass reconstruction. However, positive bias in RM is expected for CSN and the IMPROVE network where total particulate NO3 − measured on a nylon-membrane filter includes volatilized NO3 − that is not part of the gravimetric mass on Teflon-membrane filters. To account for this bias, gaseous HNO3 can be removed with a preceding denuder and volatilized NO3 − can be collected on a nylon filter or salt-impregnated filter behind one of the filters.

The OC multiplier (f) ranges from 1.2 to 2.6, depending on the extent of OM oxidation. The most commonly applied multipliers are 1.4 for urban and 1.8 for non-urban sites. The f multiplier is expected to be highest in non-urban areas due to oxidation and/or addition of secondary organic compounds during transport. Organic compounds vary by location, season, and time of day. Site-specific f values need to be measured. Future studies should focus on direct measurement of the OM/OC ratio at urban and remote locations with sampling periods covering warm and cold seasons.

Organic sampling artifacts need to be quantified using preceding carbon denuders, field blanks, and/or backup filters. Subtracting averaged field blanks from OC is the most convenient way to remove passive organic adsorption. Different thermal/optical carbon analysis protocols may result in additional uncertainties. The analysis protocol used in the CSN prior to 2007/2008 overestimated OC and consistently led to high-biased RM. Consistent carbon analysis protocol should be applied nationwide and internationally. Among the seven PM2.5 components, EC is the most straightforward as a single component without any multiplier. However, the abundance of EC is method dependent as OC and EC are operationally defined.

For geological minerals containing Al, Si, Ca, and Fe, compounds are assumed to be Al2O3, SiO2, CaO, and Fe2O3, respectively, with variations including or excluding FeO, K2O, and TiO2. The IMPROVE “soil” formula applies a factor of 1.16 to account for unmeasured compounds and tends to overestimate geological minerals. This can be examined empirically by measuring the chemical composition of local geological samples after subtracting OM and ionic concentrations. Since geological minerals are not a major component of PM2.5, variations in the assumptions regarding metal oxides or multipliers do not contribute to large variations in RM, but they are important for PM10–2.5 and PM10 RMs. Trace elements as a sum of remaining elements by XRF (excluding S and geological elements) or as complicated trace element oxides only account for a small fraction (0.5–1.6 %) of PM2.5 mass.

There is no standard method to estimate salt. It is mainly based on: (1) the sum of elements (excluding Cl and Cl−) to Na or Na+ ratio in seawater; (2) straight sum of Na+ and Cl−; or (3) estimated as 1.8Cl− as in the revised IMPROVE equation. Depletion of Cl− by reaction with sea salt particles with a strong acid (e.g., H2SO4 and HNO3) is difficult to estimate without additional measurement. However, the salt component should be accounted for at sampling sites near coastal areas, salt lakes, or desert playas, as it may comprise up to 20–30 % of PM2.5 mass.

Potential bias in measured mass due to the absorption of water by hygroscopic species on the Teflon-membrane filter from which PM2.5 mass is determined can be estimated theoretically from concentrations of water-soluble species measured on nylon-membrane or quartz-fiber filters using a thermodynamic model.

In conclusion, the principal sources of uncertainty are: (1) ammonium and nitrate volatilization and inconsistency between total particulate NO3 − on nylon-membrane filters and non-volatilized NO3 − on Teflon-membrane filters; (2) unknown OC multipliers (f) to estimate OM; (3) inaccurately accounting for OC sampling artifacts; (4) differences among OC and EC analytical protocols; (5) inaccurate conversion of crustal element concentrations to geological minerals; (6) various degrees of Cl− depletion at coastal locations; and (7) particle-bound water on the Teflon-membrane filter deposits. Reasonably accurate PM2.5 mass reconstruction can be accomplished by minimizing sampling artifacts and conducting comprehensive chemical analyses to ensure mass closure.

Below is the link to the electronic supplementary material.

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    Chow JC, Watson JG, Lowenthal DH, Hackney R, Magliano KL, Lehrman DE, Smith TB. Temporal variations of PM2.5, PM10, and gaseous precursors during the 1995 Integrated monitoring study in central California. J Air Waste Manage Assoc. 1999;49:PM16-PM24.

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    Chow JC, Watson JG, Edgerton SA, Vega E. Chemical composition of PM10 and PM2.5 in Mexico City during winter 1997. Sci Total Environ. 2002;287:177-201.

    Not in our library10.1016/s0048-9697(01)00982-2 (opens in a new tab)

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    Chow JC, Watson JG, Edgerton SA, Vega E, Ortiz E. Spatial differences in outdoor PM10 mass and aerosol composition in Mexico City. J Air Waste Manage Assoc. 2002;52:423-434.

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    Chow JC, Watson JG, Ashbaugh LL, Magliano KL. Similarities and differences in PM10 chemical source profiles for geological dust from the San Joaquin Valley, California. Atmos Environ. 2003;37:1317-1340.

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    Chow JC, Watson JG, Chen L-WA, Arnott WP, Moosmüller H, Fung KK. Equivalence of elemental carbon by thermal/optical reflectance and transmittance with different temperature protocols. Environ Sci Technol. 2004;38:4414-4422.

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    Chow JC, Watson JG, Lowenthal DH, Magliano KL. Loss of PM2.5 nitrate from filter samples in central California. J Air Waste Manage Assoc. 2005;55:1158-1168.

    Not in our library10.1080/10473289.2005.10464704 (opens in a new tab)

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    Chow JC, Watson JG, Lowenthal DH, Chen L-WA, Magliano KL. Particulate carbon measurements in California’s San Joaquin Valley. Chemosphere. 2006;62:337-348.

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    Chow JC, Chen L-WA, Watson JG, Lowenthal DH, Magliano KL, Turkiewicz K, Lehrman DE (2006b) PM2.5 chemical composition and spatiotemporal variability during the California Regional PM10/PM2.5 Air Quality Study (CRPAQS). J Geophys Res - Atmos 111:1–17

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    Chow JC, Watson JG, Feldman HJ, Nolan J, Wallerstein BR, Hidy GM, Lioy PJ, McKee HC, Mobley JD, Bauges K, Bachmann JD. 2007 critical review discussion - will the circle be unbroken: a history of the U.S. National ambient air quality standards. J Air Waste Manage Assoc. 2007;57:1151-1163.

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    Chow JC, Watson JG, Lowenthal DH, Chen L-WA, Zielinska B, Mazzoleni LR, Magliano KL. Evaluation of organic markers for chemical mass balance source apportionment at the Fresno supersite. Atmos Chem Phys. 2007;7:1741-1754.

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    Chow JC, Watson JG, Chen L-WA, Chang M-CO, Robinson NF, Trimble DL, Kohl SD. The IMPROVE_A temperature protocol for thermal/optical carbon analysis: maintaining consistency with a long-term database. J Air Waste Manage Assoc. 2007;57:1014-1023.

    Not in our library10.3155/1047-3289.57.9.1014 (opens in a new tab)

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    Chow JC, Watson JG, Chen L-WA, Rice J, Frank NH. Quantification of PM2.5 organic carbon sampling artifacts in US networks. Atmos Chem Phys. 2010;10:5223-5239.

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    Chow JC, Watson JG, Robles J, Wang XL, Chen L-WA, Trimble DL, Kohl SD, Tropp RJ, Fung KK. Quality assurance and quality control for thermal/optical analysis of aerosol samples for organic and elemental carbon. Anal Bioanal Chem. 2011;401:3141-3152.

    Not in our library10.1007/s00216-011-5103-3 (opens in a new tab)

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    Chow JC, Watson JG, Ruzer L, Harley NH. Chemical analyses of particle filter deposits. Aerosols handbook: measurement, dosimetry, and health effects. 2013;179-204.

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