Organic Geochemistry 33 (2002) 171–180
www.elsevier.com/locate/orggeochem
The application of electrospray ionization mass
spectrometry (ESI MS) to the structural characterization
of natural organic matter
Elizabeth B. Kujawinskia, Michael A. Freitasa,*, Xu Zanga,
Patrick G. Hatchera, Kari B. Green-Churchb, R. Benjamin Jonesb
a
Department of Chemistry, The Ohio State University, 100 W. 18th Avenue, Columbus, OH 43210, USA
b
Campus Chemical Instrumentation Center, The Ohio State University, Columbus, OH 43210, USA
Abstract
This report describes the application of electrospray ionization (ESI) mass spectrometry to the structural characterization of soil organic material, a critical component of environmental processes and the global carbon cycle. Quadrupole time-of-flight (QqTOF) mass spectrometry provided a routine screening of aqueous ions in humic and fulvic
acid mixtures and MS/MS capabilities for selected ions. Fourier transform ion cyclotron resonance (FT–ICR) mass
spectrometry required longer analysis time but achieved resolving powers > 80,000 and mass accuracies of < 1 ppm,
which allowed exact molecular formula determination for selected peaks. This technique represents a significant
advance in the identification of compounds within humic substances. # 2002 Published by Elsevier Science Ltd.
1. Introduction
Soil is a complex biogeochemical system that is a
component of numerous global processes (e.g. carbon
and nitrogen cycling, biological productivity, and erosion). The chemistry of organic matter in this system is
dependent on the interactions of biological material with
mineral substrates and refractory soil organic matter
(SOM) known as humic material. The inherent difficulties
in defining the structure of individual components of
humic material derive from the fact that they are macromolecular ( > 500 Daltons), polar in nature, and not
easily examined by instrumentation designed to provide
detailed chemical structures. Significant progress has
been made recently in the structural determination of
large biomolecules (e.g. proteins) using ‘‘soft’’ ionization
* Corresponding author. Tel.: +1-614-688-8432; fax: +1614-292-0559.
E-mail address: freitas@chemistry.ohio-state.edu
(M.A. Freitas).
techniques such as electrospray ionization (ESI). In ESI,
polar hydrophilic macromolecules are de-solvated and
charged prior to acceleration into mass spectrometers.
This approach appears promising for structural characterization of humic substances. Recent reports have
shown that humic substances can be ionized readily, but
the mass spectrometric data are very complex with
multiple peaks at every m/z (Novotny et al., 1995;
Fievre et al., 1997; McIntyre et al., 1997; Solouki et al.,
1999; Brown and Rice, 2000; Klaus et al., 2000; Persson
et al., 2000). Furthermore, insufficient resolution and
mass accuracy has limited the determination of exact
molecular formulas.
McIntyre et al. (1997) first demonstrated the application of ESI MS to the analysis of organic materials
found in drinking water. Fievre et al. (1997) used ESI
combined with an ultrahigh resolution Fourier transform ion cyclotron resonance (FT–ICR) mass spectrometer to evaluate the molecular weight distribution of
humic and fulvic acids isolated from the Suwannee
River, GA. However, the sheer complexity of the mixture
prevented Fievre et al. (1997) from obtaining ultrahigh
0146-6380/02/$ - see front matter # 2002 Published by Elsevier Science Ltd.
PII: S0146-6380(01)00149-8
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E.B. Kujawinski et al. / Organic Geochemistry 33 (2002) 171–180
resolution mass spectra. Nonetheless, they were able to
enhance the resolution by using high performance liquid
chromatography (HPLC) to separate fractions of the
humic and fulvic acids prior to analysis. In a more
recent study, Brown and Rice (2000) selectively isolated
narrow mass ranges of electrospray-generated positive
ions of humic acids with tandem FT–ICR MS to obtain
high resolving power. However, the reported resolution
was still insufficient to assign accurate molecular weights
and subsequently molecular formulas for the observed
ions. To date, there have been no studies of the structural characteristics of humic acids using a quadrupole
time-of-flight mass spectrometer.
Two mass analyzers are the focus of this manuscript,
a quadrupole time-of-flight mass spectrometer (QqTOF
MS) and the Fourier transform ion cyclotron resonance
mass spectrometer. Each mass analyzer was coupled to
an electrospray ionization source. The QqTOF MS
consists of two quadrupoles coupled to a time-of-flight
analyzer. For rapid screening analyses, the quadrupoles
are operated in RF mode, allowing all ions to pass into
the time-of-flight MS for analysis. The initial screening
analysis requires little time (15 min or less) and the mass
resolving power of 10,000 is sufficient to determine the
general mass distribution of compounds within each
sample. The resolution achieved is greater than that of
conventional triple quadrupole mass spectrometers. The
FT–ICR MS consists of an external ESI source coupled
to an ICR cell residing within a high magnetic field. Ions
are accumulated in an external hexapole prior to acceleration into the ICR cell. Analysis time is often a function of sample complexity, with hours required for high
resolution spectra for very complex mixtures. In general,
though, FT–ICR mass spectrometry has the ability to
achieve mass resolving powers > 100,000 routinely. MS/
MS can be performed with both techniques on selected
ions to elucidate exact molecular structure and formulas
of particular compounds.
The increased sensitivity and resolution of FT–ICR
MS are a result of the difference in detection methods
between the ICR cell and the time-of-flight analyzer. In
the time-of-flight analyzer, ions are directly detected
through their collision with the detector plate at the end
of the flight tube. In the ICR MS technique, ions are
indirectly measured by the detection of cyclotron frequencies of the ions within the cell. The cyclotron frequency of each ion is a function of both the m/z of the
ion and the magnetic field. Once a cyclotron frequency
spectrum is attained from the Fourier transform of the
time domain transient, it can be converted to a mass
spectrum via a simple algebraic equation.
The inherent differences in the ion physics between
the QqTOF analyzer and the ICR cell lead to different
limitations in the mass spectra. The flight tube in the
QqTOF has a wider mass range and constant mass
resolving power across a wide m/z range. However,
minor components of complex mixtures with low absolute
concentrations (e.g. high molecular weight material within
humic or fulvic acids) are difficult to observe due to insufficient resolution. Averaging a number of QqTOF scans
increases the signal-to-noise ratio of minor components
but not significantly.
Within the ICR cell, ions are confined inside a threedimensional ion trap in the ICR cell at very low pressure
( < 109 Torr) and at high magnetic field ( > 3 T). The
ion trap has a fixed volume and therefore has limited
capacity for charged species. If the number of ions
inside the cell increases beyond a certain limit, the performance of the instrument deteriorates (often called
‘‘space-charge’’ effects) (Marshall et al., 1998). To
obtain an ultrahigh resolution mass spectrum, the ion
number must remain low. During the analysis of complex mixtures, however, ion number increases rapidly as
the complexity of the sample increases. For humic acid
mixtures, the effect of ‘‘space charge’’ interactions
becomes significant due to the high ion number necessary
to observe a signal and as a result, only low-resolution
spectra have been obtained (Marshall et al., 1998). In
earlier reports, researchers attempted to reduce ‘‘space
charge’’ effects by (1) the isolation of a selected range of
ions prior to detection (Brown and Rice, 2000) and/or
(2) chromatographic separation of the components prior
to ionization and trapping (Fievre et al., 1997; Marshall
et al., 1998). However, both procedures insufficiently
reduced the ion number to the degree necessary to
obtain ultra-high resolution and separate the isobaric
ions present in the mass spectrum.
In this report, we have used ESI coupled with QqTOF
MS and high resolution FT–ICR MS to screen a series
of humic and fulvic acid samples. Several well-studied
humic substances were examined by electrospray ionization coupled to the QqTOF mass spectrometer to
demonstrate the applicability of the approach and to
show that significant changes in structural characteristics
are reflected in the ‘‘low-resolution’’ MS data obtained.
The FT–ICR MS achieved higher resolution and was
used to determine exact molecular formulas for mass
analyzed peaks for two select samples: a humic acid
extract of degraded wood (Hatcher, 1987) and dissolved
organic matter (DOM) from Suwannee River, GA
(Serkiz and Perdue, 1990).
2. Methods
2.1. Sample preparation
Five samples were examined in this study: humic
acids from a degraded wood sample from Mt. Rainier,
WA (Hatcher, 1987); DOM (primarily fulvic acids) from
Suwannee River, GA (Serkiz and Perdue, 1990); humic
and fulvic acid fractions from Armadale soil (Ogner and
E.B. Kujawinski et al. / Organic Geochemistry 33 (2002) 171–180
Schnitzer, 1971; Matsuda and Schnitzer, 1972); and humic
acids from a diluvial soil from Iwata, Japan (Matsuda and
Schnitzer, 1972; Hatcher et al., 1989). Samples were provided by E.M. Purdue (Georgia Institute of Technology,
Atlanta, GA—DOM) and M. Schnitzer (Agriculture
Canada, Ottawa, Ontario–Armadale and diluvial soils).
Each sample was obtained as dried, ash-free humic or
fulvic acids. Stock solutions were made by dissolving the
dried sample in either double-distilled water (Suwannee
River DOM) or pH 8 NH4OH to make solutions of 5 mg
ml1 (Suwannee River and Mt. Rainier) or 1 mg ml1
(Armadale and diluvial). Stock solutions were diluted with
methanol or isopropyl alcohol prior to mass analysis.
2.2. Instrument parameters: Qq-TOF MS
All experiments were performed on a Micromass QTofTM II (Micromass, Wythenshawe, UK) mass spectrometer equipped with an orthogonal electrospray
source (Z-spray) operated in positive ion mode. Polyalanine and alanine were used for mass calibration for
the 100–2000 m/z range. Humic and fulvic acids were
prepared in a 50:50 water: alcohol (methanol or isopropyl alcohol) solution and infused into the electrospray
source at a rate of 5–10 ml min1. Optimal ESI conditions were: capillary voltage=3 kV, source temperature= 110 C and cone voltage=60 V. The ESI gas was
nitrogen. The first quadrupole, Q1, was set to pass ions
from m/z 100–2000 and all ions transmitted into the
pusher region of the TOF analyzer were scanned over
m/z 100–3000 with a 1 s integration time. Data were
acquired in continuum mode until acceptable averaged
data were obtained (10–15 min).
2.3. Instrument parameters: FT–ICR MS
Two samples were chosen for further analysis by FT–
ICR mass spectrometry. Analyses were performed on
both a commercially available 7 T ESI FT–ICR mass
spectrometer model Apex II 7e (Bruker, Billerica, MA)
and a previously described 9.4 T ESI FT–ICR mass
spectrometer (Marshall and Guan, 1996). Both were
configured for external ion accumulation in the positive
ion mode. For the 7 T ESI FT–ICR mass spectrometer,
humic and fulvic acid samples were prepared in 25:75
water: methanol (1.25 mg ml1) and infused into a
tapered 50 mm i.d. fused silica micro-ESI needle at a rate
of 250 nl min1. Typical ESI conditions were: needle
voltage=2.4 kV and heated capillary temperature=
80 C. Ions were accumulated in a linear hexapole ion
trap for 1.1 s and then transferred to a 300 -Penning trap
(1.5 V trapping voltage) by electrostatic ion transfer
optics. Typical initial base pressure for the instrument was
91010 Torr. A MIDAS data station controlled all
experiments (Senko et al., 1996). Numerous scans (18,000–
19,000) were accumulated to reduce signal-to-noise ratios
173
and increase resolution. The time-domain ICR signal
was subjected to a baseline correction, Hanning apodization, and one zero fill before Fourier transform and
magnitude calculation.
For the 9.4 T FT–ICR mass spectrometer, humic acid
samples prepared in 50:50 water: methanol were infused
into a tapered 50 mm i.d. fused silica micro-ESI needle at
a rate of 300 nl min1 and a concentration of 0.5 mg
ml1 for Mt. Rainier humic acid and 2.5 mg ml1 for
Suwannee River DOM. Typical ESI conditions were:
needle voltage=2.5 kV and heated capillary current= 2.5
A. Ions were accumulated in a linear octapole ion trap
(operated at 1.8 MHz) for 10–30 s and then transferred to
a 400 -Penning trap (2 V trapping voltage) through a second
octapole ion guide (operated at 1.5 MHz). Typical initial
base pressure for the instrument was 71010 Torr. A
MIDAS data station controlled all experiments (Senko
et al., 1996). The time-domain ICR signal (average of
650 scans) was subjected to baseline correction followed
by Hanning apodization and one zero-fill before Fourier
transformation and magnitude calculation.
3. Results
All five samples were analyzed via ESI QqTOF MS
and two (Mt. Rainier humic acid and Suwannee River
DOM) were further analyzed using ESI FT–ICR MS.
We will focus first on the samples analyzed with both
mass analyzers to highlight the similarities and differences in the mass spectra generated by each technique.
The Mt. Rainier humic acid spectra from both ESI mass
analyzers are encouragingly similar (QqTOF MS in
Fig. 1 and FT–ICR MS in Figs. 2 and 3). Both spectra
are complex with peaks at almost every m/z. In the ESI
QqTOF spectrum (Fig. 1), peaks associated with low
molecular weight compounds dominate the vertical scale
due to high resolution and narrow peak width. Peaks at
higher molecular weight (> 600 m/z) are broader and
most likely represent more than one compound. While
the intense and visible signals at low m/z could be due to
contaminants or specific molecules of exact composition
present in significant but low amounts, the low-level
signals at every nominal mass sum together to account
for the majority of peak intensity throughout the mass
range.
The general distribution of compounds in the 7 T FT–
ICR mass spectrum (Fig. 2) is nearly identical to the ESI
Qq-TOF spectrum with the exception of the 100–200 m/z
range. The absence of peaks in this range in the FT–
ICR spectrum has been observed previously in our lab
and may be due to inefficient ion transfer and trapping
of low m/z species in the FT–ICR experiment. The mass
resolving power for low molecular weight compounds
was 80,000 (at 321 m/z) for the 7 T instrument after
18,000 scans. Higher resolution was achieved with the
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E.B. Kujawinski et al. / Organic Geochemistry 33 (2002) 171–180
Fig. 1. ESI QqTOF positive ion mass spectrum of the humic acid extract of a degraded wood sample from Mt. Rainier, WA. The
sample was prepared in 50:50 water: methanol at a concentration of 2.5 mg ml1. The spectrum represents the average of 300 scans.
Fig. 2. ESI FT–ICR positive ion mass spectrum of the humic acid extract of a degraded wood sample from Mt. Rainier, WA,
acquired on a 7 T FT–ICR MS. The sample was prepared in 25:75 water: methanol at a concentration of 1.25 mg ml1. The spectrum
represents the average of 18,000 scans. The inset is an expansion of the region around 321 m/z where the mass resolving power was
approximately 80,000.
E.B. Kujawinski et al. / Organic Geochemistry 33 (2002) 171–180
175
Fig. 3. Comparison of expanded spectra of Mt. Rainier humic acid. The ESI Qq-TOF spectrum (bottom) is an expansion of the 771–774 m/z
range from Fig. 1. The ESI FT-ICR spectrum (middle) was acquired on a 9.4 T FT–ICR MS and the mass resolving power in this region
was approximately 60,000. The top two mass spectra are further expansions of the FT–ICR spectrum. The resolution of peaks in these
regions was sufficient to allow the assignment of unique molecular formulas derived from proposed structures (values and errors in Table 1).
9.4 T instrument after 650 signal transients (mass resolving power in excess of 100,000 at 500 m/z). An important
characteristic of the spectra presented in Figs. 2 and 3 is
that they were obtained without ion isolation or prior
fractionation. Instead, we were able to achieve high resolution by reducing the number of ions trapped in the FT–
ICR cell and performing extensive signal averaging.
The enhanced resolution of the FT–ICR MS over the
QqTOF MS is evident when comparing small regions of
each spectrum (e.g. 771–774 m/z in Fig. 3). Broad peaks
present in the QqTOF mass spectrum are further
resolved into clusters of discrete compounds by the 9.4
T FT–ICR MS. With mass resolving power of 60,000 in
this region, all the species present in this mixture appear
to be fully resolved. Using polyethylene glycol with an
average molecular weight of 600 as an internal mass
calibrant, accurate molecular weights for all the species
observed in the mass spectrum were assigned with an
average mass accuracy better than 1 ppm. Exact molecular masses were calculated for a series of hypothetical
lignin oxidation products (specifically, oxidation of
pendant alcohols at the a and g carbons of lignin tetramer side chains) and compared to the experimentally
observed molecular weight for selected components in
the mixture (Table 1). Differences of approximately 1
ppm were considered to be positive identifications for
these selected compounds. Nitrogen was not included in
molecular formula determinations because the sample
was derived from nitrogen-free lignin.
The dissolved organic matter (DOM) sample from
Suwannee River, GA was also analyzed using the 7 T
FT–ICR MS (Fig. 4). This sample is comprised primarily of fulvic acids (Serkiz and Perdue, 1990). The
mass spectrum is significantly more complex than that
obtained for the humic acid sample from Mt. Rainier
and there are multiple peaks at every nominal mass.
Some of the peaks match those in the Mt. Rainier sample but a large fraction occur at higher mass defect,
suggesting a source of aliphatic compounds that is not
present in the Mt. Rainier humic acid.
Three other humic acid samples were examined with
the ESI QqTOF MS; the diluvial humic acid sample
from Iwata, Japan (Fig. 5) and the humic and fulvic
acid fractions from Armadale soil (Fig. 6). In all three
cases, the insets show solid-state 13C nuclear magnetic
resonance (NMR) data obtained by a ramp-CPMAS
method. The Armadale fulvic and humic acid mass
spectra are nearly identical with clusters of peaks in the
80–200, 300–400, and 550–800 m/z range. Sharp peaks
stand out prominently above a background of peaks at
virtually every nominal mass extending from the low
mass end of the scale to 3000 m/z. As observed in both
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E.B. Kujawinski et al. / Organic Geochemistry 33 (2002) 171–180
Table 1
Accurate and measured m/z values for compounds proposed in Fig. 3. Accurate mass values were calculated from elemental formulas
of each compound. The error on the measured m/z is expressed in terms of ppm
Proposed compound
+
C38H36O16Na
C39H40O15Na+
C40H44O14Na+
C36H30O18Na+
C37H34O17Na+
C38H38O16Na+
C39H42O15Na+
Accurate mass
Measured m/z
Error (ppm)
771.189260
771.226848
771.26302
773.13213
773.16948
773.205530
773.24216
771.190589
771.227443
771.2638
773.134421
773.169177
773.206002
773.242749
+1.7
+0.8
+1.0
+3.0
-0.4
+0.6
+0.8
the Mt. Rainier and Suwannee River samples, the
majority of peak intensity is contained within the broad
clusters at every nominal mass. To illustrate this, Fig. 5
shows an expanded region of the spectrum for the diluvial humic acid but identical characteristics were
observed in both Armadale spectra.
4. Discussion
4.1. General characteristics of ESI MS
Before discussing specific aspects of each mass spectrum, there are two general characteristics of ESI mass
spectra that merit reflection. The first important question
is whether the mass spectra accurately reflect the composition of the sample. Electrospray ionization ionizes
only polar compounds and the purely aliphatic fraction
within humic and fulvic acids will not be detected.
However, this fraction is a very minor component of
most humic acids (Anderson et al., 1989). Within the
polar fraction, combinations of particular functional
groups such as carboxylic acids, alcohols, and especially
amines, result in a wide range of ionization efficiencies.
The differences in ionization efficiencies will affect the
relative abundances of compounds within the spectrum
and limit the ability of the technique to obtain quantitative information. Until relative ionization efficiencies
are determined for humic-like compounds, ESI is best
suited for qualitative analyses.
Fig. 4. ESI FT–ICR positive ion mass spectrum of dissolved organic matter (DOM) from Suwannee River. The spectrum was
acquired in the same manner as that in Fig. 2.
E.B. Kujawinski et al. / Organic Geochemistry 33 (2002) 171–180
177
Fig. 5. ESI Qq-TOF positive ion mass spectrum of diluvial humic acids from Iwata, Japan. The full spectrum is shown in the top
panel. This sample was prepared in 50:50 water: methanol solution at a concentration of 1 mg ml1. The inset on the top panel is
solid-state 13C NMR data using ramp-CPMAS. The bottom panel represents a 16 vertical magnification of the full spectrum. An
expansion of the 332–344 m/z range is also presented.
The second question for general ESI MS is whether
the observed molecular weight range and distribution
are accurate. Numerous values for the molecular weight
range of humic substances have been determined using
size exclusion chromatography (SEC) (e.g. 1500–5000
amu (Chin et al., 1997); 800–18,000 amu (Muller et al.,
2000)). It has been noted, though, that molecular weight
determinations using SEC are difficult to interpret given
the range of values observed (de Nobili et al., 1989;
Swift, 1989). In addition, recent reports have suggested
that humic and fulvic acids may be aggregates of lower
molecular weight material instead of covalently-linked
macromolecules (MacCarthy and Rice, 1985; Piccolo
and Conte, 1999), consistent with the molecular weight
ranges observed in our mass spectra obtained from two
very different mass analyzers. Fragmentation of high
molecular weight material is one possible explanation
put forth for the relatively low molecular weight distribution observed in these mass spectra. Leenheer et al.
(2001) have suggested that compounds with high carboxylic acid content may be susceptible to fragmentation during electrospray ionization. However, because
ESI is regarded as a ‘‘soft’’ ionization technique, more
work with standards and fractionated samples is needed
to ascertain the extent to which this effect is affecting the
molecular weight distribution of the humic and fulvic
acids in natural samples.
4.2. Comparison of spectra for Mt. Rainier humic acid
The humic acid extract of a degraded wood sample
was chosen for detailed work because it is composed of
partially-humified lignin (de Montigny et al., 1993) and
is representative of degraded wood in forests of the
Northwest Pacific region. The ESI QqTOF MS enabled
us to determine quickly the general characteristics of the
compounds within the Mt. Rainier degraded wood
humic acids, such as molecular weight range and distribution, which were then confirmed with ultra-high
resolution ESI FT–ICR MS. The high-resolution mass
spectra in Figs. 2 and 3 provide sufficient resolving
power and mass accuracy to determine a unique formula weight and, in some cases, a unique structure. If
the mass region between 771 and 774 m/z is expanded to
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E.B. Kujawinski et al. / Organic Geochemistry 33 (2002) 171–180
Fig. 6. ESI Qq-TOF positive ion mass spectra of Armadale humic acids (top) and fulvic acids (bottom). The spectra were acquired in
the same manner as in Fig. 5. The insets for both spectra are the respective solid-state 13C NMR data using ramp-CPMAS.
examine the individual peaks (Fig. 3), we observe clusters of peaks at each nominal mass unit, as well as at
half mass units representing potentially doubly charged
species. These characteristics are observed throughout
the mass spectrum. By analyzing the clusters of ions at
each nominal mass and measuring their exact mass to a
precision of 1 ppm, we can calculate a molecular formula for each of the peaks (Table 1). The molecular
formulas shown in Fig. 3 were derived from formulas
for structures expected from degraded lignin; specifically, oxidation of pendant alcohols at the a and g carbons of lignin tetramer side chains. It is important to
note that the molecular formula is a sodium adduct, a
well known artifact of positive-ion electrospray ionization methods, especially when sodium hydroxide is used
during sample preparation.
We then compared the humic acids from Mt. Rainier
to DOM from Suwannee River. Lignin oxidation products would presumably exist in both samples since lignin should be a common source for both types of
organic matter. Thus, common peaks in both samples
could be presumed to derive from similar sources, e.g.
humified lignin. In addition, DOM should have a variety
of non-lignin sources which should be reflected in peaks
that appear only in the Suwannee River sample. Using
the high resolution achieved with the FT–ICR MS, we
compared selected m/z regions to determine the extent
of compound similarity in the two samples. For example, one can compare the insets of Figs. 2 and 4 which
show the expanded region around 321 m/z. Mt. Rainier
humic acid has two peaks in this region whereas the
Suwannee River DOM has at least five peaks and at
least three of them could be due to non-lignin sources.
Using FT–ICR MS, we can now compare humic or fulvic acid samples on a molecular level and correlate these
differences to changes in space and time. Combining this
work with nuclear magnetic resonance and wet chemical
degradation studies will allow us to propose molecular
formulas that are consistent with all three data sets and
approach a true picture of the structure of complex
humic material.
We have not been able to determine the cause for the
discrepancy between the two spectra in the low (100–
200) m/z range. Although this region is susceptible to
background contamination on both instruments, proper
control experiments have not been performed to ascertain
E.B. Kujawinski et al. / Organic Geochemistry 33 (2002) 171–180
the degree to which background peaks appear in this
region. In addition, QqTOF spectra for analyses of the
Armadale and diluvial samples did not contain these
peaks (Figs. 5 and 6), suggesting that low molecular
weight peaks in the Mt. Rainier spectrum reflect actual
compounds within the sample. While it is possible that
the FT–ICR MS is unable to detect these low molecular
weight compounds due to mass discrimination, standard
peaks have been observed in this m/z range. In addition,
we have not yet optimized the ICR cell for detection of
low molecular weight compounds.
4.3. Comparison of QqTOF mass spectra of different
humic and fulvic acids
The QqTOF mass spectra obtained for the diluvial
humic acid (Fig. 5) and the Armadale humic and fulvic
acids (Fig. 6) were compared with one another as well as
with the solid-state 13C NMR data for each sample. The
NMR data indicate that the Armadale humic substances
are rich in aliphatic structures with a low abundance of
aromatic compounds. The fulvic acid is more aromatic
than the humic acid and also contains increased abundance of carboxyl and carbonyl carbons. In contrast, the
diluvial humic acids are predominantly aromatic carboxylic acid-like structures; specifically, carbon-linked
benzene-polycarboxylic acids (Hatcher et al., 1989).
The ESI QqTOF mass spectra reflect the differences
and similarities in the two sample sets predicted by the
NMR spectra. In both Armadale spectra (Fig. 5), sharp
peaks dominate a background of broad peaks at virtually every nominal mass throughout the range analyzed (80–3000 m/z). These sharp peaks are most likely
due to discrete molecules such as fatty acids (consistent
with data in Schnitzer and Nayroud, 1975). Fatty acids
are recognized easily due to their high mass discrimination that separates them from the clustered masses. The
other peaks at each nominal mass are multiplets due to
a mixture of various structures with the same nominal
but slightly different exact masses. The clusters occur at
every nominal mass with little or no signals at fractional
masses, indicating that the ions are singly charged. At
high masses, additional clusters grow in at fractional
masses, indicating the presence of doubly charged ions,
whose probability increases with increasing mass. It is
noteworthy that the intense signals for the two Armadale samples are virtually identical, as anticipated for
samples from the same soil. This indicates similarity in
the molecular constituents attributed to the intense
peaks. It is possible that some of these peaks are derived
from contaminants in the tubing lines to the electrospray unit. However, these peaks are not observed in the
humic acids from the diluvial soil, except for those at
292 and 394 m/z.
An observation worthy of mention is the exact mass
for each cluster, especially in the case of the diluvial
179
humic acids. The clustered masses do not have a significant mass discrimination, usually centered at about
0.1 to 0.2 amu above the nominal mass. This indicates
that structures assigned to these ions are generally
hydrogen poor compared with structures containing
long-alkyl substituents. Oxygen atoms with a negative
mass discrimination and the paucity of hydrogens associated with condensed aromatic rings could explain the
low mass discriminations observed for the clusters.
While a great deal more information can be gleaned
from the QqTOF data set, more experiments are necessary to identify and eliminate possible contamination. In
addition, instrument parameters require further optimization to provide a more quantitative representation of
the various structures present in humic substances. The
data can only be regarded as qualitative at the moment,
due largely to the fact that little is known of the ionization efficiencies and relative detection for various structures. At the very least, the QqTOF MS technique
provides us with a rapid means of examining qualitative
differences among various humic substances prior to
detailed studies by FT–ICR MS where exact formula
weights can be discerned.
5. Conclusions
The combined techniques of ESI QqTOF MS and
ESI FT–ICR MS represent an advance in the study of
the structural characterization of natural organic matter. While the samples employed in our study were
composed primarily of humic and fulvic acids, other
organic matter samples can be studied using these techniques by simply altering instrument conditions. The
simultaneous use of ESI MS with other structural characterization methods such as high-resolution multidimensional NMR will provide the basis for constructing
possible structures whose exact formula weights can be
calculated and compared to observed peaks in highresolution mass spectra. Furthermore, the characterization of relatively simple humic and fulvic acid fractions
may allow us to rapidly identify components in more
complex samples based solely on species mass. It is our
firm belief that the unique advantages offered by ESI
QqTOF MS and ESI FT–ICR MS open the door to
detailed molecular characterizations of natural organic
matter that have eluded many previous studies.
Acknowledgements
This study was funded by the National Science Foundation (OCE-98-96239, DEB-99-04047) and startup
funds from Ohio State University. The authors thank the
Campus Chemical Instrumentation Center for use of the
Micromass Q-TofTM II mass spectrometer which was
180
E.B. Kujawinski et al. / Organic Geochemistry 33 (2002) 171–180
funded by the Hayes Investment Fund. The authors
would like to acknowledge Alan G. Marshall (National
High Magnetic Field Laboratory, Tallahassee Florida)
for allowing us access to the 9.4 T FT–ICR at the
National High Field FT–ICR Facility (CHE-94-13008,
CHE-93-22824). The manuscript was improved by the
constructive comments of two anonymous reviewers.
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