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Analytical techniques for boron quantification supporting desalination processes:A review
Ali Farhat, Farrukh Ahmad, Hassan Arafat
Water and Environmental Engineering Program, Masdar Institute of Science and Technology, PO Box 54224, Abu Dhabi, United Arab Emirates
a b s t r a c ta r t i c l e i n f o
Article history:
Received 27 October 2011
Accepted 24 December 2011Available online xxxx
Keywords:
Boron
Analytical techniques
Desalination
ICP-MS
Isotopic analysis
Severalstudies have been reported overthe last twodecades to improve theanalysisof boron andto determineits
isotopic composition. The isotopic composition of boron is of significance to SWRObecause second pass processes
resultin a boron isotopic shift in thepermeate, thereby creating a unique process signature. This paper reviews the
different boron detection and quantification techniques ranging fromplasma-based techniques,to thermal ioniza-
tion mass spectrometry (TIMS), andotherMS-basedand non-MSbasedtechniques. Themost recent precisionand
detection levels are reported, and the complexity of analysis and sample preparation, as well as the major disad-
vantages and limitations associated with the measurements of boron and its isotopic composition (e.g., spectral
and isobaric interferences, mass fractionation, and memory effect) are compared among analysis techniques.
While positive-TIMS (PTIMS) has been reported as the most precise, and the negative-TIMS (NTIMS) as the
most sensitive, plasma-based techniques such as multi-collector inductively coupled plasma-mass spectrometry
(MC-ICP-MS) are characterized by their fast speed of analysis and high sample throughput. Several recent
improvements have increased precision and lowered the detection level of the MC-ICP-MS, making it capable of
competing with PTIMS and NTIMS.
2011 Elsevier B.V. All rights reserved.
Contents
1. Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
1.1. Boron: its occurrence and toxicity . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
1.2. Boron removal in desalination plants . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2. Techniques for boron and boron isotopes analysis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2.1. Available techniques and their principles of operation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2.1.1. Plasma-based techniques . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2 .1.2. Thermal ionization mass spe ctrome try (TIMS)-based te chnique s . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2.1.3. Non-MS-based techniques . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2.2. Precision and detection limits . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2.3. Complexity of operation and sample preparation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2.4. Compliance with regulatory levels . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2.5. Interferences and limitations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2.5.1. Spectral and isobaric interferences . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2.5.2. Mass fractionation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2.5.3. Memory effect . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
2.5.4. Other limitations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 03. Boron isotope tracer analysis in applications related to desalination . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
4. Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0
1. Introduction
1.1. Boron: its occurrence and toxicity
Boron is a nonmetallic element, which has five protons in its nu-
cleus along with five to six neutrons, resulting in two stable isotope
Desalination xxx (2012) xxxxxx
Corresponding author.
E-mail address:[email protected](H. Arafat).
DES-11194; No of Pages 9
0011-9164/$ see front matter 2011 Elsevier B.V. All rights reserved.
doi:10.1016/j.desal.2011.12.020
Contents lists available at SciVerse ScienceDirect
Desalination
j o u r n a l h o m e p a g e : w w w . e l s e v i e r . c o m / l o c a t e / d e s a l
Please cite this article as: A. Farhat, et al., Analytical techniques for boron quantification supporting desalination processes: A review, Desalination(2012), doi:10.1016/j.desal.2011.12.020
http://dx.doi.org/10.1016/j.desal.2011.12.020http://dx.doi.org/10.1016/j.desal.2011.12.020http://dx.doi.org/10.1016/j.desal.2011.12.020mailto:[email protected]://dx.doi.org/10.1016/j.desal.2011.12.020http://www.sciencedirect.com/science/journal/00119164http://dx.doi.org/10.1016/j.desal.2011.12.020http://dx.doi.org/10.1016/j.desal.2011.12.020http://www.sciencedirect.com/science/journal/00119164http://dx.doi.org/10.1016/j.desal.2011.12.020mailto:[email protected]://dx.doi.org/10.1016/j.desal.2011.12.0208/10/2019 Analytical Techniques for Boron Quantification Supporting Desalination Processes-libre
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forms: 10B (abundance of 19.8%) and 11B (abundance of 80.2%), aver-
aging its atomic weight at 10.81 Da[1]. Boron exists in nature in the
form of boric acid (H3BO3) or borates, mainly sodium borate (Na2B4-O710H2O), also known as borax. Boric acid and sodium borates are
considered to be medicinally important compounds and they are clas-
sified by the United States Pharmacopeia-National Formulary[2]and
the British Pharmacopeia [3] as two pharmaceutical necessities,
where they are used as antibacterial[4]and antifungal agents[57],
as well as components of dental cement [8]. Despite the fact thatboron exists in fertilizers, where it is described as an essential constit-
uent for the growth of plants and vegetation, boron contamination is
a serious threat to crops, because they are very sensitive to high levels
of boron in the irrigation waters [9]. In animals, high boron concen-
trations have been observed to affect male reproductive capabilities
[10], unlike in humans where no such negative findings have been
reported[11].
Boron is detected in surface water and groundwater in various lo-
cations around the world, including sea and river waters, where it is
present mainly in the form of boric acid. In seawater, the boron con-
centration ranges from 0.5 to 9.6 ppm [12], averaging at a value of
4.5 ppm[13,14]to 4.6 ppm[1]. Geographical location and seasonal
effects play a significant role in the boron concentration in the oceans
and seas. Boron levels in the Arabian Gulf have been reported at
7 ppm [14]. In freshwater, concentrations of boron have been
reported ranging from b0.01 to 1.5 ppm [1] in most cases. For in-
stance, boron levels measured in many US and Canadian surface
water bodies range from 0.01 to 0.4 mg/L, and in UK and Italy river
waters reach 0.9 mg/L. Meanwhile, studies measuring boron levels
in potable water supplies in northern Chile report values from
0.31 mg/L to 15.2 mg/L due to nearby boron-containing soil deposits
[15]. In brackish water, boron levels are generally lower than 5 ppm.
Yet, concentrations might get as high as 23.5 ppm, as in the case
reported by Rahardianto et al. [16].Hence, the geographic source of
water is the major determinant of these widely variable levels of
boron in the drinking waters.
The 4.5 ppm mean boron level in ocean waters is higher than the
USEPA Health Advisory Committee's maximum boron concentration
of 0.6 ppm in drinking water[17]. In the same vein, the World HealthOrganization (WHO, 2004) recommends a stricter goal for the boron
concentration. WHO defines the guideline value of boron concentra-
tion in drinking water as 0.5 ppm with the non-observed adverse ef-
fect level (NOAEL) of boron in drinking water at 0.3 mg/L[18].In this
recommendation, WHO considered the maximum tolerable intake in
one day as 0.16 mg of boron per kg body weight [13]. The WHO
guideline value of 0.5 ppm is provisional owing to the lack of detailed
toxicological studies on boron. Thus, it is not a mandatory water qual-
ity parameter in the US and it is not yet enforced in the Safe Drinking
Water Act, despite the fact the Boron is classified as a U.S. EPA's
Drinking Water Contaminant Candidate[1]. In the US, only the state
of California issued a regulation with a notification level of Boron ex-
ceeding 1 ppm, the same value adopted by the European Union (EU)
[19]. Thus, countries relying on seawater desalination must reducethe high levels of boron in seawater to below 0.6 ppm before any
water usage by humans and animals, as well as any usage for crop
irrigation.
1.2. Boron removal in desalination plants
In thermal desalination processes, such as Multi-Stage Flash Desali-
nation (MSF) and Multi-Effect Desalination (MED), where the product
water is reported with Total Dissolved Solids (TDS) values between
5 ppm and 50 ppm[20], the boron problem has never been reported.
The boron problem is exclusively reported in membrane technologies
[21,22], where the membrane rejects most ionic species but fails to pre-
vent the boron from passing through because it is present in its un-
charged boric acid form (pKa=9.2 at 25 C[23]). Thus, boron removal
is gaining significant attention in membrane desalination where several
specialized boron removal processes and plant configurations have
been tested. Plant configurations evaluated include those using a
second-pass Reverse Osmosis (RO)unit following pH increase to values
above the boric acid pKa[24,25], as well as the ones employing a post-
RO ion-exchange process with boron-specific resins [26]. Non-RO plant
configurations evaluated for boron removal include electrodialysis de-
salination using specialized membranes [27] and adsorption membrane
filtration (AMF) [28]. Readers interested in boron removal technologiesfrom saline water are referred to a recently published detailed review
on this topic[28].
The analysis of boron in feed waters and desalinated waters is of
crucial importance to assessing the effectiveness of boron removal
in desalination. Consequently, this requires the availability of robust
instrumental techniques and analytical methods for monitoring
and quantifying boron and its isotopic composition with significant
sensitivity, precision, as well as convenience.This paper reviews the dif-
ferent contemporary boron measurement and instrumentation tech-
niques, which include plasma-based techniques, thermal ionization
mass spectrometry (TIMS), and other MS-based and non-MS based
techniques. A comparison of the precision, detection levels, complexity
of operation, sample preparation, and major limitations and interfer-
ences among these analytical techniques is detailed. Moreover, the
paper explores boron isotopic ratio analysis as an emerging technique
for evaluating the performance of membrane-based boron removal
processes, and the mixing of waters containing different isotopic ratios
of boron in cases such as aquifer recharge and brine discharge.
2. Techniques for boron and boron isotopes analysis
2.1. Available techniques and their principles of operation
The detection and quantification of boron and its stable isotopes
have been conducted using several different techniques reported in
literature. These techniques are summarized in Table 1. The most
widespread of these are plasma-based techniques, mainly the induc-
tively coupled plasma (ICP) technique[29
39], which has recentlybeen coupled to different types of mass spectrometers (MS) to im-
prove method sensitivity and reliability. Positive thermal ionization
mass spectrometry (PTIMS)[4050]is recognized as the most precise
technique, whereas negative thermal ionization MS (NTIMS)[5160]
is reported for being the most sensitive one. Other non-MS-based
Table 1
Principle of the major boron analyses techniques.
Technique Principle of the technique
Plasma-
based
ICP-OES Ionizing boron into B+ ions then monitors
the wavelength emissions from these excited
ions at its corresponding wavelengths
ICP-MS Ionizing boron into B+ ions, then measuring
B isotopes abundance based on theirmass-to-charge ratio (m/z 10 and 11)
TIMS PTIMS Converting boron into alkali or metal
metaborate cations such as Na2BO2+
(m/z 88 and 89), and Cs2BO2+ (m/z 308
and 309) then measuring their
corresponding m/z
NTI MS Conver ting b or on int o metab or at e anions
of BO2 (m/z 42 and 43) then measuring
their corresponding m/z
Non-MS-
based
Spectrophotometry Adding specific reagents to the boron
samples for color development, then
measuring the absorbance at
wavelengths, respective of the reagent
Nuclear Bombarding boron with neutrons causing
the production of a-particles and g-particles
that are monitored to measure 10B isotope
abundance
2 A. Farhat et al. / Desalination xxx (2012) xxxxxx
Please cite this article as: A. Farhat, et al., Analyticaltechniques for boron quantification supporting desalination processes: A review, Desalination(2012), doi:10.1016/j.desal.2011.12.020
http://dx.doi.org/10.1016/j.desal.2011.12.020http://dx.doi.org/10.1016/j.desal.2011.12.0208/10/2019 Analytical Techniques for Boron Quantification Supporting Desalination Processes-libre
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techniques [6165], such as spectrophotometry, are also employed
for boron analysis.
2.1.1. Plasma-based techniques
Plasma is a state of matter similar to gas, described to be an elec-
trically conducting gaseous mixture that is ionized into cations, an-
ions, and electrons with a net charge of zero [66]. Inductively
coupled plasma (ICP) technique is the most widely used plasma-
based techniques for boron analysis. ICP is a type of plasma source
formed from electric currents that are caused by electromagnetic in-
duction on a rarefied gas such as Argon. Samples are usually prepared
in aqueous phase using steps involving extraction and purification,
and are then introduced into the plasma of the instrument via a neb-
ulizer and spray chamber [67]. The nebulizer is responsible for the
aerosolization of the aqueous sample into fine droplets. However,
since any large droplets formed cannot be further dissociated by the
plasma discharge, a spray chamber is utilized to permit the entrance
of only small droplets into the plasma torch. Other plasma-basedtechniques besides ICP, include direct current plasma (DCP) [68,69],
which is less sensitive and requires more maintenance compared to
ICP, as well as microwave induced plasma (MIP)[70]and glow dis-
charge plasma (GDP)[71], which are less commercially available for
general elemental analysis and not widely reported for boron
analysis.
In the ICP method, the boron-containing liquid sample is purified
and pre-concentrated, then atomized (i.e. converting boric acids and
other borates into elemental boron (B)), and ionized into B+, which
is analyzed via different types of detectors. The ICP optical emission
spectroscopy (ICP-OES), also known as ICP atomic emission spectros-
copy (ICP-AES), is one type of ICP that detects boron and was pub-
lished as standard method ISO 11885:1996 (E) [72]. This type of
emission spectroscopy detects electromagnetic radiation emitted
from excited atoms and ions produced by the plasma source, where
the wavelength of the radiation emitted is characteristic of an ele-
ment. The wavelengths typically monitored for the boron analysisare 249.678 nm, 249.773 nm [59], and 182.52 nm[73]. This method
was reported for aqueous samples including fresh and saline water
[31,45], as well as solid samples[40,59] including soil, rocks, plant,
and biological samples. The coupling of ICP with a mass spectral de-
tector (ICP-MS), introduced by Gregoire [39], revolutionized the
boron determination with its simultaneous measurement of boron
concentration and its isotope abundance (11B and 10B) leading to
lower detection limits and higher sensitivity[67]. Instead of monitor-
ing wavelength-specific emissions of the excited ions as in ICP-OES,
the ICP-MS method measures the ions based on their mass-to-
charge ratio (m/z), thus simultaneously measuring boron concentra-
tion and its stable isotope abundance.
Configurations involving different types of MS have been developed
to enhance the performance of the ICP-MS instrumental analysis tech-
nique. One configuration comprises of combining ICP with a quadruple
MS (ICP-qMS) [38], where the qMS provides higher precision than nor-
mal MS. Others include double-focusing magnetic sector ICP-MS, also
referred to as high resolution ICP-MS[34], which reduces the effect of
interferences induced from any mass overlaps, but is complex to oper-
ate and maintain and requires a higher capital cost compared to the
ICP-qMS. The configuration utilizing a multi collector MS, known as
multi-collector ICP-MS (MC-ICP-MS) [33], is described as the most
promisingICP-MS technique combining the advantages of superior ion-
ization of ICP with the precision of a double focusing magnetic sector
mass spectrometer with multiple Faraday cups and ion counters[30].
MC-ICP-MS (Fig. 1) overweighs other ICP configurations by its preci-
sion, sensitivity and ability to analyze a broader range of elements. Re-
cently, Le Roux et al. [29] and Fietzke et al. [32]used the multiple-
multiplier laser-ablation ICP-MS (MM-LA-ICP-MS) and laser-ablationMC-ICP-MS (LA-MC-ICP-MS), respectively, for in-situ boron isotope
analysis, but these techniques were primarily used for solid samples.
In fact, the different ICP-MS instruments for boron measurement have
been applied to samples ranging from surface and ground water
[3436]to volcanic fluids[74], marine carbonates [75,76], and other
geological materials[39].
The ICP techniques are characterized by their fast analyses and
high sample throughput[30,76,77] compared to thermal ionization
MS techniques. In fact, MC-ICP-MS is the most preferred among the
plasma-based technologies due to its high precision and the relatively
small sample size requirements[35,36], allowing it to potentially
compete with the very precise positive thermal ionization mass spec-
trometry (PTIMS) and the sensitive negative TIMS (NTIMS) boron
analysis techniques [76], albeit at a significant capital investmentcost.
2.1.2. Thermal ionization mass spectrometry (TIMS)-based techniques
Positive TIMS (PTIMS): PTIMS, which is considered to be the most
precise instrumental analysis technique for measuring boron isotopic
ratios [78], is an MS detection technique working in positive ionmode
to analyze for boron ions generated by a thermal ionization source
(Fig. 2). In PTIMS, the boron in the sample is converted into positively
charged metaborate ions (BO2+) that are not solely present as BO2
+,
but exist in the form of alkali or metal metaborate cations (M2BO2+)
[44,79,80].In fact, this technique requires boron separation from the
sample and this step should be preceded by offline sample prepara-
tion. Subsequent to the separation, an alkali salt (carbonate or hy-
droxide) is added to form the alkali or metal metaborate complex,
Fig. 1. Schematic drawing of MC-ICPMS with its different components: plasma torch,
electrostatic analyzer (ESA), magnet, and the multi-collector.
Fig. 2.Schematic drawing the thermal ionization source of PTIMS.
3A. Farhat et al. / Desalination xxx (2012) xxxxxx
Please cite this article as: A. Farhat, et al., Analytical techniques for boron quantification supporting desalination processes: A review, Desalination(2012), doi:10.1016/j.desal.2011.12.020
http://dx.doi.org/10.1016/j.desal.2011.12.020http://dx.doi.org/10.1016/j.desal.2011.12.0208/10/2019 Analytical Techniques for Boron Quantification Supporting Desalination Processes-libre
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which is then thermally ionized before being introduced into the
mass spectrometer for m/z filtering and measurement [67,81].The
various types of alkali metaborate ions analyzed depend on the alkali
salt used in preparing them. Such alkali or metallic metaborate ions
reported in literature include K2BO2+ [77], Na2BO2
+ [79,80,82,83],
Cs2BO2+ [4145,78,8486], Rb2BO2
+ [87], and Li2BO2+ [88]. PTIMS is
different from ICP-MS because it analyzes boron in the form of
M2BO2+, rather than an elemental form of boron (B+) as analyzed
by ICP-MS[34]. Initially, sodium metaborate (Na2BO2+
of m/z 88 and89) was widely used; in fact, two National Institute of Standards
and Technology (NIST) standards, SRM951 and SRM952, were both
certified via monitoring Na2BO2+ in PTIMS[89]. The same is true for
the Central Bureau for Nuclear Measurement (CBNM) standard of
boric acid [90]. However, Na2BO2+ has since been substituted by
Cs2BO2+ (of m/z 308 and 309)[4144]because the latter is more pre-
cise and sensitive compared to Na2BO2+, K2BO2
+, and Rb2BO2+, all of
which suffer from spectral interferences[67,77,81]. The PTIMS instru-
mental technique has been applied to aqueous samples[44](includ-
ing seawater[63], groundwater[47,82], and volcanic thermal water
[45]), geological samples [45,51,55,91], as well as crop plants [85]
and nuclear materials[83].
Negative TIMS (NTIMS): NTIMS operates in a similar way to PTIMS
but produces and analyzes for metaborate anions (BO2) in a negative
ion mode of operation. At variance with PTIMS, NTIMS requires no al-
kali salts or metals to be added to the sample as no alkali or metal
metaborate anions are required for mass measurement. Thus, simpler
mass measurements are conducted for 10BO2 and 11BO2
, at m/z of 42
and 43, respectively. Developed by Zeininger and Heumann[91]and
Duchateau and De Bievre[92], this technique is characterized by an
ion yield that is 1000 times higher than yields in PTIMS, leading to
higher sensitivity and less sample purification requirements [77].
Barth[55,56]reported a boron isotopic analysis of fresh and saline
water using NTIMS. Furthermore, Barth [57], along with other re-
searchers[52,60], used NTIMS to investigate boron in groundwater
as a tracer, showing that NTIMS is more suitable for aqueous samples
when precision is not of significance. Other applications of NTIMS
were reported on solid carbonate samples[51,53,58,93], and air sam-
ples[54].
2.1.3. Non-MS-based techniques
Spectrophotometric methods for boron determination are simply
based on the addition of specific reagents to aqueous samples for
the development of colored boron complexes, which are then mea-
sured using light absorbance at wavelengths corresponding to the
chromophore of the reagent used. These reagents include the red cur-
cumin, measuring its absorbance at 550 nm [94], blue carmine at
605 nm[95], and yellow azomethine-H at 410 nm[96]. USEPA Meth-
od 212.3, ASTM Method D3082-03 and AWWA Method 4500-B B are
published standardized methods for boron analysis using the curcu-
min [97], while AWWA Method 4500-B C and ISO 9390:1990 [98]
are for carmine and azomethine-H respectively. Azomethine-H meth-
od is the most commonly employed boron spectrophotometric method,mainly because it is fast, simple, sensitive, andreported to have the least
interferences among all spectrophotometric methods [67]. This method
has been employed to investigate boron geochemistry in groundwater
[47], seawater [61,63], and geothermal waters [64]. In addition, the
curcumin colorimetric method forms the basis of the American Society
of Testing and Materials (ASTM) method D3082 and Standard Methods
4500-B, which measure boron dissolved in aqueous samples. Thecurcu-
min method is prone to interferences from nitrate ions and hardness
constituents, even though it can detect boron concentrations as low as
0.1 mg/L or at minimum loading of 0.2 g boron [99]. Furthermore,
other spectrophotometric methods such as the fluorimetric methods
are also available to measure thefluorescence of samples after the addi-
tion of reagents that cause the formation of fl
uorescent boroncompounds.
Non-spectrophotometric methods include the ionometric method,
where boron in the sample is converted into tetrafluoroborate (BF4)
which is then measured viaselective ion selectiveelectrode. In addition,
boron analysis is of interest in nuclear industry, where boric acid is used
in the primary coolant to control the nuclear reaction, and high boron
concentrations might cause metal oxides to deposit on the fuel rods
[100]. In order to monitorthe boron concentration,several nuclear reac-
tion analytical (NRA) methods were reported as powerful independent
measurement technique that can be employed at nuclear reactor sites
withminimal sample preparation. Boron samplesin nuclear techniques
are bombardedwith neutrons causing theproduction of-particles and-particles, oneor bothof which aremonitoredto correlate to 10B stable
isotope abundance.
2.2. Precision and detection limits
Table 2 summarizes detection limits and precisions for all men-
tioned techniques. PTIMS has been widely reported as the most precise
among all instrumental techniques for boron isotope ratio analysis. The
Cs2BO2+ PTIMS method is considered to be the most precise with rela-
tive standard deviation (RSD) precisions in the range of 0.2 0.5
[40,4447,50,59,63,77,86] at detection levels of 0.15 g. Rao et al.
[79,80,83,87]reported boron isotopic ratio with RSD precision values
of 0.242.0for Na2BO2+ and 0.22.5for Rb2BO2
+. On the other
hand, NTIMS is described as the most sensitive technique, able to detect
boron at concentrations of 110 ng, while PTIMS detection levels are
higher in the range of 0.15 g. Further improvements applied on the
Cs2BO2+ PTIMS method by Nakano and Nakamura [43] and Deyhle[78]increased the precision and detection by 10-fold, reaching preci-
sion values of 0.070.25(2mean) for 1 g of B, and 0.150.32
(2mean) for 0.1 g of B by the former [43], and 0.06 for 0.1 g
boron by the latter [78]. Below 0.1 g boron, Ishikawa et al. [42]
reported 0.1 precision for 0.050.1 g, and 0.2 for 0.01 g
boron samples [42]. Nonetheless, PTIMS is not yet able to compete
with the sensitive detection capabilities of NTIMS, where 110 ng
boron loadings are reported with comparable precisions of
0.240.8 (2)[5557,93]. ICP-MS, ICP-qMS, and double-focusing
magnetic sector ICP-MS are less precise than PTIMS and NTIMS, with
reported precisions for the plasma-based techniques in the range of
714for ICP-MS[39,77], 310for ICP-qMS[80], and 12for the
double-focusing magnetic sector ICP-MS[34]. However, the introduc-
tion of the MC-ICP-MS improved the precision of the plasma-basedtechniques. In fact, the most recent publications report precision values
for MC-ICP-MS in the range of 0.20.4 (for 250 ng B [30], for 100 ngB
[35,36], and for 1050 ng B[7476]). This precision range at such low
detection levels (10100 ng) has made MC-ICP-MS very competitive
Table 2
Precision and detection levels of the major boron analyses techniques.
Precision and detection levels
1000 ng 100250 ng 50100 ng 1050 ng 110 ng
MC-ICP-MS 0.20.4for 250 ng[30] 0.20.4for 100 ng[35] 0.20.4[7880]
PTIMS (Cs2BO2+ method) 0.070.25[43] 0.06for 100 ng[83] 0.1for 50100 ng[42] 0.2for 10 ng[42]
NTIMS 0.240.8[5557]
4 A. Farhat et al. / Desalination xxx (2012) xxxxxx
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compared to both TIMS (0.240.8 for 110 ng) and PTIMS
(0.10.2for 10100 ng), especially since MC-ICP-MS is a relatively
faster technique that is characterized by its higher sample throughput.
The major non-MS based technique, ICP-OES, reported 10% pre-
cision in quantifying boron concentrations of solid samples[40], and
only 12% for aqueous samples[74]. Furthermore, the spectrophoto-
metric azomethine-H method reported a precision of 210% in the
aqueous samples[47,63]and 5% for the solid samples [45]. Where-
as, the nuclear reaction analytical (NRA) method, prompt-gammaneutron activation, determined boron concentrations with even
higher analytical precision of 515%[46]. The detection limits for
these techniques range from 13 ppb-B for spectrophotometric
methods to 10100 ppb-B in ICP-OES, and 1 ppm-B in the NRA method
[67], depending on type of the reagent and the sample matrix.
2.3. Complexity of operation and sample preparation
MC-ICP-MS outperforms PTIMS, NTIMS, and all other MS-based
techniques in terms of simplicity of operation because of its fast analysis
times and high sample throughput (up to 100 samples per day)[77].
The speed of sample acquisition in MC-ICP-MS has been reported with-
in 4 min per sample for samples containing 250 ng-B to a 0.2 preci-
sion [30], compared to 0.254.0 h reported for the TIMS technique
[44,59,80]. Improvements in NTIMS[93]have shortened its sample ac-
quisition time to 20 min, which is still longer than MC-ICP-MS, yet sim-
pler with itsfewer samplepreparation requirements. As a matter of fact,
to achieve high precision and low detection levels for the aforemen-
tioned boron analysis techniques, extensive and laborious sampleprep-
aration steps are required for almost all techniques. Samplepreparation
procedures involve boron extraction and separation/purification, pri-
marily by ion-exchange resins in order to pre-concentrate boron and
eliminate the effects of the samplematrix [30,50,76,78]. NTIMS isan ex-
ception and only requires minimal sample preparation especially for
aqueous samples [56,57], where it entails the addition of free-
seawater or Ba(OH)2+MgCl2to enhance BO2 formation[80]. Hence,
NTIMS has been recognized as the most suitable technique for water
samples.
2.4. Compliance with regulatory levels
As can be observed, with the exception of the nuclear reaction ana-
lytical methods, whose detectionlimit is 15 ppm witha 15% precision
[67], almost all the above reported techniques for the determination of
boron have their detection limits significantly below the seawater
boron levels of 4.5 ppm [14] and possess relatively high precision.
More importantly, these detection limits are well below the regulatory
guidance levels for boron of 0.5 and 0.6 ppm [13], as advised by the
WHO and USEPA. Hence, all of the aforementioned techniques can be
applied to ascertain regulatory compliance of aqueous samples.
2.5. Interferences and limitations
Each of the techniques discussed so far for Boron analysis suffers
one or more limitations (Table 3), although in most cases, there are
ways to deal with these limitations. Below is a discussion of these
limitations.
2.5.1. Spectral and isobaric interferences
Each of the MS based techniques described earlier is prone to iso-
baric interferences owing to the absence of an inline compound sep-
aration procedure (e.g., chromatography) prior to mass spectral
analysis. Isobaric interferences occur when the m/z ratios of the tar-
get ion and an interfering ion have a difference of less than one unit[66], making it difficult to separate ions given the resolution of the
mass spectral filter. ICP-MS measuring elemental boron abundance
at m/z 10 and 11 suffers from interference with 12C due to spectral
overlap with 11B [67]. It is not widely reported in MC-ICP-MS, but
others such as 40Ar4+ (m/z of 10) and 10BH+ (m/z of 11) interfering
with 10B and 11B, respectively, are noted [76]. Furthermore, NTIMS
suffers from isobaric interferences of BO2+ at m/z 42 with cyanogens
(CNO) formed when the samples contain organic materials
[53,80]. In PTIMS, the following isobaric interferences have been
identified: Cs2CNO+ with Cs2BO2
+ (m/z 308), when HNO3is present
in the sample, and 88Sr with Na2BO2+ (m/z 88) [77,80]. Wei et al.
[41]used an ionization depressor, 1% H3PO4, to effectively eliminate
isobaric interferences by preventing the formation of Cs2CNO+ and
CNO. The CNO interference was also corrected by applying an ex-
trapolation technique described by Kasemann et al. [59].
In techniques measuring light absorbance, several spectral inter-
ferences occur with a number of elements because the wavelength
of the investigated boron is near the wavelength of these elements.
Interferences with Fe, Al, Cu, Zn, and Mo are reported in spectropho-
tometric techniques utilizing the measurement of colored complexes
[101], whereas, in ICP-OES, interferences with Fe, Al, Ni, Cr, Si, and V
are observed[67].
2.5.2. Mass fractionation
This phenomenon occurs due to space-charge effects, which result
in unequal and preferential transmission of the heavier isotope
through the machine parts[80,81]. When the heavier isotopes pass
through the interface, skimmer cone, quadruple mass filter, and the
detector, they are slightly delayed compared to the lighter isotopes.Therefore, the concentration of the heavier isotope in the measured
results will be reported lower; causing a substantial alteration in the
ratio of the heavier isotope to the lighter isotope. ICP-MS techniques
measure boron by monitoring m/z 10 and 11, while NTIMS monitors
m/z 42 and 43, and with such low masses monitored, mass fraction-
ation is inevitable[30,81]. This is also observed in PTIMS monitoring
Na2BO2+ (m/z 88 and 89) but not in Cs2BO2
+ (m/z 308 and 309)
[80]. Yet, the measurement of the total boron concentration in the sam-
ple is not significantly affected by this phenomenon. In any case, such
limitations are corrected by using defined boron isotopic standards
such as SRM 951 and SRM 952 available from NIST, where the drift of
the results of themeasured standards from thepre-definedboron isoto-
pic ratios is quantified and corrected to all experimental runs. This is at
variance with matrix induced mass fractionation, which is another typeof mass discrimination effect caused by the sample preparation proce-
dure employed. This is especially observed when using ion-exchange
Table 3
Summary of the major advantages and disadvantages on the boron analyses techniques.
MC-ICP-MS PTIMS NTIMS
Convenienc e of analysis V er y f ast
[34,76]
Slow
[30]
Fast
[53]
Limitations Memory effect and mass fractionation
[30,67]
Mass fractionation
(Na-PTIMS)
[77,81]
Mass fractionation
[42,53]
Interferences 40Ar4+ and 10BH+
[53,76]
Cs2CNO+ (with Cs-PTIMS) and 88Sr (with Na-PTIMS)
[77,80]
CNO
[53,59]
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Amberlite IRA-743 resin[76], and cannot be corrected for by using a
defined boron isotopic standard. An exception is NTIMS, which was ap-
plied to water samples without the need for ion exchange preparatory
procedure[56].
2.5.3. Memory effect
In spectrometric instruments, boron adheres to the instrumental
components and is retained in the system. This affects the reading of
the instrument for subsequent sample runs, and is defi
ned in literatureas thememory effect[65]. The memory effect is exclusively reported
in plasma-based techniques and causes substantial suppression of 10B
relative to 11B. The memory effect presents a major problem in boron
analyses[67]despite several attempts to minimize it by performing
washouts between runs using NH3, NaF, and Mannitol blanks [80].
The ICP spray chamber is one of the major instrumental components
to which boron adheres to cause the memory effect. Aggarwal et al.
[30]reported using direct injector nebulizer instead of spray chamber
in their ICPto introduce thesample directly into theplasmato minimize
the memoryeffect, but this approach causedsignal intensity to decrease
in half.
2.5.4. Other limitations
Other general limitations are reported in PTIMS which is charac-
terized by its low ionization efficiency, requiring laborious sample
preparation for purification[55]. It is also limited by its generation
of its alkali or metallic metaborate (M2BO2+) ion, which is dependent
on the ratio of the metal (M) to the boron (M/B ratio) in the prepared
sample, especially in the case of Cs2BO2+ [80].
3. Boron isotopetracer analysis in applications related to desalination
The removal of boron from seawater or brackish water using
membrane desalination is not a straightforward process. Under neu-
tral feed water pH, boron exists in the form of boric acid, which is a
small and uncharged molecular compound that is poorly rejected by
membranes. However, one of the merits of boron's complicated
chemistry is that the rejection of boron by Reverse Osmosis (RO)
membranes increases with the increase of the pH of the systemabove a value significantly higher than the acid dissociation constant
(pKa) of boric acid (Eqs. (1) and (2)). The elevated pH shifts boric
acid's dissociation equilibrium in the direction of the ionized borate
anion[22], where the borate anion is efficiently removed by the mem-
brane because the negatively charged membrane rejects the negatively
charged borate via charge repulsion and prevents its penetration
through the membrane[1].
B OH 3 H2OH
B OH 4
1
pKa log Ka log H
h i B OH 4
= B OH 3
2
Boron speciation in the form of boric acid and borate as a functionof pH is displayed inFig. 3. The point where the concentration of boric
acid equals the borate concentration is the pKa, and its value, ranging
from 8.4 to 9.5, is affected by the temperature and the ionic strength
or salinity of the feed water [22,102]. As temperature and ionic
strength (salinity) increase, the borate fraction increases and thus
the boron rejection increases.
The RO systems, used for the treatment of seawater and brackish
water, operate traditionally at low pH (66.5) to inhibit scaling, but
since the boric acid penetrates undissociated through these RO mem-
branes, an innovative system of high pH in RO plants has been devel-
oped [21,24,25], where a two-pass system of pH adjustment is
installed. The first pass is operated without pH adjustments to treat
the high salinity water with limited scaling, followed by a second
pass at a pH of 9.510. The second pass RO effectively rejects boron
to a range of 8095%[22], as it is predominantly in the form of borate,
which can easily be removed by RO membranes because it is a
charged, polar molecular molecule[103]. Once the borate is removed,
the permeate is neutralized or blended before distribution to the end
user.
Kloppmann et al. [103] studied the variation of boron isotopic
composition throughout several stages of membrane desalination
plants and reported that boron fractionation is observed in the second
passes (high operating pH at around 9.5), where permeate is enriched
in 11B(Fig. 4). The study observed that no significant boron fraction-
ation is reported for the first passes, operating at relatively low pH
values of 66.5, concluding that these isotopic variations are depen-
dent on the pH induced variations of the boron species concentra-
tions. However, the behavior and mechanism of boron speciation
and fractionation related to its removal in second-pass RO still require
deeper investigation. One toolbox for such investigation would be the
stable isotope analysis of boron (11B and 10B) to gain a clearer insight
into the chemical separation and isotopic fractionation occurring during
the boron removal process.
Moreover, this enrichment in 11B of the desalted water causes anexpected depletion of 11B in the produced brine due to mass balance
considerations. These reported fractionations are advantageous in
terms of creating a fingerprinting signature of the desalted water
and the discharged brine.
The importance of water fingerprinting emerges potential contri-
bution of the man-made fresh water to the global water balance.
The desalted water, with its wide utilization including domestic
usage, drinking purposes, and irrigation, is being introduced into
natural systems such as soils, groundwater bodies via artificial
Fig. 3.Distribution of aqueous boron species versus pH in saline water[102].
Fig. 4.Stable isotope fractionation between B(OH)3and B(OH)4 in terms of11B () as a
functionof operationalpH conditions [103]. Thevalueof11B forboth boron speciesincreases
as the pH increases showing a strong fractionation in the heavy isotope of boron while the
average of11
B in seawater is around 39.
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recharge and leaching from irrigation, as well as surface water bodies,
eventually causing changes in the water chemistry and thus in the
ecology. Therefore, backtracking the water origin using the chemical
and isotopic fingerprinting would be of great value, especially in the
case of artificial recharge (AR) of the seawater RO (SWRO) desalted
waters into coastal or continental aquifers, where mixing between
desalinated and natural waters is likely occurring [104]. The stable
isotope analysis of boron in water potentially enables the evaluation
of the natural and anthropogenic proportions in groundwater systemsand determination of the source of aquifer water recharge as well as
the salinity origin and the water residence time[60]. As a matter of
fact, the SWRO desalted waters are characterized by a distinctive
boronisotopic composition that can differentiate theseSWROpermeate
waters from surface water and meteoric rainwater, where boron iso-
topes have been reported as useful artificial tracers in stressed aquifers
[82]. Therefore, boron isotopes monitoring is considered a successful
tool for evaluating the performance of the artificial recharge systems
and assessing the mixing of the man-made fresh waters with the natu-
ral water in terms of mixing proportions of the SWRO desalted water
and the degree of its penetration into the groundwater bodies [104].
In addition, this fingerprinting tool can also be applied on the
brine discharged back into the seas or oceans, making use of the de-
pletion of 11B. Since the desalination plants discharge their brine at
relatively short distances from their pumped feed water, the mixing
of the discharge brine with the sea feed water is inevitable. Thus,
studying the boron isotopic composition of these brines as well as
the mixed water in the sea will provide a reliable estimation of the
mixed proportions. Hence, this tool would be of great potential to as-
sess the brine discharge processes and predict the most suitable loca-
tions for discharging the brine in SWRO plants.
4. Conclusions
Boron analysis is of interest to numerous areas of research ranging
from nuclear technology, marine biochemistry, and geochemistry, to
environmental sciences, hydrology, and desalination. In seawater de-
salination, the removal of boron is of paramount concern because itexists in uncharged form under ambient conditions, allowing it to
pass through desalination membranes. Furthermore, boron has been
shown to be toxic to a number of plant species. Thus, the removal of
boron from saline waters is critical and entails the availability of ro-
bust instrumentation and analytical techniques for monitoring
boron levels with considerable sensitivity and precision, as well as
ease of use. The prevailing instrumentation and analytical methods
for boron determination along with their isotopic composition have
been detailed in this study.
NTIMS is recognized as the most suitable for aqueous samples,
especially when theprecisionof such samples is not of high importance.
Yet,it isdifficult to choose a most suitable method because each one is
characterized by its characteristic advantages and disadvantages. Each
of these boron analysis techniques endures several limitations, primar-
ily those associated by the sample matrix, and spectral and isobaric in-
terferences, which render the choice of technique dependant on the
sample type and the degree of complexity acceptable for sample prep-
aration. Several recent developments in MC-ICP-MS have made this
instrumental analysis method competitive with the very precise
PTIMS and very sensitive NTIMS, especially since MC-ICP-MS analysis
is relatively faster and is characterized by a high sample throughput.
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