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Sensors
Tailor-Made Micro-Object Optical Sensor Based on Mesoporous Pellets for Visual Monitoring and Removal of Toxic Metal Ions from Aqueous Media
Sherif A. El-Safty , * M. A. Shenashen , and A. Shahat
88
Methods for the continuous monitoring and removal of ultra-trace levels of toxic inorganic species (e.g., mercury, copper, and cadmium ions) from aqueous media such as drinking water and biological fl uids are essential. In this paper, the design and engineering of a simple, pH-dependent, micro-object optical sensor is described based on mesoporous aluminosilica pellets with an adsorbed dressing receptor (a porphyrinic chelating ligand). This tailor-made optical sensor permits ultra-fast (≤ 60 s), specifi c, pH-dependent visualization and removal of Cu 2 + , Cd 2 + , and Hg 2 + at sub-picomolar concentrations ( ∼ 10 − 11 mol dm − 3 ) from aqueous media, including drinking water and a suspension of red blood cells. The acidic active acid sites of the pellets consist of heteroatoms arranged around uniformly shaped pores in 3D nanoscale gyroidal mesostructures densely coated with the chelating ligand. The sensor can be used in batch mode, as well as in a fl ow-through system in which sampling, target ion recognition and removal, and analysis are integrated in a highly automated and effi cient manner. Because the pellets exhibit long-term stability, reproducibility, and versatility over a number of analysis/regeneration cycles, they can be expected to be useful for the fabrication of inexpensive sensor devices for naked-eye detection of toxic pollutants.
1. Introduction
The determination and removal of ultra-trace levels of metal
ions (such as mercury, copper, and cadmium ions) have
attracted great interest because of their high toxicity to bio-
logical systems as well as their bioaccumulative, mutagenic,
and suspected carcinogenic properties. [ 1 ]
© 2013 Wiley-VCH Vewileyonlinelibrary.com
DOI: 10.1002/smll.201202407
Prof. S. A. El-Safty, Dr. M. A. Shenashen, Dr. A. ShahatNational Institute for Materials Science (NIMS)1-2-1 Sengen, Tsukuba-shi Ibaraki-ken, 05-0047, JapanTel: + 81-298592135; Fax: + 81-298592025 E-mail: [email protected]; [email protected]
Prof. Sherif A. El-SaftyGraduate School for Advanced Science and EngineeringWaseda University3-4-1 Okubo, Shinjuku-ku, Tokyo, 169-8555, Japan
According to the US Environmental Protection Agency
(US EPA) and World Health Organization (WHO), the per-
missible levels of inorganic Hg 2 + and Cd 2 + ions in drinking
water are around 2 and 3 parts per billion (ppb), respectively.
Despite copper being essential components in the environ-
ment, the Cu 2 + ions are considered toxic with permissible level
in drinking water of 1.3–2 mg/L (parts per million, ppm). [ 2 ]
When mercury is dispersed in the environment, it is geo-
chemically transformed into toxic species, and the effects of
these species on humans have been extensively studied. [ 3 ] The
toxicity of Hg 2 + arises mainly from its high binding affi nity
for thiol (–SH) groups of proteins. [ 3d ] For example, interac-
tion of Hg 2 + with–SH groups in red blood cell (RBC) mem-
branes induces hemolysis. [ 4 ] Low-level exposure to Hg 2 + has
been linked to subtle neurodevelopmental disabilities, likely
resulting from its ability to induce reactive oxygen species.
Mercury also induces apoptosis, reportedly by causing the
exposure of phosphatidylserine receptors on the external
membranes of nucleated and nonnucleated cells such RBCs. [ 3a ]
For freshwater organisms, the acute toxicity thresholds for
rlag GmbH & Co. KGaA, Weinheim small 2013, 9, No. 13, 2288–2296
Optical Sensor Based on Mesoporous Pellets
inorganic mercury (typically, HgCl 2 ) vary considerably, from
5–230 μ g L − 1 for crustaceans to 60–800 μ g L − 1 for fi sh, which
accumulate methyl mercury in muscle and other tissues. [ 5 ]
Copper is essential for the maintenance of normal growth
during pregnancy and lactation in humans, and disorders of
Cu 2 + metabolism are strongly associated with life-threatening
neurological diseases, such as Menkes syndrome and Wilson’s
disease. [ 6 ] Moreover, defects in Cu 2 + metabolism that result in
a higher-than-normal Cu 2 + levels are associated with physi-
ological disturbances in humans. [ 7 ] Aquatic species are partic-
ularly sensitive to environmental Cu 2 + exposure. [ 8 ] Cadmium
is a rare element. Anthropogenic sources of cadmium in the
environment include mining and smelting of metal ores, fossil
fuel combustion, and metal industries. [ 9 ] Chronic cadmium
exposure causes renal dysfunction, a bone-related syndrome
called itai-itai disease, metabolic disorders, and increased inci-
dence of certain forms of cancer, possibly owing to the direct
inhibition of DNA mismatch remediation by cadmium. [ 10 ]
Because these bioaccumulative metal ions are hazardous
to the environment and to humans, sensitive, reliable, and
cost-effective methods for their determination in and removal
from aqueous media are highly desirable. Although various
methods (such as electrothermal atomic absorption spectrom-
etry, inductively coupled plasma–optical emission spectrom-
etry, and inductively coupled plasma–mass spectrometry) can
be used to monitor toxic metal ions even at very low concen-
trations (parts per billion), [ 11 ] these methods require expen-
sive equipment and trained personnel, [ 12 ] which prevents their
widespread use, especially in developing countries. Therefore,
the development of optical nanosensors [ 13 ] has attracted great
interest for the detection and removal of toxic metal ions.
However, slow reaction kinetics and limited detection sensi-
tivity have restricted the practical use of such nanosensors. [ 14 ]
The development of optical sensor devices would overcome
some of these limitations and permit the monitoring of ultra-
Scheme 1 . (A) 3D Geometrical model of cubic Ia3d aluminosilica mesostructures. (B) The atomic charge distribution of 3D cubic Ia3d network cluster units of aluminosilica sensor pellets. The Si/Al ratio used in this cluster is equal to 9. (C) Aluminasilica sensor pellet synthesis with stepwise immobilization of TMPyP followed by sensing/removal of metal ions, such as mercury. The design indicates the feasibility of the capturing/stripping process inside the mesopores of pellets.
trace levels of metal ions by means of one-
step cycling of environmental samples.
Such sensors might also be applicable as
monitoring devices in households, where
instrument-dependent analytical methods
are prohibitively expensive. [ 15 ]
However, problems with the fabrica-
tion of optical nanosensor devices, namely,
time-consuming and complicated syntheses,
as well as high capital and operating costs,
need to be solved. Most nanosensor mate-
rials are obtained as precipitates that must
be reshaped for their fi nal use in sensing
devices. [ 13–17 ] Therefore, the production
of nanosensors into different morpho-
logical shapes and fi lm-like membranes is
needed for simple, easy-to-use, and multi-
functional cleanup optical sensors. Nano-
engineered mesoporous aluminosilica
materials show a diverse and expanding
range of applications, particularly for
adsorption, separation, and catalysis. [ 18 , 19 ]
The incorporation of aluminum into the
mesoporous framework generates cationic
© 2013 Wiley-VCH Verlag Gmbsmall 2013, 9, No. 13, 2288–2296
Brønsted or Lewis acid sites corresponding to tetrahedrally
coordinated aluminum species (AlO 4 − ) in the aluminosilica
framework. [ 20 ] We suspected that mesoporous aluminosilica
pellets with uniformly shaped pores arranged in three-dimen-
sional nanoscale gyroidal structures could be used as scaf-
folds for the construction of practical and inexpensive optical
sensors for determination and removal of toxic metals in
aqueous media.
In this paper, we describe a simple, pH-dependent,
micro-object optical sensor system based on a scaffold of 3D
gyroidal mesoporous aluminosilica pellets with an adsorbed
dressing receptor (a porphyrinic ligand) without prior modi-
fi cation of the scaffold surface with thiol or silane coupling
agents. This tailor-made system permitted ultra-fast and
selective visualization and removal of multiple toxic metals
from aqueous media (including a suspension of RBCs). An
important advantage of this design is its ability to sensitively
detect multiple analytes. To the best of our knowledge, there
have been no previous reports of micro-object optical sensors
based on aluminosilica pellets with a single dressing receptor
for specifi c visualization and removal of multiple toxic metals
from aqueous media. The sensor showed a remarkable ability
to selectively remove Hg 2 + , Cd 2 + , and Cu 2 + ions from drinking
water. Furthermore, the sensor suppressed the toxicity of
Hg 2 + ions (by ∼ 50%) in a suspension of RBCs, without
exerting any toxicological effects on the RBCs.
2. Results and Discussion
For use in the tailor-made micro-object sensor, we prepared
robust disk-like pellets with mechanically stabilized shapes,
micrometer-sized particles and tunable periodic scaffolds
consisting of cubic Ia3d mesoporous aluminosilica with low
alumina content (Si/Al = 9; Schemes 1 and S1 and Figure S1).
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S. A. EI-Safty et al.
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The pellets had large surface area-to-volume ratios and uni-formly shaped pores in three-dimensional nanoscale gyroidal
structures.
The synthesis protocol and characteristics of cubic Ia3d
aluminosilica mesocylinders as carriers are of particular inter-
ests due to the following:
a) Hand-operating and easy-to-make synthesis of mesopo-
rous pellets with micrometric particle sizes was achieved
using our simple method that requires shorter time and
simple composition.
b) Our strategy enabled fabrication of an optical gel-like
material in a graduate ingot, in which acquired the shape
and size of the cylindrical casting vessel, leading to control
the pellet-like materials without use of well- equipment
control (Scheme S1).
c) The development of ordered mesoporous pellets that fea-
ture 3D structures, 3D cylinder-shaped and uniform pore
sizes, monodispersed porosities into large particle sizes
with ultra- or micrometer-scale morphologies signifi cantly
led to densely coated with the chelating ligand (Scheme 1 ).
The inner and outer pore walls of pellets could be
directly modifi ed with a charged porphyrinic chelating
ligand, α , β , γ , δ -tetrakis(1-methylpyridinium-4-yl)porphyrin
p -toluenesulfonate (TMPyP), without the need for surface-
mounted coupling agents. The surface acidity (see Supporting
Information) of the pellets facilitated the uniform modifi -
cation of the pore walls by the TMPyP molecules without
prior decoration of the surface supports with silane or thiol
coupling agents. Strong ion-pair interactions between the
0
Figure 1 . (A,B) HRTEM micrographs and FTD (insets) patterns of cubic Ia3d aluminosilica pellets with a Si/Al ratio of 9. HRTEM and FTD patterns were recorded along the [311] (A), and the [111] (B) zone axes, respectively. (C) 3D TEM micrograph of pellets recorded along the [311] direction with 45 ° tilt. In general, there are smooth and well-ordered network surfaces over wide-range domains of cubic Ia3d structures. (D) Bright-fi eld STEM of sensor pellets.
pyridinium ion–containing TMPyP mole-
cules and the negatively charged AlO 4 −
units of the aluminosilica host material
prevented leaching of TMPyP from the
pore surfaces during the sensing assays.
Scheme 1 A shows the electron density
distribution on a structural model of the
aluminosilica pellets and the effect of the
atom arrangement in the 3D lattice on the
pore orientation is shown in Scheme 1 B
(see Supporting Information). The oxygen
atoms in the Si–O–Al linkages were more
negatively charged than the oxygen atoms
in the other linkages, which indicate that
the surface sites in the former linkages
were more acidic than other sites in the
framework. The surface acidity was con-
fi rmed by 27 Al NMR magic-angle spinning
spectroscopy and NH 3 –temperature pro-
grammed desorption studies (Figures S2
and S3, SI). Because of the acid-site sur-
faces, the amount of TMPyP adsorbed
on the pellet matrices (40 mg g − 1 ) was
suffi cient for the generation of a color
change that was visible to the naked eye
in response to the formation of complexes
between TMPyP and toxic metal ions. The
high loading capacity and the immobili-
zation of TMPyP ligand into functional
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pellets were evident from scanning transmission electron
microscopy (STEM)–energy dispersive spectroscopy map-
ping and thermogravimetry/differential thermal analyzer
(TG/DTA), (Figures S4, S5). The key to designing pellets
for optical sensors is to ensure that the accommodation of
the chelating agent (a porphyrin in this case) is densely and
uniformly immobilized on the 3D gyroidal mesopore pellet
matrices, which leads to rapid binding of the target metal
ions during the sensing assay.
The most important feature of the pellets was the uniform
arrangement and continuous ordering (that is, without distor-
tion) of gyroidally cubic Ia3d mesostructures in all directions.
The integrity of the cubically ordered frameworks in the
micrometer-sized particle and the gyroidal mesostructures
of the pellets lead to attain the porphyrin ligand interior the
3D pore-like pocket (Scheme 1 ), as shown by high-resolution
transmission electron microscopy (HRTEM), STEM, three-
dimensional TEM (3DTEM; Figure 1 ), small-angle X-ray
scattering, and N 2 isotherm profi les ( Figure 2 ). The HRTEM,
3DTEM, and STEM micrographs along the zone axes of the
pellets revealed regular arrays running along a large area of
the [311] and [111] directions, which allowed the analyte ions
to diffuse homogeneously and interact with the binding sites,
even after the pellets had been stored for a long period (one
year to date). The small-angle X-ray scattering images of the
pellets exhibited well-resolved Bragg peaks with d-spacing
ratios of 9.4, 8.1, 6.1, and 5.7, indicating highly ordered cubic
Ia3d nanophase domains (Figure 2 A). The N 2 isotherms
featured an H1-type hysteresis loop with a sharp infl ection,
which is characteristic of architectures with uniform and
erlag GmbH & Co. KGaA, Weinheim small 2013, 9, No. 13, 2288–2296
Optical Sensor Based on Mesoporous Pellets
Figure 3 . pH-dependent curves of the sensor pellets in the measurement of refl ectance spectra ‘signal’ response of the M-to-TMPyP complex during the detection/removal of Cu 2 + , Cd 2 + and Hg 2 + ions at 552 (a), 620 (b), and 636 (c) nm, respectively.
Figure 2 . SAXS patterns (A) and N 2 adsorption/desorption isotherms at 77 K (B) of the highly ordered cubic Ia3d aluminosilica scaffolds with Si/Al ratio of 9 (a), TMPyP-modifi ed pellet sensors (b), and after reuse cycles (c). Insert (A) shows the cubic Ia3d lattices ( a = d 211 √6) and (B) the textural parameters, such as surface area (S BET ), pore size (D), and pore volume (Vp).
open cylindrical pores. [ 21 ] The N 2 isotherms indicate that the
important textural parameters (e.g., surface area and pore
size and volume; Figure 2 B, inset) of the mesostructures
were retained upon noncovalent binding of a substantial of
amount of TMPyP on the inner pore surfaces, as evidenced
by the shift in the adsorption branch toward a lower relative
pressure (P/Po) and the slight reduction of the surface area
and pore volume upon functionalization with TMPyP.
We constructed a micro-object optical sensor system by
installing the singular pellet in a fl ow-through module in
which sampling, target ion recognition and removal, and anal-
ysis occurred (Scheme S2, SI). The pellets were placed in the
central reactor cavity of a sandwich-like glass cell. Laminar
fl ow predominated in this setup, thereby permitting precise
control of the sensing reaction conditions. In addition, the
minimal reagent use, controlled metal-to-ligand binding, and
containment of the pellets in the module ensured that haz-
ardous substances could be analyzed safely. The color change
that occurred upon binding of the target metal ions to the
TMPyP-containing pellets was monitored visually as well as
by UV–vis refl ectance spectroscopy. In addition, the solution
emerging from the outlet of the fl ow-through module was
analyzed by inductively coupled plasma–mass spectrometry
(ICP-MS) to determine the extent to which the target ions
were removed.
The specifi city of the pellets for the target metal ions
was controlled by means of pH adjustments. The porphyrinic
ligand immobilized on the pellets has four charged pyrid-
inium nitrogens and two pyrrole nitrogens, which can be
neutral or protonated depending on the pH of the medium
(see Supporting Information S6–S8). Therefore, by varying
the pH, we were able to control the visual detection and
selective removal of Cu 2 + , Cd 2 + , and Hg 2 + ions. In both batch
experiments (see Supporting Information) and fl ow-through
experiments conducted with solutions of Cu 2 + , Cd 2 + , and Hg 2 +
ions, we observed a rapid signaling response ( ≥ 60 s) based
on the change in the specifi c color map and the refl ectance
intensities at λ max values of 552, 620, and 636 nm for the
M–TMPyP complexes that formed in the pellets at pH values
of 5.5, 9.5, and 11.5, respectively ( Figure 3 ). These metal com-
plexes formed as a result of a defi ciency in the d-orbitals of
the metal ion centers, which caused the metals to bind fi rmly
© 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheismall 2013, 9, No. 13, 2288–2296
to the TMPyP donor molecules to form
symmetrical fi ve-membered rings in octa-
hedral complexes with high stability con-
stants (Scheme 1 ). [ 22 ]
A major advantage of the pellet sensor
in both micro-object and batch sensing
systems is its selectivity to the target Cu 2 + ,
Cd 2 + , and Hg 2 + ions, thus preventing hin-
drance from actively interfering compo-
nents, particularly the competitive ions
and species. These interfering components
may make the sensing/recovery of metal
target ions from a mixture containing sev-
eral competitive components diffi cult. The
selectivity of the pellet sensor for Cu 2 + ,
Cd 2 + , and Hg 2 + ions was checked in both
micro-object and batch sensing systems.
The interfering cations and anions were initially added at
high concentration range to the pellet sensor ( Figures 4 , S6
and S7) at ion-sensing conditions of pH 5.5, 9.5, and 11.5 for
Cu 2 + , Cd 2 + , and Hg 2 + , respectively. First, we studied the spe-
cifi c behavior of the pellets that permitted the selective deter-
mination of Cu 2 + , Cd 2 + , and Hg 2 + , by separately adding each
of a series of interfering transition metal ions and group I and
II metal ions at pH values of 5.5, 9.5, and 11.5, respectively
(Figures 4 and S6). We found that alkali and alkaline earth
metals (including Na + , Li + , Mg 2 + , and Ca 2 + ions) at a concen-
tration of 10 ppm did not exhibit any appreciable interfer-
ence. In contrast, the addition of an equivalent amount of
transition metal ions (Cu 2 + , Ni 2 + , Co 2 + , Pb 2 + , and Zn 2 + ) to the
Hg(II) ion-sensing system interfered slightly ( ± 2%) with the
quantitative determination and removal of the target ions. At
high doses (up to 10 times of target concentration), competi-
tive cations (particularly Ni 2 + , Fe 3 + , Pd 2 + , and other Cu 2 + and
Cd 2 + target ions) produced positive errors in the refl ectance
signal of the Hg(II) ion-sensor pellets. The addition of 0.05 M
oxalate, citrate, thiosulphate, or tartrate to the sensing system
increased the tolerable concentration of the active targets
at each ion-sensing by up to 20 times the concentration of
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S. A. EI-Safty et al.
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Figure 4 . Effect of the additive cations and anions as interfered components on the refl ectance spectra at 636 nm and color response, respectively, of Hg-to-TMPyP complexes, recorded using a 20 mg/L sensor pellet at pH 11.5, and with the addition of 1 ppm of Hg 2 + ions. Note the interfered (10 ppm) alkali and alkaline-earth metals (that is, Na + , K + , Li + , and Mg 2 + ions). The other cations’ concentrations were at 1 ppm. In addition, the interfered [50 ppm] anions from the four groups (G-b to G-e) are as follows: G-b (CTAB, SDS, Triton X, NO 3 − , and SO 3 2 − ), G-c (C 2 O 4 2 − , C 8 H 4 O 4 − , and C 4 H 4 O 6 2 − ), G-d (C 6 H 5 O 7 3 − , CO 3 2 − , and NO 2 − ) , and G-e (CH 3 COO − , SO 4 2 − , and PO 4 3 − ), respectively.
Figure 5 . Refl ectance spectra for aluminasilica sensor pellets with different concentrations of Hg 2 + ions at the optimum pH = 11.5. (A, insert) Calibration plots of the refl ectance spectra for our fabricated sensor with various concentrations of Hg 2 + ions at λ 636 nm (contact time of 1 minute, at 25 ° C), based on the relationship between the R–R o and metal ion concentrations. Calibration was done by measuring the relative refl ectance of Hg-TMPyP complexes (R) formed with respect to a blank solid of sensor (R 0 ) at the specifi c λ of 636 nm. The inserts show the amplifi cation for the linear colorimetric response, and the calculated limit of detection for mercury ions was 1.4 × 10 − 9 M. The error bars denote a relative standard deviation of approximately 0.03% for the analytical data of ten replicate analyses.
the Cu 2 + , Hg 2 + , and Cd 2 + target ions. Second, we investigated
the selectivity of the TMPyP-modifi ed pellet sensors in the
presence of interfering surfactants [cetyl trimethylammo-
nium bromide (CTAB), Triton X, and sodium dodecyl sulfate
(SDS)] and organic [citrate: C 6 H 5 O 7 3 − , oxlate: C 2 O 4
2 − , tar-
trate: C 4 H 4 O 6 2 − , phthalate: C 8 H 4 O 4 − ,and acetate: CH 3 COO − ]
and inorganic [NO 2 − , NO 3
− , SO 3 2 − , SO 4
2 − , CO 3 2 − , and PO 4
3 − ]
anions, respectively, that may coexist with our target ions in
water and the environment. In our study, the experiment was
carried out by separately studying the effect of each inter-
fering surfactants and anions (Figure S7), and then studying
their effect as a group (Figure 4 C). Interestingly, we found
that the addition of inorganic anions (i.e., NO 2 − , NO 3
− , SO 3 2 − ,
SO 4 2 − , CO 3
2 − , and PO 4 3 − ), which we thought might impede the
detection and removal processes, had no appreciable effect on
the TMPyP-modifi ed pellets; these anions were tolerated at
www.small-journal.com © 2013 Wiley-VCH V
concentrations of up to 50-times the concentrations of Cu 2 + ,
Cd 2 + , and Hg 2 + ions (Figure 4 C and S7). In addition, there is
no signifi cant interference or effect from the used surfactants
and organic anions on the signal responses or color profi les
of TMPyP-modifi ed pellet sensors (Figure S7), indicating the
ion-selective sensor with high tolerable limits of interfering
matrix concentrations. The selectivity of the pellets can be
ascribed to their high binding affi nity for the target metal
ions, the stability of the formed [M-TMPyP] n + complexes (see
Figure S6 and S7), and TMPyP-to-M complexation affi nities
among all interfered metals at optimized pH conditions.
We measured UV–vis refl ectance spectra to monitor the
change in the pellets upon formation of the M–TMPyP com-
plexes in the micro-object sensor system ( Figures 5 and S6,
SI). We measured the refl ectance spectra of the complexes
at λ max values of 552, 620, and 636 nm for Cu 2 + , Cd 2 + , and
erlag GmbH & Co. KGaA, Weinheim small 2013, 9, No. 13, 2288–2296
Optical Sensor Based on Mesoporous Pellets
Figure 6 . Feasible application of sensor pellets on the batch sensing/capturing process of Cd 2 + , Cu 2 + , and Hg 2 + ions from real water with sequential color changes upon interaction with each metal at the optimized pH values.
Hg 2 + ions, respectively, to monitor the
uptake of M n + target ions by the TMPyP
ligand (Figure S6, SI). In addition, metal
ion concentrations in the sample solu-
tions before and after exposure to the pel-
lets were measured by means of ICP-MS
(Scheme S2). The wavelength of the
charge-transfer refl ection band of the com-
plexes depended on the ligand-binding
affi nity of the central metal ion and on
the nature of the complex formed under
the sensing conditions. Moreover, the vis-
ible color change provided a simple way to
sensitively and selectively detect M n + ions
without the need for sophisticated instru-
ments. The rapid detection and extraction
and the M n + -to-TMPyP binding events
that formed on the pellet surfaces resulted
in the separation and preconcentration of
divalent metal ions even at trace concen-
trations. We prepared calibration curves
by analyzing standard solutions with a
wide range of Cu 2 + , Cd 2 + , and Hg 2 + con-
centrations (0.005 μ g dm − 3 to 5 mg dm − 3 ;
10 replicates for each concentration)
at the optimum pH for each metal ion
(Figure S6, SI). The standard deviation for the quantitative
analysis data for Cu 2 + , Cd 2 + , and Hg 2 + ions was 0.02–0.06%, as
indicated by the curve fi tted to the calibration data (Figures 5
and S6, SI). The limits of detection (LOD) of the pellets were
estimated from the linear regions of the calibration curves
(Figures 5 and S6, insets). The LOD values indicated that the
sensing system could detect Cu 2 + , Cd 2 + , and Hg 2 + ions at con-
centrations down to ∼ 10 − 11 mol dm − 3 , even in the presence
of the matrices (as shown by calibration curves (Figure 5 B)
dotted lines).
To evaluate the practical applicability of the pellets, we
performed batch detection and removal of Cu 2 + , Cd 2 + , and
Hg 2 + ions from samples of environmental fl uids at 25 ° C and
pH values of 5.5, 9.5, and 11.5, respectively. ICP-MS was used
to determine the concentrations of the various constituents
before and after each experiment. The samples contained
alkali and alkaline earth metal ions (12.8–31.1 mg dm − 3 ) and
traces of Zn 2 + , Mn 2 + , Sn 2 + , Fe 2 + , and Fe 3 + ions (0.02–0.083 mg
dm − 3 ). The samples were spiked with Cu 2 + , Hg 2 + , and Cd 2 +
ions (0.001–0.5 mg dm − 3 ). Langmuir isotherms were used to
verify the effi ciency of metal ion absorption by the TMPyP-
bearing pellets in terms of the loading capacities and binding
effi ciencies of Cu 2 + , Hg 2 + , and Cd 2 + ions at ultra-trace concen-
trations. [ 23 ] Our results indicate that the use of the pellets for
colorimetric assays in the fi eld and in the laboratory is a viable
alternative to the currently used laboratory methodology in
terms of time and cost savings ( Figure 6 ). The linear adsorp-
tion curves (Figure S7, SI) revealed two features of the sensor
system: (1) metal ions at a wide range of concentrations could
be removed without the need for preconcentration of the
samples, and (2) the metal ions formed a monolayer on the
interior pore surfaces of the pellets in this sensor system. The
practical adsorption capacity ( q m ) and the Langmuir coverage
© 2013 Wiley-VCH Verlag Gmbsmall 2013, 9, No. 13, 2288–2296
constant ( K L ) were obtained from the slope and intercept of
the linear regions of the Langmuir plots. The metal ions could
be removed from the aqueous medium with high adsorption
effi ciencies (94–96%). Thus, removal of 0.114–0.14 g of Cu 2 + ,
Hg 2 + , or Cd 2 + ions from an aqueous solution would require
1 g of TMPyP-containing pellets. The pellets displayed sub-
stantial adsorption effi ciency, comparable to that of commer-
cial adsorbents such as nanoporous silica, activated carbon,
sphagnum moss peat, TiO 2 , coconut shell charcoal, organi-
cally modifi ed clays, polypyrrole/reduced graphene oxide,
and ion-exchange resins. [ 23 ] In addition, these adsorbents are
complicated to design and complicated to use for detection
and removal of metal ions. [ 23 ]
If these pellets are to be used for waste management and
decontamination of polluted media, they must exhibit repro-
ducible high performance, recyclability, and durability. [ 24 ] To
demonstrate that the pellets could be recycled by decompl-
exation of the bound metal ions, we treated the metal-con-
taining pellets with a solution of 0.02 M ClO 4 − or 0.05 M
ethylenediaminetetraacetic acid “stripping agents” to remove
the Cu 2 + , Hg 2 + , and Cd 2 + ions. The solution of stripping agents
was injected into the pellets containing 0.6 ppm of metal
target ions (with a syringe) for several hours (Scheme 1 ). The
gradual change in the pellet color as the regeneration time
was increased was visible to the naked eye and was quanti-
tatively confi rmed by UV–vis refl ectance spectroscopy and
ICP-MS. Approximately 98% ( ± 2.3%) of the initial amount
of metal ions was recovered. The pellets could generate and
transduce an optical color signal and exhibit fast TMPyP–M
binding (on the order of minutes), even after multiple regen-
eration/reuse cycles ( Figure 7 ), with only a slight decrease in
effi ciency as the number of cycles was increased, indicating
that the mesostructured functionality and features were
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Figure 7 . Evaluation of the effi ciency changes for the recognition and capturing properties of 1 ppm of Hg 2 + , Cu 2 + , and Cd 2 + ions using 20 mg/L of TMPyP-modifi ed sensor pellet after six regeneration/reuse cycles at 25 ° C.
retained. The retention of functionality was confi rmed by
TEM and fi eld emission SEM ( Figure 8 ), which indicated that
the three-dimensional architecture ordering and the pellet
morphology (size and shape) were retained to a high degree.
These features could lead to long-term stability, reproduc-
ibility, and versatility of the pellets over a number of reuse/
cycles (Figure 8 ).
We also evaluated the use of the pellets to remove metal
ions from a physiological fl uid. Mercury ions interact rapidly
with–SH groups in RBC membranes, leading to peroxida-
tion of membrane lipids and, eventually, to cellular lysis. [ 4 , 25 ]
Therefore, we investigated the removal of Hg 2 + ions from a
suspension of RBCs to determine whether removal would
inhibit Hg 2 + -induced RBC hemolysis (Figure S8, SI). Mer-
cury ions (3 μ M) were added to a suspension of RBCs, which
was incubated for 12 h with ground pellets (0.02%, 0.05%
and 0.07% w/v). The absorbance of released hemoglobin
at 540 nm ( n = 3) was used as a marker of RBC hemolysis.
Upon the addition of the ground sensor pellets (0.05% w/v)
at physiological pH (7.4),–ve effect of the sensor on RBCs
was observed. Furthermore, the Hg 2 + -induced hemolysis
decreased by approximately 40% (Figure S8), and we attrib-
uted the decrease to the removal of some of the Hg 2 + ions
by the pellets. This fi nding revealed that the Hg 2 + ions might
have been removed if the process had been carried out at
www.small-journal.com © 2013 Wiley-VCH V
Figure 8 . (A) TEM, (B) FESEM micrographs of sensor pellets after releasingCd 2 + ions from the sensor surfaces.
the optimal pH for Hg 2 + (11.5, as described above) instead
of at physiological pH 7.4. In general, such inhibition of the
mercury-induced hemolysis is the key to exploring the appli-
cability of micro-object-device sensor in controlling the tox-
icity of mercury in blood through the removal and capture of
mercury ions.
3. Conclusion
In this study, we monitored and removed ultra-trace concen-
trations Cu 2 + , Hg 2 + , and Cd 2 + ions from aqueous solutions and
a suspension of RBCs by means of a tailor-made micro-object
optical sensor that integrated sampling, chemical reaction, sep-
aration, detection, and data processing in a highly automated
and effi cient system. The system enabled ultra-fast and specifi c
detection and removal of multiple toxic metals by means of
mesoporous aluminosilica pellets bearing an adsorbed single
dressing receptor (a porphyrinic ligand). The pellets had large
surface area-to-volume ratios and uniformly shaped pores
in three-dimensional nanoscale gyroidal structures and per-
mitted rapid detection ( ≥ 60 s) of ultra-trace concentrations
( ∼ 10 − 11 mol dm − 3 ) of the target metals by means of a colori-
metric signal visible to the naked eye, as well as by means of
UV–vis refl ectance spectroscopy. In addition, the metal ions
captured by the pellets could be removed from the pore sur-
faces via chemical stripping, and the pellets could be reused.
This capture-and-release process concentrates on the col-
lected elements up to 98% effi ciency in controlled waste man-
agement. Pellet-based micro-object sensing devices like the
one described here can be expected to be important for use in
portable and remote sensing systems, especially for household
use, where instrumental methods are prohibitively expensive.
4. Experimental Section
Details on the fabrication and characterization of the sensor pel-lets, as well as their use to remove metal ions from a suspension of RBCs, are presented in the Supporting Information.
The micrometric sensor pellets were synthesized as follows. Cubic Ia3d mesocylinder aluminosilica pellets (Scheme S1, SI) were used as solid scaffolds for functionalization with a porphy-rinic ligand, α , β , γ , δ -tetrakis(1-methylpyridinium-4-yl)porphyrin
erlag GmbH & Co. KGaA,
the Hg 2 + , Cu 2 + , and
p -toluenesulfonate (TMPyP). TMPyP in ethanol solution was immobilized on the pellets by means of a dispersion process at 45–50 ° C. The immobilization process was repeated several times until the equilibrium adsorption capacity of the pellets for TMPyP molecules was saturated, as indicated by spectrophotom-etry. The solid sensor pellets were thoroughly washed with deionized water until no elution of the TMPyP was observed. We determined the equilibrium adsorption capacity of the pel-lets for TMPyP by measuring its absorbance at various time intervals. The amount of TMPyP adsorbed onto the scaffolds was estimated to be 40 mg g − 1 .
Weinheim small 2013, 9, No. 13, 2288–2296
Optical Sensor Based on Mesoporous Pellets
Next, we tested the utility of the sensor pellets for detection and removal of ultra-trace concentrations of Cu 2 + , Cd 2 + , and Hg 2 + ions in aqueous solutions at pH 5.5, 9.5, and 11.5, respectively. The concentrations of the metal ions were monitored in a fl ow-through module, which was connected to pellets housed in a sandwich-like glass cell with a central reactor cavity that was 3 mm high and ∼ 15 mm in diameter (Scheme S2, SI). Laminar fl ow pre-dominated in this setup, which permitted precise control of reac-tion parameters, such as concentration gradients, temperature, and pH. The sample solutions were pumped into the reactor cavity containing the pellets at a fl ow rate of 1.5 μ L min − 1 by means of an autosampler pump through silicon tubes (inner diameter 1 mm). The glass cell device was connected to a deuterium-halogen light source (AvaLight-DH-S, Avantes), which has a deep UV bulb (190–400 nm), a deuterium lamp (215–400 nm), and a halogen lamp (360–1,500 nm). A fi ber optic spectrometer system (CIMPS-Abs-UV, Zahner, Germany; AvaSpec-2048 × 14, Avantes) was used to measure the signal from the molecular recognition event.
The optical color intensity of the solid TMPyP sensor pellet was estimated with a UV–vis spectrometer (CIMPS-Abs-UV, Zahner, Ger-many) installed with AvaSoft 7.6 software (Avantes; Scheme S2, SI). ICP-MS was used to determine the effi ciency of Cu 2 + , Cd 2 + , and Hg 2 + ion removal by the pellets by measuring the metal ion concentrations in the aqueous samples after exposure to the pel-lets and comparison of the measured concentrations to the initial concentrations.
Supporting Information
Supporting Information is available from the Wiley Online Library or from the author.
Acknowledgements
M. Shenashen and A. Shahat thank the Egyptian Petroleum Research Institute (EPRI), and Suez University, Egypt, respectively, for granting a leave of absence.
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Received: September 30, 2012 Revised: November 6, 2012Published online: January 29, 2013
erlag GmbH & Co. KGaA, Weinheim small 2013, 9, No. 13, 2288–2296