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Journal of Radioanalytical andNuclear ChemistryAn International Journal Dealing withAll Aspects and Applications of NuclearChemistry ISSN 0236-5731 J Radioanal Nucl ChemDOI 10.1007/s10967-014-3249-0
Mechanism of sorption of pertechnetateonto ordered mesoporous carbon
Đ. Petrović, A. Đukić, K. Kumrić,B. Babić, M. Momčilović, N. Ivanović &Lj. Matović
1 23
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Mechanism of sorption of pertechnetate onto ordered mesoporouscarbon
Ð. Petrovic • A. Ðukic • K. Kumric •
B. Babic • M. Momcilovic • N. Ivanovic •
Lj. Matovic
Received: 14 February 2014
� Akademiai Kiado, Budapest, Hungary 2014
Abstract Ordered mesoporous carbon (OMC) was used
as an adsorbent for the removal of pertechnetate (TcO4-)
anion. The maximum uptake (93 %) of TcO4- was
obtained after 60 min of contact. The adsorption of TcO4-
is almost pH-independent in very wide pH region (from 4.0
to 10.0). Maximum Kd of 6.6 9 103 cm3 g-1 was found at
pH 2.0. TcO4- interacts with carboxylic functional groups
present at the surface of the OMC by displacing the OH-
ions with TcO4- via ion exchange mechanism.
Keywords Technetium-99 � Adsorption � Ordered
mesoporous carbon � Surface functional groups
Introduction
The presence of the radionuclide 99Tc in the environment
comes from anthropogenic nuclear activities such as nuclear
power plants, nuclear weapons testing facilities, reprocess-
ing of spent nuclear fuel, nuclear accidents and medical
application of 99mTc. The predominant chemical form of the
long-lived radionuclide 99Tc (t1/2 = 2.1 9 105 year) is the
highly soluble and environmentally mobile pertechnetate
anion (TcO4-), that easily penetrates the ecosystems [1]. The
control of environment pollution by 99Tc is therefore con-
sidered a primary task. Many investigations are orientated
toward the immobilization of 99Tc, as well as its adsorption
from contaminated groundwaters using various adsorbent
materials.
In recent years, many synthetic and natural materials,
including clay minerals [2–4], inorganic compounds [5, 6],
strongly magnetic iron-sulfide materials [7], organic poly-
mers [8], activated carbons [9–13], various synthetic resins
and sponges [14–17] have been evaluated for use in long-
term immobilization of 99Tc and its removal from con-
taminated groundwaters. Compared to other materials,
removal of TcO4- by activated carbons is one of the most
efficient processes, because of large specific surface area,
porous structure and variety of surface functional groups of
activated carbons. Gu et al. [10] used commercial activated
carbon (Nuchar WV-G) for adsorbing TcO4- from syn-
thetic groundwater over a wide range of pH values. The
distribution coefficient (Kd) of TcO4- was determined to
range from 2.1 9 103 to 2.7 9 104 cm3 g-1. In contrast to
this material, the activated carbon (Merck KGaA/Merk-
Schuchart) used by Holm et al. [11] has Kd in the order of
106 at pH 2–4. Wang et al. [12] grouped commercial acti-
vated carbon materials into two distinct types: (i) type I
materials that have high sorption capabilities with the Kd
varying from 9.5 9 105 to 3.2 9 103 cm3 g-1 (in the pH
range from 4.5 to 9.5) and (ii) type II materials that have
relatively low sorption capabilities with Kd remaining more
or less constant (1.1 9 103–1.8 9 103 cm3 g-1) over a
similar pH range. The difference in sorption behavior
between the two types of materials was attributed to the
different distribution of surface functional groups (carbox-
ylic and phenolic). The presence of a large fraction of more
acidic carboxylic subgroups is found to be responsible for
the high sorption capabilities observed for type I materials.
The ordered mesoporous carbon (OMC) belongs to a
family of porous materials which attracted great attention
in recent years because of its unique features, such as high
surface area and uniform, large and tunable pore channels.
These features make OMC more attractive for use in the
Ð. Petrovic � A. Ðukic � K. Kumric � B. Babic �M. Momcilovic � N. Ivanovic � Lj. Matovic (&)
Vinca Institute of Nuclear Sciences, University of Belgrade,
P.O. Box 522, 11001 Belgrade, Serbia
e-mail: [email protected]
123
J Radioanal Nucl Chem
DOI 10.1007/s10967-014-3249-0
Author's personal copy
adsorption processes and thus, we found interesting to
investigate sorption properties and mechanism of sorption
of TcO4- onto the OMC which, to our knowledge, has not
been investigated previously. Recently, the OMC has been
investigated for the removal of bromate [18], uranium(VI)
[19] and dye molecules [20] from the aqueous solutions.
Experimental part
Material characterization
The OMC was synthesized under acidic conditions as
previously described by Momcilovic et al [21]. The
structure of the ordered mesoporous material has been
investigated using various characterization techniques:
X-ray diffraction (XRD), laser scattering particle size
analysis system, Fourier transform infrared spectroscopy
(FT-IR), Boehm method and batch equilibrium method for
determination of point of zero charge (pHPZC).
XRD pattern of the sample was recorded using a Sie-
mens D5000 diffractometer with filtered Cu Ka radiation
(k = 1.5406 A). The scanning range was 2h = 2�–80�,
with the scanning rate of 0.02�/s.
A Malvern 2000SM Mastersizer laser scattering particle
size analysis system was used to obtain quantitative parti-
cle size distributions (PSD) of the sample. The specified
resolution range of the system was from 0.02 to 2,000 lm.
Approximately 0.05 g of the OMC powder was dispersed
in 10 cm3 of water with a sonication in a water bath for
3 min. Particle and dispersant reflection indexes were
1.590 and 1.330, respectively.
The functional groups of the sample were determinate
by PerkinElmer Spectrum Two FT-IR spectrometer using
the pressed KBr pellets (1:100) technique.
The acidic and basic surface groups of the studied OMC
were determined by the Boehm method. The acidic sites were
determined by mixing 0.15 g of the OMC with 20 cm3 of
different bases (0.1 mol dm-3 NaOH, 0.05 mol dm-3
NaHCO3 or 0.05 mol dm-3 Na2CO3) in 25 cm3 beakers. The
beakers were sealed and shaken for 24 h. The solutions were
then filtered and titrated with 0.1 mol dm-3 HCl. Similarly,
the basic sites were determined by mixing 0.15 g of the OMC
with 20 cm3 of 0.1 mol dm-3 HCl. The obtained solution was
titrated with 0.1 mol dm-3 NaOH. The equation for deter-
mining the number of moles of surface acidic and basic func-
tional groups on the surface of OMC (nCSF, mmol g-1) is [22]:
nCSF ¼ cNaOH � VNaOHð Þinitial� cHCl � Vekv:HClð Þtitrant
� �
� V
Valiquot
� 1; 000 ð1Þ
where cNaOH and VNaOH are the concentration and volume
of the reaction base (NaOH) mixed with the OMC, cHCl
and Vekv.HCl are the concentration and equivalent volume of
titrant (HCl) added to the aliquot (Valiquot) taken from the
original sample (V).
The point of zero charge of the OMC sample was
determined by batch equilibration method using KNO3
(0.01 and 0.1 mol dm-3) as a background electrolyte.
Batch experiments were carried out at room temperature by
mixing 0.125 g of the OMC and 25 cm3 of the working
KNO3 solution with different initial pH values in PVC
bottles. Initial pH values of solution were adjusted with
0.1 mol dm-3 HNO3 and 0.1 mol dm-3 KOH. The solu-
tion with different initial pH values (pHi) were shaken on
mechanical shaker (Promax 2020, Heidolph, Schwabach,
Germany) for 24 h. After that, the liquid phases were
separated by filtration through a 0.45 lm microporous
membrane filter (Membrane Solutions LLC, Plano, TX)
and the final pH values of solutions (pHf) were measured.
Adsorption studies
Radioactive technetium (in the form of pertechnetate) was
obtained from a 99Mo/99mTc generator (Vinca Institute of
Nuclear Sciences, Belgrade, Serbia) and its radioactive
concentration was determined by a Capintec CRC-15 dose
calibrator (Capintec, Inc. Ramsey, NJ, United States).
CRC-15 dose calibrator has 6 cm diameter and 25 cm deep
ionization chamber well that allows convenient measure-
ments of virtually any radioisotope geometry. Ionization
chamber is filled with high pressure Argon gas. The effects
of the sample container, sample volume and activity con-
centration are minimized by optimizing the counting
geometries. Assays may be made reliably in the chamber
from as low as 1 lCi for most radioisotopes to as high as
8 Ci of 99mTc. The resolution of the instrument is
0.001 MBq, i.e. 0.01 lCi. The measurements of 99mTc
activity in aliquots were made using vial geometry.
Batch experiments were performed at room temperature
by mixing 0.04 g of well powdered OMC adsorbent and
10 cm3 of working 99mTcO4- solution in closed glass vials.
Experimental set-up is presented in Fig. 1. The total99mTcO4
- radioactive concentration in the working solu-
tion was 1.4 MBq cm-3 (37.8 lCi cm-3) at pH 4.0. The
initial pH was adjusted by adding 0.1 mol dm-3 HCl. The
samples were shaken on a laboratory shaker for 60 min at a
stirring speed 200 rpm for better mass transport with high
interfacial area of contact. After that, the liquid phases
were separated from the solid phases by filtration through a
0.45 lm microporous membrane filter. The residual
radioactive concentration of 99mTcO4- in each aliquot was
determined with a Capintec CRC-15 dose calibrator.
The effects of different experimental parameters, such
as contact time (1–180 min), solution pH (2.0–12.0), ionic
strength (0.01 and 0.1 M NaCl) and initial 99mTcO4-
J Radioanal Nucl Chem
123
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radioactive concentration (0.07–2.89 mCi cm-3) were
investigated with respect to the removal efficiency of
TcO4-. All experiments were carried out in duplicate, and
the data obtained were used for analysis.
Calculations
The removal efficiency (E, %), the distribution coefficient
(Kd, cm3 g-1) and the adsorption capacity (qe, mCi g-1) of99mTcO4
- were calculated using the following equations:
E ¼ Ai � Afð ÞAi
� 100 ð2Þ
Kd ¼Ai � Afð Þ
Af
� V
mð3Þ
qe ¼Ai � Aeð Þ
m� V ð4Þ
where Ai, Af and Ae are the initial, the final and the equi-
librium 99mTcO4- radioactive concentrations in the liquid
phase (MBq cm-3), V the volume of the solution (cm3) and
m the mass of adsorbent (g).
Results and discussion
Microstructural characterization
XRD pattern of the synthesized OMC is presented on
Fig. 2. Broad peaks located at the positions 2h = 22.5� and
2h = 43.6�, respectively, correspond to the amorphous
carbon and demonstrate that OMC has an amorphous
structure. Two resolved diffraction peaks attributed to the
(002) and (100) reflections are typical for the OMC [23,
24].
Figure 3 shows a PSD curve of the synthesized OMC.
The sample has a bimodal distribution of particles in the
range from 4.4 to 1905.5 lm, with the mean particle size of
7.5 and 447.2 lm. The percentage of the smaller particles
is about 1.5 % which indicates that the larger particles with
mean size of 447.2 lm are dominant in the sample. As
previously described by Momcilovic et al. [21], specific
surface area calculated by BET equation, SBET, is
712 m2 g-1. Also, calculated porosity parameters con-
firmed that OMC is mesoporous with certain amount of
micropores.
Distribution of positive and negative charge on the
surface of the particles of the adsorbent is one of the major
factors that influence the sorption uptake. In order to
understand the sorption mechanism, it is necessary to
determine the pH at which the surface has net neutral
charge (pHPZC). In the state when the sorbent surface has
zero point of charge, adsorption of target solute is carried
Fig. 1 Experimental set-up for the sorption of TcO4- onto the OMC
Fig. 2 XRD pattern of the ordered mesoporous carbon
Fig. 3 PSD curve of the ordered mesoporous carbon
J Radioanal Nucl Chem
123
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out by diffusion into micropores and mesopores. If the pH
of the solution is greater than values of the pHPZC, the
surface will have a negative charge and sorption of positive
ions will be favored due to the electrostatic attraction. The
sorption of negatively ions will be favored at pH values
lower than pHPZC [25]. In order to determine the pHPZC of
the OMC, the batch equilibration method was used. The
experimental results are represented in Fig. 4 as a function
of final pH values, pHf, from initial pH values, pHi, of the
solutions. The plateau obtained at pH 8.1 ± 0.2 correspond
to the pHPZC of the OMC. The same results of the values of
the pHPZC for all electrolyte concentrations (0.01 and
0.1 mol dm-3) indicate that the pHPZC of the OMC is
independent of the ionic strength of inert electrolyte
(KNO3). The high pHPZC value of the OMC of 8.1 ± 0.2 is
due to the basic oxygen groups (chromene and pyrone) and
the p-electron system of the basal planes of carbons [26].
The type and concentration of functional groups give the
amphoteric characteristics to activated carbons in aqueous
solution. Since infrared spectroscopy provides information
on the chemical structure of the adsorbent material, FT-IR
analysis was performed in order to identify surface func-
tional groups responsible for TcO4- sorption. The FT-IR
spectra is showed in Fig. 5, while the corresponding
assignments of FT-IR bands to the specific chemical bonds
are presented in Table 1.
The FT-IR spectra of the OMC shows absorption bands
due to aliphatic (bands at 2,974 and 2,886 cm-1 originate
from C–H stretching in –CH2– [27, 28], 1,450 cm-1
originate from –CH2– deformation [28]) and aromatic
structures (bands at 818, 756 and 700 cm-1 that originate
from the in-plane and out-of-plane aromatic ring defor-
mation vibrations of C–H in variously substituted benzene
rings [28, 29]). Bands at 1,111, 1,613 and 1,717 cm-1 are
vibrational modes assigned to stretching vibrations of C–O
and C=O, and indicate the significant presence of oxygen-
containing functional groups: carboxylic and phenolic
groups. Weak sharp absorption bands at 3,594 and
3,733 cm-1 present in spectra may be ascribed to isolated
O–H groups [27, 28]. However, the relative portions of
these groups cannot be determined from these spectra
because of the qualitative nature of FT-IR measurements.
It is well known that the most common functional
groups (containing oxygen) on the activated carbon sur-
faces are carboxyl, lactonic, carbonyl and phenolic groups.
The chemical titration method, such as proposed by Boehm
[22], determines the amount of acidic (carboxyl, lactonic
and phenol) and basic groups on the surface of carbon
materials. This method is especially useful when it is used
in combination with other techniques such as FT-IR ana-
lysis. The number of acidic and basic groups is presented in
the Table 2.
Fig. 4 Determination of the pHPZC of the ordered mesoporous carbonFig. 5 FT-IR spectra of the ordered mesoporous carbon
Table 1 FT-IR spectra band assignments for the ordered mesoporous
carbon
Band
number
(cm-1)
Assignment References
\820 C–H deformation modes in in-plane and
out-of-plane aromatic ring
[28, 29]
*1,115 C–O stretching vibration in phenolic and
carboxylic group
[26–28,
30]
*1,450 –CH2– deformation [28]
*1,613 C=O stretching vibration [27, 30]
*1,717 C=O in the carboxylic group [26–28]
*2,886,
2,974
C–H stretching vibration in methylene
and methyl group
[27, 28]
*3,594,
3,733
O–H stretching vibration in free O–H in
phenolic and carboxylic groups
[26–28]
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123
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As can be seen from the Table 2, on the surface of the
OMC dominates acidic groups, among which the most
prominent are phenolic groups. This is expected since the
resorcinol (1,3-isomer of benzenediol with the formula
C6H4(OH)2) was used as a precursor for the synthesis of the
OMC.
Adsorption studies
Effect of contact time
The effect of contact time on the sorption of TcO4- onto
the OMC was investigated at different contact times
ranging from 1 to 180 min (Fig. 6). As can be seen in
Fig. 6, the equilibrium adsorption was established after
60 min of contact and the maximum uptake (93 %) of
TcO4- was reached. Also, it is evident that the adsorption
rate increased rapidly in the first 5 min of adsorption, and
87 % of the TcO4- was adsorbed during this period of
time. This means that, after only 5 min of adsorption, the
removal efficiency of TcO4- exceeded 94 % of its value at
equilibrium. Such a rapid process indicates that the sorp-
tion is primarily a surface phenomenon, and the OMC
surface adsorbing sites (functional groups) are readily
available for TcO4- ions from the solution.
After equilibrium was reached, the contact time no
longer had an influence on the TcO4- sorption, and the
removal efficiency remained constant over the time period
observed (180 min). In addition, the distribution coeffi-
cient, Kd, as shown in the insert in Fig. 6, remained con-
stant at equilibrium state with the mean value of 3.5 9 103.
Therefore, the adsorption time of 60 min was selected as a
fixed parameter for the rest of the study.
Effect of initial pH and ionic strength
The effect of the solution pH and ionic strength, I, on the
adsorption of TcO4- using the OMC was investigated at
varying pH values from 2.0 to 12.0. The obtained results
are presented in Fig. 7. It is evident that the adsorption of
TcO4- was pH-dependent, with maximum removal effi-
ciency of 99 % at the pH value 2.0. Then, the removal
efficiency slightly decrease and reach the value of 93 % at
the pH values between 4.0 and 10.0. At the pH values
beyond 10.0, the adsorption of TcO4- decreased sharply
and the removal efficiency of TcO4- fell to 72 %. The
distribution coefficients, presented in the insert in Fig. 7,
behaved in a similar manner as a function of solution pH,
with the maximum Kd value of 6.6 9 103 at the pH 2.0,
plateau with the mean Kd of 2.9 9 103 at the pH range
from 4.0 to 10.0, and the Kd value less than 1 9 103 at the
pH [ 10.0. Under the investigated experimental condi-
tions, E and Kd values are insensitive to ionic strength
changes, indicating that the sorption of TcO4- was not
affected by the presence of competing Cl- ions. Xu et al.
[18] also found that the bromat removal from water using
OMC was independent on the presence of competing
anions.
As can be seen from Fig. 7, high removal efficiency of
TcO4- is achieved at pH B 10.0. Since the adsorption of
anions is favored at pH \ pHPZC, and having in mind that
pHPZC for the OMC is 8.1 ± 0.2, high removal efficiency
of TcO4- was expected to be achieved at pH \ 8.1 ± 0.2.
However, as known from the literature [31], the specific
adsorption of cations, shifts pHPZC toward lower values,
and the specific adsorption of anions shifts pHPZC to the
opposite direction. This enables the high yield of removal
efficiencies of anions, like TcO4- ions on the OMC, in
wider range of pH values (from 2.0 to 10.0).
Effect of initial radioactive concentration
The effect of the initial radioactive concentration on the
adsorption of TcO4- onto the OMC was studied by varying the
Table 2 Functional groups on
the OMC determined by Boehm
method
Adsorbent Basic groups
(mmol g-1)
Acidic groups
(mmol g-1)
Carboxylic groups
(mmol g-1)
Phenolic groups
(mmol g-1)
Lactonic groups
(mmol g-1)
OMC 0.1325 1.3367 0.0200 1.3033 0.0134
Fig. 6 Effect of contact time on the adsorption of TcO4- by the
OMC (at an initial radioactive concentration 1.3 MBq cm-3). Insert
variation of Kd values with contact time. Conditions: pH 4.0; stirring
speed, 200 rpm; concentration of adsorbent, 4 g dm-3. Vertical error
bars represent standard errors
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123
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99mTcO4- concentration from 0.07 to 2.89 mCi cm-3 in the
solution at pH 4.0. The obtained results are presented in
Table 3. As can be seen, the adsorption capacity of TcO4-
increased with increasing in the initial radioactive concen-
tration, whereas the removal efficiency remained more or less
constant (94.0–91.3 %) over the same concentration range.
Adsorption of TcO4- onto the OMC yielded linear adsorption
isotherm (Fig. 8), with an estimated Kd = 2.6 9 103 cm3 g-1
and the correlation coefficient R2 = 0.9961. The plateau was
not reached due to the fact that the TcO4- concentration in the
simulated groundwater was extremely low (in the order of
1.3 9 10-10 to 5.6 9 10-9mol dm-3, which is comparable
with the 99Tc activity found in the environment [1, 10, 11]),
and under the investigated experimental conditions the sur-
face of the OMC was far from being saturated with TcO4-.
Mechanism of TcO4- sorption onto OMC
Comparison of Kd value(s) obtained in this study with those
of other researchers [10–12] indicate that the TcO4-
adsorption by the OMC is well classed compared to other
carbon materials (adsorbents). Depending on the influence
of pH on the Kd values of the investigated activated car-
bons, Wang et al. [12] grouped them into two distinct
types. Type I materials have high sorption capabilities with
the Kd varying from 9.5 9 105 to 3.2 9 103 cm3 g-1 (in
the pH range from 4.5 to 9.5). Type II materials have
relatively low sorption capabilities with the Kd remaining
more or less constant (1.1 9 103–1.8 9 103 cm3 g-1) over
a similar pH range. In the same pH region (from 4.0 to
10.0) OMC exhibits plateau with the mean Kd of 2.9 9 103
as presented in Fig. 7. According to the value of Kd
(2.9 9 103 cm3 g-1) obtained for the OMC, it is clear that
the OMC cannot be classified into any of these two groups,
but somewhere in between, much more closely to the
materials of type II. Different sorption behavior between
the two types of materials was attributed to the different
distribution of surface functional groups (carboxylic and
phenolic) and, in the order of increasing acidity, the car-
boxylic groups were divided into three subgroups. The
presence of a large fraction of acidic carboxylic subgroups
was found to be responsible for the high sorption capa-
bilities observed for type I materials, where direct
involvement of C–TcO4 bonding occurs:
R� C� OH þ TcO�4 ! R� C� OTcO3 þ OH� ð5Þ
The low sorption capabilities of type II materials were
attributed to the exclusive presence of phenolic and car-
boxylic groups with lower acidity. The proposed main
mechanism of attaching the TcO4- to these functional
Fig. 7 Effect of pH and ionic strength (0.01 and 0.1 M NaCl) on the
adsorption of TcO4- by the OMC (at an initial radioactive concen-
tration 1.3 MBq cm-3). Insert variation of Kd values with pH and
ionic strength. Conditions: contact time, 60 min; stirring speed,
200 rpm; concentration of adsorbent, 4 g dm-3. Vertical error bars
represent standard errors
Table 3 Effect of the initial 99mTcO4- radioactive concentration, Ai,
on the removal efficiency, E, and equilibrium radioactivity adsorbed
per unit mass, qe, of the OMC
Ai, mCi cm-3 Ae, mCi cm-3 qe, mCi g-1 E, %
0.07 4.1 9 10-3 16.5 ± 0.3 94.0 ± 1.4
0.48 0.03 112.5 ± 1.8 93.8 ± 1.4
0.98 0.07 226.8 ± 2.8 92.6 ± 1.2
1.43 0.12 326.5 ± 4.6 91.3 ± 1.3
1.92 0.16 440.3 ± 6.2 91.7 ± 1.3
2.41 0.21 551.3 ± 7.1 91.5 ± 1.2
2.89 0.25 659.8 ± 9.8 91.3 ± 1.4
Fig. 8 Effect of the initial radioactive concentration on the adsorp-
tion of TcO4- by the OMC. Conditions: contact time, 60 min; pH,
4.0; stirring speed, 200 rpm; concentration of adsorbent, 4 g dm-3.
Vertical error bars represent standard errors
J Radioanal Nucl Chem
123
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groups was through either hydrogen bonding or electro-
static attraction (Eq. 6), where no consumption or release
of H? or OH- ions occurs:
R� OH�2 þ TcO�4 ! R� OH2 � OTcO3 ð6Þ
In order to verify the exact mechanism of TcO4- sorp-
tion onto the OMC, pH value of the TcO4- solution after
adsorption (pHf) was examined as a function of the initial
pH of the TcO4- solution (pHi). The obtained results are
presented in Fig. 9. A release of OH- induces a sharp
increase of pHf values. Also, as can be seen from the insert
in Fig. 7, surface chemistry of OMC is insensitive to ionic
strength indicating that the surface chemistry is controlled
by inner sphere chemical complexation rather than by
electrostatic interactions. This implies that the main
mechanism of TcO4- sorption onto OMC is displacement
of OH- with TcO4- as presented in Eq. (5), rather than
hydrogen bonding, which is equivalent to an outer sphere
complexation. Attaching of TcO4- to carboxylic or phe-
nolic functional groups through hydrogen bonding or
electrostatic attraction is unlikely because: (1) Kd value is
independent of pH in the pH region from 4.0 to 10.0, and
(2) the sorption has not been changed with the increase of
ionic strength of the medium. As a result, the direct C–
OTcO3 bonding in carboxylic groups (Eq. (5)) is expected
to be the main mechanism of sorption of pertechnetate ion
onto the OMC. Relatively low Kd value of 2.9 9 103 for
the OMC can be explained by the substantially smaller
number of carboxylic groups compared to the number of
phenolic groups present on the surface of OMC (Table 2).
The reaction occurs very rapidly indicating the sorption is
primarily a surface phenomenon.
Conclusions
Ordered mesoporous carbon has been investigated for its
sorption capability to remove pertechnetate (TcO4-) from
water. The mechanism of TcO4- sorption was proposed
and conclusions are summarized as follows:
– OMC has amorphous structure characteristic for carbon
materials with well defined pore sizes (mesoporous
with certain amount of micropores) and bimodal
distribution of particles with the mean particle size of
7.5 and 447.2 lm;
– Maximum Kd value of 6.6 9 103 cm3 g-1 was
obtained at pH 2.0;
– The adsorption of TcO4- is almost pH-independent in
very wide pH region (from 4.0 to 10.0);
– The sorption equilibrium was established after 60 min
of contact and the maximum uptake (93 %) of TcO4-
was reached. Such a rapid process indicates that the
sorption is primarily a surface phenomenon, and the
OMC surface adsorbing sites (functional groups) are
readily available for TcO4- ions from the solution;
– TcO4- interacts with carboxyl functional groups pres-
ent at the surface of the OMC by displacing the OH-
with TcO4- via ion exchange mechanism.
The obtained results indicate that the TcO4- adsorption
by the OMC is well classed compared to other carbon
materials (adsorbents). As a material resistant to aging (to
the oxidizing conditions and the presence of water), as well
as its good sorption properties, the OMC appears to be an
efficient adsorbent for the TcO4- removal from aqueous
solutions.
Acknowledgments We acknowledge the support to this work pro-
vided by the Ministry of Education and Science of Serbia through the
project No. III 45012.
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