aqueous mercury adsorption by activated carbon
TRANSCRIPT
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Review
Aqueous mercury adsorption by activated carbons
Pejman Hadi a, Ming-Ho To a, Chi-Wai Hui a, Carol Sze Ki Lin b,Gordon McKay a,c,*
a Chemical and Biomolecular Engineering Department, Hong Kong University of Science and Technology,
Clear Water Bay Road, Hong Kongb School of Energy and Environment, City University of Hong Kong, Tat Chee Avenue, Kowloon, Hong Kongc
Division of Sustainable Development, College of Science, Engineering and Technology, Hamad Bin KhalifaUniversity, Qatar Foundation, Doha, Qatar
a r t i c l e i n f o
Article history:
Received 14 October 2014
Received in revised form
19 December 2014
Accepted 9 January 2015
Available online 21 January 2015
Keywords:Activated carbon
Adsorption
Mercury
Porous structure
Sulfur functional groups
a b s t r a c t
Due to serious public health threats resulting from mercury pollution and its rapid dis-
tribution in our food chain through the contamination of water bodies, stringent regula-
tions have been enacted on mercury-laden wastewater discharge. Activated carbons have
been widely used in the removal of mercuric ions from aqueous effluents. The surface and
textural characteristics of activated carbons are the two decisive factors in their efficiency
in mercury removal from wastewater. Herein, the structural properties and binding affinity
of mercuric ions from effluents have been presented. Also, specific attention has been
directed to the effect of sulfur-containing functional moieties on enhancing the mercuryadsorption. It has been demonstrated that surface area, pore size, pore size distribution
and surface functional groups should collectively be taken into consideration in designing
the optimal mercury removal process. Moreover, the mercury adsorption mechanism has
been addressed using equilibrium adsorption isotherm, thermodynamic and kinetic
studies. Further recommendations have been proposed with the aim of increasing the
mercury removal efficiency using carbon activation processes with lower energy input,
while achieving similar or even higher efficiencies.
2015 Elsevier Ltd. All rights reserved.
Contents
1. Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 38
2. Preparation of activated carbon . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 39
3. Effect of treatment techniques on mercury removal . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 40
3.1. Physical and chemical activation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 40
3.2. Sulfurization . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43
* Corresponding author. Chemical and Biomolecular Engineering Department, Hong Kong University of Science and Technology, ClearWater Bay Road, Hong Kong. Tel.:852 23588412; fax: 852 23580054.
E-mail address:[email protected](G. McKay).
Available online atwww.sciencedirect.com
ScienceDirect
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4. Effect of adsorption parameters . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 44
4.1. Equilibrium contact time . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 44
4.2. Initial concentration . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45
4.3. pH value . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45
4.4. Temperature . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45
4.5. Adsorbent dosage and particle size . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 46
5. Mercury affinity to various functional groups . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 46
6. Equilibrium adsorption isotherms . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 507. Conclusion and future perspectives . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 51
References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 52
1. Introduction
Mercury is categorized as an extremely toxic substance whose
health hazards have primarily been associated with inhala-
tion of mercury vapor or ingestion of organic mercury viaaquatic organisms causing mercury poisoning, widely known
as Minamata disease (Harada, 1982). The absorption of this
hazardous substance into the bloodstream, its distribution to
the entire tissues and its bioaccumulation in the receptive
sites result in many well-recognized adverse effects, such as
potent neurotoxicity, blood vessel congestion and kidney
damages (Kidd and Batchelar, 2012).
The presence of mercury in the environment as a result of
naturogenic sources, such as geothermal eruptions and
seismic activities, represents only a small fraction of the total
annual mercury emission. The anthropogenic activities are
the major contributors for mercury pollution in the
ecosystem, among which the fossil fuel combustion plays themost dominant role. An overarching estimate of anthropo-
genic input of 16 elements into the environment by Nriagu
and Pacyna has revealed that mercury releases into the at-
mosphere and aquatic bodies are in the same range
(Ebinghaus et al., 1999; Nriagu and Pacyna, 1988). The
anthropogenic sources of mercurycan be divided intoprimary
and secondary sources. The former involves the mobilization
and release of mercury of geological origin to the environ-
ment, such as mining, industrial processing of ores or fossil
fuel combustion and more specifically coal. The latter is
associated with the direct use of mercury in industrial pro-
cesses, including vinyl chloride monomer production as
catalyst, batteries as cathodes and chlor-alkali production aswell (Pacyna et al., 2010). Improper discharge of effluents and
exhaust emissions from both primary and secondary sources
accounts for the environmental concerns over this toxic
compound. Despite the constraints in the usage of certain
toxic compounds by the Restriction of Hazardous Substances
Directive (RoHS), some substances, including mercury, have
been granted exemption to narrowly-defined applications due
to the technical/scientific impracticality of the substance
prohibition (United Nations Environment Programme, 2010).
Hence, it can be evidently remarked that complete elimina-
tion of mercury from the ecosystem is unrealistic due to the
uncontrollable discharge of mercury by primary anthropo-
genic sources and the inevitable, though limited, utilization of
mercury in industrial processes (secondary anthropogenic
sources).
Accordingly, as a result of the catastrophic impacts of
mercury presence in the ecosystem and its potential fatal
health consequences, many stringent regulations and di-
rectives have been enacted regarding the control of the mer-cury discharge into the environment (Sunderlan and Chmura,
2000). Therefore, many researchers have been engaged with
the removal of mercury from aqueous media. Numerous
techniques employed for this purpose include precipitation
(Blue et al., 2010; Hutchison et al., 2008; Matlock et al., 2001 ),
coagulation (Henneberry et al., 2011; Nanseu-Njiki et al., 2009),
cementation (Ku et al., 2002; Lo and Yu, 1988), ultrafiltration
(Barron-Zambrano et al., 2002; Han et al., 2014; Uludag et al.,
1997), solvent extraction (Huebra et al., 2003; Sevdic et al.,
1980), photocatalysis (Botta et al., 2002; de la Fourniere et al.,
2007; Lopez-Mu~noz et al., 2011), adsorption (Aguado et al.,
2005; Antochshuk and Jaroniec, 2002; Bandaru et al., 2013;
Cui et al., 2013; Di Natale et al., 2011; Li et al., 2011, 2013;Mondal et al., 2013), ion exchange (Anirudhan et al., 2008;
Chiarle et al., 2000; Gash et al., 1998; Lloyd-Jones et al., 2004 )
or a combination of these methods (Barron-Zambrano et al.,
2004; Byrne and Mazyck, 2009). However, the challenges con-
cerning some of these methods include high energy demand
for process operation, large amounts of chemicals used, high
operation and/or capital costs, removal inefficiency and
unselectivity (Ismaiel et al., 2013; Li et al., 2011; Taurozzi et al.,
2013; Wajima and Sugawara, 2011). Among all these removal
techniques, adsorption has been found to be a very promising
method for the removal of heavy metals from wastewater
streams owing to the ease of operation, heavy metal removal
efficiency, high adsorption rate, selective removal and theavailability of a wide range of adsorbent materials (Hadi et al.,
2014a, 2013a, 2013b, 2013c, 2013d; Ismaiel et al., 2013; Nabais
et al., 2006; Ramadan et al., 2010; Xu et al., 2014). Among all
types of adsorbent materials including extracellular bio-
polymers (Inbaraj et al., 2009), cellulosic materials (Takagai
et al., 2011), zeolites and aluminosilicates (Liu et al., 2013;
Somerset et al., 2008), nanomaterials (Bandaru et al., 2013)
and activated carbons (Anoop Krishnan and Anirudhan, 2002;
Di Natale et al., 2011; Ranganathan, 2003), the latter has gained
considerable attention both in research-based studies and
practical industrial applications. Also, some studies have
argued the high cost of activated carbon materials is still an
important problem and have resolved the issue by using
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waste-derived activated carbons to diminish the production
cost of this adsorbent (Kadirvelu et al., 2004; Mohan et al.,
2001; Rao et al., 2009; Zabihi et al., 2010; Zhang et al., 2005).
The current work aims at reviewing the adsorptive removal
of aqueous mercury from effluents by activated carbons. The
focus of this paper is to present a comprehensive overview of
the activated carbon preparation by chemical and physical
methods, their modification techniques, their mercuryremoval efficiencies and the effect of various parameters,
such as pH, initial concentration, activated carbon amount,
adsorbent particle size and temperature, on mercury uptake.
These factors are of the utmost significance, as any change in
these parameters may considerably change the mercury
removal efficiency of an adsorbent. Therefore, a general
knowledge of the effect of these parameters is critical in
designing the appropriate mercury-laden wastewater treat-
ment facilities.
2. Preparation of activated carbon
Activated carbons have long been used as absorbent for the
removal of various pollutants. Textural properties of activated
carbons and functional groups on their surface are two of the
principal characteristics which should be enhanced by certain
modification processes in order to make them exhibit high
pollutant removal efficiencies.
Physical and chemical activation techniques are the most
commonly-used approaches to develop high internal porosity
and desired pore size and also to introduce certain functional
groups onto the adsorbent surface (Hadi et al., 2015).
The physical activation mainly involves two steps,
carbonization and activation. Carbonization includes a heattreatment of a carbonaceous precursor at moderate temper-
atures, mainly below 700 C, in an inert atmosphere to pyro-
lize the precursor material into a low surface area char.
Carbonization leads to the partial evolution of the volatile
matter from the carbonaceous precursor, enriching the pro-
duced char in carbon content and developing the preliminary
branched porous structure. For a carbonization temperature
up to 700 C, the volume of the micropores gradually in-
creases, while furtherincrease in the temperature reduces the
pore volume of the material. The produced char is subse-
quently activated at elevated temperatures, usually above
700 C, under a partial oxidizing atmosphere (primarily steam
or carbon dioxide as gasifying agents) (Hadi et al., 2015). Theaim of the activation stage is to produce a highly porous
structure from the weakly-developed porous char. The acti-
vation process entails the reaction of the oxidizing agent with
tar decomposition products blocking the pores to volatilize
carbon oxide, which, in turn, opens the closed pores, widens
the existing small pores and forms new pores. The resulting
activated product at this stage has high pore volume and
surface area, therefore enhancing its ability for the removal of
pollutants by capturing absorbate molecules in its porous
network (Budinova et al., 2006; Hadi et al., 2014b). The
simplified gasification reactions of the oxidizing agents with
carbon have been illustrated according to the following stoi-
chiometric equations:
C CO2/2CO DH 159 KJ mol1 (R1)
C H2O/CO H2 DH 117 KJ mol1 (R2)
The chemical activation technique is a one-step process in
which the carbonization and activation processes occur
simultaneously. During chemical activation, the source ma-
terial is submerged in a dehydrating compound (such asphosphoric acid, zinc chloride, alkaline hydroxides or alkaline
carbonates) resulting in the diffusion of the chemical reagent
into the particles and its incorporation into the carbon struc-
ture. The resultant slurry is then heatedup to temperatures in
the rangeof 400e600 C under an inert atmosphere. This leads
to the depolymerization of cellulose, hemicellulose or lignin
catalyzed by the chemical reagent, followed by dehydration
and condensation leading to the formation of more aromatic
and reactive products. Also, in some cases, the alkaline metals
are intercalated between the graphene layers while creating
some porosity by the oxidation of carbon into carbon oxides
(Marsh and Reinoso, 2006). This intercalation inhibits the
contraction of the carbonaceous precursor during the heattreatment.
Energy required for chemical activation process is consid-
erably lower than that of physical activation method. Signifi-
cantly lower activation temperatures, shorter reaction time
and employment of a single-step treatment in the case of
chemical activation process account for this low energy con-
sumption. Moreover, it has been reported that, in most cases,
both carbon yield and specific surface area for the materials
produced by chemical activation are higher than those of the
physical activation method. These two reasons account for
the more extensive application of the chemical activation
method compared with the physical one (Macia-Agulloet al.,
2004).Although, commercial activated carbons have been widely
used in various industries to remove mercury from waste-
water streams, their use has been recently challenged by their
high cost (Di Natale et al., 2006). Hence, much research has
recently been devoted to the exploration of alternative waste-
based carbon sources as precursor for activated carbon pro-
duction. Toles et al. found that it is highly profitable to pro-
duce almond shell-based granular activated carbon (GAC) at
US$20/ton compared with two comparable commercial GACs
at about US$3.3/kg using it as a basis for economic feasibility
study (Toles et al., 2000). Considering such a great financial
incentive, numerous researches have been conducted on
certain inexpensive waste precursors to produce cost-effective activated carbons with high pollutant removal effi-
ciencies. Among certain precursor materials to be used in
activated carbon production, high mercury adsorption ca-
pacities have been reported using coirpith (Namasivayam and
Kadirvelu, 1999), furfural (Yardim et al., 2003), walnut shell
(Zabihi et al., 2010), agricultural solid waste (Kadirvelu et al.,
2003), silk cotton hull (Roberts and Rowland, 1973), sago
waste(Kadirvelu et al., 2004), coconut tree sawdust, maize cob
and banana pith (Kadirvelu et al., 2003) while moderate to low
adsorption capacities have been observed for activated car-
bons derived from pazzolana and yellow tuff (Di Natale et al.,
2006), Fullers earth (Oubagaranadin et al., 2007), Ceiba-
pentandra hulls, Phaseolus aureus hulls and Cicerarietinum
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(Rao et al., 2009). Hence, it can be inferred that the type of
precursor is an influential factor in determining the adsorp-
tion efficiency of the activated carbons.
3. Effect of treatment techniques on mercuryremoval
3.1. Physical and chemical activation
The nature of precursor materials and their activation
methods directly influences the surface area, pore size and
functional groups on the surface of the prepared activated
carbons which can, in turn, have an influence on the mercury
removal efficiency.Tables 1 and 2show the effect of the pre-
cursor type and activation conditions on mercury adsorption
capacities of the prepared activated carbons.
A suitable activation procedure leads to the production of a
high surface area adsorbent material and thus, reasonably
high mercury removal efficiency. Budinova et al. have
demonstrated the effect of steam activation and air oxidationon the specific surface area of a carbonaceous biomass waste.
Sample activated with steam showed significantly higher
surface area than the one oxidized in air atmosphere. This
resulted in a higher mercury adsorption capacity for the
steam-activated adsorbent as compared with the air-oxidized
adsorbent (Budinova et al., 2003). A more detailed study of the
activated carbon preparation conditions under various at-
mospheres has been reported elsewhere (Budinova et al.,
2006). Water vapor has been shown to penetrate into the
carbon structure, react with the carbon at the internal surface
of the carbon and extract the carbon from the pore walls,
resulting in the enlargement of the existing pores and creation
of new pores (as shown in the reaction R2) and thereby anincrease in the adsorption capacity of the produced adsorbent.
It has been demonstrated that the pore size and pore size
distribution of activated carbons can be manipulated by using
different activating atmospheres. Molina-Sabio et al. have
shown that steam-activated carbons exhibit larger mesopores
compared to carbons activated under a CO2 atmosphere
(Molina-Sabio et al., 1996). This will, undoubtedly, influence
the adsorption behavior of these adsorbents towards various
adsorbates. However, no comprehensive study has been
conducted on the effect of activation atmosphere, which, in
turn, results in a change in the surface functionalities of the
adsorbents, to maximize mercury removal from effluents.
In addition to the activation conditions, both surface areaand functional groups are predominantly affected by the na-
ture of the precursor material used. As shown in Table 1,
Ekinci et al. have found that, under similar activation condi-
tions, the surface areas range from 460 to 720 m2:g1 for coal-
based activated carbons and 1000 and 1110 m2:g1 for apricot
stone and furfural-based activated carbons, respectively
(Ekinci et al., 2002). The difference in the textural properties of
these produced activated carbons is reflected in their mercury
adsorption capacities. Furthermore, Rao et al. compared the
mercury removal efficiencies of activated carbons prepared
from three different carbonaceous precursors under similar
activation conditions and observed huge differences in their
surface areas and adsorption capacities (Rao et al., 2009).Table1e
Effectoftheprecursortype
andphysicalactivationconditionson
themercuryremovalefficienciesof
theactivatedcarbons.
Carbonizationconditions
Activationconditions
SBET
qm
Vt
Vmicro
Vmeso
Dp
Ref.
T(C)
T(h)
HRa
(Cmin
1)
Atm.
T(C)
T(h)
HR(Cmin
1)
Atm
.
(m2
g
1)
(mgg
1)
(cm
3
g
1)
(cm
3
g
1)
(cm
3
g
1)
(nm)
200
2
750
2
20
H2O
521
25.8
8
(Raoeta
l.,
2009)
325
23.6
6
280
22.8
8
600
1
3
N2
761
0.6
81
0.2
97
0.3
21
2.3
2
(Budinovaetal.,
2006)
750
2
10
H2O
1100
174
0.8
9
0.4
25
0.1
1
(Budinovaetal.,
2003)
400
H2O
480
134
0.6
4
0.2
1
0.0
85
750
2
10
H2O
600
92
(Ekincie
tal.,
2002)
460
56
720
105
520
37
1000
153
1100
174
500e950
10
N2
(Inbaraj
andSulochana,
2006)
890
9
5
N2
&
CO2
1528
0.6
4
(Macia-A
gulloetal.,
2004)
890
22.5
5
N2
&
CO2
2487
0.8
6
800
1
5
N2
900
5
15
N2
&
CO2
997
0.3
7
(Nabaisetal.,
2006)
900
5
N2
702
140
2.7
22.5
(Choian
dJang,
2008)
850
1
N2
&
H2O
870
4.9
3
0.4
28
0.3
28
0.0
04
1.9
67
(Luetal.,
2014)
a
HRdenotesheatingrate.
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Table 2 e Effect of the precursor type and chemical activation conditions on the mercury removal efficiencies of the activated carbo
Carbonization/Activationconditions
Chemical treatment SBET qm Vt Vmicro
T (C) T (h) HRa
(C min1)Atm. Chem. Conc. Imp. Rb Imp.tc (h) (m2 g1) (mg g1) (cm3 g1) (cm3 g1)
600/600 1/1 3 H2O/N2 1290 0.939 0.471
700 2 H2O 1360 160 1.026 0.485
600 10 N2 H2SO4 Conc. 1:20 1050 154 0.827 0.38
H2SO4 Conc. 10
10
10
10
10
200/450 1 Air H2O2 629 18.1
H2SO4 & (NH4)2S2O8 50% 1:200 0.5 625 55.6
600/800 1 N2/H2O H2SO4 Conc. 1100 174 0.425
H2SO4 & (NH4)2S2O8 Conc. 3: 5 & 1:33 12 592 154
400/700 0.5/1 NaOH 20% (W/V) 2 379.4 52.7
N2 ZnCl2 98% 1:0.5 780 151.5
1:1 803 100.9
H2SO4 Conc. 1:1.8 24 208.1 109.9
K2CO3 33-75% 1:1 2 1260 129 0.492
KOH 1:2 1 1090 0.49
1:4 1 1635 0.78
1:6 1 2225 0.9
1:8 1 2420 0.94
NaOH 1:2 1 1130 0.51
1:4 1 2000 0.81
1:6 1 2541 0.96
1:8 1 3033 1.02
800/900 1/5 5/15 N2 & CO2 S 1:3 2 848 410 0.33
H2S 1 905 450 0.33
900 5 N2 Pyrrole 1:3 413 541 1.52
43:100 346 682 1.04
11:20 158 441 0.54
900 N2 922 301 0.87 0.37 900 H2S 785 351 0.78 0.31
200 SO2, H2S & N2 764 351 0.72 0.3
200/400 2/1 10 H2O, SO2 & H2S 500.5 227.3 0.43
H2O & SO2 506.5 222.2 0.48 0.04
H2O,&H2S 530.2 217.4 0.48 0.06
H2O 536.5 208.3 0.52 0.13
800 0.5 N2 K2S 1:3.6 30.0 235.7
850 0.5 30.0 243.9
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Table 2 e (continued)
Carbonization/Activationconditions
Chemical treatment SBET qm Vt Vmicro
T (C) T (h) HRa
(C min1)Atm. Chem. Conc. Imp. Rb Imp.tc (h) (m2 g1) (mg g1) (cm3 g1) (cm3 g1)
900 0.5 28.0 254.4
1000 0.5 30.0 224.1
H2O2 3:10 168 836.0 100 0.23
H2 & CS2 778.0 170 0.18H2O2 & He 950.0 110
H2O2, He & CS2 776.0 175 0.22
He 880.0 110
2 50 N2 S 2:1 645.0 467
2:1 594.0 507
2:1
2:1 1070.0 827
2:1 1045.0 427
700 4 HCl 1 N 4 311.0 9.32
H2SO4 13 M 1:5 0.33 66.0 303.03
13 M 1:5 0.33 384
H2SO4 12 M 1:9 0.5 19.0 385
12 M 1:9 0.5 526
HNO3, SOCl2 &
C2H4(NH2)2
5 M, 5%
&0.05 M
3: 20 & 3:8 7 120
H2O2 30% 1:2 829.0 5 0.413 0.318
2:5 825.0 4.2 0.408 0.315
600 10 N2 SO2 1:25 0.5 720.9 122.8
600 1:25 1 772.5 129.8
600 1:25 2 776.4 130.5
600 1:25 3 790.7 131.6
600 1:50 1 773.7 128.2
600 2:25 1 518.5 114.8
600 1:25 1 757.2 125.7
500 1:25 1 764.1 135.9
700 1:25 1 751.3 184.2
800 1:25 1 1087.0 196.8
900 1:25 1 1057.0 207.8
TOMATS 1:0.3 48 107.7 83.3
HNO3 0.01 M 72 136.7 315.8 HSCH2COOH,
(CH3CO)2O & H2SO4
13 193.7 694.9
a HR denotes heating rate.b Imp. R denotes impregnation ratio.c Imp. t denotes impregnation time.
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Nonetheless, although specific surface area is one of the fac-
tors affecting the mercury adsorption, it is not the only
influential parameter. Zabihi et al. prepared two activated
carbons with surface areas of 780 and 803 m2:g1, while their
mercury adsorption capacities were 151 and 101 m2:g1,
respectively (Zabihi et al., 2009). Also, the surface areas of the
activated carbons prepared by Roa et al. ranged from 280 to
521 m2:g1, whereas their mercury adsorption capacitiesunder similar adsorption conditions did not exhibit a signifi-
cant difference (Rao et al., 2009). Wang et al. demonstrated
that an activated carbon with a surface area of 1896 m2:g1
had a much smaller adsorption capacity than an activated
carbon with a surface area of 1070 m2:g1 (160 vs 827 m2:g1,
respectively) (Wang et al., 2009). Since the size of the solvated
mercury is much larger than the nitrogen molecules, the pore
size and pore size distribution of the produced activated car-
bons besides their specific surface area is of significance.
Hence, it can be concluded that other factors, such as surface
functional groups, pore size and pore size distribution also
have considerable effects besides surface area in mercury
removal. Nevertheless, few studies have simultaneouslyinvestigated the effects of pore structure and functional
groups on mercury removal.
Considering the surface areas listed inTables 1 and 2, it is
noticeable that the chemical activation technique has greater
performance in pore formation at appropriate chemical re-
agent to adsorbent ratio. Comparing the surface areas ob-
tained by chemical and physical activation of coal tar pitch
carbon fibers, it is obvious that although high surface area
activated carbon (2487 m2:g1) can be obtained by physical
activation, it is not an economical option in terms of energy
consumption due to prolonged activation time at a high
temperature (22 h at 890 C) causing an excessive carbon burn-
off (94%). On the contrary, chemical activation of this materialusing an alkaline solution as activating reagent(KOH or NaOH)
at an impregnation ratio of 6:1 (w/w) yields activated carbon
with similar pore width and higher surface area. Other ad-
vantages of the chemically activated carbon are higher prod-
uct yield (60% and 27%, respectively), lower activation
temperature (750 C) and shorter activation time (1 h). The
highestsurface area (3033 m2:g1) can be obtainedusing NaOH
as activating agent at an impregnation ratio of 8:1 (w/w)
(Macia-Agulloet al., 2004).
In order to enhance mercury adsorption, several authors
have studied the combination of chemical and physical acti-
vation techniques. Budinova et al. confirmed that when the
H3PO4-impregnated carbonaceous sample was treated understeam atmosphere, both the surface area and iodine number
were considerably higher than the samples pyrolyzed under
nitrogen atmosphere. They also revealed that the concentra-
tion of the chemical reagent used for impregnation has a
significant effect on pore development. When the concentra-
tion of phosphoric acid was increased from 20% to 50%, the
mercury adsorption capacity of the activated carbon was
enhanced considerably (Budinova et al., 2006; Yardim et al.,
2003). Although no in-depth reason was provided for this
phenomenon, we believe that increasing the acid concentra-
tion increases the rate of the pyrolytic decomposition of the
precursor and enhances the density of the cross-linked
structure due to the catalytic effect of the phosphoric acid
and thus results in the modification of the textural properties
of the activated carbon.
3.2. Sulfurization
The binding ability of the carbonaceous compound surfaces
with sulfur-containing functional groups is well-recognized
(Cai and Jia, 2010; Hsi et al., 2001; Korpiel and Vidic, 1997;Vitolo and Pini, 1999; Wang et al., 2009). It has been widely
verified that sulfurization of activated carbons results in
enhanced adsorption capacity and selectivity towards mer-
cury. Therefore, the application of sulfur-functionalized acti-
vated carbons in the removal of mercury has become a
common practice. A variety of techniques have been
employed to immobilize sulfur on the surface of adsorbents,
including treatment with carbon disulfide (CS2), sodium sul-
fide (Na2S), hydrogen sulfide (H2S), sulfur dioxide (SO2) or
sulfur powder, with the aim of increasing their mercury up-
takes (Feng et al., 2006a; Fouladi Tajar et al., 2009; Mohan et al.,
2001; Vitolo and Pini, 1999; Wajima et al., 2009; Zhang et al.,
2003). Nabais et al. have applied two modification tech-niques, namely impregnation with elemental sulfur and using
hydrogen sulfide gas as modifying agent. Both of these ad-
sorbents exhibited higher adsorption capacities than the un-
sulfurized activated carbons (Nabais et al., 2006). Asasian
et al. found a 50% increase in mercury adsorption capacity by
sulfurizing the activated carbon with 4% sulfur dioxide gas
stream (Asasian et al., 2014). Wang et al. have studied the ef-
fect of the impregnation of activated carbon with elemental
sulfur. Elemental sulfur not only can directly deposit on the
adsorbent surface and interact with mercury, but also can
react with the adsorbent surface and lead to the formation of
new functional groups to enhance mercury adsorption (Wang
et al., 2009). They found that the mercury adsorption capacityof the unmodified and modified activated carbons were
190 mg:g1 and 820 mg:g1, respectively. The chemical reac-
tion between elemental sulfur and the surface of the adsor-
bent leads to the formation of disulfide, thiophene, sulfoxide
and sulfone groups that have more affinity to mercuric ions
and can enhance the overall mercury adsorption capacity and
selectivity (Cai and Jia, 2010; Wang et al., 2009). Mohan et al.
have observed a doubled mercury uptake after soaking the
adsorbent in carbon disulfide (Mohan et al., 2001). Despite the
well-acknowledged sulfur effect on mercury sequestration,
the processof sulfurbinding onto the activated carbon surface
and consequently, the mechanism of mercury adsorption
onto sulfur-containing moieties have not been satisfactorilyexploited and established. An in-depth understanding of the
activation and mercury adsorption mechanisms will assist in
designing a proper activation/functionalization procedure in
order to achieve high mercury abatement. Pillay et al. have
investigated the activation and adsorption mechanisms using
Raman spectroscopy as an analytical tool to monitor the
changes in the functional groups before and after the
adsorption process (Pillay et al., 2013). They verified the
presence of S]CeS bonds (at 475 cm1, 495 cm1 and
503 cm1) associated with thiol and thioester groups after
treating the virgin carbon nanotube with phosphorus penta-
sulfide. Subsequent mercury adsorption revealed significantly
diminished intensities of the bands corresponding to the thiol
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groups and appearance of new band assigned to Hg(SH)2and
Hg2(SH)2bonds on the used adsorbent material. In addition to
interaction with thiol moieties, weak chemisorption between
the mercury and hydroxyl groups were also noticed by the
reduction of hydroxyl peak intensity at 620 cm1 and the
formation of new peak at 550 cm1 corresponding to HgeO
bond, indicating strong binding of mercury ions to the thiol
groups rather than oxygen functional groups. Furthermore,Nabais et al. have identified the presence of SeS, C]S, CeS
and SeO bonds by FT-IR analysis after sulfurization, but
changes in the intensities of these peaks after the mercury
adsorption have not been provided (Nabais et al., 2006).
Due to the affinity of sulfur functional groups with mer-
cury, higher amounts of sulfur moieties will theoretically be
advantageous in mercury removal. Several researchers have
reported the direct linear relationship between mercury up-
take and sulfur content (Cai and Jia, 2010; Pillay et al., 2013).
However, Wang et al. have ruled out this hypothesis and have
demonstrated that the activated carbon with lower sulfur
amount (22%) on its surface had a higher mercury uptake than
the adsorbent with higher sulfur content (34%) (Wang et al.,2009), but no justification has been provided in the paper.
However, the aggregation of sulfur within the large pores,
rather than the uniform distribution of sulfur on the activated
carbon, may account for this phenomenon. Also, Nabais et al.
have compared several sulfur introduction methods and
identified that mixing of activated carbon fibre (ACF) with
solid sulfur at a ratio of 1:3 (w/w), followed by treatment at
600e800 C resulted in the production of an adsorbent with
higher sulfur content compared with the introduction of sul-
fur to ACF via gas stream H2S. This may be reasonable due to
the melting, recrystallization and deposition of the solid sul-
furon the activated carbon surface at such high temperatures.
However, subsequent mercury adsorption tests showed thathigher mercury uptake was obtained by the latter method
which elucidated the importance of the type of sulfur func-
tional groups on the carbon surface besides its quantity
(Nabais et al., 2006). This may also occur due to the aggrega-
tion of the sulfur on the activated carbon when solid sulfur is
used as the surface modifying agent which diminishes the
effect of sulfur functional groups in mercury removal.
Furthermore, despite similar sulfur contents of K2S-impreg-
nated coal samples were prepared at three distinct tempera-
tures (800e1000 C), whereas the activated carbon sample
prepared at 900 C exhibited the highest and fastest adsorp-
tion (Wajima and Sugawara, 2011). This indicates that the
sulfur content on the adsorbent surface, type of sulfur func-tional groups and porous structure of the activated carbons
collectively influence their mercury adsorption efficiency.
In addition to higher capacity, exceptional affinity between
mercury and sulfur has been demonstrated in a multi-
component system of mercury, cadmium and lead where
highly-selective adsorption towards mercury was achieved
(Gomez-Serrano et al., 1998). The superior adsorption of
mercury on sulfur-grafted adsorbent is believed to originate
from the Pearson acid-base concept in which the hard acids
prefer to coordinate with hard bases and soft acids react in a
higher rate with soft bases. Accordingly, the soft acid mercury
species in the solution, such as HgCl2, (HgCl2)2, Hg(OH)2 and
HgOHCl tend to predominantly react with sulfur groups (soft
bases) on the adsorbent surface (Cai and Jia, 2010). This phe-
nomenon has also been confirmed by comparing the inter-
action of HgX2(where X is a halide) with C4H8O and C4H8S. It
has been reported that HgX2interacts weakly with C4H8O, but
much stronger with C4H8S (Farhangi and Graddon, 1973;
Fisher and Drago, 1975). Vazquezet al. have related the
higher affinity towards mercury in a multi-component system
of cadmium, zinc and mercury to the higher electronegativityof mercury (Vazquez et al., 2002).
4. Effect of adsorption parameters
4.1. Equilibrium contact time
Equilibrium contact time is the period of time required for the
adsorption and desorption processes to reach equilibrium.
When the equilibrium is reached, the amount of adsorption
from the solution to the adsorbent surface equals the amount
of desorption from the adsorbent surface to the solution and
no further increase in the uptake occurs. The adsorptionprocess involves several steps including mass transfer from
bulk fluid phase to the particle surface across the boundary
layer, adsorption on the surface of the adsorbent and diffusion
within the pores (Wang et al., 2011). Depending on which of
these steps is the rate determining stepand also depending on
the boundary layer thickness and diffusion rate, the contact
time required to reach equilibrium will be different.
Adsorption of mercury has been shown to comply with a
general trend in which the mercury uptake rate is very fast at
the beginning because of the large number of vacant func-
tional group sites on the surface of activated carbon available
for the mercury ions.As the sitesare occupied in the course of
time, the uptake rate is gradually slowed down until a plateauis reached upon equilibrium (Zabihi et al., 2009). Shorter
contact time required by the adsorbent to reach equilibrium is
economically more favorable in industry.
Kadirvelu et al. have suggested that the rate of adsorption
depends on several factors such as the type of precursor used
for adsorbent production, pore size and pore size distribution
and concentration of functional groups (Kadirvelu et al., 2004).
Namasivayam and Periasamyhave reported that the activated
carbon from bicarbonate-treated peanut hull (BPHC) exhibited
7 times higher adsorption rate compared with commercial
activated carbon. They ascribed this high adsorption rate to
higher porosity and ion exchange ability of BPHC resulting in
less adsorption time required to acquire a certain mercuryremoval percentage and thus more cost effectiveness
(Namasivayam and Periasamy, 1993). Also, rapid mercury
adsorption of less than 20 min to reach equilibrium was re-
ported for activated carbons prepared from antibiotic waste
and rice husk ash as precursors (Budinova et al., 2008; Feng
et al., 2004). It can be hypothesized that as the pore size in-
creases up to a certain extent, the diffusion path is reduced
and the adsorption rate increases. Also, higher concentration
of adsorption sites will increase the probability of contact
between mercury molecules and functional moieties and
therefore increase the uptake rate. Hence, it is believed that
more abundant adsorption sites with an optimum pore size
for mercury will increase the rate of mercuryadsorption. More
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studies are necessary to be conducted to prove these hy-
potheses regarding the relationship between mercury
adsorption rate and textural and surface properties of the
adsorbents.
It has been further demonstrated that as the initial con-
centration of mercury increases, the Lagergren rate constant
decreases and thus, longer time is required to achieve equi-
librium (Namasivayam and Kadirvelu, 1999; Namasivayamand Periasamy, 1993). This could be due to the saturation of
sites presenton the exterior of adsorbent surface by adsorbate
at an initial stage of adsorption. Further adsorption can only
occur by the diffusion of the mercury ions into the pores and
adsorption in the interior surface of the pores which requires
relatively longer contact time (Hameed, 2007). Hence, in
modeling the mercury adsorption kinetics, a combination of
pseudo-type models with diffusion models is worthy of
consideration to elucidate the adsorption mechanism. How-
ever, for certain applications, these models have been shown
to be inconclusive (Plazinski et al., 2009).
4.2. Initial concentration
In general, the mercury adsorption experiments display a
direct relationship between the metal uptake and initial con-
centration of the metal ions present in the solution up to a
certain limiting initial concentration and inverse relationship
between the removal percentage and initial metal concen-
tration. An apparent distinction has to be drawn between
removal percent and adsorption capacity. The former term
does not reflect the efficiency of the material in mercury
removal at various initial concentrations and adsorbent dos-
ages, whereas the latter takes into account the adsorbent
dosage and reveals the genuine mercury adsorption efficiency
of the material at different initial concentrations. Several au-thors have reported complete mercury removal (Mohan et al.,
2001; Rao et al., 2009; Wahi et al., 2009). But when the initial
concentration and adsorbent amount are taken into consid-
eration, the adsorption capacity is found very small in some
cases. Therefore, reporting mercury removal percentage is
highly discouraged due to misleading results (Hadi et al.,
2015). As the initial concentration of mercury in the solution
increases, the percent removal of the adsorbate decreases
because of the presence of more mercury ions and limited
adsorption sites on the adsorbent materials. On the other
hand, at low mercury concentrations, the adsorption capacity
of the adsorbent material is low, while it increases by
increasing the initial concentration. This has been related tothe fact that at low mercury concentrations, the adsorption
sites are not completely occupied (Budinova et al., 2008, 2003;
Zabihi et al., 2009), whereas increasing the initial concentra-
tion of mercury results in higher collision probability between
the adsorbate molecules and adsorbent active sites, higher
occupation of active sites and thus higher adsorption capacity
(Zabihi et al., 2010). When the initial mercury concentration is
sufficiently increased, the adsorption capacity reaches a
plateau and does not increase anymore by increasing the
initial mercury concentration. This has been attributed to the
full occupation of the active sites on the surface of the
adsorbent at a certain initial concentration above which no
more adsorption enhancement can be achieved. Inbaraj and
Sulochana have observed a similar trend and have suggested
that this effect is caused by an increase in the driving force
offered by concentration gradient at high mercury concen-
trations (Inbaraj and Sulochana, 2006).
4.3. pH value
Adsorption of mercury is a highly pH dependent process. As
the pH value of the solution increases, more mercury uptake
occurs. The increased adsorption of mercury ion has been
shown to be related to the species of mercury present in the
solution at various pH values and their solubility. Higher pH
values of the solution results in the presence of more soluble
mercuric species which, in turn, promotes the effective con-
tact between the adsorbate molecules and the adsorbent
materials thus enhancing the possibility of the mercury up-
take by the porous adsorbent particles (Adams, 1991; Lopes
et al., 2010; Namasivayam and Periasamy, 1993). Moreover,
lower pH values increase the solubility of the mercuric ions
and thus their subsequent desorption from the activated
carbon surface into the solution. Therefore, the relative
attraction between the adsorbent and adsorbate is lower than
between the adsorbate and the solvent phase at lower pH
values, leading to the lower adsorption of the mercuric ions.
Solution acidity also plays an important role in the ioni-
zation of the functional groups on the adsorbent surface. In
acidic environment, high concentration of hydronium ion
(H3O) in the solution drives the equilibrium ionization reac-
tion (reaction R4) to the left and prevents the formation of
ionized functional groups, thereby hampering the ion ex-
change reaction between metal ions and adsorbent surface
functional groups (reaction R5). When the pH level of the so-
lution increases to above 4, the hydronium ion concentration
in the solution decreases. This shifts the equilibrium reaction
R4 to the right resulting in the availability of more ionized
functional groups for ion exchange and therefore an increase
in the metal uptake (Eligwe et al., 1999).
Adsorbent COOH4Adsorbent COO Haq (R4)
Adsorbent COO Mnaq4Adsorbent COOM (R5)
It is noteworthy that, the surface properties of adsorbent
can significantly affect the adsorption of mercury. The
adsorbent can be positively or negatively charged depending
on its point of zero charge (PZC). When the pH of the medium
is lower than the PZC, the adsorbent surface becomes posi-tively charged leading to electrostatic repulsion of the mer-
cury ions and the adsorbent surface and reduction in mercury
adsorption (Budinova et al., 2008; Rao et al., 2009).
4.4. Temperature
Many researchers have shown that increasing the tempera-
ture results in higher mercury uptake due to the endothermic
nature of this process. Inbaraj and Sulochana have used the
thermodynamic parameters to study the effect of temperature
on the mercury adsorption behavior of fruit shell-based acti-
vatedcarbon and found a decrease in Gibbs free energy,DG, as
well as a positive enthalpy value, DH, by raising the
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temperature which revealed that the adsorption process is
endothermic (Inbaraj and Sulochana, 2006). Also, Giles et al.
believe that high temperatures increase the mobility of the
mercuric ion and widen the pore on the sorbent surface
leading to enhanced intra-particle diffusion rate (Giles et al.,
1974). However, no justification has been provided regarding
the pore widening phenomenon. The effect could not be due
to physical widening, but apparent widening because of anincrease in compressibility of the particles with increasing
temperature. Since porous structure of carbonaceous mate-
rials usually forms at very high temperatures, it is particularly
implausible to alter the pore sizes at adsorption temperatures
as low as 20e80 C.
On the contrary,Mohan et al.have reported the exothermic
nature of the mercury adsorption using activated carbon
derived from fertilizer waste. This is confirmed with the
negative enthalpy value, DH, and an increase in Gibbs free
energy DG by an increase in temperature. They have related
this behavior to the physical adsorption mechanism of mer-
cury by the adsorbent material. Physical adsorption caused by
the van der Waals forces between the adsorbent surface andthe adsorbate molecules is typically favored at low tempera-
tures. This explains the higher adsorption capacity of the
fertilizer-based adsorbent for mercury at low temperatures
(Mohan et al., 2001).
4.5. Adsorbent dosage and particle size
Well-documented researches have proven that an increase in
the dosage of adsorbent at a constant pH and adsorbate con-
centration has positive effect on the removal of pollutants
from wastewater (Gupta et al., 2003; Namasivayam et al.,
2001). Although many researchers have reported that the
mercury removal percent increases as the adsorbent dosage isincreased, as discussed in preceding sections, removal per-
centage is an entirely relative term changing by initial con-
centration of mercury and adsorbent dosage and thus it is not
appropriate to evaluate the efficiency of an adsorbent using
this parameter. Percentage mercury removal increased from
40% to nearly 100% when the C. pentandrahull adsorbent dose
increased from 25 to 200 mg (equal to 0.5 g:L1 and 4 g:L1,
respectively) (Rao et al., 2009). Increasing the dose of Indian
almond fruit shell from 0.05 to 5 g:L1 also led to a maximum
mercury removal of 99.5% (Inbaraj and Sulochana, 2006).
Similar mercury adsorption trends have been reported using
activated carbon from sago waste and commercial activated
carbon (Kadirvelu et al., 2004). Typically, an increase in theadsorbent dosage results in the availability of higher surface
area and larger number of functional groups for ion exchange
in the system and leads to more chemisorption and/or phys-
isorption as well as higher rate of adsorbate removal (Wahi
et al., 2009). It is suggested that more tangible adsorption ca-
pacities should be reported in this context instead of simply
quoting the percent removal.
On the other hand, although the removal percentage in-
creases by increasing adsorbent load, the mercury adsorption
capacity of the adsorbent has been shown to steadily
decrease. This has been related to the decrease in the avail-
ability of mercury ions in aqueous phase per adsorbent site
and unsaturation of the adsorbent surface active sites. Rao
et al. used three types of adsorbents for mercury removal and
all of the adsorbents exhibited a decrease in the adsorption
capacity and an increase in the mercury removal percentage
by increasing the adsorbent dosage (Rao et al., 2009).
In addition, particle size also plays an important role in
altering the rate and capacity of mercury adsorption. It has
been demonstrated that when the size of the adsorbent par-
ticles decreased from 1.25e2.5mmto0.21e1 mm,the mercuryadsorption capacity showed a two-fold increase (430 mg:g1
versus 815 mg:g1, respectively) (Mckay et al., 1989; Peniche-
Covas et al., 1992). Similarly, Kadirvelu et al. have also
demonstrated that a stepwise decrease of activated carbon
particle size produced from sago waste (750e500 mm,
500e250 mm and 250e125 mm) resulted in an increase in
mercury adsorption (85%, 90% and 93% removal, respectively)
(Kadirvelu et al., 2004). Similar results have also been reported
by Mohan et al. (Mohan et al., 2001) and Feng et al. (Feng et al.,
2004). It has been shown that reducing the adsorbent particle
size increases the effective surface area and enhances the
availability of adsorption sites (Kara et al., 2007). Also, the
diffusion path becomes shorter and the adsorbate moleculescan more easily penetrate into the internal pores of the
adsorbent (Gupta et al., 2011).
5. Mercury affinity to various functionalgroups
The adsorption of adsorbate by activated carbon can be cate-
gorized into chemical and physical adsorption. Briefly, phys-
ical adsorption is mediated by the weak van der Waal
interaction between the adsorbate and adsorbent, while
chemical adsorption is governed by the bonding between the
functional groups on the adsorbent surface and adsorbate.Weak van der Waal interaction have beenproven inefficient in
promoting mercury adsorption, however surface functional
groups, specially the oxygen containing groups of the adsor-
bent, exhibit a key role on the adsorption of mercury (Sun
et al., 2011). The behavior of enhanced mercury adsorption
by oxygen-containing functional groups has been explained
by the Lewis characteristic of Hg (II) which can be bonded to
the basic functional groups of the adsorbent surface (Nabais
et al., 2006). In the aqueous medium, the oxygen-containing
functional groups on the surface of the adsorbent tend to
lose their protons and become ionized, thus leading to un-
balanced charge on the adsorbent surface where ion exchange
with the mercuric ion can occur (Sun et al., 2011). This ac-counts for the critical effect of pH level of the mercury-laden
solution on the adsorption of mercuric ions. As discussed in
the preceding sections, changing the pH level significantly
changes the adsorbent surface charge, thus resulting in a
considerable difference in the adsorption capacity of the
adsorbent. Moreover, electron lone pairs on nitrogen-
containing functional groups can interact with mercury ions
and assist in their removal (Zhu et al., 2009).
Although functional groups of the activated carbons have
long been consideredto be crucial in chemisorption, the effect
of oxygen-containing functional group quantity on mercury
adsorption capacity and rate has not been comprehensively
examined. It is also noteworthy that despite an inverse
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relationship between the percentage of oxygen functional
groups and the total surface area of the adsorbent material,
both of which are regarded positive factors for mercury
adsorption capacity, no trade-off graph between these two
crucial parameters has been provided to optimize the effi-
ciency of adsorption.
As functional groups largely determine the surface prop-
erties and thus the intensity of ion exchange, manipulation ofthe surface functional group have been of great interest. Sul-
fur group has been widely reported to promote mercury
adsorption. Rao et al. have observed an increase in the mer-
cury adsorption capacity of activated carbon with the intro-
duction of sulfur groups on the activated carbon surface and
ascribed the higher removal efficiency of the sulfur-
containing activated carbon to the interaction of various
Hg(II) species, such as HgCl2, (HgCl2)2, Hg(OH)2 and HgOHCl,
with surface sulfur groups. The following redox reaction has
been proposed as the adsorption mechanism of the activated
carbon for mercury (Rao et al., 2009).
2Hg2
SO23 2OH
4Hg
22 SO
24 H2O (R6)
This reaction is in good agreement with the effect of pH
value on the adsorption capacity, where increasing the pH
level of the solution increases the hydroxide ion content,
driving the reaction to theright side, and thus leads to a higher
mercury adsorption capacity.
Enhancement in the removal of mercury has also been
carried out by grafting thiol group onto the surface of the
activated coke, where the adsorption capacity has been
increased from 315.8 mg:g1 for the unmodified material to
694.9 mg:g1 for the modified material (Li et al., 2013). Anoop
Krishnan and Anirudhan have verified the effect of sulfur
modification by H2S and SO2 on the adsorption capacity of
mercury (Anoop Krishnan and Anirudhan, 2002). They
observed that irrespective of the type of modifying agent
(either H2S or SO2), the mercury adsorption capacity of the
activated carbon increases. This can be due to the similar
types of sulfur functional groups doped on the adsorbent
surface by gas surface modification. These results are
different from the gas-phase adsorption of mercury which canbe related to the different mechanism in gas-phase and
aqueous-phase mercury adsorption (Feng et al., 2006b).
Studies concerning the effect of activation parameters on
the type and quantity of the functional groups are listed in
Table 3. Toles et al. have identified that the type of precursor
has minor effect on the functional groups of the produced
activated carbons and implicated the importance of activation
temperature in the formation of the functional groups (Toles
et al., 1999). The oxygen-containing functional groups can be
formed by exposing the carbonaceous precursor to oxygen at
temperatures between 200 and 700 C (Bansal et al., 1988).
Also, more carbonyl groups can be formed by oxidizing the
activated carbon at 400 C, but subsequent oxidization of theactivated carbon destroys the carbonyl group and produces
more phenol, lactones and carboxylic acid group (Toles et al.,
1999). Furthermore, it has been observed that the carboxylic
groups begin to decompose at 200e500 C and all the acidsites
are destroyed at 700 C(Budinova et al., 2008). Although such
manipulation can be carried out on the surface functional
groups of activatedcarbons, it can be criticized that there is no
comprehensive study to compare the effects of various func-
tional groups on mercury removal.
The type of the activating agent has also been considered
effective in the manipulation of the surface functional groups
Table 3 e Acid-base neutralization capacity (meq/g) of the activated carbon adsorbents.
Precursor material Name Base uptake Acid uptake Reference
NaHCO3 Na2CO3 NaOH EtONa HCL
Mengen 0.092 0.120 0.184 1.900 1.120 (Ekinci et al., 2002)
Seyitomer e 0.120 0.250 2.040 2.670
Some 0.100 0.110 0.183 1.570 1.120
Bulluca e 0.110 0.320 1.900 2.010
Apricot Stones 0.130 0.210 0.360 1.350 0.842
Furfural 0.120 0.160 0.230 1.500 0.600
Furfural Carbon A 0.120 0.160 0.230 1.500 0.600 (Budinova et al., 2003)
Mixture of steam pyrolysis
tar and furfural (30:70)
Carbon B 0.030 0.080 0.250 1.300 0.560
Air oxidized Furfural Carbon C 1.900 1.930 3.660 6.340 e
Woody biomass birch N600-1 0.744 0.126 0.480 2.234 0.083 (Budinova et al., 2006)
NS600-1 0.124 0.034 0.572 2.530 1.100
S700-2 e 0.123 0.422 2.355 0.902
Walnut shell Walnut shell 0.450 0.490 0.390 0.520 0.520 (Zabihi et al., 2009)
Carbon A 0.540 0.480 0.350 0.420 0.420
Carbon B 0.720 0.420 0.300 0.290 0.290
Coconut activated carbon AC 1.097 0.627 0.561 0.495 e (Lu et al., 2014)
AC1 1.174 0.594 0.693 0.341
AC1-1 1.295 0.341 0.726 0.572
AC1-2 1.328 0.099 0.869 0.594
Sago 1.200 1.800 0.900 1.600 1.100 (Kadirvelu et al., 2004)
Furfural 0.120 0.160 0.230 1.500 0.600 (Yardim et al., 2003)
Antibiotic waste BDLa BDL 0.230 2.300 1.300 (Budinova et al., 2008)
a
Below detection limit.
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45 472 0.0090 0.9800 15.9 0.560 0.940
60 578 0.0080 0.8900 15 0.600 0.890
Sulfur impregnation of (AC) with
4%(v/v) SO2at 700 C for 60 min
30 523 0.0220 0.9600 71.2 0.330 0.990
45 496 0.0740 0.9200 129.2 0.250 0.980
60 510 0.0860 0.9500 148.2 0.230 0.960
Steam activation of bagasse
pith (SA-C)
Langmuir 30 172.4 0.0072 e e
40 181.8 0.008
50 200 0.0086
60 208.3 0.0106
Steam activation of bagassepith in presence of SO2
(SAeSO2eC)
30 185.2 0.019540 204.1 0.0202
50 208.3 0.0229
60 222.2 0.0262
Steam activation of bagasse
pith in presence of H2S
(SAeH2SeC)
30 181.8 0.0113
40 200 0.0123
50 204.1 0.0164
60 217.4 0.0229
Steam activation of bagasse
pith in presence of SO2 & H2S
(SAeSO2eH2SeC)
30 188.7 0.0281
40 208.3 0.0273
50 212.8 0.0367
60 227.3 0.0480
Rice husk ash Langmuir and Freundlich 15 9.3 0.0115 0.9868 0.42 0.493 0.973
30 6.7 0.0158 0.9900 0.54 0.469 0.965
Sulfuric acid treated with rice
husk (dry sorbent)
Langmuir and Freundlich 25 303 0.0052 0.9990 7.1 0.5579 0.981
35 336.7 0.0107 0.9992 28.7 0.377 0.98745 384.6 0.0219 0.9988 48.9 0.3407 0.986
Sulfuric acid treated with rice
husk (wet sorbent)
25 227.3 0.0052 0.9991 8.7 0.4607 0.952
35 270.3 0.0088 0.9998 15.0 0.428 0.928
45 303 0.0129 0.9993 18.1 0.448 0.959
Sulfuric acid treated with
flax shave (dry sorbent)
Langmuir 45 416 0.0805 0.9980
Sulfuric acid treated with
flax shave (wet sorbent)
344 0.0468 0.9990
Commercial activated carbon (AC) Langmuir and Freundlich 10 4.1 0.2083 0.9522 0.8 0.974 0.956
25 3.5 0.1053 0.9827 0.3 1.262 0.971
50 3 0.1330 0.9828 0.4 1.150 0.970
Steam activated AC (AC-1) 10 4.9 0.6870 0.9889 2.8 0.790 0.975
25 4.5 0.1540 0.9914 0.6 1.248 0.982
50 4.1 0.3862 0.9866 1.4 0.750 0.952
AC1 was oxidized with H2O2at 1:2 (m:v)
(AC1-1)
10 5.0 0.2329 0.9828 1.1 0.914 0.986
25 5 0.2000 0.9914 1 0.858 0.984
50 4.6 0.2618 0.9949 1.6 0.857 0.985
AC1 was oxidized with H2O2at 2:5 (m:v)
(AC1-2)
10 5.2 0.7795 0.9835 3.4 0.823 0.976
25 5.1 0.4491 0.9841 2.3 1.031 0.979
50 4.6 0.9287 0.9521 2.7 0.720 0.980
PSAC grafted with TOMATS Langmuir and Freundlich 20 76.9 0.0588 0.9920 5.5 0.630 0.916
25 76.9 0.0778 0.9940 6.9 0.590 0.906
30 83.3 0.1100 0.9930 9.4 0.560 0.892
35 83.3 0.1250 0.9910 10.2 0.570 0.898
Activated coke (AC) Langmuir and Freundlich 25 315.8 0.0500 0.9770 12.2 0.714 0.980
Thiol-functionalized activated coke (SH-AC) 694.9 0.0600 0.9840 71.1 0.526 0.954
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for better mercury uptake. Nabais et al. have demonstrated
that the type of sulfur doped onto the adsorbent surface is a
more critical factor than its quantity. They observed that the
increase in the sulfur content of the activated carbon using
solid sulfur as the modifying agent did not improve mercury
uptake, whereas the modification of the adsorbent by H2S
resulted in a considerable increase in mercury adsorption.
They related this phenomenon to better accessibility of thesulfurto mercury by gas modification compared with the solid
modification (Nabais et al., 2006).
The activation atmosphere can also affect the surface
functionality of activated carbon. Budinovaet al. have found
that activated carbons pyrolyzed under nitrogen atmosphere
have high carboxylic group on the material surface, but
consecutive pyrolysis and steam activation results in a sig-
nificant drop in the content of carboxylic and lactone groups
and formation of more hydroxyl and carbonyl groups
(Budinova et al., 2006). It has also been highlighted that acti-
vation in the presence of air and water vapor results in an
increase and decrease of oxygen content of the final modified
product, respectively (Budinova et al., 2003).Besides physical activation, chemical activation can also
alter the functional groups on the activated carbon surface.
Most activated carbons contain varying amounts of functional
groups such aseOH, eCH]O and COOH without any treat-
ment. When activated carbons are treated with oxidizing
agent such as HNO3, H2O2, or (NH4)2S2O8, chemical reaction
occurs between the activating agent and the adsorbent sur-
face which alters the surface functionality and pKa of the
activated carbons as well as their porous structure and
adsorption capacity (Bandosz et al., 1993; Montagnaro and
Santoro, 2009).
X-ray photoelectron spectroscopy has demonstrated that
that oxygen- and nitrogen-containing functional groups actas electron donors during mercury adsorption and it has
been hypothesized that chemical coordination of mercury
with these functional groups are accountable for mercury
adsorption (Zhu et al., 2009). Therefore, higher oxygen- and
nitrogen-containing functional groups favor the mercury
adsorption. Zhu et al. studied the effect of activating agent
and chemical activation time on the surface functionality of
the activated carbons and detected the formation of hy-
droxyl, carboxylic and carboxylic anhydride group by nitric
acid treatment (Zhu et al., 2009). When the contact time be-
tween activated carbon and the nitric acid increases, signif-
icant amount of phenolic group forms while the content of
lactone group is reduced. Increase in the concentration ofnitric acid also leads to the formation of higher carboxylic
acid and carbonyl group content (Xianglan et al., 2011).
Xianglan et al. have investigated the use of hydrogen
peroxide as modifying agent and found that the lactone
moieties are decomposed into carbonyl and phenol groups by
increasing the chemical concentration and reaction time
(Xianglan et al., 2011). Danish et al. have explored the effect
of two chemical agents and have found that phosphoric acid-
treated activated carbon contains higher amount of acidic
functional group as compared with using zinc chloride
(Danish et al., 2013). However, when acid treatment becomes
more intense, no further oxygen functional groups, crucial
for the adsorption capacity of the activated carbons, are
detected. Thus altering the type and concentration of the
activating agent is an important factor to be studied for
adsorption purposes. Ahmad et al. used 2 Mhydrochloric acid
to treat cocoa shell for 2 h at a relatively high temperature
and found that, despite the high surface area obtained, the
oxygen functional group was not detected. It has been hy-
pothesized that the oxygen attached to the minerals are
removed by intense acid treatment (Ahmad et al., 2013).
6. Equilibrium adsorption isotherms
Langmuir and Freundlich isotherm models have been mostly
applied to describe the equilibrium adsorption of mercury (II)
on the adsorbent.
The Langmuir isotherm model was originally developed to
describe gasesolid adsorption onto adsorbent. The model
assumes irreversible homogeneous monolayer adsorption
and each adsorbate being adsorbed only to one adsorption
site. It also assumes that all the adsorption sites are identical.Therefore, the affinity of each adsorbate to adsorbent is
equivalent resulting in constant enthalpies and sorption
activation energy, without lateral interaction and steric hin-
drance between the adsorbed molecules on the adjacent sites
(Langmuir, 1918). The mathematical expression for this model
can be represented as:
qe qmaLCe1 aLCe
(1)
whereqeis the adsorption capacity of the adsorbent (mg:g1);
qm is the maximum adsorption capacity of the adsorbent
(mg:g1);Ce is the equilibrium concentration of the adsorbate
in the solution (mg:L1
); and aL is the Langmuir constant. Amathematical expression developed by Webber and Chakk-
ravorti has been used to test the favourability of the adsorp-
tion process (Weber and Chakravorti, 1974):
RL 1
1 aLC0(2)
where RL, called separation factor, is a dimensionless term
and Co is the adsorbate initial concentration (mg:L1). The
separation factor (RL) indicates the adsorption nature to be
unfavorable (RL >1), linear (RL 1), favorable (0
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adsorption process is favorable and the adsorbent surface is
considered heterogeneous (Jodeh et al., 2014).
Although both the Langmuir and Freundlich isotherm
models are popular tools in the prediction of equilibrium
adsorption isotherm, these models are sometimes criticized
due to their limitations of oversimplified assumptions for the
former and lack of fundamental basis for the latter isotherm
model. In addition, other hybrid forms of the Langmuir andFreundlich adsorption models are also established. Redlich-
Peterson and Sips isotherm models are the modified
isotherm models that incorporate the features of both the
Langmuir and Freundlich equations.
The Redlich-Peterson model can be applied either in ho-
mogeneous and heterogeneous adsorption (Redlich and
Peterson, 1959):
qe qmaRCe
1 aRCbe
(4)
whereaR is the Redlich-Peterson isotherm constant and b is
the Redlich-Peterson isotherm exponent, which lies between
0 and 1. The two extremes of the exponent b transform thisequation to the Henry's law and Langmuir equations when its
value is the lowest and highest, respectively. For any other
exponent values, this equation can be considered as an
incorporation of the features of the Langmuir and Freundlich
models.
Sips isotherm model is applied for the prediction of het-
erogeneous adsorption system and assumes the occurrence of
dissociative adsorption (Sips, 1948). At low adsorbate con-
centration, the isotherm can be reduced to Freundlich
isotherm, while at high concentration, it complies with ho-
mogenous adsorption characteristic of the Langmuir isotherm
(Diaz et al., 2007). The Sips isotherm is still criticized not to
follow the Henry's law at low adsorbent concentration. TheSips isotherm model is expressed through the following
equation:
qe qmaSCbse1 aSC
bse
(5)
where as is the Sips isotherm model constant andbsisthe Sips
isotherm model exponent.
Table 4 summarizes the Langmuir and Freundlich con-
stants obtained for the removal of aqueous mercury by
various adsorbent materials. Pena-Rodriguez et al. have
tested the mercury adsorption behavior of three adsorbents
obtained from calcined mussel shell, finely ground musselshell and coarsely ground mussel shell and identified that
the KF value obtained from Freundlich isotherm model is
not closely correlated with the surface area, given that the
highest KF value corresponds to the calcined shell with
surface area lower than that of finely ground mussel ( Pe~na-
Rodrguez et al., 2013). Cai and Jia showed the S-shaped
relationship between SBET and mercury adsorption and
suggested that the high porosity contributed by micropore
might not be accessible to mercury and its species, such as
HgCl2 and HgOHCl, instead a better linear correlation was
found between the adsorption capacity and mesopore sur-
face area (Cai and Jia, 2010). This phenomenon suggested
that the surface area alone is not sufficient to reflect the
adsorption capacity of the adsorbent, but several other
factors such as pore size, surface structure and adsorbate
species will also interfere with the overall adsorption
capacity.
Cai and Jia have found a positive correlation between the
mercury adsorption capacity of activated carbons and its
sulfur content (Cai and Jia, 2010). Wang et al. have also
determined that although sulfur impregnation results in sig-nificant reduction in SBET of the activated carbons, a stag-
gering enhancement in the mercury adsorption capacity was
achieved (Wang et al., 2009). The strong affinity between
mercury and sulfur has also been reported by Asasian et al.
(Asasian et al., 2014).
Further information could be deduced regarding the
mechanism of mercury adsorption by comparing the
isotherm shapes as a means of fitting mercury adsorption
isotherms, and correlating these with Giles isotherm classifi-
cation (Giles et al., 1960). To date, no authors have attempted
to do this for aqueous mercury adsorption.
7. Conclusion and future perspectives
Removal of mercury from wastewater using activated carbons
has been shown to be very promising if proper combination of
properties is possessed by the adsorbent materials. The ef-
fects of surface area and functional groups of the activated
carbons on mercury uptake have been examined in numerous
studies. In this study, the generic misconception that higher
surface area of an adsorbent leads to higher mercury
adsorption has been criticized. Herein, it has been demon-
strated that a combination of medium-to-high surface area
with well-functionalized surface properties are collectivelycrucial in enhancing the mercury removal. Despite these
findings, very limited research has been carried out on
simultaneous optimization of surface and textural charac-
teristics of activated carbons. Hence, further study is neces-
sary for such optimization to save the high amount of energy
required to obtain unnecessary very high surface area acti-
vated carbons.
Furthermore, although a lot of studies are concerned with
sulfurization of activated carbons with the aim of higher
mercury uptake, the mechanism of sulfurization process,
including the type and quantity of sulfur-containing moieties
doped onto the activated carbon surfaces and their function-
alization process, and consequently the mercury adsorptionmechanism are not thoroughly examined. A profound insight
into the activation and adsorption mechanisms will assist in
designing a proper adsorbent-adsorbate system for optimal
mercury abatement from effluents.
In addition, the mercury adsorption is believed to take
place in two stages; initially the surface active sites are
involved in the adsorption process and when the surface sites
are less available, the mercuric ions have to diffuse into the
pores. Therefore, a combination of pseudo and diffusion
models has to be considered for modeling the mercury
adsorption kinetic results. Nevertheless, this modeling strat-
egy has been disregarded.
Further recommendations can be presented as follows:
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Mercury forms complexes in real wastewater systems and
is rarely found in ionic form. Therefore, study of the effi-
ciency of the activated carbon adsorbents using industrial
wastewater seems to be of high priority.
The presence of other metallic compounds in the effluent
will unequivocally affect the mercury removal efficiency of
the activated carbon samples. Therefore, more detailed
study of the multi-component adsorption systems have tobe carried out.
The regeneration of the activated carbon samples has to be
conducted for economic feasibility enhancement. Unfor-
tunately, in adsorption processes, the regeneration is
overlooked.
If not regenerated, due to its hazardous nature, mercury-
loaded activated carbon needs to be stabilized or vitrified
and then disposed of in hazardous landfill. Nonetheless,
this landfilled carbon is not reusable, therefore empha-
sizing the importance of the production cost of the acti-
vated carbon.
Typically, the focus of the research in mercury adsorption
systems is lab-scale batch adsorption studies. However,the studies should not be confined only to these lab-scale
experiments and column studies have to be performed
for better understanding the industrial-scale operation
challenges.
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