Yinying Ren1, Xianwen Mao1, T Alan Hatton1. 1. Department of Chemical Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, United States.
Abstract
Conducting polymers modified with redox-active moieties or amphiphilic surfactants are promising adsorbent materials for the separation of neutral organic species from water. We develop an asymmetric system combining a polyvinylferrocene-polypyrrole hybrid (PVF-PPy) and an amphiphilic surfactant dioctyl sulfosuccinate (AOT)-doped polypyrrole (PPy(AOT)) that have complementary hydrophobicity tunability in response to electrochemical modulations. Both materials are hydrophobic in their respective neutral states, exhibiting high affinities toward organics. Upon application of a mild potential to oxidize PVF-PPy and reduce PPy(AOT), these polymers can be simultaneously rendered hydrophilic, thereby driving desorption of organics and regeneration of the materials. The asymmetric system can be used in a cyclic fashion, through repeated electrical shorting of the two electrodes to program the capture of organics from a large volume of feed solution, and application of a potential (above 0.9 V) to stimulate the release of the adsorbed organics into a small volume of desorption solution. The asymmetric configuration has multiple benefits, including suppression of water parasitic reactions, high energetic efficiency, and selectivity for target organic species. Therefore, the electrode system has the potential to reduce the energy consumption in the mitigation of organic contaminants over conventional methods, with the additional ability to recover valuable organic products, opening up new possibilities for addressing the water-energy nexus.
Conducting polymers modified with redox-active moieties or amphiphilic surfactants are promising adsorbent materials for the separation of neutral organic species from water. We develop an asymmetric system combining a polyvinylferrocene-polypyrrole hybrid (PVF-PPy) and an amphiphilic surfactant dioctyl sulfosuccinate (AOT)-doped polypyrrole (PPy(AOT)) that have complementary hydrophobicity tunability in response to electrochemical modulations. Both materials are hydrophobic in their respective neutral states, exhibiting high affinities toward organics. Upon application of a mild potential to oxidize PVF-PPy and reduce PPy(AOT), these polymers can be simultaneously rendered hydrophilic, thereby driving desorption of organics and regeneration of the materials. The asymmetric system can be used in a cyclic fashion, through repeated electrical shorting of the two electrodes to program the capture of organics from a large volume of feed solution, and application of a potential (above 0.9 V) to stimulate the release of the adsorbed organics into a small volume of desorption solution. The asymmetric configuration has multiple benefits, including suppression of water parasitic reactions, high energetic efficiency, and selectivity for target organic species. Therefore, the electrode system has the potential to reduce the energy consumption in the mitigation of organic contaminants over conventional methods, with the additional ability to recover valuable organic products, opening up new possibilities for addressing the water-energy nexus.
Chemical
separations processes are energy-intensive and are responsible
for 10–15% of the world’s total energy consumption,
with distillation, evaporation, and other conventional technologies
accounting for more than 80% of this energy expenditure.[1] Improved separation efficiencies can be achieved
through more recent technologies such as reverse osmosis, nanofiltration,
and capacitive deionization, which are particularly effective for
removing charged ions from water.[1−3] The separation of nonionic
organic species in processes such as wastewater treatment and pharmaceutical
product purification is also of importance. Indeed, water pollution
by neutral organic contaminants, such as industrial chemicals, pesticides,
pharmaceuticals, and personal care products, is an emerging issue
globally, and their presence at low concentrations (in the range of
μg L–1 to mg L–1 at the
point of discharge or from treatment facilities) complicates the separation
processes.[4−11] Among different chemical separation technologies, air stripping,
pervaporation, biological treatment, and carbon adsorption are more
suitable for organics at low concentrations,[12] with adsorption by activated carbon being the most efficient and
widely adopted.[13]Current wastewater
or drinking water treatment plants are not specifically
equipped for eliminating neutral organic contaminants[6,9] which can therefore pass through domestic and industrial wastewater
discharges and end up in the aquatic environment. Many neutral organic
contaminants have proven to have ecotoxicological effects on aquatic
life, animals, and even human beings, that include short-term and
long-term toxicity, endocrine disrupting effects, and antibiotic resistance
of microorganisms.[5−7] Similar to wastewater treatment, purification of
pharmaceutical compounds involves a wide array of organic compounds
and is essential for ensuring the quality of medications. Removal
of neutral organic species by adsorbents such as activated carbon
(AC) is a common practice, but sorbent regeneration through thermal
processes, pH adjustment, or solvent extraction is often challenging
or costly.[14] Therefore, AC regeneration
is usually done in centralized treatment facilities, adding transportation
cost to the operations.[15] Electrical energy
is inexpensive and widely available and can be more efficient compared
to the aforementioned alternative ways to regenerate adsorbents.[16] Adsorbents that can be regenerated by electricity
present a practical and scalable point-of-use solution for separating
neutral organic compounds from aqueous solutions.Several electrochemical
methods have been developed for the separation
of organic compounds: Electrocoagulation consumes iron or aluminum
to generate coagulants and can have disadvantages with respect to
sustainability and cost of metal electrodes.[17] Electrochemical regeneration of activated carbons applies a current
to desorb and destroy adsorbed organics, but the relatively high current
(10–100 mA) and long charging period (5–40 h) may be
prohibitive for industrial applications.[18] A cyclical electrochemical stage process proposed by Jemaa et al.
that uses complexing agents dissolved in a contacting phase to transfer
organic species from a feed phase to a receiving phase is promising
because the complexation between the organics and the agents is reversible
and can be modulated by electrochemical redox reactions.[16] To recycle the complexing agents and avoid contamination
of the feed and stripping solutions, the contacting phase must be
immiscible with these solutions, in which the agents should also be
insoluble.To work around the stringent solubility requirements
of this electrochemical
separation process, we immobilized the mass separation agents on conductive
solid substrates to form adsorbents responsive to electrochemical
modulations. The benefits are 2-fold: first, electrons are transferred
directly from the electrodes to the immobilized adsorbents, in contrast
to the approach taken by Jemaa et al., in which the complexing agents
needed to migrate to be within the vicinity of the electrode for redox
reactions to take place; second, the solid electrodes can be contacted
with the feed or receiving phase in a swing process akin to that used
in traditional adsorption operations, but with voltage swings rather
than changes in temperature, pressure, or solution conditions. Electrodes
functionalized with redox-active materials have been developed to
remove ionic species and charged biomacromolecules from aqueous solutions
in a reversible manner,[3,19−23] and we have shown recently that electrically conductive
materials with immobilized redox-responsive moieties can be applied
also to the separation of neutral organic species from solution.[2,24] We used polypyrrole (PPy) deposited on carbon substrates as the
adsorbent and adopted two different approaches to modulate its hydrophobicity
and hence affinity toward organic solutes in water: incorporation
of a polyvinylferrocene (PVF) redox-responsive polymer in the PPy
electrode coating[2] and doping of the PPy
with the amphiphilic surfactant dioctyl sulfosuccinate (AOT).[24] We refer here to the two types of material as
PVF–PPy and PPy(AOT), respectively. Building on the previous
efforts on material design, we explore the synergistic properties
of PVF–PPy and PPy(AOT) in electrochemically mediated separations
of organics by pairing them as opposing electrodes in an asymmetric
electrochemical cell.As in the electrosorption of ionic species
by redox-active materials,
the trade-off between energy cost and extent of separation warrants
careful choice of electrochemical cell configurations, electrode material,
and process parameters to achieve the most efficient separation.[2,3] Since PVF–PPy is more hydrophobic when reduced, and hydrophilic
when oxidized, while PPy(AOT) behaves in the opposite manner, i.e.,
is more hydrophilic when reduced and more hydrophobic when oxidized,
the PVF–PPy and PPy(AOT) electrodes form an attractive pair
for an asymmetric system to work in tandem. With no voltage applied
to the cell, both electrodes are relatively hydrophobic and able to
adsorb neutral organic molecules, but when an appropriate electrical
potential is applied to the cell to charge both electrodes, the organics
will desorb from the loaded electrodes. Reactivation of the two electrodes
to prepare them for the next adsorption cycle is spontaneous on simple
shorting of the two electrodes. With only the desorption step costing
energy, the asymmetric system has the potential to achieve high energetic
efficiency. The asymmetric electrode system for capturing organic
compounds from water can be used in conjunction with degradation methods,
such as electrochemical advanced oxidation processes, to transform
toxic organic compounds to less harmful forms or useful compounds.[25]In this work, we first demonstrate experimentally
that the asymmetric
system can be used reversibly to remove model organic species from
water, with limited decay in capacity over a number of cycles and
an ability to suppress parasitic reactions in water. We then analyze
the energetic efficiency and economic viability of electrochemically
mediated separations of organics relative to conventional adsorption
by activated carbons regenerated by thermal desorption or solvent
extraction. We finally show the generality and selectivity of the
PPy-based asymmetric system in the context of a separation that is
of direct relevance to pharmaceutical purification.
Results and Discussion
The functional materials in an asymmetric
system for electrochemically
mediated separations need to exhibit three properties: (1) electrical
conductivity to respond to applied potentials, (2) different affinities
toward organic species depending on the applied electrochemical modulation,
and (3) high surface area for interactions with organic species to
foster a high adsorption capacity. Therefore, we functionalized polypyrrole,
a common intrinsically conducting polymer, coated on carbon fibers
to serve as an underlying conductive network, with two approaches,
involving ferrocene moieties and amphiphilic AOT surfactants, to modulate
the affinities of the materials toward organic species.[2,24] The PVF–PPy hybrids and doped PPy(AOT) were synthesized using
electropolymerization techniques. The resulting polymer films coated
on commercial carbon cloth substrates possessed the desired highly
porous morphology (Figure a,c). An asymmetric system was assembled with a PVF–PPy
positive electrode and a PPy(AOT) negative electrode (Figure b).
Figure 1
Scanning electron microscopy
(SEM) images of (a) PPy(AOT) and (c)
PVF–PPy. (b) Schematic of the asymmetric system.
Scanning electron microscopy
(SEM) images of (a) PPy(AOT) and (c)
PVF–PPy. (b) Schematic of the asymmetric system.
Asymmetric PPy-Based System
It is
important to balance the charges of the positive and negative electrodes
constituting the asymmetric system. One common approach is to adjust
the mass of the functional materials on the two electrodes such that
the capacitances are equalized.[26] We therefore
first estimated the specific capacitances (C) of
the PVF–PPy and PPy(AOT) electrodes using three-electrode cyclic
voltammetry (CV) profiles according to the following equation (Figure S1):[27]where I is the current (A), ΔV is the applied
potential window (V), m is the mass of the polymer
on the electrode, and v is the potential scan rate
(V s–1). The specific
capacitance of PPy(AOT) is approximately twice that of PVF–PPy
at low scan rates (49.5 versus 22.8 F g–1). Therefore,
we adjusted the electropolymerization reaction times such that the
mass loading ratio of the PVF–PPy to PPy(AOT) was approximately
2:1.The electrochemical behavior of the asymmetric system with
PVF–PPy and PPy(AOT) electrodes of balanced charges was investigated
by cyclic voltammetry (CV) in a two-electrode configuration. We monitored
the CV responses of the full cell by setting a potential window of
1.2 V and recorded the responses of the individual electrodes versus
a Ag/AgCl reference electrode (Figure ). The paired Faradaic reactions on the two electrodes
are the oxidation and reduction, respectively, of the ferrocene moieties
in PVF–PPy hybrids,[28] and potassium
insertion and repulsion accompanied by reorientation of the surfactant
dopants in PPy(AOT).[29] The latter happens
because the AOT doping anions are largely immobilized within the polymer
during the oxidative polymerization due to their size and, hence,
rely on cation (potassium in this case) exchange with the solution
to maintain the electroneutrality of the PPy film during electrochemical
modulation.[30]
Figure 2
Cyclic voltammograms
of (a) the full cell and (b) the individual
electrodes in the PVF–PPy//PPy(AOT) asymmetric system in a
two-electrode configuration (scan rates 10 mV s–1). The arrows indicate the direction of voltage scans for the whole
cell and the individual electrodes.
Cyclic voltammograms
of (a) the full cell and (b) the individual
electrodes in the PVF–PPy//PPy(AOT) asymmetric system in a
two-electrode configuration (scan rates 10 mV s–1). The arrows indicate the direction of voltage scans for the whole
cell and the individual electrodes.The two adsorbent materials exhibited differences in hydrophobicity
depending on the electrochemical signals. For PVF–PPy, when
the applied potential (E) is lower than the formal
potential of ferrocene (E0 = 0.34 V versus
Ag/AgCl), the PVF–PPy adsorbent is hydrophobic; most ferrocene
moieties are reduced, and organics can be taken up by reduced PVF–PPy.
For E ≫ E0, the
PVF–PPy adsorbent becomes relatively hydrophilic; most ferrocene
moieties are oxidized and positively charged, and therefore water
molecules interact more favorably with the adsorbent and displace
neutral organic species previously adsorbed on the polymer.[2] In contrast, for PPy(AOT), when the applied potential
(E) is higher than the formal potential of potassium
insertion and repulsion (E0 = −0.21
V versus Ag/AgCl), the polymer is hydrophobic, since the positively
charged PPy backbone attracts the negatively charged sulfonate groups
of AOT such that the hydrophobic tails of the surfactant rearrange
to be on the surface of the material. When E≪ E0, PPy(AOT) is more hydrophilic as the relatively
neutral PPy backbone induces AOT anions to reorient themselves such
that the hydrophobic tails move closer to the polymer chains; the
sulfonate groups are exposed on the surface.[24]The Nernst equation describes the impact of applied potential
on
the relative amounts (R) of the oxidized to reduced
moieties on the polymers (i.e., a measure of the relative hydrophilicity
of the ferrocene-containing electrodes and of the hydrophobicity of
the AOT-doped PPy coating):where kB is the
Boltzmann constant, T the temperature, and e the elementary charge. Therefore, by adjusting the potential,
we can modulate the affinities of the two PPy-based polymers for organics.The CV profile of the full PVF–PPy//PPy(AOT) system shows
a pair of redox peaks around 0.55 V (Figure a). This suggests that a potential drop across
the two electrodes of greater than 0.55 V should be applied to render
both materials hydrophilic to release adsorbed compounds. Subsequently,
we can apply a potential below 0.55 V or simply short the two dual-functionalized
electrodes (0 V) to reoxidize PPy(AOT) and reduce PVF–PPy,
thereby reactivating the materials for further adsorption in their
hydrophobic states.
Electrochemically Mediated
Separations of
Organics
The adsorption capability of the asymmetric system
is demonstrated with a common azo dye compound widely used in the
textile industry, Sudan Orange G (SOG), as a model contaminant. The
equilibrium adsorption of SOG by the PVF–PPy//PPy(AOT) asymmetric
system can be fitted well by the Freundlich adsorption isotherm[31]where the Freundlich exponent 1/n, an indication
of the extent to which adsorption is favored, increases
as 1/n approaches zero (Figure a). While the Freundlich and Langmuir models
both provide good fits for the batch adsorption data based on R2 (Section S2, Supporting
Information), the Freundlich isotherm was selected for this study
because it is commonly applied to the adsorption of organic molecules
on activated carbons or molecular sieves, and its parameters capture
differences in surface heterogeneity of adsorbents (prefactor) and
cooperative adsorption (exponent).[13] When
the asymmetric system is charged at a high potential of 1.2 V, 1/n takes on a value close to unity (1.01); i.e., the isotherm
is almost linear, following Henry’s Law. For the shorted asymmetric
system in which PPy(AOT) is oxidized and PVF–PPy reduced, the
fitted 1/n value was 0.54, consistent with the fact
that the oxidized PPy(AOT) and reduced PVF–PPy have higher
affinities for SOG in their hydrophobic states.[2,24]
Figure 3
(a) Adsorption
isotherms for Sudan Orange dye on the PVF–PPy//PPy(AOT)
asymmetric system modulated by various applied potentials as fitted
with the Freundlich equation. (b) Linear dependence of the fitting
parameters of the Freundlich equation on applied potentials/charges.
The R2 values for ln(k) and 1/n vs applied potential, and charges vs applied
potential were 0.983, 0.967, and 0.951, respectively. (c) Linear correlation
between the two Freundlich parameters obtained at different potentials
(R2 = 0.997).
(a) Adsorption
isotherms for Sudan Orange dye on the PVF–PPy//PPy(AOT)
asymmetric system modulated by various applied potentials as fitted
with the Freundlich equation. (b) Linear dependence of the fitting
parameters of the Freundlich equation on applied potentials/charges.
The R2 values for ln(k) and 1/n vs applied potential, and charges vs applied
potential were 0.983, 0.967, and 0.951, respectively. (c) Linear correlation
between the two Freundlich parameters obtained at different potentials
(R2 = 0.997).The Freundlich isotherm parameters ln(k)
and 1/n correlate linearly with the applied potential
(Figure b), reflecting
the
changes in hydrophilicity of the adsorbent with charging of the electrodes;
the linearity arises because the electrochemical cell exhibited capacitance-like
features such that, for a fixed charging time of 10 min, the total
number of charges exchanged (and hence hydrophilicity) increased linearly
with the applied potential, as shown in the inset in Figure b. Moreover, Figure c shows that the Freundlich
equation parameters are themselves correlated linearly, as has been
observed by others for the adsorption of a wide range of organic compounds
from aqueous solution onto activated carbons.[32,33] This behavior can be interpreted in terms of the Polanyi adsorption
theory on the adsorption of organic compounds from an aqueous solution
to a heterogeneous surface.[32,34−36] Polanyi defined the adsorption potential (ϵs) as
the energy required to remove the molecule from a saturated solution
to a point outside the attractive force field of the adsorbentwhere Cs and Ce are, respectively,
the solubility limit and
bulk equilibrium concentrations of the solutes in the liquid phase.
Dubinin related the volume of solutes adsorbed on 1 g of adsorbent
to the adsorption potential via the equationwhere W0 is the
limiting volume per gram of the adsorbent available for adsorption, a is a parameter characteristic of the adsorbent and independent
of adsorbates, and Vs is the molar volume
of solutes.[32,35−37] With Qe = ρW, where ρ
is the solute density, and with ϵs given by eq , the mass of solute on
the polymer can be written aswhich is of the form given in eq , and from which the fitting
parameters
of the Freundlich equations can be identified asandThereforeThe intercept in eq reflects the limiting
capacity of the adsorbent, which should be
independent of solute for solutes of similar density.[32,35−37] The value of ρW0 estimated for our system is 130 mg g–1, which
is of similar magnitude to the value of 227 mg g–1 obtained by Abe et al. for a wide range of organic compounds on
activated carbon.[32]The disparity
in hydrophobicity and hence affinity for organics
under different charging conditions allows for the simultaneous reversibility
of sorption by the two adsorbents that is crucial for a swing separation
process. The electroswing separation is more effective for the separation
of solutes present at low concentrations where the availability of
the sites for adsorption is modulated by electrochemical stimuli.
Cyclic Adsorption
As was previously
shown with individual PVF–PPy and PPy(AOT) polymers, the potential-dependent
affinity permits the use of electrochemical means to program adsorption
and desorption, thereby enabling the loading and regeneration of the
sorbent materials.[2,24]Figure a depicts the application of a PVF–PPy//PPy(AOT)
asymmetric electrochemical cell for removing organics from water.
The electrode pair is immersed in the feed solution, and after reaching
equilibrium, the system can be charged for 10 min, for example at
1.2 V, to render both polymers hydrophilic and to drive the desorption
of the organics. Subsequently, the system can be discharged at 0 V
for 10 min to return the polymers to their hydrophobic states for
adsorption in the next cycle. The electrochemical characterization
of the electrode cell has suggested that the half-cell potential of
the asymmetric system is 0.55 V (Figure a), and therefore we may also charge and
discharge at less extreme potentials, for example, at 0.9 and 0.3
V, respectively.
Figure 4
(a) Schematic illustration of the cyclic adsorption process.
(b)
Removal (left y axis and bars) and regeneration (right y axis and squares) efficiencies of the PVF–PPy//PPy(AOT)
asymmetric system discharged/charged at 0 V/1.2 V and 0.3 V/0.9 V
over five consecutive adsorption/desorption cycles.
(a) Schematic illustration of the cyclic adsorption process.
(b)
Removal (left y axis and bars) and regeneration (right y axis and squares) efficiencies of the PVF–PPy//PPy(AOT)
asymmetric system discharged/charged at 0 V/1.2 V and 0.3 V/0.9 V
over five consecutive adsorption/desorption cycles.We explored the reusability of both materials by
conducting adsorption
and desorption of SOG using the asymmetric system for five consecutive
cycles. Figure b shows
the evolution over the course of five cycles of pollutant removal
efficiency (left y axis), defined as the percentage
of contaminants removed from the feed, and regeneration efficiency
(RE, right y axis) defined as the fraction of contaminants
removed in a later cycle relative to those removed in the first cycle.
The charge/discharge cycle at more extreme potentials (1.2 and 0 V
versus 0.9 and 0.3 V) allows roughly 10% more organics to be removed
in each cycle. Moreover, most of the adsorption capacity of the asymmetric
system can be recovered through electrochemical modulations, indicated
by RE greater than 91% over the five cycles for either pair of applied
potentials. The video in the Supporting Information shows the ability to stimulate the desorption of dyes into the desorption
solution upon application of a potential of 0.9 V.Since the
electrochemically mediated separation process is not
thermodynamically spontaneous, it requires electrochemical energy
to charge the system to drive desorption, the amount of which is dependent
on the potentials applied. Therefore, we need to determine the optimum
pair of applied potentials by considering the trade-off between energy
expenditure (more extreme potentials) and separation extent (more
contaminant removal), as discussed below.
Suppression
of Parasitic Reactions
A major challenge for electrochemical
devices operating in an aqueous
environment is the narrow stable operating voltage window afforded
by water. Water splitting can cause loss of energy to side reactions
and pH fluctuations that may impact the adsorption capacity. The thermodynamic
potential for water electrolysis is only 1.23 V, beyond which undesired
parasitic reactions will occur:[38−40]under acidic conditions, orunder basic conditions, at the cathode, andat the anode, where eqs and 11 are the hydrogen
evolution (HER) and oxygen evolution (OER) reactions, respectively.
In addition to the effects of the whole-cell potential, a side reaction
can occur if the potential window of an individual cathode or anode
reaches its respective stability limit.[41] The equilibrium potential of eq varies as a function of pH in water:where E0 = 0 V is the
standard reduction potential of the HER (SHE),
and aH, ae, and aH are the activities of the reactants and reaction products.
For example, with an initial pH of 6.94 in an aqueous solution, the
HER can take place when the potential on the cathode reaches −0.42
V versus SHE or −0.60 V versus Ag/AgCl.Cells in which
the anode is functionalized with PVF-containing materials are prone
to the HER side reaction when the anode is paired with various types
of materials on the cathode, including platinum (Pt), carbon nanotubes,
or chemically identical PVF-based material in the neutral state.[3] In the desorption step of an electrochemically
mediated separation, an electrode functionalized with PVF–PPy
is oxidized to render the polymer hydrophilic. If the negative electrode
is Pt, the HER with H+ consumption or OH– production can occur to a significant extent.Table shows the
final solution phase pH after potentials are applied to electrochemical
cells consisting of a PVF–PPy positive electrode and a PPy(AOT)
counter electrode, or of the two PPy-based materials independently
paired with Pt. Even when a constant 1.2 V was applied to the asymmetric
PVF–PPy//PPy(AOT) system for 10 min, where the relative potentials
on PVF–PPy and PPy(AOT) were approximately 0.7 and −0.5
V versus Ag/AgCl, respectively (Section S1, Supporting Information), the pH increase (from an initial pH of
6.94) for the asymmetric system is quite limited because the Faradaic
reaction occurring during the reduction of the PPy(AOT) electrode
accommodates electrons from the oxidation of the PVF–PPy in
lieu of the HER that would otherwise occur. Without a dual-functionalized
asymmetric system, water splitting reactions occur to provide the
necessary electrons to complement the redox reactions of PVF–PPy
or PPy(AOT). The fast kinetics of the HER on Pt allows the regeneration
of the PVF–PPy electrode at 0.7 V versus Ag/AgCl in a PVF–PPy//Pt
system to proceed without retardation, and with an increase in the
solution phase pH from nearly neutral (6.94) to 10.41. Similarly,
with Pt as the counter electrode to PPy(AOT), the OER occurs to provide
electrons for the reduction of PPy(AOT) at −0.5 V versus Ag/AgCl,
with a resultant decrease in the pH to 5.48. The
asymmetric electrochemical cell configuration is clearly successful
in preventing pH fluctuations during the electroswing operation (Figure a).
Table 1
Final Solution Phase pH after Different
Applied Potentials Were Applied to Electrochemical Cells Assembled
with Electrodes Coated with Different PPy-Based Polymers or Platinum
(Pt), Allowing the Deduction of Loss of Charge Towards Water Splitting
Based on an Initial pH of 6.94
positive electrode
negative electrode
potential (V)
final pH
% charge toward
water splitting
PVF–PPy
PPy(AOT)
0.0
6.97
0.00
PVF–PPy
PPy(AOT)
0.3
7.13
0.04
PVF–PPy
PPy(AOT)
0.9
7.29
0.04
PVF–PPy
PPy(AOT)
1.2
7.30
0.03
PVF–PPy
Pt
0.7
10.41
42.0
Pt
PPy(AOT)
0.5
5.48
0.81
Figure 5
(a) pH evolution during
charging of the PVF–PPy(AOT)//Pt,
Pt//PPy(AOT), and PVF–PPy//PPy(AOT) systems. (b) Amount of
charge (mC) going toward water splitting OH– production
and the HER in the course of modulating the PVF–PPy//PPy(AOT)
asymmetric system and either PVF–PPy or PPy(AOT) paired with
a Pt counter electrode.
(a) pH evolution during
charging of the PVF–PPy(AOT)//Pt,
Pt//PPy(AOT), and PVF–PPy//PPy(AOT) systems. (b) Amount of
charge (mC) going toward water splitting OH– production
and the HER in the course of modulating the PVF–PPy//PPy(AOT)
asymmetric system and either PVF–PPy or PPy(AOT) paired with
a Pt counter electrode.The other benefit of suppressing parasitic reactions
is that the
Faradaic efficiency of the electrochemical modulations is enhanced. Figure b shows the loss
of charges to water splitting reactions in the PVF–PPy//Pt,
PVF–PPy//PPy(AOT), and Pt//PPy(AOT) systems, where the positive
charge refers to the production of hydroxide, and negative magnitude
represents the proton generation. The dual-functionalized asymmetric
system PPy(AOT) counter electrode allows over 99% of the charges to
be utilized in electrochemical modulation of the polymers whereas
almost 42% of charges are lost to OH– production
when PVF–PPy is paired with Pt. The dramatic reduction in HER
enhances current efficiencies by eliminating parasitic water splitting
reactions.
Energetic Efficiency
Adsorption has
proven to be an effective unit operation for the removal of organics
from wastewater.[5,6,11,13,42] The ability
to regenerate the adsorbent efficiently is important to avoid merely
transferring contaminants from the liquid phase to the solids for
disposal, and to enable reuse of the sorbent.[43] To assess the practicality of the PPy-based asymmetric system, we
evaluate the economic viability and environmental impact of electrochemically
mediated separations using the PPy-based system under different applied
potentials and compare them with those of conventional activated carbons
used extensively for the mitigation of organic contaminants, and which
are regenerated by thermal desorption or solvent extraction.[44,45] As with the comparison between capacitive deionization and reverse
osmosis in desalination,[46] we use the concept
of specific energy consumption (SE), defined as energy consumption
per gram of organic contaminants removed, to evaluate the energetic
efficiencies of alternative adsorbents and regeneration strategies:where E is the energy consumed
per gram of adsorbent during the regeneration step (J g–1 adsorbent), Qe is the adsorption capacity
(g contaminant g–1 adsorbent), and RE is the regeneration
efficiency.Thermal regeneration of activated carbons typically
involves heating the saturated AC to remove the retained adsorbate.
The intensive heating may cause changes in the carbonaceous structure
of, or mass losses in, the adsorbent, or charred residues may be left
behind on the AC, all of which contribute to the loss of activity
in the regenerated AC.[44] To estimate the
energy consumption during the thermal regeneration of activated carbons,
we calculate the heat requirements according to[47,48]where n is the total purge
gas used (mol of purge gas per gram of activated carbons), Cp is the heat capacity of the purge gas, and TR and T0 are the
regeneration and reference temperatures, respectively.Activated
carbons can also be regenerated through extraction of
adsorbates with organic solvents, followed by removal of any retained
solvent. Although this method may prevent mass losses or damage to
the porous structure of AC, the use of a solvent can incur high economic
costs or raise toxicity concerns.[45] Poey
et al. have shown that thermal regeneration is more cost-competitive
than solvent regeneration and becomes increasingly more so at higher
throughput.[49] Solvent regeneration may
take days of soaking of the AC, and the high cost of solvent and capital
requirements for solvent regeneration may be prohibitive for industrial-scale
applications. We therefore focus on benchmarking thermal regeneration
of AC for comparison with the electrochemical regeneration operations.For the PVF–PPy//PPy(AOT) asymmetric system, the energy
consumption for the electrochemical regeneration is obtained from
the electrical energy involved in the discharge process at the defined
applied potentials:where q is the total charge
transferred between the electrodes at the cell potential Eapp applied to the PVF–PPy//PPy(AOT) system, and m is the total mass of polymers on the electrodes. Further
details are given in the Supporting Information, Section S3.Table lists the
key parameters and compares the energetic efficiencies of the activated
carbons and the PPy-based system with their respective regeneration
methods. The PVF–PPy//PPy(AOT) asymmetric system, when regenerated
at 0.9 V and reactivated at 0.3 V, is more efficient than when electrochemical
modulations at 1.2 V/0 V are used, and than the thermal regeneration
of activated carbons. The SEs of the thermally regenerated activated
carbons for organic compounds and the PVF–PPy//PPy(AOT) system
are quite similar in magnitude. An additional sensitivity analysis
on the relative efficiencies of thermal regeneration of activated
carbons and the electrochemical regeneration of the PVF–PPy//PPy(AOT)
systems is given in the Supporting Information, Section S3.
Table 2
Comparison of the
Energy Efficiencies
for Activated Carbons Regenerated by Thermal Desorption, and PVF–PPy//PPy(AOT)
Regenerated Electrochemically
activated carbons
PVF–PPy//PPy(AOT)
metric
thermal
0–1.2 V
0.3–0.9 V
energy consumption (J g–1 adsorbent)
235
27
12
specific energy consumption (SE) (J g–1 contaminant)
1474
2395
1258
Capital cost and material costs are also important factors for
determining the economic viability of these alternative technologies.
The high-temperature operations demand deployment of stainless-steel
equipment, incurring high capital costs, and require large-scale centralized
facilities to achieve economy of scale.[42] For the PPy-based asymmetric system, the manufacturing cost of the
novel materials on a large scale are yet to be determined.On
the basis of this analysis, we conclude that the PVF–PPy//PPy(AOT)
cell regenerated at 0.9 V and subsequently reactivated by charging
the system at 0.3 V which is competitive in terms of specific energy
consumption (SE) among the cases considered here. The SE values for
the electrochemically regenerated PVF–PPy//PPy(AOT) are conservative
and can be enhanced if the energy in the reactivation (shorting) step
can be recovered and stored for subsequent desorption processes. Moreover,
the adsorption capacity of the PVF–PPy//PPy(AOT) used in the
calculation is obtained from the cyclic experiment where the system
was exposed to very dilute solutions containing Sudan Orange G and
is only ∼1/5 of the maximum value measured. These considerations
warrant further investigation of the electrochemically mediated separation
technology and adsorbent materials to improve their robustness and
economic viability.
Selective Separation of
Organic Pharmaceutical
Compounds
We have previously shown the robustness of the
two polypyrrole-based adsorbent materials in the adsorption and release
of organic species, including pharmaceuticals such as propranolol
hydrochloride (PP) and carcinogenic aromatics such as bisphenol A.[2,24] Many separation scenarios involve mixtures of organic compounds
to remove impurities or recover valuable molecules.[3] For example, in the manufacture of PP, a β-adrenergic
blocking agent widely used to treat hypertension and angina pectoris,
many intermediate products emerge from the multistep synthesis pathway
and, hence, need to be removed to be compliant with the regulatory
requirement that the relative concentrations of individual impurities
be below 0.2%.[50] We explored the ability
of the PVF–PPy//PPy(AOT) system to separate a mixture of propranolol
hydrochloride (PP) and one of the impurities found in the synthesis
mixture, unreacted 1-naphthol (1-NO), which participates in an alkylation
reaction with epichlorohydrin, the first reaction in the pathway to
produce PP.[51]We first compared the
individual propensities of PP and 1-NO to adsorb on the PVF–PPy
and PPy(AOT) electrodes by measuring their equilibrium distribution
coefficients in single component solutions.Here, Qe (mg g–1) is the mass of the adsorbed organic compound (PP
or 1-NO) per gram of polymer, and Ce (mg
L–1) is the concentration of the respective compound
in the liquid phase. As shown in Figure a, the Kd values
for 1-NO are higher than those for PP at the corresponding potentials,
suggesting that higher selectivity for 1-NO impurities over PP will
be afforded by the asymmetric system. The separation factor (α)
defined as the ratio of the distribution coefficients for 1-NO and
PPis on average 8.5 for the different
applied
potentials (Figure a).
Figure 6
(a) Equilibrium distribution coefficients Kd for 1-NO and PP between the PVF–PPy// PPy(AOT) electrodes
and the aqueous solutions containing a single component when the asymmetric
system is subjected to different potentials prior to the adsorption
(left y axis and bars). The resulting separation
coefficients deduced from ratios of the measured Kd values (right y axis and squares).
(b) Removal efficiencies (left y axis and bars) and
separation factors (right y axis and squares) for
five consecutive cycles of separations of a PP and 1-NO mixture.
(a) Equilibrium distribution coefficients Kd for 1-NO and PP between the PVF–PPy// PPy(AOT) electrodes
and the aqueous solutions containing a single component when the asymmetric
system is subjected to different potentials prior to the adsorption
(left y axis and bars). The resulting separation
coefficients deduced from ratios of the measured Kd values (right y axis and squares).
(b) Removal efficiencies (left y axis and bars) and
separation factors (right y axis and squares) for
five consecutive cycles of separations of a PP and 1-NO mixture.We tested the selectivity and
reusability of the PVF–PPy//PPy(AOT)
asymmetric system by conducting five consecutive separations of a
binary mixture of 30.6 mg L–1 PP and 3.6 mg L–1 1-NO, a concentration ratio which simulates that
of a typical product–impurity mixture. Figure b shows that up to 85% of 1-NO can be removed
while only roughly 40% of PP is taken up in the first cycle. Moreover,
the removal efficiency of PP suffers a greater loss compared to that
of 1-NO in subsequent cycles. The observed separation factor when
the binary mixture of PP and 1-NO (Figure b) is challenged is on average 7.0, slightly
lower than that deduced from the ratio of Kd values measured with a single component present in the solution,
likely due to the competitive binding of PP and 1-NO onto PVF–PPy//PPy(AOT).
The interplay between different organics and their impact on the selectivity,
capacity, and reversibility of the electrochemically regenerable adsorbent
warrant further investigation but are beyond the scope of this paper.
Stability of the PPy-Based Polymers
We
have demonstrated that the asymmetric system can maintain over
91% of the initial capacity over five consecutive adsorption/desorption
cycles. Past studies have shown that the PVF–PPy and PPy(AOT)
materials can sustain greater than 50 cycles of electrochemical charging/discharging.[2,24] One potential source of instability is the leaching of the AOT dopants
due to a decrease in electrostatic interaction when PPy(AOT) is reduced.
If AOT anions leached into the desorption solution they would become
new contaminants as well as cause a decrease in the ability to modulate
the hydrophobicity of the PPypolymer. An AOT surfactant of the monomer
form is less toxic than that at higher concentrations (3 mM or 96
ppm sulfur) at which micelles are formed, according to an in vitro study of AOT stabilized silver nanoparticles.[52] Due to the geometry of AOT, however, it is difficult
for AOT surfactants alone to form micelles in water.We investigated
the leaching of AOT dopants by monitoring the sulfur content in the
desorption solution using an inductively coupled plasma optical emission
spectrometer (ICP-OES) with a detection limit down to 0.1 ppm. We
were unable to detect any sulfur content in the desorption solution
after applying 1.2 V to the asymmetric system, the highest potential
considered in this study (Section S4, Supporting
Information), suggesting stability of the materials suitable for the
application.The robustness of the polymer-coated electrodes
may be further
challenged by the presence of larger organic matter (e.g., humic acids)
in the aqueous streams. Additional research is required to determine
the likelihood of fouling on the two dissimilar polypyrrole-based
adsorbents. Alternatively, organic matter can be removed using membrane-based
technologies prior to application of the asymmetric system for the
targeting of organic molecules in solution.
Conclusion
We have designed an asymmetric system consisting
of PPy(AOT) and
PVF–PPypolymers for electrochemically mediated separations
of organics from water, exploiting their complementary tunabilities
in hydrophobicity. We demonstrated reusability of the system for 5
cycles. The asymmetric system showed improvements in suppressing parasitic
water splitting reactions to maintain solution pH and to reduce loss
of electrical energy to side reactions. In energetic efficiency terms,
the electrochemically mediated separation technology using the PVF–PPy//PPy(AOT)
system is competitive in comparison with thermally regenerated activated
carbons. The system also shows selectivity for certain organics present
in mixtures, suggesting potential applications in pharmaceutical and
other such purifications. The ease of implementation of the PVF–PPy//PPy(AOT)
system, only requiring mild electrical energy for regeneration which
can potentially be derived from renewable sources, permits electrochemically
mediated separations to be performed both in industrial settings and
at distributed or remote locations.
Experimental
Section
Electrochemical Synthesis and Characterizations
of Polymers
The two types of polypyrrole-based electrodes
were prepared through reported electropolymerization methods[2,24,28] on a PARSTAT MC 2000 potentiostat
with an auxiliary electrometer (Princeton Applied Research) in a three-electrode
configuration. The working, counter, and reference electrodes were
carbon fiber cloth (ElectroChem Inc.), a platinum wire (BASi), and
Ag/AgCl (3 M NaCl), respectively. For PPy(AOT), the electropolymerization
bath contained 0.3 M pyrrole (Millipore Sigma), 0.3 mg mL–1 bipyrrole (Toronto Research Chemicals), and 0.1 M sodium dioctyl
sulfosuccinate (Millipore Sigma).[24] A constant
current density of 2.5 mA cm–2 was applied for 5
min to yield a polymer loading of 2.85 ± 0.08 mg cm–2.[24] For PVF–PPy, the bath contained
2 mg mL–1 PVF (molecular weight 50 000 g
mol–1, Polysciences), 0.2 M pyrrole, and 0.1 M tetrabutylammonia
perchlorate (Millipore Sigma) in chloroform.[24] A constant current potential of 0.7 V was applied for 10 min to
yield a polymer loading of 5.68 ± 0.47 mg cm–2. Cyclic voltammetry (CV) measurements were done in 0.1 M potassium
chloride (KCl) aqueous solution.
Separation
of Organic Solutes
Adsorption
studies were performed at ambient temperature in 20 mL scintillation
vials continuously shaken at 150 rpm to increase mixing. The concentrations
of the model contaminant Sudan Orange G and pharmaceutical
synthesis compounds propranolol hydrochloride (PP) and 1-naphthol
(1-NO) (Millipore Sigma) in the aqueous phase (Ce) were measured by a Cary 60 ultraviolet–visible (UV–vis)
spectroscope. The mass of solute adsorbed to PPy(AOT)- and PVF–PPy-coated
electrodes was determined as , where Qe (mg
g–1 polymer) is the solute adsorbed per gram of
polymer, C0 (mg L–1)
and Ce (mg L–1) are
the initial and final solute concentrations in the solution phase,
respectively, m (g) is the mass of the particular
type of polymer on the carbon fiber cloth substrate, and Vol (L) is
the volume of solution. The Freundlich isotherm equation was fitted
to the batch adsorption data. We assembled the two electrodes into
the PVF–PPy//PPy(AOT) asymmetric system for adsorption studies,
rendered both materials hydrophobic by discharging at 0 or 0.3 V,
waited until equilibrium was reached, and then regenerated the system
by applying a positive potential (0.9 or 1.2 V) for 10 min in 5 mL
of 0.1 M KCl solution. The adsorption process was monitored for up
to 24 h, and equilibrium was typically reached with 10 h. To reuse
the electrodes in subsequent cycles of adsorption, the polymer was
reactivated for adsorption by applying 0 or 0.3 V for 10 min in the
same 0.1 M KCl desorption solution. Concentrations of PP and 1-NO
in the binary mixture were determined using high-performance liquid
chromatography (HPLC) equipped with a flame-ionization detector (FID)
(Agilent) and a ZORBAX Extend 80 Å C18 (4.6 × 50 mm, 5 μm)
analytical column (2.1 mm × 50 mm, particle size 3.5 μm).
Samples for the HPLC analysis were prepared by adding 20 μL
of N-benzylmethylamine as internal standards to 1
mL of solutions. Samples of 5 μL were injected and eluted using
a gradient pump delivering 1 mL min–1 of a water
and acetonitrile mobile phase, each containing 0.1 vol % formic acid.
OpenLab CDS software was used to determine the area under the peaks
in the chromatograms and to carry out baseline correction. All results
reported are based on the average of three replicates.
pH Monitoring
To assess the impact
of parasitic reactions due to water electrolysis, pH was monitored in situ during electrochemical modulation of the hydrophobicity
of the materials through potential swings. A custom LabView program
and the Orion ROSS Combination Semimicro pH electrode were used to
collect the pH data. The evolution of OH– was directly
computed from pH fluctuations and subsequently converted to the charges
lost to hydrogen or oxygen evolution reactions, respectively.
Assessment of AOT Leaching
To assess
the leaching of AOT during desorption, an inductively coupled plasma
optical emission spectrometer (ICP-OES Optima 8000, PerkinElmer) equipped
with a GemTip cross-flow II nebulizer and a Ryton HF-resistant Scott-type
spray chamber was used to determine the sulfur content in the desorption
solution. Standard solutions for creating the sulfur calibration curve
(Figure S3 in the Supporting Information)
were prepared by sequential dilution of a stock solution (Millipore
Sigma 1000 mg L–1 S in H2O). The operating
conditions for the ICP-OES analysis were as follows: wavelength, 180.669
nm; radio frequency power, 1500 W; principal plasma gas flow-rate,
10.0 L min–1; auxiliary gas flow-rate, 0.2 L min–1; and nebulizer gas flow-rate, 0.7 L min–1.
Safety Statement
No unexpected or
unusually high safety hazards were encountered.
Authors: René P Schwarzenbach; Beate I Escher; Kathrin Fenner; Thomas B Hofstetter; C Annette Johnson; Urs von Gunten; Bernhard Wehrli Journal: Science Date: 2006-08-25 Impact factor: 47.728
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