energies
Article Improving the Energy Efficiency of Direct Formate Fuel Cells with a Pd/C-CeO2 Anode Catalyst and Anion Exchange Ionomer in the Catalyst Layer
Hamish Andrew Miller 1,*, Jacopo Ruggeri 1,2, Andrea Marchionni 1 ID , Marco Bellini 1, Maria Vincenza Pagliaro 1, Carlo Bartoli 1, Andrea Pucci 2 ID , Elisa Passaglia 3 ID and Francesco Vizza 1,*
1 Istituto di Chimica dei Composti Organometallici (CNR-ICCOM), Via Madonna del Piano 10, 50019 Sesto Fiorentino, Firenze, Italy; [email protected] (J.R.); [email protected] (A.M.); [email protected] (M.B.); [email protected] (M.V.P.); [email protected] (C.B.) 2 Department of Chemistry and Industrial Chemistry, University of Pisa, Via Moruzzi 13, 56124 Pisa, Italy; [email protected] 3 Istituto di Chimica dei Composti Organometallici (CNR-ICCOM), Area della Ricerca, Via G. Moruzzi 1, 56124 Pisa, Italy; [email protected] * Correspondence: [email protected] (H.A.M.); [email protected] (F.V.); Tel.: +39-055-5225336 (H.A.M.); +39-055-5225286 (F.V.)
Received: 12 January 2018; Accepted: 31 January 2018; Published: 5 February 2018
Abstract: This article describes the development of a high power density Direct Formate Fuel Cell (DFFC) fed with potassium formate (KCOOH). The membrane electrode assembly (MEA) contains no platinum metal. The cathode catalyst is FeCo/C combined with a commercial anion exchange membrane (AEM). To enhance the power output and energy efficiency we have employed a nanostructured Pd/C-CeO2 anode catalyst. The activity for the formate oxidation reaction (FOR) is enhanced when compared to a Pd/C catalyst with the same Pd loading. Fuel cell tests at 60 ◦C show a peak power density of almost 250 mW cm−2. The discharge energy (14 kJ), faradic efficiency (89%) and energy efficiency (46%) were determined for a single fuel charge (30 mL of 4 M KCOOH and 4 M KOH). Energy analysis demonstrates that removal of the expensive KOH electrolyte is essential for the future development of these devices. To compensate we apply for the first time a polymeric ionomer in the catalyst layer of the anode electrode. A homopolymer is synthesized by the radical polymerization of vinyl benzene chloride followed by amination with 1,4-diazabicyclo[2.2.2]octane (DABCO). The energy delivered, energy efficiency and fuel consumption efficiency of DFFCs fed with 4 M KCOOH are doubled with the use of the ionomer.
Keywords: direct alcohol fuel cells; formate; alkaline membrane; palladium; ceria; ionomer; energy efficiency
1. Introduction Direct Formate Fuel Cells (DFFCs) are attractive power sources because as a fuel formate salts have specific advantages compared to alcohols like methanol and ethanol [1]. Formate salts can be easily stored, transported, and handled in their solid state and can be combined with water to form a liquid fuel solution [2]. Worldwide production of its precursor formic acid is around 7.2 × 105 t·y−1. Although industrial production involves fossil fuel derived precursors, formic acid can be obtained by renewable means such as the electrochemical reduction or catalytic hydrogenation of CO2 (the energy or hydrogen used in such processes must be derived from renewable energy sources) [3–7]. DFFCs operate under alkaline conditions, which is advantageous as both the formate
Energies 2018, 11, 369; doi:10.3390/en11020369 www.mdpi.com/journal/energies Energies 2018, 11, 369 2 of 12 oxidation reaction (FOR) and the oxygen reduction reaction (ORR) have high kinetics. Under basic conditions non-platinum catalysts can be used in the electrodes [8]. At high pH, the FOR does not pass through poisoning intermediates such as CO that can quickly passivate catalyst metal surfaces. A fuel cell running on formate and air at the cathode has a theoretical cell potential as high as 1.45 V (Equations (1)–(3)) which means DFFCs can produce high power densities:
− − 2− − ◦ HCOO + 3OH → CO3 + 2H2O + 2e Ea = −1.05 V (1)
− − ◦ 1/2O2 + H2O + 2e → 2OH Ec = 0.4 V (2) − − 2− ◦ HCOO + 1/2O2 + OH → CO3 + H2OE = 1.45 V (3) Recent examples of platinum-free DFFCs equipped with a combination of anion exchange membranes (AEMs) and air or oxygen fed cathodes show the potential for high power devices −2 ◦ with peak power densities in the range of 250–300 mW cm (Tcell = 60 C) [9–14]. We have recently reported a study of the energy efficiency of Pt-free DFFCs (Pd/C anode, FeCo/C cathode and AEM). The highest energy efficiency (42%) is obtained using high energy density fuel (4 M KCOOH and 4 M KOH) with a maximum operating temperature of 60 ◦C[15]. Another important aspect is that formate oxidation has fast kinetics, even when the OH− electrolyte (KOH or NaOH) is not present in the fuel solution, meaning that the fuel cell can also operate at intermediate pH values [9,16,17]. Haan et al. demonstrated that the FOR is not dependent on pH between 9 and 14, which permits the use of formate fuel without added hydroxide [18]. Alkaline direct alcohol fuel cells (DAFCs) that operate with an electrolyte consume at least one mole of base for every oxidized fuel molecule. A high pH (13–14) is also required to guarantee sufficient alcohol oxidation kinetics [19]. In general, these constraints make the fuel energy efficiencies of alkaline DAFCs very low (less than 7%) [20]. To this, we must also consider the energy cost of the base consumed in the fuel cell reaction which results in a negative energy yield for alkaline DAFCs [21]. Hence, removal of the costly electrolyte (e.g., KOH) is essential for a practical application of these devices as power sources. This is possible with formate as fuel. Haan and coworkers achieved 105 mW cm−2 peak power density with a 1 M aqueous HCOOK fuel solution [18]. Zhao et al. reached a peak power density of 130 mW cm−2 with 5 M HCOOK [14]. Instantaneous power density output (obtained from fuel cell polarization curves) is valuable in understanding the activity of the fuel cell system at its beginning of life. However, it must also be demonstrated that a DFFC operating with no added electrolyte can also produce sufficient discharge energy, fuel energy efficiency and fuel conversion efficiency on every single fuel loading. Without added electrolyte, the ionic conductivity of the membrane electrode assembly (MEA) is reduced significantly, leading to large ohmic losses. Improving the ionic conductivity within the catalyst layer is a key factor in overcoming the loss of ionic conductivity that is usually guaranteed by the liquid electrolyte. A number of research groups have developed anion exchange ionomers for inclusion in the catalyst layer of anion exchange MEAs. As far as we know these materials have been exclusively developed for H2/air or H2/O2 AEM-FCs [22,23]. Improved anodic catalyst materials are also required to increase the energy output and efficiency of DFFCs [24]. The activity and efficiency of Pd based nanoparticle anode catalysts for alkaline DAFCs have been shown to improve with the addition of certain metal oxides to the conductive carbon support [20,24,25]. The most successful demonstration of this phenomenon has been the addition of CeO2 to Vulcan XC-72 carbon [20]. This mixed support with deposited Pd nanoparticles showed enhanced activity for ethanol electrooxidation in DAFCs. The ceria contributes to the decrease of the onset potential of ethanol oxidation. It was proposed that CeO2 promotes the formation at low potentials of species adsorbed on Pd, (e.g., Pd(I)-OHads), that are involved in ethanol oxidation. The energy efficiency of the DAFC with Pd/C-CeO2 was shown to be double that of the same fuel cell with a Pd/C anode catalyst [20]. Here we report for the first time the use of a Pd/C-CeO2 anode catalyst for the FOR in DFFCs. We demonstrate that this catalyst has enhanced activity and fuel energy efficiency. In this paper, Energies 2018, 11, 369 3 of 12 we also address the issue of removal of the liquid KOH electrolyte from the fuel solution. We include an energy analysis that shows that any added KOH electrolyte in the fuel solution results in a negative Energies 2018, 11, x FOR PEER REVIEW 3 of 12 net energy delivery from the fuel cell. For the first time a polymeric ionomer is applied to improve the efficiencyenergy analysis of DFFCs. that shows Hence that we any report added the KOH synthesis electrolyte and in characterization the fuel solution ofresults a polymeric in a negative ionomer basednet upon energy a styrenic delivery 1,4-diazabicyclo[2.2.2]octane from the fuel cell. For the first time (DABCO) a polymeric salt repeating ionomer is unit. applied The to application improve of this ionomerthe efficiency in the of anodeDFFCs. catalyst Hence we layer report leads the synthesis to a doubling and characterization of the DFFC energy of a polymeric efficiency ionomer with 4 M ◦ HCOOKbased as upon fuel a (T styreniccell = 60 1,4-diazabicyclo[2.2.2]octaneC). The faradaic efficiency (DABCO) (fuel salt conversion) repeating unit. matches The application that of a cell of fed with 4this M ionomer KOH electrolyte. in the anode The catalyst results layer of thisleads study to a doubling help to pushof thethe DFFC development energy efficiency of DFFCs with 4 closer M to practicalHCOOK application. as fuel (Tcell = 60 °C). The faradaic efficiency (fuel conversion) matches that of a cell fed with 4 M KOH electrolyte. The results of this study help to push the development of DFFCs closer to 2. Resultspractical and application. Discussion
2. Results and Discussion 2.1. Pd/C-CeO2 Catalyst FOR Activity
Two2.1. Pd/C-CeO anode FOR2 Catalyst catalysts FOR areActivity compared (Pd/C and Pd/C-CeO2) each with 10 wt % loading of Pd nanoparticles (NPs). Each was prepared as described in our previous publication [26]. In particular, Two anode FOR catalysts are compared (Pd/C and Pd/C-CeO2) each with 10 wt % loading of Pd Pd/C-CeOnanoparticles2 was prepared(NPs). Each by was the prepared reduction as described and deposition in our previous of Pd onto publication a mixed [26]. conductive In particular, support (50 wtPd/C-CeO % carbon2 was and prepared 50 wt % by CeO the2 reduction(C-CeO2 )).and A deposition cyclic voltammetry of Pd onto a (CV) mixed investigation conductive support of Pd/C-CeO (50 2 was undertakenwt % carbon inand N 502-saturated wt % CeO2 2 (C-CeO M aqueous2)). A cyclic KOH voltammetry solution at room(CV) investigation temperature of (Figure Pd/C-CeO1A).2 was The CV curveundertaken shows features in N2-saturated characteristic 2 M foraqueous both PdKOH and solution CeO2 centeredat room temperature transitions assigned(Figure 1A). by The comparison CV to literaturecurve shows data as features follows. characteristic On the forward for anodicboth Pd scan and (0 toCeO 1.42 V),centered there aretransitions three transitions. assigned Thereby is a broadcomparison peak centered to literature at 0.4 Vdata due as to follows. the oxidative On the desorptionforward anodic of hydrogen scan (0 to (A 1.41). V), The there peak are at three 0.6 V (A2) transitions. There is a broad peak centered at 0.4 V due to the oxidative desorption of hydrogen (A1). is ascribed to the formation of palladium hydroxides. At higher potentials (0.9−1.4 V), the formation The peak at 0.6 V (A2) is ascribed to the formation of palladium hydroxides. At higher potentials of palladium oxides takes place. On the reverse cathodic scan (1.4 to 0 V), the peak at 0.7 V (C1) is (0.9−1.4 V), the formation of palladium oxides takes place. On the reverse cathodic scan (1.4 to 0 V), assignedthe peak to the at reduction0.7 V (C1) is of assigned Pd oxides, to the whereas reduction the of broad Pd oxid cathodices, whereas transition the broad at potentialscathodic transition between 0.4 2 to 0.2at V potentials (C ) is attributed between 0.4 to hydrogento 0.2 V (C2) adsorption. is attributed to hydrogen adsorption.
Figure 1. (A) Typical CV of Pd/C-CeO2 in N2 saturated 2 M KOH (scan rate: 10 mV·s−1) and −(B1) Figure 1. (A) Typical CV of Pd/C-CeO2 in N2 saturated 2 M KOH (scan rate: 10 mV·s ) and Comparison of CVs obtained at room temperature of Pd/C-CeO2 and Pd/C in N2 saturated 2 M (B) Comparison of CVs obtained at room temperature of Pd/C-CeO2 and Pd/C in N2 saturated 2 M HCOOK + 0.5 M KOH (scan rate: 10 mV·s−1). HCOOK + 0.5 M KOH (scan rate: 10 mV·s−1).
The electrochemical activity of Pd/C-CeO2 and Pd/C toward the oxidation of formate was Theinvestigated electrochemical with an aqueous activity solution of Pd/C-CeO of 2 M HC2 andOOK Pd/Cand added toward KOH the electrolyte oxidation (0.5 of M) formate (Figure was investigated1B). The with onset an potential aqueous for solution both catalysts of 2 M HCOOKis around and0.2 V added (RHE). KOH The electrolyteoxidizing current (0.5 M) density (Figure 1B). The onsetincreases potential linearly for over both the catalystscomplete potential is around range 0.2 V(0 (RHE).to 1.4 V). The With oxidizing the same Pd current loading density the C-CeO increases2 supported catalyst reaches 140 mA·cm−2 at 1.4 V compared to 80 for the Pd/C catalyst. On the forward linearly over the complete potential range (0 to 1.4 V). With the same Pd loading the C-CeO2 supported scan Pd/C-CeO2 maintains a higher current density for all potentials above 0.4 V. The enhanced catalyst reaches 140 mA·cm−2 at 1.4 V compared to 80 for the Pd/C catalyst. On the forward scan activity for the FOR with Pd/C-CeO2 with respect to Pd/C is due to the oxophilic nature of the CeO2 Pd/C-CeO2 maintains a higher current density for all potentials above 0.4 V. The enhanced activity in the mixed C-CeO2 support and the three-phase (C, CeO2 and Pd) nanostructure. The CeO2 for the FOR with Pd/C-CeO with respect to Pd/C is due to the oxophilic nature of the CeO in the promotes the transfer of OH2 − to the Pd surface thus forming Pd-OHad species at low overpotentials2 mixedthat C-CeO are involved2 support in the and FOR the [20]. three-phase The surface (C, nano CeOstructure2 and Pd) of nanostructure.this catalyst has Thebeen CeOthoroughly2 promotes − the transfercharacterized of OH in toour the Pdrecent surface publications thus forming [25,26]. Pd-OH A combinationad species atof low techniques overpotentials including that are involvedmorphological in the FOR studies [20]. Thei.e., HR-TEM, surface nanostructure Z-contrast STEM, of this EDX catalyst mapping has and been XAS thoroughly spectroscopy characterized (XAFS,
Energies 2018, 11, 369 4 of 12 in our recent publications [25,26]. A combination of techniques including morphological studies i.e., HR-TEM,Energies Z-contrast 2018, 11, x FOR STEM, PEER REVIEW EDX mapping and XAS spectroscopy (XAFS, XANES, XRD) demonstrate4 of 12 that the unique nanostructure involves small Pd NPs (2–3 nm) that are deposited preferentially on the XANES, XRD) demonstrate that the unique nanostructure involves small Pd NPs (2–3 nm) that are CeO portions of the support leaving the carbon part of the support free of Pd [26]. Such a structure 2deposited preferentially on the CeO2 portions of the support leaving the carbon part of the support enhancesfree of the Pd Pd-CeO[26]. Such2 interactionsa structure enhances and consequently the Pd-CeO2 theinteractions FOR activity. and consequently Indeed this the effect FOR resultsactivity. in the enhancementIndeed this in effect activity results and in energy the enhancement efficiency in when activity applied and energy in DFFCs efficiency as described when applied in the in nextDFFCs section. as described in the next section. 2.2. DFFC Performance 2.2. DFFC Performance Anode electrodes were prepared by coating a nickel foam support with a homogeneous mixture −2 of PTFE andAnode Pd/C-CeO electrodes2 (Pd were loading prepared of by 2 mg coating·cm a ).nickel The foam membrane support electrode with a homogeneous assembly (MEA) mixture for cell testingof PTFE was formed and Pd/C-CeO by pressing2 (Pd loading this anode of 2 mg·cm electrode−2). The within membrane the cell electrode hardware assembly together (MEA) with for ancell anion exchangetesting membrane was formed (A201, by pressing Tokuyama this anode Corp., electrode Tokyo, within Japan) the and cell ahardware FeCo/C together on carbon with cloth an anion cathode. exchange membrane (A201, Tokuyama Corp., Tokyo, Japan) and a FeCo/C on carbon cloth cathode. The 4 M HCOOK fuel solution (30 mL) containing various concentrations of KOH (0, 1, 2 and 4 M) The 4 M HCOOK fuel solution (30 mL) containing various concentrations of KOH (0, 1, 2 and 4 M) was recycled through the anode compartment while humidified O was flowed across the cathode. was recycled through the anode compartment while humidified O2 was2 flowed across the cathode. ◦ Cell potentialCell potential scans scans and and constant constant current current experiments experiments were were carried carried out out at a at cell a cell temperature temperature of 60 of°C. 60 C. Cell voltageCell voltage and and power power density density curves curves are are shownshown in Figure Figure 22 andand important important fuel fuel cell cell data data is listed is listed in in TableTable1. 1.
Figure 2. Potential and power density (vs. current density) curves for the DFFC containing the Pd/C- Figure 2. Potential (A) and power density (B) (vs. current density) curves for the DFFC containing CeO2 anode, FeCo/C cathode, A201 AEM and fueled with 4 M HCOOK and various concentrations the Pd/C-CeO2 anode, FeCo/C cathode, A201 AEM and fueled with 4 M HCOOK and various of KOH electrolyte (0, 1, 2 and 4 M) (Tcell 60 °C and Vscan 10 mV·s−1). ◦ −1 concentrations of KOH electrolyte (0, 1, 2 and 4 M) (Tcell 60 C and Vscan 10 mV·s ). The performance of the DFFC is highly dependent upon the KOH electrolyte concentration. As Thecan be performance seen in Table of1 the the peak DFFC power is highlydensity decreases dependent from upon 243 to the 206 KOH and to electrolyte 159 (mW·cm concentration.−2) as the As canKOH be seenconcentration in Table 1drops the peakfrom power4 to 2 and density 1 M. Ma decreasesss transport from limited 243 to cell 206 performance and to 159 is (mW observed·cm− 2) as the KOHin the concentration 4/1 fuel solution drops at higher from4 current to 2 and densiti 1 M.es Mass due transportto excessive limited consumption cell performance of KOH near is observed the electrode surface. The voltage curve obtained with no added KOH shows a significant drop in the in the 4/1 fuel solution at higher current densities due to excessive consumption of KOH near the cell potential at low current densities caused by poor FOR activity of the anode catalyst at the mildly electrode surface. The voltage curve obtained with no added KOH shows a significant drop in the alkaline conditions of the 4 M HCOOK solution. A peak power density of 89 mW·cm−2 is obtained cell potentialwith no KOH, at low 40% current of that densities obtained causedwith an by equivalent poor FOR molar activity amount of theof KOH anode in catalystthe electrolyte at the (4 mildly −2 alkalineM). conditions of the 4 M HCOOK solution. A peak power density of 89 mW·cm is obtained with no KOH,The energy 40% of delivery that obtained of the DFFC with anwith equivalent single fuel molar batches amount (30 cc) ofwas KOH studied in the by electrolyteperforming (4 M). Theconstant energy current delivery density ofexperiments the DFFC (50 withmA·cm single−2) while fuel monitoring batches the (30 cell cc) potential. was studied Each by performingexperiment constant was stopped current when density the experimentscell potential re (50ached mA 0·cm V. −Three2) while consecutive monitoring experiments the cell were potential. Eachcarried experiment out for was each stopped fuel composition when thecell replacing potential the reachedspent solution 0 V. Three each consecutive time with fresh experiments fuel. The were carriedvalues out forof discharge each fuel energy composition (kJ), faradic replacing efficiency thespent (%) and solution energy each efficiency time with(%) were fresh calculated fuel. The as values shown in the supporting information (SI). The data shown in Table 1 are the average of three of discharge energy (kJ), faradic efficiency (%) and energy efficiency (%) were calculated as shown experiments. Typical cell voltage vs. time curves are shown in Figure 3. The best power delivery is in the supporting information (SI). The data shown in Table1 are the average of three experiments. obtained with the 4 M HCOOK, 4 M KOH fuel. The values of discharge energy (14 kJ), faradic Typicalefficiency cell voltage (89%) vs.and timeenergy curves efficiency are shownEE (46%) in ca Figurelculated3. Theas the best average power of three delivery consecutive is obtained 30 cc with the 4 M HCOOK, 4 M KOH fuel. The values of discharge energy (14 kJ), faradic efficiency (89%) Energies 2018, 11, 369 5 of 12 and energy efficiency EE (46%) calculated as the average of three consecutive 30 cc fuel batches are better than the values obtained under identical conditions with a Pd/C catalyst at the anode (12.5 kJ, 88% and 42% respectively) in our recent study [15]. Such high values are obtained with the aid of the KOHEnergies electrolyte 2018, 11, x FOR present PEER REVIEW in the fuel solution. The DFFC running with 4 M HCOOK (no5 of 12 KOH) performs poorly (2 kJ, 51% and 7% respectively). When KOH is present in the fuel solution one mole is consumedfuel batches with everyare better oxidized than the formate values obtained molecule unde (Equationr identical (3)). conditions We can with estimate a Pd/C the catalyst additional at the cost in energyanode terms (12.5 kJ, of 88% the baseand 42% consumed respectively) in the in reaction our recent (6.2 study kJ/g [15]. is the Such net high energy values cost are of obtained electrolytic KOHwith production) the aid of [the27] KOH and calculateelectrolyte whetherpresent in the the addition fuel solution. of KOH The DFFC to the running fuel solution with 4 M is HCOOK energetically (no KOH) performs poorly (2 kJ, 51% and 7% respectively). When KOH is present in the fuel solution convenient (Table2). The data shows clearly that the use of added KOH electrolyte results in a net one mole is consumed with every oxidized formate molecule (Equation (3)). We can estimate the negative energy balance. The energy obtained from the cell is less than that used in the production additional cost in energy terms of the base consumed in the reaction (6.2 kJ/g is the net energy cost of − of theelectrolytic OH consumed KOH production) in the fuel [27] cell and reaction. calculate Only whet aher formate the addition fuel solutionof KOH to without the fuel KOH solution results is in a positiveenergetically energy convenient gain. When (Table no base 2). The ispresent data show ins the clearly fuel solutionthat the use the of product added KOH of oxidation electrolyte CO 2 is releasedresults as gasin a (Equationnet negative (4)) energy [9,10 balance.,18,28]. The energy obtained from the cell is less than that used in the production of the OH− consumed in the fuel cell reaction. Only a formate fuel solution without − − KOH results in a positiveHCOOH energy gain.+ 2OH When no→ baseCO 2is+ present2H2O in+ the2e fuel solution the product of (4) oxidation CO2 is released as gas (Equation (4)) [9,10,18,28].