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Selective Electrochemical Reduction of Nitrogen to Ammonia by Adjusting the Three-Phase Interface
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Haiyan Wang, Yuzhuo Chen, Ruxue Fan, Jiadong Chen, Zhe Wang, Shanjun Mao, Yong Wang
Research. Vol 2019 Article ID 1401209
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Research. Vol 2019 Article ID 1401209
• Research Article •
Selective Electrochemical Reduction of Nitrogen to Ammonia by Adjusting the Three-Phase Interface
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Haiyan Wang, Yuzhuo Chen, Ruxue Fan, Jiadong Chen, Zhe Wang, Shanjun Mao, Yong Wang
Affiliations
  • Advanced Materials and Catalysis Group, Institute of Catalysis, Department of Chemistry, Zhejiang University, Hangzhou 310028, China
About Author:

Authors’ Contributions

H. Wang and Y. Wang conceived and designed the experiments. H. Wang synthesized the catalysts and conducted the experimental work. Y. Chen performed the DFT calculations. R. Fan, Z. Wang, and S. Mao assisted in the experimental work. H. Wang and Y. Wang cowrote the paper. Y. Wang supervised the work.

Published: 2019-11-20 doi: 10.34133/2019/1401209
Outline
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The electrochemical nitrogen reduction reaction (NRR) provides a sustainable and alternative avenue to the Haber-Bosch process for ammonia (NH3) synthesis. Despite the great efforts made on catalysts and electrolytes, unfortunately, current NRR suffers from low selectivity due to the overwhelming competition with the hydrogen evolution reaction (HER). Here, we present an adjusted three-phase interface to enhance nitrogen (N2) coverage on a catalyst surface and achieve a record-high Faradic efficiency (FE) up to 97% in aqueous solution. The almost entirely suppressed HER process combined with the enhanced NRR activity, benefiting from the efficient three-interface contact line, is responsible for the excellent selectivity toward NH3, as evidenced by the theoretical and experimental results. Our strategy also demonstrates the applicability to other catalysts that feature strong H adsorption ability, to boost the FE for NH3 synthesis above 90% and to improve the NRR activity by engineering the catalysts.

Haiyan Wang, Yuzhuo Chen, Ruxue Fan, Jiadong Chen, Zhe Wang, Shanjun Mao, Yong Wang. Selective Electrochemical Reduction of Nitrogen to Ammonia by Adjusting the Three-Phase Interface[J]. Research, 2019 , 2019 (11) : 1401209 - . DOI: 10.34133/2019/1401209
The electrochemical nitrogen reduction reaction (NRR) to ammonia (NH3) at ambient conditions provides a sustainable and distributed alternative to the Haber-Bosch process for making fertilizers and energy carriers [1–5]. However, the inertness of nitrogen (N2) with a strong N≡N triple bond (bonding energy of 940.95 kJ mol-1), nonpolarity, and negative electron affinity typically result in a large overpotential and a very low Faradic efficiency (FE) (typically <10%) for NRR [6–8]. In addition, the NRR competes fiercely with the hydrogen evolution reaction (HER). Most metal catalysts with low NRR overpotentials favor adsorption of H over N2, resulting in a tendency to produce hydrogen (H2) rather than NH3 [9–11]. Furthermore, the large energy gap (10.82 eV) between the highest occupied and the lowest unoccupied molecular orbitals of N2 does not favor the one- or two-electron transfer process and therefore endows the NRR with sluggish kinetics [12–14]; most protons and electrons go toward generating H2. Consequently, the selectivity remains a major challenge for the multielectron and multiproton NRR pathways in competing with the dominant HER for active catalysts.
Substantial efforts have been dedicated to optimization of the NRR selectivity by developing various heterogeneous electrocatalysts including metals, metal oxides, and nonmetallic materials, particularly focused on tailoring the particle size, crystallinity, morphology, defect density, and surface active sites [15–28]. For example, single-atom catalysts were demonstrated to have an atomic ensemble effect on suppressing the HER since it was perceived that only the top site of single-atom catalysts with positive relative energies contributed to H adsorption, with respect to the multiple adsorption sites (top, bridge, and hollow) for bulk metal surfaces [29]. But to date, the highest FE achieved for these single-atom catalysts is limited to 56.6% as the HER remains to be a highly competitive reaction [30]. Recently, the rates of NH3 and H2 production were deemed to be, respectively, zeroth order and first order in the electron and proton concentrations [31]. Thus, it was suggested that reducing the proton and electron supply would slow down the HER kinetics and make N2 more accessible to the surface active sites, thereby promoting the NRR conversion. In this respect, a number of strategies were implemented to expect an improvement on the selectivity toward NH3 by using an aprotic solvent with extremely few proton donors [32, 33], a hydrophobic protection layer to hinder proton transport [33, 34], or an insulator-metal-catalyst electrode to slow down the electron tunneling [16, 31]. Yet in spite of the small increase in selectivity, the NH3 yield decreased significantly due to the proton-coupled electron transfer reaction mechanism [35]. Conventionally, a gas reactant needs to dissolve in the electrolyte solution and electrochemical reactions take place in the solid-liquid two-phase interface [36]. Thus, the electrocatalytic activity was limited by the inefficient gas mass transport seriously. Accordingly, another method for preferential production of NH3 is to increase the concentration of N2 in electrolyte solution in view of the fact that most organic solvents can dissolve N2 by one or two orders of magnitude higher than water. An impressive FE of 60% was achieved by adopting an aprotic fluorinated ionic liquid which had higher N2 solubility compared with water (17 vs. 0.66 mmol L-1) [37]. Nevertheless, the NH3 production rate was limited to 10-12 mol s-1 cm-2. A recent work achieved high NRR selectivity (90%) via a superhydrophobic MOF layer to repel water molecules and trap N2, but at a cost of low activity [34]. Hence, the accessibility of adequate N2 molecules to the catalyst is critical but generally deficient, and it is difficult to obtain orders of magnitude improvement in selectivity while maintaining the activity by only manipulating the concentration of N2 [31], although a theoretical study has pointed out the preference for NH3 formation if the catalyst surface is covered with N2 rather than H adatoms [10]. Previous reports have found that the selectivity and activity of CO2 reduction are significantly affected by the CO2 concentration at the catalyst surface and both can be improved by adjusting the reaction interface [38, 39]. Besides, the solid-state electrochemical NRR cell with electrodes exposed to N2 also demonstrates the promise to overcome the low conversion of the conventional catalytic reactors, but its performance is limited by the relative poor transport of protons and electronics [40]. Therefore, we believe that effective electrochemical reduction of nitrogen to ammonia requires efficient contact of N2 (gas), H+ (liquid), and catalyst (solid).
In the present work, we proposed a simple strategy to enhance the coverage of N2 on the catalyst surface in aqueous acid and promote the gas-solid catalyst-liquid electrolyte three-phase reaction interface. Different from the traditional reaction interface, in the adjusted three-phase interface, N2 does not have to be dissolved in the electrolyte and N2 bubbles surrounded the catalyst to promote substantial N2 molecules adsorbing and occupying the active sites preferentially. A high FE to NH3 of ~97% was achieved on a common supported Pd catalyst at 0.1 V vs. the reversible hydrogen electrode (RHE) in an acidic aqueous solution (0.1 M HCl). Our strategy could be easily extended to other catalysts such as Ir and RuPd, though they feature strong H adsorption ability to boost the FE for electrocatalytic NRR. Moreover, excellent NRR activity was then achieved by employing the adjusted three-phase interface and engineering catalysts with more active sites. Our results offer a new outlook to break through the limitations in selectivity toward NH3 from renewable energy sources especially in aqueous solution and also provide valuable insights to enhance the electrocatalytic performance of solid catalysts in a proton-sensitive competition system.
Increasing N2 coverage (θN2) on the electrocatalyst should be an effective strategy to increase the N2 selectivity to NH3, and the HER process can be suppressed seriously (see Supplemental Information: Effect of θN2 on selectivity). In order to gain a theoretical insight into the suppression of HER with the increase in θN2 on the Pd surface, a p3×3 model for Pd(111), Pd(100), and Pd(211) facets with various θN2 was built and the following H adsorption has been investigated using density functional theory (DFT) calculations in this work. The adsorption configuration of N2 was chosen to be vertical rather than parallel (Figure S1), which means θN2 can vary from 1/9 ML to 1 ML on Pd(111) and Pd(100) facets and 1/9 ML to 6/9 ML on Pd(211) theoretically owing to its step-like property and the repulsion between vertical adsorbed N2. As shown in Figure 1(a), EadsH decreases with the increase in θN2 on the Pd(100) facet and quickly approaches 0 at 7/9 ML of θN2, implying the gradually weakened adsorption of H. Additionally, H prefers permeating into Pd bulk, forming a PdH compound, rather than being on the surface stably at high θN2 such as 7/9 ML (Figure 1(a)). As a result, the HER process, which requires surface-adsorbed H on the Pd(100) surface, was extensively suppressed. Similar phenomena could occur on other facets such as Pd(211) and Pd(111) (Figures S2 and S3). Hence, one can conclude that the HER process can be greatly repressed with the increase in θN2 on the Pd surface via inhibiting the stable adsorption of H on active sites, thereby enhancing N2 reduction selectivity toward NH3. However, traditionally, N2 is dissolved in the electrolyte and the NRR occurs in the solid-liquid two-phase interface, solid catalyst-electrolyte solution, as shown in Figure 1(b). As the solubility of N2 in water is as low as 0.66 mmol L-1 under standard temperature and pressure, corresponding to ~5 orders of magnitude fewer N2 molecules than water molecules, the NRR activity is severely limited by the inefficient N2 mass transport and H (or H2O) has the priority over N2 to occupy the active sites, leading to a dominant HER process and poor selectivity to NH3. Therefore, in order to increase the coverage of N2 instead of H adatoms on the catalyst surface, the gas- (N2) solid- (catalyst) liquid (electrolyte solution) three-phase contact line should be enhanced to promote efficient gas mass transport. In the adjusted three-phase interface (Figure 1(c)), contrary to the traditional reaction interface (Figure 1(b)), N2 does not have to be dissolved in the electrolyte and the catalysts are surrounded by N2 bubbles, and thereby adequate N2 molecules can adsorb and occupy the active sites preferentially, consequently hindering the stable adsorption of H and suppressing the HER. With N2 bubbles covering catalyst surfaces, NRR can take place at the interface where N2 bubbles, solid catalysts, and electrolytes contact meanwhile, thus improving the electrocatalytic NRR performances.
To demonstrate the feasibility of the adjusted three-phase interface for electrochemical NRR, a common Pd/activated carbon cloth (Pd/ACC) catalyst was prepared via an ultrasound-assisted reduction technique. The ACC support had a microporous structure and a specific surface area of 96 m2 g-1 (Figure S4). The representative high-angle annular dark-field scanning transmission electron microscopy (HADDF-STEM) image revealed well-dispersed nanoparticles with an average size centered at 4.5 nm (Figure 2(a)). The lattice spacing of the nanoparticles was measured to be 0.196 nm and 0.225 nm, corresponding to the (200) and (111) planes of Pd, respectively (Figure 2(b)). The X-ray diffraction (XRD) pattern of Pd/ACC could be indexed to face-centered cubic (fcc) Pd (PDF#65-6174) (Figure 2(c)). Additionally, X-ray photoelectron spectroscopy (XPS) results showed the presence of C, O, and Pd in the catalyst without the signal of N (Figure S5), and the surface Pd was mainly in a metallic state and partially oxidized to Pd2+ and Pd4+ (Figure 2(d)).
The electrocatalytic NRR activities of the Pd/ACC catalyst were then measured in 0.1 M HCl solution in a gas-tight two-compartment electrochemical cell separated with a Nafion 211 membrane and connected with a gas absorber (Figure 3(a)). To reduce a false positive from potential contaminant in the input gas stream, ultra-high-purity N2 (99.9999% purity) was used as the feeding gas and the potential NOx in N2 was detected with a nitrite assay kit and by gas chromatography and diffuse reflectance infrared Fourier transform spectroscopy (DRIFTS) before NRR tests (see Supplemental Information and Determination of NOx Contamination in Ultra-High-Purity N2 Gas). Almost no nitrite was detected after N2 flowing for 2 h (~1 ppb, Figure S6), indicating that the NOx in ultra-high-purity N2 could be ignored. Gas chromatographic curve (Figure S7) and DRIFTS spectrum (Figure S8) both show no signal of NOx which corresponds well with the nitrite assay kit result, further demonstrating the high purity of feeding gas. Then, N2 gas was supplied in a continuous feed stream with a flow rate of 130 sccm to the cathode compartment. The gas tube was positioned near the electrode to ensure that the entire Pd/ACC catalyst was surrounded by a mass of N2 bubbles during the electrocatalytic process (Movie S1), expecting to adjust the gas-solid-liquid three-phase contact interface and increase the coverage of N2 on the catalyst surface.
In order to verify the feasibility of this strategy, linear sweep voltammetry (LSV) was conducted on Pd/ACC in N2-saturated and Ar-saturated HCl solution with bubbles covering the catalyst in the same cell. As shown in Figure S9(a), the reduction current density of N2 bubbles covering Pd/ACC is slightly smaller than that of Ar bubbles, implying that some nitrogen species may be adsorbed on the catalysts hindering the HER activity when Ar was changed to N2 [41]. In addition, once N2 flow (red curve in Figure S9(b)) was changed to Ar with the same cell assembly, the current density increased immediately, reconfirming that the decreased current density was due to the impeditive HER in the N2-catalyst-electrolyte three-phase interface. These phenomena were repeated and became more obvious with chronoamperometry. Catalysts surrounded by N2 bubbles might have two mechanisms in impeding H2 production: (1) reducing the proton donors with bubbles and (2) occupying more active sites of the catalyst with nitrogen. To gain further insight into the suppressed HER, Ar gas was injected into the cathode compartment and LSV was tested on Pd/ACC with or without Ar bubbles covering by adjusting the position of the gas tube. As shown in Figure S9(c), the LSV curves coincide well with each other, suggesting that the inert Ar bubbles have no discernible effect on H2 production in the three-phase interface, and therefore, one could conclude that nitrogen adsorbed on the active sites is the main reason for the inhibited HER under the adjusted three-phase interface, which corresponds well with the DFT results. Based on the above, we believe that the possible mechanism of this three-phase boundary control is that once the catalyst sites are exposed to the nitrogen gas (via bubbles), the hydrogen is replaced by it and NRR can take place at the interface where N2 bubbles, solid catalysts, and electrolytes contact meanwhile.
Subsequently, to further study the impact of this adjusted three-phase interface, chronoamperometry was tested on Pd/ACC and the electrochemical NRR performances were systematically investigated. Unless otherwise specified, all the potentials were converted and reported as values vs. RHE. As shown in Figure 3(b), Pd/ACC with N2 bubbles produces a smaller current density after continuous electrolysis at 0.1 V for 2 h than that with Ar bubbles, which demonstrates that the competing HER was suppressed during the NRR process obviously. These results correspond well with those obtained from the above LSVs. The primary NRR product NH3 was further quantified by the indophenol blue (Figure S10) and salicylic acid methods (Figure S11) simultaneously, while the yield of the by-product N2H4 was determined by the para-dimethylaminobenzaldehyde method (Figure S12). In our system, only NH3 was detected without the presence of N2H4 (Figure S13), implying good selectivity for N2 reduction to NH3 on the Pd/ACC catalyst. The average NH3 production rates and the corresponding FEs at various applied potentials are plotted in Figure 3(c) and Figure S14. The values obtained from the two methods were in good agreement (Figure S15). The average rate reached a maximum of 5.5×10−11 mol s-1 cm-2 at 0.1 V, which was normalized by the area of the working electrode. More importantly, a high FE of 97% for NH3 production was achieved, which may be attributed to the adjusted three-phase interface and the relative positive potential. The value was several times to one order of magnitude higher than that reported in aqueous solutions up to date (Table S1). The NRR performances were evaluated with the same kind of Pd/ACC catalyst in N2-saturated HCl at constant voltage for 2 h for three times, and the results are shown in Figure S16. To demonstrate the almost inhibited HER, the produced H2 was then detected by gas chromatography and no signals of H2 was detected (note that the HER process can occur at positive potentials; see Figure S17 and Supplemental Information: Calculation of equilibrium potential of HER). The metal nanoparticles were still homogenously dispersed on the ACC support after 2 h of continuous electrolysis (Figure S18). Recycling experiments also found that the chronoamperometry curves exhibited little change and the FE maintained around 90% during recycling for nine times, manifesting the repeatability and the stability of the adjusted three-phase interface (Figure S19 and Figure 3(d)). The Pd/ACC catalyst after NRR was further characterized. Compared with pristine Pd/ACC and a reference sample prepared by heating Pd/ACC in a tube furnace with a N2 flow, the catalyst after NRR showed diffraction peaks slightly shifted toward lower diffraction angles in the XRD pattern and enlarged lattice distances in the HRTEM image, suggesting that Pd hydride might form after the NRR test (Figures S20–S23). The solid-state NMR measurement further confirmed it (Figure S24), consistent with the above DFT results and the previous reports that H atoms can enter into the lattice of Pd to form stable PdH under operating potentials [42, 43].
A series of control experiments were then performed to demonstrate that the detected NH3 was truly generated from the electrochemical NRR (Figures S25 and S26). When Pd/ACC was evaluated in N2 at an open circuit, no signal of NH3 was detected, indicating the absence of NH3 impurity in the external environment and N2. Also, no NH3 was found after controlled electrolysis of Pd/ACC at 0.1 V in Ar for 2 h, which was consistent with the absence of N in the Pd/ACC XPS spectrum. In addition, no NH3 was produced on the pure ACC support. To further confirm the origin of NH3 production during the NRR test, an isotopic labeling experiment with 15N2 as the feed gas was conducted. As shown in Figure 3(e), the 1H nuclear magnetic resonance (1H NMR) spectrum of 15NH4+ shows a doublet coupling with a JN‐H of 73.2 Hz, while a triple coupling with a JN‐H of 52.2 Hz was found for 14NH4+. Only 14NH4+ was observed when 14N2 gas was fed into the cell. By contrast, the 15N2 sample showed distinguished peaks for 15NH4+, and no signal for 14NH4+ was observed in 1H NMR spectra, suggesting the negligible amount of background NH3 and coinciding with the control experiment under Ar electrolysis. These results all proved that the produced NH3 was entirely derived from the electrochemical reduction of N2.
To prove the validity and the importance of the adjusted three-phase interface, we investigated the influence of N2 coverage on the NRR performance by altering the N2 flow rate (50, 80, 100, and 130 sccm) and controlling the position of the gas tube. The results show that the current densities and total electric charges diminish with the increase in the N2 flow rate and achieve the lowest values at 130 sccm (Figure 4(a) and Figure S27), while the FE exhibits an opposite trend (Figure 4(b)). To explore the side reaction along with the NRR process at 50 sccm of N2, the produced H2 was detected by gas chromatography. As shown in Figure S17, the H2 signal is found, indicating that HER occurs at 50 sccm of N2. These phenomena all proved that the HER process was suppressed with the increase in bubbles accessible to the electrode under 130 sccm of N2. Moreover, if the gas tube was positioned near the Pd/ACC catalyst to ensure that N2 bubbles surrounded the electrode, the current densities increased quickly in the chronoamperometry curves (Figures 4(c)–4(e)). Also, FE and NH3 yield increased prominently (Figure 4(f)), manifesting that the NRR activity could be enhanced with the N2 bubbles covering. Based on the above results, the significantly improved NRR selectivity of the Pd/ACC catalyst can be attributed to the synergistic effect of inhibited HER and promoted NRR activity with the enhanced three-phase interface.
Furthermore, to demonstrate the feasibility of this strategy and explore the applicability of the adjusted three-phase interface on other catalysts, Ir-based and RuPd-based catalysts with strong H adsorption ability were prepared via an ultrasound-assisted reduction method and then characterized using XRD, XPS, and HRTEM techniques. The results are shown in Figures S29–S31, and their corresponding NRR properties were then examined. Maximum FEs of 93% and 99% for NH3 synthesis were achieved with the Ir/ACC and RuPd/ACC catalysts, respectively (Figures 4(g) and 4(h)). Additionally, it was found that more N2 coverage on Ir and RuPd surfaces could accelerate NH3 production and inhibit the HER process simultaneously (Figures S32–S34), therefore improving the NRR selectivity and activity synergistically. These findings were consistent with those for Pd/ACC, which could open up a new outlook to break through the selectivity limitations in electrochemical NRR, especially in aqueous solution. In addition, it was reasonable to expect an excellent NRR performance with the enhanced three-phase interface by engineering catalysts with more active sites. We found that the developed Pd clusters/ACC and IrPd/ACC catalysts with supersmall metal nanoparticle sizes (Figures S35–S38) could achieve improved ammonia yield rates of 106  μg h-1 mgmetal-1 and 93  μg h-1 mgmetal-1, respectively, while the high FEs remains (97% and 87%, Figures S39–S41). These all demonstrated the wide applicability of the enhanced three-phase interface.
In summary, we demonstrate a theory-guided design of the adjusted three-phase interface as an effective strategy for favoring NRR over HER and achieve high NH3 production selectivity with FE up to 97% in an aqueous acid solution under ambient condition. N2 does not have to be dissolved in electrolyte, and the increased N2 coverage on the catalyst surface weakens H adsorption, leading to a suppressed HER and improved selectivity toward NH3, as evidenced by the theoretical and experimental results. This strategy is also extended to Ir- and RuPd-based catalysts for selective reduction of N2 to NH3, even though they both possess strong H adsorption ability, thereby demonstrating its feasibility for electrochemical NRR especially in aqueous solutions. The NRR activity and selectivity can also be improved simultaneously by employing the three-phase interface and engineering catalysts with more active sites such as Pd clusters/ACC and IrPd/ACC. Thus, the results should provide a new perspective for enhancing the electrocatalytic performance of solid catalysts in a gas-involved and/or proton-sensitive competition system.
Sodium tetrachloropalladate (Cl4Na2Pd), ruthenium chloride hydrate (RuCl3·xH2O), chloroiridic acid hydrate (H2IrCl6·xH2O), sodium borohydride (NaBH4), hydrazine monohydrate (N2H4·H2O, >98% (T)), sodium nitroferricyanide dihydrate (C5FeN6Na2O·2H2O), sodium citrate (C6H5Na3O7), sodium salicylate (C7H5NaO3), sodium hypochlorite solution (NaClO, 5% Cl-), ammonium chloride (NH4Cl), and 15N enrichment of ammonium chloride (15NH4Cl, 99 atom% 15N) were purchased from Sigma-Aldrich. Hydrochloric acid (HCl, 35%-38%), sodium hydroxide (NaOH), and ethyl alcohol (C2H5OH) were purchased from Sinopharm Chemical Reagent Co. Ltd. Para-dimethylaminobenzaldehyde (C9H11NO) was purchased from Macklin Biochemical Co., Ltd. A nitrite assay kit was purchased from Nanjing Jiancheng Bioengineering Institute. Carbon cloth (HCCP330) was purchased from Shanghai Hesen Electric Co. Ltd. Nafion 211 membranes were purchased from Fuel Cell Store. Ultra-high-purity N2 gas (99.9999%) and ultra-high-purity Ar gas (99.999%) were purchased from Jingong Material Gas Co. Ltd. 15N2 gas (chemical purity: ≥98.5%) was purchased from Newradar Special Gas Co., Ltd. Ultrapure water with a resistivity of 18.2 MΩ cm was produced using a Millipore Milli-Q grade. All of the chemicals were used without any further purification.
ACC was synthesized according to the previous report [44]. Typically, a piece of CC was heated to 600°C with a heating rate of 10°C min-1 and kept at 600°C for 1 h under flowing industry N2 (99% purity) at 300 sccm to obtain ACC.
2.5 mL of 0.01 g mL-1 Cl4Na2Pd solution was dispersed in 20 mL of ultrapure water. A piece of ACC was immersed in the solution under ultrasound for 10 min. Next, 2.5 mL of 2 mg mL-1 NaBH4 solution was added in the as-prepared solution with an ultrasonic dispersion for 30 min. Finally, the as-obtained Pd/ACC catalyst was further washed and dried at 60°C in a vacuum oven. The content of Pd on the Pd/ACC catalyst was determined to be ~0.4 mg cm-2 according to the ICP-AES result.
The X-ray diffraction (XRD) data of the samples were obtained on D/tex-Ultima TV wide-angle X-ray diffractometer equipped with Cu Kα radiation (λ=0.15406 nm). High-resolution TEM (HRTEM) and high-angle annular dark-field scanning transmission electron microscopy (HADDF-STEM) analyses were performed on an FEI Tecnai G2 F20 S-TWIN microscope operating at an acceleration voltage of 300 kV. The X-ray photoelectron (XPS) data were accomplished with an ESCALAB MARK II spherical analyzer with an Al Kα (Al 1486.6 eV) X-ray source. The inductively coupled plasma-atomic emission spectrometry (ICP-AES) was carried out on PerkinElmer Optima OES 800. The content of Pd was obtained with inductively coupled plasma-atomic emission spectrometry (ICP-AES, PerkinElmer Optima OES 8000), which was dissolved by HNO3. The concentration of ammonia was measured on a UV-vis spectrophotometer (TU-1901). The specific surface area and pore size distribution were calculated based on the N2 adsorption analysis performed at 77 K on Micromeritics ASAP 2020. 600 M 1H nuclear magnetic resonance (NMR) was detected on Agilent DD2-600. Diffuse reflectance infrared Fourier transform spectroscopy (DRIFTS) was collected with Nicolet 6700 FTIR fitted with an MCT detector with a resolution of 4 cm-1 and 32 scans. Gas chromatography was performed on Fuli 9790 equipped with tandem connect of PorparkQ and a thermal conductivity detector with Ar as the carrier gas (injector, oven, and detector temperatures were set at 150°C, 120°C, and 200°C, respectively).
The electrochemical experiments were carried out in a three-electrode configuration at an electrochemical station (CHI660E). Typically, the catalysts were freestanding, which were directly used as the working electrode without the addition of any additives. The area of the working electrode was controlled to be 0.8 cm2. Pt foil and Ag/AgCl electrode (saturated KCl electrolyte) were used as the counter electrode and reference electrode, respectively. In this work, all potentials were converted to reversible hydrogen electrode (RHE) scaling by E vs. RHE=E vs. Ag/AgCl+0.1989 V+0.0591×pH.
For electrochemical NRR measurements, the tests were conducted in a two-compartment cell with 40 mL electrolyte in each cell which was separated with a Nafion 211 membrane and connected with a gas absorption cell. Before experiments, the Nafion 211 membrane was pretreated with H2O2 (5%) aqueous solution and ultrapure water each for 1 h. Ultra-high-purity N2 (99.9999% purity) was used as the feeding gas to reduce a false positive from potential contaminant from the input gas stream. In addition, before NRR tests, the potential NOx in ultra-high-purity N2 gas (99.9999% purity) was first detected with a nitrite assay kit by using colorimetric tests, gas chromatography, and DRIFTS (see Determination of NOx Contamination in Ultra-High-Purity N2 Gas). These results all show that almost no NOx in the feeding gas was detected. Then, the ultra-high-purity N2 was continuously purged into the cathodic compartment for at least 1 h before NRR tests. Then, potentiostatic tests were performed in N2-saturated 0.1 M HCl solution for 2 h at room temperature under atmosphere pressure for evaluating the average ammonia yield rate. The gas tube was positioned to ensure that the entire cathode was surrounded by gas bubbles during the whole process. In order to absorb the gas and electrolyte out with the large flow rate of N2, 0.1 M HCl was also used as an absorber in a gas absorption cell. To reduce the contaminations from the environment, the whole cell was sealed and soaked in 0.1 M HCl solution when not in use and it was thoroughly rinsed with deionized water and 0.1 M HCl electrolyte each for more than three times. Before LSV tests, Ar flowed into the cell for 1 h. Then, polarization curves in Ar were tested with a scan rate of 5 mV s-1, and this step was repeated to obtain a steady curve. Next, the gas was changed to ultra-high-purity N2 and it flowed in the cell to 1 h to guarantee a N2 atmosphere. For comparison, the LSV curves in N2 were obtained at 5 mV s-1 with the same cell assembly. Then, N2 gas was changed to Ar again and Ar was inputted in the cell for 1 h before collecting the LSV curves in N2 at 5 mV s-1. All the polarization curves shown were the steady ones. The chronoamperometry test of Ar was conducted on a Pd/ACC sample from the same batch of catalyst in 0.1 M Ar-saturated HCl at 0.1 V for 2 h with 130 sccm of Ar flow rate before the NRR test. Repeated tests were run on Pd/ACC with the same electrode or from different batches in 0.1 M HCl solution at constant voltage for 2 h with 130 sccm of N2 flow rate. Recycling experiments were repeated for nine times, and each was evaluated by NRR tests on the same Pd/ACC electrode in 0.1 M HCl solution at 0.1 V for 2 h with 130 sccm of N2 flow rate.
The potential NOx in ultra-high-purity N2 gas should be noticed to avoid a false positive. The nitrite assay kit, gas chromatography, and DRIFTS were used to detect the potential NOx in the ultra-high-purity N2. Similar to the NRR test, N2 was purged into the electrolytic cell for 2 h, and then, the solution was detected with the nitrite assay kit according to the previous report [45]. Ultrapure water and 20  μmol/L NaNO2 sample added with nitrite assay kits were also prepared as the blank sample and standard sample, respectively. After color development for 15 min at room temperature, these samples were measured at a wavelength of 546 nm on a UV-vis spectrophotometer. As shown in Figure S6, the UV-vis spectrum of the test solution is consistent with that of the blank solution. The concentration of nitrite in the test solution was low to 1 ppb, and thus, the NOx in the ultra-high-purity N2 could be ignored. Also, the feeding gas was further detected by gas chromatography and DRIFTS. Ar was used as the carrier gas, and the flow rate was 30 sccm for gas chromatographic analysis. As shown in Figure S7, only the peak of N2 is found and no other peak is detected, indicating a negligible NOx in the N2 feeding gas. For DRIFTS, Ar was used as the background and the final spectrum of N2 was obtained by subtracting that from the Ar background (Figure S8). Similarly, no vibrations of NO, NO2, and other NOx were observed. The results all demonstrated the negligible NOx in the feeding N2.
Concentration of ammonia was determined by the indophenol blue method. In detail, 3 mL of solution after NRR tests was first removed to a colorimetric tube. Then, 3 mL of 1 M NaOH solution containing 5 wt% sodium citrate and 5.79 wt% sodium salicylate was added, followed by the addition of 1.5 mL of 0.05 M NaClO and 0.3 mL of 1 wt% sodium nitroferricyanide dehydrate. After color development for 2 h at room temperature, the adsorption spectrum was obtained on a UV-vis spectrophotometer. The absorbance at a wavelength of 655 nm was used for qualitative determination of indophenol blue. The blank control was prepared by replacing 3 mL of sample with 3 mL of 0.1 M HCl solution without ammonia. The concentration-absorbance curve was calibrated using standard ammonia chloride solutions with a series of concentrations. To reduce other influence factors, the background was corrected by subtracting the value of the blank control from all readings of samples.
Concentration of ammonia was also confirmed with the salicylic acid method [8]. 4 mL of solution after NRR tests was first removed to an empty bottle. Then, 4 mL of ultrapure water was added, followed by the addition of 50 μL of oxidizing solution containing 0.75 M NaOH and NaClO (ρCl=4‐4.9) and 500  μL of coloring solution containing 0.4 M sodium salicylate and 0.32 M NaOH. Finally, 50  μL of catalyst solution containing 1 wt% sodium nitroferricyanide dehydrate was added. After color development for 1.5 h at room temperature, the adsorption measurement was conducted at a wavelength of 670 nm on a UV-vis spectrophotometer. The blank control was prepared by replacing 4 mL of sample with 4 mL of 0.1 M HCl solution without ammonia. The concentration-absorbance curve was calibrated using standard ammonia chloride solutions with a series of concentrations. To reduce other influence factors, the background was corrected by subtracting the value of the blank control from all readings of samples.
The hydrazine present was estimated by the method of Watt and Chrisp [46]. A mixture of para-dimethylaminobenzaldehyde (5.99 g) and HCl (concentrated, 30 mL) and ethanol (300 mL) was used as a color reagent. First, 2 mL of solution after NRR tests was mixed with 2 mL water. Then, 1 mL of 1 M KOH solution and 5 mL of color reagent were added, followed by sitting for 10 min at room temperature for color development. The absorbance of the resulting solution was measured at 456 nm. The blank control was prepared by replacing 2 mL of sample with 2 mL of 0.1 M HCl solution without hydrazine. The concentration-absorbance curve was calibrated using standard hydrazine hydrate solutions with a series of concentrations. To reduce other influence factors, the background was corrected by subtracting the value of the blank control from all readings of samples. The calibration curve was plotted with 2 mL of hydrazine hydrate-water solution of certain concentration, 2 mL of 0.1 M HCl solution, 1 mL of 1 M KOH solution, and 5 mL of color reagent.
15N2 was used as the feeding gas for the isotopic labeling experiment to confirm the source of ammonia. 15N2 (≥98.5% chemical purity) was purchased from Newradar Special Gas Co., Ltd. Before the NRR test, 15N2 was fed into the electrolytic cell with a flow rate of 10 sccm for 30 min. Pd/ACC was tested at 0.1 V vs. RHE for 4 h in the airtight device. This procedure was repeated for 2 times. The obtained acid electrolyte solution was concentrated, added with D2O, and then identified by 600 M 1H NMR (Agilent, DD2-600).
DFT calculations were carried out using the Vienna Ab initio Simulation Package (VASP) [47] according to the projector augmented wave (PAW) method [48]. A cutoff energy of 400 eV for plane waves was set through all the calculations, and exchange-correlation functional approximation was treated in Perdew-Burke-Ernzerhof (PBE) functional [49]. The (211) slabs were built with 4 atomic layers in a p1×3 supercell with the bottom two layers fixed during structural relaxation. A p3×3 supercell containing 4 atomic layers for (111) and (100) slabs was modeled with the bottom two layers fixed during structural relaxation. The periodic condition was employed along the x and y directions, and the vacuum space along the z direction was set to be 15 Å in all slab calculations. The Monkhorst-Pack scheme was used for sampling the Brillouin zone, and the k-point grid of 3×3×1 is selected. During structural optimizations, the residual force between atoms was converged to a value below 0.02 eV/Å.
The average adsorption energies for N2 chemisorption with given N2 coverage are defined as
(1)EadsN2=Etot1−Eslab−EN2nN2,
where nN2 is the number of N2 adsorbed on the catalyst, Etot1 is the total energy after nN2 of N2 is adsorbed on the catalyst, Eslab is the energy of the clean catalyst alone, and EN2 is the energy of the molecule N2 in the gas phase.
The adsorption energies for H atom chemisorption are defined as
(2)EadsH=Etot2−Etot1−EH,
where Etot2 is the total energy after an H atom is adsorbed on the catalyst with given N2 coverage and EH is the half of the energy of the molecule H2 in the gas phase.
  • Fundamental Research Funds for the Central Universities(2017XZZX002-16)
  • Natural Science Foundation of Zhejiang Province(LZ18B060002)
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Year 2019 volume 2019 Issue 11
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doi: 10.34133/2019/1401209
  • Receive Date:2019-10-06
  • Online Date:2026-10-27
  • Published:2019-11-20
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  • Received:2019-10-06
  • Accepted:2019-11-13
Funding
Fundamental Research Funds for the Central Universities(2017XZZX002-16)
Natural Science Foundation of Zhejiang Province(LZ18B060002)
Affiliations
    Advanced Materials and Catalysis Group, Institute of Catalysis, Department of Chemistry, Zhejiang University, Hangzhou 310028, China
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表12种不同金属材料的力学参数
科
Family
属数
Number of
genus
种数
Number of
species
占总种数比例
Percentage of
total species (%)
属
Genus
种数
Number of
species
占总种数比例
Percentage of total
species (%)
鹅膏菌科Amanitaceae 2 11 5.26 鹅膏菌属 Amanita 10 4.78
小菇科 Mycenaceae 2 12 5.74 丝盖伞属 Inocybe 5 2.39
多孔菌科 Polyporaceae 8 14 6.70 蜡蘑属 Laccaria 5 2.39
红菇科 Russulaceae 3 23 11.00 小皮伞属 Marasmius 6 2.87
小菇属 Mycena 11 5.26
光柄菇属 Pluteus 5 2.39
红菇属 Russula 17 8.13
栓菌属 Trametes 5 2.39
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