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SN Applied Sciences

, 1:206 | Cite as

Synthesis of highly electrically conductive and electrochemically stable porous boron-doped carbon microspheres

  • Anima B. BoseEmail author
  • Junbing YangEmail author
  • Wei Li
Research Article
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Part of the following topical collections:
  1. 4. Materials (general)

Abstract

Corrosion resistant carbon with enriched electrical conductivity is advantages for long lasting electrochemical device development. In this study, boron-doped carbon microspheres (BCMS) were prepared by a chemical vapor deposition process from p-xylene and boron trichloride, followed by a mild oxidation step to alter their surface properties and pore structure. XPS study confirmed the formation of the BCMS with a B:C nominal ratio of 1:10.9. Morphological study illustrated the formation of smooth BCMS microspheres with uniform distribution with an average diameter 0.5–1.0 μm. N2 sorption measurements revealed that as synthesized BCMS has a pore structure of less than 2 nm with a maximum distribution around 0.4 nm and a surface area of 213 m2 g−1. Compared to the traditionally used Vulcan XC-72 in polymer electrolyte membrane fuel cells and reversible fuel cells, the BCMS material has similar pore structure and surface area but exhibits higher electrochemical stability. BCMS also exhibits excellent low electrical resistivity (37.2 Ω sq−1) and thermal stability (up to 400 °C) as carbon nanotubes. These superior properties suggest that the BCMS is a very promising candidate as supports for electrocatalysts in electrochemical devices, such as polymer electrolyte membrane fuel cells, reversible fuel cells, lithium-air batteries, etc.

Keywords

Nano-porous microsphere Boron-doped carbon Chemical-vapor-deposition Electrically conductive Thermal stability 

1 Introduction

During the past two decades, tremendous efforts have been made in developing various geometric shaped carbon-based micro/nanostructured materials for a wide range of applications including energy devices. Among different shapes of carbon materials, spheres, tubes, fibers/wires, flasks, etc., spherical particles pose utmost benefits over others in uniform packaging [1, 2, 3, 4]. Carbon spheres are thus receiving enormous attention in electrochemical energy conversion and energy storage device development. Electrocatalysts are deemed as the heart of many electrochemical systems, and electrocatalyst supports play a vital role in achieving high performing device development such as various type of fuel cells, lithium–air batteries, anode materials in lithium-ion batteries, sulphur host in lithium–sulphur batteries, electrode materials in supercapacitors, and many others applications [5, 6, 7, 8, 9, 10, 11, 12]. In fact, carbon based materials remain the most effective electrocatalyst in highly demanding chemical and electrochemical environments. For example, in polymer electrolyte membrane fuel cells (PEMFC), carbon support highly influence on enduring nano-structured catalyst for redox reductions without getting corroded of the sluggish electrode-kinetics.

It is generally expected that electrode materials and electrocatalyst supports must propound essential properties as high electrical conductivity, high electrochemical stability, competent to generate appropriate pore structure from a standpoint of effectiveness. In addition to the high electrical conductivity, foreseeable electrode materials are required to minimize internal electrical resistance, reduce ohmic over potential and thus improve the performance of the electrochemical devices. In general, electrochemically stable catalyst support has a great deal of influences on the durability of the electrochemical devices. For instance, carbon oxidation causes effective surface area loss in PEMFCs, one of the major factors resulting in the degradation of the cathodes leading to unfortunate aggregation of nano-catalysts and the structural failures of electrodes [13, 14, 15]. It is well established that carbon material used in the electrodes at a high electrode potential, such as the cathodes of PEMFCs, reversible fuel cells, lithium-air batteries, is subject to severe deterioration and needs electrochemically stable noble conducting materials for electrochemical device development [10, 13, 14, 15, 16]. Undoubtedly, the pore size and surface area play key roles when carbon is used as electrocatalyst supports in an electrochemical device with solid electrolyte, such as PEMFCs, where the pores of the carbon spheres should not be larger than the catalyst nanoparticle with typical size about 3–5 nm to avoid nanoparticles entering the pores, which significantly reduces the catalyst utilization efficiency lacking from three-phase boundary for protons conduction [16, 17]. Whereas in the cathodes of lithium–air batteries, the carbon spheres should have large pores to accommodate the catalyst nanoparticles and the solid Li2O2 product from the charging process [18]. Above few examples validate that pore structure and surface area of supporting materials does vary depending on device while other collective properties persist.

Globally, significant efforts have been devoted to evolving boron/nitrogen doping into carbon materials, which have been known to change the physical and chemical properties of carbon. Intensive attention in recent years has been given to improve such properties, i.e., electrical conductivity, corrosion resistance by doping boron/nitrogen into carbon materials to meet the state-of-the-art requirements of their applications [19, 20, 21, 22, 23, 24, 25]. In principle, carbon materials hold good electrical conductivity owing to the delocalized π-electron throughout the covalently bonded carbon network created by sp2 hybridized orbitals. Boron is an ideal doping agent due to its electronic compatibility and configuration of sp2 hybridized orbitals, thus forming a covalent bonding network with neighboring carbons. Besides, the presence of a vacant pπ orbital to effectively engage in π-electron delocalization that primarily contributes to the electrical conductivity. Studies also show that boron is a unique and efficient dopant for improving the oxidation resistance of graphite, carbon fibers, carbon/carbon composites, carbon nanotubes and various other carbon materials [26, 27]. However, it needs to be noted that the improvements of the properties usually depend on the percentage of B-dopant. For instance, Mondal et al. [16] demonstrated two order conductivity drop in boron-doped carbon microsphere compared to the un- doped microspheres.

Carbon spheres with customized properties are advantageous over many geometric structures, and have been prepared in many routes, such as templating [9, 10], pyrolysis [11, 28], reduction [29], and chemical vapor deposition (CVD) [30]. Compared with the many studies on boron-doped carbon nano-tubes, boron doping of spherically shaped carbon materials have not yet provoked much study. In this report, we present a synthesis protocol for preparing boron-doped carbon microspheres through a CVD process that allows controlled tuning of the size and doping amount. A two-step process involved in material synthesis is presented here: (1) grow nanoporous boron-doped carbon microspheres and (2) open the porous structure via mild oxidation. The obtained properties, such as pore structure, electrical conductivity, thermal stability and electrochemical oxidation of BCMS were compared with other carbon based materials such as carbon nanotubes, and traditional catalyst support material, Vulcan XC-72 for PEMFCs and reversible fuel cells (RFCs). The results discussed in this report evidently advocate that the BCMS is a highly promising candidate as catalyst supports for electrocatalysts development of PEMFCs, RFCs, lithium-air batteries and other electrochemical devices.

2 Experimental

2.1 Synthesis and activation

BCMS were prepared using a CVD process inside a quartz tube inserted through a low-temperature heating section (Zone I, 200 °C) and a high-temperature heating section (Zones II, 950 °C). 0.34 g ferrocene (Sigma-Aldrich) was dissolved in 23.6 g boron trichloride solution in p-xylene (1.0 M, Sigma-Aldrich) and used as the precursor for BCMS synthesis. It was injected at rate of 2 mL/min and vaporized in the quartz tube at Zone I. The vapor was transported to Zone II by a mixture of H2 and Ar gases at flow rates of 60 and 90 mL min−1, respectively. The BCMS was grown on a polished quartz plate inside the quartz tube at Zone II. After 30 min, the solution injection was stopped, and the furnaces were turned off and naturally cooled down to room temperature maintaining the flow of H2 and Ar gases at the same flow rate as was during synthesis.

In the second step of synthesis; as-synthesized BCMS was activated by a mild oxidation in water steam to open the pore structure. For this phase of synthesis, Zone I and Zone II were kept at 500 and 850 °C, respectively. Deionized water was injected at the rate of 0.225 mL min−1 into and evaporated inside the quartz tube in the middle of Zone I. The steam was carried by flowing Ar gas at 140 mL min−1 to Zone II to react with the BCMS synthesized in the step 1. The injection of water continued for 30 min before cooling the furnaces to room temperature under inert environment before collect the product.

2.2 BCMS characterization

The boron to carbon ratio (B:C) of the activated BCMS sample was evaluated using X-ray photo-electron Spectroscopy (XPS, Kratos AXIS-165) equipped with a monochromatic Al Kα X-ray source. The morphology and microstructure of the activated BCMS sample were examined on a scanning electron microscope (SEM, Hitachi S-4700) operated at 10 kV. Energy-dispersive X-ray spectroscopy (EDS/EDX) was performed at 10 kV to determine the bulk composition of the activated BCMS microspheres. Thermogravimetric analysis (TGA) experiments were performed on Shimadzu, TGA-50 with a 10–12 mg sample in air at a heating rate of 10 °C min−1. Surface area and pore-size distribution of the activated BCMS sample were characterized with N2 sorption measurements on an automated Micromeritics ASAP 2010 sorption analyzer at 77 K and determined by means of Brunauer–Emmett–Teller (BET) method and Horvath–Kawazoe (HK) model, respectively. Prior to surface area and pore-size analysis, the sample was degassed (vacuum-degassed) at 120 °C for 4 h. The BET equation was used to calculate the surface area [31]. Four-point-probe method was adopted to measure the sheet resistance of the activated BCMS on the original quartz substrate. BCMS resistance data was then compared with the carbon nanotubes (CNT, hollow structure multi-wall carbon nanotubes, 30 nm in diameter, 1–5 μm in length, PD30L1-5, NanoLab) in a compressed state.

2.3 Electrochemical evaluation

The electrochemical performances of the activated BCMS were evaluated through cyclic voltammetry (CV) experiments conducted with a potentiostat (CHI 1140A) in a three-electrode configuration: a Pt wire as the counter electrode, a glassy carbon rotating disk electrode (RDE, 5 mm diameter, Pine instrument) as the working electrode, and Ag/AgCl (sat. KCl) as the reference electrode. An Ar saturated 0.10 M HClO4 was used as electrolyte in this study. Carbon inks (2.0 mg mL−1) made of BCMS, CNT and Vulcan XC-72 were prepared separately by well dispersing the carbon into a 1:5 deionized water/isopropanol mixture. The sample loading on a freshly polished mirror-like RDE tip was 20.0 μg and was cycled between 0–1.2 V versus Ag/AgCl at a scan rate of 50 mV s−1.

3 Results and discussion

BCMS in this study were prepared from a reactant mixture of a boron source (boron trichloride), carbon sources (p-xylene, xylene), and a catalyst (ferrocene) on a quartz slide by a CVD process. The present study distinctly focused on understanding the causes behind the formation of conductive porous BCMS microspheres, as well as how the boron doping affect the electrical conductivity and its oxidation resistance of the BCMS.

The molecular structure of the precursor(s) and the synthesis environment enfolds a crucial effect on carbon network. The synthesis of highly pure conductive BCMS was carried out via a two-step process: (1) in the first step pyrolysis of xylene was done in the vapor-phase; and followed by (2) the steam activation for tailoring the BCMS in high purity texture. Fundamentally, hydrocarbon vapor separate hydrogen by dissolving carbon in hot metal iron of ferrocene at a relatively high temperature of 950 °C and precipitated out as a sphere, BCMS. Ferrocene participated in this synthesis as a catalyst, at this operating temperature also as a second source of hydrocarbon and provided the stronger adhesion to the growing carbon network. At this highly reducing atmosphere, cyclic hydrocarbon first separate out and intend to curve to bridge inside to form carbon sphere [32]. It can be theorized that at above 700 °C xylene might separate when Fe2+ catalyst reduced by aliphatic ligand of xylene, and in order to minimize the interfacial energy, the clusters rearrange themselves in simultaneous delocalization of π electrons of carbon. Though, morphology of BCMS is greatly impacted by the aromatic structure of carbon sources xylene and ferrocene, but iron to carbon ratio in the range 0.016–0.033 range contribute to spheres formation and pore-size structure [33]. The remaining iron of first step synthesized BCMS was removed through partial oxidation occurred during second step of synthesis. The steam activation at 850 °C is assisted to remove portion of the impurities including amorphous carbon and residual Iron of ferrocene, which helps to create porous structure inside the carbon microspheres [33].

It is well understood, incorporating boron into carbon changes the physicochemical properties of carbon materials such as the surface energy, conductivity and ferromagnetic properties. The carbon oxidation can be minimized by incorporating boron in carbon lattice and substitution in the graphitic lattice effectively happens when boron content below one atomic percent [3, 14, 16, 34, 35]. XPS attained atomic ratio of boron to carbon (B:C) of the activated BCMS is 1:10.9. The analysis displays that product consists of 7.5% B, 81.5% C and 11.0% O as listed in Table 1; indicates the effective boron doping occurred in the process. Figure 1 presents the XPS characterized peaks position of BCMS composition; B 1s, C 1s, and O 1s are at 191, 284 and 532 eV, respectively. Figure 1 shows the B1s peak at 191 eV which should have been at 188 eV for pure boron; evident the boron bondage to carbon network, i.e., boron partially substitutes carbon into the sp2 carbon plane. The oxygen presence in the BCMS analysis is mainly from the surface oxidation of carbon during the steam activation process, in which some carbon was oxidized into active functional groups containing oxygen in the process [36]. The bulk composition of the activated BCMS showed a Boron to Carbon atomic ratio between 1:7.3 and 1:10.2, matching relatively well with the ratio from XPS (B/C nominal atomic ratio = 1:10.9). The Boron to carbon ratio obtained through EDX analysis are included in the supporting information (Figure S1 and Table S1).
Table 1

Quantification analysis of the XPS spectrum of the activated BCMS with a nominal B/C atomic ratio of 1:10.9

Peak

Position (eV)

FWHM (eV)

Raw area (CPS)

RSF

Atomic ratio (%)

B 1s

191.0

4.2

8630.1

0.16

7.5

C 1s

284.0

3.2

165,112.6

0.28

81.5

O 1s

532.0

3.5

62,512.7

0.78

11.0

Fig. 1

XPS spectrum of the activated BCMS with a B/C nominal atomic ratio of 1:10.9

Carbon materials generally possess good electrical conductivity and various studies have proven that electron deficient or acceptor boron dopant in carbon network can further enhance the electronic conductivity of carbon when B/C ratio below 0.5 [35, 37, 38]. According to analyzed data of BCMS microspheres, the B/C value of BCMS is 0.092, distinctly even far lower than 0.5 reported range. The four-point-probe sheet resistance of the activated BCMS microspheres measured of 37.2 Ω sq−1 agrees with the boron carbon ratio on electrical conductivity stated above, which is lower than the CNT (57.6 Ω sq−1) though the packing states of both samples were slightly different. The four-point-probe testing was done at room temperature for both samples. The enhanced electrical conductivity results from boron bonding through sp2 network of carbon that expected to increase the density of free charge carriers, thus increases the electrical and thermal conductivity. The obtained BCMS microspheres hypothetically could be an excellent candidate for electrically conductive material and would be very appropriate supports for electrocatalysts in electrochemical devices.

SEM images of the activated BCMS sample in Fig. 2 exhibit uniform distribution of smooth spheres without any tiny fragments attached. As mentioned above the steam activation at 850 °C is assisted to remove impurities including amorphous carbon and residual Iron of ferrocene. The estimated diameter of pure BCMS are in the range of 0.5–1.0 μm, which is larger than carbon nanospheres (100–150 nm) prepared from sucrose through a non-catalytic hydrothermal route [39], but smaller than other carbon microspheres (1–7 μm) [40, 41, 42]. The uniform shape and size, and clean and smooth surface certainly would benefit in uniformly packing the sample particles for preparing electrodes with a uniform pore structure in fabricating electrode for electrochemical device design [1].
Fig. 2

a Low magnification and b high magnification SEM images of the activated BCMS with a B/C nominal atomic ratio of 1:10.9

Surface area and porosity are critical parameters of carbon materials especially as supports for catalysts of electrochemical devices. The increase of surface area can be achieved through a special treatment, i.e., in this study partial oxidation was employed to increase the porosity and surface area of the BCMS microspheres. The activated microspheres is presumed to have an opened-and-enlarged porous structure, which was achieved by evaporating steam at a relatively low temperature gradient without disturbing the sample matrix that prepared in first step of synthesis. Figure 3 shows the N2 adsorption–desorption isotherm and pore-size distribution of the activated BCMS microspheres with a B/C atomic ratio of 1:10.9. The isotherm in Fig. 3a can be analogous to IUPAC (International Union of Pure and Applied Chemistry) type I physisorption isotherm with type H4 hysteresis loop, which is indicative of the existence of narrow slit-like microspores and the connectivity of inside pores [43]. The pore-size distribution in Fig. 3b derived from HK method shows that most of pores are in the range of < 2 nm in size with a maximum distribution around 0.4 nm, verifying that the activated BCMS is microporous. The BET surface area (SBET) of the microspheres obtained from the isotherm experiment is 213 m2 g−1, which is very close to that of a commonly used carbon black (Vulcan XC-72, 250 m2 g−1) [44] and within the range of multi-wall carbon nanotubes (MWCNT, between 60 and 250 m2 g−1) reported in the literature [45]. Considering the similar pore size and surface area to Vulcan XC-72, the activated BCMS is an appropriate candidate for supporting nano-sized electrocatalysts for a wide range of applications including electrochemical device development.
Fig. 3

a Nitrogen adsorption–desorption isotherm and b Horvath–Kawazoe differential pore volume plot of the activated BCMS with a B/C nominal atomic ratio of 1:10.9

Carbon materials are susceptible to microstructural and morphological degradation under oxidizing conditions in the electrodes with a high electrode potential [14, 15, 17]. In addition to the mechanistic explanation given above, the oxidation stability and corrosion resistance were tested further by using TGA and cyclic voltammetry experiments, respectively. The activated BCMS microspheres exhibit a very comparable oxidation stability or thermal stability to CNT via TGA as shown in Fig. 4. With the evidences in the literature that CNT has better thermal stability than Vulcan XC-72, it is reasonable to conclude that the BCMS is qualified in thermal stability as support for electrocatalysts in fuel cells and other electrochemical devices.
Fig. 4

Comparison of thermal stability by TGA measurements of the activated BCMS with a B/C nominal atomic ratio of 1:10.9 and the commercial CNT

The corrosion resistances of different carbon materials are usually studied by electrochemical characterization [14, 17]. Furthermore, BCMS microsphere has been tested and compared at the onset potentials and currents of the oxidation wave of the cyclic voltammograms in 0.10 M Ar saturated HClO4. Higher onset potential and lower oxidation current signify a better corrosion resistance of activated BCMS shown in Fig. 5 compared to XC-72 carbon and CNT. The voltammogram in Fig. 5 reveals an oxidation peak at ca. 0.4 V of XC-72 carbon and oxidation starting ca. 0.7 V. The oxidation peak and curve are, respectively, attributed to the oxidation of surface oxides on XC-72 carbon and the oxidation of carbon itself, i.e., carbon corrosion [34]. A similar voltammogram is observed for the CNT (Fig. 5) indicates a similar oxidation peak but a different oxidation curve with a higher onset potential (ca. 1.0 V) but smaller current. Voltammogram does not show oxidation peak at ca. 0.4 V for BCMS, which suggests no detectable surface oxides for BCMS. The current in that particular region is actually capacitive current of the electrode. The electrochemical study suggests that the both BCMS and CNT assimilate comparable corrosion behavior and possess better electrochemical stability than XC-72 carbon in acidic media. It has been recognized and possible reasoning given by various researchers that boron doping of carbon improves the crystallinity [16, 17, 34]. Thus boron doped carbon frame decreases the total number of accessible carbon site for oxygen and expected to form a barrier layer, B2O3 during oxidation above 450 °C [43, 46]. Based on obtained result of pure BCMS microsphere prepared at 950 °C followed by partial oxidation process, the rational explanation for oxidation and thermal stability would be the following. The existence of boron increases the activation energy for the C–O2 reaction; restrict CO chemical decomposition via electron transfer between carbon and substitutional boron; in fact acts as a catalyst [26, 47].
Fig. 5

Cyclic voltammograms of a XC-72 carbon black, b CNT, and c activated BCMS (B/C nominal atomic ratio = 1:10.9) in 0.1 M HClO4 saturated with Ar gas. The potential scanning rate is 50 mV s−1

4 Conclusions

Corrosion resistant carbon with enriched electrical conductivity is advantages for long lasting electrochemical device development. In this study, boron-doped carbon microspheres (BCMS) were prepared by a chemical vapor deposition (CVD) process from p-xylene and boron trichloride, followed by a mild oxidation step to alter their surface properties and pore structure. XPS confirmed the formation of the BCMS with a B:C nominal ratio of 1:10.9. Morphological study illustrated the formation of smooth BCMS microspheres with uniform distribution with an average diameter 0.5–1.0 μm. N2 sorption measurements revealed that as synthesized BCMS has a pore structure of less than 2 nm with a maximum distribution around 0.4 nm and a surface area of 213 m2 g−1. Compared to the traditionally used Vulcan XC-72 in polymer electrolyte membrane fuel cells (PEMFC) and reversible fuel cells, the BCMS material has similar pore structure and surface area but exhibits higher electrochemical stability. BCMS also exhibits excellent low electrical resistivity (37.2 Ω sq−1) and thermal stability (up to 400 °C) as carbon nanotubes. These superior properties suggest that the BCMS is a very promising candidate as supports for electrocatalysts in electrochemical devices, such as polymer electrolyte membrane fuel cells, reversible fuel cells, lithium-air batteries, etc.

Notes

Acknowledgements

The authors are grateful to the U.S. Department of Transportation (IL 26-7006), University of Houston, and Texas Center for Superconductivity at the University of Houston for the support of this work. We appreciate the collaboration of Chemical Sciences and Engineering Division of Argonne National Laboratory and their facilities for part of the data generation. We also thank Dr. Xinwei Cai and Dr. Rajesh Sahadevan for their technical assistance in manuscript preparation.

Compliance with ethical standards

Conflict of interest

The authors declare no conflict of interest.

Supplementary material

42452_2019_217_MOESM1_ESM.docx (27 kb)
Supplementary material 1 (DOCX 27 kb)

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Copyright information

© Springer Nature Switzerland AG 2019

Authors and Affiliations

  1. 1.Department of Engineering TechnologyThe University of HoustonHoustonUSA
  2. 2.Texas Center for SuperconductivityThe University of HoustonHoustonUSA
  3. 3.California Lithium BatteryLos AngelesUSA

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