CA2848104A1 - N-doped carbon materials - Google Patents
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Abstract
Description
CROSS-REFERENCE TO RELATED APPLICATIONS
[0001] This application claims the benefit under 35 USC 119(e) of United States provisional application serial no. 61/531,731 filed September 7, 2011 the entire disclosure of which is herein incorporated by reference.
TECHNICAL FIELD
BACKGROUND
materials such as Fe304, which yields synergistic CO2 capture and heavy metal absorption performance.
Unfortunately nitrogen - rich carbonized materials are expensive to manufacture, normally requiring intense chemical treatments, such as acid boiling or exposure to high temperature ammonia vapors, in order to make their surfaces rich in nitrogen atoms.
Moreover since these atoms are only at the outermost surface layer, the nitrogen-induced functionality wears out with prolonged use. Ideally the high (near 10% by weight) content would be in the bulk of the carbonaceous material, rather than at the surface. This would require high nitrogen content in the feedstock. A major economic advantage of such feedstock is that it would not require additional chemical treatments but would rely simply on pyrolysis and activation.
Many such materials come from esoteric sources such as certain forms of seaweed.
SUMMARY
The porous template may be mesoporous. The method may comprise removing the porous template after pyrolizing. The method may comprise functionalizing the activated carbon.
The activated carbon may contain nitrogen.
BRIEF DESCRIPTION OF THE FIGURES
image of activated CESM; (D) Illustration of the carbon-carbon core-shell structure of activated CESM.
H2SO4 (F). A
and B: at -0.4 (A) and 0.4 (B) along the X-axis, the curves from top to bottom are: CESM-300, AC-KOH, CESM-AP, CESM-AP, AC-KOH, and CESM-300. C: upper graph - curve with leftmost peak is AC-KOH, next is CESM-300, lower graph ¨ curve with leftmost peak is AC-KOH, next is CESM-300. D: curves from top to bottom are CESM-300 (1M
KOH), CESM-300 (1M H2SO4), AC-KOH (1M KOH), AC-KOH (1M H2SO4). E: both graphs ¨
top curve is CESM-300 (in 1M KOH), bottom curve is CESM-300 (in 1M H2SO4). F:
both graphs ¨ left curve is CESM-300, right curve is AC-KOH.
half-cell configuration. (A) Cyclic voltammograms of MPEw-650, tested at 0.1 mV/s; (B) charge/discharge curves of MPEw-650, tested at 0.1 A g-1; (C) charge/discharge capacity versus cycle number for the three carbons. A: lower curve is 1st, upper curve is 2nd and 3rd overlying each other, B: charge graph ¨ curves from top to bottom are 100th, 101h, 2nd, 1st, discharge graph ¨ curves from top to bottom are 1st, 2nd, IU ¨th, 100th, C: between 0-20 and 90-100 on the x-axis - curves from top to bottom are MPE-650, MPE-750, MPE-850, between 20-70 on the x-axis ¨ curves from top to bottom are MPE-650, MPE-850, MPE-750, between 70-80 on the x-axis ¨ top curve is MPE-850 overlying MPE-650, bottom curve is MPE-750, between 80-90 on the x-axis ¨ curves from bottom to top are MPE-850, MPE-650, MPE-750.
charge graph ¨
curves from top to bottom are 100th, 10th, 2nd, et, discharge graph ¨ curves from top to bottom are 1st, 2nd, 10th, 100th, C: MPE-750, MPE-850, MPE-650 curves overlie each other, on the left side of the graph MPE-750 is slightly above and MPE-650 is slightly below MPE-850, D: curves from top to bottom are MPE-650, MPE-850, MPE-750.
DETAILED DESCRIPTION
In an embodiment, the eggshell membrane is heated up in an inert atmosphere for pyrolysis.
After pyrolysis, the eggshell membrane may be cleaned, for example, using KOH
and HCI, and is partially activated to increase the surface area (in the outer "shell") and to incorporate oxygen. In the preferred embodiment, the nitrogen content and interconnected fibrous structure of the eggshell membrane remain largely intact after treatment, and the treated .eggshell membrane is a capacitive material with a continuous conducting core and a porous shell. The nitrogen-rich (through the bulk) product is suited for supercapacitors, battery electrodes, CO2 capture, oxygen reduction reaction, catalysis, macromolecule sorption, and environmental remediation, such as heavy metal capture, hydrocarbon absorption, and chemical spill sorption. In the case of egg whites, egg white protein may be adsorbed onto a mesoporous or microporous template and pyrolized to form activated carbon. The mesoporous or microporous template may then be removed, leaving a stand alone structure, or a structure that may be placed on a support for further use, such as for for supercapacitors, battery electrodes, CO2 capture, oxygen reduction reaction, catalysis, macromolecule sorption, and environmental remediation, such as heavy metal capture, hydrocarbon absorption, and chemical spill sorption.
The utility of mesoporous and microporous activated carbon depends for example on the application (super capacitor vs. battery), electrolyte (aqueous vs. polymer) and scan rate. In general small microporosity is useful for aqueous supercapacitor electrolytes and at lower scan rates.
At higher scan rates and in polymer electrolytes (almost always the case for LIB batteries) small mesopores are better. Too many large mesopores result in a low surface area, which is generally undesirable, but some large mesopores are useful for electrolyte transfer. Very small micropores ((1 nm or so) tend not to be very useful for most applications since even in aqueous electrolytes they give transport problems at higher scan rates. For use as a supercapacitor or as an electrode in a battery, the structured carbon materials are typically combined with binder and carbon black in conventional manner.
Chemical activation techniques may also be used in certain embodiments, and may involve soaking the membrane in acid, base, or salt, and then heating the membrane in a single pyrolysis/activation step.
chemical vapor deposition; electrodeposition; and wet chemical methods, such as sol-gel synthesis, hydrothermal processing, precipitation, and ionothermal processing.
The carbonized eggshell membrane (CESM) supported on carbon disc is washed in 20%
KOH at 70 C for 2 hours and then in 2M HC1 for 15 hours at room temperature to remove the impurities. The CESM supported on carbon disc is activated at 300 C for 2 hours in air at a heating rate of 10 C min-1. During the activation process, 10% weight loss is detected.
The chemically activated eggshell membrane (AC-KOH) is prepared by heating the mixture of dry eggshell membrane and KOH (1:4 by weight) to 700 C for 2 hours under argon atmosphere. The obtained fine carbon powder is washed with 2M HC1 and DI water before use.
and 5 %
PVDF (binder) in N-methylpyrrolidone solvent is coated on glassy carbon disc and then dried at 110 C overnight in vacuum oven to obtain the electrode. The electrochemical experiments are performed in Teflon beakers with Pt wire as counter electrodes. Hg/Hg0 (1M NaOH) and Hg/HgSO4 (saturated K2SO4) are used as reference electrodes individually in 1M KOH or 1M H2SO4. For convenience, all the potentials discussed in this paper have been converted to potential versus normal hydrogen electrode (NHE). The Cyclic voltammetry and galvanostatic charge-discharge cycling and impedance analysis are performed on a Solatron 1470E Multichannel Potentiostat/CellTest System. The specific capacitance of CESM is calculated as It/mAE, where I is the change/discharge current, t is the discharging time, m is the mass of electrode materials and AF stands for the potential window.
films is a good estimation of the CESM carbonized on glassy carbon disc. The porous texture of carbon materials is characterized by nitrogen adsorption at 77k (Quantachrome Autosorb-1).
A Hitachi S-4800 scanning electron microscope (SEM) equipped with field emission gun and a JEOL 2100 transmission electron microscopes (TEM) are used to study the morphologies of CESM. X-ray photoelectron spectroscopy (XPS) is obtained on an Axis Ultra spectrometer. The element analysis are performed on Thermo Fisher Scientific (formerly Carlo Erba) EA 1108 CHNS-0 elemental analyzer and Perkin Elmer 's Elan 6000 for metals. Before XPS and element analysis, the samples were dried at 110 C
in vacuum oven over night to remove the absorbed water. The conductivity of CESM is measured by Pro4 from Lucas Labs.
After carbonization, the N content in as-prepared CESM is around 8% by the combustion element analysis shown in Table 1 below. In fact, the eggshell membranes are mainly proteins (rich in N) with very small amount of carbohydrates (no N). It is not surprising that CESM contains more N than chars from biomaterials rich in cellulose and lignin (for example, woods). The N atoms would contribute to the good conductivity of CESM
since the electrical conductivity of N-containing carbons is known to be normally higher than that of N-free carbons. When further activated, the CESM-300 keeps similar N
content.
However, the chemically activated eggshell membrane (AC-KOH) contains only 1.3% N
indicating most of N functional groups are destroyed in the chemical activation process. The 0 content in as-prepared CESM is 9.4% which increases to 10.67% after the further activation. AC-KOH contains slightly more 0 than CESM-300 but the atomic ratio between 0 and C (0/C) is almost same for both samples. XPS is also used identify the content of N
and O. It is interesting to compare the atomic N/C and O/C ratios obtained by combustion element analysis to those by XPS since XPS provides the information at the top layers (1-10 nm) of surface. The N/C ratios obtained by both technologies are relatively consistent in all samples. However, the O/C ratio obtained by XPS is significant higher than that from combustion element analysis in activated CESM. The differences of 0.0285 in O/C ratio indicate the oxygen content on surface is 1.25 times of that in bulk materials in CESM-300.
This is important for the application of supercapacitors since only the oxygen on surface has contribution to pseudocapacitance. It can also be concluded that the 0 content on surface increase 30.1% while the 0 content in bulk materials increase only 14% during the activation process in hot air. That clearly indicates the activation (oxidation) of CESM
only happens on the surface of carbon fibers and the cores of the carbon fibers are unlikely activated or at least not fully activated. Besides C, N, and 0, activated CESM also contains around 3-5%
other impurities (mainly Si, Ca, K, Cl, see ICP trace metal analysis in Table 2 below).
Element analysis XPS
C wt% O wt% N wt% o/c [a] N/C [a] 0/C N/C
CESM-AP 77.51 9.72 8.15 0.0941 0.0901 0.1013 0.0942 CESM-300 76.52 10.99 8.48 0.1077 0.0951 0.1362 0.0921 AC-KOH 81.93 12.26 1.31 0.1123 0.0137 0.1202 0.0147 [a] Atomic ratio from combustion element analysis. [b] atomic ratio from XPS
The contents of metals in activated CESM by trace metal analysis.
Metal Li Be B Na Mg Al Si DL[a] (ppm) 0.05 0.1 2 0.5 2 0.2 5 5 Content (ppm) 4.41 (DL <DL 1146 249 236 421 1236 Metal K Ca Ti V Cr Fe Mn Co DL[al (ppm) 6 31 0.09 0.05 0.05 3.7 0.03 0.03 Content (ppm) 10705 10179 28.0 (DL 55.5 518 9.94 23.1 Metal Ni Cu Zn Ga Ge As Se Rb DL[a] (ppm) 0.06 0.03 0.08 0.01 = 0.02 0.06 0.2 0.04 Content (ppm) 68.6 537 890 0.02 0.09 25.1 <DL 12.5 Metal Sr Y Zr Nb Mo Ru Pd Ag DL[a] (ppm) 0.03 0.02 0.09 0.04 0.02 0.01 0.01 0.01 Content (ppm) 10.7 0.23 10.1 2.61 89.2 0.23 6.35 5.28 Metal Cd Sn Sb Te Cs Ba La Ce DL[a] (ppm) 0.06 0.06 0.01 0.02 - 0.02 0.03 0.03 0.03 Content (ppm) 0.22 = 5.46 0.63 0.43 (DL = 5.94 0.57 1.76 Metal Pr Nd Sm Eu Gd Tb Dy Ho DL[a] (ppm) 0.004 0.03 0.04 0.03 0.03 0.03 0.04 0.02 Content (ppm) 0.037 0.14 (DL <DL (DL (DL <DL <DL
Metal Er Tm Yb Lu Hf To W Re DLIal (ppm) 0.04 0.006 0.05 0.04 0.05 0.02 0.08 0.003 Content (ppm) (DL (DL (DL (DL 0.83 9.37 1.90 0.046 Metal Os Ir Pt Au T1 Pb Th U
DL[a] (ppm) 0.08 0.04 0.01 0.01 0.05 0.03 0.01 0.03 Content (ppm) 0.14 (DL 1.67 2.19 0.06 21.2 0.16 0.06 [a] detection limits of the equipment.
software by 4 peaks representing pyridinic N (N-6 at 398.0 0.2 eV), pyrrolic or pyridonic N
(N-5 at 399.7 0.2 eV), quaternary N (N-Q at 400.8 0.2 eV) and oxidized N (N-X at 402.5 0.2 eV).
The percentage of each component is shown in Table 3 below. It is interesting to find that the percentage of N-6 decreased from 39.88% to 20.83% while the percentage of increased from 25.74% to 47.49% after the activation process in air. That indicates around half of pyridinic N converted into pyrrolic N or pyridonic N. We are also interested in the N
at the edge of graphite plane (N-5, N-6, and N-X) which is known to be more active than that located in the middle of graphite plane (N-Q). The percentage of N on edge in our CESM is very high, 72.51% in CESM-AP and 76.96% in CESM-300.
% of total N ls Functional groups N-Q N-5 N-6 N-X
B. E. (eV) 400.8 399.7 398.0 402.5 CESM-AP 27.49 25.74 39.88 6.89 CESM-300 23.04 47.85 20.83 8.28
calculated by the t-plot method is 0 m2 g-1 for as-prepared CESM and 193 m2 g-1 for activated CESM. Obviously, mainly micropores are formed on CESM surface during the partially oxidation and removing of carbon in hot air which leads to the increase of specific surface area and porosity. However, even after activation, the specific surface area and porosity of CESM is only about 1/7 of those of chemically activated eggshell membrane (AC-KOH). That also suggests the CESM is only partially activated on the surface.
SBET Smicro[al Vtotalibl APD1c1 Resistance C [d]
1112/g m2/g cm3/g nm m F/g CESM-AP 17.03 0 0.068 8.07 4.6X10-4 120 CESM-300 221.2 193.1 0.13 1.2 8.9X10-4 297 AC-KOH 1575 709.1 0.98 1.25 1.8X10-2 203 [a] surface area of micropores calculated by t-plot method. [b] Total pore volume. [c]
Average pore diameter. [d] Capacitance at current density of 0.2 A g-1 in 1M
KOH.
1A), it can be seen that the activated CESM is a highly porous film with a thickness of around 10 gm. Given the measured weight of activated CESM is 0.5 mg cm-2, its density is calculated to be 0.5 g cm-3, similar to activated carbons. The macroporous network structure composed of interwoven and coalescing carbon fibers ranging mainly from 0.2-2 gm in diameter can be observed in planview (Fig. 1B). Clearly the typical structure of eggshell membrane is successfully preserved by using our carbonization and activation procedure.
SEM analysis revealed no difference in the microscope structures of the CESM
before and after activation. This is expected since the pores introduced by the activation process are mainly micropores. The macropores between carbon fibers and the micropores on the carbon fibers form a hierarchical porous structure evenly distributed in activated CESM in large scale. This kind of long-range continuity of the pore network is known to be critical for fast electrolytes transfer. With TEM (Fig. 1C), we can start to see the disordered texture of activated CESM and some pores at the edge of a thin flake. As mentioned in the previous discussion, the significant 0 content increase on surface and relative low surface area and porosity after activation indicate the activation process mainly happened on the surface of carbon fibers of CESM and therefore a carbon-carbon core-shell structure is likely formed (Fig. 1D). The activated shell containing more 0 and micropores (surface area) is great for the application of supercapacitors. But it also has a higher electrical resistance due to the micropores generated. The un-activated core can serve as electron collector.
One of the advantages of 3D coalescing structure of CESM is that there is no contact resistance between fibers. Although the less conductive micropore-rich shell formed on top of fibers during activation, the highly conductive internal cores of fibers still coalesced into one piece, which makes the activated CESM an excellent conductive system. The electrical resistance measured by 4 point probing method is 4.6X10-4 ûm for as-prepared CESM and 8.9X10-4 11m for activated CESM. The increase of resistance is caused by the micropores formed during activation. They are much lower than the resistance of chemically activated eggshell membrane (1.8X10-2 flm) compacted under 20 MPa (10-100 MPa is the most common pressure used to make carbon electrodes). For the commercial high surface area activated carbon, the resistance is in the range of 0.5-3.0X10-2 ûm in compacted form.
The Raman spectra (Fig S1) demonstrate that the CESM is composed of disordered carbon, similar to activated carbon. However, due to its unique structure, the systematic conductivity of CESM
is one order magnitude higher than that of activated carbon, which makes it an ideal electrode material for high power density supercapacitors.
H2SO4, suggesting big contribution from pseudocapacitance. Notably, the C.V
humps of activated CESM in 1M H2SO4 shift to 0.6-0.7V (vs NHE) indicating the pseudocapacitive contribution is not only from the 0 functionalities but also from the N
functionalities.
Different from the activated CESM, the as-prepared CESM shows a triangle-like CV. The difference may relate to the change of surface functionalities during activation, such as the N
functionalities discussed in XPS analysis. More CVs at different sweeping rate can be found in Fig. S2. The reversible capacitive behavior of activated CESM can also be proven by its triangle-like charge-discharge curves in both basic and acidic electrolytes (Fig. 2C). The asymmetry is caused by the pseudocapacitive behavior of the functional groups.
The specific capacitance of activated CESM calculated by the galvanostatic charge/discharge is 297 F g-1 in 1M KOH and 284 F g-1 in 1M H2SO4 at current density of 0.2 A g-1 (Fig. 2D).
Those are among the best performance carbon materials for supercapacitors as compared with results reported by L. L. Zhang, X. S. Zhao, Chem. Soc. Rev. 2009, 38, 2520; C. O.
Ania, V. Khomenko, E. Raymundo-Pinero, J. B. Parra, F. Beguin, Adv. Funct. Mater. 2007, 17, 1828;
E.
Raymundo-Pinero, F. Leroux, F. Beguin, Adv. Mater. 2006, 18, 1877; E. Raymundo-Pinero, M. Cadek, F. Beguin, Adv. Funct. Mater. 2009, 19, 1032; L. Zhao, L. Z. Fan, M.
Q. Zhou, H.
Guan, S. Y. Qiao, M. Antonietti, M. M. Titirici, Adv. Mater. 2010, 22, 5202.
Considering the surface area of activated CESM is significant lower (221 m2 g-1) comparing to activated carbon (typically 500-3000 m2 g-1), the capacitance per surface area reaches 120 F cm-2, much higher than the theoretical EDL capacitance (15-25 pf cm-2). That clearly indicates the capacitance is mainly the contribution of pseudocapacitance from the high-concentration N and 0 functionalities. Although the specific surface area of AC-KOH is 7 times higher than that of activated CESM, its specific capacitance is only 60%-70% of the specific capacitance of activated CESM. Considering both materials containing similar amount of 0, it can be concluded that activated CESM out-performs AC-KOH mainly due to its high N
content and the unique 3D structure. In fact, it is a common phenomenon that the specific capacitance of N-rich carbon materials is closely related to the N contents rather than the specific surface area. With the dramatic increase of specific surface area by further activation, only a small portion of capacitance increase can be achieved. With proper N
content, high capacitance can be achieved even with relative low specific surface area of around 100-200 m2 g-1. That is an advantage of the N-rich carbon materials since high specific surface area normally also means high porosity and poor conductivity.
shows a specific capacitance of 196 F g-1 in 1M KOH and 172 F g-1 in 1M H2SO4 even at high current density of 20 A g-1. The cycle life of activated CESM was also evaluated at high current load (Fig. 2E). After 10,000 charge/discharge cycles at 4 A g-1, capacitance loss is only 3% in KOH and 5% in H2SO4. In fact, the capacitance stabilized after the first 100 cycles (the inset of Fig. 2E). It has been proven that the N-rich carbons obtained by carbonization of biomass have long cycle life because the N and 0 are incorporated in the carbon frame. However, the durability of activated CESM in cycling is even significantly better than those of N-rich carbons which are at the range of 5-7% loss in 2,000 cycles and 10-15 % loss in 10,000 cycles as reported by C. O. Ania, V. Khomenko, E.
Raymundo-Pinero, J. B. Parra, F. Beguin, Adv. Funct. Mater. 2007, 17, 1828., E. Raymundo-Pinero, F. Leroux, F.
Beguin, Adv. Mater. 2006, 18, 1877., L. Zhao, L. Z. Fan, M. Q. Zhou, H. Guan, S. Y. Qiao, M.
Antonietti, M. M. Titirici, Adv. Mater. 2010, 22, 5202. This may be related to unique structures. Since the carbon fibers in activated CESM are coalesced into one piece, no active materials will physically loss contact with electrode and lead to capacitance fading during the cycling.
H2SO4. The ion diffusion process can be characterized by the length of the Warburg-type line (the slope of the 45 portion of the Nyquist lots). The Warbug-type line of activated CESM is much shorter than that of AC-KOH. That demonstrates the fast ion transfer in the hierarchical porous structure of activated CESM. The "onset" frequency is defined as the highest frequency where the impedance of electrode starts to be dominated by capacitive behavior (Nyquist plot starts to go vertical). It reflects the highest frequency to achieve most of the capacitance. The "onset" frequency of activated CESM is 50 Hz higher than that of AC-KOH (6.8 Hz), indicating the fast capacitive responds of activated CESM.
and 0 contents, the activated CESM shows a high specific capacitance of 297 F
g-1 and excellent reversibility with cycling efficiency of 97% after 10,000 cycles in 1M KOH.
Considering over 1,000 billion eggs are consumed per year globally, and that 30-40 mg finished carbon is derivable from one egg, the eggshell membrane is indeed a reliable and sustainable resource for clean energy storage.
Technologies. All other reagents were purchased from Aldrich, unless otherwise specified and were used without further purification.
In a typical experiment, 4.0 g P-123 was dissolved in 200 ml HC1 (2M) at 40 C. Then 11.2g TEOS and 4.0 g TMB were added to the solution and kept stirring for 24h. The mixture was transferred into an autoclave with Teflon inline and heated to 95 C for 3 days. When cooled down, the white powder was separated from the mixture. The powder was calcined at 5500C
in air for 5h to remove the surfactant. The obtained mesoporous silica was then thiol-modified by dispersing lg MCF in 100 ml MPTES ethanol solution (1%) for 2 hours. The SH-MCF was separated, washed with ethanol and dried at 60 C.
LiPF6 in ethylene carbonate/dimethyl carbonate) in argon atmosphere.
lysozyme and small amount of other components. To allow for the effective adsorption of these huge proteins a MCF was used as the template, since they possess much higher mass transfer efficiency than traditional cylindrical mesoporous silica. MCFs are composed of uniform, large cellular cells (25-30 nm, in this work) that are interconnected by windows forming a continuous 3D porous structure. The proteins adsorbed in MCF were pyrolyzed at 650 C, 750 C or 850 C under an inert atmosphere, with the template being subsequently removed.
The resultant carbons are henceforth termed MPEw-650, MPEw-750 and MPEw-850, with the end numbers corresponding to the pyrolysis temperature.
SBET Smicro [a] Composition [b] Cg [c] Cs [d] CLI [e]
[m2g-1] [m2g- c wt% N wt% 0 wt% {Fe] [gm-2] [mAhg-1]
MCF 553.1 83.1 MPEw650 805.7 43.2 87.17 9.30 3.35 390.4 48.5 1780 MPEw750 803.9 47.9 88.79 6.45 4.76 312.8 38.9 1229 MPEw850 810.3 49.3 88.60 5.36 6.04 235.7 29.1 1102 [a] micropore surface area calculated by t-plot method; [b] weight percent of elements obtained from XPS analysis; [c], [d] capacitance and surface area normalized capacitance at current density of 0.25 A gl in 11\ii H2SO4; [e] discharge capacity at the 2"
cycle, tested in a LIB half-cell configuration.
Wang, C.
Zhang, Z. Liu, L. Wang, P. Han, H. Xu, K. Zhang, S. Dong, J. Yao, G. Cui, J.
Mater. Chem.
2011, 21, 5430; L. S. Panchokarla, K. S. Subrahmanyam, S. K. Saha, A.
Govindaraj, H. R.
Krishnamurthy, U. V. Waghmare, C. N. R. Rao, Adv. Mater. 2009, 21, 4726.
Although the Li-ion storage mechanism in N-rich carbon is still unclear, it is believed to relate to the strong electronegativity of nitrogen and the hybridization of nitrogen lone pair electrons with the n electrons in carbon, which makes favorable binding sites for Li-ions.
The high-resolution N 1s core level XPS spectra can be deconvoluted into 4 peaks () representing pyridinic N (N-6 at 398.0 0.2 eV), pyrrolic or pyridonic N (N-5 at 399.7 0.2 eV), quaternary N (N-Q at 400.8 0.2 eV) and oxidized N (N-X at 402.5 0.2 eV).
Comparing with the samples carbonized at higher temperature, MPEw-650 contains more N-6 and less N-Q functionalities, see table 6 below. Although MPEw-650 has slightly lower N-content than the reported polypyrrole-derived CNF (10.25%), it contains significantly more pyridinic-N. Known theoretical calculation suggests that pyridinic-N doped graphene is more favorable than pyrrolic-N doped for Li-ion storage.
% of total N ls Functional groups N-Q N-5 N-6 N-X
B. E. (eV) 400.8 399.7 398.0 402.5 MPEw650 25.9 29.4 40.8 3.9 MPEw750 31.3 34.1 31.0 3.7 MPEw850 36.4 25.2 31.4 7.1
The intensity ratio of these two peaks partially depends on the graphitization degree. The intensity of D band (-1350 cm-1) of MPEw-850 was significantly lower than its G band (-1600 cm-1) with /0//D=1.30, indicating that MPEw-850 is partially graphitized. With the decrease of pyrolysis temperature, the /G//D ratio dropped to 1.18 (MPEw-750) and 1.07 (MPEw-650). The partial graphitization of MPEw carbons may be related to the nature of proteins and ions in the egg white that could induce graphitization at such a relatively low temperature.
Such a continuous integrated macro structure is known to be highly electrically conductive.
Fig. 4B shows a low magnification TEM micrograph highlighting one thin MPEw-fragment resting on a holey carbon support. The figure illustrates the carbon's general frame structure that is composed of well-distributed large mesopores. These large mesopores were typically 20-30 nm in diameter with a wall thickness of 3-5 nm. Fig. 4C shows a high-resolution TEM micrograph of MPEw-850. The partial graphitization of this carbon is demonstrated by the distorted lattice fringes visible in the mesopore walls.
At lower pyrolysis temperatures the lattice fringes are still present, but are less pronounced, indicating a lower degree of graphitization (Fig. 5). Some smaller mesopores are also present in the structure, being marked by the arrows in Fig. 4C. They likely originate from the uneven filing of the MCF template by the proteins. Egg white is composed of mainly 4 proteins whose molecular weights vary from 28,000 to 76,000 g mol-1. Driven by a number of non-covalent interactions such as hydrogen bonding, ionic interactions, Van Der Waals forces and hydrophobic packing, proteins filled in the pores can further fold into different specific spatial configurations that will generate pores smaller than the pore size of the MCF
template.
LiPF6 in ethylene carbonate/dimethyl carbonate (1:1 in volume) electrolyte. Figs. 6A and 68 show the cyclic voltammograms (CV) and charge/discharge curves of MPEw-650. The charge/discharge curves of MPE-750 and of MPE-850 are shown in Fig. 7. MPEw-650 exhibits a typical CV
curve of a non-graphite carbon anode material, with a pronounced cathodic peak at 0 - 1 V
during cycle 1 and at 0 - 0.3 V during cycles 2 and 3. Moreover the intensity of this peak at cycle 1 is much stronger than at 2 and 3. These differences are related to the irreversible consumption of charge via the formation of the solid electrolyte interphase (SEI) layer, as well as to the irreversible loss of some Li storage sites within the carbon.
For the same reason, the discharge curve of MPEw-650 at cycle 1 shows a much higher capacity (3,094 mAh al, at 0.1 A g-1) than at cycle 2 (1,780 mAh al) (Fig. 6B). Overall, the measured capacities of MPEw-650 are extraordinarily high. Even comparing with the CNF
derived from polypyrrole web (with 10.25% N) [L. Qie, W. M. Chen, Z. H. Wang, Q. G.
Shao, X.
Li, L. X. Yuan, X. L. Hu, W. X. Zhang, Y. H. Huang, Adv. Mater. 2012, 24, 2047], which represents the state-of-the-art in carbon electrode energy density, MPEw-650 still demonstrates a higher capacity. This may be attributed to the large amount of mesopores serving as Li-ion reservoirs and a much higher pyridinic-N content in our materials. In fact, the 1,780 mAh al value is the highest reversible capacity ever reported for any carbon-based material. Even the capacity at the 100th cycle (1,365 mAh al) is more than 3 times higher than the theoretical capacity of graphite (372 mAh g 1).
S. Zhou, S.
M. Zhu, M. Hibino, I. Honma, M. Ichihara, Adv. Mater. 2003, 15, 2107], suggesting that the N functionalities and/or the partially graphitized structure can reduce the extent of the irreversible capacity loss reactions that occur during the first cycle. Fig.
7C demonstrates that during the subsequent cycling, the coulombic efficiency of all three carbons is above 95%. With the increase of charge/discharge current, the capacities of MPEw carbons drops to 865, 535 and 560 mAh g- at 0.3 A g-1, and 460, 295 and 355 mAh g- 'at 1.0 A
g-1. It is notable to observe that the carbon with the highest graphitization (MPEw-850) shows the best rate capability, showing the highest capacity (205 mAh g 1) at 4 A g-1.
For example, the 2thi cycle reversible discharge capacities of MPEw-650 (9.3%
N), MPEw-750, (6.3% N) and MPEw-850 (5.6% N) are 1,780, 1,389 and 1,210 mAh Wl, respectively.
These values stabilize at 1,550, 1,050 and 920 mAh g- 1 in the 7th-10th cycle.
In the last 10 cycles (91-100), when charge/discharge current rolls back to 0.1 A g-1, the three carbons show nearly constant discharge capacities of 1,365, 830 and 730 mAh g-1, respectively.
Fig. 3A are the CV curves at 20 mV/s, while Fig. 3B shows the current density dependence of the specific capacitance. MPEw-650 demonstrates the most developed redox humps, and has the highest specific capacitance (390.4 F g-1 at 0.25 A g-1). The surface area normalized capacitances of MPEw-650, MPEw-750, and MPEw-850 are 48.5, 38. and 29.1 piF cm-respectively, much higher than the theoretical EDLC capacitance of carbon (10-25 F cm-2).
Therefore there is a major pseudocapacitive contribution of the surface functionalities in addition to the always-present EDLC. Even at 30 A g-1, MPEw-650, MPEw-750, and MPEw-850 still maintain specific capacitances of 265.3 F g-', 186.3 F g' and 162.8 F gl, respectively. This is attributable to the mesoporous structure of the carbons that facilitate rapid electrolyte transfer and the relatively high degree of graphitization that imparts good electrical conductivity to the electrode. All MPEw carbons show excellent cycle life with less than 7% capacitance loss after 10,000 cycles.
Qiao, M.
Antonietti, M. M. Titirici, Adv. Mater. 2010, 22, 5202; L. Zhao, N. Baccile, S. Gross, Y. J.
Zhang, W. Wei, Y. H. Sun, M. Antonietti, M. M. Titirici, Carbon 2010, 48, 3778]. Further chemical activations will increase the surface area, but will also significantly decrease the N-content [L. Zhao, L. Z. Fan, M. Q. Zhou, H. Guan, S. Y. Qiao, M. Antonietti, M. M. Titirici, Adv. Mater. 2010, 22, 5202]. As a balance, the achieved specific surface area of carbons containing more than 6% N is normally less than 250 m2 al [ L. Zhao, L. Z.
Fan, M. Q.
Zhou, H. Guan, S. Y. Qiao, M. Antonietti, M. M. Titirici, Adv. Mater. 2010, 22, 5202; E.
Raymundo-Pinero, M. Cadek, F. Beguin, Adv. Funct. Mater. 2009, 19, 1032.; L.
Zhao, N.
Baccile, S. Gross, Y. J. Zhang, W. Wei, Y. H. Sun, M. Antonietti, M. M.
Titirici, Carbon 2010, 48, 3778]. In this work, we templated a MCF structure with proteins to obtain carbons rich in nitrogen (as high as 9.3% N) and yet with a high specific surface area (805.7 m2 g'), a favorable pore size distribution, and a sufficient degree of graphitization.
This material exhibits the highest reported reversible capacity of any carbon-based LIB
anode (1,780 mAh g), and among the highest reported specific capacitances for any carbon-based electrochemical capacitor electrode (390.4 F g-1).
is used in its inclusive sense and does not exclude other elements being present. The indefinite articles "a" and "an" before a claim feature do not exclude more than one of the feature being present. Each one of the individual features described here may be used in one or more embodiments and is not, by virtue only of being described here, to be construed as essential to all embodiments as defined by the claims.
Claims (20)
OR PRIVILEGE IS CLAIMED ARE DEFINED AS FOLLOWS:
adsorbing proteins onto a porous template; and pyrolizing the proteins on the porous template to form activated carbon.
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| CN106935415B (en) * | 2017-05-03 | 2019-09-06 | 王馨瑜 | The method for improving specific capacity of double-layer capacitor |
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