Michael Ayiania1, Aidan Garcia2, Sohrab Haghighi Mood1, Jean-Sabin McEwen1,2,3,4,5, Manuel Garcia-Perez1. 1. Department of Biological Systems Engineering, Washington State University, Pullman, Washington 99164, United States. 2. Gene and Linda Voiland School of Chemical Engineering and Bioengineering, Pullman, Washington 99164, United States. 3. Department of Physics and Astronomy, Washington State University, Pullman, Washington 99164, United States. 4. Department of Chemistry, Washington State University, Pullman, Washington 99164, United States. 5. Institute for Integrated Catalysis, Pacific Northwest National Laboratory, Richland, Washington 99352, United States.
Abstract
Due to phosphate's necessity in agriculture and its danger to the environment, the development of adsorbents for its removal has been the subject of intensive research activity. Although the introduction of nitrogen functionality to chars and modification of biochar with metals have proven to change the character of the char structure, making it more active toward nutrients, there is no study regarding the doping of biochar with metals and nitrogen simultaneously for the adsorption of phosphates. This paper is the first of two in which we report the production, characterization, and evaluation of N-metal-doped biochars from cellulose for phosphate removal from liquid effluents. In this part, we describe the production and characterization of N-Ca-, N-Fe-, and N-Mg-doped biochars. The elemental composition and surface area of each of the materials produced is reported. Elemental and surface characterization of the chars are reported with the largest N content appearing at a temperature of 800 °C (12.5 wt %) and a maximum surface area for biochar produced at 900 °C (1314 m2/g). All of the adsorbents were visualized by scanning electron microscope (SEM), confirming that although there are some crystals on the surface of the biochar produced, most of the N, Mg, and Ca are part of the polyaromatic ring structure. Transmission electron microscope (TEM) images clearly show the formation of nanoclusters with the metals in the case of N-Fe and N-Ca biochars. The N-Mg biochars show a uniform distribution of the Mg through the carbon surface. X-ray photoelectron spectroscopy (XPS) studies of the biochars produced with metals and varying nitrogen levels clearly show Mg and Ca peaks shifting their position in the presence of N, suggesting the formation of stable structures between metals and N in the carbon polyaromatic ring system. To elucidate the nature of these structures, we conducted DFT-based calculations on different configurations of the nitrogenated structures. The calculated binding energy shifts were found to closely match the XPS experimental binding energy, confirming the likelihood of these structures in biochar. Finally, based on our experimental and modeling results, we hypothesize that an important fraction of the Mg and Ca is introduced to these biochars at the edges. Another fraction of Mg and Ca is in the form of phthalocyanine-like internal structures. More experimental studies are needed to confirm the formation of these very interesting structures and their potential use as adsorbents or catalysts.
Due to phosphate's necessity in agriculture and its danger to the environment, the development of adsorbents for its removal has been the subject of intensive research activity. Although the introduction of nitrogen functionality to chars and modification of biochar with metals have proven to change the character of the char structure, making it more active toward nutrients, there is no study regarding the doping of biochar with metals and nitrogen simultaneously for the adsorption of phosphates. This paper is the first of two in which we report the production, characterization, and evaluation of N-metal-doped biochars from cellulose for phosphate removal from liquid effluents. In this part, we describe the production and characterization of N-Ca-, N-Fe-, and N-Mg-doped biochars. The elemental composition and surface area of each of the materials produced is reported. Elemental and surface characterization of the chars are reported with the largest N content appearing at a temperature of 800 °C (12.5 wt %) and a maximum surface area for biochar produced at 900 °C (1314 m2/g). All of the adsorbents were visualized by scanning electron microscope (SEM), confirming that although there are some crystals on the surface of the biochar produced, most of the N, Mg, and Ca are part of the polyaromatic ring structure. Transmission electron microscope (TEM) images clearly show the formation of nanoclusters with the metals in the case of N-Fe and N-Ca biochars. The N-Mg biochars show a uniform distribution of the Mg through the carbon surface. X-ray photoelectron spectroscopy (XPS) studies of the biochars produced with metals and varying nitrogen levels clearly show Mg and Ca peaks shifting their position in the presence of N, suggesting the formation of stable structures between metals and N in the carbon polyaromatic ring system. To elucidate the nature of these structures, we conducted DFT-based calculations on different configurations of the nitrogenated structures. The calculated binding energy shifts were found to closely match the XPS experimental binding energy, confirming the likelihood of these structures in biochar. Finally, based on our experimental and modeling results, we hypothesize that an important fraction of the Mg and Ca is introduced to these biochars at the edges. Another fraction of Mg and Ca is in the form of phthalocyanine-like internal structures. More experimental studies are needed to confirm the formation of these very interesting structures and their potential use as adsorbents or catalysts.
Nitrogenated carbon materials
are of recent interest due to their
excellent properties in a variety of applications, such as carbon
electrodes[1] and heterogeneous catalysis.[2−5] There are also several studies where nitrogenated carbons show efficient
adsorption capacities toward pollutants[6−9] and good performance in batteries.[10−12] Phosphate is essential
for modern agriculture but is a dangerous pollutant when released
into the environment. While uncontrolled nutrient disposal in water
bodies results in dead zones and eutrophication, adsorbents such as
biochar have shown promise in controlling these pollutants.[13−16] Previous studies show that biochar does not perform well for the
removal of phosphate without modification[17−19] but is suitable
for the removal of several pollutants from wastewater when metals
are added. In other studies, the introduction of nitrogen functionality
to chars has proven to characteristically change its structure, making
it more active toward foreign molecules such as metals and nutrients.[20] In spite of the promising characteristics of
both modifications, there is a limited number of studies with regard
to the doping of biochar with metals as well as nitrogen. Understanding
the chemical nature of the metal in N-doped biochar, whether the metal
is in the form of nanocrystals on the surface of the biochar or embedded
in the matrix of the carbon materials, is critical to designing better
adsorbents. Hence, the main goal of this paper is to produce and characterize
N-metal-doped biochar. In the second part, the capacity of biochars
doped with nitrogen and metals with regard to phosphate adsorption
is evaluated.
Methods and Materials
Sample Preparation
Magnesium chloride
hexahydrate (MgCl2·6H2O), calcium chloride
(CaCl2), and iron (III) chloride (FeCl3) were
purchased from Sigma-Aldrich to prepare the solutions and pretreat
the feedstocks. All solutions used in this work were prepared with
deionized (DI) water, which was also used to rinse and clean the samples.
Briefly, 5 wt % solution was prepared, and each feedstock was immersed
into the solution for 1 h. The mixture of biomass and solution was
then oven-dried 24 h at 105 °C to remove the water.
Nitrogen-Metal-Doped Biochar Production
To better control
the structure of the resulting biochar, Avicel
cellulose was used as a starting material. N-doped biochars were produced
using ammonia through a one-step ammonization process at five different
temperatures (500, 600, 700, 800, 900 °C). This was conducted
in a Quartz Tube furnace reactor with 50 mm OD by 44 mm ID at a length
of 1.0 m. Briefly, cellulose was kept in a tubular furnace in contact
with N2 for 30 min at 25 °C. Then, the temperature
was increased from 25 °C to the desired set temperature at a
heating rate of 10 °C min–1 under an ammonia
environment. When the final temperature is reached, the sample is
allowed a residence time of 30 min in the reactor. A flow rate of
1000 mL min–1 for ammonia was employed. The final
biochar produced was cooled down to 25 °C at the same rate before
storage and characterization.Nitrogen-metal biochars were also
produced using avicel cellulose and three different metals, but all
of these studies were conducted at 800 °C (at this temperature,
we obtained the highest incorporation of nitrogen). Solutions of 5
wt % Mg, Ca, and Fe were prepared from MgCl2, CaCl2, and FeCl3, respectively, and later mixed with
cellulose in a ratio of 2.8:1 (Solution/Cellulose). The cellulose
was fully covered with the solution to ensure uniform distribution.
The mixtures were then oven-dried for 24 h. Figure is a block diagram outlining the course
of the methodology and the manuscript.
Figure 1
Schematic representation
of tasks described in this paper.
Schematic representation
of tasks described in this paper.
Elemental Analysis
Elemental analysis
was performed using a TruSpec-CHN elemental analyzer (LECO). Briefly,
0.15 g of the sample was used to determine total carbon (C),
nitrogen (N), and hydrogen (H) contents. Oxygen (O) mass fraction
was determined by subtracting the ash, C, N, and H contents from the
total mass of the sample.
Proximate Analysis
Moisture, fixed
carbon, volatile matter, and ash content in all biochars produced
were determined using a thermogravimetric analyzer, SDTA851e (Mettler
Toledo). The percentage of fixed carbon was determined by subtracting
the ash percentage from the volatile matter percentage after assigning
all weight loss up to 120 °C to loss of free and non-structural
water. Briefly, moisture content was measured as the weight loss after
the char was heated in a crucible from 25 to 120 °C and
held at this temperature for 3 min under a nitrogen gas environment
at a flow rate of 50 mL/min. Then, the char was heated from
120 to 950 °C under a nitrogen gas environment to determine
volatile content. It was then held at this temperature for 5 min
and cooled down to 450 °C. Ash was determined after heating
the char from 450 to 600 °C under oxygen gas flow (50 mL/min).
Gas Physisorption Analysis for Biochar Surface
Area and Porosity
Carbon dioxide (CO2) and nitrogen
adsorption isotherms were measured at 273 and 77 K, respectively,
on micromeritics TriStar II PLUS surface area and porosity analyzer
(Norcross, GA). Before each analysis, biochar samples were degassed
at 250 °C for 18 h under a vacuum of 0.05–0.1 mbar (the
degassing temperature was chosen based on the production temperature
of the biochar to avoid sample degradation during preparation). CO2 adsorption isotherms were measured between the partial pressure
range of P/Po = 10–5 to P/Po = 0.03 using 75 set equilibration points, and nitrogen isotherms
were measured between P/Po = 10–5 to 0.99 and desorption between P/Po = 0.99 to 0.01, where the
relative pressure (P/Po) is the ratio of absolute gas pressure to saturation pressure. The
saturation pressure of N2 at 77 K is 101.3 kPa[21] while the surface area, and micropore volumes
were estimated for CO2 and N2 adsorption using
the Dubinin–Radushkevich (DR) equation and BET model, respectively.[22,23]
SEM and TEM
Scanning electron micrographs
of all chars were collected using an Apreo VolumeScope equipped with
a field emission gun electron source. All samples were prepared by
coating with 3 nm of gold to enhance resolution using a Cressington
Hi-Res Sputter Coater. The images were collected under vacuum with
a chamber pressure below 10 mPa. The accelerating voltage was set
at 30 kV for all samples. Specimens for the transmission electron
microscope (TEM) study were prepared by grinding the biochar into
a fine powder. A suspension of DI water and the powdered biochar were
prepared and deposited onto copper grids. Imaging was carried out
at 200 kV and under vacuum conditions with a FEI Tecnai G2 20 Twin.
Care was taken to minimize exposure to a focused electron beam to
avoid specimen damage.
X-Ray Photoelectron Spectroscopy
Analysis using XPS was performed using an AXIS-165 upgraded to
an
Ultra manufactured by Kratos Analytical Inc. Achromatic X-ray radiation
of 1253.6 eV (MgKα) was used to analyze each material. All high-resolution
spectra were recorded using a pass energy of 40 eV and a spot size
of approximately 120 μm. The spectrometer was calibrated against
both the Au 4f7/2 peak at 84.0 eV and
the Ag 3d5/2 peak at 368.3 eV. The minimum
full width at half maximum (FWHM) for the Au 4f7/2 peak is approximately 0.85 eV, representing the absolute
minimum possible broadness achievable for this configuration. Survey
scans have been obtained using a pass energy of 80 eV and step sizes
of 1 eV to determine the overall chemical composition of each sample.
To determine the speciation of carbon, nitrogen, and oxygen groups,
high-resolution scans of the C 1s, N 1s, O 1s, and Mg 2p regions (280–295,
394–404, 527–538, and 45–60 eV, respectively)
were collected for each material using 0.1 eV step sizes.
X-ray Powder Diffraction (XRD)
X-ray
diffraction (XRD) analysis was conducted to identify crystallographic
structures in the biochar samples using a Rigaku (Miniflex 600) with
Cu K α radiation operated at 40 kV, 15 mA in steps of 0.01°,
with a scanning rate at 0.5 ° min–1 from 10
to 100°.
Computational Calculations
To better
understand the effect of nitrogen functionality and metals (Mg/Ca),
we computationally quantified the stability of Mg/Ca centers supported
by various types of nitrogen functional groups. Using the energies
generated computationally, adsorption energies for magnesium and calcium
were calculated using the following equationwhere Eads denotes
the calculated adsorption energy, (EMg/Ca), the energy of the entire surface-Mg/Ca structure, Esurf the energy of the functionalized carbon
surface, and (EMg), the calculated energy of the bulk material. We have further
quantified the adsorption energy of water on N-Mg-doped graphene and
quantified the adsorption strength of water usingwhere EadsH denotes the adsorption
energy of water on the N-Mg-doped structure, EMg, the energy of the entire surface-Mg structure,
and EH, the energy of
the water molecule in the gas phase. DFT calculations were carried
out using the Vienna Ab initio Simulation Package
(VASP).[24−26] The projector-augmented wave (PAW) method[27,28] was used to model the core electrons (POTCARs released in 2002 for
C, and N and 2001 for H, Mg, and 2000 for Ca), and a plane-wave basis
set with an energy cutoff of 450 eV was used to model the valence
electrons. To model the electron exchange and correlation, the Perdew–Burke–Ernzerhof
(PBE) functional[29] was applied (POTCAR
set updated 2007). The Gaussian smearing method was used to set partial
occupancies of bands with a smearing width of 0.2 eV to facilitate
Brillouin zone integration convergence, followed by extrapolation
to zero Kelvin for the total energy calculation.[30,31] All ground state optimizations used the conjugate gradient method
and were considered converged when the relaxed interatomic cartesian
forces were smaller than 0.025 eV/Å. The SCF energy tolerance
was set to 10–5 eV. Spin polarization was also used
for all calculations to account for any magnetization. Calculations
for bulk Mg were optimized to confirm a simple hexagonal cell with
a lattice constant 3.19 Å and an a/c ratio of 1.624 using a (10 × 10 × 10) Monkhorst–Pack
grid. Bulk Ca was optimized in the same fashion to obtain a face-centered
cubic cell with a lattice constant of 5.68 Å. Nitrogen and metal
functionalization was studied in a graphene nanoribbon within a hydrogen-terminated
edge model with dimensions of (29 × 17 × 21 Å). These
ribbons allow for edge site adsorption and were used across all tested
structures to provide comparable results. The graphene lattice constant
was 2.467 Å, consistent with previous results.[32−34] The integration
of the Brillouin zone was conducted using a (1 × 2 × 3)
Monkhorst–Pack grid. All structures were visualized using VESTA[35]Figure shows the strategy used to generate the model of N-metal-doped
biochar structures for our DFT calculations. We proposed various structural
configurations of nitrogen and metal (Mg/Ca) based on our experimental
results and calculated the stability and the core-level binding energy
shifts (CLBES) of these structures.
Figure 2
Schematic representation of the creation
of the N-metal graphene
models, where (a) is the creation of a single point defect. (b) Introduction
of nitrogen to replace the dangling carbon forming pyridinic groups.
(c) Metal atom is embedded in the matrix of the graphene. The black,
orange, and blue spheres represent carbon, magnesium, and nitrogen
atoms, respectively.
Schematic representation of the creation
of the N-metal graphene
models, where (a) is the creation of a single point defect. (b) Introduction
of nitrogen to replace the dangling carbon forming pyridinic groups.
(c) Metal atom is embedded in the matrix of the graphene. The black,
orange, and blue spheres represent carbon, magnesium, and nitrogen
atoms, respectively.The structure with metal
atoms at the center of the pyridine-nitrogen
or the pyrrolic-nitrogen in graphene was created through two steps:
(i) the creation of a pyridine-nitrogen/pyrrolic-nitrogen, the substitution
of under-coordinated carbons by N atoms to form a single vacancy or
di-vacancy, as shown in Figure a,b; (ii) metal atom incorporation in the center of single-
or double-point defect, as shown in Figure 2c.To compare the DFT-based model systems of N-metal-doped
carbon
to the experimentally measured XPS spectra, the core-level energy
shifts (ECLS) of the metal 2p states were
calculated according towhere nc is the
total number of core electrons in the system, EN-Me-Doped (nc –
1) is the total energy of the N-Metal-doped H-edge graphene model
with a single core electron removed from the metal 2p state, EN-Me-Doped (nc) is the total energy of the N-Metal-doped H-edge model
with all core electrons present in the system, Ebulk-Me (nc – 1)
is the total energy of a bulk metal with a single core electron removed
from a 2p state, and Ebulk-Me(nc) is the total energy of a bulk metal with
all core electrons present in the system. The core-level binding energy
shift was calculated using the final state approximation.[36] To obtain the core-level binding energies from
the core-level binding energy shift values, we used the experimental
binding of bulk metal (Magnesium) as the reference with a binding
energy of 49.80 eV.[37]
Results and Discussion
Biochar Yield
Table presents the
biochar yield of N-chars and
N-metal biochars. The yield of N-char decreased with increasing temperature
due to the loss of volatiles by the pyrolysis reactions, as expected.[37] The N-metal biochars present a higher yield
than the N-chars because of the impregnated metal content in these
biochars.
Table 1
Char Yield of N-Char and N-Metal Biochars
(wt %)
sample
500 °C
600 °C
700 °C
800 °C
900 °C
N-char
20.3 ± 0.2
17.9 + 0.2
17.5 ± 0.4
16.8 ± 0.3
15.5 ± 0.6
Mg-char
34.0 ± 0.3
Mg-N-char
30.1 ± 0.4
Ca-N-char
32.5 ± 0.9
Fe-N-char
29.8 ± 0.4
Characterization of N-Doped Biochars
Table shows the
elemental analysis of all N-doped biochars produced. Nitrogen content
in the samples generally increased with processing temperature. The
greatest nitrogen content appears at a temperature of 800 °C
(12.5 wt %) (Table ). The C, H, and O contents in the char decrease with temperature.
If we multiply the yield of char reported in Table by the content of the elements reported
in Table , it is possible
to explain these trends. Effectively, the quantity of C gradually
decreases from 17.57 wt % at 500 °C to 13.88 wt % at 900 °C.
The reduction in the content of C can be explained by the cleavage
of some weak bridges between small polyaromatic structures that could
lead to the removal of small polyaromatic rings. In the case of H,
it gradually decreased from 2.7 wt % at 500 °C to 0.53 wt %.
The hydrogen is removed as part of the removed small polyaromatic
rings and during the formation of a larger poly-condensed ring system.
The amount of N, on the other hand, remains almost constant at 500
and 600 °C and then increases rapidly at 700 and 800 °C.
This increase can be explained by the reaction between the polyaromatic
rings and ammonia. At 900 °C, the N in polyaromatic structures
seems to be thermally removed. Our group[17] recently examined the thermodynamic stability of nitrogen functionalities
on different graphene and graphene using DFT-calculated Gibbs reaction
energies. The most stable nitrogen functionality was pyridinic nitrogen,
followed by graphitic nitrogen.
Table 2
Elemental Content
of N-Doped Biochars
from Cellulose (Dry Basis)
dry
basis
samples
C (wt %)
H (wt %)
N (wt %)
O* (wt %)
Ash (wt %)
N-dopedchar_500
86.6 ± 0.4
3.1 ± 0.03
7.4 ± 0.1
2.9 ± 0.2
<0.1
N-dopedchar_600
87.5 ± 0.5
2.2 ± 0.01
7.8 ± 0.02
2.6 ± 0.2
<0.1
N-dopedchar_700
85.4 ± 0.5
1.2 ± 0.01
11.0 ± 0.05
2.4 ± 0.2
<0.1
N-dopedchar_800
84.7 ± 0.7
0.9 ± 0.01
12.5 ± 0.2
1.9 ± 0.3
<0.1
N-dopedchar_900
89.6 ± 0.7
0.6 ± 0.03
7.6 ± 0.1
2.1 ± 0.3
0.1
Figure shows the
CO2 and N2 adsorption isotherms for all of the
N-doped biochars produced. A high surface area was achieved through
ammonia-doping of cellulose biochar, with ammonia serving as an activating
agent. The surface area analysis shows an increase in biochar surface
area as the production temperatures are increased (500–900
°C). Note that specific surface area and pore volume are commonly
determined by the measurement of physisorption of N2 and/or
CO2. The maximum surface area (1314 m2 g–1, see Table ) was achieved at 900 °C. The surface area measured in
the range between 500 and 700 °C for chars produced under NH3 was between 13 and 20% lower than the chars produced under
N2 reported by Smith et al.[38] It is worth mentioning that high surface area and pore volume are
key biochar properties pertaining to water and nutrient cycling, microbial
activity, and sorption of organic and inorganic compounds and gaseous
pollutants.
Figure 3
Adsorption isotherms of nitrogen-doped biochars produced from cellulose.
(A) is the N2 adsorption isotherm and (B) is the CO2 adsorption isotherm.
Table 3
Surface Area (Sa) and Pore Volume
(PV) of N-Doped Biochars from Cellulose
sample
SaN2 (m2 g–1)
SaCO2 (m2 g–1)
PVmicro (cm3 g–1)
PVmeso (cm3 g–1)
PVtotal (cm3 g–1)
N-dopedchar_500
331.7
0.13
N-dopedchar_600
386.2
0.15
N-dopedchar_700
453.2
470.9
0.19
0.02
0.21
N-dopedchar_800
934.1
761.0
0.30
0.12
0.42
N-dopedchar_850
1169.9
764.2
0.31
0.20
0.51
N-dopedchar_900
1314.8
793.4
0.32
0.27
0.59
Adsorption isotherms of nitrogen-doped biochars produced from cellulose.
(A) is the N2 adsorption isotherm and (B) is the CO2 adsorption isotherm.
Characterization of N-Metal-Doped Biochars
The elemental and proximate analysis of biochar doped with metals
and nitrogen is presented in Table . The presence of metals had a significant influence
on the carbonization process, namely by incorporating more nitrogen
into the structure of the biochar. The presence of metals in chars
has a catalytic effect on the formation of the nitrogen dopant.[39,40] This is particularly evident for the N-Mg-char, which contains 15.5
wt % nitrogen as compared to the 12.5 for its N-doped counterpart
(Table ). However,
the carbon content decreases dramatically as compared to biochar without
metals.
Table 4
Elemental Composition (wt %) of Metal-N-Doped
Biochar Derived from Cellulose Produced at 800 °Ca
Our SEM-EDS studies aimed to determine if metals were in the form
of crystals on the surface of the chars or embedded within the matrix
of the biochar. The results of these studies are shown in Figures –6 for N-Mg-Char, N-Ca-Char, and N-Fe-Char, respectively. Figure shows the presence
of both a smooth and a rough surface with some microcracks and shallow
pores as a result of ammonia etching in the N-Mg-Char. Interestingly,
metals were observed both in the form of crystals and embedded in
the carbonaceous surface of the biochar. The EDS test results show
Mg is present in both the crystals and the carbonaceous structure.
Because only a small fraction of the surface is covered by crystals,
we can hypothesize that most of the Mg is embedded within the carbon
matrix.
Figure 4
SEM-EDS images of N-Mg-Char in the two different regions. Region
1 shows the presence of crystals, while region 2 is smooth. The X- and Y-axes represent the energy of the
X-rays emitted (measured in KeV) and the measured intensity in counts,
respectively.
Figure 6
SEM-EDS
images of N-Fe-Char. Only region 4 does not show any presence
of crystals. Note that region 5 was not shown in the figure because
it has similar spectra to regions 1, 2, and 3.
SEM-EDS images of N-Mg-Char in the two different regions. Region
1 shows the presence of crystals, while region 2 is smooth. The X- and Y-axes represent the energy of the
X-rays emitted (measured in KeV) and the measured intensity in counts,
respectively.Figure shows the
presence of a smooth surface rich in Ca without pores. Figure shows the SEM-EDS of the N-Fe-doped biochar. It was observed
that most of the Fe is in the form of crystals deposited on the surface.
The content of Fe in the carbonaceous matrix (see Figure ) is very low, with crystals
making up the majority of iron in the char.
Figure 5
SEM-EDS images of N-Ca-Char.
Region 1, 2, and 3 are regions without
any Ca pores. The X- and Y-axes
represent the energy of the X-rays emitted (measured in KeV) and the
measured intensity in counts, respectively.
SEM-EDS images of N-Ca-Char.
Region 1, 2, and 3 are regions without
any Ca pores. The X- and Y-axes
represent the energy of the X-rays emitted (measured in KeV) and the
measured intensity in counts, respectively.SEM-EDS
images of N-Fe-Char. Only region 4 does not show any presence
of crystals. Note that region 5 was not shown in the figure because
it has similar spectra to regions 1, 2, and 3.
TEM and XRD
Figure shows the TEM picture of the N-Mg-doped
biochar. We do not see in this figure any evidence of the Mg forming
nanocrystals. Although there are some crystals as indicated by the
XRD peaks, EDS indicates most Mg is part of the polyaromatic carbon
structure.
Figure 7
TEM of N-Mg-doped char.
TEM of N-Mg-doped char.Figure shows the
TEM picture of the N-Ca-doped biochar. We can clearly see in the figure
the presence of clusters or regions (likely nanocrystals in the range
of 20–30 nm). This means that although the Ca can be found
as part of the carbonaceous structure, it may also form nanoparticles.
Figure 8
TEM of
N-Ca-doped biochar.
TEM of
N-Ca-doped biochar.Figure shows the
TEM of the N-Fe-doped biochars. Here, we observed the formation of
very small nanoparticles of less than 5 nm in the carbon matrix.
Figure 9
TEM picture
of N-Fe-doped biochars.
TEM picture
of N-Fe-doped biochars.Figure shows
the wide-angle XRD patterns of N-Mg, and N-Fe-biochar samples. The
XRD data from N-Mg-Char confirm the presence of highly crystalline
MgO particles. We found the presence of MgC2N2 with a crystallite size of about 9.5 nm. The broadness of the XRD
peaks was used to calculate the crystalline size of MgO particles
using the Scherrer equation. The results showed the presence of particles
with a size between 9.5 nm and 50 nm (Table ). The XRD of N-Fe-char only presents crystals
of iron oxides with a crystallite size between 14.9 and 164.5 nm (Table ).
Figure 10
XRD of (a) N-Mg-Char
and (b) N-Fe-Char.
Table 5
Crystallite
Size of the Correlated
Phases in the N-Mg-Char
2θ [deg]
correlated phase(s)
crystallite size [nm]
18.68
C5Cl5N, Mg (OH)2
9.45
33.93
C5Cl5N
28.04
36.79
MgO
20.12
45.24
C5Cl5N
31.3
55.99
C5Cl5N, Mg (C N)2
9.56
62.14
MgO, C5Cl5N, Mg (OH)2
21.37
67.19
C5CL5N_300K
18.68
74.65
MgO, C5Cl5N
21.59
78.6
MgO, C5Cl5N
50.19
93.85
MgO, C5Cl5N
17.63
Table 6
Crystallite Size
of the Correlated
Phases in the N-Fe-Char
2θ [deg]
correlated phase(s)
crystallite size [nm]
37.45
Fe3N, Fe2N
14.91
40.74
Fe3N, Fe2N
44.24
42.82
Fe3N, Fe2N
164.5
56.54
Fe3N, Fe2N
24.78
67.85
Fe3N, Fe2N
22.63
75.75
Fe3N, Fe2N
24.59
82.22
Fe3N, Fe2N
24.45
83.43
Fe3N, Fe2N
24.68
XRD of (a) N-Mg-Char
and (b) N-Fe-Char.
High-Resolution
XPS Spectra
The high-resolution
spectra taken for each of N-Mg and N-Ca biochars are shown in Figure . The first figure
(a) is the N 1s spectra, the middle figure (b) is
the O 1s, while the third figure shows Mg 2p spectra (c). Here, it is worth noting that the Mg-Char
presents a peak at 56 eV in the absence of nitrogen, but in the presence
of nitrogen in the structure (N-Mg-Char), this peak is replaced by
one at to 53.15 eV, in addition to an entirely new peak at about 49.85
eV is likely related to the bonding between N and Mg. The nitrogen
dramatically affects the O 1s spectra as well, eliminating
a peak that was present at 538 eV for char without N. These findings
indicate that the nitrogen might have a stronger affinity toward the
metal than the oxygen.
Figure 11
XPS spectra. The top figures consists of N-doped
char, Mg-Char,
and N-Mg-doped char. The bottom figures consist of N-doped char (a),
Ca-Char (b), and N-Ca-doped biochar (c).
XPS spectra. The top figures consists of N-doped
char, Mg-Char,
and N-Mg-doped char. The bottom figures consist of N-doped char (a),
Ca-Char (b), and N-Ca-doped biochar (c).
Computational Investigation of Site Stability
and XPS Core-Level Binding Shifts (CLBES)
To better understand
the specific functionalities formed, we computationally quantified
the stability of magnesium and calcium on internal and edge active
sites, supported by various types of nitrogen functional groups. Below
are the different types of structures that were tested.The
results (see Figure , this figure is based on data shown in Figures –15) indicate that the number of nitrogen
functional groups and the configuration of those groups have a tremendous
effect on metal binding stability. The internal active sites (metals
held within the sheet by multiple nitrogen groups) turned out to be
more favorable (since the adsorption energies are nearly all exothermic,
i.e., negative) than the edge active sites (since they are either
highly endothermic, i.e., positive or only slightly exothermic).
Figure 16
Adsorption energies of Mg and Ca with increasing number
of pyridine
and pyrrolic functional groups. (a) N-Mg-doped sheet and (b) N-Ca-doped
sheet.
Figure 12
Molecular
scheme of Mg-N-doped biochars within a graphene model
structure with a (a) 3P6N-MgH2, (b) 3P5N-Mg, (c) 3P6N-Mg, (d) 4P5N-Mg, and (e) 4P6N-Mg functionality, where the black, blue, white, and orange
spheres represent carbon, nitrogen, hydrogen, and magnesium atoms,
respectively.
Figure 15
Calcium adsorption energies
at the edge of graphene with pyrrolic
and pyridinic groups with a (a) P6N-Mg, (b) 2P6N-Mg, (c) P5N-Mg, and (d) 2P5N-Mg functionality.
There sphere legend is as given in Figure .
Molecular
scheme of Mg-N-doped biochars within a graphene model
structure with a (a) 3P6N-MgH2, (b) 3P5N-Mg, (c) 3P6N-Mg, (d) 4P5N-Mg, and (e) 4P6N-Mg functionality, where the black, blue, white, and orange
spheres represent carbon, nitrogen, hydrogen, and magnesium atoms,
respectively.Magnesium adsorption energies at the
edge of graphene with pyrrolic
and pyridinic groups with a (a) P6N-Mg, (b) 2P6N-Mg, (c) P5N-Mg, and (d) 2P5N-Mg functionality.
The sphere legend is as given in Figure .Calcium
adsorption energies at the center of graphene with pyrrolic
and pyridine groups with a (a) 3P6N-MgH2, (b)
3P5N-Mg, (c) 3P6N-Mg, (d) 4P5N-Mg,
and (e) 4P6N-Mg functionality, where the black, blue, blue-green,
and white spheres represent carbon, nitrogen, calcium, and hydrogen
atoms, respectively.Calcium adsorption energies
at the edge of graphene with pyrrolic
and pyridinic groups with a (a) P6N-Mg, (b) 2P6N-Mg, (c) P5N-Mg, and (d) 2P5N-Mg functionality.
There sphere legend is as given in Figure .
Figure 14
Calcium
adsorption energies at the center of graphene with pyrrolic
and pyridine groups with a (a) 3P6N-MgH2, (b)
3P5N-Mg, (c) 3P6N-Mg, (d) 4P5N-Mg,
and (e) 4P6N-Mg functionality, where the black, blue, blue-green,
and white spheres represent carbon, nitrogen, calcium, and hydrogen
atoms, respectively.
As shown in Figure , the nitrogen species that bind to Mg/Ca have a noticeable effect
on the adsorption energy. While the monofunctional group at the edge
sites, with the corresponding structures as shown in Figures and 15, does not bind favorably (since a positive value indicates an unfavorable
adsorption), a pronounced effect is shown on the adsorption energy
with a difunctional group at the edge, with pyridine and pyrrole. Figure also explores
the effect of increasing the pyridine/pyrrolic group on the stability
of Mg/Ca within a di-and tri-vacancy defect. With these configurations,
the adsorption of Mg/Ca becomes energetically favorable (since the
adsorption energies are negative). However, a monovacancy region with
three pyridine groups (see Figures c and 14c, 3P6N-Mg)
coordinated to a Mg/Ca is not energetically stable due to steric effects.
This structure becomes even less stable with the addition of two hydrogen
atoms coordinated separately to nitrogen atoms, as shown in Figures a and 14a.
Figure 13
Magnesium adsorption energies at the
edge of graphene with pyrrolic
and pyridinic groups with a (a) P6N-Mg, (b) 2P6N-Mg, (c) P5N-Mg, and (d) 2P5N-Mg functionality.
The sphere legend is as given in Figure .
Adsorption energies of Mg and Ca with increasing number
of pyridine
and pyrrolic functional groups. (a) N-Mg-doped sheet and (b) N-Ca-doped
sheet.Table depicts
the core-level binding energies of the magnesium centers in structures,
as shown in Figures and 13. The goal of this study is to identify
the type of structure in which the Mg could occupy the polyaromatic
ring structure. Using bulk magnesium as the reference structure, the
energy shifts were calculated based on eq . Note that there are significant shifts in
the core-level binding energies for the 4P5N-Mg and the
P5N-Mg structures with corresponding core-level binding
of energies 51.86 and 52.06 eV, respectively. These energies are closest
to the observed peak occurring at higher energies (53.15 eV), as shown
in Figure for N-Mg-Char
but do not seem close enough to explain it. Structures 4P6N-Mg, 3P6N-MgH2, 3P6N-Mg, 2P6N-Mg, and 2P5N-Mg show energies that closely
match the lower experimental binding energy peak (49.85 eV) (see Figure , N-Mg-Char). Of
these, 4P6N-Mg represents the only structure with a favorable
Mg adsorption energy, meaning it is likely responsible for the lower
energy peak seen under the initial analysis.
Table 7
CLBE Shifts
of N-Mg-Model Coordination
in a Graphene Sheet
structures
CLBEs
computed binding energy (eV)
experimental (eV) ref [36]
N-Mg-Structures (Centered Active Sites)
3P6N-MgH2
1.03
50.83
3P5N-Mg
–0.68
49.12
3P6N-Mg
–0.39
49.41
4P5N-Mg
2.06
51.86
4P6N-Mg
–0.36
49.44
4P6N-Mg-H2O
0.02
49.82
49.80
N-Mg-Structures (Edge Active Sites)
2P6N-Mg
–0.11
49.69
P5N-Mg
2.26
52.06
2P5N-Mg
1.34
51.14
However,
it should also be noted that the results from this initial
analysis do not necessarily transfer to the analysis of their use
case. The presence of water is shown in Table and Figure to have both a strong adsorption on magnesium and
a marked effect on its XPS binding energy. As such, these results
should be interpreted with the associated uncertainty under the aqueous
conditions in which they will be applied.
Figure 17
Adsorption structure
and energy of free water onto the 4P6N-Mg functionality.
The sphere legend is as given in Figure , with the addition of red
spheres to represent oxygen.
Adsorption structure
and energy of free water onto the 4P6N-Mg functionality.
The sphere legend is as given in Figure , with the addition of red
spheres to represent oxygen.
Conclusions
In the case of the N-Fe-doped
biochar, we not only see the formation
of large quantified of macro-crystals in the micrometer range size,
but also observed the presence of nanocrystals (less than 5 nm). In
the case of N-Ca-doped biochars, we see the formation of nanometer-size
crystals (between 20 and 30 nm) and Ca-N structures embedded on the
carbonaceous matrix. In the case of the N-Mg biochars, it seems that
most of it is part of the polyaromatic ring structure. According to
the adsorption energies computed, the edge active sites bind metals
less favorably and might have the highest potential of binding to
phosphate ions than the centered active sites. The XPS results clearly
show an interaction between Mg and N in the polyaromatic ring system,
resulting in pronounced Mg 2p core-level binding
energy shifts. DFT-based calculations confirm that the shift in the
Mg 2p core-level binding energy could be due to the
formation of phthalocyanine-like structures and N-Mg complexes formed
on the edges of the graphene sheet. In a nutshell, cellulose char
doped with nitrogen and metals, such as Mg and Ca, could produce phthalocyanine-like
structures; these structures are more stable and highly not favorable
in terms of binding to phosphate ions. However, nitrogenated and metallic
structures at the edges of the carbon network, per the DFT-based calculations,
are less favorable structures, and we hypothesize they have the highest
probability to bind to phosphate ions. The second part of this paper
shows the results of the phosphate adsorption with the characterized
char in this paper.