Published at : 28 Jun 2023
Volume : IJtech
Vol 14, No 4 (2023)
DOI : https://doi.org/10.14716/ijtech.v14i4.4960
Gyan Prameswara | Mineral-Chemical Engineering Department, Politeknik ATI Makassar, Jl. Sunu No. 220, Makassar, 90211, Indonesia |
Iga Trisnawati | Polytechnic Institute of Nuclear Technology, National Research and Innovation Agency, Yogyakarta, 55281 Indonesia |
Tri Handini | Research Center for Mining Technology, BRIN, Jl. Babarsari, Tambak Bayan, Caturtunggal, Kec. Depok, Kabupaten Sleman, Daerah Istimewa Yogyakarta, 55281, Indonesia |
Herry Poernomo | Research Center for Mining Technology, BRIN, Jl. Babarsari, Tambak Bayan, Caturtunggal, Kec. Depok, Kabupaten Sleman, Daerah Istimewa Yogyakarta, 55281, Indonesia |
Panut Mulyono | 1. Department of Chemical Engineering (Sustainable Mineral Processing Research Group), Faculty Engineering, Universitas Gadjah Mada, Jl. Grafika No. 2, Kampus UGM, Yogyakarta, 55281, Indonesia, 2. Unc |
Agus Prasetya | 1. Department of Chemical Engineering (Sustainable Mineral Processing Research Group), Faculty Engineering, Universitas Gadjah Mada, Jl. Grafika No. 2, Kampus UGM, Yogyakarta, 55281, Indonesia, 2. Unc |
Himawan Tri Murti Bayu Petrus | 1. Department of Chemical Engineering (Sustainable Mineral Processing Research Group), Faculty Engineering, Universitas Gadjah Mada, Jl. Grafika No. 2, Kampus UGM, Yogyakarta, 55281, Indonesia, 2. Unc |
Rare earth metals are important today, especially
for heavy rare earth elements (HREEs). Dy and Yb, included in the HREE group,
are widely used for permanent magnets and sensors. On the other hand,
accumulated solid waste of zircon tailings is an environmental issue in mineral
processing. Valuable minerals such as rare earth elements (REEs) also remain in
the tailings. This study aims to determine the optimum conditions of the
experimental parameters and obtain an appropriate kinetic model. The leaching
process was carried out in a flat bottom three-neck flask equipped with a
thermometer and reflux condenser. Observation of the effect of process conditions
on recovery and kinetics analysis obtained satisfactory results. In this study,
Dy and Yb leaching from solid REE-hydroxide using HCl solution afforded a total
of 61.71% and 74.55% recovery of Dy and Yb, respectively, at operating
conditions of 1 M HCl, 60°C, 10 g/100 mL (solid-to-liquid ratio), at
60 min (leaching duration), and 150 rpm (stirring speed). It was found that the
leaching process was controlled by chemical reactions with apparent activation
energies of 31.68 kJ/mol and 11.95 kJ/mol for Dy and Yb leaching, respectively.
Dysprosium; Kinetics analysis; Leaching; Ytterbium; Zircon tailings
The need for clean processes is increasing as industrial development progressively turns green. Among the elements used to support the green industry are rare earth elements (REEs). The need for REEs is increasing while primary sources such as bastnaesite, xenotime, and monazite mining are decreasing. REEs are relatively abundant in the earth's crust but not in large concentrations compared to other minerals. REE-oxide production in 2019 and 2020 was 220,000 tones and 240,000 tones, respectively, while the worldwide REEs reserve reached 120,000,000 tones (U.S. Geological Survey, 2021). Developments in optimally processing REEs, and efforts to discover alternative secondary sources, must be encouraged.
Dysprosium (Dy) and
ytterbium (Yb) are two elements found in the lanthanide group. Dy and Yb are
classified as heavy rare earth elements (HREEs) based on their atomic numbers.
These metals are included in the list of critical metals and are among the most
widely used in the energy sector (Guyonnet et al., 2015). Dy metal
is used in permanent magnets, phosphors, and metal halide lamps, while Yb is
widely used for optical lenses, pressure sensors, and lasers (Lucas et al.,
2014). The need for Dy and Yb metals in the future is
predicted to increase (Supriadi et al., 2023).
REEs demand is
predicted to increase by 2035 to reach around 374,000 metric tons, with the
most used as permanent magnet products at approximately 80,000 metric tons (Yang et al., 2017). In
contrast to Dy, Yb has begun to be widely used for memory devices and as a
catalyst in the industry to replace other catalysts categorized as too toxic
and polluting.
Currently, the primary
sources of REEs are the minerals bastnaesite, monazite, and xenotime.
Bastnaesite is the primary source, with REEs content of approximately 57% (Boulanger, Bazin, and Turgeon,
2019). Monazite and xenotime are often found in minerals
bearing cassiterite and zircon (Trisnawati et al., 2022). The
presence of this mineral is usually concentrated in the by-products of
cassiterite/zircon processing (Gediga et al., 2019). REEs
processing from zircon by-products solve solid waste accumulation and add value
to the zircon beneficiation process.
Several studies have
observed the REEs leaching kinetics from different material sources. The REEs
leaching mechanism is usually influenced by the ore properties, mass transfer
behavior, and reaction kinetics. In general, three models can describe the leaching
process: homogeneous, shrinking core, and grain models (Petrus et al., 2022; Wanta et al.,
2022; Liu et al., 2012). Shrinking-core models can be used to
describe the leaching process for systems containing non-porous solid particles
and reactant fluids.
Research into REEs
leaching has been conducted extensively. Extraction was carried out using
various secondary REE sources. Stopic and Friedrich (2016) researched
the kinetics of yttrium leaching from ceramic waste dust. Under optimal
operating conditions, a yttrium dissolution of 98.6% was achieved. Yttrium
dissolution can be described using a kinetic model based on a chemical reaction
as the limiting step. The observed activation energy was 31.2 kJ/mol. Obuz et al.
(2018) studied the leaching kinetics of REEs in complex
ores. The reaction constants for the solutions of Ce, La, Nd, and Pr were
determined. Research on REE recovery from secondary sources from Indonesia has
also been carried out. Rosita et al. (2019) observed the yttrium
recovery from coal fly ash (CFA) using sulfuric acid, while Prihutami et al.
(2020) also recovered yttrium from CFA using citric acid
with the highest recovery of 83.35%.
This study aims to
investigate the leaching of Dy and Yb from secondary sources (zircon tailings)
and determine optimal conditions for HREE leaching using HCl from
REE-hydroxide. The study also aims to analyze the kinetics of the leaching
process and obtain recovery data, such as a kinetic model and its activation energy
value.
2.1. Roasting
The raw
material is zircon tailings from Monokem Surya, Ltd., mined and processed in
Bangka Island and Central Kalimantan. The zircon tailings sample contained
monazite and xenotime minerals. The Dy and Yb contents in the zircon tailings
sample were 1.45% and 1.29%, respectively (Prameswara et
al., 2020; Trisnawati et al., 2020).
REE-hydroxide was prepared by reacting zircon tailings with NaOH flakes at a
temperature of 450°C for 3 hours and a 1:1 wt ratio of zircon tailings and NaOH
flakes. The roasting process was carried out in a muffle furnace. Our previous
work has thoroughly described the REE-hydroxide preparation stage, sample
characterization, mineral composition analysis, and elemental analysis (Prameswara
et al., 2020).
2.2. Leaching experiment
The leaching process was carried out in
a flat bottom three-neck flask equipped with a thermometer, reflux condenser,
and hot plate with magnetic stirrer Thermo Scientific Cimarec. The experimental
schematic illustration is presented in Figure 1. Leaching was performed under
several operating conditions: temperature, solid-to-liquid ratio (S/L), and
acid concentration. A total of 5 g of REE-hydroxide with a particle size of 44
µm was leached for each data collection. Analytical grade HCl (37%, Merck &
Co., Inc.) was used. The leaching process was carried out in 0.125–2 M HCl
concentration, temperatures ranging from 30–110°C, and a solid-to-liquid (S/L)
ratio of 5–25 g/100 mL, a stirring speed of 150 rpm. Based on several studies,
higher stirring speed does not significantly affect REE recovery (Kurnia et al., 2016). Elemental analyses of Dy and Yb were performed on
the leaching residue. Leaching recovery was calculated using Equation 1.
where x0 is the REE concentration in the feed
multiplied by the mass of the feed (%), and Xi is the REE
concentration in the residue multiplied by the mass of the residue (%).
Elemental analysis was performed using an X-ray fluorescence spectrometer
(Rigaku NEX QC, S/N QC1202) on the solid residue. Residue characterization at
the optimum leaching process was carried out using Rigaku Miniflex 600 Benchtop
X-ray diffractometer (XRD). The leaching process was repeated twice to ensure
an acceptable measurement error (less than 10%).
2.3. Kinetic analysis
Kinetic analysis was performed using a shrinking-core model. The kinetic
models to be tested are the chemical reaction limiting step, diffusion through
the ash layer limiting step, and the diffusion model developed by Zhuravlev,
Leshokin, and Templeman (ZLT). These three models are expressed in Equations
(2)–(4), respectively.
where x is the percentage leaching recovery divided by 100. kc,
kd, and kz are the rate constant for the chemical reactions
control kinetics model, diffusion through the ash layer kinetic model, and ZLT
kinetic model, respectively. While t (min) is the leaching duration. The
kinetic model selected to determine the kinetic parameters (frequency factor
and activation energy) is the model that exhibits the highest R-squared value.
The kinetic parameters were evaluated using the Arrhenius equation (Equations 5
and 6).
where k
is the rate constant (kc/kd/kz), A is the frequency factor, Ea
is the activation energy (kJ/mol), R = 8.314462 (J/(mol·K)), and T
is the leaching temperature (K). The activation energy was obtained from the
slope of the curve 1000/T vs. ln k, and the frequency factor was obtained from
the intercept.
Figure
1 Experiment scheme
3.1. Roasting
At this stage, REE-phosphate and
zirconium silicate contained in monazite and xenotime naturally react with the
NaOH flakes. As mentioned in da-Silva, Dutra, and Afonso (2012), the typical
reaction is as follows (Equations 7-9). Based on our previous research, there
was a decrease in the zircon concentration in the leaching residue. This
indicates that zircon also reacted in the alkaline fusion process. The
phosphate concentration is also reduced, indicating that most of the phosphate
that binds to REE reacts with NaOH to produce Na3PO4 (Prameswara et
al., 2020; Trisnawati et al., 2020).
Separating the major and unwanted elements from the final product appears
effective during the alkaline fusion process. This successful separation also
optimizes the REEs leaching process later.
3.2. Effect of operating conditions on
Dy and Yb leaching recovery
Observations
were made on the effect of the leaching operating conditions on Dy and Yb
recovery. As shown in Figure 2a, the recovery for Dy and Yb increased
drastically in the HCl concentration range of 0.125–1 M. The recoveries for Dy
and Yb reached 47.38% and 72.74%, respectively. The recoveries did not show any
increase in HCl concentrations above 1 M. Dy and Yb recovery reach plateau
shows that the limiting effects have been reached. Increasing
the HCl concentration would only increase the dissolution of unwanted elements,
such as Si, P, and Al (Walawalkar,
Nichol, and Azimi, 2016).
Tabel 1 Thermodynamic parameter for leaching Dy(OH)3 and Yb(OH)3
The effect of temperature on the recovery of Dy and Yb is shown in Figure 2b. Increasing the temperature increased the recovery of Dy and Yb. The higher the temperature, the higher the kinetic energy of the reactants, causing the REE-hydroxide solid to collide and react faster with the HCl solution. The increase in recovery occurred in the temperature range of 30–60°C. Furthermore, there was no increase in the recovery of Dy and Yb. The increase in the leaching temperature did not increase the Dy and Yb recoveries. Temperatures above 90°C decrease REE leaching recovery by causing the solvent to evaporate, reducing the amount of solvent needed for the reaction. Additionally, high temperatures generate new issues in the reaction due to the solvent's boiling point. The exothermic nature of the REE-hydroxide leaching reaction with HCl is indicated by a negative value of enthalpy obtained from the database and a negative value of Gibbs free energy indicating the reaction can occur spontaneously. The low activation energy value (section 3.3) shows that the rate of heat generated during the reaction is fast.
Figure
2c indicates that an increase in recovery occurred at a solid-to-liquid (S/L)
ratio of 10 g/100 mL. Subsequently, there was a decrease in the recovery of Dy.
However, Yb recovery remained at 74.55% until the S/L ratio was 20 g/100 mL.
Meanwhile, at an S/L ratio of 10 g/100 mL, Dy recovery reached 59.56% and then
slowly decreased as the S/L ratio increased. Yb recovery is higher than Dy
recovery at the same operating condition. This is because the solubility of Yb
is higher than the solubility of Dy. In general, the solubility increases with
increasing atomic number (Kim
et al., 2018).
The decrease in recovery occurs because the limit for REEs solubility has been
reached, but other major elements continue to dissolve. The increase in the S/L
ratio will lead to an increase in the density of the solution, which will then
decrease the mobility of the Cl- ion. Therefore, it will be slowing down the
rate of REE3+ transfer into the solution body. Thus, the product
contains higher concentrations of major elements such as P, Zr, Si, and Al at a
higher S/L ratio (Dupont
and Binnemans, 2015).
Therefore, an S/L ratio of 10g/100 mL was chosen as the optimum S/L ratio.
Figure 2 Effect
of leaching operating conditions on Dy and Yb recoveries: (a) effect of HCl
concentration (80°C, S/L=10 g/100 mL, 150 rpm, and 60 min); (b) effect of
temperature (2 M HCl, S/L=10 g/100 mL, 150 rpm, and 60 min); and (c) effect of
S/L ratio (2 M HCl, 80°C, 150 rpm, and 60 min)
The components in the leaching residues were analyzed using XRD to determine the components contained. The results of the XRD analysis are presented in Figure 3. ZrSiO4 and SiO2 represent the initial content of the tailings. The REE concentration is not significantly different from that of the undesirable elements. These data accurately indicate that most of the REEs are in the dissolved form in REE-Cl3.
Elemental
analysis was performed on solid product samples (residual leaching) under
optimum operating conditions. Figure 4 shows the concentrations for some major
impurity elements and HREEs (Dy and Yb) in the solid product. Major elements
also appear to be much dissolved in the leaching process under optimum leaching
conditions because the solubility of P, Zr, Si, and Al in HCl is higher than Dy
and Yb.
Figure
3 XRD analysis of leaching feed and residue (solid
product) at optimum operating conditions (1 M HCl, 60°C, 10 g/100
mL, and 60 min)
Figure
4 Elemental analysis on the solid product at optimum
operating conditions (1 M HCl, 60°C, 10 g/100 mL, and 60 min)
3.3. Kinetics
analysis of Dy and Yb leaching process
Kinetic analysis was performed for the Dy and Yb leaching processes at
a temperature of 80–100°C. A shrinking-core model was used to
describe the leaching process. The limiting step or control in this leaching
kinetic model describes the most dominant process that occurs. Chemical
reaction control, ash layer diffusion control, and ZLT kinetics models
evaluated the REEs leaching recovery. The kinetics analysis was performed for a
leaching duration of 0–7.5 minutes because there was no significant recovery
increase above 7.5 minutes. Figures 5a and 5b show that the recovery of Dy and
Yb constantly increased up to 7.5 min and then reached a plateau with a longer
leaching duration.
Figure 5 Dy (a) and Yb (b) Recovery (2 M HCl, S/L =10 g/100 mL, and 150 rpm)
The selection of the
most suitable kinetic model was based on the highest R-square value. In
leaching Dy from solid REE-hydroxide using an HCl solution, the highest
R-square value was found in the chemical reaction limiting step kinetics model
(Table 2). As much
as 0.97485, 0.99851, and 0.90976 at 80°C, 90°C, and 100°C,
respectively. In the kinetics analysis using the chemical reaction limiting
step model, the value of the rate constant (kc) for the Dy leaching process was
0.024 min-1, 0.034 min-1,
and 0.043 min-1 for 80, 90, and 100°C, respectively.
For Yb leaching, the kinetics model that showed the highest R-square value
was the chemical reaction limiting step kinetics model. The R-squared values
for 80°C, 90°C, and 100°C were 0.94964, 0.97875, and 0.98763, respectively. The rate constant (kc)
values were 0.040 min-1, 0.046 min-1,
and 0.050 min-1 for 80, 90, and 100°C.
Stopic and Friedrich (2016) have also reported that
the chemical reaction limiting step kinetics model is more suitable than the
diffusion-based kinetics model for the HREE (yttrium) leaching process using an
HCl solution. Kim et al. (2014) found that
REEs leaching recovery followed a chemical reaction limiting step kinetics
model in the first 20 minutes, likely due to the temperature's significant
effect. Linearisation was satisfactory at all temperatures studied (60, 80, and
100ºC), with a straight line starting from the origin at each temperature
(intercept = 0).
The leaching kinetic parameters Dy and Yb, such as the activation energy
(Ea), were determined graphically using the Arrhenius plot in
Figures 6 and 7. The slope value of the Arrhenius graph is the value of -EA/R,
where R is the gas constant (R = 8.314472 J.mol-1.K-1).
The activation energy values of leaching Dy and Yb were 31.68 kJ/mol and 11.95
kJ/mol, respectively.
Table 2 Selection of
the leaching kinetic model listed
|
|
Chemical
reaction limiting step |
Ash
layer diffusion limiting step |
ZLT | ||||||
|
|
80°C |
90°C |
100°C |
80°C |
90°C |
100°C |
80°C |
90°C |
100°C |
Dy
leaching |
R2 |
0.9749 |
0.9985 |
0.9098 |
0.8844 |
0.9511 |
0.9501 |
0.8513 |
0.9053 |
0.9646 |
k |
0.0241 |
0.0341 |
0.043 |
0.01 |
0.0179 |
0.0256 |
0.0054 |
0.0114 |
0.0175 | |
Yb
leaching |
R2 |
0.9496 |
0.9788 |
0.9876 |
0.8873 |
0.9292 |
0.9633 |
0.8748 |
0.9028 |
0.9291 |
k |
0.0405 |
0.0463 |
0.0504 |
0.026 |
0.0313 |
0.0356 |
0.0202 |
0.0261 |
0.0316 |
Figure 6 Kinetics analysis on Dy
leaching, chemical reaction limiting kinetic model vs time (left) and Arrhenius
plot using k data on chemical reaction limiting kinetic model (right)
Figure 7 Kinetics analysis on Yb leaching, chemical
reaction limiting kinetic model vs time (left) and Arrhenius plot using k data
on chemical reaction limiting kinetic model (right)
The activation energy value
of Dy is greater than that of Yb, indicating that Dy is more difficult to
dissolve (Meshram,
Pandey, and Mankhand, 2016). Activation energy is the minimum energy required for a reaction to
occur. When molecules collide, kinetic energy can stretch and break the bonds
that cause reactions to occur.
The higher the activation
energy, the stronger the bond between molecules, the more complex the reaction,
and the smaller the recovery obtained.
Several operating conditions such as HCl concentration,
leaching temperature, and the S/L ratio of the leaching process were observed.
Leaching kinetics were also carried out to obtain the kinetic parameters for
the Dy and Yb leaching processes from REE-hydroxide. The optimal conditions for
leaching occurred at 1 M, 60ºC, and 10 g/100 mL HCl with a fixed process
condition of 150 rpm and a leaching duration of 60 min. The Dy and Yb
recoveries were 61.71% and 74.55%, respectively, under these operating
conditions. The leaching process was found to follow a chemical reaction as a
limiting step. The apparent activation energy (Ea) obtained from the
kinetics model was 31.68 kJ/mol and 11.95 kJ/mol for Dy and Yb, respectively.
The
authors are grateful to Universitas Gadjah Mada for supporting this research. This study was funded by RIIM (Riset dan Inovasi untuk
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