- Open Access
- Total Downloads : 359
- Authors : B. Kwakye-Awuah, E. Von-Kiti, I. Nkrumah, C. Williams
- Paper ID : IJERTV2IS100222
- Volume & Issue : Volume 02, Issue 10 (October 2013)
- Published (First Online): 16-10-2013
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Towards the Zeolitization of Bauxite: Thermal Behaviour of Gibbsite in High-Alumina- Ghanaian Bauxite
B. Kwakye-Awuap *, E. Von-Kiti1, I. Nkrumap, and C. Williams3
1 Department of Physics (Materials Science Group), KNUST, Kumasi Ghana. Email:
3 Research Centre in Applied Sciences, University of Wolverhampton, WV1 1LY, United Kingdom
Bauxite samples from Awaso mines in Ghana were heated at 100, 300, 500, 800 and 1000 oC and changes in the Al2O3.H2O phase/composition were investigated using X-ray diffraction (XRD), scanning electron microscopy (SEM), energy dispersive X-ray analysis (EDX), Fourier transformed infrared spectroscopy (FTIR) and particle size analysis. The thermal behaviour of
bauxite with time was monitored by Thermogravimetric analysis. The results obtained showed that heating bauxite at 100 oC is enough to obtain the sodalite structure needed for the zeolitization of bauxite. Heating the bauxite at higher temperatures resulted in the loss of the alumina composition as a result of decomposition of metal carbonates to metal oxides and subsequently the formation of a metal aluminosilicate. The particles size decreased with temperature with average particle size distribution ranging from 8 10 µm and 15.5 42 µm
in the un-heated and treated bauxite respectively.
Keywords: Bauxite, thermal, gibbsite, characterization, zeolite
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Bauxite has been found to be major source of aluminium in our industrial world. It contains alumina (Al2O3), silica (SiO2), Iron (Fe2O3) and titanium (TiO2) and balanced water as the major constituents [8, 10, 13]. The major aluminium bearing mineral phases in bauxite include gibbsite, boehmite and diaspore. Other commonly observed phases include, kaolinites, quartz, goethites, kyanites and hematites. The percentage composition of the aluminium bearing phases in bauxite varies with location and history of formation [8, 10, 14]. For example, Mediterranean type bauxite consists mostly of the boehmite whilst thermal action or low-grade metamorphism favours diaspore formation [14]. Alumina refineries extract pure alumina from bauxite by dissolution in hot caustic soda followed by purification and precipitation of alumina powder which is aluminium oxide (Al2O3). During the extraction stage an insoluble sodium aluminosilicate (NaAlSiO3) is produced and precipitated [1, 3, 6, 8, 12, 14]. The precipitated sodium aluminosilicate if modified can be transformed into a more important mineral called zeolite. Zeolites are hydrated crystalline aluminosilicates consisting of
pores and cavities that allow ion exchange and reversible dehydration [4, 5]. The central atom consists of either aluminium or silicon that is bonded with oxygen at the corners of tetrahedra and regularly arranged such that channels form [5]. Zeolites have very wide applications from catalysis to ion exchange, from water softening to odour control, from solar heating to refrigeration as well as antimicrobial agents. There are about 40 naturally occurring zeolites and 160 synthetic ones. Depending on the Si/Al ratio the zeolite is used in a particular application. Whilst natural zeolites are cheaper compared with synthetic ones, synthesized zeolites are purer and have the added advantage of modifying the structural content during synthesis to suit a particular application [4,5]. Nevertheless cost benefit of using natural zeolites in addition to the benefit to the environment far outweighs the benefits of using synthetic zeolites. The study of the thermal transformations of aluminium (oxy) hydroxides has resulted in many contradictory findings. Much of this is probably related to the experimental techniques and conditions used to determine these thermal transformations. To date, little have been studied regarding the potential use of the aluminosilicate. The main aim of this research is to transform low grade bauxite from Awaso Mines in Ghana to high-grade, more useful zeolites that can be used to remove heavy metals such as arsenic, lead, manganese among others in mining wastewater in order for it to be drinkable. To achieve this aim, the bauxite phases need to be investigated when thermally treated. This will help understand the kinetics and dynamics of the zeolitization process and the resultant zeolite type that will be produced.
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Materials and Samples Preparation
The raw bauxite ore was collected from Awaso in the Western region of Ghana. The ore was washed, crushed and milled using a Thomas ball mill machine. The milled sample was passed through a 75 µm sieve to obtain a particle size of at most 75
µm. 75 µm was used because it has been accepted as the boundary between coarse grains and fine grains according to the American Society for Testing and Materials [ASTM E-11-70 (1995)] and British [BS 410 (1986)] standard sieve sizes. 75 µm sieve, grinder, crucibles (Teflon bowls), digital balance and marker were obtained from the Material Engineering laboratory, KNUST. Electric furnace was obtained from the Department of Physics, KNUST.
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Thermal Treatment
10 g portion of the grounded bauxite were heated at 100 oC (A), 300 oC (B), 500 oC
(C) 800 oC (D) and 1000 oC (E). At the
end of the heating time, each sample was quenched in air and allowed to cool overnight. The heated samples after cooling were analyzed by XRD, SEM/EDX, FTIR and particle size analysis. The Table 1 gives a summary of the heat treatments that were performed for the bauxite samples.
Table 1: Summary of thermal treatment procedures for the Awaso bauxite
Samples
Heating time (hr)
Temperature
(
Un-heated
–
–
bauxite
Sample A
1
100
Sample B
2
300
Sample C
3
500
Sample D
3
800
Sample E
3
1000
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Characterization techniques
To confirm the crystal structure and the composition of the synthesized zeolite, it was essential to characterize the zeolite. The X-ray diifraction XRD) pattern of the un-heated and heated bauxite which gives a measure of phase purity were recorded were recorded on Empyrean X-ray powder diffractometer over range of 3o to 70o (PANalytical, UK Ltd, Cambridge). The diffractometer was equipped with a graphite monochromated radiation
source (8987 eV; ). Data processing was carried out using High Score Plus software with a search/match
facility and an ICDD database on a DEC
Microvax Minicomputer interfaced to the diffractometer. The surface morphology of the un-heated and heated bauxite as well as the elemental composition was examined by scanning electron microscopy (SEM) using a Zeiss EVO 50 equipped with energy dispersive X-ray spectrometer (EDX) (Zeiss, UK). Aluminium stubs were prepared prior to the analysis with an adhesive coating. The samples were sprinkled on the stubs. Where necessary, the samples were gold-coated using an
Emscope SC500 Sputter coater to reduce static charging. Electron micrographs were obtained at various magnifications. Particle size distribution per unit volume was analyzed using a Mastersizer long bed analyzer (Malvern Instruments, UK). Samples of the un-heated and heated bauxite were taken for particle size analysis. Before measurements were made, the laser lenses were aligned in a staight line. Settings were set to obscuration value of 0.2. After steady conditions, 0.1 mg of each sample was loaded into an MSX 15 sample handling unit that uses the mechanical action of stirring to ensure that the zeolite particles did not flocculate. Sodium Amalgam was then added to disperse adhering particles. Measurements were then recorded on a computer connected to the instrument. The vibrational properties were investigated by Fourier transformed infrared spectrometry (FTIR). Measurements were done using
-1
100 scans at 4 cm resolution, units of log
(1/R) (absorbance), over the mid-infrared
-1
mid-IR region of 1200-400 cm . An air
background spectrum was collected at the start of the sample analysis. A small sample of each of the un-heated or heated bauxite was centred on the ZnSe plate to ensure that it covered the entire crystal surface, and a pressure clamp was used to apply pressure on the sample. The zeolite samples were analyzed three times for three different samples. A background spectrum was measured before samples were scanned to compensate for atmospheric conditions around the FT-IR instrument. Thermogravimetric analysis (TG DTA) was performed using a Perkin Elmer TGA 7 (Perkin Elmer, UK) with differential thermal analysis. The study was carried out by heating at 10 °C /min heating rate starting from room temperature, with sensitivity of 0.2 mV in atmospheric conditions, and the changes in the sample due to heating were observed.
The temperature range for the analysis was 50 oC to 800 oC.
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Results and discussions
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Characterization results
Results from the EDX analysis (Table 2) showed that bauxite was found to contain high amount of alumina as compared to the other compounds; silicon oxide, titanium oxide and iron oxide.
The alumina/silica ratio for each heating time and temperature with respect to their atomic weight were 49.3:1 in un-heated bauxite, 116:1 for bauxite heated at 100 oC, 152:1 for bauxite heated at 300 C and 17.6:1 at 500 oC. The alumina/silica ratio however, decreased (11.7:1) at 800 oC and further decreased to 15.8:1 at 1000 oC. The associated spectrum of elemental composition is presented in Figure. 1: Results from the XRD analysis indicated changes in the phases of the bauxite at the various heat treatments are shown in
Figure 2. Rietvield analysis (not shown) showed that the main composition of the un-heated bauxite was almost gibbsite (Table 3). After heating the bauxite at 100 oC sodalite phase appeared. Sodalite is a mineral consisting of aluminosilicate framework with SiO4 and AlO4 tetrahedra
present in approximately equal numbers having rings of either four-fold or six-fold. It has a cubic structure with crystallographic parameters:
[10]. The formation of the sodalite structure gives an insight of the zeolitization process since many zeolite structures are based on the formation of sodalite cages. When heated above 100 oC, the sodalite structure was converted to Gibbsite (at 300 oC) and remained same up at 500, 800 and 1000 oC. However, most of the gibbsite peaks disappeared ato
between 24 and 50 oC showing that the bauxite was highly crystalline and that the proportion of absorbed water is very small. A small weight loss of 1 % the temperature range of 30 100 oC can be
attributed to loss of water on the surface of the bauxite. This is the initial step of the decomposition of bauxite which involves the diffusion of protons and the reaction with hydroxyl ions to form water [7, 8, 13, 14, 22]. This process removes the binding forces between subsequent units in the gibbsite structure and causes changes in the chemical composition and density [6, 10, 16, 17]. The more pronounced weight
loss at 330 oC with a mass change of
24.70 % could be attributed to the loss of chemically bound water in the bauxite. The lost chemically bound water could be mainly attributed to the decomposition of gibbsite (Al(OH)3) to alumina (Al2O3) and H2O as shown by the XRD (Figure 2) and FTIR spectra (Figure 6). The loss in peaks in both XRD and FTIR spectra indicate that the lost chemically bound water reacted with sodium, calcium or magnesium oxide to form trisodium, trimagnesium or tricalcium aluminate [9].
The endotherms around 410 and 534 oC could be attributed to the release of CO2 according to the equations (using calcium
for example) [2, 3, 4, 7, 8, 19]:
(R1)
(R2)
The calcium oxide may also have reacted with the alumina and silica as presented by the equation:
(R3)
temperatures above 500 C. This may be
due to the fact that hematite and rutile were the dominant phases (Figure 2). Thermal treatment kinetics graph is presented in Figure 3. Weight loss of
1.26 % of its total weight occurred
Thus the formation of the metal aluminosilicates was responsible for the loss of peaks in both the XRD and FTIR
spectra. SEM images (Figure 4) confirmed the crystal morphology of the bauxite samples heated. The particles are very fine in size (5 20 µm) with irregular shapes.
The white crystal obtained at 500, 800 and 1000 oC showed the dominance of hematite phase at the expense of alumina phase. This is because the alumina phase is likely to have formed the metal aluminosilicate resulting in their disappearance. Such changes in phase/composition confirm in both the un- heated bauxite and the thermally treated bauxite is consistent with previous report [10, 11, 17, 18]. Modal size distribution
obtained for the un-heated bauxite was
22.9 µm (Figure 5). On heating the bauxite to 100 oC the modal distribution was reduced to 26. 3 µm. This is likely to be attributed to the formation of the sodalite structure which opened the structure as result of the formation of pores or voids in the structure. When heated to 300 oC the mode decreased to 17. 4 µm. This may be an indication of the loss of the chemically bound water in the bauxite. The mode increased to 19.9 µm on heating the bauxite to 300 oC. This is attributed to the formation of the metal aluminosilicate. Heating the bauxite at 800 and 1000 oC resulted in a in the modal distribution of
19.9 and 10.2 µm respectively. FIG. VI(a-
f) shows the FTIR spectrum of un-heated bauxite and bauxite that of bauxite heated at 100 oC, 300 oC, 500 oC, 800 oC and 1000 oC. For sample of the un-heated bauxite, peaks occurred at 3618, 3524, 3452, 3392, 3370, 1017, 966, 730, 662, 555, 477, 448 and 407 cm-1. The peaks at 3618, 3524, 3452, 3392, 3370 cm-1 is assigned to the OH stretching of gibbsite [3, 10, 11, 14, 15]. These peaks disappeared on heating the bauxite from 100 oC. The OH bending peak at 1017 cm-
1 which is the strongest in the un-heated bauxite broadened and shifted to a lower wavenumber (939 cm-1) at 100 oC, disappeared at 300, 500 and 800 oC and re- appeared (920 cm-1) with moderate strength at 1000 oC. The peak at 939 cm-1
may be may be attributed to the formation sodalite structure at 100 oC [11, 12, 18, 20, 21]. The disappearance of the peaks at higher temperatures ) corresponds with the endotherms around 509 and 534 oC in the DTA pattern [10, 13]. The metallic vibrations which are assigned to peaks at 1650 cm-1 was not observed.
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Bauxite tailings from Awaso mines in Ghana has been characterized and thermally investigated at different temperatures. Heating the bauxite at 100 oC was enough for the sodalite structure
which is the basic structure of most zeolites. Heating at higher temperatures ) resulted in the loss of peaks in both XRD and FTIR spectra and a resulting endotherms in the TG-DTA curve. Heating the bauxite at higher temperatures resulted in the loss of the alumina composition as a result of decomposition of metal carbonates to metal oxides and subsequently the formation of a metal aluminosilicate. The particles size decreased with temperature with average particle size distribution ranging from 8 10 µm to 15.5 42 µm in the un-heated an treated bauxite respectively.
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Figure 1: EDX spectrum of bauxite showing the major elements in the bauxite
Table 2: Elemental composition of bauxite and that of bauxite heated at (a): 100 oC, (b): 300 oC,
(c) 500Temperature ( oC) Elemental composition (%)
oC, (d): 800 oC and (E): |
1000 |
oC |
|||||
Na2O |
CaO |
L.O.I. |
|||||
Un-heated |
69.30 |
1.41 |
1.67 |
3.42 |
1.03 |
0.08 |
23.09 |
100 oC |
69.59 |
0.60 |
0.53 |
4.183 |
1.01 |
0.09 |
24.00 |
300 oC |
69.96 |
0.46 |
1.14 |
3.22 |
1.02 |
0.08 |
24.12 |
500 oC |
65.28 |
0.37 |
0.38 |
2.85 |
1.02 |
0.08 |
30.02 |
800 oC |
62.06 |
0.53 |
1.10 |
5.63 |
1.01 |
0.09 |
29.58 |
1000 oC |
59.97 |
3.79 |
0.71 |
4.30 |
1.03 |
0.06 |
30.14 |
Gibbsite
Sodalite
Figure 2: XRD spectrum of (a): unheated bauxite and for bauxite heated at (b): 100 oC, (c): 300 oC, (d): 500 oC (e): 800 oC and (f): 1000 oC
Figure 3: TGA with DTA curves of bauxite within the temperature range of 24 oC and 800 oC
Figure 4: Scanning electron micrograph of (a): unheated bauxite and for bauxite heated at (b): 100
oC, (c): 300 oC, (d): 500 oC, (e): 800 oC and (f): 1000 oC
Figure 5: Particle size distribution of bauxite (a) and bauxite heated at (b) 100 oC, (c): 300 oC, (d): 500 oC, (e): 800 oC and (f): 1000 oC.
240
220
200
Transmission (AU)
Transmission (AU)
180
160
140
120
100
80
60
4000
3500
3000
2500
2000
1500
1000
500
Wavenumber (cm-1)
Figure 6: FTIR spectrum of (a): un-heated bauxite and for bauxite heated at (b): 100 oC, (c): 300 oC, (d): 500 oC, (e): 800 oC and (f): 1000 oC.