20
This may be the author’s version of a work that was submitted/accepted for publication in the following source: Liu, Haibo, Chen, Tianhu, Zou, Xuehua, Qing, Chengsong, & Frost, Ray (2013) Thermal treatment of natural goethite: Thermal transformation and physi- cal properties. Thermochimica Acta, 568, pp. 115-121. This file was downloaded from: https://eprints.qut.edu.au/61772/ c Consult author(s) regarding copyright matters This work is covered by copyright. Unless the document is being made available under a Creative Commons Licence, you must assume that re-use is limited to personal use and that permission from the copyright owner must be obtained for all other uses. If the docu- ment is available under a Creative Commons License (or other specified license) then refer to the Licence for details of permitted re-use. It is a condition of access that users recog- nise and abide by the legal requirements associated with these rights. If you believe that this work infringes copyright please provide details by email to [email protected] License: Creative Commons: Attribution-Noncommercial-No Derivative Works 2.5 Notice: Please note that this document may not be the Version of Record (i.e. published version) of the work. Author manuscript versions (as Sub- mitted for peer review or as Accepted for publication after peer review) can be identified by an absence of publisher branding and/or typeset appear- ance. If there is any doubt, please refer to the published source. https://doi.org/10.1016/j.tca.2013.06.027

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Page 1: c Consult author(s) regarding copyright matters License · 2 29 30 1. Introduction 31 Goethite, -FeOOH, is widely distributed, occurs in rocks, soils and throughout the 32 global

This may be the author’s version of a work that was submitted/acceptedfor publication in the following source:

Liu, Haibo, Chen, Tianhu, Zou, Xuehua, Qing, Chengsong, & Frost, Ray(2013)Thermal treatment of natural goethite: Thermal transformation and physi-cal properties.Thermochimica Acta, 568, pp. 115-121.

This file was downloaded from: https://eprints.qut.edu.au/61772/

c© Consult author(s) regarding copyright matters

This work is covered by copyright. Unless the document is being made available under aCreative Commons Licence, you must assume that re-use is limited to personal use andthat permission from the copyright owner must be obtained for all other uses. If the docu-ment is available under a Creative Commons License (or other specified license) then referto the Licence for details of permitted re-use. It is a condition of access that users recog-nise and abide by the legal requirements associated with these rights. If you believe thatthis work infringes copyright please provide details by email to [email protected]

License: Creative Commons: Attribution-Noncommercial-No DerivativeWorks 2.5

Notice: Please note that this document may not be the Version of Record(i.e. published version) of the work. Author manuscript versions (as Sub-mitted for peer review or as Accepted for publication after peer review) canbe identified by an absence of publisher branding and/or typeset appear-ance. If there is any doubt, please refer to the published source.

https://doi.org/10.1016/j.tca.2013.06.027

Page 2: c Consult author(s) regarding copyright matters License · 2 29 30 1. Introduction 31 Goethite, -FeOOH, is widely distributed, occurs in rocks, soils and throughout the 32 global

1

Thermal treatment of natural goethite: thermal transformation and 1

physical properties 2

Haibo Liua,b, Tianhu Chena,, Xuehua Zoua, Chengsong Qinga, Ray L. Frost b 3

4

aLaboratory for Nanomineralogy and Environmental Material, School of Resources & 5

Environmental Engineering, Hefei University of Technology, China 6

7 bSchool of Chemistry, Physics and Mechanical Engineering, Science and Engineering 8

Faculty, Queensland University of Technology, Australia 9

10

Abstract: XRD (X-ray diffraction), XRF (X-ray fluorescence), TG (Thermogravimetry), 11

FT-IES (Fourier transform infrared emission spectroscopy), FESEM (Field emission 12

scanning electron microscope), TEM (Transmission electron microscope) and nitrogen-13

adsorption-desorption analysis were used to characterize the composition and thermal 14

evolution of the structure of natural goethite. The in-situ FT-IES demonstrated the start 15

temperature (250 oC) of the transformation of natural goethite to hematite and the 16

thermodynamic stability of protohematite between 250 and 600 oC. The heated products 17

showed a topotactic relationship to the original mineral based on SEM analysis. Finally, the 18

nitrogen-adsorption-desorption isotherm provided the variation of surface area and pore size 19

distribution as a function of temperature. The surface area displayed a remarkable increase 20

up to 350 oC, and then decreased above this temperature. The significant increase in surface 21

area was attributed to the formation of regularly arranged slit-shaped micropores running 22

parallel to elongated direction of hematite microcrystal. The main pore size varied from 0.99 23

nm to 3.5 nm when heating temperature increases from 300 to 400 oC. The hematite derived 24

from heating goethite possesses high surface area and favors the possible application of 25

hematite as an adsorbent as well as catalyst carrier. 26

Keywords: Goethite, Thermogravimetry, Hematite, Specific surface area, topotactic 27

relationship 28

Corresponding author. Tel.: +86 13956099615, +86 0551 2903990. E-mail address: [email protected]; [email protected] Author to whom correspondence should be addressed ([email protected]) P +61 7 3138 2407 F: +61 7 3138 1804

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29

1. Introduction 30

Goethite, -FeOOH, is widely distributed, occurs in rocks, soils and throughout the 31

global ecosystem, and has the diaspore structure which is based on hexagonal close packing 32

[1]. Generally, goethite is an oxidation, decomposition, weathering and hydrolyzation 33

product of pyrite, siderite, magnetite and Fe-containing silicates [1]. Although goethite 34

displays a range of shapes and sizes, the most basic morphology is acicular with the length 35

varying from tens of nanometer to several microns. Goethite is one of the most abundant and 36

thermodynamically stable Fe-containing crystalline compounds, therefore, goethite is the 37

first oxide to form or is the end member of many transformations [1-3] in which the 38

transformation of goethite to hematite generally occurs after heating between 180 and 300 oC 39

[4, 5]. 40

In past decades, many studies have been carried out to investigate the adsorption 41

capability of hematite for organic molecules including protein [6], methanol [7], C4-42

dicarboxylic (maleic, fumaric, and succinic acids) [8] and inorganic compounds contaniing 43

heavy metals [9-13], metalloids [14-16], and radionuclides [17-19]. A number of studies 44

have reported [20, 21] that ferric oxide surfaces are hydrated upon exposure to water. The 45

report of Jones et al. [22] shows that the most stable of the hydrated plane of hematite is the 46

O-terminated plane, however, the extremely unstable plane is the Fe-terminated plane in the 47

presence of excess water (>=67% coverage). As for organic compounds, more attention is 48

paid to the adsorption between natural waters and soils. Ishikawa et al. [7] investigated the 49

adsorption of CH3OH, CCl4, C6H6 and C6H5Cl on well-defined slit-shaped hematite. The 50

result indicated that the surface Fe-OH groups function as the adsorption sites. As for 51

inorganic compounds, both synthetic and natural hematite surfaces have been studied in 52

detail with respect to adsorption of contaminants [7]. It has been reported that iron-oxide-53

coated sand was utilized as a filling material for a fixed bed configuration for simultaneous 54

filtration of particular matter and adsorption of dissolved metals [9]. These space-filling 55

materials displayed great adsorption ability in removing uncomplexed and ammonia-56

complexed cationic metals (Cu, Cd, Pb, Ni, Zn), as well as some oxyanionic metalloid 57

(SeO32-, AsO3

-). Commercially prepared hematite nanoparticles have been employed for 58

adsorption of bivalent metals (Pb, Cu, Zn, Cd) and the results proved that nanohematite 59

could be applicable in water treatment technology for removing metals [23]. Besides, the 60

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adsorption of hematite to phosphate, arsenic, sulfate and radionuclide (uranium, nickel) has 61

been researched in details [14, 18, 19, 24, 25]. The effect of relative parameters such as 62

temperature, different iron oxides, pH and materials preparation methods on adsorption of 63

contaminants also has been reported in previous reports [10-13, 15-17, 23, 26]. Furthermore, 64

as is well-known, nanomaterials possess some advantages over their bulk counterparts, such 65

as an increased specific surface area and high reactivity, which makes them more effective 66

and feasible for engineering application. Thereby, Zhang et al. [27] and Zeng et al. [28] 67

investigated the effect of nanoscale size on the adsorption ability of hematite. A natural 68

goethite was used as a catalysts carrier supporting nickel catalytic cracking of biomass tar 69

and displays a good catalytic reactivity [29]. 70

As mentioned above, goethite distributes widely and generally displays acicular 71

morphology with the length varying from tens of nanometer to several microns. It has been 72

demonstrated hematite could be used in water treatment as well being used as a catalyst 73

carrier. Nanohematite possesses more advantages in adsorption ability. Therefore, in this 74

present study, thermal treatment of natural goethite is carried out and physical properties of 75

thermally treated natural goethite (hematite) is investigated using modern analytical 76

techniques, such as FESEM, XRD, specific surface area and pore distribution analyzer, etc. 77

The objective is to characterize the natural goethite before and after thermal treatment, to 78

investigate the physical properties of hematite derived from goethite and to find a kind of 79

low cost material for possible application in water treatment and catalysis. 80

1. Experimental 81

2.1 Materials 82

Natural goethite (-FeOOH) was collected from Tongling city, Anhui province, China. 83

The natural goethite was crushed and sieved into a desired particle size. The obtained 84

goethite particles were annealed at different temperature for 2h (100, 150, 200, 250, 300, 350, 85

400, 500, 600, 700, 800 oC) and retained for further characterization. The goethite labeled as 86

G25 and the heated goethite labeled as G100, where G denotes goethite and the number 87

denotes the thermal treatment temperature. 88

2.2 Characterizations 89

X-ray diffraction (XRD) patterns were recorded using Cu Kα radiation (λ = 1.5406 Å) 90

on a Philips PANalytical XPert Pro muti purpose diffractometer. The tube voltage was 40kV 91

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and the current, 40mA. All XRD diffraction patterns were taken in the range of 15-75o at a 92

scan speed of 2o min−1 with 0.5o divergence slit size. Phase identification was carried out by 93

comparison with those included in the Inorganic Crystal Structure Database (ICSD). 94

Chemical composition was measured on an X-ray fluorescence (XRF) spectrometer 95

(Shimadzu XRF-1800) with Rh radiation. 96

Thermogravimetry (TG) was measured on TA instruments thermogravimetric analyser 97

(TGA, Q500). High-purity nitrogen was used as purging gas with a flowing rate for balance 98

(40 mL/min) and a flowing rate for sample (60 mL/min). The natural goethite was loaded 99

onto platinum sample pan and heated to 1000 oC at a high resolution heating rate of 6 oC/min, 100

where the heating rate was dynamically and continuously modified in response to the 101

changes in the rate of sample’s mass loss, termed as controlled rate thermal analysis (CRTA). 102

Fourier transform infrared emission spectroscopy (FT-IES) was carried out on a Nicolet 103

spectrometer equipped with a TGS detector, which was modified by replacing the IR source 104

with an emission cell. A thin layer (approximately 0.2 microns) on a platinum surface with 6 105

mm diameter and held in an inert atmosphere within a nitrogen-purged cell during heating. 106

The spectra was acquired by co-addition of 1024 scans at the temperature of 150, 200, 512 107

scans at 250, 256 scans at 300, 350, and 128 scans at temperature from 400 to 800 oC. 108

109

Transmission electron microscope (TEM) measurements were performed on JEM-1010. 110

The samples were mixed with alcohol and deposited on a Cu grid. Images of the 111

microstructure were acquired using an analytical electron microscope. 112

113

Field emission scanning electron microscope (FESEM) measurements were performed 114

on JEOL JSM-7001F with an energy dispersive x-ray detector. All samples were coated gold 115

by spraying before analysis. 116

13-point BET-nitrogen isotherms were used to quantify changes in the specific surface 117

area. All samples were degassed at 110 oC for 12 h before analysis were conducted. The 118

multi-point BET surface area of each sample was measured at atmospheric pressure using 119

TriStar Ⅱ 3020 Surface Area and Pore Size Analyzer. The adsorption isotherms achieved a 120

p/po range of 0.009-0.25. Pore size distribution was evaluated by BJH desorption pore 121

distribution report between 1.7 nm and 20 nm. 122

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123

2. Results and discussion 124

3.1 XRD and XRF 125

Fig. 1 displays the XRD patterns of goethite and thermally treated goethite at different 126

temperatures. These peaks are observed in the XRD pattern of G25 and identified as goethite 127

when compared with the standard pattern (ICSD (96-900-2159)). All the peak intensity 128

shows a small decrease with the increasing temperatures, and then disappears as the 129

temperature reaches 300 oC and the peaks were replaced by several new reflections. The new 130

reflections with low intensity appear after heating at 250 oC and indentified as hematite after 131

comparison with the pattern of ICSD (96-900-0140). It indicates the transformation of 132

goethite to hematite basically occurs below 250 oC with a slow transformation rate. The 133

result is consistent with that reported previously [30, 31]. The characteristic reflection 134

intensity of hematite has a dramatic increase with the increased temperature because of the 135

increase of crystal size and the improvement of crystallinity of newly formed hematite. In 136

addition, the result of XRF analysis show the natural goethite contains Fe2O3 84.8% 137

(FeOOH 94.3 %), SiO2 1.9%, MnO2 0.8%, Al2O3 0.6%, ZnO 0.4%, and ignition loss 12.1 %. 138

It indicates the goethite still includes some impurities, such as quartz and clay which is for 139

natural mineral, or is a kind of (Mn, Al, Zn)-substituted goethite which has been reported for 140

a long time [1, 32]. 141

20 30 40 50 60 70

H HHHHHH

HHH---HematiteG---Goethite

G

G G GGGGG

GG

GG 25oC

200oC

250oC

300oC

350oC

400oC

500oC

600oC

Rel

ativ

e in

ten

sity

/C.p

.s

2 theta/degree

800oC

G

142

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143

144

3.2 TG and DTG 145

Thermogravimetry (TG) and derivative thermogravimetry (DTG) curves of natural 146

goethite are displayed in Fig. 2. The total mass loss is 12.08% from ambient to 1000 oC 147

temperature, which is different from that of goethite in theory. Four mass loss steps are 148

observed according to the TG curves. Combining with the DTG curve, these mass loss steps 149

should be ascribed to different hydroxyl/water. 150

(1) A mass loss (0.34%) of adsorbed water is observed at ambient temperature, as is 151

indicated by the TG curve. This loss is caused by the purging gas and contributed to the 152

physically adsorbed water just held by van der Waals forces. Liu et al. [2] reported 153

similar results for synthetic goethite. 154

(2) The second mass loss (0.88%) attributed to a second kind of adsorbed water is observed 155

over ambient to 172 oC. This loss results from desorption of adsorbed water bound by 156

hydrogen bonding. The proposed interface stoichiometry ((H2O)-(H2O)-OH2-OH-Fe-O-157

O-Fe-R) for goethite was reported by Ghose et al. [33]. It indicates at least two layers of 158

adsorbed water exists on the surface of goethite. In the present study, the mass loss 159

between ambient to 172 oC temperatures agrees well with the report. 160

(3) The third mass loss (9.37%) occurs between 172 and 310 oC as is readily observed in the 161

DTG curve. The loss is assigned to the dehydroxylation resulting in the transformation of 162

goethite to hematite. This dehydroxylation is attributed to structural hydroxyl units in 163

goethite. This result is in agreement with previously reported results [34, 35]. In addition, 164

two peaks are observed in the DTG curve between 172 and 310 oC which arise from the 165

high crystallinity of natural goethite according to the report of Schwertmann [36]. This 166

report illustrated that low crystallinity leads to a complete transformation to hematite 167

before the change of unit cell size. However, high crystallinity results in the change in 168

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unit cell size and occurs at a higher temperature. Therefore, the dehydroxylation peak 169

splits into two peaks. 170

(4) The fourth mass loss (1.49%) occurs between 310 and 1000 oC. This loss belongs to the 171

decomposition of remnant structural hydroxyl and partly to nonstoichiometric hydroxyl 172

units. An evidence for the assignment is total mass loss of the third and the fourth steps. 173

The theoretic mass loss of goethite to hematite should be precisely 10.1%. The mass loss 174

of the third step is 9.37%, however, the combined mass loss of the third and the forth 175

step is 10.86%.Thereby, it is speculated that the fourth mass loss step is attributed to the 176

remnant hydroxyl and non-stoichiometric hydroxyl units. Previous studies also gave a 177

further demonstration about the existence of non-stoichiometric hydroxyl units in heated 178

goethite over 300 oC and were explained as the formation of hydrohematite [37-39]. 179

180

0 200 400 600 800

85

90

95

100

12.08%

1.49%

9.37%

0.88%

Temperature/oC

Mas

s L

oss/

%

0.34%

0.0

0.2

0.4

0.6

0.8

310oC172oC

Der

ivat

ive

Mas

s/%

/o C

255oC

279oC

181

Fig. 2. TG and DTG curves of natural goethite 182

183

3.3 FT-IES 184

In order to assess to the structural changes of goethite as a function of treatment 185

temperature, the complimentary technique of infrared emission spectra is utilized. This 186

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8

technique takes the infrared spectra of goethite in situ at an elevated temperature. Two 187

changes can reflect the transformation of goethite to hematite. One is the hydroxyl groups 188

deformation in this low wavenumber centered upon 891 and 790 cm-1 and labelled as (OH) 189

and (OH) which are really important diagnostic bands about crystallinity of goethite [40, 190

41]. The other is the high wavenumber belonging to a combination of hydroxyl groups and 191

water molecular stretching vibration. A remarkable decrease occurs in the low wavenumber 192

and high wavenumber when the temperature increases to 250 oC as is displayed in Fig. 3. 193

The decrease is contributed to the occurrence of dehydroxylation of goethite and the start of 194

the transformation of goethite to hematite. In addition, the band at 1014 cm-1 is retained till 195

the temperature of 600 oC, and then shifts to the low wavenumber of 966 cm-1 as the 196

temperature reaches 600 oC, meantime, the intensity of the high wavenumber bands almost 197

approaches zero. All that happens at the 600 oC is attributed to the complete dehydroxylation 198

and the restructure of Fe and O resulting to the formation of well crystallized hematite. It has 199

been reported that the transformation of goethite to hematite goes through a hydrohematite 200

stage [37, 42]. Therefore, the beginning of the transformation of goethite to hematite takes 201

place at 250 oC and the intermediate product (hydrohematite) retains till to 600 oC for this 202

experimental natural goethite. 203

4000 3500 3000 2500 2000 1500 1000

0.02

0.04

0.06

0.08

0.10

0.12

0.14

966891

790

Em

itta

nce

/a.u

.

Wavenumber/cm-1

150 oC

200 oC

250 oC

300 oC

350 oC

400 oC

500 oC

600 oC

700 oC

800 oC

1014

204

Fig. 3. In situ infrared emission spectra of thermally treated goethite 205

206

3.4 Electron spectroscope analysis 207

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The morphology of natural goethite and thermally treated goethite at 300, 400, 500, 800 208 oC can be observed by TEM images shown in Fig. 4. Some acicular and virgulate substances 209

as well as aggregation are displayed in Fig. 4 (a, b). As mentioned in the results of XRD and 210

XRF, the natural goethite used in this work still probably contains a handful of clays which 211

is conventional phenomenon for natural mineral Therefore, the acicular and virgulate 212

substances are believed to be goethite and the aggregation is speculated as clay like. All the 213

samples after heating over 250 oC are indentified as hematite according to the results of 214

XRD patterns. It can be clearly observed in Fig. 4 (c) a large number of slit-shaped 215

micropores running parallel to the elongated direction of hematite microcrystal and the size 216

of slit-shaped micropores is practically uniform (below 1 nm). In addition, the surface also 217

becomes smooth corresponding to that reported previously [30, 43]. The two reports showed 218

slit-shaped micropores with a width 0.6 and 0.8 nm were obtained after heating at 250 and 219

300 oC, respectively. Without a doubt, the formation of slit-shaped micropores is ascribed to 220

the dehydroxylation in goethite crystal structure due to transformation of goethite to hematite. 221

In case of the pores size, it is difficult to determine precisely the width of micropores 222

because the pores size formed by dehydroxylation would be broadened further by the effect 223

of electron beams of electron microscopy, which has been demonstrated in the study [44]. 224

However, it does not affect the analysis of pore textures. Fig. 4 (d) and (e) present the TEM 225

image of G400 and its amplification, respectively. It seems the slit-shape shows a little 226

broadening after heating at 400 oC. A mass of spherical mesoporous appear instead of the 227

silt-shaped micropores when the sample is heated at 500 oC as displayed in Fig. 4 (f, g). 228

When the temperature reaches 800 oC, mesoporous are destroyed and replaced by 229

cumularspharolith due to sintering between interparticles. Meanwhile, spherical mesoporous 230

still retain in crystal with larger size in spite of the temperature reaching 800 oC. The reports 231

give the confirmation that some hydroxyl groups cannot be removed in hematite structure 232

untill the thermal treatment temperature exceeds 900 oC and substituted goethite also hinders 233

the dehydroxylation [2, 45-47], which should be taken into consideration to explain the 234

existence of mesoporous at 800 oC. In conclusion, the external appearances of the 235

decomposed samples from G300 to G800 are similar to those of natural goethite. That is to 236

say, this decomposition reaction occurs basically within the microcrystal without 237

considerable changes in crystal size and shape except the variation of pore size. 238

Fig. 5 shows the FESEM images of natural goethite and thermally treated goethite as 239

well as the EDS of natural goethite. A bulk mainly composed of acicular substance is 240

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observed from the Fig. 5 (a, c). Moreover, these acicular substances also congregate into a 241

stalactitic bulk as seen in Fig. 5(d) corresponding to the morphology reported previously[32, 242

48]. In addition, the EDS displayed in Fig. 5(b) indicates this bulk in Fig. 5(a) mainly 243

contains Fe, O, Si, Zn, Mn, Al consistent with the results of XRF. Thereby, the natural 244

mineral used in this work is goethite and its shape primarily presents acicular appearance. 245

The following images as displayed in Fig. 5(e-p) present the effect of thermal treatment 246

temperature on the appearance of goethite. The images in Fig. 5(e, g, i, f) show no obvious 247

changes take place for the appearance of samples after heating at 200 and 300 oC. In the 248

contrary, slit-shaped micropores are formed in the TEM images due to the high resolution in 249

this technique. Meanwhile, the Fig. 5(f, h) suggest that acicular goethite with nanoscale 250

length occurs in the natural goethite except the several microns length conforming the report 251

[1]. Besides, radial bulk displays another type of appearance of goethite aggregation, 252

however, which is not composed of acicular goethite replaced by grains as is observed in Fig. 253

5(k) and its amplification in Fig. 5(l). It is speculated this grain-shaped goethite is formed by 254

transformation of other Fe-containing oxides [49]. Until thermal temperature up to 600 oC, 255

many pores are observed on the well crystallized goethite as is shown in Fig. 5(m) and its 256

amplification in Fig. 5(n). The pores still retain and meanwhile a quantity of crystallinity is 257

divided into several pieces occurring for the poorly crystallized goethite when the 258

temperature increases to 700 oC as is seen in Fig. 5(o, p). While the natural goethite is heated 259

over 500 oC, the change tendency is consistent with the results of TEM images. Therefore, 260

the used natural goethite bulk presents different shape, such as stalactitic and radial, mainly 261

composed of acicular and granular crystal according to the electron microscope observations. 262

The external appearances of the thermally treated samples resemble those of untreated 263

sample despite experiencing high temperature treatment. The kind of thermal treatment 264

provides so many pores and large surface area which would improve the properties of 265

hematite and favor the adsorption of hematite to contaminants and the utilization as catalyst 266

carrier. 267

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268

Fig. 4. TEM images of natural goethite (a, b) and thermally treated natural goethite 300 oC 269 (c), 400 oC (d, e), 500 oC (f, g), 800 oC (h, i) 270

271

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272

Fig. 5. FESEM images of natural goethite (a, b (EDS), c, d) and thermally treated goethite 273 200 oC (e, f), 300 oC (g, h), 400 oC (i, j), 500 oC (k, l), 600 oC (m, n), 700 oC (o, p) 274

275

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3.5 Surface area and pore size distribution 276

To investigate the specific surface area and confirm the pore size distribution of natural 277

goethite and thermally treated goethite, nitrogen-adsorption-desorption (BET) is carried out 278

for each sample. As shown in Fig. 6, it is clearly observed that the surface area has a 279

dramatic increase from 12.7 to the maximum of 111.6 m2/g when the temperature increases 280

to 350 oC, which is ascribed to the formation of slit-shaped micropores due to the 281

dehydroxylation of goethite, and then substantially decrease to 13.7 m2/g after heating at 800 282

oC, where internal and interparticles sintering occurs. The presence and change of slit-shaped 283

micropores is consistent with the results of TEM images and gives a confirmation for the 284

results of XRD and TG. Furthermore, the results correspond to the pore size distribution of 285

experimental samples as displayed in Fig. 6. These curves (Fig. 6) show the changes of pore 286

size distribution between 1.7-20 nm. The peak at 3.9 nm for the untreated natural goethite 287

should be ascribed to the micropores arising from the interparticles clearance. A peak is 288

apparently exists before 1.7 nm with respect to the change tendency of curves for the four 289

samples after heating at 200, 250, 300 and 350 oC. Thereby, a possible simulated curve is 290

given for these samples. The simulated pore size The evaluated pore size peak should be at 291

0.99 nm after heating at 300 oC, which is not very consistent with the previous report that 0.6 292

and 0.8 nm for thermally treated goethite at 250 and 300 oC [30, 43]. The peak shifts to 3.5 293

nm as the goethite is heated over 400 oC and experiences a gradual decrease with the 294

increasing temperature. These results indicate that slit-shaped micropores resulting from the 295

dehydroxylation of goethite cause the dramatic increase of surface area. These newly formed 296

micropores are coalesced to mesoporous and further to macropores resulting to the increase 297

of pore size and decrease of surface area with an increase of temperature. It is proposed that 298

the surface area would attain the maximum as the temperature up to between 300 and 350 oC 299

in case of the relationship between thermal treatment temperature and surface area. 300

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0 4 8 12 16 200.00

0.02

0.04

0.06

0.99

G25 G200

G250G300G350

G400

G500

G600

G700

G800

3.9

3.5

Incr

emen

tal p

ore

volu

me/

cm3 /g

Pore size/nmG25 G200 G250 G300 G350 G400 G500 G600 G700 G800

0

30

60

90

120

Sp

ecif

ic s

urf

ace

area

/m2 /g

Samples 301

Fig. 6. Pore size distribution and surface area of natural goethite and thermally treated 302 natural goethite 303

3. Conclusions 304

Composition analysis and SEM images indicate the natural goethite is mainly 305

composed of goethite (over 94%) and the goethite displays different appearances varying 306

from nanoscale to several microns in length. On the whole, this goethite is well crystallized 307

according to the double peak in the curve of DTG. Meantime, the TEM images also provide 308

the information of existence of poorly crystallized goethite due to the sintering of 309

microcrystal in contrast to the appearance of mesoporous and macropores on well 310

crystallized goethite after heating at 800 oC. The TG and BET results shows the 311

dehydroxylation occurs at below 200 oC, however, the phase transformation takes place at 312

250 oC. The intermediate product is proved to be hydrohematite based on the results of FT-313

IES and TG. What is more important, the surface area has a dramatic increase till to 350 oC 314

due to the formation of slit-shaped micropores, which would favor the behavior of 315

adsorption of hematite as well as catalyst carrier. The potential application of the hematite 316

derived from goethite is devised. The thermal treatment temperature between 300 and 350 oC 317

produces the hematite with large surface area and so many micropores which is significant 318

properties for adsorption and catalyst carrier. This kind of thermally treated goethite at least 319

could be utilized as filling material for fixing heavy metal. 320

321

4. Acknowledgement 322

This study was financially supported by the Natural Science Foundation of China (No. 323

41130206, 41072036) and Ph.D. Programs Foundation of Ministry of Education of China 324

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(No.20110111110003). The authors appreciate the financial and infrastructure support of the 325

School of Chemistry, Physics and Mechanical Engineering, Science and Engineering Faculty, 326

Queensland University of Technology, for this research. 327

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