• Nenhum resultado encontrado

Sintering behaviour of a ZnO waste powder obtained as by-product from brass smelting

N/A
N/A
Protected

Academic year: 2021

Share "Sintering behaviour of a ZnO waste powder obtained as by-product from brass smelting"

Copied!
21
0
0

Texto

(1)

1

Sintering behaviour of a ZnO waste powder obtained as by-product from

brass smelting

S. I. H. Sequeira, R. C. C. Monteiro*

CENIMAT/I3N, Department of Materials Science, Faculty of Science and Technology, Universidade Nova de Lisboa, 2829-516 Caparica, Portugal

*Corresponding author (Regina Monteiro) : Tel +351 212948564; Fax +351 212957810 Email: rcm@fct.unl.pt

Abstract

The effect of two sintering methods (conventional sintering and two-step sintering) and of alumina addition on the sintering behaviour of a ZnO-rich waste powder (ZnO > 95 wt%), a by-product from brass smelting industry, was studied aiming to improve the sintered density and grain size. Both conventional sintering and two-step sintering methods did not lead to fully dense powder compacts, as densification was

conditioned by abnormal grain growth and the particle size of the ZnO-rich residue. When two-step sintering was used the grain growth was reduced comparatively to conventional sintering method. The highest relative sintered density (about 90 %) was achieved when samples of ZnO waste and samples of ZnO waste with 2 wt % added Al2O3 were processed by two-step sintering and corresponded to a mean grain size of around 18 μm and 7 μm, respectively. XRD and SEM results indicated that alumina addition helped to inhibit grain growth due to the formation of gahnite spinel (ZnAl2O4) precipitates in the grain boundaries of zincite (ZnO) grains.

(2)

2

1. Introduction

Zinc oxide, an important ceramic material, is used mainly in electrical and optical devices such as varistors, gas sensors, ultrasonic transducers and surface-acoustic-wave devices [1, 2]. Both optical and electrical properties strongly depend on microstructure uniformity and density.

Over the past years, several studies have been focused on microstructure refinement of doped and pure zinc oxide on a search for a link between sintering process, sintering conditions and grain growth [1], [3-5]. Microstructure refinement can be provided by many densification techniques, though most of these processes, such as hot pressing [6], hot isostatic pressing [7] and spark plasma sintering [8] are pressure assisted [9]. Among the pressureless and low complexity densification techniques, two-step

sintering successfully achieves full densification, while simultaneously suppresses grain growth [2], [10-14].

Two-step sintering (TSS) is a two-step process. In the first step, the sample is heated at a constant rate until a sufficiently high relative density (70% or higher) is achieved [14]. This step guarantees the disappearance of supercritical pores while the other pores become unstable allowing for subsequent sintering at lower temperature. In the second step, the temperature is decreased several degrees, typically 100 ⁰C, and sintered for at least ten hours at this temperature. The lower temperature of this step limits the grain growth and thus the sample treated by TSS has identical density but smaller grains compared to single-step sintering or conventional sintering (CS) [10,14].

(3)

3

In this work, the sintering behaviour of a zinc oxide rich waste powder (with a ZnO content higher than 95 wt%) has been studied. This waste comes from the brass smelting industrial process, where it is filter-collected as flue dust. The present study is part of a more general work focusing on the recycling and potential valorisation of such waste. A ceramic powder technology route has been applied to process this non-conventional ZnO source.

In a previous work performed by some of the authors [15], the possibility of preparing ceramic targets from this ZnO waste powder and the application of the targets on the processing of ZnO thin films by radio-frequency magnetron sputtering were studied. It was found that the sintered targets exhibited non-homogeneous microstructures due to the presence of dense micro-aggregates, and it was pointed out that further work should be developed to investigate a sintering procedure for this ZnO waste powder leading to a homogeneous and dense microstructure.

Most of the works studying this type of ZnO waste powder, a by-product originated in the brass smelting industrial process, have been focussed towards the recovery of zinc by application of metallurgical processes [16, 17]. In a recent work Lee et al [18] developed a process to prepare high purity ZnO nanopowders from brass ash and then studied the densification of the produced ZnO powder. The processing of the brass ash before the sintering procedure involved a calcination step at 700 °C followed by a hydrothermal process for Zn purification and separation from liquor and then a drying and thermal processing of the solid precipitate [18]. This multistep treatment method, apart from producing high purity ZnO nanoparticles leaves also some residues.

(4)

4

In this study, the effect of different sintering parameters on the densification and grain growth of the as-received ZnO waste powder was investigated. The influence of

temperature, holding time and sintering process (conventional sintering vs two-step sintering), as well as addition of alumina on the densification and grain growth was investigated. It is aimed to define the sintering conditions leading to a homogeneous and highly dense ceramics with potential application as sputtering targets to be used in the deposition of ZnO films with photocatalytic or UV detection properties.

2. Materials and Methods

The ZnO-rich waste is originated in brass factories, where copper-zinc metal alloy is melted at 1100˚C, or higher, and under such conditions partial zinc volatilization occurs. The zinc vapor reacts with oxygen from air producing a fine ZnO dust that is collected in the off-gas cleaning system being filter-retained. Particle size analysis of the waste powder by diffraction laser granulometry indicated a mean particle size of around 1 m.

The chemical composition of the as-received waste powder was analysed by X-ray fluorescence (XRF) with a PANalytical XRF-WDS 4 kW AXIOS sequential spectrometer (Rh X-Ray tube) under Helium flow. XRF analysis revealed that the major component of the residue is ZnO (95.4 wt%), presented together with PbO (1.1 wt%), CuO (0.94 wt%), MgO (0.62 wt%), Fe2O3 (0.61 wt%), Al2O3 (0.56 wt%), SiO2 (0.41 wt%), SO3 (0.16 wt%), CdO (0.18 wt%), Cl (0.15 wt%), CaO (0.13 wt%), and NiO (0.023 wt%). Zincite was the only crystalline phase identified by XRD analysis in the ZnO waste powder.

(5)

5

Samples of ZnO waste powder (named as Zw) and samples of ZnO waste with the addition of 2 wt % Al2O3 (named as Zw:A) were prepared. The powders with alumina addition were mixed for 4 hours (Turbula WAB, T2F). For each heat-treatment

schedule, six cylindrical powder compacts were uniaxially pressed (148 MPa) and green disks with 13 mm diameter and ≈2 mm height were obtained.

Sintering of the green compacts was carried out in air using an electric furnace with a heating rate of 10 ⁰C/min, using either conventional sintering (CS) or two-step

sintering (TSS) methods. CS was carried out at different temperatures (900 ⁰C, 1050 ⁰C, 1200 ⁰C, 1300 ⁰C and 1400 ⁰C) and held at each selected temperature for various times (90 min, 3 h, 6 h or 12 h). For the first step of TSS, the samples were heated at a

temperature (T1) of 900 ⁰C, 1050 ⁰C and 1300 ⁰C during 1 minute and then rapidly cooled to the second step temperature (T2). The selected T2 temperature was 50 ⁰C or 100 ⁰C lower than T1. The samples were held at T2 for 12 h in order to reach higher density.

The bulk density of the sintered samples was determined by the Archimedes method. The measurements were performed in an analytical balance using distilled water as buoyancy liquid. For the determination of the relative density, a theoretical density of 5.61 g/cm3 and 5.59 g/cm3 was assumed for Z

w and Zw:A samples, respectively. At least three powder compacts of Zw and of Zw:A were sintered under the same conditions and the mean values of the bulk density of the sintered samples were determined. The mineralogical composition of sintered sampleswas investigated by X-ray diffraction (DMAX-IIIC, Rigaku Diffractometer Industrial Corporation), with a

(6)

6

were carried out from 20⁰ to 75⁰ (2θ), with a scanning step size of 0.08⁰ and an acquisition time of 1s.

The microstructure of the sintered samples was characterized by scanning electron microscopy (TM3030 plus, Hitachi) after polishing and thermal etching. The thermal etching was performed for 15 min at a temperature 150 ⁰C lower than the previous thermal treatment. The average grain size of each Zw and Zw:A sample sintered under specific conditions was determined from 3 to 4 different SEM images using ImageJ software and the associated error was evaluated.

3. Results and discussion

3.1. Conventional Sintering (CS)

Relative densities of the prepared specimens (Zw and Zw:A) as a function of sintering temperature and for the different sintering times are presented in Fig. 1. The samples have been processed by a conventional sintering method at a sintering temperature in the range between 900 and 1400⁰C for the holding times of 90 min, 3 h, 6 h and 12 h. For both Zw and Zw:A samples, the results reveal a noticeable increase in density from the green density (around 47%) up to a sintering temperature of 1050 ⁰C, while the influence of temperature on the final density is much less accentuated in the range 1200-1400 ⁰C. For Zw samples, it is verified that the relative density tends to decrease slightly after sintering at a temperature of 1400 ⁰C, and that for Zw:A samples sintered at 1400 ⁰C, the density reaches the highest value (89.8 %) after a holding time of 90 min, or it maintains the same value as after sintering at 1300 ⁰C for longer holding times. Similarly to what is shown in Fig. 1 for the ZnO waste powder samples (Zw), the

(7)

7

decrease in the sintered density of samples made from commercially available pure ZnO when fired at 1400 ⁰C was also observed and it has been attributed to ZnO volatilization [4].

Fig.1 - Relative density of sintered samples as a function of sintering temperature for different holding times.

The effect of holding time on the relative density is distinct when both samples were sintered at 900 ⁰C and at 1050 ⁰C: Zw samples show a much higher density when sintered during 12h comparatively to that achieved after shorter sintering times (90 min to 6 h), while Zw:A samples show a gradual increase in density with the increase in the holding time. It is verified that the relative density of Zw and of Zw:A samples does not increase continuously with the holding time when sintered at the highest sintering

(8)

8

temperatures (1300 ⁰C and 1400 ⁰C) as a decrease in density is observed for samples sintered for the longest time (12h).

Controlled grain growth during sintering is of great importance to obtain a small and homogeneous grain, which in turn prevents mechanical failure and degradation of service behaviour, and contributes to attain sintered samples with reduced

microstructural defects.

From Fig. 2, the change of the grain size with sintering temperature can be observed. For Zw samples, the grain size moderately increases with sintering temperature and holding time for the sintering temperatures up to 1050 ⁰C. Above this temperature, a severe grain growth occurred with sintering temperature, and it is particularly

accentuated for the case of the samples sintered during 12 h, where exaggerated grain growth is observed

In the case of Zw:A samples, the grain size moderately increases with sintering temperature and holding time for the sintering temperatures up to 1200 ⁰C, the

sudden increase in the grain size occurring at a temperature comparatively higher than for Zw samples, independently on the holding time. At a sintering temperature of 1200 ⁰C, the grain size of Zw:A samples sintered for 90 min and for 12h was 6.5 μm and 9.8 μm, respectively, while for Zw samples the grain size was 10.9 μm and 25.6 μm, respectively.

Nevertheless, comparing these two types of samples (Zw and Zw:A) for heat treatments above 1200 ⁰C, the effect of alumina addition on grain growth is noticeable, and regardless the holding time, the mean grain size in Zw:A is smaller than in Zw samples, indicating that grain growth is inhibited by the presence of this oxide.

(9)

9

Fig. 2 – Mean grain size of Zw and Zw:A samples sintered at different temperatures and holding times.

To illustrate the effect of sintering temperature and alumina addition on the densification and grain size, the microstructures of Zw and Zw:A samples sintered at 900 ⁰C, 1200 ⁰C and 1400 ⁰C for 90 min are shown in Fig. 3.

The SEM images of both Zw and Zw:A samples sintered at 900 ⁰C, Fig. 3a and 3b, respectively, reveal highly porous microstructures (with open porosity) having similar grain size (about 2 m). With the increase in sintering temperature, denser

microstructures are observed, however the presence of intra and intergranular

porosity is also depicted. The SEM images clearly evidence the increase in grain growth with sintering temperature and the presence of residual porosity in all the samples, explaining the reason why densification was hindered above 1200 ⁰C, the highest

(10)

10

density values being around 90 % (see Fig. 1). At the highest sintering temperature (1400 ⁰C), the uniformity of grain shape disappears and some abnormal grain growth can be detected, especially for Zw samples (see Fig. 3a2). Microstructural observation of samples sintered at temperatures ≥ 1200 ⁰C revealed that the mean grain size was always higher for Zw samples than for Zw:A samples.

Fig. 3 - SEM images of Zw samples sintered at a) 900 ⁰C, a1) 1200 ⁰C and a2) 1400 ⁰C, and of Zw:A samples sintered at b) 900 ⁰C, b1) 1200 ⁰C and b2) 1400 ⁰C) for 90 min.

(11)

11

The XRD patterns of Zw and Zw:A samples sintered in air for 12 h at three different temperatures are depicted in Fig. 4.

At the lowest sintering temperature (900 ⁰C), independently of the holding time and alumina addition, all the peaks were identified as zincite, ZnO (JCPDS 00-036-1451). In the case of Zw samples, a secondary phase identified as willemite, Zn2SiO4 (JCPDS 00-037-1485) was identified in samples sintered at 1050 ⁰C for 12 h and in samples sintered at 1200 ⁰C for 90 min. For Zw:A samples, zincite, willemite and gahnite spinel, ZnAl2O4 (JCPDS 00-005-0669) coexist when sintered at temperatures ≥ 1050 ⁰C, independently of the holding time.

Fig. 4 - X-ray diffraction of Zw and Zw:A sintered at 900 ⁰C, 1050 ⁰C and 1400 ⁰C for 12hours.

(12)

12

3.2. Two-Step Sintering (TSS)

In order to understand the impact of the presence of the crystalline phases (zincite, willemite and gahnite spinel) on the density and mean grain size evolution, the samples were submitted to a two-step sintering process and the results were

compared with the ones obtained by conventional sintering. Based on the XRD results, three initial heat treatment temperatures (T1 = 900 ⁰C, 1050 ⁰C or 1300 ⁰C) were chosen.

The relative sintered density and grain size of Zw samples prepared by CS, considering a holding time of 12 h, and by TSS method are presented in Fig. 5. As the first step temperature (T1) increased, the density of the compacts prepared by TSS method became closer to the ones obtained by CS method. For the highest first step treatment temperature (1300 ⁰C), the density of Zw samples prepared by TSS method exceeded that obtained by CS method, and the highest sintered density of 88.4 % was achieved after sintering at T1=1300 ⁰C and T2=1200 ⁰C.

For all the initial heat treatment temperatures, sintering by TSS method resulted in grain size decrease comparatively to CS method, and the grain size became even smaller with further difference between T1 and T2 (see Fig. 5). For example, considering the case where T1 was 1300 °C, the average grain size of Zw compacts sintered by CS method was 43 μm, while by TSS method it decreased to 28 μm and to 18 μm when T2 was 1250 °C and 1200 °C, respectively.

(13)

13

Fig. 5 - Relative sintered density and mean grain size of Zw samples after conventional sintering (CS) and two-step sintering (TSS).

Figure 6 shows the microstructures of Zw samples sintered at 1300 °C, giving evidence of the higher porosity and of the larger grain size of the main phase (zincite, ZnO) in samples sintered by CS than by TSS method.

According to T. Roy et al. [19], the presence of willemite (Zn2SiO4), which is less dense than zincite, should decrease the density values of pure ZnO-based samples with the addition of 2-10 wt % of silica (SiO2). The same authors [19], reported also that when willemite precipitates were located at the grain boundaries should limit the migration of Zn2+ cations and consequently inhibited the grain growth of the main phase (zincite). In our case, where the ZnO waste powder has a small silica content (about 0.4 wt %, as detected by XRF), the presence of willemite was identified in the XRD patterns of the sintered samples (see Fig. 4), but by SEM analysis the formation of willemite

precipitates in the grain boundaries was not observed (see Fig. 6). Comparing the willemite peaks detected by XRD, they were more intense when CS method was used rather than TSS method. As the grain size of the Zw samples after CS was comparatively higher than after TSS (see Fig. 5), it is suggested that in this particular case the grain

(14)

14

growth was more likely to be influenced by the sintering temperature and method than it is by the presence of the willemite precipitates.

Fig. 6 - SEM images of Zw samples sintered by: a) CS (1300 ⁰C, 12 h), and b) TSS (T1=1300 ⁰C, T2=1250 ⁰C).

M. Wu [13] applied similar pressureless sintering methodologies to pure ZnO powder, with a median particle size of 0.4 μm, and by the use of TSS method, where T1= 1300 °C and T2=1250 °C, he obtained a relative density of 95.1 % and a grain size of 12 μm. In the present study, where the ZnO rich residue with a comparatively higher mean particle size (~1 μm) was sintered under similar conditions, the corresponding values

(15)

15

for density and mean grain size were 87.9 % and 28 μm, respectively. In our case, both pressureless sintering methodologies could not successfully densify this particular ZnO rich residue above 90%, and TSS proved to be inefficient on the densification of Zw probably due to two main reasons: the exaggerated grain growth observed in ZnO containing such amount of impurities, and the coarse particle size of the starting powder, as discussed by M. Wu [13].

For comparison, Fig. 7 illustrates the sintered density and mean grain size of Zw:A samples, after conventional and two-step methods, as a function of the initial treatment temperature. Similarly to what has been observed for the Zw samples, the relative density increases with initial heat treatment temperature (T1) until it reaches the maximum value of 88 % for TSS, at the conditions T1=1300 ⁰C and T2=1200 ⁰C.

Fig. 7 - Relative sintered density and mean grain size of Zw:A samples after conventional sintering (CS) and two-step sintering (TSS).

Figure 8 shows the microstructures of Zw:A samples sintered by CS and by TSS. Once more, the results show that these pressureless sintering methods were not favourable to the complete densification of Zw:A, as supercritical pores remained even at the highest first step treatment temperature used in TSS method (1300 ⁰C).

(16)

16

A closer look into the microstructures of Zw:A samples prepared by CS and TSS (shown in Fig. 8) confirms the presence of a main phase (zincite) and of a secondary phase (spinel) mainly located at the grain boundaries (indicated by the white arrows and shown at higher magnification in the inserts).

Fig. 8 - SEM images of Zw:A samples sintered by: a) CS (1300 ⁰C, 12 h), and b) TSS (T1=1300 ⁰C, T2=1250 ⁰C).

Although TSS method seems to be unsuitable for the full densification of Zw:A samples, the grain size was greatly influenced by the heat-treatment conditions used in TSS method. For the highest sintering temperature (1300 ⁰C), grain growth inhibition could

(17)

17

be observed for TSS method comparatively to CS method. After CS at 1300 ⁰C for a sintering time of 12 h, the grain size of Zw:A was about 29 μm, while with TSS the grain size was reduced to 22 μm ( when T2=1250 ⁰C) and to about 7 μm (when T2=1200 ⁰C). Similar behaviour has been found in different ZnO-based samples as reported by M. Wu [5]and [13]. A possible explanation for this decrease in grain size is the presence of spinel in the grain boundaries, which inhibits the grain growth by its dragging effect on the migration of grain boundaries.

4. Conclusions

The sintering behaviour of a ZnO rich residue (>95 wt %) from the brass industry was studied and the influence of the sintering temperature, holding time and sintering process (CS vs TSS) as well as addition of alumina on the densification and grain growth has been discussed.

The micron-size ZnO rich waste powder could not be fully densified by both

pressureless methodologies (CS or TSS) probably due to abnormal grain growth and to the coarse particle size of the waste powder. Comparing the two sintering methods, TSS significantly supressed grain growth relatively to CS method, and the grain size became even smaller by increasing the difference between the temperatures selected for the first and second heat-treatment steps of TSS.

Addition of 2 wt% alumina to ZnO waste powder did not improve densification, the highest sintering density obtained was around 90 %, but it significantly contributed to grain growth inhibition due to the formation of spinel in the grain boundaries.

(18)

18

Future studies should be dedicated to establish the relationships between powder particle size and the densification behaviour of this residue in order to define the sintering conditions that allow to obtain a fully dense compact. A potential application is the production of high density ceramic sputtering targets to be used in the

deposition of ZnO films with photocatalytic or UV detection properties.

Acknowledgments

This work was funded by FEDER funds (COMPETE 2020 Programe) and national funds (FCT- Portuguese Foundation for Science and Technology) under the project

UID/CTM/50025/2013 and funded by the project M-ERA.NET/0010/2012.

References

[1] N. Canikoǧlu, N. Toplan, K. Yildiz, H.Ö. Toplan, Densification and grain growth of SiO2-doped ZnO, Ceram. Int. 32 (2006) 127–132.

doi:10.1016/j.ceramint.2005.01.007.

[2] M. Mazaheri, A.M. Zahedi, S.K. Sadrnezhaad, Two-step sintering of

nanocrystalline ZnO compacts: Effect of temperature on densification and grain growth, J. Am. Ceram. Soc. 91 (2008) 56–63.

doi:10.1111/j.1551-2916.2007.02029.x.

[3] A. Sedky, T.A. El-Brolossy, S.B. Mohamed, Correlation between sintering temperature and properties of ZnO ceramic varistors, J. Phys. Chem. Solids. 73 (2012) 505–510. doi:10.1016/j.jpcs.2011.11.035.

[4] J. Han, P.Q. Mantas, M.R. Senos, Densification and grain growth of Al-doped ZnO, J. Mater. Res. 16 (2001) 459–468. doi:10.1557/JMR.2001.0069.

[5] M.W. Wu, D.S. Liu, Y.H. Su, The densification, microstructure, and electrical properties of aluminum-doped zinc oxide sputtering target for transparent conductive oxide film, J. Eur. Ceram. Soc. 32 (2012) 3265–3275.

doi:10.1016/j.jeurceramsoc.2012.04.030.

[6] M. Mazaheri, S.A. Hassanzadeh-Tabrizi, S.K. Sadrnezhaad, Hot pressing of nanocrystalline zinc oxide compacts: Densification and grain growth during sintering, Ceram. Int. 35 (2009) 991–995. doi:10.1016/j.ceramint.2008.04.015.

(19)

19

[7] M.W. Wu, P.C. Tsai, Y.C. Huang, Enhancement of the densification and

mechanical properties of aluminum-doped zinc oxide ceramics by hot isostatic pressing, J. Alloys Compd. 650 (2015) 514–519.

doi:10.1016/j.jallcom.2015.08.053.

[8] Y. Beynet, A. Izoulet, S. Guillemet-Fritsch, G. Chevallier, V. Bley, T. Pérel, et al., ZnO-based varistors prepared by spark plasma sintering, J. Eur. Ceram. Soc. 35 (2015) 1199–1208. doi:10.1016/j.jeurceramsoc.2014.10.007.

[9] K. Bodišová, D. Galusek, P. Švančárek, V. Pouchlý, K. Maca, Grain growth

suppression in alumina via doping and two-step sintering, Ceram. Int. 41 (2015) 11975–11983. doi:http://dx.doi.org/10.1016/j.ceramint.2015.05.162.

[10] K. Maca, V. Pouchly, P. Zalud, Two-Step Sintering of oxide ceramics with various crystal structures, J. Eur. Ceram. Soc. 30 (2010) 583–589.

doi:10.1016/j.jeurceramsoc.2009.06.008.

[11] X.H. Wang, P.L. Chen, I.W. Chen, Two-step sintering of ceramics with constant grain-size, I. Y2O3, J. Am. Ceram. Soc. 89 (2006) 431–437. doi:10.1111/j.1551-2916.2005.00763.x.

[12] M.M. Shahraki, S.A. Shojaee, M.A.F. Sani, A. Nemati, I. Safaee, Two-step sintering of ZnO varistors, Solid State Ionics. 190 (2011) 99–105.

doi:10.1016/j.ssi.2010.06.026.

[13] M.W. Wu, Two-step sintering of aluminum-doped zinc oxide sputtering target by using a submicrometer zinc oxide powder, Ceram. Int. 38 (2012) 6229–6234. doi:10.1016/j.ceramint.2012.04.076.

[14] N.J. Lóh, L. Simão, J. Jiusti, A. De Noni Jr., O.R.K. Montedo, Effect of temperature and holding time on the densification of alumina obtained by two-step sintering, Ceram. Int. 43 (2017) 8269–8275. doi:10.1016/ j.ceramint.2017.03.159.

[15] R.C.C. Monteiro, A.T. Kullberg, A.A.S. Lopes, J.V. Pinto, D. Nunes, A.

Gonçalves, E. Fortunato, F. Castro, Brass smelting dust as a source of ZnO in the production of targets used in magnetron sputtering thin film deposition,

in: C. Vilarinho, F. Castro, J. Carvalho, M. Russo, J. Araújo (Eds.), 3rd

International Conference WASTES: Solutions, Treatments and Opportunities, Viana do Castelo, September 2015, pp. 91–93.

[16] V. Cvetkovski, V. Jonanovic, G. Durasevic, Pyrometallurgical purification of brass smelter furnace flue dust, in: R.W. Sarsby, T. Meggyes (Eds.), Green3,

3rd International Symposium on Geotechnics related to the European

Environment, Berlim, June 2000, pp. 75–78.

[17] M Dattilo, E.R Cole, T.J O'Keefe, Recycling of zinc waste for electrogalvanizing Conservation & Recycling. 8 (1985) 399-409.

[18] T-H. Lee, H.H. Nersisyan, S-C. Kwon, S-H. Joo, K-T. Park, J-H. Lee, ZnO nanopowder derived from brass ash: Sintering behavior and mechanical properties, Int. J. Mineral Processing 37 (2015) 87–94.

(20)

20

[19] T.K. Roy, A. Ghosh, D. Bhowmick, D. Sanyal, S. Koley, A. Chakrabarti, Effect of silica doping on the densification and grain growth in zinc oxide, Ceram. Int. 37 (2011) 2679–2687. doi:10.1016/j.ceramint.2011.04.017.

(21)

Imagem

Fig. 2 – Mean grain size of Z w  and Z w :A samples sintered at different temperatures and  holding times
Fig. 3 - SEM images of Z w  samples sintered at a) 900 ⁰C, a1) 1200 ⁰C and a2) 1400 ⁰C,  and of Z w :A samples sintered at b) 900 ⁰C, b1) 1200 ⁰C and b2) 1400 ⁰C) for 90 min
Fig.  4  -  X-ray  diffraction  of  Z w   and  Z w :A  sintered  at  900  ⁰C,  1050  ⁰C  and  1400  ⁰C  for  12hours
Fig. 5 - Relative sintered density and mean grain size of Z w  samples after conventional  sintering (CS) and two-step sintering (TSS)
+4

Referências

Documentos relacionados

Conclusão para este modelo: de fato a intensidade da máxima força de atrito depende da área EFETIVA de contato que permanece constante quando a área APARENTE

modalidades por meio de ações integradas dos poderes públicos das diferentes esferas federativas (BRASIL, 2014b). Além disso, prevê a universalização da pré-escola e

comparison between Figure 4a (conventional sintering) and Figure 4b (microwave sintering), it can be noticed that the dependence of both average grain size and relative density

Regarding the investigated composites, two efects of the LZSA addition to alumina on the suppression of the alumina grain growth must be considered: the lowering of the

The sintering process of titania can be described as plastic flow, and the mixtures show a competition in sintering mechanism between plastic flow and liquid phase. The

In order to investigate the effects of reinforcement’s amount and sintering duration through microwave-assisted sintering process on the electrical, thermal and mechanical

Harlow associa várias vezes a palavra gestão ao conceito de RP, concebendo a atividade de RP como uma função de gestão, com várias áreas de intervenção, que contribui para a

Stepanov Institute of Physics, National Academy of Sciences of Belarus, Minsk, Republic of Belarus 91 National Scientific and Educational Centre for Particle and High Energy