Advances in Materials Science and Engineering
Volume 2017 (2017), Article ID 8962986, 10 pages
https://doi.org/10.1155/2017/8962986

Research Article

Comprehensive Study on Elastic Moduli Prediction and Correlation of Glass and Glass Ceramic Derived from Waste Rice Husk

Chee Sun Lee,¹ Khamirul Amin Matori,1,2 Sidek Hj. Ab Aziz,¹ Halimah Mohamed Kamari,¹ Ismayadi Ismail,² and Mohd Hafiz Mohd Zaid1,2

¹Department of Physics, Faculty of Science, Universiti Putra Malaysia (UPM), 43400 Serdang, Selangor, Malaysia
²Materials Synthesis and Characterization Laboratory, Institute of Advanced Technology, Universiti Putra Malaysia (UPM), 43400 Serdang, Selangor, Malaysia

Correspondence should be addressed to Mohd Hafiz Mohd Zaid; mhmzaid@gmail.com

Received 2 March 2017; Accepted 24 July 2017; Published 24 August 2017

Academic Editor: Gianluca Cicala

Copyright © 2017 Chee Sun Lee et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

Zinc silicate (ZnO–SiO₂) systems were fabricated using zinc oxide (ZnO) and white rice husk ash (WRHA) with compositions of (ZnO)x(WRHA)1−x ( = 0.55, 0.60, 0.65, and 0.70 wt.%) was symbolized by S1, S2, S3, and S4, respectively. The ZnO–SiO₂ samples were fabricated by applying the melt-quench method and the physical and elastic properties of the samples were investigated. Physical properties used in this study are density and molar volume while the theoretical elastic moduli of the samples produced were obtained using direct calculation of theoretical model compared with the experimental elastic moduli obtained by acquiring ultrasonic velocities using ultrasonic pulse-echo technique. Values of experimental elastic moduli including longitudinal modulus (), shear modulus (), Young’s modulus (), bulk modulus (), and Poisson’s ratio () were compared with theoretical model calculated using Rocherulle’s model. All the configurations of the elastic moduli obtained experimentally match very well with the configuration from Rocherulle’s model but Poisson’s ratio obtained experimentally differs from the values of Poisson’s ratio obtained through Rocherulle’s model.

1. Introduction

Rice is the main source of carbohydrates and consumption for the populations in Asia and the main by-product is the waste rice husk (RH) which is produced in a vast production of paddy field in Malaysia and also throughout the globe. Rice cultivation in Malaysia has resulted in 400,000 metric tonnes of RH annually as it has been considered valueless and the main problem arises once it comes to the problem of getting rid of it [1]. RH is obtained as a worthless by-product as it cannot fetch a good price in the open market and most of the RH milling factories are massively influenced by this problem and disposing RH ethically will become unprofitable for them [2, 3]. RH produced is generally discarded or burned and this has caused a serious threat to our mother earth and by developing new ways to reuse RH, it can be a useful by-product such as substitution for conventional silica in the glass industry [4, 5]. Next, substitution silica such as white rice husk ash (WRHA) can be derived from RH by a complete combustion [6]. RH serves as good substituents for conventional silica as it possesses high concentration of silica after complete combustion of 1000°C from WRHA and it has relatively lower cost compared to its conventional silica counterpart [7, 8]. RH glass system which is derived can be doped into lithium silicate glass system and it mimics the thermal behavior and crystalline phases of the glass and glass ceramic lithium silicate systems and it also increases the fracture toughness of both systems by 100% thus implying that RH will act as an adequate replacement for conventional silica [9]. RH glass ceramic can be used to derive nepheline–forsterite glass ceramic where its main source of silica is from WRHA [10].

Zinc silicate (ZnO–SiO₂) glass is an amorphous glass with high concentration of ZnO in its major composition and it grabs much attention from researches as it possesses various applicable uses in the range of glass ceramics and technical glasses [11]. Researchers can do a lot more to understand the applications of ZnO–SiO₂ glass and by variating SiO₂ and ZnO compositions, endless possibilities can be achieved. ZnO is one of the major compositions in the samples produced and incorporating it in the glass and glass ceramic system makes ZnO–SiO₂ system a remarkable one. ZnO based glass is one of the most interesting network modifiers in the list of all the network modifiers because of its influence in the optical, electrical, and magnetic properties of the glass produced causing the glass to be environment-friendly and of low cost which grabs the attention of researches and manufacturing industry [12, 13]. Silicate glass doped with high concentration of ZnO has lower elastic moduli because of the effect presented by ZnO which acts as a network modifier and its effect is what causes these types of glass to be outstanding compared to other types of glass system [14].

In this study, ZnO and WRHA will be manipulated to study the physical and elastic properties of ZnO–SiO₂ glass and glass ceramic system. Influence of ZnO on its elastic moduli and comparison of elastic moduli obtained experimentally and elastic moduli obtained theoretically were also discussed.

2. Experimental Details

RH species used is the Oryza sativa (Asian rice) which can be found in majority of Asian countries and RH from this study is acquired from a local rice factory at Tanjung Karang, Selangor, Malaysia. RH samples used were just milled a day before the study and they are kept in an indoor compound to minimize possible unwanted contaminations from the surroundings. RH then is examined to remove sands and small rocks which jeopardize the study. Next, RH is then washed for several times to get rid of possible dirt and contaminations as it is in contact with sand and it is drenched in water for 2 hours in a vast plastic basin to have the dirt and sands sunken to the bottom of the plastic basin. RH which is clean and clear without contaminations will float on the surface and it is removed to a large plastic sieve to dry the RH with an aluminum foil on top of it to minimize contaminations from the surroundings as it will be left in the lab for 24 hours to dry at room temperature. After 24 hours, RH will be subsequently dried in the oven for 2 hours at 100°C for 24 hours to obtain a fully dried RH. After obtaining the dry RH, 500 g of the dried RH is transferred to a ceramic crucible and distributed evenly so that the combustion of RH to WRHA can be performed evenly. RH will be burned at 1000°C for 2 hours at a heating rate of 10°C/min and the changes in color of the WRHA produced are observed. Ceramic crucible selected must be flat as it delivers a complete homogeneous burning of RH. The EDXRF measurement has been done to obtain the percentage of the oxide composition in the WRHA [16].

In this study WRHA is acquired to replace conventional silica in the formation of ZnO–SiO₂ glass and glass ceramic system chemical formula of (ZnO)x(WRHA)1−x ( = 0.55, 0.60, 0.65, and 0.70 wt.%) was symbolized by S1, S2, S3, and S4, respectively, acquiring melt-quench technique. After mixing the samples, the mixture is then milled for 24 hours to ensure a fully homogenous mixture. Usually, melting silicate glass system would require up to 1700°C as it belongs to type of glass with high melting point but in this study, where the silica source is being manipulated by switching it to WRHA to form ZnO–SiO₂ glass system, a new method is being done with the lowest temperature at which ZnO–SiO₂ system can exist at 1450°C with 2 hours. After all the samples inside the crucible were successfully melted, the crucible was removed with a platinum clamp and the samples are transferred to a stainless steel mold which has been preheated at 500°C and the samples then are annealed at 500°C for 5 hours while the leftover samples were transferred into the same stainless steel base which holds the mold and is annealed at the similar condition. Finally the samples were cut using a diamond blade cutter to a dimension of (1.0 × 2.0 × 0.3) cm³ and later the samples were grinded using several grinding papers in the range of 320–1000 grit to ensure a perfect smooth surface for ultrasonic measurement. Samples thickness of (1.0 × 2.0 × 0.3) cm³ is the optimum thickness because samples which are too thick or too thin may cause the decrease in ultrasonic wave intensity.

The compositions of the glass and glass ceramic samples are confirmed using EDXRF diffractometer (Shimadzu, EDX-720). Next, the densities of the samples were determined using the Archimedes method where it acquires the weight of the samples in air and distilled water. Based on the Archimedes method, the buoyant force produced when the sample is immersed in distilled water is the same with the magnitude of the weight of distilled water displaced by the volume of the samples. Hence, the density of samples, , can be expressed as

where  g cm⁻³. Distilled water was chosen as the immersed liquid as it is the cheap, inert, and low surface tension. Molar volume () of any substance is defined as the volume occupied by one mole of any material from chemical compound or chemical element at a specified temperature and pressure formula of is equal to the total molar mass () divided by the mass density ().

The molar volumes were measured in cubic centimeters per mole (cm³ mol⁻¹) and for liquids and solids; they can be expressed as

where is the total molecular weight of the multicomponent system given by

where is the mole fraction of the th oxides, and is the molecular weight of the th oxides. Ultrasonic velocities of the samples which consist of longitudinal velocity () and shear velocity () were determined using Ritec, Ram-5000 Snap System machine with frequency of 5 MHz. Longitudinal velocity of the samples was acquired using the longitudinal probe while the shear velocity of the samples was acquired using the shear probe. Adhesive agent used for the longitudinal probe is longitudinal gel while the shear probe is shear gel. Adhesive agent is used to minimize the refraction of wave in air gap while acquiring both ultrasonic velocities.

Ultrasonic technique is a method that is useful and flexible to measure the structure and mechanical properties of materials. Next, ultrasonic waves can be transmitted through the material and detect the mechanical properties and the defects found in the material. Generally, ultrasonic measurement can be used to measure the metal and nonmetal samples. Ultrasonic pulse-echo technique can also be known as the longitudinal modulus and shear modulus.

3. Results and Discussion

Four series of ZnO–SiO₂ samples were obtained and chemical composition of the WRHA was analyzed using EDXRF and the chemical composition of the WRHA and samples produced was tabulated in Table 1.

Table 1: Analysis of chemical composition of ZnO–SiO₂ samples.

Samples
ZnO
SiO₂
K₂O
Al₂O₃
CaO
MgO
Na₂O
Fe₂O₃
CuO

S1
53.83
43.02
0.84
0.75
0.59
0.26
0.24
0.25
0.22

S2
58.40
38.84
0.78
0.66
0.58
0.23
0.20
0.22
0.09

S3
65.01
32.46
0.74
0.61
0.56
0.21
0.19
0.20
0.02

S4
70.02
28.68
0.44
0.34
0.29
0.07
0.10
0.05
0.01

Figure 1 and Table 2 show the density, molecular weight, and molar volume for ZnO–SiO₂ samples and it shows that the density of the samples increases with the increase of ZnO from 2.94 to 3.66 g cm⁻¹. Increase in density is largely due to substituting Si (28.08) with a higher atomic mass element of zinc which is (65.39). Besides, the increase in density with the increase of ZnO content occurs due to the increase in the crystallinity in the samples in which sample S1 is fully amorphous and sample S4 provides higher amounts of crystalline compared to the other samples [17, 18]. Increase in crystallinity is due to the increase in melting point of the ZnO–SiO₂ samples as its melting point increases as ZnO in the system increases as shown in Figure 2. Not only that, silica present in the system will also act as a nucleating agent for the samples to increase in crystalline [15].

Table 2: Density, molecular weight, and molar volumeof ZnO–SiO₂ samples.

Samples
S1
S2
S3
S4

Density (g cm⁻³)
2.94
3.08
3.44
3.66

(g mol⁻¹)
70.43
71.59
72.79
73.91

(cm³ mol⁻¹)
23.97
23.21
21.17
20.18

Figure 1: The density and molar volume versus wt.% of ZnO in ZnO–SiO₂ samples.

Figure 2: Binary system of ZnO–SiO₂ system [15].

Increase in density can also be explained by the increase in ZnO and the reduction of silica (SiO₂) which will increase its overall molecular weight of the samples as ZnO is much heavier relative to molecular mass of SiO₂ [19]. Increase in density of the ZnO–SiO₂ samples may also be caused by structural reorganization of the atoms thus causing a possible modification of the geometrical configuration.

Molar volume () in this study was calculated using (2) and, based on Figure 1 and Table 2, molar volumes of the ZnO–SiO₂ samples produced indicate a decrease from 23.97 to 20.18 cm³ mol⁻¹ when the amount of ZnO in the samples increases. Molar volume is vastly dependent on the overall molecular weight of a particular composition and this decrease is mainly because of greater rise in density compared to the overall molecular weight. Generally, silicate glass and glass ceramic have an opposite trend to the density of its system when it comes to the molar volume and, in this study, SiO²⁺ (0.038 nm) which is greater in ionic radius is substituted with Zn²⁺ (0.074 nm) thus causing the increase in the interatomic spacing or bond length between the atoms [20]. Besides that, the overall reduction in the interatomic distances will result in the increase of compactness of the glass matrix [21].

Decrease in can also be attributed to the addition of ZnO as it causes some kind of structural rearrangement of the atoms by entering the glass system and destroying the Si–O–Si bonds, thus creating ionic bonds between Zn²⁺ and single bonded oxygen atoms [20]. Next, there is also a possibility for the modification of the geometrical configuration upon swapping ZnO into the glass network and the structure of the studied glasses will not be expanded, which have more compact and low number of covalent bonds with high reduction in the number of bridging oxygens (BOs) [22]. Longitudinal velocity () and the shear velocity () of the samples were acquired and are presented in Table 3 and were plotted in Figure 3. Generally, and of majority of materials will increase as the density of the system increases but, for this study, and decrease as the density of the system increases. Similar trends were also observed for soda lime silicate and silicate glass system whereby the and of the samples decrease when the density in the sample increases [23]. Decrease in and of the samples is due to rise in amount of ZnO present in the samples which contains Zn²⁺ ions where its zinc atom had higher atomic radius compared to Si atom therefore encouraging the transformation of BOs to NBOs in the system.

Table 3: Density, molar volume, molecular weight, and ultrasonic velocity of ZnO–SiO₂ samples.

Samples
S1
S2
S3
S4

Density (g cm⁻³)
2.94
3.08
3.44
3.66

(cm³ mol⁻¹)
23.97
23.21
21.17
20.18

(g mol⁻¹)
70.43
71.59
72.79
73.91

(ms⁻¹)
3857.03
3609.90
2794.69
2482.31

(ms⁻¹)
1951.95
1611.21
1185.46
966.27

Figure 3: Longitudinal and shear velocity versus wt.% of ZnO in ZnO–SiO₂ samples.

Based on Table 3, values of are much smaller compared to the value of its counterpart and it can be considered half of the value of at the same compositions. For example, sample S1 which has a value of is 1951.95 ms⁻¹ while its is 3857.03 ms⁻¹ which shows that its shear velocity is half of the longitudinal velocity and the trend is constant throughout all samples. Next, the values of decrease from 3857.03 ms⁻¹ to 2482.31 ms⁻¹ while decreases from 1951.95 ms⁻¹ to 966.27 ms⁻¹ as the amount of ZnO increases. Increase in the amount of ZnO in the samples promotes the formation of NBOs and it is because ZnO which acts as a network former and Zn²⁺ ions are the main result which causes the increase in NBOs. In the glass system, average coordination number of SiO₂ gradually reduced to 3 from 4 as the values of ZnO rise and this causes the structural units of SiO₄ to be converted to SiO₃ initiating the rise of NBOs [24–26]. Decrease in both and with the rise of ZnO also indicates that the ultrasonic wave encounters more resistance in the ZnO–SiO₂ samples as the amount of ZnO increases [27, 28]. Not only that, rise of ZnO in the ZnO–SiO₂ samples also indicates that more Zn²⁺ ions exist in the samples and this caused overall more ions in samples to be opened up [29]. A result of lower ultrasonic velocity at higher content of ZnO indicates a major alteration in the structures of the samples.

Experimental values of longitudinal modulus (), shear modulus (), Young’s modulus (), bulk modulus (), Poisson’s ratio (), fractal bond connectivity (), and microhardness () were calculated from the data obtained by ultrasonic velocities. The results of the elastic properties of the ZnO–SiO₂ samples are shown in Table 4. As seen, from Table 4, all the values of the elastic moduli decrease with the rise in ZnO.

Table 4: Experimental longitudinal modulus (), shear modulus (), Young’s modulus (), bulk modulus (), Poisson’s ratio (), fractal bond connectivity (), and microhardness () of ZnO–SiO₂ samples.

Samples
(GPa)
(GPa)
(GPa)
(GPa)

(GPa)

S1
43.74
11.20
29.75
28.80
0.3279
1.5557
23.53

S2
40.10
7.99
21.98
29.45
0.3756
1.0851
10.58

S3
26.88
4.84
13.45
20.43
0.3903
0.9469
5.438

S4
22.54
3.42
9.64
17.99
0.4107
0.7596
2.971

Longitudinal modulus and shear modulus can be defined as an independent elastic constant which are produced by a small stress such as the elastic strain in an amorphous solid [30]. Longitudinal modulus is and for pure shear modulus it is , where and , respectively, are the longitudinal and shear velocities of the samples [31]. The longitudinal modulus (), shear modulus (), Young’s modulus (), bulk modulus (), Poisson’s ratio (), and microhardness can be obtained using the ultrasonic velocities by acquiring these equations from the following journals by Laoding et al. (2016) and Sidek et al. (2016) [32, 33]. Based on Table 4 and Figure 4 which illustrate the values and plot of longitudinal modulus and shear modulus of the ZnO–SiO₂ samples, it can be seen that as the amount of ZnO in the samples increases, the longitudinal modulus and shear modulus decrease. Decrease in longitudinal modulus from samples S1 to S4 is from 43.74 GPa to 22.54 GPa while decrease in shear modulus from samples S1 to S4 is from 11.20 GPa to 3.42 GPa. Longitudinal modulus for every sample is higher compared to its counterpart of shear modulus for every sample from S1 to S4 and this implies that the sample can withstand longitudinal stress compared to shear stress which indicates the samples are easier to be bent than elongated.

Figure 4: Longitudinal and shear modulus versus wt.% of ZnO in ZnO–SiO₂ samples.

Young’s modulus is defined as the ratio of stress against strain and it also represents the stiffness in a particular material which links to bonding strength between atoms in materials. Materials which have higher value of Young’s modulus imply that that particular material is more stiffer and this Young’s modulus is also affected by the dimensionality and connectivity of the system [33]. Not only that, samples that have higher value of Young’s modulus can endure more stress compared to samples which possess lower Young’s modulus and Figure 5 shows that as the amount of ZnO in the samples increases, Young’s modulus of the samples decreases which indicates the increase in number of NBOs [34]. Decrease in the NBOs further links to the decrease in connectivity of the samples network which is caused by the decrease in Young’s modulus. Lower Young’s modulus as ZnO increases shows that the ZnO–SiO₂ samples can reduce the speed of impacting mass thus causing a smaller stress compared to samples which have higher Young’s modulus [34]. Results of Young’s modulus can indicate that the samples can bear small stress acting against it even though its structure is less rigid and the decrease in Young’s modulus indicates that the samples can work well with strain.

Figure 5: Young’s modulus versus wt.% of ZnO in ZnO–SiO₂ samples.

Bulk modulus () is known as the alteration in volume of a material when a small or moderate force is performed upon the specific surface. Figure 6 shows that as the amount of ZnO in the system increases, the bulk modulus of the samples increases and the bulk modulus of the samples is higher compared to Young’s modulus which indicates that the samples work well with stress from multiple directions but not in one direction. Hence this clearly means that glass and glass ceramic acquired are usually hard if stress is applied from numerous directions simultaneously but would fracture if stress is applied at a single direction. Bergman and Kantor (1984) proposed the analysis of fractal bond connectivity with ratio of bulk to shear modulus and it can be simplified as where it gives the effective dimensionality of particular materials for any nonhomogeneous random mixture of fluid and a solid backbone near the percolation limit [35]. Value of acts as a parameter for network connectivity with a range of values obtained by the ratio [36]. Values of differ for each kind of materials subjected on its dimension and d = 1 is for 1D chain and and for 2D and 3D chain structures correspondingly [37–39]. Results shown in Figure 7 and Table 4 indicate that the fractal bond connectivity of the ZnO–SiO₂ samples ranges from 0 to 1 which shows that ZnO–SiO₂ samples possess a 1D layer structure [40]. As ZnO increases in the samples, fractal bond connectivity decreases and this will cause cross-links of the samples to be weakened and possibly break [23].

Figure 6: Bulk modulus versus wt.% of ZnO in ZnO–SiO₂ samples.

Figure 7: Fractal bond connectivity versus wt.% of ZnO in ZnO–SiO₂ samples.

Poisson ratio is the measure of ratio of the shear strain to the longitudinal strain when tensile force is applied and it makes use of the degree of cross-link density of glass and glass ceramic network to find out the order of cross-link density [41]. Poisson’s ratio measures the capability of a material to counter the alteration in volume when an incoming load acts on a certain material and the Poisson ratio (v) acquired can be in positive or negative [42]. In this study it is in the range of 0.327 to 0.410.

From Figure 8, it is observed that, as ZnO increases in the samples, results in higher values of Poisson’s ratio show that the samples have a lower resistance towards lateral expansion when compressed compared to samples with lower amount of ZnO. Rise in Poisson’s ratio also shows that the decrease in cross-link density and lateral strength with the increase in ZnO as network former does not have much significance in its cross-link density [43]. Relationship between Poisson’s ratio and cross-link density was first discussed by Bridge et al. (1983) and its relationship is known as the number of bridging bonds per cations in the structure of the system where results of the cross-link density 0, 1, and 2 are associated with the values of Poisson’s ratio obtained, 0.40, 0.30, and 0.15, correspondingly [44]. Average value of Poisson’s ratio acquired in these samples is 0.34 which suggests that the samples have 1D layer structure and values of this result correlate with the results from fractal bond connectivity which is around 1.

Figure 8: Poisson’s versus wt.% of ZnO in ZnO–SiO₂ samples.

Microhardness () is known to be the total stress which is necessary to remove the free volume or distortion of the glass and glass ceramic network [45]. Based on Figure 9, the microhardness of the samples decreases as the amount of ZnO increases in the system and indicates a decrease in the connectivity of the glass and glass ceramic system. Application of hydrostatic pressure is necessary to decrease the free volume in the glass and glass ceramic system [46].

Figure 9: Microhardness versus wt.% of ZnO in ZnO–SiO₂ samples.

After completing experimental elastic moduli, it is always interesting to predict the results of elastic moduli without performing experimental methods. Theory of elastic prediction has been brought up by Makishima and Mackenzie (1973, 1975) on the prediction of elastic moduli of oxide glass by utilizing composition of oxides and packing density of chemical composition of the glass [47, 48].

Rocherulle et al. (1989) improved the packing density of the equation approximately 20 years later and incorporated as

where and are Pauling’s ionic radius of cation A and anions O, and are the density and effective molecular weight, and is the new packing density [49]. This model offers a new derivation of elastic moduli and Poisson ratio’s for the current system as

where , , , and are the total packing density, total dissociation energy per unit volume, dissociation energy per unit volume, and the mole fraction of the oxide th component correspondingly.

Table 5 illustrates the theoretical calculated total packing density, , longitudinal modulus, , shear modulus, , Young’s modulus, , bulk modulus, , and Poisson’s ratio, , based on Rocherulle’s model. Based on the values of theoretical elastic moduli and Poisson’s ratio of ZnO–SiO₂ samples obtained, it can be observed that the all the theoretical elastic moduli and Poisson’s ratio decrease when composition of ZnO increases. Longitudinal modulus calculated decreases from 46.53 GPa to 40.93 GPa, shear modulus decreases from 15.57 GPa to 13.88 GPa, Young’s modulus decreases from 36.83 GPa to 32.71 GPa, bulk modulus decreases from 25.78 GPa to 22.42 GPa, and Poisson’s ratio decreases from 0.2626 to 0.2576. Decrease in elastic moduli and Poisson’s ratio as ZnO increases suggests that ZnO would act as network modifier thus breaking BOs and converts it to NBOs which will decrease the connectivity and elastic moduli of the samples. Elastic moduli and Poisson’s ratio predicted by using Rocherulle’s model were illustrated in Figures 10 and 11. Comparisons of the experimental elastic moduli and Poisson’s ratio and the theoretical elastic moduli and Poisson’s ratio were illustrated in Figures 12–16. Experimental elastic moduli and theoretical elastic moduli have a great agreement in similar trend but vary in value except for Poisson’s ratio.

Table 5: Theoretical calculated total packing density, elastic moduli, and Poisson’s ratio of ZnO–SiO₂ samples.

Sample

Theoretical elastic moduli and Poisson’s ratio

(GPa)
(GPa)
(GPa)
(GPa)

S1
0.5851
46.53
15.57
36.83
25.78
0.2626

S2
0.5819
44.96
15.10
35.68
24.83
0.2613

S3
0.5770
42.68
14.41
34.00
23.46
0.2592

S4
0.5731
40.93
13.88
32.71
22.42
0.2576

Figure 10: Elastic moduli versus wt.% of ZnO calculated using Rocherulle’s model.

Figure 11: Poisson’s ratio versus wt.% of ZnO calculated using Rocherulle’s model.

Figure 12: Experimental and theoretical longitudinal modulus versus wt.% of ZnO in ZnO–SiO₂ samples.

Figure 13: Experimental and theoretical shear modulus versus wt.% of ZnO in ZnO–SiO₂ samples.

Figure 14: Experimental and theoretical Young’s modulus versus wt.% of ZnO in ZnO–SiO₂ samples.

Figure 15: Experimental and theoretical bulk modulus versus wt.% of ZnO in ZnO–SiO₂ samples.

Figure 16: Experimental and theoretical Poisson’s ratio versus wt.% of ZnO in ZnO–SiO₂ samples.

4. Conclusion

(ZnO)x(WRHA)1−x ( = 0.55, 0.60, 0.65 and 0.70 wt.%) was symbolized by S1, S2, S3, and S4, respectively, samples have been successfully fabricated, and the study of elastic moduli with prediction of its correlation with the variation of composition on physical and elastic characteristics of each sample was performed and analyzed. Physical analysis of the samples shows that as ZnO increases, the density of the overall samples decreases and this is very well associated with the formation of NBOs and its molar volume increases as ZnO increase which is caused by the substitution of ions of Zn²⁺ which is greater in interatomic spacing compared to SiO²⁺. Last but not least, all the theoretical elastic moduli possess the same trend as the elastic moduli obtained experimentally suggesting that ZnO would act as network modifier thus breaking BOs and converts it to NBOs which will decrease the connectivity and elastic moduli of the samples.

Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this paper.

Acknowledgments

The researchers gratefully acknowledge the financial support for this study from the Malaysian Ministry of Higher Education (MOHE) and Universiti Putra Malaysia through the Fundamental Research Grant Scheme (FRGS) and Geran Putra Berimpak research grant.

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