Tran Van Hauac,
Pham Van Trinh*a,
Nguyen Phuong Hoai Namc,
Nguyen Van Tua,
Vu Dinh Lamb,
Doan Dinh Phuongab,
Phan Ngoc Minhb and
Bui Hung Thang*ab
aInstitute of Materials Science, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet Str., Cau Giay Distr., Hanoi, Vietnam. E-mail: trinhpv@ims.vast.vn; thangbh@ims.vast.vn; Tel: +84 94 319 0301
bGraduate University of Science and Technology, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet Str., Cau Giay Distr., Hanoi, Vietnam
cVNU University of Engineering and Technology, 144 Xuan Thuy Str., Cau Giay Distr., Hanoi, Vietnam
First published on 9th June 2020
In this study, the effect of graphene nanoplatelet (GNP) size on the microstructure and hardness of the electrodeposited nickel–graphene nanocomposite coatings were investigated. GNPs with different sizes were prepared by using a high energy ball milling technique. The experimental result revealed the high energy ball milling technique could reduce the size, increase the surface area, and improve the dispersion ability of GNPs. The microstructure, hardness, and components of the nanocomposite coatings were greatly affected by GNP sizes. The highest microhardness was measured to be 273 HV for the nanocomposite coatings containing 5 h-milled GNPs, which is increased up to ∼47% compared to pristine Ni coating. The enhancement in the hardness is attributed to the uniform dispersion of the small GNP sizes inside the Ni matrix and the Ni grain size reduction when using milled GNPs.
In the composite field, the properties of reinforcement material play an important role in the strengthening effects. Some studies have demonstrated the influence of Gr aspect ratio on the microstructure and mechanical properties of the Gr/metal composite and Gr/polymer composites. In 2014, G. Dai et al. reported the influence of the aspect ratio, shape, clustering, orientation and volume fraction of graphene platelets on the mechanical behavior and damage mechanisms of nanocomposites by 3D computational model of graphene reinforced polymer composites.37 In 2015, F. Wang et al. demonstrated that graphene nanoplatelets (GNPs)/epoxy composites had higher modulus and strength with increasing concentration of small GNP sizes.38 In addition, the effect of the aspect ratio of GNPs on mechanical properties and toughening mechanisms of GNPs/epoxy was also reported by H. Chong et al. in 2016.39 To our best knowledge, up to now, there are no experimental studies on the investigation of the effect of the size of GNPs on the properties of the metal composite coatings as well as Ni composite coatings. Thus, this work has been done to investigate the influence of GNPs sizes on the microstructure, microhardness and content of Ni composite coatings. GNPs with different sizes was prepared by high energy ball milling technique for different milling times. The prepared GNPs were functionalized with carboxyl (–COOH) functional groups then dispersed into Watts solutions and co-deposited with ion Ni2+ onto the cathode surface via electrodeposition technique to form Ni/GNPs nanocomposite coatings. The morphologies, structure and properties of GNPs and Ni/GNPs composite coatings were characterized and presented.
Fig. 1 Illustration of the fabrication process of GNPs reinforced nickel coating with the different GNPs size using the electrodeposition technique. |
Coating sample | Functionalized GNPs material | Watts solution | Current density | Temp. | pH | Stirring speed | Plating time | ||
---|---|---|---|---|---|---|---|---|---|
GNPs sample | Milled duration | Concentration | |||||||
Ni | — | — | — | 1 l | 2.5 A dm−2 | 45 °C | 4–5 | 100 rpm | 90 min |
Ni-GNPs1 | GNPs1 | 1 h | 0.3 g l−1 | ||||||
Ni-GNPs2 | GNPs2 | 2 h | |||||||
Ni-GNPs3 | GNPs3 | 3 h | |||||||
Ni-GNPs4 | GNPs4 | 4 h | |||||||
Ni-GNPs5 | GNPs5 | 5 h |
Fig. 2 FESEM images of (a) pristine GNPs and GNPs milled with different times of (b) 1 h, (c) 3 h and (d) 5 h. |
The thickness of GNPs treated with the different milling times is evaluated by AFM as shown in Fig. 3. The thickness of the initial GNPs is measured to be around 12 nm (Fig. 3a). Fig. 3e shows the thickness statistics of milled GNPs which are collected from 100 plates GNPs on the SiO2 substrates for each sample. As can be seen, the thickness of GNPs1 fluctuates from around 5 nm to about 12 nm. In the case of increasing the milling time, the thickness spectrum peaks move to the left direction, which implies the decrease of GNPs thickness. In the GNPs3 case, the thickness is distributed in a range from 2 nm to 6 nm and reached a peak of around 4.5 nm which occupy about 12%. For GNPs5, the thickness ranges from around 0.5 nm to about 4 nm and reaches a peak of 1 nm which occupies over 12%. The obtained results indicate that the GNPs thickness is decreased with the increase of the milling times.
Fig. 3 The typical AFM images of (a) GNPs (b) GNPs1, (c) GNPs3, (d) GNPs5 and (e) the thickness distributions of GNPs with different milling times. |
Raman spectra analysis is carried out to evaluate the influence of the ball milling process on GNPs structure. Fig. 4 shows the Raman spectra of GNPs with different milling times, where emerged the typical peaks of GNPs including G peak at 1580 cm−1 assigned to the graphite structure, and D peak at the range of 1340 cm−1 assigned to the defects in GNPs structure and the presence of impurity or amorphous carbon.41–43 The measured results indicated that the structure of GNPs is slightly changed with different milling times. There is almost no D peak in the initial GNPs which implies the high quality and purity of the as-received GNPs. For the milled GNPs, Raman spectra emerge D peaks in which the intensities increase with the milling times. The ID/IG intensity ratios were calculated to be 0.028, 0.058, 0.088, 0.082 and 0.085 corresponding to GNPs1, GNPs2, GNPs3, GNPs4 and GNPs5, respectively. However, the increase of the ID/IG ratio of the milled GNPs is quite small compared to that of initial GNPs. This means the defects in the structure of GNPs are inconsequential. It is interesting to note that, the G peak of the milled GNPs is slightly moved to lower wavenumber. This could be due to the compressive strain induced in the ball milling process caused a shift in the G-band position.44–46 X-ray diffraction was also employed to characterize the structural changes of GNPs during the ball milling process. Fig. 5 exhibits that compared to the diffraction peak of pristine GNPs, the interlayer diffraction (002) peak of the milled GNPs is broadened and the (004) peak gradually disappeared while the intensity of (002) declines with the milling time, these are attributed to the decrease of GNPs layer thickness.47,48
GNPs were functionalized the –COOH functional groups to enhance the dispersed ability into the plating solution. Fig. 6 shows the FTIR spectra of milled GNPs functionalized with COOH functional groups. The absorption peaks around 3400 cm−1, 1720 cm−1, 1365 cm−1 and 1080 cm−1 of wavenumber are assigned to the presence of the –OH groups of residual water, the CO bonding in –COOH groups, the –OH bonding and the C–O stretching vibrations mode in the –COOH groups, respectively. Besides, the peaks at 1630 cm−1 are assigned to the CC bonding of carbon atoms in the graphite structure.49–52 In the case of pristine GNPs, there is no presence of functional groups formed between oxygen, hydrogen and carbon element besides the CC bonding of carbon atoms. These results reveal that the –COOH functional groups are formed on the surface of GNPs after the functionalization process.
The functionalized GNPs with different sizes (GNPs1, GNPs2, GNPs3, GNPs4, GNPs5) are dispersed into distilled water in order to evaluate the dispersed ability and stability. Fig. 7a shows the size distribution of GNPs with different milling times. The peaks of the GNPs size spectra shift steadily to the small size direction, and the FWHMs narrow gradually as increasing the milling times. GNPs sizes reach a saturated size after milling time of 5 hours, its sizes were unable to reduce any more. However, FWHM narrows slightly, the peak of GNPs5 size spectrum stays at around 120 nm occupy about 15% while GNPs5 sizes over 500 nm fall dramatically occupied 2.5% amount of GNPs5. In addition, the size distribution of GNPs1, GNPs2, GNPs3, GNPs4, GNPs5 has only one peak that indicates the good dispersion of the functionalized GNPs in distilled water without any agglomerations. Besides, the measured zeta potential values of GNPs increase gradually from 17 mV to 29 mV corresponding to GNPs1 and GNPs5 (Fig. 7b). This means the milled GNPs have a pretty stable state in water.53–56 This is attributed to the decrease of GNPs sizes leading to the increase of surface area and the increase of the –COOH functional groups attached to the surface and boundary of GNPs. The obtained results demonstrate that the high energy ball milling method is an effective method to reduce the GNPs size, exfoliate GNPs into the thinner plates, increasing the surface area, the dispersion ability, and stability of GNPs in distilled water.
Fig. 7 (a) Size distribution and (b) Zeta potential and BET surface area of GNPs with different milling times. |
Fig. 8 FESEM images of the surface coatings (a) Ni, (b) Ni/GNPs1, (c) Ni/GNPs2, (d) Ni/GNPs3, (e) Ni/GNPs4, (f) Ni/GNPs5. |
Fig. 9 shows the cross-section images of the coatings. The presented results are obtained from the average value of ten points along with the cross-section image at the same position on patterns. The thickness was measured to be 33.42 μm, 30.05 μm, 31.33 μm, 32.01 μm, 32.92 μm, 33.24 μm corresponding to Ni, Ni/GNPs1, Ni/GNPs2, Ni/GNPs3, Ni/GNPs4, Ni/GNPs5 nanocomposite coating, respectively. The thickness of the GNPs reinforced Ni coatings are thinner than that of the pristine Ni coating. This result demonstrates that the presence of GNPs has declined slightly the current efficiency. In addition, as can be seen in cross-section images, the thickness of the coating depends on GNPs sizes, the smaller the GNPs sizes are, the thicker the coatings are. This indicates that the small GNPs sizes can increase the current efficiency in Watt solutions.
Fig. 9 Cross-sectional optical images of (a) Ni, (b) Ni/GNPs1, (c) Ni/GNPs2, (d) Ni/GNPs3, (e) Ni/GNPs4, (f) Ni/GNPs5. |
In order to evaluate the carbon content of the coatings, the EDS analysis is carried out. As shown in Fig. 10, there is not any carbon component inside the Ni coating, the nickel content occupies 100 wt%. For the GNPs reinforced Ni coatings, the carbon contents occupy from around 6.77 wt% to about 16.41 wt% of coatings. Although all of the Watts solutions have the same GNPs concentration, the carbon contents in coatings vary with each the GNPs sizes. The smaller the GNPs sizes are, the higher the carbon content in the coatings are. This is attributed to the high surface area of the small GNPs sizes leading to the high absorption ability in the co-deposited process of nickel ion and GNPs materials.
Fig. 11 shows the XRD patterns of Ni coating and GNPs reinforced Ni coatings. All patterns show the typical peaks of nickel components which grow along the (111), (200) and (220). It is noted that there is a slight change of preferred orientation nickel growth in coatings. For pristine Ni coating, the preferred orientation grows along (111) with the highest intensity, the next preferred orientation grows along (200) and the preferred orientation grows along (220) with the lowest intensity. In the case of the GNPs reinforced Ni coating, there is a steady decrease in the intensity of the preferred orientation growing along (200), which compared to the preferred orientation growing along (220). This demonstrates that the smaller the GNPs sizes are, the more significantly the preferred orientation growing along (200) decreases.
Basing on the XRD patterns of coatings and incorporating to Debye–Scherrer equation in which: L is the average crystalline size, K is the Scherrer constant, λ is the wavelength, β is Full width at half maximum and θ is the diffraction angle,23,29 the average nickel crystallite size of the coatings is calculated. The change of the average nickel crystallite size with the GNPs sizes as shown in Fig. 12. For the pure Ni coating, the average crystallite size is around 25.61 nm. As containing GNPs content, the average crystallite size decreases significantly to about 18.35 nm for Ni/GNPs1 coating. In the case of Ni/GNPs2, Ni/GNPs3, Ni/GNPs4, and Ni/GNPs5, the average crystallite size declines gradually to around 17.23 nm, 15.35 nm, 13.49 nm, and 12.74 nm, respectively. The obtained results again confirmed the influence of the GNPs sizes on the nickel crystal growth.
Microhardness of Ni and the Ni/GNPs nanocomposite coatings are shown in Fig. 12. The obtained results are the average of 20 measured points in a composite coating sample. For the pristine Ni coating, the hardness is 186 HV. For Ni/GNPs nanocomposite coatings, the microhardness is measured to be 229 HV, 238 HV, 256 HV, 268 HV, 273 HV corresponding to Ni/GNPs1, Ni/GNPs2, Ni/GNPs3, Ni/GNPs4, Ni/GNPs5 nanocomposite coatings, respectively. As a result, the nanocomposite coatings containing 5 h-milled GNPs have the highest microhardness, which is increased up to 47% compared to pristine Ni coating. Table 2 presents the reported microhardness of nickel–graphene nanocomposite coatings. Comparing to other reports, the obtained results are in line with the earlier report by Dong et al.,58 in which using graphene as an additive component for the nanocomposite. Some other studies reported very high hardness coatings.23,24,29,34,35 But it is noted that they used GO as a reinforcement component, higher GO concentration and/or higher surfactant concentration. For example, Yasin et al.35 reported a very high microhardness (503 HV) for the nanocomposite coating as using GO as a reinforcement component with a concentration up to 0.4 g l−1. The influence of Gr and surfactant concentration on the microhardness of the coating has not been focused on our current study. This will be done in future work to find the best conditions for preparing the nanocomposite coating with the highest performance. The enhancement in microhardness of the coating is attributed to the uniform dispersion of the small GNPs sizes in Watts solution lead to the uniform distribution of this material inside the nickel matrix. The presence of GNPs components inside the nickel matrix results in the enhancement of microhardness of nickel coatings, this is demonstrated in previous studies23,28,56,57,59 through the strengthening mechanisms such as thermal expansion coefficient mismatch, Orowan looping, load transfer.60 In addition, the small GNPs size decreases the Ni grain size causing the formation of the grain refinement effect as demonstrated in previous sections. The relationship between the hardness and grain size are demonstrated through the Hall–Petch equation: HV = H0 + kHd−1/2, where H0 and kH are constants, d is the grain size.61 This relationship indicates that the microhardness depends considerably on the grain size, the smaller the grain sizes are, the harder the coating is. This result demonstrates that the small GNPs size plays an important role in the strengthening mechanisms for nickel coating.
No. | Plating method | Reinforced material | Microhardness of coating | Ref. | ||
---|---|---|---|---|---|---|
Pristine Ni | Ni/Graphene | % Enhancing | ||||
1 | Direct current, current density 9 A dm−2, SDS 0.4 g l−1, | rGO (0.2g l−1) | — | ∼500 HV | — | 34 |
2 | Direct current, current density 5 A dm−2, SDS 0.4 g l−1 | rGO (0.2g l−1) | — | ∼500 HV | — | 40 |
3 | Direct current, SDS 0.4 g l−1 | rGO (0.4 g l−1) | 235 HV | 503 HV | 114% | 35 |
4 | Pulse current, current density 5 A dm−2, SDS 0.2 g l−1, temperature 45 °C | rGO (0.5 g l−1) | — | 492 HV | — | 24 |
5 | Direct current, current density 5 A dm−2, SDS 0.4 g l−1, temperature 45 °C | rGO (0.2 g l−1) | — | 500 HV | — | 29 |
6 | Current density 1 A dm−2, SDS 0.2 g l−1, temperature 40 °C | rGO (0.1 g l−1) | 287 HV | 385 HV | ∼34% | 23 |
7 | Direct current, current density 5 A dm−2, temperature 55 °C | GO (1 g l−1) | 1.81 GPa | 6.85 GPa | 278% | 28 |
8 | Direct current, current density 0.15 A dm−2, SDS 0.5 g l−1, temperature 50 °C | rGO (0.05 g l−1) | 3.83 GPa | 4.6 GPa | ∼20% | 27 |
9 | Pulse current, current density 1 A dm−2, SDBS 0.05 g l−1, | rGO (0.4 g l−1) | — | 223 HV | — | 58 |
10 | One-step electrodeposited Ni/graphene composite | Exfoliated graphite | 265 HV | 427 HV | ∼61% | 60 |
11 | Electrophoretic-deposition | Gr powder | — | 181.78 HV | — | 61 |
12 | Direct current, current density 2.5 A dm−2, SDS 0.1 g l−1, temperature 45 °C | GNPs (0.3 g l−1) | 186 HV | 273 HV | ∼47% | This work |
From experimental data of crystallite size and microhardness we can derive the relationship between crystallite size and microhardness as a function of milling times by experimental data fitting as the following equations:
d = Kze(−t/1.67) + dα | (1) |
Hc = KHe(−t/2.34) + Hα | (2) |
Eqn (1) describes the dependence of the crystallite size of Ni matrix on the milling time of GNPs in which dα = 12.54 is a constant with a dimension [nm], Kz = 12.74 is a scale factor depending on properties of the reinforced material. Eqn (2) is used for predicting the change of the microhardness of the nanocomposite coating, in which Hα = 283.76 is a constant with a dimension [HV], KH = −94.95 is a scale factor depending on properties of the reinforced material. Based on eqn (1) and (2) we can predict the saturated value of crystallite size around 12.54 nm and microhardness about 283.76 HV when milling time is increased to infinity. These are also reasons why we have limited milling time for 5 hours.
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