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Furthermore, in the case of sheets with FRP anchors, strains in the proximity of the FRP anchors can increase beyond those encountered at the sheet centerline.
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The procedure increases the total exfoliation yield by up to 15% (regardless of the GO sheet size) compared to continuous sonication and by up to 45% in the case of GO sheets of maximum lateral size.
In particular, in the case of ice sheets and ice caps (> 1000 km2), one potentially important topographic control on where in a landscape moraines are deposited is erosional feedback, whereby subglacial erosion causes ice masses to become less extensive over successive glacial cycles.
The values of skin-friction coefficient are higher for Al-water and lower for Au-water in stretching sheet and in the case of shrinking sheet; the values of ( -{mathit{mathsf{F}}}^{hboxhboxleft(mathsf{0}right) ) are higher for Au-water and lower for Al-water compared to other nanofluids.
It is seen that the first-order slip and the nanoparticle volume fraction parameters have an opposite effect on the velocity profile of Au-water in the case of shrinking sheet upper branch solution compared to stretching sheet.
It is observed that the second-order slip parameter increases the thermal boundary-layer thickness in the case of stretching sheet and decreases the thickness of the thermal boundary-layer in the case of shrinking sheet upper and lower branch solutions.
Figure 4a, b depicts the effects of γ and φ on the velocity profile in the case of shrinking sheet.
Figure 6a, b is plotted for F′ for different values of δ and φ in the case of shrinking sheet.
The effects of second-order slip parameter δ and nanoparticle volume fraction on F′ are shown in Fig. 5 in the case of stretching sheet.
In the case of shrinking sheet (both upper and lower branch), the reduced Nusselt number increases with γ, |δ| and Pr, and it decreases with φ.
The temperature increases as φ increases and decreases as γ increases in the case of shrinking sheet (upper and lower branch solutions [Fig. 7b, c]).
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