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By plotting the deformation process of graphene at various strain levels, the failure behavior is discussed.
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Taking into account the fibre-to-channel losses for both devices as previously measured, we can plot the peak deformation of the cell as a function of the power per side at the channel PC (Fig. 6 ).
In Fig. 3(b) we plot the equilibrium deformation DF ∞ as a function of the net applied optical force, F optical where, in the case of fixed cell parameters, F optical is an indication of the total optical power used.
A rough estimation of the energetic cost associated with the deformation of this angle was obtained by plotting the distribution of its values and by deriving energies according to the Maxwell-Boltzmann relationship.
Plotting the values ofhkl cos as a function of 4sin/Ehkl, the uniform deformation stress can be calculated from the slope of the line and from lattice strain.
Figure 4 Contour plots of the deformation charge density (∆ ρ 1 and ∆ ρ 2 ).
A time series plot of the deformation rates for region A associated with each interferogram (Online Resource 3) has been generated (Fig. 11a).
The objective of this experiment was to determine the predominant swelling mechanism by plotting deformation over time.
The linear component of the deformation is plotted as a dashed line with triangular markers in Fig. 2.
For this, the maximum σ1′ and σ3′ of the deformation steps were plotted in a p′-q′ diagram (e.g., Burland 1990; Figure 4), where p′ and q′ are Figure 4 p ′- q ′ plot determined from maximum σ 1 and σ 3 conditions achieved during triaxial testing in each deformation stage.
Furthermore, the seafloor appears to follow the morphology of the TIC indicating that seafloor topography is controlled by the underlying horst-graben morphology.To investigate effects of the subducting plate on the deformation front, we plot the location of the deformation front and the underlying structures (Figure 9).
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