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This is achieved by using the energy-based method to determine the relationship between the external forcing amplitude and the positions of the crossing points of the forced response.
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Our comparative study of the EASM behaviour in the context of coeval North Atlantic and tropical ocean climate records indicates a complex relationship between the EASM, the external forcing factor (Northern Hemisphere summer insolation), and internal feedback mechanisms which involve both high-latitude (AMOC) and low-latitude (ENSO) processes.
The mode of electrical activity of each neuron is dependent on the external forcing, connection coupling between neurons and noise in the network or external uncertain driving.
All the key points of the relationship between the external force and the maximum interface slip are defined in closed-form for both the above mentioned cases.
Initially, before the cracking, a linear elastic response was observed, corresponding to a deformation at each monitoring point proportional to the applied lateral force, being quantified the relation between the external force and the deformation at each point.
The present paper, starting from the most common assumptions of the mechanical behaviour of the various materials, proposes a fully-analytical formulation for determining the response in terms of the relationship between the external force and the corresponding maximum interface slip observed in those tests.
Figure 6 shows the relationship between the external force and the displacement of the urethane sponge.
First, the relationship between the external force and the displacement of the urethane sponge is measured and a model of the deformation is discussed.
As shown in Figure 7, the characteristics are linear below 25.0 N and nonlinear above 25.0 N. Thus, displacement could be estimated accurately using the relationship between the external force and the displacement of the urethane sponge for forces smaller than 25.0 N. Figure 7 Relationship between external force and displacement of urethane sponge from 0.0 N to 40.0 N.
It is important to note that in the sagittal plane, the proportional factor between the external force and the strains measured at heel loading and forefoot loading were not the same, since the strain gauges were attached to two different areas of the foot.
The algorithm starts by some initial contour, then the curve evolves under the influence of the internal (contour curvature) and external (image gradient) forces until it reaches the boundary of the object where balance between the internal and the external forces is achieved.
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