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In particular it needed to model the forces pilots would feel in the flight stick when they broke into a sharp turn or fell victim to a sickening stall.
In order to fulfill the maneuvers of space robotic systems it is hence necessary to properly model the forces acting on the space robot, from the main terms, such as the orbital motion, to the second order perturbations, like the gravity gradient and the orbital perturbations; also flexible excitation of the links and of the joints can be of great importance in the manipulators dynamics.
Structural analyses of such complexes may enable us to model the forces driving their assembly and stability which in turn may help us to understand these processes better.
We model the forces generated by internal oscillations as being biased in the direction parallel to the nanoridges.
To accomplish this, we used the DLVO theory to model the forces that govern interactions of opposing bilayers.
According to Koch's model, the forces along the lateral aspect of the femur taper distally from the highly tensile subtrochanteric region, becoming compressive along the distal lateral metaphysis.
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The FEMA 356 method also employs nonlinear shear springs to model the force-displacement response of individual piers.
In the GFMD model, the force is much smaller than that of the asperity model, while the contact cluster number in the GFMD model is much larger.
Thus, note that using the harmonic potential model, the force increases quadratically (or exponentially in the presence of atmospheric obscuration) as the link distance increases.
In that model, the force can be computed provided the materials shear yield stress, work hardening index, and fracture toughness in the plane of cut are known.
To model the forcing function in such cases, a method is presented which solves for an equivalent forcing function based on sound power measurements.
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