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Application 2. Consider the following nonlinear fractional-order 2-by-2 stiff system: (4.14).
Consider the following linear fractional-order 2-by-2 stiff system: (4.1).
L=128, left: Map of log10[ V x,y)] for a stiff system.
In particular, it may lead to a stiff system of differential equations and several other problems.
The model obtained from basic thermodynamical equations has the main disadvantage of being a stiff system.
The discrete model is a non-linear, large, sparse and stiff system of coupled differential equations.
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Thus, the effects of torsional coupling are higher for torsionally flexible and strongly coupled systems as compared to torsionally stiff systems installed with passive and semi-active stiffness dampers.
Further, the effects of torsional couplings are also studied for torsionally flexible, strongly coupled, and torsionally stiff systems installed with passive and resetting semi-active stiffness dampers.
Figure 9 Velocity map for stiff systems.
Figure 6 Burst distributions for stiff systems.
Figure 6 shows the burst distribution for stiff systems.
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