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  1. (1) are referred to as the reaction-diffusion equations.[1]
  2. The reaction-diffusion equations form the basis for the interpretation of the experiments reviewed above.[1]
  3. This places reaction-diffusion systems in the forefront for understanding the origin of endogenous rhythmic and patterning phenomena observed in nature and in technological applications.[1]
  4. All elements at our disposal indicate that there exists no exhaustive list and universal classification of the full set of solutions of reaction-diffusion equations.[1]
  5. We first study the effect of the original state and main parameters D, K and time t on the dynamic concentration pattern of the reaction-diffusion system.[2]
  6. When the K/D ratio increases, the reaction becomes dominant in the reaction-diffusion system and the time needed to reach steady state drops quickly.[2]
  7. To compare the computation time, we run the FEM simulation and CNN prediction to solve the reaction-diffusion equation with the same input configurations for 1,000 time steps.[2]
  8. Reaction–diffusion systems are naturally applied in chemistry.[3]
  9. Mathematically, reaction–diffusion systems take the form of semi-linear parabolic partial differential equations.[3]
  10. In addition to the reaction-diffusion equation parameters, you can also adjust the uniform scale, rotation, and X/Y offset of the image for different effects.[4]
  11. Well,if you feel that way, you will become a big fan of the reaction-diffusion systems we discussed in Section 13.6.[5]
  12. This shortcut in linear stability analysis is made possible thanks to the clear separation of reaction and diffusion terms in reaction-diffusion systems.[5]
  13. Firstly, we 'vectorize' this analysis to be applicable for a class of reaction–diffusion equations, characterized by certain conditions.[6]
  14. A reaction-diffusion model motivated by Proteus mirabilis swarm colony development is presented and analyzed in this work.[7]
  15. The theoretical results and the linear stability of these spot equilibria are confirmed by solving the nonlinear evolution of the Brusselator reaction-diffusion model by numerical means.[8]
  16. The approach adopted is extended to solve a class of non-linear reaction-diffusion equations in two-space dimensions known as the "Brusselator" system.[9]
  17. We review a series of key travelling front problems in reaction–diffusion systems with a time-delayed feedback, appearing in ecology, nonlinear optics and neurobiology.[10]
  18. In this work, we limit our review to scalar reaction–diffusion equations and concentrate on monostable and bistable front solutions.[10]
  19. Mathematical reaction–diffusion models are proposed to describe or predict the fate of some particular invasions.[10]
  20. Based on these common properties, we developed conceptual models of a mass conserved reaction–diffusion system with diffusion–driven instability.[11]
  21. Figure 2 shows one such set of patterns, obtained from a random initial distribution in a system that evolves according to a system of reaction-diffusion equations called the Gray-Scott model.[12]
  22. This suggests the intriguing possibility of organizing amorphous computing systems by starting with the particles in a random state and solving a discrete analog of a reaction-diffusion system.[12]
  23. They have been encountered in a number of physical systems and model equations but have only rarely been found in reaction-diffusion systems to date.[13]
  24. We present here examples of several types of localized patterns found in reaction-diffusion systems.[13]

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