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In this appendix, we solve the long-run equilibrium of the model presented in Sect.
The pink (solid) curve shows the position of the unique equilibrium of the model.
Section 3 deals with the global attractivity of disease-free equilibrium of the model.
More precisely, the local stability of the Schrödingerean equilibrium and endemic equilibrium of the model are discussed in detail.
It is shown that stability switching occurs for the interior equilibrium of the model with delay-dependent coefficient.
Subsequently, any solutions starting at a positive initial point eventually tend to the positive coexistence equilibrium of the model.
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We also show that for R0 < 1, the disease free-equilibrium of the model is both locally as well as globally stable.
Figure 1 shows the global asymptotical stability of the equilibrium for the model (1) with τ = 0, τ = 20, respectively.
Figure 2 shows the globally asymptotical stability of the equilibrium for the model (1) with τ = 0, τ = 20, respectively.
We investigate the stability of the equilibrium points of the model by using the linearization method for noncoexistence of equilibrium points and the Lyapunov direct method for the positive coexistence of an equilibrium point.
The bottom line is the equilibrium sensitivity of the model was a bit on the high side (about 4C/2xCO2---most models now have it closer to 3C) while the forcing scenario (B) was a bit on the low side.
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symmetry of the model
steady state of the model
equilibrium of the predator-prey
equilibrium of the solution
equilibrium of the body
equilibrium of the type
equilibrium of the church
equilibrium of the mixture
equilibrium of the system
equilibrium of the soul
equilibrium of the rank
equilibrium of the organism
equilibrium of the ring
equilibrium of the game
equilibrium of the three-stage
equilibrium of the force
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Justyna Jupowicz-Kozak
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