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Dynamical Systems in Neuroscience:

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One-Dimensional <strong>Systems</strong> 87follow approach similar to that <strong>in</strong> Nonl<strong>in</strong>ear Dynamics and Chaos by Strogatz (1994):Instead of go<strong>in</strong>g from l<strong>in</strong>ear to non-l<strong>in</strong>ear systems, we go from one-dimensional nonl<strong>in</strong>earsystems (this chapter) to two-dimensional non-l<strong>in</strong>ear systems (next chapter).Rather than burden<strong>in</strong>g the theory with a lot of mathematics, we use the geometricalapproach to stimulate the reader’s <strong>in</strong>tuition. (There is plenty of fun math <strong>in</strong> exercisesand <strong>in</strong> the later chapters.)Exercises1. Consider a neuron hav<strong>in</strong>g Na + current with fast activation k<strong>in</strong>etics. Assume that<strong>in</strong>activation of this current, as well as (<strong>in</strong>)activations of the other currents <strong>in</strong> theneuron are much slower. Prove that the <strong>in</strong>itial segment of action potential upstrokeof this neuron can be approximated by the I Na,p -model (3.5). Use Fig. 3.15to discuss the applicability of this approximation.2. Draw phase portraits of the systems <strong>in</strong> Fig. 3.36. Clearly mark all equilibria,their stability, attraction doma<strong>in</strong>s, and direction of trajectories. Determ<strong>in</strong>e thesigns of eigenvalues at each equilibrium.F(V) F(V) F(V)V V Va b cFigure 3.36: Draw phase portrait of the system ˙V = F (V ) with shown F (V ).3. Draw phase portraits of the follow<strong>in</strong>g systems(a) ẋ = −1 + x 2 ,(b) ẋ = x − x 3 .Determ<strong>in</strong>e the eigenvalues at each equilibrium.4. Determ<strong>in</strong>e stability of the equilibrium x = 0 and draw phase portraits of thefollow<strong>in</strong>g piece-wise cont<strong>in</strong>uous systems{ 2x, if x < 0(a) ẋ =x, if x ≥ 0⎧⎨ −1, if x < 0(b) ẋ = 0, if x = 0⎩1, if x > 0{ −2/x, if x ≠ 0(c) ẋ =0, if x = 0

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