Autonomous differential equations

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SUMMARY

The discussion centers on the analysis of the autonomous differential equation \(\frac{dy}{dt} = e^y - 1\). The user seeks assistance in plotting the function and determining the critical points, specifically questioning the stability classification of the critical point at \(y = 0\). The user concludes that for \(y_0 < 0\), the function is decreasing and concave down, while for \(y_0 > 0\), it is increasing and concave up. The consensus reached is that the critical point at \(y = 0\) is indeed unstable, contrary to the user's initial belief of it being semistable.

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  • Understanding of autonomous differential equations
  • Familiarity with stability analysis of critical points
  • Knowledge of plotting functions and interpreting their behavior
  • Basic calculus concepts, including derivatives and concavity
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  • Study the stability criteria for critical points in differential equations
  • Learn about phase portraits and their significance in dynamical systems
  • Explore the implications of concavity on the behavior of solutions
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Consider the autonomous differential equation that follows

[tex]\frac{dy}{dt} = e^y - 1, \qquad -\infty < y_0 < \infty \mbox{.}[/tex]

I'm supposed to plot [tex]f(y)[/tex] versus [tex]y[/tex], and determine the critical (equilibrium) points, and classify each one as asymptotically stable or unstable. Anyhow, you can find my plot at

http://mygraph.cjb.net/

which gives

[tex]y_0 < 0 \Longrightarrow \left\{ \begin{array}{ll} y^{\prime} < 0 & \mbox{(y is decreasing),} \\ y^{\prime \prime} < 0 & \mbox{(y is concave down),} \end{array} \right.[/tex]

and

[tex]y_0 > 0 \Longrightarrow \left\{ \begin{array}{ll} y^{\prime} > 0 & \mbox{(y is increasing),} \\ y^{\prime \prime} > 0 & \mbox{(y is concave up).} \end{array} \right.[/tex]

However, I picture the critical point [tex]y = \phi (t) = 0[/tex] to be semistable. The book says it is unstable, but I really can't find my mistake.

Any help is highly appreciated.
 
Last edited:
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thiago_j said:
Consider the autonomous differential equation that follows

[tex]\frac{dy}{dt} = e^y - 1, \qquad -\infty < y_0 < \infty \mbox{.}[/tex]



[tex]y_0 < 0 \Longrightarrow \left\{ \begin{array}{ll} y^{\prime} < 0 & \mbox{(y is decreasing),} \\ y^{\prime \prime} < 0 & \mbox{(y is concave down),} \end{array} \right.[/tex]

and

[tex]y_0 > 0 \Longrightarrow \left\{ \begin{array}{ll} y^{\prime} > 0 & \mbox{(y is increasing),} \\ y^{\prime \prime} > 0 & \mbox{(y is concave up).} \end{array} \right.[/tex]

However, I picture the critical point [tex]y = \phi (t) = 0[/tex] to be semistable. The book says it is unstable, but I really can't find my mistake.

When a negative number decreases its absolute value increases so it goes away further from the origin.

ehild
 
Absolutely! I see it now. Thanks
 

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