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09/29/11 - Autonomous ODEs
General first-order ODEs have the form y' = f(t,y).
First-order ODEs of the form y' = f(t) can be solved simply with integration.
First-order ODEs of the form y' = f(y) are called autonomous because they depend explicitly only on y.  There is no explicit dependence on the independent variable t.
An interesting property of autonomous ODEs is that their direction fields do not vary in the horizontal (t) direction.
Hence, a solution with initial condition y(3) = 1 is just a time-shifted version of a solution with initial condition y(0) = 1.
The roots of the function y' = f(y) = 0 correspond to equilibrium values (where the solution y approaches a constant), since no change occurs once y' = 0 (zero rate of change).
Since there is no change in the direction field or the solution as the initial condition is shifted in time, graphs of autonomous solutions can be reduced to one dimensional representations, called phase lines, which show only the vertical change.
Application of Autonomous First-order ODEs
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