Consider Mathieu’s equation for a parametric oscillator: \[ \ddot {x}+(\alpha +\beta \cos t)x=0. \]
Suppose that \(\alpha \approx 1\), \(\beta \approx 0\). Use a perturbation expansion in \(\beta \) to show that the
transition curves for Mathieu’s equation are given approximately by \[ \alpha =1-\frac {\beta ^2}{12},\qquad \alpha =1+\frac {5}{12}\beta ^2. \]
Now suppose that \(\alpha \approx 1/4+\alpha _1\beta \), \(\beta \approx 0\). In the unstable region near \(\alpha =1/4\), solutions of Mathieu’s
equation are of the form \[ c_1e^{\sigma t}q_1(t)+c_1e^{\sigma t}q_1(t) \] where \(\sigma \) is real and positive, and \(q_1,q_2\) are \(4\pi \)-periodic.
Derive the second order equation for \(q_1,q_2\) and perform a power series expansion
in \(\beta \) to show that \(\sigma \approx \pm \beta \sqrt {1/4-\alpha _1^2}\).
Use part (b) to deduce that solutions of the damped Mathieu equation \[ \ddot {x}+\kappa \dot {x}+(\alpha +\beta \cos t)x=0, \]
where \(\kappa =\kappa _1\beta +O(\beta ^2)\), are stable if to first order in \(\beta \), \[ \alpha <\frac {1}{4}-\frac {\beta }{2}\sqrt {1-\kappa _1^2} \quad \text {or}\quad \alpha >\frac {1}{4}+\frac {\beta }{2}\sqrt {1-\kappa _1^2}. \]