Find the general solution of
Try an exponential trial solution. For a linear ODE with constant coefficients, always turns the equation into an algebraic one:
Form the characteristic equation. Substituting and factoring out , which is never zero:
Solve for .
Purely imaginary roots signal pure oscillation with no growth or decay.
Convert the complex exponentials to real form. For roots the real general solution is . Here and , so the exponential envelope is :
Verify by direct substitution. With : , so . With : , again . Because the equation is linear, any combination of the two also works. Physically this is simple harmonic motion of angular frequency and period .
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