\( \frac { d ^ { 2 } y } { d x ^ { 2 } } - 2 \frac { d y } { d x } + 2 y = 0 \)
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Bonus Knowledge
This is a second-order linear homogeneous differential equation with constant coefficients. Its characteristic equation is \( r^2 - 2r + 2 = 0 \). Solving this yields complex roots \( r = 1 \pm i \). The general solution can thus be written in the form \( y(x) = e^{x}(C_1 \cos(x) + C_2 \sin(x)) \), where \( C_1 \) and \( C_2 \) are constants determined by initial conditions. In practical scenarios, such as modeling damped harmonic oscillators, these types of equations often appear. The solution captures oscillatory motion combined with exponential decay, which can describe systems like a swinging pendulum or an electrical circuit with resistive damping. By applying this knowledge, engineers can design more effective systems that take into account the decay or growth factors established by real-world parameters!