Anupama
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I came to know that time evolution in classical mechanics is highly non linear. Is there any case that it become linear?
Time evolution in classical mechanics is predominantly non-linear, with linearity achieved in specific cases such as harmonic oscillators. The equation of motion for a damped harmonic oscillator is given by m \ddot{x} + 2 m \gamma \dot{x} + m \omega^2 x = F(t), where F(t) represents an external force, \gamma is the damping coefficient, and \omega is the eigenfrequency. This linear approximation is valid for small oscillations around a stable equilibrium point, where the potential can be expressed as a quadratic function. The harmonic oscillator serves as a foundational concept in both classical and quantum mechanics.
PREREQUISITESThis discussion is beneficial for physics students, educators, and researchers interested in classical mechanics, particularly those focusing on oscillatory systems and their applications in both classical and quantum contexts.