Relating Behaviour of a Driven System to the Undriven Modes

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The discussion centers on the relationship between the behavior of driven systems and their undriven counterparts, particularly in the context of particle systems with complex interactions. It raises the question of whether the long-term behavior of a driven system can be related to its undriven state when subjected to a time-varying force. The example of a driven harmonic oscillator illustrates the presence of transient and steady-state terms, suggesting a general principle may apply. The inquiry also touches on the role of differential equations, specifically how the addition of a driving term alters the system's dynamics. The participant expresses uncertainty regarding the theoretical foundations of differential equations and seeks guidance on how to approach the topic.
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Is it generally true that if you have a system of particles with some arbitrary interactions due to their relative positions which you can solve in some way (maybe numerically, maybe analytically), you can relate the long term behaviour to the undriven case if it is being driven by a time-varying force? Like in the example of the driven harmonic oscillator, you have a transient term and a steady state term for any given driving frequency - is this a general fact? It seems like it since the differential equation governing the behaviour would simply have some driving term added:

So if you know behaviour of:
f(x,\frac{dx}{dt},\frac{d^2x}{dt^2}) = 0

Are there any immediately obvious characteristics of:
f(x,\frac{dx}{dt},\frac{d^2x}{dt^2}) = G(t)
?

I don't know if the whole business of complementary function and particular integral is specific to certain types of differential equation - my interactions involve many non-trivial terms and potentials. I'm not well grounded in the theory of differential equations and am not sure where to start. Thanks!
 
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