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The general solution is
.
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The Deep Dive
To solve the differential equation
, we start by recognizing that this is a second-order linear homogeneous differential equation with constant coefficients. The characteristic equation is
. Solving for
gives us
, leading to
.
The general solution to the differential equation can then be written as:
where
and
are arbitrary constants determined by initial conditions.
This solution represents a simple harmonic motion, where the object oscillates with a frequency determined by the coefficient of
. You can visualize the function as a wave oscillating between positive and negative values, depending on the constants
and
.