For a second-order linear partial differential equation with principal part , the discriminant is . Here , , , so
The equation is therefore a hyperbolic partial differential equation throughout its domain. The lower-order term does not affect this classification.
The characteristic curves satisfy
Integrating gives the two families . Choose coordinates constant along these families:
Their Jacobian determinant is , so they define an invertible change of variables on , with image . Write . The chain rule gives
Both the pure second partial derivatives and the first partial derivatives cancel in the original equation, leaving
This is the full canonical form of a second-order partial differential equation, including the effect of the lower-order term. Integrating shows is a function of alone, hence
with arbitrary twice differentiable functions . The representation is global on : for each fixed , the allowed form an interval, so is independent of throughout that interval; after subtracting its antiderivative, the same reasoning in the other coordinate leaves only . These are quadratic characteristic coordinates for a variable-speed wave equation.
For the data on , set , so the other argument is . The two initial conditions become
Differentiating the first equation with respect to also gives . Solving these two linear equations yields . Since ranges over all real numbers,
Consequently
Indeed , , , so the equation and both initial conditions hold directly.

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