For the two travelling profiles, the initial conditions imply
Since , is constant. One may therefore choose
where the constants cancel in the sum. The D'Alembert formula then gives
This agrees exactly with the restricted-domain solution from part (b). The whole-line cosine profile already has zero spatial derivative at both and for every time, so its restriction satisfies the Neumann boundary conditions without further modification.
The standing wave oscillates about the constant level , with time period . Suitable snapshots are
The nonconstant amplitude shrinks to zero at a quarter-period, reverses sign at half a period, and returns after a full period. The nodes of a standing wave of the oscillatory part, , remain at height .
Figure 1.
Time evolution of the whole-line Neumann-compatible standing wave
. Snapshots at phases , , and illustrate contraction, flattening and reversal of the cosine profile. A full-period snapshot repeats the initial curve. Details.

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