Put . Before either forcing term acts, Newton's law of cooling gives
Integrating the equation through gives the jump condition for an impulse
For the equation is again homogeneous, so propagation of the post-jump temperature gives
Therefore
For , the Heaviside step function contributes a constant unit forcing. Solving the resulting first-order linear differential equation from the value at gives
The cups have equal temperatures up to the intervention at . For the later recrossing, subtract the formula for from that for and set the result to zero:
Writing gives . Hence the nontrivial meeting time is
Using the Taylor expansion
we obtain
When cooling is negligible, the milk lowers the temperature by one unit at . The hot-water term begins at and raises it at one unit per unit time, so one further unit of time is needed to erase the deficit.

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