Solution

ID: past-exam-of-the-mathematics-course-of-the-year-1-of-the-natural-sciences-course-of-the-university-of-cambridge/2010/paper-1/18/b/solution

Differentiate the Airy ordinary differential equation to obtain . Combining part (a)'s derivatives yields
To make this vanish for an arbitrary Airy profile, the time powers must agree: , giving . Their common coefficient must then vanish, giving , hence . Therefore
For the two terms cancel exactly:
This is an Airy similarity solution of the linear dispersive equation. The Airy equation here is the linear partial differential equation , the reduced equation specified in the question; it is distinct from the profile's Airy ordinary differential equation. The construction works for every linear combination of its two independent profiles, including zero. No condition at is supplied, and this singular time is excluded. With real cube roots the final formula can also be used separately on .

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