Seek an integrating factor such that the differential expression becomes . Its leading coefficient requires , while the first-derivative coefficient requires . Thus
Choose the positive solution . The Sturm-Liouville form is therefore
with
The weight is positive on the open interval. The endpoints are singular because vanishes there, but the prescribed boundedness of makes the integration-by-parts boundary terms vanish.
Multiply the Sturm-Liouville form for by and subtract the equation for multiplied by . Integration gives
The boundary expression is zero because and the functions and first derivatives remain finite. Since are distinct positive integers, this proves
For the derivatives, apply integration by parts once to the same Sturm-Liouville form:
Thus the new weight is
This is derivative orthogonality when the Sturm-Liouville potential vanishes. For the derivative is identically zero, which is consistent with the identity.
Put , with . The chain rule gives
Consequently the original differential expression becomes . If , direct differentiation gives
Taking therefore yields
The apparent endpoint singularities are removable. Expansion at gives
Thus both endpoint regularity conditions hold. This is the Chebyshev polynomial of the second kind .
The trigonometric addition formula gives
Dividing by and writing gives the recurrence relation
The first two members are and . If has degree and leading coefficient , then has degree and leading coefficient , whereas has lower degree and cannot cancel that term. Mathematical induction proves
For example the sequence begins , agreeing with the Chebyshev polynomial of the second kind.

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