Seek an integrating factor such that the differential expression becomes . Its leading coefficient requires , while the first-derivative coefficient requires . ThusChoose the positive solution . The Sturm-Liouville form is thereforewithThe 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 givesThe boundary expression is zero because and the functions and first derivatives remain finite. Since are distinct positive integers, this provesFor the derivatives, apply integration by parts once to the same Sturm-Liouville form:Thus the new weight isThis 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 givesConsequently the original differential expression becomes . If , direct differentiation givesTaking therefore yieldsThe apparent endpoint singularities are removable. Expansion at givesThus both endpoint regularity conditions hold. This is the Chebyshev polynomial of the second kind .
The trigonometric addition formula givesDividing by and writing gives the recurrence relationThe 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 provesFor example the sequence begins , agreeing with the Chebyshev polynomial of the second kind.
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