Summary
This lesson proves L’Hôpital’s rule: if and tend to , or if tends to infinity, and the quotient of their derivatives has a limit, then the quotient has the same limit. The proof applies Cauchy’s mean value theorem, from the preceding lesson, on an interval with one endpoint fixed and the other variable; the case in which the denominator tends to infinity requires a finer argument, which asks nothing of the numerator. The rule holds on one side of a point, at the point and at infinity, and can be applied several times in a row: this is how one computes the limit of when the first derivatives of vanish at . The forms , , , and are reduced to a quotient. The lesson also shows when the rule does not apply or is inconclusive, why it cannot be used for the limits with which the derivatives were computed, and how it combines with equivalent infinitesimals.
Learning objectives
- Prove L’Hôpital’s rule for the forms and , on one side of a point, at the point and at infinity, from Cauchy’s mean value theorem.
- Compute limits of the indeterminate forms by reducing them to a quotient, and apply the rule several times, checking its hypotheses at each application.
- Recognize when the rule does not apply or is inconclusive: limits that are not indeterminate, quotients of derivatives without a limit, derivatives of the denominator that vanish near the point, and the limits that the computation of the derivatives presupposes.
- Combine the rule with equivalent infinitesimals and with the algebra of limits, and choose in each case the shortest route.
The form zero over zero
The corollary on the limit of a quotient, from the lesson on the algebra of limits, requires the denominator to have a nonzero limit. If the numerator and the denominator both tend to , the quotient can tend to any number, or to infinity, or have no limit: tends to , tends to , and has no limit at . That is why is called an indeterminate form: the limit of each term does not determine that of the quotient. The lesson on equivalent infinitesimals solved many of these limits by replacing each factor with an equivalent one from its table; but a difference such as is not a product of factors from the table, and its terms cannot be replaced.
The derivative suggests another route. If , if and are differentiable at and if , then dividing the numerator and the denominator by turns the quotient into a quotient of difference quotients, and the corollary on the limit of a quotient gives:
But often is also zero, or and are not defined at . L’Hôpital’s rule replaces the values of the derivatives at with the limit of their quotient near . The tool is Cauchy’s mean value theorem, from the lesson on the theorems of Fermat, Rolle, Lagrange and Cauchy: if and are continuous on , with , and differentiable at every point of , and if for every in , then and there exists a in such that . Unlike two applications of Lagrange’s theorem, which would give two different points, Cauchy’s theorem gives one and the same point for the numerator and for the denominator.
Let , and let and be functions differentiable at every point of , with for every in . Suppose that and tend to as , and that
where is a real number, or . Then for every in , and
One extends and with the value at , and Cauchy’s theorem is applied on : the quotient is a quotient of increments, equal to that of the derivatives at a point between and . The figure shows, with , and , the points : the quotient is the slope of the chord joining the origin to the point corresponding to , and the quotient of the derivatives at is the slope of the parallel tangent.
Proof
Let and be the functions equal to and on and to at . Let be in . Both are continuous on : at , because their right-hand limits are ; at the other points, by the theorem that differentiable implies continuous, from the lesson on the derivative as a limit. At every point of they are differentiable, with the derivatives of and of , by the lemma on the local character of the derivative, from the lesson on differentiation rules.
By Cauchy’s mean value theorem on , , that is, , and there exists a between and such that the quotient of increments equals that of the derivatives at .
Let be real and let . By the definition of the right-hand limit, from the lesson on one-sided limits, there exists a , which can be taken less than or equal to , such that if . If , the point from the second move satisfies . If , the same argument with a challenge gives ; if , it gives .
It is not necessary to know how depends on , nor that it is unique: it suffices that it lies between and . The hypothesis is required on the whole interval , because Cauchy’s theorem uses it on each ; since the limit depends only on nearby values, it suffices to find an interval where it holds, however small. It is not enough, on the other hand, that the derivative of the denominator vanish only at isolated points that accumulate at the point, or that are unbounded if the variable tends to infinity, as solved problem 5 shows. If and are defined on a larger set, the theorem is applied to their restrictions to , which have the same right-hand limit at .
The same holds on the left, with an interval , , and : it suffices to apply the theorem to and near on the right, by the translation and reflection proposition, from the lesson on one-sided limits; the chain rule changes the sign of both derivatives and does not alter their quotient. If the hypotheses hold on both sides of , on and on , the theorem on the limit and one-sided limits, from that lesson, gives the limit as (if is infinite, with the same argument of the smaller of the two radii). The function may be defined at or not; its value there plays no role.
Consider . The numerator and the denominator tend to , and the derivative of the denominator, , does not vanish away from . The quotient of the derivatives is , again of the form , with a denominator whose derivative is , which does not vanish away from either; and the new quotient, , tends to by the fundamental trigonometric limit:
The sequence of equalities is read from right to left: the last limit exists, and the rule, applied twice, transmits its value backward. Writing the first equals sign before knowing that the second limit exists is only a way of recording the computation, which is justified once it is finished. The second limit also follows from the table of equivalents, with ; the first does not.
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