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Topos Uranos

Equivalent infinitesimals and infinitely large functions

Summary

This lesson closes the unit on limits with a computational technique that brings together almost everything that came before it: the comparison of functions that tend to zero or to infinity. Little oo, big OO, the same order and equivalence are defined, and it is proved that, in a product or a quotient, each factor can be replaced by an equivalent one without changing the limit. The trigonometric limits, those of the exponential, the logarithm and powers, and those of polynomials, proved in the preceding lessons, are gathered into a table of equivalents, which makes it possible to compute at a glance limits that used to require several transformations. The lesson also shows the most common error with this technique, substituting inside a sum, when a sum can indeed be substituted, and how powers compare near zero and far from the origin.

Learning objectives

  1. Define little oo, big OO, the same order and the equivalence of functions at a point, on one side or at infinity, and prove their properties.
  2. Prove the theorem on substitution of equivalents in products and quotients, and recognize why it does not hold for sums.
  3. Prove the table of equivalents at zero and use it, together with composition, to compute limits and to determine the order and the principal part of an infinitesimal.
  4. Compare infinitely large powers and infinitesimal powers, and distinguish equivalence from the existence of an asymptote.

Comparing functions

The lessons on the squeeze theorem and on infinite limits showed that the forms 00\frac{0}{0} and ∞∞\frac{\infty}{\infty} have no fixed result: the limit of a quotient of two functions that tend to zero depends on how fast they do so. The idea of this lesson is to measure that speed by comparing each function with a simpler one. As in the lesson on infinite limits, PP denotes the target of the variable (aa, a+a^+, a−a^-, ∞\infty or −∞-\infty), and “near PP” means in a punctured interval, on one side or on a ray. If a function is defined only on a set AA of which aa is an accumulation point, “near aa” means at the points of AA in a punctured interval centered at aa, and the limits are those of the lesson on the limit of functions of a real variable, taken in AA; the following definitions apply in the same way in that case.

DefinitionComparison of functions

Let ff and gg be functions defined near PP, with g(x)≠0g(x) \neq 0 near PP.

  • ff is negligible compared with gg at PP, and one writes f=o⁡(g)f = \operatorname{o}(g), which is read “ff is little-o of gg”, if lim⁡x→Pf(x)g(x)=0\lim_{x \to P} \frac{f(x)}{g(x)} = 0.
  • ff is bounded by gg at PP, and one writes f=O⁡(g)f = \operatorname{O}(g), which is read “ff is big-O of gg”, if there exists C>0C > 0 such that ∣f(x)∣≤C∣g(x)∣\abs{f(x)} \leq C\abs{g(x)} near PP; that is, if the quotient f(x)g(x)\frac{f(x)}{g(x)} is bounded near PP.
  • ff and gg are of the same order at PP if f(x)g(x)\frac{f(x)}{g(x)} tends to a nonzero number.
  • ff and gg are equivalent at PP, and one writes f∼gf \sim g, if lim⁡x→Pf(x)g(x)=1\lim_{x \to P} \frac{f(x)}{g(x)} = 1.

A function that tends to 00 at PP is called an infinitesimal at PP, and one that tends to ∞\infty or to −∞-\infty, an infinitely large function. An infinitesimal at 00 has order k>0k > 0 if it is of the same order as xkx^k (at 0+0^+, if xkx^k is defined only for x>0x > 0), and then, if f(x)xk\frac{f(x)}{x^k} tends to cc, the function c xkc\,x^k is its principal part: f∼c xkf \sim c\,x^k.

The word “infinitesimal” does not denote a very small number, but a function that tends to zero; the notation o⁡(g)\operatorname{o}(g) does not denote a specific function, but any of those that are negligible compared with gg. For example, x2=o⁡(x)x^2 = \operatorname{o}(x) at 00, because x2x=x\frac{x^2}{x} = x tends to 00; on the other hand, x=o⁡(x2)x = \operatorname{o}(x^2) at ∞\infty, because xx2=1x\frac{x}{x^2} = \frac{1}{x} tends to 00. One and the same pair of functions compares in opposite ways depending on the target. Being of the same order and being equivalent are, at bottom, a single comparison: if ff and gg are of the same order with a quotient that tends to cc, then f∼c gf \sim c\,g.

PropositionProperties of the comparison

At one and the same target PP:

  • equivalence is reflexive, symmetric and transitive: f∼ff \sim f; if f∼gf \sim g, then g∼fg \sim f; and if f∼gf \sim g and g∼hg \sim h, then f∼hf \sim h;
  • f∼gf \sim g if and only if f−g=o⁡(g)f - g = \operatorname{o}(g); in particular, if h=o⁡(g)h = \operatorname{o}(g), then g+h∼gg + h \sim g;
  • if f=o⁡(h)f = \operatorname{o}(h) and g=o⁡(h)g = \operatorname{o}(h), then f+g=o⁡(h)f + g = \operatorname{o}(h) and c f=o⁡(h)c\,f = \operatorname{o}(h) for every real cc.

Each statement is a rule of the algebra of limits applied to a quotient.

Proof

  1. gf=1fg→1,fh=fg⋅gh→1⋅1=1\frac{g}{f} = \frac{1}{\frac{f}{g}} \to 1, \qquad \frac{f}{h} = \frac{f}{g} \cdot \frac{g}{h} \to 1 \cdot 1 = \resaltar{1}

    The quotient of ff by itself equals 11. If fg\frac{f}{g} tends to 11, its reciprocal tends to 11=1\frac{1}{1} = 1, by the rule for the reciprocal. If fg\frac{f}{g} and gh\frac{g}{h} tend to 11, so does their product, by the product rule.

  2. f−gg=fg−1→0⇔fg→1\frac{f - g}{g} = \frac{f}{g} - 1 \to 0 \Leftrightarrow \frac{f}{g} \to \resaltar{1}

    The quotient of f−gf - g by gg is fg−1\frac{f}{g} - 1, which tends to 00 if and only if fg\frac{f}{g} tends to 11. With f=g+hf = g + h, the difference is hh.

  3. f+gh=fh+gh→0+0=0\frac{f + g}{h} = \frac{f}{h} + \frac{g}{h} \to 0 + 0 = \resaltar{0}

    If fh\frac{f}{h} and gh\frac{g}{h} tend to 00, so do their sum and the product of each of them by a constant, by the rule for linear combinations.

Big OO does not require the quotient to have a limit, only that it not grow out of control. For example, sin⁡x=O⁡(1)\sin x = \operatorname{O}(1) at ∞\infty, even though sin⁡x\sin x has no limit there, and xsin⁡1x=O⁡(x)x \sin \frac{1}{x} = \operatorname{O}(x) at 00, because ∣xsin⁡1x∣≤∣x∣\abs{x \sin \frac{1}{x}} \leq \abs{x}. To compute limits, little oo is enough; big OO will serve to measure approximation errors, such as that of the Taylor polynomial, which will be studied in Calculus II. Its rules are the following.

PropositionRules for big O

At one and the same target PP:

  • if fg\frac{f}{g} has a finite limit at PP, then f=O⁡(g)f = \operatorname{O}(g); in particular, if f=o⁡(g)f = \operatorname{o}(g) or if f∼gf \sim g;
  • if f=O⁡(h)f = \operatorname{O}(h) and g=O⁡(h)g = \operatorname{O}(h), then f+g=O⁡(h)f + g = \operatorname{O}(h) and c f=O⁡(h)c\,f = \operatorname{O}(h) for every real cc;
  • if f1=O⁡(g1)f_1 = \operatorname{O}(g_1) and f2=O⁡(g2)f_2 = \operatorname{O}(g_2), then f1f2=O⁡(g1g2)f_1 f_2 = \operatorname{O}(g_1 g_2);
  • if f1=O⁡(g1)f_1 = \operatorname{O}(g_1) and f2=o⁡(g2)f_2 = \operatorname{o}(g_2), then f1f2=o⁡(g1g2)f_1 f_2 = \operatorname{o}(g_1 g_2).

Each rule is an inequality between absolute values; the last one combines a bound with a quotient that tends to zero.

Proof

  1. ∣f(x)g(x)∣≤∣f(x)g(x)−L∣+∣L∣<∣L∣+1\abs{\frac{f(x)}{g(x)}} \leq \abs{\frac{f(x)}{g(x)} - L} + \abs{L} < \resaltar{\abs{L} + 1}

    If fg\frac{f}{g} tends to LL, the challenge ε=1\varepsilon = 1 has a response: near PP, the distance from the quotient to LL is less than 11, and by the triangle inequality its absolute value does not exceed ∣L∣+1\abs{L} + 1.

  2. ∣f(x)+g(x)∣≤C1∣h(x)∣+C2∣h(x)∣=(C1+C2)∣h(x)∣\abs{f(x) + g(x)} \leq C_1\abs{h(x)} + C_2\abs{h(x)} = \resaltar{(C_1 + C_2)\abs{h(x)}}

    The bounds C1C_1 of ff and C2C_2 of gg hold simultaneously near PP, in the intersection of the two neighborhoods. The triangle inequality bounds the sum; the multiple has the bound ∣c∣ C1\abs{c}\,C_1.

  3. ∣f1(x)f2(x)∣≤C1∣g1(x)∣⋅C2∣g2(x)∣=C1C2∣g1(x)g2(x)∣\abs{f_1(x) f_2(x)} \leq C_1\abs{g_1(x)} \cdot C_2\abs{g_2(x)} = \resaltar{C_1 C_2 \abs{g_1(x) g_2(x)}}

    The bounds of the two factors are multiplied.

  4. 0≤∣f1(x)f2(x)g1(x)g2(x)∣≤C1∣f2(x)g2(x)∣→00 \leq \abs{\frac{f_1(x) f_2(x)}{g_1(x) g_2(x)}} \leq C_1 \abs{\frac{f_2(x)}{g_2(x)}} \to \resaltar{0}

    The quotient of the product by g1g2g_1 g_2 is the product of a quotient bounded by C1C_1 and another that tends to 00; by the squeeze theorem, it tends to 00.