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Why this matters

On the page Limit Laws we met two resistors in parallel, of 3 ohms and tt ohms, with the combined resistance

R(t)=3t3+tR(t) = \frac{3t}{3 + t}

ohms, for t>0t > 0, and we found what it approaches as tt approaches 6. Now replace the second resistor by larger and larger ones. What happens to the combined resistance? Rounded, in ohms:

The values creep up towards 3 and never reach it. Indeed, for every t>0t > 0,

3−R(t)=3(3+t)−3t3+t=93+t,3 - R(t) = \frac{3(3 + t) - 3t}{3 + t} = \frac{9}{3 + t},

which is positive, and as small as we like when tt is large enough: it is less than 0.001 as soon as t>8997t > 8997. A huge resistor in parallel lets almost no current through, so the pair behaves almost like the 3-ohm resistor alone.

This is a new kind of limit. The variable tt does not approach a number aa: it grows without bound. We will write lim⁡t→∞R(t)=3\lim_{t \to \infty} R(t) = 3, and say that the line y=3y = 3 is a horizontal asymptote of the graph of RR. We also want to describe x→−∞x \to -\infty, and values that grow without bound themselves, as x2x^2 does when xx grows. This page defines all of these precisely, carries the limit laws over to them, and uses the laws to find the limits of every rational function and of some expressions with square roots.

Limits as xx grows without bound

Informally, lim⁡x→∞f(x)=L\lim_{x \to \infty} f(x) = L means that f(x)f(x) is as close to LL as we like for all xx large enough. The ε–δ game of the definition of the limit changes in one place: the challenger still names a tolerance ε>0\eps > 0, but instead of a window 0<∣x−a∣<δ0 < \abs{x - a} < \delta around a point aa you reply with a threshold NN, and you win if every x>Nx > N has f(x)f(x) within ε\eps of LL. The window is now the ray of all x>Nx > N. For values that grow without bound, such as x2x^2, the challenger names a height BB instead, and you win if f(x)>Bf(x) > B for every x>Nx > N. Values of ff at small xx play no part; ff only has to be defined from some point on.

In words. Parts (a) and (b) are the game of the definition of the limit with the punctured window 0<∣x−a∣<δ0 < \abs{x - a} < \delta replaced by the ray x>Nx > N, or x<Nx < N. Parts (c) and (d) replace the tolerance band around LL by a height BB that the values must stay above, or below, from the threshold on. Four points to notice:

Example. lim⁡x→∞1x=0\lim_{x \to \infty} \frac{1}{x} = 0, by part (a). The function is defined at every x>0x > 0, so on (0,∞)(0, \infty). Let ε>0\eps > 0 and take N=1εN = \frac{1}{\eps}, which is positive by property 6 of the order rules. If x>Nx > N, then 0<1ε<x0 < \frac{1}{\eps} < x, and property 6 gives 1x<11/ε=ε\frac{1}{x} < \frac{1}{1/\eps} = \eps and 1x>0\frac{1}{x} > 0. So ∣1x−0∣=1x<ε\abs{\frac{1}{x} - 0} = \frac{1}{x} < \eps, by the definition of the absolute value.

Example. lim⁡x→∞x2=∞\lim_{x \to \infty} x^2 = \infty, by part (c). Let BB be a real number and take NN to be the larger of 1 and BB. If x>Nx > N, then x>1x > 1 and x>Bx > B. Multiplying x>1x > 1 by the positive number xx keeps the inequality (property 5(a) of the order rules): x2>xx^2 > x. So x2>x>Bx^2 > x > B, and x2>Bx^2 > B by transitivity.

Non-example. No real number LL is the limit of x2x^2 as x→∞x \to \infty. Take ε=1\eps = 1. Whatever NN is offered, let xx be 1 more than the larger of NN and ∣L∣+1\abs{L} + 1. Then x>Nx > N, and x>∣L∣+1≥1x > \abs{L} + 1 \ge 1, so as in the example x2>x>∣L∣+1x^2 > x > \abs{L} + 1. Adding −L-L to both sides (property 3 of the order rules), and using ∣L∣−L≥0\abs{L} - L \ge 0 (property 3 of the absolute value), gives x2−L>∣L∣−L+1≥1x^2 - L > \abs{L} - L + 1 \ge 1. So x2−Lx^2 - L is positive, and ∣x2−L∣=x2−L>1=ε\abs{x^2 - L} = x^2 - L > 1 = \eps: the threshold NN loses the round ε=1\eps = 1.

The figure shows one round of the game of part (a).

The graph of y equals (2x squared plus x) over (x squared plus 1) for x from about 1.25 to 16, shown for heights between 1.7 and 2.15 only. A horizontal band runs between the dashed lines y = 1.9 and y = 2.1, with the dotted line y = 2 in its middle. The graph rises steeply, crosses y = 2 at x = 2, leaves the band through its upper edge at x = 3, peaks just above it near x = 4, comes back to the upper edge at x = 7 and then stays inside the band, slowly approaching y = 2 from above. A dashed vertical line marks x = 7, labelled N = 7, and the region to its right is shaded.

Figure 1:The graph of f(x)=2x2+xx2+1f(x) = \frac{2x^2 + x}{x^2 + 1}, with the band 1.9<y<2.11.9 < y < 2.1 of half-width ε=0.1\eps = 0.1 around y=2y = 2; the vertical axis shows only the heights from 1.7 to 2.15. The graph crosses the line y=2y = 2 at x=2x = 2, leaves the band at x=3x = 3 and returns to it at x=7x = 7. To the right of the threshold N=7N = 7 (shaded) it stays inside the band.

For this ε\eps, the threshold N=7N = 7 wins the round, and no smaller threshold does (Exercise 5 proves both). A smaller ε\eps needs a larger NN. The graph meets the line y=2y = 2 and leaves the band before it settles: the definition does not care what happens before the threshold.

Before we use the definition, three facts that make it easier to use. The first says that we may speak of the limit at infinity.

Horizontal asymptotes

A limit at infinity describes the far ends of a graph. When the limit is a real number LL, the graph runs ever closer to the horizontal line y=Ly = L.

In words. Far to the right, or far to the left, the graph comes as close to the line y=Ly = L as we like and stays that close.

Example. The line y=3y = 3 is a horizontal asymptote of the graph of the combined resistance RR of Why this matters, which is defined only for t>0t > 0, so only the direction t→∞t \to \infty is available (Example 5 proves the limit). The line y=2y = 2 is a horizontal asymptote of the graph in Figure 1: as the figure shows, a graph may cross its horizontal asymptote.

Non-example. The graph of x2x^2 has no horizontal asymptote. As x→∞x \to \infty its limit is ∞\infty, so by property 1 of the remark it is no real number LL. As x→−∞x \to -\infty the same holds, by property 3 of the remark: g(t)=(−t)2=t2g(t) = (-t)^2 = t^2.

By property 1 of the remark, a graph has at most two horizontal asymptotes, one for each direction. Each of the two directions may give the same line, a different one, or none.

Horizontal and vertical asymptotes. The page Infinite Limits and Vertical Asymptotes defines a vertical asymptote x=ax = a: a vertical line near which f(x)f(x) tends to ∞\infty or to −∞-\infty as xx approaches the number aa from at least one side. The roles of xx and yy are exchanged. At a vertical asymptote, xx approaches a number and f(x)f(x) grows or falls without bound; at a horizontal asymptote, xx grows without bound and f(x)f(x) approaches a number. A graph may have many vertical asymptotes, but at most two horizontal ones; and it meets a vertical line x=ax = a at most once, because ff has at most one value at aa, while it may cross a horizontal asymptote. The graph of 1x\frac{1}{x} has both kinds: the line y=0y = 0, as x→∞x \to \infty by the example above, and the line x=0x = 0, since lim⁡x→0+1x=∞\lim_{x \to 0^{+}} \frac{1}{x} = \infty by part (a) of the proposition on reciprocal powers, with a=0a = 0 and n=1n = 1.

Main results

The limit laws at infinity

The limit laws of Limit Laws hold at infinity too, with the same hypotheses. Part (a) differs: the function xx has no real limit as x→∞x \to \infty, so the identity law becomes a statement about ∞\infty.

(If ff and gg are defined on two different intervals (α1,∞)(\alpha_1, \infty) and (α2,∞)(\alpha_2, \infty), both are defined on the one whose left end is the larger of α1\alpha_1 and α2\alpha_2, so one α\alpha is no restriction.)

When the laws do not apply. As on the Limit Laws page, the laws need the limits LL and MM of the parts to be real numbers. If both parts tend to ∞\infty, the laws say nothing about the difference, “∞−∞\infty - \infty”, or the quotient, “∞∞\frac{\infty}{\infty}”, and such limits can be anything. For every real number cc, the functions x+cx + c and xx both tend to ∞\infty, yet their difference is the constant cc, whose limit is cc. The quotients 2xx\frac{2x}{x} and x2x\frac{x^2}{x} are both “∞∞\frac{\infty}{\infty}”; they equal 2 and xx at every x>0x > 0, so by property 2 of the remark their limits are 2 and ∞\infty, by part (a) of the theorem. Such forms are a signal to rewrite the function first, as the next proof and the examples do.

Rational functions

For a rational function, the leading terms decide everything: far out, p(x)q(x)\frac{p(x)}{q(x)} behaves like the quotient of the leading terms. We first need that the reciprocal powers 1xj\frac{1}{x^j} tend to 0.

In words. Compare the degrees. A higher degree in the denominator pulls the quotient to 0; equal degrees give the quotient ab\frac{a}{b} of the leading coefficients; a higher degree in the numerator sends the quotient to ∞\infty or −∞-\infty, with the sign of axmbxk=abxm−k\frac{a x^m}{b x^k} = \frac{a}{b} x^{m - k} far out on that side. So the graph of rr has the horizontal asymptote y=0y = 0 in case (b), y=aby = \frac{a}{b} in case (c), in both directions, and none in case (d).

Example. 3x2−x+22x2+5\frac{3x^2 - x + 2}{2x^2 + 5} has m=k=2m = k = 2, so its limit in both directions is 32\frac{3}{2}. Non-example. For x2+1x\frac{x^2 + 1}{x}, m=2>k=1m = 2 > k = 1 and ab=1\frac{a}{b} = 1: the limit is ∞\infty as x→∞x \to \infty, and, since (−1)1⋅1<0(-1)^1 \cdot 1 < 0, −∞-\infty as x→−∞x \to -\infty. There is no horizontal asymptote.

Comparing growth

Limits at infinity let us say which of two functions grows faster. Informally, ff grows faster than gg as x→∞x \to \infty if g(x)f(x)→0\frac{g(x)}{f(x)} \to 0: eventually g(x)g(x) is a tiny fraction of f(x)f(x).

Worked examples

From the definition

Rational functions

Square roots

An application

Common mistakes

Rigorous track

Summary

Exercises

Where this leads

These topics build on this one:

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Limits at infinity return wherever “in the long run” matters: in curve sketching, where horizontal and oblique asymptotes describe the far ends of a graph; in L’Hôpital’s rule, whose general form covers “∞∞\frac{\infty}{\infty}” and x→±∞x \to \pm\infty; in improper integrals over unbounded intervals; and in sequences, where n→∞n \to \infty runs through the integers only.