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Why this matters

A magnifying glass has a focal length of 10 cm. Put a small object uu centimetres in front of it. The thin-lens equation 1u+1v=110\frac{1}{u} + \frac{1}{v} = \frac{1}{10} says where the lens forms the sharp image of the object: at distance

v(u)=10uu−10v(u) = \frac{10u}{u - 10}

behind the lens, for every u≠10u \ne 10, in centimetres. (A negative vv means that the image is on the same side as the object: the enlarged virtual image you see when you look through the glass.) What happens as the object moves towards the focal point, u=10u = 10?

uu1110.110.019.999.9
v(u)v(u)110101010 01010\,010−9990{-9990}−990{-990}

From the right, the image runs away behind the lens: 10.01 cm gives an image 100 metres away. From the left, the virtual image runs away just as fast on the other side. So v(u)v(u) approaches no number as uu approaches 10 from either side. On the page The Limit of a Function such behaviour was one of the ways a limit can fail to exist (compare its example of unbounded values, 1x2\frac{1}{x^2} near 0). But “does not exist” throws away what we see in the table: on the right the values grow beyond every bound, and on the left they fall below every bound.

This page gives that behaviour a notation, lim⁡u→10+v(u)=∞\lim_{u \to 10^{+}} v(u) = \infty and lim⁡u→10−v(u)=−∞\lim_{u \to 10^{-}} v(u) = -\infty, and a precise meaning. The notation does not make ∞\infty a number: we prove that such a limit does not exist as a real number. Then we find infinite limits of rational functions by a sign analysis, and the lines they create in the graph, the vertical asymptotes. Example 4 proves the two limits of the table, and finds how close to 10 cm the object must be for the image to be more than 10 metres away.

Limits that are infinite

Informally, lim⁡x→a+f(x)=∞\lim_{x \to a^{+}} f(x) = \infty means that f(x)f(x) is as large as we like for all xx close enough to aa and greater than aa. The game of the definition of one-sided limits changes in one place: instead of a band of half-width ε\eps around a number LL, the challenger names a height MM, and the values of ff on the half-window must lie above it.

Two graphs side by side, each for x from 0 to 4, with a dashed vertical line at x = 2. Left, the graph of y = 1/(x − 2): to the right of the dashed line it rises steeply out of view as x approaches 2, and to the left of the line it falls steeply out of view. Right, the graph of y = 1/(x − 2) squared: on both sides of the dashed line it rises steeply out of view.

Figure 1:Left: y=1x−2y = \frac{1}{x - 2} climbs beyond every height as xx approaches 2 from the right, and falls below every height as xx approaches 2 from the left. Right: y=1(x−2)2y = \frac{1}{(x - 2)^2} climbs beyond every height from both sides. The dashed line x=2x = 2 is a vertical asymptote of both graphs. A drawing shows finitely many points; Proposition 2 proves what it suggests.

“Close enough” means the same as in the definition of one-sided limits: there is a half-window a<x<a+δa < x < a + \delta (or a−δ<x<aa - \delta < x < a) on which it holds. The rigorous track states this precisely, in the dropdown below; the proofs on this page use that version.

Definition 2 (Infinite limits, precisely (rigorous track))

Let aa be a real number.

(a) Let ff be as in part (a) of Definition 1. Then lim⁡x→a+f(x)=∞\lim_{x \to a^{+}} f(x) = \infty means: for every M>0M > 0 there is a δ>0\delta > 0 such that ff is defined at every xx with a<x<a+δa < x < a + \delta, and

a<x<a+δimpliesf(x)>M.\begin{aligned} &a < x < a + \delta \\ &\quad\text{implies}\quad f(x) > M . \end{aligned}

And lim⁡x→a+f(x)=−∞\lim_{x \to a^{+}} f(x) = -\infty means the same with f(x)<−Mf(x) < -M in place of f(x)>Mf(x) > M.

(b) Let ff be as in part (b) of Definition 1. The statements lim⁡x→a−f(x)=∞\lim_{x \to a^{-}} f(x) = \infty and lim⁡x→a−f(x)=−∞\lim_{x \to a^{-}} f(x) = -\infty mean the same as in (a), with the half-window a−δ<x<aa - \delta < x < a in place of a<x<a+δa < x < a + \delta.

Part (c) of Definition 1 is defined through (a) and (b), so it needs no precise version of its own.

In words. A challenger names a height M>0M > 0; you reply with a half-window of width δ\delta next to aa; you win the round if ff is defined at every xx of the half-window and every such f(x)f(x) is above MM. The limit is ∞\infty when you can win every round. Three points to notice:

Example. lim⁡x→0+1x=∞\lim_{x \to 0^{+}} \frac{1}{x} = \infty. The function 1x\frac{1}{x} is defined at every x≠0x \ne 0. Given M>0M > 0, take δ=1M\delta = \frac{1}{M}, which is positive by property 6 of the order rules. If 0<x<1M0 < x < \frac{1}{M}, then by the same property 6 (0<u<v0 < u < v implies 1v<1u\frac{1}{v} < \frac{1}{u}, with u=xu = x and v=1Mv = \frac{1}{M}), M=11/M<1xM = \frac{1}{1/M} < \frac{1}{x}.

Non-example. lim⁡x→0−1x\lim_{x \to 0^{-}} \frac{1}{x} is not ∞\infty. Take M=1M = 1. For x<0x < 0, 1x\frac{1}{x} has the sign of xx (part (c) of the sign rules), so 1x<0<1\frac{1}{x} < 0 < 1. So every point of every half-window −δ<x<0-\delta < x < 0 fails the round M=1M = 1, and no δ\delta wins it. (From the left, 1x\frac{1}{x} tends to −∞-\infty: Proposition 2 below.)

An infinite limit at aa shows in the graph of ff as a vertical line that the graph climbs or falls along without bound, as the line x=2x = 2 in Figure 1.

In words. On at least one side of the line x=ax = a, the graph of ff climbs beyond every height or falls below every height as xx approaches aa. One side is enough, and the two sides may go in different directions. As with every limit, the value f(a)f(a) plays no part: ff may be defined at aa and still have the vertical asymptote x=ax = a. For example, F(x)=1x+1F(x) = \frac{1}{x} + 1 for x>0x > 0 and F(x)=0F(x) = 0 for x≤0x \le 0 is defined at 0, and lim⁡x→0+F(x)=∞\lim_{x \to 0^{+}} F(x) = \infty: for x>0x > 0, adding 1x\frac{1}{x} to 0<10 < 1 gives 1x<F(x)\frac{1}{x} < F(x) (property 3 of the order rules), so by transitivity (property 2) the δ=1M\delta = \frac{1}{M} of the example above wins every round MM for FF too.

Example. The line x=0x = 0 is a vertical asymptote of the graph of 1x\frac{1}{x}, by the example after Definition 2.

Non-example. Let g(x)=x2−1x−1g(x) = \dfrac{x^2 - 1}{x - 1} for x≠1x \ne 1. Although gg is undefined at 1, the line x=1x = 1 is not a vertical asymptote of its graph. For x≠1x \ne 1 we may cancel the non-zero factor x−1x - 1, so g(x)=x+1g(x) = x + 1. If 0<x<20 < x < 2, adding 1 keeps both inequalities (property 3 of the order rules): 1<g(x)<31 < g(x) < 3 for every x≠1x \ne 1 in (0,2)(0, 2). Take M=3M = 3. Every half-window 1<x<1+δ1 < x < 1 + \delta contains the point x=1+12min⁡(δ,1)x = 1 + \frac12 \min(\delta, 1), which lies in (1,2)(1, 2), so g(x)<3=Mg(x) < 3 = M there: no δ\delta wins the round M=3M = 3, and lim⁡x→1+g(x)≠∞\lim_{x \to 1^{+}} g(x) \ne \infty. At the same point g(x)>1>−3g(x) > 1 > -3, so lim⁡x→1+g(x)≠−∞\lim_{x \to 1^{+}} g(x) \ne -\infty either, and the point x=1−12min⁡(δ,1)x = 1 - \frac12 \min(\delta, 1) of the left half-window does the same from the left. A function that stays between two numbers near aa has no vertical asymptote at aa.

Main results

An infinite limit is not a real limit

If f(x)f(x) is above every height near aa, it cannot also stay within 1 of a fixed number LL, because L+1L + 1 is one of the heights.

In words. “lim⁡x→af(x)=∞\lim_{x \to a} f(x) = \infty” is a precise way of saying that the limit does not exist: it records the reason. The converse is false. A limit can fail to exist without being ∞\infty or −∞-\infty: at a jump, such as ∣x∣x\frac{\abs{x}}{x} at 0, or when the two sides go to different infinities, as 1x\frac{1}{x} does at 0 (Proposition 2 below), so that lim⁡x→01x\lim_{x \to 0} \frac{1}{x} is neither ∞\infty nor −∞-\infty, by part (c) of Definition 1.

Reciprocal powers

The simplest infinite limits are those of 1(x−a)n\frac{1}{(x - a)^n}. Their sign depends on the side and on whether nn is even or odd (Figure 1).

So for every n≥1n \ge 1 the line x=ax = a is a vertical asymptote of the graph of 1(x−a)n\frac{1}{(x - a)^n}. For odd nn the one-sided limits are ∞\infty and −∞-\infty, and lim⁡x→a1(x−a)n\lim_{x \to a} \frac{1}{(x - a)^n} is neither, by part (c) of Definition 1.

Sign analysis: a factor that stays away from 0

Near a zero aa of its denominator, after cancelling common factors, a rational function is a reciprocal power 1(x−a)k\frac{1}{(x - a)^k} times a factor h(x)h(x) that does not vanish at aa. If hh keeps one sign and stays a fixed distance away from 0 near aa, it cannot stop the reciprocal power from growing; it can only flip its sign.

In words: how to find the one-sided limits of a rational function at a zero aa of its denominator.

  1. Factor the numerator and the denominator. If the numerator is also 0 at aa, cancel the common factor x−ax - a first: for x≠ax \ne a the two expressions are the same number. What is left may have a finite limit at aa (Example 3).

  2. Sign. By the proposition on the sign of a factored rational function, ff has one sign on the interval just to the right of aa and one just to the left (up to the next number of a linear factor). These signs tell you which of ∞\infty and −∞-\infty to expect on each side.

  3. Split. On a window around aa, write f(x)=h(x)⋅1(x−a)kf(x) = h(x) \cdot \frac{1}{(x - a)^k}, where kk is the number of factors x−ax - a in the denominator. This is algebra at each point x≠ax \ne a of the window, not a statement about limits.

  4. Bound. Choose the window so small that it contains no other number of a linear factor, and find an m>0m > 0 with h(x)≥mh(x) \ge m (or h(x)≤−mh(x) \le -m) at every point of it, with the order rules.

  5. Conclude with Proposition 2, for 1(x−a)k\frac{1}{(x - a)^k}, and Proposition 3.

Worked examples

One-sided limits at a zero of the denominator

A zero of the denominator that is not an asymptote

An applied example

Common mistakes

Rigorous track

Summary

Exercises

Where this leads

These topics build on this one:

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Infinite limits at a point describe the vertical lines of a graph. The next page of the chapter lets xx itself grow without bound, which gives the horizontal ones.