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Mathematics · Ch 9 — Differential Calculus – Limits and Continuity

Infinite limits and limits at infinity

9.2.4

Infinite limits and limits at infinity

Not every limit settles down to a finite real number as xx approaches a point — sometimes the function values grow without any bound at all. This section studies that behaviour, which is entirely different from "the limit does not exist because of disagreeing one-sided limits" (Section 9.2.1's third illustration): here, both sides can behave the same way, but that common behaviour is unboundedness rather than convergence to a number.

Motivating example. Consider f(x)=1x2f(x)=\dfrac{1}{x^2}, undefined at x=0x=0. Tabulating xx-values shrinking towards 00 from either side shows f(x)f(x) growing larger without limit — from 11, to 100100, to 10,00010{,}000, to 10,00,00010{,}00{,}000, and beyond. We describe this by writing 1x2→∞\dfrac1{x^2}\to\infty as x→0−x\to0^- and as x→0+x\to0^+ (Fig. 9.22 shows both branches of the curve rising without end on either side of the yy-axis), and say x=0x=0 is a vertical asymptote. A closely related but importantly different function is f(x)=1xf(x)=\dfrac1x (Fig. 9.23): here 1x→−∞\dfrac1x\to-\infty as x→0−x\to0^- but 1x→+∞\dfrac1x\to+\infty as x→0+x\to0^+ — the two sides diverge to opposite infinities, unlike 1/x21/x^2 where both sides behave the same way.

Watch out

Even though we write lim⁡x→01x2=∞\lim_{x\to0}\frac1{x^2}=\infty, this is a statement about behaviour, not a value — the limit, strictly speaking, does not exist, because ∞\infty is not a real number the function is converging to; it is only shorthand describing how badly the function fails to converge.

Formally:

Definition 9.4. For M>0M>0, an interval of the form (M,∞)(M,\infty) is called a neighbourhood of ∞\infty; for K<0K<0, an interval of the form (−∞,K)(-\infty,K) is called a neighbourhood of −∞-\infty.

Definition 9.5. f(x)→∞f(x)\to\infty as x→x0x\to x_0 if, for every M>0M>0, there is a neighbourhood of x0x_0 within which f(x)∈(M,∞)f(x)\in(M,\infty) whenever xx lies in that neighbourhood — and similarly f(x)→−∞f(x)\to-\infty as x→x0x\to x_0 using a K<0K<0 and the interval (−∞,K)(-\infty,K).

This gives rise to six possible one-sided and two-sided "infinite limit" statements — f(x)→±∞f(x)\to\pm\infty as x→x0x\to x_0, or as x→x0−x\to x_0^-, or as x→x0+x\to x_0^+ — and whenever any one of them holds, the vertical line x=x0x=x_0 is a vertical asymptote of the graph of ff.

The general odd/even-power pattern (Example 9.22, f(x)=1(x−2)3f(x)=\dfrac{1}{(x-2)^3}, Fig. 9.24). Near a point x=ax=a where the denominator is (x−a)n(x-a)^n:

  • If nn is even, 1(x−a)n→+∞\dfrac1{(x-a)^n}\to+\infty from both sides (exactly like 1/x21/x^2 above), so the two-sided infinite-limit statement holds.
  • If nn is odd, 1(x−a)n→−∞\dfrac1{(x-a)^n}\to-\infty from the left and →+∞\to+\infty from the right (exactly like 1/x1/x above): the two sides disagree in sign, so only the one-sided statements hold, and even the infinite-sense limit does not exist two-sidedly. …
Figure 9.22$f(x)=1/x^2$ near $x=0$

What this figure shows. A symmetric curve (both branches go upward) hugging the positive yy-axis as x→0x\to0 from either side and hugging the xx-axis for large ∣x∣|x|; x=0x=0 is a vertical asymptote. …

Figure 9.23$f(x)=1/x$ near $x=0$

What this figure shows. A curve with two branches in opposite quadrants: it plunges to −∞-\infty as x→0−x\to0^- and rises to +∞+\infty as x→0+x\to0^+, again with x=0x=0 a vertical asymptote. …

Figure 9.24$f(x)=1/(x-2)^3$

What this figure shows. An odd-power reciprocal curve: it falls to −∞-\infty as x→2−x\to2^- and rises to +∞+\infty as x→2+x\to2^+, with x=2x=2 a vertical asymptote (illustrates the odd-nn sign pattern …