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Mathematics · Ch 9 — Differential Calculus – Limits and Continuity

Limits at infinity

9.2.5

Limits at infinity

Section 9.2.4 let xx approach a finite point and asked what happens to yy when yy becomes unbounded. This section reverses the roles: now xx itself is allowed to grow without bound (positively or negatively), and we ask what value, if any, y=f(x)y=f(x) settles towards.

Motivating example. For f(x)=x2−1x2+1f(x)=\dfrac{x^2-1}{x^2+1}, tabulating ff at x=0,±1,±2,…,±1000x=0,\pm1,\pm2,\dots,\pm1000 shows the values climbing steadily towards (but never quite reaching) 11 as ∣x∣|x| grows (Fig. 9.25 shows the curve flattening out and hugging the horizontal line y=1y=1 on both ends). We write lim⁡x→±∞x2−1x2+1=1\lim_{x\to\pm\infty}\dfrac{x^2-1}{x^2+1}=1.

Definition 9.6 (horizontal asymptote). The line y=ly=l is a horizontal asymptote of y=f(x)y=f(x) if lim⁡x→−∞f(x)=l\lim_{x\to-\infty}f(x)=l or lim⁡x→+∞f(x)=l\lim_{x\to+\infty}f(x)=l — the two limits, at −∞-\infty and at +∞+\infty, need not agree, so a single curve can genuinely have two different horizontal asymptotes, one on each end.

Illustration 9.4 applies this to the inverse-tangent function f(x)=tan⁡−1xf(x)=\tan^{-1}x on (−π2,π2)\left(-\tfrac\pi2,\tfrac\pi2\right) (Fig. 9.26): reading the graph gives lim⁡x→−∞tan⁡−1x=−π2\lim_{x\to-\infty}\tan^{-1}x=-\dfrac\pi2 and lim⁡x→+∞tan⁡−1x=π2\lim_{x\to+\infty}\tan^{-1}x=\dfrac\pi2 — two different horizontal asymptotes, one at each end, since the arctangent curve never actually reaches ±π2\pm\dfrac\pi2 but approaches each of them on its own side.

The indeterminate-form trap and its fix (Illustration 9.5). For 2x2−2x+3x2+4x+3\dfrac{2x^2-2x+3}{x^2+4x+3} as x→∞x\to\infty, simply noting "numerator →∞\to\infty" and "denominator →∞\to\infty" and writing ∞∞\dfrac\infty\infty tells us nothing — ∞∞\dfrac\infty\infty is called an indeterminate form, precisely because different expressions sharing that same superficial pattern can tend to entirely different limits. A table of values does suggest the answer is 22, but the reliable route is algebraic: divide every term, top and bottom, by the highest power of xx appearing in the denominator — here x2x^2:

2x2−2x+3x2+4x+3=2−2x+3x21+4x+3x2  →x→∞  2−0+01+0+0=2,\frac{2x^2-2x+3}{x^2+4x+3}=\frac{2-\frac2x+\frac3{x^2}}{1+\frac4x+\frac3{x^2}}\;\xrightarrow[x\to\infty]{}\;\frac{2-0+0}{1+0+0}=2, …

Figure 9.25$f(x)=\frac{x^2-1}{x^2+1}$

What this figure shows. An S-shaped curve through (0,−1)(0,-1) that flattens out and hugs the horizontal line y=1y=1 on both the far left and far right, showing y=1y=1 as a two-sided horizontal asymptote. …

Figure 9.26$y=\tan^{-1}x$

What this figure shows. The inverse-tangent curve rising monotonically through the origin, flattening toward the horizontal asymptote y=π/2y=\pi/2 on the right and y=−π/2y=-\pi/2 on the left …