Calculus I · Patterns That Go Somewhere

Limits that fight back

Everything so far has been gentle: substitute, simplify, read off the answer. The limits that teach you something are the ones where that fails. Look at these three:

Figure 1.5
Figure 1.5

n(1+1n−1),nn=n1/n,(1+1n)n.n\left(\sqrt{1+\tfrac1n}-1\right), \qquad \sqrt[n]{n}=n^{1/n}, \qquad \left(1+\frac1n\right)^{n}.

Try the naive move on the first. As n→∞n\to\infty, the factor nn runs off to infinity while the parenthesis 1+1n−1\sqrt{1+\frac1n}-1 collapses to 00. So the answer is… infinity times zero? That is not a number. It is a fight between a part pulling the product up and a part pulling it down, and “∞⋅0\infty\cdot 0” is just our shorthand for “the winner is not yet decided — look closer.”

These deadlocks have a name: indeterminate forms. The usual suspects are

∞⋅0,∞∞,00,1∞,∞−∞,00.\infty\cdot 0,\qquad \frac{\infty}{\infty},\qquad \frac{0}{0},\qquad 1^{\infty},\qquad \infty-\infty,\qquad 0^{0}.

When substitution lands you on one of these, you have learned exactly one thing: you cannot stop here. The limit might be 00, might be ∞\infty, might be any finite number in between — it depends on how fast each part moves, and finding out is the whole skill. Our three sequences are, in order, an ∞⋅0\infty\cdot0, an ∞0\infty^0, and a 1∞1^\infty. Let’s win all three. First we need one new tool.

Toolkit: The Squeeze Theorem

If a sequence is trapped between two others heading to the same place, it has no choice but to go there too.

Squeeze Theorem. If an≤bn≤cna_n \le b_n \le c_n for all large nn, and both an→La_n \to L and cn→Lc_n \to L, then bn→Lb_n \to L.

Use it when bnb_n itself is hard but you can bound it above and below by things you understand. The art is choosing good walls.

A quick win, to watch it move: what is lim⁡n→∞sin⁡nn\displaystyle\lim_{n\to\infty}\dfrac{\sin n}{n}? The numerator sin⁡n\sin n lurches around forever and has no limit of its own — but it never escapes the corridor −1≤sin⁡n≤1-1 \le \sin n \le 1. Divide through by nn:

−1n≤sin⁡nn≤1n.-\frac1n \;\le\; \frac{\sin n}{n} \;\le\; \frac1n.

Both walls, ±1n\pm\frac1n, go to 00. Squeezed between them, sin⁡nn→0\dfrac{\sin n}{n}\to 0 — and we never had to tame the wild numerator. We just fenced it in.

◆ Proof: the Squeeze Theorem

Play the game. Given ε>0\varepsilon>0: since an→La_n\to L there’s a cutoff N1N_1 past which an>L−εa_n > L-\varepsilon; since cn→Lc_n\to L there’s a cutoff N2N_2 past which cn<L+εc_n < L+\varepsilon. Let NN be the larger of the two. Then for every n>Nn>N, the sandwich an≤bn≤cna_n \le b_n \le c_n gives L−ε<an≤bn≤cn<L+ε,L-\varepsilon < a_n \le b_n \le c_n < L+\varepsilon, so |bn−L|<ε|b_n - L| < \varepsilon. Beaten for every ε\varepsilon, so bn→Lb_n\to L. ◼\blacksquare

Fight one: n(1+1n−1)n\left(\sqrt{1+\tfrac1n}-1\right) (an ∞⋅0\infty\cdot0)

The move with an indeterminate form is almost always to rewrite it until a shape you can finish. Here the troublemaker is the difference of a square root and 11, and the standard cure is to rationalize — multiply by the conjugate 1+1n+1\sqrt{1+\tfrac1n}+1 over itself, which turns the difference of roots into a clean difference of the things under them:

n(1+1n−1)=n⋅(1+1n)−11+1n+1=n⋅1/n1+1n+1=11+1n+1.n\left(\sqrt{1+\tfrac1n}-1\right) = n\cdot\frac{\left(1+\tfrac1n\right)-1}{\sqrt{1+\tfrac1n}+1} = n\cdot\frac{1/n}{\sqrt{1+\tfrac1n}+1} = \frac{1}{\sqrt{1+\tfrac1n}+1}.

The nn canceled the 1n\tfrac1n — the two combatants annihilated, leaving something tame. As n→∞n\to\infty, 1n→0\tfrac1n\to0, so the bottom heads to 1+1=2\sqrt{1}+1 = 2, and

n(1+1n−1)→12.n\left(\sqrt{1+\tfrac1n}-1\right) \to \frac12.

Not 00, not ∞\infty, but exactly 12\tfrac12: the growing nn and the shrinking parenthesis were perfectly matched, and they balance at one-half. (Tuck this away: in Chapter 3 you’ll recognize 12\tfrac12 as the slope of x\sqrt{x} at x=1x=1. You are computing a derivative right now without knowing it — and we’ll meet the same 00\frac00-after-rationalizing move again the moment we reach functions in Chapter 2.)

Fight two: nn\sqrt[n]{n} (an ∞0\infty^0, and a genuine surprise)

This one should bother you. Take the nn-th root of nn: 22≈1.41\sqrt[2]{2}\approx1.41, 33≈1.44\sqrt[3]{3}\approx1.44, 1010≈1.26\sqrt[10]{10}\approx1.26, 100100≈1.047\sqrt[100]{100}\approx1.047, 10001000≈1.0069\sqrt[1000]{1000}\approx1.0069. The thing under the root is racing to infinity, yet the root is settling toward 11. The form is ∞0\infty^0 — a huge base, a vanishing exponent 1n\frac1n — and the vanishing exponent wins. (Intuition: roots are ferocious levelers; a giant number rooted hard enough is tamed almost to 11.) The proof is a small gem.

◆ Proof: n1/n→1n^{1/n}\to 1

Since n1/n≥1n^{1/n}\ge1, write n1/n=1+hnn^{1/n}=1+h_n with hn≥0h_n\ge0; we must show hn→0h_n\to0. Raise to the nn-th power: n=(1+hn)nn=(1+h_n)^n. Expand by the binomial theorem and throw away every term but one — keep only the k=2k=2 term, legal because all terms are nonnegative: n=(1+hn)n≥(n2)hn2=n(n−1)2hn2.n = (1+h_n)^n \;\ge\; \binom{n}{2}h_n^2 = \frac{n(n-1)}{2}\,h_n^2. Divide by n(n−1)2\frac{n(n-1)}{2}: hn2≤2n−1\;h_n^2 \le \dfrac{2}{n-1}, so 0≤hn≤2n−10 \le h_n \le \sqrt{\dfrac{2}{n-1}}. The right wall is built from 1n−1→0\frac{1}{n-1}\to0, so it →0\to0; the left wall is 00. Squeeze: hn→0h_n\to0, hence n1/n=1+hn→1n^{1/n}=1+h_n\to1. ◼\blacksquare The trick worth stealing: when a binomial expansion is all-positive, keeping a single well-chosen term is a valid lower bound — and one term is often all you need.

Making the theorem earn its living: a sequence that defines itself

The monotone-convergence principle feels abstract until you meet a sequence with no formula at all, built by feeding each term back into itself:

Figure 1.7
Figure 1.7

a1=2,an+1=2+an.a_1=\sqrt2,\qquad a_{n+1}=\sqrt{2+a_n}.

So a2=2+2≈1.848a_2=\sqrt{2+\sqrt2}\approx1.848, a3≈1.962a_3\approx1.962, a4≈1.990a_4\approx1.990, climbing toward… something. We can’t write ana_n in closed form — but we can still find the limit exactly, and this is the principle’s finest hour.

◆ Layer 2 — Solving a self-defined sequence

Step 1 — bounded above by 22 (induction): a1=2<2a_1=\sqrt2<2; and if an<2a_n<2, then an+1=2+an<2+2=2a_{n+1}=\sqrt{2+a_n}<\sqrt{2+2}=2. So every term stays under 22. Step 2 — increasing: an+1>ana_{n+1}>a_n means 2+an>an\sqrt{2+a_n}>a_n, i.e. (square, both sides positive) 2+an>an22+a_n>a_n^2, i.e. an2−an−2<0a_n^2-a_n-2<0, i.e. (an−2)(an+1)<0(a_n-2)(a_n+1)<0 — true for every ana_n with 0<an<20<a_n<2, which Step 1 guarantees. Step 3 — therefore it converges (increasing and bounded above) to some limit LL. Step 4 — pin down LL. Take the limit of both sides of the rule an+1=2+ana_{n+1}=\sqrt{2+a_n}. The left side →L\to L; the right side →2+L\to\sqrt{2+L}. So LL must obey its own equation: L=2+L⇒L2=2+L⇒(L−2)(L+1)=0.L=\sqrt{2+L}\;\Longrightarrow\;L^2=2+L\;\Longrightarrow\;(L-2)(L+1)=0. Hence L=2L=2 (reject −1-1: the terms are positive). The sequence we couldn’t even write down converges to exactly 22. That move — let the limit satisfy the rule — is your first fixed point: a value a process leaves unchanged. It returns whenever you study how an iteration settles, including, in spirit, the iterations of Chapter 8.


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