Calculus I · Patterns That Go Somewhere

The many faces of ee

The sequence (1+1n)n\left(1+\frac1n\right)^n is the most important 1∞1^\infty fight in all of mathematics, and it has a whole family. What if we replace that 11 in the numerator with some other number xx?

(1+xn)n→ex\boxed{\;\left(1+\frac{x}{n}\right)^n \longrightarrow e^{\,x}\;}

This single fact is the bridge from this chapter to Chapter 5. It says ee is not a one-off curiosity: it spawns an entire function exe^x, and that function is born from compounding. Set x=1x=1 and recover the original →e\to e. Set x=−1x=-1: (1−1n)n→e−1=1e≈0.368\left(1-\frac1n\right)^n\to e^{-1}=\frac1e\approx0.368. Set x=2x=2: (1+2n)n→e2\left(1+\frac2n\right)^n\to e^2. Try a few on a calculator and watch them land on powers of ee.

◆ Layer 2 — Why (1+xn)n→ex\left(1+\frac{x}{n}\right)^n\to e^x (one honest loan)

Take the logarithm, which turns the frightening exponent into a product (Chapter 5 makes ln\ln rigorous; here we borrow only that ln\ln pulls a power down into a multiplier): ln⁡(1+xn)n=nln⁡(1+xn).\ln\left(1+\frac{x}{n}\right)^n = n\,\ln\!\left(1+\frac{x}{n}\right). Let t=xn→0t=\frac{x}{n}\to0, so n=xtn=\frac{x}{t}, and the right side becomes x⋅ln⁡(1+t)tx\cdot\dfrac{\ln(1+t)}{t}. One more famous limit closes it: ln⁡(1+t)t→1\dfrac{\ln(1+t)}{t}\to1 as t→0t\to0 (this is the slope of ln\ln at 11, proven in Chapter 5 — the loan). So the logarithm of our sequence →x⋅1=x\to x\cdot1=x, which means the sequence itself →ex\to e^x. ◼\blacksquare Notice it is the same smallsmall→1\frac{\text{small}}{\text{small}}\to1 shape that turned up in Fight one. The limits that fight back are almost always derivatives wearing a costume — you’ll see this confirmed in Chapters 2 and 3.

The race decides everything: three sequences, three fates

The form 1∞1^\infty is indeterminate precisely because the answer hinges on a race — how fast the base sinks toward 11 versus how fast the exponent climbs to ∞\infty. Watch three sequences that all look like “1∞1^\infty” land in three different worlds:

Figure 1.6
Figure 1.6

(1+1n)n→e,(1+1n2)n→1,(1+1n)n2→∞.\left(1+\frac1n\right)^{n}\to e,\qquad \left(1+\frac{1}{n^2}\right)^{n}\to 1,\qquad \left(1+\frac1n\right)^{n^2}\to \infty.

In the first, base and exponent are matched and balance at ee. In the second, the base rushes to 11 too fast (like 1n2\frac1{n^2}) for a mere nn in the exponent to matter — its logarithm runs like n⋅1n2=1n→0n\cdot\frac1{n^2}=\frac1n\to0, so the limit is e0=1e^0=1. In the third, the exponent n2n^2 is too strong for the base’s gentle approach — its logarithm runs like n2⋅1n=n→∞n^2\cdot\frac1n=n\to\infty, so it explodes.

Same form, three answers, decided entirely by who wins. Here’s the gauge that settles any of them at a glance: for a base near 11, look at (exponent)×(base−1)(\text{exponent})\times(\text{base}-1); whatever number kk that approaches, the limit is eke^{k}. Run the three cases through it and out pop e1=ee^1=e, then e0=1e^0=1, then e∞=∞e^\infty=\infty. That is the entire secret of 1∞1^\infty forms, and you now hold it.


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