What is Calculus I

a Limit?

The value a function approaches as its input gets arbitrarily close to a point — the very foundation that makes calculus possible.

Imagine walking toward a wall. You get closer and closer, halving the distance each step — 1 meter, 0.5 m, 0.25 m, 0.125 m... You're approaching the wall, even if you never actually touch it. That's the idea of a limit.

In mathematics, the limit of a function \(f(x)\) as \(x\) approaches some value \(a\) is the value that \(f(x)\) gets closer and closer to as \(x\) gets closer and closer to \(a\). Crucially, we don't care what happens at \(x = a\) — only what the function approaches.

This matters enormously because many functions are undefined at certain points (like \(\frac{0}{0}\)), yet they approach a perfectly clear value. Limits let us work with those cases precisely.

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Approaching from both sides

A limit exists only if the function approaches the same value from both the left and the right. If you walk toward a cliff from both directions and the height you're stepping toward is different depending on which side you come from — there's no single limit. If both sides agree, the limit exists.

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The function's value doesn't matter

The limit of \(f(x)\) as \(x \to a\) is completely independent of \(f(a)\). The function could be undefined at \(a\), it could have a hole in its graph, or its value could be something totally different — and the limit would still exist and have its own value. This is what makes limits so powerful.

The function has a hole at x = 2, yet the limit clearly exists — both sides approach the same value

Consider \(\lim_{x \to 2} \dfrac{x^2 - 4}{x - 2}\). At \(x=2\) this is \(\frac{0}{0}\) — undefined. But watch what happens as we approach:

x (from left)f(x)x (from right)f(x)
1.93.92.14.1
1.993.992.014.01
1.9993.9992.0014.001
→ 2→ 4← 2← 4

Both sides converge to 4. So \(\lim_{x \to 2} \dfrac{x^2 - 4}{x - 2} = 4\), even though \(f(2)\) is undefined.

We write \(\lim_{x \to a} f(x) = L\), and read it as "the limit of \(f(x)\) as \(x\) approaches \(a\) equals \(L\)." The precise (epsilon-delta) definition:

Epsilon-Delta Definition
$$\lim_{x \to a} f(x) = L \iff \forall\, \varepsilon > 0,\ \exists\, \delta > 0 \text{ such that } 0 < |x - a| < \delta \implies |f(x) - L| < \varepsilon$$

In plain English: no matter how small a window \(\varepsilon\) you draw around \(L\), you can always find a window \(\delta\) around \(a\) so that all \(x\) inside that window map to \(f(x)\) inside your \(\varepsilon\)-window. The function is truly, precisely approaching \(L\).

Sum\(\lim[f+g] = \lim f + \lim g\)
Product\(\lim[f \cdot g] = \lim f \cdot \lim g\)
Quotient\(\lim\dfrac{f}{g} = \dfrac{\lim f}{\lim g}\quad (\lim g \neq 0)\)
Constant\(\lim[c \cdot f] = c \cdot \lim f\)
Power\(\lim[f^n] = (\lim f)^n\)
Squeeze ThmIf \(g \leq f \leq h\) and \(\lim g = \lim h = L\), then \(\lim f = L\)
Example 1 — Direct Substitution
\(\lim_{x \to 3} (x^2 + 1)\)
Plug in directly: \(3^2 + 1 = 10\)
Example 2 — Factor & Cancel
\(\lim_{x \to 2} \dfrac{x^2-4}{x-2}\)
Factor: \(\dfrac{(x-2)(x+2)}{x-2} = x+2\)
Result: \(4\)
Example 3 — Infinity
\(\lim_{x \to \infty} \dfrac{1}{x}\)
As \(x\) grows without bound, \(\frac{1}{x} \to 0\)
Example 4 — Famous Limit
\(\lim_{x \to 0} \dfrac{\sin x}{x}\)
This equals \(1\) — proven with the Squeeze Theorem, and essential in all of calculus.
✗ Confusing the limit with the function's value
The limit as \(x \to a\) has nothing to do with \(f(a)\). A function can have a limit of 5 at a point where it equals 0, or is completely undefined.
✗ Assuming a limit always exists
If the left-hand limit and right-hand limit are different, the (two-sided) limit does not exist. Always check both sides for piecewise or discontinuous functions.
✗ Writing \(\frac{0}{0}\) = 0 or undefined without investigating
\(\frac{0}{0}\) is an indeterminate form — it tells you nothing on its own. You must simplify, factor, or apply L'Hôpital's Rule to find the actual limit.

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