TheoremComplete

Limits and Continuity - Main Theorem

The limit laws provide the algebraic foundation for computing limits without resorting to the epsilon-delta definition each time. These rules allow us to break down complex limits into simpler components.

TheoremLimit Laws

Suppose lim⁡x→af(x)=L\lim_{x \to a} f(x) = L and lim⁡x→ag(x)=M\lim_{x \to a} g(x) = M both exist. Then:

  1. Sum Rule: lim⁡x→a[f(x)+g(x)]=L+M\lim_{x \to a} [f(x) + g(x)] = L + M
  2. Difference Rule: lim⁡x→a[f(x)−g(x)]=L−M\lim_{x \to a} [f(x) - g(x)] = L - M
  3. Constant Multiple Rule: lim⁡x→a[cf(x)]=cL\lim_{x \to a} [cf(x)] = cL for any constant cc
  4. Product Rule: lim⁡x→a[f(x)⋅g(x)]=L⋅M\lim_{x \to a} [f(x) \cdot g(x)] = L \cdot M
  5. Quotient Rule: lim⁡x→af(x)g(x)=LM\lim_{x \to a} \frac{f(x)}{g(x)} = \frac{L}{M} provided M≠0M \neq 0
  6. Power Rule: lim⁡x→a[f(x)]n=Ln\lim_{x \to a} [f(x)]^n = L^n for any positive integer nn
  7. Root Rule: lim⁡x→af(x)n=Ln\lim_{x \to a} \sqrt[n]{f(x)} = \sqrt[n]{L} provided L>0L > 0 when nn is even

These laws are intuitive but require rigorous proof using the epsilon-delta definition. They extend to one-sided limits and limits at infinity with appropriate modifications.

ExampleUsing Limit Laws

Compute lim⁡x→3x2+2x−15x−3\lim_{x \to 3} \frac{x^2 + 2x - 15}{x - 3}.

Direct substitution gives 00\frac{0}{0}, an indeterminate form. Factor the numerator: x2+2x−15=(x−3)(x+5)x^2 + 2x - 15 = (x - 3)(x + 5)

For x≠3x \neq 3: x2+2x−15x−3=(x−3)(x+5)x−3=x+5\frac{x^2 + 2x - 15}{x - 3} = \frac{(x - 3)(x + 5)}{x - 3} = x + 5

By the limit laws: lim⁡x→3x2+2x−15x−3=lim⁡x→3(x+5)=3+5=8\lim_{x \to 3} \frac{x^2 + 2x - 15}{x - 3} = \lim_{x \to 3} (x + 5) = 3 + 5 = 8

TheoremSqueeze Theorem

Suppose g(x)≤f(x)≤h(x)g(x) \leq f(x) \leq h(x) for all xx in an open interval containing aa, except possibly at aa itself. If lim⁡x→ag(x)=lim⁡x→ah(x)=L\lim_{x \to a} g(x) = \lim_{x \to a} h(x) = L then lim⁡x→af(x)=L\lim_{x \to a} f(x) = L

The Squeeze Theorem is particularly powerful for functions that oscillate or are difficult to evaluate directly.

ExampleA Classic Application

Prove that lim⁡x→0x2sin⁡(1x)=0\lim_{x \to 0} x^2 \sin\left(\frac{1}{x}\right) = 0.

We know −1≤sin⁡(1x)≤1-1 \leq \sin\left(\frac{1}{x}\right) \leq 1 for all x≠0x \neq 0. Multiplying by x2≥0x^2 \geq 0: −x2≤x2sin⁡(1x)≤x2-x^2 \leq x^2 \sin\left(\frac{1}{x}\right) \leq x^2

Since lim⁡x→0(−x2)=0\lim_{x \to 0} (-x^2) = 0 and lim⁡x→0x2=0\lim_{x \to 0} x^2 = 0, by the Squeeze Theorem: lim⁡x→0x2sin⁡(1x)=0\lim_{x \to 0} x^2 \sin\left(\frac{1}{x}\right) = 0

Note that sin⁡(1x)\sin\left(\frac{1}{x}\right) oscillates infinitely as x→0x \to 0 and has no limit, but multiplication by x2x^2 dampens these oscillations.

Remark

The Squeeze Theorem is often the only practical way to evaluate limits involving trigonometric functions with oscillatory behavior or products where one factor is bounded and another approaches zero.