The Intuition of One-Sided Limits
While algebra asks "What is the value at $x=a$?", calculus asks "What value does the function approach as $x$ gets arbitrarily close to $a$?" This allows us to navigate "holes" or jumps in functions where a value might not exist.
We write $\lim_{x \to a^-} f(x) = L$ if we can make the values of $f(x)$ arbitrarily close to $L$ by taking $x$ to be sufficiently close to $a$ and $x$ less than $a$. This is the "approach from the left" seen in Figure 9.
For a two-sided limit to exist, the left and right perspectives must agree perfectly:
$$\lim_{x \to a} f(x) = L \iff \lim_{x \to a^-} f(x) = L = \lim_{x \to a^+} f(x)$$
If these do not match, such as in the Heaviside function (Figure 8), we say the limit Does Not Exist (DNE).
Infinite Limits and Asymptotes
Sometimes, a function doesn't approach a finite number; it explodes. Definition 4 states that if $f(x)$ increases without bound as $x \to a$, we say $\lim_{x \to a} f(x) = \infty$. This identifies a Vertical Asymptote (Definition 6).
Practical Examples
- Example 8: $\lim_{x \to 0} 1/x^2 = \infty$. Both sides of the graph in Figure 11 shoot upward together.
- Example 10: The function $y = \tan x$ has vertical asymptotes at $x = \pi/2 + n\pi$ because the values approach $\pm\infty$ (see Figure 16).
- Logarithmic Behavior: In Figure 17, we observe that $\lim_{x \to 0^+} \ln x = -\infty$, creating a vertical asymptote at the y-axis.