Types of Discontinuity
A Hole from a Factor That Cancels
Classify the discontinuity of $f(x) = \frac{x^2 - x - 2}{x - 2}$ at $x = 2$ and remove it.
Check where $f$ is undefined: The denominator $x - 2$ is $0$ at $x = 2$ = $f(2)$ is undefined
Factor the numerator: $x^2 - x - 2 = (x - 2)(x + 1)$ = $f(x) = \frac{(x - 2)(x + 1)}{x - 2}$
Cancel the common factor: $f(x) = x + 1$ for every $x \neq 2$ = The factor $(x - 2)$ cancels completely
Find the limit: $\lim_{x \to 2} f(x) = 2 + 1$ = $= 3$, a finite limit
Classify and fix: Limit exists, $f(2)$ does not: a hole at $(2, 3)$. Define $f(2) = 3$. = Removable discontinuity
Answer: Removable discontinuity (hole) at $(2, 3)$. Setting $f(2) = 3$ makes $f$ continuous.
A Hole with the Wrong Value
Let $g(x) = x^2$ for $x \neq 1$ and $g(1) = 4$. What type of discontinuity is at $x = 1$?
Find the limit: Near $x = 1$ the rule is $x^2$, so $\lim_{x \to 1} g(x) = 1^2$ = $= 1$
Find the function value: The definition says $g(1) = 4$ = $g(1) = 4$
Compare: $\lim_{x \to 1} g(x) = 1 \neq 4 = g(1)$ = The limit exists but differs from $g(1)$
Classify and fix: The point $(1, 4)$ sits away from the curve; redefine $g(1) = 1$ = Removable discontinuity
Answer: Removable discontinuity at $x = 1$: there is a hole at $(1, 1)$ and a separate dot at $(1, 4)$. Redefining $g(1) = 1$ removes it.
Measuring a Jump
Let $h(x) = x + 2$ for $x < 1$ and $h(x) = x^2 + 5$ for $x \geq 1$. Classify the discontinuity at $x = 1$ and find the jump size.
Left-hand limit (use the rule for $x < 1$): $\lim_{x \to 1^-} (x + 2) = 1 + 2$ = $= 3$
Right-hand limit (use the rule for $x \geq 1$): $\lim_{x \to 1^+} (x^2 + 5) = 1 + 5$ = $= 6$
Compare the one-sided limits: Both are finite, but $3 \neq 6$ = Jump discontinuity
Jump size: $|6 - 3|$ = $= 3$
Answer: Jump discontinuity at $x = 1$ with jump size $3$. The value $h(1) = 6$ does not matter: no choice of $h(1)$ can close the gap.
An Infinite Discontinuity
Classify the discontinuity of $k(x) = \frac{x + 3}{x - 4}$ at $x = 4$.
Substitute $x = 4$: Numerator $4 + 3 = 7$, denominator $4 - 4 = 0$ = $\frac{7}{0}$: a nonzero number over zero
Approach from the right: $k(4.01) = \frac{7.01}{0.01} = 701$ = $\lim_{x \to 4^+} k(x) = \infty$
Approach from the left: $k(3.99) = \frac{6.99}{-0.01} = -699$ = $\lim_{x \to 4^-} k(x) = -\infty$
Classify: The one-sided limits are infinite = Infinite discontinuity, vertical asymptote $x = 4$
Answer: Infinite discontinuity at $x = 4$: the graph has the vertical asymptote $x = 4$.
Holes and Asymptotes in One Function
Find and classify every discontinuity of $r(x) = \frac{x^2 - 9}{x^2 - x - 6}$.
Factor both parts: $r(x) = \frac{(x - 3)(x + 3)}{(x - 3)(x + 2)}$ = Undefined at $x = 3$ and $x = -2$
Cancel the common factor: $r(x) = \frac{x + 3}{x + 2}$ for $x \neq 3$ = $(x - 3)$ cancels, $(x + 2)$ stays
Handle $x = 3$: $\lim_{x \to 3} r(x) = \frac{3 + 3}{3 + 2}$ = $= \frac{6}{5}$: hole at $\left(3, \frac{6}{5}\right)$
Handle $x = -2$: Simplified numerator $-2 + 3 = 1 \neq 0$, denominator $0$ = Vertical asymptote $x = -2$
Answer: Removable discontinuity (hole) at $\left(3, \frac{6}{5}\right)$ and infinite discontinuity at $x = -2$.
Mistake: Drawing a vertical asymptote at every zero of the denominator
Why: A zero of the denominator can also be a hole. In $\frac{x^2 - x - 2}{x - 2}$ the factor $(x - 2)$ cancels, so there is no asymptote at $x = 2$.
Correct: Factor and cancel first. Only factors left in the denominator give vertical asymptotes; cancelled factors give holes.
Mistake: Calling a jump removable because both one-sided limits exist
Why: Removable needs the two-sided limit, which exists only when both sides agree. At a jump they are different numbers.
Correct: Equal one-sided limits: removable (or continuous). Different finite one-sided limits: jump.
Mistake: Using $f(a)$ as the height of the hole
Why: At a hole $f(a)$ is missing or wrong. The hole sits at the height of the limit.
Correct: Find the $y$-coordinate of a hole by substituting $x = a$ into the simplified function: the hole of $\frac{x^2 - 9}{x^2 - x - 6}$ is at $\left(3, \frac{6}{5}\right)$.
Mistake: Thinking a cancelled factor always means a hole, even when it appears twice in the denominator
Why: In $\frac{x - 1}{(x - 1)^2}$ only one factor cancels; $\frac{1}{x - 1}$ is left, which still blows up at $x = 1$.
Correct: Cancel as far as possible, then check: if $(x - a)$ is still in the denominator, it is an infinite discontinuity.
Parking Fees (Jumps)
Parking garages charge by the started hour, so the price function is constant on each hour and jumps at every full hour.
A garage charges 4 dollars for up to 1 hour and 7 dollars for more than 1 hour up to 2 hours. At $t = 1$ the price jumps by 3 dollars.
Lenses and Images at Infinity
For a lens with focal length $10$ cm, an object at distance $u$ produces an image at distance $v(u) = \frac{10u}{u - 10}$. When the object reaches the focal point, the image moves off to infinity.
At $u = 15$ cm the image is at $v = \frac{150}{5} = 30$ cm. At $u = 10.1$ cm it is already at $v = \frac{101}{0.1} = 1010$ cm.
Fixing a Division by Zero in Software
Programs often compute an average rate of change $\frac{f(t) - f(a)}{t - a}$. At $t = a$ the formula gives $\frac{0}{0}$ and the program crashes, although the values nearby are perfectly smooth: a removable discontinuity.
For $f(t) = t^2$ and $a = 3$, the rate $\frac{t^2 - 9}{t - 3}$ simplifies to $t + 3$, so the programmer stores the value $6$ for $t = 3$.
A discontinuity at $x = a$ means $\lim_{x \to a} f(x) = f(a)$ fails
Removable (hole): the limit $L$ exists, but $f(a)$ is missing or different; redefine $f(a) = L$ to fix it
Jump: finite one-sided limits that differ; jump size $= \left| \lim_{x \to a^+} f(x) - \lim_{x \to a^-} f(x) \right|$
Infinite: a one-sided limit is $\pm\infty$; the graph has a vertical asymptote $x = a$
For rational functions, factor first: cancelled factors give holes, factors left in the denominator give asymptotes
The $y$-coordinate of a hole comes from the simplified function, never from $f(a)$
Q: Why is a hole called removable?
A: Because one point is enough to repair it. The limit $L$ already exists, so defining (or redefining) $f(a) = L$ makes $\lim_{x \to a} f(x) = f(a)$ true, and the function becomes continuous at $a$.
Q: Can a jump discontinuity ever be removed?
A: No. The left side heads to one height and the right side to another. Whatever value you give $f(a)$, it can match at most one side, so the two-sided limit still does not exist.
Q: Does a function value at $x = a$ change the type?
A: No. The type depends only on the limits near $a$. A jump stays a jump whether $f(a)$ is the left value, the right value or undefined, and a hole stays removable whether $f(a)$ is missing or wrong.
Q: Are there other types of discontinuity?
A: Yes, but they are rarer. For example $\sin\left(\frac{1}{x}\right)$ oscillates faster and faster near $x = 0$, so it has no one-sided limits at all (an oscillating discontinuity). Jumps, infinite and oscillating discontinuities are all non-removable; many books call only the infinite and oscillating ones essential.
Types of Discontinuity
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Types of Discontinuity
Learn to tell removable discontinuities (holes), jump discontinuities and infinite discontinuities apart, from graphs and from formulas.