Infinite Limits: Definition, Asymptotes and Examples

#Calculus
TL;DR
An infinite limit means f(x) grows without bound as x approaches a, so the graph has a vertical asymptote there. This guide covers infinite limits, sign analysis, asymptotes and limits at infinity.
MV
Madhukar VLast updated on October 9, 202615 min read

What Are Infinite Limits?

Infinite limits describe a function whose values grow without bound, positively or negatively, as xx approaches a finite number aa. If f(x)f(x) can be made larger than any number you choose by taking xx close enough to aa, we write lim⁑xβ†’af(x)=+∞\lim_{x \to a} f(x) = +\infty. If f(x)f(x) can be made more negative than any number you choose, we write lim⁑xβ†’af(x)=βˆ’βˆž\lim_{x \to a} f(x) = -\infty.

The idea comes in one-sided and two-sided versions, just like the ordinary limit of a function:

lim⁑xβ†’aβˆ’f(x)=±∞lim⁑xβ†’a+f(x)=±∞lim⁑xβ†’af(x)=±∞\lim_{x \to a^{-}} f(x) = \pm\infty \qquad \lim_{x \to a^{+}} f(x) = \pm\infty \qquad \lim_{x \to a} f(x) = \pm\infty

  • xβ†’aβˆ’x \to a^{-} uses only values below aa, and xβ†’a+x \to a^{+} uses only values above aa.

  • +∞+\infty means "increases without bound" and βˆ’βˆž-\infty means "decreases without bound". Neither is a real number.

  • The two-sided statement lim⁑xβ†’af(x)=+∞\lim_{x \to a} f(x) = +\infty requires both one-sided limits to be +∞+\infty (and the same for βˆ’βˆž-\infty).

The precise definition replaces the usual Ξ΅\varepsilon with a height MM. The statement lim⁑xβ†’af(x)=+∞\lim_{x \to a} f(x) = +\infty means: for every M>0M > 0 there is a Ξ΄>0\delta > 0 such that

0<∣xβˆ’a∣<δ⟹f(x)>M0 < \lvert x - a \rvert < \delta \quad \Longrightarrow \quad f(x) > M

An infinite limit is a description, not a value. In standard calculus, a limit "exists" only when it is a real number LL. Writing lim⁑xβ†’01x2=+∞\lim_{x \to 0} \frac{1}{x^2} = +\infty records exactly how the limit fails to exist: the values climb past every bound. OpenStax makes the same point in Calculus Volume 1, Section 2.2, and courses that use the extended real line (where +∞+\infty and βˆ’βˆž-\infty are added as points) are the only exception.

How Do You Evaluate Infinite Limits?

Most infinite limits come from a quotient whose denominator heads to 0 while the numerator heads to a nonzero number. The job is to decide the size (it blows up) and the sign (plus or minus) on each side.

A Table Of Values Near Zero

A table shows the pattern before any rule does. For f(x)=1xf(x) = \frac{1}{x} near 0:

xx (left of 0)

1x\frac{1}{x}

xx (right of 0)

1x\frac{1}{x}

βˆ’0.1-0.1

βˆ’10-10

0.10.1

1010

βˆ’0.01-0.01

βˆ’100-100

0.010.01

100100

βˆ’0.001-0.001

βˆ’1000-1000

0.0010.001

10001000

βˆ’0.0001-0.0001

βˆ’10000-10000

0.00010.0001

1000010000

Each step closer to 0 multiplies the size by 10, and the sign matches the sign of xx. So lim⁑xβ†’0+1x=+∞\lim_{x \to 0^{+}} \frac{1}{x} = +\infty and lim⁑xβ†’0βˆ’1x=βˆ’βˆž\lim_{x \to 0^{-}} \frac{1}{x} = -\infty. Because the two sides disagree, the two-sided limit has no single description, so it simply does not exist.

The Sign Method

Tables can mislead when the blow-up is slow, so the reliable method is a sign analysis:

  1. Substitute x=ax = a first. A result of the form c0\frac{c}{0} with c≠0c \neq 0 signals an infinite limit. A result of 00\frac{0}{0} is different: simplify first, because the limit might be finite.

  2. Find the sign of the numerator near aa. It matches the sign of cc.

  3. Find the sign of the denominator on each side. Test one value just left and one just right of aa, or reason from the factors.

  4. Combine. Same signs give +∞+\infty, opposite signs give βˆ’βˆž-\infty.

For x+1xβˆ’2\frac{x + 1}{x - 2} at x=2x = 2: the numerator heads to 3 (positive), the denominator is positive for x>2x > 2 and negative for x<2x < 2. So the right-hand limit is +∞+\infty and the left-hand limit is βˆ’βˆž-\infty.

Writing The Answer: Undefined, Infinity Or Does Not Exist

These three words do different jobs, and mixing them costs marks. "Undefined" describes the function value: f(2)f(2) is undefined for x+1xβˆ’2\frac{x + 1}{x - 2} because of division by zero. "+∞+\infty" or "βˆ’βˆž-\infty" describes a limit whose values grow without bound in one direction. "Does not exist" is the umbrella verdict whenever no real-number limit exists.

So the most informative answer is the most specific true one:

  • If both sides go to +∞+\infty, write lim⁑xβ†’af(x)=+∞\lim_{x \to a} f(x) = +\infty.

  • If the sides go to opposite infinities, give each one-sided limit and say the two-sided limit does not exist.

  • Never write "the limit is undefined". A limit either exists, is ±∞\pm\infty, or does not exist.

Infinite Limits Of Reciprocal Powers: Even Versus Odd

The cleanest family of infinite limits is f(x)=1(xβˆ’a)nf(x) = \frac{1}{(x - a)^n} for a positive integer nn, and the parity of nn decides everything. An even power makes the denominator positive on both sides of aa, while an odd power keeps the sign of xβˆ’ax - a.

nΒ even:lim⁑xβ†’a1(xβˆ’a)n=+∞n \text{ even:} \quad \lim_{x \to a} \frac{1}{(x - a)^n} = +\infty

nΒ odd:lim⁑xβ†’aβˆ’1(xβˆ’a)n=βˆ’βˆž,lim⁑xβ†’a+1(xβˆ’a)n=+∞n \text{ odd:} \quad \lim_{x \to a^{-}} \frac{1}{(x - a)^n} = -\infty, \qquad \lim_{x \to a^{+}} \frac{1}{(x - a)^n} = +\infty

That is why 1x2\frac{1}{x^2} shoots up on both sides of 0 while 1x\frac{1}{x} splits. For 1x2\frac{1}{x^2} both one-sided limits are +∞+\infty, so the two-sided statement lim⁑xβ†’01x2=+∞\lim_{x \to 0} \frac{1}{x^2} = +\infty is correct, even though no real-number limit exists. A multiplying constant only scales the picture: βˆ’3x2\frac{-3}{x^2} goes to βˆ’βˆž-\infty on both sides.

A vertical asymptote is the graphical name for an infinite limit. The line x=ax = a is a vertical asymptote of ff if at least one of these holds:

lim⁑xβ†’aβˆ’f(x)=±∞orlim⁑xβ†’a+f(x)=±∞\lim_{x \to a^{-}} f(x) = \pm\infty \qquad \text{or} \qquad \lim_{x \to a^{+}} f(x) = \pm\infty

One side is enough. The graph of ln⁑x\ln x has a vertical asymptote at x=0x = 0 even though only the right-hand limit makes sense there, because lim⁑xβ†’0+ln⁑x=βˆ’βˆž\lim_{x \to 0^{+}} \ln x = -\infty (the natural logarithm is only defined for x>0x > 0). In the language of discontinuities, every vertical asymptote marks an infinite discontinuity.

For rational functions, the asymptotes sit where the denominator is zero after cancelling common factors:

  1. Factor the numerator and the denominator.

  2. Cancel any common factor (xβˆ’a)(x - a). Its zero becomes a hole, a removable discontinuity, not an asymptote.

  3. Read the asymptotes from the zeros of the denominator that remain.

Trigonometric functions carry asymptotes too. The tangent function blows up at odd multiples of Ο€2\frac{\pi}{2}, with lim⁑xβ†’(Ο€/2)βˆ’tan⁑x=+∞\lim_{x \to (\pi/2)^{-}} \tan x = +\infty and lim⁑xβ†’(Ο€/2)+tan⁑x=βˆ’βˆž\lim_{x \to (\pi/2)^{+}} \tan x = -\infty, and the same sign reasoning handles sec⁑x\sec x, csc⁑x\csc x and cot⁑x\cot x (all ratios built from the trigonometric functions sine and cosine).

Infinite Limits Vs Limits At Infinity

Infinite limits and limits at infinity sound alike but ask opposite questions. An infinite limit sends xx to a finite number and watches the output explode, while a limit at infinity sends xx off to infinity and watches where the output settles.

Infinite limit

Limit at infinity

Input

x→ax \to a (a finite number)

xβ†’+∞x \to +\infty or xβ†’βˆ’βˆžx \to -\infty

Output

f(x)β†’Β±βˆžf(x) \to \pm\infty

f(x)β†’Lf(x) \to L (often a finite number)

Typical example

lim⁑xβ†’01x2=+∞\lim_{x \to 0} \frac{1}{x^2} = +\infty

lim⁑xβ†’βˆž1x2=0\lim_{x \to \infty} \frac{1}{x^2} = 0

Graph feature

Vertical asymptote x=ax = a

Horizontal asymptote y=Ly = L

The two can combine. lim⁑xβ†’βˆžx2=+∞\lim_{x \to \infty} x^2 = +\infty is an infinite limit at infinity, which says the output grows without bound as the input does. The full method for the right-hand column lives in limits at infinity.

What Are The Rules For Infinite Limits?

Infinite limits follow their own arithmetic, and a few combinations have no fixed answer. Suppose lim⁑xβ†’af(x)=+∞\lim_{x \to a} f(x) = +\infty and lim⁑xβ†’ag(x)=L\lim_{x \to a} g(x) = L, where LL is a real number. Then:

  • Sum: lim⁑xβ†’a[f(x)+g(x)]=+∞\lim_{x \to a} \left[f(x) + g(x)\right] = +\infty. A finite amount cannot stop unbounded growth.

  • Product with L>0L > 0: lim⁑xβ†’af(x),g(x)=+∞\lim_{x \to a} f(x),g(x) = +\infty.

  • Product with L<0L < 0: lim⁑xβ†’af(x),g(x)=βˆ’βˆž\lim_{x \to a} f(x),g(x) = -\infty.

  • Quotient: lim⁑xβ†’ag(x)f(x)=0\lim_{x \to a} \frac{g(x)}{f(x)} = 0. A fixed number divided by a growing one shrinks to 0.

Two combinations stay open. When L=0L = 0, the product f(x),g(x)f(x),g(x) has the form 0β‹…βˆž0 \cdot \infty, and when two functions both go to +∞+\infty, their difference has the form βˆžβˆ’βˆž\infty - \infty. Both are indeterminate forms: the answer depends on how fast each part moves, so you have to rewrite the expression before deciding. Example 5 below works one.

Examples Of Infinite Limits

Example 1

Find lim⁑xβ†’3+5xβˆ’3\lim_{x \to 3^{+}} \frac{5}{x - 3} and lim⁑xβ†’3βˆ’5xβˆ’3\lim_{x \to 3^{-}} \frac{5}{x - 3}.

Substituting gives 50\frac{5}{0}, so both limits are infinite. The numerator is positive.

For x>3x > 3, xβˆ’3>0x - 3 > 0:

lim⁑xβ†’3+5xβˆ’3=+∞\lim_{x \to 3^{+}} \frac{5}{x - 3} = +\infty

For x<3x < 3, xβˆ’3<0x - 3 < 0:

lim⁑xβ†’3βˆ’5xβˆ’3=βˆ’βˆž\lim_{x \to 3^{-}} \frac{5}{x - 3} = -\infty

Final answer: +∞+\infty from the right, βˆ’βˆž-\infty from the left. The two-sided limit does not exist, and x=3x = 3 is a vertical asymptote.

Example 2

Find lim⁑xβ†’1xβˆ’4(xβˆ’1)2\lim_{x \to 1} \frac{x - 4}{(x - 1)^2}.

The tempting move is to spot the zero denominator and the even power, remember that 1x2\frac{1}{x^2} goes to +∞+\infty, and stop there:

xβˆ’4(xβˆ’1)2β†’something0+soΒ theΒ answerΒ isΒ +∞?\frac{x - 4}{(x - 1)^2} \to \frac{\text{something}}{0^{+}} \quad \text{so the answer is } +\infty\text{?}

Test a value before trusting that. At x=1.1x = 1.1, the numerator is βˆ’2.9-2.9 and the denominator is 0.010.01, so the quotient is βˆ’290-290. The values are going down, not up. The even power fixed the sign of the denominator, but the numerator was never checked.

The full sign analysis:

lim⁑xβ†’1(xβˆ’4)=βˆ’3(negative)\lim_{x \to 1} (x - 4) = -3 \quad \text{(negative)}

(xβˆ’1)2>0onΒ bothΒ sidesΒ ofΒ 1(x - 1)^2 > 0 \quad \text{on both sides of } 1

negativesmallΒ positiveβ†’βˆ’βˆž\frac{\text{negative}}{\text{small positive}} \to -\infty

Final answer: lim⁑xβ†’1xβˆ’4(xβˆ’1)2=βˆ’βˆž\lim_{x \to 1} \frac{x - 4}{(x - 1)^2} = -\infty, from both sides.

Example 3

For f(x)=x2βˆ’4x2βˆ’xβˆ’2f(x) = \frac{x^2 - 4}{x^2 - x - 2}, find the vertical asymptotes and the one-sided limits there.

Factor both parts:

f(x)=(xβˆ’2)(x+2)(xβˆ’2)(x+1)=x+2x+1,xβ‰ 2f(x) = \frac{(x - 2)(x + 2)}{(x - 2)(x + 1)} = \frac{x + 2}{x + 1}, \quad x \neq 2

The factor (xβˆ’2)(x - 2) cancels, so x=2x = 2 is a hole, with lim⁑xβ†’2f(x)=43\lim_{x \to 2} f(x) = \frac{4}{3}. The remaining zero x=βˆ’1x = -1 gives the asymptote. Near βˆ’1-1 the numerator heads to 11 (positive):

lim⁑xβ†’βˆ’1+x+2x+1=+∞\lim_{x \to -1^{+}} \frac{x + 2}{x + 1} = +\infty

lim⁑xβ†’βˆ’1βˆ’x+2x+1=βˆ’βˆž\lim_{x \to -1^{-}} \frac{x + 2}{x + 1} = -\infty

Final answer: one vertical asymptote, x=βˆ’1x = -1 (+∞+\infty from the right, βˆ’βˆž-\infty from the left), and a hole at (2,43)\left(2, \frac{4}{3}\right).

Example 4

Find lim⁑xβ†’Ο€βˆ’cot⁑x\lim_{x \to \pi^{-}} \cot x and lim⁑xβ†’Ο€+cot⁑x\lim_{x \to \pi^{+}} \cot x.

Write cot⁑x=cos⁑xsin⁑x\cot x = \frac{\cos x}{\sin x}. Near Ο€\pi, cos⁑xβ†’βˆ’1\cos x \to -1 and sin⁑xβ†’0\sin x \to 0.

For xx just below Ο€\pi (second quadrant), sin⁑x>0\sin x > 0:

lim⁑xβ†’Ο€βˆ’cos⁑xsin⁑x=βˆ’10+β†’βˆ’βˆž\lim_{x \to \pi^{-}} \frac{\cos x}{\sin x} = \frac{-1}{0^{+}} \to -\infty

For xx just above Ο€\pi (third quadrant), sin⁑x<0\sin x < 0:

lim⁑xβ†’Ο€+cos⁑xsin⁑x=βˆ’10βˆ’β†’+∞\lim_{x \to \pi^{+}} \frac{\cos x}{\sin x} = \frac{-1}{0^{-}} \to +\infty

Final answer: βˆ’βˆž-\infty from the left and +∞+\infty from the right, so x=Ο€x = \pi is a vertical asymptote of cot⁑x\cot x.

Example 5

Find lim⁑xβ†’0+(1x+ln⁑x)\lim_{x \to 0^{+}} \left(\frac{1}{x} + \ln x\right).

As xβ†’0+x \to 0^{+}, 1xβ†’+∞\frac{1}{x} \to +\infty and ln⁑xβ†’βˆ’βˆž\ln x \to -\infty. That is the indeterminate form βˆžβˆ’βˆž\infty - \infty, so combine into one fraction:

1x+ln⁑x=1+xln⁑xx\frac{1}{x} + \ln x = \frac{1 + x\ln x}{x}

The product xln⁑xx \ln x tends to 0 as xβ†’0+x \to 0^{+} (the factor xx shrinks faster than ln⁑x\ln x grows), so

lim⁑xβ†’0+(1+xln⁑x)=1\lim_{x \to 0^{+}} (1 + x\ln x) = 1

The numerator heads to 1 and the denominator to 0+0^{+}:

lim⁑xβ†’0+1+xln⁑xx=+∞\lim_{x \to 0^{+}} \frac{1 + x\ln x}{x} = +\infty

Final answer: +∞+\infty. The 1x\frac{1}{x} term wins the race.

Example 6

The Lorentz factor is Ξ³(v)=11βˆ’v2/c2\gamma(v) = \frac{1}{\sqrt{1 - v^2/c^2}}. Find lim⁑vβ†’cβˆ’Ξ³(v)\lim_{v \to c^{-}} \gamma(v) and compute Ξ³\gamma at v=0.99cv = 0.99c, 0.999c0.999c and 0.9999c0.9999c.

Write Ξ²=vc\beta = \frac{v}{c}, so Ξ³=11βˆ’Ξ²2\gamma = \frac{1}{\sqrt{1 - \beta^2}}. As Ξ²β†’1βˆ’\beta \to 1^{-}, 1βˆ’Ξ²2β†’0+1 - \beta^2 \to 0^{+}, so its square root heads to 0+0^{+}:

lim⁑β→1βˆ’11βˆ’Ξ²2=+∞\lim_{\beta \to 1^{-}} \frac{1}{\sqrt{1 - \beta^2}} = +\infty

The values show the climb:

Ξ³(0.99c)=11βˆ’0.9801β‰ˆ7.0888\gamma(0.99c) = \frac{1}{\sqrt{1 - 0.9801}} \approx 7.0888

Ξ³(0.999c)β‰ˆ22.3663\gamma(0.999c) \approx 22.3663

Ξ³(0.9999c)β‰ˆ70.7124\gamma(0.9999c) \approx 70.7124

Final answer: lim⁑vβ†’cβˆ’Ξ³(v)=+∞\lim_{v \to c^{-}} \gamma(v) = +\infty. Only the left-hand limit is meaningful, because speeds above cc make the square root undefined.

Why Do Infinite Limits Matter? "No Object With Mass Reaches Light Speed"

Infinite limits matter because they mark the places where a model, a graph or an integral changes character. An infinite limit is a warning sign that a formula has hit a wall. Reading that warning correctly is useful well beyond the limit chapter.

  • Physical limits. The Lorentz factor in Example 6 is why particle accelerators can push particles ever closer to light speed but never to it: the energy needed has an infinite limit as vβ†’cβˆ’v \to c^{-}. OpenStax uses the same relativity formula as a worked example in its limits chapter.

  • Graph sketching. Every vertical asymptote of a graph comes from an infinite limit, so finding them is a standard step in curve sketching. Knowing the sign on each side tells you which way each branch bends.

  • Areas next to an asymptote. An infinite limit does not always mean infinite area. Even though lim⁑xβ†’0+1x=+∞\lim_{x \to 0^{+}} \frac{1}{\sqrt{x}} = +\infty, the area ∫011x,dx\int_{0}^{1} \frac{1}{\sqrt{x}},dx equals 2, while ∫011x,dx\int_{0}^{1} \frac{1}{x},dx diverges. Those questions belong to improper integrals, and every one of them starts by spotting an infinite limit.

  • Where models stop. An inverse-square law such as kr2\frac{k}{r^2} predicts an unbounded value as rβ†’0+r \to 0^{+}. The infinite limit is the formula's way of saying it no longer describes the physics at that scale.

Infinite Limits: Common Confusions Cleared Up

Almost every lost mark on infinite limits comes from either treating ∞\infty like a number or skipping the sign check. These three errors cover most of them.

Mistake 1: Doing Arithmetic With Infinity

Where it slips in:

Sums and differences of two pieces that both blow up, as in Example 5.

Don't do this:

Do not write βˆžβˆ’βˆž=0\infty - \infty = 0 or ∞∞=1\frac{\infty}{\infty} = 1.

The correct way:

Treat βˆžβˆ’βˆž\infty - \infty and ∞∞\frac{\infty}{\infty} as indeterminate forms. Combine into a single fraction, factor, or compare growth rates before deciding.

The memorizer is most exposed here, having learned "anything minus itself is zero" as a reflex. It helps to remember that ∞\infty is shorthand for a process, two processes can run at different speeds, and only the algebra reveals which one wins.

Mistake 2: Skipping The Sign Check

Where it slips in:

Any c0\frac{c}{0} result, especially with an even power in the denominator, as in Example 2.

Don't do this:

Do not answer +∞+\infty just because the denominator heads to 0.

The correct way:

Find the sign of the numerator and the sign of the denominator on each side, then combine them.

The rusher sees the zero denominator, writes +∞+\infty, and moves on. The first instinct on xβˆ’4(xβˆ’1)2\frac{x - 4}{(x - 1)^2} is to think about the squared denominator and forget the numerator entirely, and testing a single value such as x=1.1x = 1.1 catches it in seconds.

Mistake 3: Calling Every Zero Of The Denominator An Asymptote

Where it slips in:

Rational functions with a common factor in the numerator and denominator, as in Example 3.

Don't do this:

Do not list x=2x = 2 as an asymptote of x2βˆ’4x2βˆ’xβˆ’2\frac{x^2 - 4}{x^2 - x - 2} just because the denominator is 0 there.

The correct way:

Factor and cancel first. A cancelled factor gives a hole with a finite limit. Only the surviving zeros give infinite limits.

The second-guesser often gets the factoring right and then doubts it, adding x=2x = 2 back to the asymptote list "to be safe". Checking the limit at the cancelled point, 43\frac{4}{3} here, settles the doubt, because a finite limit cannot sit on an asymptote.

Mistake 2 has an expensive real-world cousin: forgetting what happens when a divisor reaches zero. On 21 September 1997, the US Navy cruiser USS Yorktown lost propulsion after a crew member entered a zero into a database field and the ship's software divided by it. Atlantic Fleet officials said the ship was dead in the water for about 2 hours and 45 minutes.

Practice Problems On Infinite Limits

  1. Find lim⁑xβ†’βˆ’4+3x+4\lim_{x \to -4^{+}} \frac{3}{x + 4} and lim⁑xβ†’βˆ’4βˆ’3x+4\lim_{x \to -4^{-}} \frac{3}{x + 4}.

  2. Find lim⁑xβ†’2x+1(xβˆ’2)2\lim_{x \to 2} \frac{x + 1}{(x - 2)^2}.

  3. For h(x)=x2βˆ’9x2βˆ’2xβˆ’3h(x) = \frac{x^2 - 9}{x^2 - 2x - 3}, find every vertical asymptote and every hole, with the one-sided limits at each asymptote.

  4. Find lim⁑xβ†’(Ο€/2)βˆ’sec⁑x\lim_{x \to (\pi/2)^{-}} \sec x and lim⁑xβ†’(Ο€/2)+sec⁑x\lim_{x \to (\pi/2)^{+}} \sec x.

  5. Find lim⁑xβ†’0+e1/x\lim_{x \to 0^{+}} e^{1/x} and lim⁑xβ†’0βˆ’e1/x\lim_{x \to 0^{-}} e^{1/x}. Is x=0x = 0 a vertical asymptote?

Answer to Question 1: +∞+\infty from the right and βˆ’βˆž-\infty from the left.

Answer to Question 2: +∞+\infty, since the numerator heads to 3 and the denominator is positive on both sides.

Answer to Question 3: h(x)=(xβˆ’3)(x+3)(xβˆ’3)(x+1)h(x) = \frac{(x - 3)(x + 3)}{(x - 3)(x + 1)}, so there is a hole at (3,32)\left(3, \frac{3}{2}\right) and an asymptote at x=βˆ’1x = -1, with +∞+\infty from the right and βˆ’βˆž-\infty from the left.

Answer to Question 4: +∞+\infty from the left and βˆ’βˆž-\infty from the right.

Answer to Question 5: +∞+\infty from the right and 0 from the left. Yes, x=0x = 0 is a vertical asymptote, because one infinite one-sided limit is enough.

What To Remember About Infinite Limits

  • Infinite limits describe outputs that grow without bound, positively or negatively, as xx approaches a finite number aa.

  • Writing ±∞\pm\infty describes how the limit fails to exist and is not a real-number value.

  • A c0\frac{c}{0} form with cβ‰ 0c \neq 0 signals an infinite limit, and the signs of the numerator and denominator on each side decide +∞+\infty or βˆ’βˆž-\infty.

  • Every infinite one-sided limit gives a vertical asymptote, while a cancelled factor gives a hole instead.

  • Infinite limits send xx to a number, while limits at infinity send xx to infinity.

Where To Go From Here

Work through practice problems 1 to 5; if Question 3 trips you up, return to the section on vertical asymptotes and redo Example 3.

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Frequently Asked Questions

An infinite limit exists or doesn't exist?
It does not exist as a real number, in standard calculus. Writing +∞+\infty or βˆ’βˆž-\infty is a precise way of saying how it fails to exist, and only courses that work on the extended real line count it as existing.
Can the value of a limit be infinity?
No, not as a real-number value. We still write lim⁑xβ†’af(x)=+∞\lim_{x \to a} f(x) = +\infty when the values grow without bound, because that tells the reader much more than "does not exist" alone.
Is the limit of 1/x^2 as x approaches 0 unbounded or infinity?
Both words describe the same behaviour. The values of 1x2\frac{1}{x^2} are unbounded above near 0, and the standard notation for that is lim⁑xβ†’01x2=+∞\lim_{x \to 0} \frac{1}{x^2} = +\infty.
Does the limit as x approaches 0 of the function 1/(x)^2 exist? Both the left and right hand limits approach infinity.
Both one-sided limits are +∞+\infty, so the two-sided infinite limit lim⁑xβ†’01x2=+∞\lim_{x \to 0} \frac{1}{x^2} = +\infty holds. As a real number, though, the limit does not exist. This is the even-power case covered above.
Undefined or infinity as the answer: which do you write for infinite limits?
Use "undefined" for the function value at the point and ±∞\pm\infty for the limit. For 1x2\frac{1}{x^2}, f(0)f(0) is undefined while the limit is +∞+\infty.
How can limits at infinity fail to exist, and how is that different from infinite limits?
A limit at infinity fails when the output keeps oscillating, as sin⁑x\sin x does as xβ†’βˆžx \to \infty, or when it grows without bound, as x2x^2 does. Infinite limits are a different question: the input approaches a finite number aa and the output blows up, which produces a vertical asymptote rather than a horizontal one.
✍️ Written By
Madhukar V
Madhukar V
Math Columnist & Analyst
I see mathematics as more than just numbers and formulasβ€”it is a way of thinking, questioning, and understanding the world around us. I work at the intersection of mathematics, EdTech, technology, and AI-powered learning, I enjoy exploring how mathematical ideas can be made simple, meaningful, and relatable. Through my articles, I aim to present mathematics with curiosity and a practical perspective, helping readers see the beauty and relevance behind every concept in a Bhanzu way.
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