Infinite Limits and Limits at Infinity

What does it mean to say that 1/x21/x^2 "goes to infinity" as xx approaches 00? What does it mean that 1/x1/x "goes to zero" as xx grows without bound? These phrases feel intuitive. Yet infinity is not a real number. So the ordinary The Epsilon-Delta Definition of a Limit cannot literally apply. That definition promises f(x)f(x) gets arbitrarily close to some finite value LL. The task of this article is to repair that gap. We will build precise, quantifier-driven definitions. These definitions capture "blows up" and "tends to infinity" exactly. They use the same logical architecture as the finite epsilon-delta definition. Infinity simply plays the role once held by LL or by a finite input value aa. This matters because calculus is full of behavior naturally described using infinity. Examples include vertical asymptotes of rational functions, the growth of ln⁡x\ln x as x→∞x\to\infty, the decay of e−xe^{-x}, and the long-run behavior of sequences and series. Without a rigorous vocabulary, statements like "f(x)→∞f(x)\to\infty" remain metaphors. With one, they become theorems with proofs. They become amenable to the same algebra of limits (sums, products, composition) that ordinary finite limits obey. This holds once the right adjustments are made, since ∞\infty cannot be added, multiplied, or canceled like a number. The big picture is that there are really four flavors of "limit involving infinity." They combine two independent choices. First, whether the input variable tends to a finite point or to ±∞\pm\infty. Second, whether the output value tends to a finite number or diverges to ±∞\pm\infty. Ordinary limits fix both choices to "finite." This article completes the picture by handling the remaining three combinations. These are infinite limits at a finite point, finite limits at infinity, and infinite limits at infinity. All are handled via analogous ε\varepsilon–δ\delta, ε\varepsilon–MM, NN–δ\delta, and NN–MM definitions. By the end, you will have exact definitions for each of these four cases. You will also have a unified theorem describing how algebraic combinations of such limits behave. This includes the classic exceptions like ∞−∞\infty - \infty. There are fully worked examples with asymptotic and growth-rate computations. Finally, a counterexample shows why the boundedness/monotonicity-type hypotheses cannot be dropped. This applies specifically to the algebra-of-limits theorem. This sets the stage for the Classification of Discontinuities, where infinite limits identify a specific type of discontinuity.

Key takeaways
  • "lim⁡x→af(x)=∞\lim_{x\to a} f(x) = \infty" means f(x)f(x) can be forced above any bound MM by taking xx close enough to aa — made precise with an ε\varepsilon-free, δ\delta-MM definition.
  • "lim⁡x→∞f(x)=L\lim_{x\to\infty} f(x) = L" means f(x)f(x) can be forced within ε\varepsilon of LL by taking xx larger than some threshold NN — an NN-ε\varepsilon definition.
  • "lim⁡x→∞f(x)=∞\lim_{x\to\infty} f(x) = \infty" combines both ideas into an NN-MM definition with no finite target on either side.
  • These are not limits in the sense of the original epsilon-delta definition (infinity is not a real number); they are separate, formally analogous definitions with their own algebra.
  • The algebra of infinite/at-infinity limits mirrors the finite algebra of limits, but forms like ∞−∞\infty - \infty, 0⋅∞0\cdot\infty, ∞/∞\infty/\infty are genuinely indeterminate and require separate analysis (e.g. L'Hôpital's rule, algebraic manipulation).
  • Vertical and horizontal asymptotes of a function's graph are exactly the geometric shadows of infinite limits and limits at infinity, respectively.
  • Key idea: replace "close to a finite target" with "eventually beyond any bound," using the same quantifier structure (∀\forall tolerance ∃\exists threshold) as the ordinary limit definition.

Where this lives today

Infinite limits and limits at infinity are the backbone of asymptotic analysis: determining the long-run behavior of algorithms (Big-OO notation in computer science is literally a statement about lim⁡n→∞\lim_{n\to\infty} ratios and bounds), the decay of probability tails in statistics (e.g. showing a density →0\to 0 as x→±∞x\to\pm\infty so that it can integrate to 11), and the classification of singularities in complex analysis, where poles are precisely points at which ∣f(z)∣→∞|f(z)|\to\infty. In physics, limits at infinity describe boundary conditions at spatial infinity (e.g. potentials vanishing far from a charge), while infinite limits capture divergences that signal a breakdown of a model (e.g. an electric field blowing up at a point charge's location). In cryptography and complexity theory, statements like "the running time grows as Θ(nlog⁡n)\Theta(n\log n)" are limits-at-infinity statements dressed in different notation. Finally, this material directly feeds the Classification of Discontinuities: a function has an infinite discontinuity exactly when one of its one-sided limits at a point is +∞+\infty or −∞-\infty, distinguishing this case sharply from removable and jump discontinuities.

Ask the tutor: Can you walk through how to determine, using only the MM-δ\delta definition, whether lim⁡x→32(x−3)3\lim_{x\to 3} \frac{2}{(x-3)^3} is +∞+\infty, −∞-\infty, or does not exist as an infinite limit at all?

DefinitionInfinite limits and limits at infinity

Let ff be a real-valued function.

(1) Infinite limit at a point. Suppose ff is defined on some set containing a punctured neighborhood of a∈Ra\in\mathbb R (i.e. (a−r,a)∪(a,a+r)⊆dom⁡f(a-r,a)\cup(a,a+r)\subseteq \operatorname{dom} f for some r>0r>0). We say

lim⁡x→af(x)=∞\lim_{x\to a} f(x) = \infty

if for every M∈RM\in\mathbb R there exists δ>0\delta>0 such that

0<∣x−a∣<δ  ⟹  f(x)>M.0<|x-a|<\delta \implies f(x) > M.

Similarly, lim⁡x→af(x)=−∞\lim_{x\to a} f(x) = -\infty if for every M∈RM\in\mathbb R there is δ>0\delta>0 with 0<∣x−a∣<δ  ⟹  f(x)<M0<|x-a|<\delta \implies f(x)<M. One-sided versions (x→a+x\to a^+, x→a−x\to a^-) are defined by restricting to a<x<a+δa<x<a+\delta or a−δ<x<aa-\delta<x<a respectively, exactly as in One-Sided Limits.

(2) Finite limit at infinity. Suppose ff is defined on (c,∞)(c,\infty) for some c∈Rc\in\mathbb R. We say

lim⁡x→∞f(x)=L\lim_{x\to\infty} f(x) = L

if for every ε>0\varepsilon>0 there exists N∈RN\in\mathbb R (equivalently N>cN>c) such that

x>N  ⟹  ∣f(x)−L∣<ε.x>N \implies |f(x)-L|<\varepsilon.

The definition of lim⁡x→−∞f(x)=L\lim_{x\to-\infty} f(x)=L is analogous, with ff defined on (−∞,c)(-\infty,c) and the conclusion x<N  ⟹  ∣f(x)−L∣<εx<N \implies |f(x)-L|<\varepsilon.

(3) Infinite limit at infinity. Suppose ff is defined on (c,∞)(c,\infty). We say

lim⁡x→∞f(x)=∞\lim_{x\to\infty} f(x) = \infty

if for every M∈RM\in\mathbb R there exists N∈RN\in\mathbb R such that

x>N  ⟹  f(x)>M.x>N \implies f(x) > M.

The three remaining sign combinations (x→∞, f→−∞x\to\infty,\, f\to-\infty; x→−∞, f→∞x\to-\infty,\, f\to\infty; x→−∞, f→−∞x\to-\infty,\, f\to-\infty) are defined by the evident analogous modifications. In all cases, ∞\infty and −∞-\infty are not real numbers; these are separate definitions, not special cases of the finite ε\varepsilon-δ\delta limit. A limit (in the original finite sense) is said to exist only when case fits the classical definition with a real number LL; when f(x)→±∞f(x)\to\pm\infty, we say the limit diverges to infinity, a distinct and weaker piece of information than "the limit exists."

Intuition

Look again at the classical definition: for every tolerance ε>0\varepsilon>0 around the target LL, there is a window of radius δ\delta around the input aa that lands inside the tolerance. Each of the new definitions is obtained by replacing one or both "closeness" requirements with an "eventually beyond a bound" requirement. If the target is infinite, "∣f(x)−L∣<ε|f(x)-L|<\varepsilon" is replaced by "f(x)>Mf(x)>M" — there is no finite target to be close to, only a bound to exceed, and MM can be taken arbitrarily large. If the input tends to infinity, "0<∣x−a∣<δ0<|x-a|<\delta" is replaced by "x>Nx>N" — there is no finite point to approach, only a threshold to exceed. This uniformity is the entire content of the topic: once you see that MM plays the role ε\varepsilon used to play (a challenge to be met) and NN plays the role δ\delta used to play (a response that meets it), all four definitions are the same skeleton with different flesh. The direction of the inequality with MM (whether f(x)>Mf(x)>M or f(x)<Mf(x)<M) encodes +∞+\infty versus −∞-\infty; whether the domain condition is 0<∣x−a∣<δ0<|x-a|<\delta or x>Nx>N (or x<Nx<N) encodes whether the input approaches a finite point or ±∞\pm\infty. Geometrically, an infinite limit at aa produces a vertical asymptote at x=ax=a: the graph shoots up or down without bound as x→ax\to a. A finite limit at infinity produces a horizontal asymptote at height LL: the graph flattens out approaching the line y=Ly=L. An infinite limit at infinity means the graph keeps climbing (or falling) forever, without leveling off — no horizontal asymptote, but a definite long-run trend.

Figure
Two asymptotic behaviors of f(x)=1x−2+1f(x)=\dfrac{1}{x-2}+1: vertical asymptote at x=2x=2 from an infinite limit, horizontal asymptote at y=1y=1 from a limit at infinity
x y x = 2 y = 1 as x→2⁻, f(x)→ −∞ as x→2⁺, f(x)→ +∞ as x→∞, f(x)→1 f(x) = 1/(x−2) + 1
TheoremAlgebra of infinite limits and limits at infinity

Let f,gf,g be functions defined on a punctured neighborhood of a∈R∪{±∞}a\in\mathbb R\cup\{\pm\infty\} (interpreting "neighborhood of ∞\infty" as (c,∞)(c,\infty) and similarly for −∞-\infty), and suppose the relevant limits below exist in the extended sense of the Definition of Infinite limits and limits at infinity. Fix a real constant c∈Rc\in\mathbb R.

(a) Sum with a finite limit. If lim⁡x→af(x)=∞\lim_{x\to a} f(x) = \infty and lim⁡x→ag(x)=L∈R\lim_{x\to a} g(x) = L\in\mathbb R (an ordinary finite limit), then

lim⁡x→a(f(x)+g(x))=∞.\lim_{x\to a} \big(f(x)+g(x)\big) = \infty.

(b) Product with a positive finite limit. If lim⁡x→af(x)=∞\lim_{x\to a} f(x) = \infty and lim⁡x→ag(x)=L∈R\lim_{x\to a} g(x) = L\in\mathbb R with L>0L>0, then

lim⁡x→a(f(x)g(x))=∞.\lim_{x\to a} \big(f(x)g(x)\big) = \infty.

(If L<0L<0 the limit is −∞-\infty; if L=0L = 0 the product may fail to have any limit, finite or infinite — see the counterexample below.)

(c) Reciprocal. If lim⁡x→af(x)=∞\lim_{x\to a} f(x) = \infty, then f(x)≠0f(x)\neq 0 for xx near aa (excluding aa), and

lim⁡x→a1f(x)=0.\lim_{x\to a} \frac{1}{f(x)} = 0.

Conversely, if lim⁡x→af(x)=0\lim_{x\to a} f(x) = 0 and f(x)>0f(x)>0 for all xx in some punctured neighborhood of aa, then lim⁡x→a1/f(x)=∞\lim_{x\to a} 1/f(x) = \infty.

(d) No general sum/product rule when both diverge. If lim⁡x→af(x)=∞\lim_{x\to a} f(x) = \infty and lim⁡x→ag(x)=∞\lim_{x\to a} g(x) = \infty, then lim⁡x→a(f(x)+g(x))=∞\lim_{x\to a}(f(x)+g(x)) = \infty; but lim⁡x→a(f(x)−g(x))\lim_{x\to a}(f(x)-g(x)) and lim⁡x→af(x)/g(x)\lim_{x\to a} f(x)/g(x) need not exist in any sense (finite or infinite), and no universal formula computes them from the two individual limits alone. All statements (a)–(c) hold equally, with identical proofs after replacing "0<∣x−a∣<δ0<|x-a|<\delta" by "x>Nx>N" (or "x<Nx<N"), for limits as x→∞x\to \infty or x→−∞x\to-\infty.

Proof

We prove (a), (b), (c) for the case x→ax\to a, a∈Ra\in\mathbb R; the x→±∞x\to\pm\infty cases follow by the indicated substitution and are otherwise word-for-word identical, so we do not repeat them. Throughout, the technique is direct verification from the ε/M\varepsilon/M–δ\delta definitions: given a challenge, we exhibit a response and check it works.

(a) Let M∈RM\in\mathbb R be given; we must produce δ>0\delta>0 such that 0<∣x−a∣<δ  ⟹  f(x)+g(x)>M0<|x-a|<\delta \implies f(x)+g(x) > M. Since lim⁡x→ag(x)=L\lim_{x\to a} g(x) = L, apply the ordinary ε\varepsilon-δ\delta definition with ε=1\varepsilon = 1: there is δ1>0\delta_1>0 such that 0<∣x−a∣<δ1  ⟹  ∣g(x)−L∣<10<|x-a|<\delta_1 \implies |g(x)-L|<1, hence g(x)>L−1g(x) > L-1. Since lim⁡x→af(x)=∞\lim_{x\to a} f(x) = \infty, apply the definition with challenge M′:=M−L+1M' := M - L + 1: there is δ2>0\delta_2>0 such that 0<∣x−a∣<δ2  ⟹  f(x)>M−L+10<|x-a|<\delta_2 \implies f(x) > M-L+1. Let δ=min⁡(δ1,δ2)>0\delta = \min(\delta_1,\delta_2) > 0. If 0<∣x−a∣<δ0<|x-a|<\delta, both conditions hold, so

f(x)+g(x)>(M−L+1)+(L−1)=M.f(x)+g(x) > (M-L+1) + (L-1) = M.

Since MM was arbitrary, lim⁡x→a(f(x)+g(x))=∞\lim_{x\to a}(f(x)+g(x))=\infty. ■\blacksquare (for part a)

(b) Assume L>0L>0. Let M∈RM\in\mathbb R be given; we must find δ>0\delta>0 forcing f(x)g(x)>Mf(x)g(x)>M on 0<∣x−a∣<δ0<|x-a|<\delta. Apply the definition of lim⁡g=L\lim g = L with ε=L/2>0\varepsilon = L/2>0: there is δ1>0\delta_1>0 such that 0<∣x−a∣<δ1  ⟹  ∣g(x)−L∣<L/20<|x-a|<\delta_1 \implies |g(x)-L|<L/2, hence

g(x)>L−L/2=L/2>0.g(x) > L - L/2 = L/2 > 0.

Case M≤0M \le 0: since g(x)>0g(x)>0 and, applying lim⁡f=∞\lim f=\infty with challenge M′=1M'=1, there is δ2\delta_2 with f(x)>1>0f(x)>1>0 on 0<∣x−a∣<δ20<|x-a|<\delta_2; on δ=min⁡(δ1,δ2)\delta=\min(\delta_1,\delta_2) we get f(x)g(x)>1⋅(L/2)>0≥Mf(x)g(x) > 1\cdot (L/2) > 0 \ge M, done. (This handles small/negative MM where the bound L/2L/2 alone already suffices once f>0f>0; we fold it into the general case below for uniformity.) General case: apply the definition of lim⁡f=∞\lim f=\infty with challenge M′:=2(∣M∣+1)L>0M' := \dfrac{2(|M|+1)}{L}>0 (this is a valid positive real challenge since L>0L>0): there is δ2>0\delta_2>0 such that 0<∣x−a∣<δ2  ⟹  f(x)>2(∣M∣+1)L0<|x-a|<\delta_2 \implies f(x) > \dfrac{2(|M|+1)}{L}. Let δ=min⁡(δ1,δ2)\delta=\min(\delta_1,\delta_2). For 0<∣x−a∣<δ0<|x-a|<\delta, using g(x)>L/2>0g(x)>L/2>0 and f(x)>0f(x)>0 (since f(x)>M′>0f(x) > M' > 0), multiply the two positive inequalities:

f(x)g(x)>2(∣M∣+1)L⋅L2=∣M∣+1>M.f(x)g(x) > \frac{2(|M|+1)}{L}\cdot \frac{L}{2} = |M|+1 > M.

As MM was arbitrary, lim⁡x→af(x)g(x)=∞\lim_{x\to a} f(x)g(x) = \infty. The case L<0L<0 reduces to this one by writing f⋅g=−(f⋅(−g))f\cdot g = -(f\cdot(-g)) and noting lim⁡(−g)=−L>0\lim(-g)=-L>0, then using part (b) already proved together with the evident fact that lim⁡h=∞  ⟹  lim⁡(−h)=−∞\lim h = \infty \implies \lim(-h) = -\infty (immediate from the definitions: h(x)>M  ⟺  −h(x)<−Mh(x)>M \iff -h(x) < -M, and MM ranges over all reals iff −M-M does).

(c) Suppose lim⁡x→af(x)=∞\lim_{x\to a} f(x)=\infty. Applying the definition with M=1M=1 gives δ0>0\delta_0>0 with 0<∣x−a∣<δ0  ⟹  f(x)>1>00<|x-a|<\delta_0 \implies f(x)>1>0; in particular f(x)≠0f(x)\neq 0 on this punctured neighborhood, so 1/f(x)1/f(x) is well-defined there. Now let ε>0\varepsilon>0 be given; we must find δ>0\delta>0 such that 0<∣x−a∣<δ  ⟹  ∣1/f(x)−0∣<ε0<|x-a|<\delta \implies |1/f(x) - 0| < \varepsilon, i.e. 1/f(x)<ε1/f(x) < \varepsilon (using f(x)>0f(x)>0 from above, so 1/f(x)>01/f(x)>0 automatically once xx is in that neighborhood). Apply the definition of lim⁡f=∞\lim f=\infty with challenge M=1/εM = 1/\varepsilon: there is δ1>0\delta_1>0 with 0<∣x−a∣<δ1  ⟹  f(x)>1/ε0<|x-a|<\delta_1 \implies f(x) > 1/\varepsilon. Let δ=min⁡(δ0,δ1)\delta = \min(\delta_0,\delta_1). For 0<∣x−a∣<δ0<|x-a|<\delta: f(x)>1/ε>0f(x) > 1/\varepsilon > 0, so taking reciprocals of positive numbers (an order-reversing, well-defined operation for positive reals) gives 0<1/f(x)<ε0 < 1/f(x) < \varepsilon, i.e. ∣1/f(x)−0∣<ε|1/f(x)-0|<\varepsilon. Hence lim⁡x→a1/f(x)=0\lim_{x\to a} 1/f(x) = 0. For the converse: suppose lim⁡x→af(x)=0\lim_{x\to a} f(x) = 0 and f(x)>0f(x) > 0 on a punctured neighborhood (a−r,a)∪(a,a+r)(a-r,a)\cup(a,a+r). Let M∈RM\in\mathbb R be given. If M≤0M\le 0, then since 1/f(x)>01/f(x)>0 always (as f(x)>0f(x)>0), any δ≤r\delta \le r works trivially: 1/f(x)>0≥M1/f(x) > 0 \ge M. If M>0M>0, apply the definition of lim⁡f=0\lim f = 0 with ε=1/M>0\varepsilon = 1/M>0: there is δ1≤r\delta_1 \le r such that 0<∣x−a∣<δ1  ⟹  ∣f(x)−0∣<1/M0<|x-a|<\delta_1 \implies |f(x)-0|<1/M, i.e. (since f(x)>0f(x)>0) 0<f(x)<1/M0<f(x)<1/M. Taking reciprocals of positive quantities reverses the inequality: 1/f(x)>M1/f(x) > M. Setting δ=δ1\delta=\delta_1 establishes lim⁡x→a1/f(x)=∞\lim_{x\to a} 1/f(x)=\infty.

(d) The sum case: given MM, use lim⁡f=∞\lim f=\infty with challenge M−0M-0... more carefully, this is exactly part (a)'s argument with the roles symmetrized (or apply (a) is not literally applicable since g→∞g\to\infty is not finite, so we argue directly): given MM, apply lim⁡f=∞\lim f=\infty with challenge M/2M/2 to get δ1\delta_1 with f(x)>M/2f(x)>M/2 on 0<∣x−a∣<δ10<|x-a|<\delta_1, and apply lim⁡g=∞\lim g=\infty with challenge M/2M/2 to get δ2\delta_2 with g(x)>M/2g(x)>M/2 there; on δ=min⁡(δ1,δ2)\delta=\min(\delta_1,\delta_2), f(x)+g(x)>Mf(x)+g(x) > M. This proves the sum claim. The impossibility of a universal rule for f−gf-g or f/gf/g is established by the counterexample below, which exhibits two specific functions f,gf,g with lim⁡f=lim⁡g=∞\lim f=\lim g=\infty at a point aa, for which f−gf-g and f/gf/g have different limiting behaviors than another pair f′,g′f',g' with the same individual limits — showing no formula in terms of "∞\infty and ∞\infty" alone can determine the answer. ■\blacksquare

∎

Worked examples

Example 1 (an infinite limit at a finite point, verified directly from the definition). Let f(x)=3(x−1)2f(x) = \dfrac{3}{(x-1)^2}. Claim: lim⁡x→1f(x)=∞\displaystyle\lim_{x\to 1} f(x) = \infty. Proof from the definition. Let M∈RM\in\mathbb R be given. We must find δ>0\delta>0 such that 0<∣x−1∣<δ  ⟹  3(x−1)2>M0<|x-1|<\delta \implies \dfrac{3}{(x-1)^2} > M. If M≤0M\le 0, any δ>0\delta>0 works since 3(x−1)2>0≥M\dfrac{3}{(x-1)^2}>0\ge M automatically for x≠1x\ne 1. So assume M>0M>0. We want

3(x−1)2>M  ⟺  (x−1)2<3M  ⟺  ∣x−1∣<3M.\frac{3}{(x-1)^2} > M \iff (x-1)^2 < \frac{3}{M} \iff |x-1| < \sqrt{\frac{3}{M}}.

So choose δ=3/M\delta = \sqrt{3/M}. Then for 0<∣x−1∣<δ0<|x-1|<\delta, reversing the (valid, since both sides are positive) chain of equivalences above gives f(x)>Mf(x) > M. Since MM was arbitrary, lim⁡x→1f(x)=∞\lim_{x\to1} f(x)=\infty, confirmed directly, not just by "plugging in." Numerically: to force f(x)>10,000f(x) > 10{,}000, we need δ=3/10000=0.0003≈0.01732\delta = \sqrt{3/10000} = \sqrt{0.0003}\approx 0.01732; indeed at x=1.01x=1.01, f(1.01)=3/(0.01)2=30,000>10,000f(1.01) = 3/(0.01)^2 = 30{,}000 > 10{,}000. ✓.

Example 2 (a finite limit at infinity and an infinite limit at infinity, combined via the algebra theorem). Let

g(x)=7x2−2x+52x2+3,h(x)=x3−100x.g(x) = \frac{7x^2 - 2x + 5}{2x^2 + 3}, \qquad h(x) = x^3 - 100x.

We compute lim⁡x→∞g(x)\lim_{x\to\infty} g(x) and lim⁡x→∞h(x)\lim_{x\to\infty} h(x), then combine them via part (a) of the Theorem: Algebra of infinite limits and limits at infinity. Step 1: lim⁡x→∞g(x)\lim_{x\to\infty} g(x). Divide numerator and denominator by x2x^2 (valid for x≠0x\ne 0):

g(x)=7−2/x+5/x22+3/x2.g(x) = \frac{7 - 2/x + 5/x^2}{2+3/x^2}.

We use (without reproof, as it is the elementary case L=0L=0 analog of part (c) applied to f(x)=xf(x)=x, or direct verification): lim⁡x→∞1/x=0\lim_{x\to\infty} 1/x = 0 and lim⁡x→∞1/x2=0\lim_{x\to\infty} 1/x^2=0. Both follow directly from the NN–ε\varepsilon definition: given ε>0\varepsilon>0, take N=1/εN=1/\varepsilon; then x>N  ⟹  0<1/x<εx>N \implies 0<1/x<\varepsilon, and similarly x>N=max⁡(1,1/ε)  ⟹  1/x2<εx>N=\max(1,1/\sqrt\varepsilon)\implies 1/x^2<\varepsilon. By the ordinary (finite) algebra of limits — sums and quotients of finite limits, applicable here since all four numerator/denominator pieces have finite limits and the denominator's limit 2≠02\neq 0 — we get

lim⁡x→∞g(x)=7−0+02+0=72.\lim_{x\to\infty} g(x) = \frac{7-0+0}{2+0} = \frac{7}{2}.

So gg has a horizontal asymptote y=7/2y=7/2 as x→∞x\to\infty. Let's double check numerically: g(1000)=7,000,000−2000+52,000,000+3=6,998,0052,000,003≈3.49900g(1000) = \frac{7,000,000 - 2000+5}{2,000,000+3} = \frac{6{,}998{,}005}{2{,}000{,}003} \approx 3.49900, close to 3.53.5. ✓ Step 2: lim⁡x→∞h(x)=∞\lim_{x\to\infty} h(x) = \infty. Write h(x)=x3(1−100/x2)h(x) = x^3(1 - 100/x^2). Given M∈RM\in\mathbb R, first note 1−100/x2→11-100/x^2 \to 1 as x→∞x\to\infty (again by the 1/x2→01/x^2\to0 fact above and finite-limit algebra), so there is N1N_1 with x>N1  ⟹  1−100/x2>1/2x>N_1 \implies 1-100/x^2 > 1/2. Also x3→∞x^3 \to \infty (direct: given any bound M′M', take N=max⁡(1,M′1/3)N=\max(1,M'^{1/3}); then x>N  ⟹  x3>M′x>N\implies x^3>M'). By part (b) of the theorem (product of an infinite limit with a finite positive limit 1/21/2... more precisely we apply it with the roles f(x)=x3→∞f(x)=x^3\to\infty, g(x)=1−100/x2→1>0g(x) = 1-100/x^2 \to 1 > 0), lim⁡x→∞h(x)=∞\lim_{x\to\infty} h(x) = \infty. Numerically: h(20)=8000−2000=6000h(20) = 8000 - 2000 = 6000; h(100)=1,000,000−10,000=990,000h(100)=1{,}000{,}000-10{,}000 = 990{,}000, confirming rapid, unbounded growth despite the "−100x-100x" correction term. ✓ Step 3: combine via part (a). Consider k(x)=h(x)+g(x)=x3−100x+7x2−2x+52x2+3k(x) = h(x) + g(x) = x^3-100x + \dfrac{7x^2-2x+5}{2x^2+3}. Since lim⁡h=∞\lim h=\infty and lim⁡g=7/2\lim g = 7/2 (finite), part (a) of the theorem gives immediately, with no further computation,

lim⁡x→∞k(x)=∞.\lim_{x\to\infty} k(x) = \infty.

This illustrates the payoff of the algebra theorem: once the two pieces' limits are known, the combination's limit requires no new ε\varepsilon-MM-NN argument.

Counterexamplewhy the "L>0L>0 finite" hypothesis in part (b), and the restriction to sums (not differences) of two infinite limits in part (d), cannot be dropped

Dropping "LL finite, nonzero" in the product rule. Consider x→0x\to 0, with

f(x)=1x2(→∞),g1(x)=x2(→0),g2(x)=x(→0).f(x) = \frac{1}{x^2} \quad(\to \infty), \qquad g_1(x) = x^2 \quad (\to 0),\qquad g_2(x) = x \quad(\to 0).

Both g1,g2→0g_1,g_2\to 0 as x→0x\to 0, matching the excluded case "L=0L=0" in part (b). But

f(x)g1(x)=x2x2=1 →x→0 1,f(x)g_1(x) = \frac{x^2}{x^2} = 1 \ \xrightarrow[x\to0]{}\ 1,

a finite, nonzero limit, while

f(x)g2(x)=xx2=1x,f(x)g_2(x) = \frac{x}{x^2} = \frac{1}{x},

which has no limit at all, finite or infinite, at x=0x=0 (its one-sided limits are +∞+\infty and −∞-\infty, disagreeing). So with lim⁡f=∞\lim f = \infty and lim⁡g=0\lim g = 0 held fixed, the product's behavior ranges over "finite limit 11", and "no limit exists" — genuinely indeterminate, exactly the phenomenon flagged as "∞⋅0\infty\cdot 0" in elementary calculus. This shows the hypothesis L≠0L\neq 0 (indeed L>0L>0 or L<0L<0, with LL a fixed finite nonzero real) is essential to part (b); no universal conclusion is possible when L=0L=0.

Dropping "sum" in favor of "difference" or "quotient" in part (d). Let a=0a=0 and take two pairs of functions, both satisfying lim⁡x→0f=∞\lim_{x\to0} f=\infty, lim⁡x→0g=∞\lim_{x\to0} g=\infty:

Pair A: fA(x)=2x2, gA(x)=1x2Pair B: fB(x)=1x2+1x4, gB(x)=1x4.\text{Pair A: } f_A(x)=\frac{2}{x^2},\ g_A(x)=\frac{1}{x^2} \qquad\text{Pair B: } f_B(x)=\frac{1}{x^2}+\frac1{x^4},\ g_B(x)=\frac{1}{x^4}.

For pair A: fA(x)−gA(x)=1x2→∞f_A(x)-g_A(x) = \dfrac{1}{x^2}\to \infty, and fA(x)/gA(x)=2→2f_A(x)/g_A(x) = 2 \to 2 (finite!). For pair B: fB(x)−gB(x)=1x2→∞f_B(x)-g_B(x) = \dfrac{1}{x^2}\to\infty as well, but fB(x)/gB(x)=x2+11⋅1x2⋅x2f_B(x)/g_B(x) = \dfrac{x^2+1}{1}\cdot\frac{1}{x^2}\cdot x^2... let us recompute directly: fB(x)/gB(x)=1/x2+1/x41/x4=x2+1→∞f_B(x)/g_B(x) = \dfrac{1/x^2+1/x^4}{1/x^4} = x^2+1 \to \infty as x→0x\to 0? Wait — check as x→0x\to 0: x2+1→1x^2+1\to 1. So fB/gB→1f_B/g_B \to 1 (finite, different value than pair A's 22). Both pairs have lim⁡f=lim⁡g=∞\lim f=\lim g=\infty, yet the quotients tend to different finite limits (22 versus 11) — and one can similarly rig examples where the quotient has no limit at all (e.g. oscillating ratio), or diverges to ∞\infty. This proves no formula depending only on "lim⁡f=∞\lim f=\infty, lim⁡g=∞\lim g=\infty" can determine lim⁡(f/g)\lim(f/g) or, by similar constructions, lim⁡(f−g)\lim(f-g): these are the indeterminate forms "∞/∞\infty/\infty" and "∞−∞\infty-\infty." The hypothesis in part (a)/(d) that one of the two functions has a finite limit (for the sum rule) is what made the earlier proof go through; once both diverge, the cancellation in the proof of part (a) (bounding gg below by L−1L-1) is no longer available, since there is no finite LL.

Scope, edge cases & common traps

SituationCorrect statementCommon trap
lim⁡x→af(x)=∞\lim_{x\to a} f(x) = \inftyff diverges to infinity; the limit does not exist as a real numberSaying "the limit exists and equals infinity" — infinity is not a value the limit takes in the classical sense
lim⁡x→∞f(x)=L\lim_{x\to\infty} f(x) = LA genuine, finite limit; horizontal asymptote y=Ly=LConfusing this with lim⁡x→af(x)=L\lim_{x\to a} f(x)=L for finite aa; the threshold is NN, not δ\delta
One-sided infinite limits, e.g. lim⁡x→a+f=∞\lim_{x\to a^+} f=\infty, lim⁡x→a−f=−∞\lim_{x\to a^-}f=-\inftyTwo-sided limit does not exist (in any sense) even though each one-sided limit "exists" as an infinite limitAveraging or otherwise combining +∞+\infty and −∞-\infty into a single verdict
f(x)→∞f(x)\to \infty and g(x)→∞g(x)\to \inftyf+g→∞f+g\to\infty always; f−gf-g, f/gf/g indeterminateAssuming symmetric treatment of +,−,×,÷+,-,\times,\div once both diverge
Vertical asymptote at x=ax=aRequires some one-sided (or two-sided) limit to be ±∞\pm\infty at aaAssuming every point where ff is undefined gives a vertical asymptote (removable discontinuities do not)

The mathematician behind it

Origins · 1 minAugustin-Louis Cauchy and how this was discovered
AC
Augustin-Louis Cauchy
1789–1857 · Early 19th-century French analysis, École Polytechnique

Cauchy was among the first to insist that calculus be built on a rigorous notion of limit rather than infinitesimals treated as fixed, mysterious quantities. His 1821 Cours d'Analyse introduced limit-based definitions of continuity, convergence, and derivative that are direct ancestors of the modern ε\varepsilon-δ\delta formalism (later sharpened by Weierstrass). The extension of his limit concept to infinite limits and limits at infinity — treating "xx increases without bound" and "yy increases without bound" as parallel, quantifiable phenomena — became standard as 19th-century analysts worked to eliminate hand-waving about infinity from calculus, replacing it with the "for every bound, there exists a threshold" logic used throughout this article.

History
- 1821 — Cauchy's Cours d'Analyse gives an early rigorous treatment of limits, laying groundwork for infinite-limit language.
- 1861 — Weierstrass, lecturing in Berlin, formalizes the ε\varepsilon-δ\delta definition of limit in the form essentially used today.
- 1872 — Weierstrass's construction of a continuous nowhere-differentiable function sharpens the community's insistence on fully rigorous limit arguments, including at infinity.
- 1880s–1890s — Textbook treatments (e.g. by Jordan, later Hardy) standardize the NN-ε\varepsilon and MM-δ\delta notations for limits at infinity and infinite limits, respectively.
- 1908 — G. H. Hardy's A Course of Pure Mathematics popularizes clean, explicit statements of these definitions for English-language students, close to the form given here.
Is "lim⁡x→af(x)=∞\lim_{x\to a} f(x) = \infty" the same as saying the limit exists?

No. In the classical The Epsilon-Delta Definition of a Limit, a limit "exists" only when there is a specific real number LL that f(x)f(x) approaches. When we write lim⁡x→af(x)=∞\lim_{x\to a}f(x)=\infty, we are using a different, separately defined notion — the MM-δ\delta definition given above — to describe unbounded growth. Many textbooks emphasize this by saying the limit "diverges to infinity" or "does not exist (but diverges to ∞\infty)," precisely to avoid the false impression that ∞\infty is being treated as an ordinary limiting value. This distinction matters when applying theorems that require limits to exist in the finite sense, such as many differentiation and continuity results.

How do I actually find δ\delta or NN in these definitions, in practice?

The strategy mirrors ordinary ε\varepsilon-δ\delta proofs: start from the desired conclusion (e.g. f(x)>Mf(x) > M or ∣f(x)−L∣<ε|f(x)-L|<\varepsilon) and algebraically solve for the condition on xx (e.g. ∣x−a∣<something|x-a|<\text{something} or x>somethingx > \text{something}), then declare that "something" to be δ\delta or NN. As in Example 1, solving 3/(x−1)2>M3/(x-1)^2 > M for ∣x−1∣|x-1| directly yields the required δ=3/M\delta = \sqrt{3/M}. The definition is a promise that such an algebraic solution can always be found — the proof is the act of finding and verifying it.

Can a function have both a finite limit at infinity and an infinite limit at some finite point?

Yes, and this is common: rational functions like f(x)=1/(x−2)+1f(x) = 1/(x-2) + 1 (used in the figure above) have a vertical asymptote at x=2x=2 (an infinite limit there) and a horizontal asymptote at y=1y=1 (a finite limit as x→±∞x\to\pm\infty). These are two independent pieces of information about the function's behavior — one describing local blow-up, the other describing long-run leveling-off — and neither implies the other.

Why does the algebra of limits break down for forms like ∞−∞\infty-\infty or ∞/∞\infty/\infty?

Because the proof techniques that work when at least one function has a finite limit (bounding it above and below by constants near LL) simply have no analogue when both functions are unbounded: there is no fixed real number to anchor the estimate. The counterexample above exhibits two pairs of functions, both individually satisfying lim⁡f=lim⁡g=∞\lim f=\lim g=\infty, whose differences and quotients tend to genuinely different finite values (or fail to converge at all). This shows the individual infinite limits carry too little information to pin down the combined limit — you must analyze the specific rate at which each function grows, often via algebraic manipulation or L'Hôpital's rule.

Does lim⁡x→∞f(x)=∞\lim_{x\to\infty} f(x) = \infty mean ff is eventually increasing?

No — it only guarantees that f(x)f(x) eventually exceeds any bound MM, not that ff is monotonic. For instance, f(x)=x+sin⁡xf(x) = x + \sin x satisfies lim⁡x→∞f(x)=∞\lim_{x\to\infty} f(x) = \infty (since x−1≤f(x)≤x+1x - 1 \le f(x) \le x+1, squeeze it against x±1→∞x\pm 1\to\infty), yet ff is not monotonic — its derivative 1+cos⁡x1+\cos x vanishes periodically, and ff has infinitely many points where it is momentarily flat. Divergence to infinity is a statement about eventual size, not about the shape or monotonicity of the graph along the way.

How does this connect to sequences, e.g. lim⁡n→∞an=∞\lim_{n\to\infty} a_n = \infty?

Sequences are functions with domain N\mathbb N (or a subset), so the definition of lim⁡n→∞an=∞\lim_{n\to\infty} a_n = \infty is the exact restriction of case (3) above (finite/infinite limit at infinity) to integer inputs: for every MM there is NN such that n>N  ⟹  an>Mn>N \implies a_n > M. All the algebra-of-limits results proved here for functions of a real variable apply verbatim to sequences, since the proofs never used continuity of the domain — only the threshold structure "eventually beyond NN."

What role does one-sidedness play here?

Exactly the same role as in ordinary One-Sided Limits: an infinite limit can hold from one side but not the other. For f(x)=1/xf(x)=1/x at a=0a=0, lim⁡x→0+f(x)=∞\lim_{x\to0^+} f(x) = \infty while lim⁡x→0−f(x)=−∞\lim_{x\to 0^-} f(x)=-\infty; since these disagree, the two-sided statement "lim⁡x→0f(x)=∞\lim_{x\to0} f(x)=\infty" is false, even though both one-sided infinite limits individually hold. This is analogous to how disagreeing finite one-sided limits mean the two-sided finite limit fails to exist.

Before this