Evanalysis
5.3Estimated reading time: 27 min

5.3 Delta-epsilon limits, limit laws, and continuity

Move from sequence limits to function limits, learn the delta-epsilon definition, and organize the first toolkit of nonexistence tests, limit laws, sequential criteria, and continuity.

Course contents

Chapter 5 now shifts from sequences to functions. The new difficulty is that a sequence approaches its limit through the discrete parameter nn, while a function argument xx can move toward a point aa through infinitely many nearby real values from both sides.

This is why the δ\delta-ε\varepsilon definition is needed.

From sequence limits to function limits

For sequences, the definition of

lim⁡n→∞xn=L\lim_{n\to\infty}x_n=L

said that every small tolerance around LL can be achieved by going far enough out in the sequence.

For functions, we want an analogous sentence:

as xx approaches aa, the function value f(x)f(x) approaches LL.

But now “going far enough out” no longer makes sense. We need a new way to say that xx is close enough to aa. That role is played by δ\delta.

Open intervals and punctured domains

First specify the kind of domains involved.

Definition

Open interval

An open interval is a subset of RR of one of the forms

(b,c)={x∈R∣b<x<c},(b,c)=\{x\in R\mid b\lt x\lt c\},(−∞,c)={x∈R∣x<c},(-\infty,c)=\{x\in R\mid x\lt c\},(b,∞)={x∈R∣b<x},(b,\infty)=\{x\in R\mid b\lt x\},

where b,c∈Rb,c\in R and b<cb\lt c.

To define a limit at a point aa, consider functions defined on an open interval with the point aa removed. That removal is important: a limit is about what happens near aa, not necessarily what happens at aa.

The formal delta-epsilon definition

Definition

Limit of a function at a point

Suppose II is an open interval containing a∈Ra\in R, and let f:I∖{a}→Rf:I\setminus\{a\}\to R. We say

lim⁡x→af(x)=L\lim_{x\to a}f(x)=L

if and only if for every ε>0\varepsilon\gt0, there exists δ>0\delta\gt0 such that

0<∣x−a∣<δ  ⟹  ∣f(x)−L∣<ε.0\lt|x-a|\lt\delta \implies |f(x)-L|\lt\varepsilon.

The implication is required for every x∈I∖{a}x\in I\setminus\{a\}. The number δ\delta may depend on ε\varepsilon, but not on the input xx.

Read the implication carefully:

  • 0<∣x−a∣<δ0\lt|x-a|\lt\delta means xx is close to aa, but not equal to aa;
  • ∣f(x)−L∣<ε|f(x)-L|\lt\varepsilon means the function value lands inside the ε\varepsilon-band around LL.

So the definition says:

Every requested output accuracy ε\varepsilon can be guaranteed by forcing the input xx into a sufficiently small punctured neighborhood of aa.

Common mistake

The limit definition ignores the value at a

The condition 0<∣x−a∣0\lt|x-a| removes the point aa itself. So f(a)f(a) may be undefined, or may differ from LL, while the limit still exists.

First example: lim⁡x→3(2x+1)=7\lim_{x\to 3}(2x+1)=7

The basic linear test case is the function f(x)=2x+1f(x)=2x+1 at a=3a=3.

Worked example

Choosing δ=ε/2\delta=\varepsilon/2

Let f(x)=2x+1f(x)=2x+1, a=3a=3, and L=7L=7. Then

∣f(x)−7∣=∣(2x+1)−7∣=∣2x−6∣=2∣x−3∣.|f(x)-7| = |(2x+1)-7| = |2x-6| = 2|x-3|.

So in order to force ∣f(x)−7∣<ε|f(x)-7|\lt\varepsilon, it is enough to make

∣x−3∣<ε2.|x-3|\lt\frac{\varepsilon}{2}.

Therefore choose

δ=ε2.\delta=\frac{\varepsilon}{2}.

Then whenever 0<∣x−3∣<δ0\lt|x-3|\lt\delta,

∣f(x)−7∣=2∣x−3∣<2δ=2⋅ε2=ε.|f(x)-7|=2|x-3|\lt2\delta=2\cdot \frac{\varepsilon}{2}=\varepsilon.

Hence

lim⁡x→3(2x+1)=7.\lim_{x\to 3}(2x+1)=7.

This example shows the standard proof pattern:

  1. start with ∣f(x)−L∣|f(x)-L|,
  2. simplify it into an expression involving ∣x−a∣|x-a|,
  3. choose δ\delta to make that expression smaller than ε\varepsilon.

Two more basic examples

Worked example

Constant functions

If f(x)=cf(x)=c for all xx, then

∣f(x)−c∣=∣c−c∣=0<ε|f(x)-c|=|c-c|=0\lt\varepsilon

for every ε>0\varepsilon\gt0 and every xx.

So any positive number can be chosen as δ\delta, and

lim⁡x→ac=c.\lim_{x\to a}c=c.

Worked example

A function with a hole

Consider

f:(0,∞)∖{2}→R,f(x)=x2−4x−2.f:(0,\infty)\setminus\{2\}\to R,\qquad f(x)=\frac{x^2-4}{x-2}.

The formula is undefined at x=2x=2, but for x≠2x\ne 2 it simplifies to

f(x)=x+2.f(x)=x+2.

So near x=2x=2,

∣f(x)−4∣=∣(x+2)−4∣=∣x−2∣.|f(x)-4|=|(x+2)-4|=|x-2|.

Therefore choosing δ=ε\delta=\varepsilon works. If 0<∣x−2∣<δ0\lt|x-2|\lt\delta, then

∣f(x)−4∣<ε.|f(x)-4|\lt\varepsilon.

Hence

lim⁡x→2x2−4x−2=4,\lim_{x\to 2}\frac{x^2-4}{x-2}=4,

even though f(2)f(2) is not defined.

A delta-neighbourhood mapped into an epsilon-band

Figure. The δ\delta-ε\varepsilon definition links an input neighborhood of aa to an output band around LL. The proof task is to choose δ\delta so that this implication always succeeds.

Explore the definition interactively

The explorer below lets you choose one of the examples, select ε\varepsilon, and test sample inputs xx. The point is to see the implication

0<∣x−a∣<δ  ⟹  ∣f(x)−L∣<ε0\lt|x-a|\lt\delta \implies |f(x)-L|\lt\varepsilon

as a relationship between an input strip and an output band.

Read and try

Check one delta-epsilon implication geometrically

The condition 0<|x-a|<delta must imply |f(x)-L|<epsilon for every permitted x. A sample illustrates this implication; an algebraic error bound proves it for the whole punctured interval.

0 < |x - a| < δ, with δ = 0.25

3

x = 2.8

|f(x) - L| < ε, with ε = 0.5

7

f(x) = 6.6

0 < |x - a| < δ

|2.8 - 3| = 0.2

The chosen x really lies inside the delta-neighbourhood.

|f(x) - L| < ε

|6.6 - 7| = 0.4

The function value lands inside the epsilon-band around L.

How limits can fail to exist

Next, consider how to show that a proposed limit does not exist.

To prove lim⁡x→af(x)≠L\lim_{x\to a}f(x)\ne L, one must find a single ε>0\varepsilon\gt0 such that no matter how small δ\delta is chosen, some point xx with 0<∣x−a∣<δ0\lt|x-a|\lt\delta still satisfies

∣f(x)−L∣≥ε.|f(x)-L|\ge \varepsilon.

Consider

f(x)=∣x∣x,f(x)=\frac{|x|}{x},

which equals 11 for x>0x\gt0 and −1-1 for x<0x\lt0.

Worked example

Why ∣x∣/x|x|/x has no limit at 00

Take ε=1\varepsilon=1. For any δ>0\delta\gt0, choose

x1=δ2>0,x2=−δ2<0.x_1=\frac{\delta}{2}\gt0, \qquad x_2=-\frac{\delta}{2}\lt0.

Then both satisfy ∣xi∣<δ|x_i|\lt\delta, but

f(x1)=1,f(x2)=−1.f(x_1)=1,\qquad f(x_2)=-1.

No single real number LL can lie within distance 11 of both 11 and −1-1. Therefore the function has no limit at 00.

For a nonexistence proof, the quantifiers reverse the practical strategy. To show that ff cannot have limit LL, it is enough to find one fixed ε0>0\varepsilon_0\gt0 such that every δ>0\delta\gt0 admits a punctured point with ∣f(x)−L∣≥ε0|f(x)-L|\ge\varepsilon_0. For f(x)=∣x∣/xf(x)=|x|/x at zero, any proposed LL fails: the positive and negative sides give values 11 and −1-1. If L≥0L\ge0, take a negative-side point and obtain ∣−1−L∣≥1|{-1}-L|\ge1; if L<0L\lt0, take a positive-side point and obtain ∣1−L∣>1|1-L|\gt1. Both points can be chosen inside every prescribed punctured neighborhood. This is a direct epsilon contradiction, rather than the informal statement that the graph “jumps.”

This example captures a common failure mode: left-hand and right-hand behavior do not agree.

Algebra of limits

Once some basic limits are known, limit laws show how to build new ones from old ones.

Theorem

Limit laws

If 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, then:

  • lim⁡x→a(f(x)+g(x))=L+M\lim_{x\to a}(f(x)+g(x))=L+M,
  • lim⁡x→a(f(x)g(x))=LM\lim_{x\to a}(f(x)g(x))=LM,
  • if M≠0M\ne 0, then
lim⁡x→af(x)g(x)=LM.\lim_{x\to a}\frac{f(x)}{g(x)}=\frac{L}{M}.

One neighborhood for the sum law

The sum law illustrates the quantifier pattern in its shortest complete form. Suppose f(x)→Lf(x)→L and g(x)→Mg(x)→M, and fix ε>0\varepsilon\gt0. The first limit supplies δf>0\delta_f\gt0 such that ∣f(x)−L∣<ε/2|f(x)-L|\lt\varepsilon/2 whenever 0<∣x−a∣<δf0\lt|x-a|\lt\delta_f; the second supplies δg>0\delta_g\gt0 with the analogous bound for gg. Set δ=min⁡(δf,δg)\delta=\min(\delta_f,\delta_g). The same xx then satisfies both estimates, and therefore

∣(f(x)+g(x))−(L+M)∣≤∣f(x)−L∣+∣g(x)−M∣<ε2+ε2=ε.\bigl|(f(x)+g(x))-(L+M)\bigr| \le |f(x)-L|+|g(x)-M| \lt\frac\varepsilon2+\frac\varepsilon2=\varepsilon.

The minimum is essential: it creates one neighborhood on which every required estimate holds simultaneously. A proof that chooses two unrelated input points, or that lets δ\delta depend on xx, has not established the quantified implication.

Proofs of the product and quotient laws

The product law is more than a symbolic rule: its proof must control two errors at once. Assume f:I∖{a}→Rf:I\setminus\{a\}\to R and g:I∖{a}→Rg:I\setminus\{a\}\to R have limits LL and MM at aa, and let ε>0\varepsilon\gt0 be given. No value f(a)f(a) is needed: every estimate below concerns the punctured domain. First use the limit of ff with tolerance 11 to choose δ0>0\delta_0\gt0 such that every x∈I∖{a}x\in I\setminus\{a\} with 0<∣x−a∣<δ00\lt|x-a|\lt\delta_0 satisfies

∣f(x)−L∣<1,∣f(x)∣<∣L∣+1=:A.|f(x)-L|\lt1,\qquad |f(x)|\lt|L|+1=:A.

Here A>0A\gt0 is a local bound, obtained before the final epsilon budget. Choose δ1\delta_1 so that every x∈I∖{a}x\in I\setminus\{a\} with 0<∣x−a∣<δ10\lt|x-a|\lt\delta_1 gives ∣g(x)−M∣<ε/(2A)|g(x)-M|\lt\varepsilon/(2A). Choose δ2\delta_2 so that every such xx with 0<∣x−a∣<δ20\lt|x-a|\lt\delta_2 gives ∣f(x)−L∣<ε/(2B)|f(x)-L|\lt\varepsilon/(2B), where B=max⁡(1,∣M∣)B=\max(1,|M|). Set δ=min⁡(δ0,δ1,δ2)\delta=\min(\delta_0,\delta_1,\delta_2). For any x∈I∖{a}x\in I\setminus\{a\} with 0<∣x−a∣<δ0\lt|x-a|\lt\delta, all three estimates hold; the identity

f(x)g(x)−LM=f(x)(g(x)−M)+M(f(x)−L)f(x)g(x)-LM=f(x)(g(x)-M)+M(f(x)-L)

and the triangle inequality give

∣f(x)g(x)−LM∣<Aε2A+∣M∣ε2B≤ε2+ε2=ε.|f(x)g(x)-LM| \lt A\frac{\varepsilon}{2A}+|M|\frac{\varepsilon}{2B} \le\frac{\varepsilon}{2}+\frac{\varepsilon}{2}=\varepsilon.

This proves f(x)g(x)→LMf(x)g(x)→LM, including the case M=0M=0; the use of BB avoids dividing by zero in that case.

For the quotient, the assumption M≠0M\ne0 is essential. Since g:I∖{a}→Rg:I\setminus\{a\}\to R has limit MM at aa, choose δ0>0\delta_0\gt0 so that every x∈I∖{a}x\in I\setminus\{a\} with 0<∣x−a∣<δ00\lt|x-a|\lt\delta_0 satisfies ∣g(x)−M∣<∣M∣/2|g(x)-M|\lt|M|/2. Then

∣g(x)∣≥∣M∣−∣g(x)−M∣>∣M∣/2.|g(x)|\ge |M|-|g(x)-M|\gt|M|/2.

On this same neighborhood, the reciprocal error satisfies

∣1g(x)−1M∣=∣g(x)−M∣∣g(x)∣∣M∣≤2∣g(x)−M∣∣M∣2.\left|\frac1{g(x)}-\frac1M\right| =\frac{|g(x)-M|}{|g(x)||M|} \le\frac{2|g(x)-M|}{|M|^2}.

Given ε>0\varepsilon\gt0, additionally choose δ1\delta_1 so that every x∈I∖{a}x\in I\setminus\{a\} with 0<∣x−a∣<δ10\lt|x-a|\lt\delta_1 satisfies ∣g(x)−M∣<ε∣M∣2/2|g(x)-M|\lt\varepsilon|M|^2/2; intersecting the two neighborhoods proves 1/g(x)→1/M1/g(x)→1/M. Applying the product law to f(x)f(x) and 1/g(x)1/g(x) now gives

f(x)g(x)⟶LM.\frac{f(x)}{g(x)}\longrightarrow \frac{L}{M}.

Every budget and every denominator condition is visible: first local boundedness, then the two half-errors, and then the lower bound that makes reciprocation legal.

Worked example

Using the sum law

Consider f(x)=2x+1f(x)=2x+1 and g(x)=xg(x)=\sqrt{x} near x=4x=4. Once the basic limits

lim⁡x→4(2x+1)=9,lim⁡x→4x=2\lim_{x\to 4}(2x+1)=9, \qquad \lim_{x\to 4}\sqrt{x}=2

are known, the sum law gives

lim⁡x→4((2x+1)+x)=9+2=11.\lim_{x\to 4}\bigl((2x+1)+\sqrt{x}\bigr)=9+2=11.

Worked example

Two divergent limits whose sum converges

A sum can have a limit even when neither summand does. On the punctured real line near 00, define

f(x)=sin⁡(1/x),g(x)=−sin⁡(1/x).f(x)=\sin(1/x),\qquad g(x)=-\sin(1/x).

Neither function has a limit at 00: for n≥1n\ge1, the two sequences 1/(2πn)1/(2\pi n) and 1/(2πn+π/2)1/(2\pi n+\pi/2) give output limits 00 and 11 for ff, and the corresponding outputs 00 and −1-1 for gg. Nevertheless, f(x)+g(x)=0f(x)+g(x)=0 for every allowed xx, so the sum has limit 00. This is why a limit-law hypothesis cannot be inferred from the existence of the combined expression.

Worked example

The continuous limit x/(1+x)x/(1+x) at zero

For f(x)=x/(1+x)f(x)=x/(1+x), the candidate limit at zero is L=0L=0. Restrict to ∣x∣<1/2|x|\lt1/2, which guarantees ∣1+x∣≥1−∣x∣>1/2|1+x|\ge1-|x|\gt1/2. Hence

∣x1+x−0∣≤2∣x∣.\left|\frac{x}{1+x}-0\right| \le 2|x|.

Given ε>0\varepsilon\gt0, choose

δ=min⁡(12,ε2).\delta=\min\left(\frac12,\frac\varepsilon2\right).

Then 0<∣x∣<δ0\lt|x|\lt\delta implies the denominator is nonzero and the displayed error is less than ε\varepsilon. Therefore

lim⁡x→0x1+x=0.\lim_{x\to0}\frac{x}{1+x}=0.

The sequential characterization

The sequential criterion connects function limits back to sequence limits.

Theorem

Sequential characterization of function limits

Let f:I∖{a}→Rf:I\setminus\{a\}\to R. Then

lim⁡x→af(x)=L\lim_{x\to a}f(x)=L

if and only if for every sequence (xn)(x_n) with xn∈I∖{a}x_n\in I\setminus\{a\} for all nn and xn→ax_n\to a, we have

lim⁡n→∞f(xn)=L.\lim_{n\to\infty}f(x_n)=L.

This theorem is extremely useful because it gives two complementary methods:

  1. to prove a limit exists, check every sequence approaching aa;
  2. to prove a limit does not exist, find two sequences approaching aa that give incompatible output behavior.

Apply this criterion to the oscillating function f(x)=sin⁡(1/x)f(x)=\sin(1/x) near 00.

Worked example

Two sequences proving that sin⁡(1/x)\sin(1/x) has no limit at 00

Take the indices n≥1n≥1. Then

xn=12πn,yn=12πn+π/2.x_n=\frac{1}{2\pi n}, \qquad y_n=\frac{1}{2\pi n+\pi/2}.

Then xn→0x_n\to 0 and yn→0y_n\to 0, but

f(xn)=sin⁡(2πn)=0→0,f(x_n)=\sin(2\pi n)=0\to 0,

while

f(yn)=sin⁡(2πn+π/2)=1→1.f(y_n)=\sin(2\pi n+\pi/2)=1\to 1.

Since two sequences approaching the same point produce different limiting function values, lim⁡x→0sin⁡(1/x)\lim_{x\to 0}\sin(1/x) does not exist.

Proof of the sequential characterization

The theorem has two directions, and each uses a different quantifier order.

Function limit implies every sequence limit

Assume the punctured function limit is LL. Let (xn)(x_n) be any sequence in I∖{a}I\setminus\{a\} with xn→ax_n→a. Given ε>0\varepsilon\gt0, choose δ>0\delta\gt0 from the delta-epsilon definition, so 0<∣x−a∣<δ0\lt|x-a|\lt\delta implies ∣f(x)−L∣<ε|f(x)-L|\lt\varepsilon. Since xn→ax_n→a, choose NN so that every n>Nn\gt N has ∣xn−a∣<δ|x_n-a|\lt\delta. The sequence stays in the punctured domain, so 0<∣xn−a∣<δ0\lt|x_n-a|\lt\delta and therefore ∣f(xn)−L∣<ε|f(x_n)-L|\lt\varepsilon for every n>Nn\gt N. This is exactly f(xn)→Lf(x_n)→L.

Every sequence limit implies the function limit

For the converse, argue by contrapositive. Suppose the function limit is not LL. Then there is a fixed ε0>0\varepsilon_0\gt0 such that for every δ>0\delta\gt0 one can find a point in the punctured domain with ∣f(x)−L∣≥ε0|f(x)-L|≥\varepsilon_0. For each n≥0n≥0, apply this failure with δ=1/(n+1)\delta=1/(n+1) and choose xnx_n satisfying

xn∈I∖{a},0<∣xn−a∣<1n+1,∣f(xn)−L∣≥ε0. x_n\in I\setminus\{a\},\qquad 0\lt|x_n-a|\lt\frac1{n+1},\qquad |f(x_n)-L|\ge\varepsilon_0.

The middle inequality proves xn→ax_n→a, but the last inequality prevents f(xn)→Lf(x_n)→L, since the same positive error ε0\varepsilon_0 survives at every index. This contradicts the assumed sequential property. Thus the function limit must be LL. The choice explicitly avoids aa, even when f(a)f(a) is undefined.

Continuity

One of the main purposes of limits is to make the idea of continuity precise.

Definition

Continuity at a point

Let f:I→Rf:I\to R and a∈Ia\in I. The function ff is continuous at aa if

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

Equivalently, in ε\varepsilon-δ\delta language:

∀ε>0 ∃δ>0 such that ∣x−a∣<δ  ⟹  ∣f(x)−f(a)∣<ε.\forall \varepsilon\gt0\ \exists \delta\gt0\text{ such that } |x-a|\lt\delta \implies |f(x)-f(a)|\lt\varepsilon.

Notice what changed: the condition 0<∣x−a∣0\lt|x-a| disappeared. Continuity really does care about the function value at the point.

A standard discontinuous example is:

f(x)={0,x≠0,1,x=0.f(x)= \begin{cases} 0,& x\ne 0,\\ 1,& x=0. \end{cases}

Here the nearby values are all 00, so the limit near 00 is not f(0)=1f(0)=1. Therefore the function is discontinuous at 00.

Common mistake

A function can have a limit at a without being defined at a

The hole example shows this clearly. Limits are about nearby values. Continuity adds the extra requirement that the function is defined at the point and that its value agrees with the limit.

Quick checks

Checkpoint

Why does the function-limit definition use 0<∣x−a∣<δ0 \lt |x-a| \lt \delta instead of only ∣x−a∣<δ|x-a| \lt \delta?

Think about whether the value at aa should matter for the limit.

Solution · Answer

Because the limit concerns points near aa, not necessarily the point aa itself. The strict inequality 0<∣x−a∣0\lt|x-a| removes x=ax=a from the condition.

Checkpoint

Why does the sum-law proof use min⁡(δf,δg)\min(\delta_f,\delta_g) instead of max⁡(δf,δg)\max(\delta_f,\delta_g)?

State what must be true of the same input point for both estimates to apply.

Solution · Answer

The input must satisfy both ∣x−a∣<δf|x-a|<\delta_f and ∣x−a∣<δg|x-a|<\delta_g. Taking the minimum guarantees both. Taking the maximum can admit points outside the smaller neighborhood, where one of the two error estimates is no longer guaranteed.

Checkpoint

Why must a reciprocal-limit proof first show that the denominator stays away from zero?

Identify the quantity that could magnify an otherwise small numerator error.

Solution · Answer

The reciprocal error is ∣g(x)−M∣/(∣g(x)∣∣M∣)|g(x)-M|/(|g(x)||M|). Even a small numerator gives no control if ∣g(x)∣|g(x)| can be arbitrarily close to zero. When M≠0M\ne0, the preliminary bound ∣g(x)∣>∣M∣/2|g(x)|>|M|/2 replaces the denominator by a fixed positive lower bound and makes the subsequent error estimate valid.

Exercises

Checkpoint

Prove that lim⁡x→4x=2\lim_{x\to 4}\sqrt{x}=2.

Rationalize ∣x−2∣|\sqrt{x}-2| and also keep x near 4 so the denominator stays away from zero.

Solution · Guided solution

We use

∣x−2∣=∣x−4∣x+2.|\sqrt{x}-2| = \frac{|x-4|}{\sqrt{x}+2}.

Choose

δ=min⁡(1,2ε).\delta=\min(1,2\varepsilon).

If 0<∣x−4∣<δ0\lt|x-4|\lt\delta, then in particular x∈(3,5)x\in(3,5), so x+2>2\sqrt{x}+2\gt2. Hence

∣x−2∣=∣x−4∣x+2<∣x−4∣2<δ2≤ε.|\sqrt{x}-2| = \frac{|x-4|}{\sqrt{x}+2} \lt \frac{|x-4|}{2} \lt \frac{\delta}{2} \le \varepsilon.

Therefore lim⁡x→4x=2\lim_{x\to 4}\sqrt{x}=2.

Checkpoint

Two sequences approach zero and both give output zero for f(x)=sin⁡(1/x)f(x)=\sin(1/x) . Does that prove the function limit is zero? Use xn=1/(2πn)x_n=1/(2\pi n) and yn=1/((2n+1)π)y_n=1/((2n+1)\pi) , n≥1n\ge1, and justify your answer.

Compare the universal quantifier in the sequential criterion with what two examples establish.

Solution · Model solution

Both displayed sequences tend to zero and both output sequences are constantly zero. This is insufficient because the criterion requires every sequence in the punctured domain. The additional sequence zn=1/(2πn+π/2)z_n=1/(2\pi n+\pi/2) also tends to zero, but f(zn)=1f(z_n)=1 for every n≥1n\ge1. Thus the candidate limit zero fails, and the conflicting output limits show that no function limit exists.

Checkpoint

What extra condition must be added to ‘the limit of f(x) as x approaches a exists’ in order to conclude that f is continuous at a?

Compare the definitions of limit and continuity.

Solution · Guided solution

You must also have f(a)f(a) defined and equal to the limit:

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

That equality is exactly the definition of continuity at aa.

Prerequisites and continuation

Read this after 5.1 Sequences and epsilon-N limits and 5.2 Cauchy sequences and another model of the reals. For the order-theoretic background behind completeness, see 4.3 Completeness and gaps in Q.

Practice

Work out your answer, then check it. You can revise and try again.

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Key terms in this unit