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Limit of a function

From Wikipedia, the free encyclopedia
Point to which functions converge in analysis
For the mathematical concept in general, seeLimit (mathematics).
"Delta-epsilon" redirects here. For for the fraternity, seeDelta Epsilon (fraternity).

x{\displaystyle x}sinxx{\displaystyle {\frac {\sin x}{x}}}
10.841471...
0.10.998334...
0.010.999983...

Although the functionsinxx{\displaystyle {\tfrac {\sin x}{x}}} is not defined at zero, asx becomes closer and closer to zero,sinxx{\displaystyle {\tfrac {\sin x}{x}}} becomes arbitrarily close to 1. In other words, the limit ofsinxx,{\displaystyle {\tfrac {\sin x}{x}},} asx approaches zero, equals 1.

Part of a series of articles about
Calculus
abf(t)dt=f(b)f(a){\displaystyle \int _{a}^{b}f'(t)\,dt=f(b)-f(a)}

Inmathematics, thelimit of a function is a fundamental concept incalculus andanalysis concerning the behavior of thatfunction near a particularinput which may or may not be in thedomain of the function.

Formal definitions, first devised in the early 19th century, are given below. Informally, a functionf assigns anoutputf(x) to every inputx. We say that the function has a limitL at an inputp, iff(x) gets closer and closer toL asx moves closer and closer top. More specifically, the output value can be madearbitrarily close toL if the input tof is takensufficiently close top. On the other hand, if some inputs very close top are taken to outputs that stay a fixed distance apart, then we say the limitdoes not exist.

The notion of a limit has many applications inmodern calculus. In particular, the many definitions ofcontinuity employ the concept of limit: roughly, a function is continuous if all of its limits agree with the values of the function. The concept of limit also appears in the definition of thederivative: in the calculus of one variable, this is the limiting value of theslope ofsecant lines to thegraph of a function.

History

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Although implicit in thedevelopment of calculus of the 17th and 18th centuries, the modern idea of the limit of a function goes back toBernard Bolzano who, in 1817, introduced the basics of the epsilon-delta technique (see(ε, δ)-definition of limit below) to define continuous functions. However, his work was not known during his lifetime.[1] Bruce Pourciau argues thatIsaac Newton, in his 1687Principia, demonstrates a more sophisticated understanding of limits than he is generally given credit for, including being the first to present an epsilon argument.[2][3]

In his 1821 bookCours d'analyse,Augustin-Louis Cauchy discussed variable quantities,infinitesimals and limits, and defined continuity ofy=f(x){\displaystyle y=f(x)} by saying that an infinitesimal change inx necessarily produces an infinitesimal change iny, while Grabiner claims that he used a rigorous epsilon-delta definition in proofs.[4] In 1861,Karl Weierstrass first introduced the epsilon-delta definition of limit in the form it is usually written today.[5] He also introduced the notationslim{\textstyle \lim } andlimxx0.{\textstyle \textstyle \lim \limits _{x\to x_{0}}.\displaystyle }[6]

The modern notation of placing the arrow below the limit symbol is due toG. H. Hardy, which is introduced in his bookA Course of Pure Mathematics in 1908.[7]

Motivation

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Imagine a person walking on a landscape represented by the graphy =f(x). Their horizontal position is given byx, much like the position given by a map of the land or by aglobal positioning system. Their altitude is given by the coordinatey. Suppose they walk towards a positionx =p, as they get closer and closer to this point, they will notice that their altitude approaches a specific valueL. If asked about the altitude corresponding tox =p, they would reply by sayingy =L.

What, then, does it mean to say, their altitude is approachingL? It means that their altitude gets nearer and nearer toL—except for a possible small error in accuracy. For example, suppose we set a particular accuracy goal for our traveler: they must get within ten meters ofL. They report back that indeed, they can get within ten vertical meters ofL, arguing that as long as they are within fifty horizontal meters ofp, their altitude isalways within ten meters ofL.

The accuracy goal is then changed: can they get within one vertical meter? Yes, supposing that they are able to move within five horizontal meters ofp, their altitude will always remain within one meter from the target altitudeL. Summarizing the aforementioned concept we can say that the traveler's altitudef(x) approachesL as their horizontal positionx approachesp, so as to say that for every target accuracy goal, however small it may be, there is some neighbourhood ofp, within which for every memberx' the target accuracy goal is fulfilled by an altidudef'(x) , except for maybe the horizontal positionp itself.

The initial informal statement can now be explicated:

The limit of a functionf(x) asx approachesp is a numberL with the following property: given any target distance fromL, there is a distance fromp within which the values off(x) remain within the target distance.

In fact, this explicit statement is quite close to the formal definition of the limit of a function, with values in atopological space.

More specifically, to say thatlimxpf(x)=L,{\displaystyle \lim _{x\to p}f(x)=L,}is to say thatf(x) can be made as close toL as desired, by makingx close enough, but not equal, to p.[8]

The following definitions, known as(ε,δ)-definitions, are the generally accepted definitions for the limit of a function in various contexts.

Functions of a single variable

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(ε,δ)-definition of limit

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For the depictedf,a, andb, we can ensure that the valuef(x) is within an arbitrarily small interval(b – ε,b + ε) by restrictingx to a sufficiently small interval(a – δ,a + δ). Hencef(x) →b asxa.

Supposef:RR{\displaystyle f:\mathbb {R} \rightarrow \mathbb {R} } is a function defined on thereal line, and there are two real numbersp andL. One would say: "The limit off ofx, asx approachesp, exists, and it equalsL". and write,[9]limxpf(x)=L,{\displaystyle \lim _{x\to p}f(x)=L,}or alternatively, say "f(x) tends toL asx tends top", and write,f(x)L as xp,{\displaystyle f(x)\to L{\text{ as }}x\to p,}if the following property holds: for every realε > 0, there exists a realδ > 0 such that for all realx, 0 < |xp| <δ implies|f(x) −L| <ε.[9] Symbolically,(ε>0)(δ>0)(xR)(0<|xp|<δ|f(x)L|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in \mathbb {R} )\,(0<|x-p|<\delta \implies |f(x)-L|<\varepsilon ).}

For example, one may saylimx2(4x+1)=9{\displaystyle \lim _{x\to 2}(4x+1)=9}because for every realε > 0, we can takeδ =ε/4, so that for all realx, if0 < |x − 2| <δ, then|4x + 1 − 9| <ε.

A more general definition applies for functions defined onsubsets of the real line. LetS be a subset ofR.{\displaystyle \mathbb {R} .} Letf:SR{\displaystyle f:S\to \mathbb {R} } be areal-valued function. Letp be a point such that there exists some open interval(a,b) containingp with(a,p)(p,b)S.{\displaystyle (a,p)\cup (p,b)\subset S.} It is then said that the limit off asx approachesp isL, if:

For every realε > 0, there exists a realδ > 0 such that for allx ∈ (a,b),0 < |xp| <δ implies that|f(x) −L| <ε.

Symbolically,(ε>0)(δ>0)(x(a,b))(0<|xp|<δ|f(x)L|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in (a,b))\,(0<|x-p|<\delta \implies |f(x)-L|<\varepsilon ).}

For example, one may saylimx1x+3=2{\displaystyle \lim _{x\to 1}{\sqrt {x+3}}=2}because for every realε > 0, we can takeδ =ε, so that for all realx ≥ −3, if0 < |x − 1| <δ, then|f(x) − 2| <ε. In this example,S = [−3, ∞) contains open intervals around the point 1 (for example, the interval (0, 2)).

Here, note that the value of the limit does not depend onf being defined atp, nor on the valuef(p)—if it is defined. For example, letf:[0,1)(1,2]R,f(x)=2x2x1x1.{\displaystyle f:[0,1)\cup (1,2]\to \mathbb {R} ,f(x)={\tfrac {2x^{2}-x-1}{x-1}}.}limx1f(x)=3{\displaystyle \lim _{x\to 1}f(x)=3}because for everyε > 0, we can takeδ =ε/2, so that for all realx ≠ 1, if0 < |x − 1| <δ, then|f(x) − 3| <ε. Note that heref(1) is undefined.

In fact, a limit can exist in{pR|(a,b)R:p(a,b) and (a,p)(p,b)S},{\displaystyle \{p\in \mathbb {R} \,|\,\exists (a,b)\subset \mathbb {R} :\,p\in (a,b){\text{ and }}(a,p)\cup (p,b)\subset S\},} which equalsintSisoSc,{\displaystyle \operatorname {int} S\cup \operatorname {iso} S^{c},} whereintS is theinterior ofS, andisoSc are theisolated points of the complement ofS. In our previous example whereS=[0,1)(1,2],{\displaystyle S=[0,1)\cup (1,2],}intS=(0,1)(1,2),{\displaystyle \operatorname {int} S=(0,1)\cup (1,2),}isoSc={1}.{\displaystyle \operatorname {iso} S^{c}=\{1\}.} We see, specifically, this definition of limit allows a limit to exist at 1, but not at 0 or 2.

The lettersε andδ can be understood as "error" and "distance". In fact, Cauchy usedε as an abbreviation for "error" in some of his work,[4] though in his definition of continuity, he used an infinitesimalα{\displaystyle \alpha } rather than eitherε orδ (seeCours d'Analyse). In these terms, the error (ε) in the measurement of the value at the limit can be made as small as desired by reducing the distance (δ) to the limit point. As discussed below, this definition also works for functions in a more general context. The idea thatδ andε represent distances helps suggest these generalizations.

Existence and one-sided limits

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Main article:One-sided limit
The limit asxx0+{\displaystyle x\to x_{0}^{+}} differs from that asxx0.{\displaystyle x\to x_{0}^{-}.} Therefore, the limit asxx0 does not exist.

Alternatively,x may approachp from above (right) or below (left), in which case the limits may be written as

limxp+f(x)=L{\displaystyle \lim _{x\to p^{+}}f(x)=L}

or

limxpf(x)=L{\displaystyle \lim _{x\to p^{-}}f(x)=L}

The first three functions have points for which the limit does not exist, while the functionf(x)=sin(x)x{\displaystyle f(x)={\frac {\sin(x)}{x}}}is not defined atx=0{\displaystyle x=0}, but its limit does exist.

respectively. If these limits exist at p and are equal there, then this can be referred to asthe limit off(x) atp.[10] If the one-sided limits exist atp, but are unequal, then there is no limit atp (i.e., the limit atp does not exist). If either one-sided limit does not exist atp, then the limit atp also does not exist.

A formal definition is as follows. Thelimit off asx approachesp from above isL if:

For everyε > 0, there exists aδ > 0 such that whenever0 <xp <δ, we have|f(x) −L| <ε.

(ε>0)(δ>0)(x(a,b))(0<xp<δ|f(x)L|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in (a,b))\,(0<x-p<\delta \implies |f(x)-L|<\varepsilon ).}

Thelimit off asx approachesp from below isL if:

For everyε > 0, there exists aδ > 0 such that whenever0 <px <δ, we have|f(x) −L| <ε.

(ε>0)(δ>0)(x(a,b))(0<px<δ|f(x)L|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in (a,b))\,(0<p-x<\delta \implies |f(x)-L|<\varepsilon ).}

If the limit does not exist, then theoscillation off atp is non-zero.

More general definition using limit points and subsets

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Further information:Limit point

Limits can also be defined by approaching from subsets of the domain.

In general:[11] Letf:SR{\displaystyle f:S\to \mathbb {R} } be a real-valued function defined on someSR.{\displaystyle S\subseteq \mathbb {R} .} Letp be alimit point of someTS{\displaystyle T\subset S}—that is,p is the limit of some sequence of elements ofT distinct fromp. Then we saythe limit off, asx approachesp from values inT, isL, writtenlimxpxTf(x)=L{\displaystyle \lim _{{x\to p} \atop {x\in T}}f(x)=L}if the following holds:

For everyε >0, there exists aδ >0 such that for allxT,0 < |xp| <δ implies that|f(x) −L| <ε.

(ε>0)(δ>0)(xT)(0<|xp|<δ|f(x)L|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in T)\,(0<|x-p|<\delta \implies |f(x)-L|<\varepsilon ).}

Note,T can be any subset ofS, the domain off. And the limit might depend on the selection ofT. This generalization includes as special cases limits on an interval, as well as left-handed limits of real-valued functions (e.g., by takingT to be an open interval of the form(–∞,a)), and right-handed limits (e.g., by takingT to be an open interval of the form(a, ∞)). It also extends the notion of one-sided limits to the included endpoints of (half-)closed intervals, so thesquare root functionf(x)=x{\displaystyle f(x)={\sqrt {x}}} can have limit 0 asx approaches 0 from above:limx0x[0,)x=0{\displaystyle \lim _{{x\to 0} \atop {x\in [0,\infty )}}{\sqrt {x}}=0}since for everyε > 0, we may takeδ =ε2 such that for allx ≥ 0, if0 < |x − 0| <δ, then|f(x) − 0| <ε.

This definition allows a limit to be defined at limit points of the domainS, if a suitable subsetT which has the same limit point is chosen.

Notably, the previous two-sided definition works onintSisoSc,{\displaystyle \operatorname {int} S\cup \operatorname {iso} S^{c},} which is a subset of the limit points ofS.

For example, letS=[0,1)(1,2].{\displaystyle S=[0,1)\cup (1,2].} The previous two-sided definition would work at1isoSc={1},{\displaystyle 1\in \operatorname {iso} S^{c}=\{1\},} but it wouldn't work at 0 or 2, which are limit points ofS.

Deleted versus non-deleted limits

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The definition of limit given here does not depend on how (or whether)f is defined atp. Bartle[12] refers to this as adeleted limit, because it excludes the value off atp. The correspondingnon-deleted limit does depend on the value off atp, ifp is in the domain off. Letf:SR{\displaystyle f:S\to \mathbb {R} } be a real-valued function.The non-deleted limit off, asx approachesp, isL if

For everyε > 0, there exists aδ > 0 such that for allxS,|xp| <δ implies|f(x) −L| <ε.

(ε>0)(δ>0)(xS)(|xp|<δ|f(x)L|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in S)\,(|x-p|<\delta \implies |f(x)-L|<\varepsilon ).}

The definition is the same, except that the neighborhood|xp| <δ now includes the pointp, in contrast to thedeleted neighborhood0 < |xp| <δ. This makes the definition of a non-deleted limit less general. One of the advantages of working with non-deleted limits is that they allow to state thetheorem about limits of compositions without any constraints on the functions (other than the existence of their non-deleted limits).[13]

Bartle[12] notes that although by "limit" some authors do mean this non-deleted limit, deleted limits are the most popular.[14]

Examples

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Non-existence of one-sided limit(s)

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Function without a limit at anessential discontinuity

The functionf(x)={sin5x1 for x<10 for x=1110x10 for x>1{\displaystyle f(x)={\begin{cases}\sin {\frac {5}{x-1}}&{\text{ for }}x<1\\0&{\text{ for }}x=1\\[2pt]{\frac {1}{10x-10}}&{\text{ for }}x>1\end{cases}}}has no limit atx0 = 1 (the left-hand limit does not exist due to the oscillatory nature of the sine function, and the right-hand limit does not exist due to the asymptotic behaviour of the reciprocal function, see picture), but has a limit at every otherx-coordinate.

The functionf(x)={1x rational 0x irrational {\displaystyle f(x)={\begin{cases}1&x{\text{ rational }}\\0&x{\text{ irrational }}\end{cases}}}(a.k.a., theDirichlet function) has no limit at anyx-coordinate.

Non-equality of one-sided limits

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The functionf(x)={1 for x<02 for x0{\displaystyle f(x)={\begin{cases}1&{\text{ for }}x<0\\2&{\text{ for }}x\geq 0\end{cases}}}has a limit at every non-zerox-coordinate (the limit equals 1 for negativex and equals 2 for positivex). The limit atx = 0 does not exist (the left-hand limit equals 1, whereas the right-hand limit equals 2).

Limits at only one point

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The functionsf(x)={xx rational 0x irrational {\displaystyle f(x)={\begin{cases}x&x{\text{ rational }}\\0&x{\text{ irrational }}\end{cases}}}andf(x)={|x|x rational 0x irrational {\displaystyle f(x)={\begin{cases}|x|&x{\text{ rational }}\\0&x{\text{ irrational }}\end{cases}}}both have a limit atx = 0 and it equals 0.

Limits at countably many points

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The functionf(x)={sinxx irrational 1x rational {\displaystyle f(x)={\begin{cases}\sin x&x{\text{ irrational }}\\1&x{\text{ rational }}\end{cases}}}has a limit at anyx-coordinate of the formπ2+2nπ,{\displaystyle {\tfrac {\pi }{2}}+2n\pi ,} wheren is any integer.

Limits involving infinity

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Limits at infinity

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The limit of this function at infinity exists

Letf:SR{\displaystyle f:S\to \mathbb {R} } be a function defined onSR.{\displaystyle S\subseteq \mathbb {R} .}The limit off asx approaches infinity isL, denoted

limxf(x)=L,{\displaystyle \lim _{x\to \infty }f(x)=L,}

means that:

For everyε > 0, there exists ac > 0 such that whenever+x >c, we have|f(x) −L| <ε.

(ε>0)(c>0)(xS)(x>c|f(x)L|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists c>0)\,(\forall x\in S)\,(x>c\implies |f(x)-L|<\varepsilon ).}

Similarly,the limit off asx approaches minus infinity isL, denoted

limxf(x)=L,{\displaystyle \lim _{x\to -\infty }f(x)=L,}

means that:

For everyε > 0, there exists ac > 0 such that wheneverx < −c, we have|f(x) −L| <ε.

(ε>0)(c>0)(xS)(x<c|f(x)L|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists c>0)\,(\forall x\in S)\,(x<-c\implies |f(x)-L|<\varepsilon ).}

For example,limx(3sinxx+4)=4{\displaystyle \lim _{x\to \infty }\left(-{\frac {3\sin x}{x}}+4\right)=4}because for everyε > 0, we can takec = 3/ε such that for all realx, ifx >c, then|f(x) − 4| <ε.

Another example is thatlimxex=0{\displaystyle \lim _{x\to -\infty }e^{x}=0}because for everyε > 0, we can takec = max{1, −ln(ε)} such that for all realx, ifx < −c, then|f(x) − 0| <ε.

Infinite limits

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For a function whose values grow without bound, the function diverges and the usual limit does not exist. However, in this case one may introduce limits with infinite values.

Letf:SR{\displaystyle f:S\to \mathbb {R} } be a function defined onSR.{\displaystyle S\subseteq \mathbb {R} .} The statementthe limit off asx approachesp is infinity, denoted

limxpf(x)=,{\displaystyle \lim _{x\to p}f(x)=\infty ,}

means that:

For everyN > 0, there exists aδ > 0 such that whenever0 < |xp| <δ, we havef(x) >N.

(N>0)(δ>0)(xS)(0<|xp|<δf(x)>N).{\displaystyle (\forall N>0)\,(\exists \delta >0)\,(\forall x\in S)\,(0<|x-p|<\delta \implies f(x)>N).}

The statementthe limit off asx approachesp is minus infinity, denoted

limxpf(x)=,{\displaystyle \lim _{x\to p}f(x)=-\infty ,}

means that:

For everyN > 0, there exists aδ > 0 such that whenever0 < |xp| <δ, we havef(x) < −N.

(N>0)(δ>0)(xS)(0<|xp|<δf(x)<N).{\displaystyle (\forall N>0)\,(\exists \delta >0)\,(\forall x\in S)\,(0<|x-p|<\delta \implies f(x)<-N).}

For example,limx11(x1)2={\displaystyle \lim _{x\to 1}{\frac {1}{(x-1)^{2}}}=\infty }because for everyN > 0, we can takeδ=1Nδ=1N{\textstyle \delta ={\tfrac {1}{{\sqrt {N}}\delta }}={\tfrac {1}{\sqrt {N}}}} such that for all realx > 0, if0 <x − 1 <δ, thenf(x) >N.

These ideas can be used together to produce definitions for different combinations, such as

limxf(x)=,{\displaystyle \lim _{x\to \infty }f(x)=\infty ,} orlimxp+f(x)=.{\displaystyle \lim _{x\to p^{+}}f(x)=-\infty .}

For example,limx0+lnx={\displaystyle \lim _{x\to 0^{+}}\ln x=-\infty }because for everyN > 0, we can takeδ =eN such that for all realx > 0, if0 <x − 0 <δ, thenf(x) < −N.

Limits involving infinity are connected with the concept ofasymptotes.

These notions of a limit attempt to provide a metric space interpretation to limits at infinity. In fact, they are consistent with the topological space definition of limit if

In this case,R¯{\displaystyle {\overline {\mathbb {R} }}} is a topological space and any function of the formf:XY{\displaystyle f:X\to Y} withX,YR¯{\displaystyle X,Y\subseteq {\overline {\mathbb {R} }}} is subject to the topological definition of a limit. Note that with this topological definition, it is easy to define infinite limits at finite points, which have not been defined above in the metric sense.

Alternative notation

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Many authors[15] allow for theprojectively extended real line to be used as a way to include infinite values as well asextended real line. With this notation, the extended real line is given asR{,+}{\displaystyle \mathbb {R} \cup \{-\infty ,+\infty \}} and the projectively extended real line isR{}{\displaystyle \mathbb {R} \cup \{\infty \}} where a neighborhood of ∞ is a set of the form{x:|x|>c}.{\displaystyle \{x:|x|>c\}.} The advantage is that one only needs three definitions for limits (left, right, and central) to cover all the cases.As presented above, for a completely rigorous account, we would need to consider 15 separate cases for each combination of infinities (five directions: −∞, left, central, right, and +∞; three bounds: −∞, finite, or +∞). There are also noteworthy pitfalls. For example, when working with the extended real line,x1{\displaystyle x^{-1}} does not possess a central limit (which is normal):

limx0+1x=+,limx01x=.{\displaystyle \lim _{x\to 0^{+}}{1 \over x}=+\infty ,\quad \lim _{x\to 0^{-}}{1 \over x}=-\infty .}

In contrast, when working with the projective real line, infinities (much like 0) are unsigned, so, the central limitdoes exist in that context:

limx0+1x=limx01x=limx01x=.{\displaystyle \lim _{x\to 0^{+}}{1 \over x}=\lim _{x\to 0^{-}}{1 \over x}=\lim _{x\to 0}{1 \over x}=\infty .}

In fact there are a plethora of conflicting formal systems in use.In certain applications ofnumerical differentiation and integration, it is, for example, convenient to havesigned zeroes. A simple reason has to do with the converse oflimx0x1=,{\displaystyle \lim _{x\to 0^{-}}{x^{-1}}=-\infty ,} namely, it is convenient forlimxx1=0{\displaystyle \lim _{x\to -\infty }{x^{-1}}=-0} to be considered true.Such zeroes can be seen as an approximation toinfinitesimals.

Limits at infinity for rational functions

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Horizontal asymptote abouty = 4

There are three basic rules for evaluating limits at infinity for arational functionf(x)=p(x)q(x){\displaystyle f(x)={\tfrac {p(x)}{q(x)}}} (wherep andq are polynomials):

  • If thedegree ofp is greater than the degree ofq, then the limit is positive or negative infinity depending on the signs of the leading coefficients;
  • If the degree ofp andq are equal, the limit is the leading coefficient ofp divided by the leading coefficient ofq;
  • If the degree ofp is less than the degree ofq, the limit is 0.

If the limit at infinity exists, it represents a horizontal asymptote aty =L. Polynomials do not have horizontal asymptotes; such asymptotes may however occur with rational functions.

Functions of more than one variable

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Ordinary limits

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By noting that|xp| represents adistance, the definition of a limit can be extended to functions of more than one variable. In the case of a functionf:S×TR{\displaystyle f:S\times T\to \mathbb {R} } defined onS×TR2,{\displaystyle S\times T\subseteq \mathbb {R} ^{2},} we defined the limit as follows:the limit off as(x,y) approaches(p,q) isL, written

lim(x,y)(p,q)f(x,y)=L{\displaystyle \lim _{(x,y)\to (p,q)}f(x,y)=L}

if the following condition holds:

For everyε > 0, there exists aδ > 0 such that for allx inS andy inT, whenever0<(xp)2+(yq)2<δ,{\textstyle 0<{\sqrt {(x-p)^{2}+(y-q)^{2}}}<\delta ,} we have|f(x,y) −L| <ε,[16]

or formally:(ε>0)(δ>0)(xS)(yT)(0<(xp)2+(yq)2<δ|f(x,y)L|<ε)).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in S)\,(\forall y\in T)\,(0<{\sqrt {(x-p)^{2}+(y-q)^{2}}}<\delta \implies |f(x,y)-L|<\varepsilon )).}

Here(xp)2+(yq)2{\textstyle {\sqrt {(x-p)^{2}+(y-q)^{2}}}} is theEuclidean distance between(x,y) and(p,q). (This can in fact be replaced by anynorm||(x,y) − (p,q)||, and be extended to any number of variables.)

For example, we may saylim(x,y)(0,0)x4x2+y2=0{\displaystyle \lim _{(x,y)\to (0,0)}{\frac {x^{4}}{x^{2}+y^{2}}}=0}because for everyε > 0, we can takeδ=ε{\textstyle \delta ={\sqrt {\varepsilon }}} such that for all realx ≠ 0 and realy ≠ 0, if0<(x0)2+(y0)2<δ,{\textstyle 0<{\sqrt {(x-0)^{2}+(y-0)^{2}}}<\delta ,} then|f(x,y) − 0| <ε.

Similar to the case in single variable, the value off at(p,q) does not matter in this definition of limit.

For such a multivariable limit to exist, this definition requires the value off approachesL along every possible path approaching(p,q).[17] In the above example, the functionf(x,y)=x4x2+y2{\displaystyle f(x,y)={\frac {x^{4}}{x^{2}+y^{2}}}}satisfies this condition. This can be seen by considering thepolar coordinates(x,y)=(rcosθ,rsinθ)(0,0),{\displaystyle (x,y)=(r\cos \theta ,r\sin \theta )\to (0,0),}which giveslimr0f(rcosθ,rsinθ)=limr0r4cos4θr2=limr0r2cos4θ.{\displaystyle \lim _{r\to 0}f(r\cos \theta ,r\sin \theta )=\lim _{r\to 0}{\frac {r^{4}\cos ^{4}\theta }{r^{2}}}=\lim _{r\to 0}r^{2}\cos ^{4}\theta .}Hereθ =θ(r) is a function ofr which controls the shape of the path along whichf is approaching(p,q). Sincecosθ is bounded between [−1, 1], by thesandwich theorem, this limit tends to 0.

In contrast, the functionf(x,y)=xyx2+y2{\displaystyle f(x,y)={\frac {xy}{x^{2}+y^{2}}}}does not have a limit at(0, 0). Taking the path(x,y) = (t, 0) → (0, 0), we obtainlimt0f(t,0)=limt00t2=0,{\displaystyle \lim _{t\to 0}f(t,0)=\lim _{t\to 0}{\frac {0}{t^{2}}}=0,}while taking the path(x,y) = (t,t) → (0, 0), we obtainlimt0f(t,t)=limt0t2t2+t2=12.{\displaystyle \lim _{t\to 0}f(t,t)=\lim _{t\to 0}{\frac {t^{2}}{t^{2}+t^{2}}}={\frac {1}{2}}.}

Since the two values do not agree,f does not tend to a single value as(x,y) approaches(0, 0).

Multiple limits

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Although less commonly used, there is another type of limit for a multivariable function, known as themultiple limit. For a two-variable function, this is thedouble limit.[18] Letf:S×TR{\displaystyle f:S\times T\to \mathbb {R} } be defined onS×TR2,{\displaystyle S\times T\subseteq \mathbb {R} ^{2},} we saythe double limit off asx approachesp andy approachesq isL, written

limxpyqf(x,y)=L{\displaystyle \lim _{{x\to p} \atop {y\to q}}f(x,y)=L}

if the following condition holds:

For everyε > 0, there exists aδ > 0 such that for allx inS andy inT, whenever0 < |xp| <δ and0 < |yq| <δ, we have|f(x,y) −L| <ε.[18]

(ε>0)(δ>0)(xS)(yT)((0<|xp|<δ)(0<|yq|<δ)|f(x,y)L|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in S)\,(\forall y\in T)\,((0<|x-p|<\delta )\land (0<|y-q|<\delta )\implies |f(x,y)-L|<\varepsilon ).}

For such a double limit to exist, this definition requires the value off approachesL along every possible path approaching(p,q), excluding the two linesx =p andy =q. As a result, the multiple limit is a weaker notion than the ordinary limit: if the ordinary limit exists and equalsL, then the multiple limit exists and also equalsL. The converse is not true: the existence of the multiple limits does not imply the existence of the ordinary limit. Consider the examplef(x,y)={1forxy00forxy=0{\displaystyle f(x,y)={\begin{cases}1\quad {\text{for}}\quad xy\neq 0\\0\quad {\text{for}}\quad xy=0\end{cases}}}wherelimx0y0f(x,y)=1{\displaystyle \lim _{{x\to 0} \atop {y\to 0}}f(x,y)=1}butlim(x,y)(0,0)f(x,y){\displaystyle \lim _{(x,y)\to (0,0)}f(x,y)} does not exist.

If the domain off is restricted to(S{p})×(T{q}),{\displaystyle (S\setminus \{p\})\times (T\setminus \{q\}),} then the two definitions of limits coincide.[18]

Multiple limits at infinity

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The concept of multiple limit can extend to the limit at infinity, in a way similar to that of a single variable function. Forf:S×TR,{\displaystyle f:S\times T\to \mathbb {R} ,} we saythe double limit off asx andy approaches infinity isL, writtenlimxyf(x,y)=L{\displaystyle \lim _{{x\to \infty } \atop {y\to \infty }}f(x,y)=L}

if the following condition holds:

For everyε > 0, there exists ac > 0 such that for allx inS andy inT, wheneverx >c andy >c, we have|f(x,y) −L| <ε.

(ε>0)(c>0)(xS)(yT)((x>c)(y>c)|f(x,y)L|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists c>0)\,(\forall x\in S)\,(\forall y\in T)\,((x>c)\land (y>c)\implies |f(x,y)-L|<\varepsilon ).}

We saythe double limit off asx andy approaches minus infinity isL, writtenlimxyf(x,y)=L{\displaystyle \lim _{{x\to -\infty } \atop {y\to -\infty }}f(x,y)=L}

if the following condition holds:

For everyε > 0, there exists ac > 0 such thatx inS andy inT, wheneverx < −c andy < −c, we have|f(x,y) −L| <ε.

(ε>0)(c>0)(xS)(yT)((x<c)(y<c)|f(x,y)L|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists c>0)\,(\forall x\in S)\,(\forall y\in T)\,((x<-c)\land (y<-c)\implies |f(x,y)-L|<\varepsilon ).}

Pointwise limits and uniform limits

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Main articles:Pointwise convergence andUniform convergence

Letf:S×TR.{\displaystyle f:S\times T\to \mathbb {R} .} Instead of taking limit as(x,y) → (p,q), we may consider taking the limit of just one variable, say,xp, to obtain a single-variable function ofy, namelyg:TR.{\displaystyle g:T\to \mathbb {R} .} In fact, this limiting process can be done in two distinct ways. The first one is calledpointwise limit. We saythe pointwise limit off asx approachesp isg, denotedlimxpf(x,y)=g(y),{\displaystyle \lim _{x\to p}f(x,y)=g(y),} orlimxpf(x,y)=g(y)pointwise.{\displaystyle \lim _{x\to p}f(x,y)=g(y)\;\;{\text{pointwise}}.}

Alternatively, we may sayf tends tog pointwise asx approachesp, denotedf(x,y)g(y)asxp,{\displaystyle f(x,y)\to g(y)\;\;{\text{as}}\;\;x\to p,} orf(x,y)g(y)pointwiseasxp.{\displaystyle f(x,y)\to g(y)\;\;{\text{pointwise}}\;\;{\text{as}}\;\;x\to p.}

This limit exists if the following holds:

For everyε > 0 and every fixedy inT, there exists aδ(ε,y) > 0 such that for allx inS, whenever0 < |xp| <δ, we have|f(x,y) −g(y)| <ε.[19]

(ε>0)(yT)(δ>0)(xS)(0<|xp|<δ|f(x,y)g(y)|<ε).{\displaystyle (\forall \varepsilon >0)\,(\forall y\in T)\,(\exists \delta >0)\,(\forall x\in S)\,(0<|x-p|<\delta \implies |f(x,y)-g(y)|<\varepsilon ).}

Here,δ =δ(ε,y) is a function of bothε andy. Eachδ is chosen for aspecific point ofy. Hence we say the limit is pointwise iny. For example,f(x,y)=xcosy{\displaystyle f(x,y)={\frac {x}{\cos y}}}has a pointwise limit of constant zero functionlimx0f(x,y)=0(y)pointwise{\displaystyle \lim _{x\to 0}f(x,y)=0(y)\;\;{\text{pointwise}}}because for every fixedy, the limit is clearly 0. This argument fails ify is not fixed: ify is very close toπ/2, the value of the fraction may deviate from 0.

This leads to another definition of limit, namely theuniform limit. We saythe uniform limit off onT asx approachesp isg, denoteduniflimxpyTf(x,y)=g(y),{\displaystyle {\underset {{x\to p} \atop {y\in T}}{\mathrm {unif} \lim \;}}f(x,y)=g(y),} orlimxpf(x,y)=g(y)uniformly onT.{\displaystyle \lim _{x\to p}f(x,y)=g(y)\;\;{\text{uniformly on}}\;T.}

Alternatively, we may sayf tends tog uniformly onT asx approachesp, denotedf(x,y)g(y)onTasxp,{\displaystyle f(x,y)\rightrightarrows g(y)\;{\text{on}}\;T\;\;{\text{as}}\;\;x\to p,} orf(x,y)g(y)uniformly onTasxp.{\displaystyle f(x,y)\to g(y)\;\;{\text{uniformly on}}\;T\;\;{\text{as}}\;\;x\to p.}

This limit exists if the following holds:

For everyε > 0, there exists aδ(ε) > 0 such that for allx inS andy inT, whenever0 < |xp| <δ, we have|f(x,y) −g(y)| <ε.[19]

(ε>0)(δ>0)(xS)(yT)(0<|xp|<δ|f(x,y)g(y)|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in S)\,(\forall y\in T)\,(0<|x-p|<\delta \implies |f(x,y)-g(y)|<\varepsilon ).}

Here,δ =δ(ε) is a function of onlyε but noty. In other words,δ isuniformly applicable to ally inT. Hence we say the limit is uniform iny. For example,f(x,y)=xcosy{\displaystyle f(x,y)=x\cos y}has a uniform limit of constant zero functionlimx0f(x,y)=0(y) uniformly onR{\displaystyle \lim _{x\to 0}f(x,y)=0(y)\;\;{\text{ uniformly on}}\;\mathbb {R} }because for all realy,cosy is bounded between[−1, 1]. Hence no matter howy behaves, we may use thesandwich theorem to show that the limit is 0.

Iterated limits

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Main article:Iterated limits

Letf:S×TR.{\displaystyle f:S\times T\to \mathbb {R} .} We may consider taking the limit of just one variable, say,xp, to obtain a single-variable function ofy, namelyg:TR,{\displaystyle g:T\to \mathbb {R} ,} and then take limit in the other variable, namelyyq, to get a numberL. Symbolically,limyqlimxpf(x,y)=limyqg(y)=L.{\displaystyle \lim _{y\to q}\lim _{x\to p}f(x,y)=\lim _{y\to q}g(y)=L.}

This limit is known asiterated limit of the multivariable function.[20] The order of taking limits may affect the result, i.e.,

limyqlimxpf(x,y)limxplimyqf(x,y){\displaystyle \lim _{y\to q}\lim _{x\to p}f(x,y)\neq \lim _{x\to p}\lim _{y\to q}f(x,y)} in general.

A sufficient condition of equality is given by theMoore-Osgood theorem, which requires the limitlimxpf(x,y)=g(y){\displaystyle \lim _{x\to p}f(x,y)=g(y)} to be uniform onT.[21]

Functions on metric spaces

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SupposeM andN are subsets ofmetric spacesA andB, respectively, andf :MN is defined betweenM andN, withxM,p alimit point ofM andLN. It is said thatthe limit off asx approachesp isL and write

limxpf(x)=L{\displaystyle \lim _{x\to p}f(x)=L}

if the following property holds:

For everyε > 0, there exists aδ > 0 such that for all pointsxM,0 <dA(x,p) <δ impliesdB(f(x),L) <ε.[22]

(ε>0)(δ>0)(xM)(0<dA(x,p)<δdB(f(x),L)<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in M)\,(0<d_{A}(x,p)<\delta \implies d_{B}(f(x),L)<\varepsilon ).}

Again, note thatp need not be in the domain off, nor doesL need to be in the range off, and even iff(p) is defined it need not be equal toL.

Euclidean metric

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The limit inEuclidean space is a direct generalization of limits tovector-valued functions. For example, we may consider a functionf:S×TR3{\displaystyle f:S\times T\to \mathbb {R} ^{3}} such thatf(x,y)=(f1(x,y),f2(x,y),f3(x,y)).{\displaystyle f(x,y)=(f_{1}(x,y),f_{2}(x,y),f_{3}(x,y)).}Then, under the usualEuclidean metric,lim(x,y)(p,q)f(x,y)=(L1,L2,L3){\displaystyle \lim _{(x,y)\to (p,q)}f(x,y)=(L_{1},L_{2},L_{3})}if the following holds:

For everyε > 0, there exists aδ > 0 such that for allx inS andy inT,0<(xp)2+(yq)2<δ{\textstyle 0<{\sqrt {(x-p)^{2}+(y-q)^{2}}}<\delta } implies(f1L1)2+(f2L2)2+(f3L3)2<ε.{\textstyle {\sqrt {(f_{1}-L_{1})^{2}+(f_{2}-L_{2})^{2}+(f_{3}-L_{3})^{2}}}<\varepsilon .}[23]

(ε>0)(δ>0)(xS)(yT)(0<(xp)2+(yq)2<δ(f1L1)2+(f2L2)2+(f3L3)2<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in S)\,(\forall y\in T)\,\left(0<{\sqrt {(x-p)^{2}+(y-q)^{2}}}<\delta \implies {\sqrt {(f_{1}-L_{1})^{2}+(f_{2}-L_{2})^{2}+(f_{3}-L_{3})^{2}}}<\varepsilon \right).}

In this example, the function concerned are finite-dimension vector-valued function. In this case, thelimit theorem for vector-valued function states that if the limit of each component exists, then the limit of a vector-valued function equals the vector with each component taken the limit:[23]lim(x,y)(p,q)(f1(x,y),f2(x,y),f3(x,y))=(lim(x,y)(p,q)f1(x,y),lim(x,y)(p,q)f2(x,y),lim(x,y)(p,q)f3(x,y)).{\displaystyle \lim _{(x,y)\to (p,q)}{\Bigl (}f_{1}(x,y),f_{2}(x,y),f_{3}(x,y){\Bigr )}=\left(\lim _{(x,y)\to (p,q)}f_{1}(x,y),\lim _{(x,y)\to (p,q)}f_{2}(x,y),\lim _{(x,y)\to (p,q)}f_{3}(x,y)\right).}

Manhattan metric

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One might also want to consider spaces other than Euclidean space. An example would be the Manhattan space. Considerf:SR2{\displaystyle f:S\to \mathbb {R} ^{2}} such thatf(x)=(f1(x),f2(x)).{\displaystyle f(x)=(f_{1}(x),f_{2}(x)).}Then, under theManhattan metric,limxpf(x)=(L1,L2){\displaystyle \lim _{x\to p}f(x)=(L_{1},L_{2})}if the following holds:

For everyε > 0, there exists aδ > 0 such that for allx inS,0 < |xp| <δ implies|f1L1| + |f2L2| <ε.

(ε>0)(δ>0)(xS)(0<|xp|<δ|f1L1|+|f2L2|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in S)\,(0<|x-p|<\delta \implies |f_{1}-L_{1}|+|f_{2}-L_{2}|<\varepsilon ).}

Since this is also a finite-dimension vector-valued function, the limit theorem stated above also applies.[24]

Uniform metric

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Finally, we will discuss the limit infunction space, which has infinite dimensions. Consider a functionf(x,y) in the function spaceS×TR.{\displaystyle S\times T\to \mathbb {R} .} We want to find out asx approachesp, howf(x,y) will tend to another functiong(y), which is in the function spaceTR.{\displaystyle T\to \mathbb {R} .} The "closeness" in this function space may be measured under theuniform metric.[25] Then, we will saythe uniform limit off onT asx approachesp isg and writeuniflimxpyTf(x,y)=g(y),{\displaystyle {\underset {{x\to p} \atop {y\in T}}{\mathrm {unif} \lim \;}}f(x,y)=g(y),} orlimxpf(x,y)=g(y)uniformly onT,{\displaystyle \lim _{x\to p}f(x,y)=g(y)\;\;{\text{uniformly on}}\;T,}

if the following holds:

For everyε > 0, there exists aδ > 0 such that for allx inS,0 < |xp| <δ impliessupyT|f(x,y)g(y)|<ε.{\displaystyle \sup _{y\in T}|f(x,y)-g(y)|<\varepsilon .}

(ε>0)(δ>0)(xS)(0<|xp|<δsupyT|f(x,y)g(y)|<ε).{\displaystyle (\forall \varepsilon >0)\,(\exists \delta >0)\,(\forall x\in S)\,(0<|x-p|<\delta \implies \sup _{y\in T}|f(x,y)-g(y)|<\varepsilon ).}

In fact, one can see that this definition is equivalent to that of the uniform limit of a multivariable function introduced in the previous section.

Functions on topological spaces

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See also:Filters in topology § Limits of functions

SupposeX{\displaystyle X} andY{\displaystyle Y} aretopological spaces withY{\displaystyle Y} aHausdorff space. Letp{\displaystyle p} be alimit point ofΩX{\displaystyle \Omega \subseteq X}, andLY{\displaystyle L\in Y}. For a functionf:ΩY{\displaystyle f:\Omega \to Y}, it is said that thelimit off{\displaystyle f} asx{\displaystyle x} approachesp{\displaystyle p} isL{\displaystyle L}, written

limxpf(x)=L,{\displaystyle \lim _{x\to p}f(x)=L,}

if the following property holds:

for every openneighborhoodV{\displaystyle V} ofL{\displaystyle L}, there exists an open neighborhoodU{\displaystyle U} ofp{\displaystyle p} such thatf(UΩ{p})V{\displaystyle f(U\cap \Omega -\{p\})\subseteq V}.

This last part of the definition can also be phrased as "there exists an openpunctured neighbourhoodU{\displaystyle U} ofp{\displaystyle p} such thatf(UΩ)V{\displaystyle f(U\cap \Omega )\subseteq V}.

The domain off{\displaystyle f} does not need to containp{\displaystyle p}. If it does, then the value off{\displaystyle f} atp{\displaystyle p} is irrelevant to the definition of the limit. In particular, if the domain off{\displaystyle f} isX{p}{\displaystyle X\setminus \{p\}} (or all ofX{\displaystyle X}), then the limit off{\displaystyle f} asxp{\displaystyle x\to p} exists and is equal toL if, for all subsetsΩ ofX with limit pointp{\displaystyle p}, the limit of the restriction off{\displaystyle f} toΩ exists and is equal toL. Sometimes this criterion is used to establish thenon-existence of the two-sided limit of a function onR{\displaystyle \mathbb {R} } by showing that theone-sided limits either fail to exist or do not agree. Such a view is fundamental in the field ofgeneral topology, where limits and continuity at a point are defined in terms of special families of subsets, calledfilters, or generalized sequences known asnets.

Alternatively, the requirement thatY{\displaystyle Y} be a Hausdorff space can be relaxed to the assumption thatY{\displaystyle Y} be a general topological space, but then the limit of a function may not be unique. In particular, one can no longer talk aboutthe limit of a function at a point, but rathera limit orthe set of limits at a point.

A function is continuous at a limit pointp{\displaystyle p} of and in its domain if and only iff(p){\displaystyle f(p)} isthe (or, in the general case,a) limit off(x){\displaystyle f(x)} asx{\displaystyle x} tends top{\displaystyle p}.

There is another type of limit of a function, namely thesequential limit. Letf:XY{\displaystyle f:X\to Y} be a mapping from a topological spaceX into a Hausdorff spaceY,pX{\displaystyle p\in X} a limit point ofX andLY. The sequential limit off{\displaystyle f} asx{\displaystyle x} tends top{\displaystyle p} isL if

For everysequence(xn){\displaystyle (x_{n})} inX{p}{\displaystyle X\setminus \{p\}} thatconverges top{\displaystyle p}, the sequencef(xn){\displaystyle f(x_{n})}converges toL.

IfL is the limit (in the sense above) off{\displaystyle f} asx{\displaystyle x} approachesp{\displaystyle p}, then it is a sequential limit as well; however, the converse need not hold in general. If in additionX ismetrizable, thenL is the sequential limit off{\displaystyle f} asx{\displaystyle x} approachesp{\displaystyle p} if and only if it is the limit (in the sense above) off{\displaystyle f} asx{\displaystyle x} approachesp{\displaystyle p}.

Other characterizations

[edit]

In terms of sequences

[edit]

For functions on the real line, one way to define the limit of a function is in terms of the limit of sequences. (This definition is usually attributed toEduard Heine.) In this setting:limxaf(x)=L{\displaystyle \lim _{x\to a}f(x)=L}if, and only if, for all sequencesxn (with, for alln,xn not equal toa) converging toa the sequencef(xn) converges toL. It was shown bySierpiński in 1916 that proving the equivalence of this definition and the definition above, requires and is equivalent to a weak form of theaxiom of choice. Note that defining what it means for a sequencexn to converge toa requires theepsilon, delta method.

Similarly as it was the case of Weierstrass's definition, a more general Heine definition applies to functions defined onsubsets of the real line. Letf be a real-valued function with the domainDm(f ). Leta be the limit of a sequence of elements ofDm(f ) \ {a}. Then the limit (in this sense) off isL asx approachesa if for every sequencexnDm(f ) \ {a} (so that for alln,xn is not equal toa) that converges toa, the sequencef(xn) converges toL. This is the same as the definition of a sequential limit in the preceding section obtained by regarding the subsetDm(f ) ofR{\displaystyle \mathbb {R} } as a metric space with the induced metric.

In non-standard calculus

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In non-standard calculus the limit of a function is defined by:limxaf(x)=L{\displaystyle \lim _{x\to a}f(x)=L}if and only if for allxR,{\displaystyle x\in \mathbb {R} ^{*},}f(x)L{\displaystyle f^{*}(x)-L} is infinitesimal wheneverxa is infinitesimal. HereR{\displaystyle \mathbb {R} ^{*}} are thehyperreal numbers andf* is the natural extension off to the non-standard real numbers.Keisler proved that such a hyperrealdefinition of limit reduces the quantifier complexity by two quantifiers.[26] On the other hand, Hrbacek writes that for the definitions to be valid for all hyperreal numbers they must implicitly be grounded in the ε-δ method, and claims that, from the pedagogical point of view, the hope that non-standard calculus could be done without ε-δ methods cannot be realized in full.[27] Bŀaszczyk et al. detail the usefulness ofmicrocontinuity in developing a transparent definition ofuniform continuity, and characterize Hrbacek's criticism as a "dubious lament".[28]

In terms of nearness

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At the 1908 international congress of mathematicsF. Riesz introduced an alternate way defining limits and continuity in concept called "nearness".[29] A pointx is defined to be near a setAR{\displaystyle A\subseteq \mathbb {R} } if for everyr > 0 there is a pointaA so that|xa| <r. In this setting thelimxaf(x)=L{\displaystyle \lim _{x\to a}f(x)=L}if and only if for allAR,{\displaystyle A\subseteq \mathbb {R} ,}L is nearf(A) whenevera is nearA.Heref(A) is the set{f(x)|xA}.{\displaystyle \{f(x)|x\in A\}.} This definition can also be extended to metric and topological spaces.

Relationship to continuity

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Main article:Continuous function

The notion of the limit of a function is very closely related to the concept of continuity. A functionf is said to becontinuous atc if it is both defined atc and its value atc equals the limit off asx approachesc:

limxcf(x)=f(c).{\displaystyle \lim _{x\to c}f(x)=f(c).}We have here assumed thatc is alimit point of the domain off.

Properties

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If a functionf is real-valued, then the limit off atp isL if and only if both the right-handed limit and left-handed limit off atp exist and are equal toL.[30]

The functionf iscontinuous atp if and only if the limit off(x) asx approachesp exists and is equal tof(p). Iff :MN is a function between metric spacesM andN, then it is equivalent thatf transforms every sequence inM which converges towardsp into a sequence inN which converges towardsf(p).

IfN is anormed vector space, then the limit operation is linear in the following sense: if the limit off(x) asx approachesp isL and the limit ofg(x) asx approachesp isP, then the limit off(x) + g(x) asx approachesp isL +P. Ifa is a scalar from the basefield, then the limit ofaf(x) asx approachesp isaL.

Iff andg are real-valued (or complex-valued) functions, then taking the limit of an operation onf(x) andg(x) (e.g.,f +g,fg,f ×g,f /g,f g) under certain conditions is compatible with the operation of limits off(x) andg(x). This fact is often called thealgebraic limit theorem. The main condition needed to apply the following rules is that the limits on the right-hand sides of the equations exist (in other words, these limits are finite values including 0). Additionally, the identity for division requires that the denominator on the right-hand side is non-zero (division by 0 is not defined), and the identity for exponentiation requires that the base is positive, or zero while the exponent is positive (finite).

limxp(f(x)+g(x))=limxpf(x)+limxpg(x)limxp(f(x)g(x))=limxpf(x)limxpg(x)limxp(f(x)g(x))=limxpf(x)limxpg(x)limxp(f(x)/g(x))=limxpf(x)/limxpg(x)limxpf(x)g(x)=limxpf(x)limxpg(x){\displaystyle {\begin{array}{lcl}\displaystyle \lim _{x\to p}(f(x)+g(x))&=&\displaystyle \lim _{x\to p}f(x)+\lim _{x\to p}g(x)\\\displaystyle \lim _{x\to p}(f(x)-g(x))&=&\displaystyle \lim _{x\to p}f(x)-\lim _{x\to p}g(x)\\\displaystyle \lim _{x\to p}(f(x)\cdot g(x))&=&\displaystyle \lim _{x\to p}f(x)\cdot \lim _{x\to p}g(x)\\\displaystyle \lim _{x\to p}(f(x)/g(x))&=&\displaystyle {\lim _{x\to p}f(x)/\lim _{x\to p}g(x)}\\\displaystyle \lim _{x\to p}f(x)^{g(x)}&=&\displaystyle {\lim _{x\to p}f(x)^{\lim _{x\to p}g(x)}}\end{array}}}

These rules are also valid for one-sided limits, including whenp is ∞ or −∞. In each rule above, when one of the limits on the right is ∞ or −∞, the limit on the left may sometimes still be determined by the following rules.

q+= if qq×={if q>0if q<0q=0 if q and qq={0if q<0if q>0q={0if 0<q<1if q>1q={if 0<q<10if q>1{\displaystyle {\begin{array}{rcl}q+\infty &=&\infty {\text{ if }}q\neq -\infty \\[8pt]q\times \infty &=&{\begin{cases}\infty &{\text{if }}q>0\\-\infty &{\text{if }}q<0\end{cases}}\\[6pt]\displaystyle {\frac {q}{\infty }}&=&0{\text{ if }}q\neq \infty {\text{ and }}q\neq -\infty \\[6pt]\infty ^{q}&=&{\begin{cases}0&{\text{if }}q<0\\\infty &{\text{if }}q>0\end{cases}}\\[4pt]q^{\infty }&=&{\begin{cases}0&{\text{if }}0<q<1\\\infty &{\text{if }}q>1\end{cases}}\\[4pt]q^{-\infty }&=&{\begin{cases}\infty &{\text{if }}0<q<1\\0&{\text{if }}q>1\end{cases}}\end{array}}}

(see alsoExtended real number line).

In other cases the limit on the left may still exist, although the right-hand side, called anindeterminate form, does not allow one to determine the result. This depends on the functionsf andg. These indeterminate forms are:

00±±0×±+0001±{\displaystyle {\begin{array}{cc}\displaystyle {\frac {0}{0}}&\displaystyle {\frac {\pm \infty }{\pm \infty }}\\[6pt]0\times \pm \infty &\infty +-\infty \\[8pt]\qquad 0^{0}\qquad &\qquad \infty ^{0}\qquad \\[8pt]1^{\pm \infty }\end{array}}}

See furtherL'Hôpital's rule below andIndeterminate form.

Limits of compositions of functions

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In general, from knowing thatlimybf(y)=c{\displaystyle \lim _{y\to b}f(y)=c} andlimxag(x)=b,{\displaystyle \lim _{x\to a}g(x)=b,} it doesnot follow thatlimxaf(g(x))=c.{\displaystyle \lim _{x\to a}f(g(x))=c.} However, this "chain rule" does hold if one of the followingadditional conditions holds:

  • f(b) =c (that is,f is continuous atb), or
  • g does not take the valueb neara (that is, there exists aδ > 0 such that if0 < |xa| <δ then|g(x) −b| > 0).

As an example of this phenomenon, consider the following function that violates both additional restrictions:

f(x)=g(x)={0if x01if x=0{\displaystyle f(x)=g(x)={\begin{cases}0&{\text{if }}x\neq 0\\1&{\text{if }}x=0\end{cases}}}

Since the value atf(0) is aremovable discontinuity,limxaf(x)=0{\displaystyle \lim _{x\to a}f(x)=0} for alla.Thus, the naïve chain rule would suggest that the limit off(f(x)) is 0. However, it is the case thatf(f(x))={1if x00if x=0{\displaystyle f(f(x))={\begin{cases}1&{\text{if }}x\neq 0\\0&{\text{if }}x=0\end{cases}}}and solimxaf(f(x))=1{\displaystyle \lim _{x\to a}f(f(x))=1} for alla.

Limits of special interest

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Main article:List of limits

Rational functions

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Forn a nonnegative integer and constantsa1,a2,a3,,an{\displaystyle a_{1},a_{2},a_{3},\ldots ,a_{n}} andb1,b2,b3,,bn,{\displaystyle b_{1},b_{2},b_{3},\ldots ,b_{n},}

limxa1xn+a2xn1+a3xn2++anb1xn+b2xn1+b3xn2++bn=a1b1{\displaystyle \lim _{x\to \infty }{\frac {a_{1}x^{n}+a_{2}x^{n-1}+a_{3}x^{n-2}+\dots +a_{n}}{b_{1}x^{n}+b_{2}x^{n-1}+b_{3}x^{n-2}+\dots +b_{n}}}={\frac {a_{1}}{b_{1}}}}

This can be proven by dividing both the numerator and denominator byxn. If the numerator is a polynomial of higher degree, the limit does not exist. If the denominator is of higher degree, the limit is 0.

Trigonometric functions

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limx0sinxx=1limx01cosxx=0{\displaystyle {\begin{array}{lcl}\displaystyle \lim _{x\to 0}{\frac {\sin x}{x}}&=&1\\[4pt]\displaystyle \lim _{x\to 0}{\frac {1-\cos x}{x}}&=&0\end{array}}}

Exponential functions

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limx0(1+x)1x=limr(1+1r)r=elimx0ex1x=1limx0eax1bx=ablimx0cax1bx=ablnclimx0+xx=1{\displaystyle {\begin{array}{lcl}\displaystyle \lim _{x\to 0}(1+x)^{\frac {1}{x}}&=&\displaystyle \lim _{r\to \infty }\left(1+{\frac {1}{r}}\right)^{r}=e\\[4pt]\displaystyle \lim _{x\to 0}{\frac {e^{x}-1}{x}}&=&1\\[4pt]\displaystyle \lim _{x\to 0}{\frac {e^{ax}-1}{bx}}&=&\displaystyle {\frac {a}{b}}\\[4pt]\displaystyle \lim _{x\to 0}{\frac {c^{ax}-1}{bx}}&=&\displaystyle {\frac {a}{b}}\ln c\\[4pt]\displaystyle \lim _{x\to 0^{+}}x^{x}&=&1\end{array}}}

Logarithmic functions

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limx0ln(1+x)x=1limx0ln(1+ax)bx=ablimx0logc(1+ax)bx=ablnc{\displaystyle {\begin{array}{lcl}\displaystyle \lim _{x\to 0}{\frac {\ln(1+x)}{x}}&=&1\\[4pt]\displaystyle \lim _{x\to 0}{\frac {\ln(1+ax)}{bx}}&=&\displaystyle {\frac {a}{b}}\\[4pt]\displaystyle \lim _{x\to 0}{\frac {\log _{c}(1+ax)}{bx}}&=&\displaystyle {\frac {a}{b\ln c}}\end{array}}}

L'Hôpital's rule

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Main article:l'Hôpital's rule

This rule usesderivatives to find limits ofindeterminate forms0/0 or±∞/∞, and only applies to such cases. Other indeterminate forms may be manipulated into this form. Given two functionsf(x) andg(x), defined over anopen intervalI containing the desired limit pointc, then if:

  1. limxcf(x)=limxcg(x)=0,{\displaystyle \lim _{x\to c}f(x)=\lim _{x\to c}g(x)=0,} orlimxcf(x)=±limxcg(x)=±,{\displaystyle \lim _{x\to c}f(x)=\pm \lim _{x\to c}g(x)=\pm \infty ,} and
  2. f{\displaystyle f} andg{\displaystyle g} are differentiable overI{c},{\displaystyle I\setminus \{c\},} and
  3. g(x)0{\displaystyle g'(x)\neq 0} for allxI{c},{\displaystyle x\in I\setminus \{c\},} and
  4. limxcf(x)g(x){\displaystyle \lim _{x\to c}{\tfrac {f'(x)}{g'(x)}}} exists,

then:limxcf(x)g(x)=limxcf(x)g(x).{\displaystyle \lim _{x\to c}{\frac {f(x)}{g(x)}}=\lim _{x\to c}{\frac {f'(x)}{g'(x)}}.}

Normally, the first condition is the most important one.

For example:limx0sin(2x)sin(3x)=limx02cos(2x)3cos(3x)=2131=23.{\displaystyle \lim _{x\to 0}{\frac {\sin(2x)}{\sin(3x)}}=\lim _{x\to 0}{\frac {2\cos(2x)}{3\cos(3x)}}={\frac {2\cdot 1}{3\cdot 1}}={\frac {2}{3}}.}

Summations and integrals

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Specifying an infinite bound on a summation or integral is a common shorthand for specifying a limit.

A short way to write the limitlimni=snf(i){\displaystyle \lim _{n\to \infty }\sum _{i=s}^{n}f(i)}isi=sf(i).{\displaystyle \sum _{i=s}^{\infty }f(i).} An important example of limits of sums such as these areseries.

A short way to write the limitlimxaxf(t)dt{\displaystyle \lim _{x\to \infty }\int _{a}^{x}f(t)\;dt}isaf(t)dt.{\displaystyle \int _{a}^{\infty }f(t)\;dt.}

A short way to write the limitlimxxbf(t)dt{\displaystyle \lim _{x\to -\infty }\int _{x}^{b}f(t)\;dt}isbf(t)dt.{\displaystyle \int _{-\infty }^{b}f(t)\;dt.}

See also

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Wikimedia Commons has media related toLimit of a function.

Notes

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  1. ^Felscher, Walter (2000), "Bolzano, Cauchy, Epsilon, Delta",American Mathematical Monthly,107 (9):844–862,doi:10.2307/2695743,JSTOR 2695743
  2. ^Pourciau, Bruce (2001)."Newton and the Notion of Limit".Historia Mathematica.28 (1):18–30.doi:10.1006/hmat.2000.2301.
  3. ^Pourciau, Bruce (2009)."Proposition II (Book I) of Newton's "Principia"".Archive for History of Exact Sciences.63 (2):129–167.doi:10.1007/s00407-008-0033-y.ISSN 0003-9519.JSTOR 41134303.
  4. ^abGrabiner, Judith V. (1983), "Who Gave You the Epsilon? Cauchy and the Origins of Rigorous Calculus",American Mathematical Monthly,90 (3):185–194,doi:10.2307/2975545,JSTOR 2975545, collected inWho Gave You the Epsilon?,ISBN 978-0-88385-569-0 pp. 5–13. Also available at:http://www.maa.org/pubs/Calc_articles/ma002.pdf
  5. ^Sinkevich, G. I. (2017), "Historia epsylontyki",Antiquitates Mathematicae,10, Cornell University,arXiv:1502.06942,doi:10.14708/am.v10i0.805
  6. ^Burton, David M. (1997),The History of Mathematics: An introduction (Third ed.), New York: McGraw–Hill, pp. 558–559,ISBN 978-0-07-009465-9
  7. ^Miller, Jeff (1 December 2004),Earliest Uses of Symbols of Calculus, retrieved18 December 2008
  8. ^Varberg, Dale E.; Purcell, Edwin J.; Rigdon, Steven E. (2007),Calculus (9th ed.),Pearson Prentice Hall, p. 57,ISBN 978-0131469686
  9. ^abSwokowski, Earl W. (1979),Calculus with Analytic Geometry (2nd ed.), Taylor & Francis, p. 58,ISBN 978-0-87150-268-1
  10. ^Swokowski (1979), p. 72–73.
  11. ^(Bartle & Sherbert 2000)
  12. ^abBartle (1967)
  13. ^Hubbard (2015)
  14. ^For example,Apostol (1974),Courant (1924),Hardy (1921),Rudin (1964),Whittaker & Watson (1904) all take "limit" to mean the deleted limit.
  15. ^For example,Limit atEncyclopedia of Mathematics
  16. ^Stewart, James (2020), "Chapter 14.2 Limits and Continuity",Multivariable Calculus (9th ed.), Cengage Learning, p. 952,ISBN 9780357042922
  17. ^Stewart (2020), p. 953.
  18. ^abcZakon, Elias (2011), "Chapter 4. Function Limits and Continuity",Mathematical Anaylysis, Volume I, University of Windsor, pp. 219–220,ISBN 9781617386473
  19. ^abZakon (2011), p. 220.
  20. ^Zakon (2011), p. 223.
  21. ^Taylor, Angus E. (2012),General Theory of Functions and Integration, Dover Books on Mathematics Series, pp. 139–140,ISBN 9780486152141
  22. ^Rudin, W. (1986),Principles of mathematical analysis, McGraw - Hill Book C, p. 84,OCLC 962920758
  23. ^abHartman, Gregory (2019),The Calculus of Vector-Valued Functions II, retrieved31 October 2022
  24. ^Zakon (2011), p. 172.
  25. ^Rudin, W (1986),Principles of mathematical analysis, McGraw - Hill Book C, pp. 150–151,OCLC 962920758
  26. ^Keisler, H. Jerome (2008),"Quantifiers in limits"(PDF),Andrzej Mostowski and foundational studies, IOS, Amsterdam, pp. 151–170
  27. ^Hrbacek, K. (2007), "Stratified Analysis?", in Van Den Berg, I.; Neves, V. (eds.),The Strength of Nonstandard Analysis, Springer
  28. ^Bŀaszczyk, Piotr;Katz, Mikhail; Sherry, David (2012), "Ten misconceptions from the history of analysis and their debunking",Foundations of Science,18 (1):43–74,arXiv:1202.4153,doi:10.1007/s10699-012-9285-8,S2CID 119134151
  29. ^F. Riesz (7 April 1908), "Stetigkeitsbegriff und abstrakte Mengenlehre (The Concept of Continuity and Abstract Set Theory)",1908 International Congress of Mathematicians
  30. ^Swokowski (1979), p. 73.

References

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  • Apostol, Tom M. (1974).Mathematical Analysis (2 ed.). Addison–Wesley.ISBN 0-201-00288-4.
  • Bartle, Robert (1967).The elements of real analysis. Wiley.
  • Bartle, Robert G.; Sherbert, Donald R. (2000).Introduction to real analysis. Wiley.
  • Courant, Richard (1924).Vorlesungen über Differential- und Integralrechnung (in German). Springer.
  • Hardy, G. H. (1921).A course in pure mathematics. Cambridge University Press.
  • Hubbard, John H. (2015).Vector calculus, linear algebra, and differential forms: A unified approach (5th ed.). Matrix Editions.
  • Page, Warren; Hersh, Reuben; Selden, Annie; et al., eds. (2002). "Media Highlights".The College Mathematics.33 (2):147–154.JSTOR 2687124..
  • Rudin, Walter (1964).Principles of mathematical analysis. McGraw-Hill.
  • Sutherland, W. A. (1975).Introduction to Metric and Topological Spaces. Oxford: Oxford University Press.ISBN 0-19-853161-3.
  • Whittaker;Watson (1904).A Course of Modern Analysis. Cambridge University Press.

External links

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