x |
| |||
---|---|---|---|---|
1 | 0.841471... | |||
0.1 | 0.998334... | |||
0.01 | 0.999983... |
Although the function is not defined at zero, as becomes closer and closer to zero, becomes arbitrarily close to 1. In other words, the limit of as approaches zero, equals 1.
In mathematics, the limit of a function is a fundamental concept in calculus and analysis concerning the behavior of that function near a particular input which may or may not be in the domain of the function.
Formal definitions, first devised in the early 19th century, are given below. Informally, a function assigns an output to every input . We say that the function has a limit at an input, if gets closer and closer to as moves closer and closer to . More specifically, the output value can be made arbitrarily close to if the input to is taken sufficiently close to . On the other hand, if some inputs very close to are taken to outputs that stay a fixed distance apart, then we say the limit does not exist.
The notion of a limit has many applications in modern calculus. In particular, the many definitions of continuity 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 the derivative: in the calculus of one variable, this is the limiting value of the slope of secant lines to the graph of a function.
Although implicit in the development of calculus of the 17th and 18th centuries, the modern idea of the limit of a function goes back to 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.
In his 1821 book French: [[Cours d'analyse]], Augustin-Louis Cauchy discussed variable quantities, infinitesimals and limits, and defined continuity of
y=f(x)
The modern notation of placing the arrow below the limit symbol is due to Hardy, which is introduced in his book A Course of Pure Mathematics in 1908.
Imagine a person walking on a landscape represented by the graph . Their horizontal position is given by, much like the position given by a map of the land or by a global positioning system. Their altitude is given by the coordinate . Suppose they walk towards a position, as they get closer and closer to this point, they will notice that their altitude approaches a specific value . If asked about the altitude corresponding to, they would reply by saying .
What, then, does it mean to say, their altitude is approaching ? It means that their altitude gets nearer and nearer to —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 of . They report back that indeed, they can get within ten vertical meters of, arguing that as long as they are within fifty horizontal meters of, their altitude is always within ten meters of .
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 of, their altitude will always remain within one meter from the target altitude . Summarizing the aforementioned concept we can say that the traveler's altitude approaches as their horizontal position approaches, so as to say that for every target accuracy goal, however small it may be, there is some neighbourhood of where all (not just some) altitudes correspond to all the horizontal positions, except maybe the horizontal position itself, in that neighbourhood fulfill that accuracy goal.
The initial informal statement can now be explicated:
In fact, this explicit statement is quite close to the formal definition of the limit of a function, with values in a topological space.
More specifically, to say that
is to say that can be made as close to as desired, by making close enough, but not equal, to .
The following definitions, known as -definitions, are the generally accepted definitions for the limit of a function in various contexts.
Suppose
f:\R → \R
or alternatively, say tends to as tends to , and written:
if the following property holds: for every real, there exists a real such that for all real, implies . Symbolically,
For example, we may saybecause for every real, we can take, so that for all real, if, then .
A more general definition applies for functions defined on subsets of the real line. Let be a subset of Let
f:S\to\R
(a,p)\cup(p,b)\subsetS.
Or, symbolically:
For example, we may saybecause for every real, we can take, so that for all real, if, then . In this example, contains open intervals around the point 1 (for example, the interval (0, 2)).
Here, note that the value of the limit does not depend on being defined at, nor on the value —if it is defined. For example, let
f:[0,1)\cup(1,2]\to\R,f(x)=\tfrac{2x2-x-1}{x-1}.
In fact, a limit can exist in
\{x\in\R|\exists(a,b)\subset\R p\in(a,b)and(a,p)\cup(p,b)\subsetS\},
\operatorname{int}S\cup\operatorname{iso}Sc,
S=[0,1)\cup(1,2],
\operatorname{int}S=(0,1)\cup(1,2),
\operatorname{iso}Sc=\{1\}.
The letters and can be understood as "error" and "distance". In fact, Cauchy used as an abbreviation for "error" in some of his work, though in his definition of continuity, he used an infinitesimal
\alpha
See main article: One-sided limit.
Alternatively, may approach from above (right) or below (left), in which case the limits may be written as
or
respectively. If these limits exist at p and are equal there, then this can be referred to as the limit of at . If the one-sided limits exist at, but are unequal, then there is no limit at (i.e., the limit at does not exist). If either one-sided limit does not exist at, then the limit at also does not exist.
A formal definition is as follows. The limit of as approaches from above is if:
For every, there exists a such that whenever, we have .
The limit of as approaches from below is if:
For every, there exists a such that whenever, we have .
If the limit does not exist, then the oscillation of at is non-zero.
Limits can also be defined by approaching from subsets of the domain.
In general: Let
f:S\to\R
S\subseteq\R.
T\subsetS
f(x)=\sqrtx
This definition allows a limit to be defined at limit points of the domain, if a suitable subset which has the same limit point is chosen.
Notably, the previous two-sided definition works on
\operatorname{int}S\cup\operatorname{iso}Sc,
For example, let
S=[0,1)\cup(1,2].
1\in\operatorname{iso}Sc=\{1\},
The definition of limit given here does not depend on how (or whether) is defined at . Bartle refers to this as a deleted limit, because it excludes the value of at . The corresponding non-deleted limit does depend on the value of at, if is in the domain of . Let
f:S\to\R
The definition is the same, except that the neighborhood now includes the point, in contrast to the deleted neighborhood . 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 the theorem about limits of compositions without any constraints on the functions (other than the existence of their non-deleted limits).
Bartle notes that although by "limit" some authors do mean this non-deleted limit, deleted limits are the most popular.[2]
The function has no limit at (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 other -coordinate.
The function (a.k.a., the Dirichlet function) has no limit at any -coordinate.
The function has a limit at every non-zero -coordinate (the limit equals 1 for negative and equals 2 for positive). The limit at does not exist (the left-hand limit equals 1, whereas the right-hand limit equals 2).
The functionsandboth have a limit at and it equals 0.
The function has a limit at any -coordinate of the form
\tfrac{\pi}{2}+2n\pi,
Let
f:S\to\R
S\subseteq\R.
means that:
Similarly, the limit of as approaches minus infinity is , denoted
means that:
For example, because for every, we can take such that for all real, if, then .
Another example is thatbecause for every, we can take such that for all real, if, then .
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.
Let
f:S\toR
S\subseteqR.
means that:
The statement the limit of as approaches is minus infinity, denoted
means that:
For example,because for every, we can take such that for all real, if, then .
These ideas can be used together to produce definitions for different combinations, such as
or
\lim | |
x\top+ |
f(x)=-infty.
For example,because for every, we can take such that for all real, if, then .
Limits involving infinity are connected with the concept of asymptotes.
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, is a topological space and any function of the form
f:X\toY
X,Y\subseteq\overline\R
Many authors[3] allow for the projectively extended real line to be used as a way to include infinite values as well as extended real line. With this notation, the extended real line is given as and the projectively extended real line is where a neighborhood of ∞ is a set of the form
\{x:|x|>c\}.
x-1
In contrast, when working with the projective real line, infinities (much like 0) are unsigned, so, the central limit does exist in that context:
In fact there are a plethora of conflicting formal systems in use.In certain applications of numerical differentiation and integration, it is, for example, convenient to have signed zeroes. A simple reason has to do with the converse of
\lim | |
x\to0- |
{x-1
\limx{x-1
f(x)=\tfrac{p(x)}{q(x)}
If the limit at infinity exists, it represents a horizontal asymptote at . Polynomials do not have horizontal asymptotes; such asymptotes may however occur with rational functions.
By noting that represents a distance, the definition of a limit can be extended to functions of more than one variable. In the case of a function
f:S x T\to\R
S x T\subseteq\R2,
if the following condition holds:
For every, there exists a such that for all in and in, whenever we have,
or formally:
Here is the Euclidean distance between and . (This can in fact be replaced by any norm, and be extended to any number of variables.)
For example, we may saybecause for every, we can take such that for all real and real, if then .
Similar to the case in single variable, the value of at does not matter in this definition of limit.
For such a multivariable limit to exist, this definition requires the value of approaches along every possible path approaching . In the above example, the functionsatisfies this condition. This can be seen by considering the polar coordinates which givesHere is a function of r which controls the shape of the path along which is approaching . Since is bounded between [−1, 1], by the sandwich theorem, this limit tends to 0.
In contrast, the functiondoes not have a limit at . Taking the path, we obtainwhile taking the path, we obtain
Since the two values do not agree, does not tend to a single value as approaches .
Although less commonly used, there is another type of limit for a multivariable function, known as the multiple limit. For a two-variable function, this is the double limit. Let
f:S x T\to\R
S x T\subseteq\R2,
if the following condition holds:
For such a double limit to exist, this definition requires the value of approaches along every possible path approaching, excluding the two lines and . As a result, the multiple limit is a weaker notion than the ordinary limit: if the ordinary limit exists and equals, then the multiple limit exists and also equals . The converse is not true: the existence of the multiple limits does not imply the existence of the ordinary limit. Consider the examplewherebut does not exist.
If the domain of is restricted to
(S\setminus\{p\}) x (T\setminus\{q\}),
The concept of multiple limit can extend to the limit at infinity, in a way similar to that of a single variable function. For
f:S x T\to\R,
if the following condition holds:
We say the double limit of as and approaches minus infinity is , written
if the following condition holds:
See main article: Pointwise convergence and Uniform convergence.
Let
f:S x T\to\R.
g:T\to\R.
Alternatively, we may say tends to pointwise as approaches , denoted or
This limit exists if the following holds:
Here, is a function of both and . Each is chosen for a specific point of . Hence we say the limit is pointwise in . For example,has a pointwise limit of constant zero functionbecause for every fixed, the limit is clearly 0. This argument fails if is not fixed: if is very close to, the value of the fraction may deviate from 0.
This leads to another definition of limit, namely the uniform limit. We say the uniform limit of on as approaches is , denoted or
Alternatively, we may say tends to uniformly on as approaches , denoted or
This limit exists if the following holds:
Here, is a function of only but not . In other words, δ is uniformly applicable to all in . Hence we say the limit is uniform in . For example,has a uniform limit of constant zero functionbecause for all real, is bounded between . Hence no matter how behaves, we may use the sandwich theorem to show that the limit is 0.
See main article: Iterated limits.
Let
f:S x T\to\R.
g:T\to\R,
This limit is known as iterated limit of the multivariable function. The order of taking limits may affect the result, i.e.,
in general.
A sufficient condition of equality is given by the Moore-Osgood theorem, which requires the limit
\limxf(x,y)=g(y)
Suppose and are subsets of metric spaces and, respectively, and is defined between and, with, a limit point of and . It is said that the limit of as approaches is and write
if the following property holds:
Again, note that need not be in the domain of, nor does need to be in the range of, and even if is defined it need not be equal to .
The limit in Euclidean space is a direct generalization of limits to vector-valued functions. For example, we may consider a function
f:S x T\to\R3
In this example, the function concerned are finite-dimension vector-valued function. In this case, the limit 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:
One might also want to consider spaces other than Euclidean space. An example would be the Manhattan space. Consider
f:S\to\R2
Since this is also a finite-dimension vector-valued function, the limit theorem stated above also applies.
Finally, we will discuss the limit in function space, which has infinite dimensions. Consider a function in the function space
S x T\to\R.
T\to\R.
if the following holds:
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.
Suppose and are topological spaces with a Hausdorff space. Let be a limit point of, and . For a function, it is said that the limit of as approaches is , written
if the following property holds:
This last part of the definition can also be phrased "there exists an open punctured neighbourhood of such that ".
The domain of does not need to contain . If it does, then the value of at is irrelevant to the definition of the limit. In particular, if the domain of is (or all of), then the limit of as exists and is equal to if, for all subsets of with limit point, the limit of the restriction of to exists and is equal to . Sometimes this criterion is used to establish the non-existence of the two-sided limit of a function on by showing that the one-sided limits either fail to exist or do not agree. Such a view is fundamental in the field of general topology, where limits and continuity at a point are defined in terms of special families of subsets, called filters, or generalized sequences known as nets.
Alternatively, the requirement that be a Hausdorff space can be relaxed to the assumption that be a general topological space, but then the limit of a function may not be unique. In particular, one can no longer talk about the limit of a function at a point, but rather a limit or the set of limits at a point.
A function is continuous at a limit point of and in its domain if and only if is the (or, in the general case, a) limit of as tends to .
There is another type of limit of a function, namely the sequential limit. Let be a mapping from a topological space into a Hausdorff space, a limit point of and . The sequential limit of as tends to is if
For every sequence in that converges to, the sequence converges to .
If is the limit (in the sense above) of as approaches, then it is a sequential limit as well, however the converse need not hold in general. If in addition is metrizable, then is the sequential limit of as approaches if and only if it is the limit (in the sense above) of as approaches .
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 to Eduard Heine.) In this setting:if, and only if, for all sequences (with not equal to for all) converging to the sequence converges to . It was shown by Sierpiński in 1916 that proving the equivalence of this definition and the definition above, requires and is equivalent to a weak form of the axiom of choice. Note that defining what it means for a sequence to converge to requires the epsilon, delta method.
Similarly as it was the case of Weierstrass's definition, a more general Heine definition applies to functions defined on subsets of the real line. Let be a real-valued function with the domain . Let be the limit of a sequence of elements of Then the limit (in this sense) of is as approaches if for every sequence (so that for all, is not equal to) that converges to, the sequence converges to . This is the same as the definition of a sequential limit in the preceding section obtained by regarding the subset of as a metric space with the induced metric.
In non-standard calculus the limit of a function is defined by:if and only if for all
x\in\R*,
f*(x)-L
\R*
At the 1908 international congress of mathematics F. Riesz introduced an alternate way defining limits and continuity in concept called "nearness". A point is defined to be near a set
A\subseteq\R
A\subseteq\R,
\{f(x)|x\inA\}.
See main article: Continuous function.
The notion of the limit of a function is very closely related to the concept of continuity. A function is said to be continuous at if it is both defined at and its value at equals the limit of as approaches :
We have here assumed that is a limit point of the domain of .
If a function is real-valued, then the limit of at is if and only if both the right-handed limit and left-handed limit of at exist and are equal to .
The function is continuous at if and only if the limit of as approaches exists and is equal to . If is a function between metric spaces and, then it is equivalent that transforms every sequence in which converges towards into a sequence in which converges towards .
If is a normed vector space, then the limit operation is linear in the following sense: if the limit of as approaches is and the limit of as approaches is, then the limit of as approaches is . If is a scalar from the base field, then the limit of as approaches is .
If and are real-valued (or complex-valued) functions, then taking the limit of an operation on and (e.g.,,,,,) under certain conditions is compatible with the operation of limits of and . This fact is often called the algebraic 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).
These rules are also valid for one-sided limits, including when 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.
(see also Extended real number line).
In other cases the limit on the left may still exist, although the right-hand side, called an indeterminate form, does not allow one to determine the result. This depends on the functions and . These indeterminate forms are:
See further L'Hôpital's rule below and Indeterminate form.
In general, from knowing that
\limyf(y)=c
\limxg(x)=b,
\limxf(g(x))=c.
As an example of this phenomenon, consider the following function that violates both additional restrictions:
Since the value at is a removable discontinuity, for all .Thus, the naïve chain rule would suggest that the limit of is 0. However, it is the case thatand so for all .
See main article: List of limits.
For a nonnegative integer and constants
a1,a2,a3,\ldots,an
b1,b2,b3,\ldots,bn,
This can be proven by dividing both the numerator and denominator by . 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.
This rule uses derivatives to find limits of indeterminate forms or, and only applies to such cases. Other indeterminate forms may be manipulated into this form. Given two functions and, defined over an open interval containing the desired limit point, then if:
\limxf(x)=\limxg(x)=0,
\limxf(x)=\pm\limxg(x)=\pminfty,
f
g
I\setminus\{c\},
g'(x) ≠ 0
x\inI\setminus\{c\},
\limx\to\tfrac{f'(x)}{g'(x)}
Normally, the first condition is the most important one.
For example:
\limx
\sin(2x) | |
\sin(3x) |
= \limx
2\cos(2x) | = | |
3\cos(3x) |
2\sdot1 | = | |
3\sdot1 |
2 | |
3 |
.
Specifying an infinite bound on a summation or integral is a common shorthand for specifying a limit.
A short way to write the limit
\limn
n | |
\sum | |
i=s |
f(i)
infty | |
\sum | |
i=s |
f(i).
A short way to write the limit
\limx
x | |
\int | |
a |
f(t) dt
infty | |
\int | |
a |
f(t) dt.
A short way to write the limit
\limx
b | |
\int | |
x |
f(t) dt
b | |
\int | |
-infty |
f(t) dt.