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One-sided limit

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(Redirected from One sided limit) Limit of a function approaching a value point from values below or above the value point
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The function f ( x ) = x 2 + sign ( x ) , {\displaystyle f(x)=x^{2}+\operatorname {sign} (x),} where sign ( x ) {\displaystyle \operatorname {sign} (x)} denotes the sign function, has a left limit of 1 , {\displaystyle -1,} a right limit of + 1 , {\displaystyle +1,} and a function value of 0 {\displaystyle 0} at the point x = 0. {\displaystyle x=0.}

In calculus, a one-sided limit refers to either one of the two limits of a function f ( x ) {\displaystyle f(x)} of a real variable x {\displaystyle x} as x {\displaystyle x} approaches a specified point either from the left or from the right.

The limit as x {\displaystyle x} decreases in value approaching a {\displaystyle a} ( x {\displaystyle x} approaches a {\displaystyle a} "from the right" or "from above") can be denoted:

lim x a + f ( x )  or  lim x a f ( x )  or  lim x a f ( x )  or  f ( x + ) {\displaystyle \lim _{x\to a^{+}}f(x)\quad {\text{ or }}\quad \lim _{x\,\downarrow \,a}\,f(x)\quad {\text{ or }}\quad \lim _{x\searrow a}\,f(x)\quad {\text{ or }}\quad f(x+)}

The limit as x {\displaystyle x} increases in value approaching a {\displaystyle a} ( x {\displaystyle x} approaches a {\displaystyle a} "from the left" or "from below") can be denoted:

lim x a f ( x )  or  lim x a f ( x )  or  lim x a f ( x )  or  f ( x ) {\displaystyle \lim _{x\to a^{-}}f(x)\quad {\text{ or }}\quad \lim _{x\,\uparrow \,a}\,f(x)\quad {\text{ or }}\quad \lim _{x\nearrow a}\,f(x)\quad {\text{ or }}\quad f(x-)}

If the limit of f ( x ) {\displaystyle f(x)} as x {\displaystyle x} approaches a {\displaystyle a} exists then the limits from the left and from the right both exist and are equal. In some cases in which the limit lim x a f ( x ) {\displaystyle \lim _{x\to a}f(x)} does not exist, the two one-sided limits nonetheless exist. Consequently, the limit as x {\displaystyle x} approaches a {\displaystyle a} is sometimes called a "two-sided limit".

It is possible for exactly one of the two one-sided limits to exist (while the other does not exist). It is also possible for neither of the two one-sided limits to exist.

Formal definition

Definition

If I {\displaystyle I} represents some interval that is contained in the domain of f {\displaystyle f} and if a {\displaystyle a} is a point in I {\displaystyle I} then the right-sided limit as x {\displaystyle x} approaches a {\displaystyle a} can be rigorously defined as the value R {\displaystyle R} that satisfies: for all  ε > 0  there exists some  δ > 0  such that for all  x I ,  if  0 < x a < δ  then  | f ( x ) R | < ε , {\displaystyle {\text{for all }}\varepsilon >0\;{\text{ there exists some }}\delta >0\;{\text{ such that for all }}x\in I,{\text{ if }}\;0<x-a<\delta {\text{ then }}|f(x)-R|<\varepsilon ,} and the left-sided limit as x {\displaystyle x} approaches a {\displaystyle a} can be rigorously defined as the value L {\displaystyle L} that satisfies: for all  ε > 0  there exists some  δ > 0  such that for all  x I ,  if  0 < a x < δ  then  | f ( x ) L | < ε . {\displaystyle {\text{for all }}\varepsilon >0\;{\text{ there exists some }}\delta >0\;{\text{ such that for all }}x\in I,{\text{ if }}\;0<a-x<\delta {\text{ then }}|f(x)-L|<\varepsilon .}

We can represent the same thing more symbolically, as follows.

Let I {\displaystyle I} represent an interval, where I d o m a i n ( f ) {\displaystyle I\subseteq \mathrm {domain} (f)} , and a I {\displaystyle a\in I} .

lim x a + f ( x ) = R             ( ε R + , δ R + , x I , ( 0 < x a < δ | f ( x ) R | < ε ) ) {\displaystyle \lim _{x\to a^{+}}f(x)=R~~~\iff ~~~(\forall \varepsilon \in \mathbb {R} _{+},\exists \delta \in \mathbb {R} _{+},\forall x\in I,(0<x-a<\delta \longrightarrow |f(x)-R|<\varepsilon ))}
lim x a f ( x ) = L             ( ε R + , δ R + , x I , ( 0 < a x < δ | f ( x ) L | < ε ) ) {\displaystyle \lim _{x\to a^{-}}f(x)=L~~~\iff ~~~(\forall \varepsilon \in \mathbb {R} _{+},\exists \delta \in \mathbb {R} _{+},\forall x\in I,(0<a-x<\delta \longrightarrow |f(x)-L|<\varepsilon ))}

Intuition

In comparison to the formal definition for the limit of a function at a point, the one-sided limit (as the name would suggest) only deals with input values to one side of the approached input value.

For reference, the formal definition for the limit of a function at a point is as follows:

lim x a f ( x ) = L             ε R + , δ R + , x I , 0 < | x a | < δ | f ( x ) L | < ε . {\displaystyle \lim _{x\to a}f(x)=L~~~\iff ~~~\forall \varepsilon \in \mathbb {R} _{+},\exists \delta \in \mathbb {R} _{+},\forall x\in I,0<|x-a|<\delta \implies |f(x)-L|<\varepsilon .}

To define a one-sided limit, we must modify this inequality. Note that the absolute distance between x {\displaystyle x} and a {\displaystyle a} is

| x a | = | ( 1 ) ( x + a ) | = | ( 1 ) ( a x ) | = | ( 1 ) | | a x | = | a x | . {\displaystyle |x-a|=|(-1)(-x+a)|=|(-1)(a-x)|=|(-1)||a-x|=|a-x|.}

For the limit from the right, we want x {\displaystyle x} to be to the right of a {\displaystyle a} , which means that a < x {\displaystyle a<x} , so x a {\displaystyle x-a} is positive. From above, x a {\displaystyle x-a} is the distance between x {\displaystyle x} and a {\displaystyle a} . We want to bound this distance by our value of δ {\displaystyle \delta } , giving the inequality x a < δ {\displaystyle x-a<\delta } . Putting together the inequalities 0 < x a {\displaystyle 0<x-a} and x a < δ {\displaystyle x-a<\delta } and using the transitivity property of inequalities, we have the compound inequality 0 < x a < δ {\displaystyle 0<x-a<\delta } .

Similarly, for the limit from the left, we want x {\displaystyle x} to be to the left of a {\displaystyle a} , which means that x < a {\displaystyle x<a} . In this case, it is a x {\displaystyle a-x} that is positive and represents the distance between x {\displaystyle x} and a {\displaystyle a} . Again, we want to bound this distance by our value of δ {\displaystyle \delta } , leading to the compound inequality 0 < a x < δ {\displaystyle 0<a-x<\delta } .

Now, when our value of x {\displaystyle x} is in its desired interval, we expect that the value of f ( x ) {\displaystyle f(x)} is also within its desired interval. The distance between f ( x ) {\displaystyle f(x)} and L {\displaystyle L} , the limiting value of the left sided limit, is | f ( x ) L | {\displaystyle |f(x)-L|} . Similarly, the distance between f ( x ) {\displaystyle f(x)} and R {\displaystyle R} , the limiting value of the right sided limit, is | f ( x ) R | {\displaystyle |f(x)-R|} . In both cases, we want to bound this distance by ε {\displaystyle \varepsilon } , so we get the following: | f ( x ) L | < ε {\displaystyle |f(x)-L|<\varepsilon } for the left sided limit, and | f ( x ) R | < ε {\displaystyle |f(x)-R|<\varepsilon } for the right sided limit.

Examples

Example 1: The limits from the left and from the right of g ( x ) := 1 x {\displaystyle g(x):=-{\frac {1}{x}}} as x {\displaystyle x} approaches a := 0 {\displaystyle a:=0} are lim x 0 1 / x = +  and  lim x 0 + 1 / x = {\displaystyle \lim _{x\to 0^{-}}{-1/x}=+\infty \qquad {\text{ and }}\qquad \lim _{x\to 0^{+}}{-1/x}=-\infty } The reason why lim x 0 1 / x = + {\displaystyle \lim _{x\to 0^{-}}{-1/x}=+\infty } is because x {\displaystyle x} is always negative (since x 0 {\displaystyle x\to 0^{-}} means that x 0 {\displaystyle x\to 0} with all values of x {\displaystyle x} satisfying x < 0 {\displaystyle x<0} ), which implies that 1 / x {\displaystyle -1/x} is always positive so that lim x 0 1 / x {\displaystyle \lim _{x\to 0^{-}}{-1/x}} diverges to + {\displaystyle +\infty } (and not to {\displaystyle -\infty } ) as x {\displaystyle x} approaches 0 {\displaystyle 0} from the left. Similarly, lim x 0 + 1 / x = {\displaystyle \lim _{x\to 0^{+}}{-1/x}=-\infty } since all values of x {\displaystyle x} satisfy x > 0 {\displaystyle x>0} (said differently, x {\displaystyle x} is always positive) as x {\displaystyle x} approaches 0 {\displaystyle 0} from the right, which implies that 1 / x {\displaystyle -1/x} is always negative so that lim x 0 + 1 / x {\displaystyle \lim _{x\to 0^{+}}{-1/x}} diverges to . {\displaystyle -\infty .}

Plot of the function 1 / ( 1 + 2 1 / x ) . {\displaystyle 1/(1+2^{-1/x}).}

Example 2: One example of a function with different one-sided limits is f ( x ) = 1 1 + 2 1 / x , {\displaystyle f(x)={\frac {1}{1+2^{-1/x}}},} (cf. picture) where the limit from the left is lim x 0 f ( x ) = 0 {\displaystyle \lim _{x\to 0^{-}}f(x)=0} and the limit from the right is lim x 0 + f ( x ) = 1. {\displaystyle \lim _{x\to 0^{+}}f(x)=1.} To calculate these limits, first show that lim x 0 2 1 / x =  and  lim x 0 + 2 1 / x = 0 {\displaystyle \lim _{x\to 0^{-}}2^{-1/x}=\infty \qquad {\text{ and }}\qquad \lim _{x\to 0^{+}}2^{-1/x}=0} (which is true because lim x 0 1 / x = +  and  lim x 0 + 1 / x = {\displaystyle \lim _{x\to 0^{-}}{-1/x}=+\infty {\text{ and }}\lim _{x\to 0^{+}}{-1/x}=-\infty } ) so that consequently, lim x 0 + 1 1 + 2 1 / x = 1 1 + lim x 0 + 2 1 / x = 1 1 + 0 = 1 {\displaystyle \lim _{x\to 0^{+}}{\frac {1}{1+2^{-1/x}}}={\frac {1}{1+\displaystyle \lim _{x\to 0^{+}}2^{-1/x}}}={\frac {1}{1+0}}=1} whereas lim x 0 1 1 + 2 1 / x = 0 {\displaystyle \lim _{x\to 0^{-}}{\frac {1}{1+2^{-1/x}}}=0} because the denominator diverges to infinity; that is, because lim x 0 1 + 2 1 / x = . {\displaystyle \lim _{x\to 0^{-}}1+2^{-1/x}=\infty .} Since lim x 0 f ( x ) lim x 0 + f ( x ) , {\displaystyle \lim _{x\to 0^{-}}f(x)\neq \lim _{x\to 0^{+}}f(x),} the limit lim x 0 f ( x ) {\displaystyle \lim _{x\to 0}f(x)} does not exist.

Relation to topological definition of limit

See also: Filters in topology

The one-sided limit to a point p {\displaystyle p} corresponds to the general definition of limit, with the domain of the function restricted to one side, by either allowing that the function domain is a subset of the topological space, or by considering a one-sided subspace, including p . {\displaystyle p.} Alternatively, one may consider the domain with a half-open interval topology.

Abel's theorem

Main article: Abel's Theorem

A noteworthy theorem treating one-sided limits of certain power series at the boundaries of their intervals of convergence is Abel's theorem.

Notes

  1. A limit that is equal to {\displaystyle \infty } is said to diverge to {\displaystyle \infty } rather than converge to . {\displaystyle \infty .} The same is true when a limit is equal to . {\displaystyle -\infty .}

References

  1. ^ "One-sided limit - Encyclopedia of Mathematics". encyclopediaofmath.org. Retrieved 7 August 2021.
  2. ^ Fridy, J. A. (24 January 2020). Introductory Analysis: The Theory of Calculus. Gulf Professional Publishing. p. 48. ISBN 978-0-12-267655-0. Retrieved 7 August 2021.
  3. Hasan, Osman; Khayam, Syed (2014-01-02). "Towards Formal Linear Cryptanalysis using HOL4" (PDF). Journal of Universal Computer Science. 20 (2): 209. doi:10.3217/jucs-020-02-0193. ISSN 0948-6968.
  4. Gasic, Andrei G. (2020-12-12). Phase Phenomena of Proteins in Living Matter (Thesis thesis).
  5. Brokate, Martin; Manchanda, Pammy; Siddiqi, Abul Hasan (2019), "Limit and Continuity", Calculus for Scientists and Engineers, Industrial and Applied Mathematics, Singapore: Springer Singapore, pp. 39–53, doi:10.1007/978-981-13-8464-6_2, ISBN 978-981-13-8463-9, S2CID 201484118, retrieved 2022-01-11
  6. Giv, Hossein Hosseini (28 September 2016). Mathematical Analysis and Its Inherent Nature. American Mathematical Soc. p. 130. ISBN 978-1-4704-2807-5. Retrieved 7 August 2021.

See also

Calculus
Precalculus
Limits
Differential calculus
Integral calculus
Vector calculus
Multivariable calculus
Sequences and series
Special functions
and numbers
History of calculus
Lists
Integrals
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