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Function of a real variable

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Inmathematical analysis, and applications ingeometry,applied mathematics,engineering, andnatural sciences, afunction of a real variable is afunction whosedomain is thereal numbersR{\displaystyle \mathbb {R} }, or asubset ofR{\displaystyle \mathbb {R} } that contains aninterval of positive length. Most real functions that are considered and studied aredifferentiable in some interval.The most widely considered such functions are thereal functions, which are thereal-valued functions of a real variable, that is, the functions of a real variable whosecodomain is the set of real numbers.

Nevertheless, the codomain of a function of a real variable may be any set. However, it is often assumed to have a structure ofR{\displaystyle \mathbb {R} }-vector space over the reals. That is, the codomain may be aEuclidean space, acoordinate vector, the set ofmatrices of real numbers of a given size, or anR{\displaystyle \mathbb {R} }-algebra, such as thecomplex numbers or thequaternions. The structureR{\displaystyle \mathbb {R} }-vector space of the codomain induces a structure ofR{\displaystyle \mathbb {R} }-vector space on the functions. If the codomain has a structure ofR{\displaystyle \mathbb {R} }-algebra, the same is true for the functions.

Theimage of a function of a real variable is acurve in the codomain. In this context, a function that defines curve is called aparametric equation of the curve.

When the codomain of a function of a real variable is afinite-dimensional vector space, the function may be viewed as a sequence of real functions. This is often used in applications.

Real function

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The graph of a real function

A real function is afunction from a subset ofR{\displaystyle \mathbb {R} } toR,{\displaystyle \mathbb {R} ,} whereR{\displaystyle \mathbb {R} } denotes as usual the set ofreal numbers. That is, thedomain of a real function is a subsetR{\displaystyle \mathbb {R} }, and itscodomain isR.{\displaystyle \mathbb {R} .} It is generally assumed that the domain contains aninterval of positive length.

Basic examples

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For many commonly used real functions, the domain is the whole set of real numbers, and the function iscontinuous anddifferentiable at every point of the domain. One says that these functions are defined, continuous and differentiable everywhere. This is the case of:

Some functions are defined everywhere, but not continuous at some points. For example

Some functions are defined and continuous everywhere, but not everywhere differentiable. For example

  • Theabsolute value is defined and continuous everywhere, and is differentiable everywhere, except for zero.
  • Thecubic root is defined and continuous everywhere, and is differentiable everywhere, except for zero.

Many common functions are not defined everywhere, but are continuous and differentiable everywhere where they are defined. For example:

Some functions are continuous in their whole domain, and not differentiable at some points. This is the case of:

  • Thesquare root is defined only for nonnegative values of the variable, and not differentiable at 0 (it is differentiable for all positive values of the variable).

General definition

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Areal-valued function of a real variable is afunction that takes as input areal number, commonly represented by thevariablex, for producing another real number, thevalue of the function, commonly denotedf(x). For simplicity, in this article a real-valued function of a real variable will be simply called afunction. To avoid any ambiguity, the other types of functions that may occur will be explicitly specified.

Some functions are defined for all real values of the variables (one says that they are everywhere defined), but some other functions are defined only if the value of the variable is taken in a subsetX ofR{\displaystyle \mathbb {R} }, thedomain of the function, which is always supposed to contain aninterval of positive length. In other words, a real-valued function of a real variable is a function

f:XR{\displaystyle f:X\to \mathbb {R} }

such that its domainX is a subset ofR{\displaystyle \mathbb {R} } that contains an interval of positive length.

A simple example of a function in one variable could be:

f:XR{\displaystyle f:X\to \mathbb {R} }
X={xR:x0}{\displaystyle X=\{x\in \mathbb {R} \,:\,x\geq 0\}}
f(x)=x{\displaystyle f(x)={\sqrt {x}}}

which is thesquare root ofx.

Image

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Main article:Image (mathematics)

Theimage of a functionf(x){\displaystyle f(x)} is the set of all values off when the variablex runs in the whole domain off. For a continuous (see below for a definition) real-valued function with a connected domain, the image is either aninterval or a single value. In the latter case, the function is aconstant function.

Thepreimage of a given real numbery is the set of the solutions of theequationy =f(x).

Domain

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Thedomain of a function of several real variables is a subset ofR{\displaystyle \mathbb {R} } that is sometimes explicitly defined. In fact, if one restricts the domainX of a functionf to a subsetYX, one gets formally a different function, therestriction off toY, which is denotedf|Y. In practice, it is often not harmful to identifyf andf|Y, and to omit the subscript|Y.

Conversely, it is sometimes possible to enlarge naturally the domain of a given function, for example bycontinuity or byanalytic continuation. This means that it is not worthy to explicitly define the domain of a function of a real variable.

Algebraic structure

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The arithmetic operations may be applied to the functions in the following way:

It follows that the functions ofn variables that are everywhere defined and the functions ofn variables that are defined in someneighbourhood of a given point both formcommutative algebras over the reals (R{\displaystyle \mathbb {R} }-algebras).

One may similarly define1/f:(x)1/f(x),{\displaystyle 1/f:(x)\mapsto 1/f(x),} which is a function only if the set of the points(x) in the domain off such thatf(x) ≠ 0 contains an open subset ofR{\displaystyle \mathbb {R} }. This constraint implies that the above two algebras are notfields.

Continuity and limit

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Limit of a real function of a real variable.

Until the second part of 19th century, onlycontinuous functions were considered by mathematicians. At that time, the notion of continuity was elaborated for the functions of one or several real variables a rather long time before the formal definition of atopological space and acontinuous map between topological spaces. As continuous functions of a real variable are ubiquitous in mathematics, it is worth defining this notion without reference to the general notion of continuous maps between topological space.

For defining the continuity, it is useful to consider thedistance function ofR{\displaystyle \mathbb {R} }, which is an everywhere defined function of 2 real variables:d(x,y)=|xy|{\displaystyle d(x,y)=|x-y|}

A functionf iscontinuous at a pointa{\displaystyle a} which isinterior to its domain, if, for every positive real numberε, there is a positive real numberδ such that|f(x)f(a)|<ε{\displaystyle |f(x)-f(a)|<\varepsilon } for allx{\displaystyle x} such thatd(x,a)<δ.{\displaystyle d(x,a)<\delta .} In other words,δ may be chosen small enough for having the image byf of the interval of radiusδ centered ata{\displaystyle a} contained in the interval of length2ε centered atf(a).{\displaystyle f(a).} A function is continuous if it is continuous at every point of its domain.

Thelimit of a real-valued function of a real variable is as follows.[1] Leta be a point intopological closure of the domainX of the functionf. The function,f has a limitL whenx tends towarda, denoted

L=limxaf(x),{\displaystyle L=\lim _{x\to a}f(x),}

if the following condition is satisfied:For every positive real numberε > 0, there is a positive real numberδ > 0 such that

|f(x)L|<ε{\displaystyle |f(x)-L|<\varepsilon }

for allx in the domain such that

d(x,a)<δ.{\displaystyle d(x,a)<\delta .}

If the limit exists, it is unique. Ifa is in the interior of the domain, the limit exists if and only if the function is continuous ata. In this case, we have

f(a)=limxaf(x).{\displaystyle f(a)=\lim _{x\to a}f(x).}

Whena is in theboundary of the domain off, and iff has a limit ata, the latter formula allows to "extend by continuity" the domain off toa.

Calculus

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One can collect a number of functions each of a real variable, say

y1=f1(x),y2=f2(x),,yn=fn(x){\displaystyle y_{1}=f_{1}(x)\,,\quad y_{2}=f_{2}(x)\,,\ldots ,y_{n}=f_{n}(x)}

into a vector parametrized byx:

y=(y1,y2,,yn)=[f1(x),f2(x),,fn(x)]{\displaystyle \mathbf {y} =(y_{1},y_{2},\ldots ,y_{n})=[f_{1}(x),f_{2}(x),\ldots ,f_{n}(x)]}

The derivative of the vectory is the vector derivatives offi(x) fori = 1, 2, ...,n:

dydx=(dy1dx,dy2dx,,dyndx){\displaystyle {\frac {d\mathbf {y} }{dx}}=\left({\frac {dy_{1}}{dx}},{\frac {dy_{2}}{dx}},\ldots ,{\frac {dy_{n}}{dx}}\right)}

One can also performline integrals along aspace curve parametrized byx, withposition vectorr =r(x), by integrating with respect to the variablex:

aby(x)dr=aby(x)dr(x)dxdx{\displaystyle \int _{a}^{b}\mathbf {y} (x)\cdot d\mathbf {r} =\int _{a}^{b}\mathbf {y} (x)\cdot {\frac {d\mathbf {r} (x)}{dx}}dx}

where · is thedot product, andx =a andx =b are the start and endpoints of the curve.

Theorems

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With the definitions of integration and derivatives, key theorems can be formulated, including thefundamental theorem of calculus,integration by parts, andTaylor's theorem. Evaluating a mixture of integrals and derivatives can be done by using theoremdifferentiation under the integral sign.

Implicit functions

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Areal-valuedimplicit function of a real variable is not written in the form "y =f(x)". Instead, the mapping is from the spaceR{\displaystyle \mathbb {R} }2 to thezero element inR{\displaystyle \mathbb {R} } (just the ordinary zero 0):

ϕ:R2{0}{\displaystyle \phi :\mathbb {R} ^{2}\to \{0\}}

and

ϕ(x,y)=0{\displaystyle \phi (x,y)=0}

is an equation in the variables. Implicit functions are a more general way to represent functions, since if:

y=f(x){\displaystyle y=f(x)}

then we can always define:

ϕ(x,y)=yf(x)=0{\displaystyle \phi (x,y)=y-f(x)=0}

but the converse is not always possible, i.e. not all implicit functions have the form of this equation.

One-dimensional space curves inR{\displaystyle \mathbb {R} }n

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Space curve in 3d. Theposition vectorr is parametrized by a scalart. Atr =a the red line is the tangent to the curve, and the blue plane is normal to the curve.

Formulation

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Given the functionsr1 =r1(t),r2 =r2(t), ...,rn =rn(t) all of a common variablet, so that:

r1:RRr2:RRrn:RRr1=r1(t)r2=r2(t)rn=rn(t){\displaystyle {\begin{aligned}r_{1}:\mathbb {R} \rightarrow \mathbb {R} &\quad r_{2}:\mathbb {R} \rightarrow \mathbb {R} &\cdots &\quad r_{n}:\mathbb {R} \rightarrow \mathbb {R} \\r_{1}=r_{1}(t)&\quad r_{2}=r_{2}(t)&\cdots &\quad r_{n}=r_{n}(t)\\\end{aligned}}}

or taken together:

r:RRn,r=r(t){\displaystyle \mathbf {r} :\mathbb {R} \rightarrow \mathbb {R} ^{n}\,,\quad \mathbf {r} =\mathbf {r} (t)}

then the parametrizedn-tuple,

r(t)=[r1(t),r2(t),,rn(t)]{\displaystyle \mathbf {r} (t)=[r_{1}(t),r_{2}(t),\ldots ,r_{n}(t)]}

describes a one-dimensionalspace curve.

Tangent line to curve

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At a pointr(t =c) =a = (a1,a2, ...,an) for some constantt =c, the equations of the one-dimensional tangent line to the curve at that point are given in terms of theordinary derivatives ofr1(t),r2(t), ...,rn(t), andr with respect tot:

r1(t)a1dr1(t)/dt=r2(t)a2dr2(t)/dt==rn(t)andrn(t)/dt{\displaystyle {\frac {r_{1}(t)-a_{1}}{dr_{1}(t)/dt}}={\frac {r_{2}(t)-a_{2}}{dr_{2}(t)/dt}}=\cdots ={\frac {r_{n}(t)-a_{n}}{dr_{n}(t)/dt}}}

Normal plane to curve

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The equation of then-dimensionalhyperplane normal to the tangent line atr =a is:

(p1a1)dr1(t)dt+(p2a2)dr2(t)dt++(pnan)drn(t)dt=0{\displaystyle (p_{1}-a_{1}){\frac {dr_{1}(t)}{dt}}+(p_{2}-a_{2}){\frac {dr_{2}(t)}{dt}}+\cdots +(p_{n}-a_{n}){\frac {dr_{n}(t)}{dt}}=0}

or in terms of thedot product:

(pa)dr(t)dt=0{\displaystyle (\mathbf {p} -\mathbf {a} )\cdot {\frac {d\mathbf {r} (t)}{dt}}=0}

wherep = (p1,p2, ...,pn) are pointsin the plane, not on the space curve.

Relation to kinematics

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Kinematic quantities of a classical particle: massm, positionr, velocityv, accelerationa.

The physical and geometric interpretation ofdr(t)/dt is the "velocity" of a point-likeparticle moving along the pathr(t), treatingr as the spatialposition vector coordinates parametrized by timet, and is a vector tangent to the space curve for allt in the instantaneous direction of motion. Att =c, the space curve has a tangent vectordr(t)/dt|t =c, and the hyperplane normal to the space curve att =c is also normal to the tangent att =c. Any vector in this plane (pa) must be normal todr(t)/dt|t =c.

Similarly,d2r(t)/dt2 is the "acceleration" of the particle, and is a vector normal to the curve directed along theradius of curvature.

Matrix valued functions

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Amatrix can also be a function of a single variable. For example, therotation matrix in 2d:

R(θ)=[cosθsinθsinθcosθ]{\displaystyle R(\theta )={\begin{bmatrix}\cos \theta &-\sin \theta \\\sin \theta &\cos \theta \\\end{bmatrix}}}

is a matrix valued function of rotation angle of about the origin. Similarly, inspecial relativity, theLorentz transformation matrix for a pure boost (without rotations):

Λ(β)=[11β2β1β200β1β211β20000100001]{\displaystyle \Lambda (\beta )={\begin{bmatrix}{\frac {1}{\sqrt {1-\beta ^{2}}}}&-{\frac {\beta }{\sqrt {1-\beta ^{2}}}}&0&0\\-{\frac {\beta }{\sqrt {1-\beta ^{2}}}}&{\frac {1}{\sqrt {1-\beta ^{2}}}}&0&0\\0&0&1&0\\0&0&0&1\\\end{bmatrix}}}

is a function of the boost parameterβ =v/c, in whichv is therelative velocity between the frames of reference (a continuous variable), andc is thespeed of light, a constant.

Banach and Hilbert spaces and quantum mechanics

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Generalizing the previous section, the output of a function of a real variable can also lie in aBanach space or aHilbert space. In these spaces, division and multiplication and limits are all defined, so notions such as derivative and integral still apply. This occurs especially often in quantum mechanics, where one takes the derivative of aket or anoperator. This occurs, for instance, in the general time-dependentSchrödinger equation:

itΨ=H^Ψ{\displaystyle i\hbar {\frac {\partial }{\partial t}}\Psi ={\hat {H}}\Psi }

where one takes the derivative of a wave function, which can be an element of several different Hilbert spaces.

Complex-valued function of a real variable

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Acomplex-valued function of a real variable may be defined by relaxing, in the definition of the real-valued functions, the restriction of the codomain to the real numbers, and allowingcomplex values.

Iff(x) is such a complex valued function, it may be decomposed as

f(x) =g(x) +ih(x),

whereg andh are real-valued functions. In other words, the study of the complex valued functions reduces easily to the study of the pairs of real valued functions.

Cardinality of sets of functions of a real variable

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Thecardinality of the set of real-valued functions of a real variable,RR={f:RR}{\displaystyle \mathbb {R} ^{\mathbb {R} }=\{f:\mathbb {R} \to \mathbb {R} \}}, is2=2c{\displaystyle \beth _{2}=2^{\mathfrak {c}}}, which is strictly larger than the cardinality of thecontinuum (i.e., set of all real numbers). This fact is easily verified by cardinal arithmetic:

card(RR)=card(R)card(R)=cc=(20)c=20c=2c.{\displaystyle \mathrm {card} (\mathbb {R} ^{\mathbb {R} })=\mathrm {card} (\mathbb {R} )^{\mathrm {card} (\mathbb {R} )}={\mathfrak {c}}^{\mathfrak {c}}=(2^{\aleph _{0}})^{\mathfrak {c}}=2^{\aleph _{0}\cdot {\mathfrak {c}}}=2^{\mathfrak {c}}.}

Furthermore, ifX{\displaystyle X} is a set such that2card(X)c{\displaystyle 2\leq \mathrm {card} (X)\leq {\mathfrak {c}}}, then the cardinality of the setXR={f:RX}{\displaystyle X^{\mathbb {R} }=\{f:\mathbb {R} \to X\}} is also2c{\displaystyle 2^{\mathfrak {c}}}, since

2c=card(2R)card(XR)card(RR)=2c.{\displaystyle 2^{\mathfrak {c}}=\mathrm {card} (2^{\mathbb {R} })\leq \mathrm {card} (X^{\mathbb {R} })\leq \mathrm {card} (\mathbb {R} ^{\mathbb {R} })=2^{\mathfrak {c}}.}

However, the set ofcontinuous functionsC0(R)={f:RR:f continuous}{\displaystyle C^{0}(\mathbb {R} )=\{f:\mathbb {R} \to \mathbb {R} :f\ \mathrm {continuous} \}} has a strictly smaller cardinality, the cardinality of the continuum,c{\displaystyle {\mathfrak {c}}}. This follows from the fact that a continuous function is completely determined by its value on a dense subset of its domain.[2] Thus, the cardinality of the set of continuous real-valued functions on the reals is no greater than the cardinality of the set of real-valued functions of a rational variable. By cardinal arithmetic:

card(C0(R))card(RQ)=(20)0=200=20=c.{\displaystyle \mathrm {card} (C^{0}(\mathbb {R} ))\leq \mathrm {card} (\mathbb {R} ^{\mathbb {Q} })=(2^{\aleph _{0}})^{\aleph _{0}}=2^{\aleph _{0}\cdot \aleph _{0}}=2^{\aleph _{0}}={\mathfrak {c}}.}

On the other hand, since there is a clearbijection betweenR{\displaystyle \mathbb {R} } and the set of constant functions{f:RR:f(x)x0}{\displaystyle \{f:\mathbb {R} \to \mathbb {R} :f(x)\equiv x_{0}\}}, which forms a subset ofC0(R){\displaystyle C^{0}(\mathbb {R} )},card(C0(R))c{\displaystyle \mathrm {card} (C^{0}(\mathbb {R} ))\geq {\mathfrak {c}}} must also hold. Hence,card(C0(R))=c{\displaystyle \mathrm {card} (C^{0}(\mathbb {R} ))={\mathfrak {c}}}.

See also

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References

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  1. ^R. Courant (23 February 1988).Differential and Integral Calculus. Vol. 2. Wiley Classics Library. pp. 46–47.ISBN 0-471-60840-8.
  2. ^Rudin, W. (1976).Principles of Mathematical Analysis. New York: McGraw-Hill. pp. 98–99.ISBN 0-07-054235X.

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