Antiderivative
In calculus, an antiderivative, primitive function, primitive integral or indefinite integral[Note 1] of a function f is a differentiable function F whose derivative is equal to the original function f. This can be stated symbolically as .[1][2] The process of solving for antiderivatives is called antidifferentiation (or indefinite integration) and its opposite operation is called differentiation, which is the process of finding a derivative.
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Antiderivatives are related to definite integrals through the fundamental theorem of calculus: the definite integral of a function over an interval is equal to the difference between the values of an antiderivative evaluated at the endpoints of the interval.
The discrete equivalent of the notion of antiderivative is antidifference.
Examples
The function is an antiderivative of , as the derivative of is . As the derivative of a constant is zero, will have an infinite number of antiderivatives, such as , etc. Thus, all the antiderivatives of can be obtained by changing the value of c in , where c is an arbitrary constant known as the constant of integration. Essentially, the graphs of antiderivatives of a given function are vertical translations of each other; each graph's vertical location depending upon the value c.
More generally, the power function has antiderivative if n ≠ −1, and if n = −1.
In physics, the integration of acceleration yields velocity plus a constant. The constant is the initial velocity term that would be lost upon taking the derivative of velocity because the derivative of a constant term is zero. This same pattern applies to further integrations and derivatives of motion (position, velocity, acceleration, and so on).
Uses and properties
Antiderivatives can be used to compute definite integrals, using the fundamental theorem of calculus: if F is an antiderivative of the integrable function f over the interval , then:
Because of this, each of the infinitely many antiderivatives of a given function f is sometimes called the "general integral" or "indefinite integral" of f and is written using the integral symbol with no bounds:
If F is an antiderivative of f, and the function f is defined on some interval, then every other antiderivative G of f differs from F by a constant: there exists a number c such that for all x. c is called the constant of integration. If the domain of F is a disjoint union of two or more (open) intervals, then a different constant of integration may be chosen for each of the intervals. For instance
is the most general antiderivative of on its natural domain
Every continuous function f has an antiderivative, and one antiderivative F is given by the definite integral of f with variable upper boundary:
Varying the lower boundary produces other antiderivatives (but not necessarily all possible antiderivatives). This is another formulation of the fundamental theorem of calculus.
There are many functions whose antiderivatives, even though they exist, cannot be expressed in terms of elementary functions (like polynomials, exponential functions, logarithms, trigonometric functions, inverse trigonometric functions and their combinations). Examples of these are
From left to right, the first four are the error function, the Fresnel function, the trigonometric integral, and the logarithmic integral function.
See also Differential Galois theory for a more detailed discussion.
Techniques of integration
Finding antiderivatives of elementary functions is often considerably harder than finding their derivatives. For some elementary functions, it is impossible to find an antiderivative in terms of other elementary functions. See the articles on elementary functions and nonelementary integral for further information.
There are various methods available:
 the linearity of integration allows us to break complicated integrals into simpler ones
 integration by substitution, often combined with trigonometric identities or the natural logarithm
 the inverse chain rule method, a special case of integration by substitution
 integration by parts to integrate products of functions
 Inverse function integration, a formula that expresses the antiderivative of the inverse of an invertible and continuous function in terms of the antiderivative of and of .
 the method of partial fractions in integration allows us to integrate all rational functions (fractions of two polynomials)
 the Risch algorithm
 when integrating multiple times, certain additional techniques can be used, see for instance double integrals and polar coordinates, the Jacobian and the Stokes' theorem
 if a function has no elementary antiderivative (for instance, ), its definite integral can be approximated using numerical integration
 it is often convenient to algebraically manipulate the integrand such that other integration techniques, such as integration by substitution, may be used.
 to calculate the (n times) repeated antiderivative of a function f, Cauchy's formula is useful (cf. Cauchy formula for repeated integration):
Computer algebra systems can be used to automate some or all of the work involved in the symbolic techniques above, which is particularly useful when the algebraic manipulations involved are very complex or lengthy. Integrals which have already been derived can be looked up in a table of integrals.
Of noncontinuous functions
Noncontinuous functions can have antiderivatives. While there are still open questions in this area, it is known that:
 Some highly pathological functions with large sets of discontinuities may nevertheless have antiderivatives.
 In some cases, the antiderivatives of such pathological functions may be found by Riemann integration, while in other cases these functions are not Riemann integrable.
Assuming that the domains of the functions are open intervals:
 A necessary, but not sufficient, condition for a function f to have an antiderivative is that f have the intermediate value property. That is, if [a, b] is a subinterval of the domain of f and y is any real number between f(a) and f(b), then there exists a c between a and b such that f(c) = y. This is a consequence of Darboux's theorem.
 The set of discontinuities of f must be a meagre set. This set must also be an Fsigma set (since the set of discontinuities of any function must be of this type). Moreover, for any meagre Fsigma set, one can construct some function f having an antiderivative, which has the given set as its set of discontinuities.
 If f has an antiderivative, is bounded on closed finite subintervals of the domain and has a set of discontinuities of Lebesgue measure 0, then an antiderivative may be found by integration in the sense of Lebesgue. In fact, using more powerful integrals like the Henstock–Kurzweil integral, every function for which an antiderivative exists is integrable, and its general integral coincides with its antiderivative.
 If f has an antiderivative F on a closed interval , then for any choice of partition if one chooses sample points as specified by the mean value theorem, then the corresponding Riemann sum telescopes to the value .
 However if f is unbounded, or if f is bounded but the set of discontinuities of f has positive Lebesgue measure, a different choice of sample points may give a significantly different value for the Riemann sum, no matter how fine the partition. See Example 4 below.
Some examples
 The function
with is not continuous at but has the antiderivative
 The function
with is not continuous at but has the antiderivative
 If f(x) is the function in Example 1 and F is its antiderivative, and is a dense countable subset of the open interval then the function
has an antiderivative
 Let be a dense countable subset of the open interval Consider the everywhere continuous strictly increasing function
It can be shown that
for all values x where the series converges, and that the graph of F(x) has vertical tangent lines at all other values of x. In particular the graph has vertical tangent lines at all points in the set .
Moreover for all x where the derivative is defined. It follows that the inverse function is differentiable everywhere and that
for all x in the set which is dense in the interval Thus g has an antiderivative G. On the other hand, it can not be true that
 In Examples 3 and 4, the sets of discontinuities of the functions g are dense only in a finite open interval However, these examples can be easily modified so as to have sets of discontinuities which are dense on the entire real line . Let
 Using a similar method as in Example 5, one can modify g in Example 4 so as to vanish at all rational numbers. If one uses a naive version of the Riemann integral defined as the limit of lefthand or righthand Riemann sums over regular partitions, one will obtain that the integral of such a function g over an interval is 0 whenever a and b are both rational, instead of . Thus the fundamental theorem of calculus will fail spectacularly.
 A function which has an antiderivative may still fail to be Riemann integrable. The derivative of Volterra's function is an example.
Notes
 Antiderivatives are also called general integrals, and sometimes integrals. The latter term is generic, and refers not only to indefinite integrals (antiderivatives), but also to definite integrals. When the word integral is used without additional specification, the reader is supposed to deduce from the context whether it refers to a definite or indefinite integral. Some authors define the indefinite integral of a function as the set of its infinitely many possible antiderivatives. Others define it as an arbitrarily selected element of that set. This article adopts the latter approach.
References
 Stewart, James (2008). Calculus: Early Transcendentals (6th ed.). Brooks/Cole. ISBN 0495011665.
 Larson, Ron; Edwards, Bruce H. (2009). Calculus (9th ed.). Brooks/Cole. ISBN 0547167024.
Further reading
 Introduction to Classical Real Analysis, by Karl R. Stromberg; Wadsworth, 1981 (see also)
 Historical Essay On Continuity Of Derivatives by Dave L. Renfro
External links
 Wolfram Integrator — Free online symbolic integration with Mathematica
 Mathematical Assistant on Web — symbolic computations online. Allows users to integrate in small steps (with hints for next step (integration by parts, substitution, partial fractions, application of formulas and others), powered by Maxima
 Function Calculator from WIMS
 Integral at HyperPhysics
 Antiderivatives and indefinite integrals at the Khan Academy
 Integral calculator at Symbolab
 The Antiderivative at MIT
 Introduction to Integrals at SparkNotes
 Antiderivatives at Harvy Mudd College