TheInfoList

In the
mathematical Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and their changes (cal ...
fields of
differential geometry Differential geometry is a Mathematics, mathematical discipline that studies the geometry of smooth shapes and smooth spaces, otherwise known as smooth manifolds, using the techniques of differential calculus, integral calculus, linear algebra a ...
and
tensor calculus In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ...
, differential forms are an approach to
multivariable calculus Multivariable calculus (also known as multivariate calculus) is the extension of calculus in one Variable (mathematics), variable to calculus with function of several variables, functions of several variables: the Differential calculus, different ...
that is independent of
coordinate In geometry Geometry (from the grc, γεωμετρία; ''wikt:γῆ, geo-'' "earth", ''wikt:μέτρον, -metron'' "measurement") is, with arithmetic, one of the oldest branches of mathematics. It is concerned with properties of space t ... s. Differential forms provide a unified approach to define
integrand In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). ...
s over curves, surfaces, solids, and higher-dimensional
manifold The real projective plane is a two-dimensional manifold that cannot be realized in three dimensions without self-intersection, shown here as Boy's surface. In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of su ... s. The modern notion of differential forms was pioneered by
Élie Cartan Élie Joseph Cartan, ForMemRS Fellowship of the Royal Society (FRS, ForMemRS and HonFRS) is an award granted by the judges of the Royal Society The Royal Society, formally The Royal Society of London for Improving Natural Knowledge, is a ...
. It has many applications, especially in geometry, topology and physics. For instance, the expression from one-variable calculus is an example of a '' -form'', and can be
integrated Integration may refer to: Biology *Modular integration, where different parts in a module have a tendency to vary together *Multisensory integration *Path integration * Pre-integration complex, viral genetic material used to insert a viral genome ... over an oriented interval in the domain of : :$\int_a^b f\left(x\right)\,dx.$ Similarly, the expression is a -form that has a
surface integral In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ... over an
oriented is non-orientable In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical a ... surface File:Water droplet lying on a damask.jpg, Water droplet lying on a damask. Surface tension is high enough to prevent floating below the textile. A surface, as the term is most generally used, is the outermost or uppermost layer of a physical obje ...
: :$\int_S \left(f\left(x,y,z\right)\,dx\wedge dy + g\left(x,y,z\right)\,dz\wedge dx + h\left(x,y,z\right)\,dy\wedge dz\right).$ The symbol denotes the
exterior product In topology s, which have only one surface and one edge, are a kind of object studied in topology. In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical struc ...
, sometimes called the ''wedge product'', of two differential forms. Likewise, a -form represents a
volume elementIn mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ha ...
that can be integrated over an oriented region of space. In general, a -form is an object that may be integrated over a -dimensional oriented manifold, and is homogeneous of degree in the coordinate differentials. On an -dimensional manifold, the top-dimensional form (-form) is called a ''
volume formIn mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ha ...
''. The
algebra Algebra (from ar, الجبر, lit=reunion of broken parts, bonesetting, translit=al-jabr) is one of the areas of mathematics, broad areas of mathematics, together with number theory, geometry and mathematical analysis, analysis. In its most ge ...
of differential forms is organized in a way that naturally reflects the
orientation Orientation may refer to: Positioning in physical space * Map orientation, the relationship between directions on a map and compass directions * Orientation (housing), the position of a building with respect to the sun, a concept in building design ...
of the domain of integration. There is an operation on differential forms known as the
exterior derivative On a differentiable manifold In mathematics, a differentiable manifold (also differential manifold) is a type of manifold The real projective plane is a two-dimensional manifold that cannot be realized in three dimensions without self-interse ...
that, when given a -form as input, produces a -form as output. This operation extends the
differential of a function In calculus Calculus, originally called infinitesimal calculus or "the calculus of infinitesimal In mathematics, infinitesimals or infinitesimal numbers are quantities that are closer to zero than any standard real number, but are not zero. ...
, and is directly related to the
divergence In vector calculus Vector calculus, or vector analysis, is concerned with derivative, differentiation and integral, integration of vector fields, primarily in 3-dimensional Euclidean space \mathbb^3. The term "vector calculus" is sometimes ... and the
curl Curl or CURL may refer to: Science and technology * Curl (mathematics) In vector calculus Vector calculus, or vector analysis, is concerned with derivative, differentiation and integral, integration of vector fields, primarily in 3-dimension ...
of a vector field in a manner that makes the
fundamental theorem of calculus The fundamental theorem of calculus is a theorem that links the concept of derivative, differentiating a function (mathematics), function (calculating the gradient) with the concept of integral, integrating a function (calculating the area under t ...
, the
divergence theorem In vector calculus, the divergence theorem, also known as Gauss's theorem or Ostrogradsky's theorem, reprinted in is a theorem which relates the flux of a vector field through a closed surface (mathematics), surface to the divergence of the fie ... ,
Green's theorem In vector calculus, Green's theorem relates a line integral In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geome ...
, and
Stokes' theorem Stokes' theorem, also known as Kelvin–Stokes theorem Nagayoshi Iwahori, et al.:"Bi-Bun-Seki-Bun-Gaku" :ja:裳華房, Sho-Ka-Bou(jp) 1983/12Written in Japanese)Atsuo Fujimoto;"Vector-Kai-Seki Gendai su-gaku rekucha zu. C(1)" :ja:培風館, Ba ...
special cases of the same general result, known in this context also as the
generalized Stokes theorem In vector calculus and differential geometry the generalized Stokes theorem (sometimes with apostrophe as Stokes' theorem or Stokes's theorem), also called the Stokes–Cartan theorem, is a statement about the integral, integration of differen ...
. In a deeper way, this theorem relates the
topology In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities ... of the domain of integration to the structure of the differential forms themselves; the precise connection is known as
de Rham's theorem#Redirect DE {{Redirect category shell, 1= {{Redirect from other capitalisation {{Redirect from ambiguous term ...
. The general setting for the study of differential forms is on a
differentiable manifold In mathematics, a differentiable manifold (also differential manifold) is a type of manifold The real projective plane is a two-dimensional manifold that cannot be realized in three dimensions without self-intersection, shown here as Boy's surfa ...
. Differential -forms are naturally dual to
vector field In vector calculus Vector calculus, or vector analysis, is concerned with differentiation Differentiation may refer to: Business * Differentiation (economics), the process of making a product different from other similar products * Product ... s on a manifold, and the pairing between vector fields and -forms is extended to arbitrary differential forms by the
interior product In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ...
. The algebra of differential forms along with the exterior derivative defined on it is preserved by the
pullback In mathematics, a pullback is either of two different, but related processes: precomposition and fiber-product. Its dual is a Pushforward (disambiguation), pushforward. Precomposition Precomposition with a Function (mathematics), function probabl ...
under smooth functions between two manifolds. This feature allows geometrically invariant information to be moved from one space to another via the pullback, provided that the information is expressed in terms of differential forms. As an example, the
change of variables formula In calculus Calculus, originally called infinitesimal calculus or "the calculus of infinitesimal In mathematics, infinitesimals or infinitesimal numbers are quantities that are closer to zero than any standard real number, but are not zero. ...
for integration becomes a simple statement that an integral is preserved under pullback.

# History

Differential forms are part of the field of differential geometry, influenced by linear algebra. Although the notion of a differential is quite old, the initial attempt at an algebraic organization of differential forms is usually credited to
Élie Cartan Élie Joseph Cartan, ForMemRS Fellowship of the Royal Society (FRS, ForMemRS and HonFRS) is an award granted by the judges of the Royal Society The Royal Society, formally The Royal Society of London for Improving Natural Knowledge, is a ...
with reference to his 1899 paper. Some aspects of the
exterior algebra In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ...
of differential forms appears in
Hermann Grassmann Hermann Günther Grassmann (german: link=no, Graßmann, ; 15 April 1809 – 26 September 1877) was a German polymath, known in his day as a linguistics, linguist and now also as a mathematics, mathematician. He was also a physics, physicist, gener ...
's 1844 work, ''Die Lineale Ausdehnungslehre, ein neuer Zweig der Mathematik (The Theory of Linear Extension, a New Branch of Mathematics)''.

# Concept

Differential forms provide an approach to
multivariable calculus Multivariable calculus (also known as multivariate calculus) is the extension of calculus in one Variable (mathematics), variable to calculus with function of several variables, functions of several variables: the Differential calculus, different ...
that is independent of
coordinate In geometry Geometry (from the grc, γεωμετρία; ''wikt:γῆ, geo-'' "earth", ''wikt:μέτρον, -metron'' "measurement") is, with arithmetic, one of the oldest branches of mathematics. It is concerned with properties of space t ... s.

## Integration and orientation

A differential -form can be integrated over an oriented
manifold In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities a ...
of dimension . A differential -form can be thought of as measuring an infinitesimal oriented length, or 1-dimensional oriented density. A differential -form can be thought of as measuring an infinitesimal oriented area, or 2-dimensional oriented density. And so on. Integration of differential forms is well-defined only on
oriented is non-orientable In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical a ...
manifolds The real projective plane is a two-dimensional manifold that cannot be realized in three dimensions without self-intersection, shown here as Boy's surface. In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of suc ...
. An example of a 1-dimensional manifold is an interval , and intervals can be given an orientation: they are positively oriented if , and negatively oriented otherwise. If then the integral of the differential -form over the interval (with its natural positive orientation) is :$\int_a^b f\left(x\right) \,dx$ which is the negative of the integral of the same differential form over the same interval, when equipped with the opposite orientation. That is: :$\int_b^a f\left(x\right)\,dx = -\int_a^b f\left(x\right)\,dx$ This gives a geometrical context to the
conventions for one-dimensional integrals, that the sign changes when the orientation of the interval is reversed. A standard explanation of this in one-variable integration theory is that, when the limits of integration are in the opposite order (), the increment is negative in the direction of integration. More generally, an -form is an oriented density that can be integrated over an -dimensional oriented manifold. (For example, a -form can be integrated over an oriented curve, a -form can be integrated over an oriented surface, etc.) If is an oriented -dimensional manifold, and is the same manifold with opposite orientation and is an -form, then one has: :$\int_M \omega = - \int_ \omega \,.$ These conventions correspond to interpreting the integrand as a differential form, integrated over a
chain A chain is a wikt:series#Noun, serial assembly of connected pieces, called links, typically made of metal, with an overall character similar to that of a rope in that it is flexible and curved in compression (physics), compression but line (g ...
. In
measure theory Measure is a fundamental concept of mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contai ...
, by contrast, one interprets the integrand as a function with respect to a measure and integrates over a subset , without any notion of orientation; one writes $\int_A f\,d\mu = \int_ f\,d\mu$ to indicate integration over a subset . This is a minor distinction in one dimension, but becomes subtler on higher-dimensional manifolds; see
below Below may refer to: *Earth *Ground (disambiguation) *Soil *Floor *Bottom (disambiguation) *Less than *Temperatures below freezing *Hell or underworld People with the surname *Fred Below (1926–1988), American blues drummer *Fritz von Below (1853� ...
for details. Making the notion of an oriented density precise, and thus of a differential form, involves the
exterior algebra In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ...
. The differentials of a set of coordinates, , ..., can be used as a basis for all -forms. Each of these represents a
covector In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and t ...
at each point on the manifold that may be thought of as measuring a small displacement in the corresponding coordinate direction. A general -form is a linear combination of these differentials at every point on the manifold: :$f_1\,dx^1+\cdots+f_n\,dx^n ,$ where the are functions of all the coordinates. A differential -form is integrated along an oriented curve as a line integral. The expressions , where can be used as a basis at every point on the manifold for all -forms. This may be thought of as an infinitesimal oriented square parallel to the –-plane. A general -form is a linear combination of these at every point on the manifold: and it is integrated just like a surface integral. A fundamental operation defined on differential forms is the
exterior product In topology s, which have only one surface and one edge, are a kind of object studied in topology. In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical struc ...
(the symbol is the
wedge A wedge is a triangular A triangle is a polygon In geometry Geometry (from the grc, γεωμετρία; ''wikt:γῆ, geo-'' "earth", ''wikt:μέτρον, -metron'' "measurement") is, with arithmetic, one of the oldest branche ...
). This is similar to the
cross product In , the cross product or vector product (occasionally directed area product, to emphasize its geometric significance) is a on two s in a three-dimensional (named here E), and is denoted by the symbol \times. Given two and , the cross produc ... from vector calculus, in that it is an alternating product. For instance, :$dx^1\wedge dx^2=-dx^2\wedge dx^1$ because the square whose first side is and second side is is to be regarded as having the opposite orientation as the square whose first side is and whose second side is . This is why we only need to sum over expressions , with ; for example: . The exterior product allows higher-degree differential forms to be built out of lower-degree ones, in much the same way that the
cross product In , the cross product or vector product (occasionally directed area product, to emphasize its geometric significance) is a on two s in a three-dimensional (named here E), and is denoted by the symbol \times. Given two and , the cross produc ... in vector calculus allows one to compute the area vector of a parallelogram from vectors pointing up the two sides. Alternating also implies that , in the same way that the cross product of parallel vectors, whose magnitude is the area of the parallelogram spanned by those vectors, is zero. In higher dimensions, if any two of the indices , ..., are equal, in the same way that the "volume" enclosed by a parallelotope whose edge vectors are
linearly dependent In the theory of vector spaces, a set of vectors is said to be if at least one of the vectors in the set can be defined as a linear combinationIn mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics ...
is zero.

## Multi-index notation

A common notation for the wedge product of elementary -forms is so called
multi-index notation Multi-index notation is a mathematical notation that simplifies formulas used in multivariable calculus, partial differential equations and the theory of distributions, by generalising the concept of an integer index Index may refer to: Arts, ...
: in an -dimensional context, for we define Another useful notation is obtained by defining the set of all strictly increasing multi-indices of length , in a space of dimension , denoted Then locally (wherever the coordinates apply), $\_$ spans the space of differential -forms in a manifold of dimension , when viewed as a module over the ring of smooth functions on . By calculating the size of $\mathcal_$ combinatorially, the module of -forms on a -dimensional manifold, and in general space of -covectors on an -dimensional vector space, is  choose : This also demonstrates that there are no nonzero differential forms of degree greater than the dimension of the underlying manifold.

## The exterior derivative

In addition to the exterior product, there is also the
exterior derivative On a differentiable manifold In mathematics, a differentiable manifold (also differential manifold) is a type of manifold The real projective plane is a two-dimensional manifold that cannot be realized in three dimensions without self-interse ...
operator . The exterior derivative of a differential form is a generalization of the
differential of a function In calculus Calculus, originally called infinitesimal calculus or "the calculus of infinitesimal In mathematics, infinitesimals or infinitesimal numbers are quantities that are closer to zero than any standard real number, but are not zero. ...
, in the sense that the exterior derivative of is exactly the differential of . When generalized to higher forms, if is a simple -form, then its exterior derivative is a -form defined by taking the differential of the coefficient functions: :$d\omega = \sum_^n \frac \, dx^i \wedge dx^I.$ with extension to general -forms through linearity: if then its exterior derivative is : $d\tau = \sum_\left\left(\sum_^n \frac \, dx^j\right\right)\wedge dx^I \in \Omega^\left(M\right)$ In , with the
Hodge star operator In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It h ...
, the exterior derivative corresponds to
gradient In vector calculus Vector calculus, or vector analysis, is concerned with differentiation Differentiation may refer to: Business * Differentiation (economics), the process of making a product different from other similar products * Prod ... ,
curl Curl or CURL may refer to: Science and technology * Curl (mathematics) In vector calculus Vector calculus, or vector analysis, is concerned with differentiation Differentiation may refer to: Business * Differentiation (economics), the p ...
, and
divergence In vector calculus Vector calculus, or vector analysis, is concerned with derivative, differentiation and integral, integration of vector fields, primarily in 3-dimensional Euclidean space \mathbb^3. The term "vector calculus" is sometimes ... , although this correspondence, like the cross product, does not generalize to higher dimensions, and should be treated with some caution. The exterior derivative itself applies in an arbitrary finite number of dimensions, and is a flexible and powerful tool with wide application in
differential geometry Differential geometry is a Mathematics, mathematical discipline that studies the geometry of smooth shapes and smooth spaces, otherwise known as smooth manifolds, using the techniques of differential calculus, integral calculus, linear algebra a ...
,
differential topology In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ...
, and many areas in physics. Of note, although the above definition of the exterior derivative was defined with respect to local coordinates, it can be defined in an entirely coordinate-free manner, as an
antiderivationIn mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ha ...
of degree 1 on the
exterior algebra In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ...
of differential forms. The benefit of this more general approach is that it allows for a natural coordinate-free approach to integration on
manifold The real projective plane is a two-dimensional manifold that cannot be realized in three dimensions without self-intersection, shown here as Boy's surface. In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of su ... s. It also allows for a natural generalization of the
fundamental theorem of calculus The fundamental theorem of calculus is a theorem that links the concept of derivative, differentiating a function (mathematics), function (calculating the gradient) with the concept of integral, integrating a function (calculating the area under t ...
, called the (generalized)
Stokes' theorem Stokes' theorem, also known as Kelvin–Stokes theorem Nagayoshi Iwahori, et al.:"Bi-Bun-Seki-Bun-Gaku" :ja:裳華房, Sho-Ka-Bou(jp) 1983/12Written in Japanese)Atsuo Fujimoto;"Vector-Kai-Seki Gendai su-gaku rekucha zu. C(1)" :ja:培風館, Ba ...
, which is a central result in the theory of integration on manifolds.

## Differential calculus

Let be an
open set In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and ...
in . A differential -form ("zero-form") is defined to be a
smooth function In mathematical analysis Analysis is the branch of mathematics dealing with Limit (mathematics), limits and related theories, such as Derivative, differentiation, Integral, integration, Measure (mathematics), measure, sequences, Series (mat ... on – the set of which is denoted . If is any vector in , then has a
directional derivative In mathematics, the directional derivative of a multivariate differentiable function, differentiable (scalar) function along a given vector (mathematics), vector v at a given point x intuitively represents the instantaneous rate of change of the ...
, which is another function on whose value at a point is the rate of change (at ) of in the direction: :$\left(\partial_v f\right)\left(p\right) = \left. \frac f\left(p+tv\right)\_ .$ (This notion can be extended point-wise to the case that is a
vector field In vector calculus Vector calculus, or vector analysis, is concerned with differentiation Differentiation may refer to: Business * Differentiation (economics), the process of making a product different from other similar products * Product ... on by evaluating at the point in the definition.) In particular, if is the th
coordinate vector In linear algebra, a coordinate vector is a representation of a vector as an ordered list of numbers that describes the vector in terms of a particular ordered basis. Coordinates are always specified relative to an ordered basis. Bases and their a ...
then is the
partial derivative In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and ... of with respect to the th coordinate function, i.e., , where , , ..., are the coordinate functions on . By their very definition, partial derivatives depend upon the choice of coordinates: if new coordinates , , ..., are introduced, then :$\frac = \sum_^n\frac\frac .$ The first idea leading to differential forms is the observation that is a
linear function In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and t ... of : :$\begin \left(\partial_ f\right)\left(p\right) &= \left(\partial_v f\right)\left(p\right) + \left(\partial_w f\right)\left(p\right) \\ \left(\partial_ f\right)\left(p\right) &= c \left(\partial_v f\right)\left(p\right) \end$ for any vectors , and any real number . At each point ''p'', this
linear map In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and ... from to is denoted and called the
derivative In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities ... or differential of at . Thus . Extended over the whole set, the object can be viewed as a function that takes a vector field on , and returns a real-valued function whose value at each point is the derivative along the vector field of the function . Note that at each , the differential is not a real number, but a linear functional on tangent vectors, and a prototypical example of a differential -form. Since any vector is a
linear combination In mathematics, a linear combination is an Expression (mathematics), expression constructed from a Set (mathematics), set of terms by multiplying each term by a constant and adding the results (e.g. a linear combination of ''x'' and ''y'' would be ...
of its
components Component may refer to: In engineering, science, and technology Generic systems *System A system is a group of Interaction, interacting or interrelated elements that act according to a set of rules to form a unified whole. A system, surrounde ... , is uniquely determined by for each and each , which are just the partial derivatives of on . Thus provides a way of encoding the partial derivatives of . It can be decoded by noticing that the coordinates , , ..., are themselves functions on , and so define differential -forms , , ..., . Let . Since , the
Kronecker delta function In mathematics, the Kronecker delta (named after Leopold Kronecker) is a Function (mathematics), function of two Variable (mathematics), variables, usually just non-negative integers. The function is 1 if the variables are equal, and 0 otherwise: ...
, it follows that The meaning of this expression is given by evaluating both sides at an arbitrary point : on the right hand side, the sum is defined "
pointwiseIn mathematics, the qualifier pointwise is used to indicate that a certain property is defined by considering each value f(x) of some function f. An important class of pointwise concepts are the ''pointwise operations'', that is, operations defined o ...
", so that :$df_p = \sum_^n \frac\left(p\right) \left(dx^i\right)_p .$ Applying both sides to , the result on each side is the th partial derivative of at . Since and were arbitrary, this proves the formula . More generally, for any smooth functions and on , we define the differential -form pointwise by :$\alpha_p = \sum_i g_i\left(p\right) \left(dh_i\right)_p$ for each . Any differential -form arises this way, and by using it follows that any differential -form on may be expressed in coordinates as :$\alpha = \sum_^n f_i\, dx^i$ for some smooth functions on . The second idea leading to differential forms arises from the following question: given a differential -form on , when does there exist a function on such that ? The above expansion reduces this question to the search for a function whose partial derivatives are equal to given functions . For , such a function does not always exist: any smooth function satisfies :$\frac = \frac ,$ so it will be impossible to find such an unless :$\frac - \frac = 0$ for all and . The skew-symmetry of the left hand side in and suggests introducing an antisymmetric product on differential -forms, the
exterior product In topology s, which have only one surface and one edge, are a kind of object studied in topology. In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical struc ...
, so that these equations can be combined into a single condition :$\sum_^n \frac \, dx^i \wedge dx^j = 0 ,$ where is defined so that: : $dx^i \wedge dx^j = - dx^j \wedge dx^i.$ This is an example of a differential -form. This -form is called the
exterior derivative On a differentiable manifold In mathematics, a differentiable manifold (also differential manifold) is a type of manifold The real projective plane is a two-dimensional manifold that cannot be realized in three dimensions without self-interse ...
of . It is given by :$d\alpha = \sum_^n df_j \wedge dx^j = \sum_^n \frac \, dx^i \wedge dx^j .$ To summarize: is a necessary condition for the existence of a function with . Differential -forms, -forms, and -forms are special cases of differential forms. For each , there is a space of differential -forms, which can be expressed in terms of the coordinates as :$\sum_^n f_ \, dx^ \wedge dx^ \wedge\cdots \wedge dx^$ for a collection of functions . Antisymmetry, which was already present for -forms, makes it possible to restrict the sum to those sets of indices for which . Differential forms can be multiplied together using the exterior product, and for any differential -form , there is a differential -form called the exterior derivative of . Differential forms, the exterior product and the exterior derivative are independent of a choice of coordinates. Consequently, they may be defined on any
smooth manifold In mathematics, a differentiable manifold (also differential manifold) is a type of manifold The real projective plane is a two-dimensional manifold that cannot be realized in three dimensions without self-intersection, shown here as Boy's s ...
. One way to do this is cover with
coordinate chartIn topology, a branch of mathematics, a topological manifold is a topological space which locally resembles real numbers, real ''n''-dimension (mathematics), dimensional Euclidean space. Topological manifolds are an important class of topological spa ...
s and define a differential -form on to be a family of differential -forms on each chart which agree on the overlaps. However, there are more intrinsic definitions which make the independence of coordinates manifest.

# Intrinsic definitions

Let be a
smooth manifold In mathematics, a differentiable manifold (also differential manifold) is a type of manifold The real projective plane is a two-dimensional manifold that cannot be realized in three dimensions without self-intersection, shown here as Boy's s ...
. A smooth differential form of degree is a smooth section of the th
exterior power In topology s, which have only one surface and one edge, are a kind of object studied in topology. In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical struc ...
of the
cotangent bundle In mathematics, especially differential geometry, the cotangent bundle of a smooth manifold is the vector bundle of all the cotangent spaces at every point in the manifold. It may be described also as the dual bundle to the tangent bundle. This may ...
of . The set of all differential -forms on a manifold is a
vector space In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities a ...
, often denoted . The definition of a differential form may be restated as follows. At any point , a -form defines an element :$\beta_p \in ^k T_p^* M,$ where is the
tangent space In , the tangent space of a generalizes to higher dimensions the notion of tangent planes to surfaces in three dimensions and tangent lines to curves in two dimensions. In the context of physics the tangent space to a manifold at a point can ...
to at and is its
dual space In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers ( and ), formulas and related structures (), shapes and spaces in which they are contained (), and quantities and their changes ( and ). There is no gen ...
. This space is to the fiber at of the dual bundle of the th exterior power of the
tangent bundle Image:Tangent bundle.svg, Informally, the tangent bundle of a manifold (which in this case is a circle) is obtained by considering all the tangent spaces (top), and joining them together in a smooth and non-overlapping manner (bottom). In differen ... of . That is, is also a linear functional $\beta_p \colon ^k T_pM \to \mathbf$, i.e. the dual of the th exterior power is isomorphic to the th exterior power of the dual: : $^k T^*_p M \cong \Big\left(^k T_p M\Big\right)^*$ By the universal property of exterior powers, this is equivalently an alternating
multilinear map In linear algebra, a multilinear map is a function of several variables that is linear separately in each variable. More precisely, a multilinear map is a function :f\colon V_1 \times \cdots \times V_n \to W\text where V_1,\ldots,V_n and W ar ...
: :$\beta_p\colon \bigoplus_^k T_p M \to \mathbf.$ Consequently, a differential -form may be evaluated against any -tuple of tangent vectors to the same point of . For example, a differential -form assigns to each point a
linear functional In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and t ...
on . In the presence of an
inner product In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and ...
on (induced by a
Riemannian metric In differential geometry, a Riemannian manifold or Riemannian space is a real manifold, real, smooth manifold ''M'' equipped with a positive-definite Inner product space, inner product ''g'p'' on the tangent space ''T'p'M'' at each poin ...
on ), may be represented as the inner product with a
tangent vector :''For a more general — but much more technical — treatment of tangent vectors, see tangent space.'' In mathematics, a tangent vector is a Vector (geometry), vector that is tangent to a curve or Surface (mathematics), surface at a given point. T ...
. Differential -forms are sometimes called covariant vector fields, covector fields, or "dual vector fields", particularly within physics. The exterior algebra may be embedded in the tensor algebra by means of the alternation map. The alternation map is defined as a mapping : $\operatorname \colon ^k T^*M \to ^k T^*M.$ For a tensor $\tau$ at a point , :$\operatorname\left(\tau_p\right)\left(x_1, \dots, x_k\right) = \frac\sum_ \sgn\left(\sigma\right) \tau_p\left(x_, \dots, x_\right),$ where is the
symmetric group In abstract algebra In algebra, which is a broad division of mathematics, abstract algebra (occasionally called modern algebra) is the study of algebraic structures. Algebraic structures include group (mathematics), groups, ring (mathemati ...
on elements. The alternation map is constant on the cosets of the ideal in the tensor algebra generated by the symmetric 2-forms, and therefore descends to an embedding : $\operatorname \colon ^k T^*M \to ^k T^*M.$ This map exhibits as a totally antisymmetric covariant
tensor field In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and t ...
of rank . The differential forms on are in one-to-one correspondence with such tensor fields.

# Operations

As well as the addition and multiplication by scalar operations which arise from the vector space structure, there are several other standard operations defined on differential forms. The most important operations are the
exterior product In topology s, which have only one surface and one edge, are a kind of object studied in topology. In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical struc ...
of two differential forms, the
exterior derivative On a differentiable manifold In mathematics, a differentiable manifold (also differential manifold) is a type of manifold The real projective plane is a two-dimensional manifold that cannot be realized in three dimensions without self-interse ...
of a single differential form, the
interior product In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ...
of a differential form and a vector field, the
Lie derivative In differential geometry Differential geometry is a Mathematics, mathematical discipline that studies the geometry of smooth shapes and smooth spaces, otherwise known as smooth manifolds, using the techniques of differential calculus, integral ...
of a differential form with respect to a vector field and the
covariant derivative In mathematics, the covariant derivative is a way of specifying a derivative along tangent vectors of a manifold. Alternatively, the covariant derivative is a way of introducing and working with a connection (mathematics), connection on a manifold ...
of a differential form with respect to a vector field on a manifold with a defined connection.

## Exterior product

The exterior product of a -form and an -form , denoted , is a ()-form. At each point of the manifold , the forms and are elements of an exterior power of the cotangent space at . When the exterior algebra is viewed as a quotient of the tensor algebra, the exterior product corresponds to the tensor product (modulo the equivalence relation defining the exterior algebra). The antisymmetry inherent in the exterior algebra means that when is viewed as a multilinear functional, it is alternating. However, when the exterior algebra is embedded as a subspace of the tensor algebra by means of the alternation map, the tensor product is not alternating. There is an explicit formula which describes the exterior product in this situation. The exterior product is :$\alpha \wedge \beta = \operatorname\left(\alpha \otimes \beta\right).$ If the embedding of $^n T^*M$ into $^n T^*M$ is done via the map $n!\operatorname$ instead of $\operatorname$, the exterior product is :$\alpha \wedge \beta = \frac\operatorname\left(\alpha \otimes \beta\right).$ This description is useful for explicit computations. For example, if , then is the -form whose value at a point is the alternating bilinear form defined by :$\left(\alpha\wedge\beta\right)_p\left(v,w\right)=\alpha_p\left(v\right)\beta_p\left(w\right) - \alpha_p\left(w\right)\beta_p\left(v\right)$ for . The exterior product is bilinear: If , , and are any differential forms, and if is any smooth function, then :$\alpha \wedge \left(\beta + \gamma\right) = \alpha \wedge \beta + \alpha \wedge \gamma,$ :$\alpha \wedge \left(f \cdot \beta\right) = f \cdot \left(\alpha \wedge \beta\right).$ It is ''skew commutative'' (also known as ''graded commutative''), meaning that it satisfies a variant of
anticommutativity In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It h ...
that depends on the degrees of the forms: if is a -form and is an -form, then :$\alpha \wedge \beta = \left(-1\right)^ \beta \wedge \alpha .$

## Riemannian manifold

On a
Riemannian manifold In differential geometry Differential geometry is a Mathematics, mathematical discipline that studies the geometry of smooth shapes and smooth spaces, otherwise known as smooth manifolds, using the techniques of differential calculus, integr ...
, or more generally a
pseudo-Riemannian manifold In differential geometry Differential geometry is a Mathematics, mathematical discipline that uses the techniques of differential calculus, integral calculus, linear algebra and multilinear algebra to study problems in geometry. The Differenti ...
, the metric defines a fibre-wise isomorphism of the tangent and cotangent bundles. This makes it possible to convert vector fields to covector fields and vice versa. It also enables the definition of additional operations such as the
Hodge star operator In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It h ...
$\star \colon \Omega^k\left(M\right)\ \stackrel\ \Omega^\left(M\right)$ and the codifferential $\delta\colon \Omega^k\left(M\right)\rightarrow \Omega^\left(M\right)$, which has degree and is adjoint to the exterior differential .

### Vector field structures

On a pseudo-Riemannian manifold, -forms can be identified with vector fields; vector fields have additional distinct algebraic structures, which are listed here for context and to avoid confusion. Firstly, each (co)tangent space generates a
Clifford algebra In mathematics, a Clifford algebra is an algebra over a field, algebra generated by a vector space with a quadratic form, and is a Unital algebra, unital associative algebra. As algebra over a field, ''K''-algebras, they generalize the real nu ...
, where the product of a (co)vector with itself is given by the value of a quadratic form – in this case, the natural one induced by the
metric METRIC (Mapping EvapoTranspiration at high Resolution with Internalized Calibration) is a computer model Computer simulation is the process of mathematical modelling, performed on a computer, which is designed to predict the behaviour of or th ...
. This algebra is ''distinct'' from the
exterior algebra In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ...
of differential forms, which can be viewed as a Clifford algebra where the quadratic form vanishes (since the exterior product of any vector with itself is zero). Clifford algebras are thus non-anticommutative ("quantum") deformations of the exterior algebra. They are studied in
geometric algebra In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ...
. Another alternative is to consider vector fields as derivations. The (noncommutative) algebra of
differential operator 300px, A harmonic function defined on an annulus. Harmonic functions are exactly those functions which lie in the kernel of the Laplace operator, an important differential operator. In mathematics, a differential operator is an Operator (mathe ...
s they generate is the
Weyl algebra In abstract algebra, the Weyl algebra is the ring of differential operator 300px, A harmonic function defined on an annulus. Harmonic functions are exactly those functions which lie in the kernel of the Laplace operator, an important differe ...
and is a noncommutative ("quantum") deformation of the ''symmetric'' algebra in the vector fields.

## Exterior differential complex

One important property of the exterior derivative is that . This means that the exterior derivative defines a
cochain complex In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ...
: :$0\ \to\ \Omega^0\left(M\right)\ \stackrel\ \Omega^1\left(M\right)\ \stackrel\ \Omega^2\left(M\right)\ \stackrel\ \Omega^3\left(M\right)\ \to\ \cdots \ \to\ \Omega^n\left(M\right)\ \to \ 0.$ This complex is called the de Rham complex, and its
cohomology In mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It h ...
is by definition the de Rham cohomology of . By the Poincaré lemma, the de Rham complex is locally exact except at . The kernel at is the space of
locally constant function In mathematics, a function (mathematics), function ''f'' from a topological space ''A'' to a Set (mathematics), set ''B'' is called locally constant if for every ''a'' in ''A'' there exists a neighborhood (topology), neighborhood ''U'' of ''a'' suc ...
s on . Therefore, the complex is a resolution of the constant sheaf (mathematics), sheaf , which in turn implies a form of de Rham's theorem: de Rham cohomology computes the sheaf cohomology of .

# Pullback

Suppose that is smooth. The differential of is a smooth map between the tangent bundles of and . This map is also denoted and called the pushforward. For any point and any tangent vector , there is a well-defined pushforward vector in . However, the same is not true of a vector field. If is not injective, say because has two or more preimages, then the vector field may determine two or more distinct vectors in . If is not surjective, then there will be a point at which does not determine any tangent vector at all. Since a vector field on determines, by definition, a unique tangent vector at every point of , the pushforward of a vector field does not always exist. By contrast, it is always possible to pull back a differential form. A differential form on may be viewed as a linear functional on each tangent space. Precomposing this functional with the differential defines a linear functional on each tangent space of and therefore a differential form on . The existence of pullbacks is one of the key features of the theory of differential forms. It leads to the existence of pullback maps in other situations, such as pullback homomorphisms in de Rham cohomology. Formally, let be smooth, and let be a smooth -form on . Then there is a differential form on , called the pullback of , which captures the behavior of as seen relative to . To define the pullback, fix a point of and tangent vectors , ..., to at . The pullback of is defined by the formula :$\left(f^*\omega\right)_p\left(v_1, \ldots, v_k\right) = \omega_\left(f_*v_1, \ldots, f_*v_k\right).$ There are several more abstract ways to view this definition. If is a -form on , then it may be viewed as a section of the cotangent bundle of . Using to denote a dual map, the dual to the differential of is . The pullback of may be defined to be the composite :$M\ \stackrel\ N\ \stackrel\ T^*N\ \stackrel\ T^*M.$ This is a section of the cotangent bundle of and hence a differential -form on . In full generality, let $\bigwedge^k (df)^*$ denote the th exterior power of the dual map to the differential. Then the pullback of a -form is the composite :$M\ \stackrel\ N\ \stackrel\ ^k T^*N\ \stackrel\ ^k T^*M.$ Another abstract way to view the pullback comes from viewing a -form as a linear functional on tangent spaces. From this point of view, is a morphism of vector bundles :$^k TN\ \stackrel\ N \times \mathbf,$ where is the trivial rank one bundle on . The composite map :$^k TM\ \stackrel\ ^k TN\ \stackrel\ N \times \mathbf$ defines a linear functional on each tangent space of , and therefore it factors through the trivial bundle . The vector bundle morphism $^k TM \to M \times \mathbf$ defined in this way is . Pullback respects all of the basic operations on forms. If and are forms and is a real number, then :$\begin f^*\left(c\omega\right) &= c\left(f^*\omega\right), \\ f^*\left(\omega + \eta\right) &= f^*\omega + f^*\eta, \\ f^*\left(\omega \wedge \eta\right) &= f^*\omega \wedge f^*\eta, \\ f^*\left(d\omega\right) &= d\left(f^*\omega\right). \end$ The pullback of a form can also be written in coordinates. Assume that , ..., are coordinates on , that , ..., are coordinates on , and that these coordinate systems are related by the formulas for all . Locally on , can be written as :$\omega = \sum_ \omega_ \, dy^ \wedge \cdots \wedge dy^,$ where, for each choice of , ..., , is a real-valued function of , ..., . Using the linearity of pullback and its compatibility with exterior product, the pullback of has the formula :$f^*\omega = \sum_ \left(\omega_\circ f\right) \, df_ \wedge \cdots \wedge df_.$ Each exterior derivative can be expanded in terms of , ..., . The resulting -form can be written using Jacobian matrix and determinant, Jacobian matrices: :$f^*\omega = \sum_ \sum_ \left(\omega_\circ f\right)\frac \, dx^ \wedge \cdots \wedge dx^.$ Here, $\frac$ denotes the determinant of the matrix whose entries are $\frac$, $1\leq m,n\leq k$.

# Integration

A differential -form can be integrated over an oriented -dimensional manifold. When the -form is defined on an -dimensional manifold with , then the -form can be integrated over oriented -dimensional submanifolds. If , integration over oriented 0-dimensional submanifolds is just the summation of the integrand evaluated at points, with according to the orientation of those points. Other values of correspond to line integrals, surface integrals, volume integrals, and so on. There are several equivalent ways to formally define the integral of a differential form, all of which depend on reducing to the case of Euclidean space.

## Integration on Euclidean space

Let be an open subset of . Give its standard orientation and the restriction of that orientation. Every smooth -form on has the form :$\omega = f\left(x\right)\,dx^1 \wedge \cdots \wedge dx^n$ for some smooth function . Such a function has an integral in the usual Riemann or Lebesgue sense. This allows us to define the integral of to be the integral of : :$\int_U \omega\ \stackrel \int_U f\left(x\right)\,dx^1 \cdots dx^n.$ Fixing an orientation is necessary for this to be well-defined. The skew-symmetry of differential forms means that the integral of, say, must be the negative of the integral of . Riemann and Lebesgue integrals cannot see this dependence on the ordering of the coordinates, so they leave the sign of the integral undetermined. The orientation resolves this ambiguity.

## Integration over chains

Let be an -manifold and an -form on . First, assume that there is a parametrization of by an open subset of Euclidean space. That is, assume that there exists a diffeomorphism :$\varphi \colon D \to M$ where . Give the orientation induced by . Then defines the integral of over to be the integral of over . In coordinates, this has the following expression. Fix a chart on with coordinates . Then :$\omega = \sum_ a_\left(\right)\,dx^ \wedge \cdots \wedge dx^.$ Suppose that is defined by :$\varphi\left(\right) = \left(x^1\left(\right),\ldots,x^n\left(\right)\right).$ Then the integral may be written in coordinates as :$\int_M \omega = \int_D \sum_ a_\left(\varphi\left(\right)\right) \frac\,du^1 \cdots du^n,$ where :$\frac$ is the determinant of the Jacobian matrix and determinant, Jacobian. The Jacobian exists because is differentiable. In general, an -manifold cannot be parametrized by an open subset of . But such a parametrization is always possible locally, so it is possible to define integrals over arbitrary manifolds by defining them as sums of integrals over collections of local parametrizations. Moreover, it is also possible to define parametrizations of -dimensional subsets for , and this makes it possible to define integrals of -forms. To make this precise, it is convenient to fix a standard domain in , usually a cube or a simplex. A -chain is a formal sum of smooth embeddings . That is, it is a collection of smooth embeddings, each of which is assigned an integer multiplicity. Each smooth embedding determines a -dimensional submanifold of . If the chain is :$c = \sum_^r m_i \varphi_i,$ then the integral of a -form over is defined to be the sum of the integrals over the terms of : :$\int_c \omega = \sum_^r m_i \int_D \varphi_i^*\omega.$ This approach to defining integration does not assign a direct meaning to integration over the whole manifold . However, it is still possible to assign such a meaning indirectly because every smooth manifold may be smoothly Triangulation (topology), triangulated in an essentially unique way, and the integral over may be defined to be the integral over the chain determined by a triangulation.

## Integration using partitions of unity

There is another approach, expounded in , which does directly assign a meaning to integration over , but this approach requires fixing an orientation of . The integral of an -form on an -dimensional manifold is defined by working in charts. Suppose first that is supported on a single positively oriented chart. On this chart, it may be pulled back to an -form on an open subset of . Here, the form has a well-defined Riemann or Lebesgue integral as before. The change of variables formula and the assumption that the chart is positively oriented together ensure that the integral of is independent of the chosen chart. In the general case, use a partition of unity to write as a sum of -forms, each of which is supported in a single positively oriented chart, and define the integral of to be the sum of the integrals of each term in the partition of unity. It is also possible to integrate -forms on oriented -dimensional submanifolds using this more intrinsic approach. The form is pulled back to the submanifold, where the integral is defined using charts as before. For example, given a path , integrating a -form on the path is simply pulling back the form to a form on , and this integral is the integral of the function on the interval.

## Integration along fibers

Fubini's theorem states that the integral over a set that is a product may be computed as an iterated integral over the two factors in the product. This suggests that the integral of a differential form over a product ought to be computable as an iterated integral as well. The geometric flexibility of differential forms ensures that this is possible not just for products, but in more general situations as well. Under some hypotheses, it is possible to integrate along the fibers of a smooth map, and the analog of Fubini's theorem is the case where this map is the projection from a product to one of its factors. Because integrating a differential form over a submanifold requires fixing an orientation, a prerequisite to integration along fibers is the existence of a well-defined orientation on those fibers. Let and be two orientable manifolds of pure dimensions and , respectively. Suppose that is a surjective submersion. This implies that each fiber is -dimensional and that, around each point of , there is a chart on which looks like the projection from a product onto one of its factors. Fix and set . Suppose that :$\begin \omega_x &\in ^m T_x^*M, \\ \eta_y &\in ^n T_y^*N, \end$ and that does not vanish. Following , there is a unique :$\sigma_x \in ^ T_x^*\left(f^\left(y\right)\right)$ which may be thought of as the fibral part of with respect to . More precisely, define to be the inclusion. Then is defined by the property that :$\omega_x = \left(f^*\eta_y\right)_x \wedge \sigma\text{'}_x \in ^m T_x^*M,$ where :$\sigma\text{'}_x \in ^ T_x^*M$ is any -covector for which :$\sigma_x = j^*\sigma\text{'}_x.$ The form may also be notated . Moreover, for fixed , varies smoothly with respect to . That is, suppose that :$\omega \colon f^\left(y\right) \to T^*M$ is a smooth section of the projection map; we say that is a smooth differential -form on along . Then there is a smooth differential -form on such that, at each , :$\sigma_x = \omega_x / \eta_y.$ This form is denoted . The same construction works if is an -form in a neighborhood of the fiber, and the same notation is used. A consequence is that each fiber is orientable. In particular, a choice of orientation forms on and defines an orientation of every fiber of . The analog of Fubini's theorem is as follows. As before, and are two orientable manifolds of pure dimensions and , and is a surjective submersion. Fix orientations of and , and give each fiber of the induced orientation. Let be an -form on , and let be an -form on that is almost everywhere positive with respect to the orientation of . Then, for almost every , the form is a well-defined integrable form on . Moreover, there is an integrable -form on defined by :$y \mapsto \bigg\left(\int_ \theta / \zeta_y\bigg\right)\,\zeta_y.$ Denote this form by :$\bigg\left(\int_ \theta / \zeta\bigg\right)\,\zeta.$ Then proves the generalized Fubini formula :$\int_M \theta = \int_N \bigg\left(\int_ \theta / \zeta\bigg\right)\,\zeta.$ It is also possible to integrate forms of other degrees along the fibers of a submersion. Assume the same hypotheses as before, and let be a compactly supported -form on . Then there is a -form on which is the result of integrating along the fibers of . The form is defined by specifying, at each , how pairs against each -vector at , and the value of that pairing is an integral over that depends only on , , and the orientations of and . More precisely, at each , there is an isomorphism :$^k T_yN \to ^ T_y^*N$ defined by the interior product :$\mathbf \mapsto \mathbf\,\lrcorner\,\zeta_y.$ If , then a -vector at determines an -covector at by pullback: :$f^*\left(\mathbf\,\lrcorner\,\zeta_y\right) \in ^ T_x^*M.$ Each of these covectors has an exterior product against , so there is an -form on along defined by :$\left(\beta_\right)_x = \left\left(\alpha_x \wedge f^*\left(\mathbf\,\lrcorner\,\zeta_y\right)\right\right) \big/ \zeta_y \in ^ T_x^*M.$ This form depends on the orientation of but not the choice of . Then the -form is uniquely defined by the property :$\langle\gamma_y, \mathbf\rangle = \int_ \beta_\left(x\right),$ and is smooth . This form also denoted and called the integral of along the fibers of . Integration along fibers is important for the construction of Gysin maps in de Rham cohomology. Integration along fibers satisfies the projection formula . If is any -form on , then :$\alpha^\flat \wedge \lambda = \left(\alpha \wedge f^*\lambda\right)^\flat.$

## Stokes's theorem

The fundamental relationship between the exterior derivative and integration is given by the
Stokes' theorem Stokes' theorem, also known as Kelvin–Stokes theorem Nagayoshi Iwahori, et al.:"Bi-Bun-Seki-Bun-Gaku" :ja:裳華房, Sho-Ka-Bou(jp) 1983/12Written in Japanese)Atsuo Fujimoto;"Vector-Kai-Seki Gendai su-gaku rekucha zu. C(1)" :ja:培風館, Ba ...
: If is an ()-form with compact support on and denotes the manifold, boundary of with its induced Orientation (mathematics), orientation, then :$\int_M d\omega = \int_ \omega.$ A key consequence of this is that "the integral of a closed form over homologous chains is equal": If is a closed -form and and are -chains that are homologous (such that is the boundary of a -chain ), then $\textstyle$, since the difference is the integral $\textstyle\int_W d\omega = \int_W 0 = 0$. For example, if is the derivative of a potential function on the plane or , then the integral of over a path from to does not depend on the choice of path (the integral is ), since different paths with given endpoints are homotopic, hence homologous (a weaker condition). This case is called the gradient theorem, and generalizes the
fundamental theorem of calculus The fundamental theorem of calculus is a theorem that links the concept of derivative, differentiating a function (mathematics), function (calculating the gradient) with the concept of integral, integrating a function (calculating the area under t ...
. This path independence is very useful in contour integration. This theorem also underlies the duality between de Rham cohomology and the homology (mathematics), homology of chains.

## Relation with measures

On a ''general'' differentiable manifold (without additional structure), differential forms ''cannot'' be integrated over subsets of the manifold; this distinction is key to the distinction between differential forms, which are integrated over chains or oriented submanifolds, and measures, which are integrated over subsets. The simplest example is attempting to integrate the -form over the interval . Assuming the usual distance (and thus measure) on the real line, this integral is either or , depending on ''orientation:'' $\textstyle$, while $\textstyle$. By contrast, the integral of the ''measure'' on the interval is unambiguously (i.e. the integral of the constant function with respect to this measure is ). Similarly, under a change of coordinates a differential -form changes by the Jacobian determinant , while a measure changes by the ''absolute value'' of the Jacobian determinant, , which further reflects the issue of orientation. For example, under the map on the line, the differential form pulls back to ; orientation has reversed; while the Lebesgue measure, which here we denote , pulls back to ; it does not change. In the presence of the additional data of an ''orientation'', it is possible to integrate -forms (top-dimensional forms) over the entire manifold or over compact subsets; integration over the entire manifold corresponds to integrating the form over the fundamental class of the manifold, . Formally, in the presence of an orientation, one may identify -forms with densities on a manifold; densities in turn define a measure, and thus can be integrated . On an orientable but not oriented manifold, there are two choices of orientation; either choice allows one to integrate -forms over compact subsets, with the two choices differing by a sign. On non-orientable manifold, -forms and densities cannot be identified —notably, any top-dimensional form must vanish somewhere (there are no
volume formIn mathematics Mathematics (from Ancient Greek, Greek: ) includes the study of such topics as quantity (number theory), mathematical structure, structure (algebra), space (geometry), and calculus, change (mathematical analysis, analysis). It ha ...
s on non-orientable manifolds), but there are nowhere-vanishing densities— thus while one can integrate densities over compact subsets, one cannot integrate -forms. One can instead identify densities with top-dimensional Volume form#Relation to measures, pseudoforms. Even in the presence of an orientation, there is in general no meaningful way to integrate -forms over subsets for because there is no consistent way to use the ambient orientation to orient -dimensional subsets. Geometrically, a -dimensional subset can be turned around in place, yielding the same subset with the opposite orientation; for example, the horizontal axis in a plane can be rotated by 180 degrees. Compare the Gram determinant of a set of vectors in an -dimensional space, which, unlike the determinant of vectors, is always positive, corresponding to a squared number. An orientation of a -submanifold is therefore extra data not derivable from the ambient manifold. On a Riemannian manifold, one may define a -dimensional Hausdorff measure for any (integer or real), which may be integrated over -dimensional subsets of the manifold. A function times this Hausdorff measure can then be integrated over -dimensional subsets, providing a measure-theoretic analog to integration of -forms. The -dimensional Hausdorff measure yields a density, as above.

## Currents

The differential form analog of a distribution (mathematics), distribution or generalized function is called a Current (mathematics), current. The space of -currents on is the dual space to an appropriate space of differential -forms. Currents play the role of generalized domains of integration, similar to but even more flexible than chains.

# Applications in physics

Differential forms arise in some important physical contexts. For example, in Maxwell's theory of electromagnetism, the Faraday 2-form, or electromagnetic field strength, is :$\textbf = \frac 1 2 f_\, dx^a \wedge dx^b\,,$ where the are formed from the electromagnetic fields $\vec E$ and $\vec B$; e.g., , , or equivalent definitions. This form is a special case of the curvature form on the principal bundle on which both electromagnetism and general gauge theories may be described. The connection form for the principal bundle is the vector potential, typically denoted by , when represented in some gauge. One then has :$\textbf = d\textbf.$ The current -form is : $\textbf = \frac 1 6 j^a\, \varepsilon_\, dx^b \wedge dx^c \wedge dx^d\,,$ where are the four components of the current density. (Here it is a matter of convention to write instead of , i.e. to use capital letters, and to write instead of . However, the vector rsp. tensor components and the above-mentioned forms have different physical dimensions. Moreover, by decision of an international commission of the International Union of Pure and Applied Physics, the magnetic polarization vector has been called $\vec J$ for several decades, and by some publishers ; i.e., the same name is used for different quantities.) Using the above-mentioned definitions, Maxwell's equations can be written very compactly in geometrized units as :$\begin d &= \textbf \\ d &= \textbf, \end$ where $\star$ denotes the Hodge star operator. Similar considerations describe the geometry of gauge theories in general. The -form $\mathbf$, which is duality (mathematics), dual to the Faraday form, is also called Maxwell 2-form. Electromagnetism is an example of a gauge theory. Here the Lie group is , the one-dimensional unitary group, which is in particular abelian group, abelian. There are gauge theories, such as Yang–Mills theory, in which the Lie group is not abelian. In that case, one gets relations which are similar to those described here. The analog of the field in such theories is the curvature form of the connection, which is represented in a gauge by a Lie algebra-valued one-form . The Yang–Mills field is then defined by :$\mathbf = d\mathbf + \mathbf\wedge\mathbf.$ In the abelian case, such as electromagnetism, , but this does not hold in general. Likewise the field equations are modified by additional terms involving exterior products of and , owing to the Maurer–Cartan form, structure equations of the gauge group.

# Applications in geometric measure theory

Numerous minimality results for complex analytic manifolds are based on the Wirtinger inequality (2-forms), Wirtinger inequality for 2-forms. A succinct proof may be found in Herbert Federer's classic text ''Geometric Measure Theory''. The Wirtinger inequality is also a key ingredient in Gromov's inequality for complex projective space in systolic geometry.