FACTOID # 138: Libya’s full name is the Great Socialist People’s Libyan Arab Jamahiriya.
 
 Home   Encyclopedia   Statistics   Countries A-Z   Flags   Maps   Education   Forum   FAQ   About 
 
WHAT'S NEW
RECENT ARTICLES
More Recent Articles »
 

FACTS & STATISTICS    Simple view

  1. Select countries to view: (hold down Control key and click to select several)

     

     

    Compare:

     

     

  1. Select fact or statistic: (* = graphable)

     

     

     

  2. (OPTIONAL) Compare to statistic: (both need to be graphable)

     

     

     

  3. View result as:

     

       
(OR) SEARCH ALL encyclopedia, stats & forums:   

Encyclopedia > Push forward

In mathematics, the push forward (or pushforward) of a smooth map F : MN between smooth manifolds at a point p is, in some sense, the best linear approximation of F near p. It can be viewed as generalization of the total derivative of ordinary calculus. Explicitly, it is a linear map from the tangent space of M at p to the tangent space of N at F(p). For other meanings of mathematics or math, see mathematics (disambiguation). ... In mathematics, a smooth function is one that is infinitely differentiable, i. ... In mathematics, a manifold M is a type of space, characterized in one of two equivalent ways: near every point of the space, we have a coordinate system; or near every point, the environment is like that in Euclidean space of a given dimension. ... In mathematics, a total derivative may be either. ... In mathematics, a linear transformation (also called linear operator or linear map) is a function between two vector spaces that respects the arithmetical operations addition and scalar multiplication defined on vector spaces, or, in other words, it preserves linear combinations. Definition and first consequences Formally, if V and W are... The tangent space of a manifold is a concept which facilitates the generalization of vectors from affine spaces to general manifolds, since in the latter case one cannot simply subtract two points to obtain a vector pointing from one to the other. ...


The push forward of a map F is also called, by various authors, the derivative, total derivative, or differential of F.


The notion of push forward also exists in measure theory as the measure induced on Y by a measurable function f : X to Y, given a measure on X. In mathematics, a measure is a function that assigns a number, e. ...

Contents

Motivation

Let F:Uto V be a smooth map from an open subset, U, of mathbb R^n to an open subset, V, of mathbb R^m. Let (x^1,ldots,x^n) be the coordinates in U and (y^1,ldots,y^m) those in V. For any pin U, the Jacobian of F is the matrix representation of the total derivative In mathematics, a smooth function is one that is infinitely (indefinitely) differentiable, i. ... In topology and related fields of mathematics, a set U is called open if, intuitively speaking, you can wiggle or change any point x in U by a small amount in any direction and still be inside U. In other words, if x is surrounded only by elements of U... In mathematics as applied to geometry, physics or engineering, a coordinate system is a system for assigning a tuple of numbers to each point in an n-dimensional space. ... In vector calculus, the Jacobian is shorthand for either the Jacobian matrix or its determinant, the Jacobian determinant. ... In mathematics, a matrix (plural matrices) is a rectangular table of numbers or, more generally, a table consisting of abstract quantities that can be added and multiplied. ...

DF(p):mathbb R^ntomathbb R^m.

We wish to generalize this to the case that F is a smooth function between any smooth manifolds M and N. On a sphere, the sum of the angles of a triangle is not equal to 180°. A sphere is not a Euclidean space, but locally the laws of the Euclidean geometry are good approximations. ...


Definition

Let F:Mto N be a smooth map of smooth manifolds. Given some pin M, the push forward is a linear map

F_*:T_pMto T_{F(p)}N,

from the tangent space of M at p to the tangent space of N at F(p). The exact definition depends on the definition one uses for tangent vectors (for the various definitions see tangent space). The tangent space of a manifold is a concept which facilitates the generalization of vectors from affine spaces to general manifolds, since in the latter case one cannot simply subtract two points to obtain a vector pointing from one to the other. ... The tangent space of a manifold is a concept which facilitates the generalization of vectors from affine spaces to general manifolds, since in the latter case one cannot simply subtract two points to obtain a vector pointing from one to the other. ...


If one defines tangent vectors as equivalence classes of curves through p then the push forward is given by

F_{*}(gamma'(0)) = (F circ gamma)'(0)

Here γ is a curve in M with γ(0) = p. The push forward is just the tangent vector to the curve Fcirc gamma at 0.


Alternatively, if tangent vectors are defined as derivations acting on smooth real-valued functions the push forward is given by In abstract algebra, a derivation on an algebra A over a field k is a linear map D : A → A that satisfies Leibniz law: D(ab) = (Da)b + a(Db). ...

F_{*}(X)(f) = X(f circ F)

Here X in T_pM, therefore x is a derivative defined on M and f is a smooth real-valued function on N. By definition, the push-forward of X is in TF(p)N and therefore itself is a derivative. In component notation the definition becomes,

(F_*(X))^apartial_a (f)=X^bpartial_b F^apartial_a f

therefore by identifying the following relation,

(F_*)^a_{;b}= frac{partial F^a}{partial x^b}

one can understand push-forward roughly as a coordinate transformation. Note that the push-forward is not guaranteed to have an inverse. Therefore in general we cannot define pullback for vectors. This article needs to be cleaned up to conform to a higher standard of quality. ...


The push forward is frequently expressed using a variety of other notations such as

dF_p,;DF_p,;F'(p)

Properties

One can show that push forward of a composition is the composition of push forwards (i.e., functorial behaviour), and the push forward of a local diffeomorphism is an isomorphism of tangent spaces. In mathematics, a composite function, formed by the composition of one function on another, represents the application of the former to the result of the application of the latter to the argument of the composite. ... Did somebody just say functor? In category theory, a functor is a special type of mapping between categories. ... In mathematics, a local diffeomorphism is a smooth map f : M → N between smooth manifolds such that for every point p of M there exists an open neighbourhood U of p such that f(U) is open in N and f|U : U → f(U) is a diffeomorphism. ... In mathematics, an isomorphism (in Greek isos = equal and morphe = shape) is a kind of mapping between objects, devised by Eilhard Mitscherlich, which shows a relation between two properties or operations. ...


Returning to the motivating example, it can be shown that the push forward of Fcolon Uto V, in the given standard coordinates, is the matrix J whose entries are J_{ij}=partial F^{i}/partial x^j(p). This is the Jacobian of F. More generally, given a smooth map F:Mto N the push forward of F written in local coordinates will always be given by the Jacobian of F in those coordinates.


The push forward of F induces in an obvious manner a vector bundle morphism from the tangent bundle of M to the tangent bundle of N: In mathematics, a vector bundle is a geometrical construct where to every point of a topological space (or manifold, or algebraic variety) we attach a vector space in a compatible way, so that all those vector spaces, glued together, form another topological space (or manifold or variety). ... In mathematics, the tangent bundle of a differentiable manifold M, denoted by T(M) or just TM, is the disjoint union of the tangent spaces to each point of M An element of T(M) is a pair (x,v) where x ∈ M and v ∈ Tx(M), the tangent space...

Wikipedia does not have an article with this exact name. ...

Push forwards of vector fields

Although one can always push forward tangent vectors, the push forward of a vector field does not always make sense. For example, if the map F is not surjective how should one define the vector outside the range of F? Conversely, if F is not injective there may be more than one choice of the push forward of the field at a given point. Vector field given by vectors of the form (-y, x) In mathematics a vector field is a construction in vector calculus which associates a vector to every point in a Euclidean space. ...


There is one special situation where one can push forward vector fields, namely if the map F is a diffeomorphism. In this case, suppose X is a vector field on M, the push forward defines a vector field Y on N, given by Y = F * X with In mathematics, a diffeomorphism is a kind of isomorphism of smooth manifolds. ...

Y_p=F_*(X_{F^{-1}(p)})

Here, F − 1(p) maps the point p back from the manifold N to the manifold M. Then X_{F^{-1}(p)} is the vector field at the point F − 1(p) on M.


Push forward in measure theory

Given two measurable spaces (X, mathcal{A}) and (Y, mathcal{B}), a function f : X to Y is called measurable if the pre-image of any measurable set in Y is measurable in X: In mathematics, a σ-algebra (or σ-field) X over a set S is a family of subsets of S which is closed under countable set operations; σ-algebras are mainly used in order to define measures on S. The concept is important in mathematical analysis and probability theory. ...

B in mathcal{B} implies f^{-1} (B) in mathcal{A}.

If the space (X, mathcal{A}) is equipped with a measure mu : mathcal{A} to [0, + infty], the push forward of μ by a measurable function f : X to Y is the measure f_{*} (mu) : mathcal{B} to [0, + infty] defined by In mathematics, a measure is a function that assigns a number, e. ...

(f_{*} (mu)) (B) := mu left( f^{-1} (B) right).

See also

This article needs to be cleaned up to conform to a higher standard of quality. ...

References

  • John M. Lee, Introduction to Smooth Manifolds, (2003) Springer Graduate Texts in Mathematics 218.
  • Jurgen Jost, Riemannian Geometry and Geometric Analysis, (2002) Springer-Verlag, Berlin ISBN 3-540-42627-2 See section 1.6.
  • Ralph Abraham and Jarrold E. Marsden, Foundations of Mechanics, (1978) Benjamin-Cummings, London ISBN 0-8053-0102-X See section 1.7 and 2.3.

  Results from FactBites:
 
Forward Stroking For Greater Efficiency- Speedskating Santa Barbara (1289 words)
What is novel is that you can push for an unexpectedly large range of angles around the forward direction and still maintain an efficiency in the 90% range (the angle between the applied force and the forward direction is twice the angle plotted here so this range is even greater than it appears).
The situation is the same in the double push where the forward push is handled with body shifts, rotations, or thrusts depending on style.
Because of this limitation the amount of forward push is not too great and is best used briefly -- for example as the termination of a standard sideways push to develop additional forward thrust (see drawings here).
  More results at FactBites »


 

COMMENTARY     


Share your thoughts, questions and commentary here
Your name
Your comments
Please enter the 5-letter protection code

Want to know more?
Search encyclopedia, statistics and forums:

 


Lesson Plans | Student Area | Student FAQ | Reviews | Press Releases |  Feeds | Contact
The Wikipedia article included on this page is licensed under the GFDL.
Images may be subject to relevant owners' copyright.
All other elements are (c) copyright NationMaster.com 2003-5. All Rights Reserved.
Usage implies agreement with terms.