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Geometric transformation

From Wikipedia, the free encyclopedia
Bijection of a set using properties of shapes in space
For broader coverage of this topic, seeTransformation (mathematics).

Inmathematics, ageometric transformation is anybijection of aset to itself (or to another such set) with some salientgeometrical underpinning, such as preserving distances,angles, or ratios (scale). More specifically, it is afunction whosedomain andrange are sets ofpoints – most often areal coordinate space,R2{\displaystyle \mathbb {R} ^{2}} orR3{\displaystyle \mathbb {R} ^{3}} – such that the function is bijective so that itsinverse exists.[1] The study of geometry may be approached by the study of these transformations, such as intransformation geometry.[2]

Classifications

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Geometric transformations can be classified by the dimension of their operand sets (thus distinguishing between, say, planar transformations and spatial transformations). They can also be classified according to the properties they preserve:

Each of these classes contains the previous one.[8]

  • Conformal transformations preserve angles, and are, in the first order, similarities.
  • Equiareal transformations, preserve areas in the planar case or volumes in the three dimensional case.[9] and are, in the first order, affine transformations ofdeterminant 1.
  • Homeomorphisms (bicontinuous transformations) preserve the neighborhoods of points.
  • Diffeomorphisms (bidifferentiable transformations) are the transformations that are affine in the first order; they contain the preceding ones as special cases, and can be further refined.

Transformations of the same type formgroups that may be sub-groups of other transformation groups.

Opposite group actions

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Main articles:Group action andOpposite group

Many geometric transformations are expressed with linear algebra. The bijective linear transformations are elements of ageneral linear group. Thelinear transformationA is non-singular. For arow vectorv, thematrix productvA gives another row vectorw =vA.

Thetranspose of a row vectorv is a column vectorvT, and the transpose of the above equality iswT=(vA)T=ATvT.{\displaystyle w^{T}=(vA)^{T}=A^{T}v^{T}.} HereAT provides a left action on column vectors.

In transformation geometry there arecompositionsAB. Starting with a row vectorv, the right action of the composed transformation isw =vAB. After transposition,

wT=(vAB)T=(AB)TvT=BTATvT.{\displaystyle w^{T}=(vAB)^{T}=(AB)^{T}v^{T}=B^{T}A^{T}v^{T}.}

Thus forAB the associated leftgroup action isBTAT.{\displaystyle B^{T}A^{T}.} In the study ofopposite groups, the distinction is made between opposite group actions becausecommutative groups are the only groups for which these opposites are equal.

Active and passive transformations

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This section is an excerpt fromActive and passive transformation.[edit]
In the active transformation (left), a pointP is transformed to pointP by rotating clockwise byangleθ about theorigin of a fixed coordinate system. In the passive transformation (right), pointP stays fixed, while the coordinate system rotates counterclockwise by an angleθ about its origin. The coordinates ofP after the active transformation relative to the original coordinate system are the same as the coordinates ofP relative to the rotated coordinate system.

Geometric transformations can be distinguished into two types:active or alibi transformations which change the physical position of a set ofpoints relative to a fixedframe of reference orcoordinate system (alibi meaning "being somewhere else at the same time"); and passive or alias transformations which leave points fixed but change the frame of reference or coordinate system relative to which they are described (alias meaning "going under a different name").[10][11] Bytransformation,mathematicians usually refer to active transformations, whilephysicists andengineers could mean either.[citation needed]

For instance, active transformations are useful to describe successive positions of arigid body. On the other hand, passive transformations may be useful in human motion analysis to observe the motion of thetibia relative to thefemur, that is, its motion relative to a (local) coordinate system which moves together with the femur, rather than a (global) coordinate system which is fixed to the floor.[11]

Inthree-dimensional Euclidean space, anyproper rigid transformation, whether active or passive, can be represented as ascrew displacement, the composition of atranslation along an axis and arotation about that axis.

The termsactive transformation andpassive transformation were first introduced in 1957 byValentine Bargmann for describingLorentz transformations inspecial relativity.[12]

See also

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References

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  1. ^Usiskin, Zalman; Peressini, Anthony L.;Marchisotto, Elena; Stanley, Dick (2003).Mathematics for High School Teachers: An Advanced Perspective. Pearson Education. p. 84.ISBN 0-13-044941-5.OCLC 50004269.
  2. ^Venema, Gerard A. (2006),Foundations of Geometry,Pearson Prentice Hall, p. 285,ISBN 9780131437005
  3. ^"Geometry Translation".www.mathsisfun.com. Retrieved2020-05-02.
  4. ^"Geometric Transformations — Euclidean Transformations".pages.mtu.edu. Retrieved2020-05-02.
  5. ^abGeometric transformation, p. 131, atGoogle Books
  6. ^"Transformations".www.mathsisfun.com. Retrieved2020-05-02.
  7. ^"Geometric Transformations — Affine Transformations".pages.mtu.edu. Retrieved2020-05-02.
  8. ^abLeland Wilkinson, D. Wills, D. Rope, A. Norton, R. Dubbs – 'Geometric transformation, p. 182, atGoogle Books
  9. ^Geometric transformation, p. 191, atGoogle Books Bruce E. Meserve – Fundamental Concepts of Geometry, page 191.]
  10. ^Crampin, M.; Pirani, F.A.E. (1986).Applicable Differential Geometry. Cambridge University Press. p. 22.ISBN 978-0-521-23190-9.
  11. ^abJoseph K. Davidson, Kenneth Henderson Hunt (2004)."§4.4.1 The active interpretation and the active transformation".Robots and screw theory: applications of kinematics and statics to robotics. Oxford University Press. p. 74ff.ISBN 0-19-856245-4.
  12. ^Bargmann, Valentine (1957). "Relativity".Reviews of Modern Physics.29 (2):161–174.Bibcode:1957RvMP...29..161B.doi:10.1103/RevModPhys.29.161.

Further reading

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