Transformations géométriques : rotation et translation
une rotation autour de l'origine d'un angle θ antihoraire. • Opération linéaire* : multiplication de matrice. 179 x y θ. 2. 1 cos sin.
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La matrice (vecteur) de translation opère selon l'axe 0 y . La matrice de rotation (d'angle nul) est telle que : 0. 1. 0. 1.
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// compose avec une matrice de translation. (multiplication à droite) m1. rotate ( angle axisX
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Si on tourne ce repère de l'angle de la rotation ces vecteurs se confondent avec les axes. Si l'on considère les deux vecteurs colonnes de la sous matrice et.
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Cette relation permet donc d'exprimer toute matrice de translation en fonction des matrices composantes de . 2 Les rotations. Une rotation peut être définie
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17/06/2003 la matrice de rotation d'angle θ. On peut le voir simplement ... En utilisant la conjugaison par la matrice de la translation de vecteur. −− ...
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16 janv. 2017 sense i.e.
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22 janv. 2014 mouvements (translation) des informations sur les surfaces ... z
Untitled
matrix to rotation and translation? Page 7. [ ]×. = E t R. = t E 0. T. : Left nullspace of the essential matrix is the epipole in image 2.
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4 sept. 2020 Point + Vecteur = Point (translation du point). • Point + Point = rien ! ... Matrice de rotation autour de l'axe des z :.
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translation and rotation cause fundamentally different flow fields on the tion that involves the fundamental or essential matrix between the two images.
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on multiplie les matrices représentant les transformations élémentaires. ? Exemple: Rotation autour d'un axe // à l 'axe x. ? Matrice
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vector by a rotation matrix R and addition of a translation vector t. For this purpose we work in an orthogonal Cartesian system in a?ngstro?ms: conversion
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translation: 3 units right reflection across the y-axis rotation 90° clockwise about the origin translation: 1 unit right and 3 units uprotation 180° about the origin Create your own worksheets like this one with Infinite Algebra 2 Free trial available at KutaSoftware com
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The rststepistousetranslationtoreducetheproblemtothatof rotationabouttheorigin: =T(p0)RT( p0): To ndtherotationmatrixRforrotationaroundthevectoru we rstalignuwiththezaxis usingtworotations xand y Thenwecanapply rotationof aroundthez-axisandafterwardsundothealignments thus =Rx( x)Ry( y)Rz( )Ry( y)Rx( x):
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ROTATIONS AND REFLECTIONS USING MATRICES Earlier in your course you looked at a variety of ways in which a shape could be moved around on squared paper We studied: translation reflection rotation In each of these the size of the original shape remained fixed
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The standard rotation matrix is used to rotate about the origin (00) cos(?) -sin(?) 0 Affine matrix = translation x shearing x scaling x rotation
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Rotationofskewsymmetricmatrices ForanyrotationmatrixR: ?T RwR= ations ? (Rw) 3 inR The (described (described by {A}) to its new position by{B}) vector inthesecondpositionorientation 10 SE () 3 = http://www seas upenn edu/~meam520/notes02/RigidBodyMotion3 pdf 12 SE(3)isaLiegroup SE(3)satisfiesthefouraxiomsthatmustbesatisfiedbytheelementsofan
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What is rotation matrix?
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How do you describe a rotation about the origin followed by translation?
A rotation about the origin followed by a translation may be described by a single matrix where is the rotation matrix, is the translation, and is the vector of zeros. Since the last row of the rotation-translation matrix is always , they are sometimes shorthanded to a augmented matrix
How do you combine translation and rotation in robotics?
Combining translation and rotation Suppose a rotation by is performed, followed by a translation by . This can be used to place the robot in any desired position and orientation. Note that translations and rotations do not commute!
Least-Squares Rigid Motion Using SVD
Olga Sorkine-Hornung and Michael Rabinovich
Department of Computer Science, ETH Zurich
January 16, 2017Abstract
This note summarizes the steps to computing the best-tting rigid transformation that aligns two sets of corresponding points. Keywords:Shape matching, rigid alignment, rotation, SVD1 Problem statement LetP=fp1;p2;:::;pngandQ=fq1;q2;:::;qngbe two sets of corresponding points inRd. We wish to nd a rigid transformation that optimally aligns the two sets in the least squares sense, i.e., we seek a rotationRand a translation vectortsuch that (R;t) = argminR2SO(d);t2Rdn
X i=1w ik(Rpi+t)qik2;(1) wherewi>0 are weights for each point pair. In the following we detail the derivation ofRandt; readers that are interested in the nal recipe may skip the proofs and go directly Section 4.2 Computing the translation
AssumeRis xed and denoteF(t) =Pn
i=1wik(Rpi+t)qik2. We can nd the optimal translation by taking the derivative ofFw.r.t.tand searching for its roots: 0 = @F@t=nX i=12wi(Rpi+tqi) = = 2t nX i=1w i! + 2R nX i=1w ipi! 2nX i=1w iqi:(2)Denote
p=P n i=1wipiP n i=1wi;q=P n i=1wiqiP n i=1wi:(3) 1By rearranging the terms of (2) we get
t=qRp:(4) In other words, the optimal translationtmaps the transformed weighted centroid ofPto the weighted centroid ofQ. Let us plug the optimaltinto our objective function: n X i=1w ik(Rpi+t)qik2=nX i=1w ikRpi+qRpqik2= (5) nX i=1w ikR(pip)(qiq)k2:(6) We can thus concentrate on computing the rotationRby restating the problem such that the translation would be zero: x i:=pip;yi:=qiq:(7)So we look for the optimal rotationRsuch that
R= argmin
R2SO(d)n
X i=1w ikRxiyik2:(8)3 Computing the rotation
Let us simplify the expression we are trying to minimize in (8): kRxiyik2= (Rxiyi)T(Rxiyi) = (xTiRTyTi)(Rxiyi) = =xTiRTRxiyTiRxixTiRTyi+yTiyi= =xTixiyTiRxixTiRTyi+yTiyi:(9) We got the last step by remembering that rotation matrices implyRTR=I(Iis the identity matrix). Note thatxTiRTyiis a scalar:xTihas dimension 1d,RTisddandyiisd1. For any scalar awe trivially havea=aT, therefore xTiRTyi= (xTiRTyi)T=yTiRxi:(10)
Therefore we have
kRxiyik2=xTixi2yTiRxi+yTiyi:(11) Let us look at the minimization and substitute the above expression: argminR2SO(d)n
X i=1w ikRxiyik2= argminR2SO(d)n
X i=1w i(xTixi2yTiRxi+yTiyi) = = argminR2SO(d)
nX i=1w ixTixi2nX i=1w iyTiRxi+nX i=1w iyTiyi! = argminR2SO(d)
2nX i=1w iyTiRxi! :(12) 2 2 6 664w1 w 2... w n3 7 7752
6
664|yT1|
|yT2| |yTn|3 7 77524 R3 52
4j j j
x1x2:::xn
j j j3 5 2 6664|w1yT1|
|w2yT2| |wnyTn|3 7 77524j j j
Rx1Rx2::: Rxn
j j j3 5 =2 6 664w1yT1Rx1
w2yT2Rx2...
wnyTnRxn3 7 775Figure 1: Schematic explanation of
Pn i=1wiyTiRxi= tr(WYTRX).The last step (removing
Pn i=1wixTixiandPn i=1wiyTiyi) holds because these expressions do not depend onRat all, so excluding them would not aect the minimizer. The same holds for multiplication of the minimization expression by a scalar, so we have argminR2SO(d)
2nX i=1w iyTiRxi! = argmaxR2SO(d)n
X i=1w iyTiRxi:(13)We note that
nX i=1w iyTiRxi= tr WYTRX ;(14) whereW= diag(w1;:::;wn) is annndiagonal matrix with the weightwion diagonal entryi; Yis thednmatrix withyias its columns andXis thednmatrix withxias its columns. We remind the reader that the trace of a square matrix is the sum of the elements on the diagonal: tr(A) =Pn i=1aii. See Figure 1 for an illustration of the algebraic manipulation. Therefore we are looking for a rotationRthat maximizes trWYTRX. Matrix trace has the property tr(AB) = tr(BA) (15) for any matricesA;Bof compatible dimensions. Therefore tr WYTRX = tr (WYT)(RX) = tr RXWYT :(16) Let us denote thedd\covariance" matrixS=XWYT. Take SVD ofS:S=UVT:(17)
Now substitute the decomposition into the trace we are trying to maximize: tr RXWYT = tr(RS) = tr RUVT = tr VTRU :(18) The last step was achieved using the property of trace (15). Note thatV,RandUare all orthogonal matrices, soM=VTRUis also an orthogonal matrix. This means that the columns ofMare orthonormal vectors, and in particular,mTjmj= 1 for eachM's columnmj. Therefore all entriesmijofMare1 in magnitude:1 =mTjmj=dX
i=1m2ij)m2ij1) jmijj 1:(19)
3 So what is the maximum possible value fortr(M)? Remember that is a diagonal matrix with non-negative values1;2;:::;d0 on the diagonal. Therefore: tr(M) =12...d!
m11m12::: m1dm21m22::: m2d............md1md2::: mdd! =dX i=1 imiidX i=1 i:(20) Therefore the trace is maximized ifmii= 1. SinceMis an orthogonal matrix, this means thatMwould have to be the identity matrix!
I=M=VTRU)V=RU)R=V UT:(21)
Orientation rectication.The process we just described nds the optimalorthogonalma- trix, which could potentially contain re ections in addition to rotations. Imagine that the point setPis a perfect re ection ofQ. We will then nd that re ection, which aligns the two point sets perfectly and yields zero energy in (8), the global minimum in this case. However, if werestrict ourselves to rotations only, there might not be a rotation that perfectly aligns the points.
Checking whetherR=V UTis a rotation is simple: if det(V UT) =1 then it contains a re ection, otherwise det(V UT) = +1. Assume det(V UT) =1. RestrictingRto a rotation is equivalent to restrictingMto a re ection. We now want to nd a re ectionMthat maximizes: tr(M) =1m11+2m22+:::+dmdd=:f(m11;:::;mdd):(22) Note thatfonly depends on the diagonal ofM, not its other entries. We now consider themii's as variables (m11;:::;mdd). This is the set of all diagonals of re ection matrices of ordern. Surprisingly, it has a very simple structure. Indeed, a result by A. Horn [1] states that the set of all diagonals of rotation matrices of ordernis equal to the convex hull of the points (1;:::;1) with an even number of coordinates that are1. Since any re ection matrix can be constructed by inverting the sign of a row of a rotation matrix and vice versa, it follows that the set we are optimizing on is the convex hull of the points (1;:::;1) with anunevennumber of1's. Since our domain is a convex polyhedron, the linear functionfattains its extrema at its vertices. The diagonal (1;1;:::;1) is not in the domain since it has an even number of1's (namely, zero), and therefore the next best shot is (1;1;:::;1;1): tr(M) =1+2+:::+d1d:(23) This value is attained at a vertex of our domain, and is larger than any other combination of the form (1;:::;1) except (1;1;:::;1), becausedis the smallest singular value. To summarize, we arrive at the fact that if det(V UT) =1, we needM=VTRU=0
@11...111
A )R=V0 @11...111
AUT:(24)
We can write a general formula that encompasses both cases, det(V UT) = 1 and det(V UT) =1: R=V0 B @1 1...1 det(V UT)1 CAUT:(25)
44 Rigid motion computation { summary
Let us summarize the steps to computing the optimal translationtand rotationRthat minimize n X i=1w ik(Rpi+t)qik2:1. Compute the weighted centroids of both point sets:
p=P n i=1wipiP n i=1wi;q=P n i=1wiqiP n i=1wi:2. Compute the centered vectors
x i:=pip;yi:=qiq; i= 1;2;:::;n:3. Compute theddcovariance matrix
S=XWYT;
whereXandYare thednmatrices that havexiandyias their columns, respectively, andW= diag(w1;w2;:::;wn).4. Compute the singular value decompositionS=UVT. The rotation we are looking for is
then R=V0 B @1 1...1 det(V UT)1 C AUT:5. Compute the optimal translation as
t=qRp:Acknowledgments
We are grateful to Julian Panetta, Zohar Levi and Mario Botsch for their help with improving this note.References
[1] A. Horn,Doubly stochastic matrices and the diagonal of a rotation matrix. Amer. J. Math.76:620{630 (1954).
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