For the newcomer to CliffordAlgebra This is about mathematics which many people find so magical that they want to share it with everyone else. The problem that they have is of explaining clearly just what it is that is so special. People are also inclined to ask,
"If it so good why did nobody tell me about it?" and that is a long story. My personal response when I found out about
QuaternionMathematics about 15 years ago, was to ask,
"What else have I not been told?" and I had to wait another 10 years or so to find the answer,
CliffordAlgebra. I came back from a seminar and typed into a search engine "
WilliamKingdonClifford" and entered in through a door from which I have never completely returned.
It is as though someone had a large mirror on which mathematics was written. It got broken and during the nineteenth century different mathematicians found different pieces of the mirror. They started to put the pieces together, but somehow they couldn't get them to fit and then they argued and threw some of the pieces into a dark cupboard. Only since about 1966 have different people started to find the pieces and fit them together, and we have for a hundred years been taught that the pieces are separate and unrelated. So we go on teaching the fragments, when we could teach the whole.
Hestenes, who started the "putting together" has now proposed that physics teaching should be reformed to use the whole pattern. (see
HestenesOerstedMedalLecture)
For more on the history see
HistoryOfVectorAnalysis and
HistoryOfCliffordAlgebra
The late
PerttiLounesto, author of
CliffordAlgebrasAndSpinors http://users.tkk.fi/~ppuska/mirror/Lounesto/ (lots of stuff, e.g. links to dozens of researchers in applications of Clifford Algebra)
- "In physics, the concept of Clifford algebra, as such or in a disguise, is a necessity in the description of electron spin, because spinors cannot be constructed by tensorial methods, in terms of exterior powers of the vector space."
- "Clifford algebra might make its curriculum debut in high schools by replacing the cross product, in undergraduate courses by replacing rotation matrices, and in graduate courses by condensing the Maxwell equations in a vacuum into a single equation in terms of Cl3."
See also GeometricAlgebra.
One very good introduction to the simplest Clifford algebra, exterior algebra, is a series of
YouTube videos by David Metzler, available here:
http://www.youtube.com/playlist?list=PLB8F2D70E034E9C29
For another good introduction see
CliffordAlgebraaVisualIntroduction by Steven Lahar.
--
JohnFletcher
Note: Some authors talk about
Geometric Algebra and some about
Clifford Algebra. The usual use of this is that those who say
Geometric Algebra are emphasising the geometric explanations. Hestenes (see
HestenesOerstedMedalLecture) also uses the term
Geometric Calculus. The algebra is the same, the difference is in emphasis on the different ways of looking at things. For more information look at this web page by Hestenes which gives a diagram of the evolution of the ideas. There is also a list of recent books. --
JohnFletcher
http://modelingnts.la.asu.edu/html/Evolution.html
(broken link 20120711 but found using the
WaybackMachine here:
http://web.archive.org/web/20090603010039/http://modelingnts.la.asu.edu/html/evolution.html )
The use of two titles for the algebra are not new.
CliffordAlgebrasAndSpinors (Lounesto) has the following p.320.
Clifford's geometric algebras were created by William K. Clifford in 1878/1882,... Clifford algebras were independently rediscovered by Lipschitz 1880/1886, who also presented their first application to geometry,...
--
JohnFletcher
- Clifford Algebra Introduction
The essential core of
CliffordAlgebra, and the main difference from vector algebra as taught, is that multiplying two vector objects
a and
b can be written as
ab = a.b + a
b
in a space of any number of dimensions. It is not assumed that
ab = ba
and in general it will not be. Here the two parts are defined as
a.b = (ab + ba)/2 = b.a
a
b = (ab - ba)/2 = -b
a
a.b is a scalar quantity and is the equivalent of the vector dot product. If
a.b = 0 for two nonzero vectors, they are orthogonal.
a
b is known as the exterior product, defined in the work of Grassmann. It is related to, but
not the same as, the vector cross product
a
b which is only defined in three dimensions. If
a
b = 0 for two nonzero vectors, then they are parallel.
Notice that this definition does not depend in any way on a choice of axes for the space.
(For a fuller description, see
HestenesOerstedMedalLecture pages 9-14.)
--
JohnFletcher
- Clifford Algebra in 2 dimensions
The power of CliffordAlgebra can be illustrated with the following, adapted from HestenesOerstedMedalLecture pages 10-11.
The algebra describes a plane containing two orthogonal unit vectors
e1 and
e2 which each square to +1
e1^2 = e2^2 = 1
A unit bivector
i for the plane is given by the product
i = e1 e2 = e1
e2 = -e2 e1
since
e1.e2 = 0
The symbol
i is chosen because
i^2 = (e1 e2)(e1 e2) = -(e1 e2)(e2 e1) = -1
and thus
i is a number which squares to -1. Also
e1 = i e2
e2 = e1 i = -i e1
Multiplication by
i rotates any vector in the plane by a right angle. If a complex number
z is written using this
i, where
a and
b are scalars,
z = a + b i
then multiplying
z by
e1 gives the following
z e1 = a e1 + b e1 i = a e1 + b e2
One interpretation of this is that there is a length
a along
e1 followed by a length
b along
e1 rotated by a right angle, viz
e2. Another interpretation is that
ComplexNumbersArePoints once a direction is chosen for the real axis.
For me this is the beginning of the healing of the broken algebra - complex numbers and 2D vectors are rejoined. --
JohnFletcher
- Clifford Algebra in 3 dimensions
A basis for the whole algebra in three dimensions can be generated from three orthogonal unit vectors
e1,
e2 and
e3 which each square to +1.
This basis generates a unique
trivector which is the
pseudoscalar i for the basis. This represents an
oriented unit volume.
i = e1 e2 e3
There are three
bivectors in the basis. These represent
oriented unit areas.
e1 e2 = i e3
e2 e3 = i e1
e3 e1 = i e2
In these equations the multiplication by
i is called the
dual operation. In this case the
dual of a vector is a bivector and viceversa. In three dimensions the
dual of an area is the vector normal to the plane.
Note that all the bivectors and the trivector square to -1.
The outer product and the vector cross product can now be related through a
dual operation.
a
b = i a
b
This is a key result which can be used to unify
CliffordAlgebra and
VectorAlgebra in 3 dimensions. What this means is that
a
b is the vector normal to the bivector
a
b which defines a plane. When formulating equations in
GeometricAlgebra of 3 dimensions, this is the crucial difference. Bivectors are distinct items from vectors in any object.
[edit notes] This is quite a long and important topic and will take some time. If you want to find out more without waiting, look at the HestenesOerstedMedalLecture from page 14 onwards. --
JohnFletcher
Some other wiki pages which are related.
See also...
Books
[edit notes]
I would like to see these pages better edited. Please put more meat on the main page (this page). It would be useful for this page to start with the definition, an example and a discussion as to why it is an important concept and where it applies. As it stands now,
CliffordAlgebra page starts with justifications and moves on to contain just a directory of links.
DeleteWhenCooked.
I agree, but John is in fact working on it, so it'll be better soon. I'll add a motivation if he doesn't get around to it soon -- but I think he will.
I appreciate comments on what should be where. I have not finished sorting out the tangle, particularly on
CliffordAlgebraDetails. What matters for me is what works for those who have not met this before. More to come. --
JohnFletcher
MathWorld has some very useful information at
http://mathworld.wolfram.com/CliffordAlgebra.html
Interest in this and the related pages in
DecemberZeroFive.
CategoryMath