Geometric Algebra. Gary Snethen Crystal Dynamics
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1 Geometric Algebra Gary Snethen Crystal Dynamics
2 Questions How are dot and cross products related? Why do cross products only exist in 3D? Generalize cross products to any dimension? Is it possible to divide by a vector? What does an imaginary number look like? Complex have two, but Quaternions have four. Why? Why do quaternions rotate vectors? Generalize quaternions to any dimension?
3 History Babylonia 1800 BC First known use of algebraic equations Number system was base-60 Multiplication table impractical (3600 entries to remember!) Used table of squares to multiply any two integers And this equation: ab a b 2 a 2 b 2 2
4 History Babylonia 1800 BC B A AB B B 2 A A 2 AB
5 History Greece 300 BC Euclid wrote Elements Covered Geometry From Geo meaning Earth And Metric meaning Measurement Geometry was the study of Earth Measurements Extended: Earth to space, space-time and beyond Alexandria 50 AD Heron tried to find volume of a frustum, but it required using the square root of a negative number
6 Persia 820 History Al-Khwarizmi wrote a mathematics text based on Al-jabr w al-muqabala Al-jabr: Reunion of broken parts W al-muqabala: through balance and opposition Pisa 1202 Leonardo Fibonacci introduces the method to Europe Name is shortened to Al-jabr Westernized to Algebra
7 History 1637 René Descartes Coined the term imaginary number 1777 Leonard Euler Introduced the symbol i for imaginary numbers 1799 Caspar Wessel Described complex numbers geometrically Made them acceptable to mainstream mathematicians 1831 Carl Gauss Discovered that complex numbers could be written a + i b
8 History 1843 Rowan Hamilton Discovered quaternions (3D complex numbers) Coined the term vector to represent the non-scalar part Invented dot and cross products 1844 Hermann Grassmann Exterior product (generalization of cross product) 1870 William Kingdon Clifford Generalized complex numbers, dot and cross products Died young, and his approach didn t catch on Variants of his approach are often called Clifford Algebras 1966 David Orlin Hestenes Rediscovered, refined and renamed Geometric Algebra Claims that Geometric Algebra is the name Clifford wanted
9 Geometric Algebra Introduction How do we represent direction? Direction is similar to a unit, like mass or energy, but even more similar to - and + Pick a symbol that represents one unit of direction like i. We live in a 3D universe, so we need three directions: i, j and k
10 Geometric Algebra Introduction i+i = 2i i+j = i+j How do we add direction? Parallel directions combine Orthogonal directions do not combine No matter how many terms we add together, we ll wind up with some combination of i, j and k: (ai + bj + ck) We call these vectors
11 Geometric Algebra Simplifying Products How do we multiply orthogonal directions? ( i)( j) ij j i = ij (2 i)(3 j) 6ij 3j = 6ij 2i We call these bivectors
12 Geometric Algebra Introduction What are the unit directions in 2D & 3D? 2D 3D Scalar: 1 1 Vector: i j i j k Bivector: ij jk ki ij Trivector: ijk Note: In 3D, there are three vector directions and three bivector directions this leads to confusion!
13 Geometric Algebra Introduction Which are vectors? Which are bivectors? Velocity Angular velocity Force Torque Normal Direction of rotation Direction of reflection Cross product of two vectors The vector portion of a quaternion
14 Geometric Algebra Introduction What does a negative bivector represent? j ( i)( j) ij ( i)( j) ij ( j)( i) ij ji ij j i -i i -j = = = -ij -ij -ij
15 Geometric Algebra Introduction How do we multiply parallel directions? ii=? i represents direction, like 1 or -1 on a number line (1)(1) = 1 (-1)(-1) = 1 (i)(i) = 1 ii = 1 i is its own inverse!
16 Geometric Algebra Introduction How do we multiply directions? Rule 1: If i and j are orthogonal unit vectors, then: Rule 2: For any unit vector i: ji = -ij ii = 1 Just like the cross dot product! That s it! Now we can multiply arbitrary vectors!
17 Geometric Algebra Simplifying Products Try simplifying these expressions iijj 1 ijik -jk ijkjkij -j kjijk i
18 Geometric Product How do we multiply two vectors? (ai + bj + ck) (xi + yj + zk)
19 Geometric Product (ai + bj + ck) (xi + yj + zk) = + axii + ayij + azik + bxji + byjj + bzjk + cxki + cykj + czkk
20 Geometric Product Simplify (ai + bj + ck) (xi + yj + zk) + axii + ayij + azik = + bxji + byjj + bzjk + cxki + cykj + czkk ii = 1 jj = 1 kk = 1
21 Geometric Product Simplify (ai + bj + ck) (xi + yj + zk) + ax + ayij + azik = + bxji + by + bzjk + cxki + cykj + cz ii = 1 jj = 1 kk = 1
22 Geometric Product Simplify (ai + bj + ck) (xi + yj + zk) + ax + ayij + azik = + bxji + by + bzjk + cxki + cykj + cz ji = -ij ik = -ki kj = -jk
23 Geometric Product Simplify (ai + bj + ck) (xi + yj + zk) + ax + ayij + azik = - bxij + by + bzjk + cxki + cykj + cz ji = -ij ik = -ki kj = -jk
24 Geometric Product Simplify (ai + bj + ck) (xi + yj + zk) + ax + ayij - azki = - bxij + by + bzjk + cxki + cykj + cz ji = -ij ik = -ki kj = -jk
25 Geometric Product Simplify (ai + bj + ck) (xi + yj + zk) + ax + ayij - azki = - bxij + by + bzjk + cxki - cyjk + cz ji = -ij ik = -ki kj = -jk
26 Geometric Product Group Terms (ai + bj + ck) (xi + yj + zk) = + ax + ayij - azki - bxij + by + bzjk + cxki - cyjk + cz = (ax + by + cz) +
27 Geometric Product Group Terms (ai + bj + ck) (xi + yj + zk) = + ax + ayij + azik - bxij + by + bzjk - cxik - cyjk + cz = (ax + by + cz) + (bz cy) jk + (cx az) ki + (ay bx) ij
28 Geometric Product Inner & Outer Products (ai + bj + ck) (xi + yj + zk) + ax + ayij + azik = - bxij + by + bzjk - cxik - cyjk + cz = (ax + by + cz) + (bz cy) jk + (cx az) ki + (ay bx) ij AB...
29 Geometric Product Inner & Outer Products (ai + bj + ck) (xi + yj + zk) + ax + ayij + azik = - bxij + by + bzjk - cxik - cyjk + cz = (ax + by + cz) + (bz cy) jk + (cx az) ki + (ay bx) ij AB A B
30 Geometric Product Inner & Outer Products (ai + bj + ck) (xi + yj + zk) + ax + ayij + azik = - bxij + by + bzjk - cxik - cyjk + cz = (ax + by + cz) + (bz cy) jk + (cx az) ki + (ay bx) ij A B A B
31 Geometric Product Inverse Vectors can be inverted! aa 1 1 aaa 1 a aa a 1 a a 1 a aa
32 2D Product A = ai + bj B = xi + yj AB = (ax + by) + (ay bx) ij Point-like vector (a scalar) Captures the parallel relationship between A and B Plane-like vector (a bivector) The perpendicular relationship between A and B
33 2D Rotation v v = vnm n nm m nm v = v(nm) = vnm Note: This only works when n, m and v are in the same plane!
34 A Complex Connection What is the square of ij? (ij)(ij) = (-ji)(ij) = -jiij = -j(ii)j = -jj = -1 2 ( ) 1 ij!!! ij 1!!! ij = i!!! So (a + bij) is a complex number!!!
35 The Complex Connection This gives a geometric interpretation to imaginary numbers: Imaginary numbers are bivectors (plane-like vectors). The planar product ( 2D cross product ) of two vectors. The full geometric product of a pair of 2D vectors has a scalar (real) part and a bivector (imaginary) part. It s a complex number! (2 + 3ij is the same as 2 + 3i) So, complex numbers can be used to represent a 2D rotation. This is the major reason they appear in real-world physics!
36 2D Reflection v v n vn v = n(vn) = nvn
37 Rotation by Double Reflection v v n m v v = nvn v = m(v )m = m(nvn)m = mnvnm = (mn)v(nm) Angle of rotation is equal to twice the angle between n and m. Note: Rotation by double reflection works in any dimension!
38 Rotation by Double Reflection v v n m v v = nvn v = m(v )m = m(nvn)m = mnvnm = (mn)v(nm) Angle of rotation is equal to twice the angle between n and m. The product mn is a quaternion and nm is its conjugate!
A = 3 B = A 1 1 matrix is the same as a number or scalar, 3 = [3].
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