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Math 304–504 Linear Algebra Lecture 24: Orthogonal subspaces.
Math 304–504 Linear Algebra Lecture 24: Orthogonal subspaces.

... dim V + dim V ⊥ = n. Proof: Pick a basis v1 , . . . , vk for V . Let A be the k×n matrix whose rows are vectors v1 , . . . , vk . Then V = R(AT ) and V ⊥ = N(A). Consequently, dim V and dim V ⊥ are rank and nullity of A. Therefore dim V + dim V ⊥ equals the number of columns of A, which is n. ...
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... The number of pivot columns of a matrix equals the dimension of its column space. TRUE Remember these columns and linearly independent and span the column space. A plane in R3 is a two dimensional subspace of R3 . FALSE unless the plane is through the origin. The dimension of the vector space P4 is ...
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... Calculating the angle  between two G. Vectors was based on their dot product  use the dot product of the corresponding A. Vectors ...
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... Note that one check the two closure requirements at once by verifying the following property, called the closure under linear combination: C0. cx + dy  V whenever x, y  V and c, d  . Definition Vector spaces that are important in DEs (as well as other branches of mathematics) are function spaces. ...
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... So 2 + 5(k + 1) ≤ 3k+1 (we actually proved the stronger result that 2 + 5(k + 1) < 3k+1 , but that certainly makes the ≤ claim true also, because ≤ represents an “or” statement), whence by PMI it is true that 2 + 5n ≤ 3n for all integers n ≥ 3. (To be rigorous, one really should formally prove the ...
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... A tensor is a difficult beast to understand intuitively, but we can start by getting a sense for what each index means. From our simple examples, we can glean three basic ideas about the nature of tensors. First, each contravariant index in a tensor behaves like a vector. This means that rank-(n,0) ...
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PHYS 101 Lecture 2 - Simon Fraser University
PHYS 101 Lecture 2 - Simon Fraser University

< 1 ... 37 38 39 40 41 42 43 44 45 ... 54 >

Exterior algebra



In mathematics, the exterior product or wedge product of vectors is an algebraic construction used in geometry to study areas, volumes, and their higher-dimensional analogs. The exterior product of two vectors u and v, denoted by u ∧ v, is called a bivector and lives in a space called the exterior square, a vector space that is distinct from the original space of vectors. The magnitude of u ∧ v can be interpreted as the area of the parallelogram with sides u and v, which in three dimensions can also be computed using the cross product of the two vectors. Like the cross product, the exterior product is anticommutative, meaning that u ∧ v = −(v ∧ u) for all vectors u and v. One way to visualize a bivector is as a family of parallelograms all lying in the same plane, having the same area, and with the same orientation of their boundaries—a choice of clockwise or counterclockwise.When regarded in this manner, the exterior product of two vectors is called a 2-blade. More generally, the exterior product of any number k of vectors can be defined and is sometimes called a k-blade. It lives in a space known as the kth exterior power. The magnitude of the resulting k-blade is the volume of the k-dimensional parallelotope whose edges are the given vectors, just as the magnitude of the scalar triple product of vectors in three dimensions gives the volume of the parallelepiped generated by those vectors.The exterior algebra, or Grassmann algebra after Hermann Grassmann, is the algebraic system whose product is the exterior product. The exterior algebra provides an algebraic setting in which to answer geometric questions. For instance, blades have a concrete geometric interpretation, and objects in the exterior algebra can be manipulated according to a set of unambiguous rules. The exterior algebra contains objects that are not just k-blades, but sums of k-blades; such a sum is called a k-vector. The k-blades, because they are simple products of vectors, are called the simple elements of the algebra. The rank of any k-vector is defined to be the smallest number of simple elements of which it is a sum. The exterior product extends to the full exterior algebra, so that it makes sense to multiply any two elements of the algebra. Equipped with this product, the exterior algebra is an associative algebra, which means that α ∧ (β ∧ γ) = (α ∧ β) ∧ γ for any elements α, β, γ. The k-vectors have degree k, meaning that they are sums of products of k vectors. When elements of different degrees are multiplied, the degrees add like multiplication of polynomials. This means that the exterior algebra is a graded algebra.The definition of the exterior algebra makes sense for spaces not just of geometric vectors, but of other vector-like objects such as vector fields or functions. In full generality, the exterior algebra can be defined for modules over a commutative ring, and for other structures of interest in abstract algebra. It is one of these more general constructions where the exterior algebra finds one of its most important applications, where it appears as the algebra of differential forms that is fundamental in areas that use differential geometry. Differential forms are mathematical objects that represent infinitesimal areas of infinitesimal parallelograms (and higher-dimensional bodies), and so can be integrated over surfaces and higher dimensional manifolds in a way that generalizes the line integrals from calculus. The exterior algebra also has many algebraic properties that make it a convenient tool in algebra itself. The association of the exterior algebra to a vector space is a type of functor on vector spaces, which means that it is compatible in a certain way with linear transformations of vector spaces. The exterior algebra is one example of a bialgebra, meaning that its dual space also possesses a product, and this dual product is compatible with the exterior product. This dual algebra is precisely the algebra of alternating multilinear forms, and the pairing between the exterior algebra and its dual is given by the interior product.
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