Inner Products, Length and Orthogonality
An inner product gives a real vector space length and angle. Orthogonal sets of nonzero vectors are independent. Inner products with an orthonormal basis give a vector's coordinates.
What a learner can do afterwards
- Verify the inner product axioms for a given rule
- Show that an orthogonal set of nonzero vectors is independent
- Compute coordinates in orthogonal bases using inner products, including the nonunit norm-squared denominator and the orthonormal special case
- Compute dot products in R2 and R3, and compute lengths from a stated real inner product
- Decide orthogonality of small vectors from a zero inner product
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The dot product is the model inner product, written <u, v>. In R squared, (a, b) dot (c, d) = ac + bd. In R to the n, multiply matching components and add all n products. For nonzero u and v, cos theta = <u, v> / (length(u) length(v)). Vectors are orthogonal when their inner product is zero. The dot product of (3, -1) and (1, 3) is 3 - 3 = 0.
A real inner product must be symmetric: <u, v> = <v, u>. It must be linear in the first input: <a u + b w, v> = a<u, v> + b<w, v>. Symmetry gives linearity in the second input. Linearity in each input is called bilinearity. It must also be positive definite: <v, v> >= 0, with equality only for v = 0. These rules must hold for all vectors and real scalars. One successful numerical check cannot prove them.
An orthogonal set of nonzero vectors is independent. If c1 v1 + ... + ck vk = 0, take the inner product with vj. Orthogonality removes every term except cj<vj, vj>. Positive definiteness gives <vj, vj> > 0, so cj = 0. This works for every j. Thus a two-dimensional space can contain at most two mutually orthogonal nonzero vectors.
An orthonormal basis consists of mutually orthogonal unit vectors. The coordinate along ej is <v, ej>. For e1 = (3/5, 4/5), e2 = (-4/5, 3/5), and v = (2, 1), the coordinates are 2 and -1. Both basis vectors have length one and their dot product is zero. A negative coordinate means the component points opposite to that basis vector.
For an orthogonal basis that is not normalised, the coordinate along uj is <v, uj> / <uj, uj>. This follows by taking the inner product of v = sum cj uj with uj. For an orthonormal basis the denominator is one. Coordinates depend on direction: if e2 = (0, -1), then <(a, b), e2> = -b, not b.
Length in any real inner-product space is sqrt(<v, v>). For the dot product, length(a, b) = sqrt(a squared + b squared). Other inner products can give other lengths. The rule <u, v> = u1 v1 + 4 u2 v2 is symmetric and bilinear, and <v, v> = v1 squared + 4 v2 squared is positive for every nonzero v. In contrast, u1 v1 alone gives zero squared length to (0, 1), so it is not positive definite.
Test the axioms. Use dot products to find lengths and right angles, and read orthonormal coordinates directly from the inner product.
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