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Unit 1 Relevant Electrostatics and Magnetostatics (Old and New)
Unit 1 Relevant Electrostatics and Magnetostatics (Old and New)

Matrix Worksheet 7
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... Note that aij is used to denote the element which appears at the ith row and jth column of the matrix. The identity matrix and null matrix are represented as I and O respectively. Skill Check 1: 1. In May, Suzanne bought 32 styrofoam balls and decorated them as toy figurines. In June, she sold 12 fi ...
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... Eg: The map c:V-->V multiplication by a scalar c, has diagonal matrix c.I in any basis. Thus every basis is an eigenbasis for the identity map. Eg. The map f:R2-->R2 sending (1,0) to (1,0) and (0,1) to (0,2) has diagonal matrix with columns (1,0) and (0,2) in the standard basis, i.e. the standard b ...
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... n  m (where m  n), the products AB and BA are of different orders and so cannot be equal to each other. Not all square matrices have inverses. If, however, a matrix does have an inverse, that inverse is unique. Example 2 shows how to use a system of equations to find the inverse of a matrix. ...
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< 1 ... 102 103 104 105 106 107 108 109 110 ... 214 >

Four-vector

In the theory of relativity, a four-vector or 4-vector is a vector in Minkowski space, a four-dimensional real vector space. It differs from a Euclidean vector in how its magnitude is determined. The transformations that preserve this magnitude are the Lorentz transformations, which include spatial rotations, boosts (a change by a constant velocity to another inertial reference frame), and temporal and spatial inversions. Regarded as a homogeneous space, the transformation group of Minkowski space is the Poincaré group, which adds to the Lorentz group the group of translations. The Lorentz group may be represented by 4×4 matrices.The article considers four-vectors in the context of special relativity. Although the concept of four-vectors also extends to general relativity, some of the results stated in this article require modification in general relativity.
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