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Homework # 2 Solutions
Homework # 2 Solutions

... Solution: For any vectors u, v ∈ Rn , T (u + v) = A(u + v) + b T (u) + T (v) = Au + b + Av + b = A(u + v) + 2b 6= T (u + v) unless b = 0. Therefore, T is not a linear transformation when b 6= 0. Alternate solution: T (0) = A(0) + b = b 6= 0, so T is not a linear transformation when b 6= 0. 36. Let T ...
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L. A. G. final exam n.1, june 27, 2016 Name: 1. Let P = (1,0,0) and
L. A. G. final exam n.1, june 27, 2016 Name: 1. Let P = (1,0,0) and

< 1 ... 155 156 157 158 159 160 161 162 163 ... 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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