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MATH 32A: MIDTERM 1 REVIEW 1. Vectors 1. Let v = . a
MATH 32A: MIDTERM 1 REVIEW 1. Vectors 1. Let v = . a

... Solution: Three points determine the plane containing them, except in the rare case that they happen to be collinear. In this problem P is not on the line x = y = z, so we’re free to pick two points on the line. For simplicity, take Q = (0, 0, 0) and R = (1, 1, 1) (of course any other two points on ...
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... and we shall also use the notation B(x, r) = {y ∈ X | d(x, y) ≤ r} for the closed ball. Such a metric need not be translation invariant, but it will usually be so in the cases we consider; translation invariance (also just called invariance) here means that d(x + a, y + a) = d(x, y) for x, y, a ∈ X ...
Interval-valued Fuzzy Vector Space
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... Definition 5. Let F be an IVFS and x, y ∈ F where x = [a1 , b1 ] and y = [a2 , b2 ] , then x = y if and only if a1 = a2 and b1 = b2 . The logical operators ≤ and < are given in the following definitions. Definition 6. Let F be an IVFS and x, y ∈ F where x = [a1 , b1 ] and y = [a2 , b2 ] , then x ≤ y ...
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< 1 ... 72 73 74 75 76 77 78 79 80 ... 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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