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advanced mathematics, especially in tensor analysis. Years ago, he made the statement that in working with tensors, one must learn to find—and feel—the rhythm inherent in the indices. He certainly felt that rhythm, and his ability to do so made a major difference in his approach to teaching the material and enabling his students to comprehend it. He read this work and made many valuable and Mathematical Physics, pp. 349-361 (2011) Accordingly, the co- and contravariant vectors x μ and xμ differ solely by their spatial components. Contrary to the threedimensional Euclidean case, the norm of a four-vector is not positive definite. Instead, the following cases can occur: x μx μ = x2 0 −x 2 = c2t2 −x2 ⎧ ⎪⎪ ⎨ ⎪⎪ ⎩ > 0 (time-like) = 0 (light-like) < 0 Preface These course notes are intended for students of all TU/e departments that wish to learn the basics of tensor calculus and differential geometry. Covariance and contravariance may refer to: Covariance and contravariance of vectors, in mathematics and theoretical physics Covariance and contravariance of functors, in category theory Covariance and contravariance (computer science), whether a type system preserves the ordering ≤ of types See also [ edit] You can represent "contravariant vectors" as rows and "covariant vectors" as columns all right if you want. It's just a convention. The dual space of the space of column vectors can be naturally identified with the space of row vectors, because matrix multiplication can then correspond to the "pairing" between a "covariant vector" and a "contravariant vector". The covariance or a contravariance of certain quantities tell you how to transform them to keep the result invariant from the choice of the coordinate system. You transform covariant quantities one-way while you do the inverse with the contravariant ones. To describe a vector you need coordinates v j and basis vectors e j. A Lorentz covariant classical field theory is developed which covers both electro-and gravita-tional dynamics. Starting points are Maxwell's equations for the electrodynamic and the co-variant A covariant vector or cotangent vector (often abbreviated as covector) has components that co-vary with a change of basis. That is, the components must be transformed by the same matrix as the change of basis matrix. The components of covectors (as opposed to those of vectors) are said to be covariant. Euclidean plane. In the Euclidean plane, the dot product allows for vectors to be identified with covectors. If is a basis, then the dual basis satisfies. Thus, e 1 and e 2 are perpendicular to each other, as are e 2 and e 1, and the lengths of e 1 and e 2 normalized against e 1 and e 2, respectively. Example. For example, suppose that we are given a basis e 1, e 2 consisting of a pair of I'm reading a Quora answer on an intuitive explanation of covariant/contravariant components of vectors.If we have a coordinate system with straight coordinate axes, the ge
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