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Relativity, decays and electromagnetic fields
Relativity, decays and electromagnetic fields
Relativity, decays and electromagnetic fields
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Relativity, decays and electromagnetic fields

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After introducing the metric in classical Euclidean space, we move on to Minkowski's concept of four-vector in space-time, dealing with topics of restricted relativity, such as Lorentz transformations and Lorentz invariants. Relativistic expressions for the total energy of a free particle, energy at rest and kinetic energy are obtained, showing also their non-relativistic limits and the so-called mass-shell relation. Subsequently, from the point of view of relativistic kinematics, the decay of particles is analyzed, in particular showing the impossibility of the decay of a free photon and analyzing the decay of the muon. The electromagnetic field tensor is introduced, with components related to those of the electric and magnetic field vectors, and it is calculated its transformation between inertial reference frames. It is explicitly shown, as an example, that in a reference frame in motion with respect to an electric charge, the latter generates both an electric and a magnetic field which depend on time. Finally, Maxwell's equations are treated, both in differential and in covariant form, showing how to obtain the equation of electromagnetic waves in vacuum. 

Author: dr. Alessio Mangoni, PhD, theoretical physicist.
LanguageEnglish
PublisherDr. Alessio Mangoni
Release dateFeb 29, 2020
ISBN9788835379225
Relativity, decays and electromagnetic fields

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    Relativity, decays and electromagnetic fields - Alessio Mangoni

    Euclidean space

    Vectors and metrics

    Vector

    A vector in the three-dimensional euclidean space can be written, in terms of its components, as

    image.png

    where the superscript distinguishes the coordinates and it does not represent an exponentiation. We have chosen to distinguish the components of a vector in euclidean space with superscript rather than subscript to immediately introduce the formalism of special relativity. In fact, when we talk about four-vector (four-component generalization of a vector) we will see that we must distinguish components with index at the top (superscript) and components with index at the bottom (subscript).

    So we can write the i-th component as

    image-1.png

    Scalar product

    The scalar product between two vectors is written as

    image-2.png

    or

    image-3.png

    The scalar product of a vector with itself is

    image-4.png

    image-5.png

    and corresponds to the squared norm of the vector.

    Metric

    The formula for the scalar product of a vector with itself

    image-6.png

    can be written also as a combination

    image-7.png

    with constant coefficients equal to 1, i.e.

    image-8.png

    A generalization of the latter formula is

    image-9.png

    with

    image-10.png

    in fact with this choice the terms which include mixed products of components that do not appear in the scalar product are null.

    The coefficients of the combination of the coordinates of the vector can be interpreted as the elements of a diagonal matrix (elements that are not null only if the indices are equal). This 3-dimensional matrix in the euclidean space takes the form

    image-11.png

    and we can write the square of a vector as a product between vectors and matrix in the following way

    image-12.png
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