Συναλλοιότης


Αναλλοιότητα

Συναλλοιότητα

Ανταλλοιότητα
Εφαπτομενικότητα
Καθετότητα

Μοναδιαίο Διάνυσμα

Ανταλλοιότητα
Εφαπτομενικότητα
Καθετότητα
- Μία ιδιότητα
Ετυμολογία[]
Η ονομασία "Συναλλοιότητα" σχετίζεται ετυμολογικά με την λέξη "αλλοίωση".
Εισαγωγή[]
In theoretical physics, general covariance (also known as diffeomorphism covariance or general invariance) is the invariance of the form of physical laws under arbitrary differentiable coordinate transformations. The essential idea is that coordinates do not exist a priori in nature, but are only artifices used in describing nature, and hence should play no role in the formulation of fundamental physical laws.
A physical law expressed in a generally covariant fashion takes the same mathematical form in all coordinate systems,[1] and is usually expressed in terms of tensor fields. The classical (non-quantum) theory of electrodynamics is one theory that has such a formulation.
Albert Einstein proposed this principle for his special theory of relativity; however, that theory was limited to space-time coordinate systems related to each other by uniform relative motions only, the so-called "inertial frames." Einstein recognized that the General principle of relativity should also apply to accelerated relative motions, and he used the newly developed tool of tensor calculus to extend the special theory's global Lorentz covariance (applying only to inertial frames) to the more general local Lorentz covariance (which applies to all frames), eventually producing his general theory of relativity. The local reduction of the general metric tensor to the Minkowski metric corresponds to free-falling (geodesic) motion, in this theory, thus encompassing the phenomenon of gravitation.
Much of the work on classical unified field theories consisted of attempts to further extend the general theory of relativity to interpret additional physical phenomena, particularly electromagnetism, within the framework of general covariance, and more specifically as purely geometric objects in the space-time continuum.
Remarks[]
The relationship between general covariance and general relativity may be summarized by quoting a standard textbook:[2]
A more modern interpretation of the physical content of the original principle of general covariance is that the Lie group GL4(R) is a fundamental "external" symmetry of the world. Other symmetries, including "internal" symmetries based on compact groups, now play a major role in fundamental physical theories.
- When a physical quantity or equation remains unchanged under a certain co-ordinate transformation, they are called invariant under that transformation.
- When an equation keeps its mathematical form same under a certain co-ordinate transformation, that is called co-variant under that transformation.
- Example:
- Various classical vectors are invariant and Newtonian force law is co-variant under Galilean transformation.
- Special Relativistic scalars are invariant and Lorentz force law is co-variant under Lorentz transformation.
Σημείωση[]
Let be a smooth map between smooth manifolds and . Then there is an associated linear map from the space of 1-forms on (the linear space of sections (fiber bundle) of the cotangent bundle) to the space of 1-forms on .
This linear map is known as the pullback (by ), and is frequently denoted by .
More generally, any covariant tensor field – in particular any differential form –
on may be pulled back to using .
When the map is a diffeomorphism, then the pullback,
together with the pushforward, can be used to transform any tensor field from to or vice versa.
In particular, if is a diffeomorphism between open subsets of and ,
viewed as a change of coordinates (perhaps between different charts on a manifold ),
then the pullback and pushforward describe
the transformation properties of covariant and contravariant tensors
used in more traditional (coordinate dependent) approaches to the subject.
In the lexicon of category theory, covariance and contravariance are properties of functors;
unfortunately,
it is the lower-index objects (covectors) that generically have pullbacks, which are contravariant,
while the upper-index objects (vectors) instead have pushforwards, which are covariant.
Υποσημειώσεις[]
Εσωτερική Αρθρογραφία[]
- συναλλοίωτος Τανυστής
- Γενική Συναλλοιότητα, Πρόδηλη Συναλλοιότητα, Λωρένσεια Συναλλοιότητα
- Lorentz covariance, manifest covariance, general covariance, Galilean invariance
- αναλλοιότητα, ανταλλοιότητα, ανταλλοιότητα
- παγκοσμιότητα, τοπικότητα
- Coordinate conditions
- Coordinate-free
- Covariance, contravariance
- Covariant derivative
- Diffeomorphism, Υποβαθριακή Ανεξαρτησία
- Fictitious force
- Gauge covariant derivative
- General covariant transformations
- Harmonic coordinate condition
- Inertial frame of reference
- Principle of covariance
- Special relativity
- Symmetry in physics
Βιβλιογραφία[]
Ιστογραφία[]
- Ομώνυμο άρθρο στην Βικιπαίδεια
- Ομώνυμο άρθρο στην Livepedia
- βικιπαίδεια συνδιακύμανση
- Συναλλοιότητα Μπαντές
- researchgate.net-Covariance Descriptor for Target Detection
- quantum covariance, Flaminia Giacomini
- CONTRAVARIANCE, COVARIANCE, CHRIS TIEE
- [https://www.nature.com/articles/s41467-018-08155-0 Quantum mechanics and the covariance of physical laws in quantum reference frames}
- [https://www.youtube.com/watch?v=AociwKxaB-s video for covariant physical μεγέθη)
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