Difference Between Covariant & Contravariant Vectors Explained

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Covariant and contravariant vectors differ primarily in their transformation properties under coordinate changes. Covariant vectors, or covectors, are often used to approximate scalar fields, while contravariant vectors typically represent tangent vectors to curves, such as velocity. The mathematical distinction lies in how their components transform: covariant components change in the same way as the coordinates, while contravariant components change oppositely. Understanding these differences is crucial in fields like differential geometry and relativity. This foundational knowledge aids in grasping more complex concepts in physics and mathematics.
LeonPierreX
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Can someone explain to me what is the difference between covariant and contravariant vectors ? Thank You
 
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LeonPierreX said:
Can someone explain to me what is the difference between covariant and contravariant vectors ? Thank You

Given Bill's pointer to a web page talking about the difference, I'm not sure if it's appropriate to add anything, but what I find most useful is not the mathematics for how the two kinds of vectors transform, but what they are good for. The typical use for a regular vector is as a "tangent" or "local approximation" to a parametrized curve--for example, a velocity vector \vec{v} describes how a position as a function of time is behaving locally. The typical use for a covector is a "local approximation" to a scalar field (a scalar field is a real-valued function of location, such as altitude or temperature on the Earth at a given time). In vector calculus in Cartesian coordinates, you would use \nabla T to describe how the scalar field T changes locally. The components of the two types of vectors transform in opposite ways under a change of coordinates.
 
In an inertial frame of reference (IFR), there are two fixed points, A and B, which share an entangled state $$ \frac{1}{\sqrt{2}}(|0>_A|1>_B+|1>_A|0>_B) $$ At point A, a measurement is made. The state then collapses to $$ |a>_A|b>_B, \{a,b\}=\{0,1\} $$ We assume that A has the state ##|a>_A## and B has ##|b>_B## simultaneously, i.e., when their synchronized clocks both read time T However, in other inertial frames, due to the relativity of simultaneity, the moment when B has ##|b>_B##...

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