- #1
Je m'appelle
- 120
- 0
Are all vector fields invariants or is this a particular characteristic to some fields?
For example, suppose the vector field E = x^2 x + xy y.
If I write it in terms of covariant and contravariant basis through the polar coordinates I get the same results, or in other words
[tex]\vec{E} = \bar{E^i} \bar{e_i} = \bar{E_i} \bar{e^i}[/tex]
Where
[tex]\bar{E^i} \bar{e_i} \equiv \frac{\partial \bar{x^i}}{\partial x^j} E^j \bar{e_i}[/tex]
is the vector field in it's contravariant basis and[tex]\bar{E_i} \bar{e^i} \equiv \frac{\partial x^j}{\partial \bar{x^i}} E_j \bar{e^i}[/tex]
is the vector field in it's covariant basis.
By evaluating the above I found out that
[tex]\bar{E^i} = \bar{E_i} = r^2 cos \theta [/tex]
Or in other words
[tex]r^2 cos \theta \ \hat{r_n} = r^2 cos \theta \ \hat{r_t}[/tex]
Where
[tex]\hat{r_n} \equiv \bar{e^i} [/tex]
is the normal vector of the contravariant basis and
[tex]\hat{r_t} \equiv \bar{e_i} [/tex]
is the tangent vector of the covariant basis.
Then, I picked another vector field F = x x + y y and wrote it in terms of it's contravariant and covariant basis through the polar coordinates system, and my results were that
[tex]\vec{F} = \bar{F^i} \bar{e_i} = \bar{F_i} \bar{e^i}[/tex]
That is, F is just as invariant as E.
So my question is, are all vector fields invariants or is this just some coincidence that I picked two arbitrary vector fields and they came out to be invariants?
For example, suppose the vector field E = x^2 x + xy y.
If I write it in terms of covariant and contravariant basis through the polar coordinates I get the same results, or in other words
[tex]\vec{E} = \bar{E^i} \bar{e_i} = \bar{E_i} \bar{e^i}[/tex]
Where
[tex]\bar{E^i} \bar{e_i} \equiv \frac{\partial \bar{x^i}}{\partial x^j} E^j \bar{e_i}[/tex]
is the vector field in it's contravariant basis and[tex]\bar{E_i} \bar{e^i} \equiv \frac{\partial x^j}{\partial \bar{x^i}} E_j \bar{e^i}[/tex]
is the vector field in it's covariant basis.
By evaluating the above I found out that
[tex]\bar{E^i} = \bar{E_i} = r^2 cos \theta [/tex]
Or in other words
[tex]r^2 cos \theta \ \hat{r_n} = r^2 cos \theta \ \hat{r_t}[/tex]
Where
[tex]\hat{r_n} \equiv \bar{e^i} [/tex]
is the normal vector of the contravariant basis and
[tex]\hat{r_t} \equiv \bar{e_i} [/tex]
is the tangent vector of the covariant basis.
Then, I picked another vector field F = x x + y y and wrote it in terms of it's contravariant and covariant basis through the polar coordinates system, and my results were that
[tex]\vec{F} = \bar{F^i} \bar{e_i} = \bar{F_i} \bar{e^i}[/tex]
That is, F is just as invariant as E.
So my question is, are all vector fields invariants or is this just some coincidence that I picked two arbitrary vector fields and they came out to be invariants?
Last edited: