Derivatives of contravariant and covariant vectors

Join the discussion
Registration is free. Start your own thread to ask a follow-up.
4 replies · 4K views
nigelscott
Messages
133
Reaction score
4
Can someone explain why the derivative with respect to a contravariant coordinate transforms as a
covariant 4-vector and the derivative with respect to a covariant coordinate transforms as a
contravariant 4-vector.
 
Physics news on Phys.org
Take a scalar field. Then its differential is
[tex]\mathrm{d} \phi=\mathrm{d} x^{\mu} \frac{\partial \phi}{\partial x^{\mu}}[/tex]
is also a scalar. Thus, since [itex]\mathrm{d} x^{\mu}[/itex] transforms contravariantly the four-gradient must transform covariantly, i.e., the correct notation is
[tex]\mathrm{d} \phi=\mathrm{d} x^{\mu} \partial_{\mu} \phi.[/tex]
In the same way you can show that deriving with respect to the covariant components leads to a contravariant object.
 
The title says "Derivatives of contravariant and covariant vectors," which would be stuff like [itex]\nabla_a v_b[/itex] versus [itex]\nabla_a v^b[/itex]. But #1 seems to be talking about [itex]\nabla_a v_b[/itex] versus [itex]\nabla^a v_b[/itex] , and #2 seems to be talking about the gradient of a scalar, [itex]\nabla_a\phi[/itex] versus [itex]\nabla^a\phi[/itex]. Which are we really talking about here?

Not to be too pedantic, but we also don't have contravariant coordinates and covariant coordinates. Coordinates are always upper-index, and an ntuple of coordinates is not a vector or covector (at least not in GR). An infinitesimal *change* in the coordinates is an upper-index vector.

Assuming that the question is really the one posed in #1, then an easy way to see this is in terms of scaling. For example, suppose you change your units from meters to centimeters. All of your coordinates (which are upper-index quantities) get bigger by a factor of 100. Now suppose you have a scalar such as the electrical potential, and you take a gradient in order to find the electric field. The electric field is *smaller* in units of V/cm than it is in units of V/m. So the coordinates transform in one way under scaling, while a gradient transforms in the opposite way. This is what we expect for covariant quantities compared to contravariant ones.
 
Thanks for your responses. I think my question should really have asked about the 4-gradient in SR.

∂μ = ∂/xμ = [∂/∂t, ∇]

and

∂μ = ∂/xμ = [∂/∂t, -∇]

c = 1

So in these cases the indeces are just telling you that there is a change of sign in the spatial
coordinates. What I don't understand is how the process of taking the derivative of the contravariant components results in a covariant vector and vice versa.
 
Last edited: