Levi-Civita Connection: Properties and Examples

In summary, the conversation discussed the properties of a Levi-Civita connection and its application to a function and one form on a manifold. The correct formula for ##\nabla_\nu f## was clarified as being equivalent to treating ##\partial_\nu f## as a vector field. The difference between ##\nabla_\mu \partial_\nu f## and ##\partial_\mu \partial_\nu f## was also noted.
  • #1
Silviu
624
11

Homework Statement


Let V be a Levi-Civita connection.
a) Let ##f \in F(M)##, (function defined on the manifold M). Show that: ##\nabla_\mu \nabla_\nu f = \nabla_\nu \nabla_\mu f ##
b) Let ##\omega \in \Omega^1(M)## (one form on M). Show that ##d \omega = (\nabla_\mu \omega)_\nu dx^\mu \wedge dx^\nu##

Homework Equations


Levi-Civita is a symmetric connection, i.e. ##\Gamma^\alpha_{\mu \nu} = \Gamma^\alpha_{\nu \mu}##

The Attempt at a Solution


a) For any connection, function f and vector X, we have ##\nabla_X f = X[f]##. So in our case ##\nabla_\mu \nabla_nu f = \frac{\partial}{\partial x_\mu}\frac{\partial}{\partial x_\nu} f = \frac{\partial}{\partial x_\nu}\frac{\partial}{\partial x_\mu} f = \nabla_\nu \nabla_\mu f ##. Is this correct? And if so, why does the connection has to be Levi-Civita, it seems to work for any connection?

b) ##\omega = a_\nu dx^\nu##. By definition, ##d\omega = \frac{\partial a_\nu}{\partial x_\mu}dx^\mu \wedge dx^\nu##. But ##(\nabla_\mu \omega)_\nu = \frac{\partial a_\nu}{\partial x_\mu} - \Gamma^\lambda_{\mu\nu}a_\lambda##. I am a bit confused of what I did wrong here, as the 2 results don't match and ##\Gamma^\lambda_{\mu\nu}## doesn't vanish, even in a Levi Civita connection. Can someone help me? Thank you!
 
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  • #2
Silviu said:
Is this correct?
No, it is not correct. ##\nabla_\nu f## is not a scalar. It is the components of a covector.

In (b) you are not taking into account that the wedge product is anti-symmetric.
 
  • #3
Orodruin said:
No, it is not correct. ##\nabla_\nu f## is not a scalar. It is the components of a covector.

In (b) you are not taking into account that the wedge product is anti-symmetric.
So for part b), ##\Gamma^{\lambda}_{\mu \nu}a_\lambda dx^\mu \wedge dx^\nu## vanishes because we multiply a symmetric term with an antisymmetric term. Thank you! For part a) I am not sure I understand. Isn't ##\nabla_\nu f = \frac{\partial}{\partial x^\nu}f##, which is just the derivative of a function, which is a number, so it creates a scalar field?
 
  • #4
Silviu said:
Isn't ∇νf=∂∂xνf∇νf=∂∂xνf\nabla_\nu f = \frac{\partial}{\partial x^\nu}f, which is just the derivative of a function, which is a number, so it creates a scalar field?
No.
 
  • #5
Orodruin said:
No.
Then, what is the right formula for ##\nabla_\nu f##?
 
  • #6
Silviu said:
Then, what is the right formula for ##\nabla_\nu f##?
For a scalar field ##\nabla_\nu f = \partial_\nu f##, but ##\partial_\nu f## is not a scalar field so generally ##\nabla_\mu \partial_\nu f \neq \partial_\mu \partial_\nu f##. Compare to the components of the gradient in regular Euclidean space.
 
  • #7
Orodruin said:
For a scalar field ##\nabla_\nu f = \partial_\nu f##, but ##\partial_\nu f## is not a scalar field so generally ##\nabla_\mu \partial_\nu f \neq \partial_\mu \partial_\nu f##. Compare to the components of the gradient in regular Euclidean space.
So do you mean to treat ##\partial_\nu f## as a vector field?
 
  • #8
Silviu said:
So do you mean to treat ##\partial_\nu f## as a vector field?
You should, because it is a (dual) vector field.
 
  • #9
Orodruin said:
You should, because it is a (dual) vector field.
Thanks a lot!
 

1. What is the Levi-Civita connection?

The Levi-Civita connection, also known as the Christoffel connection, is a mathematical concept used in differential geometry to describe the notion of parallel transport on a smooth manifold. It is a type of affine connection that assigns a unique tangent space at each point on a manifold, allowing for the calculation of directional derivatives and the definition of geodesics.

2. Who discovered the Levi-Civita connection?

The Levi-Civita connection was independently discovered by mathematicians Tullio Levi-Civita and Elwin Bruno Christoffel in the late 19th century. Levi-Civita published his findings in 1917, while Christoffel's work was published posthumously in 1904.

3. What is the difference between the Levi-Civita connection and other types of connections?

The Levi-Civita connection is a type of torsion-free connection, meaning that the directional derivatives it produces are independent of the order in which they are taken. This is in contrast to other types of connections, such as the affine connection, which may exhibit torsion or non-zero curvature.

4. How is the Levi-Civita connection used in physics?

The Levi-Civita connection is used in physics, specifically in the field of general relativity, to describe the curvature of spacetime. It is essential for calculating the equations of motion for particles and the behavior of light in the presence of massive objects, such as planets or black holes.

5. Are there any applications of the Levi-Civita connection outside of mathematics and physics?

Yes, the Levi-Civita connection has applications in other fields such as computer graphics, where it is used to calculate the curvature of surfaces and to deform objects smoothly. It also has applications in robotics, where it is used to describe the motion of robotic arms and other mechanical systems.

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