- #1
noospace
- 75
- 0
I asked this question in the tensor analysis formum but did we did not reach a satisfactory conclusion.
Here is the problem:
Let [itex]\mathbf{x} : U \subset\mathbb{R}^2 \to S[/itex] be a local parametrization of a regular surface S. Then the coefficients of the second derivatives of x in the basis of the tangent space are defined to be the Christoffel symbols.
On the other hand, if we write the first fundamental form [itex]ds^2 = E du^2 + 2F du dv + G dv^2[/itex] in differential form we have an extremization problem of the arc-length
Then the coefficients of of the corresponding Euler-Lagrange equations are essentially the Christoffel symbols.
Are there any interesting examples where the Lagrangian method of computing Christoffel symbols breaks down?
Here is the problem:
Let [itex]\mathbf{x} : U \subset\mathbb{R}^2 \to S[/itex] be a local parametrization of a regular surface S. Then the coefficients of the second derivatives of x in the basis of the tangent space are defined to be the Christoffel symbols.
On the other hand, if we write the first fundamental form [itex]ds^2 = E du^2 + 2F du dv + G dv^2[/itex] in differential form we have an extremization problem of the arc-length
Then the coefficients of of the corresponding Euler-Lagrange equations are essentially the Christoffel symbols.
Are there any interesting examples where the Lagrangian method of computing Christoffel symbols breaks down?