The vector Laplacian can be generalized to yield
the tensor Laplacian
where
is a covariant derivative,
is the metric tensor,
,
is the comma
derivative (Arfken 1985, p. 165), and
 |
(6)
|
is a Christoffel symbol of the second
kind.
See also
Laplacian,
Vector
Laplacian
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References
Arfken, G. Mathematical Methods for Physicists, 3rd ed. Orlando, FL: Academic Press, pp. 165-166,
1985.Moon, P. and Spencer, D. E. Field
Theory Handbook, Including Coordinate Systems, Differential Equations, and Their
Solutions, 2nd ed. New York: Springer-Verlag, 1988.Referenced
on Wolfram|Alpha
Tensor Laplacian
Cite this as:
Weisstein, Eric W. "Tensor Laplacian."
From MathWorld--A Wolfram Web Resource. https://mathworld.wolfram.com/TensorLaplacian.html
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