| 释义 | 
		Covariant TensorA covariant tensor is a Tensor having specific transformation properties (c.f., a Contravariant Tensor).  Toexamine the transformation properties of a covariant tensor, first consider the Gradient
    | (1) |  
  for which
   | (2) |  
  where  .  Now let 
   | (3) |  
  then any set of quantities   which transform according to
   | (4) |  
  or, defining 
   | (5) |  
  according to 
   | (6) |  
  is a covariant tensor.  Covariant tensors are indicated with lowered indices, i.e.,  .
 
 Contravariant Tensors are a type of Tensor with differing transformation properties,denoted  .  However, in 3-D Cartesian Coordinates,
    | (7) |  
  for  , 2, 3, meaning that contravariant and covariant tensors are equivalent.  The two types of tensors do differin higher dimensions, however.   Covariant Four-Vectors satisfy
   | (8) |  
  where   is a Lorentz Tensor.
 
 To turn a Contravariant Tensor into a covariant tensor, use the Metric Tensor   to write
    | (9) |  
  Covariant and contravariant indices can be used simultaneously in a Mixed Tensor.See also Contravariant Tensor, Four-Vector, Lorentz Tensor, Metric Tensor, Mixed Tensor,Tensor References
 Arfken, G.  ``Noncartesian Tensors, Covariant Differentiation.''  §3.8 in  Mathematical Methods for Physicists, 3rd ed.  Orlando, FL: Academic Press, pp. 158-164,  1985.Morse, P. M. and Feshbach, H.  Methods of Theoretical Physics, Part I.  New York: McGraw-Hill, pp. 44-46, 1953.   |