7.8 Tensor Vector Component Case
In tensor algebra, vector components transform under coordinate changes, forming the basis for tensor structures and invariance.
Tensor Vector Component Case is the instance of a tensor's component structure in which exactly one index is present, upper in the standard convention, so that the tensor's components form a single list of (n) numbers rather than the empty structure of a scalar or the multi-axis array of higher-rank tensors.
Definition and Scope
Rank One With a Single Upper Index
A tensor in the vector component case has type ((1,0)), giving components
with (i) ranging over (1,\dots,n) in an (n)-dimensional space, producing exactly (n) scalar entries arranged along a single axis, one more index than the scalar case and one fewer axis than any rank-2 or higher case.
Components as Coefficients of a Basis Expansion
The vector component case arises directly from expanding a vector (v) in terms of basis vectors (e_i):
with the coefficients (v^i) constituting the full component structure of (v) relative to that basis, and changing entirely if a different basis is chosen.
Structural Properties
Transformation as the Simplest Nontrivial Case
The vector component case is the first rank at which basis dependence becomes visible, since the scalar case is unaffected by a change of basis while a vector's components transform with a single factor of the inverse change-of-basis matrix:
serving as the simplest setting in which contravariant transformation behavior can be illustrated without the added complexity of multiple interacting indices.
Absence of Internal Symmetry
With only one index present, there is no second index of matching variance to compare it against, so the vector component case has no internal symmetry or antisymmetry to speak of; questions of index exchange and symmetric versus antisymmetric behavior only become meaningful once a tensor carries at least two indices of the same variance.
Pairing With the Covector Case
The vector component case has a direct counterpart in the covector, or ((0,1)), case, whose single lower index transforms with the change-of-basis matrix directly rather than its inverse; the two cases together, contravariant and covariant single-index structures, exhaust the possibilities for a tensor carrying exactly one index.
Role Within Tensor Algebra
Building Block for Higher-Rank Constructions
The vector component case, together with the covector case, supplies the elementary pieces from which higher-rank tensors are constructed through the tensor product, each additional factor contributing one more index and extending the vector case toward richer multi-index structures.
Common Occurrence in Applications
Because a great many quantities of interest, positions, velocities, forces, and gradients among them, are naturally described by a single direction-dependent list of numbers, the vector component case is the most frequently encountered nontrivial tensor structure in applied settings, serving as the starting point before more elaborate rank-2 and higher structures are introduced.