vectors and tensors
vectors and tensors the dependency chain
that makes vectors and tensors necessary, rather than around historical
chronology. The original sequence runs algebra → calculus → vectors →
quaternions → Maxwell → vector analysis → spacetime → curvature →
tensors → relativity.
TOC
Part I — Representation Debt
Scalar description
1.1 Magnitude-only quantities
1.2 Why one number is insufficient
1.3 Physical versus informational dimensions
1.4 SOURCE ≠ coordinate descriptionCoordinates and components
2.1 Coordinate systems
2.2 Basis choice
2.3 Components as representation
2.4 Object versus component list
2.5 Representation change as the first GRM transport problem
Part II — Vector Necessity
Vector space
3.1 Addition and scalar multiplication
3.2 Linear independence
3.3 Dimension
3.4 Basis and coordinate expansion
3.5 Directed physical quantities as one application, not the definitionChange of basis
4.1 Same vector, different components
4.2 Transformation matrices
4.3 Equivalence across representations
4.4 Invariant consequencesDual space
5.1 Linear functionals
5.2 Dual basis
5.3 V versus V*
5.4 Natural pairing
5.5 Why vectors and covectors must remain distinct
Part III — Arity Forces Tensors
From one slot to many
6.1 Linear maps
6.2 Bilinear maps
6.3 Multilinear maps
6.4 Native arity as structural necessityTensor product
7.1 Construction from V and V*
7.2 Tensor type
7.3 Covariant, contravariant, mixed
7.4 Tensor as intrinsic object
7.5 Components as carrier onlyContraction
8.1 Natural V*–V pairing
8.2 Rank reduction
8.3 Scalar invariants
8.4 Why contraction does not require a metric
Part IV — Extra Geometry
Metric
9.1 Bilinear form
9.2 Length and angle
9.3 Metric as rank-2 tensor
9.4 V ↔ V*
9.5 Raising and lowering
9.6 Metric is additional structure, not tensor prerequisiteTransformation and invariance
10.1 Tensor transformation law
10.2 Same tensor → different basis → different components
10.3 Same multilinear consequences
10.4 Symmetry and antisymmetry
10.5 Coordinate independence
The book itself eventually reaches this modern distinction: tensors are not merely component arrays; their components transform while the intrinsic object is preserved.
Part V — Differential Structure
Tensor fields
Connections
Parallel transport
Covariant derivative
Torsion
Curvature
Metric compatibility
Levi-Civita reconstruction
Part VI — Physical Closure
Stress as bilinear structure
Maxwell: vectors → spacetime tensor
Minkowski metric
Riemann curvature
Ricci contraction
Einstein tensor
Matter-energy tensor
Field equations
Bianchi identities and conservation
Noether symmetry → conserved structure
Final GRM kernel:
object
→ representation
→ transformation
→ invariant relation
→ multilinear arity
→ tensor
→ optional metric
→ connection
→ curvature
→ intrinsic field law.
Quaternions, Maxwell, Minkowski, Ricci, and Einstein should become case studies attached to the dependency they expose, not the spine itself.
Comments
Post a Comment