Linear Algebra
13.98 min read

Alternative Derivation of the Tangent Vector

There is an instructive alternative way to arrive at the tangent vector formula using the local linear approximation. The LLA of the trajectory γ\boldsymbol{\gamma} at t0t_0 is γ(t0+h)γ(t0)+γ(t0)h\boldsymbol{\gamma}(t_0+h) \approx \boldsymbol{\gamma}(t_0) + \boldsymbol{\gamma}'(t_0)h.

This means: near t0t_0, the curve γ\boldsymbol{\gamma} is well-approximated by the straight-line trajectory tγ(t0)+(tt0)γ(t0)t \mapsto \boldsymbol{\gamma}(t_0) + (t-t_0)\boldsymbol{\gamma}'(t_0). The tangent line to the curve is exactly this linear approximation.

More explicitly: γ(t0)\boldsymbol{\gamma}'(t_0) is the unique vector v\mathbf{v} such that γ(t0+h)γ(t0)hv=o(h)\boldsymbol{\gamma}(t_0+h) - \boldsymbol{\gamma}(t_0) - h\mathbf{v} = o(h) as h0h \to 0. This is the 1D special case of the Jacobian definition: Jγ(t0)=γ(t0)J\boldsymbol{\gamma}(t_0) = \boldsymbol{\gamma}'(t_0) is an m×1m\times 1 column vector.

Formal View

Theorem 13.3 — Tangent Vector as Jacobian
For γ:IRm\boldsymbol{\gamma}: I \to \mathbb{R}^m (IRI \subseteq \mathbb{R}), the Jacobian Jγ(t0)Rm×1J\boldsymbol{\gamma}(t_0) \in \mathbb{R}^{m\times 1} is the column vector γ(t0)\boldsymbol{\gamma}'(t_0). It is the unique vector satisfying
limh0γ(t0+h)γ(t0)hγ(t0)h=0\lim_{h\to 0}\frac{\|\boldsymbol{\gamma}(t_0+h)-\boldsymbol{\gamma}(t_0)-h\boldsymbol{\gamma}'(t_0)\|}{|h|}=0

This shows that tangent vectors are simply the n=1n=1 case of the general Jacobian framework.

Remark 13.1 — Consistency of Notation
The tangent vector γ(t0)\boldsymbol{\gamma}'(t_0) can also be written as Dγ(t0)D\boldsymbol{\gamma}(t_0) or Jγ(t0)J\boldsymbol{\gamma}(t_0) — all refer to the same object, the derivative of γ\boldsymbol{\gamma} at t0t_0, viewed as a linear map from R\mathbb{R} to Rm\mathbb{R}^m (represented by an m×1m\times 1 column vector).

Why This Matters

Connecting tangent vectors to the Jacobian framework shows that all derivative concepts (gradient, Jacobian, tangent vector) are special cases of the same abstract idea.

  • Chain rule for compositions of trajectories with scalar-valued functions
  • Path integrals: integrating a scalar field along a curve uses the tangent vector
  • Frenet-Serret formulas in differential geometry use higher-order derivatives

Quiz

Question 1

The Jacobian Jγ(t0)J\boldsymbol{\gamma}(t_0) for a trajectory γ:RRm\boldsymbol{\gamma}: \mathbb{R} \to \mathbb{R}^m is:

Question 2

The tangent vector γ(t0)\boldsymbol{\gamma}'(t_0) can be computed component-wise: γ(t0)i=fi(t0)\boldsymbol{\gamma}'(t_0)_i = f_i'(t_0) for each component fif_i of γ\boldsymbol{\gamma}.

Common Mistakes

  • Treating the Jacobian of a trajectory as a scalar instead of a column vector.
  • Confusing the m×1m\times 1 tangent vector with the 1×n1\times n gradient (they apply to opposite types of functions).
  • Forgetting that the LLA of a trajectory is a straight-line approximation, not the exact curve.