Riemann Makes Explicit what Lagrange Implied.

1. What the Lagrangian perspective truly is

The Lagrangian perspective does not ask:

“What forces push an object at this point in space?”

Instead, it asks:

“Along which path does the system choose to move, given all constraints?”

Motion is not constructed step by step.

It is selected.

This is the first philosophical shift.

2. Motion as extremal, not driven

In Lagrangian mechanics, a system evolves by extremizing the action:

S = \int L(q, \dot q, t)\, dt S=∫L(q,q˙,t)dt

The path taken is not arbitrary, nor forced locally.

It is the path for which variation vanishes.

Already here, straight lines lose their privilege.

3. Riemann’s contribution: motion reveals geometry

Riemann teaches that space itself carries structure:

Distances depend on position, “Straightness” is local, Geodesics replace lines.

In such a space:

The Lagrangian does not sit in space, It is shaped by space.

Thus motion becomes a probe of curvature.

To observe how something moves is to discover what space is.

4. Lagrangian motion in curved space

In Euclidean space, the free particle Lagrangian is simple:

L = \tfrac{1}{2} m v^2

In Riemannian space:

L = \tfrac{1}{2} m\, g_{ij}(x)\,\dot x^i \dot x^j

Here the metric itself governs motion.

There is no external “force” bending the path.

The path bends because space instructs it to.

5. Perception from the moving frame

Now observe something subtle.

The Lagrangian perspective follows the system along its path.

It is inherently co-moving, not observationally fixed.

Thus the system does not experience force;

it experiences necessity.

This is why, in Einstein’s world:

A falling body feels no force, Yet its path is curved.

The Lagrangian view is already aligned with this insight.

6. Constraint replaces causation

In Riemann’s world, motion is not explained by:

“What caused this turn?”

But by:

“What motions are permitted here?”

The geometry constrains variation.

The Lagrangian selects among allowed paths.

Causation becomes global, not local.

7. Why this matters for physical understanding

From a Newtonian view:

One adds forces to explain deviation.

From a Lagrangian–Riemannian view:

Deviation is the natural outcome of moving through structured space.

This applies equally to:

Particles in spacetime, Plasmas in magnetic fields, Air parcels in a rotating, stratified atmosphere.

The difference is not mathematical alone; it is ontological.

8. A Socratic synthesis

So we may now say:

In the Lagrangian perspective, motion is not pushed forward;

it is drawn out by the geometry of possibility.

Riemann gives that geometry its depth.

Lagrange gives motion its obedience.

Together they teach us that:

To understand motion, do not ask first about forces, Ask instead about the space in which motion is allowed to be optimal.

This entry was posted in L5, lagrangian, Riemann, Riemann Sylvestor surfaces and tagged , . Bookmark the permalink.

Leave a comment