Gradient-Based Interactions

In FM, physical interaction does not begin with objects pushing each other.

It begins with structures responding to gradients in the medium.

A gradient is a spatial difference in how FM is organized.
Where such a difference exists, the conditions for stability are not the same in all directions.

This means that interaction is not something added afterward.
It is already present wherever structure and gradient coexist.

Why gradients are fundamental

A push is usually local and short-lived.

A gradient is more fundamental because it defines the direction in which reorganization is easier or harder to sustain.

This is why so much of physics can be understood through gradients:

falling and orbiting
fluid motion
current in conductors
attraction and repulsion
chemical reorganization
propagation of waves

In each case, what happens depends on how structure responds to the surrounding difference in FM conditions.

Interaction begins before contact

Two structures do not need to collide directly in order to interact.

If their gradient fields overlap, they already affect one another.

The overlap changes:

what local configurations are supported
how much reorganizational work is required
whether coherent sharing of structure is possible

Interaction therefore begins before contact.

Contact is only the stronger local form of an already existing gradient relation.

The same law, different outcomes

The same gradient principle acts on all structures.

What changes from case to case is the structure itself.

This is why identical surroundings can produce different responses:

one structure may remain stable
another may polarize
another may reorganize
another may be repelled

The difference does not come from multiple laws.
It comes from compatibility, geometry and capacity.

Compatibility and interface

When structures approach one another, the outcome depends on whether their interface can reorganize FM coherently.

If the meeting surfaces are compatible:

support can be shared
reorganizational cost falls
a more stable collective structure may form

If the meeting surfaces are incompatible:

support cannot be shared coherently
internal resistance rises
further approach becomes harder or impossible

Attraction and repulsion are therefore not separate principles.
They are different outcomes of the same gradient logic.

Orientation toward the strongest compatible gradient

Structures do not bind randomly.

When several interactions are possible, a structure tends to orient toward the strongest compatible gradient support.

This means that:

preferred orientations are expected
opposite structures bind in specific ways rather than by arbitrary contact
like structures may fail to bind even under the same general gradient conditions
larger ordered patterns can emerge from locally asymmetric parts

A structure may be internally directional and still show stable or nearly symmetric large-scale behavior, because it reorients toward the best-supported configuration.

Why binding is selective

Binding does not occur simply because one structure “attracts” another.

It occurs only when three things can be maintained together:

sufficient gradient support
compatible interface geometry
enough reorganizational capacity for both structures to remain stable

This is why many potential interactions never become stable bonds.

The structures may influence one another, but no compatible shared organization can be sustained.

Local stability and global response

Every structure is locally supported by its own gradient relations.

But no structure exists in isolation.

The total behavior depends on:

internal gradient support
surrounding gradient conditions
neighboring structures
and the capacity of FM to maintain coherent organization

This is why a structure may remain stable under one condition and reorganize under another, even though its core has not changed.

The local support remains in part, but the total surrounding field no longer does.

Selective response

Not all parts of a system respond equally to a changed gradient.

Some structures are deeply supported and barely affected.
Others are near the edge of stability and respond quickly.

This is why:

outer electrons reorganize before inner ones
surface chemistry changes before bulk material
some atomic groups react while others remain unchanged
local dipoles reorient before larger structures reorganize

Gradient-based interaction is therefore selective, not uniform.

From interaction to structure

Gradient-based interaction does not only move things.

It also determines what structures can exist.

If a new gradient configuration allows a more stable shared organization, matter can bind.
If not, it remains separate or becomes unstable.

This makes gradients central not only to motion, but also to:

atoms
molecules
dipoles
magnetic ordering
and stored chemical structure in batteries

Why pushes are secondary

Many processes that appear as pushes can be understood more fundamentally as gradient-following behavior.

A push may still exist as a local expression of overpressure or direct mechanical constraint.
But in most cases, what matters physically is that the system has a preferred direction in which reorganizational cost is lower.

This is why gradient language often reaches deeper than push language.

One physical logic

In FM, the same physical logic can therefore be used broadly:

a structure exists because FM supports it
that support appears as a surrounding gradient
overlapping gradients create interaction
compatibility determines outcome
orientation selects the strongest supported relation
reorganization proceeds toward a new stable configuration

This gives one continuous explanation from simple interactions to complex material behavior.

Final statement

In FM, interactions are gradient-based because structure and gradient are inseparable.

A structure is maintained by the way FM is organized around it,
and when that organization overlaps with other structures, interaction begins.

Attraction, repulsion, binding, motion and reorganization are all consequences of how gradients shape what the medium can support.

Where more than one interaction is possible, structures tend to orient toward the strongest compatible gradient.
This is why binding is selective, directional, and non-random.