Seeking licensing and collaboration with allied Defence departments, global space agencies, leading QS-ranked universities, advanced technology institutes, AI and robotics leaders, and sector-specific corporations.
HOW CAN MOVEMENT POWER THE MACHINE?
The passive KRA core already turns movement into bilateral motion and lift assistance. Once spring-loaded nodes travel on linear rails, that same movement also leaves a measurable trace: displacement, oscillation and force change. The pathway can therefore support the body and describe what the body just did.
How one network changes the load
The limbs remain the endpoints. The user moves the mass of the arms, wearable and any object held in the hands while configured KRA force assists, resists or transfers demand between sides.
Attach the tether to a tool, cargo point or carried system and the mechanism supports the object itself. Within its configured range, the load can remain suspended when the hands release it.
Residual demand is the attached load minus the effective KRA support at that position. Below balance, the user carries the difference. At balance, the supported load approaches neutral. Above balance, excess assistance creates upward bias.
The same routing architecture can place additional redirection nodes through limbs, suit structures, rucksacks, steering mechanisms or robotic joints without changing the continuous bilateral core.
For load-balance studies, generation testing or supporting resources, contact AORTE.
How parallel W-nodes change the mathematics
The calculation begins with cord-length compatibility, not an assumed output. For an ideal low-stretch path, endpoint travel and every moving node satisfy one shared constraint: ΔℓL + ΔℓR + Σ njΔxj ≈ 0. The signed coefficients nj come from the actual W routing and change when another sheave, wrap or linear stage is added.
WW or multi-W branches can move together, but their ratios depend on whether they share one cord, separate cords, equal spring rates, a common carriage or independent clutch states. Identical equal-displacement branches give keq = Σki. Series and compound stages follow different relationships. More bearings may expose more stroke while adding friction, inertia and bend loss.
In a simple two-end normalization, sL = TL/(TL+TR) and sR = 1−sL. A 50/50 reading is the calibrated equilibrium zone, not a guarantee. If one endpoint is tethered at its exit limit, the fixed boundary receives reaction while the cord and movable nodes can still change state.
A node can remain passive, carry a dial clutch or one-way pawl, couple to an electromagnetic or piezoelectric pickup, drive a piston, or compress air. Each addition changes the local spring, damping, friction, clutch and generator-reaction terms.
MODEL BOUNDARY · Node count alone does not determine travel, suspension or electrical output. The routing matrix, component properties, boundary conditions and measured losses must be defined for each configuration.
AORTE’s issued KRA architecture establishes a bilateral cord path, movable sheaves, linear-bearing travel, configurable resistance, sensing and a generator-coupling foundation. Complementary patents accessible through collaboration can extend that pathway with mechanical rectification, one-direction rotary output, flywheel smoothing, generation, conditioning and storage without confusing a development pathway with measured performance.
Measure free-end travel, bearing travel, cord angle, repetition rate and hysteresis to identify the effective ratio.
Record tension, track load, preload, parasitic resistance and lift assistance before and during harvesting.
Measure rectifier efficiency, shaft speed, torque, generator voltage and current, conditioning loss and stored energy.
Define mass, duty cycle, thermal rise, durability, fault behavior and applicable dust, water, vacuum or suit-interface conditions.



