Whip-Torsion · Confidential preview for invited evaluator
Locomotion Efficiency — Prize Explorer
An auditable, first-principles tool for sizing the energy prize in bipedal locomotion.
Every number below derives from textbook spring-mass physics and your own inputs. Move the
assumptions, stress the model, change your fleet — the math is yours to break.
What this is and isn't: this sizes the opportunity from public physics.
It does not contain, reveal, or prove the Whip-Torsion method. The "how" is disclosed only
under a paid evaluation, validated on your own hardware.
Size the prize — honest dilution of a textbook mechanism
In an isolated reduced-order model, elastic storage-and-return cuts leg energy by
roughly 90% versus a stiff actuator that brakes and re-drives every step. That is the ceiling, not
the claim. Dilute it honestly for how much energy is actually recoverable on your hardware, and for
locomotion's share of total power, and you bracket the whole-robot prize — expressed throughout this tool as W, the whole-robot cost-of-transport reduction.
Per-step leg energy: stiff actuator vs. elastic storage-and-return, after your recoverable-fraction dilution.
Whole-robot cost-of-transport reduction
Mechanism ceiling (isolated leg energy)90%
Locomotion-energy reduction (L)49.5%
Whole-robot reduction (W)27.2%
Honest framing brackets 15–50% whole-robot: low end on existing actuators, high end with compliant co-design. W carries into tabs 2 and 4.
Your fleet economics — make the prize concrete
Enter your own platform's numbers. This applies the whole-robot reduction W = 27%
(from tab 1 — adjust there) to runtime, energy spend, and lower-limb actuator wear across your fleet.
Everything is editable; nothing here assumes our method, only its size.
Fleet size (units)
Usable battery (kWh)
Avg. total power draw in operation (W)
Operating hours / day
Operating days / year
Energy cost ($/kWh)
Lower-limb actuator set ($/unit)
Baseline actuator life (years)
Defaults are illustrative (≈ a 2.3 kWh class humanoid). Replace with yours.
Runtime per charge — uplift
+37%
Baseline runtime per charge5.1 h
With W7.0 h
Hard physics: a whole-robot energy reduction W lifts runtime per charge by W/(1−W). Operationally that is more work per charge, or fewer units and chargers for the same coverage.
Annual fleet energy savings
$—
Energy saved (kWh / year)—
Actuator wear avoided / yr (illustrative)$—
Energy savings are hard — your inputs × W. The actuator line is a directional illustration only: lower-limb wear scales with locomotion load (≈ L = 49%). Treat it as an upside signal, not a quote.
Where robots stand today — the gap, in published numbers
Dimensionless cost of transport (energy ÷ weight ÷ distance; lower is better). Humans and
passive-dynamic walkers sit near 0.2; today's powered humanoids run an order of magnitude higher.
That spread is the room the prize lives in. Pick a starting platform and watch W move it.
Apply W to:ASIMO (3.23)
Selected platform CoT3.23
After W reduction2.35
Still vs. human walking (0.2)11.8×
The point isn't to reach human efficiency in one step — it's that even a fraction of this gap is
large, recurring energy cost across a deployed fleet. Tab 2 turns this into dollars.
Break it yourself — where does the prize disappear?
Don't take the headline on faith. This is the full surface of whole-robot reduction W
across both honest dilution knobs. Find the corner where your assumptions live. If the prize is only
real in the optimistic corner, you should know that before any conversation — so here it is, exposed.
Your current point (tab 1)0.55 / 0.55
W here27%
X axis: recoverable elastic fraction (0.40 → 0.80). Y axis: locomotion's share of power (0.40 → 0.70). Contours: 15%, 25%, 35%, 45% whole-robot reduction. Marker: your current assumptions.
The honest read: W stays at or above ~15% across essentially the entire plausible region, and
only reaches the high-40s in the compliant-co-design corner. That is the claim, stated as a
surface instead of a slogan.