Calculate the whole chain from the blood to the cooling medium, for any cooling method. Pick a scenario and a product, and you are done. The sliders are still there under the plus signs if you want to dig, but nobody needs to touch them.
Sets skin temperature, blood-flow ceiling, grip moisture and how hard the body defends itself against cold.
Same model, but fed with pessimistic, middle or optimistic assumptions within the range we have support for.
These are the sliders where the answer changes in a way that matters for the product. Everything else is either a property of the product you have chosen, or a physiological constant. If you move something here you are still building the same product, you are just asking a question about it.
The model calculates the whole chain from the blood to the cooling medium:
Q = (skin temperature − surface temperature) × contact area / (contact resistance + tissue resistance + product resistance),
limited by what the blood flow can carry away and by the product's own capacity.
The tissue resistance is not constant. It rises when the skin gets cold and the vessels constrict, which is the
feedback that makes a product that is too cold worse in the end, not better.
KYLA's internal construction is not published. It is represented by lumped, measured quantities: stored energy as a
function of temperature, the internal base resistance, how fast the melt front develops, and the contact area. The results
are identical to the full model. Competitor products are built from their published specifications and the physics of their
architecture; none of them has been tested by us.
These are set by the scenario and by the literature. They do not need to be touched to use the tool, but this is where the uncertainty lives. If you want to know how much our numbers are really worth, drag the AVA threshold and see how much everything moves.
With the grip pattern below, and counted until the product is no longer usable.
The boxes above show equilibrium, that is what the product gives if you hold it for as long as you like. That is not how it is used. Here a real pattern is run instead: short grips with rest in between, where each grip both drains the reservoir and benefits from the skin not yet having had time to get cold.
Grip length and rest are set under What if… in the left column.
First grip versus last grip shows whether the product holds its output or fades. A product that starts high and drops is a different kind of product from one that stays flat, even if the average happens to be the same.
How long the product stays cold without being used, in the selected storage.
All methods calculated with the same user and environment, so the comparison is fair.
All figures are for the WHOLE system, that is both hands for the products that cool two hands (whether as two pieces or one double-sided unit)
and one hand for those that only cool one. The Units · hands column shows both how many pieces the product consists of and how many hands it cools. These are not the same thing: Therabody and NICE ROCC are ONE unit that cools both palms, while our cylinder and Apex Narwhals are two separate pieces.
Both power columns come from the same simulation, so the difference between them is purely
degradation over the session and not two different definitions.
The table is sorted on SUSTAINED W, that is the average over the first ten active minutes.
A product that runs out after five minutes therefore gets half the average, because the remaining
minutes count as zero. It is the only column that penalises a strong but short-lived product
fairly.
Thermal W is what a calorimeter would measure. To the core W is what actually lowers
body temperature, after vasoconstriction and after non-glabrous skin insulates the core.
The difference between the two columns is the whole point of palm cooling.
Two units give 2.0x thermally but 1.65x to the core, because two hands together
approach the perfusion limit. The factor can be changed under Physiology.
| Term | Value | Comment |
|---|---|---|
| Cooling medium temperature | PCM or liquid inside | |
| Surface against the skin | what the palm actually meets under load. For Apex it should land close to their published 12.8 C. | |
| Skin surface temperature | controls the vasoconstriction | |
| Temperature difference | deep skin minus cooling surface | |
| R contact | 1 / contact conductance | |
| R tissue | rises when the vessels constrict | |
| R product | architecture dependent | |
| Vessel opening | share of the palm's MAXIMUM AVA flow that is still open. 100% = the shunts wide open, blood rushing just under the skin. 10% = they have closed and only ordinary capillary flow remains. Controls both the blood ceiling and the core coupling. | |
| Blood-borne ceiling | what the circulation can carry | |
| Core coupling | the body part's anatomy | |
| Plate drift under load | Peltier: how far above its advertised setpoint the plate ends up under a warm palm. Larger = weaker element or heat sink; the setpoint holds only unloaded | |
| Hot side temperature | Peltier: must be cooled away | |
| Calculated COP | falls when the hot side gets hot | |
| Heat flux per cm² | compare with Heller and Grahn's measured 0.17 W/cm² at a 16 C surface, and 0.23 with negative pressure | |
| Stored energy | usable, per unit | |
| Passive leakage | what the surroundings steal |