9
Hypercycle Stability and Parasitic Challenge
HYC-1979 Lesson 2: Catalytic, Which, System
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A hypercycle is a closed loop of catalytic support: each member assists the next, and the loop returns to its own start. That architecture makes the cycle self-reinforcing, but it also opens a door. Any element that receives catalytic help from the loop while returning nothing can multiply inside the same reactor, living off the very products the hypercycle generates. Such an element is a parasite.

What counts as a parasite

A parasite is a self-reproductive element that exploits the hypercycle without contributing to it. It is not an inert mutant that merely decays: it replicates on its own, drawing on catalytic support supplied by the cycle, yet it adds no catalysis of its own to the loop. Because the hypercycle must sustain that growth without receiving anything back, the parasite is a direct competitor for the same finite pool of material.

Constant organization and the T.13.8 system

The competition is analysed under constant total concentration, , where is the parasite concentration and x is the concentration of the hypercycle component. With k the catalytic constant of the hypercycle and that of the parasite, the coupled dynamics are:

  • Parasite:
  • Hypercycle component:

In both equations the first term is growth and the second term is the constant-organization dilution or outflow that holds the total fixed. The parasite grows quadratically in its own concentration, kAcA2, which is exactly what makes it self-reproductive, whereas the hypercycle component grows only through the cross term .

Two-corner phase portrait on the concentration simplex S2 Constant organization holds the total cA + x = c0 fixed, so only the composition changes. 1 c0 < k / kA ⇒ ẋ > 0 the hypercycle component still grows Parasite corner cA = c0, x = 0 unstable Hypercycle corner x = c0, cA = 0 stable 2 c0 > k / kA ⇒ ẋ < 0 the parasite displaces it Parasite corner cA = c0, x = 0 stable Hypercycle corner x = c0, cA = 0 unstable Decision threshold THRESHOLD c0 = k / kA Two terms per equation Growth kAcA2 and k cAx Dilution (cA / c0)(kAcA2 + k cAx) Winner takes all The flow settles at one of the two corners — there is no stable interior coexistence.

Two corner fixed points and a concentration threshold

The system has two fixed points, and both sit at corners of the concentration simplex: a parasite-dominated state (, ) and a hypercycle-dominated state (, ). Which corner the flow reaches depends on the rate constants together with the total concentration. The decisive comparison is

for , and for .

Below the threshold the hypercycle component still increases and the flow is driven towards the hypercycle corner; above it the component is diluted away faster than it is produced and the flow is driven towards the parasite corner. Crossing therefore flips the sign of ẋ and reverses which corner wins. In the generic case the phase flow settles at one of the two corners instead of at a stable interior state of coexistence.

Where this simplified model stops
The system assumes a well-mixed reactor under constant organization. Spatial structure, compartmentalization, mutation and selection acting between higher-level units are deliberately excluded, so the corner-attractor result is a property of the simplified model only. On its own, this model does not yet resolve the parasite challenge; it defines it.