Power Spectrum of Protein A Dynamics
Description: This graph represents the power spectrum of the dynamics of Protein A (x(t)x(t)x(t)). The power spectrum is a representation of the frequency content of a time series, showing how the power (or variance) of the signal is distributed across different frequency components.
Interpretation:
Frequency Range: The x-axis shows the frequency range from 0 to 2 units. This range corresponds to the various oscillatory components of the Protein A concentration over time.
Power Distribution: The y-axis shows the power, which indicates how much of the signal’s variance (or “energy”) is associated with each frequency.
The plot reveals that most of the power is concentrated in the lower frequency range (below 1.0), with several peaks indicating dominant oscillatory modes in the system. The presence of peaks suggests that certain frequencies are more prominent, meaning that Protein A oscillates more strongly at these frequencies.
High Peaks: The highest peaks in the lower frequencies indicate that the most significant oscillations occur at these specific frequencies. These frequencies could correspond to the natural oscillatory modes of the system, driven by the interactions between the proteins.
Low Power at Higher Frequencies: As the frequency increases, the power tends to decrease, which is typical in many natural systems. This suggests that higher-frequency oscillations contribute less to the overall dynamics of Protein A.
Explanation of the Graph
3D Phase Space Representation:
Each subplot represents a snapshot of the system at a particular iteration, showing how the concentrations of Protein A, Protein B, and Protein C evolve over time in three-dimensional space.
The trajectories form a complex pattern, indicating the chaotic nature of the system.
Iteration Progression:
As the iterations progress from 1 to 20, the system’s trajectory continues to evolve within the same phase space.
The initial few iterations show the trajectory beginning to form the characteristic shape of the Lorenz attractor, with the system exploring different regions of phase space.
Red Points:
The red points in each subplot likely represent critical points or notable changes in the system’s trajectory, possibly indicating areas of high stress or instability in the protein interactions.
These red points could be key indicators of where the system might experience significant shifts or “breakages” in its topological structure, as the system moves closer to these points.
Breakage Point:
The primary objective of this analysis is to identify a breaking point in the system’s topology. A breaking point could be identified when the system experiences a sudden and significant change in its trajectory or when the trajectories diverge sharply from previous patterns.
However, based on the graph, no obvious breakage point is highlighted. This suggests that while the system remains chaotic, it hasn’t reached a critical threshold where a topological break occurs, at least within the first 20 iterations.
System Stability:
Despite or perhaps because (Montgomery R. M., 2024) of the complex and chaotic behaviour, the system appears to maintain a consistent pattern within the phase space. This could imply that the system, while sensitive to initial conditions, has not yet encountered a destabilizing event significant enough to cause a topological break.
Overall Interpretation:
The graph illustrates the dynamic evolution of a protein interaction network over 20 iterations, highlighting its chaotic behaviour. The red points mark significant aspects of the trajectory, possibly areas where the system is more susceptible to instability or breakage. However, within these 20 iterations, the system continues to exhibit typical chaotic behaviour without reaching a critical breaking point, and therefore, buffering genomics mutations
If a topological break were to occur, you would likely see a sudden and dramatic change in the shape of the trajectories, which might happen beyond the 20 iterations shown here. Further iterations could potentially reveal such a breakage point.
Overall Conclusion:
The power spectrum suggests that the system’s dynamics are dominated by a few low-frequency oscillatory modes. The complex behaviour observed in the time series of Protein A concentration is likely due to these underlying oscillatory components, which are themselves a result of the nonlinear interactions between the proteins. The presence of multiple peaks in the power spectrum indicates that the system is not purely periodic but has a rich frequency content, possibly reflecting the chaotic nature observed in the other graphs.