Entropy, Information, and Life: Exploring the Interplay of Shannon and Boltzmann Entropies in Biological Systems

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Introduction

Entropy plays a pivotal role in understanding the behavior of biological systems, both as a thermodynamic measure (Boltzmann entropy) and as a probabilistic measure of information (Shannon entropy). While organisms locally reduce entropy through evolution and natural selection, this reduction occurs at the expense of increasing entropy in their surroundings. Mathematical models and real-world case studies help elucidate the mechanisms underlying this phenomenon, demonstrating how entropy exchange sustains life and drives evolutionary complexity.


1. Entropy and Biological Systems

1.1 Boltzmann Entropy in Living Systems

The Boltzmann entropy equation is:S=kBln⁡ΩS = k_B \ln \OmegaS=kB​lnΩ

where:

  • SSS is entropy,
  • kBk_BkB​ is the Boltzmann constant,
  • Ω\OmegaΩ is the number of microstates corresponding to a macrostate.

In biological terms, living organisms exist in highly constrained macrostates (low Ω\OmegaΩ), requiring energy input to maintain this organization. Consider a simple case study of cellular respiration:

  • Input: Glucose (low-entropy molecule) and oxygen.
  • Output: CO₂, water, and ATP.
  • Entropy Change: Cellular metabolism increases the entropy of the surroundings, releasing heat and waste products.

Mathematical model of metabolic entropy: The Gibbs free energy equation quantifies this process:ΔG=ΔH−TΔS\Delta G = \Delta H – T\Delta SΔG=ΔH−TΔS

where:

  • ΔG\Delta GΔG: Change in free energy,
  • ΔH\Delta HΔH: Change in enthalpy,
  • TTT: Temperature,
  • ΔS\Delta SΔS: Change in entropy.

Organisms extract usable energy (ΔG<0\Delta G < 0ΔG<0) while increasing ΔS\Delta SΔS, thus adhering to thermodynamic laws.


1.2 Shannon Entropy in Biological Systems

Shannon entropy is expressed as:H=−∑ip(xi)log⁡2p(xi)H = – \sum_{i} p(x_i) \log_2 p(x_i)H=−i∑​p(xi​)log2​p(xi​)

where:

  • HHH is the entropy,
  • p(xi)p(x_i)p(xi​) is the probability of outcome xix_ixi​.

In genetic terms, HHH measures the uncertainty in nucleotide sequences. As evolution progresses, certain sequences become favored, reducing HHH. For example:

  • A random DNA sequence has high Shannon entropy.
  • After selective pressures (e.g., environmental factors), the sequence becomes structured, lowering HHH.

Case Study: Evolution of antibiotic resistance.

  • Initial state: Diverse bacterial population with high Shannon entropy.
  • Selective pressure: Antibiotics eliminate less resistant strains.
  • Final state: Dominant resistant strain reduces population-level HHH, but the process generates mutations, contributing to environmental entropy.

2. Evolution as an Entropy-Reducing Process

2.1 Fisher Information and Natural Selection

Steven A. Frank’s works provide a quantitative foundation for understanding how natural selection maximizes Fisher information, a measure closely tied to Shannon entropy.

Fisher information equation:I(θ)=∫(∂ln⁡f(x∣θ)∂θ)2f(x∣θ)dxI(\theta) = \int \left( \frac{\partial \ln f(x|\theta)}{\partial \theta} \right)^2 f(x|\theta) dxI(θ)=∫(∂θ∂lnf(x∣θ)​)2f(x∣θ)dx

where:

  • I(θ)I(\theta)I(θ): Fisher information,
  • f(x∣θ)f(x|\theta)f(x∣θ): Likelihood function,
  • θ\thetaθ: Parameter of interest.

Fisher information quantifies how much information a trait (e.g., genetic variability) provides about an environment. Evolution increases I(θ)I(\theta)I(θ) by selecting traits that better “fit” environmental constraints, thereby reducing Shannon entropy.

Case Study: Peppered moths during the Industrial Revolution.

  • Before industrialization: Light-colored moths dominated (low HHH).
  • During industrialization: Dark-colored moths became dominant due to selective pressure (reduction in HHH).
  • Entropy export: Increased environmental entropy from soot and pollution altered the ecosystem’s informational landscape.

2.2 Thermodynamic Costs of Selection

Natural selection operates within thermodynamic limits, as shown by the Landauer principle:ΔSenv≥kBln⁡2TΔHsys\Delta S_{\text{env}} \geq \frac{k_B \ln 2}{T} \Delta H_{\text{sys}}ΔSenv​≥TkB​ln2​ΔHsys​

This principle connects information erasure (entropy reduction) in a system to entropy increase in the environment. For example:

  • As organisms adapt to reduce genetic entropy, the biochemical processes (e.g., protein synthesis) release heat, increasing environmental SSS.

3. Linking Shannon and Boltzmann Entropies

3.1 Unified Entropy Framework

Arieh Ben-Naim’s work provides a theoretical bridge between Shannon and Boltzmann entropies. For a biological system, the two forms of entropy relate as follows:

  • Boltzmann entropy represents the physical state-space constraints.
  • Shannon entropy reflects probabilistic uncertainty within those constraints.

Example: Protein folding.

  • Initial state: High Boltzmann entropy (unfolded state with many microstates).
  • Final state: Low Boltzmann entropy (folded state with fewer microstates).
  • Information gain (Shannon entropy reduction): Folding encodes functional information, increasing the system’s order.

Mathematical model: The entropy change during folding can be expressed as:ΔStotal=ΔSsystem+ΔSsurroundings\Delta S_{\text{total}} = \Delta S_{\text{system}} + \Delta S_{\text{surroundings}}ΔStotal​=ΔSsystem​+ΔSsurroundings​


3.2 Entropy Export in Evolution

As biological systems reduce internal entropy, they export entropy to their environment. For example, the waste products of metabolism and ecological interactions create high-entropy states in surrounding systems.

Case Study: Coral reefs.

  • Internal entropy reduction: Corals organize calcium carbonate into low-entropy structures.
  • Entropy export: Heat dissipation and metabolic byproducts increase oceanic entropy.

4. Implications and Broader Perspectives

4.1 Abiogenesis and Entropy

The emergence of life likely involved local reductions in entropy, driven by environmental energy flows. Early self-replicating molecules acted as “entropy transducers,” decreasing internal entropy while increasing the entropy of surrounding chemical environments.

Mathematical model of prebiotic entropy:ΔSprebiotic=ΔSreplicator+ΔSchemical\Delta S_{\text{prebiotic}} = \Delta S_{\text{replicator}} + \Delta S_{\text{chemical}}ΔSprebiotic​=ΔSreplicator​+ΔSchemical​

Experimental simulations, like the Miller-Urey experiment, demonstrate how energy inputs can drive the formation of low-entropy organic molecules from high-entropy precursors.


4.2 Artificial Systems and Entropy

Machine learning and artificial intelligence systems parallel biological entropy dynamics. Neural networks, for example, reduce internal Shannon entropy as they optimize model parameters, at the cost of computational energy.

Mathematical model of entropy reduction in neural networks: During backpropagation, the cross-entropy loss function is minimized:H(p,q)=−∑ip(xi)log⁡q(xi)H(p, q) = – \sum_{i} p(x_i) \log q(x_i)H(p,q)=−i∑​p(xi​)logq(xi​)

where:

  • p(xi)p(x_i)p(xi​): True probability distribution,
  • q(xi)q(x_i)q(xi​): Model’s predicted distribution.

Case Study: Autonomous vehicle training.

  • Initial state: High Shannon entropy (poor model accuracy).
  • Final state: Low Shannon entropy (optimized predictions).
  • Entropy export: Energy dissipation from GPUs increases environmental entropy.

5. Conclusion

The interplay between Shannon and Boltzmann entropies offers a compelling framework for understanding life as an information-preserving phenomenon. Through processes like natural selection, living systems reduce internal entropy by increasing environmental entropy, mirroring thermodynamic principles. Mathematical models and case studies—from protein folding to ecosystem dynamics—illustrate these principles in action, highlighting the intricate balance that sustains life. By integrating insights from biology, thermodynamics, and information theory, we deepen our understanding of life’s complexity and its place within the broader universe.


References

  1. Arieh Ben-Naim, “Entropy, Shannon’s Measure of Information and Boltzmann’s H-Theorem,” MDPI (2017).
  2. Steven A. Frank, “Natural Selection Maximizes Fisher Information,” Arxiv (2009).
  3. Steven A. Frank, “Natural Selection: How to Read the Fundamental Equations of Evolutionary Change in Terms of Information Theory,” Arxiv (2012).
  4. “Entropy and Life,” Wikipedia.
  5. “Entropy in Thermodynamics and Information Theory,” Wikipedia.

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