Motility Powered by Supramolecular Springs and Ratchets

Author:

Mahadevan L.1,Matsudaira P.23

Affiliation:

1. Department of Mechanical Engineering,

2. Department of Biology and Division of Bioengineering and Environmental Health, Massachusetts Institute of Technology,

3. Whitehead Institute for Biomedical Research, Cambridge, MA 02142, USA.

Abstract

Not all biological movements are caused by molecular motors sliding along filaments or tubules. Just as springs and ratchets can store or release energy and rectify motion in physical systems, their analogs can perform similar functions in biological systems. The energy of biological springs is derived from hydrolysis of a nucleotide or the binding of a ligand, whereas biological ratchets are powered by Brownian movements of polymerizing filaments. However, the viscous and fluctuating cellular environment and the mechanochemistry of soft biological systems constrain the modes of motion generated and the mechanisms for energy storage, control, and release.

Publisher

American Association for the Advancement of Science (AAAS)

Subject

Multidisciplinary

Reference62 articles.

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2. An engine is a device that converts one form of energy to another. A muscle is a mechanochemical engine; rhodopsin is a photochemical engine.

3. Because springs convert some form of energy to mechanical motion a natural basis for their understanding arises from the thermodynamics of these systems. By combining the first and second laws of thermodynamics we can relate the internal energy dU of a system to the work dW done by it and to the change in entropy dS by dU = TdS − dW. The work done dW can arise from many causes; if a system expands by a volume dV against a pressure p it does mechanical work equal to pdV. If a contractile fiber shortens by an amount − dl under a force f it performs mechanical work equal to − fdl. If the system transports − dn i moles of the i th component from itself to its surroundings at a chemical potential μ i it performs chemical work equal to − μ i dn i etc. so that dU=TdS−pdV+fdl+∑i μidni+ψde+….To determine the force generated by mechanochemical springs such as the spasmoneme and the Limulus acrosome one would need to consider only the subset of relevant terms that contribute to that particular system. For example energetic and entropic effects associated with contracting filaments lead to f=∂U∂l e T ni−T ∂S∂l e T niwhere e T and n are constant. In principle we can calculate U μ and S from a microscopic description or write a phenomenological form based on the symmetries of the system. Using this force in the equation of motion for the contraction of the fiber complemented by structural information leads to a physicochemical description of the dynamics.

4. Amos W. B., Nature 229, 127 (1971).

5. Moriyama Y., Hiyama S., Asai H., Biophys. J. 75, 487 (1998).

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