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DOI: 10.1201/9781003336433-2
2
Orientation for the
Bio-Curious
The Basics of Biology for the Physical
Scientist
If you want to understand function, study structure. [I was supposed to have said in my
molecular biology days.]
—Francis Crick, What Mad Pursuit: A Personal View
of Scientific Discovery (1988, p. 150)
General Idea: This chapter outlines the essential details of the life sciences that physical
scientists need to get to grips with, including the architecture of organisms, tissues, cells, and
biomolecules as well as the core concepts of processes such as the central dogma of molecular
biology, and discusses the key differences in the scientific terminology of physical parameters.
2.1 INTRODUCTION: THE MATERIAL STUFF OF LIFE
The material properties of living things for many physical scientists can be summarized as
those of soft condensed matter. This phrase describes a range of physical states that in essence
are relatively easily transformed or deformed by thermal energy fluctuations at or around
room temperature. This means that the free energy scale of transitions between different
physical states of the soft condensed matter is similar to those of the thermal reservoir of the
system, namely, that of ∼kBT, where kB is the Boltzmann constant of 1.38 × 10−23 m2 kg s−2 K−1
at absolute temperature T. In the case of this living soft condensed matter, the thermal res
ervoir can be treated as the surrounding water solvent environment. However, a key feature
of living soft matter is that it is not in thermal equilibrium with this water solvent reservoir.
Biological matter, rather, is composed of structures that require an external energy input to
be sustained. Without knowing anything about the fine details of the structures or the types
of energy inputs, this means that the system can be treated as an example of nonequilibrium
statistical thermodynamics. The only example of biological soft condensed matter, which is
in a state of thermal equilibrium, is something that is dead.
KEY POINT 2.1
Thermal equilibrium = death
Much insight can be gained by modeling biological material as a subset of nonequilibrium
soft condensed matter, but the key weakness of this approach lies in the coarse graining and
statistical nature of such approximations. For example, to apply the techniques of statistical