Public
Lecture: Electricity
in Biology
4 pm, McNamara Alumni Center Atrium
Living
organisms are electrical. Our brains instruct our muscles
to move by transmitting information,
which is encoded in the form of electrical impulses that
travel along nerve fibers. Our ability to experience our
world through vision, smell, taste, hearing and touch depends
upon the transmission of electrical signals. Even our ability
to think is based upon the complex electrical interactions
of neurons in our central nervous system. How does ‘animal
electricity’ work? How does it relate to inanimate
electrical devices such as electric toasters, televisions
and computers? The history of ‘animal electricity’ and
how scientists figured it out is very interesting. It is
interesting not only because it leads us to an understanding
of the subject, but also because it exemplifies the strange
and unexpected manner in which scientific ideas evolve. In
this lecture I will describe from a historical perspective
how studies of ‘animal electricity’ actually
advanced the understanding of electricity in physics. I will
also explain our modern understanding of life’s electrical
system by describing ion channels as the conductors of electricity
in living cells.
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Colloquium: The
Principles of Ion Selectivity in Potassium Channels
9:45 am, Smith 331
Ion channels,
like enzymes, have their specific substrates: potassium, sodium,
calcium, and chloride channels permit only their namesake ions to
diffuse through their pores. Potassium channels exhibit a remarkable
ability to discriminate between potassium and sodium—by a factor
of nearly 10,000—even though these ions are similar in size
(1.33 and 0.95 Å, respectively). Such exquisite selectivity
is impressive when one considers that potassium flows though the
pore at a rate approaching the diffusion limit. My laboratory has
determined the atomic structures of several potassium channels. The
architecture of the pore allows potassium ions to remain hydrated
at the center of the membrane, where the dielectric barrier to ion
flow is expected to be greatest. The selectivity filter coordinates
dehydrated potassium ions, but not sodium ions, thus accounting for
ion selectivity. Structural and thermodynamic data on the binding
of various ions to the selectivity filter will be discussed. A detailed
conduction mechanism in which two potassium ions adopt two configurations
within four binding sites is hypothesized to account for near diffusion-limited
conduction rates.
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