Slide 1Slide 2Slide 3Slide 4Slide 5Slide 6Slide 7Slide 8Reminder on Ion Distribution and Transport in CellsSlide 10Slide 11Slide 12How We Know: StructureHow We Know: Current-Pressure RelationshipSlide 15Slide 16Slide 17Slide 18Slide 19Slide 20Slide 21Slide 22Slide 23Slide 24Slide 25Slide 26Slide 27Slide 28BE/APh161 – Physical Biology of the CellBE/APh161 – Physical Biology of the CellRob PhillipsApplied Physics and BioengineeringCalifornia Institute of TechnologyLife at the cell surfaceLife at the cell surface• We now undertake a real case study, that of cellular signaling. This will take us a few weeks.• The stars of the show will be membrane proteins.High resolution imaging of chemotaxis proteinsHigh resolution imaging of chemotaxis proteins• PALM is a high-resolution technique that permits beating the diffraction limit.•In this case, they are looking at chemotaxis proteins in E. coli.(Greenfield, Liphardt et al, PLoS Biology, 2009.)How do cells talk to each other?How do cells talk to each other?The signaling conceptThe signaling concept• Our goal will be to find out what kinds of measurements people can do about such systems and then how we can turn the cartoon into a mathematical description.Paramecium and the avoidance responseParamecium and the avoidance response•We begin our story of signaling with the BEHAVIOR of Paramecium as manifested in its avoidance response.• H. S. Jennings, “The behavior of the lower organisms”, 1906.• Most of the figures on Paramecium are from “An Introduction to Nervous Systems” by Ralph Greenspan.Paramecium and the tree of lifeParamecium and the tree of life• This diagram reiterates my earlier statements about the amazing diversity of life. • Note that in this case our tree only reflects on the relatedness of eukaryotes.• Question: how does one construct such a tree?(Ralph Greenspan, An Introduction to Nervous Systems)The avoidance responseThe avoidance response• These single-celled eukaryotes manage a sophisticated response to their environment.• One of the things I am most excited to tell you is that this response is mediated by similar tricks to those we are used to in the context of nervous systems.• We need to take a little detour and talk about ion channels. The first of the membrane proteins that we will study in some detail.(Ralph Greenspan, An Introduction to Nervous Systems)Reminder on Ion Distribution and Transport in CellsCells (eukaryotes) divided into a number of membrane-bound compartments.Concentrations in different compartments can be orders of magnitude different.Proteins (ion channels, transporters) mediate these concentration gradients.Membrane proteins central to huge range of processes – cell signaling, nerve impulses, nutrient transport, etc.Membrane permeabilityMembrane permeability• Membrane susceptibility to mass transport characterized by a “material parameter” known as the permeability. • Notice that the permeability ranges over 16 orders of magnitude.Ion channels under external driving forceIon channels under external driving force• The probability for ion channels of being in open or closed states can be tuned by various external agents: Change of the V across the membraneA mechanical stressBinding of a ligandIon channelsIon channels• Ion channels - transmembrane proteins that mediate the transport of ions in and out of cellsStructure of a bacterial K+ channel. The channel is made from 4 identical transmembrane subunits (only 2 are shown) which together form a central pore through the membraneHow We Know: StructureKnowledge of the structures of different membrane proteins gives us a substrate to reason on about how they work.K ChannelNicotinic acetylcholinereceptor(Unwin et al.)(Rees et al.)EM & X Ray structuresSynchrotronMscL and MscSHow We Know: Current-Pressure RelationshippA currents lasting several milliseconds.The idea: grab a patch of membrane and apply a potential difference to measure the currents.Fraction of time spent open depends upon magnitude of driving force.(Sukharev et al.)The avoidance response revisitedThe avoidance response revisited• This schematic traces the series of processes that occur when a Paramecium is subjected to a mechanical stimulus.(Ralph Greenspan, An Introduction to Nervous Systems)Ion channels and the implementation of decisions Ion channels and the implementation of decisions • The particular scheme exploited by Paramecium has several facets involving both mechanosensitive and voltage-gated ion channels.(Ralph Greenspan, An Introduction to Nervous Systems)Which Ion species Mediates the Process?Which Ion species Mediates the Process?• The clever experiment involves tuning the extracellular concentrations of the different ion species in turn and then examining the resulting membrane potential.(Ralph Greenspan, An Introduction to Nervous Systems)The action potentialThe action potential• Action potentials are a stereotyped response once a critical threshold has been crossed. • The shape and duration of the action potential are key variables.• NOTE: Helmholtz measured the velocity of propagation of nerve impulses.The avoidance response: detailsThe avoidance response: details• These single-celled eukaryotes manage a sophisticated response to their environment.• One of the things I am most excited to tell you is that this response is mediated by similar tricks to those we are used to in the context of nervous systems.(Ralph Greenspan, An Introduction to Nervous Systems)Ion transport rates in ion channelsIon transport rates in ion channels• Another way in which cells manipulate transport rates: selectively and transiently altering the permeability of cell membranes through protein channels and pumpsA typical ion channel, which fluctuates btw closed and open conformation Estimate the flux of ions trough the channel, assuming purely diffusive motion • Ion channel = • Dsmall ions ≈ 2000 m2/s (e.g., Na+) 5 nm (width of lipid bilayer)0.5 nm (size of hydrated ion)• Fick’s law (details - later): where c = difference in ion c across the cell membrane, l = distance btw the two “reservoirs”• mammal.cell: c ≈ 100 mM (≈ 610–2 molecules/nm3); l ≈5 nm • Achannel = d2/4 ≈ 0.2 nm2 => N of ions traversing the membrane per second:€ Jion≈ DΔcl€ Jion≈ 2 ×109nm2s×6 ×10−2molecules / nm35nm€ ≈2 ×107nm−2s−1€ dNiondt≈ JionAchannel€ ≈2
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