Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Review • • • • Membrane structure and composition Cell to cell adhesions Membrane transport Pgs 52-73 New • Membrane potentials • Pgs 73-83 Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Plasma Membrane • Forms outer boundary of every cell • Controls movement of molecules between the cell and its environment • Joins cells to form tissues and organs • Plays important role in the ability of a cell to respond to changes in the cell’s environment Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Plasma Membrane Structure • Fluid lipid bilayer embedded with proteins – Most abundant lipids are phospholipids • Also has small amount of carbohydrates – On outer surface only • Cholesterol – Tucked between phospholipid molecules – Contributes to fluidity and stability of cell membrane • Proteins – Attached to or inserted within lipid bilayer Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Plasma Membrane Structure • Channels • Carrier molecules • Docking marker acceptors • Membrane bound enzymes • Receptor sites • Cell adhesion molecules (CAMs) – Integrin, cadherin • Cell surface markers Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Cell-To-Cell Adhesions – Extracellular matrix • Serves as biological “glue” • Major types of protein fibers interwoven in matrix – Collagen, elastin, fibronectin – CAMs in cells’ plasma membranes – Specialized cell junctions • Desmosomes • Tight junctions (impermeable junctions) • Gap junctions (communicating junctions Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Specialized Cell Junctions Desmosomes Gap junctions • Act like “spot rivets” that anchor two • Small connecting tunnels formed by closely adjacent nontouching cells connexons • Most abundant in tissues that are • Especially abundant in cardiac and subject to considerable stretching smooth muscle • In nonmuscle tissues permit unrestricted passage of small nutrient molecules between cells • Also serve as method for direct transfer of small signaling molecules from one cell to the next Tight junctions • Firmly bond adjacent cells together • Seal off the passageway between the two cells • Found primarily in sheets of epithelial tissue • Prevent undesirable leaks within epithelial sheets • C Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Membrane Transport • Unassisted membrane transport – Diffusion – Osmosis • Assisted membrane transport – Carrier-mediated transport – Facilitated transport – Active transport Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Membrane Transport Diffusion Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Membrane Transport Factors affecting rate of diffusion collectively make up Fick’s law of diffusion: • Magnitude (or steepness) of the concentration gradient • Permeability of the membrane to the substance – Charge? • Surface area of the membrane across which diffusion is taking place • Molecular weight of the substance • Distance through which diffusion takes place Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Table 3-1, p. 62 Membrane Transport • Osmosis – Net diffusion of water down its own concentration gradient Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Fig. 3-9, p. 63 Membrane Transport • Tonicity of a solution – Determines whether cell remains same size, swells, or shrinks when a solution surrounds the cell • Isotonic solution – Has same concentration of nonpenetrating solutes as normal body cells – Cell volume remains constant • Hypotonic solution – Lower concentration of nonpenetrating solutes than normal body cells – Water enters cell causing cell to swell or perhaps rupture • Hypertonic solution – Higher concentration of nonpenetrating solutes than normal body cells – Cells shrink as they lose water by osmosis Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Membrane Transport Assisted membrane transport • Carrier-mediated transport – Accomplished by membrane carrier flipping its shape – Can be active or passive – Characteristics that determine the kind and amount of material that can be transferred across the membrane • Specificity • Saturation • Competition Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Membrane Transport Types of assisted membrane transport • Facilitated diffusion • Active transport • Vesicular transport Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Membrane Transport Facilitated diffusion • Substances move from a higher concentration to a lower concentration • Requires carrier molecule • Means by which glucose is transported into cells Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Membrane Transport Active transport • Moves a substance against its concentration gradient • Requires a carrier molecule • Primary active transport – Requires direct use of ATP • Secondary active transport – Driven by an ion concentration gradient established by a primary active transport system Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Active Transport Concentration gradient Na+ Phosphorylated conformation Y of carrier Step 1 Molecule to be transported Phosphorylated conformation Y of carrier has high affinity for passenger. Molecule to be transported binds to carrier on low-concentration side. Dephosphorylated conformation X of carrier ECF (High) ICF (Low) Direction of transport Step 2 Dephosphorylated conformation X = phosphate of carrier has low affinity for passenger. Transported molecule detaches from carrier on high-concentration side. Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Fig. 3-16, p. 70 Sodium Potassium Pump When open to the ECF, the carrier drops off Na+ on its high-concentration side and picks up K+ from its low-concentration side ECF ICF When open to the ICF, the carrier picks up Na+ from its low-concentration side and drops off K+ on its high-concentration side Phosphorylated conformation Y of Na+–K+ pump has high affinity for Na+ and low affinity for K+ when exposed to ICF = Sodium (Na+) Dephosphorylated conformation X of Na+–K+ pump has high affinity for K+ and low affinity for Na+ when exposed to ECF Chapter 3 The Plasma Membrane and Membrane Potential + Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning = Potassium (K ) = Phosphate Fig. 3-17, p. 70 Secondary Active transport Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Fig. 3-18, p. 72 Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Table 3-2c, p. 74 Membrane Transport • Vesicular transport – Material is moved into or out of the cell wrapped in membrane – Active method of membrane transport – Two types of vesicular transport • Endocytosis – Process by which substances move into cell – Pinocytosis – nonselective uptake of ECF – Phagocytosis – selective uptake of multimolecular particle • Exocytosis – Provides mechanism for secreting large polar molecules – Enables cell to add specific components to membrane Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning • • • • • Carrier-mediated transport: (a) involves a specific membrane protein that serves as a carrier molecule. (b) always moves substances against a concentration gradient. (c) always requires energy expenditure. (d) two of these answers. (e) all of these answers. • • • • • Facilitated diffusion: (a) involves a carrier molecule. (b) requires energy expenditure. (c) is how glucose enters the cells. (d) both (a) and (c) above. (e) all of these answers. • • • • • Select the correct statement about diffusion. (a) It depends on the random motion (b) It involves active forces. (c) Its rate increases as the temperature decreases. (d) Molecules move from a lower concentration to a higher concentration. (e) The chemical gradient of a substance does not affect it. Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Membrane Potential • Plasma membrane of all living cells has a membrane potential (polarized electrically) • Separation of opposite charges across plasma membrane • Due to differences in concentration and permeability of key ions • Separated charges create the ability to do work ( hydroelectric dam) millivolt- 1/1000 volt Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Membrane Potential Which has the greatest membrane potential? Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Membrane Potential • Nerve and muscle cells – Excitable cells – Have ability to produce rapid, transient changes in their membrane potential when excited • Resting membrane potential – Constant membrane potential present in cells of nonexcitable tissues and those of excitable tissues when they are at rest – Na+, K+, AChapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Membrane Potential • Effect of sodium-potassium pump on membrane potential – Makes only a small direct contribution to membrane potential through its unequal transport of positive ions Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning Table 3-3, p. 75 Resting potential (Er) Rp + -75mv Variable from one cell to another Poison eliminates this potential Generated by the imbalance of ions in the intracellular and extracellular spaces. Ion Out mM In mM Pot mV K 5.5 150 -90 Na 150 15 60 Perm. 50-75 1 Cl 125 9 Chapter 3 The Plasma Membrane and Membrane Potential Human Physiology by Lauralee Sherwood ©2007 Brooks/Cole-Thomson Learning -70 Ion Concentration Resting Potential Fig. 3-22, p. 78 Plasma membrane ICF ECF Electrical gradient for K+ Concentration gradient for K+ EK+ = –90 mV Fig. 3-20, p. 76 Plasma membrane ICF ECF Concentration gradient for Na+ Electrical gradient for Na+ ENa+ = +60 mV Fig. 3-21, p. 78 Plasma membrane ECF ICF Relatively large net diffusion of K+ outward establishes an EK+ of –90 mV No diffusion of A– across membrane Relatively small net diffusion of Na+ inward neutralizes some of the potential created by K+ alone Resting membrane potential = –70 mV (A– = Large intracellular anionic proteins) Fig. 3-22, p. 78 Fig. 3-23, p. 79 ECF Na+–K+ pump (Passive) Na+ channel K+ channel (Passive) (Active) (Active) ICF Fig. 3-23, p. 79 Points to Ponder 3, p. 83 Nernst equation • • • • • • E=(61) log Co/Ci For Potassium Ek=(61) log 5mM/150mM For sodium ENa=(61) log 150mM/15mM Co concentration in the ECF Ci concentration in the ICF Used to calculate the contribution of ions to the resting potential of -70mv Resting potential • • • • EK = -90mv ENa = 60mv ECl = -70mv K and Na drive Cl gradient Usefulness? • Neurons and muscle fibers can alter membrane potential to send signals and create motion.