6021 fall 2004

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MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science, Department of Mechanical Engineering, Division of Bioengineering and Environmental Health, Harvard-MIT Division of Health Sciences and Technology Quantitative Physiology: Cells and Tissues 2.791J/2.794J/6.021J/6.521J/BE.370J/BE.470J/HST.541J Homework Assignment #1 Issued: September 8, 2004 Due: September 16, 2004 Reading Lecture 2 — V olume 1: 3.1-3.1.3 3.2-3.2.2 Lecture 3 — V olume 1: 3.1.4 -3.1.5 3.5-3.5.2.1 Lecture 4 — V olume 1: 3.6-3.6.1.2 3.7-3.7.2 Announcements Homework will consist of  Exercis es and Problems. Exercises are generally more conceptual and require less number crunching. Exercises often require writing sentences to explain what you hav e learned. Written solutions should be submitted for both Exercises and Problems. Exercise 1. According to the random walk model, solute molecules move and thereby diffuse be cause of collisions with water molecules. Solute collisions with other solute molecules are gener ally ignored under the assumption that the water molecules vastly outnumber the solute molecules. To get a feeling for the validity of this assumption, and to appreciate the number of particles and spatial scales involved, consider the diffusion of potassium ions in the cytoplasm of a red blood cell. Assume that the volume of the cell is 90 fL, and that the concentration of po tassium ions in the cytoplasm is 150 mmol/L. Part a. Estimate the number of potassium ions in the cytoplasm of the cell. Part b. Estimate the average distance between potassium ions in the cell. Part c. Estimate the number of water molecules in the cytoplasm of the cell. Part d. Estimate the average distance between water molecules in cytoplasm. Part e. Determine the ratio of water molecules to potassium ions in cytoplasm. Exercise 2. At a junction between two neurons, called a synapse, there is a 20 nm cleft that separates the cell membranes. A chemical transmitter substance is released by one cell (the pre synaptic cell), diffuses across the cleft, and arrives at the membrane of the other (post-synaptic) cell. Assume that the diffusion coefcient of the chemical transmitter substance is D = 5 × 10 6 cm 2  /s. Make a rough estimate of the delay caused by diffusion of the transmitter substance across the cleft. What are the limitations of this estimat e? Explain. 1

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    MASSACHUSETTS INSTITUTE OF TECHNOLOGY

    Department of Electrical Engineering and Computer Science,

    Department of Mechanical Engineering,

    Division of Bioengineering and Environmental Health,

    Harvard-MIT Division of Health Sciences and Technology

    Quantitative Physiology: Cells and Tissues

    2.791J/2.794J/6.021J/6.521J/BE.370J/BE.470J/HST.541J

    Homework Assignment #1 Issued: September 8, 2004

    Due: September 16, 2004

    Reading

    Lecture 2 Volume 1: 3.1-3.1.3 3.2-3.2.2

    Lecture 3 Volume 1: 3.1.4-3.1.5 3.5-3.5.2.1

    Lecture 4 Volume 1: 3.6-3.6.1.2 3.7-3.7.2

    AnnouncementsHomework will consist ofExercises and Problems. Exercises are generally more conceptual and

    require less number crunching. Exercises often require writing sentences to explain what you have

    learned. Written solutions should be submitted for both Exercises and Problems.

    Exercise 1. According to the random walk model, solute molecules move and thereby diffuse be

    cause of collisions with water molecules. Solute collisions with other solute molecules are gener

    ally ignored under the assumption that the water molecules vastly outnumber the solute molecules.

    To get a feeling for the validity of this assumption, and to appreciate the number of particles and

    spatial scales involved, consider the diffusion of potassium ions in the cytoplasm of a red blood

    cell. Assume that the volume of the cell is 90 fL, and that the concentration of potassium ions in

    the cytoplasm is 150 mmol/L.

    Part a. Estimate the number of potassium ions in the cytoplasm of the cell.

    Part b. Estimate the average distance between potassium ions in the cell.

    Part c. Estimate the number of water molecules in the cytoplasm of the cell.

    Part d. Estimate the average distance between water molecules in cytoplasm.

    Part e. Determine the ratio of water molecules to potassium ions in cytoplasm.

    Exercise 2. At a junction between two neurons, called a synapse, there is a 20 nm cleft that

    separates the cell membranes. A chemical transmitter substance is released by one cell (the presynaptic cell), diffuses across the cleft, and arrives at the membrane of the other (post-synaptic)

    cell. Assume that the diffusion coefficient of the chemical transmitter substance is D = 5106cm2/s. Make a rough estimate of the delay caused by diffusion of the transmitter substanceacross the cleft. What are the limitations of this estimate? Explain.

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    Exercise 3. The time course of one-dimensional diffusion of a solute from a point source in space

    and time has the form

    cn(x, t) = no

    4Dtex

    2/4Dt,

    where no is the number of moles of solute per unit area placed at x = 0 at t = 0. cn(x, t) iscomputed as a function of time for locationsxaand xb, and shown in the following figure.

    t

    xa

    xb

    cn

    (x,t)

    Isxa> xb or isxa < xb? Explain.

    Problem 1. A general solution to a first-order linear differential equation with constant coefficients

    can be written as

    n(t) =n+ (n0

    n)et/.

    a) Determine the slopem0=dn/dtatt= 0in terms of the constantsn,n0and .

    b) If this slope were extended for t > 0 (i.e., ifn(t) = n0+ m0t), for what value oft willn(t) =n?

    c) Plotn(t)and n(t)whenn0= 10,n= 10, and= 1.

    Problem 2. Four solutions to the differential equation

    dx(t)

    dt +Ax(t) +B = 0

    are shown in the following plot.

    0 5 10

    0

    3

    3

    Part a. Find values ofA and B that are consistent with curvea. Are these values unique? If not,find a second set of constants that are consistent.

    Part b. Repeat part a for curveb. Compare these results to those of part a. Explain similarities anddifferences.

    Part c. Repeat part a for curve c. Compare these results to those of parts a and b. Explainsimilarities and differences.

    Part d. Repeat part a for curved. Determine all possible values ofAandB for this case.

    2

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    Problem 3. Assume that nomol/cm2 of sucrose (with a diffusion constant D0.5105cm2/s)

    are placed in a trough of water at a point x= 0 at time t= 0. Assume that the concentration ofsucrose is a function of xand tonly.

    2a) Show that for any fixed point xp the maximum concentration occurs at time tm =xp/2D.

    b) How long does it take for the concentration to reach a maximum at x= 1 cm?

    Problem 4. The following figure illustrates a cascaded system of two water tanks. Water flows out

    of the first tank and into the second at a rate r1(t), and out of the second tank at a rate r2(t).

    h1 r1

    h2r2

    (t) (t)

    (t)(t)

    The rates of flow out of the tanks are proportional to the heights of the water in the tanks: r1(t) =k1h1(t) and r2(t) = k2h2(t), where k1 and k2are each 0.02 m

    2/minute. The height of tank 1 is 1 m

    and that of tank 2 is 2 m. The cross-sectional area of tank 1 is A1 = 4 m2 and that of the second

    tank is A2 = 2 m2. At time t= 0, tank 1 is full and tank 2 is empty.

    a. If the height of water in tank 2 ever exceeds the height of the tank (2 m), the water will

    overflow. Will the water ever overflow? Explain.

    b. Set up a system of differential equations to determine h2(t). Solve the equations to determinean expression for h2(t).

    c. At what time does the water in tank 2 reach its peak? What will be the maximum height of

    water ever achieved in tank 2?

    d. At what time will the water stop flowing out of tank 1? Explain your answer in mathematical

    terms and then in physical terms.

    e. If both tanks were full at t= 0, would the second tank ever overflow? Explain.

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    Problem 5. Transport by diffusion tends to move solutes from regions of high concentration to

    regions of low concentration, thereby making the spatial distribution of solute more uniform. Thus

    diffusion is often associated with mixing. However, diffusion can also be used to separate solutes in

    a mixture. Such separation is important as a mechanism to purify mixtures of biological materials

    (such as mixtures of DNA fragments) and is currently being exploited in microfabricated systems

    for biological and medical analysis (which we will look at in greater detail in the Microfluidics

    Laboratory Project).Assume that a mixture of two molecular species is loaded into a long and narrow channel filled

    with water. Let x represent distance in the the longitudinal direction and assume that n0 moleculesof solute A and n0 molecules of solute B are loaded into location x=0at time t=0. Assume thatsolutes A and B have different molecular weights and that their diffusivities are DA =10

    7 cm2/s

    and DB =4107 cm2/s, respectively. The following figure illustrates how the two species tend

    to separate as they diffuse.

    0

    x (

    i

    10 10

    m)Co

    ncentratons

    ofA

    andB

    Part a. As time elapses, the number of molecules of solute A that remain in a test region within

    the 10m of the starting position (i.e., 10m< x

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    MASSACHUSETTS INSTITUTE OF TECHNOLOGY

    Department of Electrical Engineering and Computer Science,

    Department of Mechanical Engineering,

    Division of Bioengineering and Environmental Health,

    Harvard-MIT Division of Health Sciences and Technology

    Quantitative Physiology: Cells and Tissues

    2.791J/2.794J/6.021J/6.521J/BE.370J/BE.470J/HST.541J

    Homework Assignment #2 Issued: September 16, 2004

    Due: September 23, 2004

    Reading

    Lecture 5 Volume 1: 3.8-3.8.5

    Lecture 6 Volume 1: 4.1-4.3.2.3 4.4-4.5.1.2

    Lecture 7 Volume 1: 4.7-4.7.1.2

    Lecture 8 Volume 1: 4.7.2-p.230 Fig.4.26 Fig.4.28 4.8.2-4.8.3

    Exercise 1. Describe the dissolve-diffuse theory for diffusion through cellular membranes.

    Exercise 2. Two time constants are involved in two-compartment diffusion through a membrane:

    the steady-state time constant of the membrane (ss) and the equilibrium time constant for the two

    compartments (eq). Without the use of equations, describe these two time constants.

    Exercise 3. A solute n

    diffuses through a membrane that separates two compartments that have

    different initial concentrations. The concentrations in the two compartments as a function of time,a bcn(t)and cn(t), are shown in the following figure.

    t

    c

    a

    n(t)

    c

    b

    n(t)

    The volumes of the two compartments are Va and Vb. Is Va >Vb or is Va

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    concentration of 0.1 mol/L. Based on these measurements, de Vries determined the correct formula

    for raffinose. Which formula would you choose and why would you choose it?

    Problem 1. Consider diffusion through a thin membrane that separates two otherwise closed com

    partments. As illustrated in Figure 1, the membrane and both compartments have cross sectional

    areas A = 1cm2. Compartment 1 has length L1 = 50cm, compartment 2 has length L2 = 10

    c( )c1(t) c2(t)

    2

    W 4 cm

    L1

    x,t

    Area=1cm

    =10

    =50cm L2 =10cm

    Figure 1: Two compartments separated by a membrane.

    cm, and the membrane thickness is W = 104 cm. Assume that (1) the compartments containsugar solutions and that both compartments are well stirred so that the concentration of sugar in

    compartment 1 can be written as c1(t)and that in compartment 2 can be written as c2(t); (2) the

    concentration of sugar in the membrane can be written as c(x,

    t), where x

    represents distancethrough the membrane; (3) the diffusivity of sugar in the membrane is Dsugar =10

    5 cm2/s and

    the membrane:water partition coefficient km:w is 1; (4) the concentration of sugar in the membrane

    has reached steady state at time t=0and that c1(0)=1mol/L and c2(0)=0mol/L.

    a) Compute the flux of sugar through the membrane at time t=0, s(0).

    b) Compute the final value of concentration of sugar in compartment 1, c1().

    c) Let eq characterize the amount of time required to reach equilibrium. What would happen

    to eq if the diffusivity of sugar in the membrane were doubled? Explain your reasoning.

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    Problem 2. A thin membrane and a thick membrane, that are otherwise identical, are used to

    separate identical solutions of volume V

    = 1 cm3 (Figure 2). All the membrane surfaces facingthe solutions have area A

    = 1 cm2. The thin membrane has thickness ds = 104cm; the thick

    membrane has thickness dl = 1 cm. For t

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    Problem 3. Glucose is dripped at a constant rate R = 2mol/s into a bath that contains 1012

    identical red blood cells, as shown in the following figure.

    Assume that each red blood cell has a volume = 25 (VC m)3 and a surface area AC =80 (m)2

    ,

    and that neither of these changes over the time interval considered in this problem. Assume that

    the volume of the bath is 1 L, and that the bath is well stirred. (You may assume that the amount

    of water dripped into the bath is negligibly small.) The concentration of glucose in the bath, cb(t),if found to increase as a function of time t, as shown in the following plot.

    cb(t) (mmol/L)

    5

    t (s)00 300 600 900

    Part a. Is the following logic True or False?

    The flux of glucose through each of the cell membranes cannot be constant over the

    time 0 < t < 900s, because if it were, the concentration cb(t)would be a linearfunction of time.

    If the truthfulness of this statement cannot be determined from the information provided, describe

    what additional information is needed.

    Part b.Determine the flux of glucose through the membrane of each cell at time t =

    900

    s.Use our normal convention that outward flux (i.e., flux leaving the cell) is positive and inward

    flux is negative. Determine the numerical value (or numerical expression) and units. If you

    cannot determine the numerical value from the information provided, describe what additional

    information is needed.

    Part c. Determine the flux of glucose through the membrane of each cell at time t = 0s. Useour normal convention that outward flux (i.e., flux leaving the cell) is positive and inward flux

    is negative. Determine the numerical value (or numerical expression) and units. If you cannot

    determine the numerical value from the information provided, describe what additional information

    is needed.

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    Problem 4. All cells are surrounded by a cell membrane. The cytoplasm of most cells contains a

    variety of organelles that are also enclosed within membranes. Assume that a spherical cell with

    radius R=50m contains a spherical organelle called a vesicle, with radius r= 1m, as shown

    in the following figure.

    i l icl

    i m

    i l ll

    i m

    spher ca ves e

    rad us r = 1

    spher ca ce

    rad us R = 50

    bath

    Assume that the membranes surrounding the cell and vesicle are uniform lipid bilayers with iden

    tical compositions and the same thickness d=10nm. Assume that solute Xis transported across

    both the cell and vesicle membrane via the dissolve and diffuse mechanism. Assume that X

    dissolves equally well in the bath and in the aqueous interiors of the vesicle and cell. Assume that

    the solute Xdissolves 100 times less readily in the membrane (i.e., the partitioning coefficient is

    0.01). Assume the diffusivity of Xin the membranes is 107cm2/s.Initially, the concentration of Xis zero inside the cell and inside the vesicle. At time t=0, the

    cell is plunged into a bath that contains Xwith concentration 1 mmol/L.

    a) Estimate the time that is required for the concentration of X

    in the cell to reach 0.5 mmol/L.

    Find a numerical value or explain why it is not possible to obtain a numerical value with the

    information that is given.

    b) Estimate the time that is required for the concentration of X

    in the vesicle to reach0.5 mmol/L. Find a numerical value or explain why it is not possible to obtain a numeri

    cal value with the information that is given.

    5

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    Problem 5. As your first assignment at Tinyfluidics Inc., you are asked to design a microfluidic

    device that will remove small molecules from a sample of fluid that contains both large molecules

    and small molecules. After some thinking, you design the laminar flow device shown below.

    L

    W

    in

    in

    le in fild

    buffer

    buffer

    samp

    waste out

    waste out

    trate out

    The sample is injected in a port with width . The sample flow is surrounded by buffers injected

    on both sides of the sample. The combined flow then passes through a channel that has width W

    and length L after which the fluids are separated into a desired filtrate output (in a channel of width

    d) and two waste outputs. Assume that the fluid moves with the same speed v in all parts of the

    microfluidic device (although this is not generally true, it is a convenient starting point). Assume

    that L0.

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    MASSACHUSETTS INSTITUTE OF TECHNOLOGY

    Department of Electrical Engineering and Computer Science,

    Department of Mechanical Engineering,

    Division of Bioengineering and Environmental Health,

    Harvard-MIT Division of Health Sciences and Technology

    Quantitative Physiology: Cells and Tissues

    2.791J/2.794J/6.021J/6.521J/BE.370J/BE.470J/HST.541J

    Homework Assignment #3 Issued: September 23, 2004

    Due: September 30, 2004

    Reading

    Lecture 8 Volume 1: 6.1-6.2.1.4

    Lecture 9 Volume 1: 6.4-6.4.1.4

    Lecture 10 Volume 1: 6.4.2-6.4.3 6.6-6.7.4

    Lecture 11 Volume 1: 7.2.1 7.2.3 7.2.4.1 7.4

    Announcements

    Exam 1 will be held on Thursday, October 7, 2004 from 7:30 PM to 9:30 PM

    The exam is closed-book: notes on both sides of one 8111sheet of paper2

    may be used for reference. Calculators may be used, but computers and wireless

    devices may not be used.

    There will be no recitations on the day of the exam.

    Exercise 1. It is known that the membrane of a certain type of cell is highly permeable to water,

    but relatively impermeable to L-glucose, sodium ions, and chloride ions. When the cell is removed

    from interstitial fluids and placed in a 150 mmol/L NaCl solution, the cell neither shrinks nor

    swells.

    a) Would the cell shrink, swell, or remain at constant volume if placed in 150 mmol/L solution

    of L-glucose? Explain.

    b) Would the cell shrink, swell, or remain at constant volume if placed in a 300 mmol/L solution

    of L-glucose? Explain.

    Exercise 2. If Equation 4.68 in volume 1 of the text is multiplied by A(t), the result can be writtenas

    dVi(t) =A(t)LVRT (t)C

    iCo (t) .dt

    Using no mathematical formulas or equations, describe the meaning of of this equation in a few

    well chosen English sentences.

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    Exercise 3. The following figure shows schematic diagrams of two cells that have the same volume

    but quite different shapes.

    One cell (left panel) is spherical, the other is approximately cylindrical but contains a large number

    of microvilli. The cell membranes have the same hydraulic conductivity to water. If the two cells

    are subjected to the same decrease in extracellular osmolarity, which cell swells more rapidly?

    Explain.

    Exercise 4. Consider the simple, symmetric, four-state carrier model. For each of the following

    E, NESi , Noconditions, find NE

    i , No ES, and S. Explain the physical significance of each of youranswers.

    a) = 0.

    b) = 0.

    c) K

    = 0.

    i oExercise 5. Consider the simple, symmetric, four-state carrier model when c = cS

    = 0. SketchS

    the carrier density in each of its four states as a function of /. Give a physical interpretation ofyour results.

    2

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    Problem 1. A volume element with constant cross-sectional area Ahas rigid walls and is dividedinto two parts by a rigid, semipermeable membrane that is mounted on frictionless bearings so that

    the membrane is free to move in the x-direction as shown in the following figure.

    c1 c2

    0 x 10(cm)

    The semipermeable membrane is permeable to water but not to the solutes (glucose or NaCl or

    CaCl2). At t = 0, solute 1 is added to side 1 to give an initial concentration of c1(0)and solute2 is added to side 2 to give an initial concentration of c2(0). Concentrations are specified as thenumber of millimoles of glucose or NaCl or CaCl2 per liter of solution. The initial position of

    the membrane is x(0). For each of the following parts, find the final (equilibrium) values of themembrane position x(), and the concentrations, c1()and c2().

    1 2(a.) cglucose(0)=0; cglucose(0)=10; x(0)=5.

    1 2c(b.) glucose(0)=30; cglucose(0)=70; x(0)=7.

    1 2(c.) cglucose(0)=20; cglucose(0)=10; x(0)=3.

    1 2(d.) cglucose(0)=30; cNaCl(0)=20; x(0)=4.

    2(e.) 1 (0)=20; cN

    aCl

    (0)=30; x(0)=3.cCaCl2

    Problem 2. A spherical cell has a freely distensible membrane that is permeable to solute A, im

    permeant to solute B, and permeable to water. The cell contains NI

    moles of impermeant solutes,

    and is allowed to equilibrate in a bath in which the concentration of A is zero and the concentration

    of B is c1. The bath is large compared to the cell. The cell volume in this bath is V0. At t=0, the1cell is moved to a bath that contains equal concentrations of A and B, cA =cB = 2c1.

    a. Is the new bath hyper-, hypo-, or iso-osmotic with the cell at t

    =

    0?

    b. If the hydraulic conductivity of the cell is LV

    , what is the rate of increase of the volume,

    dV(t)/dtjust after the cell is moved (i.e., at t=0+)?

    c. What is the equilibrium volume of the cell in terms of V0? Explain briefly.

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    Problem 3. The following figure shows the design of a miniature pump that can be implanted in

    the body to deliver a drug. No batteries are required to run this pump!

    Rigid, Frictionless,semipermeable impermeable

    Chamber 1 Chamber 2

    Drug

    0.7 cm(solute) (drug)

    orifice

    membrane piston

    3 cm

    The pump contains two cylindrical chambers filled with incompressible fluids: the two chambers

    together have a length of 3 cm and a diameter of 0.7 cm. Chamber 1 is filled with a solution whose

    concentration is 10 mol/L; the osmolarity of this solution greatly exceeds that of body fluids.

    Chamber 2 is filled with the drug solution. The two chambers are separated by a frictionless, mass

    less, and impermeable piston. The piston moves freely and supports no difference in hydraulicpressure between the chambers; the piston allows no transport of water, solute or drug between

    chambers. The pump walls are rigid, impermeable and cylindrical with an orifice at one end for

    delivering the drug and a rigid, semipermeable membrane at the other end. The orifice diameter is

    sufficiently large that the hydraulic pressure drop across this orifice is negligible and sufficiently

    small so that the diffusion of drug through the orifice is also negligible. The semipermeable mem

    brane is permeable to water only, and not permeable to the solute. Assume that T =300K.

    a) Provide a discussion of 50 words or fewer for each of the following:

    i) What is the physical mechanism of drug delivery implied by the pump design?

    ii) What is(are) the source(s) of energy for pumping the drug?

    iii) Assume there is an adequate supply of drug in the pump for the lifetime of the im

    planted subject and that it is necessary to provide a constant rate of drug delivery.

    Which fundamental factors limit the useful lifetime of this pump in the body?

    b) When implanted in the body, the pump delivers the drug at a rate of 1 L/h. Find the valueof the hydraulic conductivity, LV

    , of the semipermeable membrane.

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    Problem 4. A large fraction of the molecules in a cell membrane are phospholipids, which have a

    hydrophilic head and hydrophobic tails. When purified phospholipids are added to a saline solu-

    tion, the phospholipids self assemble into a variety of stable structures, one of which is spherical

    and is called a liposome.

    Liposome

    Bath

    Liposomes have saline interiors and exteriors that are separated

    by a phospholipid bilayer, much like a biological cell. Liposomes

    can be used as artificial cells to test theories about membrane trans-port.

    Assume that a liposome is created in a solution that contains

    200 mmol/L of a solute Ithat cannot permeate the phospholipid bi-

    layer. Assume that the inner solution initially contains 200 mmol/L

    of solute I and the initial radius is30m. Assume that the thicknessof the bilayer is much smaller than the diameter of the liposome.

    Assume that water can permeate the phospholipid bilayer, and that hydraulic pressure gradients

    across the bilayer can be ignored. Assume that the temperature is 300 K.

    Assume that the liposome is transfered at time t = 0 to a bath that contains 200 mmol/L of

    solute A and 100 mmol/L of solute B. The liposome initially shrinks but then swells and reachesan ultimate radius of approximately38m as shown in the following plots. The left plot shows thetime course for the first 1000 seconds. The right plot shows just the first 100 seconds of the same

    data.

    0 500 1000

    25

    30

    35

    40

    Radius(m)

    Radius(m)

    Time (seconds) Time (seconds)

    0 50 100

    28

    29

    30

    Part a. Determine the asymptotic value of concentration cI(t)of solute I in the liposome as timeincreases, i.e., determine

    limt

    cI(t).

    Provide a numerical value (or numerical expression) with units. If it is not possible to determine

    the concentration from the information provided, explain why.Part b. Indicate which, if either, of the solutes A and B can permeate through the artificial mem-

    brane? If it is not possible to determine this information, explain why.

    Part c. Determine the hydraulic conductivity LV of the artificial membrane. Provide a numer-

    ical value (or numerical expression) with units. If it is not possible to determine the hydraulic

    conductivity from the information provided, explain why.

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    Problem 5. A large fraction of the molecules in a cell membrane are phospholipids, which have

    a hydrophobic head and hydrophilic tails. When purified phospholipids are added to a saline

    solution, the phospholipids self assemble into a variety of stable structures, one of which is called

    a liposome.

    Liposome

    Bath

    Liposomes have saline interiors and exteriors that are separated by a phospholipid bilayer, much

    like a biological cell, as illustrated above. Liposomes can be used as artificial cells to test the

    ories about membrane transport. Assume that a liposome is created in a solution that contains

    100 mmol/L of a solute Athat cannot permeate the phospholipid bilayer. Assume that water canpermeate the phospholipid bilayer, and that the liposome comes to equilibrium with a volume of

    1 pL (1012 L) of internal solution containing A with concentration 100 mmol/L.The liposome is then transferred to one of the following solutions

    solution 1: 100 mmol/L of A plus 10 mmol/L of B solution 2: 90 mmol/L of A plus 10 mmol/L of B solution 3: 100 mmol/L of B

    where Bis a solute that can permeate the phospholipid bilayer. Both A and Bare nonelectrolytes,and the baths are large compared to the volume of the liposome. Assume that transport of water

    and transport of the permeant solute Bare independent of each other, i.e., water transport does noteffect transport of Band vice versa.

    (a.) Calculate the equilibrium volume of the liposome in solution 1. Discuss your result briefly.

    (b.) Calculate the equilibrium volume of the liposome in solution 2. Discuss your result briefly.

    (c.) Calculate the equilibrium volume of the liposome in solution 3. Discuss your result briefly.

    Problem 6. A monosaccharide, M, is known to be transported through a cell membrane by acarrier so that

    oci(t) c=max oK+ci(t) K+c

    o

    where c

    i

    (t)

    is the intracellular concentration of M, c is the external concentration of M,

    is theoutward flux of M (mol/cm2s) and max

    is the maximum flux with which the carrier system

    is capable of transporting M. The area of the cell, A, is 106cm2, and K is 100 mmol/L. Thefollowing experiment is performed: the cell initially contains zero moles of M, and at t = 0thecell is placed in an isotonic solution containing a concentration of Mequal to co (constant), where

    oc K. The internal concentration of M is found to bei oc(t)=c (1et/), t0

    where =100s. The volume of the cell remained roughly constant at 1010 mL throughout theexperiment. Determine max.

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    MASSACHUSETTS INSTITUTE OF TECHNOLOGY

    Department of Electrical Engineering and Computer Science,

    Department of Mechanical Engineering,

    Division of Bioengineering and Environmental Health,

    Harvard-MIT Division of Health Sciences and Technology

    Quantitative Physiology: Cells and Tissues

    2.791J/2.794J/6.021J/6.521J/BE.370J/BE.470J/HST.541J

    Homework Assignment #4 Issued: October 8, 2004

    Due: Thursday October 14, 2004

    Reading

    Lecture 15 Volume 1: 7.5

    Lecture 16 Volume 1: 7.5

    Announcements

    This homework assignment is smaller than average to give you time to work on your lab reports.

    First drafts of your lab reports are due Friday, October 15, 2004 at 10:00 AM. Bring 3 copies.

    One will be reviewed by the technical staff. One will be reviewed by the writing staff. One will

    be reviewed by a peer student group. You and your partner will be assigned to review the report of

    another student group. All reviews are due Tuesday October 19, 2004 when they will be discussed

    at the Writing Clinic, to be held at 7:30 PM.

    Exercise 1. Define electroneutrality and briefly explain its physical basis.

    Exercise 2. Define the Nernst equilibrium potential and briefly explain its physical basis.

    Problem 1. Two compartments of a fluid-filled chamber are separated by a membrane as shown in

    the following figure.

    I

    V

    1 mmol/L NaCl0.1 mmol/L KCl

    0.1 mmol/L NaCl

    1 mmol/L KCl

    Compartment 1

    Membrane

    Compartment 2

    +

    The area of the membrane is 100 cm2

    and the volume of each compartment is 1000 cm3

    . Thesolution in compartment #1 contains 1 mmol/L NaCl and 0.1 mmol/L KCL. The solution in com

    partment #2 contains 0.1 mmol/L NaCl and 1 mmol/L KCL. The temperatures of the solutions are

    24C. The membrane is known to be permeable to a single ion, but it is not known if that ion issodium, potassium, or chloride. Electrodes connect the solutions in the compartments to a battery.

    The current Iwas measured with the battery voltage V =0and was found to be I=1mA.

    a) Identify the permeant ion species. Explain your reasoning.

    b) Draw an equivalent circuit for the entire system, including the battery. Indicate values for

    those components whose values can be determined.

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    c) Determine the current I that would result if the battery voltage were set to 1 volt. Explainyour reasoning.

    Problem 2. Three compartments are separated from each other by semi-permeable membranes, as

    illustrated in the following figure.

    Vm

    Im

    +

    cNa

    = 100

    cK= 0

    cCl= 100

    cNa

    = 20

    cK= 80

    cCl= 100

    cNa

    = 10

    cK= 0

    cCl= 10

    compartment 1 compartment 2 compartment 3

    permeant to permeant toNa+only Clonly

    Each compartment contains well-stirred solutions of sodium, potassium, and chloride ions, with

    concentrations indicated in the figure (in mmol/L). The membrane between compartment 1 and 2

    is permeant to sodium ions only, and its specific electrical conductivity GNa is 5 mS/cm2. The

    membrane between compartment 2 and 3 is permeant to chloride ions only, and its specific electri

    cal conductivityGCl is 2 mS/cm2. Both membranes have areasA=10cm2. The temperature T issuch that RT/(Floge)=60mV.

    a) Sketch an electrical circuit that represents the steady-state relation between current and volt

    age for the three compartments. Label the nodes that correspond to compartments 1, 2, and

    3. Include the switch in your sketch. Label Im, Vm, and the conductances.

    b) Let V1 and V2 represent the steady-state potentials in compartments 1 and 2 with referenceto compartment 3 when the switch is open. Calculate numerical values for V1 and V2.

    c) Compute the steady-state value of the current Im when the switch is closed.

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    MASSACHUSETTS INSTITUTE OF TECHNOLOGY

    Department of Electrical Engineering and Computer Science,

    Department of Mechanical Engineering,

    Division of Bioengineering and Environmental Health,

    Harvard-MIT Division of Health Sciences and Technology

    Quantitative Physiology: Cells and Tissues

    2.791J/2.794J/6.021J/6.521J/BE.370J/BE.470J/HST.541J

    Homework Assignment #5 Issued: October 14, 2004

    Due: October 21, 2004

    Reading

    Lecture 17 Volume 2: Chapter 1

    Lecture 18 Volume 2: 2.1-2.4.2

    Lecture 19 Volume 2: 2.4.3-2.5

    Announcements

    The recitation on October 19 is cancelled so that we can meet that evening for a Writing Clinic. The

    Writing Clinic will be heldfrom 7:30 to 9:30 PM. Please return your written critiquesof your

    peers laboratory report at that time. You will also receive critiques from the technical and

    writing staffs.

    Exercise 1. Active ion transport is said to have a direct and an indirect effect on the resting

    potential of a cell. Define both effects and discuss the distinction between the two effects.

    Exercise 2. Describe the distinctions between the following terms that refer to ion transport across

    a cellular membrane: electrodiffusive equilibrium, steady-state, resting conditions, and cellular

    quasi-equilibrium.

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    0

    Exercise 3. Figure 1 shows measurements of the resting potential of a glial cell for different values

    of extracellular potassium concentration (left panel). These measurements are to be interpreted in

    terms of the network model shown in the right panel of the same figure. Assume that co =150N a

    Mud puppy

    Slope:

    glial cell

    59 mV/decade

    +

    +

    Im

    Ip

    Ip

    K

    IaKI

    a

    G GK

    VK

    Na

    Na

    Na

    Restingpotential(m

    V)

    20 +

    40

    60 Vom

    80VNa

    100

    120

    0.1 1 10 100co

    K(mmol/L)

    Figure 1: Measurements and model of electrical responses of a glial cell.

    immol/L, c = 15mmol/L and that the external solution is maintained isotonic with the cyto-Na plasm by controlling impermeant solutes. Assume that sodium and potassium concentrations are

    o aconstant, except for cK, and that the pump system, which consists of Ia and IK, is nonelectro-N a

    genic.

    a) Consider only the region for which the data are well fit by the straight line of slope 59

    mV/decade. Indicate whether the following statements are true or false and give a brief

    reason for each answer.

    i Im =

    0.ii) Vo VK.m

    iii) GNa GK.

    iv) VNa > VK.iv) cK =100mmol/L.a avi) I =IN a.K

    p pvii) I =IN a.K

    aviii) I =GN a(Vo VN a).N a m

    b) It is proposed that deviation of the data from the straight line for the lowest co is a result ofKa change in GK that occurs when Vo < 110

    mV. For the data shown, is this a reasonablemhypothesis? Does it require that GK for V

    o = 125mV is larger or smaller than GK formVo > 100mV? Explain.m

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    Exercise 4. The ionic concentrations of a uniform isolated cell are given in the following table.

    Concentration (mmol/L)

    Inside Outside

    Potassium 150 15

    Sodium 15 150

    An electrode is inserted into the cell and connected to a current source so that the current throughthe cell membrane is Im. The steady-state voltage across the cell membrane Vm is determined as afunction of the current as shown in the following figure.

    +

    +

    +

    +

    (mV)

    0

    40

    0.40

    Vm

    Vm

    VmIm

    Im

    IK

    I

    V VK

    G GK

    Im (nA)

    Na

    Na

    Na

    Assume that: (1) the cell membrane is permeable to only K+ and Na+ ions; (2) the Nernst equi

    librium potentials are Vn = (60/zn)log10(cn/cion)(mV); (3) ion concentrations are constant; (4)

    active transport processes make no contribution to these measurements.

    a) Determine the equilibrium potentials for sodium and potassium ions, VN a and VK.

    b) What is the resting potential of the cell with these ionic concentrations?

    c) With the current Im adjusted so that Vm =VK, what is the ratio of the sodium current to thetotal membrane current, IN a/Im?

    d) What is the total conductance of the cell membrane Gm =GN a +GK?

    e) Determine GNa and GK.

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    Problem 1. The resting membrane potential, Vo , of two uniform, isolated cells is measured as amofunction of the external concentration of potassium, cK, with the sodium concentration held fixed

    on oat its normal value, cN a, and then as a function of the external sodium concentration, cNa , withthe potassium concentration held fixed at its normal value, con. The results for these two cells areKshown in the following figure.

    Cell 1 Cell 2

    150

    100

    50

    0

    50

    Slope: 60 mV/decade Slope: 48 mV/decadeRestingpotential(mV)

    150

    100

    50

    0

    50

    1 10 100 1000 1 10 100 1000co

    (mmol/L) co (mmol/L)K K

    Slope: 12 mV/decadeSlope: 0 mV/decadeRestin

    gpotential(mV)

    150

    100

    50

    0

    50

    150

    100

    50

    0

    50

    1 10 100 1000 1 10 100 1000o ocN

    a

    (mmol/L) cN

    a

    (mmol/L)

    You may assume that for each cell: (1) external solutions are isotonic; (2) the membranes are

    impermeable to ions other than potassium and sodium; (3) the internal concentrations of potassium

    and sodium are maintained constant by a non-electrogenic active transport mechanism; (4) the

    total membrane conductance is 10 nS; (5) the normal resting potential is 60mV; (6) the internal

    concentration of sodium is 20 mmol/L.

    G

    a) For each cell, determine the total conductance of the membrane to potassium and to sodium,

    K and GNa , respectively. If either value is indeterminate from the information given, de

    scribe what additional information would be needed.

    b) For each cell, determine the internal and external concentrations of potassium and the ex

    ternal concentration of sodium at the normal resting potential (60 mV). If the value isindeterminate from the information given, describe what additional information would be

    needed.

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    c) For each cell, determine the simplest equivalent electric network model that relates the de

    pendence of the resting potential of the cell on the ion concentrations. Indicate the values of

    all elements in the network.

    Problem 2. The membrane of a cell is known to be permeable to Na+ and K+ only, with

    passive ionic conductances of GN a = 106 S/cm2 and GK = 10

    3 S/cm2, and contains a

    (Na+ K+)ATPase active transport mechanism that transports 3 molecules of Na+ outward and

    2 molecules of K+ inward through the membrane for each molecule of ATP split into ADP and

    phosphate. In the experiment shown in Figure 2, the cell is kept at a temperature of 24C. For

    tt

    t

    60 60

    80

    Injectionof Perfusion

    sodiumions withouabain

    V

    om

    Figure 2: Effect of sodium injection and ouabain on resting potential.

    t < t1, the cell is in its normal resting state with resting potential Vo 60mV, and resting ionm

    concentrations shown in the following table.

    Ion Concentration (mmol/L)

    Internal External

    Sodium 15 135

    Potassium 156 15

    At t=t1, Na+ is injected rapidly into the cell interior, without the passage of any current through

    the membrane, to double the intracellular sodium concentration. When the injection is completed,

    the membrane potential hyperpolarizes to approximately 80

    mV. At t

    =

    t2 ouabain, a blockerof the active transport mechanism, is applied to the cell and the membrane potential returns to

    approximately its normal resting value.

    a) Is the active transport mechanism electrogenic or nonelectrogenic? Explain!

    b) Does the active transport mechanism contribute appreciably to the resting potential for t

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    Problem 3. The membrane of a cell contains an active transport mechanism that pumps three

    sodium ions out of the cell for every two potassium ions that it pumps into the cell. The membrane

    also supports the passive transport of sodium and potassium ions, but is impermeant to all other ions

    and is impermeant to water. The sodium conductivity is 105S/cm2and the potassium conductivityis 104S/cm2. The cell is allowed to come to steady state and its membrane potential is 52.5mV.The Nernst equilibrium potential for sodium is 60mV and the Nernst equilibrium potential for

    60

    3

    potassium is mV. The net outward current density due to active transport is A/cm2

    .8

    a) Draw an electrical circuit to represent ionic transport across the membrane of this cell. In

    clude labels for each of the 6 numbered parameters provided in the problem statement.

    b) Is the cell at rest? If yes, prove that it is at rest. If no, explain why not.

    c) Is the cell in quasi-equilibrium? If yes, prove that it is at quasi-equilibrium. If no, explain

    why not.

    d) Is the active transport mechanism electrogenic? Explain.

    Problem 4. Consider the model of a cell shown in the following figure.

    +

    +

    +

    Vom

    Im

    Ip

    IpK

    IaKI

    a

    G GK

    V VK+

    IpCl

    GCl

    VCl

    Na

    Na

    Na

    Na

    The cell has channels for the passive transport of sodium, potassium, and chloride as well as a

    pump that actively transports sodium out of the cell and potassium into the cell. The pump ratio

    is Ia K = 1.5. The following table shows the intracellular and extracellular concentrations,Nernst equilibrium potentials, and conductance ratios for sodium and potassium. Some informa

    tion is also given for chloride; blank entries represent unknown quantities.

    N a/Ia

    cin con Vn Gn/GK

    (mmol/L) (mV)Na+ 10 140 +68 0.1K+ 140 10 68 1Cl 150 1

    The cell also contains impermeant intracellular ions. Assume that the cell is in equilibrium at t=0,i.e., assume that at t= 0the cell has reached a condition for which all solute concentrations, thecell volume, and the membrane potential are constant.

    a) Choose one of the following statements and explain why it is true.

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    i) The cell resting potential depends on GCl .

    ii) The cell resting potential depends on VCl .

    iii) The cell resting potential depends on both GCl and VCl.

    iv) The cell resting potential does not depend on GCl .

    v) The cell resting potential does not depend on VCl .

    vi) The cell resting potential does not depend on eitherG

    Cl or VCl .

    b) Determine Vo.m

    c) At t=0, the external concentration of chloride is reduced from 150 mmol/L to 50 mmol/Lby substituting an isosmotic quantity of an impermeant anion for chloride. Assume that the

    concentrations of sodium and potassium both inside and outside the cell remain the same

    and that the volume of the cell does not change.

    i) Determine Vom(0+), the value of the membrane potential immediately after the change

    in solution. You may ignore the effect of the membrane capacitance.

    ii) Determine Vom(), the value of the membrane potential after the cell has equilibrated.i

    iii) Determine cCl (

    ), the intracellular chloride concentration after the cell has equilibrated.

    iv) Give a physical interpretation of your results in i), ii), and iii).

    v) Discuss the validity of the assumptions that the sodium and potassium concentrations

    in the cell are constant and that the volume does not change.

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    MASSACHUSETTS INSTITUTE OF TECHNOLOGY

    Department of Electrical Engineering and Computer Science,

    Department of Mechanical Engineering,

    Division of Bioengineering and Environmental Health,

    Harvard-MIT Division of Health Sciences and Technology

    Quantitative Physiology: Cells and Tissues

    2.791J/2.794J/6.021J/6.521J/BE.370J/BE.470J/HST.541J

    Homework Assignment #6 Issued: October 21, 2004

    Due: October 28, 2004

    Reading

    Lecture 20 Volume 2: 4.1-4.1.2.3 4.2-4.2.2.2

    Lecture 21 Volume 2: 4.2.3-4.2.3.1

    Lecture 22 Volume 2: 4.2.3-4.2.3.2

    Announcements

    Laboratory reports are DUE Monday October 25 at noon. You should submit one copy of the

    final draft of the report. You should include the following items in an appendix: final proposal,

    copy of your critique of a peers first draft, peer critique of your first draft, critique of your first

    draft by writing program, critique of your first draft by technical staff, photocopies of notes taken

    during original lab session. Note that there is a SEVERE LATENESS PENALTY. The grade for

    a late report will be multiplied by a lateness factor

    t/72L= 0.3et/4 + 0.7e

    where tis the number of hours late. The lateness factor is plotted below. Notice that the maximum

    grade for a report that is more than ONE DAY LATE is less than 50%.

    8 1The exam is closed-book: notes on both sides of two

    Lateness

    factorL

    1.0

    0.5

    0.0one day

    1 10 100

    Time t past deadline (hours)

    This lateness factor is applied regardless of the reason for the lateness, except for health related

    problems or personal problems certified by the Deans office. Specifically, lateness due to computer

    and/or printer problems is not exempt.

    Exam 2 will be held on Thursday, November 4 from 7:30 PM to 9:30 PM

    11 sheets of paper may be2

    used for reference. Calculators may be used, but computers and wireless devices may not be used.

    There will be no recitations on the day of the exam.

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    Exercise 1. Give aphysical explanation for why the conduction velocity is larger in larger diameter

    fibers, if all other factors are the same.

    Exercise 2. Give aphysical explanation of the meaning of Equation 2.18 (in volume 2 of the text)

    without the use of equations.

    Exercise 3. Let the function f(z, t) represent a solution to the wave equation. This solution isshown in the following figure as a function of time t at the position z= 0.

    0 1 20

    1

    f(0

    )

    ,t

    t(ms)

    Notice that f(0, t) is non-zero for 0

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    Problem 2. A fine platinum wire with a resistance per unit length of 130 /cm is inserted inside aportion of a squid axon as illustrated below.

    V1(t) V2(t)

    iial Wi

    z

    Axonact on

    potent re

    (cm)

    z1 z2

    The wire is so thin that its volume can be ignored. The axon (500 m diameter) is electrically stimulated to produce a propagated action potential traveling in the +zdirection. The action potentialis recorded at two intracellular sites: V1(t)is recorded at z =z1 and V2(t)is recorded at z =z2.The distance between the stimulus electrode (not shown) and z1 is 2 cm. Results are shown in thefollowing figure.

    0

    V1(t) V2(t)+50

    50

    100Intracellularpotential

    (mV)

    0 5 10 15 20 25

    Time (ms)

    The resistivity of the axoplasm of this axon is 23 -cm. The resistance per unit length of theexternal solution is 1.2 /cm. The wire begins at some location between z1 and z2, but the exactposition of the beginning is not known and should not be used in any of your calculations.

    a) Determine the instantaneous speed of the action potential as its peak passes the point z=z1.

    b) Determine the instantaneous speed of the action potential as its peak passes the point z=z2.

    c) Sketch the extracellular potential as a function of space (z) that results at the time that thepeak of the action potential passes the point z=z1. Include distances z14< z < z1+4cm.Indicate the scale for the y axis. Describe the important features of this plot.

    d) Sketch the extracellular potential as a function of space (z) that results at the time that thepeak of the action potential passes the point z=z2. Include distances z24< z < z2+4cm.Indicate the scale for the y axis. Describe the important features of this plot.

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    Problem 3. In measurement 1, a cylindrical unmyelinated axon of radius ais placed in a largevolume of isotonic sea water and the conduction velocity of the action potential is measured to

    be 1. The osmotic pressure of the sea water is then doubled by increasing the salt concentration,and the axon is allowed to come to osmotic equilibrium. Then, in measurement 2, the conduction

    velocity is measured to be 2. Assume that during these experiments

    the number of ions transported through the axon membrane is negligible compared to the

    number of ions inside the axon, the volume of the axon is negligible compared to the volume of the bath,

    the specific electric properties of the membrane (the capacitance per unit area and the con

    ductance per unit area) are the same in both measurements,

    the length of the axon remains unchanged, and

    the external resistance per unit length of the axon, ro, is negligible compared to the internalresistance per unit length of the axon.

    Part a. Let ri1 and ri2represent the internal resistance per unit length of the axon in measurements1 and 2, respectively. Determine the numerical value (or a numerical expression) for the ratio of

    these resistances:ri2

    /ri1. Briefly explain your reasoning.

    Part b. Determine the numerical value (or a numerical expression) for the ratio of speeds: 2/1.Briefly explain your reasoning.

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    MASSACHUSETTS INSTITUTE OF TECHNOLOGY

    Department of Electrical Engineering and Computer Science,

    Department of Mechanical Engineering,

    Division of Bioengineering and Environmental Health,

    Harvard-MIT Division of Health Sciences and Technology

    Quantitative Physiology: Cells and Tissues

    2.791J/2.794J/6.021J/6.521J/BE.370J/BE.470J/HST.541J

    Homework Assignment #7 Issued: November 8, 2004

    Due: November 18, 2004

    Reading

    Lecture 23 Volume 2: 4.3

    Lecture 24 Volume 2: 4.4.8

    Lecture 25 Volume 2: 4.4.1

    Lecture 26 Volume 2: 3.1-3.2.1 3.3-3.4.2.1

    Lecture 27 Preparing an oral presentation

    Lecture 28 Volume 2: 3.4.2.4-3.4.3.1 3.4.3.3-3.5

    Lecture 29 Volume 2: 5.1-5.2.4.4

    Lecture 30 Volume 2: 5.3-5.7

    Lecture 31 Volume 2: 6.1-6.1.1 6.4-6.4.1.5 6.2-6.2.2 6.5-p407

    Announcements

    There is no homework assignment due this week, because of Veterans day. This assignment is due

    on the Thursday after Veterans day (November 18).

    First Drafts of your HH project is due on November 19 (one day after this homework is due!).

    The first draft should consist of hardcopies of 3-5 technical slides of the type you plan to show

    during your final oral presentation. Each slide should be accompanied by a separate sheet of paper

    that lists approximately three bullet points that you will discuss in your presentation of this slide.

    The first draft should also contain a 1 page extended abstract for your HH project. The abstract

    should summarize your findings and explain why they are interesting.

    Please take advantage of THIS week to work on your project plus the HH portion of this

    homework assignment!

    Exercise 1. The following assertions apply to responses calculated according to the Hodgkin-

    Huxley model in response to a step of membrane potential applied at t = 0. For each assertion,state if it is true or false and explain your answer.

    a) The leakage conductance is constant.

    b) The sodium conductance is discontinuous at t=0.

    c) The potassium conductance is discontinuous at t=0.

    d) The leakage current is constant.

    e) The sodium current is discontinuous at t=0.

    f) The potassium current is discontinuous at t=0.

    g) The factors n(t), m(t), and h(t)are discontinuous at t=0.

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    h) The time constants n, m, and h are discontinuous at t= 0.

    i) The steady-state values n, m, and h

    are discontinuous at t= 0.

    Exercise 2. Figure 1 shows the relation between the membrane potential and the membrane current

    density during a propagated action potential as computed from the Hodgkin-Huxley model. The

    2

    Vm

    (mV)

    Jm

    (mA/cm

    )

    0

    Jm

    Vm

    0.4

    40

    080

    0.41 2 3 4

    Time (ms)

    Figure 1: Relation of membrane potential and membrane current density during a propagated

    action potential. The dotted vertical line marks the time of occurrence of the peak of the action

    potential.

    membrane current density consists of an initial outward current followed by an early inward current

    whose peak occurs before the peak in the action potential.

    a) The initial outward current is due primarily to which of the following:

    i) an ionic current carried by sodium ions.

    ii) an ionic current carried by potassium ions.

    iii) an ionic current carried by chloride ions.

    iv) an ionic current carried by calcium ions.

    v) a capacitance current.

    b) The early inward current is due primarily to which of the following:

    i) an ionic current carried by sodium ions.

    ii) an ionic current carried by potassium ions.

    iii) an ionic current carried by chloride ions.iv) an ionic current carried by calcium ions.

    v) a capacitance current.

    c) Before the peak of the action potential, the membrane potential increases from its resting

    value whereas the membrane current density is first outward (increasing and then decreasing)

    and then reverses polarity to become inward (decreasing and then increasing again). Discuss

    this complex relation between membrane potential and current. In particular, explain how

    the Hodgkin-Huxley model accounts for the fact that the current can be both inward and

    outward during an interval of time when the membrane potential is depolarizing.

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    Exercise 3. Does the time constant of a cylindrical cell depend on its dimensions? Does the space

    constant of a cylindrical cell depend on its dimensions?

    Exercise 4. For each of the following statements, assume that the electrical properties of a patch

    of the membrane of the cell can be represented as a parallel resistance and capacitance. Assume

    that the cell has a cylindrical shape with a radius that is small compared to the length of the cell.Determine if each assertion is true or false and give a reason for your choice.

    a) For an electrically small cell, the membrane potential in response to a step of current through

    the membrane is an exponential function of time.

    b) If a step of current is applied through one part of the membrane of an electrically small cell,

    the resulting changes in membrane potential will be constant along the length of the cell for

    all times after the step.

    c) For an electrically large cell, the steady-state value of the membrane potential in response to a

    step of current applied through the membrane at one position along the cell is an exponential

    function of longitudinal position along the cell.

    d) For an electrically large cell, the steady-state value of the membrane potential in response to

    a step of current applied through the membrane at one position along the cell is a Gaussian

    function of position along the cell.

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    Problem 1. The Hodgkin-Huxley model was used to compute propagated action potentials for

    default values of the parameters and for 4 test cases. The following plots show the spatial depen

    dence of membrane potential that results 1 ms after the stimulus current was applied at z= 0.

    60 60

    Membranepotential

    Membranepoten

    tial

    (mV)

    (mV)

    A B

    C

    Membranepotential

    Membranepoten

    tial

    (mV)

    (mV)

    40 4020 20

    0 0

    20 20

    40 40

    60 60

    80 80

    0 1 2 3 0 1 2

    Distance (cm) Distance (cm)

    60 60 D40 4020 20

    0 0

    20 20

    40 40

    60 60

    80 80

    0 1 2 3 0 1 2

    Distance (cm) Distance (cm)

    Each of AD shows a plot with two curves: the thin gray curve was obtained for default parameters

    and the thick black curve was obtained for one of the tests cases. In each test case, a single

    parameter was changed from its default value. Default values of the axon characteristics are as

    follows length: 3 cm, radius: 0.0238 cm, cytoplasm resistivity: 35.4 cm, extracellular specificresistance: 0 /cm.

    a. Which of AD shows results when intracellular sodium concentration was reduced fromicNa

    = 50 to 25 mmol/L. Explain.

    b. Which of AD shows results when the maximum potassium conductance GK was increased

    from 36 to 72 mS/cm2

    ? Explain.

    c. Which of AD shows results when cytoplasmic resistivity was decreased from 35.4 to

    30 cm? Explain.

    4

    3

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    Problem 2. Ionic currents are calculated for a space-clamped squid giant axon using the Hodgkin-

    Huxley model, with all parameters set to their default values (as listed on page 191 of volume 2

    of the text) except for one parameter. For timest < 0, the membrane potential is held at 75mV

    and the model is at steady state. Att = 0, the membrane potential is stepped to +5mV and the

    resulting ionic current density is computed. Results for six calculations are shown in the following

    figure.

    0 1000

    Time (ms)

    IonicCurrentDensity

    (mA/cm

    2)

    2000

    2

    1

    0

    1

    2

    J2

    J3

    J5

    J4

    J6

    J1

    Part a. Which curve represents the ionic current that results when all parameters have default

    values exceptcoNa

    = 50mmol/L? Explain.

    Part b. Which curve represents the ionic current that results when all parameters have default

    values exceptcoK

    = 400mmol/L? Explain.

    Part c. Which curve represents the ionic current that results when all parameters have default

    values exceptGNa = 0? Explain.

    Part d. Which curve represents the ionic current that results when all parameters have default

    values exceptGK = 0? Explain.

    Problem 3. Space-clamped responses of the Hodgkin-Huxley model were calculated with the

    leakage conductance set to zero, GL = 0, and with all other parameters set to their default val-

    ues. The model was stimulated with a pulse of membrane current density of duration 0.5 ms; the

    amplitude was varied. The following figure shows the response for an amplitude of 40A/cm2.

    500

    400

    300

    200

    100

    0

    100

    0 0.5 1 1.5 2 2.5 3

    VmJion

    Jm

    mV

    andA/c

    m2

    Time (ms)

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    For each amplitude of the pulse of membrane current density, the ionic current density Jion andthe membrane potential Vm were determined at t = 0.7ms, where t = 0marks the onset of thecurrent pulse. The relation between Jion at t = 0.7ms and Vm at t = 0.7ms that results whenthe pulse amplitude is varied is shown in the following figures. The left panel shows results for a

    broad range of membrane potential, from 80to +60mV. The right panel shows results for thenarrower range from 76to 62mV.

    400

    300

    200

    100

    0

    0.2

    0.1

    0

    Jion

    (t

    .

    A/cm

    2

    )

    =

    07ms)(

    806040 20 0 20 40 60 76 74727068666462

    Vm(t=0.7ms)(mV)

    Part a. Determine the value of the resting potential to within 1 mV. Explain your choice.

    Part b. If the current stimulus is such that Vm(t) =66mV at t= 0.7ms, does the membranepotential increase with time or decrease with time? Explain.

    Part c. Determine the value of the threshold potential to within 1 mV. Explain your choice.

    Part d. Between the resting potential and this threshold potential, determine whether |JNa|>|JK|,|JNa |=|JK|, or |JNa| |JK|, |JNa | = |JK|, or

    |JNa |

    >ro.

    b) Describe a method by which the data in Figure 4 could be analyzed to estimate the current

    densityKm flowing out of an internode. Apply your method to determine whether current is

    flowing into or out of the internode between nodes 5 and 6 at t0 =0.75ms.

    Problem 4. Although there is considerable scatter, the ratio of the inner diameter dto outer diameter Dof the layer of myelin that encircles a myelinated fiber tends to be about 0.74, as shown inthe following figure, where every symbol represents measurements of d/Dand dfor a differentfiber.

    0.9

    vagus nerve

    sciatic nerve

    d/D

    0.85

    0.8

    0.75

    0.7

    0.65

    0.6

    0.55

    0.5

    Dd

    0.5 1 1.5 2 2.5 3 3.5 4 4.5 5d(m)

    The point of this problem is to investigate the hypothesis that this relation between d

    and D

    resultsfrom an evolutionary optimization of the cable model.

    Part a. Assume that the myelinated part (the internode) of a myelinated fiber can be represented by

    the cable model. Assume the myelin can be represented by a homogeneous electrical material with

    resistivity mand permittivity m. Assume the intracellular conductor is a homogeneous conductorwith resistivity w. Assume that the extracellular conductor has negligible resistance. Determinean expression for the space constant C of this model in terms of the inner diameter dand the outerdiameter Dof the layer of myelin. Hint: The radial resistance of a cylindrical shell is given below.

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    Dd

    o

    +

    V

    lnR = =I 2L d

    Part b. The expression derived in part a is plotted below

    0.6

    0.4

    C/o

    0.2

    0

    0 0.5 1

    d/D

    where o =D m/8w. Thus, if Dis fixed (i.e., if the axon is constrained to fit into a constantvolume), then o is a constant, and C is maximum when d0.6D.

    b1) Explain in physical terms why the space constant gets smaller as the value of ddecreasesbelow 0.6D.

    b2) Explain in physical terms why the space constant gets smaller as the value of d

    increasesabove 0.6D.

    Part c. The value of d/Dthat maximizes the space constant of the cable model is remarkably closeto the ratio of 0.74 seen experimentally. Nevertheless, it is smaller. One possible reason why it is

    smaller is that we ignored the resistance of the outer conductor ro. How would the space constantsdependence on d/D change if the resistance of a thin layer of saline (thickness = 0.1D) wereincluded in the calculation. Make a plot that contains both the old relation (shown in the previous

    plot) and the new relation. Briefly describe how the addition of the outer resistance changes the

    predicted space constant.

    D

    L

    d

    V D

    5

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    MASSACHUSETTS INSTITUTE OF TECHNOLOGY

    Department of Electrical Engineering and Computer Science,

    Department of Mechanical Engineering,

    Division of Bioengineering and Environmental Health,

    Harvard-MIT Division of Health Sciences and Technology

    Quantitative Physiology: Cells and Tissues

    2.791J/2.794J/6.021J/6.521J/BE.370J/BE.470J/HST.541J

    Homework Assignment #9 Issued: December 2, 2004

    This homework assignment will not be collected.

    Exercise 1. Explain the origin of gating current.

    Exercise 2. State whether each of the following are true or false and give a reason for your answer.

    a) Tetrodotoxin blocks the flow of potassium through the sodium channel.

    b) The macroscopic sodium current recorded by an electrode in a cell is a sum of the single-

    channel sodium currents that flow through single sodium channels.

    c) The macroscopic sodium current recorded by an electrode in a cell is the average of the

    single-channel sodium currents that flow through single sodium channels.

    d) Ionic and gating currents give identical information about channel kinetic properties.

    Exercise 3. Explain why the gating current is outward in response to a depolarization independent

    of the sign of the charge on the gate.

    Exercise 4. List 4 distinct properties shown by ionic currents measured from single voltage-gatedion channels.

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    Problem 1. The voltage across a membrane patch is stepped from Vo to Vf at t= 0and single-m mchannel ionic currents are recorded as a function of time. Typical records at 6 different values of

    Vf are shown in the following figure.m

    Vfm

    (mV)00

    10

    201.4

    0

    401.8

    60

    2.2

    80

    100

    Current(pA) 0

    0

    2.60

    3

    0 8Time (ms)

    a) Is the open-channel voltage-current characteristic of this channel linear or nonlinear?

    b) What is the conductance of the open channel?

    c) What is the equilibrium (reversal) potential for this channel?

    d) It is proposed that this channel is the voltage-gated sodium channel responsible for sodium-

    activated action potentials. Discuss this suggestion.

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    Problem 3. This problem deals with the relation of current to voltage for single ion channels.

    Assume that conduction through an open ion channel is governed by the equation

    I=(VmVe),

    VwhereI

    is current through a single open channel,

    is the conductance of a single open channel,m is the membrane potential across the channel, and Ve is the equilibrium (reversal) potential for

    the channel. For each of the channels in this problem, assume that = 25 pS and Ve = 20 mV.

    a) The membrane potential Vm and the average single-channel current iobtained from threedifferent single channels (A, B, and C) are shown in Figure 1. Both the membrane potential

    Channel A Channel B Channel C

    t t

    t60 60

    20 20 +10

    +80

    t t

    t

    1

    0.50.50.75 -0.2

    +0.3

    Vm(t

    i(t

    Vm(t

    i(t

    Vm(t

    i(t

    ) (mV)

    ) (pA)

    ) (mV)

    ) (pA)

    ) (mV)

    ) (pA)

    Figure 1: Average single-channel currents.

    and current are plotted on a time scale such that the changes appear instantaneous and only

    the final values of these variables can be discerned in the plots; i.e., the kinetics are not

    shown. For each of these channels, answer the following questions and explain your answers:

    i) Is this channel voltage-gated for the illustrated depolarization?

    ii) Is the channel activated (opened) or inactivated (closed) by the illustrated depolariza

    tion?

    b) Assume that each voltage-gated channel contains one two-state gate where is the timeconstant of transition between states. For each of the channels, sketch the time course of i(t)on a normalized time scale t/. Clearly show the current near t= 0.

    Problem 4. Three three-state voltage-gated channels (channels a, b, and c) have the kinetic dia

    gram and state occupancy probabilities shown in Figure 2. These channels have the same voltagedependent rate constants and the same equilibrium potential which is +40 mV. For the membrane

    potential shown, the channels are in state 1 with probability 1 for t0. The channels differ only in their state conductances and state gating charges asshown in Figure 3. Denote the expected values of the single-channel random variables as follows:

    the conductance as ga(t), gb(t), and gc(t); the ionic currents as ia(t), ib(t), and ic(t); the gatingcharges as qa(t), qb(t), and qc(t); the gating currents as iga(t), igb(t), and igc(t).

    a) Which of the waveforms shown in Figure 4 best represents gb(t)? Explain.

    b) Which of the waveforms shown in Figure 4 best represents gc(t)? Explain.

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    5

    1

    10

    1

    0

    0.5

    1

    0 0.5 1 1.5

    State

    occupancy

    probability

    Vm(t)

    S1 S2 S3

    x1(t)

    x2(t)

    x3(t)

    Time (ms)

    Figure 2: State diagram and occupancy probabilities for a three-state channel. The state occupancy

    probabilities for states S1, S2, and S3 are x1(t), x2(t), and x3(t), respectively.

    Channel a

    5

    1

    10

    1

    5

    1

    10

    1

    Channel b

    1

    1

    2

    2 3

    3

    S1 S2 S3

    S1 S2 S3

    Q1 = 1

    Q1

    Q2

    Q2

    Q3

    Q3

    = 10

    = 0

    = 0

    = 10 = 0

    = 0

    = 0

    = 0

    = 0

    = 0

    = 1

    Channel c

    5

    1

    10

    1

    1

    2

    3

    S1

    S2

    S3

    Q1 Q2 Q3

    = 0 = 0 = 10

    = 1 = 0 = 0

    Figure 3: State diagrams of three three-state channel models. The models differ in state conduc

    tances and state gating charge but not in rate constants.

    c) Which of the waveforms shown in Figure 4 best represents iga(t)? Explain.

    d) Which of the waveforms shown in Figure 4 best represents igc(t)? Explain.

    e) Which of these channel models exhibits activation followed by inactivation of the ionic cur

    rent? Explain.

    f) Which of these channel models exhibits an ionic current that does not inactivate? Explain.

    g) Which of these channel models represents a channel that closes on depolarization? Explain.

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    t tVm(t)Vm(t)

    w1(t)

    w2(t)

    w3(t)

    w4(t)

    w5(t)

    w6(t)

    w7(t)

    w8(t)

    Figure 4: Waveforms of responses. The horizontal axis corresponds to w(t) = 0, and the verticalaxis to t= 0.

    Problem 5. Figure 5 shows a model of a voltage-gated ion channel with one three-state gate plus

    representative single-channel ionic and gating current records.

    a) Assume that the voltage-current characteristic of the channel is the same for states 1 and 3

    and is linear. Determine the open channel conductance and equilibrium (reversal) potentialfor this channel.

    b) The ionic current trace shown in Figure 5 has three non-zero segments. Determine which

    state the gate is in during each non-zero segment. Explain your reasoning.

    c) Figure 6 illustrates the dependence of the steady-state probability that the channel will be

    in each of its three states on the membrane potential. Let iss represent the average valueof the ionic current that results after steady-state conditions are reached in a voltage clamp

    experiment in which Vm is held constant. Assume that the experiment is repeated for anumber of different values of membrane potential Vm. Plot the relation between iss and Vm.Describe the important features of your plot.

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    state 1

    t

    (ms)

    +50

    50

    inside

    outside

    +Vm (mV)

    state 2 i(pA)

    t (ms)

    32

    1

    inside

    outside

    +

    state 3

    t (ms)

    inside

    outside

    +

    ig (pA)

    Figure 5: Channel with one three-state gate. The left panels illustrate the three states: states 1 and

    3 are open states, state 2 is a closed state. The right panels illustrate the responses of the channel

    to a step in membrane potential Vm(t) at time t= 0 (top right) which gives rise to the ionic currenti(t) and gating current ig(t) illustrated in the middle right and lower right panels, respectively.

    100 1000

    0.5

    1

    x1 x2 x3

    Membrane potential (mV)

    Figure 6: Steady-state probabilities for a channel with one three-state gate. x1, x2, and x3represent the steady-state probabilities of being in state 1, state 2, and state 3, respectively, as a

    function of membrane potential.

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    MASSACHUSETTS

    INSTITUTE

    OF

    TECHNOLOGY

    Department

    of

    Electrical

    Engineering

    and

    Computer

    Science,

    Department

    of

    Mechanical

    Engineering,

    Division

    of

    Bioengineering

    and

    Environmental

    Health,

    Harvard-MIT

    Division

    of

    Health

    Sciences

    and

    Technology

    QuantitativePhysiology:CellsandTissues

    2.791J/2.794J/6.021J/6.521J/BE.370J/BE.470J/HST.541J

    Hodgkin-HuxleyProject

    This

    theoretical

    project

    is

    intended

    to

    provide

    an

    opportunity

    to

    learn

    about

    the

    complex

    behav

    iors

    that

    can

    be

    exhibited

    by

    the

    Hodgkin-Huxley

    model

    and

    to

    compare

    behaviors

    of

    the

    model

    with

    behaviors

    of

    electrically

    excitable

    cells.

    We

    have

    two

    simulations.

    The

    first

    models

    a

    space-

    clamped

    axon.

    That

    model

    generatesmembraneactionpotentials. Thesecondmodelsanaxon

    without

    space-clamp

    (although

    the

    second

    model

    can

    simulate

    a

    space

    clamp

    since

    the

    longitudi

    nalresistancescanbesettozero). Thesecondmodelcanproducepropagatedactionpotentials.

    Thesecondmodelcanbeused toexploreawiderrangeofphenomena than thefirst. Thefirst

    model

    is

    faster

    and

    simpler

    than

    the

    second.

    Thus

    both

    models

    are

    useful,

    and

    your

    project

    can

    use

    eitherorbothofthemodels.

    StudentsareSTRONGLYencouraged toworkinpairs,however, individualprojectswillbe

    approvedifthereareextenuatingcircumstances.Ifapairofstudentscollaborateonaprojectthey

    shouldsubmitasingleproposalandasinglereportwhichidentifiesbothmembersoftheteamand

    gives

    both

    email

    addresses.

    Proposals

    should

    be

    submitted

    via

    the

    form

    available

    on theMIT

    server. Proposalswillbereturnedassoonaspossiblesothatstudentscanrevisethem. Onlythe

    final,

    accepted

    proposal

    will

    be

    given

    a

    grade.

    Thedemonstrationprojectperformedinlectureontheeffectoftemperaturecannotbethebasis

    ofastudentproject.

    Practicalconsiderationsinthechoiceofatopic

    ProjectscaninvolvealmostanyofthepropertiesoftheHodgkin-Huxleymodel.However,toavoid

    projectswhoseaimsarevague(e.g.,IwouldliketounderstandhowtheHodgkin-Huxleymodel

    works)theproposedprojectshouldbeintheformofaspecificandtestablehypothesis.Projects

    thatinvolvemonthsofcomputationshouldobviouslybeavoided.Theamountofcomputationtime

    shouldbeexplicitlytakenintoaccountinplanningaproject.Forexample,anyprojectthatinvolves

    measuringthethresholdofoccurrenceofanactionpotentialformanydifferentparametervaluesis

    boundtobeverytimeconsuming,becausedeterminingthethresholdforasinglesetofparameters

    itself

    involves

    many

    computations.

    The

    task

    is

    to

    choose

    a

    physiological

    property

    of

    the

    excitation

    of

    the

    action

    potential

    that

    is

    of

    interest,

    and

    then

    to

    define

    a

    specific,

    feasible

    project.

    Choiceoftopics

    Topics

    can

    involve

    comparing

    predictions

    of

    the

    Hodgkin-Huxley

    model

    with

    measurements

    on

    cells.

    For

    example,

    the

    text

    contains

    data

    on

    the

    effects

    of

    many

    external

    parameters

    (e.g.,

    ionic

    concentrations,cell type)onactionpotentials. Aprojectmightinvolvereadingtheoriginalpa

    persthatdescribesuchmeasurements(someweremadebeforetheHodgkin-Huxleymodelwas

    formulated),and testingthehypothesisthatthesemeasurementsare(orarenot)consistentwith

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    the

    Hodgkin-Huxley

    model.

    Similarly,

    a

    project

    might

    involve

    examining

    the

    effect

    of

    some

    phar

    macological

    substance

    on

    measurements

    of

    the

    action

    potential

    and

    testing

    the

    hypothesis

    that

    the

    substance

    produces

    its

    effect

    by

    changing

    one

    or

    another

    parameter

    of

    the

    model.

    These

    projects

    will

    require

    some

    reading

    of

    original

    literature

    which

    is

    often

    difficult

    and

    usually

    time

    consuming.

    However,

    such

    a

    project

    can

    lead

    to

    a

    very

    rewarding

    educational

    experience.

    Alternatively,

    the

    projectmightinvolveapurelytheoreticaltopicinwhichsomepropertyofthemodelisexplained

    in

    terms

    of

    its

    underlying

    structure.

    This

    type

    of

    project

    does

    not

    necessarily

    involve

    reading

    theoriginalliterature.

    Examplesofhypotheses

    1.

    Hypothesis

    The

    effect

    of

    temperature

    on

    the

    conduction

    velocity

    of

    the

    squid

    giant

    axon

    can

    be

    fit

    by

    the

    Hodgkin-Huxley

    model.

    Articles

    in

    the

    literature

    should

    be

    consulted

    for

    this

    project:

    Chapman,R.A.(1967).Dependenceontemperatureoftheconductionvelocityofthe

    actionpotentialofthesquidgiantaxon.J.Physiol.213:1143-1144.

    Easton,D.M.andSwenberg,C.E.(1975).Temperatureandimpulsevelocityingiant

    axon

    of

    squidloligopealei.Am.J.Physiol.229:1249-1253.

    2. HypothesisWhentwoactionpotentialsareelicited,onejustafteranother, thevelocity

    ofthesecondisslowerthanthevelocityofthefirstactionpotential. Thisphenomenonis

    predicted

    by

    the

    Hodgkin-Huxley

    model.

    Articles

    in

    the

    literature

    should

    be

    consulted

    for

    this

    project:

    George,S.A.,Mastronarde,D.N.,andDubin,M.W.(1984).Prioractivityinfluences

    thevelocityofimpulsesinfrogandcatopticnervefibers.BrainRes.304:121-126.

    3.

    Hypothesis

    The

    threshold

    current

    for

    eliciting

    an

    action

    potential

    with

    an

    intracellular

    electrode

    is

    higher

    for

    a

    space-clamped

    than

    for

    an

    unclamped

    model

    of

    an

    axon.

    4. HypothesisIncreasingthemembranecapacitancewilldecreasetheconductionvelocity.

    5.

    Hypothesis

    Increasing

    the

    membrane

    conductance

    (by

    scaling

    all

    the

    ionic

    conductances)

    will

    increase

    the

    conduction

    velocity.

    6. HypothesisIncreasingtheexternalconcentrationofsodiumwillincreasetheconduction

    velocity.

    7.

    Hypothesis

    Increasing

    the

    external

    concentration

    of

    potassium

    will

    increase

    the

    conduc

    tion

    velocity.

    8. HypothesisIncreasingtheexternalconcentrationofcalciumwillincreasetheconduction

    velocity.

    9.

    Hypothesis

    Increasing

    the

    temperature

    will

    increase

    the

    conduction

    velocity.

    10. HypothesisThedifferenceinwaveformoftheactionpotentialofafrognodeofRanvier

    andofasquidgiantaxon(Figure1.9 involume2of the text)canbe reproducedby the

    Hodgkin-Huxley

    model

    of

    a

    squid

    giant

    axon

    by

    a

    change

    in

    temperature.

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    11.

    Hypothesis

    The

    membrane

    capacitance

    determines

    the

    time

    course

    of

    the

    rising

    phase

    of

    the

    action

    potential.

    Increasing

    the

    membrane

    capacitance

    decreases

    the

    rate

    of

    increase

    of

    the

    rising

    phase

    of

    the

    action

    potential.

    12.

    Hypothesis

    The

    falling

    phase

    of

    the

    action

    potential

    (repolarization)

    can

    occur

    in

    the

    absence

    of

    a

    change

    in

    potassium

    conductance.

    13.

    Hypothesis

    Increasing

    the

    temperature

    sufficiently

    blocks

    the

    occurrence

    of

    the

    action

    potential

    because

    the

    membrane

    time

    constant

    limits

    the

    rate

    at

    which

    the

    membrane

    vari

    ables

    can

    change

    and

    prevents

    the

    difference

    in

    time

    course

    of

    the

    sodium

    and

    potassium

    activation

    which

    is

    responsible

    for

    initiation

    of

    the

    action

    potential.

    14.

    Hypothesis

    The

    initiation

    of

    the

    action

    potential

    is

    independent

    of

    the

    potassium

    conduc

    tance.

    15.

    Hypothesis

    The

    prolonged

    plateau

    of

    the

    cardiac

    muscle

    action

    potential

    can

    be

    accounted

    for

    by

    the

    Hodgkin-Huxley

    model

    with

    a

    potassium

    conductance

    that

    has

    a

    slow

    activation.

    16.

    Hypothesis

    The

    effect

    of

    tetraethylammonium

    chloride

    (TEA)

    on

    the

    action

    potential

    of

    the

    squid

    giant

    axon

    can

    be

    modelled

    with

    the

    Hodgkin

    Huxley

    model

    by

    decreasing

    Kn

    and

    increasing

    Kh.Articlesintheliteratureshouldbeconsultedforthisproject:

    Armstrong,C.M.(1966). TimecourseofTEA+-inducedanamalousrectificationin

    squid

    giant

    axons.J.Gen.Physiol.50:491-503.

    Armstrong,C.M.andBinstock,L.(1965).Anomalousrectificationinthesquidgiant

    axon

    injected

    with

    tetraethylammonium

    chloride.J.Gen.Physiol.48:859-872.

    Tasaki,I.andHagiwara,S.(1957).Demonstrationoftwostablepotentialstatesinthe

    squidgiantaxonundertetraethylammoniumchloride.J.Gen.Physiol.40:859-885.

    17.

    Hypothesis

    The

    shape

    of

    the

    action

    potential

    in

    the

    presence

    of

    tetraethylammonium

    chloride(TEA)canbeaccountedforbytheHodgkin-Huxleymodelwithareducedmaximum

    valueofthepotassiumconductance. Articlesintheliteratureshouldbeconsultedforthis

    project:

    Armstrong,C.M.(1966). TimecourseofTEA+-inducedanamalousrectificationin

    squidgiantaxons.J.Gen.Physiol.50:491-503.

    Armstrong,C.M.andBinstock,L.(1965).Anomalousrectificationinthesquidgiant

    axoninjectedwithtetraethylammoniumchloride.J.Gen.Physiol.48:859-872.

    Tasaki,I.andHagiwara,S.(1957).Demonstrationoftwostablepotentialstatesinthe

    squid

    giant

    axon

    under

    tetraethylammonium

    chloride.

    J.

    Gen.

    Physiol.

    40:859-885.

    18.

    Hypothesis

    Increasing

    the

    external

    calcium

    concentration

    will

    block

    the

    occurrence

    of

    the

    actionpotentialbecausethiswillreducethedifferenceinthetimeconstantofsodiumand

    potassiumactivationwhichisresponsiblefortheinitiationoftheactionpotential.

    19.

    Hypothesis

    Increasing

    the

    external

    concentration

    of

    potassium

    will

    decrease

    the

    refractory

    period;decreasingthisconcentrationwilllengthentherefractoryperiod.

    20.

    Hypothesis

    Increasing

    the

    external

    concentration

    of

    sodium

    will

    decrease

    the

    refractory

    period;decreasingthisconcentrationwilllengthentherefractoryperiod.

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    21.

    Hypothesis

    Absolute

    and

    relative

    refractory

    periods

    are

    decreased

    by

    increasing

    the

    rate

    constants

    for

    sodium

    inactivation

    and

    for

    potassium

    activation.

    22. HypothesisRepolarizationcannotoccurifthepotassiumactivationrateconstantiszero.

    23. HypothesisThethresholdoftheactionpotentialtoabriefpulseofcurrentdecreasesas

    theexternalpotassiumcurrentisincreased.

    24.

    The

    Hodgkin-Huxley

    model

    with

    default

    parameters

    does

    not

    exhibit

    accommodation.

    Hy

    pothesis

    Accommodation

    occurs

    if

    the

    leakage

    conductance

    is

    increased.

    25. TheHodgkin-Huxleymodelwithdefaultparametersdoesnotexhibitaccommodation.Hy

    pothesisAccommodationoccursifthepotassiumconductanceisincreased.

    26. HypothesisIncreasingtheleakageequilibriumpotentialwillblocktheactionpotential.

    27.

    Hypothesis

    The

    effect

    of

    the

    changes

    in

    concentration

    of

    sodium

    ions

    on

    the

    action

    po

    tential

    of

    the

    giant

    axon

    of

    the

    squid

    can

    be

    accounted

    for

    by

    the

    Hodgkin-Huxley

    model.

    Articles

    in

    the

    literature

    should

    be

    consulted

    for

    this

    project:

    HodgkinA.L.andKatz,B.(1949).Theeffectofsodiumionsontheelectricalactivity

    of

    the

    giant

    axon

    of

    the

    squid.J.Physiol.108:37-77.

    Baker,P.F.,Hodgkin,A.L.,andShaw,T.I.(1961).Replacementoftheprotoplasmof

    agiantnervefibrewithartificialsolutions.Nature190:885-887.

    28.

    Hypothesis

    In

    response

    to

    rectangular

    pulses

    of

    current,

    the

    rheobase

    of

    the

    strength-

    duration

    relation

    increases

    as

    temperature

    increases.

    29. HypothesisAnincreaseintemperatureresultsinadecreaseinthedurationoftherefrac

    toryperiod.

    30. HypothesisThethresholdmembranepotentialatwhichtheHodgkin-Huxleymodelpro

    ducesanactionpotentialinresponsetoabriefpulseofcurrent isequal to themembrane

    potentialforwhichthelinearizedHodgkin-Huxleyequationshaveunstableeigenvalues.

    31.

    Application

    of

    a

    long-duration

    constant

    current

    to

    the

    Hodgkin-Huxley

    model

    produces

    a

    train

    of

    action

    potentials.

    Hypothesis

    The

    frequency

    of

    the

    action

    potentials

    increases

    withincreasingcurrentamplitude.

    32.

    Application

    of

    a

    long-duration

    constant

    current

    to

    the

    Hodgkin-Huxley

    mod