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Diffusion and Osmosis

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Osmotic swelling is an unavoidable problem for all cells. The swelling arises from the presence of negatively-charged proteins trapped in the cytoplasm ... – PowerPoint PPT presentation

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Title: Diffusion and Osmosis


1
Diffusion and Osmosis
2
Diffusion defined
  • Migration of atoms, ions, molecules or even small
    particles through random motion due to thermal
    energy
  • A particle at any absolute temperature T has an
    average kinetic energy of 3kT/2, where k is
    Bolzmanns Constant. The value of kT at 300oK is
    4.14X10-14 g/cm2/sec2. Particle size is not a
    factor in this calculation.
  • Therefore, the mean velocity of a diffusing
    particle depends on its mass, so that particles
    of different masses have different diffusion
    coefficients.

3
Diffusing particles undergo random walks
  • Because of collisions with other particles, a
    diffusing particle changes direction on a
    picosecond time scale. Therefore, individual
    particles move about randomly and tend to return
    to the same spots.
  • However, if there is a concentration gradient,
    the average number of particles moving down the
    gradient at any instant will be greater than the
    number moving up the gradient there will be a
    net flux (Jnet) of particles from the higher
    concentration toward the lower concentration.
    Therefore, it helps to think of the concentration
    gradient as a force that drives particle
    movement, even though from the point of view of
    an individual particle, all movements are random.

4
What a random movement looks like
N18,050 steps the particle has moved a
distance made good of 196 step lengths
5
Ficks Law of Diffusion
  • The net flux of a solute S in one dimension x is
    described by the Fick Eq.as the product of the
    concentration gradient (dCs) and the diffusion
    coefficient for that solute (Ds).
  • Jnet -Ds(dCs/dx)
  • The units of J are moles/cm2sec and of the
    concentration gradient, moles/cm3/cm.
  • If diffusion is occurring in a 3-dimensional
    setting, a cross-sectional area term must be
    inserted into the equation.

6
Net movement by diffusion is rapid over short
distances, slow over long distances
  • Einstein solved the Fick Eq. to show that, on the
    average, in a interval of time t, an average
    diffusing particle will travel a distance of
    (2Dst)1/2 away from its starting point. (For the
    model particle in slide 4, this solution would
    have predicted a distance made good of 190
    steplengths)
  • So, the distance gained by diffusional motion
    increases as the square root of time, rather than
    as a direct proportion to time as in linear
    motion.
  • For a particle with Ds 2X10-5 cm2/sec,
    instantaneous velocity will average about
    566m/sec,
  • but speed made good will be much slower this
    particle will travel a distance of 1 micron in
    about 250 microsec, 10 microns in 25 msec, 100
    microns in 2.5 sec, and a meter in about a month.

7
Permeation through membranes
  • If a barrier to free diffusion is inserted into
    the system (such as a cells plasma membrane), a
    permeability coefficient replaces the term for
    the diffusion coefficient.

8
How does diffusion physics relate to physiology?
  • Delivery and removal of substances by diffusion
    sets an upper limit on cell diameter of about 100
    microns.
  • Since surface area is a term in the 3D Fick
    equation, structures that must maximize
    diffusional flux tend to show expanded surface
    area and attenuated linear dimensions. (Think of
    the anatomy of the lung or the surface of the
    intestine).

9
Osmotic flow
  • In osmosis, water diffuses along a gradient of
    water concentration that is the result of
    dilution of water by the presence of solvents
    i.e. the higher the solvent concentration, the
    lower the water concentration
  • The potential energy for water movement
    represented by a solute concentration gradient is
    given by the van tHoff Equation
  • Posm MRT
  • Where the units of Posm are atmospheres, M is the
    osmolality of the solution, R is the gas
    constant, and T is the absolute temperature.
    Generally, a correction has to be added to the
    van tHoff eq. to correct for non-ideal behavior
    of the solute.

10
Colligative properties of solutions
  • Osmotic pressure
  • Freezing point
  • Vapor pressure or boiling point
  • Colligative means tied together.The higher the
    solute concentration, the higher the osmotic
    pressure, the lower the freezing point and the
    higher the boiling point, compared to pure water.

11
Two kinds of water potential energy
  • Osmotic force a form of chemical potential
    energy
  • Hydrostatic force a form of mechanical potential
    energy
  • These forces are interconvertible, so the net
    driving force for water between a cell and the
    extracellular solution is
  • RT (Osmcell - Osmext) (Pcell Pext)

12
Osmotic swelling is an unavoidable problem for
all cells
  • The swelling arises from the presence of
    negatively-charged proteins trapped in the
    cytoplasm
  • First, imagine that a water-permeable membrane
    separates two rigid compartments.
  • One compartment has a 150 mmolal concentration
    of NaCl.
  • The other one has 150 mEq/liter of Na and an
    equal quantity of anionic charge as protein
    however, the protein concentration is only 1
    mmolal.
  • Is there an osmotic gradient?
  • Is there a solute gradient?

13
Initial conditions
Intermediate conditions Cl- diffused down its
gradient why did Na move against its gradient?
Notice that there is now a gradient of electrical
charge this is a Donnan potential.
Now imagine water trying to move osmotically is
there a gradient of hydrostatic pressure? The
system has come into Gibbs-Donnan equilibrium
all forces are balanced.
14
Animal cells could never attain Gibbs-Donnan
Equilibrium
  • Why not? The plasma membrane cannot sustain a
    hydrostatic pressure gradient.
  • Without the evolution of some means of avoiding
    Gibbs-Donnan equilibrium, there would be no
    protein-containing cells.

15
The Na/K Pump counteracts G-D equilibration
The Na/K pump undergoes cycles in which it
spends an ATP to eject 3 Na from the cell and at
the same time to take 2 K into the cell. On the
average, this counteracts leakage of Na and K
across the membrane down their electrochemical
gradients. The bottom-line effect of this is to
make the cell effectively impermeable to NaCl.
Gibbs-Donnan equilibrium is not approached and
the cell does not swell, in spite of the presence
of protein anion (X-).
16
What if the Na/K pump stops working?
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