Transcript Document

Osmotic Pressure
Jim Parker
Osmotic Pressure = Pressure to stop inward flow of
solvent into volume
• Pressure proportional to concentration
• P=ckT
van’t Hoff relation
where c = N / V
Same form as Ideal Gas Law
• Osmotic Pressure
– Derive from Free-Energy F= - k T ln Z
– Similar to Ideal gas derivation
• Same constraints -- particles do not interact (internal
energies - affect chemical potentials not discussed)
• At high enough concentrations these relations break
down
– Partition function formed from all combinations of r
and p times the Boltzmann factor.
• In continuous media, sums -> integrals
•These are either gaussian integrals, constants or just L
• Z(L) = constant * V
where V = L3
–Fixed Volume
•F = - k T N ln V + constant
•P = - d F/ dV = k T N / V (ideal gas law)
– Need to find change in Free Energy / volume to
get dimensions of pressure (force / area)
– Fixed Pressure - find average L displacement of piston
Kinetic Energy of Piston
Potential Energy of gas
– Average value of thermodynamic property is
<L> = integral L x P and integral of P = 1
• In P, only 1 factor depends upon L -- exp( -fl/ kT)
• All other terms will cancel lots of terms to yield eq 7.5
• Make substitutions f = p A and L = V / A
Biological import
• Importance of osmotic pressure to cells
– Concentration of protein in cell computed from
volume fraction
– V(protein) / V(total) = N/V(total) * V(protein)/N
= c * V(1 protein molecule)
– Surface tension comparison to osmotic pressure
• Osmotic pressure = 300 Pa (from 0.12 mM protein conc)
R
Surface Tension  must
balance osmotic pressure
Therefore for Energy balance
p dV -  dA = 0
– Lysis (cell burst) when unable to balance
osmotic pressure
• For protein conc 0.12 mM, near rupture
threshold
• Salts at 1 M conc, 10,000 x stronger pressure burst without compensating mechanism
• Depletion force
– Push larger molecules together by smaller
– Volume 1R around large molecule excludes small
molecule
– Small molecule could use that volume for more
states (higher entropy)
– Thus when large molecules get close, they tend to
get closer
Depletion Force Experiment
• 0.24 micron and 0.04 micron spheres
• Circular boundary
• b & c histogram plots -- white=many observations
Osmotic Flow
– Transfer of momentum from solute to fluid
– Low Reynolds numbers of solute particles
• Negligible inertial forces
• Reynolds = v R 
– Viscous drag balanced by force on solute
– Action/reaction - viscous drag net force on
solvent
– Barrier acts in only 1 direction
Osmotic Flow
B) Pressure for solute
C) Osmotic pressure at
equilibrium (no pressure on
left)
D) Solid Line
- Pressure on left = right
- pressure gradient in
membrane --> flow to right,
- put in osmotic pressure drop,
- connect pressures with steady
gradient (quasi-steady state)
D) Reverse osmosis, push
solvent out of “dirty solution”