2. ORGANIZATION OF THE CELL
• cells consist of a nucleus surrounded by a nuclear
membrane, and a cytoplasm surrounded by plasma
membrane.
• cellular components (protoplasm) are made of :
1- water
2- Ions
3- proteins
4- lipids
5- carbohydrates
3. Cell membrane
• Thin, pliable and almost entirely made of
proteins and lipids
the lipid bilayer impedes water penetration
cell membrane proteins are of two types:
integral and peripheral, these proteins
perform various functions (channels, carriers,
receptors, enzymes, controllers)
4. TRANSPORT THROUGH CELL
MEMBRANE
• The lipid bilayer prevents mixing of ECF & ICF water
and water-soluble substances cannot move freely
through it.
• lipid-soluble substances move freely through the
plasma membrane
• Water, ions and water-soluble substances are
transported through proteins (channel proteins &
carriers)
8. Simple diffusion
• Diffusion of a matter through the lipid bilayer is
determined by its lipid solubility (O2, N2 ,CO2 move
easily through the membrane)
• Water and some water-soluble substances (urea) pass
through channels “pores” in proteins that penetrate all
the way through the membrane
• Diffusion through channels is characterized by:
1-selective permeability (charge) , (size)
2-controled by opening and closing gates (voltage,
ligand)
9. • Carrier-mediated diffusion
• the rate of diffusion reaches a maximum (Vmax)
• According to Fick’s law, the rate of diffusion
depends on:
1-the magnitude of the concentration gradient
2-the permeability of the plasma membrane to a
substance.
3-the surface area of the membrane across which
diffusion takes place
4-the molecular weight of a substance
5-the distance through which diffusion takes place
Facilitated diffusion
10.
11.
12. Fig. 3-14a, p. 56
Step 1
Conformation X of
carrier (binding sites
exposed to ECF)
Molecule to be
transported binds to
carrier
Molecule to be
transported
Concentration
gradient
Plasma
membrane
Carrier molecule
(Low)
(High)ECF
ICF
13. Fig. 3-14b, p. 56
Step 2
On binding with
molecules to be
transported, carrier
changes its
conformation
Conformation X of carrier
ConformationY
of carrier
14. Fig. 3-14c, p. 56
Step 3
ConformationY of
carrier (binding sites
exposed to ICF)
Transported molecule
detaches from carrier
Direction of
transport
ECF
ICF
15. Fig. 3-14d, p. 56
Step 4
ECF
ICF
Conformation X of
carrier (binding sites
exposed to ECF)
After detachment,
carrier reverts to
original shape
18. Fig. 3-16, p. 58
Phosphorylated
conformationY
of carrier
Step 1
Phosphorylated conformationY of
carrier has high affinity for passenger.
Molecule to be transported binds to
carrier on low-concentration side.
Molecule to be
transported Step 2
Dephosphorylated conformation X
of carrier has low affinity for
passenger. Transported molecule
detaches from carrier on high-concentration side.
= phosphate
Direction of
transport
Concentration
gradient
(High)
(Low)
Dephosphorylated
conformation X
of carrier
ICF
ECF
Na+
19. Fig. 3-17, p
= Sodium (Na+) = Potassium (K+) = Phosphate
When open to the ECF, the carrier drops off Na+ on its high-concentration
side and picks up K+ from its low-concentration side
Phosphorylated conformationY
of Na+–K+ pump has high affinity
for Na+ and low affinity for K+
when exposed to ICF
When open to the ICF, the carrier picks up Na+ from its low-concentration
side and drops off K+ on its high-concentration side
Dephosphorylated
conformation X of Na+–K+
pump has high affinity for
K+ and low affinity for Na+
when exposed to ECF
ICF
ECF
20.
21.
22. Transport of big particles
- Endocytosis
- Exocytosis
- Pancytosis
23. •Basic principles of osmosis:
water diffuses from high [H2O] to
region of lower [H2O] . (Kinetics).
Osmosis
24.
25. OSMOTIC PRESSURE
•the exact amount of pressure required to stop osmosis.
•osmotic pressure is determined by the number of particles
rather than their mass.
•osmole: 1 gram molecular weight of osmotically active
solute
“ a solution having 1 osmole of solute
dissolved in each Kg of water is said to have
an osmolality of 1 osmole/Kg”
• 1 milliosmole/liter 19.3 mmHg osmotic pressure at
normal body temperature
29. Fig. 3-11, p. 53
Membrane (permeable to both water and solute)
Side 1 Side 2
Higher H2O concentration,
lower solute concentration
Lower H2O concentration,
higher solute concentration
H2O moves from side 1 to side 2
down its concentration gradient
Solute moves from side 2 to side 1
down its concentration gradient
• Water concentrations equal
• Solute concentrations equal
• No further net diffusion
• Steady state exists
Side 1 Side 2
= Water molecule
= Solute molecule
H2O
Solute
30. Fig. 3-12, p. 54
= Water molecule
= Solute molecule
Membrane (permeable to H2O but impermeable to solute)
Higher H2O concentration,
lower solute concentration
Lower H2O concentration,
higher solute concentration
H2O moves from side 1 to side 2
down its concentration gradient
• Water concentrations equal
• Solute concentrations equal
• No further net diffusion
• Steady state exists
Solute unable to move from side 2 to
side 1 down its concentration gradient
Side 1 Side 2
Side 1 Side 2
Original
level of
solutions
H2O
31. Fig. 3-13, p. 54
= Water molecule
= Solute molecule
Membrane (permeable to H2O but impermeable to solute)
Pure water Lower H2O concentration,
higher solute concentration
H2O moves from side 1 to side 2
down its concentration gradient
Solute unable to move from side 2 to
side 1 down its concentration gradient
Side 1 Side 2
Side 1 Side 2
Original
level of
solutions
H2O
• Water concentrations not equal
• Solute concentrations not equal
• Tendency for water to diffuse by
osmosis into side 2 is exactly
balanced by opposing tendency for
hydrostatic pressure difference to
push water into side 1
• Osmosis ceases
• Opposing pressure necessary to
completely stop osmosis is equal
to osmotic pressure of solution
Hydrostatic
(fluid)
pressure
difference
Osmosis
Hydrostatic
pressure
34. •Osmotic pressure : pressure that prevents
the osmosis .
•The higher the osmotic pressure of a
solution, the lower its [H2O] but the higher its
[solute].
•According to van’t hoff’s law:
π = CRT
π= 19300 mm Hg for 1 osmole/liter at body
temp.
π(osmotic pr.) C(solute con. In osmole/liter)
R (ideal gas const.) T(absolute temp.)
35. • osmotic pr. = osmolarity(mOsm/L) X 19.3 mmHg
• the calculated value is not 100% correct due to intraionic
and intermolecular interactions between the particles and
it has to be multiplied by the “osmotic coefficient” of the
particles to reach the true value.
• the osmolarity of the body fluids is around 300 mOsm/L,
the plasma being 1mOsm/L higher because of the
osmotic effect of plasma proteins