Cell Physiology Flashcards
Structure of phospholipid membrane
Glycerol backbone = hydrophilic
2 fatty acid tails = hydrophobic
Substances that are soluble across the lipid bilayer
Lipid-soluble substances (O2, CO2, steroid hormones)
Substances that are NOT soluble across the lipid bilayer
Water-soluble substances (H2O, Na, Cl, glucose)
Integral proteins
Anchored in the membrane via hydrophobic interactions
Peripheral proteins
NOT embedded within the membrane; NOT covalently bound to the membrane - instead interact loosely with electrostatic interactions
Tight junctions
aka zona occludens; attachments between cells
Two types of tight junctions
- tight (impermeable)
2. leaky (permeable)
Gap junctions
the attachments between cells that permit intercellular communication
Characteristics of simple diffusion
- only form of transport that is NOT carrier mediated
- downhill (down an electrochemical gradient)
- passive (does not require metabolic energy)
Diffusion equation
J = -PA(C1 - C2)
*the minus sign indicates the direction of flow is from high to low concentration
Permeability (P)
The ease with which a solute diffuses through a membrane; depends on characteristics of both the solute and the membrane
Factors that increase permeability
- increase oil/water partition coefficient of the solute–>increased solubility in the lipid membrane–>increased permeability
- decreased radius of the solute–>increases the diffusion coefficient and speed of diffusion
- decreased membrane thickness–>decreased diffusion distance
Features of solutes with the highest permeability in lipid membranes
- small
2. hydrophobic/lipophilic
Two types of carrier mediated transport
- facilitated diffusion
2. primary and secondary active transport
Facilitated diffusion
Diffusion down a gradient, just via a transporter
Three general characteristics of carrier-mediated transport
- stereospecificity
- saturation
- competition
Characteristics of facilitated diffusion
- downhill
- passive
- more rapid than simple diffusion
Example of facilitated diffusion
glucose transport in muscle and adipose tissue
Characteristics of primary active transpot
- uphill (against an electrochemical gradient)
2. requires direct input of metabolic energy in the form of ATP
Examples of primary active transport
- Na-K-ATPase (3Na/2K)–>provides energy in the terminal bond of ATP
- Ca2+-ATPase (Ca2+ pump)
- H-K-ATPase (proton pump
Specific inhibitors of Na-K-ATPase
Cardiac glycoside drugs:
- ouabain
- digitalis
Location of the calcium pump
- sarcoplasmic reticulum
- endoplasmic reticulum
- cell membranes
Location of the proton pump
- gastric parietal cells
2. renal alpha-intercalated cells
Characteristics of secondary active transport
- transport of 2 or more solutes is coupled
- one of the solutes (usually Na) is transported downhill to provide energy for the uphill transport of the other solute(s)
- metabolic energy is provided indirectly
Effect of inhibition of Na-K-ATPase on secondary active transport
it inhibits secondary active transport because you won’t get any energy produced from moving Na in that direction
Cotransport
= symport; solutes move in the SAME direction across the membrane
Examples of cotransport
- Na-glucose cotransport
2. Na-K-2Cl cotransport
Locations of Na-glucose cotransport
- small intestines
2. renal early proximal tubule
Locations of Na-K-2Cl cotransporter
- renal thick ascending limb
Countertransport
= exchange/antiport; solutes move in OPPOSITE directions across the cell membrane
Examples of countertransport
- Na-Ca2+ exchange
2. Na-H exchange
MOA of Na-glucose cotransport
glucose is transported uphill (into the cell); Na is transported down hill (into the cell) - energy comes from moving Na downhill
*NOTE: inhibition of the Na-K-ATPase will inhibit Na-glucose cotransport
MOA of the Na-Ca2+ cotransport /exchange
Ca moves uphill from low intracellular Ca to high extracellular Ca; Na and Ca move in opposite directions across the cell membrane; energy comes from moving Na downhill (into the cell)
Osmolarity
The concentration of osmotically active particles in a solution (Osm/L)
Osmolarity equation
osmolarity = g x C g = the number of particles in solution (Osm/mol) C = concentration (mol/L)
Example of how to count the number of particles in solution (g)
NaCl = 2; glucose = 1
van’t Hoff’s law
= the equation used to calculate osmotic pressure; the osmotic pressure depends on the concentration of osmotically active particles
Equation = pi = g x C x RT
pi = osmotic pressure (mmHg or atm)
g = number of particles in solution (osm/mol)
C = concentration (mol/L)
R = gas constant (0.082 Latm/molK
T = absolute temperature (K)
Example of osmotic pressure increasing
Osmotic pressure increases as the solute concentration increases; a solution of 1 M CaCl2 has a HIGHER osmotic pressure than a solution of 1 M KCl because the number of osmotically active particles is HIGHER in the former
Colloid osmotic pressure
= oncotic pressure = the osmotic pressure created by proteins (e.g. plasma proteins)
Reflection coefficient
Epsilon; a number between zero and one that describes the ease with which a solute permeates a membrane
Reflection coefficient = 1
= the solute is impermeable
–>retained in the original solution–>creates an osmotic pressure–>causes water flow
Example: serum albumin
Reflection coefficient = 0
= the solute is completely permeable
–>will NOT exert an osmotic effect–>will NOT cause water flow
Example: urea = an ineffective osmole
Effective osmotic pressure
= the osmotic pressure calculated by van’t Hoff’s law multiplied by the reflection coefficient
Ion channels
Integral proteins that span the membrane and when open, permit the passage of certain ions
Features of ion channels
- selective (based on size of channel and distribution of charges that line it)
- may be open or closed
- conductance of the channel depends on the probability that the channel is open
Example of a ligand-gated channel
Nicotinic receptor for acetylcholine at the motor end plate; the ion channel opens when Ach binds to it–>permeable to Na and K–>motor endplate depolarizes
Diffusion potential
= the potential difference generated across a membrane because of a concentration difference of an ion
Features of diffusion potential
- size of diffusion potential - depends on the size of the concentration gradient
- sign of the diffusion potential - depends on whether the diffusing ion is positively or negatively charged
- created by diffusion of VERY FEW ions–>do NOT result in changes in concentration of the diffusing ions
Equilibrium potential
= the potential difference that would exactly balance (oppose) the tendency for diffusion down a concentration difference
Electrochemical equilibrium
= the chemical and electrical driving forces that act on an ion are equal and opposite = no further net diffusion of ions occurs
Nernst equation
= equation used to calculate the equilibrium potential at a given concentration difference of a permeable ion across a cell membrane; tells us at what potential would the ion be at electrochemical equilibrium
Intuitive approach to determine if the sign for the equilibrium potential is correct
intracellular Na = 15mM vs. extracellular Na = 150mM
The Na is HIGHER in the extracellular fluid than the intracellular fluid–>Na ions will diffuse from the extracellular to the intracellular space, making the INSIDE of the cell positive, so Ena = +65mV
movement into the cell = +
Approximate values for equilibrium potentials in nerve and skeletal muscle
Ena = +65mV Eca = +120mV Ek = -85mV Ecl = -85mV *NOTE: the positive ions that have higher extracellular concentrations will have a POSITIVE equilibrium potential; the positive ions that have lower extracellular concentrations and will move OUT of the cell will have a negative into cell positive ion = + out of cell positive ion = -
Driving force on an ion
= the difference between the actual membrane potential (Em) and the ion’s equilibrium potential (calculated with the Nernst equation); i.e. the difference between the actual membrane potential and what the ion would “like” the membrane potential to be (= at its equilibrium potential)
Current flow
= occurs if there is a a driving force on the ion AND the membrane is permeable to that ion
Direction of flow
= same as the direction of the driving force
Factors determining the magnitude of current flow
- size of driving force
2. permeability of the ion
Resting membrane potential
= the measured potential difference across the cell membrane; expressed as the intracellular potential relative to the extracellular potential; example: the resting membrane potential of -70mV = 70mV with the cell NEGATIVE compared to the extracellular space
Ion with the highest permeability
= the ion whose equilibrium potential the membrane potential is closest to; example: the resting membrane potential of a nerve = -70mV, which is closer to the K+ equilibrium potential of -85 than Na of +65, therefore, at rest, the never membrane is MORE PERMEABLE to K+ than to Na+
Depolarization
= makes the membrane potential less negative (i.e. the inside of the cell becomes LESS NEGATIVE due to the influx of positive ions)
Hyperpolarization
= makes the membrane potential MORE NEGATIVE (the inside becomes more negative due to the efflux of positive ions)
Inward current
= the flow of positive charge into the cell–>depolarization of the cell membrane
Outward current
= the flow of positive charge out of the cell–>hyperpolarization of the cell membrane
Threshold
= the membrane potential at which the action potential is inevitable; where the net inward current becomes larger than the net outward current
Features of action potentials (3)
- stereotypical size and shape
- are propagating
- are all-or-none
Ionic basis of nerve action potentials
At rest, inactivation gates for Na are open (opened by repolarization of the membrane), but the activation gates are closed (only open at the time of depolarization)