Physiology
Environmental Conditions Required for Life
Cellular Physiology and The Body Fluid Compartments
Total Body Water
Extracellular Fluid
Interstitial Fluid
Plasma
Intracellular Fluid
Distribution of Solutes between compartments
osmolarity
osmolality
tonicity
isotoníc
hypotonic
hypertonic
changes when water is added
Cellular Membranes
Types
Plasma Membrane
Functions
Components
Lipids
Cholesterol
Phostophlipids
Components
Glycerol-Phosphate Head
Two Fatty Acid Tails
Products
Lipid Bilayer
Fluid Mosaic Model
the phospholipids are arranged in a bilayer → creating a semi-permeable membrane
the hydrophilic phosphate heads face the aqueous solutions inside and outside the cell
the hydrophobic lipid tails are “hidden” in the center of the membrane
protein molecules of various kinds are inserted into and through the phospholipid bilayer
glycolipids and glycoproteins are formed when carbohydrates bind to proteins and lipids on the extracellular surface
Glycolipids
Sphngolipids
Products
Lipid Rafts
Components
Fatty Acid Tail
Phospho-lipid or GLycolipid Head
Carbohydrates
Glycoproteins
Membrane Proteins
Structural Classification
Integral Proteins
Extracellular Loops
Intracellular Loops
Lipid Anchored Proteins
Peripheral Proteins
Functional Classification
Membrane-Spanning Proteins
Membrane Transporters
Carrier Proteins
Uniport
Symport
Antiport
Channel Proteins
Gated
Voltage
Ligand/Chemical
Mechanically (not for ions?)
Open/"Leak"
Membrane Receptors
Functions
are part of the body’s chemical signaling system
• the binding of a receptor with its ligand usually triggers another event at the membrane
- such as activation of an enzyme
- can play an important role in some forms of vesicle transport
Structural Proteins
Functions
• connect the membrane to the cytoskeleton to maintain the shape of the cell
create cell junctions that hold tissue together, such as tight junctions and gap junctions
attach cells to the extracellular matrix by linking cytoskeleton fibers to extracellular collagen
and other protein fibers
Membrane Enzymes
Functions
catalyze chemical reactions that take place either on the cell’s external surface or just inside the cell
• enzymes attached to the intracellular surface play an important role in transferring signals from the extracellular compartment to the cytoplasm
Organelle Membranes
Functions
Physical Isolation
Regulation of Exchange with Environment
Simple Diffusion
properties
passive process
molecules move from high to low concentration.
mvmt continues until molecules are equal everywhere.
Rapid over short distances, much slower under longer ones.
related to temperature
inversely related to molecular size
can take place in an open system or across a partition separating 2 systems
rates
Fick's Law
membrane permeability
osmosis
osmotic pressure
example
Mediated Transport
Types
Facilitated Diffusion
example: Glucose
Active Transport
Primary
Na+/k+ - ATPase
ca2+ - ATPase
H+ - ATPase or proton pump
H+k+ - ATPase
Secondary
Symport
Sodium Dependent Carriers
Antiport
Sodium Dependent Carriers
non sodium dependent transporters
Examples
Secondary Active Transport in the GI Tract
Absorption of AAs
for larger molecules
endocytosis
phagocytosis
pinocytosis
classifications
physical requirements
for movement through the phospholipid bilayer
transported with the aid of a membrane protein
transported by using vesicles
energy requirements
Classification
passive transport
does not require the direct input of energy
Two types
simple diffusion
Any solute will tend to uniformly occupy the entire space available to it.
This movement, known as diffusion, is a result of the spontaneous Brownian (random) movement that all molecules experience.
The net result of diffusion is the movement of substances according to their difference in concentrations, from regions of high concentration to regions of low concentration
Diffusion has the following seven properties:
diffusion is a passive process which means the energy used for molecular movement is only the kinetic energy possessed by all molecules
molecules move from an area of high concentration to an area of lower concentration
net movement of molecules continues until the concentration is equal everywhere
diffusion is rapid over short distances but much slower over long distances
diffusion is directly related to temperature
diffusion is inversely related to molecular size;
the bigger → the slower
diffusion can take place in an open system or across a partition that separates two systems
OSMOSIS AND OSMOTIC PRESSURE
OSMOSIS ACROSS A SEMIPERMEABLE MEMBRANE
Osmosis
The spontaneous movement of water across a membrane driven by a gradient of water concentration is the process known as osmosis.
Concentration
the number of particles per unit volume:
a solution with a high concentration of solutes has a low concentration of water and visa versa.
Osmosis can be viewed as the movement of water from a solution of high water concentration (low concentration of solute) toward a solution with a lower concentration of water (high solute concentration).
Osmosis is a passive transport mechanism that tends to equalize the total solute concentrations of the solutions on both sides of every membrane.
Water is able to move freely between cells and the extracellular fluid, and will distribute itself until water concentrations are equal throughout the body
the body is in a state of osmotic equilibrium.
THE MEASUREMENT OF OSMOTIC PRESSURE
The driving force for the movement of water across the plasma membrane is the difference in water concentration between the two sides of the membrane.
Osmotic Pressure
the pressure necessary to stop net movement of water across a selectively permeable membrane that separates the solution from pure water.
a concentration gradient across the membrane exist for glucose, but the membrane is not permeable to glucose
water can move across the membrane freely by osmosis, thus water moves from compartment A to dilute the more concentrated solution in compartment B
the pressure that must be exerted to exactly oppose the osmotic movement off ater into compartment B is the osmotic pressure of solution B
units of the osmotic pressure are mm Hg
DISTRIBUTION OF SOLUTES IN THE BODY FLUID COMPARTMENTS
The distribution of solutes between the extracellular and intracellular fluid is summarized in the above set of graphs.
The composition of the of the intracellular fluid (C ) is maintained by the action of various specific membrane transport proteins.
Principle among these transporters is the Na+/K+-ATPase, which converts the energy in ATP into ion and electrical gradients, which in turn can be used to drive the transport of other ions and molecules.
The composition of the plasma (P) and interstitial fluid compartments (I) of the ECF is similar because they are separated only by the capillary endothelium
, a barrier that is freely permeable to ions and small molecules.
The major difference between interstitial fluid and plasma is that the plasma contains significantly more protein (primarily albumen).
The terms osmolarity and osmolality are frequently confused and incorrectly interchanged:
osmolarity
refers to the osmotic pressure generated by the dissolved solute molecules in 1 L of solvent
measurements of osmolarity are dependent on temperature because the volume of solvent varies with temperature
osmolarity = concentration x number of dissociable particles
mOsm/L = mmol/L x number of particles/mol
example 1
one mole of glucose dissolved in enough water to create 1 liter of solution yields a 1 molar solution (1 M),
glucose does not dissociate therefore
1 M glucose x 1 particle per glucose molecule = 1 OsM glucose
Example 2
add NaCl which dissociates into two ions
thus 1 mole NaCl results in 2 moles of particles
one of Na and one of Cl = a 2 Osm NaCl
1 M NaCl x 2 ions per NaCl = 2 Osm NaCl
osmolality
number of molecules dissolved in 1 kg of solvent (water)
independent of temperature
expressed as osmoles of solute/Kg H2O
usually used in clinical situations because it is easy to estimate people’s body water content by weighing them
TONICITY DEPENDS ON THE RELATIVE CONCENTRATION OF NONPENTRATING SOLUTES
Tonicity
the physiological term used to describe a solution and how that solution affects cell volume
; it describes the cell volume once the cell has come to equilibrium with the solution
key in predicting tonicity is knowing the relative concentrations of nonpenetrating solutes in the cell and in the solution:
if the cell has a higher concentration of nonpenetrating solutes than the solution, there will be net movement of water into the cell
the cell swells and the solution is hypotonic (figure a)
if the cell has a lower concentration of nonpenetrating solutes than the solution, there will be net movement of water out of the cell
the cell shrinks and the solution is hypertonic
if the concentrations of nonpenetrating solutes are the same in the cell and the solution, there is no net movement of water at equilibrium
the solution is isotonic to the cell, no change in intracellular volume (figure b)
The differences between tonicity and osmolarity are
osmolarity describes the number of particles dissolved in a volume of solution and it has units (ex. osmoles/liter);
tonicity has no units and is only a comparative term
osmolarity can be used to compare two solutions, and the relationship is reciprocal (solution A is hyperosmotic to solution B; therefore , solution B is hyposmotic to solution A);
tonicity always compares an extracellular solution to the intracellular fluid
osmolarity alone does not predict what happens to a cell when placed in a solution
tonicity by definition predicts what happens to cell volume when the cell is placed in the solution
ECF AND ICF CHANGES WHEN PURE WATER IS ADDED
Despite the different compositions of ICF and ECF, the total solute concentration (osmolality) of these two fluid compartments is normally the same
ICF and ECF are in osmotic equilibrium because of the high water permeability of cell membranes, which does not permit an osmolality difference to be sustained
If the osmolality changes in one compartment, water moves so as to restore a new osmotic equilibrium
The distribution of water between intracellular and extracellular compartments changes in a variety of circumstances.
In the above figures
the y-axis represents total solute concentration or osmolality (mOsm/Kg H2O)
the x-axis the volume (L)
the area of a box gives the amount of solute present in a compartment
note that the height of the boxes is always equal, because osmotic equilibrium (or equal osmolalities) has been achieved
the dashed lines indicate the normal condition, and the solid lines the situation after a new osmotic equilibrium has been attained
In the normal situation (figure A)
⅔ of total body water (28 L) is in the ICF
⅓ in the ECF (14 L)
the osmolality of both fluids is 285 mOsm/Kg H2O.
When 2 L of pure water is added to the ECF (figure B)
plasma osmolality is lowered and water moves into the cell compartment along the osmotic gradient
the entry of water into the cells causes them to swell (water is therefore hypotonic)
the intracellular osmolality falls until a new equilibrium (solid lines) is achieved
the new total body water volume is 44 L
no solute was added, so the new osmolality at equilibrium is 272 mOsm/Kg H2O
⅔ of the added water ends up in the intracellular compartment and ⅓ stays in the ECF
ECF AND ICF CHANGES WHEN AN ISOTONIC AND HYPERTONIC SOLUTION ARE ADDED
Since isotonic saline is isosmotic to plasma or ECF by definition, when 2.0 L of isotonic saline (0.9% NaCl solution) is added to the ECF (figure C), there is no change in cell volume
Therefore all of the isotonic saline is retained in the ECF and there is no change in osmolality.
The effects of infusing intravenously 1.0 L of a 5% NaCl solution (osmolality about 1580 mOsm/Kg H2O) are shown in figure “D”:
all the salt stays in the ECF which creates a hypertonic environment for the cells
water leaves the cells leaving behind the solutes making the ICF more concentrated
a new equilibrium will be established, with a final osmolality higher than normal (about 315 mOsm/Kg H2O) but equal inside and outside of the cells
the addition of a hypertonic saline solution to the ECF increased the volume in the extracellular compartment in part because of water loss from the intracellular compartment
the final ECF volume is increased by 3.7 L
1 L from the intravenous infusion
2.7 L from the intracellular comparment
People normally stay in a stable water balance
that is, water input and output are equa
Body fluid volumes and plasma osmolality are kept constant by three major aspects to control water balance:
arginine vasopressin (antidiuretic hormone, ADH
excretion of water by the kidneys
drinking habits and the perception of thirst
facilitated diffusion
THE PASSIVE MOVEMENT OF SOLUTES ACROSS A CELL MEMBRANE
DIFFUSION THROUGH A LIPID BILAYER
The diffusion of a solute across a cell membrane is driven by the difference in the concentration on the two sides of the membrane;
the solute molecules move randomly by Brownian movement.
Initially, random movement from left to right across the membrane is more frequent than movement in the opposite direction because there are more molecules on the left.
This results in a net movement of solute from left to right across the membrane until the concentration of solute is the same on both sides (figure on the left).
Diffusion across a membrane has no preferential direction; it can occur from the outside of the cell toward the inside or visa versa.
THE RATE OF SOLUTE TRANSPORT BY SIMPLE DIFFUSION
The graph on the right shows solute transport across a plasma membrane by simple diffusion according to concentration gradients; inside vs. outside, high to low.
The rate of solute entry increases linearly with extracellular concentration, increasing the extracellular concentration increases the gradient that drives solute entry.
The rules for simple diffusion can be combined mathematically into an equation known as Fick’s law of diffusion, a relationship that is expressed as:
Rate of diffusion = surface area x concentration gradient x membrane permeability
 membrane thickness
Membrane permeability is the most complex (variable) of the four terms in Fick’s law because several factors influence it:
the size of the diffusing molecules
the lipid-solubility of the molecule
the composition of the lipid bilayer across which it is diffusing
In most physiological systems, membrane thickness is a constant (stable); therefore Fick’s law equation can be rearranged to:
Diffusion rate = concentration gradient x membrane permeability
 Surface area
active transport
requires the input of energy from some outside source, such 
 as the high-energy phosphate bond of ATP
Communication between the Cell and Its Environment
Structural Support
Membrane Potentials
Resting Membrane Potential
Electrochemical Potential Difference
Electrical Potential Difference
Separation of CHarges
In theory, a cell can be filled with neutral molecules that dissociate into positive and negative ions
The cell can be placed in a solution that is also electrically neutral and contains the same types of positive and negative ions
The phospholipid bilayer of the artificial cell, like the bilayer of a real cell, acts as an insulator to prevent free movement of ions between the intracellular and extracellular compartments.
Water can freely cross this cell membrane, making the extracellular and intracellular osmotic pressures equal.
This makes the system shown in figure (a) to be in osmotic, chemical, and electrical equilibrium.
An active transport carrier is now inserted into the membrane and uses energy to move positive ions out of the cell against their concentration gradient shown in figure (b).
. as soon as the first positive ion leaves the cell, the electrical equilibrium between the ECF and ICF is disrupted
• the cell’s interior has a net charge of -1 while the cell’s exterior has a net charge of +1 (absolute charge)
the input of energy to transport ions across the membrane has created an electrical gradient, a difference in the net charge between two regions
In living systems, electrical gradients are measured on a relative scale rather than an absolute scale because we cannot measure electrical charge as numbers of electrons gained or lost.
. On an absolute charge scale, the extracellular fluid (ECF) would be at +1 and the intracellular fluid (ICF) would be at -1.
Physiological measurements are always on a relative scale, on which the ECF is assigned a value of zero. This shifts the scale to the left and gives the inside of the cell a relative charge of -2 (figure c).
When positive ions are pumped out of the cell this creates a separation of charge known as a dipole layer.
at rest, the cell has an excess of positive charges on the outside of the membrane and an excess of negative charges on the inside
this separation of charge is maintained because the lipid bilayer acts as a barrier to the diffusion of ions
. the charge separation gives rise to an electrical potential difference across the membrane - The resting membrane potential
- it is directly proportional to the charge separation across the membrane
Principle of LEctric Neutrality
Creation of the Electric Capacitator
an incredibly small number of ions need to be transferred through the membrane to establish a membrane potential of -90 mV
this allows for very rapid changes in the membrane potential
less energy is required to reestablish normal ion concentrations when disrupted
Chemical Potential Difference
Nernst Potential
Nernest Equation
EMF = +/- 61 xlog (conc inside)/(Conc outside)
Ion Potentials
Potassium
. in a cell permeable only to K+ the resting membrane potential is generated by the efflux of K+ down its concentration gradient (figure A)
the continued efflux of K+ builds up an excess of positive charge on the outside of the cell and leaves behind on the inside an excess of negative charge (figure B)
this buildup of charge acts to impede the further efflux of K+, so that eventually an equilibrium is reached
when the electrical and chemical driving forces are equal and opposite, this is known as the equilibrium potential
Effects of Inserting Potassium Leak Channels into a theoretical cell
The artificial cell in figure (a) has a membrane that is impermeable to ions and large negatively charged proteins, represented by Pr-.
The cell is placed in a solution of Na+ and Cl-. Both the cell and the solution are electrically neutral, and the system is in electrical equilibrium.
However, it is not in chemical equilibrium:
there are concentration gradients for all four types of ions in the system
all the ions would all diffuse down their respective concentration gradients if they could cross the cell membrane
A potassium ion leak channel is inserted into the cell membrane and potassium leaks out of the cell because of the concentration gradient (figure b):
as K+ leaves the cell, the negatively charged proteins (Pr-) are unable to follow which results in a gradual build up of a negative charge on the inside of the cell
if only the force acting on K+ were the concentration gradient, K+ would leak out until he K+ concentration inside the cell equaled the K+ concentration outside
the loss of positive ions from the cell creates an electrical gradient
Because opposite charges attract each other, the negative proteins inside the cell try to pull K+ back into the cell (figure c).
When the electrical force attracting K+ into the cell becomes equal in magnitude to the chemical concentration gradient driving K+ out of the cell, there is an equilibrium potential generated.
Calculating the Electrochemical Equilibrium for Potassium Ions
The Nernst equation reveals that at an electrical potential difference (EA - EB) of -60 mV, K+ is in electrochemical equilibrium; K+ tends to move from side B to side A due to the electrical potential difference, which counteracts the tendency for K+ to move from side A to side B due to the concentration difference.
Note that an electrical potential difference of about 60 mV is required to balance a 10-fold concentration difference of a univalent ion (this is a useful rule of thumb to remember).
Sodium
The same artificial cell model used in the previous page (K+, Pr-, and Na+ inside; Na+ and Cl- outside) is now used to explain the effects of making the membrane only permeable to Na+.
Because Na+ is more concentrated outside the cell, some Na+ moves into the cell and accumulates there.
meanwhile, Cl- left behind in the extracellular fluid gives that compartment a negative charge
this imbalance creates an electrical gradient that tends to “pull” Na+ back out of the cell
when the Na+ concentration is 150 mM outside and 15 mM inside, the equilibriumpotential for Na+ is about +60 mV
the concentration gradient moving Na+ into the cell is exactly opposed by a positive membrane potential of +60 mV
Normal Ion Concentraions
Potassium
Extracellular = 5nM (bw 3-5nM)
Intracellular = 150 nM
Eion at 37degrees = -90mV
Sodium
Extracellular = 145nM (135-145)
Intracellular = 15nM
Eion at 37degrees = +60mV
Chloride
Extracellular = 108nM (bw 100-108nM)
Intracellular = 10 nM (5-15)
Eion at 37degrees = -63mV
Calcium
Extracellular = 1 mM
Intracellular = 0.0001 nM
Diffusion Potentials (no active transport)
Electrical potentials exist across the membranes of essentially all cells of the body. The above figure illustrates the generation of the equilibrium potential for both potassium and sodium ions, there is no active transport.
. the establishment of an equilibrium potential across a cell membrane, caused by potassium ions diffusing from inside the cell to the outside through a membrane selectively permeable only to potassium (shown in figure A)
the equilibrium potential for potassium is -94 mV, this is the voltage required at the inside surface of the membrane for the net diffusion of potassium tobe zero. - the electrical gradient force is equal but opposite to the chemical gradient force
the establishment of an equilibrium potential when the membrane is permeable to only to sodium ions is shown in figure B
• the equilibrium potential for sodium is +61 mV, this is the voltage required at the inside surface of the membrane for the net diffusion of sodium to be zero; the electrical gradient force is equal but opposite to the chemical gradient force
note that the internal membrane potential is negative when potassium ions diffuse out and positive when sodium ions diffuse in because of the opposite concentration gradients of these two ions
Three factors affecting diffusion potentials
the polarity of the electrical charge of each ion
the permeability of the membrane (P) to each ion
the concentrations (C) of the respective ions on the inside (i) and outside (o)
Golfman-Hodgkins-Katz Equation
Thus the following formula, called the Goldman-Hodgkin-Katz equation, gives the calculated membrane potential on the inside of the membrane when the membrane is permeable to more than one univalent ion:
EMF (mV) = log CNa+i PNa+ + CK+i PK+ + CCl-o PCl-
CNa+o PNa+ + CK+o PK+ + CCl-i PCl-
The importance and meaning of the Goldman-Hodgkin-Katz equation are
sodium, potassium, and chloride ions are the ions most importantly involved in the
development of the membrane potential
the degree of importance of each of the ions in determining the voltage is proportional to the membrane permeability for that particular ion
the resting membrane potential will be primarily determined by the most permeable ion and the voltage will be closest to the electrical potential of that ion
the permeability of the membrane to potassium is about 100 times greater as to sodium
- using this value in the Goldman equation gives an internal membrane potential of -86 mV, which is near to the potassium potential shown above
a positive ion concentration gradient from inside the membrane to the outside causes electronegativity inside the membrane
the permeabilities of the sodium and potassium channels undergo rapid changes during conduction of an action potential
Na+/K+ - ATPase Pump
Functions
The pump counterbalances the tendency of sodium ions to enter the cell passively and the tendency of potassium ions to leave passively.
It maintains a high intracellular potassium concentration, which is necessary for protein synthesis.
It also plays a role in the resting membrane potential by maintaining ion gradients which are required for the ion “leak” channels to function.
Mechanisms
Binding of intracellular Na+ and phosphorylation by adenosine triphosphate (ATP) inside the cell may induce a conformational change that transfers Na+ to the outside of the cell (steps 1 - 3).
Subsequent binding of extracellular K+ and dephosphorylation return the protein to its original form and transfer K+ into the cell.
During one cycle, three Na+ are exchanged for two K+, and one ATP molecule is hydrolyzed to ADP and phosphate (Pi), illustrated in steps 4 - 5 above.
The fact that the number of ions exchanged is not equal, a net movement of positive ions out of the cell occurs creating positivity outside the cell and leaves a deficit of positive ions inside the cell; that is, it causes negativity on the inside.
The sodium-potassium pump is said to be an “electrogenic pump” because it creates an electrical potential across the cell membrane as it cycles, adding to its influence on the resting membrane potential.
Comparison of Resting Membrane Potential with Pump Added to Membrane
the resting membrane potential generated when the membrane is onlypermeable to potassium ions = -94 mV
this occurs when the [K+]i = 140 mEq/L and [K+]o = 4 mEq/L
the resting membrane potential generated when the membrane is permeable to both sodium ions (+61 mV) and potassium ions (-94 mV) = -86 mV
this occurs when the [Na+]i = 14 mEq/L and [Na+]o = 142 mEq/L
- the ratio is: [Na+]i / [Na+]o = 0.1
this occurs when the [K+]i = 140 mEq/L and [K+]o = 4 mEq/L
- the ratio is: [K+]i / [K+]o = 35.0
the resting membrane potential generated when the membrane is permeable to both sodium ions (+61 mV) and potassium ions (-94 mV) plus pumping of both of these ions by the Na+/ K+ -ATPase pump = -90 mV
Balance of Ion Exchange
Conditions Required for Resting Membrane Potential
Conditions Required for Actional Potential in the Refractory Period
Measuring Membrane Potential Difference
Equipment
Electrodes/Micropipettes
Voltemeter
REcording Electrode
Reference Electrode
CHart Recorder
Reading the Measurement
Variability in Resting Membrane Potentials across different Tissues
Smooth Muscle Cells
The smooth muscle of the gastrointestinal tract is subject to almost continual but slow electrical activity (figure on the left). This activity tends to have two basic types of electrical waves:
Slow Wave Potentials
Spike/Pacemaker Potentials
SA Nodal Cells
The membrane potential for the SA node is small and unstable (figure on the right).
The initial potential is only -50 to -70 mV because the nodal cells possess fewer K+ leak channels, which are responsible for the big, stable resting membrane potential of atrial and ventricular myocytes.
fewer active ion channels → fewer positive ions leaving the cell → more positive ions are left within the cell → resting membrane potential becomes more positive (or remains positive).
Effects of Extracellular Potassium
at normal K+ levels, subthreshold graded potentials (figure a) do not trigger action potentials, and suprathreshold graded potentials do (figure b)
if the blood K+ level is abnormally elevated, hyperkalemia (figure c), the membrane potential becomes more positive and shifts the resting membrane potential closer to threshold
this causes the cells to fire action potentials in response to smaller graded potentials
if the blood level falls too low, hyperkalemia, the resting membrane potential becomes more negative (hyperpolarized) moving farther from threshold
a stimulus of normal strength will not reach the threshold value (figure d)
Primary Hyperkalemic Paralysis and Effects on Na+ Channels
Some patients with this disorder have mutations of voltage-gated Na+ channels that result in a decreased rate of voltage inactivation, which results in longer-lasting action potentials in skeletal muscle cells and increased efflux of K+ during each action potential.
This will result in an increase in the extracellular [K+].
A pathological condition which is due to an abnormal “leakage” of intracellular potassium ions will result in an elevation in extracellular [K+] causing the resting membrane potential of the skeletal muscle cells to become more positive.
As the depolarization of cells increases, the cells become refractory because of inactivation of the voltage-gated Na+ channels (the inactivation gates are closed due to the less negative membrane potential).
Consequently, the cells become unable to fire action potentials and are not able to contract in response to action potentials generated within their motor axons (paralysis).
Conditions Leading to Arrhythmias
an increase in action potential impulse pathway length, therefore it takes a longer time to travel the circuit (shown in figure above)
a decrease in action potential impulse conduction velocity
a shortening of the absolute refractory period
ACTION POTENTIALS AND THEIR CONDUCTION
TERMINOLOGY ASSOCIATED WITH CHANGESIN THE MEMBRANE POTENTIAL
If the cell’s permeability to an ion changes, the change in the cell’s membrane potential can be monitored by recording electrodes (illustrated in the above figure).
The membrane potential (Vm) begins at a steady resting value of -70 mV
When the trace moves upward (becomes less negative), the potential difference between the inside of the cell and the outside (set at 0 mV) decreases, and the cell is said to have depolarized
If the membrane potential difference is decreasing, the value of Vm is moving closer to the ground value of 0 mV and is becoming less negative.
A return to the resting membrane potential is termed repolarization.
If the membrane potential difference is increasing, the value of Vm must be moving away from the ground value of 0 mV and becoming more negative.
When the resting membrane potential moves away from the 0 mV becoming more negative, it is called hyperpolarization.
THE EFFECTS OF STIMULATION ON THE MEMBRANE POTENTIAL OF AN EXCITABLE CELL
Basically, any factor that causes sodium ions to begin to diffuse inward through the membrane in sufficient numbers will set off the automatic regenerative opening of the sodium ion channels.
This can result from
simple mechanical disturbance of the membrane
chemical effects on the membrane
passage of electricity through the membrane
The effects of successively applied stimuli of progressive strength are shown above
a very weak stimulus may not be able to produce any change in the resting membrane potential
at point “A” a weak stimulus causes the membrane potential to change from -90 mV to -85 mV, but this change is not sufficient for the automatic regenerative processes of the action potential to develop

at point “B”, the stimulus is greater but the intensity is still not enough to excite the cell membrane
the stimulus is strong enough to disturb the membrane potentially locally
these local potential changes are called acute local potentials and when they fail to elicit and action potential, they are called acute subthreshold potentials
at point “C”, the stimulus is even stronger and the local potential change barely reaches the level to elicit an action potential, called the threshold
at point “D”, the stimulus is now strong enough to increase the acute local potential change to rise to a threshold level and generate an action potential
an action potential is defined as an electrical signal that propagates over a long distance without a change in magnitude
action potentials depend on a regenerative wave of ion channels opening and closing
PHASES OF AN ACTION POTENTIAL
The action potential is a transient change in the membrane potential from its resting level (the resting membrane potential) characterized by
a gradual depolarization from the resting level to threshold
the membrane potential becomes more positive due to an influx of positive ions
a rapid rising phase - a significant influx of positive ions becomes great enough for the membrane potential to become less negative (depolarize)
this increase in the membrane potential will initiate the mechanisms responsible for the propagation of the action potential
an overshoot
the influx of positive ions may continue long enough for the 
membrane potential to become a positive value
repolarization
the efflux of positive ions out of the cell will result in the membrane potential returning back towards its resting level
afterhyperpolarization
the efflux of positive ions may continue long enough for the membrane potential to become a more negative value than its resting membranepotential
regulated membrane ion exchange (Na+/K+ pump) will return the membrane potential to its normal resting level
THE GENERATION OF AN ACTION POTENTIAL
Action potentials occur when voltage-gated ion channels open, altering membrane permeability to Na+ and K+.
The figure above illustrates the voltage and ion permeability changes that take place in one section of the membrane during the generation of an action potential.
The lower graph shows the action potential can be divided into three phases:
the rising phase (depolarization)
due to a sudden temporary increase in the cell’s permeability to Na+, causing the inside of the cell to progressively become less negative and possibly positive (> 0 mV)
an action potential begins when a graded potential reaching the trigger zone (“2” in upper figure) depolarizes the membrane to threshold (-55 mV, “3” in upper figure)
the falling phase (repolarization)
corresponds to an increase in K+ permeability
at a positive membrane potential, the concentration and electrical gradients for K+ favors movement of K+ out of the cell
as K+ moves out of the cell, the membrane potential rapidly becomes more negative, creating a falling phase of the action potential (“6” in upper figure) and moving the cell towards its resting potential
the after-hyperpolarization phase
occurs because when the falling membrane potential reaches -70 mV
the voltage-gated K+ channels have not yet closed
potassium continues to leave the cell through both voltage-gated and K+ leak channels, and the cell hyperpolarizes (“7” in upper figure)
Before and after the action potential (“1” and “9” in upper figure), the cell membrane is at its resting membrane potential of -70 mV.
THE STATES OF Na+ AND K+ CHANNELS CORRELATEDWITH THE COURSE OF AN ACTION POTENTIAL
As discussed earlier, the depolarizing and repolarizing phases of the action potential can be explained by the relative changes in membrane conductance (permeability) to sodium and potassium ions
During the rising phase, the cell membrane becomes more permeable to sodium;
as a consequence, the membrane potential begins to shift more towards the equilibrium potential for sodium
However, before the membrane potential reaches ENa, sodium permeability begins to decrease and potassium permeability increases
This change in membrane conductance again drives the membrane potential towards EK, accounting for repolarization of the membrane.
The action potential can be viewed in terms of the flow of charged ions through selective ion channels as illustrated above:
. figure “A” shows the resting membrane potential with both Na+ and K+ voltage-gated ion channels closed (inactive but excitable)
the cell membrane is in a “resting state” with no ion exchange through the voltage--gated channels
figure “B” shows that during the depolarization phase of the action potential, the voltage-gated Na+ channels are activated (open)
opening of the activation gate allows sodium ions to flow into the cell which results in depolarization
the potassium channels open more slowly and, therefore, have not yet responded to the depolarization
the potassium channels open more slowly and, therefore, have not yet responded to the depolarization
figure “D” shows that during the after-hyperpolarization , the sodium channels are closed and the potassium channels remain in their active state
the K+ channels will close and the Na+ channels will become excitable with the membrane potential returning to its resting level
note the K+ channels have no inactivated state
ACTION POTENTIAL REFRACTORY PERIODS
The explosive depolarizing phase of the action potential may be compared to a chemical explosion.
A chemical explosion requires a critical mass of material
the spike of the action potential can be generated only if a critical number of Na+ channels are recruited (activated),
this is the threshold value.
When a cell is partly depolarized, the pool of excitable voltage-gated Na+ channels is reduced
consequently, a stimulus may not be able to recruit a sufficient number of Na+ channels to generate an action potential
Voltage inactivation of Na+ channels partially accounts for important properties of excitable cells, such as the refractory periods.
During much of the action potential, the membrane is completely refractory (unexcitable) to further stimulation.
This means that no matter how strongly the cell is stimulated, it is unable to fire a second action potential
this unresponsive state is called the absolute refractory period.
The cell is refractory because most of its Na+ voltage-gated channels are inactivated and cannot be reopened until the membrane is repolarized.
During the latter part of the action potential, the cell is able to fire a second action potential, but a stronger-than-normal stimulus is required
this is called the relative refractory period
Early in the relative refractory period, before the membrane potential has returned to the resting potential level, some Na+ voltage-gated channels are becoming excitable while others remain inactivated thus requiring a stronger stimulus to open the critical number of Na+ channels needed to trigger an action potential (threshold)
The resetting of the inactivation gate determines when the absolute refractory period ends and the relative refractory period begins.
Throughout the relative refractory period, the conductance of K+ is elevated, which opposes depolarization of the membrane adding to the refractoriness.
A single channel during a phase in the above figure means that the majority of channels are in this state.
Where more than one channel of a particular type is shown, the population is split between the states.
ION EXCHANGE IN A CARDIAC MUSCLE CELL
Note the complexity of ion exchange that is occurring during a ventricular electrical action potential. There is an incredible degree of balancing the chemical and electrical gradients for each ion to achieve the desired results.
TYPICAL TRANSMEMBRANE ACTION POTENTIALSOF VARIOUS CARDIAC MUSCLE CELLS
The parts of the heart normally beat in an orderly sequence: contraction of the atria is followed by contraction of the ventricles, and during diastole all four chambers are relaxed.
The heart beat originates in a specialized cardiac conduction system and spreads via this system to all parts of the myocardium.
The structures that make up the conduction system are the
sinoatrial node (SA node),
the internodal atrial pathways
the atrioventricular node (AV node)
the bundle of His and its branches
and the Purkinje system
The transmembrane action potentials along with the correlation to the extracellular electrical activity (ECG) are shown in the figure above.
VARIOUS CHEMICALS CAN INACTIVATE THE VOLTAGE-GATED Na+ AND K+ CHANNELS
tetrodotoxin (TTX)
The ovaries of certain species of puffer fish, also known as blowfish, contain tetrodotoxin (TTX) which is one of the most potent poisons known.
It binds to the extracellular side of the voltage-gated Na+ channels causing inactivation of the channel (blocks the activation gate), therefore no action potentials can be generated in nerve and/or muscle fibers.
Raw puffer fish is a highly prized Japanese food dish. Connoisseurs of puffer fish enjoy the tingling numbness of the lips that is caused by very small amounts of TTX present in the flesh.
What are the possible causes for this sensation?
Sushi chefs are trained to remove the ovaries safely and are licensed by the government. Nevertheless, several people die each year from eating improperly prepared puffer fish.
What are the possible causes of death from ingesting TTX?
Saxitoxin
is another voltage-gated Na+ channel blocker
Saxitoxin is produced by red dinoflagellates that are responsible for the so-called “red tide”.
Shellfish eat the dino-flagellates, and saxitoxin becomes concentrated in their tissue.
Shellfish eat the dino-flagellates, and saxitoxin becomes concentrated in their tissue.
What could be the possible causes of death?
Tetra ethylammonium (TEA+)
blocks the voltage-gated K+ channels by entering the channel from the cytoplasmic side and completely blocks the membrane channel.
What effect will this have on the repolarization process?
What will this do to further development of generating additional action potentials (propagation of an impulse)?
What could be the possible causes of death?
GRADED POTENTIALS DECREASE IN STRENGTH AS THEY SPREAD OUT FROM POINT OF ORIGIN
Graded potentials in neurons are depolarizations that occur in the dendrites and cell body or, less frequently near the axon terminals.
These changes in membrane potential are called “graded” because their size, or amplitude is directly proportional to the strength of the triggering event.
A large stimulus causes a strong graded potential, and a weak stimulus results in a weak graded potential.
A graded potential that begins when a stimulus opens monovalent cation channels on the cell body of a neuron. Sodium ions move into the neuron, bringing in electrical energy.
The positive charge carried by the Na+ spreads as a wave of depolarization through the cytoplasm, just as a stone thrown into water creates ripples or waves that spread outward from the point of entry.
The wave of depolarization that moves through the cell is known as local current flow.
By convention, current in biological systems is the net movement of positive electrical charge.
If more Na+ channels open, more Na+ enters, and the graded potential has a higher initial amplitude.
The stronger the initial amplitude, the farther the graded potential can spread through the neuron before dying out.
The reasons that graded potentials lose strength as they move through the cytoplasm is because of two reasons:
current leak
due to some of the positive ions leaking back across the membrane due to some of the positive ions leaking back across the membrane
the membrane in the neuron cell body is not a good insulator and has open leak the membrane in the neuron cell body is not a good insulator and has open leak channels that allow positive charge to flow out of the cell
cytoplasmic resistance
to the electrical flow is provided by the cytoplasm itself, just like water creates resistance that diminishes the wave from the stone
GRADED STRENGTH OF A STIMULUS
Two neurons with three recording electrodes placed at intervals along the cell body and trigger zone are shown in this figure.
A single stimulus triggers a subthreshold graded potential, one that is below threshold by the time it reaches the trigger zone.
Although the cell is depolarized to -40 mV at the site where the graded potential begins, the current decreases as it travels through the cell body.
As a result the graded potential is below threshold by the time it reaches the trigger zone (figure a).
A stronger initial that initiates a stronger depolarization and ultimately causes an action potential stimulus (figure b).
Although this graded potential also diminishes with distance through the neuron, its higher initial strength ensures that it is above threshold at the trigger zone.
In muscle cells, the graded potential occurs at the neuromuscular junction and is referred to as the End Plate Potential (EPP), this will be discussed in more detail in the neuromuscular junction lecture.
A COMPARISON OF GRADED POTENTIALSTO ACTION POTENTIALS
THE FREQUENCY OF ACTION POTENTIAL FIRING INDICATES THE STRENGTH OF A STIMULUS
One distinguishing characteristic of action potentials is that every action potential in a given neuron or muscle fiber is identical to every other action potential in that neuron or muscle.
The transmission of information is not dependent on the strength and/or duration of the stimulus,
therefore it is not the amplitude of the action potential, but the frequency of the action potentials that results in transmitting the desired information.
A graded potential reaching the trigger zone does not usually trigger a single action potential, instead it triggers a burst of action potentials (figure b)

CONDUCTION OF AN ACTION POTENTIAL
The high speed movement of an action potential along the axon or muscle fiber is called conduction of the action potential.
In action potentials, the flow of electrical energy is a process that constantly replenishes lost energy, which is why an action potential does not lose strength over distance as a graded potential does.
The action potential that reaches the end of the axon or muscle fiber is identical to the action potential that started at the trigger zone on an axon or the site of stimulation on a muscle fiber.
At the cellular level, the depolarization of a section of an axon or muscle fiber causes positive current to spread through the cytoplasm in all directions by local current flow, as illustrated in the figure above.
Simultaneously, on the outside of the cell membranes, current flows back toward the depolarized section.
The current flow in the cytoplasm diminishes over distance as energy dissipates, and would eventually die out if not for voltage-gated channels.
The axon or muscle cell membrane is well supplied with voltage-gated Na+ channels.
Whenever depolarization reaches those channels, they open, allowing more Na+ to enter the cell reinforcing the depolarization.
This process initiates the positive feedback loop or the propagation of the action potential
Mechanism
The initiation and the sequential propagation of an action potential down an axon or across a muscle fiber is illustrated above
” a stimulus that is a graded potential above threshold that enters the trigger zone an axon or is generated at the motor endplate of the neuromuscular junction
shows that depolarization opens voltage-gated Na+ channels and Na+ enters the cell and the local area depolarizes (trigger zone or motor endplate)
shows that a positive charge from the depolarized region spreads to adjacent sections of the membrane
repelled by the Na+ that entered the cytoplasm and attracted by the negative charge of the resting membrane potential
charge of the resting membrane potential
the voltage-gated Na+ channels on the cell membrane distal to the depolarized region begin to open, allowing Na+ to enter into the cell
this starts the positive feedback loop:
depolarization opens Na+ channels
Na+ enters
causing more depolarization and opening more Na+ channels in the adjacent membrane
continuous entry of Na+ down the axon toward the axon terminal (or muscle fiber) means that the strength of the signal does not diminish as the action potential propagates itself (compare this to a graded potential)
at the peak of each action potential, the Na+ channels become inactivated and K+ channels open allowing K+ to exit the cell initiating repolarization
the section of cell membrane proximal to the active area is in an absolute refractory period
therefore the direction of propagation is in one direction
THE GENERATION OF ACTION POTENTIALS ALONG AN AXON
When talking about action potentials, it is important to realize that there is no single action potential that moves through the cell.
The action potential that occurs at the trigger zone (or motor endplate) is like the movement in the first domino of a series of dominos standing on end (top figure).
As the first domino falls, it strikes the next, passing on its kinetic energy to the second domino which then falls, and so on.
As the first domino falls, it strikes the next, passing on its kinetic energy to the second domino which then falls, and so on.
AXON DIAMETER CORRELATES TO THE SPEED OFACTION POTENTIAL CONDUCTION
After an action potential is generated, it propagates along the axon toward the axon terminal:
: it is conducted along the axon with no decrement in amplitude.
The speed with which action potentials propagate depends on two key physical parameters:
Diameter
the diameter of the axon will influence the speed of propagation because of a decrease in the resistance to electrical current flow
will influence the speed of propagation because of a decrease in the resistance to electrical current flow
diameter pipe because of their decreased resistance, large-diameter axons have less cytoplasmic resistance, thereby permitting a greater flow of ions
this increase in ion flow in the cytoplasm causes greater lengths of the axon to be depolarized, decreasing the time needed for the action potential to travel the length of the axon
the space constant (λ) determines the length along the axon that a voltage change is observed after a local stimulus is applied in this case, the local stimulus is the inward sodium current that accompanies the action potential
the larger the space constant, the farther along the membrane a voltage change is observed after a local stimulus is applied
the speed at which an action potentials are conducted, or conduction velocity, increases as a function of increasing axon diameter and concomitant increase in the space constant
Myelination
SCHWANN CELLS FORM MYELIN AROUND PERIPHERAL NERVES
The second key parameter that is involved with determining the conduction velocity of an action potential traveling down a membrane is myelin
Two different cell types in the CNS produce myelin
Schwann cells in the peripheral nervous system (PNS)
Each Schwann cell wraps around a 1.0 - 1.5 mm segment of the axon leaving tiny gaps
nodes of Ranvier
At each node a tiny section of axon remains in direct contact with the extracellular fluid and has ion channels through which current can leak
therefore the node plays an important role in the transmission of electrical signals along the axon.
SALTATORY CONDUCTION
In myelinated axons, voltage-gated Na+ channels are highly concentrated in the nodes of Ranvier where the myelin sheath is absent and are in low density beneath the segments of myelin.
When an action potential is initiated, the influx of Na+ causes the adjacent node of Ranvier to depolarize, resulting in an action potential at the node.
Action potentials are successively generated at neighboring nodes of Ranvier, therefore the action potential in a myelinated axon appears to jump from one node to the next
a process called saltatory conduction
This process results in a faster conduction velocity for myelinated than for unmyelinated axons
The conduction velocity in mammals ranges from 3 to 120 m/sec for myelinated axons and 0.5 to 2.0 m/sec for unmyelinated axons.
The reason that conduction velocity is more rapid in myelinated axons is because the mechanical process of ion channel opening slows conduction slightly.
In unmyelinated axons, channels must open all the way down the axon membrane to maintain the amplitude of the action potential.
In myelinated axons, only the nodes need Na+ channels because of the insulating properties of the myelin sheath.
As the action potential passes along myelinated segments, conduction is not slowed by channel opening.
oligodendrocytes in the central nervous system (CNS)
They wrap themselves around axons to form myelin, a substance composed of multiple concentric layers of phospholipid.
Myelin forms when these glial cells wrap around an axon, squeezing out the glial cytoplasm so that each wrap becomes two membrane layers
This myelin sheath insulates the axon and prevents the passage of ions through the axonal membrane
creates a high-resistance wall
MODES OF ACTION POTENTIAL CONDUCTION
The above figure summarizes the modes of action potential conduction in unmyelinated and myelinated axons:
Figure “A” shows the propagation of an action potential in an unmyelinated axon
by sequentially depolarizing adjacent segments of the axon, the action potential propagates or moves along the length of the axon from point to point, like a traveling wave
figure “B” shows a sheath of myelin surrounding an axon
figure “C” shows the propagation of an action potential in a myelinated
the initiation of an action potential in one node of Ranvier depolarizes the next node
jumping from one node to the next is referred to as Saltatory Conduction
DEMYELINATING DISEASES AFFECT CONDUCTION VELOCITY
The normal saltatory conduction of an action potential down a myelinated axon is illustrated in this figure.
In demyelinating diseases, the loss of myelin from vertebrate neurons can have devastating effects on neural signaling.
In the central and peripheral nervous systems, the loss of myelin slows the conduction velocity of action potentials
In addition, when ions leak out of the now-uninsulated regions of membrane, between the channel-rich nodes of Ranvier, the depolarization that reaches a node may not be above threshold and conduction may fail.

Most demyelinating diseases are either inherited or autoimmune disorders and result in the deterioration of the myelin sheath
These diseases are characterized by a variety of neurological complaints such as:
Basic Biological Concepts Involved with Maintaining Human Life
Homeostasis
Types of Control Loops
Negative Feedback System
Long Distance Control via Reflex Responses: Systemic Changes
Physiological Control Systems/Reflexive Pathways
(Regulated Variable)
Outside of Desired Range
1. Stimulus
2. Sensor
3. (Input Signal) Afferent Signal
4. (Controller) Integration Centre
5. (Output Signal)/Efferent Pathway
6. Effectors
7. Response
Successful
Example
Water Temperature is below the set point
Thermometer senses the decrease
Signal passes from centre to control box through wire
Control box is programmed to response to a temperature below 29 degrees
Signal Passes from wire to heater
Heater turns on
Water temperature increases
Not Successful
Internal Failure
External Failure
Within the desired range (homeostasis)
No Action Required
Signalling System involved
Nervous System
Endocrine
Neuroendocrine
Local Control: Isolated Changes
Signalling Systems Involved
Autocrine
Paracrine
Cell to Cell
Feedforward Control
Gain
Examples
Mean Arterial Blood Pressure
Subtopic
Cardiovascular Response to Hemorrhage
Arterial Baroreceptor Reflex
Non-Homeostatic - Positive Feedback System
Parturition
Other Examples
Initiation of Urination when Bladder is full
during the follicular phase of the menstrual cycle, estrogen stimulates the release of luteinizing hormone which in turn stimulates further estrogen synthesis by the ovaries
the calcium-induced calcium ion release in cardiac cells during each heart beat
the propagation of an action potential
the blood clotting cascade
Pathological Effects
Biological Energy Use
Structural-Functional Relationships
Compartmentalization
Mechanical Properties of Cells, Tissues and Organs
Molecular Interactions
Communication
Information Flow
Information Type
Chemical
Electrical
Distance Travelled
Long Distance
Short Distance
Mass Flow
Subtopic
The Physiological Components of the Body
respiratory System
Lungs
Cardiovascular System
Blood Vessels
Heart
Digestive System
Mouth
Stomach
Intestines
Immune System
Lymph Nodes
Nervius System
Brain
Endocrine System
Thyroid Gland
Reproductive System
Testes
Ovaries
Uterus
Urinary System
Bladder
Kidneys
Intgumentary System
Musculoskeletal System
Muscle Physiology
Types of Muscles
Striated
Skeletal
Structure of Skeletal Muscle
Muscle ensheathed by Epimysium
Composed of Fascicles ensheathed by Perimysium
Composed of Myofibres ensheathed by Epimysium
Length: Can be very long (length of a muscle)
Diameter: 10-80 micrometers
Plasma Membrane: Sarcolemma
Nucleus: Multi-nucleated
Mitochondria: Many
ER: Extensive sarcoplasmic reticulum
Composed of 100s - 1000s of Myofibrils
Composed of very organized system of Myofilaments
Contractile Filaments
Composed of fibres/proteins
Primary Contractile Fibres
Actin
3000 per myofibril
About twice as many actin filaments as myosin filaments
Each actin is one micrometer long, anchored in Z line
Components
Double helix of F-actin protein (backbone)
made of G-actin molecules .
Each bead is a G-actin.
Each G-actin molecule has one ACTIVE SITE where ADP is attached.
Tropomyosin
fiber like” molecule 50nm long
wrap around F-actin helix.
Cover active sites on G-actin molecules preventing attachment of myosin cross bridges.
Function is to keep active sites covered.
Troponin
attached to tropomyosin has strong affinity for
Tropomyosin
Actin
Ca++
When Ca++ influx occurs and Ca++ binds with troponin, it pulls on tropomyosin causing a conformational change that exposes actin binding sites.
Myosin
1500 per myofibril
Components
200 Myosin Molecules
Each molecule is composed of
heavy chain tail,
head
Subcomponents
Heavy Chain Molecules
Light Chain Molecules
Important characteristics
it has ATP-binding sites into which fit molecules of ATP
arranged with tails bunched together so that arms & heads are free to swivel
Heads face out in all directions.
Hinges at two places
Head
Arm
Ancillary Proteins
Nebulin
Titin
filaments (MW of 3,000,000).
Very flexible and springy.
Holds microfilaments in place and provides elastic recoil.
Troponin Complex
Tropomyosing
Organized functionally into sarcomeres
Might be considered the functional units of the muscle.
Regular organization with six actin filaments surrounding each myosin filament.
Shared by adjacent myosin filaments
Overall light/dark areas depend on density of fibers.
I Band
(light) contains only actin at rest.
A band
dark) contains both actin and myosin.
H zone
in center contains only myosin
Z line
(disc) separates sarcomeres.
Actin filaments pierce Z line and have an end in each of two sarcomeres.
They are anchored here
M Line
Bare Zone
A small area close to the M-line contains no crossbridge heads.
As actin fibers move close together and enter this zone, they cannot produce additional force.
Note that the sheaths travel length of muscle to form tendons at each end
Cardiac
Smooth
Skeletal and SMooth muscle
Myosin
Sarcoplasm = Cytoplasm
Contains normal organelles and cytoskeleton
Sarcoplasmic Reticulum = Endoplasmic Reticulum
Smooth
Extensive network for storage of Ca++ ions in terminal cisternae.
Can release or clear sarcoplasm of Ca++ ions (clears Ca++ via active transport).
Smooth SR surrounds each myofibril
T-Tubules
Transverse (t) tubules carry electrical signal from sarcolemma into fiber.
They branch when inside the cell forming extensive "plates" for efficient delivery of the electrical signal.
Where t-tubules contact terminal cisternae. Forms a "triad" including t-tubule with cisternae on both sides.
Mammalian skeletal muscle has two T tubules per sarcomere.
Rough
Covered with ribosomes.
Protein synthesis.
Constant replacement / synthesis of contractile proteins.
Sliding Filament Theory
Excitation
Signal at neuromuscular junction (motor end plate)
Depolarization of sarcolemma from center toward ends of cell
Signal moves down t-tubules to SR
Change in voltage of SR induces release of Ca++ from cisternae (voltage-gated Ca++ channels in SR)
Ca++ receptors along the SR open even more Ca++ channels
Ca++ floods the muscle cell
A muscle fiber is excited via a motor nerve that generates an action potential that spreads along the surface membrane (sarcolemma) and the transverse tubular system into the deeper parts of the muscle fiber.
A receptor protein dihydropyridine receptor (DHP) senses the membrane depolarization, alters its conformation, and
activates the ryanodine receptor (RyR) that releases Ca2+ from the SR.
Ca2+ then bind to troponin and activates the contraction process (Jurkat-Rott and Lehmann-Horn 2005)
Contraction
Ca++ binds with troponin (on the actin filament) causing conformational change that removes inhibition from binding site.
ATP in myosin cross bridge head already cleaved to ADP + Pi by ATPase in head but all are still bound to head. It puts arm and head into “cocked” position.
Myosin cross bridge binds to site on actin filament, creating ACTOMYOSIN.
Continued Contraction
ADP and Pi leave the myosin head triggering Power Stroke.
New ATP then binds head, causing release from actin.
New ATP splits and the released energy “cocks” head again for next stroke.
“Walk-Along or “Ratchet” theory
As long as Ca++ remains in sarcoplasm, actin sites remain exposed, and ATP is available, the heads will recycle rapidly repeatedly pulling actin past their position.
Changes in Resting vs. Active Sarcomere
Length-Tension Relationship Sarcomeres
At point 1 in Graph, the sarcomere is overly contracted. There is a high degree of overlap between the thin and thick filaments. Muscle contraction causes actin filaments to slide over one another and the ends of myosin filaments. Further muscular contraction is halted by the butting of myosin filaments against the Z-discs. Tension decreases due to this pause in cross-bridge cycling and formation.
Maximum tension is produced when sarcomeres are about 2.1 to 2.2 μm long, as seen at point 2. This is the optimal resting length for producing the maximal tension.At point 3, there is little interaction between the filaments. Very few cross-bridges can form. Less tension is produced.
When the filaments are pulled too far from one another, as seen at point 4, they no longer interact and cross-bridges fail to form. Zero tension results
The Motor End Plate
Innervated by myelinated somatic neurons (alpha)
Branch to stimulate 3 – 100s of muscle fibers at motor end plates (neuromuscular junction). Each branch is myelinated by schwann cells.
Typically near center of muscle fiber. Extremely long fibers may have two neuromuscular junctions.
Lots of mitochondria in neuron terminal to provide ATP energy for synthesis of ACh.
Picture Captions
Invagination of post-synaptic membrane called a “trough” or “gutter”. 20-30nm wide.
Acetylcholinesterase in synaptic cleft to lyse and clear ACh from cleft when signal ends.
Folds in the bottom of the trough, “subneural clefts”, to increase surface area for stimulation by Ach.
Release of Ach at the neuromuscular Junction
Depolarization reaches axon terminal.
Voltage gated Ca++ channels open.
Terminal vesicles containing ACh move to the membrane
Bound to membrane with docking proteins.
Exocytosis releases ACh into cleft.
Diffuses across to post-synaptic side.
Post-synaptic membrane receives signal
lots of ACh receptors located near mouths of subneural clefts.
Excitation Contraction Coupling
Simply means the process that excites the cell membrane at the neuromuscular junction is coupled to the processes that cause muscle contraction.
Removal of Ca++ from the sarcoplasm (relaxation)
Calcium pump actively transports Ca++ out of the sarcoplasm to end the contraction. Very efficient in clearing the intracellular fluid almost entirely of Ca++.
SR is very effective storage unit for calcium and calcium ions. Pump actively moves ions into cisternae.
Large additional stores of un-ionized calcium is bound in SR by a protein called calsequestrin. Will be released as ionized Ca++ to maintain stores in cisternae if they get low.
Mechanisms of Skeletal Muscle Contraction
Muscle contraction is based on a twitch of the muscle fiber which is like an action potential is an all or nothing event.
A twitch is the mechanical response of an individual muscle fiber, an individual motor unit, or a whole muscle to a single action potential.
Phases of the the Twitch
When a stimulus is applied and a fiber contracts the twitch can be divided into three phases
Latent
Ca build up?
is the delay of a few milliseconds between an action potential and the start of a contraction and reflects the time for excitation-contraction coupling.
Contraction
starts at the end of the latent period and ends when the muscle tension peaks (tension = force expressed in grams). During this time cytosolic calcium levels are increasing as released calcium exceeds uptake.
Relaxation
is the time between peak tension and the end of the contraction when the tension returns to zero. During this time cytosolic calcium is decreasing as reuptake exceeds release.
Types of Twitch
Isometric Twitch
When the load (force opposing contraction) is greater than the force of contraction of the muscle, the muscle creates tension when it contracts but does not shorten.
An isometric twitch is measured by keeping the muscle immobile while stimulating it and measuring the tension that develops during contraction.
The rise and fall of tension traces a bell-shaped curve.
Isotonic Twitch
When the force of contraction of the muscle is at least equal to the load so that the muscle shortens, the muscle is said to contract isotonically.
An isotonic twitch is measured by attaching the muscle to a moveable load.
The tension curve for an isotonic twitch shows a plateau during which the force or tension is constant (iso-same; tonic- tension).
Relationship between Isotonic and Isometric Contraction in Real Life
When the load exceeds the amount of force the muscle can generate, an isometric twitch results which is always of the same size and shape.
The greater the load the higher the plateau and the greater the time lag between stimuli and the start of muscle shortening.
The motor unit consists of a motor neuron and all the muscle fibers it innervates.
Factors Affecting the Force Generation of Individual Muscle Fibers
Frequency of Stimulation
When a muscle is stimulated at a frequency so that twitches follow one another closely, the peak in tension rises in a step-wise fashion.
This phenomenon is called treppe.
Treppe may occur because Ca++ released from previous twitches exceeds Ca++ reuptake and this results in an increase in Ca++ concentration.
This in turn increases the number of crossbridges that form in the following contractions.
Another possibility is that frequent stimulation "warms up" the muscle and thereby increases the enzymatic rate.
As muscle twitch is fairly slow compared to an action potential many action potentials can arrive before a single twitch is completed. This causes the twitches to bunch up and results in the generation of a force that is greater than a single twitch. This process is called summation.
Increasing action potential frequency increases force by SUMMATION.
When the frequency of stimulation is so high that Ca++ levels rise to peak levels, summation results in the level of tension reaching a plateau called tetanus.
When the frequency of stimuli is high enough to cause tetanus but tension oscillates around an average level, the tetanus is called incomplete or unfused.
At greater frequencies of stimulus, levels of Ca++ peak and cause a maximum number of crossbridges to cycle.
At this point the tension plateau smoothes out and tetanus is called complete or fused.
Fiber Diameter
The greater the number of sarcomeres arranged in parallel, the greater the force generating capacity.
The number of sarcomeres arranged in parallel correlates with a fiber's diameter.
The greater the cross-sectional area of a fiber, the more force it can generate.
Changes in Fiber Length
When the muscle is at the optimum length the number of active cross bridges is the greatest.
When the muscle is stretched beyond this length the number of active cross bridges decreases because the overlap between the actin and myosin fibers decrease.
As the muscle becomes shorter than the optimum length the thin filaments at opposite ends of the sarcomere first begin to overlap one another and interfere with each other's movements.
This results in a slow decrease in tension as the sarcomeres get shorter.
Then as the sarcomeres get shorter the thick filaments come into contact with the Z lines and the decrease in tension with decreasing length becomes even steeper.
Preload and Afterload
Example - outstretched arm picking up bucket of water - hold it straight - preload - stretching sarcomeres to optimal length
when you actually bend and lift - afterload
Preload is blood coming to hear to stretch it; afterload is blood in aorta and pushing it out into the vascular system
Preload
is the load on a muscle in a relaxed state, prior to contraction.
Stretching a muscle to optimize actin and myosin filament interaction is known as Preloading.
Too little - you will fall on the left side of the curve.
Too much - you will fall on the right side of the curve
Afterload
the load the muscle is working against or trying to move during stimulation.
Afterload also determines how fast a muscle contracts during a lift.
Minimal loads allow the muscle to contract at maximal velocity.
Isometric Contractions occur when afterload is too heavy to lift
Velocity of Shortening
When a muscle contracts isotonically under increasing loads the contractions display the following effects:
The latent period (time lag between stimulation and shortening) increases.
The duration of shortening decreases.
The velocity of shortening decreases
Graph of velocity against load
add distance shortening - time
preload - isotonic - isotonic - isometric (rt. side = afterload)
Zero load -
latent phase is shortest;
highest velocity of shortening
Longest duration of contraction
Heavy load
latent phase is increased the most.
Lowest velocity of shortening
Shortest duration of contraction
When the velocity of shortening is plotted as a function of load, as the load increases the velocity of shortening gradually decreases
add velocity of shortening
Different types of fibers differ in their velocity of shortening
ADD tension-time graph for different muscles
This is because there are fast-twitch and slow-twitch fibers.
Slow Twitch Oxidative (aerobic)
Certain muscles (e.g. soleus) contain mostly slow twitch fibers and will contract slowly.
Red in color.
Highly vascularized.
Lots of mitochondria.
Low strength,
high endurance.
Fast Twitch
Glycolytic
White in color, lacking much vascularization.
Lots of contractile protein (large fiber size).
Extensive SR.
Lots of constituents and enzymes for glycolysis.
Few mitochondria.
Contains "fast myosin" which is able to hydrolyze ATP at a faster rate.
High strength
Low endurance
Oxidative Glycolytic
crossover fiber.
Can mimic actions of FTG or STO fibers in response to specific muscle training.
Some contain predominantly fast-twitch fibers (e.g. extraocular) and contract quickly.
E.g. extraocular muscles
Fast-twitch fibers also have higher maximum shortening velocities compared to slow-twitch.
Energetics of Muscle Contraction
insert energetics of muscle contraction
Phosphagen System
addd phosphagen system
ATP is the immediate source of energy for muscle contraction.
However, the ATP stores in the muscle can sustain muscle contraction for up to 3 seconds.
In about 3 sec, all the ATP is depleted from the muscle cell.
Thereafter, ATP is regenerated using the energy released by the dephosphorylation of creatine phosphate reserves of the muscle fiber.
Creatine phosphate + ADP-------------------- > creatine + ATP
The creatine phosphate reserves of the muscle fiber can sustain contraction for about 5 to 8 seconds.
Creatine phosphate (CP) releases stored energy to convert ADP to ATP:
Returns energy to ATP via enzyme creatine phosphokinase (CPK)
excess in blood with muscle damage.
Aerobic metabolism (requires O2) provides most ATP needed for contraction:
Glycolysis in cytoplasm;
oxidative phosphorylation in mitochondria
At peak activity, anaerobic glycolysis needed to generate ATP:
Fermentation- lactate from pyruvate
temporarily maintains glycolysis without O2
far less ATP produced
Muscle blood flow during exercise
add muscle blood flow in exercise
resting = 3-6 ml/100g/min
max work = 90 ml/100g/min
the increase is due to vasodilation and increase BP
Muscle blood flow may increase more than 20 fold during exercise
States of Muscle Tone
Hypertrophy (fibers)
Increase in number of contractile proteins causing an increase in size of myofibrils up to 50%.
Increase in enzymes for glycolysis and in the number and size of mitochondria.
More sarcomeres added to increase length if muscle is repeatedly over-stretched.
Muscle atrophy
Occurs at approximately the same rate as hypertrophy during periods of non-exercise.
Happens more quickly when muscle is prevented from moving as in a cast following injury.
Happens very quickly in cases of loss of nerve supply.
Needs the signals that maintain muscle tone to keep the muscle at a normal size.
Muscle dystrophy :
Recessive X –linked mutation in dystrophin gene in Duchenne muscular dystrophy.
Eventually causes death because of paralysis of respiratory muscles
Rigor mortis:
Muscle stiffen after death.
ATP reserves are quickly exhausted from the muscle contraction and other cellular processes.
This means that the actin and myosin fibers will remain linked until the muscles themselves start to decompose.
Regulation of Muscular Contraction
Muscle Spindle
add muscle spindle 1 and 2
Diagrammatic cross-section of a muscle spindle showing
Intrafusal Fibres
add muscle spindle 3
Afferent
add muscle spindle 4
There are two types of sensory receptors associated with the intrafusal fibers that detect the degree of stretch of these fibers which in turn monitors the degree of stretch of the entire muscle:
Annulospiral endings
This is the end of a type Ia afferent fiber that wraps around the central bag region.
Flower-spray endings
The branching end of the type II afferent fibers of these neurons are located on either side of the central bag region
Efferent
Alpha
to extrafusal (normal) muscle fibres
Gamma
to intrafusal muscle fibres
Keep muscles stretched to keep signal going again and again to know how much load there is
important in preventing muscle injury
don't stop sending signals
Normal musccle fibers that surround the spindle are called extrafusal fibers.
Reflexes
Stretch Reflexes
The stretch reflex is generated as a protective mechanism when the spindle and its skeletal muscles are being stretched.
During stretch, an action potential is transmitted to the central nervous system (CNS) at the spinal cord; the frequency of the action potential is proportional to the degree of stretching.
As the skeletal muscles contract, the intrafusal muscles shorten;
this relaxes the tension on the muscle spindles, and reduces the discharge rate of the gamma efferents on the annulospiral endings.
Patellar Reflex (GTOs)
Add patellar reflex
Striking the patellar tendonwith a tendon hammer just below the patella stretches the muscle spindle in the quadriceps femoris muscle. This produces a signal which travels back to the spinal cord and synapses (without interneurons) at the level of L4 in the spinal cord, completely independent of higher centres.
From there, an alpha-motor neuron conducts an efferent impulse back to the quadriceps femoris muscle, triggering contraction.
This contraction, coordinated with the relaxation of the antagonistic flexor hamstring muscle causes the leg to kick.
otherwise its a monosynaptic reflex
This reflex is a reflex of proprioception which helps maintain posture and balance, allowing to keep one's balance with little effort or conscious thought.
It tests L2, L3, and L4
Write out steps from picture.
Cardiac Muscle
Smooth Muscle
Spindle shaped cells
Relatively small compared to skeletal and cardiac muscle
2-5 mm wide; 50-200 mm long.
Actin/myosin ratio:
greater in smooth muscle (10:1) than in skeletal muscle.
Overall architecture
add smooth muscle architecture
The arrangement of dense bodies with connective-tissue fibers running throughout the cell and into adjacent gives structural integrity to the entire smooth muscle tissue, and anchor points for actin filaments
Contractile Apparatus
add smooth muscle apparatus
myosin (thick, white filament).
add myosin in smooth
Light Chains - Play a key regulatory role
The organization of myosin molecules on the myosin filament is somewhat different than in skeletal muscle.
A main difference is the lack of a bare region in the middle lacking cross-bridges.
So there are cross-bridge heads along the entire length of the myosin filament.
Location and action of the myosin light chains allows it to control activation of myosin cross-bridge heads.
actin (thin-filament)
F-Actin strands of G-Actin pearls
Tropomyosin present in smooth muscle actin but:
Exact functional role, if any, unclear.
No troponin present at all
Therefore, Troponin-I does not inhibit cross-bridge cycling in smooth muscle as it does in skeletal muscle.
Lack neat hexagonal arrangement of actin and myosin
Intermediate Filaments
Cytoskeletal elements which form a structural backbone against which contraction occurs.
Dense Bodies.
Serve as anchors for the thin-filament protein actin.
Analogous to z-lines in striated muscle
GAP JUNCTIONS
Allow direct electrical communications between adjacent smooth muscle cells
Lots of gap junctions in smooth muscle, but density varies from tissue to tissue.
No T-tubules or terminal cistern system.
Small size of smooth muscle cells.
Smooth muscle has no t-tubules, and a much less developed SR. Result is a slower, often less precise response
Smooth muscle does not always require action potential to contract.
May involve graded potentials, that sometimes build into action potentials.
Poorly developed sarcoplasmic reticulum.
Smooth muscle does have a SR containing Ca++, so Ca++ can be released from intracellular stores.
Often needs additional extracellular Ca++ for activation and/or contraction.
Compare: Dependence on extracellular Ca++
cardiac muscle (partial-dependence)
skeletal muscle (negligible-dependence).
Smooth Muscle Innervation
Innervated by the autonomic nervous system.
Autonomic neurons do not form synapses with specific cells but with groups of cells.
Neurotransmitter is released at varicosities (swellings) found along the length of the axon
add smooth muscle varicosities
no specialized nerve cell junction
This causes a neighboring group of cells to contract together. Smooth muscle cells contract in groups also because of gap junctions between cells that allow electrical signals to spread from one cell to another.
Mechanism of Smooth Muscle COntraction
Add mechanism of smooth muscle contraction
Calcium ions combine with calmodulin to cause activation of myosin light chain kinase (MLCK )and phosphorylation of myosin light chain (head)
Myosin light chain phosphatase (MLCP) is important for cessation of contraction i.e relaxation of muscle.
High Ca++ therefore causes contraction by increasing MLCK activity (increased in comparison with MLCP activity)
High MLCK/MLCP Activity Ratio initiates smooth muscle contraction
Mechanism of Smooth Muscle Relaxation
Low intracellular [Ca++] will cause the cell to relax.
Calcium extrusion from the cell eg. 3Na+/Ca++ exchanger
Sarcolemma Ca++ATPase
Reuptake by the sarcoplasmic reticulum by SR.
Phospholamban (PLB) is an intracellular protein, when phosphorylated, it increases Ca++ re-uptake into SR by sarcoplasmic reticulum calcium pump (SERCA), clearing Ca++ from the cytosol.
High cAMP causes relaxation by effectively lowering myosin light chain kinase [MLCK]
c AMP activates PKA which phosphorylates MLCK into a state where Ca+/calmodulin cannot bind.
Nitric oxide causes smooth muscle relaxation in the same manner.
c GMP mediated response.
Note: Both cAMP/PKA, and cGMP/PKG can phosphorylate phospholamban (PLB).
Ischemia (decrease in blood flow) opens ATP-sensitive K+ channels, hyperpolarization, closes Ca++ channels
Ca++ channel blockers (L-type channels)
Muscarinic Receptors
M2 receptors
Use Gi proteins to inhibit adenylyl cyclase, lowering cAMP and thus causing smooth muscle contraction.
M3 receptors (and a smaller number of M1 receptors)
Use Gq protein to increase intracellular Ca++ and cause smooth muscle contraction.
For relaxation of a sphincter (such as for urination) M3 receptors use their Gq protein to increase Ca++ in endothelial cells that produce NO.
The NO then diffuses into the sphincter muscle and causes it to relax.
Comparison of SMooth and Skeletal Muscle Contraction
add comparison of smooth and skeletal muscle contraction
Slow cycling of actin and myosin cross bridges. About 1/10 to 1/300 that in skeletal muscles.
Low energy requirement to sustain the same tension. About 1/10 to 1/300 that in skeletal muscles.
Contraction time is 1 to 3 sec, about 30 times longer than in skeletal muscle.
Maximum force of contraction is more. 4-6kg/cm sq. Skeletal muscle about 3-4 kg.
Stress-relaxation: Hollow organs maintain same pressure despite changes in pressure.
Latch mechanism:
After reaching full contraction even if force of stimulus decreases the contraction is maintained for a long time
Latch State
Contraction of SM is much slower than that of skeletal muscle. Force production can be equal to skeletal muscle.
With latch state, ENERGY EXPENDITURE economy is high:
Sustained smooth muscle contractions are executed with minimal expenditure of ATP.
Slow cycling and long attachment of cross-bridges take place due to decrease in ATPase activity, and possibly a reduction in both MLCK and MLCP activity.
Types of smooth muscle-
add multi-unit and single unit smooth muscle
Multi-Unit Extreme end of Spectrum
Each smooth muscle cell acts mostly independently (more like skeletal muscle).
Less gap junctions between cells
Higher innervation ratios than visceral smooth muscle.
These are found in places where fine control of contraction is needed
Ciliary muscles of the eye
Tracheal Muscle
GI Sphincters
Larger Blood Vessels
Bronchial muscles
Iris Muscle
Vas deferens
All sphincters of the body
Electrical Characteristics
Multiunit smooth muscle is neurogenic- that is, its contraction must be initiated by a motor neuron.
Membrane potential of multiunit smooth muscle is stable, and lacks many voltage-gated channels
Typically, do not display action potentials when stimulated to contract but displays graded potentials.
Multiunit Smooth Muscle uses graded potentials (PSPs)
add multiunity smooth muscles graded potentials
Multi-unit smooth muscle cell membrane lacks the voltage-gated channels that can cause action potentials.
More stimulation causes graded-depolarization and graded response.
Tone:
Constant and stable low level of contraction
Example:
GI sphincters.
Tone is intrinsic property of the muscle itself -- does not depend on nerves (unlike skeletal muscle)
Tone may be modified by:
nerves
hormones
drugs
Contraction Mechanism
add multiunit smooth muscle contraction mechanism
actin and myosin interact according to the sliding filament mechanism
Ca2+ is released from the SR and from the extracellular space
Ca2+ interacts with calmodulin and myosin light chain kinase to activate myosin
Ca2+ binds to calmodulin and activates it
activated calmodulin activates the kinase enzyme
phosphorylated cross bridges interact with actin to produce shortening
Single-Unit Extreme end of Spectrum
add single unit smoothh muscle
Also called unitary or visceral smooth muscle.
Behaves in a syncytial manner.
In this organization the smooth muscle cells are connected by gap junctions and there are fewer neurons..
Relatively sparse innervation
This organization is present in
the wall of the gastrointestinal tract
Ureters and urinary bladder
Smaller arteries / arterioles / smaller veins
Lymphatic vessels
Uterus
Electrical Characteristics:
Single-unit visceral smooth muscle is myogenic; it can contract regularly without input from a motor neuron .
Slow Wave Potentials:
Slow wave potential are unstable resting membrane potentials that continuously cycle through depolarization- and repolarization phases. However, not every cycle reaches depolarization threshold and thus an action potential (AP) will not always fir
Graph 1
GRaph 2
Resting Membrane Potential
Relatively positive (perhaps -55 mV) due to high Na+ leak.
Threshold potential is about -30mV
Single-unit muscle cell membrane has voltage-gated channels, so can create an action potential when stimulated
Action potentials (all or none) spikes.
add single smooth unit action potentials
Almost always cause an associated contraction. Cell membrane depolarization will periodically reach depolarization threshold and an action potential will fire, triggering contraction of the myocyte.
Subtopic
Organ Systems of the Body and their Function
Representative Functions
Transport of Materials between all cells of the body
Conversion of Food into particles that can be transported into wastes
Coordination of body function through synthesis and release of reguatory molecules.
Defense against foreign invaders
Protection from the external environment
Support and Movement
Coordination of body function through electrical signals and the release of regulatory molecules
Perpetuation of the species
Exchange of oxygen and carbon dioxide between the internal and external environments