MAMMALIAN PHYSIOLOGY
TENTATIVE LECTURE SCHEDULE
Page Numbers Refer to Guyton and Hall
Textbook of Medical Physiology (10th ed.)
Wed Jan 14 - Course Introduction and Expectations
Membrane Transport (Diffusion and Active Transport)
Chapter 4, pp. 40-50
Fri Jan 16 - Electrical Properties of Mammalian Tissues
Basic Physics of Membrane Potentials
Chapter 5, pp. 52-55
Mon Jan 19 - Martin Luther King Day - NO CLASS
Wed Jan 21 - Electrical Properties of Mammalian Tissues
Action Potentials
Chapter 5, pp. 55-65
Fri Jan 23 - Skeletal Muscle Physiology
Neuromuscular Physiology
Chapter 7, pp. 80-86
QUIZ #1 - Transport through Action Potentials
Mon Jan 26 - Skeletal Muscle Physiology
Skeletal Muscle Contraction
Chapter 6, pp.67-78
Wed Jan 28 - Smooth Muscle Physiology
Excitation and Contraction of Smooth Muscle
Chapter 8, pp. 87-94
Fri Jan 30 - Smooth Muscle Physiology
Contraction of Smooth Muscle
Chapter 8, pp. 87-94
QUIZ #2 - Skeletal Muscle Physiology through Smooth Muscle Physiology
Mon Feb 2 - EXAM #1 - Transport through Smooth Muscle Contraction
Wed Feb 4 - The Heart
Mechanical Functions of the Heart
Electrical Properties of Cardiac Tissue
Chapter 9, pp. 96-106
Fri Feb 6 - Rhythmic Excitation of the Heart
Chapter 10, pp. 107-112
Mon Feb 9 - EKGs - Flow of Current Around the Heart
Chapter 11, pp. 114-119
Wed Feb 11 - Analysis of EKGs
Chapter 12, pp. 120-133
QUIZ #3 - Mechanical Functions of the Heart through EKGs
Fri Feb 13 - Cardiac Arrhythmias
Chapter 13, pp. 134-142
Mon Feb 16 - Circulation
Physical Characteristics
Chapter 14, pp. 144-151
Wed Feb 18 - Cardiac Output, Venous Return, and Their Regulation
Chapter 20, pp. 210-221
QUIZ #4 - Analysis of EKGs through Physical Characteristics of Circulation
Fri Feb 20 - Functions of the Arterial and Venous System
Chapter 15, pp. 152-160
TERM PAPER OUTLINE DUE
Mon Feb 23 - The Microcirculation and Lymphatic System
Chapter 16, pp. 162-174
Wed Feb 25 - Local Control of Blood Flow by Tissues and Humoral Regulation
Chapter 17, pp. 175-182
Fri Feb 27 - EXAM #2 - The Heart through Microcirculation & Lymphatic System
Mon Mar 1 - Nervous Regulation of Circulation
Chapter 18, pp. 184-193
Wed Mar 3 - Renal Involvement in the Regulation of Blood Pressure
Chapter 19, pp. 195-208
QUIZ #5 - Cardiac Output through Nervous Regulation of Circulation
Fri Mar 5 - Special Circulation (Skeletal and Cardiac Muscle)
Chapter 21, pp. 223-233
Mon Mar 8 - Cardiac Failure
Chapter 22, pp. 235-244
Wed Mar 10 - Congenital Heart Defects
Chapter 23, pp. 245-252
Fri Mar 12 - Circulatory Shock
Chapter 24, pp. 253-262
QUIZ #6 - Renal Involvement in the Regulation of Blood Pressure through Congenital Heart Defects
Mon Mar 15 - Pulmonary Ventilation
Chapter 37, pp. 432-442
Wed Mar 17 - Pulmonary Circulation, Pulmonary Edema
Chapter 38, pp. 444-450
Fri Mar 19 - EXAM #3 - Local Control of Blood Flow through Circulatory Shock
Mon Mar 22 - SPRING BREAK
Wen Mar 24 - SPRING BREAK
Fri Mar 26 - SPRING BREAK
Mon Mar 29 - Physical Principles of Gas Exchange
Chapter 39, pp. 452-461
Wed Mar 31 - Gas Transport through the Blood and Body Fluids
Chapter 40, pp. 463-472
QUIZ #7 - Pulmonary Ventilation through Physical Principles of Gas Exchange
Fri Apr 2 - Gas Transport through the Blood and Body Fluids
Chapter 40, pp. 463-472
Mon Apr 5 RBCs, Anemia, and Polycythemia
Chapter 32, pp. 382-391
Wed Apr 7 - Regulation of Ventilation
Chapter 41, pp. 474-482
Fri Apr 9 - Respiratory Pathophysiology
Chapter 42, pp. 484-492
QUIZ #8 - Gas Transport through Regulation of Ventilation
Mon Apr 12 - Special Circumstances for Respiratory Physiology
Chapters 43 and 44, pp. 496-502
Wed Apr 14 - The Body Fluid Compartments
Chapter 25, pp. 264-278
Fri Apr 16 - KANSAS ACADEMY OF SCIENCES
Mon Apr 19 - Renal Blood Flow and Glomerular Filtration
Chapter 26, pp. 279-293
Wed Apr 21 - EXAM #4 - Pulmonary Ventilation through Special Circumstances for Respiratory Physiology
Fri Apr 23 - Renal Blood Flow and Glomerular Filtration
Chapter 26, pp. 279-293
Mon Apr 26 - Tubular Reabsorption and Secretion
Chapter 27, pp. 295-312
QUIZ #9 - Body Fluid Compartments through Blood Flow and Glomerular Filtration
Wed Apr 28 - Renal Control of Osmolality
Chapter 28, pp. 313-328
Fri Apr 30 - Renal Regulation of Blood Volume and Extracellular Fluid Volume
Chapter 29, pp. 329-344
Mon May 3 - Regulation of Acid Base Balance
Chapter 30, pp. 346-363
Wed May 5 - Diuretics and Kidney Disease
Chapter 31, pp. 364-378
Fri May 7 - Diuretics and Kidney Disease
QUIZ #10 - Tubular Reabsroption through Diuretics and Kidney Disease
Chapter 31, pp. 364-378
FINAL DRAFT OF TERM PAPER DUE
FINAL EXAM - MONDAY MAY 10 - 10:10 - 12:00
Body Fluid Compartments through Kidney Disease
DIFFUSION THROUGH THE CELL MEMBRANE
I. Simple Diffusion
Requires a concentration gradient
A. Two Types of Simple Diffusion (Fig 4-2, p. 41)
1. Diffusion through interstices of the lipid bilayer
a. rate of diffusion dependent upon substances
lipid solubility
Oxygen, Carbon Dioxide, Nitrogen and
Alcohols are very lipid soluble, thus
diffuse readily through cell membrane
Hydrogen, Sodium, Potassium and other ions
are not very lipid soluble, thus do not
readily diffuse through the cell membrane
2. Diffusion through protein channels of cell membrane
a. selectively permeable to certain substances
mostly as a result of the size and/or charge of the
protein channel (Fig 4-4, p. 42)
- urea is a larger molecule than water, how does
its diffusion through the membrane compare to
water?
- does significant amounts of urea pass through the
cell membrane?
b. many protein channels can be opened or closed by gates
(Fig 4-4, p. 42)
II. Gating of Protein Channels
A. Two principal ways of controlling the opening and closing
of protein channels
1. Voltage Gating
a. potential voltage differences between the inside and
outside of the cell determines if the gates of the
channel will be open or closed
Ex. Inside of the cell is strongly negative, sodium
gates will remain closed
If the inside of the cell should become less
negative, the sodium gates open allowing sodium
to rush in (nerve impulse).
2. Ligand (Chemical) Gating
a. substance binds to the protein channel causing a
conformational change in the protein structure that
either opens or closes the gate
Ex. Acetylcholine binding to the protein channels
located on muscle membranes making the membrane
permeable to sodium (muscle contraction).
- what is the patch-clamp method and why is it used?
III. Facilitated Diffusion (Carrier-mediated Diffusion)
a. carrier proteins facilitate the diffusion of substances through
protein channels
b. rate of diffusion is determined by rate at which the channel
protein can undergo a conformational change
c. as a result, facilitated diffusion has a maximum rate at which
substances can diffuse regardless of diffusing conditions (Vmax)
(See next section: Factors that Affect Net Rate of Diffusion)
(Fig 4-6, p. 44)
IV. Factors that Affect Net Rate of Diffusion
a. Concentration Gradient (4-8a, p. 45)
Net Diffusion ∞ (Co - Ci)
b. Electrical Gradient (4-8b, p. 45)
Nernst Equation - the voltage at which no net movement
of a particular ion occurs for a given
concentration gradient
Electromotive Force (EMF) = + 61 log C1/C2
c. Pressure Gradient (Fig 4-8c, p. 45)
V. Osmosis (Fig 4-9, p. 46)
a. Defined as: the net movement of water caused by a concentration
difference of water
b. Osmotic Pressure
- the pressure required to exactly stop osmosis
- Fig 4-10, p.46
c. Importance of Molar Concentration
- osmotic pressure is exerted by the NUMBER of particles
in solution (solutes) and not by their size
- due to large particles moving slower
- k = mv2/2
where k is average kinetic energy
m is the mass of particles
v is the velocity particles
d. Osmolality
- the number of solutes in solution
- one mole per kilogram = 1 osmole
- Thus, in order to make a 1 osmole solution of glucose
(180 grams per mole) would need to add 180 grams of
glucose to 1Kg of distilled water
- if the chemical in question can dissociate into two ions
(NaCl) then the the osmolality is twice the molecular weight
Ex. NaCl has a MW of 58.5 g/Mole
58.5 grams of NaCl in 1 Kg water = 2 Osmoles
- due to 1 Osmole contribution of Na and 1 Osmole
contribution of Cl - assumes complete dissociation
- a milliosmole is 1/1000 of an osmole
- How much water diffuses through a red blood cell per second relative to
its normal cell volume?
- How much NET diffusion occurs through a red blood cell
- How does osmolality differ from osmolarity?
V. Active Transport
Allows for movement of substances uphill against a concentration
gradient but requires energy derived from ATP.
A. Two Types of Active Transport
1. Primary Active Transport
- energy derived directly from the breakdown of a high-energy
phosphate compound (ex. ATP)
2. Secondary Active Transport
- energy derived from stored (potential) energy source that was
created via the breakdown of a high-energy phosphate cmpd.
- Both primary and secondary active transport require carrier proteins\
B. Sodium-Potassium "Pump" (Fig 4-11, p. 47)
- a primary active transport mechanism present in all cells of the body
- allows for the establishment of a negative electrical
potential inside the cell
1) How the sodium-potassium pump works
a) 3 Na+ bind to the inside of the protein channel
and 2 K+ to the outside of the channel
b) causes the activation of an ATPase also located
on the protein channel near the Na+ binding site
c) ATPase splits ATP into ADP + Pi which releases energy
d) The energy released is used to bring about a conformational change in the protein channel
e) conformational change results in the 3 Na+ being
moved out of the cell and the 2 K+ being moved
into the cell
2) Result of the sodium-potassium pump
a) one net positive charge is moved out of the cell
causing the interior of the cell to become more
negative with respect to the fluid surrounding
the cell
3) Importance of the sodium-potassium pump
a) control of cell volume
- large number of proteins and organic cmpds in cell
creating an osmotic gradient pulling water into the cell
- left unchecked the cell would burst
- recall remove 3 Na+ from interior and brings into the cell
2 K+. Net loss of one ion from interior of the cell, water
follows
- cell swelling activates the sodium-potassium pump
b) electrogenic pump
- recall remove 3 Na+ from interior and brings into the cell
2 K+. Net loss of one positive ion from interior of the cell,
results in the cell interior becoming more negative relative
to cell exterior.
B. Calcium Pump
1. In most cells the amount of Ca++ inside the cell is
10,000 times less than that of Ca++ surrounding the
cell.
2. This gradient is maintained by the Calcium pumps
a) cell membrane bound calcium pumps, pump calcium
to the cell exterior
B) pump calcium into cytoplasmic organelles
(sarcoplasmic reticulum and mitochondria)
C) Hydrogen Ion Pumps
- where in the body do these occur?
- what is there function in those parts of the body
D) Co-transport (Secondary Active Transport)
1) Glucose and Amino Acids along with Sodium Ions (4-12, p. 49)
- when sodium and glucose bind to their respective binding
sites on the same receptor protein, a conformational change
occurs in which sodium travels down its concentration
gradient providing the energy for glucose to be moved up
its concentration gradient
E) Counter-transport
1) Sodium Counter-transport of Calcium and Hydrogen
- same as above except that sodium is moved in a direction
opposite that of calcium or hydrogen
- in what cells does this occur?
F) Active Transport through Cellular Sheets
- transport through a lining of cells (sheet)
- where does this occur?
- Fig 4-13, p. 50
PHYSICS OF MEMBRANE POTENTIALS
I. Movements of Ions
A) Concentration Gradient
1) substances tend to go from places of higher concentrations
to places of lower concentrations
B) Electrical Gradient
1) unlike charges attract; like charges repel each other
II. Concentration Gradients Across the Cell Membrane (Fig 4-1, p. 41)
A. Concentration of selected ions inside and outside a
typical cell at rest.
Concentration (mEq/L)
Ion Inside Cell Outside Cell
Na+ 10 142
K+ 140 4
Cl- 4 103
B. Given the above table, what would be the forces working on
sodium in a typical cell at rest.
1) Concentration gradient forces
there would be a tendency for sodium to diffuse from
outside the cell toward the inside
2) Electrical gradient forces
there would be a tendency for sodium to be pulled into
the cell
III. The Nernst Potential
- the potential voltage across a membrane that would prevent net
diffusion of an ion in either direction
A. The Nernst Potential for a given ion can be calculated using
the Nernst Equation
+ 61 mV log10 concentration of a given ion inside the cell
concentration of a the same ion outside the cell
When the ion is negative (Cl-) use + 61 log
When the ion is positive (K+ or Na+) use - 61 log
Example for Na+
- 61 mV log10 [10 mEq/L] = 70mV
[142 mEq/L]
IV. Goldman-Hodgkin-Katz Equation
- Used to calculate the membrane potential on the inside of the membrane
when the membrane is permeable to several different ions
EMF = - 61 mV log10 C Na(i) + P Na + C K(i) + P K + C Cl(o) + P Cl
C Na(o) + P Na + C K(o) + P K + C Cl(i) + P Cl
Where: C = concentration, P = Permeability of the ion
RESTING MEMBRANE POTENTIAL OF NERVES
I. Resting Membrane Potential
- the membrane potential of a nerve cell when it is not carrying an
impulse (i.e. resting)
- Resting membrane potential is usually about -90 mV, that is the
inside of the nerve cell is 90 mV more negative with respect to
the fluid surrounding the nerve cell
II. Ion Concentration of Resting Nerve Cells
Concentration (mEq/L)
Ion Inside Outside
Potassium 140 4
Sodium 14 142
A) Why this concentration for potassium and sodium?
1) Sodium-potassium pumps
- recall pump 3 Na+ out for every 2 K+ pumped in
2. The nerve cell membrane is much more permeable to
K+ than to Na+, in fact 100X more permeable to K+
- As a result, the K+ plays a much larger role in
the determination of the membrane resting potential
- 61 mV log10 [140 mEq/L] = -94mV
[4 mEq/L]
NERVE ACTION POTENTIALS
I. Nerve action potentials are rapid changes in the membrane potential
that allows for the transmission of nerve signals (Fig 5-6, p. 56)
II. How Are Nerve Action Potentials Brought About?
1. A stimulus (neurotransmitter for example) causes the nerve
membrane to become less negative
2. at a certain point called threshold (usually between - 70 and
- 50 mV) a conformational change occurs in the sodium channel
(Activated State)
3. this conformational change opens up sodium gates (Fig 5-7, p. 56)
increasing the permeability of the membrane to sodium by
500 to 5000 fold (Voltage Gating)
4. due to the concentration and electrical gradients, sodium comes
rushing into the cell
5. the entrance of sodium into the cell causes the inside of the
cell to become more positive (depolarization) This change
occurs very rapidly
6. Once the membrane potential reaches approximates + 35 mV, the
gates of the sodium channels close (Fig 5-7, p. 62)
7. Sodium gates will not become activated again until the resting
membrane potential is nearly back to normal (i.e. must be
below threshold)
III. How Is The Membrane Potential Returned Back To Resting?
1. When the membrane potential hits threshold, the potassium
gates also open but open up much more slowly than do the
sodium gates (Fig 5-9, p. 57)
2. The opening of the K+ gates allows for the movement of K+ out
of the cell
3. The decrease in the entry of Na+ into the cell and the increase
of K+ out of the cell will make the inside of the cell more
negative (repolarization)
4. Not only do the K+ gates open slower but also remain open
longer than do the Na+ gates. As a result, the membrane
potential goes more negative than the resting membrane
potential (positive afterpotential)
5. Even though repolarization has taken place and the resting
membrane potential is back to normal, the ion concentration
inside the cell is not back to normal.
6. Sodium-Potassium Pumps work to get the initial concentration
of these two ions back
IV. Influence of Ion Concentrations on Action Potentials
A. Hypopolarization
- occurs when the resting membrane potential moves closer
to threshold value
- for example if the resting membrane value is normally - 90mV
and it becomes less negative and closer to the threshold
value (-75mV), the membrane is said to be hypopolarized
1. How does this occur?
A. a increase in the potassium concentration outside the
nerve cell
For example
- 61 mV + log [140 mEq/L K+] = - 75.8mV
[8 mEq/L K+]
Recall that the normal Nernst Potential for K+
was - 94mV. If one finds the difference between
the normal Nernst potential and the calculated
value, the effect on the membrane potential can
be determined
- 94mV (normal value) + X = - 75.8mV
X = + 18.2mV
Recall that normal Resting Membrane Potential was
- 90 mV. A increase in potassium surrounding the
cell to a value of 8 mEq/L leads to a + 18.2mV
change. Thus new resting membrane potential is
- 90mV + 18.2mV = - 71.8mV
B. Hyperpolarization
- said to occur when the resting membrane potential
becomes even more negative than normal
- example is if the normal resting membrane potential
where - 90mV then it became more negative, - 110mV
the membrane would be hyperpolarized
- can result due to a decrease in K+ surrounding the
cell
IV. Propagation of an Action Potential
A. All-or-None Principle
- if the membrane potential does not reach threshold, there
will be no action potential
- if the membrane potential does reach threshold, there will
be an action potential
B. Direction of Propagation (Fig 5-11, p. 60)
- an action potential at any point on the membrane will cause
depolarization of adjacent areas
V. Propagation of an Action Potential: Myelinated v.s. Unmyelinated Axons
A. Unmyelinated Axons
- must have ion movements down the entire length of the
membrane
- very slow impulse conduction
B. Myelinated Axons
- surrounded by multiple layers of membranes consisting of a
lipid substance called sphingomyelin
- acts as a very good insulator, preventing the flow of ions
through the membrane
- only area where ions can freely flow are at unmyelinated
areas termed the Nodes of Ranvier
- myelinated axons use saltatory conduction in which the impulse
is carried from node to node
- greatly increases the speed of impulse conduction
VI. Nerve Conduction Velocity
A. Speed at which an impulse is carried down a nerve depends upon
1. Myelination
- myelinated axons conduct nerve impulses much faster
than unmyelinated axons
2. Size
- larger diameter axons carry impulses much faster than
do smaller diameter axons
3. Examples of the Influence of Myelination and Size
- small unmyelinated fibers - 0.5m/sec
- large myelinated fibers - 100m/sec
VII. Rhythmicity
- Self-induced discharge of cells
- Examples include
a. heart
b. smooth muscle - peristalsis
c. Central Nervous System - rhythmic control of breathing
A. Processes Necessary for Rhythmicity to Occur
1. membrane at rest must be more permeable to Na+ or Ca++
2. this ensures that the resting membrane potential is
closer to threshold
3. once threshold is reached Na+ channels open up and Na+
rushes in and an action potential occurs
4. repolarization occurs slowly due to slow opening and
closing of K+ gates (Fig 5-14, p. 61)
CONTRACTION OF SKELETAL MUSCLE
I. Transmission of a Nerve Impulse to Skeletal Muscle
- Contraction of skeletal muscle requires a nerve impulse
A. Neuromuscular Junction (Fig 7-1, p. 81)
1. Motor end-plate
- consist of the nerve terminals that invaginate
into the muscle fiber
- the space between the nerve and the muscle membrane
is termed the synaptic cleft (Fig 7-1C, p. 81)
- folds of the muscle membrane are termed subneural
synaptic clefts and increase the surface area for
neural transmission
B. Release of Acetylcholine (ACh)
1. ACh is stored within synaptic vesicles located in the axon
terminal
2. as the nerve impulse reaches the nerve terminal, it is thought
that the impulse opens up the gates of Ca++ channels (Fig 7-2, p. 81)
3. Ca++ rushes into the axon terminal
4. Ca++ is thought to attract ACh vesicles toward the nerve
membrane adjacent to the calcium channels
5. about 300 vesicles fuse to the membrane of the axon terminal
and release ACh into the synaptic cleft by exocytosis
C. Effect of ACh on the Skeletal Muscle Membrane
1. ACh binds to ACh receptors (ligand-gated channels) located
on the muscle membrane at the subneural clefts (Fig 7-2, p. 81)