1. Excitable tissues include nervous, muscle and glandular epithelial tissues. They have the ability to generate action potentials in response to stimuli.
2. Galvani discovered "animal electricity" by stimulating muscles in a frog's leg with two different metals, founding the field of electrophysiology. Volta proved the electricity came from the metals, not from within the animal.
3. The membrane potential of cells is measured using microelectrodes. At rest, excitable cells maintain a negative interior potential of around -70mV due to ion pumps and selective ion permeability.
2. Plan
• Properties of excitable tissues
• History of the study of bioelectric phenomena
• Resting potential
• Action potential of nerve cell
• Excitability change at excitation
• Propagation of an action potential in nerve
fibers
3. What is the tissues?
Tissues (biology, histology)
are groups of cells with
• a common origin
• a common structure
• and a similar function
7. Why are they called excitable
tissues?
• Stimulus acts on tissue
• Response of Excitable tissue is excitation or
irritation
8. Non-excitable tissues
• Red cells
• Intestinal cells
• Fibroblasts and etc.
Why are they called non-excitable tissues?
• Response of Non-Excitable tissue is only irritation
14. Classification of stimuli:
• By the nature
- the external: physical, chemical, biological
- the internal: physiologically active substances
• By force
- Subthreshold
- Threshold
- Suprathreshold
• The Threshold is the minimal stimulus capable to
cause tissue response.
15. THE GENERAL PROPERTIES OF EXCITABLE
TISSUES
•
1. EXCITABILITY
- is the ability of tissue to react to the stimulation with change of
physiological properties and generation of process of excitation. Excitability
of cells and tissues is a basic function of life.
2. CONDUCTIVITY
- ability to conduct impulse.
3. LABILITY
- ability to conduct certain quantity of impulses per
time.
4. CONTRACTILITY
- ability to change the size (to contract) and tension.
17. Electrophysiology
• is the study of the electrical properties of
biological cells and tissues.
• It involves measurements of voltage change or
electric current on a wide variety of scales
from single ion channel proteins to whole
organs like the heart.
19. Luigi Aloisio Galvani
• 1737 – 1798
• was an Italian physician,
physicist and
philosopher
• Founder of
electrophysiology
• he discovered “animal
electricity”
20. The 1st Galvani’s experiment
In 1771, Galvani was able to cause
muscular contraction without a
source of electrostatic charge by
touching the frog’s nerve with
different metals. After further
experimenting with natural (i.e.
lightning) and artificial (i.e. friction)
electricity, he concluded that
animal tissue contained its own
innate vital force, which he termed
"animal electricity."
21. • A.Volta repeated L.Galvani’s experiments
and
• By 1800, Volta proved that the source of
the electricity was metals.
23. Galvani vs. Volta:
• animal electricity or chemical energy of two
different types of metal converted into
electrical energy?
• So is there an animal electricity or
not?
24. The 2nd Galvani’s experiment
Cut across the hip muscle of the
other leg of the frog
Place the buttock’s nerve of
the paw in the cross-section on
the leg muscle and observe the
reaction
30. Electrical potentials exist across the
membranes of virtually all cells of the body.
In addition, some cells, such as nerve and
muscle cells, are capable of generating rapidly
changing electrochemical impulses at their
membranes, and these impulses are used to
transmit signals along the nerve or muscle
membranes. In still other types of cells, such
as glandular cells, local changes in membrane
potentials also activate many of the cells’
functions.
31. Diffusion potentials
• A diffusion potential is the potential difference generated
across a membrane because of a concentration difference
of an ion.
• A diffusion potential can be generated only if the
membrane is permeable to the ion.
• The size of the diffusion potential depends on the size of
the concentration gradient.
• The sign of the diffusion potential depends on whether the
diffusing ion is positively or negatively charged.
• Diffusion potentials are created by the diffusion of very few
ions and, therefore, do not result in changes in
concentration of the diffusing ions.
33. Equilibrium Potential
The equilibrium potential is
the potential difference
that would exactly balance (oppose)
the tendency
for diffusion down
a concentration difference.
At electrochemical equilibrium,
the chemical and
electrical driving forces
that act on an ion are equal and
opposite, and no more
net diffusion of the ion occurs.
34. Equilibrium potential Nernst Equation
• Eion = 2.303 RT/zF log [Cion]o/[Cion]in
• Eion = equilibrium potential
• Z= charge of ion
• F= Faraday’s constant
• T= absolute temperature (0Kelvin/-273°C)
• R= gas constant
The Nernst equation is used to calculate the equilibrium
potential at a given concentration difference of a permeable ion
across a cell membrane. It tells us what potential would exactly
balance the tendency for diffusion down the concentration
gradient; in other words, at what potential would the ion be at
electrochemical equilibrium?
38. Generation of Resting Membrane
Potential (-70mV)
• Action of ion pumps 3Na/2K ATPase that
maintain ion concentrations
• Unequal distribution of ions across
membrane
• Selective permeability, permeable to K+, not
Na+
39. Goldman-Hodgkin-Katz equation (G-
H-K equation, Goldman equation)
• The actual resting membrane potential (Em) for a
system involving more than one permeable ion is
calculated by the Goldman-Hodgkin-Katz equation
(G-H-K equation), which takes into account the
permeabilities and concentrations of the multiple
ions.
45. ACTION POTENTIAL of NERVE CELL
Step 1: Resting membrane potential
Step 2: Some of the voltage-gated Na-channels
open and Na+ enters the cell
Step 3: Opening of more voltage-gated
Na-channels and further depolarization (rapid upstroke)
Step 4: Reaches to peak level
Step 5: Direction of electrical gradient for Na is reversed + Na-
channels rapidly enter a closed state “inactivated state” +
voltage – gated K-channels open (start of repolarization)
Step 6: Slow return of K-channels to the closed state
(hyperpolarization)
Step 7: Return to the resting membrane potential
46. Voltage-gated channels
How voltage-gated channels work
At the resting potential, voltage-
gated Na+ channels are closed.
Conformational changes open
voltage-gated channels when
the membrane is depolarized.
Two important types:
1.) Na+ voltage gated channels
2.) K+ voltage gated channels
48. Initial Depolarization - Some Na+ channels open. If enough Na+
channels open, then the threshold is surpassed and an action
potential is initiated.
53. An Action Potentials has 2 Refractory Periods
1. Absolute Refractory Period: During this period, the cell is
unresponsive to any further stimuli. No other action potential can
be fired at this point, regardless of the strength of the stimuli.
Explanation: Recall that the inactivation gates of the Na+ channels
are closed when the membrane potential is depolarized. They remain
closed until repolarization occurs. No action potential can occur until
the inactivation gates open.
The role of the Absolute refractory period is to ensure one-way
propagation of action potentials.
2. Relative Refractory Period: During this period, another action
potential can be produced but the strength of the stimuli must be
greater than normal to trigger an action potential.
The role of the Relative refractory period: helps to limit the
frequency of action potentials.
57. Propagation of action potential
occurs by the spread of local currents to adjacent areas of membrane,
which are then depolarized to threshold and generate action potentials.
An important characteristic of action potential
propagation is that it occurs away from the point of
initiation; it cannot travel back toward its origin. As the
action potential is conducted, the area of the
membrane directly behind the action potential is still in
the absolute refractory state due to Na+ channel
inactivation, preventing retrograde conduction.
.
58. CONDUCTION of the ACTION POTENTIAL
• Unmyelinated nerve
axon:
– Positive charges from the
membrane ahead and behind
the action potential flow into
the area of negativity.
– By drawing off (+) charges,
this flow decreases the
polarity of the membrane
ahead of the action potential.
– This initiates a local response.
– When the threshold level is
reached, a propagated
response occurs that in turn
electronically depolarizes the
membrane in front of it.
59. CONDUCTION of the ACTION POTENTIAL
• Myelinated nerve
axon:
– Myelin is an effective
insulator.
– Depolarization travels
from one node of
Ranvier (where there are
gaps in the myelin
sheath, D=0.5μm) to the
next.
- This jumping of
depolarization from node to
node is called “saltatory
conduction”
– Faster than
unmyelinated axons.
60. Action Potential of Contractile Cardiac cells
Phase 0 - depolarization
Phase 1 - Rapid, partial, early
repolarization
Phase 2 - plateau
Phase 3 – slow repolarization
Phase 4 – resting membrane
potential (RMP)
Phase Membrane channels
PX = Permeability to ion X
+20
-20
-40
-60
-80
-100
Membranepotential(mV)
0
0 100 200 300
Time (msec)
PK and PCa
PNa
PK and PCa
PNa
Na+ channels open
Na+ channels close , K channels open
Ca2+ channels open; K+ channels open
Ca2+ channels close; K+ channels open
Resting potential
1
2
30
4 4
0
1
2
3
4
61. The main physiological characteristics of the AP
1. Obeys the law of "all or nothing." This means that:
• AP occurs when the stimulus, the power which is no less
than certain thresholds;
• Physical characteristics of the AP (amplitude, duration,
shape) does not depend on the power of stimulus.
2. Ability to autospread along the cell membrane without damping, i.e.
without changing their physical characteristics.
3. AP accompanied with refractory.
4 AP is no capable to summation.
62. QUESTIONS
1. The terms "tissue” and "excitable tissues."
2. Irritability and excitability as the main types of tissue response to stimulation.
3. Properties of excitable tissues.
Stimuli and their classification.
4. History of the study of bioelectric phenomena:
4.1. The first experience L.Galvani.
4.2. The second experiment L.Galvani without metals.
5. Methods for measuring the membrane potential.
6. Diffusion potential.
7. Equilibrium potential. Nernst equation.
8. Resting membrane potential of nerves. Origin of resting membrane potential.
9. Goldman-Hodgkin-Katz equition
10. The nerve action potential. Depolarization, repolarization, hyperpolarization, threshold stimulus,
local response.
11. Stages of the nerve action potential. Ionic bases of the action potential.
12. Propagation of an action potential in the unmyelinated nerve fibers.
13. Propagation of an action potential in myelinated nerve fibers.
14. Cardiac action potential.