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16.4. PROPAGATION OF ACTION POTENTIALS<br />

When a cell is excited and generates an action potential, an<br />

ionic current begin to flow. This process can, in turn, excite<br />

similar neighboring cells. With nerve cells that have a long fiber,<br />

the action potential is generated over a very small segment of the<br />

fiber's length, however, it is propagated in both directions from<br />

the original point of excitation. The rate at which an action potential<br />

moves down a fiber or is propagated from cell to cell is<br />

called the propagation rate. The velocity of the propagation rate<br />

varies widely. The usual velocity range in nerves cells is 20 ­<br />

140 rn/s; propagation through heart muscle is slower, with an<br />

average rate of 0.2 - 0.4 m/s,<br />

16.5. ELECTROCARDIOGRAPHY<br />

The biopotentials generated by the muscles of the heart result<br />

in the electrocardiogram (abbreviated ECG) and the technique<br />

used to measure these potentials is called electrocardiography.<br />

Each action potential in the heart originates near the top of the<br />

right atrium at a point called the sinoartrial node - a group of<br />

specialized cells that spontaneously generate action potentials at a<br />

regular rate. The action potential propagates in all directions<br />

along the surface of both<br />

atria. A graphic recording<br />

or display of the time-variant<br />

voltages produced by<br />

the myocardium during the<br />

cardiac cycle is called an<br />

electrocardiogram. Fig. 16.4<br />

shows the basic waveform<br />

of a normal electrocardiogram.<br />

The P, QRS, and<br />

T waves reflect the rhythmic<br />

electrical depolarization<br />

and repolarization of<br />

the myocardium associated<br />

with the contractions of<br />

the atria and ventricles. The<br />

124<br />

R<br />

5mm It I<br />

0.2s f-<br />

emm fo-f0-<br />

0.5mV<br />

1-1 III It<br />

Imm 0.4~ -fij1lmm<br />

25mm/s O.lmV<br />

10mm/mV<br />

P-R S T T<br />

f---P '+---0< ,<br />

....segment segment i.oI" U<br />

-I ~ .I<br />

I I •<br />

fo-P R-<br />

interval S S-T<br />

mterval- -<br />

QRS interval I I<br />

+-t--IO-T interval- -<br />

f--<br />

Fig. 16.4. The important intervals<br />

and segments in the electrocardiogram<br />

z·."<br />

'~'<br />

electrocardiogram is used clinically in diagnosting various diseases<br />

and conditions associated with the heart.<br />

16.6. THE EINTHOVEN'S TRIANGLE<br />

An ECG can be described in terms of the cardiac vector. The<br />

electrical activity of the heart corresponds to the movement of an<br />

electrical di pole which consists of a positive and a negative charge<br />

separated by a variable distance. The cardiac vector is the line<br />

joining the two charges. To fully describe the cardiac vector, its<br />

magnitude and direction must be known. Usually the cardiac<br />

0<br />

vector is described by its length in three directions at 60 to each<br />

other. The resulting geometric pattern (fig. 16.5) is known as<br />

Einthoven 's triangle. The sides of the triangle represent the lines<br />

along which the three projections of the ECG vector are measured.<br />

The magnitudes and directions of these projections depend<br />

strongly on the state of the patient's heart. The direction of normal<br />

cardiac vector runs between 0 - +90'; the other directions<br />

correspond to various pathological situations.<br />

.~ -90 0<br />

~<br />

~'<br />

a<br />

c<br />

AI<br />

AlII<br />

AI<br />

VI Fig. 16.5. The Einthoven's<br />

triangle: the dependence<br />

of the magnitudes and<br />

All directions of the ECG<br />

vector projections<br />

VIII on the state of the<br />

patient's heart<br />

125

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