Arteriosclerosis and Hypertension, with Chapters on Blood Pressure: 3rd Edition.Warfield, Louis M. (Louis Marshall)
Science
Arteriosclerosis and Hypertension, with Chapters on Blood Pressure: 3rd Edition.
Warfield, Louis M. (Louis Marshall)
Arteries -- Diseases; Blood pressure
[Illustration: Fig. 30.--Figures are to be read from left to right. The
top line records the points where sounds were heard, the figures above
the short vertical lines refer to tones (see text). Mx. B. P., maximum
blood-pressure. M. B. P., minimum blood-pressure. P. B., pressure bulb
recorder. It was impossible to lower and raise this bulb by hand without
obtaining the great irregular oscillations of the attached lever above
the mercury manometer. B. L., base line.]
Erlanger showed some years ago, that with his instrument, the point at
which diastolic pressure should be read was at the instant when the
maximum oscillation of the lever suddenly became smaller. While
checking up the graphic with the auscultatory method using Erlanger's
instrument, it was noticed that the disappearance of all sound did not
correspond with the sudden diminution of the oscillation of the lever
connected with the brachial artery. A series of records were carefully
made on patients. It was seen that during the period of the third tone
phase the oscillations of the lever on the drum reached a maximum (Fig.
31) and remained at approximately the same height for some millimeters
while the pressure was gradually falling. At a point at which the third
tone, clear and distinct, became dull, there was an appreciable decrease
in the height of the pulse wave. From this point to the disappearance of
all sound there was a gradual diminution of the size of the pulse
waves.
[Illustration: Fig. 31.--Fast drum. Sudden decrease in size of pulse
wave at 4, marking the change from clear sharp tone to dull tone.]
[Illustration: Fig. 32.--Slow drum. Sudden decrease in amplitude at 4.]
For normal pressures the difference between the fourth (dull) tone and
the fifth (disappearance of all tone) phase, amounted to 4 to 10 mm.
Occasionally the difference was so little, the change from sharp third
tone through fourth dull tone to disappearance of all sound was so
abrupt, that one could take the disappearance of all sound as the
diastolic pressure, with an error of not more than 2 to 4 mm. This is
within the limits of normal error and practically may be used by those
who have difficulty in noting the change from third to fourth phase. For
high pressures, however, the difference between fourth and fifth phases
was never less than 8 mm., and was found as much as 16 mm. The
diastolic, therefore, should always be taken at the fourth phase if
possible.
It was found that with the dial instrument the greatest fling of the
lever corresponded to the third phase and the sudden lessened amplitude
of the oscillation was at the fourth phase and was coincident with the
change of tone from sharp to dull. Thus the diastolic pressure may be
read off on the dial scale by watching the fling of the hand and with
some practice one might acquire considerable accuracy. It is better,
simpler, and, for most observers, more accurate to use the stethoscope
and hear the change of sound.
Public-domain text, read in full here on John Shaqi.
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