Fig. 34.—New venous pressure instrument. (After Eyster.)

Practically Hooker and Eyster found that the normal variation in healthy subjects was from 3 to 10 cm. of water. The pressure rose in cases of decompensated hearts with dyspnea and venous stasis, and returned to normal with improvement in the condition of the patient. It might be possible with this instrument to foretell an oncoming decompensation by the rise in venous pressure.

The venous pressure may also be estimated roughly by slowly elevating the arm and noting the instant at which a particular vein collapses. By measuring the height of the vein above the heart some idea may be obtained of the pressure within the right auricle.

The Pulse

There is nothing characteristic about the pulse of a person suffering from arteriosclerosis, except it be the difference in the pulse of high tension and of low tension. The pulse of high tension has a gradual rise, a more or less rounded apex, and the dicrotic wave is slightly marked and occurs about half-way down on the descending limb. In arteriosclerosis with low tension the radial artery is usually so rigid that very little pulse wave can be obtained. The general form of a low tension pulse is a sharp upstroke, a pointed summit, and a secondary wave on the base line, which corresponds to the dicrotic wave. Such a pulse can be easily palpated, and is known as a dicrotic pulse. However, such a pulse can occur only when the artery still retains all or a large part of its elasticity; hence in arteriosclerotic low tension we would never see such a pulse as the typical dicrotic.

The Venous Pulse

It would carry us too far to discuss fully the character of the venous pulse, but a brief summary of the essential features of the normal venous pulse is presented. The venous pulse is a term used to express the tracing obtained from the internal or external jugular vein at the root of the neck. Normally a very characteristic curve is produced, which can be readily analyzed into a series of waves corresponding to the fluctuations in the cardiac cycle. To understand these waves and their values, the accompanying figure is helpful. (Fig. 35.)