To this type belong the majority of the arterial vessels.
The valves of the veins are reduplications of the intima, and the greater part of the valvular structure consists of fibrous connective tissue and elastic fibres.
flows out with great force in a series of jerks which are synchron ous with the heart beat. When a large vein is cut, the blood also flows out rapidly, but the stream has very little force.
The first measurement of arterial pressure was made by the Rev. Dr. Stephen Hales. ("Statical Essays, containing Haema staticks" ) Since Hales' work, the chief improvements in the method have been the application of the mercury manometer by Poiseuille, the invention of the recording manometer and the kymograph by Lud wig (figure i6), and the intro duction of the more accurate membrane manometer by Hiir thle and Frank.
The manometer of Ludwig con sists of a U-tube which is half filled with mercury. On the sur face of the mercury of one limb is a float from which a stiff light rod projects, bearing on its upper end a writing point which is made to write on the smoked surface of a revolving drum. The other limb of the manometer is connected by means of a glass or metal can nula to the artery. The tube be tween the artery and the manom eter is filled with a solution of some anticoagulant salt (sodium citrate, magnesium sulphate).
The mercury manometer allows a direct reading of pressure, but on account of its inertia it does not accurately record rapid changes in the pressure. The membrane manometer, which is merely a tube filled with fluid and sealed at one end with a stretched rubber membrane, records rapid changes in pressure more accurately, but each membrane requires special calibration if absolute values are desired. The venous pressure is recorded by a similar method, but with a water manometer or a manometer with a lightly stretched membrane.
The highest pressure, which occurs while the blood is passing from the heart into the aorta, is called the systolic arterial pres sure, and the pressure at the end of diastole is the diastolic pres sure; the range between these two extremes is known as the pulse pressure. In the dog, with a mean arterial pressure of about 120 mm. of mercury, the systolic pressure may be as high as 16o mm., and the diastolic pressure as low as 65 mm. ; here the pulse pres sure would be 95 mm. of mercury. By taking the pressure at dif ferent parts of the vascular system, we obtain a result which is diagrammatically represented in figure 18.