If the vascular system were composed of a central pump, projecting at every stroke a given amount of liquid into a series of rigid tubes, the aggregate cross sections of which were equal to the cross section of the main pipe, then the velocity at the openings would be the same as at the source (making allowances for friction). The problem would then be a simple one. In the circulation of the blood no such simple condition obtains. The capillary beds is an enormous area through which the blood flows slowly. From the time the blood is thrown into the aorta the velocity begins to diminish until it reaches its minimum in the capillaries. In no two persons is the initial velocity at the heart the same, nor in the same person is it the same at all times of day. The size of the heart, the actual strength of the muscle, the amount of blood ejected at every beat, and the size and elasticity of the aorta are some of the factors which determine the velocity of blood at the aortic orifice. When to these factors are added the differences in arterial tissue, the activity or resting stage of the various organs, etc., the question becomes exceedingly complicated. In spite of these many disturbing elements, attempts more or less successful have been made to estimate the velocity of the blood in animals. Thus, in the carotid of the horse the velocity was found to be 300 mm. per second (Volkman) and 297 mm. (Chauveau); in the carotid of the dog, 260 mm. (Vierordt). In the jugular vein of the dog Vierordt found the velocity to be 225 mm. per second. These figures do not represent the actual velocity of the blood in all horses or all dogs, but they do give us some general idea of the rate of flow of the blood. For man it has been calculated that the velocity in the aorta is about 320 mm. per second. The velocity is not uniform in the large arteries, where at every heart beat there is a sudden increase followed by a decrease as the heart goes into diastole. The farther away from the heart the measurements are made the more even is the flow. Observations by W. H. Luedde with the Zeiss binocular corneal microscope on the rate of flow in the conjunctival capillaries must modify somewhat our former conceptions. He finds that "The rate varies in the different arteries, capillaries, and veins from a barely perceptible motion to a little more than 1 mm. per second. Further, some parts of the capillary network are ordinarily supplied with blood elements only occasionally. This is shown by the passage of a column of corpuscles along a certain line, followed after an interval of seconds, during which no corpuscles pass, by another column in the same line as before."