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Chapter 5<br />

Venous Hemodynamics<br />

Torvid Kiserud<br />

In recent years evaluation of the venous system has<br />

become a compulsory part of the haemodynamic assessment<br />

of the fetus, but the underlying mechanisms<br />

of our Doppler recordings are still incompletely understood.<br />

The present chapter is not intended to solve<br />

all that, but rather to address important hemodynamic<br />

issues from a clinical point of view to help clinicians<br />

use and interpret venous Doppler recordings.<br />

For the interested reader more extensive discussions<br />

of blood flow dynamics are available in the literature<br />

[1±5].<br />

Velocity Profile in Veins<br />

Parabolic Blood Velocity Profile<br />

and Flow Calculation<br />

In a straight section of the umbilical vein with a<br />

steady velocity, the distribution of the velocity across<br />

the cross-sectional area of the vessel is assumed to be<br />

parabolic with the highest velocity (V max ) in the center<br />

of the cross section (Fig. 5.1). The ratio of the<br />

average velocity across the vessel (V mean ) and the<br />

V max characterizes the velocity profile. For parabolic<br />

flow, the ratio V mean /V max is 0.5.<br />

For calculating volume flow we need the averaged<br />

velocity across the vessel area. We can derive that by<br />

tracing the weighted mean velocity (V w.mean ) of the<br />

Doppler recording. Ideally, with a strictly parabolic<br />

flow, the relation would be V w.mean =V mean = 0.5 V max .<br />

This is particularly useful since the intensity-weighted<br />

mean velocity (V w.mean ) derived from the Doppler<br />

shift is easily influenced by low-velocity signals from<br />

the vessel wall or neighboring vessels, or from loss of<br />

low-velocity recordings due to filters, or loss of the<br />

weakest signals when travelling through the tissues.<br />

Secondly, the V w.mean represents the average of the velocities<br />

recorded in the sample volume (Doppler<br />

gate), which is not identical to the vessel cross-section.<br />

The sample volume may cover the vessel incompletely<br />

or asymmetrically. The low velocities at the<br />

periphery of the vessel are more likely to be underrepresented<br />

than the high axial velocities of the center.<br />

In short, we have two ways of calculating blood<br />

flow:<br />

and<br />

p…D=2† 2 V w:mean<br />

p…D=2† 2 0:5V max<br />

Fig. 5.1. The velocity profile represents the velocity distribution<br />

across the vessel and is characterized by the V mean /<br />

V max ratio. The steady blood flow in the umbilical vein has<br />

a parabolic velocity profile (i.e. ratio 0.5). The accelerated<br />

blood at the ductus venosus inlet has a partially blunted<br />

velocity profile corresponding to a ratio of 0.7, while at the<br />

cardiac outlets the profile is even more blunted (e.g. ratio<br />

0.97). (From [17])<br />

the latter being the more robust, provided the velocity<br />

actually is parabolic.<br />

That may not always be the case. For example, the<br />

velocity profile is found to be more blunted the first<br />

few centimetres after the umbilical vein has left the<br />

placenta [6]. During acceleration or retardation the<br />

velocity profile changes, and variation in geometry,<br />

branching and curvature alter the velocity profile<br />

(Fig. 5.2). These changes are further determined by<br />

the viscosity of the blood and dimension of the vessel<br />

expressed in the Reynold's number [1]. These facts<br />

favor the use of V w.mean , which is not dependent on a<br />

known profile factor; thus, it has not been determined<br />

which method is the best, and the literature<br />

has examples of both methods [7±14].

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