CHAPTER 38 Pulmonary Circulation, Pulmonary Edema, Pleural Fluid
Special problems related to pulmonary hemodynamics have important implications for gas exchange in the lungs. The present discussion is concerned specifically with these features of the pulmonary circulation.
Direct measurement of left atrial pressure is difficult because it requires passing a catheter retrograde through the left ventricle. The pulmonary wedge pressure can be measured by floating a balloon-tipped catheter through the right heart and pulmonary artery until the catheter wedges tightly in a smaller branch of the artery. Because all blood flow has been stopped in the blood vessels extending from the plugged artery, an almost direct connection is made through the pulmonary capillaries with the blood in the pulmonary veins. The wedge pressure is usually only 2 to 3 mm Hg higher than the left atrial pressure. Wedge pressure measurements are used often for studying changes in left atrial pressure in persons with various types of heart failure.
The pulmonary blood volume is about 450 mL, or about 9% of the total blood volume. Under various physiological and pathological conditions, the quantity of blood in the lungs can vary from as little as one-half to two times normal.
Left heart failure, mitral stenosis, or mitral regurgitation causes blood to dam up in the pulmonary circulation, greatly increasing pulmonary vascular pressures and volumes. Because the volume of the systemic circulation is about nine times that of the pulmonary system, a shift of blood from one system to the other affects the pulmonary system greatly but usually has only mild effects on the systemic circulation.
Under most conditions, the pulmonary vessels act as passive, distensible tubes that enlarge with increasing pressure and narrow with decreasing pressure. Blood is distributed to the segments of the lungs in which the alveoli are best oxygenated. This is achieved via the following mechanism.
When the alveolar oxygen concentration decreases below normal, the adjacent blood vessels constrict. This is opposite to the effect normally observed in systemic vessels. This vasoconstrictor effect of a low oxygen level distributes blood flow away from poorly ventilated alveoli.
However, sympathetic stimulation has a significant effect in constricting the large pulmonary capacitative vessels, especially the veins. This constriction of large pulmonary veins provides a means by which sympathetic stimulation can displace much of the extra blood in the lungs into other segments of the circulation when needed to combat low blood pressure.
In the normal adult, the distance between the apex and base of the lungs is about 30 cm, which creates a 23 mm Hg difference in blood pressure. This pressure gradient has a marked effect on blood flow in the various regions of the lung.
Under normal and various pathologic lung conditions, any one of three possible zones of pulmonary blood flow can be found:
During exercise the blood flow through the lungs increases fourfold to sevenfold. This extra flow is accommodated in the lungs in two ways: (1) by increasing the number of open capillaries, sometimes as much as threefold, and (2) by distending the capillaries and increasing the flow through each capillary by more than twofold. In the normal person, these two changes together decrease the pulmonary vascular resistance so much that the pulmonary arterial pressure rises very little, even during maximum exercise.
The alveolar walls are lined with so many capillaries that the capillaries almost touch one another; therefore, the capillary blood flows in the alveolar walls as a “sheet” rather than through individual vessels.
Quantitatively, however, there are several important differences:
This value is derived as follows:
Therefore, except in the mildest cases of pulmonary edema, the edema fluid enters the alveoli.
All the following factors must be overcome before edema can occur: (1) normal negativity of the interstitial fluid pressure, (2) lymphatic pumping of fluid out of the interstitial spaces, and (3) decreased colloid osmotic pressure of the interstitial fluid caused by “washout” resulting from increased loss of fluid from the pulmonary capillaries.
In the human being, who normally has a plasma colloid osmotic pressure of 28 mm Hg, the pulmonary capillary pressure must rise from the normal level of 7 mm Hg to more than 28 mm Hg to cause pulmonary edema, giving an acute safety factor against pulmonary edema of about 21 mm Hg.
The lymph vessels can expand greatly and proliferate over a period of several weeks to months, increasing their ability to carry fluid away from the interstitial spaces by perhaps as much as 10-fold. In a patient with chronic mitral stenosis, a pulmonary capillary pressure of 40 to 45 mm Hg has been measured without the development of significant pulmonary edema.
When the pulmonary capillary pressure does rise even slightly above the safety factor level, lethal pulmonary edema can occur within minutes to hours. With acute left-sided heart failure, in which the pulmonary capillary pressure occasionally rises to 50 mm Hg, death often ensues within less than 30 minutes from the onset of acute pulmonary edema.
Small amounts of interstitial fluid transudate continually across the pleural membranes into the pleural space. These fluids contain proteins, which give the pleural fluid a mucoid character, allowing easy slippage of the moving lungs. The total amount of fluid in the pleural cavities is only a few milliliters. The pleural space—the space between the parietal and visceral pleurae—is called a potential space because it normally is so narrow it is not obviously a physical space.
The possible causes of effusion are the following: