Pulmonary circulation

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Chapter 8 Pulmonary circulation

The pulmonary circulation is contained wholly within the thorax. It is, therefore, much shorter than most regional beds of the systemic circulation. As well, all segments of the pulmonary vessels are slightly larger in radius than the corresponding segments of the systemic vasculature. The net result of these two factors is that the pulmonary circulation exerts a resistance to flow only around 15% of that in the systemic circuit. Hence it requires a correspondingly far lower pressure gradient in order to move the same cardiac output. At rest, pulmonary arterial pressure is typically 25/8 mmHg, giving a mean arterial pressure of the order of 14 mmHg, and mean pulmonary capillary pressure is 7–8 mmHg rather than the 25–30 mmHg seen in systemic vascular beds.

FUNCTIONAL CONSEQUENCES OF LOW PULMONARY BLOOD PRESSURE

Gas diffusion

In systemic capillaries the balance between oncotic and hydrostatic pressures mean that small increases in hydrostatic pressure caused, for example, by reduced arteriolar resistance will result in significant movement of plasma water into the interstitium. When a large tissue mass, such as skeletal muscle, is involved, this movement will cause a substantial reduction of plasma volume (see Chapter 9, p. 112), but the increased interstitial volume does not prejudice diffusion of solutes between cells and bloodstream because the intercellular connective tissue minimizes tissue expansion. In the lung, by contrast, there is little supporting tissue. If water moves into the interstitial space separating the pulmonary capillaries from the alveoli, it pushes these two structures further apart and increases the distance over which gases must diffuse between air and plasma.

The speed of this diffusional process decreases very rapidly with increased distance, so efficient lung function depends on minimizing the interstitial space by keeping it free of extra water. A pulmonary capillary hydrostatic pressure of 7–8 mmHg is three times less than plasma oncotic pressure. Therefore, there is normally quite a large net inward osmotic gradient to maintain this situation. If, however, capillary pressure rises to levels similar to those in systemic capillaries, then interstitial water starts to accumulate (pulmonary oedema) and gas exchange may become compromised.

This situation results commonly from damage to the mitral valve that separates left atrium and ventricle. Either valvular stenosis or incompetence will elevate left atrial pressure and this will cause a proportionate change in capillary pressure, which may rise as high as 40–50 mmHg with severe valve damage. Paradoxically, patients in whom chronic valve damage has led to a progressive, slow rise in left atrial pressure often have far less pulmonary oedema than would be expected from the absolute pressure changes. This seems to be because, under these circumstances, the lymphatic system within the lung becomes more efficient in recycling fluid from the interstitial spaces.

The practising exercise physiologist is most likely to encounter pulmonary oedema as a consequence of high altitude, since it occurs in many healthy individuals who ascend to heights greater than 3000 m, well below the altitude of many ski resorts and permanent settlements. We will return to examine the reasons for this response to altitude in Chapter 12 (p. 151).

REGIONAL MATCHING OF VENTILATION AND PERFUSION

Vertical variations

In a resting, upright individual, dramatic differences in both respiratory ventilation and pulmonary perfusion exist along the vertical axis of the lung. Resting inspiration is due to elevation of the ribs and lowering of the diaphragm, but the shape of the ribcage means that the increase in thoracic volume that occurs becomes progressively more pronounced towards the lung bases. The fact that the lung apices are around 10 cm higher than the heart means that the vessels there are perfused only when pulmonary arterial pressure exceeds this value (10 cm H2O = 14 mmHg). Thus, there is only intermittent apical perfusion, especially during expiration when intra-thoracic pressure rises and compresses the capillaries. By contrast, the lung bases are gravitationally lower than the heart; therefore, the perfusion pressure for vessels in this region is several mmHg higher than that at heart level and perfusion is correspondingly greater.

Although both ventilation and perfusion rise towards the base of the lungs, the gravitational effect on regional blood flow is rather more powerful than the vertical variation in ventilation, with the result that the ratio of ventilation image to perfusion image is around 3 at the apices and around 0.5 at the bases. Exact matching of the two is achieved only over a relatively narrow region of lung corresponding to about the mid-sternal level (Fig. 8.1).

Effects of intrapulmonary gas tensions

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