Effects of high altitude

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Chapter 12 Effects of high altitude

ALTITUDE AND OXYGEN TRANSPORT

Effects of altitude on plasma oxygen uptake

The standard atmospheric pressure of 760 mmHg (101 kPa) at sea level reflects the weight exerted by the gas molecules that make up the air, under gravitational force. As one ascends from sea level, the air becomes progressively less compressed and so the constituent gas molecules become less tightly packed. In consequence, a given volume of inspired air contains fewer molecules of all gases, including oxygen. The relationship between altitude and atmospheric pressure is not a strictly linear one because the air volume increases in 3 dimensions but, in rough terms, pressure falls by around 100 mmHg for every 1000 m (3300 ft) of ascent up to 3000 m (10 000 ft) (Fig. 12.1).

The absolute change in oxygen availability imposed by a given ascent can be calculated easily. Since oxygen represents 21% of normal air, the partial pressure of oxygen (PO2) at sea level is (21%.760) or 160 mmHg. Once inspired, the air becomes saturated with water vapour (partial pressure 47 mmHg) so that the total gas pressure is reduced to 713 mmHg and PO2 falls to (21%.713) or 150 mmHg. In the alveoli, the oxygen is diluted further by approximately 50 mmHg, due primarily to the presence of carbon dioxide, resulting in a local PO2 (PAO2) of around 100 mmHg: at equilibrium with the plasma, arterial PO2 (PaO2) is, therefore, usually also around 100 mmHg.

At an atmospheric pressure of 560 mmHg, which corresponds to an altitude of around 2300 m (7600 ft) or just higher than Mexico City, PAO2 can be estimated to be around 60 mmHg (21%.[560–47] – 50). Many of the major ski resorts like Aspen and Zermatt involve slopes at heights in excess of 3500 m (11 000 ft), where atmospheric pressure is 500 mmHg and so PAO2 will be around (21%.[500–47] – 50) or 45 mmHg, while permanent settlements in the Himalayas and Andes are found as high as 5000 m (17 500 ft) where atmospheric pressure is only 390 mmHg and calculated PAO2 is around 25 mmHg.

Effects of altitude on oxygen carriage

Because of the sigmoid shape of the haemoglobin dissociation curve, the falls in PaO2 associated with acute exposure to altitudes up to around 2000 m (6700 ft) cause only a slight reduction in haemoglobin saturation (Fig. 12.2) and so do not reduce oxygen delivery at rest. During exercise, however, the combination of reduced binding and reduced pulmonary capillary transit time leads to a greater degree of desaturation that is proportional both to altitude and to cardiac output. Thus, the threshold altitude for oxygen limitation of maximum exercise in sedentary individuals is typically around 1500 m (5000 ft), but, in trained athletes with substantially greater cardiac outputs, maximum work capacity begins to fall at much lower altitudes (Johnson et al 1994). In the only Summer Olympics held at a significant altitude, in Mexico City in 1968, winning times for all track events longer than 800 m were well above the existing records.

COMPENSATION FOR HYPOXIA

Respiratory stimulation

The reduced oxygen carriage associated with moderate altitude results in more rapid fatigue during exercise, but no respiratory compensation occurs because ventilation is still driven by the central chemoreceptors. These respond to rises in local proton concentration (that is, reduced pH) secondary to arterial carbon dioxide diffusing into the hindbrain, but are insensitive to hypoxia. The peripheral chemoreceptors responsible for monitoring arterial oxygen status are triggered only when PaO2 falls to around 60 mmHg which, as we saw earlier (p. 145), corresponds to an approximate altitude of 2300 m or 7600 ft. At or above this height, chemoreceptor stimulation initiates increased minute ventilation the magnitude of which depends both on the initial PaO2 and on whether increased ventilation is able to restore PaO2 to a value above 60 mmHg.

This acute ventilatory compensation for hypoxia occurs very rapidly, but is itself able to produce only a moderate improvement in oxygen availability. The reason is that increased ventilation necessarily results in carbon dioxide being blown off at a greater rate than before, leading to a fall in arterial carbon dioxide (PaCO2) (hypocapnia) and, therefore, to a rise in hindbrain pH and reduced central chemoreceptor drive, inhibiting the stimulant effect of the hypoxic drive.

With maintained exposure to the hypoxic environment, the inhibition of central chemoreceptor drive diminishes over the next several days. Most rapidly, there is over 1–2 days’ diffusion of excess bicarbonate ions out of the interstitial fluid around the central chemoreceptors that reduces buffering of interstitial protons. Over the next 2–3 days, renal bicarbonate excretion amplifies this process and restores central pH and respiratory drive to normal despite the maintained hypocapnia, although arterial pH remains slightly more alkaline than normal. As a result of these adjustments, minute ventilation rises progressively over the first week of hypoxic exposure, with an associated progressive increase in work capacity that is due both to the increased inspired air volume and to the fact that the enhanced ventilation has reduced alveolar PCO2 further and, therefore, the oxygen tension of alveolar air rises. At very high altitudes, the decrease in air density may also contribute to increased capacity for maximum ventilation.

ALTITUDE AND WORK CAPACITY

Benefits of adaptation for exercise capacity at high altitude

The spectrum of compensatory processes means that fully acclimated individuals have vastly better capacities for work than when they first arrive at altitude. They are, however, still not able to achieve workloads identical to those that were possible at sea level. The compensations that occur cannot overcome fully the reduced haemoglobin saturation imposed by a low PaO2 and, in addition, the adaptive processes themselves impose some limits of circulatory efficiency. One problem is that increased haematocrit increases blood viscosity and so increases cardiac workload for a given cardiac output. In addition, the rightwards shift of the haemoglobin dissociation curve induced by DPG has the effect of, under moderate-to-severely hypoxic conditions, reducing pulmonary loading of oxygen as well as increasing the unloading process (Fig. 12.3). Finally, since even slight alkalosis shifts the dissociation curve to the left, the profound hypocapnia seen in fully acclimated individuals may actually reverse the effect of DPG and reduce capillary oxygen unloading.

For athletes who live at low altitudes, a period of acclimation is obviously essential if they are to compete effectively at higher altitudes but, even then, the limits to adaptation described above are likely to restrict their performance. The same limitations are not evident to the same extent in natives of high altitude communities, who appear to possess cardiorespiratory systems that are better adapted to hypoxia. It remains uncertain to what extent these differences from low-level residents are genetically determined and to what extent they are developed during childhood.

Benefits of adaptation for exercise capacity at low altitude

The greatest significance for athletic performance of adaptations to high altitude is its potential effect on performance at low altitude. Here, the positive effects on oxygen delivery of DPG and raised haematocrit can be exploited without interference from reduced ambient oxygen availability or hypocapnia. This scenario has led to training at altitude being adopted as a routine component of preparation for competition of many athletes. Unfortunately, the value of this strategy is limited by the reduced intensity of training that is possible under hypoxic conditions. More convincing results have been obtained by allowing training to be carried out at low altitude and stimulating the haematological adaptations by exposure to a hypoxic environment overnight (Hendricksenn & Meeuwsen 2003).

The potential advantages for performance of adaptations to hypoxia have led to the administration of synthetic erythropoietin in order to increase haematocrit. Leaving aside the illegality, ‘blood doping’ with erythropoietin carries with it very substantial risks. The normal response to hypoxia incorporates both increased red cell mass and increased oxygen carriage efficiency through DPG expression. The red cells produced in response to erythropoietin do not have up-regulated DPG and so, in order to achieve a given increment in tissue oxygen delivery, there needs to be a much greater increment in red cell mass. In consequence, athletes who have taken erythropoietin may have haematocrits of the order of 70%, with massively elevated cardiac workload and a significant risk of cardiac events during exercise, as well as increased risk of venous thrombosis due to red cell clumping (see Chapter 5, p. 55).

PROBLEMS WITH EXPOSURE TO ALTITUDE

Dehydration

The progressive temperature fall not only has direct implications for thermoregulation, but also greatly affects water balance. As air temperature falls, the air becomes progressively drier, so that at 0° C (32° F) saturated water vapour pressure is only around 30% of its value at 20° C (68° F). When this air is inspired, its temperature rises to that of the body and additional water is lost from the airway mucosa in order to saturate it. Ascent to any altitude, therefore, necessarily involves increased water loss. The extent of this must be proportional to the ventilatory volume, so it becomes an increasing problem with increased exercise intensity and especially when the altitude is sufficient for activation of hypoxic respiratory drive. Respiratory dehydration has a powerful enhancing effect on the susceptibility of an individual to hypothermia, since substantial amounts of body heat are lost in warming cold inspired air, while the depletion of plasma volume potentially limits exercise capacity.

HANDY HINTS

It is often difficult to assess someone’s core temperature in the field. Peripheral vasoconstriction may lead to the skin being extremely cold regardless of internal temperature; oral temperature may be inaccurate because of heat loss through the cheeks and because normal oral thermometers cannot register temperatures below around 35°C (95°F).

Estimating the likely extent of hypothermia in a subject and knowing the implications can be helped by considering four critical body core temperatures. At around 34°C (93°F), the heat-producing process of shivering becomes so intense that large numbers of motor units contract simultaneously. This makes it impossible to undertake fine movements like unfolding a map or adjusting skis. Around 33°C (91.5°F), the limbs are so cold that peripheral axonal conduction is impaired. As a result, heat production through shivering ceases and cutaneous vasoconstriction is inhibited, leading to more rapid heat loss. At this temperature, cerebral metabolism also begins to slow, with confusion and disorientation. At 31°C (90°F), cerebral function is too inefficient to maintain consciousness, so the subject collapses. Finally, at around 27°C (81°F), the pumps that drive cardiac action potentials stop working and cardiac arrest occurs.

The first step in rewarming any hypothermic person is to prevent further heat loss by use of wind-resistant blankets. The next stage has to take into account both the circumstances of cooling and the effects of hypothermia on circulatory reflex control. Individuals who slowly become hypothermic on a hill walk will have low stores of metabolic substrates and may be unable to rewarm themselves spontaneously, while people who fall into cold water are likely to have cooled down so quickly that their metabolic status is still intact. In either case, if core temperature is below 34°C (93°F) there will be impaired baroreflex function because of reduced sympathetic nerve conduction. To maintain adequate cerebral perfusion, a near-horizontal posture needs to be maintained during rescue and transport.

Finally, if active rewarming outside a clinical setting is necessary, then the circulatory implications need to be borne in mind. Radiative heat applied to the limbs will initially warm the skin and the resultant inhibition of cutaneous cold receptor activity may lead to withdrawal of sympathetic vasoconstrictor tone and increased limb blood flow. Since the entire tissue of the limbs is hypothermic, the effect may be to cool down venous return to the extent that there is actually a further fall in body temperature before rewarming begins. This may have deleterious effects if the initial core temperature is just above one of the critical values listed – for example, by leading to a deterioration of consciousness that impairs mobility. More efficient rewarming can be achieved by use of a warm bath or by hot water bottles applied only to the trunk.

Pulmonary oedema

A small number of individuals show a more serious acute response to the same levels of ascent that induce acute mountain sickness. In these people, there is damage to the pulmonary capillary wall so that plasma leaks into the lung interstitium and may enter the alveoli. The precise mechanisms that underlie this high-altitude pulmonary oedema are not fully understood, but it almost certainly involves generation of high intracapillary pressures in response to hypoxia. Superficially, this seems counterintuitive. You will remember from Chapter 8 (pp. 94) that capillary hydrostatic pressure in the lung is normally well below the plasma oncotic pressure, so that there is a good safety margin to ensure no fluid extravasation. We also saw in Chapter 8 (pp. 96) that the pulmonary arteriolar smooth muscle possesses hypoxia receptors that induce vasoconstriction in response to reduced alveolar PO2. In theory, therefore, breathing hypoxic air should cause generalized pulmonary vasoconstriction which, while it will elevate pulmonary arterial pressure, will reduce capillary hydrostatic pressure.

In practice, the likely explanation is that, in the susceptible individuals that suffer high altitude pulmonary oedema, not all areas of the pulmonary arteriolar bed respond equally strongly to the vasoconstrictor effect of hypoxia. Under these circumstances, a disproportionate volume of right cardiac output is directed through the least constricted vessels exposing the capillaries in these areas to an intravascular pressure close to pulmonary arterial pressure (West 2004).

Case history

A class of 11–12-year-old students from a seaside Irish town travelled on an exchange trip to an alpine village in Switzerland (altitude 2800 m, 9100 ft). On the second day of the visit, one of the students (Kevin B) reported sick, with breathlessness and bluish lips and face. His parents were contacted and he was flown home, although his symptoms had disappeared by the time he had reached the Swiss airport. When the supervising teacher met Kevin’s parents they said that he has always had ‘a heart murmur’ and that medical advice had been for him to avoid strenuous activities, although nobody had mentioned any problems with high altitude. The school doctor examined him, confirmed the presence of a murmur and recorded his resting heart rate as 90 and his blood pressure as 130/60.

Discussion

Breathlessness, or dyspnoea, is a subjective feeling caused by inadequate pulmonary gas exchange activating chemoreceptors. These might be central CO2 receptors responding to hypercapnia or peripheral hypoxia receptors responding to inadequate oxygenation of arterial blood or to plasma-borne protons. In either case, the sensation of breathlessness is due partly to inputs from these receptors and partly to the respiratory muscle fatigue that results from increased respiratory work. Breathlessness associated with acute ascent to a higher altitude automatically suggests hypoxia rather than acidosis or hypercapnia and this is consistent with the fact that Kevin’s lips were bluish. Blue colouration of the mucous membranes or skin, known as cyanosis, reflects the presence in arterial blood of more than 5 g/100 ml of deoxygenated haemoglobin. Thus, cyanosis usually indicates inefficient pulmonary uptake of oxygen. In individuals who have very high haematocrits, on the other hand, it is sometimes possible to see cyanosis in the presence of normal pulmonary oxygenation, because at high rates of pulmonary blood flow there is not enough time to saturate the extra haemoglobin molecules.

Many people have detectable heart murmurs and the cause of these is not always obvious without investigations. From the discussions in Chapter 3 (pp. 24) you will remember that the only criterion for generation of a murmur is the presence of turbulent flow at some time during the cardiac cycle. In most cases, the structural distortion that produces this turbulent flow is a minor one that does not interfere with exercise but, unless the extent of the abnormality has been clarified, you cannot be sure of this. Possible causes of turbulence are valvular stenosis, valvular incompetence or a shunt that allows a proportion of stroke volume to be ejected through a narrow orifice at high velocity.

A resting heart rate of 90 beats/min is high, but not abnormal for a growing child. Similarly, a diastolic pressure of 60 mmHg is within the normal range. However, the combination of these values with a systolic pressure as high as 130 is unexpected. With a cardiac interval of about 700 ms you would expect a resting pulse pressure of around 40 mmHg or slightly below. Kevin’s pulse pressure was 70 mmHg, which suggests that stroke volume was substantially elevated above normal. The murmur cannot have been due to atrioventricular valve stenosis or incompetence, semilunar valve stenosis or an inter-atrial or an inter-ventricular shunt, because these would all reduce cardiac ejection and stroke volume. The alternatives are, therefore, semilunar incompetence, with diastolic backflow, or a shunt between the aorta and a low-pressure site. By far the most common shunt of this type in young people is a patent ductus arteriosus.

Would one of these alternatives be able to explain Kevin’s breathlessness at altitude? We know that a patent ductus arteriosus will normally shunt blood from aorta to pulmonary artery. We know also that hypoxia elevates pulmonary vascular resistance; if this elevation were large enough pulmonary arterial pressure might exceed aortic pressure, reversing the shunt and resulting in reduced pulmonary blood flow and reduced oxygen uptake. So this would be consistent with Kevin’s case, but is it realistic? The degree of hypoxia experienced at 2800 m will approximately double pulmonary blood pressure which, assuming a normal pulmonary pressure of around 25/8 mmHg, would still be lower than Kevin’s systemic blood pressure. However, the left–right shunting through a patent ductus arteriosus begins at birth, so Kevin’s pulmonary vasculature had been exposed to 12 years of elevated pressure. Arteries and arterioles respond to chronically increased transmural pressure with muscular hypertrophy and this encroaches on the vascular lumen; therefore, Kevin’s absolute pulmonary vascular resistance and pulmonary blood pressure would be much higher than normal. Under these circumstances, even a relatively small further increase in pulmonary pressure may reverse the ductus shunt and reduce pulmonary perfusion.

Pulmonary hypertension

Chronic hypoxia also has other disadvantageous consequences that are seen in long-term residents and, in particular, in individuals who have been born at high altitude. The pulmonary vasoconstrictor effect of hypoxia generates an increased afterload for the right ventricle leading to myocardial hypertrophy and the possibility of right heart failure because of inadequate coronary vascularization (see Chapter 8, p. 95). In addition, the relatively low PaO2 results in reduced efficiency of ductus arteriosus closure after birth (see Chapter 8, p. 102), so that a relatively large number of native highland children have some residual shunting between pulmonary and systemic circulations, which further increases pulmonary afterload.