Exercise Physiology 19-7
Oxygen is conveyed by convection in the upper airways and by diffusion in the lower airways to the
alveoli (lower reaches of the lung where gas exchange with the blood occurs). Oxygen must diffuse from
the alveoli, through the extremely thin alveolocapillary membrane into solution in the blood. Oxygen
diffuses further into red blood cells where it is bound chemically to hemoglobin molecules. The order of
each of these processes is reversed in the working muscles where the concentration gradient of oxygen is
in the opposite direction. Complete equilibration of oxygen between alveolar air and pulmonary blood
requires about 0.75 sec. Carbon dioxide requires somewhat less, about 0.50 sec. Thus, alveolar air more
closely reflects levels of blood carbon dioxide than oxygen.
Both respiration rate and tidal volume (the amount of air moved per breath) increase with exercise, but
above the anaerobic threshold the tidal volume no longer increases (remains at about 2 to 2.5 l). From that
point, increases in ventilation require greater increases in respiration rate. A similar limitation occurs for
stroke volume in the heart (limited to about 120 ml).
The work of respiration, representing only about 1 to 2% of the body’s oxygen consumption at rest,
increases to 8 to 10% or more of the body’s oxygen consumption during exercise. Contributing greatly to
this is the work to overcome resistance to movement of air, lung tissue, and chest wall tissue. Turbulent
airflow in the upper airways (those nearest and including the mouth and nose) contributes a great deal of
pressure drop. The lower airways are not as rigid as the upper airways and are influenced by the stretching
and contraction of the lung surrounding them. High exhalation pressures external to the airways coupled
with low static pressures inside (due to high flow rates inside) tend to close these airways somewhat and
limit exhalation airflow rates. Resistance of these airways becomes very high, and the respiratory system
appears like a flow source, but only during extreme exhalation.
19.5 Optimization
Energy demands during exercise are so great that optimal courses of action are followed for many physio-
logical responses (Table 19.2). Walking occurs most naturally at a pace that represents the smallest energy
expenditure; the transition from walking to running occurs when running expends less energy than walk-
ing; ejection of blood from the left ventricle appears to be optimized to minimize energy expenditure;
respiratory rate, breathing waveforms, the ratio of inhalation time to exhalation time, airways resistance,
tidal volume, and other respiratory parameters all appear to be regulated to minimize energy expenditure
[Johnson, 1993].
19.6 Thermal Response
When exercise extends for a long enough time, heat begins to build up in the body. In order for heat accu-
mulationto become important, exercisemust be performed at a relativelylowrate. Otherwise, performance
time would not be long enough for significant amounts of heat to be stored.
Muscular activities are at most 20–25% efficient, and, in general, the smaller the muscle, the less efficient
it is. Heat results from the other 75–80% of the energy supplied to the muscle.
Thermal challenges are met in several ways. Blood sent to the limbs and blood returning from the limbs
are normally conveyed by arteries and veins in close proximity deep inside the limb. This tends to conserve
heat by countercurrent heat exchange between the arteries and veins. Thermal stress causes blood to return
via surface veins rather than deep veins. Skin surface temperature increases and heat loss by convection
and radiation also increases. In addition, vasodilation of cutaneous blood vessels augments surface heat
loss but puts an additional burden on the heart to deliver added blood to the skin as well as the muscles.
Heart rate increases as body temperature rises.
Sweating begins. Different areas of the body begin sweating earlier than others, but soon the whole body
is involved. If sweat evaporation occurs on the skin surface, then the full cooling power of evaporating
sweat (670 W·h/kg) is felt. If the sweat is absorbed by clothing, then the full benefit of sweat evaporation
is not realized at the skin. If the sweat falls from the skin, no benefit accrues.