Oxygen and Carbon Dioxide Transport


Learning Objectives

Upon completion of this chapter, the student should be able to answer the following questions :

  • 1

    What are the basic gas diffusion principles and how do they affect O 2 and CO 2 absorption and expiration?

  • 2

    What are the chemical transport mechanisms of O 2 and CO 2 in blood?

  • 3

    How do the O 2 and CO 2 dissociation curves differ? How does these differences promote tissue O 2 delivery and CO 2 removal?

  • 4

    What is the difference between perfusion limitation and diffusion limitation? Why is the diffusion of O 2 and CO 2 considered to be perfusion limited, and why is CO is considered to be diffusion limited?

  • 5

    What is meant by a leftward or rightward shift of the oxyhemoglobin dissociation curve?

  • 6

    How do the oxyhemoglobin and carboxyhemoglobin dissociation curves differ? What is the clinical significance of the differences?

  • 7

    What is the difference between the chloride shift and the Haldane effect on CO 2 transport?

The respiratory and circulatory systems function together to transport oxygen (O 2 ) from the lungs to the tissues to sustain normal cellular activity and to transport carbon dioxide (CO 2 ) from the tissues to the lungs for expiration ( Fig. 24.1 ). To enhance uptake and transport of these gases between the lungs and tissues, specialized mechanisms (e.g., binding of O 2 and hemoglobin and HCO 3 transport of CO 2 ) have evolved that enable O 2 uptake and CO 2 expiration to occur simultaneously. To understand the mechanisms involved in the transport of these gases, gas diffusion properties, gas transport, and gas delivery mechanisms must be considered.

Fig. 24.1, Oxygen (O 2 ) and carbon dioxide (CO 2 ) transport in arterial and venous blood. Oxygen in arterial blood is transferred from arterial capillaries to tissues. The flow rates for O 2 and CO 2 are shown for 1 L of blood.

Gas Diffusion

Gas movement throughout the respiratory system occurs predominantly via diffusion. The respiratory and circulatory systems contain several unique anatomical and physiological features to facilitate gas diffusion: (1) large surface areas for gas exchange (alveolar to pulmonary capillary bed and end organ capillary bed to tissue) with short distances to travel, (2) substantial partial pressure gradient differences, and (3) gases with advantageous diffusion properties. Transport and delivery of O 2 from the lungs to the tissue and vice versa for CO 2 are dependent on basic gas diffusion laws.

Diffusion of Gases From Regions of Higher to Lower Partial Pressure in the Lungs

The process of gas diffusion is passive and similar whether diffusion occurs in a gaseous or liquid state. The rate of diffusion of a gas through a liquid is described by Graham’s law, which states that the rate is directly proportional to the solubility coefficient of the gas and inversely proportional to the square root of its molecular weight. Calculation of the diffusion properties for O 2 and CO 2 reveals that CO 2 diffuses approximately 20 times faster than O 2 . Rates of O 2 diffusion from the lungs into blood and from blood into tissue, and vice versa for CO 2 , are predicted by Fick’s law of gas diffusion ( Fig. 24.2 ). Fick’s law states that gas diffusion across a permeable membrane (
V ˙
) is proportional to the diffusion coefficient for the gas (D), the surface area of the membrane (A), and the pressure gradient across the membrane (P 1 − P 2 ). It is inversely proportional to the thickness of the membrane (T). The ratio of surface area (A) x diffusion coefficient (D) to membrane thickness (T) (or A•D/T) represents the conductance of a gas from the alveolus to the blood. The diffusing capacity of the lung (D L ) is its conductance (A•D/T) when considered for the entire lung; thus, with Fick’s equation, D L can be calculated as follows:


V ˙ gas = A D ( P 1 P 2 ) T

V ˙ = D L ( P 1 P 2 )

D L = V ˙ ( P 1 P 2 )

where V ˙ gas = gas diffusion.

Fig. 24.2, According to Fick’s law, diffusion of a gas across a sheet of tissue ( V ˙ gas ) is directly related to the surface area (A) of the tissue, the diffusion constant (D) of the specific gas, and the partial pressure difference (P 1 − P 2 ) of the gas on each side of the tissue, and it is inversely related to tissue thickness (T) .

Fick’s law of diffusion could be used to assess the diffusion properties of O 2 in the lungs, except that the capillary partial pressure of oxygen cannot be measured. This limitation can be overcome with the use of carbon monoxide (CO) rather than O 2 . Because CO has low solubility in the capillary membrane, the rate of CO equilibrium across the capillary is slow, and the partial pressure of CO in capillary blood remains close to 0. In contrast, the solubility of CO in blood is high. Thus, the only limitation for diffusion of CO is the alveolar-capillary membrane, and thus CO is a useful gas for calculating D L . The capillary partial pressure (P 2 in Eq. 24.1 ) is essentially 0 for CO, and therefore D L can be measured from the diffusion of carbon monoxide (
V ˙ CO
) and the average partial pressure of Co in the alveolus (P 1 ); that is,


V ˙ CO = D L CO(P 1 P 2 ) , or D L CO = V ˙ CO ( P 1 P 2 ) , and since P 2 is essentially zero , D L CO = V ˙ CO ( P 1 )

where D L co = diffusion capacity of the lung for carbon monoxide.

Assessment of D L co has become a classic measurement of the diffusion barrier of the alveolar-capillary membrane. It is useful in the differential diagnosis of certain obstructive lung diseases, such as emphysema. Although exposure to high levels of carbon monoxide gas can be toxic, in gas diffusion testing the total CO exposure is negligible.

IN THE CLINIC

A patient with interstitial pulmonary fibrosis (a restrictive lung disease) inhales a single breath of 0.3% CO from residual volume to total lung capacity. He holds his breath for 10 seconds and then exhales. After discarding the exhaled gas from the dead space, a representative sample of alveolar gas from late in exhalation is collected. The average alveolar CO pressure is 0.1 mm Hg, and 0.25 mL of CO has been taken up. The diffusion capacity for CO in this patient is


D L = V ˙ CO PACO = 0.25 mL/10 seconds × 60 seconds/minute 0.1 mm Hg = 15 mL/minute/mm Hg

The normal range for D L co is 20 to 30 mL/minute/mm Hg. Patients with interstitial pulmonary fibrosis have an initial alveolar inflammatory response with subsequent scar formation within the interstitial space. The inflammation and scar replace the alveoli and decrease the surface area for gas diffusion to occur, which results in decreased D L co . This is a classic characteristic of certain types of restrictive lung disease.

Oxygen and Carbon Dioxide Exchange in the Lung Is Perfusion Limited

Different gases have different solubility factors. Gases that are insoluble in blood (i.e., anesthetic gases such as nitrous oxide and ether) do not chemically combine with proteins in blood and equilibrate rapidly between alveolar gas and blood. The equilibration occurs in less time than the 0.75 to 1.0 seconds that the red blood cell spends in the capillary bed (the capillary transit time). The diffusion of insoluble gases between alveolar gas and blood is considered perfusion limited because the partial pressure of gas in the blood leaving the capillary has reached equilibrium with alveolar gas and is limited only by the amount of blood perfusing the alveolus. In contrast, a gas that is diffusion limited, such as CO, has low solubility in the alveolar-capillary membrane but high solubility in blood because of its high affinity for hemoglobin (Hgb). These features prevent the equilibration of CO between alveolar gas and blood during the red blood cell transit time.

The high affinity of CO for Hgb enables large amounts of CO to be taken up in blood with little or no appreciable increase in its partial pressure. Gases that are chemically bound to Hgb do not exert a partial pressure in blood. Like CO, both CO 2 and O 2 have relatively low solubility in the alveolar-capillary membrane but high solubility in blood because of their ability to bind to Hgb. However, their rate of equilibration is sufficiently rapid for complete equilibration to occur during the transit time of the red blood cell within the capillary. Equilibration for O 2 and CO 2 usually occurs within 0.25 seconds. Thus, O 2 and CO 2 transfer is normally perfusion limited. The partial pressure of a gas that is diffusion limited (i.e., CO) does not reach equilibrium with the alveolar pressure over the time that it spends in the capillary ( Fig. 24.3 ). Although CO 2 has a greater rate of diffusion in blood than O 2 does, it has a lower membrane-blood solubility ratio and consequently takes approximately the same amount of time to reach equilibration in blood.

Fig. 24.3, Uptake of nitrous oxide (N 2 O), carbon monoxide (CO), and O 2 in blood in relation to their partial pressures and the transit time of the red blood cell in the capillary. For gases that are perfusion limited (N 2 O and O 2 ), their partial pressures have equilibrated with alveolar pressure before exiting the capillary. In contrast, the partial pressure of CO, a gas that is diffusion limited, does not reach equilibrium with alveolar pressure. In rare conditions, O 2 uptake can become diffusion limited.

Diffusion limitation for O 2 and CO 2 would occur if red blood cells spent less than 0.25 seconds in the capillary bed. This is occasionally the case in very fit athletes during vigorous exercise and in healthy subjects who exercise at high altitude.

Oxygen Transport

Oxygen is carried in blood in two forms: O 2 dissolved in plasma and O 2 bound to Hgb. The dissolved form is measured clinically in an arterial blood gas sample as the partial pressure of arterial oxygen (Pa o 2 ). Only a small percentage of O 2 in blood is in the dissolved form, and its contribution to O 2 transport under normal conditions is almost negligible. However, dissolved O 2 can become a significant factor in conditions of severe hypoxemia. Binding of O 2 to Hgb to form oxyhemoglobin within red blood cells is the primary transport mechanism of O 2 . Hgb not bound to O 2 is referred to as deoxyhemoglobin or reduced Hgb. The O 2 -carrying capacity of blood is enhanced about 65 times by its ability to bind to Hgb.

Hemoglobin

Hgb is the major transport molecule for O 2 . The Hgb molecule is a protein with two major components: four nonprotein heme groups, each containing iron in the reduced ferric (Fe +++ ) form, which is the site of O 2 binding; and a globin portion consisting of four polypeptide chains. Normal adults have two α-globin chains and two β-globin chains (HgbA), whereas children younger than 6 months of age have predominantly fetal Hgb (HgbF), which consists of two α chains and two γ chains. This difference in the structure of HgbF increases its affinity for O 2 and aids in the transport of O 2 across the placenta. In addition, HgbF is not inhibited by 2,3-diphosphoglycerate (2,3-DPG), a product of glycolysis; thus O 2 uptake is further enhanced.

Binding of O 2 to Hgb alters the ability of Hgb to absorb light. This effect of O 2 on Hgb is responsible for the change in color between oxygenated arterial blood (bright red) and deoxygenated venous blood (dark red-bluish). Binding and dissociation of O 2 with Hgb occur in milliseconds, thus facilitating O 2 transport because red blood cells spend only 0.75 seconds in the capillaries. There are approximately 280 million Hgb molecules per red blood cell, which provides an efficient mechanism to transport O 2 . Myoglobin, a protein in striated muscle similar in structure and function to Hgb, has only one subunit of the Hgb molecule. It aids in the transfer of O 2 from blood to muscle cells and in the storage of O 2 , which is especially critical in O 2 -deprived conditions.

Abnormalities of the Hgb molecule occur with mutations in the amino acid sequence (i.e., sickle cell disease) or in the spatial arrangement of the globin polypeptide chains and result in abnormal function. Compounds such as CO, nitrites (nitric oxide), and cyanides can oxidize the iron molecule in the heme group and change it from the reduced ferrous state (Fe ++ ) to the ferric state (Fe +++ ), which reduces the ability of O 2 to bind to Hgb.

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