(N/A) The exchange of gases occurs primarily by diffusion based on pressure gradients. The following table summarizes the partial pressures (in $mm Hg$) of respiratory gases:
| Respiratory Gas | Atmospheric Air | Alveoli | Blood (Deoxygenated) | Blood (Oxygenated) | Tissues |
| $O_2$ | $159$ | $104$ | $40$ | $95$ | $40$ |
| $CO_2$ | $0.3$ | $40$ | $45$ | $40$ | $45$ |
The data indicates a concentration gradient for $O_2$ from alveoli to blood and from blood to tissues. Similarly, a gradient exists for $CO_2$ in the opposite direction, from tissues to blood and from blood to alveoli.
Since the solubility of $CO_2$ is $20-25$ times higher than that of $O_2$, the amount of $CO_2$ that can diffuse through the diffusion membrane per unit difference in partial pressure is much higher than that of $O_2$.
The diffusion membrane is composed of three major layers:
$(1)$ Thin squamous epithelium of alveoli.
$(2)$ The endothelium of alveolar capillaries.
$(3)$ The basement membrane in between them.
The total thickness of this membrane is much less than a millimeter, facilitating rapid diffusion. Thus, all factors are favourable for the diffusion of $O_2$ from alveoli to tissues and $CO_2$ from tissues to alveoli.