Diffusion and surface area The exchange of gases occurs as a result of
diffusion down a concentration gradient. Gas molecules move from a region in which they are at high concentration to one in which they are at low concentration. Diffusion is a
passive process, meaning that no energy is required to power the transport, and it follows
Fick's law: :J = -D \frac{d \varphi}{d x} In relation to a typical biological system, where two compartments ('inside' and 'outside'), are separated by a membrane barrier, and where a gas is allowed to spontaneously diffuse down its concentration gradient: •
J is the flux, the
amount of gas diffusing per unit area of membrane per unit time. Note that this is already scaled for the area of the membrane. •
D is the
diffusion coefficient, which will differ from gas to gas, and from membrane to membrane, according to the size of the gas molecule in question, and the nature of the membrane itself (particularly its
viscosity,
temperature and
hydrophobicity). •
φ is the
concentration of the gas. •
x is the position across the thickness of the membrane. • d
φ/d
x is therefore the concentration gradient across the membrane. If the two compartments are individually well-mixed, then this is simplifies to the difference in concentration of the gas between the inside and outside compartments divided by the thickness of the membrane. • The negative sign indicates that the diffusion is always in the direction that - over time - will destroy the concentration gradient,
i.e. the gas moves from high concentration to low concentration until eventually the inside and outside compartments reach
equilibrium. Gases must first dissolve in a liquid in order to diffuse across a
membrane, so all biological gas exchange systems require a moist environment. In general, the higher the concentration gradient across the gas-exchanging surface, the faster the rate of diffusion across it. Conversely, the thinner the gas-exchanging surface (for the same concentration difference), the faster the gases will diffuse across it. In the equation above,
J is the
flux expressed per unit area, so increasing the area will make no difference to its value. However, an increase in the available surface area, will increase the
amount of gas that can diffuse in a given time. but in larger organisms such as
roundworms (Nematoda) the equivalent exchange surface - the cuticle - is substantially thicker at 0.5 μm.
Interaction with circulatory systems In
multicellular organisms therefore, specialised respiratory organs such as gills or lungs are often used to provide the additional surface area for the required rate of gas exchange with the external environment. However the distances between the gas exchanger and the deeper tissues are often too great for diffusion to meet gaseous requirements of these tissues. The gas exchangers are therefore frequently coupled to gas-distributing
circulatory systems, which transport the gases evenly to all the body tissues regardless of their distance from the gas exchanger. Some multicellular organisms such as
flatworms (Platyhelminthes) are relatively large but very thin, allowing their outer body surface to act as a gas exchange surface without the need for a specialised gas exchange organ. Flatworms therefore lack gills or lungs, and also lack a circulatory system. Other multicellular organisms such as
sponges (Porifera) have an inherently high surface area, because they are very porous and/or branched. Sponges do not require a circulatory system or specialised gas exchange organs, because their feeding strategy involves one-way pumping of water through their porous bodies using
flagellated collar cells. Each cell of the sponge's body is therefore exposed to a constant flow of fresh oxygenated water. They can therefore rely on diffusion across their cell membranes to carry out the gas exchange needed for respiration. In organisms that have circulatory systems associated with their specialized gas-exchange surfaces, a great variety of systems are used for the interaction between the two. In a
countercurrent flow system, air (or, more usually, the water containing dissolved air) is drawn in the
opposite direction to the flow of blood in the gas exchanger. A countercurrent system such as this maintains a steep concentration gradient along the length of the gas-exchange surface (see lower diagram in Fig. 2). This is the situation seen in the
gills of fish and
many other aquatic creatures. Although this theoretically allows almost complete transfer of a respiratory gas from one side of the exchanger to the other, in fish less than 80% of the oxygen in the water flowing over the gills is generally transferred to the blood. and dead-end air-filled sac systems found in the
lungs of mammals. In a
cocurrent flow system, the blood and gas (or the fluid containing the gas) move in the same direction through the gas exchanger. This means the magnitude of the gradient is variable along the length of the gas-exchange surface, and the exchange will eventually stop when an equilibrium has been reached (see upper diagram in Fig. 2). Cocurrent flow gas exchange systems are not known to be used in nature. ==Mammals==