Learning Objectives

Learning Objectives

By the end of this section, you will be able to do the following:

  • Define diffusion, osmosis, dialysis, and active transport
  • Calculate diffusion rates



There is something fishy about the ice cube from your freezer—how did it pick up those food odors? How does soaking a sprained ankle in Epsom salt reduce swelling? The answer to these questions are related to atomic and molecular transport phenomena—another mode of fluid motion. Atoms and molecules are in constant motion at any temperature. In fluids, they move about randomly even in the absence of macroscopic flow. This motion is called a random walk and is illustrated in Figure 12.21. Diffusion is the movement of substances due to random thermal molecular motion. Fluids, like fish fumes or odors entering ice cubes, can even diffuse through solids.

Diffusion is a slow process over macroscopic distances. The densities of common materials are great enough that molecules cannot travel very far before having a collision that can scatter them in any direction, including straight backward. It can be shown that the average distance xrmsxrms size 12{x rSub { size 8{"rms"} } } {} that a molecule travels is proportional to the square root of time

12.94 xrms=2Dt,xrms=2Dt, size 12{x rSub { size 8{"rms"} } = sqrt {2 ital "Dt"} } {}

where xrmsxrms stands for the root-mean-square distance and is the statistical average for the process. The quantity DD size 12{D} {} is the diffusion constant for the particular molecule in a specific medium. Table 12.2 lists representative values of DD size 12{D} {} for various substances, in units of m2/s.m2/s. size 12{m rSup { size 8{2} } "/s"} {}

The figure shows the path of a random walk. The random thermal motion of a molecule is shown to begin at a start point and then the particles move about zigzag in all directions and end up at the finish point. The distance between the start and finish point is shown as x. Continuous arrows show various directions of motion.
Figure 12.21 The random thermal motion of a molecule in a fluid in time t.t. size 12{t} {} This type of motion is called a random walk.
Diffusing molecule Medium D (m2/s)
Hydrogen (H2)(H2) Air 6.4×10–56.4×10–5
Oxygen (O2)(O2) Air 1.8×10–51.8×10–5
Oxygen (O2)(O2) Water 1.0×10–91.0×10–9
Glucose (C6H12O6)(C6H12O6) Water 6.7×10–106.7×10–10
Hemoglobin Water 6.9×10–116.9×10–11
DNA Water 1.3×10–121.3×10–12
Table 12.2 Diffusion Constants for Various Molecules3

Note that DD size 12{D} {} gets progressively smaller for more massive molecules. This decrease is because the average molecular speed at a given temperature is inversely proportional to molecular mass. Thus the more massive molecules diffuse more slowly. Another interesting point is that DD size 12{D} {} for oxygen in air is much greater than DD size 12{D} {} for oxygen in water. In water, an oxygen molecule makes many more collisions in its random walk and is slowed considerably. In water, an oxygen molecule moves only about 40 μm in 1 s. Each molecule actually collides about 10101010 size 12{"10" rSup { size 8{"10"} } } {} times per second!. Finally, note that diffusion constants increase with temperature, because average molecular speed increases with temperature. This is because the average kinetic energy of molecules, 12mv212mv2 size 12{ { { size 8{1} } over { size 8{2} } } ital "mv" rSup { size 8{2} } } {}, is proportional to absolute temperature.

Example 12.11 Calculating Diffusion: How Long Does Glucose Diffusion Take?

Calculate the average time it takes a glucose molecule to move 1.0 cm in water.


We can use xrms=2Dt,xrms=2Dt, size 12{x rSub { size 8{"rms"} } = sqrt {2 ital "Dt"} } {} the expression for the average distance moved in time t,t, size 12{t} {} and solve it for t.t. size 12{t} {} All other quantities are known.


Solving for tt size 12{t} {} and substituting known values yields

12.95 t = xrms22D=(0.010 m)22(6.7×1010 m2/s) = 7.5×104 s=21 h. t = xrms22D=(0.010 m)22(6.7×1010 m2/s) = 7.5×104 s=21 h.


This is a remarkably long time for glucose to move a mere centimeter! For this reason, we stir sugar into water rather than waiting for it to diffuse.

Because diffusion is typically very slow, its most important effects occur over small distances. For example, the cornea of the eye gets most of its oxygen by diffusion through the thin tear layer covering it.

The Rate and Direction of Diffusion

The Rate and Direction of Diffusion

If you very carefully place a drop of food coloring in a still glass of water, it will slowly diffuse into the colorless surroundings until its concentration is the same everywhere. This type of diffusion is called free diffusion, because there are no barriers inhibiting it. Let us examine its direction and rate. Molecular motion is random in direction, and so simple chance dictates that more molecules will move out of a region of high concentration than into it. The net rate of diffusion is higher initially than after the process is partially completed (see Figure 12.22).

The figure shows the diffusion along a cylindrical tube of area of cross section A. The cylindrical tube is divided into three regions. The cross section is marked as A. The first region is marked as region one. The concentration there is marked C one. The molecules are shown as small sphere with an arrow pointing out from them. The concentration is high in this region. The second region is marked of width delta x. The concentration is lesser in this region as compared to region one. The third region is m
Figure 12.22 Diffusion proceeds from a region of higher concentration to a lower one. The net rate of movement is proportional to the difference in concentration.

The rate of diffusion is proportional to the concentration difference. Many more molecules will leave a region of high concentration than will enter it from a region of low concentration. In fact, if the concentrations were the same, there would be no net movement. The rate of diffusion is also proportional to the diffusion constant DD size 12{D} {}, which is determined experimentally. The farther a molecule can diffuse in a given time, the more likely it is to leave the region of high concentration. Many of the factors that affect the rate are hidden in the diffusion constant DD size 12{D} {}. For example, temperature and cohesive and adhesive forces all affect values of DD size 12{D} {}.

Diffusion is the dominant mechanism by which the exchange of nutrients and waste products occur between the blood and tissue, and between air and blood in the lungs. In the evolutionary process, as organisms became larger, they needed quicker methods of transportation than net diffusion, because of the larger distances involved in the transport, leading to the development of circulatory systems. Less sophisticated, single-celled organisms still rely totally on diffusion for the removal of waste products and the uptake of nutrients.

Osmosis and Dialysis—Diffusion across Membranes

Osmosis and Dialysis—Diffusion across Membranes

Some of the most interesting examples of diffusion occur through barriers that affect the rates of diffusion. For example, when you soak a swollen ankle in Epsom salt, water diffuses through your skin. Many substances regularly move through cell membranes; oxygen moves in, carbon dioxide moves out, nutrients go in, and wastes go out, for example. Because membranes are thin structures, typically 6.5×1096.5×109 size 12{6 "." 5 times "10" rSup { size 8{ - 9} } } {} to 10×10910×109 size 12{"10" times "10" rSup { size 8{ - 9} } } {} m across, diffusion rates through them can be high. Diffusion through membranes is an important method of transport.

Membranes are generally selectively permeable, or semipermeable (see Figure 12.23). One type of semipermeable membrane has small pores that allow only small molecules to pass through. In other types of membranes, the molecules may actually dissolve in the membrane or react with molecules in the membrane while moving across. Membrane function, in fact, is the subject of much current research, involving not only physiology but also chemistry and physics.

Part a of the figure shows a semi permeable membrane shown as small rectangular sections in a vertical line, separated by small gaps called as pores. Molecules are shown in all shapes on both the sides of the membranes. Some molecules are shown to diffuse through the pores. Part b of the diagram shows molecules in the form of small spheres packed on both sides of a single vertical rectangular membrane. Some molecules are shown to dissolve in this membrane and diffuse across it.
Figure 12.23 (a) A semipermeable membrane with small pores that allow only small molecules to pass through. (b) Certain molecules dissolve in this membrane and diffuse across it.

Osmosis is the transport of water through a semipermeable membrane from a region of high concentration to a region of low concentration. Osmosis is driven by the imbalance in water concentration. For example, water is more concentrated in your body than in Epsom salt. When you soak a swollen ankle in Epsom salt, the water moves out of your body into the lower-concentration region in the salt. Similarly, dialysis is the transport of any other molecule through a semipermeable membrane due to its concentration difference. Both osmosis and dialysis are used by the kidneys to cleanse the blood.

Osmosis can create a substantial pressure. Consider what happens if osmosis continues for some time, as illustrated in Figure 12.24. Water moves by osmosis from the left into the region on the right, where it is less concentrated, causing the solution on the right to rise. This movement will continue until the pressure ρghρgh size 12{ρ ital "gh"} {} created by the extra height of fluid on the right is large enough to stop further osmosis. This pressure is called a back pressure. The back pressure ρghρgh size 12{ρ ital "gh"} {} that stops osmosis is also called the relative osmotic pressure if neither solution is pure water, and it is called the osmotic pressure if one solution is pure water. Osmotic pressure can be large, depending on the size of the concentration difference. For example, if pure water and sea water are separated by a semipermeable membrane that passes no salt, osmotic pressure will be 25.9 atm. This value means that water will diffuse through the membrane until the salt water surface rises 268 m above the pure-water surface! One example of pressure created by osmosis is turgor in plants; many wilt when too dry. Turgor describes the condition of a plant in which the fluid in a cell exerts a pressure against the cell wall. This pressure gives the plant support. Dialysis can similarly cause substantial pressures.

Part a of the figure shows a vessel having two different concentrations of sugar in water separated by a semipermeable membrane that passes water but not sugar molecules. The sugar molecules are shown as small red color spheres and water molecules as still smaller blue colored spheres. The right side of the solution shows more of sugar molecules represented as more number of red spheres. The osmosis of water molecules is shown toward right. Part b shows the second stage for figure on part a. The osmosis o
Figure 12.24 (a) Two sugar-water solutions of different concentrations, separated by a semipermeable membrane that passes water but not sugar. Osmosis will be to the right, since water is less concentrated there. (b) The fluid level rises until the back pressure ρghρgh size 12{ρ ital "gh"} {} equals the relative osmotic pressure; then, the net transfer of water is zero.

Reverse osmosis and reverse dialysis, also called filtration, are processes that occur when back pressure is sufficient to reverse the normal direction of substances through membranes. Back pressure can be created naturally as on the right side of Figure 12.24. A piston can also create this pressure. Reverse osmosis can be used to desalinate water by simply forcing it through a membrane that will not pass salt. Similarly, reverse dialysis can be used to filter out any substance that a given membrane will not pass.

One further example of the movement of substances through membranes deserves mention. We sometimes find that substances pass in the direction opposite to what we expect. Cypress tree roots, for example, extract pure water from salt water, although osmosis would move it in the opposite direction. This is not reverse osmosis, because there is no back pressure to cause it. What is happening is called active transport, a process in which a living membrane expends energy to move substances across it. Many living membranes move water and other substances by active transport. The kidneys, for example, not only use osmosis and dialysis—they also employ significant active transport to move substances into and out of blood. In fact, it is estimated that at least 25 percent of the body's energy is expended on active transport of substances at the cellular level. The study of active transport carries us into the realms of microbiology, biophysics, and biochemistry and it is a fascinating application of the laws of nature to living structures.


  • 3 At 20°C and 1 atm