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Spec Mapping: This lesson is mapped to OCR H420 Module 2.1.5 — Biological membranes (refer to the official OCR H420 specification document for exact wording). It develops the movement of molecules across membranes by simple and facilitated diffusion, the role of channel and carrier proteins, and the factors that govern the rate of passive transport.
Cells need to move molecules across their membranes constantly: oxygen in, carbon dioxide out, glucose in, waste out. The simplest mechanism for this is diffusion, a passive process requiring no metabolic energy. This lesson develops the OCR H420 Module 2.1.5 content on the movement of molecules across membranes by simple and facilitated diffusion.
Key Definition — Diffusion: The net movement of particles (molecules or ions) from a region of higher concentration to a region of lower concentration, down a concentration gradient, as a result of their random thermal motion.
Diffusion is a passive process — it requires no ATP. The random kinetic motion of particles is the only driving force. Equilibrium is reached when particles are evenly distributed, but net movement stops long before every particle comes to rest; it is the net movement that is zero at equilibrium.
Diffusion occurs in gases, liquids and even solids (slowly). In biology the key examples are:
The rate at which substances diffuse across a surface can be expressed by Fick's law:
Rate ∝ (Surface Area × Concentration Gradient) / Diffusion Distance
This gives us the three main factors that exam answers must refer to.
The steeper the gradient, the faster the rate. A large difference in concentration means more particles move from high to low per unit time.
A bigger surface area allows more particles to cross simultaneously. Exchange surfaces in biology (alveoli, villi, gills, root hairs) are highly folded to maximise surface area.
The shorter the path, the faster the diffusion. Alveoli and capillaries share a membrane just ~0.5 μm thick; a red blood cell squeezes through a capillary so that haemoglobin is close to the alveolar air.
| Factor | Effect on rate |
|---|---|
| Larger concentration gradient | Faster |
| Larger surface area | Faster |
| Shorter distance | Faster |
| Higher temperature | Faster |
| Smaller molecules | Faster |
| Lipid-soluble molecules | Faster across bilayer |
Simple diffusion occurs directly through the phospholipid bilayer. Only certain molecules can do this:
Exam Tip: "Lipid-soluble = simple diffusion; charged or large polar = needs a protein."
When molecules cannot cross the bilayer directly, they can still move down a concentration gradient passively if a protein helps them. This is facilitated diffusion.
Key Definition — Facilitated Diffusion: The passive movement of molecules or ions across a membrane down a concentration gradient, through specific transmembrane proteins (channel or carrier proteins). Like simple diffusion, it requires no ATP.
Facilitated diffusion is passive — no ATP is used — but it differs from simple diffusion because it depends on specific proteins that determine which molecules cross.
graph TD
A[Movement across membrane] --> B["Simple diffusion<br/>through bilayer"]
A --> C["Facilitated diffusion<br/>through proteins"]
A --> D["Active transport<br/>with ATP"]
C --> C1["Channel proteins<br/>ions and water"]
C --> C2["Carrier proteins<br/>glucose amino acids"]
Channel proteins form hydrophilic pores through the bilayer that allow specific ions or polar molecules to pass. They are highly selective — a K⁺ channel admits K⁺ but not Na⁺, for example, due to the geometry of the pore and the charges lining it.
Channels are often gated:
A famous example of a channel is the aquaporin, which allows water molecules to cross the bilayer about 10× faster than they would by simple diffusion.
Carrier proteins bind a specific substrate on one side of the membrane, undergo a conformational change (shape change), and release it on the other side. Unlike channels they do not form a continuous open pore.
| Feature | Channel proteins | Carrier proteins |
|---|---|---|
| Mechanism | Open pore | Shape change |
| Selectivity | High (by size and charge) | High (by shape) |
| Rate of transport | Very high | Lower than channels |
| Typical substrates | Ions, water | Glucose, amino acids |
| Energy required | None (for facilitated diffusion) | None (for facilitated diffusion) |
If you plot rate of transport against substrate concentration:
graph LR
A[Low conc gradient] --> B[Low rate - both mechanisms]
B --> C[Rising conc gradient]
C --> D[Simple diffusion: linear rise]
C --> E[Facilitated diffusion: plateaus at Vmax]
This saturation is an excellent diagnostic for facilitated diffusion in exam data questions.
Model answer for (3): "Both simple and facilitated diffusion move substances down a concentration gradient, do not require ATP and are passive. In simple diffusion, molecules pass directly through the phospholipid bilayer, whereas in facilitated diffusion they pass through specific channel or carrier proteins. Simple diffusion is for small, non-polar molecules such as O₂ and CO₂, while facilitated diffusion is for ions and large polar molecules such as glucose. Facilitated diffusion can become saturated (Vmax) at high concentrations because there are only a limited number of transporters; simple diffusion does not saturate."
The qualitative statement rate ∝ (area × gradient) / distance is a teaching simplification of Fick's first law of diffusion, which is a quantitative differential equation:
J=−Ddxdc
where:
Integrating across a membrane of thickness d with concentration c1 on one side and c2 on the other:
J=dD(c1−c2)
Total transport rate (mol s−1) is then J×A, where A is the cross-sectional area of the membrane. This is the quantitative form of the schoolbook proportionality.
For a particular solute crossing a particular membrane, the diffusion coefficient D and the partition coefficient K (how well the solute dissolves in the bilayer vs water) are usually combined into a single permeability coefficient P:
P=dKD
J=P⋅(c1−c2)
Lipid-soluble molecules (high K, high D) have large P; ions and large polar molecules have P≈0 across a pure bilayer and rely on channels or carriers. This is the quantitative basis of the Overton rule (1899).
A gas of partial pressure p dissolves in plasma at concentration c=αp (Henry's law). For oxygen across the alveolar membrane:
Each of these three numbers multiplies the diffusion rate: doubling area or gradient doubles flux; doubling thickness halves it. Exam answers should refer to these three factors quantitatively where possible.
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