ATP synthase Created 2026-10-14 Updated 2026-10-18
ATP synthase is a molecular motor that couples downhill proton movement across a cell membrane to formation of ATP from ADP and inorganic phosphate. In oxidative phosphorylation, this is the machinery that makes chemiosmosis productive: an electrochemical gradient becomes reusable chemical driving capacity.[ref]
Its usefulness is a conversion between currencies. A membrane-spanning proton-motive force can power a local machine, while newly formed ATP can participate in energy coupling elsewhere. The enzyme supplies a route between these forms of free energy; it cannot make an energetically uphill total cycle favourable merely by accelerating its chemistry.
Define side as the higher proton electrochemical potential reservoir and side as the synthesis-side reservoir. For transfer at common temperature , define the positive downhill proton-motive force magnitude by
Here is thermodynamic activity, is electric potential, is the molar gas constant and is the Faraday constant. Thus both a higher proton thermodynamic activity and a more positive electric potential on side contribute to the driving magnitude. This definition fixes the sign; conventions for a signed proton-motive force differ. The calculation under chemiosmosis separates these two contributions numerically.
Assume fixed reservoirs, tight mechanical energy coupling, one transported proton per subunit per revolution, and three ATP produced per revolution. Neglect leaks, slipping and membrane transport of the chemical reagents. Let be the local molar Gibbs free energy cost of ATP formation at the stipulated composition, pH and magnesium-binding convention. It is not necessarily the standard state value. Adding changes in the state function gives, per mole of complete turns,
For this model net synthesis is thermodynamically favoured when . Equality is a reversible balance, not a promise of a useful reaction rate. A negative value establishes an available driving margin; it does not specify how fast the enzyme runs.
Choose , , and . These are illustrative inputs, not measurements of the preparation in the experiment below. Then
and . Per ATP, the ideal input is , leaving a driving margin of . The balance point is
At the same synthesis cycle instead has : the chosen reservoirs favour its reverse.
Figure 1.
Chosen ten-subunit model: the free energy balance determines the favoured direction
. Original calculation, not experimental data. Fixed kJ/mol, three ATP per turn, no leak or reagent transport. The second panel adds an explicitly hypothetical one-proton-equivalent transport cost per delivered ATP. Details.
The machine is reversible: sufficient ATP hydrolysis can drive opposite rotation and pump protons uphill. Actual direction also depends on inhibition and available substrates; a weak proton-motive force need not make every intact enzyme immediately run backward. Respiratory uncoupling supplies a different failure mode: a parallel proton leak dissipates the gradient without productive shaft rotation.[ref]
The motor budget is not the whole cost of ATP delivered outside a mitochondrion. Import of ADP and inorganic phosphate, and export of ATP, also draw on the electrochemical gradient.[ref] For a deliberately simplified system budget, assign these transports together one additional downhill-proton equivalent per delivered ATP, valued at the same . This is a chosen accounting convention, not a claim of one extra literal proton through , nor a universal transport stoichiometry. The total becomes equivalents and of gradient expenditure per delivered ATP at . The ratio of stored chemical free energy to that expenditure is , compared with for the motor alone. This system budget changes the resource expenditure, not the motor's balance point . Real transport terms require their own electrochemical potentials, and leaks add further cost.
The membrane motor contains a rotating ring of subunits beside stationary subunit . Two offset water-accessible half-channels connect opposite membrane sides to the ring. A proton enters one half-channel and protonates a glutamic acid residue on a subunit; neutralization permits that site to enter the hydrophobic lipid bilayer. Rotation carries it around to the other half-channel, where it releases the proton. A conserved arginine in subunit helps separate the routes and promotes release. Downhill proton transfer biases rotation; this is not a freely open transmembrane pore.[ref]
The central shaft transmits torque to ; a peripheral stalk prevents the catalytic head from simply co-rotating. Its three catalytic sites, within an head, cycle through different binding shapes. In the simplified binding-change picture, a loose site captures ADP and inorganic phosphate, a tight site favours bound ATP, and opening releases ATP. Rotation changes binding and release as well as chemistry.[ref]
Figure 1.
ATP synthase: proton transfer, shaft rotation and three catalytic sites
. Original functional schematic, not an atomic structure. The side view separates rotor and stationary support; the inset separates the two half-channels. Ten subunits are a chosen example. Details.
One complete, tightly coupled turn cycles each catalytic site once, producing three ATP molecules. If the ring has proton-binding subunits, the ideal motor budget is transferred protons per turn, or per ATP. Ring size varies between organisms; the worked example chooses , as in the studied bacterial systems, rather than assigning ten to every ATP synthase.[ref]
For this example the ring's repeat angle is , whereas the three-site catalytic cycle repeats after . Their ratio is , not an integer. Counting complete turns avoids inventing a fixed integer proton count for every catalytic event. The schematic does not require both parts to advance simultaneously as rigid gears; elasticity allows temporary twisting while their cycles proceed.[ref]