Thermodynamic barrier versus kinetic barrier
Thermodynamic barrier
- Determined by the free-energy change \(\Delta G\) of the step
- A large negative \(\Delta G\) makes the reverse reaction energetically forbidden
- Cannot be overcome by adding more enzyme
- Explains why an irreversible step cannot run backward to relieve accumulation
Kinetic barrier
- Determined by enzyme activity and substrate availability
- Controls how fast flux moves through the step
- Can be changed by altering enzyme amount or activity
- Explains the rate of accumulation, not its direction
A reversible step versus an irreversible step when blocked
Consider two steps in a pathway. Step 1 interconverts \(X\) and \(Y\) with a \(\Delta G\) near zero — it is reversible. Step 2 converts \(Y\) to \(Z\) and is coupled to ATP hydrolysis, giving it a large negative \(\Delta G\) — it is irreversible. If the enzyme for Step 1 is missing, \(X\) accumulates, but some of it can be converted back from \(Y\) because the reaction can run in reverse, so the accumulation is partially buffered. If the enzyme for Step 2 is missing, \(Y\) accumulates and cannot be converted back to \(X\) through Step 2, because that would require reversing an energy-releasing reaction. The accumulation of \(Y\) is therefore not relieved by backward flow through the blocked step.
A reversible step can partially run backward when blocked and buffer the accumulation of its substrate; an irreversible step cannot, because reversing it is thermodynamically forbidden. This is why the accumulation-depletion pattern differs between the two cases.