Leighton cycle and chemical system equations
Kinetic derivation · steady state · photochemical anticorrelation
1. Basic chemical system (NO–NO2–O3)
The so-called Leighton cycle is the dynamic closure between three species (NO, NO2 and O3), involved in the three fundamental reactions of the tropospheric photo-oxidative cycle:
- hν: UV radiation
- O(3P): ground-state atomic oxygen
- M: third body (air, N2, O2), stabilises the reaction energy
2. Complete kinetic equations
Definitions:
- \(\ce{NO}\), \(\ce{NO2}\), \(\ce{O3}\)
- J: photolysis coefficient of \(\ce{NO2}\) (s-1)
- k3: rate constant of the \(\ce{NO}\)+\(\ce{O3}\) reaction
- loss: photolysis
- production: NO oxidation
- production from photolysis
- loss via reaction with ozone
3. Elimination of O(³P)
Applying the steady-state approximation to atomic oxygen:
The ozone production rate therefore becomes:
4. Final equation for O3
5. Steady state
At photochemical equilibrium, production equals destruction:
6. Leighton relationship
7. Physical meaning
The ratio \([\ce{NO2}]/[\ce{NO}]\) depends on:
- solar radiation intensity \((J)\)
- available ozone concentration
- kinetic constant \(k_3\) of the titration reaction
As a direct consequence, if \(\ce{O3}\) increases:
- the conversion \( \ce{NO -> NO2} \) increases
- therefore \( [\ce{NO2}]/[\ce{NO}] \) increases
8. Origin of the NO2/O3 anticorrelation
NO emission (e.g. traffic, volcanism)
- \([\ce{NO}]\uparrow\) → \([\ce{O3}]\downarrow\) by titration (R3)
- \([\ce{NO2}]\uparrow\) as product of (R3)
Strong solar irradiance
- \(J\uparrow\) → \([\ce{NO2}]\downarrow\) by photolysis (R1)
- \([\ce{O3}]\uparrow\) through production via (R2)
9. Nocturnal regime
At night \(J = 0\): photolysis stops and the system is governed by (R3) alone:
The inverse proportionality follows directly:
10. When the Leighton cycle is not sufficient
Volatile Organic Compounds (VOCs)
Peroxy radicals \(\ce{RO2}\) convert \(\ce{NO}\) to \(\ce{NO2}\) without consuming ozone:
This produces \(\ce{O3}\) in excess of the Leighton prediction (breaking the anticorrelation).
Other perturbing factors
- \(\ce{HO_x}\) radicals (\(\ce{OH}\), \(\ce{HO2}\), radical chains): introduce strong non-linearities
- Long-range atmospheric transport (non-local \(\ce{O3}\), local \(\ce{NO2}\)): decouples the variables
- Volcanic emissions (\(\ce{SO2}\), secondary oxidations, aerosol formation): alters ozone chemistry
11. Complete system
Including the additional terms due to VOCs:
12. Conclusions
The Leighton cycle provides a fundamental framework for understanding ozone chemistry under steady-state conditions, but is only a starting point for describing the complexity of real atmospheric chemistry, which includes numerous additional species and processes.
References
- Leighton, P. A. (1961). Photochemistry of Air Pollution (Vol. 9). Academic Press.
- Seinfeld, J. H., & Pandis, S. N. (2016). Atmospheric Chemistry and Physics: From Air Pollution to Climate Change (3rd ed.). John Wiley & Sons.
- Finlayson-Pitts, B. J., & Pitts Jr, J. N. (2000). Chemistry of the Upper and Lower Atmosphere: Theory, Experiments, and Applications. Academic Press.
- Mannschreck, K., Gilge, S., Plass-Duelmer, C., Fricke, W., & Berresheim, H. (2004). Assessment of the applicability of NO-NO2-O3 photostationary state to long-term measurements at the Hohenpeissenberg GAW Station, Germany. Atmospheric Chemistry and Physics, 4(5), 1265–1277. https://doi.org/10.5194/acp-4-1265-2004 (Mannschreck et al., 2004)