notes/Chemilumesence.md

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# Chemiluminescence in Hydro-Flames — CH* and OH*
## Overview
Chemiluminescence in flames arises when chemical reactions produce **excited radicals** that emit photons as they relax.
The two most important species for combustion diagnostics are:
- CH* (≈ 431 nm, blue)
- OH* (≈ 310 nm, UV)
These are not just “present radicals” — they are **selectively excited products of specific reactions**, and their relative intensity encodes combustion chemistry.
---
## Key Reactions
### CH* Formation (fuel breakdown zone)
CH* is associated with hydrocarbon fragmentation and early flame chemistry.
Typical pathways:
$$
\mathrm{C_2H + O \rightarrow CH^* + CO}
$$
$$
\mathrm{CH_2 + O \rightarrow CH^* + OH}
$$
$$
\mathrm{C + H_2 \rightarrow CH^* + H}
$$
These reactions dominate in **fuel-rich or near-front regions** of the flame.
---
### OH* Formation (oxidation zone)
OH* is associated with high-temperature oxidation chemistry.
Typical pathways:
$$
\mathrm{H + O_2 \rightarrow OH^* + O}
$$
$$
\mathrm{O + H \rightarrow OH^*}
$$
$$
\mathrm{H_2 + O \rightarrow OH^* + H}
$$
These reactions dominate in **lean or well-oxidised regions**.
---
## Why Excited States Are Produced
A chemical reaction releases energy:
$$
\mathrm{A + B \rightarrow C + D + energy}
$$
This energy can be distributed into:
- Translational motion (heat)
- Vibrational energy
- Rotational energy
- **Electronic excitation**
If enough energy is deposited into the electronic degree of freedom:
$$
\mathrm{OH^* \rightarrow OH + h\nu}
$$
$$
\mathrm{CH^* \rightarrow CH + h\nu}
$$
The emitted photon is what we detect.
---
## Non-Equilibrium Nature
These reactions occur under:
- High temperature
- Fast radicalradical collisions
- Non-equilibrium conditions
Therefore:
> Products are often formed **directly in excited states**, rather than being thermally excited.
---
## Why Only Certain Species Emit Strongly
Not all reactions produce visible/UV light. Strong chemiluminescence requires:
- Sufficient reaction energy (~25 eV)
- Good overlap between reaction geometry and excited state (FranckCondon principle)
- Fast radiative decay
CH* and OH* satisfy these conditions.
---
## Energy Scale
Typical photon energies:
$$
E = h\nu
$$
CH* emission (~431 nm):
$$
E \approx 2.9 \text{ eV}
$$
OH* emission (~310 nm):
$$
E \approx 4.0 \text{ eV}
$$
---
## Spatial Structure of the Flame
- CH* peaks in the **reaction front** (fuel breakdown)
- OH* peaks slightly downstream in the **oxidation zone**
Thus, they probe different regions of the flame.
---
## The OH*/CH* Ratio
Define:
$$
R = \frac{OH^*}{CH^*}
$$
This ratio reflects:
$$
R \propto \frac{\text{oxidation rate}}{\text{fuel fragmentation rate}}
$$
---
### Interpretation
- Fuel-rich:
- High CH*
- Lower OH*
- $$R \text{ small}$$
- Lean:
- High OH*
- Lower CH*
- $$R \text{ large}$$
- Stoichiometric:
- Balanced
- $$R \text{ intermediate}$$
---
## Why the Ratio is Useful
Absolute intensity depends on:
- Optical alignment
- Flame size
- Window fouling
- Sensor gain
But the ratio:
$$
\frac{OH^*}{CH^*}
$$
cancels many of these effects and provides a **robust indicator of combustion state**.
---
## Physical Interpretation
- CH* → “fuel is still breaking apart”
- OH* → “oxidation is occurring”
So:
> The ratio indicates where the flame sits between **fuel-dominated** and **oxidation-dominated** chemistry.
---
## Deeper Insight
Even though both species arise from excited states:
- CH* is fed by **hydrocarbon radical pathways**
- OH* is fed by **oxidation pathways**
Thus the ratio is not just energy-related — it reflects:
> **Which chemical pathways dominate locally**
---
## Summary
- Chemiluminescence arises from **excited radicals formed during reactions**
- CH* and OH* originate from **different parts of the combustion network**
- Their ratio provides a **real-time optical measure of stoichiometry and flame structure**
---