Dissolved gas analysis has evolved through four distinct technology generations over the past 50 years. Understanding this evolution helps explain why Laser Photoacoustic Spectroscopy (LPAS) represents a step-change in online DGA monitoring capability.
1st Generation: Laboratory Gas Chromatography (1970s-Present)
Laboratory GC remains the reference standard for DGA accuracy. An oil sample is transported to a lab, dissolved gases are extracted via headspace or vacuum degassing, and the gas mixture is injected into a chromatographic column. Different gases travel through the column at different speeds, separating them for sequential detection by a thermal conductivity detector (TCD) or flame ionization detector (FID).
Strengths: Highest accuracy, recognized in all international standards (IEC 60599, IEEE C57.104, ASTM D3612). Limitations: 2-4 week turnaround from sampling to result, quarterly measurement frequency at best, sample handling errors, and gases can escape during transport.
2nd Generation: Online Gas Chromatography (1990s-Present)
Online GC miniaturizes the laboratory GC into a field-deployable instrument. The first-generation Serveron TM8 (now Qualitrol) brought GC to the substation. Strengths: Lab-comparable accuracy, automated measurement every 4 hours. Limitations: Requires carrier gas (helium) replacement every 2-4 months, columns degrade and need replacement every 3-5 years, and quarterly maintenance visits are required.
3rd Generation: Conventional Photoacoustic Spectroscopy (2002-Present)
Pioneered by GE Energy (Kelman) in 2002, PAS represented a paradigm shift: optical gas detection without consumables. A broadband IR lamp is modulated by a mechanical chopper, and optical bandpass filters select specific wavelengths for each target gas. Strengths: Zero consumables, 1-hour measurement interval, 10+ year sensor life. Limitations: Optical filters have finite spectral selectivity (typical bandwidth 50-200 nm), causing some cross-interference between gases with overlapping IR absorption bands.
4th Generation: Laser Photoacoustic Spectroscopy (LPAS) — Present Day
LPAS replaces the broadband IR lamp and optical filters with tunable semiconductor laser diodes — one per target gas species. The key advantage: spectral line width of just 15 femtometers (0.015 picometers), approximately 1,000× narrower than the best optical bandpass filters.
This ultra-narrow line width means the laser excites only the target gas molecule — zero cross-interference from other gas species, water vapor, or volatile organic compounds that share overlapping absorption bands with the target gas. Each laser is precisely tuned to a single rotational-vibrational absorption line unique to one gas species.
LPAS Technical Advantages
| Parameter | Conventional PAS | LPAS (4th Gen) |
|---|---|---|
| Light source | Broadband IR lamp | Tunable laser diodes |
| Spectral selectivity | 50-200 nm (filter) | 0.015 pm (laser line width) |
| Cross-interference | Low-moderate | Virtually zero |
| C₂H₂ detection limit | 0.5 ppm | 0.1 ppm |
| Modulation method | Mechanical chopper | Direct current modulation |
| Moving parts in optical path | Yes (chopper, filter wheel) | None |
| Gases measured simultaneously | 5-7 | 9 + moisture |
The DGA-900 LPAS Implementation
The PAS DGA DGA-900 is built on 4th-generation LPAS technology. Nine independent tunable laser diodes — one for each fault gas — are mounted in a thermally stabilized optical bench. Each laser fires in sequence, and the resulting photoacoustic signal is captured by a high-sensitivity microphone in a gold-coated resonant photoacoustic cell. The entire 9-gas measurement cycle completes in under 15 minutes, providing comprehensive DGA data every hour.
Deployed at China’s 1,000 kV UHV substations and ±800 kV HVDC converter stations — the world’s most demanding transformer monitoring environments — DGA-900 LPAS has demonstrated detection limits of 0.1 ppm for acetylene and 1-2 ppm for hydrogen, matching or exceeding laboratory GC performance in continuous online operation.
References
- IEC 63047 ED1 — Photoacoustic Spectroscopy for DGA (under development)
- Dumitras, D.C., et al., “Laser Photoacoustic Spectroscopy,” J. Optoelectronics Adv. Mater., 2007
- Sigrist, M.W., “Trace Gas Monitoring by Laser Photoacoustic Spectroscopy,” Infrared Physics, 1995
- CIGRE TB 783 — DGA Monitoring Systems (2019)
- Ma, Y., “QEPAS: Recent Advances,” Applied Physics Reviews, 2018