August 11, 2026 · PAS Technology

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.

PAS Technology Deep-Dive → DGA-900 Specifications →

References

  1. IEC 63047 ED1 — Photoacoustic Spectroscopy for DGA (under development)
  2. Dumitras, D.C., et al., “Laser Photoacoustic Spectroscopy,” J. Optoelectronics Adv. Mater., 2007
  3. Sigrist, M.W., “Trace Gas Monitoring by Laser Photoacoustic Spectroscopy,” Infrared Physics, 1995
  4. CIGRE TB 783 — DGA Monitoring Systems (2019)
  5. Ma, Y., “QEPAS: Recent Advances,” Applied Physics Reviews, 2018