4.7 Article

Transient thermal response of micro-thermal conductivity detector (mu TCD) for the identification of gas mixtures: An ultra-fast and low power method

Journal

MICROSYSTEMS & NANOENGINEERING
Volume 1, Issue -, Pages -

Publisher

SPRINGERNATURE
DOI: 10.1038/micronano.2015.25

Keywords

gas sensor; MEMS; micro-bridge; micro-heater; mu TCD; thermal conductivity sensor; transient heat transfer modeling

Funding

  1. Georgia Tech Research Institute
  2. KWJ Engineering Inc.
  3. NASA
  4. Samsung of America
  5. U.S. Department of Energy

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Micro-thermal conductivity detector (mu TCD) gas sensors work by detecting changes in the thermal conductivity of the surrounding medium and are used as detectors in many applications such as gas chromatography systems. Conventional TCDs use steady-state resistance (i.e., temperature) measurements of a micro-heater. In this work, we developed a new measurement method and hardware configuration based on the processing of the transient response of a low thermal mass TCD to an electric current step. The method was implemented for a 100-mu m-long and 1-mu m-thick micro-fabricated bridge that consisted of doped polysilicon conductive film passivated with a 200-nm silicon nitride layer. Transient resistance variations of the mu TCD in response to a square current pulse were studied in multiple mixtures of dilute gases in nitrogen. Simulations and experimental results are presented and compared for the time resolved and steady-state regime of the sensor response. Thermal analysis and simulation show that the sensor response is exponential in the transient state, that the time constant of this exponential variation was a linear function of the thermal conductivity of the gas ambient, and that the sensor was able to quantify the mixture composition. The level of detection in nitrogen was estimated to be from 25 ppm for helium to 178 ppm for carbon dioxide. With this novel approach, the sensor requires approximately 3.6 nJ for a single measurement and needs only 300 mu s of sampling time. This is less than the energy and time required for steady-state DC measurements.

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