NIST logo
*
Bookmark and Share

Acoustic Techniques in Fluid Metrology

Summary:

The Fluid Metrology Group leads the world in designing and using gas-filled acoustic resonators for measuring the thermodynamic temperature T, the Boltzmann constant kB, and the thermophysical properties (e.g. heat capacity, shear viscosity, acoustic and density virial coefficients) of semiconductor process gases and environmentally benign heat transfer fluids (e.g. refrigerants). Now, we are using our expertise to solve problems related to greenhouse gases and climate change.

Description:

Photoacoustic resonator
Figure 2. Photoacoustic resonator for optical absorption measurements in gases and aerosols.
  1. In collaboration with NIST’s Chemical Sciences Division, we use photoacoustic resonators
    1. for continuous monitoring of the CO2 concentration in ambient air from a tall building rooftop; (see Fig. 2) [1]
    2. for measuring the optical properties of particles (e.g. soot) in air that affect the energy balance of the earth; [2]
    3. to develop a hybrid cavity-ringdown/photoacoustic spectrometer for measuring the abundance of C-14 in samples of CO2 to verify product origin.
  2. In collaboration with China’s National Institute of Metrology, we use cylindrical acoustic resonators to re-determine the Boltzmann constant with fractional uncertainty of 3×10−6 from measurements of the speed of sound in argon. [3a, 3b]
  3. Design a Long-Wavelength Acoustic Flow Meter to measure the flux of carbon dioxide in the stack of a coal-burning power plant to facilitate a carbon tax or cap-and-trade regulations.

Major Accomplishments:

  1. Measured the thermodynamic temperature using cavities acting as simultaneous acoustic and microwave resonators from
    1. 77K to 273 K using a quasi-spherical cavity resonator
    2. 271 K to 552 K using a spherical cavity resonator
    3. documented best-in-the-world techniques of acoustic thermometry
    4. "weigh" the quantity of gas in a large tank with large temperature gradients
tank with insulationFigure 3. Acoustic resonances "weighed" the gas in this 300 liter tank while 13 K temperature differences were present. This is a model for a 30 m3 tank that will be used to calibrate flow meters.



    Resonator for measuring the bulk viscosity in xenon
    Figure 4. Hybrid cylindrical-Helmholtz resonator to measure speed of sound and 2nd viscosity over 27:1 frequency range.
  1. Designed cavity resonators (and associated ducts and transducers) for measuring the thermodynamic temperature from 4 K to 1350 K with fractional uncertainties as small as 3×10−6.[4,5,6,7,8]


  2. Developed a self-calibrating photoacoustic spectrometer with a calculable cell constant (Fig. 2) for absolute measurements of optical absorption in gases and aerosols.[9,10]


  3. Measured the 2nd viscosity (also called “bulk” or “dilation” viscosity) of xenon near its liquid-vapor critical point near 16 °C and 5.8 MPa using a novel hybrid acoustic resonator (Fig 4). [11]


  4. Greenspan acoustic viscometer
    Figure 5. Greenspan acoustic viscometer for gases.
  5. Measured the viscosities and viscosity virial coefficients of semiconductor process gases [NIST Standard Reference Database 134 - SEMIPROP] and environmentally-benign refrigerants [12, 13, REFPROP] using a novel acoustic viscometer.


  6. Cylindrical cavity resonator with acoustic waveguides
    Figure 6. Cylindrical cavity (14 cm long; 6.5 cm diameter) resonator used to measure the speed of sound in semiconductor process gases and refrigerants.
  7. Designed acoustic resonators equipped with acoustic waveguides and remote transducers, and used them to measure the thermodynamic properties of industrial gases under extreme conditions. [6,14]
The NIST Acoustic Thermometer
Figure 1. Three-liter spherical cavity resonator used to measure the thermodynamic temperature from 273 K to 552 K

End Date:

ongoing

Lead Organizational Unit:

pml

Customers/Contributors/Collaborators:

NIST Chemical Sciences Division
Joseph Hodges
David Long
Christopher Zangmeister
Zachary Reed

National Institute of Metrology, Beijing, China
Jintao Zhang
Hong Lin
XiaoJuan Feng

Staff:

Michael Moldover
Keith Gillis
JohnPaul Abbott

Contact

Michael Moldover
301-975-2459 Telephone
michael.moldover@nist.gov

Keith Gillis
301-975-2468 Telephone
keith.gillis@nist.gov