Time lag approach for measuring thermal conductivity and specific heat

• US 6,019,505 A
• Filed: 12/31/1997
• Issued: 02/01/2000
• Est. Priority Date: 12/31/1997
• Status: Expired due to Term

• Current Assignee: Honeywell Incorporated (Honeywell International Inc.)
• Original Assignee: Honeywell Incorporated (Honeywell International Inc.)
• Inventors: Bonne, Ulrich, Kubisiak, David, Matthys, Robert J., Schuldt, Spencer B.
• Primary Examiner(s): MISKA, VIT W
• Application Number:
  US09/001,530
• Time in Patent Office: 762 Days
• Field of Search: 374/40, 374/43, 374/44, 73/204.16, 73/204.17, 73/204.18, 365/556, 365/557
• US Class Current: 374/40
• CPC Class Codes: G01N 27/18 caused by changes in the thermal conductivity of a surrounding material to be tested G01N27/20 takes precedence

Abstract

A method and apparatus for providing a more direct approach to determine the thermal conductivity, thermal diffusivity and specific heat of a fluid of interest, independently of the amplitude of the sensor output. This is preferably accomplished by measuring one or more variable phase or time lags between selected input and output AC signals, and directly deriving the thermal conductivity, thermal diffusivity and specific heat therefrom. Such derivation is therefore less dependent than amplitude-based sensors on occasional or unpredictable drift in sensor resistive elements.

Claims

1. Apparatus for determining a selected property of a fluid of interest, comprising:

heater means in thermal communication with the fluid of interest, said heater means having a resistance that changes with temperature;

heater energizing means connected to said heater means for energizing said heater means, said heater energizing means providing a transient elevated temperature condition in said heater means;

sensor means in thermal communication with the fluid of interest and spaced from said heater means, said sensor means having a resistance that changes with temperature;

first time lag means for determining a first time lag between the transient elevated temperature condition of said heater means and a transient elevated temperature response of said sensor means; and

determining means for determining the selected property of the fluid of interest using the first time lag.

2. Apparatus according to claim 1 further comprising sensor energizing means for energizing said sensor means with an input power signal that has a phase relative to the periodic time-varying input signal of said heater energizing means such that substantially no heat is transferred from the fluid of interest to the sensor means during the transient elevated temperature condition.

3. Apparatus according to claim 1 wherein said determining means determines the thermal diffusivity D_t of the fluid of interest based on the relation:

space="preserve" listing-type="equation">D.sub.t =d.sup.2 /4Δ

z

where,

d=the separation distance between said heater means and said sensor means,

Δ

z=the first time lag between the transient elevated temperature condition of said heater means and said transient elevated temperature condition of said sensor means as determined by said first time lag means.

4. Apparatus according to claim 3 further comprising means for determining the specific heat C_p of the fluid of interest based on the relation:

space="preserve" listing-type="equation">C.sub.p k/D.sub.t

where,

k=the thermal conductivity of the fluid of interest,

D_t =the thermal diffusivity D_t determined in claim 3.

5. Apparatus according to claim 1 wherein said heater energizing means provides a periodic time-varying input signal to said heater means to induce a transient elevated temperature condition in said heater means, said apparatus further comprising first output means for providing a first output signal that is proportional to the resistance of said heater means.

6. Apparatus according to claim 5 further comprising sensor energizing means for energizing said sensor means, said sensor energizing means providing a periodic time-varying input signal to said sensor means that is shifted in phase relative to the periodic time-varying input signal of said heater energizing means.

7. Apparatus according claim 6 further comprising:

second output means for providing a second output signal that is proportional to the resistance of said sensor means; and

second time lag means for determining a second time lag between the input power signal provided by said sensor energizing means and the second output signal.

8. Apparatus according to claim 7 wherein said sensor energizing means comprises a phase shifter for shifting the phase of the periodic time-varying input signal provided by said heater energizing means by an amount which causes said second time lag to be substantially equivalent to a predetermined value.

9. Apparatus according to claim 8 wherein said predetermined value is equivalent to the second time lag when measured with said sensor means under a vacuum condition.

10. Apparatus according to claim 9 wherein the input power signal provided by said sensor energizing means has an amplitude, wherein said amplitude is selected to provide a power-resistance ratio in said sensor means that is substantially identical to the power-resistance ratio in said sensor means when measured under a vacuum condition.

11. Apparatus for determining selected characteristics of a fluid of interest, comprising:

heater means in thermal communication with the fluid of interest, said heater means having a resistance that changes with temperature;

heater energizing means connected to said heater means for energizing said heater means, said heater energizing means providing a periodic time-varying input signal to said heater means to induce a transient elevated temperature condition in said heater means;

sensor means in communication with the fluid of interest and spaced from said heater means, said sensor means having a resistance that changes with temperature; and

sensor energizing means connected to said sensor means for energizing said sensor means, said sensor energizing means providing a periodic time-varying input signal that has a phase relative to said time-varying input signal of said heater energizing means so that substantially no heat is transferred from the fluid of interest to said sensor means during the transient elevated temperature condition.

12. Apparatus according to claim 11 further comprising:

first output means for providing a first output signal that is proportional to the resistance of said heater means;

second output means for providing a second output signal that is proportional to the resistance of said sensor means;

time lag means for determining a time lag between the first output signal and the second output signal during the transient elevated temperature condition; and

determining means for determining the thermal diffusivity, D_t, of the fluid of interest using the time lag.

13. A method for determining selected characteristics of a fluid of interest under non-vacuum conditions using a heater means and a sensor means, wherein each of said heater means and said sensor means are in thermal communication with the fluid of interest and have a resistance that changes with temperature, the method comprising the steps of:

energizing the heater means with a periodic time-varying input signal to induce a transient elevated temperature condition in said heater means;

energizing the sensor means with a periodic time-varying input signal that has a phase relative to said period time-varying input signal that is provided to the heater means such that substantially no heat is transferred from the fluid of interest to said sensor means during the transient elevated temperature condition.

14. A method according to claim 13 further comprising the calibration steps of:

subjecting the sensor means to a vacuum condition;

applying a calibration time-varying input signal to the sensor means to provide a transient elevated temperature condition in the sensor means; and

measuring a vacuum time lag between the calibration time-varying input signal and the resulting elevated temperature response in the sensor means.

15. A method according to claim 14 further comprising the steps of:

subjecting the heater means and the sensor means to the fluid of interest;

measuring the time lag between the time-varying input signal to the sensor means and the corresponding transient elevated temperature response in the sensor means; and

shifting the periodic time-varying input signal that is provided to the sensor means by a sufficient amount to cause the measured time lag to substantially match the vacuum time lag.

16. A method according to claim 14 further comprising the calibration steps of:

measuring a power-resistance ratio between the power of the input signal to the sensor means and the resulting resistance of the sensor means during the elevated temperature condition under vacuum conditions.

17. A method according to claim 14 further comprising the steps of:

subjecting the heater means and the sensor means to the fluid of interest;

measuring the time lag between the time-varying input signal to the sensor means and the corresponding transient elevated temperature response in the sensor means;

shifting the periodic time-varying input signal that is provided to the sensor means by a sufficient amount to cause the measured time lag to substantially match the vacuum time lag;

measuring a power-resistance ratio between the power of the input signal to the sensor means and the resistance of the sensor means during the elevated temperature condition; and

modifying the amplitude of the periodic time-varying input signal that is provided the sensor means by a sufficient amount to cause the measured power-resistance ratio to substantially match a predetermined vacuum power-resistance ratio.