IP Library Granted Patent US 9,797,798
Granted Patent B2
US 9,797,798 · App. 14/163,475 · Granted Oct 24, 2017

Systems and methods for sensitive open-path gas leak and detection alarm

Inventor: Michael B. Frish (Andover, MA)
Assignee: Physical Sciences, Inc.
G01M3/202F17D5/02G01M3/22G01M3/226
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Quick Facts
Patent No.
US 9,797,798
App. No.
14/163,475
Granted
Oct 24, 2017
Kind
B2
Abstract

An apparatus for detecting leaks from a gas pipeline or storage system includes a light source configured to emit a beam with at least one spectral component capable of interacting with pipeline gas, a reflector configured to reflect a portion of the beam, an optical detector configured to detect the reflected beam, a signal processing module coupled to the output of the optical detector configured to analyze the detected beam and output a measured concentration value that characterizes the amount of target gas in the beam path, and a statistical processing module coupled to the signal processing module configured to store and analyze the measured concentration value. The statistical processing module is further configured to compute a value based on statistical information associated with the stored plurality of concentration values and compare the computed value to a first predetermined threshold, and transmit a first alarm signal if the computed value is greater than the first predetermined threshold.

Claims (105)

1. In a gas pipeline or storage system, a method for detecting gas leaks using a tunable diode laser absorption spectroscopy transceiver, a reflective target, and an open-path laser beam, the transceiver and the reflective target aligned and maintained in a fixed spatial relationship, the method comprising the steps of:

a) measuring a gas concentration over a first time interval based on a characteristic of light reflected from the open-path laser beam;

b) repeating a plurality of times the previous step of measuring a gas concentration over a first time interval, the plurality of first time intervals being continuous during a second time interval;

c) averaging the plurality of measured gas concentration values obtained over the second time interval and storing the averaged value in a memory;

d) computing a standard deviation and a higher-order statistic of the plurality of measured gas concentration values relative to the stored average value, wherein the higher-order statistic is a function of a third or higher power of a statistical sample, including a skewness, a moment, a higher order moment, an L-moment, an L-statistic, an L-cumulant, or a kurtosis;

e) computing an alarm value based on the standard deviation, the higher-order statistic and a first predetermined threshold;

f) storing the alarm value in a memory;

g) repeating a plurality of times steps a, b, c, d, e and f;

h) computing an alarm probability based on a plurality of stored alarm values; and

i) transmitting an alarm message if the alarm probability is greater than a second predetermined threshold.

2. The method of claim 1 wherein a path length of the open-path laser beam is greater than 100 feet in length.

3. The method of claim 1 , wherein the higher-order statistic comprises a skewness.

4. The method of claim 2 further comprising measuring the gas concentration via tunable diode laser absorption spectroscopy.

5. The method of claim 2 wherein the first time interval is 100 ms.

6. The method of claim 2 wherein the second time interval is 5 minutes.

7. The method of claim 3 wherein the step of computing the alarm value comprises:

calculating a parameter by multiplying the standard deviation by the skewness; and

comparing the parameter to the first predetermined threshold.

8. The method of claim 3 wherein the step of computing the alarm value is based on a polynomial of the standard deviation multiplied by a polynomial of the skewness.

9. The method of claim 2 wherein the measured gas is one of CO 2 , methane, hydrogen fluoride, hydrogen sulfide, or ammonia.

10. The method of claim 1 further comprising comparing the measured gas concentration with a third predetermined threshold and transmitting an alternate alarm message if the measured gas concentration is greater than the third predetermined threshold.

11. In a gas pipeline or storage system, a method for detecting gas leaks using a tunable diode laser absorption spectroscopy transceiver, a reflective target, and an open-path laser beam, the transceiver and the reflective target aligned and maintained in a fixed spatial relationship, the method comprising:

a) measuring and storing a gas concentration value averaged over a first time interval based on a characteristic of light reflected from the open-path laser beam;

b) repeating a plurality of times the above step of measuring and storing a gas concentration value averaged over a first time interval, the plurality of first time intervals being continuous during a second time interval;

c) computing an average value of the plurality of stored gas concentration values obtained over the second time interval and storing the average value;

d) computing a standard deviation and a skewness of the plurality of stored gas concentration values obtained over the second time interval;

e) computing an alarm value based on the standard deviation, the skewness and a first predetermined threshold;

f) storing the alarm value in a memory;

g) repeating steps a, b, c, d, e and f a plurality of times during a third time interval;

h) computing an alarm probability based on a plurality of stored alarm values obtained over the third time interval; and

i) transmitting an alarm message if the alarm probability is greater than a second predetermined threshold.

12. The method of claim 11 , wherein each time interval of the plurality of first time intervals is 100 ms.

13. The method of claim 12 , wherein the second time interval is 5 minutes.

14. The method of claim 12 , wherein the third time interval is 1 hour.

15. The method of claim 11 , wherein the step of computing an alarm value comprises:

calculating a parameter by multiplying the standard deviation by the skewness; and

comparing the parameter to the first predetermined threshold.

16. The method of claim 15 , wherein the alarm value is set to a first value if the parameter is greater than the first predetermined threshold and set to a second value if the parameter is not greater than the first predetermined threshold.

17. The method of claim 16 , wherein the step of computing an alarm probability comprises calculating the average of the plurality of stored alarm values for the third time interval.

18. The method of claim 11 , wherein the step of computing an alarm probability comprises calculating the average of the plurality of stored alarm values for the third time interval.

19. The method of claim 11 , further comprising the steps of:

comparing the average value of the plurality of stored gas concentration values obtained over the second time interval with a third predetermined threshold; and

transmitting a second alarm message if the average value of the plurality of stored gas concentration values is greater than the third predetermined threshold.

20. The method of claim 11 , wherein the gas is one of CO 2 , methane, hydrogen fluoride, hydrogen sulfide, or ammonia.

21. The method of claim 11 , wherein the skewness is obtained by the equation

g

1

=

1

N

i

=

1

N

(

x

i

-

μ

)

3

σ

3

wherein g 1 is the skewness, N is the number of stored gas concentration values x i obtained over the second time interval, μ is the average value of the stored gas concentration values over the second time interval, and σ is the standard deviation of the stored gas concentration values over the second time interval.

22. In a gas pipeline or storage system, a method for detecting gas leaks using a tunable diode laser absorption spectroscopy transceiver, a reflective target, and an open-path laser beam, the transceiver and the reflective target aligned and maintained in a fixed spatial relationship, the method comprising:

a) measuring and storing a gas concentration value averaged over a first time interval based on a characteristic of light reflected from the open-path laser beam;

b) repeating a plurality of times the above step of measuring and storing a gas concentration value averaged over a first time interval, the plurality of first time intervals being continuous during a second time interval;

c) computing an average value of the plurality of stored gas concentration values obtained over the second time interval and storing the average value;

d) computing a standard deviation and a kurtosis of the plurality of stored gas concentration values obtained over the second time interval;

e) computing an alarm value based on the standard deviation, the kurtosis and a first predetermined threshold;

f) storing the alarm value in a memory;

g) repeating steps a, b, c, d, e and f a plurality of times during a third time interval;

h) computing an alarm probability based on a plurality of stored alarm values obtained over the third time interval; and

i) transmitting an alarm message if the alarm probability is greater than a second predetermined threshold.

23. The method of claim 22 , wherein the step of computing an alarm probability comprises calculating the average of the plurality of stored alarm values for the third time interval.

24. The method of claim 22 , further comprising the steps of:

comparing the average value of the plurality of stored gas concentration values obtained over the second time interval with a third predetermined threshold; and

transmitting a second alarm message if the average value of the plurality of stored gas concentration values is greater than the third predetermined threshold.

25. The method of claim 22 , wherein the gas is one of CO 2 , methane, hydrogen fluoride, hydrogen sulfide, or ammonia.

26. The method of claim 22 , wherein the kurtosis is obtained by the equation

g

2

=

1

N

i

=

1

N

(

x

i

-

μ

)

4

σ

4

wherein g 2 is the kurtosis, N is the number of stored gas concentration values x i obtained over the second time interval, μ is the average value of the stored gas concentration values over the second time interval, and σ is the standard deviation of the stored gas concentration values over the second time interval.

Assignments (2)
CONFIRMATORY LICENSE Recorded Jun 22, 2015
From: PHYSICAL SCIENCES, INC.
To: ENERGY, UNITED STATES DEPARTMENT OF
Reel/Frame 036015/0496 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 28, 2014
From: FRISH, MICHAEL B.
To: PHYSICAL SCIENCES, INC.
Reel/Frame 032322/0045 →
Continuity (2)
Provisional Application 61868275 · Aug 21, 2013
Related Publication 20150054650A1 · Feb 26, 2015