Active measurement of gas flow temperature, including in gas turbine combustors
US-9709448-B2 · Jul 18, 2017 · US
US9702768B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9702768-B2 |
| Application number | US-201313961292-A |
| Country | US |
| Kind code | B2 |
| Filing date | Aug 7, 2013 |
| Priority date | Sep 5, 2012 |
| Publication date | Jul 11, 2017 |
| Grant date | Jul 11, 2017 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
An acoustic signal traversing a hot gas is sampled at a source and a receiver and is represented in overlapping windows that maximize useable signal content. Samples in each window are processed to represented in different sparsified bins in the frequency domain. Determining a signal delay between the source and the receiver from a summation of maximum smoothed coherence transform cross-correlation values of different data windows wherein a sparseness of a mean smoothed coherence transform cross-correlation of windows is maximized. Determining a set of delay times wherein outliers are deleted to estimate a time of flight from which a temperature of the hot gas is calculated.
Opening claim text (preview).
The invention claimed is: 1. A method for acoustic pyrometry comprising: recording, by a receiver of an acoustic pyrometer system, an acoustic signal generated by a source included in the acoustic pyrometer system and propagating through a gas medium traveling through a pipe or other channel; arranging a plurality of samples representing the acoustic signal at the source and the receiver into a plurality of windows based on a physically minimum possible propagation delay from the source to the receiver given a temperature range of interest; processing, by a processor within the acoustic pyrometer system, the plurality of samples representing the acoustic signal at the source and the receiver to generate data that represent the plurality of samples in a frequency domain; arranging, by the processor within the acoustic pyrometer system, the data that represent the samples in the frequency domain in a plurality of frequency ranges and selecting one or more frequency ranges with a minimal influence of noise; correlating, by the processor within the acoustic pyrometer system, the data in each selected frequency range of the source with corresponding data of the receiver to determine a weighted cross-spectral power estimate value for each selected frequency range related to the source corresponding to a delay time; determining, by the processor within the acoustic pyrometer system, a summation of the maximum weighted cross-spectral power estimate value of each of the selected frequency ranges by using a range of delays wherein the summation has a maximum, such that a sparseness of a mean weighted cross-spectral power estimate of the selected frequency ranges is maximized; and applying, by the processor within the acoustic pyrometer system, the determined signal delay between the source and the receiver to calculate a temperature of the gas medium. 2. The method of claim 1 , further comprising, the processor arranging the data that represent the plurality of samples in the frequency domain in a plurality of bins and selecting one or more bins with a minimal influence of noise. 3. The method of claim 1 , wherein the plurality of weighted cross-spectral power estimates apply a smoothed coherence transform (SCOT) cross-correlation. 4. The method of claim 1 , wherein a function that maximizes the sparseness is expressed as: arg max t 1 N ∑ n = 1 N R n , k , m ( τ + t n ) 1 with - d ≤ t n ≤ d , wherein t n is a time variation within a range [−d, d]; N is a number of windows; τ is a delay time of a signal; n is an index indicating a window; k is an index indicating a source; m is an index indicating a receiver; and R n,k,m (τ+t n ) represents a smoothed coherence transform cross-correlation for a signal represented in window n, from source k and received at receiver m at a time difference (τ+t n ). 5. The method of claim 1 , wherein a window is based on a physically minimum possible propagation delay from the source to the receiver given a temperature range of interest. 6. The method of claim 1 , further comprising: determining a plurality of signal delays for a plurality of signals generated by a plurality of sources and received by a plurality of receivers. 7. The method of claim 6 , wherein a preferred signal delay is determined from the plurality of signal delays by applying a physical model based on a distance traversed by the acoustical signal. 8. The method of claim 1 , wherein the method is applied to determine a temperature in a gas turbine. 9. The method of claim 1 , wherein the method is applied to determine a temperature in a nuclear power plant. 10. An acoustic pyrometry system comprising: an acoustic signal source enabled to generate an acoustic signal in a gas medium with a temperature; a receiver enabled to record the acoustic signal traveling through the gas medium; a memory enabled to store data and instructions; a processor enabled to execute instructions retrieved from the memory to perform the steps: arranging a plurality of samples representing the acoustic signal at the source and the receivers into a plurality of windows based on a physically minimum possible propagation delay from the source to the receiver given a temperature range of interest; processing the plurality of samples representing the acoustic signal at the source and the receiver to generate data that represent the plurality of samples in a frequency domain; arranging the data that represent the samples in the frequency domain in a plurality of frequency ranges and selecting one or more frequency ranges with a minimal influence of noise; correlating the data in each selected frequency range of the source with corresponding data of the receiver to determine a weighted cross-spectral power estimate value for each selected frequency range related to the source corresponding to a delay time; determining a summation of the maximum weighted cross-spectral power estimate value of each of the selected frequency ranges by using a range of delays wherein the sum
for measuring temperature of moving fluids or granular materials capable of flow · CPC title
Physics · mapped topic
of the velocity of propagation of sound · CPC title
of moving gases · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.