High temperature flame sensor
US-2016369649-A1 · Dec 22, 2016 · US
US10670464B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10670464-B2 |
| Application number | US-201815871033-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jan 14, 2018 |
| Priority date | Jun 30, 2017 |
| Publication date | Jun 2, 2020 |
| Grant date | Jun 2, 2020 |
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A method of collecting radiation information of a turbine blade, the method including: 1) collecting a radiated light from the surface of the turbine blade, analyzing the radiated light using a spectrometer to calculate compositions and corresponding concentrations of combustion gas; 2) calculating an absorption coefficient of the combustion gas at different concentrations; 3) calculating a total absorption rate of the combustion gas at different radiation wavelengths under different concentrations of component gases; 4) obtaining a relationship between the radiation and a wavelength; 5) finding at least 3 bands with a least gas absorption rate; 6) calculating a distance between a wavelength of a strongest radiation point of the turbine blade and the center wavelength, and selecting three central wavelengths closest to the wavelength with the strongest radiation; and 7) acquiring radiation data of the turbine blade in the windows obtained in 6).
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The invention claimed is: 1. A method of collecting radiation information of a turbine blade, wherein the turbine blade is rotated due to the expansion of a combustion gas and the turbine blade is heated to a temperature by the combustion gas, the method comprising: 1) collecting light radiated from a surface of the turbine blade, analyzing the light radiated from the surface of the turbine blade using a spectrometer and determining gas components of the combustion gas and respective concentrations of the gas components, and looking up absorptivities N of the gas components at various wavelengths within a wavelength range in an HITEMP spectral database; 2) calculating an absorption coefficient of the gas components at the respective concentrations of the gas components according to the formula: a=K×ECL+b, wherein a is the absorption coefficient at the concentration of a gas component, K,b are constant factors, E is a relative cross-sectional area of the combustion gas which represents a light-sensitive area of the spectrometer, C is the concentration of the gas component, and L is an optical path length which represents a distance that the light radiated from the surface of the turbine blade propagates in the combustion gas; 3) calculating a total absorption rate of the combustion gas at the various wavelengths under the respective concentrations of the gas components using the following A = ∑ i ( a i * N i ) , A=Σ i (a i *N), formula wherein a i represents an absorption coefficient of an i th gas component, N i represents an absorptivity of the i th gas component, and i is a serial number of a gas component; 4) calculating a radiance of the light radiated from the surface of the turbine blade at the various wavelengths using the formula: M ( λ , T ) = ɛ · C 1 λ 5 1 exp ( C 2 λ T ) - 1 , wherein M(λ,T) represents the radiance when a wavelength is λ and the temperature is T, ε is a radiation coefficient, and C 1 , C 2 are first and second radiation constants; and drawing a curve illustrating a relationship between the total absorption rate obtained in 3), the radiance and the wavelength at a coordinate system; 5) selecting at least 3 bands that comprise smallest total absorption rates with respect to other bands within the wavelength range from the curve obtained in 4), and calculating a center wavelength of each band; 6) calculating an absolute difference between a strongest-radiance wavelength and each center wavelength obtained in 5), and selecting a first center wavelength that has the smallest absolute difference with respect to other center wavelengths, a second center wavelength that has the second smallest absolute difference with respect to other center wavelengths, and a third center wavelength that has the third smallest absolute difference with respect to other center wavelengths; wherein a first band comprising the first center wavelength, a second band comprising the second center wavelength, and a third band comprising the third center wavelength are data acquisition windows of the turbine blade; and the turbine blade has a strongest radiance at the strongest-radiance wavelength within the wavelength range; and 7) acquiring radiation data of the turbine blade in the windows obtained in 6).
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