2015
DOI: 10.1117/12.2181042
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Review of pulse phase thermography

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Cited by 18 publications
(14 citation statements)
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“…The depth resolution of the phase is about 1.5-2μ, where μ is the thermal diffusion length. For PPT evaluations the term 'blind frequency' is often used [4,5,13], 'as a limiting frequency at which the defect presents enough phase contrast to be detected on the phase spectra' . It has been published [13] that the blind frequency and the defect depth are correlating by where C 1 has been called as a correlation constant, which is in the range of 1.5-2.…”
Section: Blind Frequencymentioning
confidence: 99%
See 1 more Smart Citation
“…The depth resolution of the phase is about 1.5-2μ, where μ is the thermal diffusion length. For PPT evaluations the term 'blind frequency' is often used [4,5,13], 'as a limiting frequency at which the defect presents enough phase contrast to be detected on the phase spectra' . It has been published [13] that the blind frequency and the defect depth are correlating by where C 1 has been called as a correlation constant, which is in the range of 1.5-2.…”
Section: Blind Frequencymentioning
confidence: 99%
“…Therefore parameters as e.g. sampling frequency or time duration have to be selected carefully [4][5][6]. In the next sections this paper deals with the consequences of using FFT instead of a Fourier transformation and how this affects the PPT evaluations.…”
Section: Introductionmentioning
confidence: 99%
“…In order to identify the delamination defects in composite materials there exist many infrared thermographic techniques but a few of the techniques are frequently used. They are Pulse Thermography (PT), Lock in Thermography (LT) [2] and Pulse Phase Thermography [3,16] etc. But these methods do suffer from certain limitations.…”
Section: Introductionmentioning
confidence: 99%
“…In PPT, originally proposed by [ 21 ] and recently reviewed by [ 23 ], data are transformed from the time domain to the frequency spectra using the 1D DFT (Discrete Fourier transform): where j is the imaginary number, n designates the frequency increment ( ), is the sampling increment, and and are the real and imaginary parts of the transform, respectively. In this case, real and imaginary parts of the complex transform are used to estimate the amplitude and the phase as described in [ 24 ]: …”
Section: Methodsmentioning
confidence: 99%