222 IEEE TRANSACTIONS ON INSTRUMENTATION ANDMEASUREMENT, VOL. 54, NO. 1, FEBRUARY 2005
Narrow-Band Frequency Analysis for Laser-Based
Glass Thickness Measurement
Bing He, François Cabestaing, Member, IEEE, Jack-Gérard Postaire, and Ruodan Zhang
Abstract—This paper presents a narrow-band frequency anal-
ysis approach for a new laser interferometric heterodyne system,
which is used for noncontact glass bottle wall thickness measure-
ment. The measurement signal consists of a number of spectral
components, the strongest of which is a reliable representation of
the above-mentioned thickness. A fast method for searching and
locating this frequency is vital for real-time implementations. As
the standard fast Fourier transform (FFT) proved to be ineffec-
tive for the given problem, we use a combination of a zero-padding
discrete Fourier transform (DFT) with a coarse-to-fine technique
to locate this frequency at a smaller processing cost. Considering
also the Chirp- transform, a comparison of the different methods
under investigation demonstrates the effectiveness of the proposed
approach for online thickness estimation.
Index Terms—Discrete Fourier transform (DFT), fast Fourier
transform (FFT), glass thickness measurement, laser interferom-
etry, narrow-band frequency analysis.
I. INTRODUCTION
I
N GLASS bottle manufacturing, the wall thickness is one
of the crucial parameters to be checked for quality control.
Since bottles often have a narrow neck, it is difficult to introduce
a mechanical sensor inside them and to access the inner surface
in a nondestructive way. The quality control of glass bottles is
traditionally performed offline by sampling, and the character-
istics of the sample are generalized to the batch from which it is
drawn [1]. However, to avoid introducing any bad bottle into the
market, manufacturers should inspect 100% of them. Therefore,
a noncontact, real-time glass wall thickness measuring system
is required to gauge the thickness of each bottle on the produc-
tion line.
Advances in optoelectronics have a considerable impact on
noncontact geometric measurement applications. Lasers usually
play an important role as an information carrier in such opto-
electronic systems because of their physical properties like fre-
quency stability, coherence, etc. [2]–[4]. A new measurement
technique, based on a glass thickness sensing device, has been
developed and patented by Saint-Gobain Cinématique et Con-
trôles (SGCC) [5]. This sensor takes advantage of the properties
of a frequency-tunable laser diode and of the optical reflection
characteristics of transparent materials. The measuring principle
and the system structure are described in Section II.
Manuscript received September 20, 2001; revised February 20, 2004.
B. He and R. Zhang are with EurAsie Synergie, 92400 Courbevoie, France
(e-mail: hebing@rocketmail.com).
F. Cabestaing and J.-G. Postaire are with the Laboratoire d’Automatique,
Génie Informatique & Signal, University of Lille, 59000 Lille, France (e-mail:
fcab@ieee.org).
Digital Object Identifier 10.1109/TIM.2004.838911
From a signal processing point of view, the signal delivered
by the sensor contains a number of components which carry
the significant information about the measured thickness. Under
some ideal conditions, the frequency component with the largest
amplitude in the signal’s frequency spectrum can be considered
as a reliable representation of this thickness. So, a fast method
for searching the spectrum and locating this frequency is the
key problem for real-time implementation. In Section III, the
emphasis is placed on a comparison between different compu-
tation techniques in the frequency domain in terms of online
computational efficiency.
After revealing the inefficiency of the standard fast
Fourier transform (FFT) for the given problem, we pro-
pose a coarse-to-fine scheme for frequency analysis. Since
the bottle rotates in front of the sensor, we combine this
narrow-band frequency analysis scheme with a predictive
model of the thickness variations around the bottle. The main
advantage of this strategy is its computational efficiency for
online implementation. This approach has been compared in
terms of complexity and precision with other procedures, like
the Chirp- transform, which is a realization of the -transform
along a spiral contour on the plane. Under specific conditions,
the Chirp- transform can be determined along the unit circle
in order to reveal details within any subband of interest in
the frequency spectrum. The results, presented in Section IV,
show that this signal processing scheme can be implemented
as an algorithm that supports real-time constraints imposed by
manufacturing rates.
II. SYSTEM STRUCTURE AND ESTIMATION BASIS
The optoelectronic part of the measuring system is composed
of a laser generator with a precisely controlled wavelength that
can be varied within a narrow bandwidth, a beam-splitter, and
a photodetector [5]. The output of the photodetector is filtered
and digitized for further numerical processing. The system con-
figuration is shown in Fig. 1.
The frequency of the monochromatic laser source is con-
trolled during a tuning period [see Fig. 2(a)], its wavelength
is tuned to follow the theoretical formula
(1)
where is the time, a constant, and the initial wavelength
at the beginning of the tuning period .
When a laser beam is projected orthogonally onto a glass
wall, one reflection arises on the outer surface and one on the
inner surface (see Fig. 1). The difference between the
lengths of the two optical paths is , where denotes the
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