Optical online sub nano dyne surface control at plastic films

Opto Dynamic Surface Tension dyne control ODSTM-1 at fast moving
plastic or packaging films, foils or other substrates as like BOPP,
LDPE, LLDPE, HDPE, MDPE, PET, PP, PE, PS, PO, EVA, PTFE, etc.
Introduction
Non-contact, real-time and optical online operation surface-tension or
surface-energy dyne - control systems for running webs as like plastic
films in general, coatings, laminates etc. does not exist world wide.
Due to the broad application field of surface-treated or surface-non-
treated webs of plastic film, non-woven, fabrics, laminates or coated
paper, there is unimaginable market potential here in respect of the
inline process measuring of the surface tension - dyne - and an inline
control of the dyne treatment level and moderate quality control.
A large number of companies are serious interest in project
cooperation, system development, prototyping, manufacturing, testing,
and world wide sales, system purchasing and licensing in order of the
working principle of the ODSTM-1 Process Measuring System and former
Patent application DE19542289.
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Current publications and copyrights targets to the ODSTM-1 subject,
contents, physical working method
Schichtbetrieb - Anforderungen an Schichtdickenmessung in der Mikro-
und Nanotechnik : MessTec & Automation 3/2003, Prof. Peter Pokrovski
Optische Schichten mit ultrahydrophoben und streuarmen Eigenschaften :
Photonik 4/2002, K.Reihs Surface Nanotechnologies GmbH, A.Duparre,
Fraunhofer IOF
Anforderungen an Spektralmessgeraete f=FCr DWDM Systeme : Photonik
4/2002, Laurant Begin, Jim Nerschook, NetTest, Utica, NY, USA
Nanopor=F6se Polymerfilme als kosteng=FCnstige und zugleich hochwertige
Antireflexbeschichtungen : Photonik 4/2002, Dr. Stefan Walheim, FZ-
Karlsruhe, Institut f=FCr Nanotechnologie
JURCA Optoelektronik GmbH : Hochgenaue schnelle
Schichtdickenbestimmung mit Wei=DFlichtinterferometrie, (Highly-accurate
and quick layer-thickness measuring with white light interferometry)
Sensor Magazine 1/2000
JURCA Optoelektronik GmbH - Dr. Gerd Jakob : Koaxiale
interferometrische Schichtdickenmessung, Photonik 9/2000
Datron-Me=DFtechnik GmbH : Mikrowellensensor f=FCr Weg- und
Geschwindigkeitsmessung, (Micro-wave sensor for distance and speed
measuring) Me=DFtech 2/2000
Franz-Patat-Zentrum : Oberfl=E4chenbehandlung - Neues h=F6chstens im
Labor, (Surface treatment =96 the latest, only in the laboratory) PKV-
Magazine 3/2000
Institut f=FCr Kunststoffverarbeitung (Institute for Plastic Processing)
Aachen IKV : Folienextrusion - Erg=E4nzendes Nebeneinander von Gie=DF- und
Flachfolienverfahren, page 39, (Film extrusion =96 complementary use of
casting and flat film techniques) PKV-Magazine 12/1999
In-Line Nahinfrarot-Spektroskopie bei der Kunststoffextrusion :
publication at GIT-Labor-Fachzeitschrift 12/2000, Dipl.Phys. Thomas
Rohe, Dipl.Ing. Sabine K=F6lle - FHG f=FCr Chemische Technologie ( ICT )
Smart Priming : publication at coating 12/2000 by Dr. Michael Bauer,
Dr. Martin Kunz
Semiconductor Metrology: Will Photonics Measure Up ?Scatterometry,
ellipsometry and optoacoustic techniques represent photonics in
metrology toolbox of next-generation integrated circuits : publication
at Photonics Spectra December 2000 by Alain C.Diebold - International
Sematech senior fellow
Enercon : Reprint from Flexo May 1988 : Statistical Quality Control
( SQC ) Applied to Corona Treating, by David Markgraf Enercon : Corona
Treatment - an overview, by David Markgraf, Enercon Industries Corp.
Light Scattering Measures Subangstrom Roughness - by Laurel M.
Sheppard, Photonics Spectra 9/1999
Basis Weight, Sensor for Sheet and Film Products : by Honeywell-
Measurex, Coating Magazine 11/1998
A comparison of 3D static light-scattering experiments with Monte
Carlo simulations : Institute for Anorganic und Physical Chemistry of
the Bremen University, IOP-Publishing Ltd. 32/1999
Was kann Oberfl=E4chenanalyse ? : Dr.J.Goschnick, coating 3/2000
Corona Technologie : Patentinformationen, Anwendungen, Mechanismen :
Dr. Ralf Quack, coating 3/2000
WO 99/23479 : Reflectometer
WO 98/06999 : Method and Device for measuring the thickness of an
insulating coating
US 5.590.560 : Apparatus for measuring viscosity or thickness, surface
tension and surface dilational elasticity
EP 0.225.590 : Verfahren und Vorrichtung zur Bestimmung von Dicken-
und/oder Orientierungs=E4nderungen innerhalb einer optisch aktiven
Materialbahn (Method and device for the measurement of thickness
changes and/or orientation changes within an optically active material
web)
Coating magazine 2-2004, Coronabehandlung von Polymerfolien,
Nachweismethoden, Einflussfaktoren und On line-Kontrolle, Dr.-Ing.
Andreas Kiesow, Dr. J=FCrgen Meinhardt, Prof. Dr. Andreas Heilmann
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Publications and patent applications relating to the state-of-the-art
of STATIC surface tension measurement have been compiled
Significant here are the recent relatively new applications which,
without exception, concern the static detection and determination of
the surface-tension value with sequentially applied liquid drops and
imaging system.
This includes: DE4102990, DE3808860, EP0237221 and DE3410778 A1.
Further information mention in the application document.
Actual situation of the ODSTM-1 development project
Further information concerning publications, patents and engineering
reports are specified in the below applications. Spectral measurements
as well the feasibility study with well known optical institutes are
positive finished. Furthermore some significant modifications and
breakthroughs of the base ODSTM-1 measuring process in using state-of-
the-art monolithic spectrometers and PC support.
Specific information of the current project status on request.
Regarding the ODSTM-1 development and project status together with a
well known optical institute specific measurements with monolithic
spectrometers wave ranges of 1200 =96 1600 nm are successful done all
measurements are based on the detection principle which are described
in the former patent application DE19542289 used non treated LDPE
films in 15 and 30 =B5m thicknesses by 28 mN/m base level comparison
measurements of LDPE films with one side corona treated of 38, 48, 52,
60 mN/m test results are positive with good prospects for further
developments.
Science/test results are to find on our website
formatting link

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Key data of Opto Dynamic Surface-Tension Measuring system ODSTM-1
=95 web widths : up to 6000 mm
=95 web speeds : up to 600 m/min
=95 substrates : PE, PP, HDPE, LDPE, PET, EVA, BOPP, etc.
=95 surface-tension measuring range : 30 - 55 mNm
=95 resolution, respectively, reproduction : +/- 0.5 mNm
=95 single-sided or double-sided measurement of the treated or untreated
sides of the film
=95 IR wavelength range : 1200 nm - 1800 nm
=95 mode of operation : dual scattered-light/multiple-sensor system with
variable wavelengths in transmission mode
=95 measuring method : similar to ellipsometry
=95 measuring gap : approx. 5 - 20 mm
=95 stationary and/or web-traversing measuring head
=95 optical fibre waveguide feed to measuring head system
=95 spatially remote, highly-stable IR light source with beam
processing
=95 wavelength variation via a monolithic optical converter
=95 industrial PC, multiple-processor system, data recording, data
analysis, product documentation, statistics, etc.
=95 actual-value output : analogue 0 - 10 V via optical fiber or serial
RS 232, etc.
S U M M A R Y
Described is a method and device for opto dynamic in-line surface-
tension measurement in which a substrate web running vertically
through a measuring gap is subjected to a chromatic light transmission
from two opto-channels displaced by 90=B0 to each other. This light
transmission is detectable by two optical detection systems located on
the other side of the web. Material-specific wavelength selection,
light transmission angle changes, polarization slot diaphragms and
transverse displacements of the light beam feeder along the optical X-
axis result in extreme scattering and diffraction of the IR light
photons in the boundary layer area on both sides of the sub nano layer
within the substrate web. Their transmitted light intensity enables,
after detection and evaluation, the determination of a direct
relationship to the absolute surface tension.
And this entirely independent of the material-specific influences
like: material and surface consistency, crystallinity, thickness,
density, structure, polar grouping, temperature and type of pre-
treatment.
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Revised contents of patent application DE19542289
The invention concerns a method and device for opto dynamic, i.e. a
non-contact, in-line surface-tension / surface-energy measurement for
running substrates whereby the detection can be in the transverse-
direction or in the running-direction of the web.
In the context of this invention, running substrates or moved web
material is to be especially understood as being plastic films like
PE, PP, LDPE, HDPE, LLDPE, EVOH, PTFE, PET, PS, PMMA, PBMA, PVC, PA
and also laminated or coated film or paper webs which still show a
measurable optical transmission in the wavelength range of 200 to 8000
nm.
A higher material wetting capacity, respectively, a higher material
adhesion capacity, which can be achieved by increasing the surface
tension, is demanded in many application cases for better
printability, coatability or adherence capacity during the
manufacture, finishing, printing and processing of running substrate
webs.
Technical literature which references can be made in respect of these
complex physical relationships, include the following:
=95 J.Hansmann : Korona Oberfl=E4chenbehandlung zur
Haftungsverbesserung, Sonderdruck Papier und Kunststoffverarbeiter
4/7/81 (Corona surface treatment for improved adhesion for special-
print paper and plastics processor)
=95 J.Reif: Physical interaction mechanisms between laser radiation and
the surface of transparent materials, lecture by Laser Colloqium
Erlangen 6.12.1989
=95 Zafiropulos: Laser Ellipsometry, Laser Magazine 5/91
=95 Prof.Dr.-Ing. L.Dorn: Klebefl=E4chen Untersuchungen mittels
Rastertunnelmikroskop Investigation of adhesion surfaces by way of a
scanning tunnel microscope
=95 Dr.Gerstenberg: Korona-Vorbehandlung zur Erzielung von Benetzung und
Haftung, coating (Corona pre-treatment for improved wetting and
adhesion of coatings)
=95 B.Johs: real-time monitoring and controlling with multi-wavelength
ellipsometry, ICSE 93
In simple terms, surface tension, respectively, surface energy, is to
be understood as being a physically measurable tensile stress which
can be determined by the molecules in the boundary layer of the
substrate and the adhesion strength of these molecules. This tensile
stress, which is to be regarded as both energy stress and mechanical
stress, is defined by the physical unit millinewton/m (mN/m), formerly
also dyne/cm.
For the purpose of simplification, the term surface tension is also
used for surface-tension energy in the following text.
As example, a few surface-tension base values of different substrates
are: PS =3D 33 mN/m, PA =3D 43 mN/m, PE =3D 31mN/m, PP =3D 29 mN/m. In
comparison, the values for a few liquids are : Water =3D 72 mN/m,
Methanol =3D 22 mN/m and Tulol =3D 28 mN/m.
An increase in the surface tension, or a 'molecular roughening', of
the material surfaces is currently achieved with industrial pre-
treatment methods using solvents, primer, plasma, UV radiation, flame-
treatment, ozone gassing and corona.
A major quality criterion for the product resulting from the finishing
or manufacturing process, and this is totally independent of the pre-
treatment method used, is the consistent compliance with material-
specific and product=96specific surface tension specifications for the
pre-treatment process. This is not only applicable for a best possible
homogenous surface formation but also for a short-term and long-term
achievement of a narrow surface-tension range which can be extremely
influenced by the external and material factors, type of pre-treatment
and treatment changes. For example, depending on the use of solvent or
water-soluble inks for the printing, the (surface-tension) base range
of extruded LDPE films after the increase in their surface tension is
36 - 46 mN/m, whereby their variations can easily be +/- 3 mN/m and
more.
The current state of the art involves the use of various static, i.e.
not in-line and mostly optical, measuring methods for the detection of
the surface tension for web-shaped or piece materials, e.g. with test
inks as per ASTM-D2578-67, as per the contact angle measuring method,
by way of Rheology for liquids, the ESCA electron spectroscopy for
chemical analysis or the ATR method. The measuring of these methods
always occurs according to the off-line principle, which means that
samples must be taken during machine stop or during the running
production process, with subsequent surface-tension measuring in order
to be able to subsequently adapt to the desired pre-treatment level,
respectively, to try to achieve the specified surface-tension values
in this way.
The significant printed patent specifications and published patent
application specifications under the IPC G01 B 11/30 to be mentioned
hereto are the : EP 003.27.10 A1/B1, EP 023.72.21, DE 28.04.975 Al,
EP 013.49.30 A1, DE 34.06.191 Al, DE 38.08.860 A1, DE 34.10.778 A1, DE
41.02.990 A1, DE 31.05.752 A1, DE 25.37.343. From the application DE
22.25.946, it is also known that there is an attempt to achieve a
differential measurement of the surface tension with two optical
devices in in-line mode before and after the pre-treatment, however,
their mode of operation is not explained. The published patent
application specification DE 38.25.416 A1 describes a dynamic
application method of test inks on running webs in order to obtain an
in-line measurement of the surface tension.
In respect of optical in-line porosity measurement on running webs,
the EP 0. 608. 544 A2 and DE 43.02.137 A 1 contain descriptions of
optical transmission methods with which material independent
measurement values can be derived as a function of the gas
permeability by way of a horizontal measuring head displacement along
the optical axis of the traversing device and over large web widths.
Also known are traversing and in-line working measuring systems, for
the web materials mentioned at the beginning, with which numerous
material-specific characteristics can be measured in the optical
transmission mode, but a surface-tension measurement or mathematical
derivation is not possible.
The static and both dynamic working methods do not full fill the
specified requirements because of the production-related performance
targets and consequently the set criteria for non-contact in-line
surface-tension measurement on running substrates with absolutely no
measurement result influence from material and surface consistency,
crystillanity, thickness, density, structure, polar formation,
temperature, type of pre-treatment and at web speeds of up to 600 m/
min and web width of up to 6000 mm.
The mentioned measuring methods also involve the disadvantage of
possible machine standstill times for sample-taking or the occurrence
of undesired surface-tension fluctuations between the test intervals.
Furthermore, a direct process control or regulation, CIM integration
and product certification are not possible because the systems work
off-line.
The cardinal requirements for a non-contact and in-line working
measuring system can be summarized from the above introductory
description as follows:
=95 useability for web materials like PE, PP, LDPE, HDPE, LLDPE, EVOH,
PTFE, PET, PS, PMMA, PBMA, PVC, PA, laminated or coated film or paper
=95 measurement-independence from material and surface consistency,
crystallinity, thickness, density, structure, polar grouping,
temperature and type of pre-treatment
=95 web speeds of up to 600 m/min and web widths of up to 6000 mm
=95 in-line, real-time and non-contact working measuring method
=95 single measuring head
=95 surface-tension measuring range of 30 to 60 mN/m with a
reproducibility of +/- 1 mN/m
=95 can be integrated into existing traversing systems
=95 computer operation and machine interfacing
=95 insensitive to external influences like dust, vapours, external
light, mechanic shock, etc.
=95 very low maintenance requirement
=95 absolute reliability
=95 easy-to-calibrate
The invention therefore involves the task of describing a method and
device which can best-possibly fulfil the described requirement
profile for opto-dynamic, i.e. a non-contact, surface-tension
measurement.
The invention method for opto-dynamic surface-tension measuring on
running substrates fulfils the set requirement by way of the features
of the patent main claim 1.
According to this, the substrate web which is to be measured and
running through the measuring gap of the system is subjected to a
chromatic light transmission via two optical channels which are
displaced by 90=B0 to each other. This light transmission can be
detected on the other side of the web by two optically identical
detection systems. A transverse displacement of both light spray or
detector units along the optical axis makes it possible to generate
optical scattering and diffraction in the boundary layer area of the
substrate by way of extreme beam angle displacement. After the
evaluation of their captured light photons and their intensity with a
conventional PC, it is possible to determine a direct relationship to
the surface tension, independent of the aforementioned material
influences.
The invention has confirmed that a two-channel, by 90=B0 displaced,
optical transmission through the running web material and extreme X-
axis displacement of the beam angle, both in the horizontal and
vertical direction, and at different wavelengths are necessary in
order to be able to generate, detect and evaluate the desired
scattering and diffraction effects in the two-sided boundary layer and
sub-nano area. It is only the combination of horizontal and vertical
beam path guidance, beam penetration angle change and the wavelength-
specific selection for the used substrate which makes it possible to
eliminate the material-specific influences so that a measurement value
which has a clear relationship to the physical surface tension can be
obtained during the optical transmission through the boundary areas
and the polar groups located there.
This occurs using a relative measuring method via the generation of
differences between two different surface-tension values with material-
identical substrates. It was on the basis of these fundamental
findings that the invention-related opto dynamical surface-tension
measurement method and device for running substrates, which ideally
full fill the aforementioned requirements and make the use of an in-
line system possible, was developed.
A further important advantage of the invention-related measuring
method is that the entire optical arrangement can be integrated in a
single measuring head housing and can therefore be mounted onto an
existing traversing system and be technically incorporated into the
process control system. It is similarly possible to also operate the
measuring head system automatically on extrusion or pre-treatment
machinery, to incorporate it into the control processes of such
machinery and to make possible an in-line certification for the
substrate products produced in such a way. This is a further advantage
of the invention-related method which opens up totally new dimensions
in a production and economic sense.
The aforementioned requirement is also fulfilled by a device for opto-
dynamic surface-tension measurement on running substrates with the
features of patent claim 7.
According to this, the device is designed so that a single wavelength
tune able light source unit supplies two optically identical channels
which make possible a transmission in a vertical and horizontal
position via two slot diffusers for the substrate web running through
the measuring gap. Both optical channels can be geometrically
displaced in the X and Y direction in respect to the detector units
which are located on the other side of the web and arranged on the
optical axes. The light photons falling into the optical lens
arrangement in the detector unit are captured, bundled and focus onto
photo-sensitive detectors. After their electrical pre-amplification,
the signal analysis and measurement value determination occur with a
conventional PC which also performs all the control tasks for the
wavelength setting, X-displacement of the optical axis and system
calibration.
There are now various ways to lay out and further-develop the system
of this invention in an advantageous way. In this respect, reference
is made to the designs described in the patent claims 1 - 15 and also
to the following explanation of a design example of the invention by
way of the drawings.
In conjunction with the explanation of the preferred design example of
the invention and by way of the drawing, the generally preferred
layout of the system is also explained.
The drawings and the additional diagrams specifically show
=95 Fig. 1 the overall view of the surface-tension measuring device
=95 Fig. 2 the optical illustration of the X and Y slot diffusers on the
photosensitive detectors in the case of optical axes equality
=95 Fig. 3 the optical illustration of the X and Y slot diffusers on the
photosensitive detectors in the case of optical axes displacement
=95 Fig. 4 a diagram of the tension profile and the transmissions
distribution for the determination of the surface tension of PP film
=95 Fig. 5 a diagram of the tension profile and the transmissions
distribution for the determination of the surface tension of PE film.
=95 Fig. 6 - 11 diagrams about the spectral range, differences in the
surface-tension values and the properties with different transmission
criteria
The following first explains the device design and its fundamental
mode of operation in order to thereafter provide a detailed
explanation of the measuring method and the determination of the
surface-tension values for running substrate webs.
Fig. 1 illustrates the entire surface-tension measuring device for
running substrate. The light source device 1 essentially consists of
an industrial broadband light source 4 (e.g. the combination of
deuterium, halogen and IR lamps and the voltage supply and control
unit 5). The joint light beam path is aligned via a lens system 6 and
polarization filter 7 onto the acousto-optic filter 8. The HF
generator 9 for e.g. 10 - 100 MHz makes an infinitely variable
wavelength tuning in the range from 200 nm to 5000 nm possible.
It is similarly possible to perform the detection at specific
wavelengths with broadband or narrow band illumination in the IR
wavelength range of, for example, 1200 - 1800 nm and monolithic
spectrometers in order to replace the expensive acousto-optic
converters.
The coupling-out of the beam occurs via a polarization filter 7 with
its following beam splitter 10 for the generation of two optical
channels, the beams of which are coupled into the broadband optic
fiber bundles 12 and 13 via the two lenses 11.
In the beam feeder housing 2 of the measuring head, the coupling-in of
the two optical channels occurs via the connected optic fiber bundles
12 and 13. The light beam from these is then projected via the lenses
14 onto the two vertically 16 and horizontally 17 arranged slot
diffusers to the web 22 running vertically through the measuring gap
31. For the axis-distant capture of the light photons on the opposite
web side there are large collection lenses 18 located on the optical X
and Y axes. These are cascaded with smaller lenses in the direction of
the detectors 20. The photosensitive detectors 20, located on the base
plate 21, can be broadband photodiodes, photodiode arrays, CCD lines
or image converters. For the coverage of the broad wavelength range of
200 - 2000 nm, it has proven advantageous to select the detectors 20
according to their spectral sensitivity for two wavelength ranges and
use them as pairs.
The measurement gap 31 preferably has a width of 10 mm so that a
sufficiently large clearance remains for the web 22 running through it
even in the case of inexact positioning, centre-guidance or position
movement. For ease of illustration, the mechanical displacement
elements for the X-displacement 23 and 24 of both optical channels to
the mid-axes 32 and 33 are not shown in Fig. 1 and 2. A very important
measurement-related aspect here is the optical detector arrangement 20
which is positioned far outside of the actual focal points 29 so that
the axes-distant and transmitted light photons resulting from the
scattered transmission and diffraction at the boundary area of the
running web can be mapped on the detectors.
Fig. 2 shows the pillow shape 34 of the first optical channel at
detector 20 produced by the vertical slot diffuser 16 and the optical
axis of the beam feeder unit 32 and the detectors 33. Analogue hereto,
the same figure shows the optical image 35 of the horizontally
arranged second channel at detector 20 in the case of axis equality 32
and 33.
An X-displacement of beam feeder unit 32 axis to detector axis 33,
whereby preferably the detector unit is moved relative to the beamer
feeder, results in an optically distorted image in the vertical 36 and
horizontal 37 direction as can be seen in figure 3. The image
distortion generated with the invention measuring methods result from
a combination of the vertical and horizontal slot diffuser geometries
and optical x-axis displacement of the detectors far outside of the
lens focal point 29.
=46rom various production applications and the aforementioned patent
applications it is known that a selection of the material-specific
characteristics of the running substrates at different wavelengths,
the so-called finger printing, is possible. In this measurement
method, this fundamental finding has led to the wavelength selection
combined with the optical X-axis displacement being used for the
compensation of the substrate characteristics in order to be able to
determine the surface-tension value without influence from the
material criteria.
The diagrams in Fig. 4 use, as an example, two material-identical PP
films 38 and 39 with different surface tensions of 37 mN/m
respectively 43 mN/m to illustrate the transmission values detected at
the same wavelength and with photo-sensitive sensors. The lower
ordinate shows the optical transmittance of both substrates 38 and 39
as a function of a one-sided axis displacement between 32 and 33,
their optical axis coverage being defined in items 32 and 33. It can
be clearly seen that the PP films 38 and 39, which are identical in
material but have different surface-tension values, experience a value
difference via the optical axis displacement whereby their substituted
area integral of 40 shows the difference between the surface-tension
values of 37mN/m to 43mN/m as a surface-tension value change. The
displacement value, respectively the displacement direction to the
right is shown on the axis.
Figure 5 make analogue use of two example PE films 41 and 42 having
surface-tension values of 36 mN/m and 42 mN/m to illustrate the area
integral 43 obtained as a difference of the surface value after the
substitution.
The electrical circuit of the optical detectors, which can consist of
individual photodiodes, photodiode arrays or CCD lines, is technically
well-known and therefore not further illustrated. Their electrical
coupling to a conventional PC by way of AD converter cards and/or
multiprocessor cards also requires no further explanation.
The signal analysis and the difference generation are also dealt with
in more depth in the following explanatory part.
As already stated in the introductory part, it is known according to
the invention that two by 90=B0 displaced optical substrate
transmissions and their beam displacement along the optical x-axis
generate scattering and diffraction effects on both sides of the
boundary layer area which are material-specifically dependent on the
used wavelength. The light quantum transmitted and detected in this
way allow, after the signal conditioning, an amount-related
determination of the relative measurement value of the surface
tension. To simplify this device description, all mechanical design
details and information on the traversing device for the left and
right displacements 23 of the optical X-axes 27/28 are not further
described because their fundamental mode of operation is assumed to be
generally known.
The transmission properties, developed with the invention measuring
method, and its derivations for the determination can be explained,
from a physical and light quantum point of view, as follows
The wavelength-dependent transmission change in optically trans
massive substrates 22 produces a material-specific transmission
property, the so-called finger prints, which is generally known and
technically used for numerous applications. For the invention method,
the wavelength change occurs in a range from 200 nm to 8000 nm by way
of a broadband light source 4 and a tune able acousto-optic filter 8.
As we know from the ellipsometric measuring method for transparent
plastic films, optically rotated and polarized beam paths make the
mathematical thickness determination of these running substrates
possible. For the method described here, the polarization filters 7
have the task of beam coupling and decoupling for the acousto-optic
filter 8. An optical and by 90=B0 rotated transmission of the running
substrates 22 is verified via the two channels 12 and 13 and the
longitudinal and transverse slot diffusers 17. This design allows the
longitudinal and transverse oriented material formation, as it often
occurs in the case of biaxial films, coated webs or multi-layers, to
be taken into account in terms of technical detection.
Special slot diffusers 16 and 17 produce extreme light scattering at
their edges and consequently the associated changes in the beam angle
by way of the light photons very distant from the optical axis line
27/28/32/33. These light scattering effects are taken into account and
used, in part, in various industrial methods for the technical
measurement of brightness, opacity, smoothness, divergence, opacity or
porosity of transmission materials. The light scattering transmitted
in the two optical channels during the coupling and decoupling in the
running substrate 22 results in adsorption and diffusion appearance at
their boundary surfaces. The investigations of the light scattering
with chromatic light has shown, contrary to the general wavelength
theory, that changes in molecular structure can be optically proven
and that these are smaller than the used wavelength by a factor of
1000. This means that for a wavelength of 400 nm, for example, it is
possible to optically detect "molecular" roughness of < 400 pm in the
boundary layer area of the respective material side. The boundary
layer areas responsible for the surface tension, material adhesion and
polar groups range between 10 to 200 angstroms, equivalent to 10 to 20
nm.
With this special geometry of the material transmission, the
transmitted light quantum experience an easier material transmission
in the case of changes in the one-sided or two-sided 'molecular
roughening' in the boundary layer area and an associated surface
tension increase and this results in a greater light quantum yield on
the detector side. This is the only way in which the practical results
- which allow a direct correlation to the surface-tension difference
40 and 43 and this totally independent of material/surface
consistency, crystallinity, thickness, density, structure, polar
grouping, temperature or the type of pre-treatment - can be
interpreted.
The transmission increases described and used for this method are
especially pronounced when the used wavelength is close or equal to
the resonance point of the web substrate, i.e. a greatly reduced
optical transmission as opaqueness occurs and a sensory detection
takes place far outside of the lens focal point. These light quantum
related resonance points are assigned material-specifically and only
change insignificantly for the running web during the running
production or finishing process =96 as the practical results show.
When one material side has higher surface-tension values than the
other, this results in detection differences which, after the
evaluation, are proportional to the difference of the surface-tension
values.
Further test series with the invention method show that sufficiently
large quantities of transmitted light quantum can be released with the
described device and the described optical X-axis displacement and its
associated scattering and diffraction effects in the sub nano layer of
the boundary layer area of the substrate web 22.
As this method is based on a relative measurement method, it is
necessary to determine the desired surface-tension values via a
correlation or comparison measurement using the same substrate types
of type groups with lower and higher surface-tension values and a two-
point method.
Based on that necessary explanations, the two-point calibration of the
opto-dynamic method can be summarized by following steps :
in the first calibration step, the substrate type (to be subsequently
dynamically measured) with a known but low surface tension e.g. a PP
film 38 with 37mN/m is placed in the measuring gap on a special device
and statically detected this is followed by the determination of the
resonance point by way of the wavelength variation in the range of,
for example, 200 nm to 8000 nm using the acusto-optical filter 8 for
both optical channels and their photo-sensitive detectors and
appropriate signal conditioning which allows a value-related
evaluation with a PC the optical axes 27/28/32 and 33 are identical
during the first wavelength wobbling procedure the described axis
displacement to the right side in the X-direction up to point 44
occurs during the second wobbling procedure analogue to this, the axis
displacement to the left side in the X-direction occurs during the
third wobbling procedure the material-specific resonance point, which
is determined by the largest adsorption value, can now be calculated
from the three recorded tension integrals by way of a simple
substitution method at the same time, the sum of the integral areas,
which have resulted from the left and right displacement of the two
optical channels 12/13 on the X-axis 27/28, determines within this
resonance point the calibration value 1 for the surface tension of
this PP substrate of 37 mN/m the detection recording of the second and
type-identical PP substrate sample of, for example, 48 mN/m, inserted
in the measuring gap 31 occurs analogue to the above in the second
calibration step whereby the substrate to be subsequently measured is
to be dynamically measured within this range
the further detection recording process is the same as that previously
described it should be noted that other value constellations of, for
example, 29 mN/m for PP film or 31 mN/m for PP film are also
conceivable the source data recording is now secured by the
calculation of the material-specific resonance point (also determined
by the largest adsorption value) by way of the same substitution
method. Tests have shown that the resonance points of both calibration
steps are almost identical, e.g. resonance points at a wavelength of
2800 nm for special PP films and at 3200 nm for special PE films can
be found.
figure 4 shows the hereby resulting tension profiles 38/39 in the
resonance point the sum of the integral areas, which resulted from the
left and right displacement of both optical channels12/13 on the X-
axis, determines the calibration value 2 for the surface-tension
difference of this type-identical PP substrate 3 of 43 mN/m
the integral difference of both calibration recordings is assigned to
the two surface-tension values of 37 mN/m and 43 mN/m, i.e. 6 mN/m, in
order to bring the opto-dynamic relative measurement system in value
agreement with the actual absolute values
the wavelength resulting from the two resonance points now remains
unchanged for the subsequent measuring procedure and during the
running measuring process
the two-point calibration is now concluded
a beam intensity monitoring or deviation is realized in a more
advantageous way in the invention device in that this always takes
place at optical axis coincidence of 32/33 (i.e. at each left/right
cycle of the X-displacement) via the sensors
The measuring procedure and determination of actual surface-tension
values for the running substrate, inline mode and for both stationary
and traversing measuring system versions can be described as follows:
the optical axes 27/28/32 and 33 are identical at measurement start
the described axis displacement to the right side in the X-direction
up to point 44 then occurs with simultaneous recording of the
detection values for the optical channel 12 and 13
this is followed by the traversing movement and detection recording to
the left side in the X-direction
figure 4 shows the recorded tension integral for PP substrates
resulting from the right movement 23 of the beam feeder 2 in relation
to the detector housing 3
on the basis of the two-point calibration values of 37 mN/m and 43 mN/
m, it is now possible to easily compute the actual surface tension
value (which has a value between these two values) by way of the
substitution method
Practical measurements have shown the surface-tension values
determined on running substrate webs with the method and device
described here vary from static measurements by +/ 1 mN/m as an
absolute value and thus remain within the desired measurement
resolution. Measuring ranges of 28 - 53 mN/m have been similarly
achieved.
Figure 5 shows a further example of this calibration, respectively
measuring method and the derived measurement values for a PE substrate
with surface-tension values of 36 mN/m and 42 mN/m.
In the case of a measuring system use in traversing mode, the
described measurement events repeat themselves cyclically over the web
width in the manner generally known for other technical process
measurement systems. In stationary mode, the measuring head usually
remains over the running substrate web although it is also conceivable
that the measuring head could be manually moved to the other side of
the web by way of a mechanical device and thus opto-dynamically
measure the surface tension there.
For the purpose of process control integration or readjustment control
for pre-treatment processes for surface tension increase, as is
commonly desired for corona or flame treatments, the determined
substitution values and the absolute values assigned via the
calibration can be fed to the external equipment in a technically
known way after signal conditioning and a conversion with the same PC.
This applies similarly for the statistical processing of the
measurement data in respect of their mean values, variation
coefficients, trends, limit value exceeding, etc. as such are required
by process measurement systems.
Finally, it is emphases that the invention knowledge is only described
and not limited by the above design examples. The invention knowledge
also allows further methods steps for opto-dynamic surface-tension
measurement on running substrate webs whereby such steps show other,
respectively further, design features.
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PATENT CLAIMS
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1.Method and device for opto-dynamic surface-tension measurement on
running substrate webs like : plastic film, laminated or coated film
or paper webs which still show a measurable optical transmission in
the wavelength range from 200 to 8000 nm, characterized in that the
optically stationary or web width traversing and in-line working
measuring device has two opto-channels (12/13), displaced by 90=B0 to
each other, which are used to subject the substrate web (2) running
vertically through the measuring gap (31) to a light transmission with
chromatic light having a moderately changeable wavelength range of 200
nm to 8000 nm and that, during the transmission, both beam feeders
(12/13) are displaced (23) transversely (left and right) in relation
the optical Y-axes (32/33) and in relation to the detectors (20)
located on the other side of the substrate web and along their optical
X-axes (27/28) so that the two Y-axes (32/33) are not aligned during
the measuring event occurring simultaneously for both channels (12/13)
and that the optical image distortion produced in this way generates
transmissions integrals from which the relative value of the surface
tension is derived.
2. Method according to claim 1, characterized in that an optical
detection of the light photon quantity passing through the running
substrate web (22) and its boundary layer areas occurs outside of the
focal points (23) of the photosensitive elements (20) on the side of
the sensor.
3. Method according to claims 1 and 2, characterized in that the wave
length for finding the largest absorption value of the material web is
infinitely tunable in the range of 200 nm to 8000 nm and that the
surface-tension measurement is taken at this adsorption point.
4. Method according to claims 1 to 3, characterized in that the
displacement process along both optical axes (27/28) involves an
integral recording as function of the transmitted light intensity.
5. Method according to claims 1 to 4, characterized in that the
surface-tension measurement value can be calculated in relation to two
known substrate measurement values of the same material type by way of
the substitution method.
6. Method according to claims 1 to 5, characterized in that two
surface-tension values for identical substrate type are statically
recorded for the purpose of measuring system calibration.
7. Device for implementing the method according to claim 1, whereby
the substrate web (22) running vertically through the measuring gap
(31) is subjected to a chromatic light transmission from one side and
the transmission light intensity is detected on the other side of the
substrate, characterized in that a displacement device geometrically
displaces the beam feeder (with its two optical channels (12/13) which
are displaced by 90 degrees to each other) in relation to the
detectors (20) and along the optical X-axis (27/28) so that their Y-
axes (32/33) are no longer aligned during the measurement process.
8. Device according to claim 7, characterized in that a common
broadband light source (4) is used for the wavelength range of 200 nm
to 8000 nm.
9. Device according to claim 8, characterized in that the wavelength
is infinitely varied by way of an acusto-optical filter (8).
10. Device according to one or several claims out of claims 7 =96 9,
characterized in that two broadband optic fiber bundles (12/13) feed
the beam to the measuring location at the running substrate web (22).
11. Device according to one or several claims out of claims 7 =96 10,
characterized in that the beam projection onto the substrate web (22)
running through the measuring gap is effected via two slot diffusers
(16/17) which are displaced by 90 degrees to each other.
12. Device according to one or several claims out of claims 7 =96 11,
characterized in that a common displacement device moves the beam
feeder (12/13) in relation to the detector housing (3) along the
optical and geometrical X-axis (22/23) to both sides during the
measuring process.
13. Device according to one or several claims out of claims 7 - 12,
characterized in that both photosensitive detectors (20) are arranged
outside of their lens focal points (29) and are displaced by 90
degrees to each other.
14. Device according to one or several claims out of claims 7 - 13,
characterized in that the surface-tension measuring device is
integrated in an autarchic and stationary respectively mechanical
manner in existing traversing systems and incorporated in-line in the
process measuring mode.
15. Device according to one or several claims out of claims 7 =96 14,
characterized in that the mathematical evaluation, the determination
of the surface-tension values and the control of the displacement
device and the acusto-optical filter (8) are effected by way of a
single PC.
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IPM - International Perforation Management
high-tech engineering =96 China =96 Germany - Thailand
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