The present invention relates to a device for calibrating a multi-roll leveller for levelling a metal strip.
Levelling is a finishing operation generally taking place after thermal treatments or rolling operations. Its purpose is to flatten the metallic sheet. It is based on converting geometrical defects into a system of variable residual strains within the thickness by means of alternating bending stresses. It can be done by means of a multi-roll leveller comprising two series of parallel rolls being arranged such that they are imbricated, as represented in
The ever-tighter tolerances, in terms of flatness and internal stresses, imposed an ever-increasing control of the levelling operations and thus of the calibration step of the levellers.
To better grasp the various adjustment parameters, the main components of a multi-roll leveller are represented in
Thus, calibrating a leveller involves adjusting many parameters such as: the transverse parallelism between the upper and lower rolls which can be set by screw-nut adjustment assemblies or counter-pressure ramps for example, the rolls imbrication at the entry and at the exit of the leveller by tilting the beam, the counter-pressure means in order to compensate for the bending of the rolls under load. In order to efficiently calibrate the leveller, the amount of play, spring and bending of the rolls during bending have to be known.
Equipment to ease the calibration have been developed. As illustrated in
An object of this invention is to solve the aforementioned issues. In particular, the object of the invention is to determine, precisely and easily, the key parameters needed to perform a reproducible under-load calibration for any multi-roll leveller without damaging the measuring means, i.e. the extensometers.
The present invention provides a calibrating bar having a neutral plane N, for calibrating a multi-roll leveller for metal strips, said calibrating bar 10
The invention, as illustrated in
This combination of thickness and yield strength is chosen in such a way that the calibration results only in the strain of the calibration bar within the elastic range. It also makes it possible to withstand the different levels of force of the machine used to flatten the products without reaching the plastic strain.
This thickness, between 1.0 and 2.0 mm, enables the formation of a groove wherein an optical fibre can be embedded.
Preferably the yield strength is between 1400 MPa and 1600 MPa.
The calibration bar is made of metal or metal alloy and preferably of steel. Even more preferably, the calibration bar is made of stainless steel.
The neutral plane is the plane along which there are no longitudinal stresses or strain during bending.
Preferably, the calibrating bar has a quadrilateral, rectangular or square section. In that case, the neutral plane is at half the thickness when no traction is applied, as illustrated in
In the context of this invention, a groove is to be understood as a canal cut. Said groove can be of any shape and form as long as an optical fibre can be embedded within. Preferably, the grooves have a quadrilateral, rectangular or square section.
The adhesive is preferably an epoxy based adhesive.
The optical fibres are configured such that an optical coupler can be connected to them. This can be done by means of a casing.
The optical fibres have a length which permits the fibres to extend over all the rolls of said multi-roll leveller. So, the calibrating bar has a grooves long enough to extend over all the rolls of said multi-roll leveller.
The principle behind the measurement, for the calibration of a multi-roll leveller, is the Fresnel reflection. It describes the reflection and transmission of an incident light on an interface between two different optical media. In this invention, interfaces are made by means of a fibre Bragg grating.
So, the percentage of reflected light varies in function of the wavelength. This percentage has a maximum at the Bragg wavelength λB. The Bragg wavelength is sensitive to strain and temperature.
The Bragg wavelength λB is shifted by change of temperature and/or strain. This shift ΔλB, is approximated by (1):
wherein λB is the Bragg wavelength, CS is the coefficient of strain, ϵ is the applied strain, CT is the coefficient of temperature and ΔT is a change in temperature.
Consequently, the strain of the calibration bar can be measured by interrogating the calibration bar using optical frequency domain reflectometry (OFDR).
This method, as illustrated in
The method comprises the following steps: the tuneable laser source 20 emits a light. An optical coupler 21, splits the light between two paths: a measurement path (i.e. the calibrating bar) and a reference path. Then the lights (i.e. the signals) from the measurement path and from the reference path are recombined using an optical coupler 21 and then sent to an optical interferometer 23.
As known per the skilled in the art, in the optical interferometer, a Fourier transform of the light signal yields the phase and amplitude of the signal as a function of the length along the sensor. The strain is obtained by comparing the signals from the measurement path and from the reference path.
In the case of this invention, at the beginning of the calibration step, the calibration bar is put between the upper and the lower rolls of a multi-roll leveller, said upper and lower rolls are not imbricated. Then the upper and lower rolls are imbricated which deforms the calibration bar and applies a strain on the embedded optical fibres and on the fibre Bragg grating. This strain on the fibre Bragg grating leads to a shift of the Bragg wavelength for each of the reflector of said grating.
However, as explained above, the Bragg wavelength is also impacted by a change of temperature which is detrimental for the calibration step as only the strain underwent by each reflector (the one plumb from the rolls) needs to be measured.
In order to solve the problem of measuring a change of temperature and a strain and not only a strain, the calibration bar comprises an optical fibre on both faces (e.g. on each side of the neutral plane) at equidistance from the neutral plane. Such an arrangement permits to have one reflector in compression and the other one in traction and enables to measure the strain.
For example, during the calibration, the reflector of the first optical fibre plumb from the second roll is in compression, with an unknown strain εCOMPRESSION, while the reflector of the second optical fibre plumb from the second roll is in traction with an unknown strain εTRACTION. Both of them undergoing the same change of temperature ΔT. The interferometer measures the shift of the Bragg wavelength for both reflector (i.e. interface), as expressed by formulas 2.1 and 2.2.
It is possible to suppress the temperature influence when combining the measured ΔλB1 and ΔλB2 by subtracting one to the other, as expressed by formula 3, which permits to find the shift of Bragg wavelength due to the strain.
Because both optical fibres are placed at equidistance from the neutral plane, the value of the strain in compression is the opposite as the one in traction so: εCOMPRESSION=−εEXTENSION which permits to find the strain as per the formula 4:
Preferably, said first groove and said second groove have a depth from 150 μm to 400 μm. An optical fibre is considered to have a diameter from 50 to 125 μm. So, this groove depth range permits to have an optical fibre, inside said the groove, from 25 μm to 350 μm below the surface of said face.
It is possible to embed an optical fibre below the surface of a face so the optical fibre does not protrude over said face, thus avoiding direct contact with the leveller rolls. Moreover, the optical fibre is kept away from the neutral plane when the calibrating bar is under tension.
Preferably, said first groove and said second groove are essentially straight and said first optical fibre 13 and said second optical fibre are essentially straight. Even more preferably, said first groove and said second groove are straight and said first optical fibre 13 and said second optical fibre are straight.
Preferably, said first optical fibre and said second optical fibre have an uniform fibre Bragg grating. For example, the optical fibre has an uniform Bragg grating wherein the reflectors are spaced from one another of a distance of 1.6 mm.
Preferably, said first optical fibre and said second optical fibre are a monomodal optical fibre. This type of optical fibre permits to increase the measurement accuracy since it allows a cleaner spectral response.
Even more preferably, said first optical fibre and said second optical fibre are monomodal optical fibres able to operate in a range from 1500 to 1600 nm.
The first and second optical fibres can be considered as a first pair of optical fibres. The calibration bar can comprise several pairs of optical fibres, and associated grooves and adhesive. For example, as illustrated in
Preferably, the calibration bar comprises a pair of optical fibres for each counter pressure ramps of the calibrated multi-roll leveller.
In order to demonstrate that the claimed calibration bar is easy to use and do not require adaption to each leveller, two different multi-rolls levellers have been calibrated using a calibration bar as illustrated in
The calibrating bar used for the experiment is a calibrating bar having a thickness of 1.8 mm, a length of 800 mm, a yield strength of 1400 MPa and made of stainless steel.
The calibrating bar comprises
The optical fibres are essentially parallel and are connected to an optical coupler.
The first multi-roll leveller comprises 19 working rolls (10 upper rolls and 9 lower rolls) having a diameter of 22 mm while the second comprises 17 working rolls (9 upper rolls and 8 lower rolls) having a diameter of 61.91 mm.
In order to calibrate the multi-roll levellers, the calibrating bar is positioned, along the strip movement direction, at the centre of the leveller width, on the lower working rolls. Then, the upper working rolls are lowered until they contact the calibrating bar. The measured strains have been plotted on
Ultimately, the measurements have been used to calibrate the leveller as known in the state of the art.
Consequently, the claimed calibration bar enables a skilled in the art to easily and precisely perform the calibration of a multi-roll leveller without damaging the measuring means, i.e. the optical fibre.
Filing Document | Filing Date | Country | Kind |
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PCT/IB2021/058489 | 9/17/2021 | WO |