This invention relates to an acoustic sensor for measuring the linear movement using sound waves.
The invention has a particularly interesting application in the field of nuclear reactors, in particular for measuring the movements of the internal structures of a nuclear reactor, such as for example the structure referred to as “core support” intended to receive the nuclear fuel.
During the years of service of a nuclear reactor, it is required to be able to provide controls as well as inspections of the services and of the internal structures of the reactor vessel. It is therefore important to be able to monitor the static deformation of the major members such as the core support structure subjected to substantial temperature and pressure stresses.
Solutions are known that make it possible to measure the deformation and the movements of the internal structures of a reactor vessel. However, regardless of the method of measurement used (for example capacitive, optical, resistive, electromagnetic, etc.), the setting in place of a sensor inside the reactor vessel is required. The sensor is therefore subjected to very severe radiation and temperature conditions that impose a design of the sensors that is particularly complex and expensive which must comply with regulations in terms of nuclear safety for the construction of equipment.
The document “Acoustic sensors for measuring linear deformation under radiation conditions. A. V. Zelenchuk, AtomnayaEnergiya, Vol. 51, No. 3, pp. 167-171, September 1981” describes an acoustic sensor for measuring a linear deformation, associated with a method for measuring, that can be used in conditions of radiation and temperature such as are present in the vessel of a nuclear reactor.
The document describes a device for measuring formed by a first waveguide adapted to guide the emission sound wave and by a second waveguide adapted to guide the reflected sound wave. The two waveguides communicate at the level of one of their ends by the arrangement of a groove on second waveguide. A mobile piston, positioned in contact with the part to be measured, modifies the opening of the groove in accordance with the movement of the part to be measured as such modifying the characteristics of the reflected wave in accordance with the linear movement of the part. Such a device is relatively expensive and complex to produce in particular in light of the number of elements required to produce the device.
On the other hand, the document also describes a method for measuring comprising a step of calibrating the device consisting in taking a measurement of a reference signal without closing off the groove by the piston in order to carry out a calibration of the sensor. Such a method of calibration does not make it possible to obtain measurements that are sufficiently precise, as the calibration is carried out periodically and the measurement conditions can vary between each calibration period, in particular when the sensor is used in an environment subjected to substantial temperature gradients along the measurement device.
The invention has for objective to overcome the aforementioned disadvantages by proposing an acoustic sensor for the measurement of a linear movement making it possible to take precise measurements regardless of the environment wherein the sensor is used and in particular in an environment subjected to severe temperature conditions, typically of a magnitude of 400° C.
For this purpose, the invention proposes an acoustic sensor for measuring a linear movement of an internal structure of a nuclear reactor using sound waves comprising:
The sensor according to the invention uses a single waveguide for the propagation of the emitted wave and of the reflected wave making it possible as such to minimise the number of parts used for the production of the sensor and to minimise the number of parts which are subjected to substantial stress in substantial temperature and radiation conditions.
The acoustic sensor for measuring a linear movement according to the invention can also have one or several of the characteristics hereinbelow taken individually or according to any technically permissible combinations:
The invention also has for object a method for measuring a linear movement of an internal structure positioned in the vessel .of a nuclear reactor using an acoustic sensor according to the invention characterised in that it comprises a step of positioning said sensor in such a way that said electro-acoustic transducer, capable of emitting said sound wave and of receiving the reflected wave, is positioned outside of the vessel of said reactor; and in that said waveguide, capable of guiding said sound wave emitted by said transducer toward a measurement area and capable of guiding the reflected wave, is positioned in the vessel of said reactor.
Advantageously, the method for measuring according to the invention comprises a step of calibrating the acoustic sensor carried out simultaneously during the measurement of the linear movement of the internal structure.
Advantageously, the method for measuring according to the invention comprises a step of analysing the reflection of said emitted wave in such a way as to determine the movement of the internal structure.
Other characteristics and advantages of the invention shall appear more clearly in the description that is provided hereinbelow, for the purposes of information and in no way restrictive, in reference to the annexed figures, among which:
For increased clarity, identical or similar elements are marked with identical reference signs in all of the figures.
The acoustic sensor 10 according to the invention is formed by a waveguide 5 constituted by:
The three sections thus form a continuous waveguide 5 capable of propagating a sound wave.
The acoustic sensor 10 further comprises;
In this first embodiment, the means 15 adapted to extend or retract the waveguide 5 in accordance with the movement of the structure 20 are formed by a metal bellows that makes it possible to decouple in stiffness the portion of the measuring section 13a, secured to the structure 20, in relation to the rest of the waveguide 5. As such, the means 15 make it possible to adapt the shape and/or the length of the waveguide 5 in accordance with the movement of the structure 20. The movement of the structure 20 modifies the length L3 of the measuring section 13 and modifying as such the response time of the reflected signal on the bottom 33 of the waveguide 5 travelling a distance in the waveguide 5 which is according to the movement of the structure 20.
The waveguide 5 is formed by a sealed stainless steel tube filled with a neutral gas. The diameter of the sections 11, 12, 13 and the frequency of the sound wave are defined in such a way as to fulfil the conditions of propagation of a sound wave in a waveguide.
The standard section 12 located between the connecting section 11 and the measuring section 13 has a diameter less than the sections 11 and 13 located on either side of the standard section 12. The difference in diameter between the various successive sections forms geometrical cracks 31, 32 on the junction of the various sections 11, 12, 13. These cracks 31, 32 as well as the bottom 33 of the waveguide 5 as such form acoustic reflectors located inside the waveguide 5.
These reflectors 31, 32 are positioned at a distance L1 and a distance L1+L2 from the transducer 14. As these distances are known and fixed during the measurement phase, the signals reflected by these reflectors will make it possible to carry out a calibration of the acoustic sensor and will also be used for deducing the linear movement of the structure 20,
The graph shows the emission signal S1 emitted by the transducer 14 as well as the echoes E2, E3, E4, E5, E6 recorded by the transducer 14. Each means the reflection of the emission sound wave S1 of which the amplitude and the delay in relation to the emission wave are sufficient to be detected by the transducer 14. The analysis of the echoes by signal processing methods make it possible as such to determine the value of the movement at the end of the acoustic sensor 10 secured to the structure 20.
The three echoes E3, E4 and E5 make it possible to take the measurement of the movement and the echoes E3 and E4 make it possible to calibrate the sensor during the taking of the measurement simultaneously,
Indeed, the echoes E3 and E4 make it possible to determine the rapidity of the sound wave propagating in the waveguide 5 during the taking of the measurement.
Thanks to the particular geometry of the acoustic sensor according to the invention, the calibration of the sensor 10 and the measurement of the movement are carried out using the same sound wave emitted by the transducer. The sensor according to the invention as such makes it possible to determine for each measurement, the rapidity of the sound wave in the waveguide 5.
As such, the acoustic sensor according to the invention can be used in severe temperature conditions, such as for example in the internal vessel of a nuclear reactor with substantial temperature gradients along the waveguide. Indeed, during the production of the measurement the temperature gradients along the waveguide 5 modifying the rapidity of the wave are taken into account during the measurement by an automatic and systematic calibration of the acoustic sensor.
As such, the acoustic sensor according to the invention can be applied perfectly to the measuring of a linear movement of an internal structure of a nuclear reactor. Indeed, the acoustic sensor according to the invention can be positioned in a nuclear reactor vessel without incidence on the precision of the measurement. The electronic portion that is sensitive to the radiation and temperature conditions (i.e. the transducer) is offset outside of the severe environment, i.e. outside of the vessel in our application example.
Such a sensor makes it possible to obtain, regardless of the temperature conditions, a precision of less than a millimetre and preferably less than 0.5 mm for a movement of a magnitude of a millimetre.
In a second embodiment of the invention shown in
Means of sealing 26 are arranged between the piston 25 and the section 13 in such a way as to render the waveguide 5 sealed from the external environment.
In a third embodiment of the invention shown in
Means of sealing 36 are arranged between the cylindrical tube and the section 13 in such a way as to render the waveguide 5 sealed from the external environment.
According to an alternative (not shown) of this embodiment, the cylindrical tube comprises a diameter greater than the third measuring, section 13 in such a way that the cylindrical tube slides outside of the measuring section.
The invention has been particularly described for the measurement of a movement of an internal structure of a nuclear reactor, such as a core support structure; however, the invention can also be applied to the measurement of a movement of any other type of part and can be applied to other fields of use.
The acoustic sensor according to the invention is particularly well suited for measuring a linear movement in an environment subjected to substantial temperatures or temperature gradients.
The other advantages of the invention are in particular the following:
Number | Date | Country | Kind |
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1161190 | Dec 2011 | FR | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP2012/074440 | 12/5/2012 | WO | 00 | 6/4/2014 |