This invention relates in general to monitoring circuitry, and, more particularly, to a monitoring device for a physical characteristic of a building material adapted to be buried inside a building material.
The strategy for implementing damage detection and the characterization of mechanical structures is commonly called Structural Health Monitoring (SHM). Damages are defined as modifications of the material and/or of the geometrical properties of a structural system, comprising modifications of boundary conditions and connections of the system, that worsen performances of the system. The SHM process implies the observation of the mechanical system over the time using periodically: measurements of dynamic responses coming from an array of sensors, extraction of data of damage characteristics sensed from these measurements, and statistical analysis of these data of characteristics for determining the present health state of the system (also called structural analysis).
The (periodically updated) output of this process is an information about the capacitance of the structure of carrying out its function, considering the unavoidable aging and of degradation in working environments. After extreme events, such as earthquakes or explosions, the SHM is used for a quick screening of the conditions of the structure for providing, almost in real time, reliable information about the integrity of the structure itself.
Nowadays, SHM systems use sensors located outside the surfaces to be controlled. For example, in bridges a number of sensors are used (anemometers for calculating the wind speed, accelerometers, extensometers, motion transducers, temperature sensors, sensors for detecting motion of weights, etc.), which are placed on the external surfaces of beams, ropes or pillars, in order to estimate the effects of loads on the bridge, evaluate the weakening of the bridge, and foresee the probable evolution of the bridge and its expected lifetime.
There are technical reasons that hinder the realization of cost efficient SHM with sensors buried in the same structures to be monitored. In particular, any sensor (of pressure, moisture, temperature, etc.) inside a block of reinforced concrete should be connected to an antenna or to a conductor for communicating outside the block itself the sensed measurements.
Let us consider for example a sensor, buried in a block of concrete, that should communicate to the outside through an antenna buried in the same block. The block of reinforced concrete may cause an attenuation that could range between 0.5 and 1 dB per cm of thickness. See Xiaohua Jin, M. Ali “Reflection and Transmission Properties of Embedded Dipoles and PIFAs inside Concrete at 915 MHz” Antennas and Propagation Society International Symposium, 2009, Print ISBN: 978-1-4244-3647-7. This imposes, at least, a maximum communication distance between the buried sensor (supposedly not supplied by a local battery) and an external sensor, fixed by an energy budget.
Moreover, electromagnetic characteristics of reinforced concrete (different from those of air) cause a reduction of the resonance frequency of the antenna (antenna detuning), that should be taken into consideration while designing. Finally, the presence of metal structures close to the antenna causes interferences that could jeopardize reliability of communications towards the outside.
If a battery connected to the sensor was used instead, there would be time limits of use of the sensor fixed by the battery charge.
The antenna and the radio part of present SHM sensors are physically connected to each other through bond-wire (or bump). This causes reliability problems because inside blocks of pre-compressed reinforced concrete in steady-state conditions (attained after about 1 month), there are pressures of the order of hundreds of atmospheres that make this physical connection between the antenna and the radio part of the SHM sensor very difficult. The poor reliability of this physical connection between antenna and radio part of the SHM sensor is the reason that explains why no sensor is simply connected to the outside through an electric wire (wired connection).
A monitoring device for a physical characteristic of a building material, adapted to be buried inside the same building material and that brilliantly overcomes limitations of known devices, has been devised.
The monitoring device comprises a sensor of the physical characteristic to be monitored, that has an inductor and a circuit adapted to provide an internal supply voltage when the switch is immersed in a variable magnetic field and to transmit a signal representative of the sensed physical characteristic, and for a wireless power supply of the sensor having a resonant L-C series circuit buried into a dielectric layer. The sensor is installed on the dielectric layer and has its inductor magnetically coupled to the inductor of the resonant circuit. The power supplier further has two current terminals that come out of the dielectric layer and that are connectable to a reading circuit of data transmitted by the sensor. The device is adapted to be buried into a block of building material such that the current terminals of the wireless supply come out of the block.
The monitoring device shows advantages of a wired connection while avoiding, at the same time, physical connection between the radio part of the SHM sensor and the “communication circuitry” toward outside of the mechanical structure. Hereinafter reference is made to the “communication circuitry” and not to an antenna for the reasons that will be explained herein below.
A basic scheme of the proposed device is depicted in
Inside the block of building material, that may be reinforced concrete, is buried a wireless power supply device having a L-C resonant circuit buried in a dielectric layer, optionally but not necessarily shielded by a double metal layer, that realizes a physical connection (WIRED) between the outside and the interface with the sensor, as shown in
The “shielded strip”, that prevents the use of the antenna inside the mechanical structure, helps eliminate power losses between antenna and the external apparatus to the mechanical structure due to the reinforced concrete, and further avoids interference problems between antenna and metal structures (reinforcement) in the same block of reinforced concrete.
Moreover, the design/fabrication of the shielded strip does not depend upon the material in which it will be buried. Moreover, this makes the device almost immediately operative because communications between the shielded strip and the sensor do not depend on the mechanical properties and on the electromagnetic parameters (electric conductivity and dielectric constant) of the material in which it will be buried. By contrast, with the known devices that use an antenna buried in a block of reinforced concrete, it is helpful to consider the issue of the antenna detuning and to wait at least 28-30 days in order to let the mechanical properties and the electromagnetic parameters of the reinforced concrete attain a steady state condition before using in a reliable manner the monitoring device.
Close to the sensor “hybrid transformer”, A. Finocchiaro, et al, “RF identification device with near-field-coupled antenna” US patent application number US2009033467, is realized between a primary inductor L1 located on the shielded strip and a secondary inductor L2 that will be interfaced with the radio part of the sensor. This hybrid transformer, that establishes a magnetic coupling between a sensor and a shielded strip, avoids the issue of realizing a bonding.
Moreover, in order to increase the effectiveness of the magnetic coupling in the hybrid transformer, it is helpful to increase both the current through the primary inductor L1 as well as the voltage generated on the secondary inductor L2. For the primary circuit, this is obtained by realizing a series resonance at the working frequency ω between the inductor L1 and the added capacitor C0, that is:
ω2L1C0=1
for the secondary circuit this is obtained by realizing a parallel resonance at the working frequency ω between the inductor L2 and the capacitor Ci, that is:
ω2L2Ci=1
wherein Ci is given by the equivalent input capacitance of the integrated circuit plus an additional contribution adapted to obtain said resonance. In general, if it is difficult to realize the capacitance C0 (high value, losses, precision or fluctuations due to variations of the pressure to which is subjected, etc.) it is possible to add a further inductor L0, thus realizing the following condition:
ω2(L0+L1)C0=1
in order to reduce the value of C0 and thus make it compatible with the materials and realization techniques of the same shielded strip. The inductor L0 and the capacitor C0 may be realized in many different ways, as shown in figures from 3 to 11.
It is possible to realize a rigid or flexible shielded strip as long as desired, because its losses are those typical of shielded conductors (fractions of dB/m compared with dB/cm of reinforced concrete). This device practically does not impose any limits to the distance from the surface at which the sensor may be buried, because it is not affected by the typical problems of power budget that affect known devices in which the sensor (or sensors) is powered using an antenna inside the block of concrete. Moreover, with the structure “shielded”, it is possible to place its sensors close to or at least advantageously anchored to the steel reinforcing rods inside the block of reinforced concrete. If two or three sensors are positioned along the directions of as many orthogonal axes of the shielded strip, as schematically shown in
The proposed structure allows easy execution of the calibration phase of the shielded strip. Indeed, by implementing the structure composed of three shielded strips depicted in
Number | Date | Country | Kind |
---|---|---|---|
VA2010A0097 | Dec 2010 | IT | national |
Number | Name | Date | Kind |
---|---|---|---|
4845311 | Schreiber et al. | Jul 1989 | A |
4943930 | Radjy | Jul 1990 | A |
5703576 | Spillman et al. | Dec 1997 | A |
6529127 | Townsend et al. | Mar 2003 | B2 |
6950767 | Yamashita et al. | Sep 2005 | B2 |
6969807 | Lin et al. | Nov 2005 | B1 |
7034660 | Watters et al. | Apr 2006 | B2 |
7148706 | Srinivasan et al. | Dec 2006 | B2 |
7180404 | Kunerth et al. | Feb 2007 | B2 |
7347101 | Thomson et al. | Mar 2008 | B2 |
7551058 | Johnson et al. | Jun 2009 | B1 |
7637166 | Hecht et al. | Dec 2009 | B2 |
7673501 | Holyoake | Mar 2010 | B2 |
7860680 | Arms et al. | Dec 2010 | B2 |
7986218 | Watters et al. | Jul 2011 | B2 |
8091432 | Hecht et al. | Jan 2012 | B2 |
8635916 | Loverich et al. | Jan 2014 | B1 |
20040153270 | Yamashita et al. | Aug 2004 | A1 |
20050204825 | Kunerth et al. | Sep 2005 | A1 |
20090033467 | Finocchiaro et al. | Feb 2009 | A1 |
20100190435 | Cook et al. | Jul 2010 | A1 |
20110199107 | Adamian et al. | Aug 2011 | A1 |
20130106447 | Bridges et al. | May 2013 | A1 |
Number | Date | Country |
---|---|---|
2466269 | Jun 2010 | GB |
2470225 | Nov 2010 | GB |
Entry |
---|
Jin et al., “Reflection and Transmission Properties of Embedded Dipoles and PIFAs inside Concrete at 915MHz” Antennas and Propagation Society International Symposium, 2009, pp. 1-4. |
Number | Date | Country | |
---|---|---|---|
20120161789 A1 | Jun 2012 | US |