Patent Application
20130027211
(1) Field of the Invention
The present invention concerns a smoke detecting device and a method of detecting smoke. Embodiments of the invention may be applied to the detection of a fire by detection of fine particles and aerosols contained in smoke emitted by a fire.
(2) Description of Related Art
Smoke is one of the first indicators of the presence of a fire. Consequently, detection of smoke may be used to alert people of the presence of a fire in a building enabling them to escape the effects of a fire in time or to put out the fire. Moreover, in the case of nocturnal fires a smoke sensor fitted with an audible alarm may awaken and warn inhabitants of the presence of a fire.
In order to detect the presence of smoke two different types of physical phenomena are typically used. The first type of physical phenomenon involves the diffusion of light by the smoke, dust or associated aerosols. The second type of physical phenomenon exploited in the detection of smoke is the modification by the presence of smoke particles of the speed of movement of ions in the presence of an electric field.
In the case of optical smoke sensors based on the diffusion of light, two operating modes are generally implemented. In the first operating mode, smoke particles block the light between an emitter, for example a light emitting diode (LED) and a receptor, for example phototransistor. The subsequent reduction of light reaching the receptor triggers an alarm. Such sensors are often referred to as reduction optic sensors. In the second operating mode, which tends to be more commonly used, smoke particles diffuse light coming from the emitter and a part of the diffused light is received by a receptor. The signal received by the receptor is then small in absence of smoke but increases significantly in the presence of smoke. When the scattered light reaches the receptor, an alarm is triggered. Such smoke sensors are often referred to as diffusion optic sensors.
Although optical smoke sensors respond rapidly to smouldering fires, reduction optic sensors are efficient only when there is a large distance between the light emitter and the light receptor while diffusion optic sensors are not efficient for the detection of combustion gas or dark smoke which are the first signs of a fire. Moreover light emitters require a substantial electrical power supply, which can be a serious drawback when the sensor operates on batteries, leading to a reduced operating time.
Smoke detectors based on the movement of electrically charged particles, or ions, comprise a source of ionization for the generation of charged particles and a drift chamber in which the charged particles particles can slowly move under the influence of an electric field between electrodes polarized at low voltage. The movement of the ions in the electric field created between the electrodes generates a measurable continuous electric current. When smoke particles enter the drift chamber, they attach to the charged particles, neutralize them or reduce their speed of movement resulting in a significant drop in measured current between the electrodes. The drop in current triggers an alarm. This type of smoke detectors is generally referred to as ionization detectors.
Ionization detectors tend to respond more rapidly and with a reduced amount of smoke particles compared to optical sensors to flaming fires emitting smaller particles. In order to create charged particles, radioactive materials such as americium-241 were previously used. However, owing to new standards, commercialization of such smoke detectors is restricted because of the presence of the radioactive source in the smoke detector.
Another way of creating the charged particles is to use an electrical discharge such as those referred to as corona discharges. In such a way it is possible to generate ions without using a radioactive source. However such devices require a relatively high voltage to produce the ionization of the surrounding gas (air) which, even with a low ionic current (but a high voltage), requires a relatively high current at the power supply level since it is at a low voltage. This again can be a serious drawback when the sensor operates on batteries, leading to a reduced operating time. Moreover the current due to a corona discharge depends significantly on parameters such as air pressure, humidity, etc which can be another serious drawback. Indeed, in a traditional ionic smoke detector the current is measured and an alarm is triggered when the measured current changes by a given percentage. As a consequence it is difficult to detect the difference between the presence of smoke or a change of environmental conditions.
The present invention has been devised to address one or more of the foregoing concerns.
According to a first aspect of the invention there is provided a smoke detector comprising: a housing provided with one or more openings for the passage of smoke particles into an interior of the housing; a first electrode and a second electrode disposed in the interior of the housing for generating an electric field by application of an electrical potential therebetween; a detection chamber defined between the first electrode and the second electrode, the detection chamber comprising an ionisation zone for the generation of charged particles by ionisation of air in the vicinity of the second electrode and a drift zone for the movement of charged particles towards the first electrode; a measurement device for measuring an electrical parameter representative of the electrical current generated between the first electrode and the second electrode by the charged particles; wherein the electrical potential between the first electrode and the second electrode is maintained at a first electrical potential level which is less than and in the vicinity of an electrical potential threshold level at which at corona phenomenon is generated such that in the absence of smoke no corona phenomenon is generated in the vicinity of the second electrode and in the presence of smoke a corona phenomenon is generated in the vicinity of the second electrode.
In embodiments, the first electrode is of planar form and the second electrode is a wire arranged parallel to the first electrode.
In embodiments, the first electrode is of cylindrical form and the second electrode is a wire disposed within the first electrode along the longitudinal axis of the first electrode.
In embodiments, the first electrode is perforated.
In embodiments, the second electrode is a conductor with a sharp tip facing towards the first electrode which has at least one portion of planar shape.
In embodiments, the second electrode is held at a positive electrical potential with respect to the first electrode.
In embodiments, the first electrical potential level is in the range of from 400V to 1000V with respect to the first electrode.
In embodiments, a metallic shielding grid connected to ground potential is provided to prevent the entrance of stray ions inside the detection chamber.
In embodiments, the electrical potential threshold level is in a range of from 400V to 500V.
In embodiments, the first electrode has a diameter in the range of from 30 mm to 50 mm and the second electrode has a diameter in the range of from 20 μm to 30 μm.
In embodiments, the second electrode has a curvature radius of the tip of less than 30 μm.
Embodiments of the invention will now be described, by way of example only, and with reference to the following drawings in which:
In a second embodiment of the invention as illustrated in
In a third embodiment of the invention as illustrated in
The second electrode (112, 212, 312) of each embodiment is connected to a high voltage power supply 55, shown on
In the particular embodiment shown in
In the particular embodiment shown in
In the particular embodiment shown in
In the particular embodiments shown in
In embodiments:
As illustrated in
An electric field E is created between the first electrode (111, 211, 311) and the second electrode (112, 212, 312) by applying a high positive voltage to the second electrode (112, 212, 312) with respect to the first electrode (111, 211, 311). The first electrode may be maintained at ground, for example. The second electrode (112, 212) in the form of a wire or 312 in the form of tip, is held at positive voltage so that a positive corona discharge may occur in the ionisation zone I and the resulting positive ions drift through the drift zone D towards the first electrode (111, 211, 311). The voltage needed to ionize the molecules of air between the first electrode (111, 211, 311) and the second electrode (112, 212, 312) depends on different parameters such as the ionization energy, the presence of particles, the gas pressure, the distance between the electrodes and their shape. The following documents which are incorporated herein by reference thereto present examples of conditions for providing corona discahrge: F. W. Peek, Dielectric phenomena in N.V. engineering, Mc Grow Hill, 1929; P. Atten, K. Adamiak, B. Khaddour, J.-L. Coulomb, “Simulation of corona discharge in configurations with a sharp electrode”, Journal of Optoelectronics and Advanced Materials, Vol. 6, pp. 1023-1028, 2004; N. Oussalah, Y. Zebboudj, “Negative corona compution in air”, Engineering with Computers, pp. 296-303, 2006.; and M. Arrayas, M. A. Fontelos, J. L. Trueba, “Ionization fronts in negative corona discharges”, Phys. Rev. E, Vol. 71, 2005.
During a corona discharge, the space between the first electrode and the second electrode is divided into the two distinct regions described above: (i) a high field ionization region I surrounding the second electrode (112, 212, 312) where the ions are created and (ii) a low field drift region D occupying the remaining space between the two elecrodes (111, 211, 311) and (112, 212, 312). These two distinct regions are illustrated in part (ii)
In air, and in the absence of smoke, the voltage threshold at which a corona phenomenon will be triggered is strongly dependent on the wire diameter of the second electrode (112, 212), or the radius of the curvature of the tip 312. In the example of the present embodiment, the corona voltage threshold is about 2.5 kV with a wire diameter of the second electrode of 25 μm and a distance between the electrodes of 18 mm.
The electrical potential between the first electrode and the second electrode is maintained at a first electrical potential level which is less than and in the vicinity of an electrical potential threshold level at which at corona phenomenon is generated such that in the absence of smoke no corona phenomenon is generated in the vicinity of the second electrode and in the presence of smoke a corona phenomenon is generated in the vicinity of the second electrode.
The voltage applied between the first electrode (111, 211, 311) and the second electrode (112, 212, 312) is set to be less than the corona threshold in order to set the system in an intermediate state such that in the absence of smoke particles a corona phenomenon is not generated, while in the presence of smoke particles a corona phenomenon is generated.
The corona phenomenon is generated in the presence of smoke particles since the smoke particles become polarised by the strong electric field in the vicinity of the second electrode (112, 212, 312) thereby increasing the electric field in the detection zone DZ such that it exceeds the corona effect triggering threshold leading to the generation of a corona effect. This effect is detected by the amplifier 50 measuring the current and triggers an alarm to indicate the presence of smoke.
A typical signal is presented in
There is a clear threshold of ionization in presence of smoke particles which is much lower than the one in the absence of smoke particles.
Although the invention has been described with reference to specific embodiments it will be appreciated that the present invention is not limited to the specific embodiments, and modifications will be apparent to a skilled person in the art which lie within the scope of the present invention.
For instance, while in the foregoing examples have been described with relation to electrodes configured in a wire-plate, cylindrical or point-plate geometries, it will be appreciated that other suitable geometrical electrode configurations may be used to ionize air to provide a corona discharge such as a two-wire geometry or spherical geometry.
Many further modifications and variations will suggest themselves to those skilled in the art upon making reference to the foregoing illustrative embodiments, which are given by way of example only and which are not intended to limit the scope of the invention, that being determined solely by the appended claims. In particular the different features from different embodiments may be interchanged, where appropriate.
In the claims, the word “comprising” does not exclude other elements or steps, and the indefinite article “a” or “an” does not exclude a plurality. The mere fact that different features are recited in mutually different dependent claims does not indicate that a combination of these features cannot be advantageously used.
