The invention relates to the field of power engineering and can be used in heating systems, more particularly in water heaters or boilers, in disposal systems fueled by the combustion of associated gas, and in electrical energy generating systems.
Pulse combustion apparatuses are known for high coefficient of efficiency and small size and weight per unit of power. However, during operation they generate a high level of vibration at the place of installation, in a heat transfer fluid hydraulic system, in smoke extraction system and in air supply system. Vibrations decrease the equipment life and lead to high level of noise and other unfavorable consequences. Vibrations may spread to rooms located far from pulse combustion apparatus. Vibrations lead to a significant deterioration of human environment.
Measures are taken to decrease vibrations generated by pulse combustion apparatuses. U.S. Pat. No. 4,919,085 employs sand in the air valve housing to reduce a pulse combustion apparatus vibration. In Fulton Pulse HW (PHW) Fully Condensing Hydronic Boiler User Manual, Page 11: How to install elastomer cube isolation mounts guideline, FULTON company indicates a need to install a vibration damper when mounting a pulse combustion apparatus (http://www.manualsdir.com/manuals/345492/fulton-pulse-hw-phw-fully-condensing-hydronic-boiler.html?page=11,).
The closest to the proposed invention is the pulse combustion apparatus according to U.S. Pat. No. 4,259,928, where the air cylinder containing an air nonreturn valve in the air supply channel is connected with the pulse combustion apparatus cover by a vibration damper; besides, the exhaust cylinder in a vent gases exhaust chamber is connected to an exhaust pipe by a vibration damper and the whole boiler is mounted on vibration dampers.
Although not all manufacturers indicate a need to connect pulse combustion apparatuses to a heat transfer fluid hydraulic system using vibration dampers, this need is obvious to specialists in the art.
The measures employed do not produce a desired result and may be improved significantly.
The technical issue addressed by the current invention is a decrease of the level of vibration in pulse combustion apparatuses by a decrease of the level of vibrations generated by a gaseous medium nonreturn valve.
The technical issue is solved by a pulse combustion apparatus comprising a combustion chamber, at least one resonant channel connected to the combustion chamber, a device for removing heat which is linked to the combustion chamber and to the resonant channel and which consists of at least one chamber and/or at least one tube for a heat-exchanging agent, a device for supplying air and combustible gas, which is connected to the combustion chamber, comprising at least one chamber and/or at least one tube for a heat-exchanging agent, a device for supplying air and combustible gas, which is connected to the combustion chamber, comprising at least one gaseous medium nonreturn valve and at least one guard chamber of at least one nonreturn valve, while at least one gaseous medium nonreturn valve is directly or indirectly linked to a the device for removing heat via a vibration isolator.
A form of embodiment is possible, where the resonant channel comprises at least one resonant tube.
Besides, a variant where the combustion chamber is located in a tube, while the resonant channel comprises a gap between the tube and the combustion chamber is possible.
It is preferrable that the walls of at least one guard chamber are lined with a material with sound absorbing properties.
A form of embodiment is possible where the apparatus comprises at least two gaseous media nonreturn valves, at least one of said valves is an air nonreturn valve and at least one of said valves is a combustion gas non-return valve, and at least two guard chambers, respectively, for at least one air nonreturn valve and at least one combustion gas nonreturn valve.
A form of embodiment is also possible where at least one gaseous media nonreturn valve is a combustion mixture nonreturn valve.
A preferrable form of embodiment includes at least one gaseous media nonreturn valve, which is a mechanical nonreturn valve.
A form of embodiment of an apparatus is possible when at least one gaseous media nonreturn valve is directly linked to a device for removing heat via a vibration isolator.
In another form of embodiment, at least one gaseous media nonreturn valve is indirectly linked to a device for removing heat via a combustion chamber using a vibration isolator, while at least one gaseous media nonreturn valve outlet is linked to a combustion chamber by two connection pipes interconnected with a vibration isolator.
Besides, at least one gaseous media nonreturn valve is indirectly linked to a device for removing heat via its guard chamber using a vibration isolator, while at least one gaseous media nonreturn valve outlet is linked to a guard chamber by two connection pipes interconnected with a vibration isolator.
A form of embodiment is also possible where at least one air nonreturn valve is indirectly linked to a device for removing heat via a guard chamber using a vibration isolator, at least one combustion gas nonreturn valve, while at least one air nonreturn valve is linked with the guard chamber, at least one combustion gas nonreturn valve linked by two connection pipes interconnected using a vibration isolator, one of which is connected to the corresponding air nonreturn valve outlet.
Besides, at least one air nonreturn valve is indirectly linked to a device for removing heat via interconnected guard chamber of an air nonreturn valve and guard chamber of combustion gas nonreturn valve, while at least one air nonreturn valve inlet is connected with a guard chamber of an air non-return valve by two connection pipes interconnected with a vibration isolator, one of which is connected to a corresponding air nonreturn valve inlet. Besides, at least one air nonreturn valve is indirectly linked to a device for removing heat via a guard chamber of an air nonreturn valve and guard chamber of combustion gas nonreturn valve, while an air nonreturn valve inlet is connected with a guard chamber of an air non-return valve, which is connected to a combustion gas nonreturn valve guard chamber by two connection pipes interconnected with a vibration isolator.
Besides, at least one air nonreturn valve is indirectly linked with a heat-exchange agent chamber via a combustion chamber using the first vibration isolator while at least one air nonreturn valve is linked directly or via a guard chamber of a combustion gas nonreturn valve, with a combustion chamber, connected to a heat-exchange agent chamber by the first vibration isolator.
Here, at least one air nonreturn valve is additionally linked with a heat-exchange agent chamber using at least one second vibration isolator indirectly via at least one resonant tube, while the end of at least one resonant tube is connected to a heat-exchange agent chamber using at least one corresponding second vibration isolator.
Besides, at least one air nonreturn valve is indirectly linked to a device for removing heat using two consecutively located vibration isolators, while at least one air nonreturn valve inlet is connected via the first vibration isolator with the inlet of a guard chamber of at least one air nonreturn valve, while an outlet of a guard chamber of an air non-return valve is linked via the second vibration isolator with a guard chamber of at least one combustion gas nonreturn valve connected to a device for removing heat.
Vibration isolator may comprise a cylinder-shaped element with at least one transverse corrugation.
Besides, a vibration isolator may comprise a cylinder-shaped element made of elastic material.
Besides, a vibration isolator may comprise a circular membrane, flat or having one or more circular corrugation.
A form of embodiment is possible where at least one shock wave damper rigidly connected to a corresponding nonreturn valve is installed along the gaseous media flow on at least one gaseous media nonreturn valve inlet and/or outlet.
Here, a gaseous media nonreturn valve and at least one damper have the same housing.
Besides, at least one gaseous media nonreturn valve with a rigidly connected shock wave damper are fixed in a required spatial position using elastic elements.
Besides, in an apparatus with any variant of vibration isolators location, at least one gaseous media nonreturn valve is connected to a device for removing heat indirectly via a combustion chamber using a vibration isolator, while at least one gaseous media nonreturn valve is linked to a combustion chamber using a pipe with coaxial connecting pipes located between a tube and a vibration isolator and interconnected forming a maze with an inlet hole made in the said pipe.
Significant vibration and noise during operation are actual issues of pulse combustion apparatuses. Mufflers used in vent gases exhaust chambers and air supply chambers as well as vibration isolation of pulse combustion apparatuses from the place of installation and from hydraulic system have little effect. Meanwhile, despite the use of mufflers and vibration isolators, a high level of noise generated by vibration of structural components of a pulse combustion apparatus remains.
It is evident to pulse combustion specialists that the main source of vibration and acoustic noise in pulse combustion apparatuses is a combustion chamber, where, according to a description of U.S. Pat. No. 4,919,085, an explosive combustion is thought to be occurring.
The studies conducted revealed, that a combustion chamber of pulse combustion apparatuses generates insignificant vibrations during operation, several fold lower as compared to a permissible level, and thus the acoustic noise generated by these vibrations is also significantly lower than the permissible level. The only source of significant vibration and acoustic noise generated by such vibrations in pulse combustion apparatuses are gaseous media nonreturn valves.
Gaseous media nonreturn valves during operation of pulse combustion apparatuses generate a steep front of gas flow velocity and pressure change with characteristics similar to that of a shock wave. This phenomenon is referred hereinafter as the shock wave. The shock wave is a source of vibration and noise of high intensity. Thus, pulse combustion apparatuses operation generates additional vibration and noise of high intensity due to the shock wave.
The shock wave in pulse combustion apparatuses is generated by nonreturn valves. The shock wave has the highest impact on the walls of a nonreturn valve where it is generated. This impact is similar to a shock with a hard object and generates high-intensity vibration of a valve walls.
Pulse combustion apparatuses may include aerodynamic nonreturn valves and mechanical nonreturn valves. The shock wave formation in a dynamic nonreturn valve occurs during the return flow of vent gases due to deceleration and collision of opposite gas flows that are increased by the fact that the velocity of back particles is higher than the velocity of front particles, while the steepness of flow rate changes increases, generating a shock valve.
The character of the shock wave formation in a mechanical nonreturn valve is similar to the shock wave formation in a dynamic nonreturn valve. The shock wave in a mechanical nonreturn valve is generated during an instant deceleration of a return gas flow.
It is known in various technical fields that nonreturn valves may generate vibrations and acoustic noise. These vibrations are generated by a shock of a locking moving element against a fixed housing of a nonreturn valve, generating vibration and noise.
It is evident for the specialists that a moving element of a valve may generate vibrations due to a shock of a moving element against a fixed nonreturn valve housing. However, vibrations in pulse combustion apparatuses are generated by a sudden change of gas flow rate.
For pulse combustions apparatuses specialists, the only evident source of vibration and acoustic noise is an explosive combustion in a combustion chamber.
According to the current invention, a decrease of vibration and acoustic noise generated by these vibrations is achieved by installation of a vibration isolator between a gaseous media nonreturn valve and a device for removing heat. Such a solution for use and location of installation of a vibration isolator is not evident for pulse combustion specialists, as the impact of gas flows rate change in a gaseous media nonreturn valve is out of consideration, while an explosive combustion in a combustion chamber is considered as the evident source of vibrations.
The shock wave is generated by a nonreturn valve. Taking a mechanical nonreturn valve as an example, the shock wave is generated as follows. During mechanical nonreturn valve closure, the membranes move from open valve position to a closed valve position by a return gas flow. As the membranes reach the closed state of the valve, the gas flow stops fast, almost instantly, generating a shock wave in a gas similar to hydraulic shock in hydraulic nonreturn valve closure. With that, a sharp pressure increase occurs on one side of a mechanical valve, while a sharp pressure decrease occurs on the other side of a valve. A valve sustains an impact similar to a shock by a hard object, the valve walls vibrate with their intrinsic resonant frequency. A shock wave spreads in a gaseous media in both directions from a nonreturn valve, generating vibration and noise of high intensity. A shock wave has a high energy, lasts for a short time and has a short front. A shock wave is generated at each pulse operating cycle of gas consumption. The time of a shock wave formation and its transitory processes is a lot shorter than a pulse operating cycle od as consumption. Thus, each shock wave behaves as a singular impact.
Shock wave generation in gaseous media nonreturn valves is similar and will be described below using as an example a mechanical gaseous media nonreturn valve shown on
When a gaseous media moves in a forward direction 5, membranes 4 are pressed against guards 3 and control ports 2 of plate 1 are open. If a pressure gradient at a nonreturn valve changes, a gaseous media moves in an opposite direction 6, membranes 4 are moved by an opposite gaseous media flow from guards 3 to plate 1, covering control ports 2 in plate 1.
When membranes 4 reach plate 1 and cover control ports 2 in plate 1, the gas flow stops fast and almost instantly, generating a shock wave. With that, a sharp pressure increase occurs on one side of plate 1, while a sharp pressure decrease occurs on the other side of plate 1. Plate 1 sustains an impact similar to a shock by a hard object, and a shock wave spreads in a gaseous environment, generating a noise of high intensity.
A shock wave in pulse combustion apparatuses mostly impacts plate 1 of a nonreturn valve, similar to a shock by a hard object. As plate 1 has an intrinsic resonant frequency, plate 1 starts vibrating with this intrinsic frequency. When a shock wave of a next cycle impacts plate 1, plate 1 still continues to vibrate due to a previous shock wave impact, so the next shock wave increases the amplitude of plate 1 vibration. Plate 1 vibration amplitude increases until the energy added by shock waves equilibrates with energy loss of plate 1 vibration during the time between shock waves impacts. Vibration energy loss of plate 1 occurs due to plastic straining of plate 1, energy transformation to acoustic vibration of gas surrounding a valve and vibration transfer to all elements of a pulse combustion apparatus. Plate 1 of a valve is usually made of resilient material, thus losses due to plastic straining are small and nearly all the energy of a shock wave impact on valve plate 1 transforms to acoustic noise and vibration.
Vibrations of gaseous media nonreturn valve have a high intensity and spreading along the whole pulse combustion apparatus generate a high level of acoustic noise and vibration at the place of a pulse combustion apparatus installation and in connected heat-exchange agent, exhaust and air and fuel supply systems. The use of guarding and isolation of gaseous media nonreturn valves allows a significant decrease of acoustic noise and vibration generated by pulse combustion apparatuses. A maximum result is achieved by vibration isolation of nonreturn valves from all elements of a pulse combustion apparatus. In some cases, vibration isolation of gaseous media nonreturn valves from a device for removing heat will be enough, as it has a large radiation area, many connected elements, and a direct contact with a heat-exchange agent.
Pulse combustion apparatuses may have various forms of embodiment that differ by the mode of a combustion mixture formation and the type of nonreturn valves used.
Several nonreturn valves may be installed in parallel for one gaseous media, as shown in
Nonreturn valves of one gaseous media installed in parallel may be placed in one guard chamber, or each nonreturn valve may be placed in an individual guard chamber.
Besides mechanical gaseous media nonreturn valves, aerodynamic gaseous media nonreturn valves may be used.
Vibration isolators should meet the requirements for airtightness, durability, and heat-resistance. In order to increase a vibration isolator heat-resistance and protect it from back surges of hot combustion products, a vibration isolator is protected by a maze. A maze is a series of concentrical cylindrical screens located with gaps and forming a long and narrow gaseous media canal between a vibration isolator and the main flow of a gaseous media.
In a preferrable form of embodiment of the current invention, a vibration isolator is executed as a cylinder-shaped corrugated element, a bellows made of rubber with wall thickness of 2 to 5 mm.
The shock wave in pulsation combustion apparatuses is generated at all gaseous media reverse mechanical valves. The shock wave intensity depends on flow characteristics of nonreturn valves.
To decrease the intensity of a shock generated by a gas flow, changes, if possible, are introduced to a design of a node generating shock in a gaseous media. For example, the intensity of a shock will be decreased if membranes of gaseous media nonreturn valve will be spring-loaded in the closing direction, leading to a decrease of reverse flow velocity at the time of a nonreturn valve closing.
Acoustic noise generated by operating pulsations of gas flow, a shock wave and vibration of gaseous media nonreturn valve walls in a closed space are reflected multiple times from the internal surface of a guard chamber walls, thus, the noise transfers almost all the energy to guard chamber walls vibration. These vibrations spread as vibrations and acoustic noise of the external surface of a guard chamber walls. For effective reverberation absorption, the internal walls of a guard chamber may be lined by a sound absorbing material.
The use of rigid structures of cavities and channels allows to decrease the level of noise generated by a shock wave impact on cavities and channels walls. For example, cylindrical and spherical walls generate less noise at a shock wave impact as compared to flat walls with the same thickness.
According to the current invention, acoustic low pass filters may be used to decrease the effect of a shock wave. The properties of low pass filters are similar to the properties of low pass filters in electrical engineering, which are well known and studied.
Acoustic low pass filter effects the gas flow variability depending on a frequency. Acoustic low pass filter has a cut-off frequency. A filter does not affect oscillations with a frequency below a cut-off value and decrease the amplitude of oscillations of gas flow with a frequency above the cut-off value.
To decrease the effect of a shock wave at a gaseous media mechanical nonreturn valve inlet and outlet, shock wave dampers may be installed sequentially.
The walls of shock wave dampers and the walls of a guard chamber of a gaseous media nonreturn valve may partially reflect a shock wave and partially transform the shock wave energy to vibrations, for example, if these walls are made of metal. The said walls may also partially reflect a shock wave and partially absorb the energy transforming it to heat, for example, is these walls are made of concrete. If the said walls are made of metal and are lined with a sound absorbing material with thermal isolation properties, the said walls also partially reflect a shock wave and partially transform a shock wave to vibrations, while partially absorbing a shock wave.
When a shock wave impacts the walls of shock wave dampers, a shock wave is partially reflected and partially transfers the energy to a wall, causing vibration of the walls of shock wave dampers with intrinsic resonant frequencies. Periodically, the next impacts of a shock wave increase the vibration amplitude of the walls of shock wave dampers to high values. Thus, the walls of a return valve and the walls of shock wave dampers installed on a nonreturn valve vibrate with high amplitudes and high vibration acceleration. In order to prevent the spread of these vibrations, according to the current invention, the air nonreturn valve 173 with shock wave dampers installed on it is connected to chamber 188 for a heat-exchange agent 189 using a vibration isolator 190, while the combustion gas nonreturn valve 191 placed in the guard chamber 192 is connected to the device for removing heat as chamber 188 for a heat-exchange agent 189 using the vibration isolator 193. With a high vibration isolation coefficient, the design of the nonreturn valve 173 with shock wave dampers installed may require additional measures for fixation in a required spatial position, such as installation of additional elastic elements 194 and 195 connecting the housing of the nonreturn valve 173 with the walls of the guard chamber 171 (
A shock wave damper may be executed as a screw-shaped channel for gas flow. In
In
In
At the air nonreturn valve 229 outlet, shock wave dampers 230 are installed, while at the air nonreturn valve 229 inlet, shock wave dampers 231 are installed. The air nonreturn valve 229 with dampers 230 and 231 installed on it, is connected via the vibration isolator 232 to the tube 233 washed by a heat-exchange agent 217 and fixed in place with elastic elements 234 and 235. The guard chamber 236 and tube 237 form the Helmholtz resonator 238. Sequentially with the Helmholtz resonator 238, Helmholtz resonator 239 comprising the chamber 240 and the tube 241 and Helmholtz resonator 242 comprising the chamber 243 and the tube 244 are installed. Inside the chamber 243, the chamber 236 and the purge fan 245 are located. The walls of chambers 236 and 243 are lined with a sound absorbing material 246 and 247 with heat isolation properties. Helmholtz resonators 236, 239 and 242 have an intrinsic resonant frequency below the pulse combustion frequency.
At the combustion gas nonreturn valve 248 inlet, shock wave dampers 249 are installed, while at the combustion gas nonreturn valve 248 outlet, shock wave dampers 250 are installed. The combustion gas nonreturn valve 248 with shock wave dampers 249 and 250 is located in the guard chamber 251, which together with tube 252 forms the Helmholtz resonator 253. Helmholtz resonator 253 is installed using the vibration isolator 254. Sequentially with the Helmholtz resonator 253, Helmholtz resonator 255 comprising the chamber 256 and the tube 257 is installed. Helmholtz resonator 253 is located inside the chamber 256 of the Helmholtz resonator 255. Helmholtz resonators 253 and 255 have an intrinsic resonant frequency below the pulse combustion frequency. The combustion gas supply regulator 258 is installed on the tube 257.
In a preferrable form of embodiment of a pulse combustion apparatus shown in
Filing Document | Filing Date | Country | Kind |
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PCT/RU2020/000030 | 1/27/2020 | WO |