WO1989011042A1 - Procede de production d'impulsions de pression dans une masse de gaz et dispositif de mise en oeuvre dudit procede - Google Patents

Procede de production d'impulsions de pression dans une masse de gaz et dispositif de mise en oeuvre dudit procede Download PDF

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Publication number
WO1989011042A1
WO1989011042A1 PCT/SE1988/000230 SE8800230W WO8911042A1 WO 1989011042 A1 WO1989011042 A1 WO 1989011042A1 SE 8800230 W SE8800230 W SE 8800230W WO 8911042 A1 WO8911042 A1 WO 8911042A1
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WO
WIPO (PCT)
Prior art keywords
pulses
machine
gas
pressure
mass
Prior art date
Application number
PCT/SE1988/000230
Other languages
English (en)
Inventor
Birger Pettersson
Stig Lundin
Original Assignee
Birger Pettersson
Stig Lundin
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Birger Pettersson, Stig Lundin filed Critical Birger Pettersson
Priority to PCT/SE1988/000230 priority Critical patent/WO1989011042A1/fr
Publication of WO1989011042A1 publication Critical patent/WO1989011042A1/fr

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Classifications

    • B—PERFORMING OPERATIONS; TRANSPORTING
    • B06—GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
    • B06B—METHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
    • B06B1/00—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
    • B06B1/20—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of a vibrating fluid
    • G—PHYSICS
    • G10—MUSICAL INSTRUMENTS; ACOUSTICS
    • G10K—SOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K15/00—Acoustics not otherwise provided for
    • G10K15/04—Sound-producing devices
    • G10K15/043—Sound-producing devices producing shock waves

Definitions

  • the present invention concerns a method for producing se ⁇ lectively controlled pressure pulses in a mass of gas, in particular contained in a space of large dimensions.
  • a mass of gas is here also included a mixture of gases e.g. air.
  • the invention also concerns a device for performing said method.
  • the energy of the pressure pulses can under certain condi ⁇ tions be used for different purposes such as preventing particles in the gas from settling on the walls of the space in which it is contained, as well as removing such particles already settled on said walls as a coating.
  • the pulses can also be used for promoting the mixing of two different gaseous media, for mixing a gas with fluid drop- lets or solid particles and for other aspects of homogeniz ⁇ ing a gas.
  • the utilization of pressure pulses thus can be applied for cleaning purposes and in different stages in e.g. the process industry for treating gases that are going to be mixed, be combustured, react chemically, perform work etc. as well as treating media in the form of solid par ⁇ ticles or fluid droplets suspended in a gas.
  • a condition for making such treatments of a mass of gas possible is that the pulses have a considerable acoustic power.
  • the pulses are of a frequency near the lower limit of audible sound. At these low frequencies the pulses are not damped out to the same extent as at higher frequencies. Furthermore the long wave length enables the pulses to propagate around obstructing partitions reaching all the parts of the space concerned at uniform level of acoustic pressure.
  • the pulse generator includes a pipe for pressurized gas provi ⁇ ded with a rotating cylindrical valve driven by an engine.
  • the pipe and the valve which are coaxially arranged, are each provided with a slot. As the slot of the valve during the rotation passes the slot of the pipe, communication is established between the pipe and the surrounding, whereby gas flows out through the aligned slots, generating a pulse.
  • the pulses are then amplified in a resonance tube.
  • the frequency is about 20 Hz.
  • This device a wave of substantially sinusodial shape is received, which results in an unfavourable distribution of energy during the pulse period.
  • the compressor required for the production of pressurized gas thus has to work all the time against the pressure in the gas pipe. This therefore requires a relatively high effective power input for the compression work in relation to the received acoustic power. A great part of this work is lost as heat.
  • pulses are generated when compressing the gas. Due to the valve, these pulses do not leave the pipe, so that their energy is not made use of. Also this energy is lost as heat.
  • the low acoustic efficiency of this method econo ⁇ mically and practically limits the achievable output power.
  • the sound pulses are generated by the flow of gas through an opening between two spaces of different pressure periodically brought in communication with each other.
  • the opening is controlled by a reciprocating slide connected to a membrane at the closed end of a resonance tube.
  • a soft low fre ⁇ quency sound is generated, affecting the membrane to 5 oscillate at a frequency determined by the resonance tube.
  • This sound gene ⁇ rator suffers from the same described drawbacks as the de- 10 vice of the Swedish patent document 80 07 150-9 does.
  • An ⁇ rV " -' advantage is received by the positive feed-back through the membrane securing harmony between the resonance frequency of the tube and the pulse frequency.
  • An object of the present invention is to attain a method for producing pressure pulses in a mass of gas, having a higher total acoustic power than can be reached by known methods.
  • a method of the kind introductionally specified involves that the pulses are generated by a valveless displacement machine, in which the pressure when the machine opens to- 35 wards its outlet port, differs from the pressure of the mass of gas.
  • Another object of the invention is to attain a device ca ⁇ pable to produce pressure pulses of higher total acoustic power than can be reached by known pressure pulse genera ⁇ tors.
  • a device of the kind introductionally specified contains a valveless displacement machine generating the pulses and so constructed that the pressure in the machine, when it opens towards its outlet port, differs from the pressure of the mass of gas.
  • the machine works as a compressor and said pressure in the machine exceeds the pressure of the mass of gas. This re ⁇ sults in an advantageous power relation between the re ⁇ ceived acoustic power and the power consumption of the machine.
  • the method according to the invention makes use of the pressure difference between two spaces periodically brought in communication with each other, for the pulse generation.
  • the pulses of the known methods are sinusodial, but through the pulse generation according to the invention a very rapid flow through the communicating opening lasting only during a short initial stage of the pulse period is achieved. During the rest of the pulse period the flow through the opening is relatively slow.
  • the strong concentration of the flow contributes in reaching a high acoustic power as the acoustic power in a wave is pro ⁇ portional to the integral of the square of the deviation in velocity from the mean velocity of the gas.
  • Another aspect of vital importance for the pulse generating method according to the invention is the fact that the pul ⁇ ses are generated directly by the means creating the pres ⁇ sure difference between the two spaces periodically strenght in communication with each other. Due to this circumstance the energy consumption of the machine used according to the invention, when working as a compressor, is limited to the energy necessary for the compression work up to the moment of opening of the machine towards the outlet. The gas flown through the outlet in this moment rapidly equalizes the pressure difference between the working chamber of the compressor and the outlet. Since the pressure in the outlet channel normally is atmospheric no more work is required for displacing the rest of the gas in the working chamber. As no pressurized gas is produced, except the gas which for a short period is compressed in a working chamber and whose energy immediately is converted into acoustic energy, a considerable increase in the acoustic efficiency is at ⁇ tained.
  • the pulse generation according to the invention is based on a principle making possible a high power of the pulses. By the distinctive features of the invention this is carried through at a high efficiency and with accentuated energy variations during the pulse period. Thereby pulses can be produced having an acoustic power considerably higher than what up to now has been achieved. This makes possible the application of pressure pulse treatment of a mass of gas for the in the introduction mentioned purposes to an extent that have not been practically possible with known techni ⁇ ques.
  • Figure 1 shows a pulse producing device used for cleaning a steam boiler.
  • Figure 2 shows an end view of the compressor in figure 3, omitting details not essential to the invention.
  • Figure 3 shows a schematic view of a pulse generator working as a compressor.
  • Figure 4 diagrammatically shows the air velocity through the outlet port of the compressor during the discharge.
  • Figure 5 shows an embodiment in which the pulses are distributed to two separate masses of gas.
  • Figure 1 shows a steam boiler 27, having inner surfaces on which a coating of soot and the like settles.
  • a device in ⁇ cluding a pulse generator 2 according to the invention is connected to the steam boiler 27 through an air pipe 4.
  • the pressure is some millibar below atmospheric pressure.
  • the pulse generator 2 is a screw compressor having meshing male 13 and female 14 rotors. As this kind of compressors is well known only a brief description of its working principle should be sufficient.
  • the male rotor 13 has two helical lobes 15, mainly located outside the pitch circle of the rotor and having convex geometry. Bet ⁇ ween the lobes 15 two likewise helical grooves are formed.
  • the female rotor 14 has in the corresponding manner three helical lobes 16 with intermediate grooves. The lobes 16 of the female rotor 14 are mainly located inside the pitch circle of the rotor and have flanks of concave geometry.
  • the lobes 15, 16 and the grooves of the rotors 13, 14 co ⁇ operate gearingly, forming chevron-shaped working chambers between the rotors 13, 14 and the surrounding barrel 25.
  • the barrel 25 has the shape of two intersecting circular cylinders, each housing one of the rotors 13, 14. At rotation the working chambers travel axially from one end of the machine 2, having an inlet, to the other end, having an outlet.
  • Each chamber is during a filling stage in communication on ⁇ ly with the inlet, when air is sucked into the chamber, during a compression stage closed off from both the inlet and the outlet, when air is transported towards the outlet while being compressed and during a discharge stage in com ⁇ munication only with the outlet when air leaves the cham ⁇ ber.
  • the compressor 2 is made to work with overcompression, i.e. it compresses the air in a working chamber to a pres ⁇ sure level exceeding the pressure in the outlet channel 4.
  • the overpressure is moderate, about 0.3 to 1 bars.
  • the rapid outflow results from the pressure difference and occurs on ⁇ ly during a short period at the beginning of the discharge of a chamber, whereby a very powerful pressure pulse is ge ⁇ nerated.
  • the momentary content of energy in a wave movement is pro ⁇ portional to the square of the deviation of the momentary velocity from the mean velocity.
  • the concentration of the acoustic energy to a short pulse during the wave period thus is still more accentuated than the course of the velo- city. This results in a considerably higher power outcome than normally can be reached with a pure sinusodial wave shape.
  • the pulse fre ⁇ quency is 20 Hz.
  • the t-coordinate T thus represents 0.05 seconds.
  • the compressor works with an overpressure of 0.32 bars at the moment of the opening of the chamber towards the outlet.
  • the outlet port 23 is radially as well as axially direct ⁇ ed.
  • the radially directed part of the port 23 is defined by three edge sections 24 a, b, c.
  • a first edge section 24 a extends obliquely outwards over the barrel half housing the male rotor 13 from a point on the barrel 25 where the two barrel halves intersect and reaches the high pressure end wall 26.
  • a second edge section 24 b likewise extends ob ⁇ liquely outwards over the barrel half housing the female rotor 14 from a point on the barrel 25 where the two barrel halves intersect but located more closed to the inlet end than said first point and reaches the high pressure end wall 26.
  • a third edge section 24 c colinear with the bar ⁇ rel intersection line, connects said two points.
  • the axially directed part of the port 23 is defined by three edge sections 24 d, e, f.
  • a first edge section 24 d extends curvilinearely inwards from a point on the outer edge of the end wall 26 where the first edge section 24 a of the radially directed part of the port 23 ends, and reaches radially the carrying body 17 of the male rotor 13.
  • a second edge section 24 e extends curvilinearely in ⁇ wards from a point on the outer edge of the end wall 26 where the second edge section 24 b of the radially directed part of the port 23 ends, and reaches radially the carrying body 18 of the female rotor 14.
  • a third edge section 24 f connects the inner ends of said first 24 d and second 24 e edge sections.
  • the lobes 15, 16 of the rotors are shaped with a sharp edge 19, 20 at the periphery so as to open momentary.
  • the edge sections 24 a, b, d, e of the outlet port are shaped to be parallel to the corresponding edges 19,
  • a lobe combination of few lobes has been chosen. This allows a large air volume in each working chamber and also results in that the total length of the edge sections 24 a, b, d, e of the outlet port 23 cooperating with the lobes can be made great.
  • a great edge length leads to an advantageous opening performance since maximal flow at the moment of opening is strived at in order to concentrate the pulse.
  • the rotors 13, 14 have unequal number of lobes 15, 16 so that both of them open simultaneously towards the outlet.
  • the rpm of the compressor 2 is chosen so that the pulse frequency is in the range between 10 and 50 Hz with a preferred value of about 20 Hz.
  • the pulses so generated can reach an acoustic power of up to 20 kW.
  • the pressure pulses propagate through a pipe system, comp- rising the channel 4 and the resonator 3, into the steam boiler 27 (figure 1).
  • the reasonator 3, located between the compressor 2 and the steam boiler 27 amplifies the funda ⁇ mental tone of the pulses generated by the compressor 2.
  • the length of the resonator 3 is matched to give the mass of air in the system a resonance frequency harmonizing the frequency of the pulses i.e. 20 Hz.
  • steering is effectuated by affecting the resonance frequency of the resonator 3.
  • the resonator 3 is provided with an end wall 7, displaceable from a reference position.
  • the resonator 3 is dimensioned to give the air in the system a resonance fre ⁇ quency roughly corresponding to the pulse frequency i.e. 20 Hz at a certain temperature and with the end wall 7 in its reference position.
  • the end wall 7 is adjusted to a position where precise resonance occurs. In this man ⁇ ner compensation can be made for deviations in the tempera ⁇ ture of the incoming air and for other parameters possibly affecting the resonance frequency of the system.
  • the dis ⁇ placeable end wall 7 also offers a possiblity to run the compressor 2 at another rpm as the position of the end wall 7 can be matched to the changed pulse frequency.
  • the position of the end wall 7 can be governed by measuring the intensity of the pulses with sensor means 8 e.g. at a point inside the steam boiler 27, and then displacing the end wall 7 to the position where maximal intensity is measured. This can preferably be automated by the use of a micro-processor 9. With the displaceable end wall 7 it is also possible to steer the pulse intensity in the steam boiler 27 to a level deviating from the maximal, which is a need that in certain cases can be present.
  • Regulation of the amplification by a displaceable end wall in the resonator can be replaced or supplemented by measures for affecting the temperature of the air in the system.
  • a change of temperature will change the resonance frequency of the system.
  • Regulation of the temperature can be carried through in many ways: By a variable restriction in the inlet channel 12 of the comp- ressor 2, by providing the compressor 2 with a slide valve regulating the internal compression rate of the compressor or by returning air from the compressor outlet channel 4 or a closed working chamber to its inlet. Also the regulation of the temperature can be governed by signals from the sound intensity sensor 8.
  • the mass of gas 1 in the steam boiler 27 can itself be used as a resonator, whereby the pulse frequency is regula- ted to match the resonance frequency of the mass of gas 1. It is also possible to utilize the pulses without any kind of resonance amplification.
  • a return channel 11 for air from the outlet channel 4 to the inlet can be necessary also in order to avoid pumping of a great amount of relatively cold air into the steam boiler 27.
  • the pressure in the steam boiler 27 is some- what below atmospheric pressure, this might require a mo ⁇ derate throttling (about 1 millibar) of the inlet air at a point upstream to the inflow of the returned air.
  • the pulses are generated by a compressor in which the air in a working chamber has been compressed to a certain over ⁇ pressure before being discharged through the outlet port. This gives an advantageous operating economy considering the energy consumption.
  • the pulses are ge ⁇ nerated at an opposite direction of flow of the air through the outlet port.
  • a displacement machine which pumps the air without compressing it, e.g. a Root type blower or a screw compressor without internal compression.
  • This alternative embodiment demands a higher power consump ⁇ tion than the one earlier described. This power is to a large extent lost as heat. A less amount of air is pumped into the boiler and the air has a higher temperature.
  • a certain operation cycle was specified. This cycle can of course be varied in respect of the length of the work and rest periods. The operation cycle can also be such that the rpm of the machine alters 5 between two work periods, in order to attain a pulse fre ⁇ quency altering between two different values. Also when the machine is continuously working the pulse generator can operate with altering frequency.
  • the illustrated device is not restricted to clean only one single space of a steam boiler plant.
  • the pulses can be transmitted to two or more separate 0 spaces 1 ' , 1 ' ' . Cleaning of separate spaces thereby can be effected simultaneously or alternating, in the latter case by use of flow altering means provided in the branch.

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  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Multimedia (AREA)
  • Mechanical Engineering (AREA)
  • Structures Of Non-Positive Displacement Pumps (AREA)

Abstract

L'invention concerne un procédé de production sélective d'impulsions de pression commandées dans une masse de gaz (1), contenue notamment dans un espace (27) de grandes dimensions. Afin de produire des impulsions d'une puissance suffisamment élevée, on utilise une machine (2) à déplacement sans clapet, dans laquelle la pression lorsque ladite machine (2) ouvre son orifice de sortie, diffère de la pression de la masse de gaz. L'écoulement rapide du fluide de travail à travers l'orifice de sortie (23) dû à la différence de pression, a pour résultat de produire l'impulsion. Les impulsions produites peuvent atteindre au moyen du procédé une puissance acoustique allant jusqu'à 20 kW. L'invention concenre également un dispositif de mise en oeuvre dudit procédé.
PCT/SE1988/000230 1988-05-05 1988-05-05 Procede de production d'impulsions de pression dans une masse de gaz et dispositif de mise en oeuvre dudit procede WO1989011042A1 (fr)

Priority Applications (1)

Application Number Priority Date Filing Date Title
PCT/SE1988/000230 WO1989011042A1 (fr) 1988-05-05 1988-05-05 Procede de production d'impulsions de pression dans une masse de gaz et dispositif de mise en oeuvre dudit procede

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
PCT/SE1988/000230 WO1989011042A1 (fr) 1988-05-05 1988-05-05 Procede de production d'impulsions de pression dans une masse de gaz et dispositif de mise en oeuvre dudit procede

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WO1989011042A1 true WO1989011042A1 (fr) 1989-11-16

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PCT/SE1988/000230 WO1989011042A1 (fr) 1988-05-05 1988-05-05 Procede de production d'impulsions de pression dans une masse de gaz et dispositif de mise en oeuvre dudit procede

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2998054A1 (fr) * 2012-11-12 2014-05-16 Peugeot Citroen Automobiles Sa Generateur de pulsation de pression dans un flux de gaz

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0006833A2 (fr) * 1978-07-03 1980-01-09 Mats Olsson Konsult Ab Générateur de sons basse fréquence
SE425597B (sv) * 1980-10-13 1982-10-18 Ekstroms Vermetekniska Ab Tvangsstyrd ljudalstrare for infraljudomradet
SE445788B (sv) * 1979-06-11 1986-07-14 Kockumation Ab Sett och anordning vid en gasdriven trycksvengningsalstrare av membranventiltyp

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0006833A2 (fr) * 1978-07-03 1980-01-09 Mats Olsson Konsult Ab Générateur de sons basse fréquence
SE445788B (sv) * 1979-06-11 1986-07-14 Kockumation Ab Sett och anordning vid en gasdriven trycksvengningsalstrare av membranventiltyp
SE425597B (sv) * 1980-10-13 1982-10-18 Ekstroms Vermetekniska Ab Tvangsstyrd ljudalstrare for infraljudomradet

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2998054A1 (fr) * 2012-11-12 2014-05-16 Peugeot Citroen Automobiles Sa Generateur de pulsation de pression dans un flux de gaz

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