GB2409991A - Electrostatic air filter - Google Patents
Electrostatic air filter Download PDFInfo
- Publication number
- GB2409991A GB2409991A GB0329767A GB0329767A GB2409991A GB 2409991 A GB2409991 A GB 2409991A GB 0329767 A GB0329767 A GB 0329767A GB 0329767 A GB0329767 A GB 0329767A GB 2409991 A GB2409991 A GB 2409991A
- Authority
- GB
- United Kingdom
- Prior art keywords
- filter
- electrostatic
- air
- particles
- droplets
- Prior art date
- Legal status (The legal status 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 status listed.)
- Granted
Links
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B03—SEPARATION OF SOLID MATERIALS USING LIQUIDS OR USING PNEUMATIC TABLES OR JIGS; MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
- B03C—MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
- B03C3/00—Separating dispersed particles from gases or vapour, e.g. air, by electrostatic effect
- B03C3/02—Plant or installations having external electricity supply
- B03C3/16—Plant or installations having external electricity supply wet type
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B03—SEPARATION OF SOLID MATERIALS USING LIQUIDS OR USING PNEUMATIC TABLES OR JIGS; MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
- B03C—MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
- B03C3/00—Separating dispersed particles from gases or vapour, e.g. air, by electrostatic effect
- B03C3/02—Plant or installations having external electricity supply
- B03C3/04—Plant or installations having external electricity supply dry type
- B03C3/12—Plant or installations having external electricity supply dry type characterised by separation of ionising and collecting stations
Landscapes
- Electrostatic Separation (AREA)
Abstract
An electrostatic air filter for separating very small air borne contaminants including chemical particles, dust or biological organisms from the air or gas in which they are carried. The filter comprises a duct, chamber or pipe to import and transport the air or gas as well as to house an electrostatic filter mechanism. The filter provides a particle charging means 1, an optional means to introduce atomized liquids 12 and a capture means 3 of collecting very small particles and recovering any atomized liquids by the use of a maze of fine wire or filament conductors 20 held at a high voltage. The particle charging means comprises a fine wire 10 held at a high positive potential relative to plates 11. Dust is charged as it passes and combines with liquid droplets in the atomizer. In the capture means the droplets migrate to the fine wire where droplets and their captured particles drip into a collection chamber. Any remaining charged particles pass through an earthing stage 4 as a final filter and charge neutraliser. A fan 6 draws the air through the duct. The capture means may be rotated or may include a cyclonic arrangement. (Not shown).
Description
240999 1 Electrostatic Air Filter.
The present invention relates to the electrostatic removal of small particulates and organisms from the air. More particularly, the invention relates to a device and method for increasing the collection efficiency of very small particles when compared with conventional electrostatic filters.
Description of the related art.
Conventional Electrostatic devices pass air (or gas) through a chamber. The chamber is arranged to electrostaticly charge small particles suspended in an air stream passed in close proximity to a high voltage corona device The small particles become charged due to the resultant electric field of the corona. The air and charged particles are then passed axially between conductive surfaces that are charged to a high voltage. The charged particles experience a force that is the product of the particles charge and the electric field strength between the plates. The charged particles migrate towards plates of opposite polarity due to the impressed electrostatic forces between the plates and the particles.
As particle sizes decrease, the drag forces predominate the inertial mass forces. As a practical consequence, the maximum velocity that can be achieved by small particles normal to the inlet/outlet air stream reduces sharply with reducing particle sizes below 0.2 microns. If it isrequired to obtain a high collection quotient of these smaller particles in conventional plate type precipitators, then the volume of air that passes through the chamber in a given unit of time will have to be de-rated or, alternatively, the size of the collection plates (and hence volume of the chamber) increased.
Description of the invention
According to the present invention there are provided separate means to enable higher collection efficiencies of very small particles for given precipitator chamber volumes and input airflow volume rates when compared to conventional means. In the context of the invention, small particles means a body or material down to the nanometer scale Accordingly, organisms such as the S.A.R.S. virus (arround 60 nano meters) could be removed from the air. The ability to filter air or gas at the nanometer level opens up the possibility of improving nuclear, chemical and biological protection systems as well as a means of capturing air borne pollutants for sample analysis.
The present invention employs the use of a spun conductive filament, or fine wire held at high voltage that takes a similar place to a high voltage plate collector in a conventional electrostatic precipitator, excepting that the air (or gas) to be cleaned is passed through the mesh of the conductive filament instead of parallel to the material, as in the case of conventional electrostatic precipitator. The effect of this arrangement is to increase the available collection surface area/plate volume ratio and reduce the mean distance between charged particles and the collection surfaces for a given volume of chamber.
Additionally, as the air passes around the filaments, the airflow will become turbulent, forming multiple eddies. The direction of travel of the particles within the eddies will become chaotic and transiently deviate the path of the particles across the direction of the average movement of the air through the chamber. In consequence of this substantially nonlaminar airflow, the charged particles will, for at least pal l of their journey through the filament collector, experience a velocity vector reinforcing the attraction force vector towards the collector.
A further enhancement may be made to the particle collection efficacy by introducing atomized droplets after the corona stage and before the collector filaments.The small droplets produced by the atomiser may be charged positively, negatively or at zero potential depending on the polarity of the corona and collector. Mixing of the charged particles arid ink atoinizecl droplets may be enhanced by Ike action of a slenh.ri c.hnnher Since the charged particles are brought into very close proximity with the atomised droplets, the electrostatic attraction between particles and droplets will be high causing small particles to collide with the relatively massive droplets. Once collision occurs, the particle will be held to the droplet under the forces of surface tension.
If the collector filaments are packed tightly, they will substantially obstruct the combined particles and atomized droplets. When the droplets impact on the filament, they will cling to it under the forces generated by surface tension, similarly, other small droplets will collide and, in turn, merge with the clinging droplets to form bigger droplets. As the bigger droplets form, a point will be reached where the gravitational forces will exceed the surface tension forces that make the droplets cling to the filaments. Furthermore, as droplets and their trapped particles merge to form larger composites, gravitational forces will dominate the surface tension forces allowing the composite droplets to fall to a collection receptacle without being swept further into the chamber by the air flowing through the chamber. It is obvious that a centrifuge or a cyclone system could be used to provide centripetal forces many times greater than the force due to Earths gravity to enhance this mechanism.
The voltage applied to the conductive filament may be arranged such that there is a large potential difference between the filament and atomized droplets purposefully introduced after the Corotron or corona stage. If the atomized droplets are of negative charge with respect to the positively charged particles (or vice versa) that have passed through the corona stage, then there will be a mutual attraction between the particles and the droplets as described above.
When the particles and droplets impact on each other, the relatively massive droplets trap the smaller particles and their charges are shared. Because the filaments are electrically arranged to be at a high voltage of differing potential of the droplets, a strong electrical field will exist between filament and the composite droplets. When the droplets and composite droplets come into close proximity of the charged filament, they will experience an electrostatic force towards the filmnent and can be accelerated to a much larger terminal velocity towards the filament before equilibrium between electrostatic and drag forces is reached when compared the terminal velocities that can be achieved by the much smaller particles alone.
It should be appreciated, that the electrostatic field within the filament maize will be at equipotential between the filaments. There will be a local distortion in the field only when a suspended charged particle or particles are present. The collection electrode is therefore insensitive to direct short circuits due to long fibers bridging the collection electrode.
The use of aerosols may also be integrated into conventional flat plate collectors where provision is made for the aerosols and smaller particles to mix thoroughly prior to the charged collector plates. The combined droplets and smaller particles may be collected from the surfaces of the flat plates. If the collector plates are mounted vertically, this orientation will assist the collected droplets and particles to run-off allowing them to be caught in a recovery vessel.
The drawings and descriptions are provided for descriptive clarity and simplicity. It is obvious that there are many other configurations including the incorporation into portable and personal air filters and facemasks as well as air conditioning filters and post filters for vacuum cleaners.
Description of the drawings.
l he following drawings illustrate the mechanisms employed in the invention. A series of schematic figures are provided for convenience. Each schematic figure is a construction of a number of modules; each module represents a cross-sectional side elevation of a functional part constructed within a box section for the purposes of simplification and identification of each module. The figures show each module slightly separated. In practice, all modules butt up to adjoining modules with no gaps between the modules so as to form a continuous chamber.
Figure 1 shows a cross-sectional schematic representation of the filter. The filter comprises a corona charging stage 1, an option for an atomizing stage 2, a filament collector stage 3, an earthed stage 4 and a fan 6 to draw air through the duct. The functionality of the filter is such that; when the air is passed through the charging stage, particles drawn in with the air become charged due to the corona induced movement of ionized gas molecules and the high electric field. The corona is formed around a fine wire and in this case, is shown to be at a high positive potential with respect to the electrodes 11 which are shown earthed. The air and positively charged particles continue to be drawn along the duct where they meet the atomizing stage. The stage may have a shaped throat 12 to provide a Venturi effect and to assist the formation and mixing of atomized droplets. The atomizer consists of a piezo vibrating plate 23 in contact with the desired liquid 15 held at some voltage, which, in this case is held at earth potential. The piezo plate is powered by an oscillating voltage generator 24. The voltage generator may be tuned from several tens of kilohertz to several megahertz depending on the required size of atomised droplets and the resonance of the piezo. Droplets 13, of size ranging in the order of between one to twenty microns can readily be formed depending on the chosen oscillation frequency and the surface tension ofthe liquid employed. The desired liquid 15 could be water, oil or contain chemicals chosen to react with specific chemical or biological particles that need to be neutralized and removed from the air. The liquid may, for example, contain finely ground carbon to absorb volatile aromatic hydrocarbons, or, alternativley, agents to destroy viruses or bacteria. As the droplets and the particles pass into close proximity with each other, many charged particles will merge with the atomized droplets as they impact due to mutual electrostatic attraction. As the remaining droplets and particles are drawn into the maize of filament 20 which is held at high negative voltage, there will be further and more effective mixing of the particles and droplets in the chaotic or turbulent airflow between the filament strands. As the droplets and particles are brought into very close proximity with each other, the mutual electrostatic attraction forces increase proportionally to the inverse square of the distances between tile droplets and particles. Additionally, electrostatic forces between the high voltage filament, particles, droplets and combined or merged droplet particles cause their migration to the filament. The larger droplets migrate the fastest due to their higher terminal drag equilibrium velocity. The smaller remaining particles migrate more slowly due to their lower terminal velocities, which are restricted by higher drag coefficients. The air streaming around the filament carries the droplets into very close proximity to the filament. Because of this close proximity, the resultant electrostatic forces on the particles are high, therefore, the resultant time that is required for even small particles to migrate to the filament is small in comparison to the migration time of small particles migrating across a laminar airflow in a comparatively widely spaced conventional flat plate electrostatic precipitator. Droplets and their captured particles Dip into the collection chamber from which the contaminated liquid can be extracted via the outlet 19. Any charged particles that manage to escape the collection chamber are then passed through the earthed filaments in the earthing stage 4 as a final filter and charge neutralizer.
The above description describes a positive charging device or Corona, an earthed liquid to be atomized and a negatively charged collector filament. Since the resultant electrostatic fields are proportional to the potential differences, It is obvious that the given polarities can be reversed or biased to achieve the substantially the same effect.
The following figures illustrate some variations achievable within the embodiment of the invention and are not intended to be restrictive. The principle functioning parts retain the same number references as in figure I unless otherwise stated.
Fig 2 shows a physical configuration that differs from Figl in that the collection chamber is aligned horizontally on the same axis of the charging and mixing stage. Droplets and their captured particles drip into the collection chamber 9, from which the contaminated liquid can be extracted via the outlet 19. It should be obvious that the orientation of each stage may be positioned to allow the maximum flexibility in the manufacturing design process.
Fig 3 shows a simple configuration whereby a motor assembly 17 rotates the inner chamber of the collection stage 5 and its contents. As the filament chamber rotates, the contaminated liquid comprised of the droplets and particles is thrown through the perforated filament support chamber onto the walls of the stationary outer collection cylinder jacket. The contaminated liquid is removed via the drain port 19.
It is obvious that there are many other electro mechanical configurations that could be used to rotate the collection stage.
Fig 4 shows a configuration whereby the collection chamber 8 incorporates a cyclone 25.
The contaminated liquid comprised of the droplets and particles is thrown onto the conductive filament 20 which is held at a high voltage and also onto the inside of the outer wall of the cyclone chamber. The contaminated liquid is removed from the bottom of the cyclone chamber via a drain port.
A conductive maze of filament or fine wire held at a high voltage 20 can be provided to enable higher collection efficiencies of very small particles for given precipitator chamber volumes and input airflow volume rates when compared to conventional means.
As described above in the invention summary, This mechanism may be employed without the inclusion of charged aerosols or an atomizing stage as shown in Fig S. The fine wire filament maze can be manufactured inexpensively and can be a disposable item.
Claims (1)
1/ An electrostatic air filter for separating very small air borne particles or organisms from the air in which they are carried. The filter comprises a duct, chamber or pipe to contain and transport the air or gas and to house the filter mechanism. The filter provides a particle charging means, a means to introduce charged or uncharged atomized liquids of a controlled size and a capture means of collecting the atomized droplets and very small air borne particles or organisms by the use of a maze of fine wire or filament conductors held at a high voltage.
2/ An electrostatic air filter as claimed in claim 1 incorporating a venturi and atomizer electrically arranged to introduce grounded or charged aerosols into a mixing stage after the corona charging stage and before the maze of fine wire or filament conductors held a a high voltage that comprise the collector stage. The atomized liquid may be chosen to react or include additives to react chemically or biologically with the small particles or organisms that need to be removed from the air.
3/An electrostatic filter as in claim 1 without an atomizer stage but including a disposable conductive filament or fine wire maze held at a high voltage to provides an electrostatic means to collect and trap the charged small air borne particles or organisms alone.
4/ An electrostatic air filter as in any preceding claim incorporating a plurality of collector stages or chambers.
5/ An electrostatic air filter as in any preceding claim whereby each collection stage may be held at different voltages and polarity.
6/ An electrostatic air filter as in any preceding claim incorporating a charge neutralizer chamber comprised of a maze of fine wire or filament conductors held at ground or earth potential.
?/ An electrostatic air filter as in any preceding claim whereby the filament collection stage or stages can be rotated the impress centripetal forces on the contents of the chamber in order to separate the contents of the collection chamber.
8/ An electrostatic air filter as in claim 6 whereby the filament collection stage or stages incorporate a cyclone separator.
9/ An electrostatic air filter as in claim 2 excepting that the filament collection stage is replaced by a conventional high voltage flat plate collector mounted in a vertical orientation to allow the attracted particles and droplets to run-off into a containment vessel.
10/ An electrostatic filter as in any preceding claim whereby the electrostatic filter is employed in line with a pressurised air or gas duct or conduit allowing the optional removal of the electrostatic filters integral fan.
11/ An electrostatic filter as in any preceding claim whereby the electrostatic filter is employed in line with a motor vehicles exhaust system.
12/ An electrostatic filter as in any preceding claim whereby the electrostatic filter is employed as a post filter in line with the exhaust airflow of a domestic or commercial vacuum cleaner.
13/ An electrostatic filter as in claim 9 whereby the electrostatic filter is employed as a post filter in line with the exhaust airflow of a cyclone separator or filter.
14/ An electrostatic filter as in claim 9 whereby the electrostatic filter is employed as a filter or post filter in air conditioning systems.
15/ An electrostatic filter as in claim 9 whereby the electrostatic filter is employed as a portable filter or sub assembly of a facemask for personal protection.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB0329767A GB2409991B (en) | 2003-12-23 | 2003-12-23 | Electrostatic air filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB0329767A GB2409991B (en) | 2003-12-23 | 2003-12-23 | Electrostatic air filter |
Publications (3)
Publication Number | Publication Date |
---|---|
GB0329767D0 GB0329767D0 (en) | 2004-01-28 |
GB2409991A true GB2409991A (en) | 2005-07-20 |
GB2409991B GB2409991B (en) | 2007-06-13 |
Family
ID=30776325
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB0329767A Expired - Fee Related GB2409991B (en) | 2003-12-23 | 2003-12-23 | Electrostatic air filter |
Country Status (1)
Country | Link |
---|---|
GB (1) | GB2409991B (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2007010173A1 (en) * | 2005-07-18 | 2007-01-25 | Colin Lawrence Amess | Electrostatic air filter |
WO2007103793A2 (en) * | 2006-03-03 | 2007-09-13 | Traceguard Technologies Inc. | Filtering optimization methods for particle inspection device |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN113786935B (en) * | 2021-08-11 | 2022-06-17 | 中国矿业大学 | System for trapping and screening large amount of nanoscale particles and generating nanoscale particles |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB901439A (en) * | 1959-04-01 | 1962-07-18 | Trion A G | Improvements in or relating to electrostatic filters |
GB1176732A (en) * | 1966-03-23 | 1970-01-07 | Messen Jaschin G A | Improvements in or relating to Electrostatic Dust Precipitators. |
GB1321735A (en) * | 1970-05-20 | 1973-06-27 | Aeromix Ets | Purification of gases or vapours |
US4871515A (en) * | 1987-07-16 | 1989-10-03 | Man Technologie Gmbh | Electrostatic filter |
-
2003
- 2003-12-23 GB GB0329767A patent/GB2409991B/en not_active Expired - Fee Related
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB901439A (en) * | 1959-04-01 | 1962-07-18 | Trion A G | Improvements in or relating to electrostatic filters |
GB1176732A (en) * | 1966-03-23 | 1970-01-07 | Messen Jaschin G A | Improvements in or relating to Electrostatic Dust Precipitators. |
GB1321735A (en) * | 1970-05-20 | 1973-06-27 | Aeromix Ets | Purification of gases or vapours |
US4871515A (en) * | 1987-07-16 | 1989-10-03 | Man Technologie Gmbh | Electrostatic filter |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2007010173A1 (en) * | 2005-07-18 | 2007-01-25 | Colin Lawrence Amess | Electrostatic air filter |
WO2007103793A2 (en) * | 2006-03-03 | 2007-09-13 | Traceguard Technologies Inc. | Filtering optimization methods for particle inspection device |
WO2007103793A3 (en) * | 2006-03-03 | 2008-03-06 | Traceguard Technologies Inc | Filtering optimization methods for particle inspection device |
Also Published As
Publication number | Publication date |
---|---|
GB0329767D0 (en) | 2004-01-28 |
GB2409991B (en) | 2007-06-13 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US20100011960A1 (en) | Electrostatic Air Filter | |
US6926758B2 (en) | Electrostatic filter | |
JP3362030B2 (en) | Dust collection device and method using ultrafine particles | |
KR100710697B1 (en) | Method and process for separating materials in the form of particles and/or drops from a gas flow | |
CN101124046B (en) | Rigid electrode ionization for packed bed scrubbers | |
US3958958A (en) | Method for electrostatic removal of particulate from a gas stream | |
JP2002536168A (en) | Charged droplet gas scrubber apparatus and method | |
US8608838B2 (en) | Tubing air purification system | |
JP2005507766A (en) | Dynamic electrostatic filter device for air cleaning using electrically charged droplets | |
EP1439911A1 (en) | Fluid utilized in apparatus for purifying air | |
GB2409991A (en) | Electrostatic air filter | |
Rezaei et al. | Airborne Nanoparticles: Control and Detection | |
KR100561550B1 (en) | method and apparatus for collecting a dust and cleaning air by electrostatic spray | |
WO2012139642A1 (en) | Apparatus for removal of particulate matter from a gas | |
JP2002195618A (en) | Kitchen exhaust system | |
Alonso et al. | Electrostatic precipitation of ultrafine particles enhanced by simultaneous diffusional deposition on wire screens | |
WO2020078573A1 (en) | Particle collector | |
Singh et al. | Scavenging of Submicron Aerosol Particles by Cloud of Charged Droplets Generated from Electro-Hydrodynamic Atomizer (EHDA) | |
KR102211713B1 (en) | Complex type electric dust collecting apparatus | |
Drehmel | Advanced electrostatic collection concepts | |
Bologa et al. | Novel wet electrostatic precipitator for sub-micron particles | |
JP2009045594A (en) | Kitchen ventilator | |
US2962115A (en) | Apparatus for separating solid and liquid particles for gases and vapours | |
AU2002218064B2 (en) | Electrostatic filter | |
RU2159683C1 (en) | Device for air cleaning of dust and aerosols |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PCNP | Patent ceased through non-payment of renewal fee |
Effective date: 20181223 |