TECHNICAL FIELD
[0001] The invention relates to an electrostatic separator, in particular for separating
particles in a gas flow which is passed through the separator in a predetermined direction,
comprising a plurality of rows of collecting electrodes arranged in a housing.
BACKGROUND
[0002] In electrostatic precipitators, the particles contained in the gas flow are charged
by an electric field of high field strength generated by means of wire electrodes,
so that they can be attracted and held by plate-shaped collector electrodes, which
are polarized opposite to the wire electrodes enabling discharge as is known, e.g.
from
US 1 791 338,
DE 2 843 211and
US 3 740 925.
[0003] A plurality of plate-shaped collecting electrodes are arranged parallel to each other
in a housing, directing the gas flow through the housing. The ribs extend parallel
to the wire electrodes, which are also arranged at intervals along the flow channel
between the plate-shaped collecting electrodes. The high voltage applied between the
wire electrodes and the collector electrodes creates an electric field which has a
relatively low but nevertheless considerable field strength in the area immediately
adjacent to the plate-shaped collector electrodes adjacent. Spark-overs between a
wire electrode and a collector electrode set the upper limit for the voltage that
can be applied between these electrodes.
[0004] Each charged particle experiences an electrostatic attraction force to the nearest
collecting electrode of a magnitude proportional to the charge on the particle and
the electric field strength. However, in the central flow region between adjacent
collection electrodes, where the velocity is relatively high, the electrostatic force
is small compared to the aerodynamic forces that entrain the particles with the gas
flow. Therefore, the electrostatic attractive force has little influence on the particle
position before the particle is brought to a region of reduced flow velocity in the
vicinity of the collecting electrode. In this region, the migration speed caused by
the electric field prevails, so that the particle is captured by the collecting electrode
and held in an accumulating layer by residual attractive forces.
[0005] It is known to provide flow areas with reduced gas flow, by means of ribs on the
collecting electrodes, intended to enable increased collection of particles. However,
the ribs also disadvantageously impede the main flow between the electrodes and reduce
the limit value of the separator's flashover voltage. The breakdown voltage limit
determines the practical upper operating limit for the electrode voltage and hence
the limit of the electric field strength in the space between the electrodes.
[0006] A high electric field strength favours a high charging of the particles. This is
desirable because the electrical attractive force exerted on the particles is proportional
to the charge on the particles. It is also desirable to have as high a field strength
as possible near the collection electrodes where the electrostatic forces cause capture,
because these forces are proportional to the field strength. It is also advantageous
that the field strength be as uniform as possible in these areas. Deviations from
the uniformity of the electric field strength along the surface of the collecting
electrodes are disadvantageous, since sharp deviations/peak values may cause arcing
and therefore a need to reduce the field strength along a collection electrode to
handle such peak values, thereby reducing the overall capture efficiency of the system.
[0007] From
DE 2 843 211it is known to use wave shaped collector plates and from "A Manual of Electrostatic
Precipitator Technology", Southern Research Institute, Birmingham, Alabama, USA, 1970,
pages 231 and 232 it is known to use collector electrodes which have a zigzag, staggered
or ribbed configuration. Such abrupt increases, however, tend to cause arcing to the
wire electrodes and cause nonuniformity in field strength along the collecting electrode,
so that problems similar to those of the ribbed collecting electrodes mentioned above
arise.
SUMMARY OF THE INVENTION
[0008] It is therefore an object of the invention to improve an electrostatic precipitator
of the type mentioned at the outset while avoiding the disadvantages and difficulties
mentioned as far as possible in such a way that the capture efficiency and/or the
particle retention capacity of the collecting electrodes can be increased preferably
without the main gas flow being significantly obstructed as a result through the separator,
which is achieved by means of a filter cassette according to claim 1 and a method
according to claim 6.
[0009] Thanks to the invention the trapping region near a collection electrode may be provided
with an optimized flow of highly charged particles, resulting in improved capture
efficiency in a cost-efficient manner and which may further assist in an improved
ability to use a more stable field strength. This is due to that at every given time,
a portion of the gas moves through the collector plates, and so, the entire gas volume
containing charges particles, will come very close to the collecting plate surface
at some instance during the passage. In other words, thanks to the invention, the
perceived average distance between the surfaces of the collector plates may be seen
as less than the actual measure, contrary to a traditional design.
[0010] Hence, thanks to the invention, the length of the device in the direction of gas
flow may be reduced while achieving the same effective surface area on which the particles
are collected. Therefore, both the length and the width of the device may potentially
be reduced with the same efficiency, which may be especially advantageous regarding
replacement of old type separators (e.g. cyclon) which normally are integrated in
spaces that are too small for conventional electrostatic separators.
BRIEF DESCRITION OF FIGURES
[0011] In the following the invention is to be explained in more detail with reference to
the figures, in which:
- FIG. 1,
- shows a schematic side view of an electrostatic filter unit according to the invention;
- FIG. 2
- shows a schematic view from above of the electrostatic filter unit in Fig. 1,
- FIG. 3
- shows a part of a first exemplary embodiment of a collector plate according to the
invention,
- FIG. 4
- shows a sectional view along the indicated lines in Fig 3, of the first exemplary
embodiment of a collector plate according to the invention,
- FIG. 5
- shows a part of a second embodiment of an exemplary collector plate according to the
invention,
- FIG. 6
- shows a sectional view along the indicated lines in Fig 5, of the second exemplary
embodiment of a collector plate according to the invention.
DETAILED DESCRIPTION
[0012] Fig. 1 illustrates an electric filter unit 1 for cleaning dust- laden waste gases
G that are supplied from one side of the electric filter unit 1 and leaves as cleaned
gas g at the opposite side. The electric filter unit 1, may be of conventional design,
comprising a a gas inlet 2, a first separator device 3, a second separator device
4, a dust collecting pocket 5, an electrostatic filter cassette 7, a third separator
device 3 and an outlet 6.
[0013] Fig. 1 shows a schematic side view of the electrostatic filter unit 1 and Fig. 2
shows a schematic view from above of the electrostatic filter unit.
[0014] It is in the novel features of electrostatic filter cassette 7 that the invention
is found. The invention is based on a new way of controlling the gas flow g7, through
the cassette 7, so that a greater number of particles can be precipitated in the cassette
7.
[0015] In the cassette 7 there are a number of parallel collector plates 70 (dash-dotted
in Fig. 2) which extend parallel to the side housing walls 72 of the cassette 7. There
is shown a main flow direction M of gas through the cassette 7, i.e. from an inlet
side 75 to an outlet side 76, which presents a traditional flow direction. Such a
traditional flow direction will have a main flow direction M comprising a first vector
Mx that basically is controlled by a bottom wall 77 and a top wall 78, which normally
are positioned parallel in a horizontal plane, i.e. which normally extends horizontally.
In a perpendicular plane there is a second vector My that traditionally is controlled
by the collector plates, i.e. in parallel with the extension of the plane P of a collector
plate 70 and accordingly corresponds to a flow vector along a channel 74 formed between
each neighboring pair of collector plates 70, which channels 74 would traditionally
control the second vector My of the gas to be parallel with the plane P of the collector
plates 70. It is to be noted that after having passed the cassette 7 the outflowing
gas g will normally slow down due to being controlled to flow in the main direction
of flow M. However, as is evident for the skilled person, the function of the invention
is not dependent on having specific directions of the main flow My, Mx, e.g. it will
basically fulfil its function also if the bottom and/or wall would not be horizontal.
[0016] The collector plates 70 are charged with a certain polarity, by means of a first
charging device (not shown). Between the collector plates 70 there are arranged wires
71 or similar devices known per se (schematically indicated in Fig. 2), which charge
the particles in the gas flow g7 with reversed polarity. Thus, a charged particle
will be attracted and precipitated against a collector plate 70 if it comes close
enough. The gas flow g7 is normally approx. 1 m/s in the cassette 7.
[0017] In the solution according to the invention, each plate 70 is provided with perforations
73 that control the flow g7, at least partly, through the collector plates 70. The
perforations 73 have the function of slanted holes extending along a hole direction
C, which will force the gas flow g7 to move at an angle α through the cassette 7,
in relation to a traditional main direction My of flow M through a cassette. Forcing
the gas flow g7 to move at an angle α will increases the probability that all particles
may arrive sufficiently close to a collector plate 70 to precipitate thereon. Further
it will increase the distance the gas flow g7 travels in the cassette 7 (compared
with a traditional flow through a cassette), which may synergistically increase efficiency.
[0018] As indicated in Fig. 2 the cassette 7 may be equipped with blocking members 9 to
assist in achieving a desired flow along a desired angle α through the cassette. The
blocking member can be in the form of a triangular body or a wall 90 forming a sharp
end directed against the inflow 75 and a wide end that seals at the outflow 76, for
a channel 74 that is next to a side 72 of the cassette 7 from which the gas flow g7
is being distanced during its passage throug the cassette 7. The blocking member may
also be (and/or) in the form of a triangular body or a wall 91 forming a sharp end
directed against the outflow 76 and a wide end that seals at the inflow 75, for a
channel 74 that is next to a side 72 of the cassette 7 to which the gas flow g7 is
approaching during its passage through the cassette 7.
[0019] One advantage with the invention is the length L of the filter cassette 7 may be
reduced compared to the needed length regarding conventional electrostatic separators,
to fulfil a certain level of separation. When replacing old type separators (e.g.
cyclon), that kind of old separators may normally be integrated in spaces that are
too small for conventional electrostatic separators, but which may be replaced by
a separator according to the invention, since thanks to the invention the length L
of the cassette 7 may be made smaller than conventionally needed. Normally there is
a need to have a relation between the length L of the cassette 7 and the collector
plate distance B (see Fig. 2) that is at least 10, i.e. L/B> 10, wherein B is the
distance between two neighboring collector plates 70. Thanks to the invention this
relation may be improved, to have 10> L/B. A standard collector plate distance B is
about 300 mm, implying a conventionally needed length L of 3 m. With the invention
it has shown to be possible to use B = 300 mm and a Length L that is about 2 m, i.e.
a L/B less than 7 which provides the advantage that many old separators may be exchanged
by means of the invention and using the existing infrastructure for the a new electric
filter separator cassette 7.
[0020] In Figs. 3 and 4 there are shown a possible embodiment of a collective plate 70 in
accordance with the invention. In Fig. 3 it is shown the face thereof and in Fig.
4 there is shown a cross-sectional view along the indicated line in Fig. 3. As shown
the collector plate 70 is provided with a plurality of holes 73, e.g. punched or drilled
holes having a center axis C. The holes are positioned at an angle β in relation to
the extension of the plate, which angle β is a smaller than 90°. The slanted holes
73 will force the gas g7 to move partly through each collective plate 70, which will
cause the main flow g7 within the cassette 7 to be forced to move along an angle α
in relation to the main extension M of each channel 74. The preferred angle β of the
holes is in the range of 5°-45°, preferably 10°-30°.
[0021] In Figs. 5 and 6 there are shown similar views as in Figs. 3 and 4 of a second embodiment
of an exemplary collective plate of the invention. In this embodiment the collective
plate is made from a so called expanded raised plate (also called stretch sheets),
e.g. a metallic plate that is punched to create through passages and thereafter stretched
to form an open structure as shown in Fig. 5. expanded raised plate holesBy directing
the punched passages in an angle the hole structure 73 of the collective plate 70
will in principle be as shown in Fig. 6, i.e. presenting rhomboid holes having surrounding
walls that are slanted at an angle β, which will force the gas flow g7 in a similar
manner as mentioned above.
[0022] The collector plate 70 would normally have a thickness in the range of 1-5mm. Preferably
the flow angle α of the gas flow g7 through the cassette 7 is such that the total
amount of gas flowing into the cassette has passed a neighboring collector plate 70
before leaving the cassette 7. Accordingly, preferably the gas flowing in G at the
inflow side 75 of the cassette 7 will enter one channel 74 between two collector plates
70 and all of those gases will leave at the outlet 76 having passed one collector
plate 70 such that they will pass out from the cassette 7 via a neighboring flow channel
74, which in many applications will result in choosing a pattern and angle β of the
holes 73 that provides a general flow angle α in a transversal plane to the collector
plates 70 that may be in the range of 5-15 degrees.
[0023] The expression cassette 7 must be interpreted in a broad manner. It may be a unit
by itself that may be exchanged by removing it as an integral unit having integrated
walls, at least at two opposing sides. However, it is also foreseen that the support
structure of the cassette 7 may be integrated into the filter unit 1 and that each
collector plate 70 may be separately removed from the cassette 7. Alternatively, the
collector plates 70 may be arranged removable pairwise or in other sets of groups.
[0024] The invention is not limited to the examples described above but may be varied within
the scope of the claims fulfilling the main purpose of the invention. For instance,
it is foreseen that the function of the principle is not dependent of a cassette but
will function also if fixedly installed a s a part within a filter unit.
1. Electrostatic separator, in particular for the separation of particles in a gas flow,
comprising a plurality of parallelly arranged collector plates (70) between an open
inflow (75) and an open outflow (76) forming a filter cassette (7), wherein between
two neighbouring collector plates (70) there is formed an open channel (74), characterized in that a plurality of said collector plates (70) are arranged with a plurality of perforations
(73), wherein said perforations (73) have a slanted function arranged to control the
gas flow (g7) to move at a flow angle (α) in relation to a second vector (My) of a
main flow direction (M) of gas through said cassette (7), wherein said a second vector
(My) of said main flow direction (M) is parallel with said collector plates (70).
2. Electrostatic separator according to claim 1, characterized in that said angle (α) is in the range of 5-20°, preferably 7°-15°.
3. Electrostatic separator according to any of claims 1-2, characterized in that each of said perforations (73) have a main direction (C) through said collector plate
(70) that form a hole angle (β) in relation to the plane (P) of said collector plate
(70), wherein preferably said main direction (C) is parallel to a first flow vector
(Mx) of said main flow direction (M), wherein said hole angle is in the range of 5°-45°,
more preferred 10°-30°.
4. Electrostatic separator according to any of claims 1-3, characterized in that the total amount of area (Ah) of perforations (73) in relation to the amount of the
total amount of area (Ap) of solid plate material (79) is in the range of 10 % to
50 %, preferably 20 % to 40 %.
5. Electrostatic separator according to any of claims 1-3, characterized in that the length (L) of the filter cassette (7) and the distance (B) between two neighbouring
collector plates (70) is such that 10> L/B >5, wherein preferably 8> L/B.
6. Method of operating an electrostatic separator, comprising the steps of providing
a filter cassette (7) with a plurality of parallelly arranged collector plates (70)
between an open inflow (75) and an open outflow (76), wherein between two neighbouring
collector plates (70) there is formed an open channel (74) presenting a main direction
of flow,
- charging said collector plates (70) with a first polarity,
- arranging for supply of incoming gas flow (G) including particles through said cassette
(7),
- charging particles in said gas flow with a second polarity,
- collecting particles by precipitation on said collector plates (70),
characterized by providing said plurality of collector plates (70) with a plurality of perforations
(73) which will control at least a part of said gas flow (g7) to pass through said
collector plates (70), controlling said gas flow (g7) to move at a flow angle (α)
in relation to a second vector (My) of said main flow direction (M) of gas through
said cassette (7).
7. Method according to claim 6, characterized in said a second vector (My) of said main flow direction (M) is parallel with said collector
plates (70), said angle (α) is in the range of 5-20°, preferably 7°-15°.
8. Method according to claim 6 or 7, characterized by controlling the flow velocity of said gas flow (g7) within the cassette (7) is in
the range of 0,5 m/s to 3 m/s, preferably above 1 m/s.
9. Method according to any of claims 6 -8, characterized by controlling the flow velocity of said gas flow (g7) within the cassette (7) to be
in the range of 101 % to 150 % of the flow velocity of said main flow (M).
10. Method according to any of claims 6 -9, characterized by controlling said gas flow (g7) by providing at least one blocking member (9) to assist
in providing a flow angle (α) in relation to a second vector (My) of said main flow
direction (M) of gas through said cassette (7).
11. Method of rebuilding a separator by means of exchanging a conventional separator by
an electrostatic separator according to any of claims 1-5, comprising the steps of
removing the conventional filter unit from its filter space in a filter housing and
installing said electrostatic separator cassette (7) in said filter space, wherein
preferably said filter space has a length (1) that is less than 3 m, more preferred
in the range of 2,5 - 1,8 m.