WO/2024/006511 | PENDULUM CONVEYOR |
WO/1998/031616 | VIBRATORY CONVEYOR APPARATUS WITH PHASE-OPTIMIZED CONVEYOR DRIVE |
GB2086003A | 1982-05-06 | |||
GB2238841A | 1991-06-12 | |||
AT360907B | 1980-02-10 |
1. | A linear vibratory conveyor which incorporates a new disposition of the reactive mass with respect to the active mass and a new spring system that gives access to the null points of the system. |
2. | A linear vibrator conveyor as 1n Claim 1 in which the electromagnetic drive operates between the null points and the reactive mass. |
3. | A linear vibratory conveyor as in claims 1 and 2 in which the null points of the system are used as the means of connecting the linear vibratory conveyor to the ground or substructure. |
4. | A linear vibratory conveyor as in Claims 1 and 2 in which the reactive mass of the system stands on shock absorbers to connect the linear vibratory conveyor to the ground or sub¬ structure. |
5. | A linear vibratory conveyor as in Claims 1 and 3 in which the drive is other than electro—magnetic. |
This invention relates to a linear vibratory conveyor.
Linear vibratory conveyors are used to carry all manner of bulk
materials.
These are usually conveyed horizontally, but some inclination to
the vertical may also be involved.
Some well-established drives exist which include electro¬
magnetic, electro-dynamic, pnue atic, hydraulic and combination
arrangements.
This invention, although applicable to any method of drive,
has been conceived especially to overcome problems associated
with an electro- magnetic method.
Figure 1 shows a typical linear vibratory conveyor in current
use.
Referring to Figure 1 , a typical conventional system has a mass
associated with the conveyor trough and its carriage, called the
active mass 1.
This is connected to the base, called the reactive mass 2, by
leaf springs or cantilever springs 3. These springs are usually
inclined to the vertical as illustrated to give the required
conveyor motion.
The typical vibratory drive 4 is usually arranged to produce a
vibratory force between the active mass and the reactive mass
and if the reactive mass is much larger than the active mass then
the oscillation or vibration is largely taken up by the active
mass. In this manner the conveyor trough and carriage is
subjected to the oscillation or vibration whilst the base
vibrates to a much smaller degree, and being mounted on shock
absorbers 5, undersirable transmission of the vibrations to the
surrounding area is reduced. Typically the oscillation used may
be at, or near the resonant frequency.
If electro-magnetic drives of this type having an air gap 6 are
employed for larger linear vibrating conveyors, there is a
conflict between having sufficient air gap to allow for the
required oscillatory displacement, and achieving a small enough
air gap to obtain the power required for the oscillation
without having to resort to the use of larger magnets and larger
1mput powers.
In regard to the typical linear vibratory conveyor illustrated
1n Figure 1, the following observations are made because of
their significance for the invention
(a) the active mass 1 and reactive mass 2
vibrate on a line through their centres
of gravity about a fixed point situated
between the two masses.
(b) There is a null point on the cantilever
springs 3, that is, a point which remains
stationary with respect to the ground.
(c) The position of this point on the cantilever
spring 3, depends on the ratio of the masses used
for the active mass and for the reactive mass.
(d) On the other hand the inclination to the vertical
of the surface of the springs in the vadnlty of
the null point will be constantly changing during
one cycle of oscillation.
In order to describe the operation of the linear vibrating
conveyor which incorporates the invention, a specific embodiment
of the invention will now be described by way of example with
reference to Figures 2 and 3.
Figure 2 illustrates by means of a simple diagram, the
disposition of the reactive mass 2 with respect to the active
mass 1 and the spring system which provides the interconnection
between these masses. This spring system consists of a set of
cantilever springs 3 joined to the active mass by spring
fixings and another set of cantilever springs 4 joined to the
reactive mass 2 by means of spring fixings and inclined at the
required angle to the vertical.
These sets of cantilever springs are joined together by means
of their common connection to the flat sections 5.
Figure 3 illustrates one example of a practical linear
vibratory conveyor which embodies the invention. The reactive
mass 2 is composed of two side pieces one on each side of the
spring system which are joined together by means of the channel
sections 8, together with additional sections 1f this is
required for strength. The illustration shows a side view of the
linear vibratory conveyor with the nearest of the side
pieces of the reactive mass 2 removed.
The sets of springs 3 and 4 are Joined together by flat sections
of material 5.
The electro-magnetic drive shown is a double system operating
in pull-pull, with the energised sections attached to the
reactive mass 2 and with the armature 1 sections, attached to
each of the flat sections 5, but alternatively the energised
sections may be attached to the flat sections 5 and the armature
I sections attached to the reactive mass.
There may be other rows of springs in addition to the two rows
shown.
The electro-magnetic drive may be a single system having one
energised section pulling on one armature I section, in which
case one of the two illustrated will be absent.
The electro-magnetic drive may be other than the type
illustrated.
The drive may be other than electro-magnetic.
The weight of the reactive mass on the cantilever springs 4
causes a small but additional stress in these springs. This can
be removed by allowing the reactive mass to rest on ordinary
compression springs inserted between the reactive mass and the
base.
One of the principle features of this linear vibratory conveyor
is that the active 1 and the reactive mass 2 are interconnected
not by one set of cantilever springs but by the use of two sets
of cantilever springs 3 and 4 Joined together through their
common connection to the flat sections of material 5.
When the linear vibratory conveyor is in action the null point on
the cantilever springs system will normally be designed to be
at, or close to, the junction of the springs 5. This is
achieved by the correct design of the cantilever springs 3 and 4
in relation to each other and in relation to the size of the
masses 1 and 2 and fulfulling a number of simultaneous
conditions. The correct design also achieves a minimum
change in the inclination to the vertical of the springs where
they make the common connection with flat section 5.
The design obtains that one set of cantilever springs
restrains the other set of cantilever springs in such a manner
as to closely maintain the same position and inclination to
the vertical at their Junction with the flat section 5, to that
which occurs statically.
Therefore the spring fixings normally present to restrain the
end of the springs to the required inclination to the vertical
are rendered redundant. For this reason, this linear vibration
conveyor is simple and easy to manufacture and much less
expensive than some other linear vibratory conveyors which have
the same objectives.
Because the position and angle of the flat section 5 is
maintained virtually constant whilst the masses are oscillating,
this flat section 5 may be used advantageously to directly
connect the linear vibratory conveyor to the ground or
sub-structure.
This may be achieved with or without a degree of shock
absorbing material , depending on the balance of the forces in
the system. This is illustrated in Figures 3, 4 and 5.
The electro-magnetic drive 7 may be applied between the active
mass 1 and the reactive mass 2 as in the conventional linear
vibratory conveyor.
Alternatively as shown by example in Figures 3, 4 and 5 the
electro-magnetic drive may be applied between the reactive mass
2 and the flat sections 5 where the springs are Joined together
or between the reactive mass 2 and the ground or sub-structure.
This allows the electro-magnetic drive to operate with smaller
magnetic air gaps or air gap 6.
In the conventional linear vibratory conveyor the air gap must
be sufficient to allow for the total movement between the
active mass and the reactive mass which means the movement of
the top carriage plus the movement of the reactive mass. In the
linear vibratory conveyor examples 1n F1g 3, 4 and 5 the air
gap need only be sufficient to allow for the movement of the
reactive mass. The invention therefore provides a solution to
the problem stated in the second paragraph of page 2 in that 1t
permits the use of smaller magnetic air gaps or air gap for the
electro—magnectic drive.
The examples illustrated in Figures 2, 4 and 5 are linear
vibratory conveyors supported on the ground or sub-structure
by means of the flat sections 5. It is sometimes preferable to
support these conveyors by means of the reactive mass, that is,
the reactive mass is connected to the ground or sub structure
through the medium of shock absorbers and this is therefore an
alternative to that illustrated in Figures 3, 4 and 5 but an
alternative that still maintains all the benefits of the
smaller magnetic air gaps or air gap.
Figures 4 and 5 illustrate further examples of a practical
linear vibratory conveyor which embody the invention-
The description and operation for these examples are exactly
the same as for the example illustrated in Figures 3 and
presented on pages 3, 4, 5 and 6 and must be read as such, with
the simple exception that the attachment of the section of the
electro-magnetic drive to the flat section 5 is achieved in a
different manner.
In Figure 4, the armature I sections are connected to the flat
sections 5 by means of the two slats 9, one on each side of the
spring system, or by other means. The diagram is drawn with the
nearest slat removed. The slat on the far side is shown
interconnecting the flat sections 5 of the two rows of springs on
either side of the magnetic drive, but these slats may also
interconnect all the other flat sections 5 that may be used.
The energised sections of the electro-magnetic drive are attached
to the reactive mass 2.
In figure 5 the energised sections of the electro-magnetic
drive are connected to the flat sections 5 by means of the two
slats 9, one on each side of the springs system, or by other
means.
The diagram is drawn with the nearest slat removed. The slat on
the far side is shown interconnecting the flat sections 5 of
the two rows of springs on either side of the electro-magnetic
drive, but these slats may also Interconnect all the other flat
sections 5 that may be used. The armature I sections of the
electro-magnetic drive are attached to the reactive mass 2.
This arrangement allows the electrical connection to the drive
to suffer little or no vibration.
In Figure 4 and 5 the electro-magnetic drive illustrated is a
double system, instead the electro-magnetic drive may be a
single system having one energised section pulling on one
armature I section, 1n which case one of the two systems
illustrated will be absent.
The weight of the reactive mass on the cantilever springs 4
causes a small but additional stress in these springs.
This can be removed or alleviated by allowing the reactive mass
to rest on ordinary compression springs 10, these being inserted
between the reactive mass 2 and the slats 9.
Each of the examples of linear vibratory conveyor illustrated
1n Figures 3, 4 and 5 benefit from being driven constantly at
their resonant frequency even when this changes due to load.
This is achieved by using a power imput, the frequency of which
is derived from its own natural movement.
The electro-magnetic drive may be other than the type
illustrated.
The drive may be other than electro—magnetic.
The illustration in figure 6 shows another embodiment of the
system of cantilever springs and the masses which they
interconnect, which constitutes the invention, but in which the
interconnecting springs are not parallel. The Springs 4 may be
set at another angle to that of the springs 3 and may be
conveniently positioned vertically as illustrated in figure 6. A
modest reduction in performance may result from this, but in
some instances the vibrator is easier to manufacture.
As a quite separate consideration the reactive mass may be
positioned between the two sets of springs, if there is an even
number of springs per row, instead of being divided into two
pieces, one on each side of the springs.
The embodiments of the invention shown in figures 3, 4 and 5, may
incorporate the spring system shown in figure 6, instead of that
which is shown. Also in these examples the reactive mass may be
positioned between two sets of springs Instead of being divided
into two pieces, one each side of the springs.
In all these embodiments the electro-magnetic drive, if used, may
be positioned to operate horizontally or closer to the
horizontal, instead of being inclined as illustrated. The drive
may be other than electro magnetic.
The illustration in figure 7 shows another embodiment of the
system of cantilever springs and the masses 1 and 2 which they
interconnect, which constitutes the invention, but which is part
of a hybrid arrangement of springs, that is, conventional
cantilever springs II are also used to interconnect the masses 1
and 2. This reduces the number of components and in some
examples makes the vibrator easier to manufacture.
The illustration in figure 7 shows two rows of each type of spring connection as an example but other combinations may be used and
in any order, with one or more row of springs being the
cantlever spring arrangement which constitutes the invention. The embodiment of the invention shown in figures 3, 4 and 5 may
incorporate the type of spring system illustrated in figure 7 and
described in the previous paragraph, instead of that which is
shown in figures 3, 4 and 5, or using that illustrated in both
- figures 6 and 7. In these examples the reactive mass may be positioned between the springs instead of being divided into two pieces one each side of the springs.
Other electro-magnetic drives may be used, or the drive may be other than electro magnetic.
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