[0001] The present invention relates to an electric centrifugal blower, in particular a
volute for an electric blower able to optimize the air suction efficiency.
[0002] In fact, with reference to new regulations, each blower is classified in the respective
energetic efficiency class on the base of the Fluid Dynamic Efficiency (FDE) parameter
calculated in the Best Efficiency Point (BEP). In particular, IEG 61591 provides for
the terms and types of instruments for the execution of tests to verify the performance
of the electric blower. Its overall efficiency descends from the aerodynamic efficiency,
that is from the handling of air flow defined by the measured values of the static
pressure and the volumetric flow rate of the blower volute, and from the electromechanical
efficiency of the motor.
In order to improve the electric blower efficiency, studies were carried out oriented
to the optimization of the suction process and, more generally, to the air flow analysis
to improve the aerodynamic aspects of the aspirated air flow by acting on the volute
of the electric blower.
[0003] So, in general, an object of the invention is to identify the best conformation of
an aspirating blower volute, able to optimize the suction process of electric centrifugal
blowers.
In particular, an object of the invention is to really enhance the air suction aerodynamic
process of electric centrifugal blowers in suction hoods, which represent the final
product into which such electric centrifugal blowers are assembled.
The mentioned and other objects are achieved by an electric centrifugal blower comprising
an impeller having an orthogonal rotation z axis coincident with the z axis of an
xyz coordinate system, the impeller having a diameter D1 and being within a blower
volute that has a discharge mouth parallel to a plane passing through the z axis and
perpendicular to the xy-plane, wherein the blower volute has a baffle in the vicinity
of the end cross-section of the discharge mouth.
[0004] Advantageously the baffle is inclined by an angle of 8 degrees towards the inside
with respect to the plane of the end cross-section of the discharge mouth.
[0005] The blower volute has an outer radius R1 at an angle of 172.66 degrees in the xy-plane,
an outer radius R2 at an angle of 256.02 degrees in the xy-plane, an outer radius
R3 at an angle of 372.34 degrees in the xy-plane, the ratios of said radii R1, R2,
R3 to the diameter D1 of the impeller being R1/D1 = 0.79 ± 5%, R2/D1= 0.70 ± 5% and
R3/D1 = 0.57 ± 5%, respectively.
[0006] Furthermore, in correspondence of the centre of said baffle, the blower volute has
an outer radius R4 at an angle of 386.35 degrees in the xy-plane, the ratio of said
outer radius R4 to the diameter D1 of the impeller being R4/D1 = 0.84 ± 5%.
[0007] From above it should be understood that the present invention, which aims to optimize
the air suction process, refers exclusively to the shape of the electric blower volute.
The advantages arising from the shape and size of the electric blower volute have
been highlighted by a comparison of the electric blower aerodynamic performance according
to the present invention with those resulting from the use of the same electric motor
assembled in other volutes of electric blowers available on the market. In this way
it was possible to study and analyse separately the different configurations of the
blower volute by identifying the correct improvements to be made to optimize the aerodynamic
efficiency of the entire casing.
[0008] According to the invention a baffle is realized on the discharge mouth of the blower
volute. In this way the load torque on the motor shaft is decreased. Since the motor
itself, being an asynchronous motor, increases its rotational speed when the load
torque decreases, the speed of the impeller is greater as compared to a configuration
of a blower volute without baffle. In this regard, however, it is well to specify
that the increase of the rotating speed of the impeller does not allows a clear improvement
of the aerodynamic suction process automatically, without suitable and proper placement
and sizing of the introduced baffle. In fact, such a baffle, if not properly analyzed,
risks creating an obstruction to output air flow without making any improvement, indeed
creating only a worsening of fluid-dynamic efficiency. Then, in order to achieve the
hypothesized improvements the various vector components of the air flow vector have
been taken into consideration; in fact, through empirical tests performed directly
on various prototypes of blower volutes examined, it was possible to identify the
correct conformation and size of the baffle to be used in order to achieve the hypothesized
improvements.
[0009] The present invention will be now described, for an illustrative but not limitative
example, with reference to the accompanying drawings, in which:
Figure 1 is a perspective view of an electric blower of the prior art without cover;
Figure 2 is a perspective view of an electric blower according to the present invention
without cover;
Figure 3 is a plan view of the interior of the electric blower in Figure 2; and
Figure 4 is a view similar to that of Figure 3 that represents the geometry of the
blower volute.
[0010] First referring to Figure 1, which is a perspective view of an electric blower 1
of the prior art shown without cover, for convenience of illustration, a blower volute
generally indicated as 2 and an impeller generally indicated as 3 can be seen.
[0011] The blower volute 2 has a discharge mouth 4. Shown in Figure 2 is a perspective view
of an electric blower 10 according to the present invention without cover. By using
the same numbers in Figure 1 to indicate identical parts, the blower volute 10 is
indicated as 20, the impeller as 3 and the discharge mouth as 4. The discharge mouth
4 of the electric blower 10 has an end cross-section 5 as shown in Figure 3. The electric
blower 10 according to the present invention has a baffle 6 in the vicinity of the
end cross-section 5 of the discharge mouth 4.
[0012] The baffle 6 is inclined by an angle of 8 degrees inwardly with respect to the plane
of the end cross-section 5 of the discharge mouth 4.
[0013] In order to define the other design features of the electric blower volute according
to the present invention, the impeller 3 has a z orthogonal rotation axis coincident
with the z axis of an xyz coordinate system, whose xy-plane is represented in Figure
4, which is a view similar to that of Figure 3. Shown in Figure 4 are the points P1,
P2, P3, P4, which represent the curvature centre of tracts of the blower volute 20
with relative radii R1, R2, R3, R4, used for the construction of the blower volute
spiral. The points P5, P6, in addition to the angle of 8.2 degrees mentioned above,
serve to define the configuration of the baffle 6.
[0014] In an embodiment, the diameter D1 of the impeller of the electric blower 10 is 147
mm as calculated at the ends of the blades of the impeller itself, having the point
P0 (0; 0) as centre of the circumference.
[0015] For the calculation of the blower volute spiral the three different external geometric
radii above mentioned were taken into consideration, applied in the points which have
as coordinates the following values expressed in mm:
Radius R1 = 116 applied at the point P1 (15.2; 8.8)
Radius R2 = 103 applied at the point P2 (2.2; 9.3)
Radius R3 = 84.5 applied at the point P3 (-2.2; -8.6)
[0016] The outer radius R1 is measured at an angle of 172.66 degrees in the xy-plane, the
outer radius R2 at an angle of 256.02 degrees in the same plane, the outer radius
R3 at an angle of 372.34 degrees. In order to make independent such radii from the
sizes of the blower volute, the ratios of these radii R1, R2, R3 to the impeller diameter
D1 are shown. These ratios are, respectively:
R1/D1 = 0.79 ± 5%,
R2/D1 = 0.70 ± 5%, and
R3/D1 = 0.57 ± 5%,
said blower volute 20 has an outer radius R1 at an angle of 172.66 degrees in the
xy-plane, an outer radius R2 at an angle of 256.02 degrees in the xy-plane, an outer
radius R3 at an angle of 372.34 degrees in the xy-plane, the ratios of said radii
R1, R2, R3 to the diameter D1 of the impeller being R1/D1 = 0.79 ± 5%, R2/D1 = 0.70
± 5%, and R3/D1 = 0.57 ± 5%, respectively.
[0017] It is also considered the radius R4 = 124.2 applied at the point P4 (-40.1; -20.7)
which corresponds to the centre of the baffle 6 at an angle of 386.35 degrees in the
xy-plane. The ratio of the radius R4 to the diameter D1 of the impeller is R4/D1 =
0.84 ± 5%.
[0018] A further point P5 (70.9; 35.1) indicates where the arc of the circumference with
radius R4 ends.
[0019] The point P5 is used to define the point of application of the angle of incidence
of 8.2 degrees that is used to connect the upper portion of the baffle 6. Finally,
the point P6 (69.7; 49.5) indicates the vertex of the baffle 6. This point is referred
to the arc of circumference of the upper connection of the baffle 6; the tangent to
this point of circumference arc has a direction parallel to the air flow outgoing
from the blower volute. All of these mentioned points are represented in Figure 4
referred to the point P0 that is the centre of the impeller circumference in the xy-plane.
[0020] Briefly, the circumferences related to the various radii are internally tangent between
them. In detail, the circumference of radius R2 is internally tangent to the circumference
of radius R1; the circumference of radius R3 is tangent internally to the circumference
of radius R2, and the circumference of radius R3 is internally tangent to the circumference
of radius R4. The circumference of radius R4 ends at the point P5. The cut-off ends
at the point P6 connected to the point P5 by means of the angle of incidence of 8.2
degrees.
[0021] If one compares the electric blower of the prior art without baffle with the electric
blower with baffle according to the present invention, in the latter, the vector of
the air flow exiting the blower has a direction almost perpendicular to the cross-section
of the discharge mouth, thus ensuring a reduction of losses of the air flow with the
increasing of the flow speed, as compared with the case of the electric blower without
baffle. Furthermore, according to the Bernoulli principle, if the air density is supposed
constant in the various input and output points of the electric blower, since the
air flow speed is inversely proportional to the pressure, it results that the blower
impeller, with the insertion of the baffle, has a higher speed than that of an electric
blower without baffle. Both the increase of the impeller speed and the presence of
the baffle allow the output air flow to impact directly on the baffle which, being
built following the tangential direction of the impeller blade curvature, allows to
cut the air flow perpendicularly to the outlet cross-section therefore ensuring the
decrease of losses of the air flow itself within the blower volute. Also the part
of the air flowing between the impeller and the baffle is the centrifugal air flow
generated by the impeller; such flow in the indicated blower volute portion has a
very high speed; therefore, according to the Bernoulli principle the pressure value
will be very low in this air flow. This can improve the suction process since the
air flow moves from a high pressure zone to a low pressure zone. Therefore, the presence
of the baffle, in addition to improving the direction of the air flow vector in the
output, also improves the air suction process, generally assuring a clear improvement
compared to the electric blower without baffle of the prior art.
[0022] Thanks to the geometry of the baffle 6 described above, the air flow is cut better
permanently, increasing the fluid-dynamic efficiency value of the entire blower volute
and avoiding the creation of vortices of the centrifugal air flow that are likely
causes of noise.
[0023] The current FDE value fully matches its target. It was possible to reach a fluid-dynamic
efficiency value FDE equal to about 36% thus obtaining a marked improvement of about
8% with respect to the electric blower without baffle.
1. An electric centrifugal blower (10) comprising an impeller (3) having an orthogonal
rotation z axis coincident with the z axis of an xyz coordinate system, the impeller
(3) having a diameter D1 and being within a blower volute (20) that has a discharge
mouth (4) parallel to a plane passing through the z axis and perpendicular to the
xy-plane, characterized in that said blower volute (20) has a baffle (6) in the vicinity of the end cross-section
(5) of said discharge mouth (4).
2. The electric centrifugal blower (10) according to claim 1, wherein said baffle (6)
is inclined inwards by 8.2 degrees with respect to the plane of the end cross-section
(5) of said discharge mouth (4).
3. The electric centrifugal blower (10) according to claim 1, wherein said blower volute
(20) has an outer radius R1 at an angle of 172.66 degrees in the xy-plane, an outer
radius R2 at an angle of 256.02 degrees in the xy-plane, an outer radius R3 at an
angle of 372.34 degrees in the xy-plane, the relationships of said radii R1, R2, R3
to the diameter D1 of the impeller being respectively R1/D1 = 0.79 ± 5%, R2/D1= 0.70
± 5% and R3/D1 = 0.57 ± 5%.
4. The electric centrifugal blower (10) according to claim 3, wherein said outer radius
R1 at an angle of 172.66° in the xy-plane has the point P1 (15.2; 8.8) as its centre
and a length of 116 mm, said outer radius R2 at an angle of 256.02 degrees in the
xy-plane has the point P2 (2.2; 9.3) as its centre and a length of 103 mm, and said
outer radius R3 at an angle of 372.34° in the xy-plane has the point P3 (-2.2; -8.6)
as its centre and a length of 84.5 mm.
5. The electric centrifugal blower (10) according to claim 2, wherein in correspondence
of the centre of said baffle (6) said blower volute (20) has an outer radius R4 at
an angle of 386.35° in the xy-plane, the ratio of said radius R4 to the diameter D1
of the impeller being R4/D1 = 0.84 ± 5%.
6. The electric centrifugal blower (10) according to claim 5, wherein said outer radius
R4=124.2 at an angle of 386.35° in the xy-plane, is applied in the point P4 (-40,1;
-0,7).