Field of the Invention.
[0001] The present invention relates to the field of fan engineering and, more specifically,
to the design of a centrifugal fan.
Prior Art.
[0002] The present invention will be most useful in the designs of centrifugal fans with
medium- and high specific rotational speed used in the ventilation and air-conditioning
systems.
[0003] The basic requirements for the design of modern fans are high aerodynamic parameters,
a wide range of economical operation, technology of manufacturing, strength and reliability
of their construction. The term aerodynamic parameters shall be understood as the
volumetric flow rate of gas passing through the fan, total pressure provided by the
fan and the efficiency of the latter. The notion "wide range of economical operation"
shall be understood as the range of its operating modes at a high efficiency.
[0004] The tendency towards developing a centrifugal fan that would meet the above requirements
has led to evolution of a centrifugal fan (T.S. Solomakhova et al. "Centrifugal fans",
1975, Mashinostroenie Publishing House, Moscow, page 6-7) whose spiral casing accommodates
a wheel formed by the carrying and overlying discs with blades therebetween. The side
surfaces of each blade have the form of a cylindrical surface with generating lines
parallel to the wheel axis. In each of said blades the angle formed by a segment of
the curve produced in the section of the blade side surface by a plane perpendicular
to the fan wheel axis, and by a circle whose centre lies on the wheel axis and which
passes through the point of said segment of the curve nearest to the wheel axis, is
constant throughout the width of the fan wheel. This angle will be referred to hereinafter
as the "blade entrance angle". Similarly, the angle of these blades formed by the
segment of the curve produced in the section of the side surface of each blade by
the plane which is perpendicular to the wheel axis and by the circle whose centre
lies on the wheel axis and which passes through the point of this segment of the curve
farthest from the wheel axis is also constant throughout the width of the fan wheel.
This angle will be referred to below as the "blade exit angle".
[0005] When the gas flow in the running fan is turned from the axial to the radial direction,
there appears nonuniformity of the field of gas flow velocities across the width of
the wheel along the entrance edges of blades or, in other words, there develop differencies
in the conditions of the gas flow around the blades along the width of the fan wheel.
This brings about nonuniform loading of the blades across the width of the fan wheel,
develops intensive secondary flows in the channels between blades and the development
of separation in the gas flow which ultimately reduces the aerodynamic parameters
of the centrifugal fan and narrows the field of its economical operation.
[0006] Besides, the practical experience gained in using such type of centrifugal fans has
shown that at high peripheral velocities of the fan wheel the blades lose their stability
and are deformed which is caused by the effect of strong centrifugal forces and insufficient
rigidity of construction. This reduces the strength and reliability of the fan wheel
and the centrifugal fan as a whole.
[0007] The strive for improving the aerodynamic parameters, step up the strength and reliability
of the centrifugal fan has resulted in the development of the centrifugal fan (DE,
C, 952547) whose spiral casing accommodates a fan wheel formed by the carrying and
overlying discs with blades therebetween. Each side surface of the blade is of a curvilinear
shape and, being intersected by any plane perpendicular to the wheel axis, forms a
segment of a curve which, jointly with the circle whose centre lies on the wheel axis
and which passes through the point of this segment of the curve nearest to the wheel
axis, forms a blade entrance angle which grows throughout the wheel width in the direction
from the carrying disc to the overlying one. In other words, the entrance angle of
each blade grows across the width of the fan wheel from the carrying to the overlying
disc. This provides for the uniform loading of blades, reduces the intensity of secondary
flows in the channels between blades and narrows the zone of separation in the gas
flow which improves the aerodynamic characteristics of the centrifugal fan and broadens
the range of its economical performance.
[0008] However, in order to ensure the growing of the entrance angle of each blade across
the wheel width from the carrying disc to the overlying disc, the blade is twisted
around its longitudinal axis in the course of manufacture. The practice of using the
centrifugal fans with such blades has demonstrated that their performance is particularly
efficient when the blade entrance angle at the overlying disc is at least one and
a half times larger than the blade entrance angle at the carrying disc. Such twisting
of the blade is possible only in case of a large axial extension of the blade at which
the relative twisting angle is small. If, however, the axial extension of the blade
is small, the relative twisting angle is large. At a large relative twisting angle
the material traditionally used for the manufacture of blades fails in the course
of manufacture. Therefore, the blades of such centrifugal fans are very long axially.
As a result, the diameter of the inlet hole of the fan wheel is large, the radial
length of each blade is small and the exit angles of blades bent against rotation
of the wheel are small. It is a known fact that at a small radial length and small
exit angles of blades the total pressure provided by the centrifugal fan is small.
[0009] Besides, twisting of blades causes residual stresses in their material which reduce
the strength parameters of blades so that at high peripheral velocities of the fan
wheel, characterized by strong centrifugal forces, the blades loss stability and become
deformed. This tells adversely on the strength and reliability of the centrifugal
fan.
[0010] Moreover, twisting of blades complicates their manufacturing technology. It concerns
particularly those cases when the blades are made from a sheet material most commonly
used in modern fan engineering. Owing to all these factors the centrifugal fans with
such blades have not become much popular in fan engineering practice.
Disclosure of the Invention.
[0011] The invention is essentially aimed at providing a centrifugal fan, wherein due to
configuration of the lateral surface of the blades, there is provided an increase
in the full pressure produced by the fan, a better strength of its structure and reliability
in operation.
[0012] This aim is achieved by providing a centrifugal fan whose spiral casing accommodates
a fan wheel comprises of a carrying disc and an overlying disc with blades secured
therebetween, at least one curvilinear surface of each blade in the section by a plane
perpendicular to the fan wheel axis defines a segment of the curve forming, together
with the circle whose centre lies on the fan wheel axis which passes through the point
of the segment of the curve, nearest to said centre, a blade entrance angle growing
across the width of the fan wheel in the direction from the carrying disc to the overlying
disc; said curvilinear side surface of the blade has the shape of a ruled developable
surface with the generating lines inclined towards the plane perpendicular to the
fan wheel axis at an angle varying from 45
oto 85
o and the projection of at least one of said generating lines on the plane perpendicular
to the fan wheel axis is a tangent to the segment of the curve in said plane.
[0013] The requirement for increasing the blade entrance angle across the width of the fan
wheel from the carrying disc to the overlying disc in the disclosed fan is ensured
by the above-stated shape of the side surface of the blade. And this shape can be
manufactured without subjecting the blade material to twisting or any other substantial
plastic deformations; it is enough to bend it in order to produce the required shape
of the side surface and blade profile. This procedure does not involve residual stresses
which limit the axial dimensions of the blade. Consequently, the disclosed centrifugal
fan can be made with blades having a variable entrance angle across the width of the
fan wheel and having any, even small, axial length. The fans with a small axial length
of their blades are characterized by an increased radial length which, all other conditions
being equal, brings about an increase in the exit angles of each blade and, accordingly,
a higher total pressure provided by the fan.
[0014] A smaller axial length of the blades and elimination of considerable residual stresses
in the material of the blades improves the strength paramaters of blades and the fan
wheel as a whole. This permits either to increase the peripheral velocity of the fan
wheel thereby improving the aerodynamic characteristics of the fan, or, by retaining
the same peripheral velocity of the fan wheel, to enhance the mechanical strength
and reliability of the centrifugal fan.
[0015] Besides, as has been stated above, in order to manufacture a blade, it is enough
to bend its material to obtain the required profile and shape of its side surface
which simplifies its manufacturing technology.
[0016] The blades made from sheet materials are used at peripheral velocities of the fan
wheel which do not exceed about 70 m/s. At peripheral velocities exceeding 70 m/s
the blades are of a profiled shape. This shape makes it possible to design the blades
both with one and two side surfaces in the form of a ruled developable surface.
[0017] In practice for the fan wheels with a relative width of the blade exit edges not
less 0.2 the ruled developable surface should be cylindrical.
[0018] In the fan wheels with a relative width at the blade exit edges varying from 0.15
to 0.2 it is practicable that the ruled developable surface should be conical. The
conical surface intensifies the changes of the blade entrance angle across the width
of the fan wheel in the direction from the carrying disc to the overlying one.
[0019] It is no less practicable that the segment of the curve formed when the side surface
of the blade is intersected by the plane of the carrying disc should form an arc of
the circle wherein the relation of the square of chord length to the difference of
squares of the diameters of the circles passing, respectively, through the exit and
entrance edges of blades should be within 0.2 to 0.25.
[0020] Thus, we receive blade profiles in various blade sections perpendicular to the fan
wheel axis which ensure the range of blade entrance and exit angles, which permits
achieving high values of efficiency and total pressure of the centrifugal fan.
[0021] It is quite reasonable that the segment of a curve which is formed when the side
surface of the blade is intersected by the plane of the carrying disc should form
on the side of the blade entrance edge an arc of the circle conjugate with the segment
of a straight line from the side of the blade exit edge and that the relation of the
square of the distance between the ends of said segment of the curve to the difference
of squares of the diameters of the circles passing, respectively, through the exit
and entrance edges of blades should vary from 0.15 to 0.22.
[0022] In the blades of such a profile the blade exit angle is increased and remains constant
across the width of the fan wheel which leads ultimately to an increase in the total
pressure of the fan. The above-stated relation of the square of the distance between
the ends of the above-mentioned segment to the difference of squares of the circle
diameters passing through the exit and entrance edges of blades ensures the range
of values of the blade entrance and exit angles at which the efficiency and total
pressure of the centrifugal fan acquire high values.
[0023] It is recommended that in the blades with the profile in the form of art arc of a
circle conjugate with a segment of a straight line, the relation of the diameter of
the circle passing through the exit edges of the blades to the diameter of the carrying
disc should vary from 0.9 to 1.1.
[0024] Thus, the blades used in the disclosed fan wheel have, each, a profile with a longer
or shorter segment of a straight line. This permits producing a selection of discrete
aerodynamic characteristics of the centrifugal fan, thereby broadening the zone of
effective operation of the fan, i.e. the zone of high efficiency performance.
[0025] Now the invention will be described by way of examples with reference to the accompanying
drawings in which:
Fig. 1 is a meridional section of the centrifugal fan according to the invention;
Fig. 2 is a section taken along line II-II in Fig. 1;
Fig. 3 shows a blade installed on the partly-illustrated carrying disc of the fan
wheel, isometric view, enlarged;
Fig. 4 is a section taken along line IV-IV in Fig. 1;
Fig. 5 is a section taken along line V-V in Fig. 1;
Fig. 6 is a section taken along line VI-VI in Fig. 1;
Fig. 7 illustrates a blade installed on the partly-shown carrying disc of the fan
wheel, another embodiment, isometric view, enlarged;
Fig. 8 is a blade installed on the partly-shown carrying disc of the fan wheel, still
another embodiment, isometric view, enlarged;
Fig. 9 is a section taken along line IX-IX in Fig. 1, a further version of the fan
wheel blade;
Fig. 10 is a section taken along line X-X in Fig. 1, a still further version of the
fan wheel blade.
[0026] Given below as an example is a centrifugal fan used, for example, in air conditioning
and ventilating systems of industrial or civic buildings. Such a centrifugal fan comprises
a spiral casing 1 (Fig. 1) having an inlet pipe 2 and an outlet pipe 3 (Fig. 2). The
chamber 4 of the spiral casing 1 houses a fan wheel 5 formed by a carrying disc 6
(Fig. 1) and an overlying disc 7 installed between which over the periphery are blades
8 forming a chamber 9 (Fig. 2) inside the fan wheel 5 and channels between blades
8a. The carrying disc 6 is secured by a hub 10 (Fig. 1) on a drive shaft 11 (not shown
in the drawings). The relative width of the fan wheel, i.e. the relation of the width
b₂ of the fan wheel 5 at the exit edges of the blades 8 to the diameter D₂ of the
circle passing through the exit edges of the blades 8 is equal to 0.25 in this embodiment
of the invention.
[0027] At least one of the side surfaces 12 (Fig. 3) of each blade 8, and in this embodiment
of the invention the blades 8 are made from a sheet material so that both side surfaces
12 of each blade 8 in the section by a plane perpendicular to axis 0₁-0₁ of the fan
wheel 5 form a segment 13 (Fig. 4) of the curve which, together with the circle 14
whose centre 0₂ lies on the axis 0₁-0₁ of the fan wheel 5 and which passes through
the point 15 of the segment 13 of the curve nearest to said centre 0₂, forms an entrance
angle β₁ of the blade 8. The entrance angle β₁ of the blade 8 grows along the width
b₁ of the fan wheel 5 in the direction from the carrying disc 6 to the overlying disc
7. In this embodiment of the centrifugal fan the entrance angle β'₁ (Fig. 5) of the
blade 8 at the carrying disc 6 amounts approximately to 15° while the entrance angle
β

of the blade 8 at the overlying disc 7 is about 21°. The exit angles β₂ (Fig. 4)
of the blade 8 are determined in a similar way. The exit angle β₂ of each blade 8
also grows along the width b₂ of the fan wheel 5 in the direction from the carrying
disc 6 to the overlying disc 7. In this particular example the blade exit angle β

(Fig. 5) at the carrying disc 6 is about 32
o while the blade exit angle β

at the overlying disc 7 is about 35
o. Each curvilinear side surface 12 (Fig. 3) of the blade 8 is a ruled developable
surface, cylindrical in this version of realization. The generating lines 16 of this
surface 12 are inclined to the plane perpendicular to the axis 0₁-0₁ of the fan wheel
5 at an angle α varying from 45
o to 85
o. In this particular realization of the centrifugal fan the angle α is 78
o and the plane perpendicular to the axis 0₁-0₁ of the fan wheel 5 is the plane of
the carrying disc 6. The projection 17 of at least one of the generating lines 16
(just one in this version) on the plane of the carrying disc 6 is a tangent to the
segment 13 of the curve in this plane. The segment 13 of the curve formed by intersection
of the side surface 12 of the blade 8 with the plane of the carrying disc 6 is an
arc 18 (Fig. 6) of the circle 19. The shape of this arc 18 of the circle 19 in such
that the relation of the square of the length l₁ of the chord 20 of said arc 18 to
the difference of squares of diameters D₂, D₁ of the circles 21, 22 passing, respectively,
through the exit edges 23 and entrance edges 24 of the blades 8 lies within the limits
from 0.2 to 0.25; in the given embodiment of the centrifugal fan this relation is
0.21.
[0028] Other realization of blades 8 are also possible. In the case, when the fan operating
conditions call for the peripheral velocity of the fan wheel 5 higher than 70 m/s,
the blades 8 should be of a profiled type. Such a blade 8 is shown in Fig. 7.
[0029] If the operating conditions of the centrifugal fan require that the relative width
of the fan wheel 5 should be less than 0.2, the aerodynamic parameters of the fan
can be raised by using the blades 8 with at least one side surface 12 being conical.
In other respects the design of the fan remains the same as that of a fan with cylindrical
blades. This version of the blade 8 appears in Fig. 8.
[0030] Besides, when the basic technical requirements for the centrifugal fans are high
values of their efficiency and total pressure each of their blades 8 (Fig. 9) should
be so constructed that when its side surface 12 is intersected by the plane of the
carrying disc 6 this forms a segment 13 of the curve which at the side of the entrance
edge 24 of the blade 8 is the arc 25 of the circle 26 conjugate with the segment 27
of the straight line 28 at the side of the exit edge 23 of this blade 8. The shape
of this segment 13 of the curve is such that the relation of the square of distance
l₂ between its ends to the difference of squares D₂, D₁ of the circles 21, 22 passing,
respectively, through the exit edges 23 and entrance edges 24 of the blades 8 lies
within the limits from 0.15 to 0.22. In the given embodiment of the centrifugal fan
this relation is 0.19. It should be emphasized that this version of the blades 8 is
possible both with the cylindrical and conical shapes of the side surface 12.
[0031] In order to broaden the range of effective performance of the centrifugal fan, the
profile of the blades 8 (Fig. 10) is made in the form of an arc 25 of the circle 26
conjugate with the segment 27 of the straight line 28 in which the relation of the
diameter D₂ of the circle 21 passing through the exit edges 23 of the blades 8 to
the diameter D₃ of the carrying disc 6 lies within the limits from 0.9 to 1.1. Shown
in Fig. 10 is a version of the centrifugal fan wherein said relation is equal to 1.05.
[0032] The centrifugal fan functions as follows. As the drive shaft 11 (not shown in the
drawings) rotates, its rotation is transmitted via the carrying disc 6 secured on
the shaft 11 by means of the hub 10 to the fan wheel 5 installed in the chamber 4
of the spiral casing 1. When the fan wheel 5 rotates along arrow A (Fig. 2), the gas
moves in the axial direction shown by arrows B (Fig. 1) through the inlet pipe 2 into
the chamber 9 inside the fan wheel 5 where it is acted upon by the vacuum near the
entrance edges 24 of the blades 8, changes its direction from axial to radial and
moves onto the blades 8 of the fan wheel 5. Turning of the gas flow through 90° causes
nonuniformity of its velocities along the entrance edges 24 of the blades 8. This
nonuniformity is such that the gas flowing around the blades 8 at the overlying disc
7 has a higher speed than at the carrying disc 6. Owing to an increasing entrance
angle β₁ of the blades 8 across the width b₁ of the fan wheel 5 in the direction from
the carrying disc 6 to the overlying disc 7 causes by the inclination of the generating
lines 16 of the side surface 12 of the blade 8 at an angle α to the plane perpendicular
to the axis 0₁-0₁ of the fan wheel 5, the gas flow moves to the blades 8 at an optimum
angle of incidence throughout the width b₁ of the fan wheel 5 which reduces pressure
losses at the entrance into the fan wheel 5.
[0033] As the gas moves further through the channels between blades 8a of the fan wheel
5, it receives energy from the drive successively via the shaft 11, hub 10, carrying
disc 6 and blades 8 which builds up a total pressure developed by the fan. This practically
eliminates the conditions for the development of separation zones of gas flow in the
channels between blades 8a, ensures a uniform load on the blades 8 across the width
b₁ of the fan wheel 5 which leads to a minimum intensity of secondary flows at the
overlying disc 7. Then the gas flows into the chamber 4 of the spiral casing 1 where
part of the dynamic pressure of the gas flow leaving the fan wheel 5 is transformed
into static pressure. Then the gas flow leaves the fan through the outlet pipe 3 in
the direction shown by arrow C in Fig. 2. The uniform field of velocities at the outlet
from the fan wheel 5 reduces the pressure losses in the chamber 4 of the spiral casing
1. All these factors increase the total pressure provided by the fan, and its efficiency.
[0034] All the centrifugal fans with blades 8 of the above-described shapes of side surfaces
12 function on the same principle.
[0035] Given below is a summary table 1 of fifteen versions of centrifugal fans where:
Z = number of blades 8 of fan wheel 5;
b₂= width of fan wheel 5 at exit edges 24 of blades 8;
D₁= diameter of circle 22 passing through entrance edges 24 of blades 8 of fan
wheel 5;
D₂= diameter of circle 21 passing through exit edges 23 of blades 8 of fan wheel
5;
D₃= diameter of carrying disc 6 of fan wheel 5;
α= inclination angle of generating line 16 of side surface 12 of each blade 8 to
the plane perpendicular to axis 0₁-0₁ of fan wheel 5;
β

= entrance angle of blade 8 at carrying disc 6 of fan wheel 5;
β

= entrance angle of blade 8 at overlying disc 7 of fan wheel 5;
β

= exit angle of blade 8 at carrying disc 6 of fan wheel 5;
β

= exit angle of blade 8 at overlying disc 7 of fan wheel 5;
l₁= length of chord 20 of arc 18 of circle 19 formed when side surface 12 of blade
8 is intersected by the plane of carrying disc 6;
l₂= distance between the ends of segment 13 of a curve, formed when the side surface
12 of the blade 8 is intersected by the plane of the carrying disc 6 and forming at
the side of the entrance edge 24 of blade 8 an arc 25 of circle 26 conjugated with
the segment 27 of a straight line 28 at the side of the exit edge 23 of blade 8;
Q = volumetric gas flow rate of the centrifugal fan;
Pv = total pressure provided by centrifugal fan;
η= efficiency of centrifugal fan.
[0036] The speed of the fan wheel is 1450 rpm, diameter D₂ = 0.63 m.

Industrial Applicability.
[0037] The present invention can most advantageously be used in centrifugal medium and high-speed
fans employed in ventilation and air conditioning systems.
1. A centrifugal fan whose spiral casing (1) houses a wheel (5) formed by a carrying
and an overlying discs (6,7) between which blades (8) are secured, at least one of
the lateral surfaces (12) of each of which is curved and defines a portion (13) of
a curve in the section formed by a plane perpendicular to the axis (0₁-0₁) of the
fan wheel (5), said portion (13) forming an entrance angle (β₁) of the blade (8) with
a circumference (14) whose centre (0₂) lies on the axis (0₁-0₁) of the wheel (5) and
which passes through a point (15) of the portion (13) of the curve closest to said
centre (0₂), said entrance angle (β₁) of the blade (8) increasing across the width
(b₁) of the wheel (5) in the direction from the carrying disc (6), to the overlying
disc (7), characterized in that the lateral surface (12) of the blade (8) is substantially a linear developable
surface having generating lines (16) inclined to the plane perpendicular to the axis
(0₁-0₁) of the wheel (5) at an angle (α) lying within the limits from 45o to 85o, and the projection (17) of at least one of said generating lines (16) on the plane
perpendicular to the axis (0₁-0₁) of the fan wheel (5) is a tangent to the portion
(13) of the curve in this plane.
2. A centrifugal fan as claimed in Claim 1, characterized in that the linear developable surface is a cylindrical surface.
3. A centrifugal fan as claimed in Claim 1, characterized in that the linear developable surface is substantially a conic surface.
4. A centrifugal fan as claimed in Claim 1, characterized in that the portion (13) of the curve formed at the intersection of the lateral surface
(12) of the blade (8) by the plane of the carrying disc (6) is substantially an arc
(18) of a circle (19), whose ration of the square of the length (l₁) of a chord (20)
to the difference of squares of diameters (D₂, D₁) of circles (21, 22) passing respectively
through the forward and entry tips (23, 24) of the blade (8) is within the range of
from 0.2 to 0.25.
5. A centrifugal fan as claimed in Claim 1, characterized in that the portion (13) of the curve, formed at the intersection of the lateral
surface (12) of the blade (8) by the plane of the carrying disc (6) is substantially
an arc (25) of a circle (26) on the side of the entry tip (24), said arc being conjugated
with a portion (27) of a straight line (28) on the side of the forward tip (23) of
the blade (8), and the ratio of the square of the distance (l₂) between ends (29)
of said portion (13) of the curve to the difference of squares of the diameters (D₂,
D₁) of the circles (21, 22) passing respectively through the forward and entry tips
(23,24) of the blades (8) is within the range of from 0.15 to 0.22.
6. A centrifugal fan as claimed in Claim 5, characterized in that the ratio of the diameter (D₂) of the circle (24) passing through the forward
tips (23) of the blades (8) to the diameter (D₃) of the carrying disc (6) is within
the range of from 0.9 to 1.1.