[0001] The invention relates to a fan shroud according to the general clause of the claim.
This type of fan shroud is generally mounted on an automotive radiator, surrounding
an axial fan of a liquid cooled internal combustion engine in order to provide a safe
guard against a manual touch to the fan.
[0002] The main purpose of the fan shroud is to surround the axial fan thereby to prevent
peripheral air from entering into a cooled area. It also serves to increase a volume
of air flow passing through the radiator thereby to promote cooling efficiency of
the radiator.
[0003] Known fan configurations often bring about the problem of producing noise caused
by an acceleration of air flow towards a position between a tip edge of a high speed
rotating fan blade and a stationary shroud. From JP-A-58 200097 there are known wing
plates disposed such that they face the top of a rotating fan on its upstream side.
Their main purpose is to reduce the relative speed of fluid flow by changing the directions
of air streams towards the top edges of the fan blades. This means that they serve
as a deflector means for providing pre-vortex flows in advance. In short, they serve
as a noise reduction means. They cannot increase volumentric flow efficiency of the
fan.
[0004] Furthermore, air stream lines peel off the fan blade near an axial rear end of the
fan blade so that a turbulent flow or vortex having attendency to emit high frequency
noise is produced. It is believed that these vortex and turbulent flow obstruct the
air flow through the radiator thereby causing a considerable decrease of volume of
the air flow.
[0005] It is therefore an object of the invention to provide a high performance fan shroud
which does not only achieve a substantial decrease of noise emitted to the surroundings,
but even brings about a significant increase of a volume of air flow through the radiator.
[0006] According to the present invention this object is achieved by providing a fan shroud
having the features of the claim.
[0007] The arrangement of the mouth portion and fin plates according to the invention has
the result that irregular patterns of turbulent flow or spiral flow running against
the inside surface of the shroud are controlled and transformed into regular patterns
flying toward axial directions, so that air flow resistance is considerably reduced
and volumetric flow efficiency of the fan is improved. According to an experiment,
a remarkable improvement of 20 percent increase of air flow and 30 percent increase
of volumetric flow efficiency were demonstrated. With respect to the fan noise, although
it showed a slight rise of sound level, in view of the fact that the volume of air
flow also increases, it has been found that a fan noise per air flow is diminished
by about 10 percent. As a further advantage of the present invention, the fin plates
provide an additional rigidity to the shroud, so that not only durability of the shroud
is improved, but also a resonant noise is eliminated.
[0008] An embodiment of the invention will now be described by way of example with reference
to the drawings, in which:
Fig. 1 is a schematic vertical sectional view illustrating an arrangement of a fan
shroud according to the present invention.
Fig. 2 is a side elevational view of Fig. 1.
Fig. 3 is a cross-sectional view taken on line III - III of Fig. 1.
Fig. 4 is a graph showing curves of experimental values while changing an angular
orientation of the fin plates.
Fig. 5 is a graph showing curves of experimental values while changing a vertical
length of the fin plates.
Fig. 6 is a graph showing curves of experimental values while changing number of the
fin plates.
Fig. 7 is a graph showing curves of experimental values while changing a distance
between the fin plates and the radiator core.
Fig. 8 is a graph showing curves of experimental values while changing a midway folding
angle of the fin plates.
Fig. 9 is a graph showing curves of experimental values while changing a distance
between the rectangular fin plates and the fan blades.
Fig. 10 is a graph showing curves of experimental values while changing a distance
between the triangular fin plates and the fan blades.
[0009] Referring to Figs. 1 to 3, there is shown a preferable embodiment of a fan shroud
according to the invention. A radiator 10 comprises a core 12, a fan shroud 14, an
upper tank located above the core and a lower tank located below the core. These tanks
are not shown for illustrative simplification. A fan 30 comprises a plurality of fan
blades 32 and a fan hub 34 for supporting the blades. The fan hub 34 is usually mounted
on a fan drive shaft which is driven by an internal combustion engine. The fan shroud
14 comprises a rectangular base frame and a mouth portion 16, which extends from the
base frame coaxially with the central axis of the fan 30 and terminates at a position
passing over a portion of the outer circumference of the fan 30. The overlapped length
is represented by "U". In these figures, the mouth portion 16 is formed in a parallel
tubular form. However, it is also possible to make the mouth portion 16 in a tapered
form which is rather common to a fan shroud. While the fan 30 is driven by the engine
and rotated toward the direction R, cooling air is compulsorily admitted through the
radiator core 12.
[0010] On the inside surface of the mouth portion 16 of the shroud 14, eight fin plates
18 are circumferentially disposed at regular intervals. These fin plates 18 project
radially inwardly into the space between the fan 30 and the radiator core 12. As shown
in Fig. 1, each of the fin plates 18 is formed in a triangular shape in such a manner
that its vertical length decreases along the direction from the core 12 to the fan
30. Further, as shown in Fig. 2, each of the fin plates 18 is arranged in an imaginary
plane which contains the central axis of the fan 30. These triangular fin plates 18
have advantages that axial overall length of the radiator 10 can be minimized. The
fin plates 18 can be made without difficulty. When the shroud is made by a metallic
plate, the fin plates can be made by a metallic plate and then welded to the shroud.
When the shroud is made from plastic materials, the fin plates can be formed integral
with the shroud through an injection moulding process.
[0011] When cooling air passes through the axial fan 30, the air is usually directed toward
the direction of the arrow F. This air pressure force F can be divided into an axial
component Fx and a radial component Fy. Apparently, as the axial component Fx goes
up and as the radial component Fy goes down, loss of energy is saved. The radial air
flow defined by the component Fy runs against the inside surface of the shroud 14,
producing turbulent flow which shows a resistance to forthcoming air. If the fin plates
18 is disposed, random air flow is forced to the axial direction, whereby occurrence
of a turbulence is considerably reduced. In particular, since the fin plates 18 project
radially inwardly adjacent the fan blades 32, near the most efficient points of the
fan blades 32 air flow is controlled and regulated, whereby the volumetric flow efficiency
of the fan 30 is significantly improved. It is the basic principle of the present
invention.
[0012] As an actual example of the arrangement, following dimensions are available: The
outside diameter D of the fan 30 is 440mm, the width W of the fan 30 is 82mm, number
of fan blades 32 is nine, the inside diameter A of the mouth portion 16 is 500mm,
the axial length T of the mouth portion 16 is 120mm, the overlapped length U is 48mm,
the base length of the triangular fin plate 18 is 80mm, and the vertical length of
the fin plate 18 is 80mm. When the eight fin plates 18 are disposed at regular intervals
as shown in Fig. 2, the most satisfactory results are obtained.
[0013] The graphs in Figs. 4 to 10 show test results achieved in accordance with the Japanese
Industrial Standard B 8330 "Testing method for Turbo-Fans and Blowers". In these tests,
fan speed N was constantly kept to 2200 rpm.
[0014] In Fig. 4, four curves of experimental values are shown. The first curve 1 represents
a case of null fin. Other curves 2 to 4 represent respective cases while an angular
orientation of the fin plate 18 is changed from zero oblique angle, that is parallel
to the central axis of the fan, to 30 degrees oblique angle toward the same direction
as the twist of the fan blade (see Fig. 3), and to 15 degrees oblique angle contrary
to the direction of the twist of the fan blade. The experimental values are plotted
in relation to the volume of air flow Q and static pressure P. The curve S represents
a peculiar permeability of the radiator 10, that is a basic resistance to air flow
passing through the radiator. In the test, permeability coefficient k was 0.037. Actual
volume of air flow through the radiator is read from the intersecting points of the
air flow curve and the permeability curve. Thus, from the curve 1 actual volume is
read as 52.2 cubic meter per minute, and from the curve 2 actual volume is read as
63.2 cubic meter per minute. Therefore, according to the arrangement of the fin plates
18 at zero oblique angle, about 20 percent increase of air flow is attained. In other
two cases shown in curves 3 and 4, each volume of air flow becomes less than in the
curve 2. As a result, it is recognized that an oblique arrangement of the fin plate
18 cannot exhibit an advantage.
[0015] At the same time, a test of absorbing horsepower of the fan was achieved in order
to measure volumetric flow efficiency thereof. As a result, it has been proved that
about 30 percent increase of efficiency is attained.
[0016] In Fig. 5, five curves are shown. The first curve 1 represents a case of null fin.
Other curves 2 to 5 represent respective cases while a vertical length of the triangular
fin plate 18 is changed by cutting off the top portion thereof in horizontal stepwise.
From these curves following tendency is recognized: As the cut-off area increases,
an advantage of the fin plate is diminished.
[0017] In Fig. 6, six curves are shown. The first curve 1 represents a case of null fin.
Other curves 2 to 6 represent respective cases while the number of frusto-triangular
or trapezoidal fin plate is changed from four to sixteen. As a result, the curve 4
in case of eight fin plates is proved to be most advantageous.
[0018] In Fig. 7, four curves are shown. The first curve 1 represents a case of null fin.
Other curves 2 to 4 represent respective cases while a distance L between the radiator
core and the fin plate is changed in stepwise by cutting off the side portion of the
fin plate. It is recognized that air flow and static pressure are not affected by
the change of the distance L.
[0019] In Fig. 8, four curves are shown. The first curve 1 represents a case of null fin.
Other curves 2 to 4 represent respective cases while a midway folding angle of the
fin plate is changed from zero, to 30 degrees in clockwise direction, and to 30 degrees
in counterclockwise direction. In both cases in which the fin plate is folded in midway,
an advantage of the fin plate is diminished.
[0020] In Fig. 9, five curves are shown. The first curve 1 represents a case of null fin.
Other curves 2 to 4 represent respective cases while a distance between the rectangular
fin plate and the fan blade is changed by cutting off the side portion of the fin
plate. It is recognized that an advantage of the fin plate is diminished as the area
of the cut-off increases.
[0021] In Fig. 10, six curves are shown. The first curve 1 represents a case of null fin.
Other curves 2 to 6 represent respective cases while a horizontal distance between
the trapezoidal fin plate and the fan blade is changed. It is recognized that an advantage
of the fin plate is diminished as the distance increases.
[0022] In connection with a fan noise, an additional experiment was achieved under the conditions
that the fan speed is 1500 rpm, and the noise is measured at a high position of vertical
distance one meter from the central axis of the fan. As a result, in a case of null
fin 84.2 decibel was measured by scale A, and in a case of eight triangular fin plates
each having a base length 110mm and a vertical length 60mm, 86.9 decibel was measured
by scale A. Although the overall noise shows an increase of 3 percent, in view of
the fact that the volume of air flow also increases, it has been found that a fan
noise per volume of air flow is diminished from 1.6 to 1.4, thereby effecting a decrease
of 12.5 percent.
[0023] Improvements and modifications may be made to the present invention without departing
from the scope of the appended claim.
1. Lüfterzarge zum Leiten eines Luftstroms um einen axialen Lüfter (30) eines flüssigkeitsgekühlten
internen Verbrennungsmotors mit einem Kühler (10), durch den die Luft mittels des
Lüfters (30) gezogen wird, und mit Leitflügeln, die derart angeordnet sind, daß sie
der Oberseite des Lüfters (30) auf seiner stromaufwärts gerichteten Seite gegenüberstehen,
dadurch gekennzeichnet,
daß die Zarge einen Mündungsabschnitt (16) aufweist, der sich koaxial zur Mittelachse
des Lüfters (30) in einer parallelen oder konischen Form erstreckt und an einer Stelle
endet, an der er sich wenigstens über einen Abschnitt des Lüfters (30) erstreckt,
und daß die Leitflügel aus einer Vielzahl von flachen Leitblechen (18) bestehen, die
in Umfangsrichtung in regelmäßigem Abstand auf der Innenfläche des Mündungsabschnitts
(16) angeordnet sind und radial nach innen in den Zwischenraum zwischen dem Lüfter
(30) und einem Kern des Kühlers (10) ragen, wobei jedes Leitblech (18) derart dreieckig
oder trapezförmig geformt ist, daß seine vertikale Länge entlang der Richtung vom
Kern des Radiators (10) zum Lüfter (30) abnimmt, und wobei jedes Leitblech (18) in
einer imaginären Ebene angeordnet ist, welche die Mittelachse des Lüfters (30) enthält.