[0001] This invention relates to compressors for air or other gases and more particularly
to centrifugal or radial flow compressors in which rotating blades are situated in
a flow passage that increases in diameter towards its outlet end.
[0002] Compressors which employ rotating vanes or blades may be divided into two broad categories
on the basis of the configuration of the air flow passage. Centrifugal or radial flow
compressors, which constitute the first category, have a flow passage which increases
in diameter in the direction of the air flow. Axial flow compressors form the second
category and have a flow passage of constant or almost constant diameter.
[0003] Centrifugal compressors are basically simpler, more compact and less costly than
those of axial flow form. These characteristics are highly desirable in many compressor
usages such as in gas turbine engines and engine turbo chargers, but heretofore, it
has been necessary to tolerate a relatively low isentropic efficiency in order to
gain the benefits of these advantages. The relatively low efficiency typical of prior
centrifugal compressors results from the fact that such mechanisms are single stage
devices except where a lengthy and complex construction, involving what amounts to
a series of such compressors coupled in tandem, is resorted to.
[0004] A single compressor stage consists of a set of revolving compressor blades followed
by at least one set of diffuser blades which may be stationary or contra -rotating.
A set of diffuser blades in addition to a set of compressor blades is required to
form a compressor stage since a sizable proportion of the energy imparted to incoming
air by the revolving set of compressor blades is initially tangential energy of motion
of the air flow. To complete the compression process the air flow must then pass through
at least one set of diffuser blades oriented at a different angle than that of the
compressor blades to convert the tangential velocity energy into static pressure head.
[0005] The degree of compression accomplished in a rotary compressor is expressed by the
pressure ratio which is the ratio of pressure at the outlet to that at the inlet.
A high pressure ratio across a single compressor stage requires a high loading on
the compressor blades, the blade loading being quantitatively expressed by the diffusion
factor at a calculated design point. Where sizable pressure ratios are to be achieved
in a single stage device. The design point diffusion factor must necessarily be high.
Isentropic efficiency, which is an inverse function of the diffusion factor, is therefore,
necessarily, low.
[0006] The high efficiency of many axial flow compressors largely results from the common
practice of employing a series of stages in such compressors. An axial flow compressor
may typically have several sets of compressor blades alternating with sets of diffuser
blades along the axial flow path, each set of compressor blades in conjunction with
a following set of diffuser blades constituting an individual stage. In such a device,
the overall pressure ratio of the compressor is the product of the lower pressure
ratios of the individual stages of the series. As each stage individually has a low
pressure ratio, each stage operates at high efficiency and the efficiency of the compressor
as a whole is also high.
[0007] Prior applications of the multiple staging principle to centrifugal compressors have
gained efficiency at the cost of sacrificing much of the inherent advantages of the
centrifugal compressor configuration. More particularly, most prior multi-staged centrifugal
compressors have as a practical matter included a series of essentially separate single
stage centrifugal compressors connected together in tandem through bulky and complex
air ducting for channeling the outlet flow from one stage radially inward to the smaller
diameter inlet of the next subsequent stage. This results in a lengthy, complex and
costly construction such as is found in axial flow compressors.
[0008] Prior centrifugal compressors also exhibit other problems apart from a relatively
low efficiency where a high pressure ratio is to be realized. Designing for a high
pressure ratio in a single staged compressor results in extremely high tangential
air velocity behind the single long set of compressor blades. This is turn dictates
that a bulky and heavy diffuser structure, including lengthly diffuser blades and
a voluminous diffusion chamber, be provided at the outlet.
[0009] A further practical problem encountered in prior centrifugal compressors arises from
the fact that different compressor usages require different pressure ratios and flow
capacities. If each compressor model in a family of compressors of different pressure
ratio and capacities must be manufactured with a large number of distinct parts usable
only in the one particular model, the cost of manufacture of the line of compressors
as a whole is increased.
[0010] According to the present invention a multi-stage centrifugal compressor having relatively
rotatable inner and outer elements defining an annular flow path of progressively
increasing diameter from an inlet end to an outlet end of the compressor, is characterized
in that a plurality of blading means are provided in the flow path to define a plurality
of compression-diffusion stages, each of the stages having a design point diffusion
factor below about 0.55.
[0011] By providing a series of sets of compressor blades alternated with sets of diffuser
blades within a radial flow path of progressively increasing diameter, the efficiency
of a centrifugal compressor is greatly increased while preserving the compactness
of prior centrifugal compressors and while preserving much of the structural simplicity
as well. For a given pressure ratio and flow capacity, gains in efficiency may in
fact exceed those realized in multiple stage axial flow compressors having a similar
number of stages as centrifugal effects aid the blade action in generating a pressure
rise. Consequently, fewer internal stages may be needed to achieve a given pressure
ratio with a given energy input.
[0012] As diffusion is largely accomplished internally in stages, a large diffuser is not
necessarily needed at the outlet of the compressor. Thus the invention may be relatively
compact in the diametrical direction relative to prior centrifugal compressors. In
addition, the multi-staged construction enables the manufacture of a family of centrifugal
compressors of different pressure ratio and/or flow capacity without requiring a large
number of different structural elements for each model.
[0013] In instances where the multi-stage centrifugal compressor is a component of a gas
turbine engine, an engine turbocharger, or the like, the high efficiency of the multi-stage
compressor significantly reduces power losses in such apparatus as a whole.
[0014] Various examples of compressors according to the invention will now be described
with reference to the accompanying drawings in which:-
Figure 1 is a broken out side elevation view of a first embodiment of a centrifugal
compressor constituting the air intake component of a gas turbine engine.
Figure 2 is an enlarged axial section view of a portion of the air compressor of Figure
1.
Figure 3 is a broken out perspective view of the impeller and stator portions of the
air compressor of Figures 1 and 2 further illustrating blading structure within the
compressor.
Figure 4 is a view taken along curved line IV-IV of Figure 2 illustrating the configurations
and relative inclinations of the blades of successive stages within the air compressor
of the preceding figures.
Figure 5 is a graph depicting input power losses as a function of blade loading or
diffusion factor in the present invention and in typical prior air compressors.
Figure 6 is an axial section view of a'portion of an air compressor basically similar
to that of Figure 2 but with modifications of the blading structure to vary the air
flow capacity.
Figures 7A to 7G are diagrammatic views illustrating further modifications of the
compressor of Figure 1 which enable realization of any of a series of different pressure
ratios and/or flow capacities utilizing much of the same basic structural components.
Figure 8 is an axial view of an engine turbocharger having a compressor section in
accordance with an embodiment of the invention.
[0015] Referring initially to Figure 1 of the drawings a radial flow or centrifugal compressor
11 has an impeller 12 disposed for rotation within an annular stator member 13 respectively
constituting relatively rotatable inner and outer elements that jointly define an
annular flow path 14.
[0016] Impeller 12 is of progressively increasing diameter from the air inlet end 16 of
the flow path 14 towards the air outlet end 17. Stator member 13 has an inner diameter
which also progressively increases along the flow path 14 but at a lesser rate so
that the spacing of the impeller from the stator diminishes towards the outlet end
17 of the flow path. The diminishing spacing of the impeller 12 from stator member
13 along flow path 14 compensates for the progressively increasing diameter of the
flow path towards the outlet end which would otherwise cause the flow path to have
a progressively increasing cross-sectional area. The decrease in spacing also compensates
for the air compression that occurs along the flow path-14 and which progressively
reduces the volume occupied by unit mass of air as it travels along the path.
[0017] In the embodiment of the invention depicted in Figure 1,' compressor 11 constitutes
the air intake component of a gas turbine engine 18 and certain structural features
of this particular compressor 11 are specialized for this context. For example, the
impeller 12 is supported on and driven by a forward extension of the main shaft 15
of the gas turbine engine 18 and the inner stator member 13 is secured to an outer
stator member 19 which is itself secured to the main housing 21 of the gas turbine
engine and supported thereby.
[0018] Aside from the air intake section defined by the compressor 11, the gas turbine engine
18 may be of a known design such as that described in prior United States Patent 4,030,288
and therefore will not be further described except for certain components which directly
coact with elements of the compressor. It should be understood that usage of a compressor
embodying the invention is not limited to the context of gas turbine engines. When
the invention is employed in other contexts or for other purposes, the impeller 12
may be journaled within the stator members 13 and 19 by suitable bearing structures
known to the art and may be driven by any of a variety of known external motors. Similarly,
the stator may be provided with appropriate support means of any of various known
forms.
[0019] The inner and outer stator members 13 and 19 jointly form an annular diffusion chamber
22 which ' receives air from the outlet end 17 of the compressor flow path 14. In
order to minimize the size of the compressor in the radial direction, outer stator
member 19 is shaped to situate most of the volume of diffusion chamber 22 adjacent
the smaller diameter forward portion of inner stator member 13. This is a practical
configuration in that the lengthy, radially extending diffuser vanes required at the
outlet end of the flow path in many conventional single stage centrifugal compressors
are not necessarily required in the present invention.
[0020] Diffusion chamber 22 is communicated with a . compressed air outlet tube 23 which
in the present example supplies the compressed air to the combustor 24 of the gas
turbine engine 18 through a heat exchanger module 26 which transfers heat from the
exhaust of the engine to the incoming compressed air. In instances where the compressor
11 is used for purposes other than in a gas turbine engine, the outlet tube 23 may
be replaced with a hose or other conduit means suitable for connection with the compressed
air utilizing device.
[0021] Compression of air within the flow path 14 is accomplished by blading means 27 depicted
on a larger scale in Figure 2, which form a plurality of internal compression-diffusion
stages 30a to 30f of low blade loading or diffusion factor within the flow path 14.
[0022] Referring now to Figures 2 and 3 in conjunction, a plurality of spaced apart sets
of compressor blades 28 extend radially from impeller 12 into the flow path 14, there
being six such sets 29a, 29b, 29c, 29d, 29e, 29f of compressor blades, proceeding
from the air inlet end 16 to the air outlet end 17, in this example. The individual
compressor blades 28 of each set 29a to 29f are equiangularly spaced around the rotational
axis of the impeller 12 and owing to the progressively diminishing thickness of the
flow path 14, the blades of each successive set extend progressively smaller distances
from the impeller.
[0023] A plurality of spaced apart stationary sets of diffuser blades 31.extend into flow
path 14 from the inner stator member 13, there being seven sets 32a, 32b, 32c, 32d,
32e, 32f, 32g of diffuser blades 31 in this example. The sets 32a to 32g'of diffuser
blades are alternated with the sets 29a to 29f of compressor blades 28 except that
the two final sets of diffuser blades 32f and 32g are both behind the final set 29f
of compressor blades. Individual blades 31 of each set 32a to 32g of diffuser blades
are also equiangularly spaced apart with respect to the rotational axis of the compressor
and the blades of each successive set 32a to 32g extend progressively shorter distances
from the stator member to accommodate to the progressively diminishing thickness of
the flow path 14.
[0024] Each set 29a to 29f of compressor blades in conjunction with the following set of
diffuser blades 31 constitutes one of the plurality of compression-diffusion stages
30a to 30f situated in the flow path 14. Thus in the present example compressor blade
set 29a and diffuser blade set 31a form a first compression-diffusion stage 30a and
compressor blade set 29b in conjunction with diffuser blade set 32b form a second
compression-diffusion stage 30b, there being six such stages in this example.
[0025] Referring now to Figure 4, the individual compressor blades 28 of each set 29a to
29g are inclined relative to the rotational axis 18' of the impeller to impart an
increment of flow velocity to intercepted air as the blades turn in the direction
indicated by arrows 33 in the drawing. The compressor blades 28 of each successive
set 29a to 29g have a progressively increasing angulation relative to axis 18' to
accommodate to the progressive increase of free stream velocity which occurs along
the flow path. The blades 31 of the successive sets 32a to 32g of diffuser blades
have an opposite angulation relative to axis 18', which also becomes progressively
greater for each successive set of diffuser blades, in order to convert tangential
velocity energy imparted to air by the preceding_set of compressor blades into static
pressure head energy.
[0026] Thus, with reference to Figures 1 and 2, the compression achieved by compressor 11
as a whole is accomplished in six distinct compression-diffusion stages .30a to 30f
along the flow path 14. The pressure ratio of each individual stage 30a to 30f may
therefore be low relative to a conventional centrifugal compressor having a single
long set of compressor blades followed by a single long set of diffuser blades, designed
to accomplish the same degree of compression. Since each component stage 30a to 30f
of compressor 11 operates at a low pressure ratio and therefore a high level of efficiency,
the aggregate efficiency of the several stages in combination is itself high in comparison
with conventional single staged devices.
[0027] In order to fully realize the gains in efficiency inherent in the multiple stage
construction, each compression-diffusion stage 30a to 30f is designed to have a free
stream flow velocity which is below supersonic throughout the region of blading means
27 and to have a diffusion factor below about 0.55 at each stage. As is known in the
art, the diffusion factor of a single compression-diffusion stage may be selected,
within limits, by an appropriate fixing of the shape, angulation and number of compressor
blades and diffuser blades in relation to the configuration of the flow path and the
rotational velocity of the compressor blades. More particularly, in a compressor stage
wherein the free stream air velocity is subsonic throughout the region of the blading
as is the case in the compressors of the present invention, diffusion factor (D.F.)
is given by the expression:
where: V1 = inlet flow velocity relative to blade row
V2 = outlet flow velocity relative to blade row
Ve = tangential flow velocity relative to . blade row
d = blade row solidity (proportion of open flow space to total cross-sectional, area
of flow path in blade region)
[0028] The benefit of establishing a design point diffusion factor below about 0.55 at each
of the several compression-diffusion stages 30a to 30f may be.seen by referring'to
Figure 5 which is a graph depicting measured input energy losses, that is energy which
does not become available as pressure energy at the outlet of the compressor, as a
function of diffusion factor for three different types of rotary compressor all of
which achieve the same overall pressure ratio or degree of compression. Rectangles
34 designate measured losses for a conventional single stage centrifugal compressor
which necessarily must have a relatively high diffusion factor to accomplish the desired
degree of compression in the single stage. Circles 36 indicate the relatively low
measured losses in a conventional.multiple stage axial flow compressor in which the
diffusion factor for each individual stage may be much lower and therefore more efficient.
Triangles 37 indicate the measured losses in a multiple stage centrifugal compressor
embodying the present invention. It should be observed that the compression is accomplished
in the present invention with a diffusion factor 37 per stage which is substantially
lower than that 36 of the lengthier and more complex axial flow compressor. The reason
for this greater efficiency of the present invention as indicated by triangles37 is
believed to be'that centrifugal force supplements the direct effect of the blading
in.' achieving compression. This effect does not occur in the non-radial flow path
of an axial flow compressor.
[0029] The significance of a design point diffusion factor value of about 0.55 as an upper
limit for the individual stages of the present invention is also evident in Figure
5. It may be seen that there is not a linear relationship between power loss and diffusion
factor. Instead, as the diffusion factor is increased from a very low value, losses
rise at a relatively moderate rate, indicated by lines 38, until a value of about
0.55 is reached. Thereafter losses increase much more sharply with increasing diffusion
factor as indicated by lines 39. Efficiency is an inverse function of power losses
and thus it may be seen that efficiency drops off relatively sharply after the diffusion
factor value of about 0.55 is passed.
[0030] Returning to Figure 1, the high efficiency of the compressor 11 in turn increases
efficiency of the gas turbine engine 18 itself as power losses in the compressor section
of the engine are reduced. As compared with a gas turbine engine utilizing an axial
flow compressor configuration for the purpose of realizing somewhat comparable efficiencies,
the engine 18 of this example is much more compact and the compressor section is simpler
and less costly.
[0031] While the compressor 11 described above is provided with six internal compression-diffusion
stages 30a to 30f, varying numbers of stages may be provided by changing the number
of sets of compressor blades 28 and diffuser blades 31. Moreover, the construction
readily lends itself to manufacture of a family of compressors of different pressure
ratio and/or flow capacities by varying only the number and disposition of the sets
of blades 28 and 31 within the flow path 14 while otherwise utilizing identical components
for the several compressor models. Referring to Figure 6 for example, a compressor
11' having a lower pressure ratio but a smaller air mass flow rate and therefore a
smaller driving power requirement may be produced simply by removing the first set
29a of compressor blades and the first set 32a of diffuser blades, shown in phantom
in Figure 6, while otherwise utilizing components, such as impeller 12 inner stator
member 13 and outer stator member 19 identical to those of the previously described
embodiment. In general, the elimination of compression-diffusion stage blading means
27 from the air inlet 16 region of the flow path 14 has an effect of reducing both
air mass flow and pressure ratio while the elimination of stages of blades from the
region nearest the air outlet end 17 has the predominate effect of reducing pressure
ratio. Adding of stages at the inlet end increases mass flow and pressure ratio while
additional stages near the outlet end predominately raise pressure ratio.
[0032] Thus while a limited number of specific blading modifications will be described with
reference to Figures 7A to 7G and specific parameters will be given, such examples
are not exhaustive of the possible modification. In accordance with the above' discussed
relationships, other modifications may be made to provide other mass flows and pressure
ratios.
[0033] Figures 7A to 7C diagramatically illustrate how a series of compressors lla, llb,
llc respectively of different pressure ratio and/or air flow capacity may be configured
by simply varying the numbers of sets of blades in the air flow path while otherwise
utilizing identical components. Where the compressors are embodied.in gas turbine
engines as previously described, this enables production of a family of engines 18a,
18b, 18c of different output power rating and fuel consumption requirements simply
by varying the blading in the compressor section.
[0034] While the gas turbine engines 18a, 18b and 18c may be of known construction apart
from the compressors lla, llb, llc, the coaction of the compressor sections with the
other portions of the engines may best be understood by briefly reviewing certain
basic structure of such engines. Referring specifically to Figure 7A, for example,
such engines 18a have a fuel burning combustor 24a receiving compressed air from compressor
lla through heat exchanger 26a. Output gasses from the combustor 24a drive a gasifier
turbine 42a that turns the impeller 12a of the compressor lla. Nozzle vanes 43a direct
the gas flow from combustor 24a and gasifier turbine 42a to a power turbine 44a which
turns the engine output shaft 46a, the exhaust gas from the power turbine being discharged
through the heat exchanger 26a to preheat the compressed air which is delivered to
the combustor.
[0035] The modified compressor lla of Figure 7A is similar to that previously described
with reference to Figure 2 except that the first two compression-diffusion stages
30a, 30b have been eliminated by removing the first two sets 29a and 29b of compressor.
blades 28 and the first two sets 32a and 32b of diffuser blades 31. As a result of
this simple modification, the compressor lla of Figure 7A has a lower air flow and
a lower pressure ratio of about 4.5. The output power rating of the gas.turbine engine
18a is then typically about .894 kW. realized with a fuel efficiency of less than
about 0.4 brake specific fuel consumption (BSFC).
[0036] Figure 7B illustrates a gas turbine engine 18b of substantially greater output power
rating but which may be structurally identical to that of Figure 7A except for another-modification
of the blading structure within the compressor llb. Compressor llb is similar to the
compressor 11 of Figure 2 except that the first and final sets 29a and 29g of compressor
blades of Figure 2 and the first and final two sets 32a, 32f, 32g of diffuser blades
31 have been eliminated. The pressure ratio achieved by the compressor llb of Figure
7B remains approximately the same as that of Figure 7A but the volume of air passing
through the compressor llb of Figure 7B and on to the combustor 24b is increased to
the extent that the power output of the turbine engine 18b is now about 149 kW.
[0037] Figure 7C depicts another modification, confined to the blading means 27c of the
compressor, by which a similar basic gas turbine engine 18c including similar impeller
12c and stator member 13c elements in the compressor may be used to produce an engine
of still higher rated output power. The compressor llc of gas turbine engine 18c is
identical to that of the first described embodiment of Figure 2 except that the final
set 29f of compressor blades of Figure 2 have been removed and the final two sets
32f and 32g of diffuser blades are now situated more forwardly in the flow passage
and configured for that changed location. This makes the pressure ratio of the compressor
llc of Figure 7C about 6.5 and provides an increase of volumetric air flow relative
to the Figure 7B embodiment. The rated power output of the gas turbine engine 18c
of Figure 7C is typically about 2609 kW.
[0038] If the modifications of the compressor blading arrangements are accompanied by modifications
of other components as well, the family of gas turbine engines may be extended to
still higher output power ratings, examples of which are depicted in Figures 7D, 7E,
and 7F. Referring initially to Figure 7D, by forming the impeller 12d and inner stator
member 13d to be relatively elongated at the front end 16d, additional compression-diffusion
stages, such as stage 30g, may be provided at the air inlet end of the compressor
lld to further increase rated power output of the engine 18d. Thus the compressor
lid of Figure 7D has an additional set of compressor blades 29g followed by an additional
set 32h of diffuser blades at the front end of the air flow path 14d. The final two
sets of compressor blades 29e and 29f of the embodiment of Figure 2 and the intermediate
set of diffuser blades 32e have been removed. The final two sets of diffuser blades
32f and 32g are again situated more forwardly in the flow passage and have configurations
appropriate to that portion of the passage. With these modifications, the pressure
ratio of the modified compressor lld of Figure 7D remains at about 6.5 but air mass
flow is sizably increased causing the rated power output of the gas turbine engine
18d to be increased to about 3728 kW.
[0039] By making Somewhat more extensive modifications, still greater power output ratings
may be obtained. For example as depicted in Figure 7E an auxiliary compressor section
47e may be added between the primary compressor lle and the heat exchanger 26e. The
auxiliary compressor section 47e may for example have two spaced apart sets 48e and
49e of compressor blades on an auxiliary impeller 50e each being followed by a set,
51e and 52e respectively of diffuser blades. An annular air duct 53e is provided to
receive the output flow from the primary compressor section lle and to return the
flow radially inward for delivery to the air inlet end of the auxiliary compressor
section 47e. Primary compressor section lie is itself identical to the compressor
lld of the previous Figure 7D. To best realize.the advantages of the compressor modification
of Figure 7E, other elements of the gas turbine engine 18e are modified to the extent
of providing an additional gasifier turbine stage 54e to drive the impeller 50e of
the auxiliary compressor stage 47e. The modifications depicted in Figure 7E produce
an overall compressor pressure ratio of about 12 and raise the rated power output
of the gas turbine engine 18e to about 4100 RW.
[0040] Figure 7F illustrates still a further modification of the gas turbine engine 18f
in which the structure remains similar to that described above with reference to Figure
7E except that in the embodiment of Figure 7F the annular air duct 53f which communicates
the primary compressor section llf with the auxiliary compressor section 47f includes
an intercooler or heat exchanger 55f which acts to cool the compressed air in passage
between the two compressor sections. Intercooling reduces the amount of power required
to drive a compressor and this power reduction is reflected in an increased power
output at the output shaft 46f of the gas turbine engine 18f. By this further modification,
the gas turbine engine 18f is made to deliver about 4846 kW.
[0041] Referring now to Figure 7G the power output and therefore the fuel consumption rate
of any of the gas turbine engines described above may be adjusted downwardly as desired
by disposing a set of air flow reducing stator vanes 56g in the inlet end of the air
flow path 14g in front of the initial set 29g of compressor blades 28g. Stator blades
56g are angled relative to the air flow path 14g in order to constrict the air flow
path and thereby reduce air mass flow to any desired extent.
[0042] As previously pointed out, the invention is not limited to compressors which function
as an air intake component of gas turbine engines, but may also advantageously be
utilized in free standing compressors for supplying compressed air to various pneumatic
systems or to other mechanisms which include a compressor as one component. Figure
8 illustrates an example of the latter category in which a compressor llh embodying
the invention constitutes an air intake component of a turbocharger 57 for an internal
combustion engine 58.
[0043] A turbocharger 57 increases the fuel efficiency of the engine 58 by boosting intake
manifold pressure and uses energy recovered from the exhaust gas of the engine for
this purpose. More specifically, the turbocharger includes'a turbine 59 driven by
the engine exhaust flow and which drives the compressor llh that supplies compressed
air to the engine 58 intake manifold. Centrifugal compressors, preferably in combination
with a centripetal turbine, are advantageous in turbochargers in view of the basic
compactness and structural simplicity of such compressors but if a conventional single
stage centrifugal compressor is used, the adiabatic efficiency of the turbocharger
is undesirably limited. This adversely affects the power output of the associated
engine 58 per unit of fuel consumed. Very high efficiency together with simplicity
and compactness in both the axial and radial direction can be realized by embodying
a multi-stage radial flow compressor llh in accordance with present invention in a
turbocharger 57.
[0044] The compressor llh and turbine 59 are secured to opposite ends of a'housing 61 which
journals a drive shaft 62 that defines the rotational axis of both the compressor
and turbine.
[0045] Compressor llh has an annular outer stator member 19h secured to the front end of
housing 61 in coaxial relationship with the drive shaft 62 and which defines a broad
air intake passage 64. Stator member 19h also forms a volute or annular collection
chamber 66 which is communicated with intake manifold 67 of engine 58, the collection
chamber being coaxial with intake passage 64 and being of greater diameter. A rotatable
impeller 12h is supported on the forward end of drive shaft 62 within stator member
19h and in conjunction with an inner.stator member 13h forms an annular air flow path
14h leading from air intake passage 64 to collection chamber 66. Impeller 12h and
inner stator member 13h have configurations which cause the air flow path 14h to be
of progressively increasing diameter in the direction of air flow while being of progressively
diminishing thickness towards the air outlet end.
[0046] Multi-stage blading means 27h of the type previously described is situated within
the flow path l4h to provde a plurality of sub-sonic internal compression-diffusion
stages 30j, 30k, 30L each having a design point diffusion factor below about 0.55.
In this example, the blading means 27h includes three spaced apart sets of compressor
blades 28h secured to impeller 12h and alternated with three spaced apart sets of
diffuser blades 31h secured to stator member 13h. Thus three compression-diffusion
stages 30k, 30j, 30L are provided in this embodiment each being defined by a set of
compressor blades 28h and the immediately following set of diffuser blades 31h.
[0047] While the multi-staged compressor llh is advantageous in a turbocharger employing
any of a variety of different types of turbine 59, very high efficiency is best realized
by using a centripetal turbine 59 which is also of a multi-staged construction.
[0048] The turbine 59 of this example has an annular stator 76 secured to the back end of
housing 61 and forming an exhaust gas outlet passage 77. A turbine rotor 78 is secured
to the back end of drive shaft 62 in coaxial relationship with the shaft and in conjunction
with an annular inner stator member 79 forms a gas flow path 81 which is of progressively
less diameter but progressively increasing thickness from a gas inlet end 82 to a
gas discharge end 83.
[0049] Stator 76 also forms an annular volute or gas receiving chamber 84 which is communicated
with the inlet end 82 of gas flow path 81 and which is also communicated with the
exhaust gas manifold 86 of engine 58. To cause the exhaust gas flow to drive the turbocharger
57, three spaced apart sets 87a, 87b, 87c of rotor vanes are secured to rotor 78 and
extend into the flow path 81, the rotor vanes being angled with respect to the direction
of gas flow. To maximize the reaction forces of the gas flow on the rotor vanes 87a,
87b and 87c, one of three sets 88a, 88b and 88c of stator vanes precedes each set
of rotor vanes 87a, 87b and 87c respectively along the gas flow path. As the pressure
drop at each individual set of rotor vanes 87a, 87b and 87c is substantially lower
than the total pressure drop through the turbine 59 as a whole, each set of vanes
operates at a relatively high efficiency in comparison with a single stage centripetal
turbine having a single long set of rotor vanes.
[0050] The above described turbocharger 57 construction enables the impeller 12h and rotor
78 to be situated on the same shaft 62 to turn at the same speed and in most cases
the two elements need not have any large disimilarity in diameters. With the rotational
speeds and diameters of both the impeller 12h and rotor 78 closely matched, centrifugal
stresses are also closely balanced at a high but tolerable level to optimize air and
gas throughput in relation to the size and weight of the turbocharger.
[0051] In the operation of the embodiment of the invention depicted in Figures 1 to 3, impeller
12 of the compressor 11 is turned by the gas turbine engine main shaft 18. The resulting
rotary motion of the several sets 29a to 29f of compressor blades causes air to be
drawn into inlet end 16 and to be forced along flow path 14 to the diffuser chamber
22 from which it is transmitted to the fuel combustor 24 of the engine 18 through
tube 23 and heat exchanger module 26.
[0052] Air is compressed in stages during passage through flow path 14 as each set of compressor
blades 29a to 29f imparts additional energy to the air flow. At each successive set
29a to 29f of compressor blades the added energy appears in part as a rise of static
pressure, in part as tangential velocity energy of motion and to some extent as heat.
The set 32a to 32g of diffuser blades 31 situated behind each set 29a to 29f of compressor
blades converts a substantial portion of the velocity energy into additional static
pressure. This process of compression followed by diffusion is repeated at each successive
compression-diffusion stage 30a to 30f and since the pressure ratio at each successive
stage is substantially less than the pressure ratio of the compressor as a whole,
each individual stage operates at high efficiency and the overall compression process
is therefore highly efficient.
[0053] Where the compressor 11 is an air intake component of a gas turbine engine 18 as
in this example, the gains in efficiency in the operation of the compressor translate
into increased efficiency of the gas turbine engine itself. To the extent that power
losses in the compressor 11 are reduced, the deliverable power output of the gas turbine
engine 18 is increased. Moreover the compressor 11 is very compact in both the axial
and radial direction enabling the gas turbine engine 18 as a whole to also exhibit
a very desirable degree of compactness.
[0054] Significant aspects of the operation of the compressors lla to llg of the gas turbine
engines 18a to 18g of Figures 7A to 7G are essentially similar except insofar as different
pressure ratios and air mass flows and therefore different output power ratings for
the gas turbine engines are realized in the manner hereinbefore described.
[0055] In the operation of the turbocharger 57 of Figure 8, the exhaust gasses from engine
58 drive turbine 59 which in turn drives the compressor llk through drive shaft 62.
The blading means 27h of the compressor llk draws air into flow path 14h and delivers
such air to the intake manifold 67 of the engine 58 through diffusion chamber 66.
Again, the multiple staged blading means 27h of the compressor llh enables the compression
and diffusion process to be accomplished in stages each of which individually exhibits
a small pressure ratio and low diffusion factor thereby providing for high efficiency
in the operation of the compressor llh and thus in the operation of the turbocharger
57 as a whole.
1. A multi-stage centrifugal compressor (11) having relatively rotatable inner (12)
and outer (13) elements defining an annular flow path (14) of progressively increasing
diameter from an inlet end (16) to an outlet end (17) of the compressor, characterized
in that a plurality of blading means (27) are provided in the flow path to define
a plurality of compression-diffusion stages (30 a-f), each of the stages having a
design point diffusion factor below about 0.55.
2. A compressor (11) according to claim 1, having a free stream flow velocity, relative
to the blading means (27) which is below supersonic through the blading means (27).
3. A compressor (11) according to claim 1 or claim 2, wherein the blading means (27)
includes a plurality of sets (29a to 29b) of compressor blades (28) extending into
the flow path (14) from a first of the elements (12, 13) and a plurality of sets (32a
to 32b) of diffuser blades (31) extending into the flow path (14) from the second
of the elements (12, 13), the sets of diffuser blades being alternated with the sets
of compressor blades along the flow path (14).
4. A compressor (11) according to claim 3, wherein the first element is the inner
element (12) and the second element is the outer element (13).
5. A compressor (11) according to claim 4, wherein the inner element (12) is a rotatable
impeller of progressively increasing outside diameter from the inlet end (16) to the
outlet end (17) of the flow path (14), and wherein the outer element (18) is a non-rotatable'stator.
member of progressively increasing inside diameter from the inlet end (16) to the
outlet end (17) of the flow path (14).
6. A compressor (11) according to any of claims 3 to 5, wherein the outward curvature
of the annular flow path (14) relative to the rotational axis of the compressor becomes
progressively greater from the inlet end (16) to the outlet end (17), and wherein
the flow path (14) is of progressively diminishing cross-sectional area from the inlet
end (16) to the outlet end (17), successive ones of the sets (29a to 29h) of compressor
blades and sets (32a to 32h) of diffuser blades have blades (28, 31) of progressively
decreasing size.
7. A compressor (11) according to any of claims 3 to 6, wherein successive ones of
the sets (29a to 29h) of compressor blades (28) and the sets (32a to 32h) of diffuser
blades (31) each have a progressively increasing number of individual blades from
the inlet end (16) to the outlet end (17) of the flow path.
8. A compressor (11) according to any of claims 1 to 7, further comprising vane means
(56) for restricting the rate of air flow into the compressor (11) at the air inlet
end (16) of the flow path (14).
9. A compressor (11) according to any of claims 1 to 8, in combination with a gas
turbine engine (18), wherein the compressor (11) constitutes the air intake element
of the gas turbine engine and wherein the impeller (12) is driven by the engine (18).
10. A compressor (llh) according to any of claims 1 to 8, in combination with an engine
turbocharger (57) turbine (59), wherein the compressor (llh) constitutes the air intake
element of the turbocharger (57) and is driven by the turbine (59).