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| United States Patent Application |
20110309187
|
| Kind Code
|
A1
|
|
Dev; Sudarshan Paul
|
December 22, 2011
|
NESTED CORE GAS TURBINE ENGINE
Abstract
An aircraft, with the ability to cruise at supersonic speeds, designed to
increase cruise lift/drag ratio, reduce sonic boom and have greater
downward visibility by having an `inverted` nose profile that has greater
inclination of the lower surfaces to the flight direction than the upper
surfaces.
| Inventors: |
Dev; Sudarshan Paul; (Ashburn, VA)
|
| Serial No.:
|
219314 |
| Series Code:
|
13
|
| Filed:
|
August 26, 2011 |
| Current U.S. Class: |
244/36; 244/119; 244/129.3 |
| Class at Publication: |
244/36; 244/119; 244/129.3 |
| International Class: |
B64C 30/00 20060101 B64C030/00; B64C 23/00 20060101 B64C023/00 |
Claims
1. An aircraft for supersonic operation at least some of the time, said
aircraft having a nose pointing above the fuselage centerline, such that
the tip of the nose is above the fuselage centerline.
2. An aircraft for supersonic operation at least some of the time, said
aircraft having a nose region configured to have greater inclination to
the flight direction, during supersonic cruising flight, on its lower
surfaces as compared to its upper surfaces.
3. An aircraft for supersonic operation at least some of the time, said
aircraft having a nose region configured to have greater intensity of
inclined shock waves, during supersonic cruising flight, on its lower
surfaces as compared to its upper surfaces.
4. An aircraft for supersonic operation at least some of the time, said
aircraft having a nose region configured to have greater static pressure,
during supersonic cruising flight, on its lower surfaces as compared to
its upper surfaces.
5. An aircraft for supersonic operation at least some of the time, said
aircraft deriving net positive lift from the nose region during
supersonic cruise conditions.
6. An aircraft for supersonic operation at least some of the time, said
aircraft having greater cockpit window areas on the lower surface of the
nose rather than the upper surface of the nose.
Description
RELATED APPLICATION(S)
[0001] This application is a continuation from co-pending application Ser.
No. 12/537,045, filed Aug. 6, 2009, which is a continuation from Ser. No.
11/682,077, filed Mar. 5, 2007, which is a continuation from application
Ser. No. 11/201,441, filed Aug. 10, 2005 which is a continuation from
application Ser. No. 10/635,956 filed Aug. 7, 2003, now issued U.S. Pat.
No. 6,988,357, which is a continuation from application Ser. No.
09/947,002, filed Sep. 5, 2001, now issued U.S. Pat. No. 6,647,707, which
claims the benefit of U.S. Provisional Application No. 60/230,891, filed
Sep. 5, 2000, and of which are incorporated by reference herein in their
entireties.
FIELD
[0002] The disclosed embodiments relate to supersonic aircraft.
Previous Developments
[0003] Conventional supersonic aircraft, such as the Concorde, have a
sharp, needle-type, quasi-conical nose, that is designed to minimize the
strength of the shock waves formed when the aircraft is traveling at
supersonic speeds. This nose is generally somewhat angled down, looking
forward from the cockpit, to enable downward visibility for the pilots.
Examined another way, the tip of the nose, viewed from the side of the
profile, is located below the centerline of the fuselage behind the nose.
[0004] This conventional design of the nose for conventional supersonic
aircraft is not advantageous from the viewpoint of aerodynamic
performance. The quasi-conical nose acts as a supersonic ramp that
compresses oncoming air. Because the ramp is not axi-symmetric, the ramp
has a greater angle to the flight direction on a part of the surface,
such as the upper surface in a conventional aircraft, and has a smaller
angle to the flight direction on another part of the surface, such as the
lower surface in a conventional aircraft. The intensity of the supersonic
shock waves thus formed along the angled surfaces of the quasi-conical
nose are not symmetric with respect to the flight direction. Parts of the
curved surface of the nose that have a greater angle to the flight
direction have a greater intensity of shock, and other parts of the
curved surface of the nose have a lesser intensity of shock. It is well
known that a greater intensity of shock creates a greater increase in
static pressure of the flow, that is the pressure normal to the local
surface.
[0005] The shockwaves on the nose surfaces also create drag for the
aircraft, due to a combination of pressure drag and increased skin
friction drag.
[0006] In conventional aircraft, with the nose angled down from the
fuselage, the upper part of the nose has the greater intensity of shock
and the greater static pressure, compared to the lower part of the nose.
As a result, the nose experiences a net downward force.
BRIEF DESCRIPTION OF THE DRAWINGS
[0007] The foregoing aspects and other features of the exemplary
embodiments are explained in the following description, taken in
connection with the accompanying drawings, wherein:
[0008] FIGS. 1-1A respectively are a schematic cross-sectional view and a
schematic perspective cut-away view of a gas turbine engine incorporating
features in accordance with a first embodiment;
[0009] FIG. 1B is a perspective view of the gas turbine engine in FIG. 1;
[0010] FIG. 1C is a perspective view of the front section of an outer
casing of the turbine engine in FIG. 1;
[0011] FIG. 1D is a perspective view of a front rotor of the turbine
engine in FIG. 1;
[0012] FIG. 1E is a perspective view of a stator section of the turbine
engine in FIG. 1;
[0013] FIG. 1F is a perspective view of a rear rotor of the turbine engine
in FIG. 1;
[0014] FIG. 1G is a perspective cut-away view of a rear end portion of the
turbine engine in FIG. 1;
[0015] FIGS. 2A-2B are graphs respectively illustrating power/weight
ratios versus rated power, and specific fuel consumption (SFC) versus
rated power for small engines of the prior art;
[0016] FIG. 3 is a cross-sectional view of a gas turbine engine in
accordance with a second embodiment;
[0017] FIG. 4 is a graph showing variation of ignition delay time at a
number of air temperatures with respect to pressure in accordance with
the prior art;
[0018] FIGS. 5 and 6 are respectively schematic cross-sectional views of a
conventional engine with centrifugal compressors and wrap-around burners,
and a conventional engine with axial compressors and in-line burners;
[0019] FIGS. 7-10 respectively are schematic cross-sectional views of a
turbo-jet engine, turbo-fan engine, high-bypass ration turbo-fan engine,
and ultra-high bypass ratio turbo-fan engine in accordance with other
embodiments;
[0020] FIGS. 11-12 respectively are schematic cross-sectional views of the
propulsion systems of high speed air vehicles in accordance with still
other embodiments;
[0021] FIGS. 13 and 14-14A respectively are schematic top plan, elevation,
and bottom plan views of an unmanned aerial vehicle (UAV) in accordance
with yet another embodiment;
[0022] FIGS. 14B-14C respectively are schematic side elevation and rear
elevation views of the UAV in FIG. 13 in a first mode of operation (e.g.
cruise mode), and FIGS. 15A-15B respectively are schematic side elevation
and rear elevation views of the UAV in FIG. 13 in a second mode of
operation (e.g. hover mode);
[0023] FIGS. 16-17 are graphs respectively illustrating the relationship
of thrust to engine diameter and engine frontal area for field engines of
the prior art and gas turbine (nested core) engines according to the
exemplary embodiments;
[0024] FIG. 18-19 are graphs respectively illustrating SFC at rated thrust
versus operating pressure ration (OPR), and thrust versus OPR for field
engines of the prior art and gas turbine engines of the exemplary
embodiments;
[0025] FIGS. 20-21 are graphs respectively illustrating SFC at rated
thrust versus rated normal thrust, and length/diameter ratio versus
engine diameter for field engines of the prior art and gas turbine
engines of the exemplary embodiments;
[0026] FIGS. 22-23 are graphs respectively illustrating thrust versus
engine volume and bulk density (engine weight/cylindrical volume) versus
engine diameter for field engines of the prior art and gas turbine
engines of the exemplary embodiments;
[0027] FIGS. 24-25 are graphs respectively illustrating thrust versus
weight, and thrust/weight versus thrust for field engines of the prior
art and gas turbine engines of the exemplary embodiments;
[0028] FIG. 26 is a schematic cross-sectional view of a gas turbine engine
in accordance with another embodiment, particularly useful for a larger
(scaled-up) engine;
[0029] FIG. 27 is a schematic cross-sectional view of a gas turbine engine
in accordance with yet another embodiment, also particularly useful for a
larger (scaled-up) engine;
[0030] FIG. 28 is a schematic cross-sectional view of a gas turbine engine
in accordance with still another embodiment, also particularly useful for
a larger (scaled-up) engine;
[0031] FIGS. 29-29A are a schematic cross-sectional views of a gas turbine
engine in accordance with still other embodiments;
[0032] FIGS. 30A-30D are respectively schematic front elevation, plan,
rear elevation and side elevation views of a high speed air vehicle
embodiment according to the exemplary embodiments;
[0033] FIGS. 31A-31D are respectively schematic front elevation, plan,
rear elevation and side elevation views of the high speed air vehicle in
FIG. 30A; and
[0034] FIGS. 32A-32D are respectively schematic front elevation, plan,
rear elevation and side elevation views of another high speed air vehicle
embodiment according to the exemplary embodiments.
DETAILED DESCRIPTION OF THE EXEMPLARY EMBODIMENTS
[0035] FIGS. 30A-30D, 31A-31D and 32A-32D show examples of high-speed
aircraft embodiments 1000-1000' that use alternative embodiments of the
nested core engines in a lift-fan configuration, deriving benefit from
the short axial length of the nested core engines. Alternative aircraft
embodiments can be made using the nested core engines in similar aircraft
configurations.
[0036] The aircraft 1000, 1000' shown in FIGS. 30-32 has a nose 1010
pointing above the fuselage centerline, such that the tip 1012 of the
nose is above the fuselage centerline 1000CL (see FIG. 30D).
[0037] The aircraft shown in FIGS. 30-32 has a nose region 1014 configured
to have greater inclination a to the flight direction (indicated in by
arrow V in FIG. 30D, during supersonic cruising flight, on its lower
surfaces 1014L as compared to its upper surfaces 1014U.
[0038] The aircraft shown in FIGS. 30-32 has a nose region 1014 configured
to have greater intensity of inclined shock waves, during supersonic
cruising flight, on its lower surfaces 1014L as compared to its upper
surfaces 1014U.
[0039] The aircraft shown in FIGS. 30-32 has a nose region 1014 configured
to have greater static pressure, during supersonic cruising flight, on
its lower surfaces 1014L as compared to its upper surfaces 1014U.
[0040] The aircraft shown in FIGS. 30-32 is configured to derive net
positive lift (indicated by arrow V in FIG. 30) from the nose region 1014
during supersonic cruise conditions.
[0041] The aircraft shown in FIGS. 30-32 has greater cockpit window areas
1014W on the lower surface 1014L of the nose rather than the upper
surface 1014U of the nose 1010.
* * * * *