TECHNICAL FIELD
[0001] The present disclosure relates to gas compressors and, more specifically but without
limitation, centrifugal gas compressor systems and methods utilizing shockwave energy.
BACKGROUND
[0002] Conventional gas compressors may create and move pressurized gas. Industries, such
as oil refineries, chemical plants, natural gas plants, typically use gas compressors
for continuous, stationary service. Additionally, ski resorts have used gas compressors
to generate large amounts of snow. Wave engines include a compression function which
compress gas using energy derived from a thermal process, such as heat transfer or
combustion, which imparts expanding hot gas into compression energy to incoming gas
from expanding heated pressurized gas. Wave engines typically utilize axial (as distinguished
from radial) flow and derive no compression energy from centrifugal action.
SUMMARY
[0003] The present invention refers to s method of compressing air according to claim 1
and a gas compressor according to claim 8. Advantageous embodiments may include features
of depending claims. Thus a first aspect of the invention is directed to a method
of compressing air involving: increasing velocity of air flow, via centrifugal energy,
within sequential channels of a centrifugal impeller; capturing the air flow from
the sequential channels; reloading at least some of the captured air flow into sequential
channels of the centrifugal impeller; increasing pressure of the reloaded air flow
by inducing at least one shockwave traveling in a same direction as the centrifugal
energy; increasing pressure of the reloaded air flow by inducing at least one shockwave
traveling opposite the centrifugal energy; and discharging the increased pressure
reloaded air flow from the sequential channels.
[0004] In another aspect, the method includes increasing pressure of the reloaded air flow
by inducing at least one additional shockwave traveling in the same direction as the
centrifugal energy.
[0005] In another aspect, the method includes the pressure of the reloaded air flow resulting
from the at least one additional shockwave traveling in the same direction as the
centrifugal energy is comparatively higher than the pressure of the reloaded air flow
resulting from pressure of the reloaded air flow by inducing at least one shockwave
traveling opposite the centrifugal energy.
[0006] In another aspect, the method includes inducing an adjustment wave after the discharging.
[0007] In another aspect, the method includes angularly locating at least one barrier adjacent
the centrifugal impeller, wherein the reloaded air flow within the sequential channels
of the centrifugal impeller collides with the at least one barrier.
[0008] In another aspect, the method includes radially locating at least one barrier adjacent
the centrifugal impeller, wherein the reloaded air flow within the sequential channels
of the centrifugal impeller collides with the at least one barrier.
[0009] In another aspect, the method includes capturing the discharged air flow; injecting
at least some of the captured discharged air flow into sequential channels of another
centrifugal impeller.
[0010] In another aspect, the method includes cooling at least some of the capturing the
air flow prior to the reloading.
[0011] In another aspect, the method includes changing a speed of the centrifugal impeller.
[0012] Another aspect of the invention is directed to a gas compressor. The gas compressor
includes a centrifugal impeller configured to increase velocity of air flow, via centrifugal
energy, within sequential channels of a centrifugal impeller; at least one port that
captures the air flow from the sequential channels; at least one reload port that
reloads the at least some captured air flow into sequential channels of the centrifugal
impeller; and a stator comprising at least one radially located barrier operable to
increase pressure of the reloaded air flow within the sequential channels by inducing
at least one shockwave of controllable strength traveling a same direction as the
centrifugal energy.
[0013] In another aspect, the gas compressor includes the stator further comprises at least
another angularly located barrier operable to increase pressure of the reloaded air
flow by inducing at least one other shockwave traveling opposite direction of the
centrifugal energy.
[0014] In another aspect, the gas compressor includes the stator further comprises at least
an additional angularly located barrier operable to increase pressure of the reloaded
air flow by inducing at least one other shockwave traveling a same direction as the
centrifugal energy.
[0015] In another aspect, the gas compressor includes a discharge port that discharges the
increased pressure reloaded air flow from the sequential channels.
[0016] In another aspect, the gas compressor includes at least some of the discharged air
flow is injected into sequential channels of another centrifugal impeller.
[0017] In another aspect, the gas compressor includes at least one cooling unit operable
to cool at least some of the discharged air flow prior to the injecting.
[0018] In another aspect, the gas compressor includes at least one cooling unit operable
to cool at least some of the captured the air flow prior to the reload port.
[0019] In another aspect, the centrifugal impeller is one of radial inlet and radial outlet
or axial inlet and axial outlet.
[0020] In another aspect, the centrifugal impeller is radial inlet and axial outlet.
[0021] In another aspect, the centrifugal impeller is axial inlet and radial outlet.
[0022] Another aspect is directed to a method of compressing air. Specifically, the method
involves: increasing velocity of air flow, via centrifugal energy, within sequential
channels of a centrifugal impeller; capturing the air flow from the sequential channels;
reloading at least some of the captured air flow into sequential channels of the centrifugal
impeller; increasing pressure of the reloaded air flow by inducing at least one shockwave
traveling in the same direction as the centrifugal energy; increasing pressure of
the reloaded air flow by inducing at least one shockwave traveling opposite the centrifugal
energy; increasing pressure of the reloaded air flow by inducing at least one other
shockwave traveling opposite the centrifugal energy; discharging the increased pressure
reloaded air flow from the sequential channels; and angularly locating at least one
barrier adjacent the centrifugal impeller, wherein the reloaded air flow within the
sequential channels of the centrifugal impeller collides with the at least one barrier.
BRIEF DESCRIPTION OF THE DRAWINGS
[0023]
FIG. 1 illustrates an example gas compressor.
FIG. 2A illustrates an example gas compressor.
FIG. 2B illustrates and describes example flow states across moving waves of a channel
of an example gas compressor.
FIG. 3 illustrates an example gas compressor an example of gas compressor timing and
sequences.
FIG. 4 is an example operating cycle diagram of an example gas compressor.
FIG. 5 is an example turndown and control cycle diagram of an example gas compressor.
FIG. 6 illustrates an example gas compressor in a complete system.
FIG. 7 illustrates an example radial inlet, radial outlet impeller section view of
an example gas compressor.
FIG. 8 illustrates an example axial inlet, axial outlet impeller of an example gas
compressor.
FIG. 9 illustrates an example axial inlet, radial outlet impeller section view of
an example gas compressor.
FIG. 10 illustrates an example axial inlet, radial outlet impeller and stator section
view with two compression stages on a single impeller of an example gas compressor.
FIG. 11A and 11B illustrate example operating cycles discharge flow data of example
gas compressors.
FIG. 12 illustrates example pressure ratio for wave processes compared to isentropic
flow process.
FIG. 13 is a block diagram illustrating an example method of operation of an gas compressor.
[0024] Corresponding reference characters indicate corresponding parts throughout the drawings.
DETAILED DESCRIPTION
[0025] Aspects of this disclosure utilize centrifugal work to drive an air flow, and controls
shockwave strength to in a way that increases the air pressure of the air flow. The
embodiments and examples described herein provide a centrifugal impeller including
sequential shrouded channels, having an open entry portion (e.g., at a small diameter)
and an open exit portion (e.g., at a comparatively larger diameter). The entry end
of a channel and the exit end of the channel become intermittently blocked by one
or more barriers as the centrifugal impeller rotates. The one or more barriers may
define one or more a stator inlet ports or exit ports, which allows gas to enter or
exit a sequential channels of the impeller as the shrouded channel passes a port and
allows gas to be contained within a channel of the impeller as the shrouded channel
passes a barrier (e.g., barrier wall). In examples, the rotor may rotate at a fixed
speed, which may maintain the integrity of the wave field and port flows.
[0026] While the impeller rotates, centrifugal force increases the velocity of the gas flow
within the sequential channels. In examples, the air flow may be captured and reloaded
into other sequential channels of the same impeller. For example, as other sequential
channels of the same impeller pass a reload port, which allows the captured air flow
to reload into the passing sequential channels. As the sequential channels pass by
a barrier, the velocity of the air flow causes the air flow to collide against the
barrier causing the air flow velocity to dramatically drop and inducing a shockwave
energized in the opposing direction of the centrifugal force. Strategic radial and/or
angular placement of the barrier and/or the channels' shape and/or area provide a
way to contain the results of the waves in increased or decreased pressure. As the
impeller continues to rotate, the moving shockwave energy increases the pressure of
the air flow located within the sequential channels. As the impeller continues to
rotate, a shockwave moving in the opposite direction increases the pressure of the
air flow located within the sequential channels. Further, if desired, as the impeller
continues to rotate, a shockwave moving in the opposite direction increases the pressure
of the air flow located within the sequential channels. After the desired number of
shockwaves have occurred, as the impeller continues to rotate, the sequential channels
to pass by a port causing an opening of an exit portion of the sequential channels.
While the channel opens, the pressurized gas flows out of the sequential channels.
[0027] While the impeller rotates, centrifugal force increases the velocity of the gas flow
during a reset phase, and shockwave energy (and in examples, centrifugal force) increases
the pressure of the air flow curing a reload phase. Further rotation of the impeller
causes the sequential channels to pass by a port causing an opening of an exit portion
of the sequential channels during a discharge phase. While the channel opens, the
pressurized gas flows out of the sequential channels. In examples, the discharge port
is delimited by an inward running expansion wave and by the arrival of a reflected
expansion wave.
[0028] Similar to typical centrifugal compressors, the gas enters the channel at low velocity
and low pressure. Rotation of the impeller causes the individual shrouded channels
to sequentially pass by a gas inlet port. As such, the individual shrouded channels
are serially exposed to the gas inlet port causing the gas to sequential enter the
shrouded channels at low velocity and low pressure. Also, similar to conventional
centrifugal compressors, rotation of the impeller creates centrifugal force that drives
the gas flow outward from the inside diameter (ID) of the stator toward the outside
diameter (OD) of the stator. The velocity of the flow through a given channel begins
at low velocity and increases as the channel rotates through the arc defined by the
inlet port [reset process.
[0029] Conventional centrifugal compressors stop applying flow work once the gas flow reaches
the stator OD, and the pressurized gas flow exits the stator through a volute moving
to gas away from the impeller and stator and downstream to next stage of the overall
system or to the user. As such, pressurized air provided by conventional centrifugal
compressors are limited based at least on size and rotational speeds.
[0030] Systems and methods herein solve the above problems of conventional centrifugal compressors
by provide a way to contain moving wave compression (e.g., shock waves) to create
more parameters that can be used to increase the gas flow's pressure, while at the
same time relying on centrifugal force to energy the gas flow's velocity, which minimizes
the complexity and component part of the systems and methods. Traditionally, conventional
centrifugal compressors viewed shock waves, which typically occur at the rotor blade
tips, as a problem that rendered conventional centrifugal compressors unstable. As
such, the industry has expended copious amounts of time, energy, and technology to
minimize, eliminate, or otherwise accomodate shock waves occurring in conventional
centrifugal compressors. As opposed to fighting shock waves, systems and methods herein
seek to harness moving shock waves within the rotor channels in a manner that increases
a gas flow's pressure. By harnessing and using shock waves (which achieve higher pressure
ratios than isentropic flow process, which allows more mass in the channels, which
permits the rotor to do more work), the same or more pressure is realized in the gas
flow. By compressing air according to systems and methods described herein the same
or more gas pressure may be generated with smaller rotors, operating at slower revolutions
per minute. The benefits also include mechanical simplicity, high delivered pressure
(for a given gas, diameter and speed) at relatively low gas flow, with a higher turn
down capability (e.g., from 100% to 0% gas flow) at the design pressure ratio.
[0031] Nonetheless, examples herein are fundamentally distinct from conventional wave engines,
which include a compression process, which compress gas using wave processes but depend
on a thermal process, such as heat transfer or combustion, which creates an increased
volume of hot gas to create compression energy. Conventional wave engines rely on
thermal energy to drive and increase the pressure of a gas flow. In contrast, examples
described herein rely on centrifugal force to drive and increase the velocity of a
gas flow. Relying on thermal energy (e.g., combustible engines) to drive an air flow
is less energy efficient, less environmentally sound, and significantly more mechanically
complex as compared to relying on centrifugal force to drive and increase the velocity
of a gas flow. Thus, examples described herein provide substantial benefits over traditional
wave engines.
[0032] In examples, the channels are shrouded, with a constant area, and the stator ID and
OD housing closely follows the curve of the impeller, and the sequential and rapid
changes in the velocity and pressure of the gas flow generate sequential moving (e.g.,
inward and outward running) shock waves and expansion waves as the shrouded channels
pass stator ports and walls.
[0033] The added centrifugal processes and moving wave processes improves the steady gas
flow discharge, as explained above. Further, the centrifugal processes are initiated
in sequence, within a single rotation of a centrifugal impeller providing improved
control. Moreover, the close running ID and OD stator walls reduce leakage from high
pressure regions to low pressure regions. The combination and sequence of centrifugal
processes and moving wave processes create a higher stage pressure ratio, at lower
gas flow, with high gas flow turndown as compared to a conventional centrifugal compressor
with similar dimensions and operating speed. Energy is imparted to the gas flow by
centrifugal work, with multiple stages of work, and compression/shockwave recovery
of pressure on the impeller allow for the higher stage pressure ratio. Since the processes
are initiated in sectors of the impeller rotation, less gas flow is processed than
in a comparable centrifugal compressor. The impeller has constant area shrouded channels,
radially oriented, with radial or axial inlets and with radial or axial channel outlets.
Further still, there are two exit port gas flows per stage, each providing an opportunity
to remove heat from the gas flow, which further increases the compressor's capacity.
[0034] In examples, changes of the angular location and of one or more stator inlet ports
shape may change the air flow presentation to the rotor, which may be leveraged to
increase optimization. In examples, changes of the angular location and shape of one
or more stator exit ports change the acceptance of air flow, which may be leveraged
to minimize flow loss. In examples, changing the angular location includes moving
the leading edge and/or trailing edge of the port. In examples, changes of shapes
and positions of exit diffusers may change the recovery of velocity head, which may
be leveraged to increase recover of velocity head.
[0035] In examples, systems and methods may vary the rotational speed up or down slightly
to mismatch the waves and resultant flows in the ports (e.g., to permit reduced flows
or recirculated flows). Systems and methods may throttle the flow at the inlet port
and/or throttle the reload flow. Systems and methods may "pinch throat" the discharge
port.
[0036] The embodiments and examples described herein improve traditional centrifugal compressors
by reusing the pressurized gas flow by injecting the pressurized gas flow back into
the ID of the impeller via a second inlet port, which adds additional centrifugal
energy to the gas flow before allowing the pressurized gas flow to be delivered to
a downstream system or otherwise exit the compressor. For example, an exit port at
the stator OD leads to a second inlet port adjacent the inner diameter of the impeller.
Thus, the pressurized gas flow exiting the first exit port connects back toward the
stator ID reenters the impeller via a second gas inlet port allowing the gas flow
to enter a sequentially rotating channel.
[0037] FIG. 1 is an exemplary block diagram illustrating an example cross sectional view
of a gas compressor 100. Gas compressor 100 includes an impeller 102 with radial channels
103a - 103n having a substantially constant area. The channels 103a-103n are enclosed
except at an opening 104 at an inner diameter (ID) and at an opening 105 at an outer
diameter (OD). Channel ID openings may be radially or axially disposed. Channel OD
openings may be radially or axially disposed.
[0038] Impeller 102 is coupled to a shaft (not shown) supported by bearings (not shown).
The shaft is driven by a motor (not shown). Gas compressor 100 includes a stator 106
with ports 107a-107d that are adjacent and in close proximity to the impeller channel
openings 104 and 105. The ports 107a-107d may be disposed at defined angular sectors
of rotation, with defined relationships between some of the port edges. Two ports
conduct gas flow to the impeller inlets. Two ports conduct gas flow away from the
impeller outlets. The stator 106 contains the various pressures created within gas
compressor 100, conducts gas flow, and converts pressure to velocity at the inlet
ports 107a-107b, which function as nozzles and converts velocity to pressure at the
exit ports 107c-107d , which function as diffusers. The stator 106 supports the bearings
(not shown) and the coupling to the drive motor (not shown). Stator walls run close
to impeller channel openings and prevent leakage of gas from high pressure regions
to low pressure regions.
[0039] In examples, shaft bearings (not shown) may be included that support the rotor. Further
the shaft bearings may permit rotation, locate rotor radially for close running of
seals, locate rotor axially for close running of seals, inhibit vibration, resist
unbalanced pressure forces - axial and radial.
[0040] Rotation of the impeller 106 exposes the impeller channel openings sequentially to
the stator ports and the leading edges and trailing edges of the ports, initiating
a sequence of gas flow processes. In examples, Port 107a is the first inlet port,
which is adjacent to the impeller channel ID and admits low pressure gas onto the
impeller 102. Port 107c is the reset port, which is adjacent to the impeller channel
(OD) and conducts gas flow away from the impeller 102 for reduction of velocity and
recovery of pressure after an initial stage of centrifugal compression. First inlet
port 107a and reload port 107c together enable gas flow on the impeller 102 to reset
from an initial state in the impeller channels of substantially zero velocity and
low pressure to a state of relatively high velocity, at low pressure and at a centrifugal
pressure distribution dictated by the impeller dimensions and rotational speed.
[0041] Port 107b is the reset port, which is adjacent to the impeller channel ID, immediately
after the inlet port 107a in the sequence of rotation and in fluid connection with
reload port 107c. Reload port 107c admits the gas flow from OD reset port 107b back
onto the impeller 102 (e.g., reentrant gas flow) driving the impeller gas flow to
an even higher velocity and pressure caused by an outward running moving shockwave
109. Ports 107a, 107b, and 107c together create a high velocity gas flow through the
impeller 102 at a first intermediate level of pressure.
[0042] The trailing edge of reload port 107c closes off the impeller OD channel exit, bringing
the gas flow to zero velocity on the impeller 102 and initiating an inward running
moving shockwave 110 that raises the pressure. When the inward running shockwave 110
reaches the ID of the impeller channel openings the trailing edge of reset port 107b
closes the opening and traps high pressure gas on the impeller 102 causing the highest
pressure within the compressor cycle, and highest temperature. The gas flow has substantially
zero velocity relative to the impeller 102 and has a centrifugal pressure distribution
from ID to OD dictated by the impeller dimensions and rotational speed.
[0043] Continued rotation of the impeller 102 exposes the channel OD to the discharge port
107d, wherein gas flow is conducted away from the impeller 102, for reduction of velocity
and recovery of pressure in a diffuser and then for delivery to a user or to a subsequent
compression stage (not shown). The static pressure in discharge port 107d is lower
than the peak pressure achieved on the impeller 102. Opening of the impeller channel
at the leading edge of discharge port 107d initiates an inward running moving expansion
wave 111 that signals expansion of the gas flow into the discharge port 107d . The
expansion wave 111 reflects from the inner stator wall adjacent to the impeller ID
as an outward running moving expansion wave 112, which brings gas flow on the impeller
102 to substantially zero velocity relative to the impeller 102, at low pressure relative
to the impeller 102, with a pressure distribution dictated by the impeller dimensions
and rotational speed. When the outward running expansion wave 112 reaches the impeller
OD, the trailing edge of discharge port 107d closes of the channel, causing completion
of the sequence, which may be repeated substantially continuously. Further, when the
outward running expansion wave 112 reaches the impeller OD, wave 113, which may be
of relatively of small strength and may be either an inward running expansion wave
or a shock wave, signals the opening of inlet port 107a and reload port 107c to begin
the reset process 114.
[0044] FIG. 2A illustrates an example gas compressor 200. In example gas compressor 200
moving waves are initiated in four ways, each following a threshold mismatch (e.g.,
near- instantaneous mismatch) of pressure and/or velocity. Shockwave 209 is initiated
by the mismatch of total pressure and velocity as the impeller ID channel opening
is exposed to the reload port 207c. Shockwave 209 drives the flow on the impeller
at the trailing edge of the inlet port 107a to a higher velocity and pressure (e.g.,
highest velocity of this partial rotation of the cycle). Shockwave 210 is initiated
by stoppage of the high velocity and intermediate pressure flow at the trailing edge
of the reset port 207b, positioned at location 214. Location 214 is enlarged on the
right side of FIG. 2. Shockwave 210 results in gas flow with zero velocity relative
to the impeller, at the highest pressure.
[0045] Expansion wave 211 is initiated by exposure of the impeller OD opening to the discharge
port 207n, at a static pressure less than the pressure on the impeller, which occurs
at location 215. Location 215 is enlarged on the left side of FIG. 2. The expansion
wave 211 signals the flow to move, off of the impeller, into the discharge port 207n.
Expansion wave 212 is formed as expansion wave 211 reflects from the ID stator wall
causing a mismatch of the velocity defined by expansion wave 211 and the boundary
condition of the stator wall which is zero velocity.
[0046] Since channel openings are not instantaneous, a wave formation event occurs, wherein
shock waves are formed initially, that steepens to a shock or a pressure decrease
that diffuses as a spread-out expansion wave. This creates wave timing differences
from exact waves, potential losses and carry-over flows that can be determined and
accounted for. Expansion waves propagate into a flow region with acoustic velocity.
Shocks propagate into a flow region with a velocity that exceeds the speed of sound
for the region. The equations for moving waves 220 and 230 are shown in FIG. 2B. Constant
area channels with a consistent shape improve propagation of moving waves as compared
to inconsistent area channels and/or inconsistently shaped channels.
[0047] FIG. 3 illustrates an example of gas compressor timing and sequences 300. Impeller
state 316n is the low pressure, zero velocity condition, after expansion and before
the reset group of processes is initiated. Impeller state 317n is the high pressure,
zero velocity condition. Stator 306 includes inlet port 307a, reset port 307b, reload
port 307c, and discharge port 307n. Reset port 307b is fluidly coupled to reload port
307c direct the collected reset flow back on to the impeller at the reload port 307c.
The positions of edges of one or more of the ports 307a-307n may be based on the flow
or wave processes. In examples, the leading edges for inlet port 307a and reset port
307b are at the same rotation angle. The angular length of the inlet port 307a is
sufficient to achieve the desired mass flow in the port and flow Mach number at the
trailing edge of the inlet port 307a. The desired mass flow and flow Mach number may
be determined, calculated, adjustable, and selectable.
[0048] The trailing edge of reset port 307b is a one wave transit time after the trailing
edge of inlet port 307a to allow for the passage of shockwave 309. The trailing edge
of reload port 307c is located by the transit time of inward running shockwave 310
and its arrival at the rotor ID. The length of discharge port 307n may be based on
the transit time of expansion waves 311 and 312. Because expansion waves are diffusive
(e.g. the wave spreads out as it travels), the location of the trailing edge of discharge
port 307n is positioned is at the point where the static pressure on the rotor moves
below (e.g., drops) the static pressure in the discharge port 307n. In examples, the
angle devoted to the highest pressure portion of the cycle may be minimized to further
reduce leakage loss. In some examples, the cycle angle duration may not match angle
available, and extra rotation angle may be left after the discharge port 307n, before
the leading edges of the inlet port 307a and reset port 307b.
[0049] In examples, the stator wall's outside diameter 306
OD and inside diameter 306
ID may be located close to the impeller ID and OD channel openings (whether axial or
radial), which improves containment of the various levels of pressure and to prevent
leakage from high pressure regions to low pressure regions that would adversely affect
the processes. Further, port leading and trailing edges may also be located close
to the impeller ID and OD channel openings (whether axial or radial), which further
improves pressure containment and leakage prevention. In some examples, the shock
waves may have a small deviation from ideal (typically less than 1.5% loss of total
pressure ratio across the shock).
[0050] Diffusion of flow to reduce velocity and recover pressure occurs in stator OD ports
(reset port 307b and discharge 307n). An exemplary static pressure for discharge 307n
may be the square root of the pressure ratio achieved at State D (shown in FIG. 4),
which is the maximum max pressure on the impeller relative to the inlet total pressure.
Positioning the ports such that static pressure for discharge 307n is at State D optimizes
compression by making use of two expansion waves of equal pressure ratio (e.g., expansion
waves 311 and 312).
[0051] FIG. 4 is an example operating cycle diagram of an example gas compressor. Diagram
400 maps an sequential processes of an example centrifugal wave compressor operating
cycle in a graph of Pressure vs. Mach number for the flow states at the rotor outside
diameter. (Mach number = (gas flow velocity / speed of sound)).
[0052] Beginning at point A, is a very low flow velocity through the impeller, at low pressure.
This is the impeller condition at the opening of the inlet and reset ports. From point
A, the flow resets to velocity and pressure point B into the reset port. The reset
port flow, having an elevated total pressure, may be loaded back onto the impeller
ID at the reload port, initiating an outward running shockwave s1 and returning the
flow on the impeller at intermediate pressure with highest velocity state point C.
[0053] The flow is stopped on the impeller at the trailing edge of the reset port, which
initiates an inward running shockwave s2, converting the velocity to high pressure
with zero velocity in the rotor channel at point D. The flow is then expanded to an
intermediate static pressure E into the discharge port. The expansion is defined by
expansion wave e1 and reflected expansion wave e2. After e2, the flow on the impeller
is at low pressure and zero velocity returning to point A. In examples, the steady
flow into the discharge port (stator) is diffused to low velocity and total pressure
Et. An optimal design may position the discharge port static pressure Pe to be the
square root of the pressure ratio of Pd/Pa, which delivers an optimal combination
of flow and pressure to the discharge port by two balanced expansion waves e1 and
e2.
[0054] FIG. 5 is an example turndown and control cycle diagram of an example gas compressor.
In examples, one or more of wave compressors described herein may turn down flow from
100% to 0% at a target delivered pressure. Reduction of Point B in M to B' results
in a reduction of mass on the impeller (B'), which reduces the mass flow delivered
at C' or Ct'. Centrifugal work is done in discrete sectors of rotation, and is positively
accelerates making surge or stall events unlikely. The recovery of velocity to pressure
on the impeller (S2) is driven by a strong moving wave. Waves S1, E1 and E3 (D1' to
D2') are accelerative.
[0055] Control (e.g., reduction of mass flow) may be implemented effected by a valve in
the inlet port and nozzle that adjusts inlet port total pressure. Additionally or
alternatively, the inlet port may include a variable leading edge that is dynamically
adjustable to change the rotational sector available for reset (e.g., reducing the
Mach number at E to E' and resulting Pa and Ma). Additionally or alternatively, the
impeller speed maybe dynamically adjustable to implement control by creating a mismatch
between the wave field and the port edges, which causes a limitation or recirculation
of flow. Control may be initiate and or terminated manually and/or automatically based
on a target pressure or a reduce pressure at a target flow. In examples, a target
pressure or a reduce pressure at a target flow may be dependent one or more characteristic
of the downstream system. Further, flow energy remaining on the rotor at reduced flow
(D1') may be recovered by an extra expansion wave A1' to a2', and the recovered total
pressure is available in the reset port, minus diffusion loss.
[0056] FIG. 6 illustrates an example gas compressor of an example system 600. In examples,
a flow enters through a filter 601, which removes particulates. Then, flow enters
the impeller through the inlet port 602. Flow exits the impeller, at an elevated pressure
and temperature, after a single stage of centrifugal compression, at the reset port
603. Following diffusion in the stator, to recover velocity as pressure, flow exits
the unit. Flow goes through a first cooler 604, wherein heat is transferred to cooling
media and liquid water condensed from the gas is drained from the cooler by a drain.
[0057] Flow is reintroduced to the impeller at the reload port 605, wherein the flow is
further compressed on the impeller and exposed to the discharge port 606 at elevated
pressure and temperature. Following diffusion in the stator, to recover velocity as
pressure, the flow exits the unit and goes to a second cooler 607, wherein heat is
transferred to cooling media, and liquid water condensed from the gas is drained from
the cooler 607 by a drain. Thereafter, the flow, flows out at 608 and is delivered
to a user or to a subsequent compression stage.
[0058] FIG. 7 illustrates an example radial inlet, radial outlet impeller 700 section view
of an example gas compressor. Inlet port 707a or reset port 707b and discharge port
707n are shown in a radial inlet and outlet configuration.
[0059] FIG. 8 illustrates an example axial inlet, axial outlet impeller 800 of an example
gas compressor. An axial face radial channel 801 is shown in an axial inlet and axial
outlet configuration.
[0060] FIG. 9 illustrates an example axial inlet, radial outlet impeller 900 section view
of an example gas compressor. Channel 901 is shown in an axial inlet radial outlet
configuration.
[0061] FIG. 10 illustrates an example axial inlet, radial outlet impeller and stator section
view with two compression stages on a single impeller of an example gas compressor
1000. Example inlet 1001 and example outlet 1002 is shown in an axial inlet and radial
outlet configuration.
[0062] FIG. 11A illustrates an example operating cycle discharge flow data of an example
three port gas compressor. X axis 1101 represents time, and Y axis 1102 represents
the flow. FIG. 11B illustrates an example operating cycle discharge flow data of an
example four port gas compressor (e.g., as shown in FIG. 1). X axis 1101B represents
time, and Y axis 1102B represents the flow. FIG. 12 shows example pressure ratio for
wave processes compared to isentropic flow process. X axis 1203 represents the flow
Mach number, and the Y axis 1204 represents pressure ratio.
[0063] FIG. 13 is an example block diagram illustrating an example method 1300 of compressing
gas. In this example method, the reset phase, reload phase, and discharge phase illustrated
in FIG. 1 is shown by way of example. FIG. 13 is an example block diagram illustrating
an example method 1300 of compressing gas. In this example method, the reset phase,
reload phase, and discharge phase illustrated in FIG. 1 is shown by way of example.
At operation 1301, example method 1300 increases velocity of air flow, via centrifugal
energy, within sequential channels of a centrifugal impeller. At operation 1302, example
method 1300 captures the air flow from the sequential channels. At operation 1303,
example method 1300 reloads at least some of the captured air flow into sequential
channels of the centrifugal impeller. At operation 1304, example method 1300 increases
pressure of the reloaded air flow by inducing at least one shockwave traveling in
the same direction as the centrifugal energy. At operation 1305, example method 1300
increases pressure of the reloaded air flow by inducing at least one shockwave traveling
opposite the centrifugal energy. At operation 1306, example method 1300 increases
pressure of the reloaded air flow by inducing at least one other shockwave traveling
opposite the centrifugal energy. At operation 1307, example method 1300 discharges
the increased pressure reloaded air flow from the sequential channels. Some steps
of example method 1300 may be skipped if desired and additional step may be added
if desired.
[0064] Example 1300 may be used according to any and/or any combination of the example impellers,
example gas compressors and/or systems described and/or illustrated herein (e.g.,
FIGs. 1-12). Further, example method 1300 may include additional aspects for example,
a temperature and pressure of the gas flow when exiting the first exit port is elevated
compared to the temperature and pressure of the gas flow prior to entering the first
inlet port. In another aspect, a temperature and pressure of the gas flow when exiting
the discharge port is elevated compared to the temperature and pressure of the gas
flow when exiting the first exit port. Another aspect also includes: after the releasing
the gas flow via the first exit port, intercooling the gas flow before the reintroducing
the gas flow via a second inlet port. Another aspect also includes, after the discharging
the gas flow via the discharge port, delivering the gas flow to a subsequent compression
stage. Another aspect also includes, detecting a characteristic of a downstream operation;
and adjusting a target pressure or a target gas flow of the centrifugal impeller.
Another aspect also includes: detecting a target pressure or a target gas flow of
the centrifugal impeller; and adjusting a mass gas flow at the first inlet port by
at least one of: adjusting a valve at the first inlet port, adjusting a nozzle at
the first inlet port, adjusting a position of an adjustable leading edge of the first
inlet port, and adjusting a rotation speed of the centrifugal impeller.
Additional Examples
[0065] A first aspect is directed to a gas compressor. Specifically, the gas compressor
involves: a centrifugal impeller comprising constant area shrouded channels and a
stator. The stator includes: an inside diameter adjacent at least two inside diameter
gas ports including a first inlet port having a leading edge and a trailing edge;
a second inlet port having a leading edge and a trailing edge; and an outside diameter
adjacent at least two outside diameter gas ports. The outside gas ports include: a
first exit port having a leading edge and a trailing edge, and a second exit port
having a leading edge and a trailing edge. A channel of the centrifugal impeller passes
the two inside diameter gas ports and the two outside diameter gas ports during a
single revolution of the centrifugal impeller.
[0066] In another aspect, the first exit port fluidly couples to the second inlet port.
[0067] In another aspect, the leading edges and the trailing edges of the two inside diameter
gas ports and two outside diameter gas ports are positioned based at least on a selected
mass gas flow, a selected gas flow Mach number, and wave trajectory.
[0068] In another aspect, the leading edge of the first inlet port and the leading edge
of the first exit port are positioned at a same rotation angle.
[0069] In another aspect, an angular length of the first inlet port is based at least on:
a selected mass gas flow of the first inlet port, and a selected gas flow Mach number
at the trailing edge of the first inlet port.
[0070] In another aspect, an angular length of the first inlet port is adjustable via adjustable
positions of the leading edge of the first inlet port.
[0071] In another aspect, an angular distance between the trailing edge of the first inlet
port and the trailing edge of the first exit port provides at least one moving shockwave
that travels from the inside diameter of the stator to the outside diameter of the
stator.
[0072] In another aspect, an angular distance between the trailing edge of the first exit
port and the trailing edge of the second inlet port provides at least one moving shockwave
that travels from the outside diameter of the stator to the inside diameter of the
stator.
[0073] In another aspect, an angular length of the second exit port is based at least on
a selected travel time of an moving expansion wave that travels from the outside diameter
of the stator to the inside diameter of the stator and a reflective expansion wave
that travels from the inside diameter of the stator to the outside diameter of the
stator.
[0074] In another aspect, the trailing edge of the second exit port is positioned at a location
that static pressure on the impeller reduces below static pressure in the second exit
port.
[0075] In another aspect, an angular distance between the trailing edge of the second inlet
port and the leading edge of the second exit port is a shorter than any other angular
distance between any other trailing edge of the stator and any other leading edge
of the stator.
[0076] Another aspect is directed to a gas compression method. Specifically, the gas compression
method includes: receiving a gas flow into one or more shrouded channels of a centrifugal
impeller via a first inlet port adjacent an inside diameter of a stator during a partial
revolution of the centrifugal impeller; releasing the gas flow from the one or more
channels of the centrifugal impeller via a first exit port adjacent an outside diameter
of the stator during a subsequent partial revolution of the centrifugal impeller;
reintroducing the gas flow into the one or more channels of the centrifugal impeller
via another inlet port adjacent the inside diameter of the stator during another subsequent
partial revolution of the centrifugal impeller; and discharging the gas flow from
the one or more channels of the centrifugal impeller via a discharge port adjacent
the outside diameter of the stator during an additionally subsequent partial revolution
of the centrifugal impeller, wherein a sum of the partial revolution, the subsequent
partial revolution, the another subsequent partial revolution, and the additionally
subsequent partial revolution is less than a single revolution of the centrifugal
impeller.
[0077] In another aspect, a temperature and pressure of the gas flow when exiting the first
exit port is elevated compared to the temperature and pressure of the gas flow prior
to entering the first inlet port.
[0078] In another aspect, a temperature and pressure of the gas flow when exiting the discharge
port is elevated compared to the temperature and pressure of the gas flow when exiting
the first exit port.
[0079] Another aspect also includes: after the releasing the gas flow via the first exit
port, intercooling the gas flow before the reintroducing the gas flow via a second
inlet port.
[0080] Another aspect also includes: after the discharging the gas flow via the discharge
port, delivering the gas flow to a subsequent compression stage.
[0081] Another aspect also includes: detecting a characteristic of a downstream operation;
and adjusting a target pressure or a target gas flow of the centrifugal impeller.
[0082] Another aspect also includes: detecting a target pressure or a target gas flow of
the centrifugal impeller; and adjusting a mass gas flow at the first inlet port by
at least one of: adjusting a valve at the first inlet port, adjusting a nozzle at
the first inlet port, adjusting a position of an adjustable leading edge of the first
inlet port, and adjusting a rotation speed of the centrifugal impeller.
[0083] Another aspect is directed to a centrifugal moving wave gas compressor. Specifically,
the centrifugal moving wave gas compressor involves: a centrifugal impeller comprising
constant area shrouded channels and a stator. The stator includes: a first gas inlet
port adjacent an inside diameter of the stator operable to receive a gas flow having
an initial pressure into the impeller, a first gas exit port adjacent an outside diameter
of the stator operable to release the gas flow from the impeller at a first elevated
pressure after a partial revolution of the impeller, a reload gas port adjacent an
inside diameter of the stator operable to reload the gas flow into the impeller, and
a discharge gas port adjacent an outside diameter of the stator operable to rerelease
the gas flow from the impeller at a second elevated pressure after a partial revolution
of the impeller. The second elevated pressure is higher than the first elevated pressure,
which is higher than the initial pressure, and wherein a channel of the centrifugal
impeller passes the two inside diameter gas ports and the two outside diameter gas
ports during a single revolution of the centrifugal impeller.
[0084] In another aspect, at least an outward moving first shockwave raises the initial
pressure to the first elevated pressure, and wherein at least an inward moving second
shock wave, an inward moving expansion wave, and an outward moving expansion wave
raises the first elevated pressure to the second elevated pressure.
[0085] The examples and designs illustrated and described herein as well as examples and
designs not specifically described herein (e.g., impellers, stators, and/or compressors
not specifically illustrated in the figures) are within the scope of aspects of the
disclosure. The order of execution or performance of the operations in examples of
the disclosure illustrated and described herein is not essential, unless otherwise
specified. That is, the operations may be performed in any order, unless otherwise
specified, and examples of the disclosure may include additional or fewer operations
than those disclosed herein. For example, it is contemplated that executing or performing
a particular operation before, contemporaneously with, or after another operation
is within the scope of aspects of the disclosure.
[0086] When introducing elements of aspects of the disclosure or the examples thereof, the
articles "a," "an," "the," and "said" are intended to mean that there are one or more
of the elements. The terms "comprising," "including," and "having" are intended to
be inclusive and mean that there may be additional elements other than the listed
elements. The term "exemplary" is intended to mean "an example of." The phrase "one
or more of the following: A, B, and C" means "at least one of A and/or at least one
of B and/or at least one of C."
[0087] Having described aspects of the disclosure in detail, it will be apparent that modifications
and variations are possible without departing from the scope of aspects of the disclosure
as defined in the appended claims. As various changes could be made in the above constructions,
products, and methods without departing from the scope of aspects of the disclosure,
it is intended that all matter contained in the above description and shown in the
accompanying drawings shall be interpreted as illustrative and not in a limiting sense.
[0088] While the disclosure is susceptible to various modifications and alternative constructions,
certain illustrated examples thereof are shown in the drawings and have been described
above in detail. It should be understood, however, that there is no intention to limit
the disclosure to the specific forms disclosed, but on the contrary, the intention
is to cover all modifications, alternative constructions, and equivalents falling
within the spirit and scope of the disclosure.
1. A method of compressing air comprising:
increasing velocity of air flow, via centrifugal energy, within sequential channels
of a centrifugal impeller;
capturing the air flow from the sequential channels;
reloading at least some of the captured air flow into sequential channels of the centrifugal
impeller;
increasing pressure of the reloaded air flow by inducing at least one shockwave traveling
in a same direction as the centrifugal energy;
increasing pressure of the reloaded air flow by inducing at least one shockwave traveling
opposite the centrifugal energy;
discharging the increased pressure reloaded air flow from the sequential channels.
2. The method of claim 1, further comprising:
increasing pressure of the reloaded air flow by inducing at least one additional shockwave
traveling in the same direction as the centrifugal energy,
wherein optionally the pressure of the reloaded air flow resulting from the at least
one additional shockwave traveling in the same direction as the centrifugal energy
is comparatively higher than the pressure of the reloaded air flow resulting from
pressure of the reloaded air flow by inducing at least one shockwave traveling opposite
the centrifugal energy.
3. The method of claim 1 or of claim 2, further comprising:
inducing an adjustment wave after the discharging.
4. The method of any one of claims 1 - 3, further comprising:
angularly or radially locating at least one barrier adjacent the centrifugal impeller,
wherein the reloaded air flow within the sequential channels of the centrifugal impeller
collides with the at least one barrier.
5. The method of any one of claims 1 - 4, further comprising:
capturing the discharged air flow;
injecting at least some of the captured discharged air flow into sequential channels
of another centrifugal impeller.
6. The method of any one of claims 1 - 5, further comprising:
cooling at least some of the capturing the air flow prior to the reloading, or
changing a speed of the centrifugal impeller.
7. The method of claim 1, further comprising:
prior to discharging the increased pressure reloaded air flow, increasing pressure
of the reloaded air flow by inducing at least one other shockwave traveling opposite
the centrifugal energy; and
angularly locating at least one barrier adjacent the centrifugal impeller, wherein
the reloaded air flow within the sequential channels of the centrifugal impeller collides
with the at least one barrier.
8. A gas compressor comprising:
a centrifugal impeller configured to increase velocity of air flow, via centrifugal
energy, within sequential channels of a centrifugal impeller;
at least one port that captures the air flow from the sequential channels;
at least one reload port that reloads the at least some captured air flow into sequential
channels of the centrifugal impeller; and
a stator comprising at least one radially located barrier operable to increase pressure
of the reloaded air flow within the sequential channels by inducing at least one shockwave
of controllable strength traveling a same direction as the centrifugal energy.
9. The gas compressor of claim 8, wherein the stator further comprises at least another
angularly located barrier operable to increase pressure of the reloaded air flow by
inducing at least one other shockwave traveling opposite direction of the centrifugal
energy.
10. The gas compressor of claim 8 wherein the stator further comprises at least an additional
angularly located barrier operable to increase pressure of the reloaded air flow by
inducing at least one other shockwave traveling a same direction as the centrifugal
energy.
11. The gas compressor of any one of claims 8 - 10, further comprising:
a discharge port that discharges the increased pressure reloaded air flow from the
sequential channels,
wherein optionally at least some of the discharged air flow is injected into sequential
channels of another centrifugal impeller and
wherein further optionally the gas compressor additionally comprises at least one
cooling unit operable to cool at least some of the discharged air flow prior to the
injecting.
12. The gas compressor of any one of claims 8 - 11, further comprising:
at least one cooling unit operable to cool at least some of the captured the air flow
prior to the reload port.
13. The gas compressor of any one of claims 8 - 12, wherein the centrifugal impeller is
one of:
- radial inlet and radial outlet;
- axial inlet and axial outlet,
- radial inlet and axial outlet; and
- axial inlet and radial outlet.