[0001] The present disclosure relates to free-piston combustion engines and, more particularly,
the present disclosure relates to control of piston trajectory in a free-piston combustion
engine.
Background
[0002] Some free-piston engines rely on position versus time control of pistons in which
a desired position versus time trajectory of a piston is determined based on an initial
position of the piston. As the system causes a piston to move, the control strategy
measures how much the piston is deviating from the desired position versus time trajectory
and attempts to compensate for any deviation in order to bring the piston closer to
the desired position versus time trajectory. Some free-piston engines rely on control
strategies that measure how much a piston is deviating from other suitable trajectories
(
e.g., position versus velocity) and attempt to compensate for any deviation in order
to bring the piston closer to the desired trajectory.
[0003] These approaches typically rely on an open-form solution for controlling a piston's
movement based on a previously determined trajectory and often do not take into account
changing conditions in the engine, which would affect the movement of the piston.
For example, after the desired trajectory is determined, conditions in the engine
can change such that the desired trajectory is no longer applicable. Movement of the
piston will still, however, be based on the original desired trajectory and deviation
therefrom.
[0004] Patent document
WO2005100764 A1 discloses a method and system for controlling a free-piston energy converter in which
effects of events, like combustion events, in at least one of at least two cylinders,
are decoupled from each other by predicting forces acting on the moving mass of the
converter during a stroke of the moving mass and by evaluating or estimating a value
representing a force which is exerted onto the moving mass, so that the moving mass
reaches a desired reference condition or state, like a desired reference kinetic energy,
at a certain position along the stroke.
Brief Description of the Drawings
[0005] The solution is provided by the features of the independent method claim 1. Variations
are as described by the dependent claims.
[0006] The present disclosure, in accordance with one or more various embodiments, is described
in detail with reference to the following figures. The drawings are provided for purposes
of illustration only and merely depict typical or example embodiments. These drawings
are provided to facilitate an understanding of the concepts disclosed herein and shall
not be considered limiting of the breadth, scope, or applicability of these concepts.
It should be noted that for clarity and ease of illustration these drawings are not
necessarily made to scale.
FIG. 1 is a diagram of three illustrative free-piston combustion engine configurations.
FIG. 2 is a cross-sectional drawing illustrating a two-piston, single-combustion section,
integrated gas springs, and separated linear electromagnetic machine engine, in accordance
with some embodiments of the present disclosure.
FIG. 3 is a diagram illustrating the two-stroke piston cycle of the two-piston integrated
gas springs engine of FIG. 2, in accordance with some embodiments of the present disclosure.
FIG. 4 is a cross-sectional drawing illustrating an alternative two-piston, separated gas
springs, and separated linear electromagnetic machine engine, in accordance with some
embodiments of the present disclosure.
FIG. 5 is a cross-sectional drawing illustrating a single-piston, integrated internal gas
spring engine, in accordance with some embodiments of the present disclosure.
FIG. 6 is a cross-sectional drawing illustrating an embodiment of a gas spring rod, in accordance
with some embodiments of the present disclosure.
FIG. 7 is a cross-sectional drawing illustrating a two-piston, integrated internal gas springs
engine, in accordance with some embodiments of the present disclosure.
FIG. 8 illustrates exemplary position, force, and power diagrams of a free-piston engine
over a compression and an expansion stroke, in accordance with some embodiments of
the present disclosure.
FIG. 9 illustrates other exemplary position, force, and power diagrams of a free-piston
engine over a compression and an expansion stroke, in accordance with some embodiments
of the present disclosure
FIG. 10 is a block diagram of an illustrative piston engine system in accordance with some
embodiments of the present disclosure.
FIG. 11 illustrates an exemplary position-velocity and position-force trajectories of a free-piston
engine over a compression and an expansion stroke, in accordance with some embodiments
of the present disclosure.
FIG. 12 shows a flow diagram of illustrative steps for causing movement of a free-piston
assembly along a propagation path in accordance with some embodiments of the present
disclosure.
FIG. 13 illustrates other exemplary position-velocity and position-force trajectories of
a free-piston engine over a compression and an expansion stroke, in accordance with
some embodiments of the present disclosure.
FIG. 14 illustrates other exemplary position-velocity and position-force trajectories of
a free-piston engine over a compression and an expansion stroke, in accordance with
some embodiments of the present disclosure.
FIG. 15 shows an illustrative state diagram for a hybrid control technique in accordance
with some embodiments of the present disclosure.
[0007] The figures are not intended to be exhaustive or to limit the disclosure to the precise
form disclosed. It should be understood that the concepts and embodiments disclosed
can be practiced with modification and alteration, and that the disclosure is limited
only by the claims.
Detailed Description
[0008] Various embodiments of the present disclosure are directed towards controlling a
free-piston linear combustion engine. In at least one embodiment, the engine comprises:
(i) a cylinder comprising a combustion section, (ii) at least one free-piston assembly
in contact with the combustion section, (iii) at least one driver section in contact
with the at least one free-piston assembly that stores energy during an expansion
stroke of the engine (iv) and at least one linear electromagnetic machine (LEM) that
directly converts between kinetic energy of the at least one free-piston assembly
and electrical energy. It should be noted, however, that further embodiments may include
various combinations of the above-identified features and physical characteristics.
[0009] The present disclosure is related to a control technique for determination and implementation
of a trajectory for one or more of the piston assemblies in a free-piston engine.
As used herein, the term "trajectory" refers to a sequence of data pairs that describe
the motion of a piston assembly in a free-piston engine, such as, for example, a position-force
trajectory (a sequence of position-force pairs), a time-position trajectory (a sequence
of time-position pairs), or a position-velocity trajectory (a sequence of position-velocity
pairs). A position-force trajectory defines the force acting on a piston assembly
at one or more specified positions of the piston assembly, a time-position trajectory
defines the position of a piston assembly at one or more specified instances in time,
and a position-velocity trajectory defines the velocity of a piston assembly at one
or more specified positions of the piston assembly. At least one of the elements in
a data pair of a trajectory may be considered the abscissa in a functional relationship
with the other data element being ordinate. In the case of multiple free-piston assemblies
in one engine (
e.g., arranged as opposed-pistons with a shared combustion section), a trajectory may
include data pairs for each respective piston assembly. It will be understood that,
while a trajectory is generally described as being a sequence of data pairs, a trajectory
may, under certain conditions, include only a single data pair (
e.g., a single position-force pair in the case of a position-force trajectory).
[0010] In accordance with the present disclosure, a processing sub-system of a free-piston
engine computes a position-force trajectory for one or more piston assemblies in a
free-piston engine based at least on a current position of the one or more piston
assemblies and a desired engine performance. As used herein with respect to control
of a free-piston engine, the term "desired engine performance" refers to operating
the engine such that the one or more piston assemblies apex at desired respective
positions, that the one or more piston assemblies reach desired respective target
positions with a respective specified velocity or acceleration, that one or more piston
assemblies reach desired respective target positions with any other suitable parameter
or condition, or any combination thereof. The processing sub-system determines particular
force values based on a position-force trajectory that are to be effected on the one
or more piston assemblies as a function of their positions along their respective
propagation paths between respective apices. It will be understood that, while the
present disclosure is described in the context of determining force values that are
effected on a piston assembly, any other suitable parameter value can be calculated
for effecting the movement of a piston assembly. For example, any suitable gas pressure
value can be used to effect movement of a piston assembly, such as, for example, with
respect to a gas pressure supplied by an external compressed gas source or effecting
a gas pressure by adjusting an aspect of a gas spring. As used herein, the term "propagation
path" refers to a positional path along which a piston assembly traverses. For example,
a processing sub-system may first calculate a position-force trajectory for the one
or more piston assemblies based at least on a current position of the one or more
piston assemblies and a desired engine performance, and then subsequently determine
force values, based on the calculated position-force trajectory, to apply to the one
or more piston assemblies over a specified time or position interval in order to achieve
the desired engine performance. The force values may be applied to the one or more
piston assemblies by, for example, exerting an electromagnetic force onto the one
or more piston assembly. In some embodiments, the processing sub-system calculates
the position-force trajectory based on the operating state of the free-piston engine.
The operating state of a free-piston engine refers to the calculated, measured, or
estimated values or indicators of the state of the engine
(i.e., its dynamical system state) and any other suitable calculated, measured, or estimated
values or indicators of the operating characteristics, performance, parameters, and
environment of the engine. For example, one or more sensors could be used to measure
pressure, temperature, forces, velocities, acceleration, position, any other suitable
parameter or condition, or any combination thereof at respective sections or components
of the free-piston engine. This sensor information can be processed by the processing
sub-system to compute a position-force trajectory to achieve a desired engine performance.
[0011] In one suitable approach, the processing sub-system calculates a position-force trajectory
for a piston assembly when a particular trigger is activated (e.g., in response to
a particular event, at a particular threshold crossing, any other suitable trigger,
or any combination thereof). In another suitable approach, the processing sub-system
calculates a position-force trajectory repeatedly throughout an engine stroke or cycle.
For example, the calculations may be performed at particular time intervals (
e.g., 1 kHz, 10 kHz,
etc.) or at particular discrete position intervals
(e.g., every 1 millimeter, every 1 micron,
etc.). In another suitable approach, as the operating state of the free-piston engine changes,
the processing sub-system may calculate a new position-force trajectory.
[0012] The calculation of each position-force trajectory is made without regard to a deviation
from a previously calculated trajectory (position-force trajectory, time-position
trajectory, or any other suitable trajectory). It will be understood that a position-force
trajectory calculation is determined using for example one or more calculations, one
or more prescriptions, or any combination thereof, including, for example, the use
of a look-up table, a curve-fitting, or both. This aspect allows for changes in and
to the operating state of the free-piston engine (rapid or slow, intended or unintended)
to be accounted for in each new position-force trajectory calculation, thereby providing
a control technique for a free-piston engine that is capable of rejecting disturbances
in the operating state of the free-piston engine. The calculation of each position-force
trajectory may also be computed without regard to the timing of a desired engine performance.
That is, each position-force trajectory is defined without a time component and is
calculated without specifying the time in which a desired engine performance occurs
(e.g., the time in which a piston assembly apices or otherwise reaches a target position).
In some instances, with suitable assumptions about engine gas properties, conditions,
and parameters, the calculation of a position-force trajectory may rely on a close-form
solution. In other instances, the calculation of a position-force trajectory may rely
on a numerically iterative solution (
e.g., using a solver to calculate a solution).
[0013] In some embodiments, the current operating parameters of a free-piston engine may
be estimated based on a preceding force applied to the one or more piston assemblies
that was calculated as part of a previous position-force trajectory. The estimated
engine operating parameters may be used in conjunction with the current position of
the one or more piston assemblies to calculate a new position-force trajectory. For
example, an immediately preceding force value as either determined or as actually
applied to a piston assembly could be used to update an estimate of current gas pressure
in a combustion section or driver section of a free-piston engine by, for example,
applying a smoothing technique (
e.g., IRR or FIR filter) to a previously estimated or measured gas pressure and adjusting
for the change in gas pressure caused at least in part by the immediately preceding
applied force. This aspect can avoid the need for expensive and unreliable sensors
(
e.g., pressure sensors) in a free-piston engine, thereby providing a low cost and high
reliability control technique for a free-piston engine.
[0014] In some embodiments, for a free-piston engine with multiple piston assemblies (e.g.,
arranged as opposed-pistons with a shared combustion section), in addition to the
processing sub-system calculating a position-force trajectory for each respective
piston assembly, the processing sub-system may also calculate synchronization forces
for the multiple piston assemblies and cause certain forces to be applied to the multiple
piston assemblies based on the calculations to synchronize the movements of the multiple
piston assemblies as desired.
[0015] In some embodiments, the processing sub-system may employ a hybrid control strategy
that switches between multiple control techniques, wherein at least one of the control
techniques is based on calculating a position-force trajectory as disclosed herein.
The processing sub-system may, for example, utilize a position-force trajectory control
technique during times when the operating state of the engine is unsteady (e.g., during
engine start-up) and utilize a different, less robust, control technique during times
when the operating state of the engine is sufficiently steady (e.g., delivering constant
and steady power). The processing sub-system may, for example, switch from a less
robust control technique to a more robust position-force trajectory control technique
when an unintended change in the operating state of the engine is detected (
e.g., a combustion misfire event, a higher than expected friction event, a change in
fuel quality event, any other suitable change in the operating state of the engine,
or any combination thereof). In some instances, a less robust control technique may
rely on a time-position trajectory that is calculated based on a previously determined
position-force trajectory (
e.g., as measured during an entire engine stroke or cycle) that was calculated while
the processing sub-system was previously employing a position-force trajectory control
technique. In some instances, the less robust control technique may depend on a deviation
from a previously determined trajectory (position-force trajectory, time-position
trajectory, or any other suitable trajectory).
[0016] Generally, free-piston combustion engine configurations can be broken down into three
categories: 1) two opposed pistons, single combustion chamber, 2) single piston, dual
combustion chambers, and 3) single piston, single combustion chamber. A diagram of
the three common free-piston combustion engine configurations is shown in
FIG. 1. Several illustrative embodiments of linear free-piston combustion engines are illustrated
in commonly assigned
U.S. Patent No. 8,662,029, issued on March 4, 2014, and entitled "High-efficiency linear combustion engine". It will be understood that
while the present disclosure is presented in the context of certain specific illustrative
embodiments of linear free-piston combustion engines, the concepts discussed herein
are applicable to any other suitable free-piston combustion engines, including, for
example, non-linear free-piston engines. Free-piston engines generally include one
or more free-piston assemblies that are free from mechanical linkages that translate
the linear motion of the piston assembly into rotary motion (
e.g., a slider-crank mechanism) or free from mechanical linkages that directly control
piston dynamics
(e.g., a locking mechanism). Free-piston engines have a number of benefits over such mechanically-linked
piston engines, which lead to increased efficiency. For example, due to the inherent
architectural limitations of mechanically-linked piston engines, free-piston engines
can be configured with higher compression ratios and expansion ratios, which lead
to higher engine efficiencies as, described in the previously referenced
[0017] U.S. Patent No. 8,662,029. Moreover, free-piston engines allow for increased variability in the compression
and expansion ratios, including allowing for the compression ratio to be greater than
the expansion ratio and allowing for the expansion ratio to be greater than the compression
ratio, which may also increase the engine efficiency. The free-piston engine architecture
also allows for increased control of the compression ratio on an engine cycle-to-cycle
basis, which allows for adjustments due to variable fuel quality and fuel type. Additionally,
due to the lack of mechanical linkages, free-piston engines result in substantially
lower side loads on the piston assemblies, which allows for oil-less operation, and
in turn, reduced friction and losses resulting therefrom.
[0018] It will be understood that while the present disclosure is presented in the context
of a free-piston internal combustion engine, the teachings and concepts presented
herein are applicable to other types of free-piston devices, such as free-piston compressors
in which combustion does not take place or free-piston compressors in which internal
combustion does take place. In such systems without combustion, electrical energy
is converted into mechanical energy by a LEM to compress a fluid (liquid or gaseous)
in a compression chamber or compression section. In such systems with combustion,
fuel energy is converted into mechanical energy, possibly in conjunction with the
conversion of electrical energy, to compress a fluid in a compression chamber or compression
section. Additionally, the teachings and concepts presented herein are applicable
to free-piston heat engines which convert an external heat resource into electricity
or to compress a fluid.
[0019] FIG. 2 is a cross-sectional drawing illustrating one embodiment of a two-piston, single-combustion
section, integrated gas springs, and separated LEM free-piston internal combustion
engine
100. This free-piston, internal combustion engine
100 directly converts the chemical energy in a fuel into electrical energy via an LEM
200. As used herein, the term "fuel" refers to matter that reacts with an oxidizer. Such
fuels include, but are not limited to: (i) hydrocarbon fuels such as natural gas,
biogas, gasoline, diesel, and biodiesel; (ii) alcohol fuels such as ethanol, methanol,
and butanol; (iii) hydrogen; and (iv) mixtures of any of the above. The engines described
herein are suitable for both stationary power generation and mobile power generation
(
e.g., for use in vehicles).
[0020] Engine
100 includes a cylinder
105 with two opposed piston assemblies
120 dimensioned to move within the cylinder
105 and meet at a combustion section
130 in the center of the cylinder
105. Each piston assembly
120 may include a piston
125 and a piston rod
145. The piston assemblies
120 are free to move linearly within the cylinder
105.
[0021] With further reference to
FIG. 2, the volume between the backside of the piston
125, piston rod
145, and the cylinder
105 is referred to herein as the driver section
160. As used herein, a "driver section" refers to a section of an engine cylinder capable
of storing energy and providing energy to displace the piston assembly without the
use of combustion. The driver section
160, in some embodiments, may contain a non-combustible fluid
(i.e., gas, liquid, or both). In the illustrated embodiment, the fluid in the driver section
160 is a gas that acts as a gas spring. Driver section
160 stores energy from an expansion stroke of the piston cycle and provides energy for
a subsequent stroke of the piston cycle,
i.e. the stroke that occurs after an expansion stroke. For example, kinetic energy of
the piston may be converted into potential energy of the gas in the driver section
during an expansion stroke of the engine. In some embodiments, the potential energy
stored in the driver section can be sufficient to perform the compression stroke (or
an exhaust stroke or any other suitable stroke occurring subsequent to the expansions
stroke) without, for example, any additional net electrical input by a motor force.
As used herein, the term "piston cycle" refers to any series of piston movements that
begin and end with the piston
125 in substantially the same configuration. One common example is a four-stroke piston
cycle, which includes an intake stroke, a compression stroke, an expansion stroke,
and an exhaust stroke. Additional alternate strokes may form part of a piston cycle
as described throughout this disclosure. A two-stroke piston cycle is characterized
as having an expansion stroke and a compression stroke. As used herein, an "expansion
stroke" refers to a stroke of a piston cycle during which the piston assembly moves
from a top-dead-center ("TDC") position to a bottom-dead-center ("BDC") position,
where TDC refers to the position of the piston assembly, or assemblies, when the combustion
section volume is at a minimum and BDC refers to the position of the piston assembly,
or assemblies, when the combustion section volume is at a maximum. As noted above,
since the compression ratio and expansion ratio of a free-piston engine can vary or
be varied from cycle-to-cycle, the TDC and BDC positions can also vary or be varied
from cycle-to-cycle, in some embodiments. Accordingly, as will be described below
in further detail, an expansion stroke may refer to an intake stroke, an expansion
stroke, or both. In some embodiments, the amount of energy to be stored by the driver
section during an expansion stroke may be determined based on various criteria and
controlled by a controller and associated processing circuitry as will be described
below in further detail.
[0022] For purposes of brevity and clarity, the driver section will primarily be described
herein in the context of a gas spring and may be referred to herein as the "gas section,"
"gas springs" or "gas springs section." It will be appreciated that in some arrangements,
the driver section
160 may include one or more other mechanisms in addition to or in place of a gas spring.
For example, such mechanisms can include one or more mechanical springs, magnetic
springs, or any suitable combination thereof. In some arrangements, a highly efficient
linear alternator may be included that operates as a motor, which may be used in place
of or in addition to a spring (pneumatic, hydrodynamic, or mechanical) for generating
compression work. It will be understood by those skilled in the art that in some embodiments,
the geometry of the driver section may be selected to minimize losses and maximize
the efficiency of the driver section. For example, the diameter and/or dead volume
of the driver section may be selected to minimize losses and maximize the efficiency
of the driver section. As used herein, the term "dead volume" refers to the volume
of the driver section when the piston assembly is at its furthest possible BDC position
(
i.e., when the volume of the combustion section is at its greatest before the piston assembly
contacts a physical stop). In some embodiments, for example, if the driver section
is a gas or hydraulic spring, the diameter of the section may be different than the
combustion section in order to provide for increased efficiency. Certain embodiments
of gas springs will be described below in further detail with reference to
FIGS. 8-12.
[0023] Combustion ignition can be achieved via, for example, compression ignition and/or
spark ignition. Fuel can be directly injected into the combustion chamber
130 ("direct injection") or intake ports
180 ("port fuel injection") via fuel injectors and/or mixed with air prior to and/or
during air intake ("premixed injection"). The engine
100 can operate with lean, stoichiometric, or rich combustion using liquid fuels, gaseous
fuels, or both, including hydrocarbons, hydrogen, alcohols, or any other suitable
fuels as described above.
[0024] Cylinder
105 may include injector ports
170, intake ports
180, exhaust ports
185, and driver gas exchange ports
190, for exchanging matter (solid, liquid, gas, or plasma) with the surroundings. As used
herein, the term "port" includes any opening or set of openings (e.g., a porous material)
which allows matter exchange between the inside of the cylinder
105 and its surroundings. It will be understood that the ports shown in
FIG. 2 are merely illustrative. In some arrangements, fewer or more ports may be used. The
above-described ports may or may not be opened and closed via valves. The term "valve"
may refer to any actuated flow controller or other actuated mechanism for selectively
passing matter through an opening. Valves may be actuated by any means, including
but not limited to: mechanical, electrical, magnetic, camshaft-driven, hydraulic,
or pneumatic means. The number, location, and types of ports and valves may depend
on the engine configuration, injection strategy, and piston cycle (
e.g., two- or four-stroke piston cycles). In some embodiments, the matter exchange of
the ports may be achieved by the movement of the piston assembly, which may cover
and/or uncover the ports as necessary to allow exchange of matter.
[0025] In some embodiments, the operation of driver section
160 may be adjustable. In some embodiments, driver gas exchange ports
190 may be utilized to control characteristics of the driver section. For example, driver
gas exchange ports
190 may be used to control the amount, temperature, pressure, any other suitable characteristics,
and/or any combination thereof of the gas in the driver section. In some embodiments,
adjusting any of the aforementioned characteristics and thus adjusting the amount
of mass in the cylinder may vary the effective spring constant of the gas spring.
In some embodiments, the geometry of driver section
160 may be adjusted to obtain desirable operation. In some embodiments, the dead volume
within the cylinder may be adjusted to vary the spring constant of the gas spring.
It will be understood that any of the aforementioned control and adjustment of the
driver section
160 and the gas therein may provide for control of the amount of energy stored by driver
section
160 during an expansion stroke of engine
100. It will also be understood that the aforementioned control of the characteristics
of the gas in driver section
160 also provides for variability in the frequency of engine
100.
[0026] Engine
100 includes a pair of LEMs
200 for directly converting the kinetic energy of the piston assemblies
120 into electrical energy (
e.g., during a compression stroke, during an expansion stroke, during an exhaust stroke,
and/or during an intake stroke). Each LEM
200 is also capable of directly converting electrical energy into kinetic energy of the
piston assembly
120. In some embodiments, the LEMs 200 may convert electrical energy into kinetic energy
of the piston in order to start-up the engine, but need not convert electrical energy
into kinetic energy during operation once the engine has started and sufficient fuel
chemical energy is being converted into kinetic energy of the piston, at least part
of which may be stored in the driver section
160 during expansion strokes. In some embodiments, start-up of the engine may be achieved
by any other suitable technique, including, for example, the use of stored compressed
gas. As illustrated, the LEM
200 includes a stator
210 and a translator
220. Specifically, the translator
220 is coupled to the piston rod
145 and moves linearly within the stator
210, which may remain stationary. In addition, the LEM
200 can be a permanent magnet machine, an induction machine, a switched reluctance machine,
or any combination thereof. The stator
210 and translator
220 can each include magnets, coils, iron, or any suitable combination thereof. Because
the LEM
200 directly transforms the kinetic energy of the pistons to and from electrical energy
(i.e., there are no mechanical linkages), the mechanical and frictional losses are minimal
compared to conventional engine-generator configurations. Furthermore, because the
LEM
200 is configured to convert portions of the kinetic energy of the piston assemblies
into electrical energy during any stroke of a piston cycle, and engine
100 includes an adjustable driver section
160 configured to store energy from an expansion stroke that can be converted to electrical
energy during a subsequent stroke, the LEM
200 may be configured to have a lower electrical capacity than, for example, an LEM or
other device that requires conversion of all energy within a single stroke of a piston
cycle (
e.g., only within the expansion stroke). Accordingly, in some embodiments, the associated
linear alternator and power electronics of the LEM
200 may be reduced in size, weight, and/or electrical capacity. This may result in decreased
size and cost of components, increased efficiency, increased reliability, and increased
utilization as will be understood by one of ordinary skill in the art. Accordingly,
the frequency and therefore power output of the engine may be increased in some embodiments.
[0027] It will be understood by one of ordinary skill in the art that each LEM
200 may be operated as both a generator and a motor. For example, when LEMs
200 convert kinetic energy of piston assemblies
120 into electrical energy they operate as generators. When acting as generators, the
forces applied to translators
220 are in the opposite direction of the motion of piston assemblies
120. Conversely, when LEMs
200 convert electric energy into kinetic energy of piston assemblies
120 they operate as motors. When acting as motors, the forces applied to translators
220 are in the same direction as the motion of piston assemblies
120. For ease of reference, the center line in
FIG. 2 (near injector ports
170) and corresponding figures may be considered the origin, with the positive direction
for each piston assembly being away from the center, in the outward direction.
[0028] The embodiment shown in
FIG. 2 operates using a two-stroke piston cycle. A diagram illustrating the two-stroke piston
cycle
300 of the two-piston integrated gas springs engine
100 of
FIG. 2 is illustrated in
FIG. 3. As illustrated in
FIG. 3, engine
100 may operate using a two-stroke piston cycle including a compression stroke and an
expansion stroke, with the pistons located at BDC prior to the compression stroke,
and at top-dead-center TDC prior to the expansion stroke. As used herein with reference
to the two-piston embodiment, BDC may refer to the point at which the pistons are
furthest from each other. As used herein with reference to the two-piston embodiment,
TDC may refer to the point at which the pistons are closest to each other. When at
or near BDC, and if the driver section is to be used to provide compression work,
the pressure of the gas within the driver section
160 is greater than the pressure of the combustion section
130, which forces the pistons
125 away from BDC and inwards towards each other,
i.e., in the negative direction. The gas in the driver section
160 can be used to provide some or all of the energy required to perform a compression
stroke. As described above, in some embodiments, the piston
125 may be forced away from BDC by any other suitable mechanism, including a mechanical
spring, a magnetic spring, or any other suitable mechanism that may be used to provide
compression work. While the LEM
200 may also provide some of the energy required to perform a compression stroke, in
a preferred embodiment, when sufficient energy is being produced during combustion,
enough energy may be stored in the driver section
160 such that LEM
200 need not convert any electrical energy into kinetic energy of the piston
125 because the energy stored in driver section
160 may be transferred to the piston to provide the requisite compression work. The LEM
200 may also extract energy during the compression stroke. For example, if the gas in
the driver section
160 (or other suitable means as described above) provides excess energy for performing
the compression stroke, the LEM
200 may convert a portion of the kinetic energy of the piston assembly
120 into electrical energy.
[0029] The amount of energy required to perform a compression stroke may depend on the desired
compression ratio, the pressure and temperature of the combustion section
130 at the beginning of the compression stroke, the mass of the piston assembly
120, system losses, as well as other properties and operating conditions of the engine.
As described above, driver section
160 may provide all of the energy needed for the compression stroke so that no other
energy input (from LEM
200 or any other source) is necessary. In some embodiments, some energy may be input
during the compression stroke from the LEM
200, but the net energy during the compression stroke is still positive (e.g., more energy
converted to electricity than input over the stroke). A compression stroke continues
until combustion occurs, which typically occurs at a time when the velocities of the
pistons
125 are at or near zero. Combustion causes an increase in the temperature and pressure
within the combustion section
130, which forces the pistons
125 outward toward the LEMs
200. During an expansion stroke, a portion of the kinetic energy of the piston assembly
120 may be converted into electrical energy by the LEM
200 and another portion of the kinetic energy does compression work on the gas (or other
compression mechanism) in the driver section
160. Alternatively, all of the kinetic energy of the piston assembly may be stored in
driver section
160. An expansion stroke continues until the velocities of the pistons
125 are zero. After the expansion stroke and before the subsequent compression stroke,
with pistons
125 at or near BDC, the engine may exhaust combustion products and intake air, an air/fuel
mixture, or an air/fuel/combustion products mixture. This process may be referred
to herein as "breathing" or "breathing at or near BDC." It will be appreciated by
those of ordinary skill in the art that breathing may be achieved in any suitable
manner, such as uniflow or cross-flow scavenging, as described in previously referenced
[0030] U.S. Patent No. 8,662,029. It will also be appreciated that although described as occurring after the expansion
stroke, in some embodiments breathing may occur during the end of the expansion stroke
and/or the beginning of the compression stroke. Similarly, in some embodiments, combustion
may occur during the end of the compression stroke and/or the beginning of the expansion
stroke.
[0031] FIG. 3 illustrates one exemplary port configuration
300 in which the intake ports
180 and exhaust ports
185 are in front of both pistons near BDC. The opening and closing of the exhaust ports
185 and intake ports
180 may be independently controlled. The location of the exhaust ports
185 and intake ports
180 can be chosen such that a range of compression ratios and/or expansion ratios is
possible. The times in a cycle when the exhaust ports
185 and intake ports
180 are activated (opened and closed) can be adjusted during and/or between cycles to
vary the compression ratio and/or expansion ratio and/or the amount of combustion
product retained in the combustion section
130 at the beginning of a compression stroke. Retaining combustion gases in the combustion
section
130 is called residual gas trapping (RGT) and can be utilized to effect combustion timing,
peak combustion temperatures, and other combustion and engine performance characteristics.
Alternatively, or in addition, exhaust gas recirculation (EGR) can be used to recirculate
combustion gasses in order to effect combustion timing, peak combustion temperatures,
and other combustion and engine performance characteristics.
[0032] Although operation of a two-stroke cycle is described above, the embodiment of
FIG. 2 may also be operated using a four-stroke piston cycle, which includes an intake stroke,
a compression stroke, a power (expansion) stroke, and an exhaust stroke. In some embodiments,
any suitable modification may be made to operate using a four-stroke piston cycle.
For example, as described in the previously referenced
U.S. Patent No. 8,662,029, the location of the ports may be modified to operate the engine using a four-stroke
piston cycle.
[0033] In some embodiments, in a four-stroke piston cycle, just as in the two-stroke cycle
described above, driver section
160 may provide all of the work necessary for the compression stroke. In some embodiments,
the driver section
160 may provide enough work to avoid net electrical energy input during the compression
stroke. In some embodiments, the driver section
160 may provide enough work to allow for net electrical energy output during the compression
stroke. The compression stroke may continue until combustion occurs,
e.g., when the velocities of pistons
125 are at or near zero. Combustion may be followed by a power stroke, during which kinetic
energy of the piston assemblies
120 may be stored in driver section
160 and/or converted into electrical energy by LEMs
200 as described above with respect to the two-stroke cycle. At some point at or near
the power-stroke BDC, exhaust ports may be opened, and an exhaust stroke may occur
until the velocities of pistons
125 are at or near zero, which marks the exhaust stroke TDC for that cycle. As described
above, the energy stored in driver section
160 during the expansion stroke may provide the work required to perform the exhaust
stroke. At some point prior to reaching exhaust stroke TDC, the combustion section
130 closes the exhaust valves while there is still exhaust in the cylinder. In some embodiments,
this trapped exhaust gas may store enough energy to perform the subsequent intake
stroke. As with the expansion stroke, the kinetic energy of the piston assemblies
120 may be stored in driver section
160 and/or converted into electrical energy by LEMs
200 during the intake stroke, which occurs until the velocities of the pistons
125 are at zero. In some embodiments, driver section
160 may store enough energy during the intake stroke to perform the subsequent compression
stroke. In some embodiments, any suitable amount of energy stored in the driver section
in excess of the amount required for a subsequent compression stroke or a subsequent
exhaust stroke may be converted into electrical energy by LEMs
200.
[0034] FIG. 4 is a cross-sectional drawing illustrating an alternative two-piston, separated gas
springs, and separated LEM engine, in accordance with the principles of the disclosure.
It will be understood that the illustrated configuration is merely for purposes of
example, and that any other suitable configuration of a two-piston, separated gas
springs, and separated LEM engine may be used in accordance with the present disclosure.
Engine
400 includes a main cylinder
105, two opposed piston assemblies
120, and a combustion section
130 located in the center of main cylinder
105. The illustrated engine
400 has certain physical differences when compared with engine
100. Specifically, engine
400 includes a pair of outer cylinders
405 that contain additional pistons
125, and the LEMs
200 are disposed between the main cylinder
105 and the outer cylinders
405. Each outer cylinder
405 includes a driver section
410 located between the piston
125 and the distal end of the outer cylinder
405 and a driver back section
420 located between the piston
125 and the proximal end of the outer cylinder
405. Main cylinder
105 includes a pair of combustion back sections
430 disposed between the pistons
125 and the distal ends of the main cylinder
105. In some embodiments, the driver back section
420 and the combustion back section
430 are maintained at or near atmospheric pressure. In some embodiments, the driver back
section
420 and the combustion back section
430 are not maintained at or near atmospheric pressure. In the illustrated configuration,
the main cylinder
105 has ports
440 for removal of blow-by gas, injector ports
170, intake ports
180, and exhaust ports
185. Driver gas exchange ports
190 are located in the outer cylinders
405. Each piston assembly
120 includes two pistons
125 and a piston rod
145. The piston assemblies are free to move linearly between the main cylinder
105 and the outer cylinders
405 as depicted in
FIG. 4. It will be understood that the embodiment of
FIG. 4 can operate using a two-stroke piston cycle using, for example, the methodology as
set forth above with respect to
FIG. 3, and a four-stroke piston cycle as described above and in previously referenced
U.S. Patent No. 8,662,029.
[0035] The configuration of
FIGS. 2 and
3, as shown, includes a single unit referred to as the engine
100 and defined by the cylinder
105, the piston assemblies
120 and the LEMs
200. Similarly, the configuration of
FIG. 4, as shown, includes a single unit referred to as the engine
400 and defined by the main cylinder
105, the piston assemblies
120, the outer cylinders
405, and the LEMs
200. However, multiple units can be placed in parallel, which could collectively be referred
to as "the engine." This type of modular arrangement in which engine units operate
in parallel may be used to enable the scale of the engine to be increased as needed
by the end user. Additionally, not all units need be the same size, operate under
the same conditions (
e.g., frequency, stoichiometry, or breathing), or operate simultaneously (
e.g., one or several units could be deactivated while one or several other units operate).
When the units are operated in parallel, there exists the potential for integration
between the engines, such as, but not limited to, gas exchange between the units and/or
feedback between the units' respective LEMs
200.
[0036] FIGS. 5-7 illustrate further embodiments featuring integrated internal gas springs in which
the gas spring is integrated inside of the piston assembly and the LEM is separated
from the combustor cylinder. As illustrated in
FIGS. 5-7, the integrated internal gas spring (IIGS) architecture may be similar in length to
the integrated gas spring with separated LEM architecture illustrated in
FIGS. 2-3. However, the IIGS architecture may eliminate issues with respect to the blow-by gases
from the combustion section entering the gas spring, which also occurs in the fully
integrated gas spring and LEM architecture.
[0037] FIG. 5 is a cross-sectional drawing illustrating a single-piston, integrated internal gas
spring engine, in accordance with some embodiments of the present disclosure. Many
components such as the combustion section
130 are similar to the components in previous embodiments (
e.g.,
FIGS. 1 and
2 ), and are labeled accordingly. The engine
500 comprises a cylinder
105 with piston assembly
520 dimensioned to move within the cylinder
105 in response to reactions within combustion section
130 near the bottom end of the cylinder
105. Piston assembly
520 comprises a piston
530, piston seals
535, and a spring rod
545. The piston assembly
520 is free to move linearly within the cylinder
105. In the illustrated embodiment, the piston rod
545 moves along bearings
560 and is sealed by piston rod seals
555 that are fixed to the cylinder
105. The cylinder
105 includes exhaust/injector ports
570, 580 for intake of air, fuel, exhaust gases, air/fuel mixtures, and/or air/exhaust gases/fuel
mixtures, exhaust of combustion products, and/or injectors. Some embodiments do not
require all of the ports depicted in
FIG. 5. The number and types of ports depends on the engine configuration, injection strategy,
and piston cycle (e.g., two- or four-stroke piston cycles).
[0038] In the illustrated embodiment, the engine
500 further comprises an LEM
550 (including stator
210 and magnets
525) for directly converting the kinetic energy of the piston assembly
520 into electrical energy. It will be understood that LEM
550 may be configured to operate substantially the same as LEMs
200 described above with respect to
FIGS. 2-4.
[0039] With further reference to
FIG. 5, piston
530 comprises a solid front section (combustor side) and a hollow back section (gas spring
side). The area inside of the hollow section of the piston assembly
520, between the front face of piston
530 and spring rod
545, comprises a gas that serves as the gas spring
160, which provides at least some of the work required to perform a compression stroke.
Piston
530 moves linearly within the combustion section
130 and the stator
210 of the LEM
550. The piston's motion is guided by bearings
560, 565, which may be solid bearings, hydraulic bearings, and/or air bearings. In the illustrated
embodiment, the engine
500 includes both external bearings
560 and internal bearings
565. In particular, the external bearings
560 are located between the combustion section
130 and the LEM
550, and the internal bearings
565 are located on the inside of the hollow section of the piston
530. The external bearings
560 are externally fixed and do not move with the piston
530. The internal bearings
565 are fixed to the piston
530 and move with the piston
530 against the spring rod
545.
[0040] With continued reference to
FIG. 5, the spring rod
545 serves as one face for the gas spring
160 and is externally fixed. The spring rod
545 has at least one seal
585 located at or near its end, which serves the purpose of keeping gas within the gas
spring section
160. Magnets
525 are attached to the back of the piston assembly
520 and move linearly with the piston assembly
520 within the stator
210 of the LEM
550. The piston assembly
520 may have seals to keep gases in the respective sections. The illustrated embodiment
includes (i) front seals
535 that are fixed to the piston
530 at or near its front end to keep to gases from being transferred from the combustion
section
130, and (ii) back seals
555 that are fixed to the cylinder
105 and keep intake gases and/or blow-by gases from being transferred to the surroundings.
[0041] FIG. 6 is a cross-sectional drawing illustrating an embodiment of a gas spring rod, in accordance
with some embodiments of the present disclosure. Specifically, the spring rod
645 includes a central lumen
610 that allows mass to be transferred between the gas spring section
160 to a reservoir section
620 that is in communication with the surroundings. The communication with the surroundings
is controlled through a valve
630. The amount of mass in the gas spring
645 may be regulated to control the pressure within the gas spring
645 in accordance with some embodiments of the present disclosure.
[0042] FIG. 7 is a cross-sectional drawing illustrating a two-piston, integrated internal gas springs
engine, in accordance with some embodiments of the present disclosure. Most of the
elements of the two-piston embodiment are similar to those of the single-piston embodiment
of
FIG. 5, and like elements are labeled accordingly. In addition, the operating characteristics
of the single- and two-piston embodiments are similar as described in previous embodiments,
including all the aspects of the linear alternator, breathing, combustion strategies,
etc.
[0043] FIG. 8 illustrates the position, force, and power of a free-piston engine, in accordance
with some embodiments of the present disclosure. As shown,
FIG. 8 illustrates exemplary position
820, force
840, and power
860 diagrams over time for a free-piston engine with a two-stroke piston cycle including
a compression stroke and a expansion stroke. With reference to position diagram
820, as labeled in
FIG. 8, for reference purposes, the positive direction corresponds to the direction from
TDC to BDC. For example, in the free-piston assemblies of
FIGS. 2-4, the centerline would correspond to the origin, and the direction away from the centerline
would be the positive direction for each free-piston assembly. As can be seen by position
diagram
820, the piston assembly starts the compression stroke at BDC and progresses to TDC, at
which point the expansion (or power) stroke begins. During the expansion stroke, the
piston assembly progresses back to BDC.
[0044] With reference to force diagram
840, the force is positive when applied in a direction from TDC to BDC. For example, in
the free-piston assemblies of
FIGS. 2-4, force applied in the direction away from the centerline would be a positive force.
As can be seen in force diagram
840, during the compression stroke, a relatively constant positive force may be applied
to the piston assembly, and during the expansion stroke, the force may be negative
(in the direction towards the centerline), allowing the LEM to extract energy during
both strokes. It will be understood that the force applied need not be constant, and
that in some embodiments, a variable force profile may be applied, for example, to
produce a relatively constant power output. It will also be understood that in some
embodiments, and as depicted herein, forces may not be applied when the piston assembly
velocity is relatively low, due to the inefficiency of doing so.
[0045] The power output is the negative product of the force and velocity of the piston
assembly. Referring specifically to power diagram
860, it can be seen that, in the ideal case illustrated, no power need be input to the
system in order to perform the compression and expansion strokes of the piston cycle.
Rather, as described above, in the ideal case, there is sufficient energy stored in
the at least one driver section during the expansion stroke to perform the subsequent
compression stroke without additional energy input into the system during the compression
stroke.
[0046] While in an ideal scenario, it may be desirable to avoid any power input during the
compression and expansion strokes as described with respect to
FIG. 8, in some embodiments it may be necessary or desirable to provide some power input.
Accordingly,
FIG. 9 illustrates the position, force, and power of a free-piston engine, in accordance
with some other embodiments of the present disclosure. Similar to
FIG. 8, FIG. 9 illustrates exemplary position
920, force
940, and power
960 diagrams over time for a free-piston engine with a two-stroke piston cycle including
a compression stroke and a expansion stroke. While the position diagram
920 is generally similar to that of position diagram
820 illustrated in
FIG. 8, it will be understood that the force diagram
940 and the power diagram
960 may differ from those illustrated in
FIG. 8. With reference to force diagram
940 during the compression stroke, it can be seen at
902 that a force may be applied in the opposite direction as originally applied for a
brief period. This is also reflected in power diagram
960, where a negative power showing power input for the same brief period may be seen
at
904. While this force application and power input may occur for a number of reasons, in
some embodiments, this may be done in order to control the speed of the piston assembly
or otherwise ensure that the piston assembly reaches the appropriate or desired TDC
position before the subsequent expansion stroke. For example, a force may be applied
to increase the speed of the piston assembly. Similarly, with further reference to
force diagram
940 during the expansion stroke, it can be seen at
906 that a force may be applied in the opposite direction as the rest of the expansion
stroke for a brief period, which is also reflected in power diagram
960, where a negative power showing power input for the same brief period may be seen
at
908. As described above, this applied force and input power may occur for a number of
reasons, but in some embodiments, force may be applied in this way and power input
in order to control the speed of the piston assembly or otherwise ensure that the
piston assembly reaches the appropriate or desired BDC position before the subsequent
compression stroke. For example, a force may be applied to increase the speed of the
piston assembly as described above.
[0047] Although the provision of input power during compression stroke and/or expansion
stroke described with respect to
FIG. 9 is not necessarily ideal operation, it will be understood that the net electrical
energy output over each stroke is still greater than zero
(i.e., there is no net electrical energy input over each stroke). This is evident from power
diagram
960, in which it can be seen that the integral over each stroke, represented by the area
of the curve above zero subtracted by the area of the curve below zero, is substantially
greater than zero. Accordingly, the amount of electrical energy output by the system
over each stroke is greater than the electrical energy input to control the piston
assembly position as described above. As used herein, the "net electrical energy"
refers to the electrical energy transfer into or out of the LEM such as that described
above with respect to
FIGS. 2-4. In some embodiments, the LEM may include a stator coupled to power electronics (including,
e.g., a DC bus, IGBTs, capacitors, and/or any other suitable components), batteries,
and/or a grid-tie inverter. Accordingly, in some embodiments, while some electrical
energy may be input into the LEM via power electronics, batteries, and/or a grid-tie
inverter coupled to the LEM, the net electrical energy over a given stroke as described
above would be output from the LEM to the power electronics, batteries, and/or grid-tie
inverter.
[0048] While
FIGS. 8 and
14 illustrate operation of the free-piston engine with no net electrical input over
a given stroke, it is understood that the principles of the present disclosure can
be applied to any suitable free-piston engine, including a free-piston engine that
operates with net electrical input during a stroke, such as during a compression stroke
(
e.g., during start up).
[0049] As stated, the embodiment described above with respect to
FIGS. 2-4 includes a two-piston, single-combustion section, two-stroke internal combustion
engine
100. Described below, and illustrated in the corresponding figures, is a control system
applicable to a free-piston combustion engine generally. Accordingly, as described
above, the control system is applicable to other free-piston combustion engine architectures,
such as those described in the previously referenced
[0050] U.S. Patent No. 8,662,029. As would be appreciated by those of ordinary skill in the art, various modifications
and alternative configurations may be utilized, and other changes may be made, without
departing from the scope of the disclosure. For example, in addition to the two-piston
architectures described above with respect to
FIGS. 2-4, the control system described herein is applicable to, for example, single-piston
architectures. Similarly, in addition to the two-stroke engine described above with
respect to
FIG. 3, the control system described herein is also applicable to, for example, four-stroke
engines.
[0051] FIG. 10 is a block diagram of an illustrative piston engine system
1000 having control system
1010 for a piston engine
1040, in accordance with some embodiments of the present disclosure. Piston engine
1040 may be, for example, any suitable free-piston engine as described above with respect
to
FIGS. 2-7. Control system
1010 may communicate with one or more sensors
1030 coupled to piston engine
1040. Control system
1010 may be configured to communicate with auxiliary systems
1020, which may be used to adjust operating aspects or properties of piston engine
1040. In some embodiments, more than one piston engine may be controlled by control system
1010. For example, control system
1010 may be configured to communicate with auxiliary systems and sensors corresponding
to any number of piston engines. In some embodiments, control system
1010 may be configured to interact with a user via user interface system
1050.
[0052] Control system
1010 may include processing equipment
1012, communications interface
1014, sensor interface
1016, control interface
1018, any other suitable components or modules, or any combination thereof. Control system
1010 may be implemented at least partially in one or more integrated circuits, ASIC, FPGA,
microcontroller, DSP, computers, terminals, control stations, handheld devices, modules,
any other suitable devices, or any combination thereof. In some embodiments, the components
of control system
1010 may be communicatively coupled via individual communications links or a communications
bus
1011, as shown in
FIG. 10. Processing equipment
1012 may include any suitable processing circuitry, such as one or more processors (e.g.,
a central processing unit), cache, random access memory (RAM), read only memory (ROM),
any other suitable hardware components or any combination thereof that may be configured
(e.g., using software, or hard-wired) to process information regarding piston engine
1040, as received by sensor interface
1016 from sensor(s)
1030. Sensor interface
1016 may include a power supply for supplying power to sensor(s)
1030, a signal conditioner, a signal pre-processor, any other suitable components, or any
combination thereof. For example, sensor interface
1016 may include a filter, an amplifier, a sampler, and an analog to digital converter
for conditioning and pre-processing signals from sensor(s) 1030. Sensor interface
1016 may communicate with sensor(s)
1030 via communicative coupling
1019, which may be a wired connection (
e.g., using IEEE 802.3 ethernet, or universal serial bus interface), wireless coupling
(
e.g., using IEEE 802.11 "Wi-Fi", or Bluetooth), optical coupling, inductive coupling,
any other suitable coupling, or any combination thereof. Control system
1010, and more particularly processing equipment
1012, may be configured to provide control of piston engine
1040 over relevant time scales. For example, a change in one or more temperatures may
be controllable in response to one or more detected engine operating characteristics,
and the control may be provided on a time scale relevant to operation of the piston
engine (e.g., fast enough response to prevent overheating and/or component failure,
to adequately provide apex control as described below, to allow for shutdown in the
case of a diagnostic event, and/or for adequate load tracking).
[0053] Sensor(s)
1030 may include any suitable type of sensor, which may be configured to sense any suitable
property or aspect of piston engine
1040. In some embodiments, sensor(s) may include one or more sensors configured to sense
an aspect and/or property of a system of auxiliary systems
1020. In some embodiments, sensor(s)
1030 may include a temperature sensor (
e.g., a thermocouple, resistance temperature detector, thermistor, or optical temperature
sensor) configured to sense the temperature of a component of piston engine
1040, a fluid introduced to or recovered from piston engine
1040, or both. In some embodiments, sensor(s)
1030 may include one or more pressure sensors (
e.g., piezoelectric pressure transducers, strain-based pressure transducers, or gas ionization
sensors) configured to sense a pressure within a section of piston engine 1040
(e.g., a combustion section, or gas driver section), of a fluid introduced to or recovered
from piston engine
1040, or both. In some embodiments, sensor(s)
1030 may include one or more force sensors (
e.g., piezoelectric force transducers or strain-based force transducers) configured to
sense a force within piston engine
1040 such as a tensile, compressive or shear force
(e.g., which may indicate a friction force or other relevant force information, pressure
information, or acceleration information). In some embodiments, sensor(s)
1030 may include one or more current and/or voltage sensors (
e.g., an ammeter and/or voltmeter coupled to a LEM of piston engine
1040) configured to sense a voltage, current, power output and/or input (
e.g., current multiplied by voltage), any other suitable electrical property of piston
engine
1040 and/or auxiliary systems
1020, or any combination thereof. In some embodiments, sensor(s)
1030 may include one or more sensors configured to sense the position of the piston assembly
and/or any other components of the engine, the speed of the piston assembly and/or
any other components of the engine, the acceleration of the piston assembly and/or
any other components of the engine, the rate of flow, oxygen or nitrogen oxide emission
levels, other emission levels, any other suitable property of piston engine
1040 and/or auxiliary systems
1020, or any combination thereof.
[0054] Control interface
1018 may include a wired connection, wireless coupling, optical coupling, inductive coupling,
any other suitable coupling, or any combination thereof, for communicating with one
or more of auxiliary systems
1020. In some embodiments, control interface
1018 may include a digital to analog converter to provide an analog control signal to
any or all of auxiliary systems
1020.
[0055] Auxiliary systems
1020 may include a cooling system
1022, a pressure control system
1024, a gas driver control system
1026, and/or any other suitable control system
1028. Cooling/heating system
1022 may include a pump, fluid reservoir, pressure regulator, bypass, radiator, fluid
conduits, electric power circuitry (e.g., for electric heaters), any other suitable
components, or any combination thereof to provide cooling, heating, or both to piston
engine
1040. Pressure control system
1024 may include a pump, compressor, fluid reservoir, pressure regulator, fluid conduits,
any other suitable components, or any combination thereof to supply (and optionally
receive) a pressure controlled fluid to piston engine
1040. Gas driver control system
1026 may include a compressor, gas reservoir, pressure regulator, fluid conduits, any
other suitable components, or any combination thereof to supply (and optionally receive)
a driver gas to piston engine
1040. In some embodiments, gas driver control system may include any suitable components
to control any of the gas spring components described above with respect to
FIGS. 2-7. In some embodiments, other system
1028 may include a valving system such as, for example, a cam-operated system, a solenoid
system, or any other electromechanical device or electric machine to supply oxidizer
and/or fuel to piston engine
1040. Valving may also be used to regulate exhaust flow out of the engine, such as in an
unported engine having, for example, a single piston assembly arrangement or dual
piston assembly arrangement. Exhaust valves may be controlled with voice coils (
e.g., linear motors) to allow uniflow scavenging.
[0056] User interface
1015 may include a wired connection, wireless coupling, optical coupling, inductive coupling,
any other suitable coupling, or any combination thereof, for communicating with one
or more of user interface systems
1050. User interface systems
1050 may include display
1052, input device
1054, mouse
1056, audio device
1058, a remote interface accessed via website, mobile application, or other internet service,
any other suitable user interface devices, or any combination thereof. In some embodiments,
a remote interface may be remote from the engine but in proximity to the site of the
engine. In other embodiments, a remote interface may be remote from both the engine
and the site of the engine. Display
1052 may include a display screen such as, for example, a cathode ray tube screen, a liquid
crystal display screen, a light emitting diode display screen, a plasma display screen,
any other suitable display screen that may provide graphics, text, images or other
visuals to a user, or any combination of screens thereof. In some embodiments, display
1052 may include a touchscreen, which may provide tactile interaction with a user by,
for example, offering one or more soft commands on a display screen. Display
1052 may display any suitable information regarding piston engine
1040 (e.g., a time series of a property of piston engine
1040), control system
1010, auxiliary systems
1020, user interface system
1050, any other suitable information, or any combination thereof. Input device
1054 may include a QWERTY keyboard, a numeric keypad, any other suitable collection of
hard command buttons, or any combination thereof. Mouse
1056 may include any suitable pointing device that may control a cursor or icon on a graphical
user interface displayed on a display screen. Mouse
1056 may include a handheld device (
e.g., capable of moving in two or three dimensions), a touchpad, any other suitable pointing
device, or any combination thereof. Audio device
1058 may include a microphone, a speaker, headphones, any other suitable device for providing
and/or receiving audio signals, or any combination thereof. For example, audio device
1058 may include a microphone, and processing equipment
1012 may process audio commands received via user interface
1015 caused by a user speaking into the microphone.
[0057] In some embodiments, control system
1010 may be configured to receive one or more user inputs to provide control. For example,
in some embodiments, control system
1010 may override control settings based on sensor feedback, and base a control signal
to auxiliary system
1020 on one or more user inputs to user interface system
1050. In a further example, a user may input a set-point value for one or more control
variables (
e.g., temperatures, pressures, flow rates, work inputs/outputs, or other variables) and
control system
1010 may execute a control algorithm based on the set-point value.
[0058] In some embodiments, operating characteristics
(e.g., one or more desired property values of piston engine
1040 or auxiliary systems
1020) may be pre-defined by a manufacturer, user, or both. For example, particular operating
characteristics may be stored in memory of processing equipment
1012, and may be accessed to provide one or more control signals. In some embodiments,
one or more of the operating characteristics may be changed by a user. Control system
1010 may be used to maintain, adjust, or otherwise manage those operating characteristics.
For example, control system
1010 may be used to alter operation based on environmental conditions such as temperature
and pressure.
[0059] In some embodiments, control system
1010 computes a position-force trajectory for the one or more piston assemblies in a free-piston
engine based at least in part on a desired engine performance (e.g., a desired apex
position) and a current position of one or more piston assemblies. Based on the calculated
position-force trajectory, control system
1010 effects the displacement of the one or more piston assemblies by applying particular
forces to the one or more piston assemblies over a specified time or position intervals.
The calculation of each position-force trajectory by control system
1010 is computed without regard to a deviation from a previously determined trajectory
(position-force, time-position, or any other suitable trajectory). Control system
1010 may calculate a position-force trajectory when a particular trigger is activated
(
e.g., in response to a particular event), repeatedly over an engine stroke or cycle,
after changes to the operating state of the engine, or any combination thereof. In
some embodiments, control system
1010 may also calculate a position-force trajectory without regard to the timing of a
desired engine performance. In some instances, control system
1010 may calculate a position-force trajectory based on the operating state of the engine.
In some embodiments, control system
1010 may estimate a current operating parameter of the engine based on a preceding force
that was calculated as part of a previous position-force trajectory or based on a
preceding force that was applied to the one or more piston assemblies. In certain
instances, control system
1010 may calculate a position-force trajectory using a closed-form solution, a numerically
iterative solution, or a combination of both. In embodiments with multiple piston
assemblies, control system
1010 may, in addition to calculating a position-force trajectory for each respective piston
assembly, also calculate synchronization forces for the multiple piston assemblies
and cause certain forces to be applied to the multiple piston assemblies based on
the synchronization calculations to synchronize the movements of the multiple piston
assemblies as desired. In some embodiments, the control system
1010 may employ a hybrid control strategy that switches between a position-force trajectory
control technique and another control technique (e.g., a control technique that relies
on the calculation of deviation from a previously determined trajectory) depending
on the operating state of the engine.
[0060] The following is a discussion of some illustrative embodiments implemented in accordance
with the concepts described above. These embodiments generally relate to single- and
dual-piston free-piston internal combustion engines with driver sections, such as
those illustrated in
FIGS. 2-7 and discussed above. In these embodiments, control system
1010 is used to cause displacement of respective piston assemblies based on a desired
engine performance. It will be understood that implementations and concepts discussed
with reference to these specific embodiments are generally applicable to other embodiments
as well. This discussion is provided for purposes of illustration and is not intended
to limit the applicability of the disclosed implementations and concepts to only these
embodiments.
[0061] FIG. 11 shows exemplary position-velocity and position-force trajectories
(1110 and
1120, respectively) of a piston assembly in a free-piston engine over a compression stroke
and an expansion stroke. The force values shown in
1120 correspond to the force values calculated by the control system
1010 and applied to the piston assembly by exerting an electromagnetic force on the piston
assembly via a LEM. The profiles illustrated in
FIG. 11 are idealized, simplified, or both for purposes of clarity and ease of illustration.
It will be understood that actual profiles may be different. Electromagnetic forces
are referred to herein as LEM forces, LEM force values, motor forces, motor force
values, forces, or force values. With reference to
FIG. 11 and the proceeding trajectory figures, the positive direction corresponds to the
direction from TDC to BDC
(e.g., a positive velocity corresponds to the piston assembly is moving from TDC to BDC
and a positive force corresponds to a force being applied in the direction toward
BDC). Additionally, with reference to
FIG. 11 and the proceeding trajectory figures, the zero position point corresponds to the
center line for an opposed-piston free-piston engine (
e.g.,
Figs. 2-4 and
FIG. 7) or the combustion section end
(i.e., the head of the combustion section) for a single-piston free-piston engine
(e.g., FIG. 5). As shown in
FIG. 11, the piston assembly cycles between BDC and TDC (its apices) while the LEM applies
a force in the opposite direction of the motion of the piston assemblies, thereby
producing net electrical energy output over both strokes. Producing net electrical
energy output over both strokes requires that a driver section is sized such that
it can store enough energy from an expansion stroke to provide more than enough energy
required to perform the subsequent compression stroke. While this paradigm is generally
assumed in the following discussion, it will be understood that the control techniques
disclosed herein can be applied to free-piston engines in which the driver section
is sized such that net electrical energy input is required during the compression
stroke and to free-piston engines in which there is no driver section and all of the
energy required to perform a compression stroke is provided by a LEM. The single motor
force values for each stroke shown in
1120 are an idealized representation of how a free-piston engine could operate. The following
is a discussion of specific embodiments in which control system
1010 may be used to control the displacement of a piston assembly in a free-piston engine
to achieve a desired engine performance.
[0062] FIG. 12 shows a flow chart
1200 of illustrative steps for control system
1010 to control the displacement of the one or more piston assemblies along a propagation
path in a free-piston engine in accordance with some embodiments of the present disclosure.
As illustrated, control system
1010 first determines, at step
1202, a current position of the one or more piston assemblies in a free-piston engine.
Next, control system
1010 calculates, at step
1204, a position-force trajectory based on a desired engine performance and the current
position of the one or more piston assemblies. Lastly, control system
1010 effects the displacement of the one or more piston assemblies by applying the one
or more force values calculated in step
1204 to the one or more piston assemblies. The sequential steps
1202, 1204, and
1206 are repeated until control system
1010 sends a command to cease. The command to cease may be sent for any suitable reason,
including, for example, control system
1010 having determined to switch to a different control technique, to turn off the engine,
that a mechanical or electronic safety switch tripped, for any other suitable reason,
or for any combination thereof. The sequential steps
1202, 1204, and
1206 can repeat based on the activation of a particular trigger or repeat throughout an
engine stroke or cycle. For example, sequential steps
1202, 1204, and
1206 can repeat in response to a particular event, at a particular threshold crossing,
any other suitable trigger, or any combination thereof. In another example, sequential
steps
1202, 1204, and
1206 can repeat at particular time intervals
(e.g., 1 kHz, 10 kHz,
etc.) or at particular discrete position intervals
(e.g., every 1 millimeter, every 1 micron,
etc.). This particular control technique, as illustrated by flow chart
1200, is referred to herein as a position-force trajectory control technique.
[0063] Control system
1010 determines a current position of the one or more piston assemblies at step
1202 using suitable sensor(s)
1030. Suitable sensors
1030 for determining position of the one or more piston assemblies include magnetic encoders,
optical encoders, optical grating encoders, laser-based encoders. The current position
can be any position between BDC and TDC, inclusive. While, in the case of a linear
free-piston engine, a current position of the one or more piston assemblies can be
represented as a single dimension along a single axis of propagation per piston assembly,
it will be understood that the teachings of the present disclosure can be applied
to a free-piston engine in which a piston assembly is able to move in more than one
dimension and in which a current position can be represented multidimensionally.
[0064] At step
1206, control system
1010 sends one or more commands to the free-piston engine and/or its auxiliaries to effect
the displacement of the one or more piston assemblies by applying the one or more
force values calculated in step
1204 to the one or more piston assemblies. The forces may be applied to the one or more
piston assemblies by, for example, exerting an electromagnetic force onto the one
or more piston assembly via a LEM. The following discussion is directed toward applying
the forces through a LEM, but it will be understood that the application of force
to the one or more piston assemblies could be applied through other techniques, such
as, for example, by adjusting properties of the driver section (
e.g., adjusting the spring stiffness or spring constant of the driver section). In some
embodiments, application of motor force can be implemented using techniques as described
in commonly assigned
U.S. Patent No. 8,624,542, issued on January 7, 2014.
[0065] The force values effected on the one or more piston assemblies in step
1206 are based on the position-force trajectory previously calculated in step
1204. It will be understood that reference to a force being "effected" on a piston assembly
refers to control system
1010 causing the mechanism that imparts a force onto the piston assembly to impart the
force as indicated by control system
1010 (including a positive force, a negative force, or a force of zero). At step
1204, control system calculates a position-force trajectory for the one or more piston
assemblies based at least in part on a desired engine performance (
e.g., a desired apex position) and the current piston of the one or more piston assemblies
determined in step
1202. The calculation of a position-force trajectory by control system
1010 is computed without regard to a deviation from a previously determined trajectory
(position-force, time-position, or any other suitable trajectory). For example, instead
of using a trajectory that was calculated at the beginning of a stroke
(i.e., a previously calculated trajectory) and then compensating for deviations from this
previously calculated trajectory during the course of propagation, an entirely new
trajectory is calculated every time sequential steps
1202, 1204, and
1206 are repeated. This type of resolution allows for changes in and to the operating
state of the free-piston engine to be accounted for with each new position-force trajectory
calculation. Control system
1010 may calculate a position-force trajectory based also on a current or past operating
state of the engine. For example, control system
1010 may calculate a position-force trajectory based on any suitable properties of the
one or more piston assemblies (
e.g., velocities, accelerations, dimensions, mechanical properties), any suitable properties
of the combustion section gas (
e.g., pressure, temperature, density, specific heat, dimensions), any suitable properties
of the driver section (
e.g., gas properties if a gas spring, mechanical properties if a mechanical spring, dimensions),
any suitable properties of the LEM (
e.g., motor force constants, motor force limits, motor current limits, motor resistance),
any suitable properties of the engine performance (e.g., efficiency, power output,
air flow, fuel flow, exhaust flow, fuel composition, exhaust composition, temperatures,
pressures), any other suitable calculated, measured, or estimated values or indicators
of the operating characteristics, performance, parameters, and environment of the
engine, or any combination thereof.
[0066] FIG. 13 shows a position-velocity trajectory and position-force trajectory
(1310 and
1320, respectively) illustrating one embodiment of the position-force trajectory control
technique disclosed herein. In this embodiment, the desired engine conditions (on
which the calculation of position-force trajectories are based) are the desired apex
positions of the piston assembly (

and

). That is, the control objective is to effect the displacement of the piston assembly
such that it has zero velocity at the desired TDC and BDC positions. The actual apex
positions of the piston assembly (
xTDC and
xBDC) are shown, for illustrative purposes, in
FIG. 13 as being different than the desired positions of the piston assembly. It will be
understood, however, that the difference between the desired and actual apex positions
of a piston assembly can be zero, positive, negative, or any combination thereof,
and can vary depending on the specific implementation of a position-force trajectory
control technique. In this embodiment, a new position-force trajectory is calculated
at a fixed time interval as illustrated by the force values shown in the position-force
trajectory plot
1320 (i.e., at higher velocities the force values are applied to the piston assembly over a longer
distance, and at lower velocities the force values are applied to the piston assembly
over a shorter distance). That is, the sequential steps
1202, 1204, and
1206 in flow chart
1200 in
FIG. 12 are repeated at a fixed time interval (e.g., 1, 5, 100 kHz). All of the force values
in the position-force trajectory plot
1320 are shown, for illustrative purposes, in
FIG. 13 as being in the opposite direction of the motion of the piston assemblies
(i.e., the LEM is always converting kinetic energy of the piston assembly into electrical
energy). It will be understood, however, that each force value can be any suitable
force value, including a positive force value
(i.e., encouraging displacement of a piston assembly during an expansion stroke and discouraging
displacement of a piston assembly during a compression stroke), a negative force value
(i.e., encouraging displacement of a piston assembly during an compression stroke and discouraging
displacement of a piston assembly during a expansion stroke), or a zero or neutral
force value (
i.e., allowing the piston assembly displacement to continue using its current momentum
without applying any force).
[0067] In this embodiment, referring to
FIG. 13, the first position-force trajectory of a compression stroke is calculated at BDC,
as illustrated by the force value
F1 in the position-force trajectory plot
1320. Control system
1010 calculates this first force value (in the position-force trajectory step
1204 of flow chart
1200 in
FIG. 12) based at least in part on the current position of the piston assembly (determined
in step
1202) and the desired apex position of the piston assembly (

), and then applies this force to the piston assembly via a LEM of the engine (in
step
1206) until a new position of the piston assembly is determined and new position-force
trajectory is calculated, which occurs, in this embodiment, based on a prescribed
time interval. These sequential steps are repeated until the piston assembly apices
at TDC (
xTDC), at which point control system
1010 then repeats the sequential steps based on a new desired apex position at BDC (

). The desired apex positions may remain constant across cycles, remain constant within
a stroke, change across cycles, change within a stroke, or any combination thereof.
[0068] In some embodiments, control system
1010 may rely the First Law of Thermodynamics
(i.e., conservation of energy) to calculate a position-force trajectory at each step
1204. For example, for a single-piston free-piston engine, a position-force trajectory
can be calculated by recognizing that, over an idealized stroke of the engine
(i.e., no losses from heat transfer, gas blow-by, or friction), the work from/to the LEM,
the work from/to the combustion section gas, the kinetic energy of the piston assembly,
and the work from/to the driver section must sum to zero. This can be captured, for
example, in equation 1, where
WLEM is the work from/to the LEM,
Wc is the work from/to the combustion section gas,
KEp is the kinetic energy of the piston assembly, and
Wd is the work from/to the driver section.

The work from/to the LEM can be calculated by integrating the motor force (
FLEM) over the change in position (x) of the piston assembly from a current position of
the piston assembly (
xc) to a desired target position of the piston assembly (
xd)
(e.g., a desired apex position). Since each force value is applied to the piston assembly
by the LEM until a new force value is calculated and then subsequently applied, the
motor force can be modeled as being constant between a current position of the piston
assembly and a desired target position of the piston assembly. This simplifies the
calculation of the work from/to the LEM to just the motor force multiplied by the
difference between the desired target position and the current position, as shown
in equation 4, where
xd can be either a TDC or BDC desired target position.

The work from/to the combustion section gas can be calculated by integrating the
pressure of combustion section gas over the change in volume of the combustion section
from a the combustion section volume at a current position of the piston assembly
(

) to the combustion section volume at a desired target position of the piston assembly
(

). In this example, for a desired TDC and BDC target positions, the work from/to the
combustion section can be calculated according to equation 2, where
Vc is the volume of the combustion section,
pc is the combustion section gas pressure as a function of the volume of the combustion
section, and

can be based on either a TDC or BDC desired target position.

The kinetic energy of the piston assembly is equal to the one half the product of
the mass of the piston assembly (
mp) and the square of the current velocity of the piston assembly (
ẋc), as shown in equation 3.

The work from/to the driver section depends on the type of driver section. If the
driver section comprises a gas spring, then the work from/to the gas spring can be
calculated similarly to the calculation of the work from/to the combustion section
gas. If the driver, comprises a mechanical spring, then the work from/to the mechanical
spring may be calculated based on Hooke's Law. If the driver section comprises both
a gas spring and a mechanical spring, then the work from/to the driver section can
be calculated using a combination of the two models. In this example, for illustrative
purpose, the driver section comprises a gas spring, and the work from/to the gas spring
(driver section) can be calculated using equation 5, where
Ws is the work from/to the gas spring,
Vs is the volume of the gas spring,
ps is the gas spring gas pressure as a function of the volume of the gas spring,

is the volume of the gas spring at a current position of the piston assembly, and

is the volume of the gas spring at the desired target position of the piston assembly
which can be based on either a TDC or BDC desired target position.

Having models for calculating the work and energy values in equation 1, a motor force
value of a position-force trajectory can be calculated by substituting equations 2-5
into equation 1, as shown in equation 6.

As can be seen in equation 6, this model for calculating a position-force trajectory
has a shrinking horizon as the current position of the piston assembly approaches
the desired target position of the piston assembly (
i.e., the denominator in equation 6 approaches zero). Practical limits can be set by
or input to control system 1010 on the minimum horizon (
i.
e., the minimum difference between the current position of the piston assembly and
the desired target position of the piston assembly) to avoid division by zero, which
may, in some embodiments, limit the effective authority of control system
1010 near a desired target position. If the cross-sectional areas of interface between
the piston assembly and the combustion section gas and the gas spring gas can be modeled
as being constant, the combustion section gas work and the gas spring gas work in
equation 6 can be calculated based on the change in piston assembly position from
a current position to a desired target position since the volume of the respective
sections is an affine function of the position of the piston assembly. This substitution
is shown in equation 7, where
pc(
x) is the combustion section gas pressure as a function of the position of the piston
assembly,
ps(
x) is the gas spring gas pressure as a function of the position of the piston assembly,
Ac is the cross-sectional area of interface between the piston assembly and the combustion
section gas, and
As is the cross-sectional area of interface between the piston assembly and the gas
spring gas.

[0069] As shown in equations 6 and 7, each position-force trajectory is calculated based
at least in part on the current position of the piston assembly and the desired apex
position
(i.e., desired target position) of the piston assembly, without regard to a deviation from
a previously determined trajectory, without regard to the time in which a new position-force
trajectory will be calculated, and without regard to the time in which the piston
assembly reaches the desired apex position. Repeatedly calculating a position-force
trajectory using this model over a stroke of an engine cycle allows for changes in
and to the operating state of the free-piston engine (rapid or slow, intended or unintended)
to be accounted for in each new position-force trajectory calculation, thereby providing
a control technique for a free-piston engine that is capable of rejecting disturbances
in the operating state of the engine. The control technique is capable of rejecting
disturbances due to, for example, combustion variability, combustion misfires, changes
in fuel energy content, changes in gas temperatures or pressures, loss of LEM phases,
changes in or to the driver section spring constant, or any other suitable disturbance,
or any combination thereof. Equations 6 and 7 were derived assuming that there were
no energy losses within the engine, such as, for example, from heat transfer, gas
blow-by, or friction. However, it will be understood that energy losses can be included
in the position-force trajectory control technique disclosed herein. For example,
heat transfer losses in a gaseous section of an engine can be modeled as a function
of gas temperature (which can be modeled as a function of position or volume), heat
transfer losses in a LEM can be modeled as a function of electrical current and resistance,
gas blow-by losses in a gaseous section of an engine can be modeled as a function
of gas pressure (which can be modeled as a function of position or volume), and friction
losses can be modeled as a function of contact forces, material properties, position,
and/or velocity.
[0070] Solving equation 6 requires integration of pressure over a change in volume for,
in this example, both the combustion section gas and gas spring gas. These integrals
can be computed using a numerically iterative solution (e.g., an ordinary differential
equation solver) based on thermodynamic property models, heat transfer models, gas
blow-by models, friction models, or any other suitable model, or any combination thereof.
These integrals can also be computed using a closed-form solution based on thermodynamic
models that may incorporate effects from heat transfer, gas blow-by, friction, and
other losses in the system. Using a closed-form solution to calculate a position-force
trajectory saves computation time compared to a numerically iterative solution. This
can allow the control system
1010 to calculate a new position-force trajectory in shorter time intervals
(i.e., at a faster frequency), which can better account for disturbances in the operating
state of the engine. For example, the compression and expansion of the gases in the
combustion section and gas spring can be modeled as being reversible. The reversible
work for the compression and expansion of a gas can be calculated using equation 8,
where
p1 is the pressure of the gas at state 1,
V1 is the volume of the gas at state 1,
V2 is the volume of the gas at state 2, and
k is the ratio of specific heats.

Modeling the compression and expansion of the combustion section gas and gas spring
gas as being isentropic, can yield a closed-form solution for calculating a position-force
trajectory, as shown in equation 9, where
kc is the ratio of specific heats for the combustion section gas and
ks is the ratio of specific heats for the gas spring gas.

As shown in equation 9, different ratios of specific heats can be used for the combustion
section gas and the gas spring gas
(e.g., to account for differences in composition). Different ratios of specific heats can
also be used for a compression stroke and an expansion stroke
(e.g., to account for the changes in composition of the combustion section gas), for specific
position intervals within a stroke (e.g., to account for changes during engine breathing
while ports are exposed), for each calculation of a position-force trajectory (e.g.,
to account for changes in gas temperature), for any other suitable purpose or reason,
or any combination thereof. A closed-form solution can also be derived by modeling
the gas compression and expansion as being a polytropic process, as shown in equation
10, where
nc is the polytropic exponent for the combustion section gas and
ns is the polytropic exponent for the gas spring gas.

Modeling the compression and expansion of gases as being a polytropic process allows
for the effects of heat transfer, gas blow-by, friction, other losses, or any combination
thereof, to be accounted for while maintaining a closed-form solution for calculating
a position-force trajectory. The polytropic exponents for the combustion section gas
and the gas spring gas can be based on modeled or empirically determined engine performance
data or information. Different polytropic exponents can be used for a compression
stroke and an expansion stroke, for specific position intervals within a stroke, for
each calculation of a position-force trajectory, for any other suitable purpose or
reason, or for any combination thereof.
[0071] In order for control system
1010 to solve equations 9 or 10, the pressure of the gases in the combustion section and
gas spring must be measured or estimated, or both, at each current position of the
piston assembly. The pressure of the gases at a current position of the piston assembly
can be measured using any suitable sensor(s)
1030 such as piezoelectric pressure transducers, strain-based pressure transducers, gas
ionization sensors, any other suitable pressure sensor, or any combination thereof.
The pressure of the gases at a current position of the piston assembly can also be
estimated. In general, relying on estimates of pressure (as opposed to measurements
of pressure) can save cost and lead to higher reliability engine operation because
it avoids the need for expensive and often unreliable pressure sensors. For example,
the compression and expansion of the gases can be modeled as being isentropic or polytropic
using equations 11 or 12, respectively, where
p̂c is the estimated gas pressure at a current position of the piston assembly,
pp is the measured or estimated gas pressure at a previously determined position of
the piston assembly, and
Vp is the measured or estimated volume of the gas at the same previously determined
position of the piston assembly. Equations 11 and 12 are applicable to estimating
the current gas pressures in any section of an engine, including a combustion section
and driver section.

In another example, for a single-piston free-piston engine with a gas spring driver
section, a force balance model can be applied to the translator to estimate a current
gas pressure of the combustion section based on a measured or estimated current gas
pressure of the gas spring, a previously applied/calculated motor force value, the
mass of the piston assembly, and a current measured or estimated acceleration of the
piston assembly. This force balance model is shown in equation 13, where

is the estimated gas pressure in the combustion section at the current position of
the piston assembly,
ẍc is a current acceleration of the piston assembly,

is a previously applied/calculated motor force, and

is the measured or estimated current gas pressure in the gas spring.

A force balance model may also be used to estimate a previous gas pressure of the
combustion section based on previously measured or estimated other values, which can
then be used to calculate a current gas pressure of the combustion section through,
for example, equations 11 or 12. This force balance model is equation 14, where

is the estimated gas pressure of a combustion section at a previous position of the
piston assembly,
ẍp is the previously determined acceleration of the piston assembly, and

is the previously determined gas pressure of the gas spring.

It will be understood that force balance models (similar to those used to derive
equations 13 and 14) can also be used to estimate the current or previous gas pressures
in other section of an engine, such as, for example, a driver section.
[0072] In some embodiments, control system
1010 may estimate a current gas pressure in a section of a free-piston engine by integrating
energy balances over a stroke of an engine cycle from a fixed previous position to
a current position of a free-piston assembly, where a fixed previous position may
be, for example, an apex position, a port opening or closing position, a combustion
event, any other suitable position, or any combination thereof. For example, for a
single-piston free-piston engine with a gas spring driver section, a current gas pressure
can be estimated by using equation 15, which models the energy balance of a free-piston
assembly from a fixed previous position to a current position, where

is the work from/to the LEM from the fixed previous position to the current position,

is the work from/to the combustion section gas from the fixed previous position to
the current position, and

is the work from/to the gas spring section gas from the fixed previous position to
the current position.

The compression and expansion of the gases in the combustion section and gas spring
section can be modeled as being reversible and/or polytropic to yield closed-form
solutions for the work from/to the respective sections. Modeling the compression and
expansion of the gases in the combustion section and gas spring section as being polytropic,
for this example, the work from/to the combustion section and from/to the gas spring
section from a fixed previous position and current position can be calculated using
equations 16 and 17, respectively, where

is the measured or estimated combustion section gas pressure at the fixed previous
position,

is the combustion section volume at the fixed previous position,

is the measured or estimated gas spring section gas pressure at the fixed previous
position, and

is the gas spring section volume at the fixed previous position.

The work from/to the LEM can be calculated using equation 18, which updates the amount
of work from/to the LEM with each calculation step, where
xip is the position of the piston assembly at the immediately preceding calculation step,

is the LEM force determined at the immediately preceding calculation step (and then
applied to the piston assembly from its position at the immediately preceding calculation
step to its current position), and

is the amount of work from/to the LEM from the fixed previous position to the position
of the piston assembly at the immediately preceding calculation step.

The kinetic energy of the piston assembly at the current position can calculated
using equation 3. Equations 16-18 and 3 can be substituted into equation 15 to estimate
a current gas pressure in the combustion section or gas spring section using a closed-form
solution. For example, equation 19 shows a closed-form solution for estimating a current
pressure of the combustion section gas.

Equations 6, 7, 9, and 10, or any other suitable First Law-based analysis used to
derive similar equations (e.g., to include losses within the engine), may also be
used, separately or in combination, to estimate a current or previous gas pressure
in a section of a free-piston engine using similar techniques as those used to derive
equations 11-14 and 19
(i.e., through the use of current and previously determined pressures, forces, volumes,
positions, velocities, and accelerations). Additionally, equations 11-14 and 19 may
be used in combination with each other and/or with other suitable estimation models
to estimate a current or previous gas pressure in a section a free-piston engine using
similar techniques as those used to derive equations 11-14 and 19
(i.e., through the use of current and previously determined pressures, forces, volumes,
positions, velocities, and accelerations).
[0073] Using previously calculated values (e.g., force, acceleration, pressure, velocity,
position) to estimate a current value (e.g., a current gas pressure) may require the
use of a smoothing filter such as an infinite impulse response (IIR) filter or finite
impulse response (FIR) filter with suitable coefficients to the values of interest,
or a dynamic estimator such as a Luenberger observer or Kalman filter. The pressure
of gases at a current or previous position of the piston assembly can be estimated
using thermodynamic relation models (e.g., equations 11 or 12), force balance models
(e.g., equations 13 or 14), or First Law analysis
(e.g., equations 6, 7, 9, 10, or 19), or any combination thereof. For example, the pressure
of the gases at a current or previous position of the piston assembly can be estimated
using two models, with one of the models being used as a primary estimate and the
other model being used to improve the primary estimate using an estimation technique,
such as an Kalman filter, Luenberger observer, or model-predictive estimation. In
another example, the pressure of the gases at a current or previous position of the
piston assembly can be estimated based on a minimization of error between the estimates
from any two models. This minimization can weight the two models and include other
costs such as, for example, acceleration estimates given several position measurements,
deviation from previous pressure measurements or estimates, deviation from pressure
measurements or estimates from prior cycles or strokes, computation time, information
on noise or disturbance statistics, any other suitable cost, or any combination thereof.
In some embodiments, estimations of the gas pressures at a current or previous position
of the piston assembly can be improved upon by measurements of pressure from any otherwise
unsuitable sensor, which may provide inadequate, noisy, or slow measurements.
[0074] When the absolute velocity of a piston assembly is low and its absolute acceleration
is high, the efficiency of a LEM may be low and the ability of a LEM to effect the
displacement of the piston assembly may be limited. In order to avoid a LEM applying
forces to the piston assembly when its efficiency is low and control authority is
limited, in some embodiments, control system
1010 may reduce or eliminate the magnitude of force applied to a piston assembly based
on specified operating parameters of a free-piston engine. Specified operating parameters
may include position, velocity, or acceleration of a piston assembly, temperature
of the stator or translator of the LEM, gas pressure in a section of the engine, any
other suitable parameter, or any combination thereof. For example, control system
1010 may cut-off the ability of the LEM to apply forces to a piston assembly based on
the position of the piston assembly as shown in
FIG. 14, which shows position-velocity trajectory
1410 and position-force trajectory
1420. In this example, control system
1010 calculates a position-force trajectory in accordance with the present disclosure,
but when the position of the piston assembly is outside of the cut-off positions,
control system
1010 determines to not apply the force values calculated in the position-force trajectory
calculation step
1204 to the piston assembly. In some embodiments, control system
1010 may determine to apply a different amount of force to a piston assembly than the
force values calculated in the position-force trajectory calculation step
1204 based on specified operating conditions of a free-piston engine. For example, control
system
1010 may apply a force-reduction function to the force values calculated in the position-force
trajectory calculation step
1204 based on a position of the piston assembly (e.g., outside of the cut-off positions)
in order to avoid abrupt changes in the operating state of the engine. In some embodiments,
control system
1010 may determine to both not calculate a position-force trajectory and not apply a force
to a piston assembly based on specified operating conditions of a free-piston engine.
[0075] While the various models for calculating a position-force trajectory and estimating
gas pressure
(i.e., equations 1-19) have been directed towards a single-piston free-piston engine, it
will be understood that the same models can be extended and applied to free-piston
engines with multiple piston assemblies, such as, but not limited to, opposed-piston
free-piston engines with respective driver sections, respective LEMs, and a shared
combustion section (e.g., as illustrated in
FIGS. 2-4 and
FIG. 7). For example, the same First Law analysis used to derive equation 1 can be applied
to each piston assembly of an opposed-piston free-piston engine with respective driver
sections, respective LEMs, and a shared combustion section. This yields energy balance
equations 20a and 20b, where
WLEM,1 and
WLEM,2 is the work from/to the two LEMs,
Wc is the work from/to the combustion section gas,
KEp,1 and
KEp,2 is the kinetic energy of the two piston assemblies, and
Wd,1 and
Wd,2 is the work from/to the two driver sections. Equations 20a and 20b can be used by
control system
1010 to calculated a position-force trajectory for each respective piston assembly using
the same or similar models as those used to derive equations 6, 7, 9, and 10.

In similar manner in which equation 1 was extended to a free-piston engine with multiple
piston assemblies (e.g., equations 20 a and 20b), it will be readily apparent that
the same force balance models used to derive equations 13 and 14, and the same First
Law analysis used to derive equation 15 can be extended to free-piston engines with
multiple piston assemblies for estimating gas pressure in a section of the engine.
[0076] A consideration that arises in the control of free-piston engines with opposed piston
assemblies, is the synchronization of the piston assemblies. In some opposed-piston
free-piston engines, it can be desired that the apices (at both TDC and BDC) of the
two piston assemblies be at least substantially synchronized in order to maintain
system stability. In other opposed-piston free-piston engines, some level of nonsynchronization
can be desired for engine performance purposes, such as, for example, engine breathing,
gas exchange, or any other suitable engine operating condition. In some embodiments
of an opposed-piston free-piston engine, control system
1010 may regulate a difference between the positions of the respective piston assembly.
As used herein, the term "regulate" refers to controlling to a reference, such as,
for example, zero. Control system
1010 may employ any suitable control technique for regulation, such as proportional-integral-derivative
(PID) control, optimal control, robust control, linear-quadratic regulator control,
model-predictive control, adaptive control, any other suitable technique, or any combination
thereof. In some embodiments, control system
1010 may use PID control to regulate and synchronize the positions of piston assemblies.
For example, control system
1010 may use PID control to determine control inputs (e.g., forces values to be applied
to the piston assemblies by respective LEMs) to regulate a difference in position
between the piston assemblies relative to their center of motion. Opposite forces
may be added to each piston assembly to synchronize each substantially equally and
minimize the disturbance on apex positions. This may be done continuously to substantially
balance net forces and, therefore, maintain sufficient synchronization. In some embodiments,
control system
1010 may use a specified Poincare map at the zero-velocity positions of the piston assemblies
(
i.e., at the respective apices). For example, control system
1010 can split a stroke into two halves and apply additional motor force in one direction
during the first half of the stroke and then apply additional motor force in the opposite
direction during the second half of the stroke. Control system
1010 can determine prior to an expansion stroke that a first piston assembly is going
to be late to BDC (e.g., using any suitable expected phasing of the two piston assemblies,
based on timing of a previous stroke, based on any other suitable technique, or any
combination thereof), and apply additional motor force to this first piston assembly
during the first half of the expansion stroke in the direction of motion
(i.e., encouraging displacement) and then apply additional motor force to this first piston
assembly during the second half of the expansion stroke in the opposite direction
of motion during
(i.e., discouraging displacement). Conversely for the second piston assembly, control system
1010 can apply additional motor force to this second piston assembly in the opposite direction
of motion during the first half of the expansion stroke
(i.e., discouraging displacement) and then apply additional motor force to this second piston
assembly in the direction of motion during the second half of the expansion stroke
(
i.e., encouraging displacement). In some embodiments, control system
1010 may determine synchronization forces based on a desired timing of a desired engine
performance. For example, control system
1010 may determine synchronization forces to be applied to one or both piston assemblies
such that the apices of the respective piston assemblies occur within a sufficiently
small time difference.
[0077] In some embodiments, control system
1010 may use a repetitive adaptive control technique. Repetitive adaptive control can
be advantageous when the operating state, condition, performance, and/or parameters
of a free-piston engine are relatively steady and the cycle-to-cycle variation is
limited. In some embodiments, control system
1010 may use a repetitive adaptive control technique that determines a position-force
trajectory at each step
1204 for a current engine cycle based on the position-force trajectory from a previous
engine cycle. In some embodiments, control system
1010 may use a repetitive adaptive control technique that drives force values toward a
known and desirable propagation path (e.g., to enforce a smoother or more continuous
force profile). For example, control system
1010 may first approximate, based on information from a previous cycle
(e.g., force values, engine performance,
etc.), a position-force trajectory as a series of discrete force values over an engine cycle.
Control system
1010 may then cause the discrete force values to be applied to the piston assembly over
each stroke of the engine cycle, and at the end of each cycle, control system
1010 may adjust the discrete force values based on engine operating characteristics, measurements,
performance, and/or conditions. Control system
1010 may alter all or some of the discrete force values prior to a subsequent cycle if,
for example, a piston assembly does not sufficiently achieve a desired target position
for a given stroke. For example, if a piston apexes short of the desired target TDC
on a previous cycle, control system
1010 may, on the subsequent cycle, reduce the magnitude of the some or all of the discrete
force values. In embodiments with opposed-piston free-piston engines with a shared
(or common) combustion section, control system
1010 may alter the discrete force values in one or more portions of a stroke for one or
both of the piston assemblies, dependently or independently, during the subsequent
cycle. For example, if on a current engine cycle an exhaust piston assembly reached
its apex at TDC after the intake piston assembly reached its apex at TDC, control
system
1010 can, on the subsequent cycle, adjust the discrete force values applied to the exhaust
piston assembly and not adjust the discrete force values applied to the intake piston
assembly in order to achieve sufficient synchronization at TDC. This can be achieved
by, for example, control system
1010 reducing the magnitude of the discrete force values applied to the exhaust piston
assembly over the first half of the stroke, thereby allowing the midpoint velocity
of the piston to increase, and then increasing the magnitude of the discrete force
values applied to the exhaust piston assembly over the second half of the stroke,
thereby achieving sufficient synchronization at TDC. In some embodiments, control
system
1010 may use a repetitive adaptive control technique that is based on calculating a deviation
from a previously determined trajectory (position-force, position-velocity, time-position,
or any suitable trajectory).
[0078] In some embodiments, control system
1010 may use a hybrid control technique that is capable of switching between multiple
control techniques. A hybrid control technique can be advantageous for controlling
a free-piston engine across a wide range of operating conditions, controlling a free-piston
engine when sufficiently fast and large disturbances in engine operation may occur
(e.g., combustion misfire, mechanical failures, gas quality changes, or any other
suitable changes), and controlling a free-piston engine under steady or stable operating
conditions (e.g., at steady and continuous power output). For example, control system
1010 can employ a position-force trajectory control technique during engine start up and
then switch to a repetitive adaptive control technique when the engine operation becomes
sufficiently stable or steady. Control system
1010 can then switch back to a position-force trajectory control technique if a sufficiently
large disturbance is detected or if a new engine operating condition is desired (e.g.,
more or less power output, engine shut down).
FIG. 15 illustrates one possible implementation of a hybrid control technique. Control system
1010 uses a position-force trajectory control technique at
1502. If control system
1010 determines that conditions become sufficiently steady based on any suitable criteria
(e.g., absence of misfires, stable power output, stable efficiencies, thermal equilibrium,
or other suitable conditions), control system
1010 switches to a repetitive adaptive control technique at
1504. If control system
1010 determines that operating conditions have or will become sufficiently unsteady based
on any suitable criteria, control system
1010 switches back to a position-force trajectory control technique at
1502.
[0079] For ease of reference, the figures may show multiple components labeled with identical
reference numerals. It will be understood that this does not necessarily indicate
that the multiple components identically labeled are identical to one another. For
example, the pistons labeled
125 may have different sizes, geometries, materials, any other suitable characteristic,
or any combination thereof.