U.S. patent number 3,743,446 [Application Number 05/161,656] was granted by the patent office on 1973-07-03 for standing wave pump.
This patent grant is currently assigned to Atek Industries, Inc.. Invention is credited to Harold Mandroian.
United States Patent |
3,743,446 |
Mandroian |
July 3, 1973 |
STANDING WAVE PUMP
Abstract
An efficient fluid pump which has a chamber for receiving the
fluid to be pumped and a transducer for establishing a travelling
wave in the fluid. The length of the chamber and the frequency of
the transducer are adjusted so that a standing wave pattern is set
up in the fluid having one or more pressure nodes and one or more
pressure antinodes in it. At least one entrance port is provided in
the chamber at the pressure nodes and at least one exit port is
provided in the chamber at the pressure antinodes so that fluid
will be drawn into the cylinder at the pressure node and will be
forced out of the cylinder at the pressure antinode to achieve a
pumping action.
Inventors: |
Mandroian; Harold (La Canada,
CA) |
Assignee: |
Atek Industries, Inc. (North
Hollywood, CA)
|
Family
ID: |
22582152 |
Appl.
No.: |
05/161,656 |
Filed: |
July 12, 1971 |
Current U.S.
Class: |
417/240; 417/322;
310/323.01; 310/322 |
Current CPC
Class: |
F04F
7/00 (20130101) |
Current International
Class: |
F04F
7/00 (20060101); F04f 007/00 () |
Field of
Search: |
;331/176
;417/53,240,241,322,437,557 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Freeh; William L.
Assistant Examiner: Winburn; John T.
Claims
What is claimed is:
1. A pump comprising:
a chamber for receiving a fluid to be pumped;
driver means, including transducer means, for establishing
travelling waves in said fluid in said chamber, said transducer
means being positioned within said chamber to create travelling
waves on both sides of said transducer;
means including said driver means and said chamber for converting
said travelling waves to standing wave patterns in said fluid in
said chamber on both sides of said transducer having one or more
pressure nodes and one or more pressure antinodes therein;
at least one entrance port in said chamber at said pressure nodes;
and
at least one exit port in said chamber at said pressure
antinodes.
2. The pump of claim 1 wherein entrance and exit ports are
positioned in said chamber on both sides of said transducer
means.
3. A pump comprising:
a chamber for receiving a fluid to be pumped;
driver means for establishing a travelling wave in said fluid in
said chamber;
means including said driver means and said chamber for converting
said travelling wave to a standing wave pattern in said fluid in
said chamber having one or more pressure nodes and one or more
pressure antinodes therein, said chamber, said driver means and
said aforesaid means forming an oscillator circuit and said
travelling wave generating a positive feedback in said oscillator
circuit to adjust the frequency of said driver means at the
resonant frequency of said chamber;
at least one entrance port in said chamber at said pressure nodes;
and
at least one exit port in said chamber at said pressure
antinodes.
4. A pump comprising:
a chamber for receiving a fluid to be pumped;
driver means for establishing a travelling wave in said fluid in
said chamber;
means including said driver means and said chamber for converting
said travelling wave to a standing wave pattern in said fluid in
said chamber having one or more pressure nodes and one or more
pressure antinodes therein;
at least one entrance port in said chamber at said pressure nodes,
said entrance port comprising a valveless opening in said chamber;
and
at least one exit port in said chamber at said pressure
antinodes.
5. The pump of claim 4 wherein said driver means includes a pair of
synchronized transducers each one positioned at one end of said
chamber to obtain a greater pressure differential in said nodes and
antinodes.
6. The pump of claim 4 wherein said chamber includes a bellows-type
section operable to expand and contract with temperature
variations.
7. The pump of claim 4 wherein said driver means includes a
transducer and said transducer is supported by a webbing coupled to
the sides of said chamber, said entrance or exit port being formed
between said transducer and said chamber sides.
8. A pump comprising:
a chamber for receiving a fluid to be pumped;
driver means for establishing a travelling wave in said fluid in
said chamber;
means including said driver means and said chamber for converting
said travelling wave to a standing wave pattern in said fluid in
said chamber having one or more pressure nodes and one or more
pressure antinodes therein;
at least one entrance port in said chamber at said pressure nodes;
and
at least one exit port in said chamber at said pressure
antinodes;
said driver means including a transducer and said transducer being
supported by a webbing coupled to the sides of said chamber, said
entrance or exit port being formed between said transducer and said
chamber sides.
Description
BACKGROUND OF THE INVENTION
1. Field of the Invention
This invention relates to apparatus for pumping fluids.
2. Description of the Prior Art
The art of pumping fluids so that they may be transported from one
place to another is extremely old, starting with such pumping
devices as the water wheel and the Archimedes screw. More recently
there have been developed reciprocating pumps of the type
comprising an enclosure or chamber communicating through intake
valves with a source of fluid under an initial pressure and through
delivery valves with a space constituting a receiver for a fluid
under a final pressure, the chamber including a movable wall to
which a reciprocating movement is imparted to expand the capacity
of it to fill it through the intake valves and then to contract the
capacity and to evacuate it through the delivery valves. Many other
variations on this technique of providing a chamber which is
expanded to receive fluid and then contracted to force it out
through the delivery valves have been devised, such as providing
the pumping action by means of a flexible membrane to change the
configuration of the chamber, a flexible tube which allows the
fluid to enter and then squeezes it out, and a two-chamber system
separated by a diaphragm in which an actuating fluid in the first
chamber means causes the diaphragm to periodically pulsate and to
displace a portion of the actuated fluid from the second chamber
means. In a somewhat different form of pumping device, a diaphragm
is actuated to cause a flow of fluid to be pumped across the throat
of an orifice and thus to establish a zone of low pressure; due to
this venturi effect, a fluid is pumped through the throat into the
main body of the system and then is ultimately forced out of the
system to achieve a pumping action.
As can be seen from the construction and operation of these prior
art devices, these devices are subject to mechanical failure and
fatigue where reciprocating pistons and valves or flexible
diaphragms are used to draw fluid into a chamber and to force it
out of the chamber and suffer from a low efficiency due to the
amount of power required to operate the moving pistons, diaphragms
and valves to achieve the pumping action and due to the presence of
the unpumped or residual volume left in the pumping chamber at the
end of the compression stroke. In addition, the pump system
utilizing the venturi effect necessitates a very fast flow of a
large bulk of fluid across the throat in order to achieve a
satisfactory zone of low pressure and thus causes a large amount of
strain and fatigue on the pumping diaphragm and the damping
diaphragm used in the construction of the pump, along with a large
amount of power input for a relatively small flow of output
fluid.
OBJECTS AND SUMMARY OF THE INVENTION
The principal object of the present invention is to provide a new
and improved pump for pumping fluids which avoids the pumping
deficiencies of the prior art apparatus.
A more specific object of the invention is to provide a pump in
which the moving elements are not utilized to provide a pumping
pressure to the fluid to be pumped.
Another object of the invention is to provide a pump which has a
high efficiency of operation.
A further object of the invention is to provide a pump in which the
pumping pressure is provided by a nearly motionless actuating
fluid.
In accordance with one embodiment of the present invention, a pump
is provided which has a cylindrical chamber having as one end wall
a fluctuating diaphragm. The diaphragm is caused to oscillate at a
preselected frequency by means of a power supply and driver to set
up a travelling wave in the fluid in the chamber. The frequency of
oscillation of the diaphragm and length of the chamber are
configured that the chamber is a resonant chamber and thus a
standing wave is set up in the fluid having a pressure antinode or
node at the wall opposite the diaphragm and a series of pressure
nodes and pressure antinodes spaced along the length of the
chamber, the particular number depending upon the length of the
chamber and the frequency of vibration of the diaphragm. An
entrance port is located in the chamber at one of the pressure
nodes and on exit port is located in the chamber at one of the
pressure antinodes. Due to the pressure differential between the
pressure node and the pressure antinode, fluid outside the chamber
at the pressure node will be forced into the chamber and fluid
outside the chamber at the pressure antinode will be forced out,
thus achieving a pumping action.
The novel features of the invention are set forth with
particularity in the appended claims. The invention will best be
understood from the following description when read in conjunction
with the accompanying drawings.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a partly schematic, partly sectional view of a pumping
device embodying the novel features of the invention;
FIG. 2 illustrates a second embodiment of the invention showing
more fully the principles of the pumping action;
FIG. 3 illustrates a third embodiment of the present invention;
FIG. 4 illustrates a fourth embodiment of the present
invention;
FIG. 5 illustrates another embodiment of the invention in which the
high efficiency of the pump is maintained.
DESCRIPTION OF THE PREFERRED EMBODIMENT
In FIG. 1, an embodiment of the present invention is illustrated. A
chamber 10 is provided which has an entrance port 12 and an exit
port 14 whose positions are determined, as explained more fully
hereafter, by the location of the pressure nodes and antinodes of a
standing wave generated in the chamber 10. Forming one wall of the
chamber 10 is a transducer element 18 comprising a flexible
diaphragm 15 which has a magnetic slug 16 attached thereto, a coil
20 and a core 22 attached to the opposite wall 24 of the transducer
18. The coil 20 of the transducer 18 is energized by a driver 26,
such as an oscillating circuit, which in turn is energized by a
power supply 28.
In operation, the driver 26 causes the coil 20 to be cyclically
energized at a predetermined frequency and thus causes the
diaphragm 15, by means of the coil's attraction on the magnetic
slug 16, to vibrate at such preselected frequency and to cause a
travelling wave to be generated in the fluid in the chamber 10. If
the length of the chamber 10 is made to be equal to an integer
times the wave length of the travelling wave in the fluid divided
by 4, i.e. n..lambda./4, the chamber 10 will act as a resonant
cavity and will have a standing wave pattern set up in it. As is
well known, the wave length of the wave in the fluid is equal to
the velocity of the wave in the fluid divided by the frequency of
the wave pattern. Thus if the fluid is water and the diaphragm 15
is excited by a five thousand cycle signal, the minimum length of
the chamber 10, that is the wave length divided by 4, would be
0.246 feet since the velocity of a 5,000-cycle wave in water under
standard conditions is 4,920 feet per second. If the frequency of
excitation were reduced to 1,000 cycles per second, then the length
of the chamber 10 would be 1.23 feet. If, on the other hand, the
fluid in the chamber 10 were air, then for a 1,000-cycle excitation
signal, the minimum length of the chamber would be 0.28 feet since
the velocity of the wave in air under standard conditions is 1,130
feet per second.
The placement of the entrance port 12 and the exit port 14 in
relation to the operation of the invention is best illustrated with
reference to FIG. 2. When the transducer 18 is excited by the
driver 26, it causes an initial wave, shown by the solid line, to
travel in the fluid in the chamber 10. When this wave hits the far
wall 32 of the chamber 10 it is reflected back, shown by the dashed
wave, 180.degree. out of phase with the initial wave. If the
chamber 10 has been configured so as to be an integral number of
quarter wavelengths long, the reflected wave, when it reaches the
diaphragm wall 15, will be reflected 180.degree. out of phase and
thus coincident with the initial wave. In addition, the reflected
wave will be reinforced by the motion of the diaphragm since it is
in synchronization therewith. Thus a standing wave pattern, as
shown in FIG. 2, is set up in the chamber 10 which has a
displacement node or a pressure antinode at the end wall 32, a
pressure node or displacement antinode at the diaphragm 15 and a
series of such nodes and antinodes between the two end walls of the
chamber. Since the pressure nodes, indicated by the numeral 36, are
points of minimum pressure in the fluid, a series of entrance ports
12, 12', 12" are placed in the wall of the chamber 10 at such
pressure nodes, while since the pressure antinodes, indicated by
the numeral 38, are points of maximum pressure in the fluid, a
series of exit ports 14, 14', 14", are placed in the wall of the
chamber 10 at such pressure antinodes. Thus, when the fluid in the
chamber 10 is excited by the action of the transducer 18 and a
standing wave pattern is set up therein consisting of pressure
nodes and antinodes, the fluid immediately outside the chamber 10
at the entrance ports 12, 12', 12" will be drawn into the chamber
10 and the fluid inside the chamber 10 at the exit ports 14, 14',
14" will be forced out of the chamber 10 due to the pressure
differentials at the pressure nodes and the pressure antinodes.
Thus the apparatus shown in FIGS. 1 and 2 produces a pumping action
due to the differential pressure in the fluid in the chamber
10.
In FIG. 3 a third embodiment of the invention is shown. In this
embodiment there are two chambers 10 and 10' having entrance ports
12 and 12' and exit ports 14 and 14'. The two chambers 10 and 10'
are separated by a transducer 18 excited by driver 26, which
transducer 18 is in this particular instance shown as a
piezoelectric crystal. Upon receiving alternating voltages from the
driver 26, the piezoelectric crystal alternately expands and
contracts to cause standing travelling and then standing waves to
exist in the chambers 10 and 10'. As should be noted from FIG. 3,
the chambers 10 and 10' are of unequal length but with each one
being an integral number of quarter wavelengths in overall length.
In this particular embodiment, the piezoelectric crystal is in a
loaded condition and acts with greater efficiency to pump the fluid
in chambers 10 and 10'. In addition, chambers 10 and 10' could
originally have been formed as a single chamber with the
piezoelectric crystal being inserted at any point therein to effect
a separation of chambers, as long as the length of each of the
chambers remains an integral number of quarter wavelengths in
length. The standing wave patterns on either side of the transducer
18 may be in phase or out of phase with each other depending on the
operation of the transducer 18.
In FIG. 4 a fourth embodiment of the invention is shown. In this
embodiment one wall of the chamber 10 is formed by the transducer
18 supported by a webbing 40 coupled to the outer wall 42 of the
chamber 10, while the opposite wall of the chamber 10 is formed by
an end plate 44 supported by a webbing 46 coupled to the outer wall
42 of the chamber 10. The entrance port 12 in this configuration is
formed between the transducer 18 and the outer wall 42 of the
chamber 10 and the exit port 14 is formed in a similar manner
between the end plate 44 and the outer wall 42 of the chamber 10.
The electrical coupling between the driver 26 and the transducer 18
is achieved through a hollowed out portion of the webbing 40.
It should be noted that in FIGS. 1 to 3 the transducer need not be
a diaphragm or a piezoelectric crystal, but may be a series of
magnets or coils driven to produce a wave in the chamber by magneto
hydrodynamic forces and that in such case the end walls could be
identical with the transducer operating through or as a part of the
outer wall 42 of the chamber 10. Thus the fluid itself in the
chamber 10 would act as a diaphragm. In addition, while it may be
preferable to have the chamber 10 an exact number of quarter
wavelengths in length, nonetheless by the introduction of reactive
elements into the chamber 10, such as a deformation or bulge in the
outer wall 42, or a side chamber connected to the outer wall 42,
the actual length of the chamber 10 may be shorter or longer than
the effective length of the chamber 10 which is kept at an integral
number of quarter wavelengths in length.
Since the efficient operation of the pump requires that it be
operated in a resonant condition, it is necessary that the length
of the chamber 10 be maintained at an integral number of quarter
wavelengths independent of the velocity of the wave in the fluid in
the chamber 10. Thus, since the velocity of the wave in the fluid
is temperature dependent, the embodiment shown in FIG. 5
illustrates the use of a temperature sensor 48 which has a feedback
path 50 coupled to the driver 26. The temperature sensor 48 may,
for example, be a thermocouple which sends back a voltage dependent
on the temperature of the fluid, which voltage serves to vary the
frequency output of the driver 26 and thus to alter the frequency
of the wave in the fluid such that the chamber 10 remains an
integral number of quarter wavelengths in length. As an alternative
to using such a temperature sensor, the chamber 10 shown in FIG. 5
has also provided therein a bellows-type section 52 which serves to
expand and contract depending on the temperature of the fluid in
the chamber 10. In this manner as the velocity of the wave in the
fluid changes due to temperature changes, so does the length of the
chamber so as to keep the length of the chamber an integral number
of quarter wavelengths in length for a fixed frequency of
excitation of the transducer 18 by the driver 26.
In lieu of either of the above methods for maintaining the pump in
a resonant condition, the chamber 10 itself may be used as the
frequency determining element in an oscillator circuit. In this
embodiment a voltage generated by a crystal oscillator circuit is
applied to a piezoelectric crystal which is part of such circuit
and which forms one wall of the chamber 10, as in FIGS. 1 or 3. The
deformation of the crystal, which is acoustically coupled to the
fluid in the chamber 10, causes a wave to be propagated the length
of the chamber 10 and to be reflected back to the crystal. The
amount of time required for the wave to return to the crystal
automatically determines the resonant frequency of the chamber 10,
and the presence of the return wave front at the crystal causes a
positive feedback therefrom which is used, as in any standard
oscillator circuit, to excite the crystal oscillator circuit to
reinforce the original wave. In this manner then the entire system
behaves as an oscillator circuit with the chamber 10 acting as the
frequency determining element. If the length of chamber 10 changes
or the temperature of the fluid, and thus the velocity of
propagation of the wave, changes, the frequency of the wave
automatically changes to keep the chamber 10 in a resonant
condition. A loosely coupled frequency ranging element may be
coupled to the system to limit its operation to the fundamental
frequency or the desired harmonic.
Although particular embodiments of the invention have been
described and illustrated herein, it is recognized that
modifications and variations may readily occur to those skilled in
the art. Thus, for example, chamber 10 could be excited from both
ends thereof by a pair of synchronized transducers in order to
obtain a greater pressure differential in the nodes and antinodes.
In addition, if the fluid to be pumped is air, one end of the
chamber 10 could be left open with the chamber 10 then being an
integral number of half wavelengths in length. If desired the
chamber 10 could be closed at both ends and still be an integral
number of half wavelengths in length with an entrance or exit port
being provided in the center and exit or entrance ports being
provided at either or both ends thereof. Finally the chamber 10
need not be tubular so long as it is resonant in some mode with the
shape and position of the entrance and exit ports being determined
by the position of the nodes and antinodes of the resonant chamber.
Consequently, it is intended that the claims be interpreted to
cover such modifications, variations, and equivalents.
* * * * *