The present invention relates to pumping devices, and more specifically to piezoelectric pump devices for delivering fluids.
Conventional motorized piston-based micropumps for various types of fluids have been constructed using electromagnetic or pneumatic motors. More recently, interest has shifted toward micropumps that use piezoelectric actuators. Micropumps based on piezoelectric actuators have the potential of being less cumbersome, consuming less power, and being less noisy as compared to more conventional designs. Piezoelectric micropumps typically comprise a diaphragm that is driven by a piezoelectric element. The diaphragm is operatively associated with an air pump chamber which has communicating inlets and outlets in the pump housing or body. In such configurations, bending piezoelectric actuators are arranged against the diaphragm. Consequently, when the piezoelectric actuators are stimulated to have bending vibrations, the movement of the actuator results in movement of the diaphragm. This movement of the diaphragm leads to a cyclical change in the volume of the air pump chamber. One limitation of the arrangement described herein is that the bending actuators are generally not capable of providing a significant amount of linear displacement. As a result, the maximum flow and pressure these pumps can provide is typically limited.
Embodiments of the present invention describe piezoelectric pumps. In a first embodiment of the invention, a pump body is provided including at least one inlet valve, at least one outlet valve, a substantially rigid top portion, a substantially rigid bottom portion, and collapsible side portions. The pump body also includes a base on or in the bottom portion and defining a rotational axis extending from the bottom portion. The pump body further includes a rotor shaft disposed along the rotational axis within the enclosure, a first end of the rotor shaft mechanically and rotatably coupled to the base, and a second end of the rotor shaft providing a cam surface for engaging the top portion and operable to cause motion of the top portion in response to rotation of the rotor shaft. The pump body also includes at least one piezoelectric actuator engaging a surface of the rotor shaft, the piezoelectric actuator configured to cause the rotation of the rotor shaft.
In a second embodiment of the invention, a pump is provided. The pump includes at least one inlet valve, at least one outlet valve, a substantially rigid top portion, a substantially rigid bottom portion, and collapsible side portions. The pump also includes a base on or in the bottom portion and defining a rotational axis extending from the bottom portion. The pump further includes a rotor shaft disposed along the rotational axis within the enclosure, a first end of the rotor shaft mechanically and rotatably coupled to the base, and a second end of the rotor shaft providing a cam surface for engaging the top portion and operable to cause motion of the top portion response to rotation of the rotor shaft. The pump also includes an annular piezoelement polarized along its thickness and having opposing upper and lower surfaces and inner and outer rim surfaces, the annular piezoelement retained on the base about the rotational axis. Additionally, the pump includes one or more flexible pushers, each of the flexible pushers having a first end mechanically coupled to the annular piezoelement and a second end extending radially to contact the rotor shaft. The pump further includes a power supply configured to excite a first-order radial vibration mode in the annular piezoelement. In the pump, the flexible pushers cause a rotation of the rotor shaft responsive to excitation of the first-order vibration mode in the annular piezoelement.
In a third embodiment of the invention, a reciprocating piezoelectric drive system is provided. The system includes a rotor shaft having an axis of rotation aligned with the shaft and a base configured for supporting the rotor shaft along the axis of rotation. The system also includes at least one piezoelectric actuator configured to apply a rotational force on the rotor shaft transverse to the axis of rotation when the piezoelectric actuator is electrically excited. The system further includes a cam surface defined on a portion of the rotor shaft and a cam follower which engages the cam surface and configured so that a rotation of the rotor shaft causes a reciprocating linear motion of the cam follower.
The present invention is described with reference to the attached figures, wherein like reference numerals are used throughout the figures to designate similar or equivalent elements. The figures are not drawn to scale and they are provided merely to illustrate the instant invention. Several aspects of the invention are described below with reference to example applications for illustration. It should be understood that numerous specific details, relationships, and methods are set forth to provide a full understanding of the invention. One having ordinary skill in the relevant art, however, will readily recognize that the invention can be practiced without one or more of the specific details or with other methods. In other instances, well-known structures or operations are not shown in detail to avoid obscuring the invention. The present invention is not limited by the illustrated ordering of acts or events, as some acts may occur in different orders and/or concurrently with other acts or events. Furthermore, not all illustrated acts or events are required to implement a methodology in accordance with the present invention.
As described above, existing piezoelectric pumps provide a relatively low fluid flow rate and small differential pressures. In these systems, even though the piezoelectric actuator is directly acting against the diaphragm, the working amplitude of the diaphragm is relatively low as compared to electromagnetic or pneumatic pumps. In general, this amplitude is several hundred microns for most conventional piezoelectric actuators. As a result, the limited amplitude limits the capacity of such systems to provide a high air flow.
In other to overcome the limitations of conventional piezoelectric pumps, a new piezoelectric pump is provided. In particular, a piezoelectric pump is provided in which the vibrations of one or more piezoelectric actuators are used to cause a rotation of a cam surface against a diaphragm. In the various embodiments of the invention, the cam surface is configured to provide a displacement that is substantially greater than the displacement provided by the piezoelectric actuator alone.
Those skilled in the art will appreciate that the piezoelectric pump described herein is operable for pumping various types of fluids. The term “fluid”, as used herein, refers to any substance that tends to continually deform or flow under an applied shear stress (i.e., substances that tend to take on the shape of a container they are disposed in). Examples of fluids include gases, liquids, plasmas, and other substances that provide little or no resistance to a deformation force.
The various embodiments of the invention provide piezoelectric pumps with functional capabilities that are improved by at least one order of magnitude, as compared to conventional piezoelectric pumps. Therefore, piezoelectric pumps in accordance with the various embodiments of the invention can operate at the same or better level of performance as conventional pumps based on electromagnetic motors. Further, piezoelectric pumps in accordance with the various embodiments of the invention preserve all the advantages of conventional piezoelectric pumps: small size, low noise, and low power consumption. An exemplary design for such a piezoelectric pump is shown in
The exemplary pump body 100 shown in
Additionally, although pump body 100 is illustrated in
In the various embodiments of the invention, the pump body 100 basically operates as a bellows. That is, a force is applied on top portion 106 to deform side portions 108 and therefore reduce an expanded length L1 of the pump body to a compressed length L2. As a result, the volume of pump body 100 is reduced by an amount proportional to the difference in lengths (ΔL=L1-L2), causing fluid within the pump body 100 to be expelled via outlet valve 112. Afterwards, when a force is applied on top portion 106 to increase a distance between the top portion 106 and bottom portion 102, side portions 108 are undeformed. As a result, the volume of pump body 100 increased, causing fluid to be drawn into the pump body 100 via inlet valve 110. In the various embodiments of the invention, the deforming and undeforming of diaphragm portion 104 is achieved via the operation of a piezoelectric actuated rotating cam mechanism 114 operating on top portion 106, as described below.
As shown in
In the various embodiments of the invention, rotor shaft 122 and base 116 can be fabricated using various types of materials. For example, some materials include metals, metal alloys, ceramics, or glass materials. In the case of metals and metal alloys, these can include ferrous and non-ferrous materials. Further, these can also include magnetic or non-magnetic materials. Further rotor shaft 122 and guide portion 118 can also be configured to accommodate one or more bearings to facilitate rotation of rotor shaft 122 in guide portion 118.
Rotation of the rotor shaft 122 is achieved via the use of a radial piezoelectric actuator 124. Piezoelectric actuator 124 can include one or more a piezoelectric elements 126 and one or more flexible pushers 128 mechanically attached thereto. In the example shown in
In operation, when pushers 128 move radially towards rotor shaft 122, pushers deform and begin to apply a restorative force against rotor shaft 122 via a friction contact. Since a portion of the pushers 128 also extends along a direction of rotation, the restorative force of the pusher 128 is preferentially applied in the direction of rotation 140. Therefore, once a sufficient deformation of pushers 128 has occurred, the aggregate restorative force of the deformed pushers 128 becomes sufficiently large to overcome any frictional forces between rotor shaft 122 and guide portion 118, causing rotor shaft 122 to rotate about rotational axis 120 in a direction 140. When pushers 128 move radially away from rotor shaft 122, the pushers 128 undeform and stop applying a force against rotor shaft 122. This process can then be repeated to maintain rotation of rotor shaft 122.
In the embodiment shown in
In the various embodiments of the invention, the piezoelectric element(s) 126 can be fabricated from piezoceramics selected from the group of piezoelectric lead-zirconate-titanate-strontium ceramics (PZT) materials. However, the present invention is not limited to the use of PZT materials. In other embodiments of the present invention, other types of piezoelectric materials can be used. Furthermore, the piezoelements can be polarized.
In the various embodiments of the invention, the pushers 128 can be configured in a variety of ways. For example, pushers 128 can be constructed from a variety of materials, including beryllium, copper, or plastic, to name a few. However, the various embodiments of the invention are not limited in this regard and pushers 128 can be construct using any other types or combinations of materials suitable for providing a cantilever-type spring. Further, pushers 128 can be attached to piezoelectric element 126 using a cement or solder material. However, the various embodiments of the invention are not limited in this regard and other attachment methods can also be used. For example, fastener devices can be used to mechanically couple pushers 128 to piezoelectric element 126. In another embodiment, at least one of pushers 128 and piezoelectric element 126 can include one or more attachment features to provide mechanical coupling.
In
In some embodiments of the invention, the top portion 106 can includes an actuating member portion 130, as described above, for engaging the cam surface 122c of rotor shaft 122. The actuating member portion 130 can include an extending portion 132 projecting from top portion 106 towards the cam surface 122c of rotor shaft 122. The actuating member portion 130 also includes a cam-follower portion 134 for physically contacting the cam surface 122c of rotor shaft 122. In the various embodiments of the invention, the components of actuating member portion 130 are fixed in position relative to the rotating cam surface 122c.
In the various embodiments of the invention, actuating member portion 130 can be fabricated using various types of materials. For example, some materials include metals, metal alloys, ceramics, or glass materials. In the case of metals and metal alloys, these can include ferrous and non-ferrous materials. Further, these can also include magnetic or non-magnetic materials. In some embodiments of the invention, the cam-follower portion 134 can include one or more bearings for engaging the cam surface 122c.
The pump body 100 operates as follows. First, mechanical vibrations are excited in each piezoelectric element 126 when the electrical power is applied to the piezoelement. These vibrations are transmitted to the pushers 128 and cause rotation of the rotor shaft 122 due to the frictional force between the pushers and the rotor, as described above with respect to
Therefore, as the actuating member 130 moves upward, as shown in
In the exemplary embodiment shown in
As described above, motion of the rotor shaft in
In another example, as shown in
where d is an average diameter of the ring (in particular the diameter of the piezoelectric ring), sjk is the coefficient of elasticity of the material (in particular the material of the piezoelectric ring), a is the form factor of the ring (in particular the form factor of the piezoelectric ring) which is determined experimentally, ρ is density of the material (in particular, density of the piezoelectric ring), and n is an integer≧0 and specifying the order of the vibrational mode. In the case of zero order radial vibrational mode (1) can be transformed into the equation:
F
r
R
=c
p/2×π[(Rp+rp)/2], (2)
where cp is the speed of propagation of sound waves in the material, Rp is the outside radius of the annular piezoelement, and rp is the inner radius of the annular piezoelement.
In order to increase the maximum flow for the pump in
In such annular piezoelement, the decrease in frequency is typically compensated for by reducing the internal radius of the annular piezoelement, thus increasing the annular width of the annular piezoelement. The term “annular width” as used herein, refers to the difference between the inner and outer diameters of an annular piezoelement. This will lead to an increase in the excitation frequency according to equation (2), but in this case the system operates as a thick ring resonator (a thick ring here is defined by the annular width of the annular piezoelement) and the quality (Q) factor decreases rapidly. As used herein, the “Q factor” is a measure of the relationship between stored energy and rate of energy dissipation in resonator. Thus a high Q factor indicates a high efficiency resonator and a low Q factor indicates a low efficiency resonator. A similar situation arises when higher order radial excitation modes are used. In such instances, the Q factor of the annular piezoelement also decreases rapidly and the motor becomes less efficient.
Therefore, in some embodiments of the present invention, the maximum pump flow rates can be achieved by providing an annular piezoelement and selecting an operating frequency for the applied voltage so as to excite the first-order longitudinal mode of vibration radially along the annular width of the annular piezoelement. In particular, an operating frequency Frp) for the excitation voltage can be provided that is described by the equation:
F
r
p
=c
p/2h, (3)
where cp is the speed of propagation of the sound waves in the annular piezoelement material and h is the annular width of the annular piezoelement (h=Rp−rp).
Accordingly, excitation of the first order vibrational longitudinal mode can be achieved by configuring the annular piezoelement to have an outer radius (Rp) that is at least twice the inner radius (rp) (i.e., Rp>2rp) and an annular width (h) that is at least twice a thickness of said piezoelectric element (i.e. h>2H). Therefore, when excited using an alternating voltage having a frequency (Frp) equal to cp/2(Rp−rp), the portions of the annular piezoelement at or near the inner rim and the outer rim surfaces of the annular piezoelement are operable to efficiently transfer oscillations of the annular piezoelement in the radial direction to the pushers to effect rotary movement of a rotor about the rotational axis with a significantly higher amount of torque than observed in conventional piezoelectric motors, including annular piezoelements. Accordingly, based on the relationships Rp>2rp and h>2H for the piezoelement and the piezoelectric material (which specifies cp), dimensions for the annular piezoelement for a particular excitation voltage frequency can be selected.
The resulting excitation of such an annular piezoelement is described in
As shown in
As the alternating excitation voltage is further applied to the annular piezoelement, compression of the width of the annular piezoelement can subsequently occur, as shown in
An exemplary configuration for a pump in accordance with an embodiment of the invention will be described below. Although the calculations below are show for pumping gases, one of ordinary skill in the art will recognize that a similar set of calculations can be provided for configuring a pump in accordance with an embodiment of the invention to pump other types of fluids, such as liquids.
In the case of a gas, the value of ECAM for the exemplary piezoelectric pump in
P1V1=P2V2, (4)
where P1 and V1 are the gas pressure and volume, respectively, for the configuration shown in
V
1
=V
2
+S×ΔL, (5)
where S is given by π(D/2)2. Equation (4) can then be written as:
P
1(V2+S×ΔL)=P2V2. (6)
Therefore, if the increase in pressure after compression is ΔP, then P2 can be expressed as:
P
2
=P
1
+ΔP, (7)
and equation (6) can be rewritten as:
ΔP/P1=(S×ΔL)/V2 (8)
However, when pump body is extended:
V
2
=S×L
1. (9)
Therefore, Equation (8) can then be reduced to:
ΔP/P1=ΔL/L1 (10)
Accordingly, based on Equation (10), the elevation variation for the cam surface 122c can be determined since ECAM=ΔL. For example, if P1=15 PSI, ΔP=2 PSI, and L1=15 mm, then ΔL=ECAM=2 mm.
In addition to selecting ECAM, the maximum gas flow rate, Q, can be selected as well in the various embodiments of the invention. First, the volume of gas expelled during one cycle of movement is S×ΔL, as shown above in Equation (5). Therefore the full gas flow Q is given by the formula:
Q=(S×ΔL)×F (11)
where F is the angular speed of rotation of the motor. Therefore, F can be expressed as:
F=Q/(S×ΔL). (12)
Accordingly Equation (12) can be used to select an angular speed for the pump body to provide a desired flow rate. For example, if Q=240 cm3 per minute=4 cm3/s, the diameter of the pump is D=2.6 cm, so that S=π(D/2)2=5.3 cm2, and ΔL=2 mm=0.2 cm, Equation (9) yields the estimate of the required angular speed as 3.8 rev/sec or 228 RPM.
Therefore, if the pump body 100 shown in
ECAM and F can also be selected for other fluids, such as liquids. In the case of liquids, a needed head and discharge rate at an access point can be obtained. Such calculations are well-known to those of ordinary skill in the art and will not be described herein.
While various embodiments of the present invention have been described above, it should be understood that they have been presented by way of example only, and not limitation. Numerous changes to the disclosed embodiments can be made in accordance with the disclosure herein without departing from the spirit or scope of the invention. Thus, the breadth and scope of the present invention should not be limited by any of the above described embodiments. Rather, the scope of the invention should be defined in accordance with the following claims and their equivalents.
Although the invention has been illustrated and described with respect to one or more implementations, equivalent alterations and modifications will occur to others skilled in the art upon the reading and understanding of this specification and the annexed drawings. In addition, while a particular feature of the invention may have been disclosed with respect to only one of several implementations, such feature may be combined with one or more other features of the other implementations as may be desired and advantageous for any given or particular application.
The terminology used herein is for the purpose of describing particular embodiments only and is not intended to be limiting of the invention. As used herein, the singular forms “a”, “an” and “the” are intended to include the plural forms as well, unless the context clearly indicates otherwise. Furthermore, to the extent that the terms “including”, “includes”, “having”, “has”, “with”, or variants thereof are used in either the detailed description and/or the claims, such terms are intended to be inclusive in a manner similar to the term “comprising.”
Unless otherwise defined, all terms (including technical and scientific terms) used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this invention belongs. It will be further understood that terms, such as those defined in commonly used dictionaries, should be interpreted as having a meaning that is consistent with their meaning in the context of the relevant art and will not be interpreted in an idealized or overly formal sense unless expressly so defined herein.
This application claims the benefit of U.S. patent application Ser. No. 12/639,232, entitled “PIEZOELECTRIC MOTOR WITH HIGH TORQUE”, filed Dec. 16, 2009, and U.S. Provisional Application Ser. No. 61/149,941, entitled “PIEZOELECTRIC CORRUGATED-PISTON MICROPUMP”, filed Feb. 4, 2009, which are herein incorporated by reference in their entirety.
Number | Date | Country | |
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61149941 | Feb 2009 | US | |
61138442 | Dec 2008 | US |
Number | Date | Country | |
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Parent | 12639232 | Dec 2009 | US |
Child | 12700319 | US |