The present invention relates generally to variable force solenoids and more particularly to variable force solenoids that include relatively long stroke and relatively low profile characteristics.
Electric solenoids have been used to provide a number of functions in automotive applications including, but not limited to idle speed control, exhaust gas recirculation valves, fuel vapor purge valves, and the like. Pneumatic actuators were used prior to electrically controlled solenoids. These solenoids were typically characterized as having either a relatively high force over a relatively short operating stroke, or having a relatively low force over a relatively long operating stroke.
The availability of space in conventional engine compartments has made it necessary to reduce the size of solenoids while maintaining their high force and stroke characteristics. One such application, i.e., that requires reduced packaging, is the solenoid actuator for a variable cam/valve timing mechanism that is used to control the opening and closing of the engine's valves.
In this application, the solenoid is required to control the mechanism over a predefined stroke. At the proximate center of the stroke, the mechanism will not change the cam/valve timing. As the solenoid moves from the proximate center of stroke to one end of the stroke, the mechanism will advance the cam/valve timing. As the solenoid moves from the proximate center of stroke to the opposite end of the stroke, the mechanism will retard the cam/valve timing. After changing the cam/valve timing, the solenoid is returned to the proximate center of stroke until a change to the cam/valve timing is required.
Controlling the cam/valve timing may provide benefits such as but not limited to higher engine power output, lower vehicle tailpipe emissions, higher fuel economy, and the like. However, conventional variable force solenoids have not been completely satisfactory with respect to their stroke and profile characteristics.
The basic construction of a traditional solenoid 10 with a flat-faced armature 12 is shown in
With respect to operation, current is first applied to the coil 16 to provide a magnetizing force. The magnetic field created by this magnetizing force then induces magnetic flux throughout the magnetic circuit and across the air gap 20 between the armature 12 and the pole piece 14. Axial force is generated at the air gap 20 due to the attraction of the armature 12 to the pole piece 14. Movement of the armature 14 to close the air gap 20 can do useful work. The force is given by the following formula: F=KA [(NI)2/(AG)2]; wherein K=a constant; A=the armature area; N=the number of turns of the coil; I=the current; and AG=the air gap between the armature and pole piece.
Two problems generally arise if this type of solenoid is used. First, it is desired for the force to be proportional to the current, but is instead proportional to the current squared. Second, the force should be independent of armature position, but instead is proportional to 1/AG2.
Therefore, there exists a need for new and improved variable force solenoids, wherein the solenoids include features such as but not limited to relatively long stroke and low profile characteristics.
In accordance with the general teachings of the present invention, new and improved variable force solenoids are provided. More specifically, the solenoids of the present invention preferably provide relatively long stroke and relatively low profile. Additionally, the solenoids of the present invention preferably include armatures with at least one tapered surface and pole pieces with at least one tapered surface. Further, the armatures and the pole pieces of the present invention can preferably be provided with tapers on more than one surface thereof.
By way of a non-limiting example, the solenoid preferably includes a magnetic circuit consisting of: (1) a first magnetic component (e.g., an armature) with at least one tapered surface; and (2) a second magnetic component (e.g., a pole piece) with at least one tapered surface. The armature and pole piece can each have tapers on more than one surface thereof. Further, the armature and/or pole piece can have multiple tapers (e.g., compound angles) formed on one or more surfaces thereof. Additionally, the armature can be open at either end thereof and preferably includes a partition member along its axis located within the armature.
A third magnetic component (e.g., a flux tube) is preferably provided including a portion that is preferably adjacent to the external diameter surface, internal diameter surface, and end surface of the armature. The flux tube preferably includes a portion that is adjacent to the partition within the bore of the armature.
As noted, the solenoid of the present invention preferably includes a long stroke, relative to its length, combined with a high and relatively linear force vs. its stroke. Without being bound to a particular theory of the operation of the present invention, the long stroke combined with a high and relatively linear force vs. its stroke is achieved by the control of the cross-sectional area and the angles of the tapered portions of the armature and/or pole piece to provide an advantageous magnetic force vector that maximizes axial force while simultaneously providing increased axial/radial force ratios for low mechanical friction.
Additional preferred features of the solenoid of the present invention include, without limitation, that: (1) the support for the stem is at least partially located within the inner diameter of the armature; (2) the solenoid has at least a portion that is overmolded with a plastic material; (3) the solenoid has an integrated bracket for attachment; (4) the integral bracket is part of one of the solenoid components; (5) the solenoid has an integrated bracket for attachment that is not attached to the solenoid; (6) the bracket is supported in the solenoid assembly by overmolded plastic; (7) and/or the solenoid has a least one non-magnetic bushing that will both guide the stem and prevent the armature from magnetically “latching” to another magnetic component.
In accordance with a first embodiment of the present invention, a solenoid is provided, comprising: (1) a first magnetic member having an outer diameter, wherein the outer diameter includes at least one tapered surface formed thereon; and (2) a second magnetic member having an inner diameter, wherein the inner diameter includes at least one tapered surface formed thereon, wherein the first magnetic member is operable to be at least partially coaxially disposed within the second magnetic member.
In accordance with a second embodiment of the present invention, a solenoid is provided, comprising: (1) a first magnetic member having an outer diameter, wherein the outer diameter includes at least two tapered surfaces formed thereon; and (2) a second magnetic member having an inner diameter, wherein the inner diameter includes at least one tapered surface formed thereon, wherein the first magnetic member is operable to be at least partially coaxially disposed within the second magnetic member.
In accordance with a third embodiment of the present invention, a solenoid is provided, comprising: (1) a first magnetic member having an inner diameter, wherein the inner diameter includes at least one tapered surface formed thereon; and (2) a second magnetic member having an outer diameter, wherein the outer diameter includes at least one tapered surface formed thereon, wherein the first magnetic member is operable to be at least partially coaxially disposed within the second magnetic member.
In accordance with a fourth embodiment of the present invention, a solenoid is provided, comprising: (1) a first magnetic member having an inner and an outer diameter, wherein the inner and outer diameters include at least one tapered surface formed thereon; and (2) a second magnetic member having an inner and an outer diameter, wherein the inner and outer diameters include at least one tapered surface formed thereon, wherein the first magnetic member is operable to be at least partially coaxially disposed within the second magnetic member.
In accordance with a fifth embodiment of the present invention, a solenoid, comprising: (1) a first magnetic member having an inner and an outer diameter, wherein the inner and diameter includes at least one tapered surface formed thereon and the outer diameter includes at least two tapered surfaces formed thereon; and (2) a second magnetic member having an inner and an outer diameter, wherein the inner and outer diameters include at least one tapered surface formed thereon, wherein the first magnetic member is operable to be at least partially coaxially disposed within the second magnetic member.
Further areas of applicability of the present invention will become apparent from the detailed description provided hereinafter. It should be understood that the detailed description and specific examples, while indicating the preferred embodiment of the invention, are intended for purposes of illustration only and are not intended to limit the scope of the invention.
The present invention will become more fully understood from the detailed description and the accompanying drawings, wherein:
The same reference numerals refer to the same parts throughout the various Figures.
The following description of the preferred embodiment(s) is merely exemplary in nature and is in no way intended to limit the invention, its application, or uses.
In accordance with the general teachings of the present invention, a solenoid design is provided that will provide relatively high force over a relatively long stroke. Without being bound to a particular theory of the operation of the present invention, the present invention will achieve this force and stroke with a solenoid length that is relatively small compared to its stroke. Additional features of the present invention include, without limitation, a design for supporting the stem of the solenoid over the entire stroke and the minimization of the radial forces and the resulting bearing friction.
Referring generally to the Figures, and more specifically to
Referring specifically to
Referring specifically to
In accordance with one embodiment of the present invention, an end of the armature member 202 that engages the flux tube member 208 preferably includes a uniform wall 202e formed by the inner diameter surface 202a and the outer diameter surface 202b. In accordance with a preferred embodiment of the present invention, the opposite end of the armature member 202 preferably includes at least one taper, and still more preferably more than one taper formed thereon. By way of a non-limiting example, taper 202f is preferably formed on the inner diameter surface 202a, and taper 202g is preferably formed on the outer diameter surface 202b. Taper 202g preferably comprises two angled taper portions, 202h and 202i, respectively. It should be appreciated that multiple tapers may be formed on either the inner and/or outer surfaces of the armature member 202.
In accordance with another embodiment of the present invention, pole piece member 216 also preferably includes tapers formed thereon. By way of a non-limiting example, taper 216c is formed on an outer diameter surface 216b, and taper 216d is formed on an inner diameter surface 216a of pole piece member 216. Taper 216d preferably includes two angled taper portions, 216e and 216f, respectively. It should be appreciated that multiple tapers may be formed on either the inner and/or outer surfaces of the pole piece member 216.
Without being bound to a particular theory of the operation of the present invention, these tapers will preferably control the magnetic flux linkage between the armature member 202 and the pole piece member 216 as the armature member 202 moves through its stroke. This control of flux linkage will preferably determine the force vs. stroke vs. current relationships. Without being bound to a particular theory of the operation of the present invention, the combination of the low cross-sectional thickness of the tapered portions of the armature member 202 and the pole piece member 216, along with the angle section, result in a high axial force/stroke ratio for a given diameter of the armature member and/or the pole piece member, and a force highly independent of stroke.
The angled surfaces of the present invention can preferably be adjusted to provide both linear and non-linear force vs. stroke relationships and force vs. current relationships. Thus, it will be appreciated that the angles of the tapers can be modified to suit the particular performance requirements of the solenoid operation. In accordance with a preferred embodiment of the present invention, the taper angles are in the range of about 4 to about 10 degrees. In accordance with a more preferred embodiment of the present invention, the taper angles are in the range of about 5 to about 7 degrees. In the situation wherein at least two tapers are provided on a surface of any of the components of the present invention, such as but not limited to the armature member and/or the pole piece member, the angles of the tapers are preferably not substantially equal. That is, the angle formed by the first tapered surface is preferably less than or greater than the angle formed by the second tapered surface.
In accordance with another embodiment of the present invention, a central portion 208b of the flux tube member 208 preferably includes a bore 208c that preferably receives bushing member 206. A portion of the central portion 208b preferably engages the inner diameter 202a of the armature member 202 as the armature member 202 moves through its stroke. An area defining a radial air gap RAG will preferably exist over the axial engagement. This engagement will preferably allow magnetic flux to link between the flux tube member 208 and the armature member 202 to improve the resulting force of the solenoid 100. The armature member 202 and the flux tube member 208 also preferably include areas defining axial air gaps AAG1 and AAG2, respectively, which can aid flux linkage and improve resulting force.
It should be noted that guide bushings are preferably located along the central axis CA and inside of the armature member 202. This additional space is generally required because the stem member 200 must extend along the central axis CA to engage with the bushing member, e.g., 214, and maintain engagement through its stroke. Furthermore, locating bushing member 214 along the central axis CA, within the armature member 202, will preferably reduce the overall length of the solenoid 100.
In accordance with one aspect of the present invention, the solenoid 100 of the present invention is intended to cooperate with a cam/valve timing mechanism that may provide the bias force to the armature member 202 that will cause it to move in a direction towards the flux tube member 208. However, an optional biasable member 234 (e.g., a spring) can be installed within the solenoid 100 if the external bias force is not available.
Referring specifically to
Without being bound to a particular theory of the operation of the present invention, the solenoid 100 of the present invention preferably operates in the following general manner. When the electric control signal is applied to the coil assembly 220 it will develop a magnetic field within the solenoid 100. The magnetic elements, i.e., the armature member 202, flux tube assembly 204, casing 232, and the pole piece assembly 212, will provide a path for the magnetic flux. The magnetic flux is preferably linked between the armature member 202, flux tube assembly 204, and pole piece assembly 212 via air gaps AG, RG, MG1, and AAG2. The magnetic field and the resulting force will preferably cause the armature member 202 to move towards the pole piece member 216. The rate and linearity of movement are preferably determined by geometric relationships between the armature member 202 and the pole piece member 216 and the characteristic of the load force, typically, but not limited to a bias spring.
As the level of the control signal changes, the stem member 200 will preferably move outwardly or inwardly to control the position of the associated mechanism, e.g., the cam/valve timing mechanism. Progressively increasing the level of the control signal will preferably increase resulting force and the outward movement of the stem member 200. Reducing the level of the control signal will preferably reduce the resulting force and the stem member 200 will move inwardly with the bias force of the cam/valve timing mechanism or optional internal bias spring 234.
With respect to the specific design and performance specifications of the solenoid of the present invention, the following illustrative specifications were established: (1) total travel available=6 mm; (2) spool valve travel=4 mm; (3) load=1.8 N at 0 mm; 9 N at 4 mm; (4) 0-1 A, 10 N force at 1 A 10V, 125° C.; operation to 150° C. with some degradation; (5) 3% maximum hysteresis at the null position; and (6) packaging of 30 mm height, 60 mm diameter. It should be appreciated that these specifications, which are illustrative in nature, can be reasonably modified without departing from the scope of the present invention.
A first alternative solenoid subassembly 400 is shown in
Additionally, the force gain with current becomes substantially more linear because of increased magnetic saturation present in the circuit throughout the range of current levels. With reference to
Because the variable force solenoids of the present invention position the spool valve open loop, hysteresis must be minimized for good system performance. There are two main causes of hysteresis, namely, side forces and material selection.
With respect to side forces, the magnetic attraction of the armature to the rest of the circuit creates not only the useful axial force but also radial forces. These radial forces become quite significant with tapered armatures at the end of the stroke. If symmetry around the armature axis is maintained, the radial forces cancel out. However, symmetry is disrupted by such factors as irregular features, runout, bearing clearance, and the like. The effects of each of these are difficult to quantify, but their effect on the system is quite noticeable as bearing friction. Suggested design solutions include, without limitation: (1) making parts as symmetrical, as possible, especially in the armature area; (2) locating the bearings for minimal true position stackup; (3) selecting low-friction bearings and appropriate stem surface finish; (4) applying a dither current to keep moving mass in motion to minimize static friction effects; and (5) reducing moving mass to facilitate dithering.
With respect to material selection, the magnetization of a piece of steel is not a fully reversible process. For example a B-H curve for a 1215 steel sample, as shown in
Although magnetic circuit analysis is reasonably accurate for simple geometry, it falls short due to the magnetic characteristic of the iron becoming non-linear as saturation is approached. Fortunately, simulation software is readily available. The software used to evaluate the solenoid performance characteristics of the present invention was a 2D axisymmetric type sold under the trade name MAGNETO, which is readily commercially available from Integrated Engineering Software Sales, Inc. (Winnipeg, Canada). This software program uses the boundary element method to calculate a solution. With this software, the geometry of the solenoid is constructed as half a section and rules of symmetry about the armature axis are applied. This software program has the following advantages: (1) geometry is constructed and modified very easily; (2) parametric solving is easily accomplished; (3) correlation to actual results is good (see
Referring to
A second alternative solenoid subassembly 500 is shown in
The performance of the embodiment was satisfactory for initial development work, although several areas of improvement were identified, including: (1) total stroke—a stackup study showed that the solenoid stroke should be increased from 6 mm to 8 mm; (2) force—the force curves had excessive droop at both ends of the total stroke; (3) dither frequency—dithering essentially stopped at 100 Hz and above. Measurement of the moving mass was 36 grams vs. 27 grams for the Phase 1 (SEGR) solenoid. A target of effective dithering at 100 Hz minimum with 0.100 Amp peak-to-peak dither current was established; and (4) hysteresis was in the 0.2-0.3 mm (5%-7.5%) range, which is acceptable for most development applications (but may not meet all OEM requirements, such as those in 3% range).
A third alternative solenoid subassembly 600 is shown in
A significant feature that enabled the stroke increase was the design of the flux tube member 606. The flux tube member 606 is provided with areas defining open ends or depressions formed therein for at least partially receiving portions of the armature member 602. This permits the establishment of at least one, more preferably at least two, still more preferably at least three, and most preferably at least four confronting surfaces to be formed therebetween. Preferably, these confronting surfaces can be either radially and/or axially opposed from one another. Without being bound to a particular theory of the operation of the present invention, these confronting surfaces are thought to be useful for at least aiding in the formation of a magnetic flux circuit (e.g., when the solenoid (e.g., the coil) is energized), especially with respect to any internal radial and/or axial confronting surfaces of the armature member 602 and flux tube member 606.
Without being bound to a particular theory of the operation of the present invention, the intended purpose of the configuration of the flux tube member 606 is to complete the magnetic circuit by coupling the flux to the armature member 602. The flatness of the force curves at the end of the stroke is highly dependent on this coupling, and this requires some minimum overlap of the armature member 602 outer diameter and the flux tube member 606 inner diameter. Although this need directly conflicts with the low solenoid profile requirement, the problem was resolved by redesigning the flux tube member 606 to a screw machine part with the stem bearing 608 pressed directly to it. This permits coupling of the armature member 602 on both the inner and outer diameters and the direct bearing mounting reduces side forces by improved concentricity. Additionally, the armature member 602 was redesigned to remove excess mass. By way of a non-limiting example, the total moving mass was reduced to 25 grams.
Functional testing of the variable force solenoids of the present invention requires measurement of both force and position. For solenoid force testing, a traditional method uses a piezoelectric transducer and a moveable sled to measure force as a function of stroke. Because the operator adjusts the stroke, it does not replicate the conditions under which the variable force solenoid operates. Additionally, the armature contacts the stationary transducer and the benefits of dither are greatly diminished. However, for force measurement, it works very well.
In order to correct the limitations of the force sled, fixturing was changed to allow the variable force solenoid of the present invention to stroke against a spring with stops, to simulate the spool valve load and travel. A Linear Variable Differential Transformer was attached to the opposite end of a variable force solenoid in accordance with the present invention to allow measurement of stroke vs. current. This was an improvement; however, in practice the mass of the transducer core added significantly to total mass, and the uncertainty of verifying the concentricity of the core to prevent rubbing against the transducer coil was always present.
A subsequent test method incorporated a laser to provide a non-contact means to measure position. A Visual Basic data acquisition custom configured program provides a user-friendly means to test variable force solenoids with selectable gate points for position and hysteresis.
In order to evaluate other designs of variable force solenoids, several requirements were established, namely: (1) low part count; (2) simplicity of components; (3) inherent alignment of critical components; (4) match process to part requirements; and (5) maintain packaging constraints. Several alternative design concepts were created and evaluated for various attributes based, in part, on these requirements.
A fourth alternative solenoid subassembly 700 is shown in
A fifth alternative solenoid subassembly 800 is shown in
A sixth alternative solenoid subassembly 900 is shown in
A force vs. stroke summary of some of the previously described solenoids of the present invention is shown in
While the embodiment depicted in
The description of the invention is merely exemplary in nature and, thus, variations that do not depart from the gist of the invention are intended to be within the scope of the invention. Such variations are not to be regarded as a departure from the spirit and scope of the invention.
This application is a continuation of U.S. patent application Ser. No. 10/863,586 filed on Jun. 8, 2004. This application claims the benefit of U.S. Provisional Application No. 60/477,309, filed Jun. 9, 2003. The disclosures of the above applications are incorporated herein by reference.
Number | Date | Country | |
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60477309 | Jun 2003 | US |
Number | Date | Country | |
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Parent | 10863586 | Jun 2004 | US |
Child | 11712345 | Feb 2007 | US |