1. Field of the Invention
The present invention relates to a linear solenoid valve for generating an electromagnetic force in proportion to an amount of current supplied to a solenoid and displacing a valve element under the generated electromagnetic force.
2. Description of the Related Art
There have been used in the art electromagnetic valves for displacing a valve element by attracting a movable core to a fixed core under an electromagnetic force that is generated when a solenoid coil is energized.
The applicant of the present application has proposed an electromagnetic apparatus, as such an electromagnetic valve, which has a movable core capable of accurately responding to magnetic forces applied thereto.
It is a general object of the present invention to provide a linear solenoid valve which is capable of applying an increased attractive force to a movable core by setting a positional relationship at which a side surface of the movable core and an inner wall surface of a housing overlap each other.
Another object of the present invention is to provide a linear solenoid valve, which is capable of applying an increased attractive force to a movable core, by setting a layout relationship between an annular flange of a fixed core and a coil stack mounted on a coil bobbin.
The above and other objects, features, and advantages of the present invention will become more apparent from the following description when taken in conjunction with the accompanying drawings in which preferred embodiments of the present invention are shown by way of illustrative example.
As shown in
The housing 14 comprises an outer hollow cylindrical member 15, a tubular yoke 22 disposed in and spaced radially inwardly a predetermined distance from the hollow cylindrical member 15, the yoke 22 extending substantially parallel to the hollow cylindrical member 15, a bottom 17 which is thicker than the hollow cylindrical member 15 and joins the left ends of the hollow cylindrical member 15 and the yoke 22, and a mountain-shaped protrusion 19 contiguous to the bottom 17 and projecting a predetermined distance outwardly from the bottom 17 in an axial direction of the housing 14. The hollow cylindrical member 15, the yoke 22, the bottom 17, and the protrusion 19 are formed integrally with each other. The tubular yoke 22 may be a substantially tubular member (not shown) separate from the housing 14 and having an axial end press-fitted and held by a press-fitting surface (not shown) on an inner circumferential surface of the bottom 17 of the housing 14.
The housing 14 has a tapered portion 21 on an inner wall thereof across which the outer hollow cylindrical member 15 and the inner yoke 22 radially confront each other. The tapered portion 21 has a slanted surface which is inclined a predetermined angle from the bottom 17 toward the yoke 22, and which is progressively smaller in diameter from the bottom 17 toward the yoke 22. As shown in
The protrusion 19 has a hole 52 defined centrally therein, which is open inwardly to receive an end of a shaft 46 (described later). The housing 14 has a flat end face 23 contiguous to the base of the protrusion 19. As shown in
The solenoid 12 includes a coil assembly 20 disposed in the housing 14, the tubular yoke 22 being formed integrally with the housing 14 at the closed end thereof and disposed in the coil assembly 20, a fixed core 24 joined to an open end of the housing 14 and axially spaced a predetermined clearance from the yoke 22 within the coil assembly 20, and the movable core 26, which is slidably fitted in both the yoke 22 and the fixed core 24.
The coil assembly 20 comprises a coil bobbin 30 made of a plastic material and having flanges 28a, 28b disposed on respective axially spaced ends thereof, and a coil 32 having a plurality of turns wound around the coil bobbin 30 and comprising a conductive wire having a square cross section, as shown in
The coil 32 has a plurality of coil layers stacked on the coil bobbin 30 in a shape having a substantially elongate rectangular cross section. The stacked coil layers will be referred to as a coil stack 33 when described in detail below.
The turns of the coil 32 having a square cross section, which is wound around the coil bobbin 30, are held in surface-to-surface contact with each other. Therefore, the turns of the coil 32 are stably arrayed in desired positions. Since the turns of the coil 32 are thus stably arrayed, one of the flanges 28a or 28b may be dispensed with as shown in
When a conventional coil, comprising a conductive wire having a circular cross section, is wound around a coil bobbin, as shown in
As shown in
The yoke 22 has an annular flat surface 34 on the right end thereof that faces the fixed core 24, and the fixed core 24 has an outer conical surface 38 on the left end thereof that faces the yoke 22. The annular flat surface 34 lies perpendicularly to the axis of the yoke 22, and the outer conical surface 38 extends on the outer circumferential surface of the fixed core 24 around a cavity 36 defined in the fixed core 24. The yoke 22 also has a tapered surface 35 formed on an end face thereof adjacent to the annular flat surface 34, serving as a circumferentially beveled surface for reducing flux leakage.
The tubular yoke 22 and the cavity 36 defined in the fixed core 24 are complementary in shape to the movable core 26, providing a linear solenoid structure in which the movable core 26 is slidable between the tubular yoke 22 and the cavity 36 defined in the fixed core 24.
As shown in
A synthetic resin sealing body 40, which is molded over the outer circumferential surface of the coil 32 as well as a portion of the coil bobbin 30, is disposed between the housing 14 and the coil 32. The synthetic resin sealing body 40 is molded from a synthetic resin material integrally with a coupler 42. The coupler 42 has a terminal 44 electrically connected to the coil 32 and an exposed terminal end 44a that is electrically connected to a power supply (not shown).
The coil 32 has its outer circumferential surface covered with the synthetic resin sealing body 40 for stable protection of the coil 32. If one of the flanges 28a (28b) on the ends of the coil bobbin 30 is dispensed with, then the portion of the coil bobbin 30 that lacks the flange 28a (28b) is also covered with the synthetic resin sealing body 40 for stable protection of the coil 32.
The shaft 46 extends centrally axially through and is fixed to the movable core 26. The shaft 46 has an end axially and slidably supported by a first plane bearing (first bearing) 48a mounted in the hole 52 provided in the protrusion 19 of the housing 14, and the other end thereof is axially and slidably supported by a second plane bearing (second bearing) 48b mounted in a through hole 50 defined centrally and axially through the fixed core 24.
The movable core 26 has axially opposite ends deformed radially inwardly and crimped onto the shaft 46, and hence the movable core 26 is integrally joined to the shaft 46. The movable core 26 and the shaft 46 need not be separate from each other, but may be formed together integrally.
Since the axially opposite ends of the shaft 46 which extend axially through the movable core 26 are slidably supported respectively by the first and second bearings 48a, 48b, the movable core 26 is supported on a dual-end support structure provided by the shaft 46. The dual-end support structure provided by the shaft 46 allows the movable core 26 to make stable axial linear movement.
The first plane bearing 48a is press-fitted securely in the hole 52 provided in the protrusion 19, and has first communication grooves 54a defined on an outer circumferential surface thereof and communicating between opposite ends thereof. The second plane bearing 48b is press-fitted securely in the through hole 50, and has second communication grooves 54b defined on an outer circumferential surface thereof and communicating between opposite ends thereof.
A ring 55 is mounted on the end face of the movable core 26 that faces the fixed core 24 and is fitted over the shaft 46. The ring 55 is made of a nonmagnetic material and functions as a spacer for preventing residual magnetism from being produced in the solenoid 12.
Specifically, when the solenoid 12 is deenergized, residual magnetism may be produced in the fixed core 24 or in the movable core 26, tending to keep the movable core 26 attracted to the fixed core 24. However, the nonmagnetic ring 55, which is mounted on the end face of the movable core 26 and fitted over the shaft 46, forms a certain clearance between the movable core 26 and the fixed core 24, thereby preventing residual magnetism from being produced.
The movable core 26 may be made of a ferrite-base stainless steel such as SUS410L, SUS405 (JIS) or the like, a general steel such as S10C (JIS) or the like, or a free-cutting steel such as SUM (JIS) or the like.
The valve mechanism 16 comprises the valve body 18 including an inlet port 56, an outlet port 58, a drain port 60, and a breather port 62 communicating with an oil tank (not shown), defined in a side wall thereof, and a spool valve (valve element) 66 axially disposed for displacement within a space 64 defined in the valve body 18.
The spool valve 66 has a first land 66a, a second land 66b and a third land 66c, which are positioned successively from the solenoid 12. The first land 66a and the second land 66b are of the same diameter, and the third land 66c is slightly smaller in diameter than the first land 66a and the second land 66b.
The space 64 within the valve body 18 is closed by an end block 68 disposed in the end of the valve body 18 remote from the solenoid 12. A return spring 70 for normally pressing the spool valve 66 toward the solenoid 12 is disposed between the end block 68 and the spool valve 66. The return spring 70 is illustrated as being a helical spring. However, the return spring 70 is not limited to a helical spring, but may be another resilient member such as a leaf spring or the like.
The spool valve 66 has an end face positioned closely to the solenoid 12 and held in abutting engagement with the end of the shaft 46. The spring force of the return spring 70 acts through the spool valve 66 and the shaft 46 on the movable core 26, pressing the movable core 26 axially in the direction indicated by the arrow X1 in
The hydraulic control valve 10 according to the present embodiment is basically constructed as described above. Operations and advantages of the hydraulic control valve 10 will be described below.
When the solenoid 12 is deenergized, the spool valve 66 is pressed axially in the direction indicated by the arrow X1 in
When the non-illustrated power supply is turned on, the coil 32 of the solenoid 12 is energized, forming a magnetic circuit 82 as shown in
Oil, which is supplied under pressure from an oil source (not shown) through a passageway (not shown), flows through the inlet port 56 and the outlet port 58 and is supplied to a hydraulic device (not shown). When the solenoid 12 is deenergized, the spool valve 66 returns to the initial position shown in
In the present embodiment, the central reference line C of the annular flange 39 of the fixed core 24 is located at a position (about L/2) dividing the axial dimension L of the coil stack 33 into substantially equal halves. Therefore, the amount of magnetic flux (magnetic flux amount) flowing through the magnetic circuit 82 is increased, as shown in
Specifically, the magnetic field intensity is strongest substantially centrally within the coil stack 33, and the annular flange 39, which serves as a magnetically attractive member, is disposed substantially centrally inside of a linear pattern, except corners, of magnetic fluxes circulating around the coil stack 33 having a substantially elongate rectangular cross section. Such features serve to orient the vector of the magnetic fluxes in one direction toward the annular flange 39.
As a result, the annular flange 39 disposed substantially centrally in the axial direction of the coil stack 33 is effective to increase the attractive forces (electromagnetic forces) imposed on the movable core 26. Alternatively, if the solenoid 12 is desired to produce the same attractive forces as a conventional solenoid, then the hydraulic control valve 10 can be reduced in overall size.
According to the present embodiment, when the coil 32 is deenergized, as shown in
As shown in
In the magnetic circuit of a conventional electromagnetic valve, when magnetic fluxes flow through the bottom 17 to the movable core 26, the magnetic fluxes flow through the bottom 17 into the tubular yoke 22, and thereafter flow only in the direction of flow A, from the yoke 22 to the movable core 26. According to the present embodiment, on the other hand, magnetic fluxes flow both in the direction of flow A, from the yoke 22 to the movable core 26, and also in the direction of flow B, from the portion of the inner circumferential surface of the tubular yoke 22 that corresponds to the bottom 17 toward the movable core 26. Therefore, the magnetic fluxes flow highly smoothly, and the amount of overall magnetic flux flowing through the magnetic circuit 82 is increased (including the flow A of magnetic fluxes as well as the flow B of magnetic fluxes).
As a result, the solenoid 12 can produce increased attractive forces. Alternatively, if the solenoid 12 is desired to produce the same attractive forces as a conventional solenoid, then the hydraulic control valve 10 can be reduced in overall size.
The end face 26a of the movable core 26 and the end face 23 of the housing 14 are not required to lie flush with each other. According to the modification shown in
In the present embodiment, the tapered portion 21 which is progressively smaller in diameter from the bottom 17 toward the yoke 22, or the rounded portion 21a of arcuate cross section, which is disposed on the inner wall of the housing 14 across which the outer hollow cylindrical member 15 and the inner yoke 22 radially confront each other, allows the magnetic fluxes to flow more smoothly through the bottom 17 of the housing 14 toward the movable core 26, thus resulting in an increased amount of magnetic flux.
Specifically, since the joint (the inner surface of the joint region) between the tubular yoke 22 and the bottom 17 of the housing 14 is tapered or rounded toward the movable core 26, the flow of circulating magnetic fluxes, which is generated by the coil stack 33 having an elongate rectangular cross section, is considered to have a more ideal configuration.
For example, according to the comparative example shown in
In the vicinity of the tapered portion 21 or the rounded portion 21a, a magnetic flux vector is oriented in one direction toward the movable core 26, to and from which the magnetic fluxes are transferred. Consequently, magnetic fluxes flow more smoothly toward the movable core 26, resulting in an increased amount of flowing magnetic flux.
Furthermore, since the tapered portion 21 or the rounded portion 21a increases the area of the inner circumferential surface of the bottom 17, which corresponds to the circumferential side surface of the movable core 26, the area of the magnetic path is increased, also resulting in an increased amount of flowing magnetic flux.
As a result, the solenoid 12 can increase the attractive force imposed on the movable core 26. Alternatively, if the solenoid 12 is desired to produce the same attractive force as a conventional solenoid, then the hydraulic control valve 10 can be reduced in overall size.
In addition, in the present embodiment the coil 32, which is wound around the coil bobbin 30 of the solenoid 12, is of a square or elongate rectangular cross section, thereby minimizing gaps between stacked turns of the coil 32. Therefore, the total cross-sectional area of the coil 32, i.e., the overall space occupied by the coil 32 wound around the coil bobbin 30, is smaller than in a conventional solenoid coil having a circular cross section with the same number of turns as the coil 32.
Stated otherwise, the ratio of the cross-sectional area of the conductor of the coil 32 to the space in which the coil 32 is wound, i.e., the conductor occupation ratio, may be greater than that of a solenoid coil having a circular cross section. Since the space in which the coil 32 is wound can be reduced, the coil bobbin 30 can be reduced in size, resulting in a reduction in overall size of the solenoid 12.
If the space in which the coil 32 is wound is made the same as the space in which a solenoid coil having a circular cross section is wound, then the number of turns of the coil 32 having a square cross section on the coil bobbin 30 can be greater than the number of turns in a solenoid coil having a circular cross section. Accordingly, the solenoid 12 can produce greater attractive forces (electromagnetic forces) than is possible in a solenoid coil having a circular cross section.
In the present embodiment, since the space in which the coil 32 is wound can be reduced, the total dimension (total length) of the continuous wire of the coil 32 can be reduced, and hence the resistance of the coil 32 can also be reduced. As a result, the electric power consumed when the coil 32 is energized can be reduced.
Alternatively, if the coil 32 having a square cross section is desired to have the same resistance as a solenoid coil having a circular cross section, then the number of turns of the coil 32 wound around the coil bobbin 30 can be increased in the present embodiment, thereby producing increased attractive forces (electromagnetic forces).
In the present embodiment, since the coil 32 having a square cross section has turns that are held in surface-to-surface contact with each other, the conductor occupation ratio within the space in which the coil 32 is wound is greater than would be possible if a coil having a circular cross section were wound within the same space.
Consequently, gaps between stacked turns of the coil 32 can be minimized, thus increasing the density of turns of the coil 32 per unit volume within the space in which the coil 32 is wound. As a result, the heat transfer capability (heat radiation capability) within the space in which the coil 32 is wound can also be increased. If the present invention is applied to an electromagnetic valve for use in an environment where the atmospheric temperature is lower than the temperature to which the coil is heated, then since the heat radiation capability can be increased along with reducing the resistance of the coil 32, the amount of heat generated by the coil 32 when it is energized is reduced. Therefore, the resistance of the coil 32 can further be reduced.
The solenoid 12 including the coil having a square cross section can be used in an electromagnetic valve for use in vehicles. Generally, there is a minimum battery voltage of 8V, for example, which is applied to electric parts for use in vehicles. Since electromagnetic valves for use in vehicles are required to maintain a minimum magnetomotive force (current value), the maximum resistance that such electromagnetic valves should have is necessarily determined if the same magnetic circuit is employed. Because resistance of the coil 32 generally increases as the temperature thereof increases, the maximum resistance must be of a value that takes into account such a temperature-dependent resistance increase. If the maximum resistance is set without taking into account the temperature-dependent resistance increase, then the electromagnetic valve may not receive the required current, and thus possibly, the electromagnetic valve may not produce the required minimum magnetomotive force. Therefore, if the solenoid 12 is used in an electromagnetic valve for use in vehicles, then a desired magnetomotive force (current value) must be maintained, even though the resistance of the coil 32 may increase due to an increase in the temperature of the coil 32 when the solenoid 12 is energized.
It is highly advantageous if the resistance of the coil 32 itself, as well as the resistance of the coil 32 when it is heated upon energization, are kept low, because in this case the coil 32 can maintain a high current value according to Ohm's law. With the coil 32 having a square cross section, the solenoid 12 can produce the same magnetomotive force as conventional solenoids, yet the resistance of the coil 32 is made smaller and the coil 32 consumes a lower amount of electric power, thus reducing the amount of heat generated by the coil 32 when it is energized, and resulting in a reduction in the resistance of the coil 32 during times when the coil 32 is energized and heated.
As a result, the resistance of the coil 32 during times when it is energized and heated can be reduced, thereby allowing an increased current to pass through the coil 32. Therefore, the solenoid 12 can appropriately be used in an electromagnetic valve for which a minimum applied voltage is limited. Furthermore, since the current value of the solenoid 12, which includes a coil 32 having a square cross section, is higher than in conventional solenoids having a coil of circular cross section, while producing the same minimum magnetomotive force, the number of turns of the coil 32 wound around the coil bobbin 30 can be smaller, and hence the coil 32 can be made smaller in size.
Although certain preferred embodiments of the present invention have been shown and described in detail, it should be understood that various changes and modifications may be made therein without departing from the scope of the appended claims.
Number | Date | Country | Kind |
---|---|---|---|
2004-100955 | Mar 2004 | JP | national |
2004-100977 | Mar 2004 | JP | national |