JP2007132196A - Fuel pump impeller and fuel pump using the same - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a fuel pump impeller for improving pumping efficiency, and to provide a fuel pump using the same. <P>SOLUTION: A backward inclination angle α formed by a line segment 110 connecting a radial inside end 37a of a backward face 37 of a vane groove 36 to a radial outside end 37b, and a line 104 extending from the radial inside end 37a along a radius 102 of the impeller 30 to the radial outside is set in a range of 15°≤α≤30°. A forward inclination angle β formed by a line segment 112 connecting a center 37c in the thickness direction of the backward face 37 to both ends 37d of the backward face 37 in the thickness direction of the impeller 30 and a line 106 extending from the center 37c in the thickness direction along the peripheral direction forward to the rotating direction is set in a range of β≤60°. The backward inclination angle α and the forward inclination angle β are set to satisfy 1≤β/α≤4 in a range of 15°≤α≤30° and β≤60°. <P>COPYRIGHT: (C)2007,JPO&INPIT

Description

  The present invention relates to a fuel pump impeller that has a plurality of blade grooves formed in the rotation direction and boosts the pressure by rotating fuel in a pump passage formed along the blade grooves, and a fuel pump using the same.

  Conventionally, a plurality of blade grooves are formed in the rotation direction of the disk-shaped impeller, the blade grooves adjacent to each other in the rotation direction are partitioned by partition walls, and the fuel in the pump passage formed along the blade grooves by rotating is used. A fuel pump for boosting pressure is known (for example, see Patent Document 1). In such a fuel pump, for example, a higher discharge pressure is required due to a demand for improving atomization of fuel spray injected from a fuel injection valve. If the current supplied to the motor unit of the fuel pump is increased, the discharge pressure of the fuel pump can be increased, but there is a problem that the power consumption of the fuel pump increases.

Therefore, in Patent Document 1, an attempt is made to improve the efficiency of the fuel pump by improving the efficiency of the pump unit by defining the inclination angle of the forming surface on which the blade groove is formed. The efficiency of the fuel pump is expressed by (motor efficiency) × (pump efficiency). Therefore, when the pump efficiency is improved, the efficiency of the fuel pump is improved. The motor efficiency and the pump efficiency are: the drive current supplied to the motor part of the fuel pump is I, the applied voltage is V, the torque of the motor part is T, the rotational speed of the motor part is N, and the discharge pressure of the fuel discharged from the fuel pump Is P and the fuel discharge amount is Q, (motor efficiency) = (T × N) / (I × V), (pump efficiency) = (P × Q) / (T × N). Therefore, (fuel pump efficiency) = (motor efficiency) × (pump efficiency) = (P × Q) / (I × V). If the pump efficiency is improved, the fuel discharge pressure can be increased without increasing the power consumption of the fuel pump.
However, there is a demand for further improving pump efficiency in response to demands for increasing the fuel discharge pressure or increasing the fuel discharge amount.

JP 2000-240582 A

  The present invention has been made to solve the above problems, and an object thereof is to provide a fuel pump impeller that improves pump efficiency and a fuel pump using the same.

  In the invention described in claims 1 to 3, a line segment connecting the radially inner end and the radially outer end of the rear surface behind the rotational direction forming the blade groove, and the diameter on the radius of the impeller from the radially inner end. The rearward inclination angle formed by the straight line extending outward in the direction is α, the line segment connecting the center in the thickness direction of the impeller on the rear surface and both ends in the thickness direction on the rear surface, and the rotation axis of the impeller from the center in the thickness direction 15 ° ≦ α ≦ 30 °, β ≦ 60 °, and 1 ≦ β / α ≦ 4, where β is a forward tilt angle formed by a straight line that is orthogonal to the straight line extending forward in the rotational direction.

  When such an impeller rotates, the fuel that flows out of the blade groove forward in the rotation direction and flows into the blade groove behind the rotation direction flows out of the blade groove that flows in and further flows into the blade groove behind the rotation direction. Then, by sequentially repeating the outflow from the blade groove and the inflow into the blade groove, the fuel flowing through the pump passage turns into a swirling flow to increase the kinetic energy and boost the fuel pressure.

  Here, if α <15 °, the swirling flow does not flow along the rear surface of the blade groove and collides with the rear surface at a large angle. Since this collision force acts on the side opposite to the direction of rotation of the impeller, the impeller is prevented from rotating. If α> 30 °, an opening occurs between the swirling flow and the rear surface, and the swirling flow does not flow along the rear surface of the blade groove, and the swirling flow is separated. The separation of the swirling flow becomes a resistance when the swirling flow flows into the blade groove. Thus, when α <15 ° or α> 30 °, the swirling flow does not flow smoothly into the blade groove, so the energy of the swirling flow is reduced and the pump efficiency is lowered.

Therefore, in the invention described in claims 1 to 3, by setting 15 ° ≦ α ≦ 30 °, the swirling flow smoothly flows into the blade groove along the rear surface of the blade groove. Reduction is prevented and pump efficiency is improved.
In addition, when β> 60 °, the angle inclined forward in the rotational direction from the center in the thickness direction of the impeller toward both sides in the thickness direction becomes small, so that the swirl flow rotates from the blade groove when flowing out from the blade groove. The energy component received toward the front in the direction is reduced. As a result, since the pitch in the rotational direction of the swirl flow is increased, the interval between the blade grooves until the swirl flow flows out of the blade groove and flows into the next blade groove behind the rotation direction is increased. That is, the number of times the swirling flow enters and exits the blade groove while flowing through the pump passage decreases, so that the fuel pressure is not sufficiently increased.

  Therefore, in the invention according to claims 1 to 3, by setting the forward tilt angle β to β ≦ 60 °, the energy component that the swirling flow receives from the blade groove toward the front in the rotation direction when flowing out from the blade groove is reduced. Since it becomes larger, the pitch in the rotational direction of the swirl flow becomes shorter. As a result, the number of times the swirling flow enters and exits the blade groove while flowing through the pump passage increases, so that the fuel boosting efficiency is improved.

Here, if the forward inclination angle β is too small or too large with respect to the backward inclination angle α, the swirling flow that flows out from the blade groove at the forward inclination angle β along the rear surface of the blade groove of the backward inclination angle α. It cannot flow smoothly into the rear surface.
Therefore, in the invention according to any one of claims 1 to 3, by setting 1 ≦ β / α ≦ 4, the blade groove is formed within the range of 15 ° ≦ α ≦ 30 ° and β ≦ 60 °. The magnitudes of the backward inclination angle α and the forward inclination angle β are adjusted so that the fuel flows smoothly. As a result, the boosting efficiency of the fuel is improved and the pump efficiency is improved.

In the second aspect of the invention, by setting 20 ° ≦ α, the angle at which the swirling flow collides with the rear surface when flowing into the blade groove becomes small. As a result, the swirl flow smoothly flows into the blade groove along the rear surface, so that the decrease in energy of the swirl flow is reduced and the pump efficiency is improved.
In the invention described in claim 3, since the impeller described in claim 1 or 2 is used, the pump efficiency of the fuel pump is improved, and as a result, the efficiency of the fuel pump is improved. Therefore, the discharge pressure or the discharge amount of the fuel discharged from the fuel pump can be increased without increasing the power supplied to the fuel pump.

Hereinafter, a plurality of embodiments of the present invention will be described with reference to the drawings.
(First embodiment)
A fuel pump using the impeller according to the first embodiment of the present invention is shown in FIG. The fuel pump 10 is an in-tank type turbine pump mounted in a fuel tank of a vehicle, for example, and supplies the fuel in the fuel tank to a fuel injection valve (not shown). The discharge pressure of the fuel pump 10 is set in the range of 0.25 to 1 MPa, the discharge amount is 50 to 300 L / h, and the rotation speed is 4000 to 12000 rpm.

The fuel pump 10 includes a pump unit 12 and a motor unit 13 that rotationally drives the pump unit 12. The housing 14 also serves as a housing for the pump unit 12 and the motor unit 13, and crimps the end cover 16 and the pump case 20.
The pump unit 12 is a turbine pump having pump cases 20 and 22 and an impeller 30. The pump case 22 is press-fitted into the housing 14 and abutted against the step portion 15 of the housing 14 in the axial direction. The pump cases 20 and 22 are case members that rotatably accommodate an impeller 30 as a rotating member. C-shaped pump passages 202 (see FIG. 3) are formed between the pump cases 20 and 22 and the impeller 30, respectively.

  As shown in FIG. 4, a plurality of blade grooves 36 are formed in the rotation direction on the outer peripheral edge portion of the impeller 30 formed in a disk shape, and the circumferential width of the blade grooves 36 is not uniform. As a result, the blade grooves 36 are arranged at unequal pitches in the rotation direction. When the impeller 30 rotates together with the shaft 51 by the rotation of the armature 50, the fuel that has flowed into the pump passage 202 from the radially outer side of the vane groove 36 at the front in the rotational direction flows into the radial inside of the blade groove 36 at the rear in the rotational direction. By repeating such outflow and inflow of the fuel many times between the blade grooves 36, the fuel becomes a swirl flow 300 and is pressurized in the pump passage 202. The fuel sucked from the suction port 200 (see FIG. 3) provided in the pump case 20 by the rotation of the impeller 30 is boosted in the pump passage 202 by the rotation of the impeller 30 and discharged to the discharge port 206 ( 3) to the motor unit 13 side. The fuel pumped to the motor unit 13 side passes through the fuel passage 208 between the permanent magnet 40 and the armature 50 and is supplied to the engine side from the discharge port 210 provided in the end cover 16. An air vent hole 204 (see FIG. 3) provided in the pump case 20 is for exhausting the air contained in the fuel in the pump passage 202 to the outside of the fuel pump 10.

Four permanent magnets 40 formed in a quarter arc shape are attached to the inner peripheral wall of the housing 14 on the circumference. The permanent magnet 40 has four magnetic poles having different poles in the rotation direction.
Since the resin cover 70 covers the end of the armature 50 on the impeller 30 side, the rotational resistance of the armature 50 is reduced. Further, a commutator 80 is assembled at the end of the armature 50 opposite to the impeller 30. A shaft 51 as a rotating shaft of the armature 50 is supported by a bearing member 24 housed and supported in the end cover 16 and the pump case 20.

  The armature 50 has a central core 52 at the center of rotation. The shaft 51 is press-fitted into a central core 52 formed in a cylindrical shape having a hexagonal cross section. The six magnetic pole cores 54 are installed on the outer periphery of the central core 52 in the rotational direction, and are fitted and coupled to the central core 52. A bobbin 60 formed of an insulating resin is fitted to the outer periphery of each magnetic pole core 54, and a coil 62 is formed by concentrating windings on the outer periphery of the bobbin 60.

  The end of each coil 62 on the commutator 80 side is electrically connected to the coil terminal 64. The coil terminal 64 corresponds to the rotational direction position of each coil 62 and is fitted and electrically connected to the terminal 84 on the commutator 80 side. The end of the coil 62 opposite to the commutator 80 on the side of the impeller 30 is electrically connected to the coil terminal 66. The six coil terminals 66 are electrically connected by an annular terminal 68.

  The commutator 80 is a cassette type integrally formed. When the shaft 51 is pressed into the central core 52 and the shaft 51 is inserted into the through hole 81 of the commutator 80 and the commutator 80 is assembled to the armature 50, the terminals projecting toward the armature 50 side of the commutator 80 84 are fitted to the coil terminals 64 of the armature 50 and are electrically connected to the coil terminals 64.

The commutator 80 has six segments 82 installed in the rotational direction. The segments 82 are made of, for example, carbon, and the segments 82 are electrically insulated from each other by a gap and an insulating resin material 86.
Each segment 82 is electrically connected to the terminal 84 via the intermediate terminal 83. The insulating resin material 86 is formed by integrating the segment 82 (excluding a sliding surface with a brush (not shown)), the intermediate terminal 83, and the terminal 84 by insert molding, thereby forming the commutator 80. As the commutator 80 rotates with the armature 50, each segment 82 sequentially contacts the brush. As the commutator 80 rotates and sequentially contacts the brush, the current supplied to the coil 62 is rectified. The permanent magnet 40, the armature 50, the commutator 80, and a brush (not shown) constitute a DC motor.

(Impeller 30)
The structure of the impeller 30 will be described in more detail.
The impeller 30 is integrally formed in a disc shape with resin. As shown in FIG. 4, the outer periphery of the impeller 30 is surrounded by an annular portion 32, and a blade groove 36 is formed on the inner peripheral side of the annular portion 32. As shown in FIG. 1, the blade groove 36 adjacent in the rotation direction has a V-shaped partition wall 34 that is inclined forward from the substantially center in the thickness direction of the impeller 30 toward both end faces 31 in the thickness direction of the impeller 30 in the rotation direction. It is partitioned by. Further, as shown in FIG. 5, the blade groove 36 is partly divided on the radially inner side by a partition wall 35 protruding from the radially inner side of the blade groove 36 toward the radially outer side. It penetrates in the direction of the rotation axis on the outside in the radial direction. The fuel that has flowed into the blade groove 36 from the pump passages 202 on both sides in the axial direction becomes a swirl flow 300 that rotates in opposite directions on both sides in the rotation axis direction by the partition wall 35.

  As shown in FIG. 1, at least the radially inner side of the rear surface 37 at the rear of the blade groove 36 in the rotational direction is inclined backward in the rotational direction from the radially inner side to the radially outer side. A line segment 110 connecting the radially inner end 37a and the radially outer end 37b of the rear surface 37 of the blade groove 36, and a straight line 104 extending radially outward from the radially inner end 37a on the radius 102 of the impeller 30, Is set to a range of 15 ° ≦ α ≦ 30 °. In FIG. 1, reference numeral 100 indicates a rotation axis of the impeller 30.

  When the rearward inclination angle α is set to α <15 °, the swirl flow 300 does not flow into the blade groove 36 along the rear surface 37 and collides with the rear surface 37 at a large angle. Since this collision force acts on the side opposite to the rotation direction of the impeller 30, the impeller 30 is prevented from rotating. Further, when the rearward inclination angle α is set to α> 30 °, the rear surface 37 is excessively inclined rearward in the rotational direction with respect to the swirling flow 300 flowing into the blade groove 36, so that the swirling flow 300 enters the blade groove 36. When flowing in, separation occurs in the swirl flow 300. As a result, the resistance when the swirling flow 300 flows into the blade groove 36 is increased.

  Therefore, in the first embodiment, by setting the backward inclination angle α in the range of 15 ° ≦ α ≦ 30 °, the swirl flow 300 flows smoothly into the blade groove 36 and the swirl flow 300 flows into the blade groove 36. The resistance is reduced as much as possible. Thereby, as shown to (A) of FIG. 6, the fall from the maximum value of pump efficiency is reduced as much as possible. The backward tilt angle α is preferably set to 20 ° ≦ α.

  Further, the rear surface 37 of the blade groove 36 is inclined forward in the rotational direction from the center 37 c in the thickness direction of the impeller 30 toward both end surfaces 31 in the thickness direction of the impeller 30. That is, the rear surface 37 is formed in a V shape from the center 37 c in the thickness direction of the impeller 30 toward both end surfaces 31 of the impeller 30. A line segment 112 connecting the thickness direction center 37c of the rear surface 37 and the thickness direction both ends 37d of the impeller 30 of the rear surface 37, and a straight line 106 extending forward in the rotational direction along the circumferential direction from the thickness direction center 37c. Is set to a range of β ≦ 60 °. The straight line 106 is orthogonal to the central axis 100.

  When the forward tilt angle β is set in a range of β> 60 °, the energy component that the swirling flow 300 receives from the vane groove 36 toward the front in the rotation direction when flowing out of the vane groove 36 is reduced. The pitch in the rotation direction becomes longer. As a result, the interval between the blade grooves 36 until the swirl flow 300 flows out of the blade groove 36 and flows into the next blade groove 36 at the rear in the rotation direction becomes longer. That is, since the number of times the swirl flow 300 enters and exits the blade groove 36 while flowing through the pump passage 202 decreases, the fuel pressure is not sufficiently increased.

  Therefore, in the first embodiment, by setting the forward tilt angle β in the range of β ≦ 60 °, the energy component that the swirl flow 300 receives from the blade groove 36 toward the front in the rotation direction when flowing out from the blade groove 36 is obtained. Since it becomes large, the pitch in the rotational direction of the swirl flow 300 is shortened. As a result, the number of times the swirl flow 300 enters and exits the blade groove 36 while flowing through the pump passage 202 increases, so that the fuel boosting efficiency is improved. Thereby, as shown to (B) of FIG. 6, the fall from the maximum value of pump efficiency is reduced as much as possible.

Here, if the forward inclination angle β is too small or too large with respect to the backward inclination angle α, the swirling flow 300 flowing out from the blade groove 36 along the rear surface 37 at the forward inclination angle β has the backward inclination angle α. It cannot smoothly flow into the rear surface 37 of the blade groove 36.
Therefore, in the first embodiment, by setting 1 ≦ β / α ≦ 4, the fuel can smoothly flow into the blade groove 36 within the range of 15 ° ≦ α ≦ 30 ° and β ≦ 60 °. The magnitudes of the inclination angle α and the forward inclination angle β are adjusted. Thereby, as shown to (C) of FIG. 6, the fall from the maximum value of pump efficiency is reduced as much as possible.

  Further, in the first embodiment, the front surface 38 in the front direction of rotation of the blade groove 36 is V-shaped from the center 37 c in the thickness direction of the impeller 30 toward both end surfaces 31 of the impeller 30, similarly to the rear surface 37. Is formed. Thus, by making the shape of the rear surface 37 and the front surface 38 of the blade groove 36 substantially the same, the amount of fuel flowing out of the blade groove 36 and the amount of fuel flowing into the blade groove 36 are substantially equal. Become. As a result, fuel boosting efficiency is improved.

  In the first embodiment, the annular portion 32 covers the radially outer side of the blade groove 36, and no pump passage is formed on the outer peripheral side of the impeller 30. As a result, the differential pressure in the rotational direction of the fuel pressure boosted in the pump passage 202 is not directly applied in the radial direction of the impeller 30, so the force applied to the impeller 30 in the radial direction is reduced. Thereby, since the rotation center of the impeller 30 can be prevented from shifting, the impeller 30 can rotate smoothly.

(Second, third, fourth and fifth embodiments)
FIG. 7 shows a second embodiment of the present invention, FIG. 8 shows a third embodiment, FIG. 9 shows a fourth embodiment, and FIG. 10 shows a fifth embodiment. In addition, the same code | symbol is attached | subjected to substantially the same component as embodiment mentioned above. The configuration of the fuel pump in which the impeller of each embodiment is used is substantially the same as that of the first embodiment.

In the second, third, fourth, and fifth embodiments, as in the first embodiment, at least the radial direction of the rear surfaces 121, 131, 141, and 151 behind the blade grooves 120, 130, 140, and 150 in the rotational direction. The inner side is inclined rearward in the rotational direction from the radially inner side to the radially outer side. A line segment connecting the radially inner ends 121a, 131a, 141a, 151a of the rear surfaces 121, 131, 141, 151 of the blade grooves 120, 130, 140, 150 and the radially outer ends 121b, 131b, 141b, 151b. 110 and the straight inclination angle α formed by the straight line 104 extending radially outward from the radial inner ends 121a, 131a, 141a, 151a on the radius 102 of the impeller is set in a range of 15 ° ≦ α ≦ 30 °. ing.
Further, the forward inclination angle β of the rear surfaces 121, 131, 141, 151 of the blade grooves 120, 130, 140, 150 is also set in a range of β ≦ 60 ° as in the first embodiment. Further, 1 ≦ β / α ≦ 4 is set.

In the second embodiment shown in FIG. 7, the four corners of the blade groove 120 are formed in an arc shape. In this case, the radially inner end 121a and the radially outer end 121b of the rear surface 121 indicate substantially the center of the arc.
In the third embodiment shown in FIG. 8, the radially outer side of the rear surface 131 of the blade groove 130 is inclined forward in the rotational direction toward the radially outer side. A smooth curved surface is formed between the radially inner side and the radially outer side of the rear surface 131.
In the fourth embodiment shown in FIG. 9, the radially outer side of the rear surface 141 of the blade groove 140 is formed substantially along the straight line 104 toward the radially outer side. A smooth curved surface is formed between the radially inner side and the radially outer side of the rear surface 141.
In the fifth embodiment shown in FIG. 10, the rear surface 151 of the blade groove 150 is a flat surface.

(Other embodiments)
In the above embodiments, the radially outer side of the blade groove is covered with the annular portion 32 (see FIG. 4). However, in the present invention, the radially outer side of the blade groove may be opened without providing the annular portion 32. Further, in the above embodiments, the shape of the front surface in the rotation direction of the blade groove is V-shaped in accordance with the shape of the rear surface, but the front surface of the blade groove may be a plane along the thickness direction. .

In the above embodiments, the motor unit of the fuel pump is a brush motor, but the motor unit may be a brushless motor.
As described above, the present invention is not limited to the above-described plurality of embodiments, and can be applied to various embodiments without departing from the gist thereof.

(A) is the schematic diagram which looked at the blade groove | channel of the impeller by 1st Embodiment from the fuel suction side, (B) is the BB sectional drawing of (A). Sectional drawing which shows the fuel pump of 1st Embodiment. (A) is explanatory drawing which shows the pump case on the discharge side, (B) is explanatory drawing which shows the pump case on the suction side. (A) is the whole view which looked at the impeller by 1st Embodiment from the fuel suction side, (B) is an enlarged view of the blade groove part of (A). The enlarged view of the pump channel | path shown in FIG. (A) is a characteristic diagram showing the relationship between the backward tilt angle α and the pump efficiency, (B) is a characteristic diagram showing the relationship between the forward tilt angle β and the pump efficiency, and (C) is a graph showing the relationship between β / α and the pump efficiency. The characteristic view which shows a relationship. The enlarged view which shows the blade groove | channel of 2nd Embodiment. The enlarged view which shows the blade groove | channel of 3rd Embodiment. The enlarged view which shows the blade groove | channel of 4th Embodiment. The enlarged view which shows the blade groove | channel of 5th Embodiment.

Explanation of symbols

DESCRIPTION OF SYMBOLS 10: Fuel pump, 12: Pump part, 13: Motor part, 20, 22: Pump case (case member), 30: Impeller, 31: End surface, 34: Partition, 36, 120, 130, 140, 150: Blade groove , 37, 121, 131, 141, 151: rear face, 37a, 121a, 131a, 141a, 151a: radially inner end, 37b, 121b, 131b, 141b, 151b: radially outer end, 37c: thickness direction center 37d: thickness direction both ends, 100: rotating shaft, 102: radius, 104, 106: straight line, 110, 112: line segment, 202: pump passage

Claims (3)

An impeller for a fuel pump, wherein the pressure is increased by rotating fuel in a pump passage formed along the rotation direction of the impeller.
A plurality of blade grooves provided in the rotation direction, and a partition wall partitioning the blade grooves adjacent in the rotation direction,
At least the radially inner side of the rear surface behind the rotational direction forming the blade groove is inclined rearward in the rotational direction from the radially inner side toward the radially outer side, and the rear surface is tilted from the center in the thickness direction of the impeller. Inclined forward in the rotational direction toward both sides in the thickness direction of
A backward inclination angle formed by a line segment connecting the radially inner end and the radially outer end of the rear surface and a straight line extending radially outward from the radially inner end of the impeller is defined as α, Before a line segment connecting the center in the thickness direction of the impeller on the rear surface and both ends in the thickness direction on the rear surface, and a straight line extending forward in the rotational direction along the circumferential direction from the center in the thickness direction are formed. An impeller characterized in that 15 ° ≦ α ≦ 30 °, β ≦ 60 °, and 1 ≦ β / α ≦ 4, where β is an inclination angle.   The impeller according to claim 1, wherein 20 ° ≦ α. A motor section;
The impeller according to claim 1 or 2, which is rotated by a rotational driving force of the motor unit,
A case member that rotatably accommodates the impeller and forms the pump passage;
A fuel pump comprising:

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