JP2003093500A - Blood pump - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide miniaturized blood pump capable of constantly keeping good state of rotation of an impeller even when a runout occurs in the impeller by causing an effect of restoring the runout. SOLUTION: The blood pump has a housing 2 having a stator 7, an impeller side magnet 8 generating magnetic force between the stator 7 and an inlet port 3, and between the stator and an outlet port 4, and the impeller 5 rotatably supported by a bearing only from a one face side. The impeller is supported by a tapered face formed on the bearing. Each opposing end face of the impeller side magnet 8 and the stator 7 is formed so that it is a curved surface approximate to a surface of an imaginary sphere using a center of a circle passing each vertex of a trapezoid which is a cross sectional shape of the bearing as a runout center.

Description

Detailed Description of the Invention

[0001]

TECHNICAL FIELD The present invention relates to a blood pump for circulating blood by rotating an impeller, and in particular,
The present invention relates to a blood pump that is small in size and always has good impeller rotation.

[0002]

2. Description of the Related Art Conventionally, as a blood pump for an extracorporeal circulation circuit, a centrifugal pump type blood pump is known in addition to a pulsating pump type for supplying a pulsating flow, a roller pump type for supplying a smooth flow. It is widely used in artificial heart-lung machines and cardiac assist circulation devices after open heart surgery. Such a centrifugal pump type blood pump includes a pump chamber that communicates with an inlet port and an outlet port, rotates an impeller in the pump chamber, and causes a smooth flow according to a centrifugal force generated by the rotation and a differential pressure before and after the pump. To supply.

On the other hand, the impeller arranged in the centrifugal pump type blood pump has a structure in which the center of rotation is rotatably supported by a bearing formed in the pump chamber, and therefore the impeller is rotated by the rotation of the impeller. There is a problem that heat is generated on the sliding surface between the support portion and the bearing, and blood is easily hemolyzed (a phenomenon in which blood cells are destroyed) in the vicinity of the heat generating portion.

Further, since the above blood pump is installed outside the body for the purpose of supplying or circulating blood, its size has not been a big problem, but in the future, the blood pump will be put into the body. It is considered to be embedded and used as an artificial heart or the like. In that case, it is necessary to make the blood pump smaller, particularly thin.

As described above, in order to reduce the heat generation that causes hemolysis and to achieve the downsizing of the blood pump,
It is effective to support the impeller only from one side thereof, and a blood pump having such a support structure is disclosed in, for example, Japanese Patent Application Laid-Open No. 4-224760. According to the blood pump disclosed in this publication, compared to a blood pump that supports an impeller on both sides, sliding parts, that is, heat generating parts can be reduced to suppress hemolysis, and a bearing is formed on only one side. Therefore, the entire blood pump can be downsized.

[0006]

However, in the above-described conventional blood pump having an impeller supported only from one side, the impeller is attached to the rotation shaft depending on various conditions such as the rotation speed and size of the impeller. There is a risk that it may shake against the impeller, and there is a problem that good rotation of the impeller cannot always be obtained.

That is, as shown in FIG. 12, in the case of the impeller I in which the second magnet M2 rotates while pulling the first magnet M1 to rotate about the axis L, structurally, the center of deflection C is the center of direction a. Of the pump chamber P due to the side surface of the impeller I.
In addition to making it easier to contact the inner surface of the pump, in order to downsize the blood pump, it is necessary to reduce the clearance between the impeller and the inner surface of the pump chamber. Even just by doing so, there was a problem that the side surface of the impeller comes into contact with the inner peripheral surface of the pump chamber.

Further, when the impeller I swings around the swing center C, the first magnet M1 and the second magnet M2
When there is a difference in the separation dimension between the first magnet M1 and the second magnet M1 on the right side,
While the clearance with the magnet M2 becomes smaller, the clearance on the left side becomes larger and the magnetic force on the smaller clearance side (that is, the right side) becomes larger. Therefore, the magnetic force acts in the direction to amplify the amplitude due to the deflection of the impeller I. There is also a problem that the side surface of the impeller I and the inner peripheral surface of the pump chamber P are easily contacted with each other.

As described above, when the side surface of the impeller comes into contact with the inner peripheral surface of the pump chamber, the rotational speed of the impeller decreases and the runout further increases, so that the rotation becomes unstable and the blood supply action is performed. There is a problem that the life of the blood pump is shortened due to damage of the impeller and the like. In addition, contact with the impeller pump chamber may generate heat, which may accelerate hemolysis, and if the contact damages the impeller surface, the damage may also cause hemolysis. Could occur.

The present invention has been made in view of the above circumstances, and even when the impeller shakes while achieving downsizing, the rotation of the impeller is always good by producing the action of returning the shake. It is to provide a blood pump that can.

[0011]

The invention according to claim 1 is
A housing having a pump chamber formed therein and having a driving magnet capable of exerting a magnetic force in the pump chamber, an inlet port communicating with the pump chamber and introducing blood into the pump chamber, and communicating with the pump chamber. And an outlet port for drawing blood from the pump chamber, and an impeller-side magnet that is disposed in the pump chamber and exerts a magnetic force between the driving magnet and
An impeller rotatably supported only from one side by a bearing extended in the pump chamber, and the impeller is rotated by a magnetic force between the driving magnet and the impeller side magnet, and the impeller is rotated from the inlet port. A blood pump for drawing out blood introduced into a pump chamber from the outlet port, the impeller being supported by a tapered surface formed on the bearing, and passing through each apex of a trapezoid which is a sectional shape of the bearing. The end face of the impeller-side magnet and the end face of the driving magnet that face each other are formed so as to form a curved surface that approximates the surface of a virtual sphere with the center of the circle as the swing center, and the impeller-side magnet and the drive are formed. So that the centers of the respective facing surfaces in the thickness direction of the magnet for use are located on straight lines extending from the center of deflection. Characterized by being arranged La-side magnet and the drive magnet.

According to this structure, when a magnetic force is exerted in the pump chamber by the driving magnet, an attractive force based on the magnetic force is generated between the driving magnet and the impeller side magnet arranged in the impeller, and the impeller is Rotates in the pump chamber around the bearing. Due to the rotation of the impeller, the blood introduced from the inlet port will be discharged from the outlet port through the pump chamber, but even if the impeller sways from its rotation axis, magnetic force will be returned in the direction to return the sway. To work.

According to a second aspect of the present invention, the impeller is supported by a spherical surface instead of the tapered surface, and the surface of a virtual sphere having a center of a circle, which is a sectional shape of a bearing thereof, as a swing center is approximated. The end surface of the impeller-side magnet and the end surface of the driving magnet that face each other are formed so as to form a curved surface.

According to a third aspect of the present invention, instead of the tapered surface, the impeller is supported at one point, and the curved surface approximates to the surface of a virtual sphere with the supporting point as the center of deflection. The end surface of the impeller-side magnet and the end surface of the driving magnet are formed.

According to a fourth aspect of the present invention, the side surface of the impeller and the inner peripheral surface of the pump chamber facing the side surface are curved surfaces approximate to the surface of an imaginary sphere centered on the swing center of the impeller. It is characterized by

According to a fifth aspect of the present invention, the driving magnet is arranged in a state in which the driving magnet applies a rotational force to the impeller and an attraction force that attracts the impeller to the bearing side. Characterize.

[0017]

BEST MODE FOR CARRYING OUT THE INVENTION Embodiments of the present invention will be specifically described below with reference to the drawings. The blood pump according to the present embodiment causes blood introduced from the inlet port to be discharged from the outlet port by the rotational force of the impeller, and as shown in FIG. 1, a housing 2 in which a pump chamber 6 is formed, It is mainly configured by an inlet port 3 and an outlet port 4 formed in communication with the pump chamber 6 and an impeller 5 arranged in the pump chamber 6.

The housing 2 is a substantially cylindrical molded product made of transparent resin, and has a base portion 2a, an upper lid 2b and a lower lid 2c.
It is mainly composed of The base portion 2a has a first recess P1 that opens downward to form a pump chamber 6 in the center.
And a second recess P2 that is opened upward so as to dispose the stator 7 around the first recess P1 is formed in an annular shape, and the opening of the first recess P1 is covered with a lower lid. Two
By closing with c, the pump chamber 6 is formed, and by closing the opening of the second recess P2 with the upper lid 2b, the stator 7 and its wiring and the like are made internal in the housing 2.

The lower lid 2c has an O-ring 10 on the contact surface with the base 2a, and a screw 11 is used to attach the base 2 to the base 2.
The upper lid 2b is joined to the lower surface of a, and the upper lid 2b has a female screw portion formed on the outer peripheral edge portion thereof screwed into a male screw formed on the outer peripheral edge portion of the base portion 2a. The upper lid 2b and the lower lid 2c may be fixed to the base portion 2a by other joining means and methods, although they are joined to the upper surface.

The stator 7 disposed in the second recess P2
As shown in FIG. 2, the yoke 12 is formed in an annular shape.
And a coil portion 7 formed by winding a conductive wire around the stator core 7a.
b) and a driving magnet that can exert a magnetic force inside the pump chamber 6. The tip end of the stator core 7a is formed so as to widen along the inner peripheral surface of the pump chamber 6, while the coil portion 7b wound around the base end side of the stator core 7a is provided with an externally provided power source, control means, etc. When a voltage is applied to the coil portion 7b by such a power source, a current flows through the coil portion 7b, and a current flows from the tip of the stator core 7a into the pump chamber 6 from the tip of the stator core 7a. It is configured to exert a magnetic force.

The inlet port 3 is formed so as to project from the upper surface of the housing 2, communicates with the pump chamber 6 and introduces blood into the pump chamber 6, and the outlet port 4 is formed so as to project from the side surface of the housing 2. Then, the blood in the pump chamber 6 is led to the outside by communicating with the pump chamber 6.
The inlet port 3 and the outlet port 4 are formed at their tips with a plurality of annular projections so that the tips of a flexible tube or the like can be fitted and locked.

As shown in FIGS. 3 and 4, the inlet port 3 is formed with a pedestal portion 3a that abuts and is screwed to the upper surface of the housing 2, and two pedestals are formed downward from the lower portion. A column portion 3b is extended, and a bearing 3c is formed at the tip thereof. The bearing 3c is formed with a through hole extending vertically through the center of the top and rotatably supporting the impeller 5, and has a tapered surface 3ca at the lower end surface, and a tapered surface corresponding to the tapered surface 3ca. It forms a sliding surface for rotation of the impeller with 5a.

The impeller 5 is arranged in the pump chamber 6,
In addition to having an impeller-side magnet 8 that exerts a magnetic force on the stator 7 by energizing the stator 7,
It is rotatably supported only from the upper surface side by a bearing 3c extending in the pump chamber 6, and as shown in FIG. 5, rotation of blades 5b radially formed from the center causes blood to flow to the blood. It has a fluidizing effect. Incidentally, FIG.
Reference numeral 9 indicates a yoke fixed to the inner peripheral surface of the impeller-side magnet 8.

When the end surface of the impeller-side magnet 8 arranged in the impeller 5 receives the magnetic force exerted from the tip end surface of the stator core 7a, the impeller 5 rotates about the bearing 3c in a predetermined direction. Part 7b
The rotation speed of the impeller 5 can be adjusted by controlling the timing of applying a voltage to the impeller 5. The shape of the blade portion 5b of the impeller 5 may be any other shape as long as it exerts a flow action on the blood in the pump chamber 6.

An annular rotation center member 5c is fitted and fixed to the central portion of the impeller 5, and the above-described tapered surface 5a is formed on the upper inner peripheral surface of the rotation center member 5c. . The tapered surface 3 of the bearing 3c is attached to the tapered surface 5a.
As shown in FIG. 4, the stator core 7a is disposed above the impeller-side magnet 8 and a suction force F is applied upward by the stator 7 so that the impeller 5 can contact the ca. It will be supported only from one side (upper surface) side while being attracted to the side.

Since the impeller 5 is supported only from one side as described above, the size can be reduced as compared with the case where the impeller 5 is supported from both sides, and the number of supporting points of the impeller 5 which are heat generating parts can be reduced. , Impeller 5
It is possible to suppress the heat generation due to the rotation of the, and suppress the hemolysis. Further, since the tapered surface 3ca of the bearing 3c and the tapered surface 5a of the rotation center member 5c are sliding surfaces when the impeller 5 rotates, centering is easy and stable rotation of the impeller 5 can be obtained. it can.

However, in the support of the impeller 5 as described above, when the impeller 5 is rotated, a shake (symbol a in FIG. 4) centering on the shake center C may occur.
The impeller according to the present embodiment has the following configuration. That is, as shown in FIG. 6, assuming a virtual sphere A having a radius r1 centered on the center of deflection C of the impeller 5, the side surface 5d of the impeller 5 is a curved surface approximate to the surface of the virtual sphere A, while the center of deflection is Assuming an imaginary sphere B having a radius r2 centered on C, the inner peripheral surface 6a of the pump chamber 6 is a curved surface approximated to the surface of the imaginary sphere B.

Here, the phantom sphere means a phantom sphere that is simply drawn on a design drawing or the like, and the swing center of the impeller means the center when the impeller sways. That is,
The clearance h between the side surface 5d of the impeller 5 and the inner peripheral surface 6a of the pump chamber 6 obtained by subtracting the radius r1 of the phantom sphere B from the radius r2 of the phantom sphere B is centered around the center C where the impeller 5 swings. Even if it swings, it is maintained, and the contact of the impeller 5 with the inner peripheral surface 6a of the pump chamber 6 can be avoided.

In the case of this embodiment, as shown in FIG.
The impeller 5 is formed by the tapered surface 3ca formed on the bearing 3c.
, The center of the circle E passing through each vertex of the trapezoid, which is the cross-sectional shape, is the center of deflection C. Here, the center of the phantom sphere A and the center of the phantom sphere B may be slightly deviated due to the machining accuracy, the assembling accuracy, and the like. Especially, in the case of the support by the tapered surface, they are deviated to some extent when the impeller 5 is swung. However, if the amount of deviation is within the range of the clearance h, the impeller side surface and the inner peripheral surface of the pump chamber still do not contact, so it is sufficient to design the above deviation amount to be the clearance h. For example, the clearance amount h is preferably about 1 to 2 mm.

In addition, as shown in FIG. 15, the bearing 3
In the case where the impeller 5 is supported by the spherical surface 3c'a formed in c ', the center of the circle F, which is the cross-sectional shape, becomes the swing center C. In this case, when the impeller swings, Since there is no deviation between the center of the phantom sphere A and the center of the phantom sphere B as described above, it is not necessary to consider the clearance h.

Further, in the blood pump according to this embodiment, as shown in FIGS. 7 and 8, the end surface 8a of the impeller-side magnet 8 and the tip surface 7aa of the stator core 7a are disposed so as to face each other, and The end surface 8a and the tip surface 7aa are curved surfaces that are approximate to the surfaces of phantom spheres A '(radius r3) and B' (radius r4) centered on the swing center C of the impeller 5. That is, the tip end surface 7aa of the stator core 7a is formed with a predetermined curvature in the circumferential direction and the up-down direction of the blood pump 1 along the surface of the phantom sphere B ', and the end surface 8a of the impeller side magnet 8 is also the phantom sphere B'. The blood pump 1 is formed with a predetermined curvature in the circumferential direction and the up-down direction along a virtual sphere A having the same center as the '.

Further, as shown in FIG.
The stator core 7a and the impeller-side magnet 8 are arranged such that the centers C1 and C2 of the tip end face 7aa and the end face 8a in the thickness direction of the a and the impeller-side magnet 8 are located on the straight line m extending from the deflection center C, respectively. Although only the left side portion in FIG. 7 is shown in FIG. 7, the stator core 7a and the impeller side magnet 8 on the right side portion are also arranged at the same positions.

Next, the operation of the blood pump 1 will be described. First, after connecting a flexible tube constituting a predetermined part (for example, a blood circuit) to the tips of the inlet port 3 and the outlet port 4, the voltage is applied to the stator 7 by the power source while controlling the application by the control means. To rotate the impeller 5. That is, a rotating magnetic field is generated by rotating the phase of the voltage applied to the plurality of stators 7 surrounding the pump chamber 6, so that the impeller 5 is given a rotational force. At this time, the impeller 5 rotates while being attracted upward by the magnetic force generated between the end surface 8a of the magnet 8 and the tip surface 7aa of the stator core 7a that are arranged so as to face each other, so that stable rotation of the impeller 5 is obtained. be able to.

That is, in addition to the rotational force on the impeller 5, a force F (see FIG. 4) that is attracted upward by the attractive force between the impeller-side magnet 8 and the stator core 7a acts, and as a result, the rotational center of the impeller 5 is applied to the bearing 3c. Since the taper surface 5a of the rotation center member 5c slides while being pressed by the taper surface 3ca of the bearing 3c, the centering effect of the taper is sufficiently exerted. At this time, the magnetic flux leakage of the magnet 8 and the stator 7 is prevented by the yokes 9 and 12, and the magnetic forces can be efficiently applied (interacted) with each other.

By the way, since the rotating impeller 5 is supported only from one side, depending on various conditions such as the rotational speed of the impeller 5 (especially when the rotational speed is low), it may swing around the center of deflection C. However, the clearance h between the side surface 5d of the impeller 5 and the inner peripheral surface 6a of the pump chamber 6 is maintained regardless of whether the impeller 5 is swung by a predetermined angle, and the impeller 5 continues to rotate while avoiding contact between them. It will be.

Further, even if the clearance h is extremely small (the clearance needs to be larger than the clearance that causes hemolysis), the contact between the impeller 5 and the pump chamber 6 can be prevented, so that the stator core 7a can be prevented.
The distance between the tip of the rotor and the impeller-side magnet 8 can be shortened to the maximum, and the rotation efficiency of the impeller 5 with respect to the voltage applied to the stator 7 can be improved.

That is, as the distance between the tip of the stator core 7a and the impeller side magnet 8 increases, the magnetic force (attracting force) exerted by the stator core 7a on the impeller side magnet 8 is increased.
However, in the past, in order to avoid contact between the impeller 5 and the pump chamber 6, the separation dimension must be increased at the expense of impeller rotation efficiency. On the other hand, according to the present invention, since such contact is avoided, the limit separation dimension can be made extremely small and the rotation efficiency of the impeller can be improved.

Further, in the present embodiment, the impeller 5
Even if the end surface 8a of the impeller-side magnet 8 and the tip end surface 7aa of the stator core 7a, where an attractive force based on the magnetic force is generated, are relatively deviated, the increase in the attractive force that amplifies the conventional shake is prevented. At the same time, the magnetic force acts on the impeller 5 so that the impeller 5 is not shaken, and the stable rotation of the impeller 5 can be maintained.

For example, as shown in FIG. 9, the end surface 8a of the impeller side magnet 8 and the tip surface 7a of the stator core 7a.
Considering the magnetic force based on the magnetic force line t (when viewed in a predetermined cross section) between a and a, if the impeller 5 shakes by a small amount, the magnetic force line t as shown in FIG. 10 is obtained. In this case, the magnetic force line t
A magnetic force (attracting force) F is generated due to the magnetic force F, and the magnetic force F causes a rotational moment about the deflection center C, and the rotational moment corrects the deflection of the impeller 5.

That is, the magnetic force F after the impeller 5 shakes is
As shown in FIG. 10, it can be decomposed into a force Fa in a direction of a straight line m extending from the shake center C and a force Fb in a direction orthogonal to the straight line m. Rotational moment N (= r × Fb)
Occurs. Although only the left side of FIG. 9 is shown in the figure, the same component force is generated on the right side as well.
A rotation moment that corrects the runout of the impeller 5 is generated, and a rotation moment of 2N acts on the impeller 5 together with the left-side rotation moment N described above.

On the other hand, when the impeller 5 further swings to the state shown in FIG. 11, the magnetic force line t generated from the end face 8a of the impeller side magnet 8 cannot reach the tip end face 7aa of the stator core 7a, and the impeller 5 cannot be reached. The force does not work in the direction to return the swing of. Therefore, when the line of magnetic force t is within an allowable range where it can reach from the impeller-side magnet 8 to the stator core 7a, the impeller 5 is in the most balanced position, and stable rotation is maintained if a slight amount of vibration occurs. Can be done.

Then, the blade portion 5b is rotated in accordance with the rotation of the impeller 5, and a pump operation for introducing blood from the inlet port 3 and discharging the blood from the outlet port 4 is performed. By stopping the voltage application, the magnetic force from the stator core 7a disappears, the rotation of the impeller 5 stops, and the driving of the blood pump 1 stops.

Although the present embodiment has been described above, the present invention is not limited to this, and may be applied to, for example, a structure in which the bearing is supported from the lower surface side of the impeller. In this case, the pump chamber The lower surface of the impeller is preferably supported by another bearing protruding from the bottom surface. Further, it is also possible to make the tip of the bearing spherical and form a concave portion corresponding to the spherical shape at the center of rotation of the impeller, and use these as sliding surfaces when the impeller rotates.

Further, as shown in FIG. 13, a permanent magnet 7'as a drive magnet for imparting the rotational force of the impeller 5 is provided.
May be used, and in this case, each impeller side magnet 8
A plurality of permanent magnets 7 ′ are formed in an annular shape so that the poles of the surfaces facing each other are alternately reversed and are rotated by the motor M, and the magnetic force in the rotation direction is applied to the impeller-side magnet 8 to rotate the impeller 5. It is preferable that it is configured as follows. In this way, in the mode in which the impeller is supported at one point, the supporting point is the swing center C.

Of course, even in this case, the end surface of the permanent magnet 7'and the end surface of the impeller-side magnet 8 are opposed to each other to generate a magnetic force between the opposed surfaces, and each of the opposed surfaces is impeller 5. Of the eccentricity center C of the impeller side magnet 8
It is necessary to arrange the permanent magnet 7'and the impeller-side magnet 8 so that the centers of the respective facing surfaces in the thickness direction of the permanent magnet 7'are located on the straight lines extending from the swing center C, respectively.

[0046]

According to the first to third aspects of the present invention, even when the impeller shakes while achieving downsizing, by causing a function of returning the shake, the rotation of the impeller is always improved. You can

According to the fourth aspect of the present invention, even if the impeller shakes while achieving downsizing, the rotation of the impeller can be always improved by producing the action of returning the shake. In addition, it is possible to prevent the side surface of the impeller from coming into contact with the inner peripheral surface of the pump chamber when the impeller swings.

According to the invention of claim 5, in addition to the effects of claims 1 to 4, since the attraction force for attracting the impeller to the bearing side is generated by the driving magnet, the impeller swings from the bearing. It is possible to suppress the occurrence of rotation, and more stable rotation can be achieved.

[Brief description of drawings]

FIG. 1 is a vertical cross-sectional view showing a blood pump according to an embodiment of the present invention.

FIG. 2 is a top view showing a blood pump according to an embodiment of the present invention.

FIG. 3 is a schematic diagram showing a bearing and an impeller in the blood pump according to the embodiment of the present invention.

FIG. 4 is a schematic diagram showing a bearing and an impeller in the blood pump according to the embodiment of the present invention.

FIG. 5 is a bottom view showing the impeller in the blood pump according to the embodiment of the present invention.

FIG. 6 is a schematic diagram showing the shapes of an impeller and a pump chamber in the blood pump according to the embodiment of the present invention.

FIG. 7 is a schematic diagram showing the positional relationship between the impeller-side magnet and the stator core in the blood pump according to the embodiment of the present invention when viewed from the side.

FIG. 8 is an enlarged schematic view of a part of FIG.

FIG. 9 is a schematic diagram showing magnetic lines of force before the impeller shakes in the blood pump according to the embodiment of the present invention.

FIG. 10 is a schematic diagram showing magnetic lines of force after a slight amount of shake of the impeller in the blood pump according to the embodiment of the present invention.

FIG. 11 is a schematic diagram showing magnetic lines of force after a large deflection of the impeller in the blood pump according to the embodiment of the present invention.

FIG. 12 is a schematic diagram for explaining runout when the impeller of the blood pump is supported at one point.

FIG. 13 is a vertical sectional view showing a blood pump according to another embodiment of the present invention.

FIG. 14 is a schematic diagram for explaining a shake center C in a blood pump that supports an impeller with a tapered surface.

FIG. 15 is a schematic diagram for explaining a shake center C in a blood pump that supports an impeller on a spherical surface.

[Explanation of symbols]

1 ... Blood pump 2 ... Housing 2a ... base part 2b ... Top lid 2c ... Lower lid 3 ... Entrance port 3a ... Pedestal part 3b ... Pillar 3c ... Bearing 3ca ... Tapered surface 4 ... Exit port 5 ... Impeller 5a ... Tapered surface 5b ... feather part 5c ... Rotation center member 5d ... side 6 ... Pump room 6a ... inner peripheral surface 7 ... Stator (drive magnet) 7a ... Stator core 7aa ... Tip surface 7b ... coil part 7 '... Driving magnet 8 ... Magnet for impeller 8a ... end face 9 ... York 10 ... O-ring 11 ... screws 12 ... York 13 ... Wiring A, B, A ', B' ... virtual sphere C ... center of shake C1, C2 ... Center of the end face P1 ... First recess P2 ... second recess

   ─────────────────────────────────────────────────── ─── Continued front page    (72) Inventor Mutsumi Kojiya             498-1 Shizuya, Haibara-cho, Haibara-gun, Shizuoka Prefecture             Shizuoka Manufacturing Co., Ltd. F term (reference) 4C077 AA02 AA04 DD08 KK01 KK21

Claims (5)

[Claims] 1. A housing having a pump chamber formed therein and having a drive magnet capable of exerting a magnetic force in the pump chamber; an inlet port communicating with the pump chamber for introducing blood into the pump chamber; The pump has an outlet port that communicates with the pump chamber and draws blood from the pump chamber, and an impeller-side magnet that is disposed in the pump chamber and exerts a magnetic force between the driving magnet and the driving magnet. An impeller rotatably supported only from one side by a bearing extended in the room,
A blood pump that rotates the impeller by magnetic force between the drive magnet and the impeller-side magnet and draws out blood introduced into the pump chamber from the inlet port from the outlet port, the blood pump being formed on the bearing. The impeller side magnets that support the impeller with a tapered surface and face each other so as to form a curved surface that approximates the surface of a virtual sphere with the center of a circle passing through each vertex of the trapezoid that is the cross-sectional shape of the bearing as the swing center. And an end surface of the driving magnet are formed, and the centers of the facing surfaces in the thickness direction of the impeller-side magnet and the driving magnet are located on straight lines extending from the swing center, respectively. A blood pump having an impeller-side magnet and a drive magnet disposed therein. 2. A spherical surface is used instead of the tapered surface to support the impeller, and the surfaces are opposed to each other so as to form a curved surface that approximates the surface of an imaginary sphere with the center of a circle, which is the sectional shape of the bearing, as the swing center. The blood pump according to claim 1, wherein an end surface of the impeller-side magnet and an end surface of the driving magnet are formed. 3. In place of the tapered surface, the impeller is supported at one point, and the impeller side magnets facing each other have a curved surface similar to the surface of a virtual sphere with the supporting point as the center of deflection. An end face and an end face of the drive magnet are formed respectively.
The described blood pump. 4. The side surface of the impeller and the inner peripheral surface of the pump chamber facing the side surface are curved surfaces approximate to the surface of a virtual sphere centered on the center of deflection of the impeller. The blood pump according to any one of claims 1 to 3. 5. The drive magnet is arranged in a state of applying a rotational force to the impeller and an attractive force to attract the impeller to the bearing side. ~ The blood pump according to claim 4.