IGNITION COIL

Abstract

A magnetic path is formed of a center core disposed inside a first coil and second coil, a first side core and second side core disposed outside the first coil and second coil and coming into contact with the center core, and a magnet disposed between the first side core and second side core, wherein a shape of a space formed by a portion of contact between the first side core and second side core is a shape that forms an insertion portion of the magnet disposed obliquely with respect to the magnetic path, and voids perpendicular with respect to the magnetic path at either end portion of the magnet.

Claims

1. An ignition coil, comprising: a center core disposed inside a first coil and second coil; a first side core and second side core disposed outside the first coil and second coil and coming into contact with the center core; and a magnet disposed between the first side core and second side core, thereby forming a magnetic path passing through the center core, the first side core and second side core, and the magnet, wherein the first side core and second side core form a space at a portion of contact between the two, and a shape of the space is a shape that forms an insertion portion of the magnet disposed obliquely with respect to the magnetic path, and voids perpendicular with respect to the magnetic path at either end portion of the magnet.

2. The ignition coil according to claim 1, wherein an inner peripheral side void of the voids is on an axial line10% from a central axis of a winding length of the first coil.

3. The ignition coil according to claim 1, wherein an interval of the voids is equal to or less than a thickness of the magnet.

4. The ignition coil according to claim 1, wherein an interval of the voids is 0.45 to 0.55 times a thickness of the magnet, and a width of the voids is of a dimension such that an angle with respect to the magnetic path is 10 to 13.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0011] FIG. 1 is a sectional view showing an ignition coil according to a first embodiment of the invention.

[0012] FIG. 2 is a top view showing side cores of FIG. 1.

[0013] FIG. 3 is a sectional view showing one example of a magnetic circuit of an existing internal combustion engine ignition coil.

[0014] FIG. 4 is a partial enlarged view of FIG. 3.

[0015] FIG. 5 is a sectional view showing a magnetic circuit of the ignition coil according to the first embodiment of the invention.

[0016] FIG. 6 is a partial enlarged view of FIG. 5.

[0017] FIG. 7 is a diagram of distribution of magnetic flux in the magnetic circuit shown in FIG. 5.

[0018] FIG. 8 is a diagram of distribution of magnetic flux in the magnetic circuit shown in FIG. 3.

[0019] FIG. 9 is a diagram representing a density ratio of magnetic flux penetrating a second coil in a position of a void between an end face of a magnet and a second side core in the ignition coil according to the first embodiment of the invention.

[0020] FIG. 10 is a diagram representing energy characteristics of an ignition coil according to a second embodiment of the invention.

[0021] FIG. 11 is a diagram representing energy characteristics of the ignition coil according to the second embodiment of the invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0022] Hereafter, referring to the drawings, a description will be given of preferred embodiments of an ignition coil according to the invention. The description will be given with an internal combustion engine ignition coil as an example.

First Embodiment

[0023] FIG. 1 is a sectional view showing an internal combustion engine ignition coil according to a first embodiment of the invention, and FIG. 2 is a top view showing side cores of FIG. 1.

[0024] As shown in FIG. 1 and FIG. 2, the internal combustion engine ignition coil according to the first embodiment is such that a first coil 2 is provided outside a practically I-shaped center core 1 configured by stacking electromagnetic steel sheets. A second coil 3 is provided outside the first coil 2. One end face of an L-shaped first side core 4 is in contact with one end face of the center core 1. One end face of a magnet 5 is in contact with another end face of the first side core 4. The magnet 5 is magnetized in a direction opposite a direction of magnetic flux generated by an energizing of the first coil 2. One end face of an L-shaped second side core 6 is in contact with another end face of the magnet 5. Another end face of the second side core 6 is in contact with the center core 1, whereby a closed magnetic path configuration is formed by the center core 1, first side core 4, magnet 5, and second side core 6. Further, the internal combustion engine ignition coil configured as heretofore described is housed in a case 7. In the description above, a closed magnetic path passing through the center core 1, first side core 4, magnet 5, and second side core 6 is configured, but a configuration passing through a closed magnetic path such that a magnet other than the magnet 5, or a magnetic body other than the center core 1, first side core 4, and second side core 6, is added to the previously described closed magnetic path may be adopted as necessary.

[0025] The first side core 4 and second side core 6 are of an L-shape formed by stacking electromagnetic steel sheets. In order to dispose the magnet 5 obliquely at an angle with respect to the magnetic path, the first side core 4 is such that an inner peripheral side of the core is longer in a longitudinal direction than an outer peripheral side, and the second side core 6 is such that an outer peripheral side of the core is longer in a longitudinal direction than an inner peripheral side. A magnet insertion portion 8 is of a dimension equal to or greater than a width of the magnet 5. Inner peripheral side end portions 9a and 9b and outer peripheral side end portions 10a and 10b of the first side core 4 and second side core 6 are cut off at =90, that is, perpendicular with respect to the magnetic path. Because of this, an angle of 90+ is formed in a portion of the outer peripheral side end portion 10a of the first side core 4, and an angle of 90+ is also formed in a portion of the inner peripheral side end portion 9b of the second side core 6. When the first side core 4 and second side core 6 are assembled across the magnet 5, voids 11a and 11b, which are perpendicular with respect to the magnetic path and are flat, are formed at either end of the magnet 5.

[0026] In this way, the internal combustion engine ignition coil according to the first embodiment is such that a magnetic circuit is formed of the center core 1 disposed inside the first coil 2 and second coil 3, the first side core 4 and second side core 6, which are two side cores disposed outside the first coil 2 and second coil 3 and coming into contact with the center core 1, and the magnet 5 disposed between the first side core 4 and second side core 6, and a shape of a space formed between the first side core 4 and second side core 6 is a shape forming the magnet insertion portion 8 disposed obliquely with respect to the magnetic path, and the voids 11a and 11b that are perpendicular with respect to the magnetic path at either end portion of the magnet 5.

[0027] As shown in FIG. 3 and in FIG. 4, which is a partial enlarged view of FIG. 3, an existing internal combustion engine ignition coil is such that an orientation of voids formed at either end of the magnet 5 is oblique with respect to a magnetic path length, because of which a magnetic path length lg: of the void is greater than a thickness t of the magnet 5, and magnetic resistance increases. As opposed to this, as shown in FIG. 5 and in FIG. 6, which is a partial enlarged view of FIG. 5, the internal combustion engine ignition coil according to the first embodiment is such that the void direction is parallel to the magnetic path length, because of which a magnetic path length lg.sub.2 of the void is the same as the thickness t of the magnet 5, magnetic resistance decreases, and a magnetic property improves.

[0028] Furthermore, when assembling, the magnet 5 is adsorbed to the first side core 4 and second side core 6 by magnetic force, but positional deviation occurring when assembling can be restricted by the angles of the outer peripheral side end portion 10a of the first side core 4 and the inner peripheral side end portion 9b of the second side core 6. Moreover, when magnetic flux generated by the first coil 2 exceeds reverse direction magnetic flux of the magnet 5 when energizing the first coil 2, the magnet 5 attempts to move due to magnetic force, but the movement is kept to a minimum by the angles of the outer peripheral side end portion 10a of the first side core 4 and the inner peripheral side end portion 9b of the second side core 6, whereby a decrease in performance can be restricted.

[0029] Also, in the first embodiment, the void 11a is configured so as to be positioned on an axial line10% from a central axis 12 of a winding length of the first coil 2, as shown in FIG. 7.

[0030] In the magnetic circuit of the existing internal combustion engine ignition coil, the void 11a nears contact faces of the center core 1 and second side core 6, because of which magnetic flux distribution is such that magnetic flux leaking from the first side core 4 avoids the second side core 6 and reaches the center core 1, as shown in FIG. 8. In this case, a number of turns of the second coil 3 with which the magnetic flux interlinks decreases, and binding properties of the first coil 2 and second coil 3 deteriorate. As opposed to this, the internal combustion engine ignition coil according to the first embodiment is configured so that the position of the void 11a is far from contact faces of the center core 1 and the first side core 4 and second side core 6 when seen in terms of magnetic path length, because of which distribution is such that the magnetic flux reaches the second side core 6 from the first side core 4, as shown in FIG. 7, the number of magnetic fluxes interlinking with the second coil 3 is increased, and binding properties can be improved. FIG. 9 shows density of magnetic flux penetrating the second coil 3 in the position of the void 11a. From FIG. 9, it is seen that, when taking a maximum value of penetrating magnetic flux density in the existing configuration to be 100%, magnetic flux density decreases by approximately one-half when the void 11a is positioned on an axial line10% from the central axis 12, and it is understood that binding properties are improved.

[0031] In addition, when an interval g.sub.1 of the voids 11a and 11b is smaller than the thickness t of the magnet 5, magnetic resistance can be reduced, because of which a high-output ignition coil can be realized with a low interruption current.

[0032] In the first embodiment, a description has been given of a case in which the magnet 5 and void 11b are disposed to the right of the position of the void 11a, but the magnet 5 and void 11b can be disposed on the opposite side in accordance with fabrication circumstances.

Second Embodiment

[0033] Next, an internal combustion engine ignition coil according to a second embodiment of the invention will be described.

[0034] FIG. 10 and FIG. 11 are diagrams representing energy characteristics of the internal combustion engine ignition coil according to the second embodiment, and show energy characteristics when the dimensions of the interval g.sub.1 and width g.sub.2 of the voids 11a and 11b shown in FIG. 6 are changed. Herein, the void dimensions are adjusted and magnetic resistance reduced so that a high output is obtained with respect to a low interruption current.

[0035] The internal combustion engine ignition coil according to the second embodiment is designed so that a primary current flowing into the first coil 2 is 6 A, and a number of turns of the first coil 2 is 114 T. Output energy is integrally calculated from ampere-turns applied to a primary side and magnetic flux passing through the center core 1. Also, calculation is carried out using magnetic field analysis.

[0036] FIG. 10 shows energy characteristics for a ratio with respect to the thickness t of the magnet 5 when the interval g.sub.1 is changed from 0 when the width g.sub.2 of the voids 11a and 11b is fixed at the same dimension as the thickness t of the magnet 5. In FIG. 10, it is seen that when energy when the void width is 0 is taken to be 1, energy is highest when the interval g is 0.45 to 0.55 times the thickness t of the magnet 5.

[0037] FIG. 11 shows energy characteristics when the width g.sub.2 is changed from 0 as far as a width at which the angle =0 when the interval g.sub.1 of the voids 11a and 11b is fixed at a ratio of 0.55 times the thickness t of the magnet 5. As the width g.sub.2 changes in accordance with the angle , FIG. 11 shows energy characteristics with respect to the angle . Herein, the angle is such that energy when the angle =13 when the width g.sub.2 is of the same dimension as the thickness t of the magnet 5 is taken to be 1. From FIG. 11, it is seen that output energy does not decrease at the width g.sub.2 at which 1013, but output energy decreases in a range other than this.

[0038] According to the above, the internal combustion engine ignition coil according to the second embodiment is such that when the interval of the voids 11a and 11b is 0.45 to 0.55 times the thickness t of the magnet 5, and the width of the voids 11a and 11b is of a dimension such that 1013, a coil that has high output at a low interruption current can be realized.

[0039] Although the first and second embodiments of the invention have been described, the embodiments can be freely combined, and each embodiment can be modified or abbreviated as appropriate, without departing from the scope of the invention.