EP0635856A1 - Zündspule - Google Patents
Zündspule Download PDFInfo
- Publication number
- EP0635856A1 EP0635856A1 EP94109288A EP94109288A EP0635856A1 EP 0635856 A1 EP0635856 A1 EP 0635856A1 EP 94109288 A EP94109288 A EP 94109288A EP 94109288 A EP94109288 A EP 94109288A EP 0635856 A1 EP0635856 A1 EP 0635856A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- permanent magnet
- iron core
- ignition coil
- sectional area
- cross
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims abstract description 62
- 238000004804 winding Methods 0.000 claims abstract description 46
- 230000005415 magnetization Effects 0.000 claims description 18
- 229910000831 Steel Inorganic materials 0.000 claims description 5
- 230000035699 permeability Effects 0.000 claims description 5
- 229920001296 polysiloxane Polymers 0.000 claims description 5
- 239000010959 steel Substances 0.000 claims description 5
- 238000002485 combustion reaction Methods 0.000 claims description 3
- 229910052772 Samarium Inorganic materials 0.000 claims 2
- 229910017052 cobalt Inorganic materials 0.000 claims 2
- 239000010941 cobalt Substances 0.000 claims 2
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 claims 2
- KZUNJOHGWZRPMI-UHFFFAOYSA-N samarium atom Chemical compound [Sm] KZUNJOHGWZRPMI-UHFFFAOYSA-N 0.000 claims 2
- 230000004907 flux Effects 0.000 abstract description 24
- 230000000593 degrading effect Effects 0.000 abstract description 3
- 238000010586 diagram Methods 0.000 description 15
- BGPVFRJUHWVFKM-UHFFFAOYSA-N N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] Chemical compound N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] BGPVFRJUHWVFKM-UHFFFAOYSA-N 0.000 description 6
- 239000000463 material Substances 0.000 description 4
- 229910000976 Electrical steel Inorganic materials 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- KPLQYGBQNPPQGA-UHFFFAOYSA-N cobalt samarium Chemical compound [Co].[Sm] KPLQYGBQNPPQGA-UHFFFAOYSA-N 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000006731 degradation reaction Methods 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000008450 motivation Effects 0.000 description 1
- 238000011056 performance test Methods 0.000 description 1
- 229910000938 samarium–cobalt magnet Inorganic materials 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F38/00—Adaptations of transformers or inductances for specific applications or functions
- H01F38/12—Ignition, e.g. for IC engines
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F02—COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
- F02P—IGNITION, OTHER THAN COMPRESSION IGNITION, FOR INTERNAL-COMBUSTION ENGINES; TESTING OF IGNITION TIMING IN COMPRESSION-IGNITION ENGINES
- F02P1/00—Installations having electric ignition energy generated by magneto- or dynamo- electric generators without subsequent storage
Definitions
- the present invention relates to an improved ignition coil mainly used for internal combustion engines for vehicles.
- FIG. 6 is a schematic view showing a fundamental magnetic circuit of an iron core which has a permanent magnet inserted into an air gap portion of the ignition coil. In a magnetic circuit shown in Fig.
- reference mark SF is a cross-sectional area of the iron core through which magnetic flux ⁇ flows
- SG is a cross-sectional area of a permanent magnet supporting portion of the iron core
- LF is a mean magnetic path length
- SM is a cross-sectional area of the permanent magnet which is hatched
- LM is a thickness of the permanent magnet.
- Figs. 7 and 8 are performance characteristic diagrams for illustrating magnetic performance of the ignition coil according to the above Japanese Patent Publication.
- a curve (a) represents a magnetization characteristic of the iron core
- a straight line (b) represents a magnetization characteristic of the permanent magnet
- a curve (c) represents a magnetization characteristic of the primary winding.
- the maximum working magnetic flux density BF of the iron core is given by a value corresponding to a point T which is a tangent point on the curve (a) with a straight line being parallel to the straight line (b) as a resultant summation of (a) and (b).
- the gradient of the magnetization curve of the primary winding is determined by permeability ⁇ of the permanent magnet, it is of significance that a permanent magnet material which has a permeability value close to 1 should be selected in order to increase the energy stored in the primary winding represented by a hatched area W in Fig. 8, so that the permeability value close to 1 may contribute as an air gap which stores energy and to decline the magnetization curve of the primary winding shown in Fig. 8.
- nIp/2 HF ⁇ LF + H ⁇ LM
- H (nIp/2 - HF ⁇ LF)/LM [AT/m]
- BG ⁇ SG BF ⁇ SF
- LM [SG/SF] ⁇ [ ⁇ (nIp/2 - HF ⁇ LF)/BF]
- SG/SF 2 ⁇ BF ⁇ LM / [ ⁇ (nIp - 2HF ⁇ LF)] (1)
- the iron core is required to be magnetized by magnetizing force of the primary winding in opposition to energy possessed by the permanent magnet, so that positive flux may pass through the iron core. Therefore, where the iron core is first magnetized to the point P close to the saturation point in the negative flux region of the iron core depicted in the lower left region in Fig. 8 by the magnetizing force of the permanent magnet as described previously. Thereafter the iron core is magnetized to the point T near the saturation point in the positive flux region depicted at upper right region in Fig. 8 by the magnetizing force nIp due to the exciting current Ip through the primary winding.
- SmCo5 sinarium cobalt
- the iron core is formed of non-oriented silicon steel plates and value of elements therefore are as follows.
- the value of the elements are substituted into the equations (1) and (2) to obtain the relationship between LM and each area ratio SG/SF and SM/SF are graphically shown in Figs. 10 and 11. Illustrated in Figs.
- a secondary voltage V2 generated in the secondary winding which is obtained from performance tests conducted for various ignition coils which have different dimensions of individual portions depending on the changes in thickness LM of the permanent magnet.
- Fig. 11 shows distribution curves of the secondary voltage V2 shown in Fig. 10 after converting them into a two-dimensional characteristic curve and as a relationship between the thickness LM of the permanent magnet and the magnitude of the secondary voltage V2.
- the ignition coil in the prior art described hereinabove and illustrated in Fig. 17 is mostly effective in a highly sophisticated ignition system which may supply 6A (Amperes) drive current constantly to the primary winding which has less than one ohm resistance even in a case when a battery voltage dropped below the specified value as to maximize the magnetic flux density.
- 6A Amperes
- the relationship between the primary cut-off current and secondary output voltage (I1-V2) of the ignition coil in the prior art which has no permanent magnet but has the same secondary output voltage at the same primary current of 6A is graphically compared in Fig. 12 by a solid and dotted lines respectively.
- the output performance at around 3A primary current range becomes very important, particularly in an engine cranking time under high temperature and low battery voltage.
- thickness LM of a permanent magnet and SM/SF ratio between two cross-sectional areas SM and SF are chosen as follows so that the working magnetizing zone of a primary winding does not reside in the curved zone of magnetization characteristics in the negative region as illustrated in Fig. 4. 0.6 mm ⁇ LM ⁇ 1.8 mm and 1.3 ⁇ SM/SF ⁇ 3.0
- Fig. 1 is a sectional view of an ignition coil according to an embodiment of this invention and Fig. 2 is a side view of the same.
- an iron core 1 is made by laminated non-oriented silicone steel sheets and forms closed magnetic flux circuit via an air gap 2 diagonally arranged in the iron core 1.
- a permanent magnet 4 is inserted into the air gap 2 of the iron core 1.
- a primary winding 6 is wound on the iron core 1.
- the permanent magnet 4 is magnetized in the opposite direction to the direction of magnetization by the exciting current flowing through the primary winding 6.
- Electrical resistance of the primary winding 6 in case of this embodiment is made to be more than 1 ohm.
- a secondary winding 8 is wound on the primary winding 6.
- the mutual relationship between of thickness LM of the permanent magnet 2, diagonal cross-sectional area SM of the permanent magnet 4 and non-diagonal or normal cross-sectional area SF of the iron core 1 at the winding portion is selected to satisfy the following condition.
- the diagonal cross-sectional area SG of the iron core 1 at the air gap portion is so formed as to be nearly equal to the cross-sectional are SM of the permanent magnet 4. 0.6 mm ⁇ LM ⁇ 1.8 mm 1.3 ⁇ SM/SF ⁇ 3.0
- Fig. 4 Left lower side of Fig. 4 illustrates that magnetization by the primary winding in the negative region does not come to the magnetic saturation zone. Excessively small negative bias of the permanent magnet causes counter-effect for purpose to minimize the ignition coil. Practically, in case when the thickness LM of the permanent magnet 4 is the same as that of the prior art, the cross-sectional area SM of the permanent magnet results in roughly 2/3 of that of the permanent magnet applied in the prior art.
- Thickness LM of the permanent magnet 4 of the present invention is selected within the same range (0.6 mm ⁇ LM ⁇ 1.8 mm) of that of the prior art, because this range provides maximum secondary voltage V2 as indicated in Fig. 11.
- the ignition coil of the present invention may use its straight line portion as the magnetization curve for the primary winding by the introduction of the 2/3 factor and SM/SF ratio of 1.5.
- the stored energy W' 1.5 on the lower current range is approximately equal to the energy W' of ignition coil which has no permanent magnet.
- Fig. 5 shows that there is no difference in the secondary output voltage V2 versus cut-off current of the primary winding 6 of both ignition coils of the present invention and the prior art which has no permanent magnet.
- the ignition coil includes an iron core (1) forming a closed magnetic circuit through an air gap (2), a primary winding (6) wound around the iron core (1) for magnetizing the iron core (1) and a permanent magnet (4) magnetized in an opposite direction to a magnetizing direction by the primary winding current.
- a cross-sectional area (SG) of the iron core (1) at which the permanent magnet (4) is inserted is made substantially equal to that (SM) of the permanent magnet (4).
- the permanent magnet (4) In order for the permanent magnet (4) to bias by 2/3 of the magnetic flux saturation point of the iron core (1), the permanent magnet (4) is so shaped that its thickness (LM) satisfies 0.6 mm ⁇ LM ⁇ 1.8 mm and its cross-sectional area (SM) and the cross-sectional area (SF) of winding portion of the iron core (1) satisfies 1.3 ⁇ SM/SF ⁇ 3.0.
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Chemical & Material Sciences (AREA)
- Combustion & Propulsion (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Ignition Installations For Internal Combustion Engines (AREA)
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP14793693A JP3391049B2 (ja) | 1993-06-18 | 1993-06-18 | 点火コイル |
JP147936/93 | 1993-06-18 | ||
JP14793693 | 1993-06-18 |
Publications (2)
Publication Number | Publication Date |
---|---|
EP0635856A1 true EP0635856A1 (de) | 1995-01-25 |
EP0635856B1 EP0635856B1 (de) | 2000-09-13 |
Family
ID=15441417
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP94109288A Expired - Lifetime EP0635856B1 (de) | 1993-06-18 | 1994-06-16 | Zündspule |
Country Status (4)
Country | Link |
---|---|
EP (1) | EP0635856B1 (de) |
JP (1) | JP3391049B2 (de) |
KR (1) | KR100242545B1 (de) |
DE (1) | DE69425853T2 (de) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE102006034574B4 (de) * | 2006-01-31 | 2019-08-29 | Mitsubishi Electric Corp. | Zündspulenvorrichtung für einen Verbrennungsmotor |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP3031158U (ja) * | 1996-05-14 | 1996-11-22 | 阪神エレクトリック株式会社 | 内燃機関用点火コイル |
EP3765730A1 (de) * | 2018-03-12 | 2021-01-20 | Diamond Electric MFG. Corp. | System und verfahren für verstärkte nichtlineare zündspule |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE656392C (de) * | 1936-02-27 | 1938-02-04 | Magnetos R B Soc D | Zuendspule |
DE1464202A1 (de) * | 1962-02-23 | 1969-05-22 | Licentia Gmbh | Permanentvormagnetisiertes induktives Element |
FR2464543A1 (fr) * | 1979-09-04 | 1981-03-06 | Bbc Brown Boveri & Cie | Accumulateur d'energie magnetique |
EP0043744A1 (de) * | 1980-07-04 | 1982-01-13 | DUCELLIER & Cie | Zündspule für Brennkraftmaschine |
EP0352453A1 (de) * | 1988-07-28 | 1990-01-31 | Nippondenso Co., Ltd. | Zündspule |
EP0431322A1 (de) * | 1989-11-10 | 1991-06-12 | Nippondenso Co., Ltd. | Zündspule |
-
1993
- 1993-06-18 JP JP14793693A patent/JP3391049B2/ja not_active Expired - Lifetime
-
1994
- 1994-06-15 KR KR1019940013472A patent/KR100242545B1/ko not_active IP Right Cessation
- 1994-06-16 EP EP94109288A patent/EP0635856B1/de not_active Expired - Lifetime
- 1994-06-16 DE DE69425853T patent/DE69425853T2/de not_active Expired - Lifetime
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE656392C (de) * | 1936-02-27 | 1938-02-04 | Magnetos R B Soc D | Zuendspule |
DE1464202A1 (de) * | 1962-02-23 | 1969-05-22 | Licentia Gmbh | Permanentvormagnetisiertes induktives Element |
FR2464543A1 (fr) * | 1979-09-04 | 1981-03-06 | Bbc Brown Boveri & Cie | Accumulateur d'energie magnetique |
EP0043744A1 (de) * | 1980-07-04 | 1982-01-13 | DUCELLIER & Cie | Zündspule für Brennkraftmaschine |
EP0352453A1 (de) * | 1988-07-28 | 1990-01-31 | Nippondenso Co., Ltd. | Zündspule |
EP0431322A1 (de) * | 1989-11-10 | 1991-06-12 | Nippondenso Co., Ltd. | Zündspule |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE102006034574B4 (de) * | 2006-01-31 | 2019-08-29 | Mitsubishi Electric Corp. | Zündspulenvorrichtung für einen Verbrennungsmotor |
Also Published As
Publication number | Publication date |
---|---|
KR950001091A (ko) | 1995-01-03 |
DE69425853T2 (de) | 2001-03-15 |
KR100242545B1 (ko) | 2000-03-02 |
JPH0722256A (ja) | 1995-01-24 |
DE69425853D1 (de) | 2000-10-19 |
EP0635856B1 (de) | 2000-09-13 |
JP3391049B2 (ja) | 2003-03-31 |
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