CA2038185A1 - Magnetic circuit for a speaker - Google Patents
Magnetic circuit for a speakerInfo
- Publication number
- CA2038185A1 CA2038185A1 CA002038185A CA2038185A CA2038185A1 CA 2038185 A1 CA2038185 A1 CA 2038185A1 CA 002038185 A CA002038185 A CA 002038185A CA 2038185 A CA2038185 A CA 2038185A CA 2038185 A1 CA2038185 A1 CA 2038185A1
- Authority
- CA
- Canada
- Prior art keywords
- magnet
- magnetic circuit
- sectional shape
- yoke base
- circuit according
- 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.)
- Abandoned
Links
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
- H04R9/00—Transducers of moving-coil, moving-strip, or moving-wire type
- H04R9/02—Details
- H04R9/025—Magnetic circuit
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
- H04R9/00—Transducers of moving-coil, moving-strip, or moving-wire type
- H04R9/02—Details
- H04R9/04—Construction, mounting, or centering of coil
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
- H04R2209/00—Details of transducers of the moving-coil, moving-strip, or moving-wire type covered by H04R9/00 but not provided for in any of its subgroups
- H04R2209/022—Aspects regarding the stray flux internal or external to the magnetic circuit, e.g. shielding, shape of magnetic circuit, flux compensation coils
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Acoustics & Sound (AREA)
- Signal Processing (AREA)
- Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)
Abstract
MAGNETIC CIRCUIT FOR A SPEAKER
Abstract of the Disclosure A magnetic circuit for a speaker having a yoke has a pole formed on the yoke base, an annular magnet mounted on the yoke base, and a top plate mounted on the magnet. A periphery of the magnet has an outwardly curved sectional shape. Peripheries of the yoke base and the top plate have outwardly or inwardly curved sectional shapes, respectively.
Abstract of the Disclosure A magnetic circuit for a speaker having a yoke has a pole formed on the yoke base, an annular magnet mounted on the yoke base, and a top plate mounted on the magnet. A periphery of the magnet has an outwardly curved sectional shape. Peripheries of the yoke base and the top plate have outwardly or inwardly curved sectional shapes, respectively.
Description
203~185 The present invention relates to a magnetic circuit for a speaker used in an audio system.
An object of the present invention is to provide a magnetic circuit for a speaker which may increase magnetic efficiency, thereby enabling improvement of the tonal quality of the speaker.
Another object of the present invention is to provide a magnetic circuit which can be light in weight and may be manufactured at a low cost.
According to the present invention, there is provided a magnetic circuit for a speaker having a yoke base, a pole formed on the yoke base, an annular magnet mounted on the yoke base, and a top plate mounted on the magnet so as to form a gap between an inside wall thereof and an outer wall of the pole. At least one of the yoke base, pole and top plate has a periphery having a non-linear sectional shape.
The non-linear sectional shape is an outwardly curved sectional shape or an inwardly curved sectional shape.
In one aspect of the invention, the magnet has a periphery having an outwardly curved sectional shape.
- 203~185 The magnet, yoke base and top plate may have peripheries having respectively outwardly curved sectional shapes.
In another aspect, at least one of the yoke base and the top plate has an inwardly curved sectional shape.
The magnet may have a periphery having a sectional shape combining straight lines.
The other objects and features of this invention will become understood from the following description with reference to the accompanying drawings, in which ~ Fig. 1 is a sectional view showing a magnetic ;~ circuit according to a first embodiment of the present invention;
Fig. 2 is a sectional view of a second embodiment;
15Figs. 3 and 4 are sectional views showing third and fourth embodiments;
Fig. 5a is an illustration showing lines of magnetic force generated in the first embodiment;
Fig. 5b is an illustration showing lines of magnetic force generated in the conventional magnetic circuit;
Figs. 6, 7a and 7b are sectional views showing modifications of the sectional shape;
Fig. 8 is a sectional view of a fifth embodiment;
- ~ :
203818~
Fig. 9 is a sectional view showing a modification of the fifth embodiment;
Fig. 10 is a sectional view explaining the effects of tapered portions;
Fig. 11 is an illustration showing lines of magnetic force generated in the magnetic circuit of Fig. 9;
Fig. 12 is a table comparing performance and weight of the magnetic circuit of Fig. 8 with conventional magnetic circuits;
Figs. 13 to 19 are sectional views showing sixth to twelfth embodiments of the present invention;
Fig. 20 is a sectional view showing a conventional cone speaker; and Figs. 21 and 22 are sectional views showing lS sectional shapes of prior art magnetic circuits.
Reference will first be made to Figures 20 - 22, illustrating prior art speakers.
Fig. 20 shows a widely used cone speaker. The speaker comprises a yoke 51 having a yoke base 53 and a cylindrical pole 52 formed on the yoke base 53, an annular top plate 54, and a magnet 55 disposed between the yoke base 53 and the top plate 54. A voice coil 56 is supported by a damper 60 and disposed in a magnetic gap G between the pole 52 and the top plate 54 so as to be moved in the direction shown by arrows a and b. A frame 57 is secured , , ~ , .
;
.
203~18~
to the plate 54, and a diaphragm 59 is provided between an edge 58 of the frame 57 and the voice coil 56. Reference numeral 61 designates a terminal and 62 is a lead.
Referring to Fig. 21, the magnetic circuit is formed by the yoke 51, magnet 55 and plate 54, each of which has a rectangular cross section. Consequently, the magnetic flux ~D in the gap G is reduced by magnetic flux leakages ~A, ~B and ~C.
Furthermore, no effective measures are taken to prevent the leakage of magnetic flux. Although the periphery of the magnet 55 serves as a magnetic guard against the magnetic flux leakage ~A, the upper and lower corners of the magnet have but a small guarding effect.
Japanese Utility Model Publication 46-8272 discloses a magnetic circuit for a speaker intended to prevent the reduction of the magnetic efficiency. Fig. 22 shows the magnetic circuit disclosed in that publication. The yoke base 53 has a tapered underside 64 which serves to reduce the leakage of the magnetic flux ~A and ~B. However, the tapered yoke base has little effect in increasing the magnetic efficiency at the gap G.
Referring to Fig. 1, the magnetic circuit according to the present invention comprises a yoke 1 having a yoke base 2 and a cylindrical pole 3 having an aperture 3a, an annular magnet 4 mounted on the yoke base 2, and an annular top plate 5. The magnet 4 is secured to the yoke base 2 with adhesive, and the top plate 5 is also secured to the magnet with adhesive.
The magnetic circuit has a compressed spherical periphery. Namely, the yoke base 2 has a convex periphery 2a and the top plate 5 also has a convex periphery 5a, and the periphery 4a of the magnet 4 has an outwardly curved sectional shape.
In the magnetic circuit shown is Fig. 2, a solid pole 6 is formed on the yoke base 2. The yoke base 2 of the third embodiment shown in Fig. 3 has an annular recess 7 on the inside wall thereof, for allowing large axial movement of the voice coil, which is designed to be used for the woofer. A pole piece 8 is mounted on the pole 3.
As shown in Fig. 4, the periphery 4a of the magnet 4 may have a sectional shape defined by straight lines.
Namely, a periphery lla has a triangle sectional shape, and peripheries llb and llc have trapezoidal sectional shapes, respectively. Although the yoke base 2 and the top plate 5 have rectangular sectional shapes, they may have curved sectional shapes as shown in Fig. 1.
" . . ., : ..
, , , ;, ,: , -, :
6 20381~5 Referring to Fig. 5a showing lines of magnetic force generated in the magnetic cir~uit of Fig. 1, most of magnetic lines gl of force generated from the north pole of the magnet 4 enter in the plate 5 and are led to the gap G as magnetic flux g2. Magnetic flux g3 in the gap G is induced in the pole 3 and the yoke base 2 as magnetic flux g4 and led to the south pole of the magnet 4.
Since the periphery of the magnet has an outwardly curved sectional shape, the magnetic flux gl in the magnet 4 is led to the plate 5 along the periphery.
Consequently, magnetic flux density is high in the gap G as indicated by the equal magnetic flux density contours Ll~ L4. On the other hand, leakages ~1 and ~2 of magnetic flux outside the magnet 4, plate 5 and yoke 2 is in low density.
To the contrary, the conventional magnetic circuit has a low magnetic flux density in the gap G and a large leakage ~1 and ~2 of magnetic flux as shown in Fig. 5b.
In a magnetic circuit according to the first embodiment having a magnet radius of 65 mm, a maximum magnetic flux density in the gap G is 1.312 tesla. In the conventional magnetic circuit of Fig. 21 having the same magnetic radius as the first embodiment, a maximum magnetic flux density in the gap G is 1.309 tesla, ,,~
--because of a large amount of the leakage ~A and the leakage ~C of the magnetic flux from the plate 54 to the pole 52.
In addition, the weight of the magnetic circuit of the present invention is reduced by 20 ~ of the weight of the conventional magnetic circuit, since edges of the yoke base 2, magnet 4 and plate 5 are rounded.
Accordingly, expensive magnetic material is reduced in quantity to lower the manufacturing cost thereof.
Furthermore, the magnetic f lux density in the magnet 4 is more equalized, so that reduction of magnetization at low temperature is prevented.
Although each of the periphery of the magnetic circuits of Figs. 1 to 3 has a continuously curved sectional shape, a discontinuous periphery may be employed as shown in Figs. 6, 7a and 7b.
Each of the magnetic circuit of Figs. 1 to 4 is a solid of revolution about a center line ~. However, another magnetic circuit having a square shape or ellipse shape in plan view may be used in embodying the present invention.
Referring to Fig. 8 showing the fifth embodiment, the periphery of a yoke base 17 of yoke 15 has a tapered surface 17a, and a top plate 18 has a tapered surface 18a. A solid pole 16 is formed on the yoke 15.
~ . ~ , , ~ ,.......... . .
~ . ; : : :
.. :
:
8 203~85 Each of the tapered surfaces 17a and 18a is inwardly curved.
Since the outer periphery of the tapered surface 17a (18a), which has a circular shape in section, has a thin thickness, leakage ~B from the circular periphery can be prevented or reduced to a very small amount.
Fig. 9 shows a most preferable tapered surface.
The periphery of each of the yoke base 17 and the top plate has no circular sectional shape. Namely, the inwardly curved surface converges on the surface of a magnet 19.
The magnetic f lux and dimension of the magnetic circuit of Fig. 9 will be described with reference to Fig. 10. In the figure, X1 designates the outer radius of the magnet 19, X2 represents the inner radius, X3 the radius of the pole 16. Thickness t of the yoke base 17 at which inner magnetic flux density Bi becomes constant will be obtained as described hereinafter.
Here it is assumed that all of the magnetic flux in the magnet 19 flows in the yoke 15, hence there is no leakages ~A and ~B.
1. When X2_X_X1, magnetic flux between X and Xl is ~m(X)=ll(X12-X2)Bm Magnetic flux in the tapered portion of the yoke base 17 is 203818~
~i(X)=2lt~X.t.Bi Since ~m=~i, X(X12-X2)Bm=2~-X-t~Bi Therefore t~X)=(X12-X2)Bm/(2X-Bi) When X3<X_X2, magnetic flux between X and Xl is ~m(X)=T~(X12-X22)Bm Magnetic flux in the tapered portion of the yoke base 17 is ~i(X)=2~X.t~Bi Therefore t(X)=(X12-X22)Bm/(2X-Bi) When X=X1, dt(X)/dX=Bm/(2Bi)-(-xl2/X2-1) dt(X)/dt(X=X1)=-Bm/Bi These are the conditions which define the dimensions of the yoke base.
The following is the analysis of these conditions.
When X2~X<X1, t(X)=(cl/X)-c2~X
(cl and c2 are constants) Consequently, the tapered portion of the yoke base becomes an inwardly curved sectional shape.
; When X3SX_X2, t(X)=c3/X (c3 is a constant) `-.
/::
;' ~ :: . : : : . .~ . ` '::
- . .
. .
A
2038~8~
Therefore, in this case also, the tapered portion becomes inwardly curved.
The above values are obtained on the assumption that the leakage of the magnetic flux ~A does not exist. Actually a part of the flux does not pass through the pole 16 because of the leakage ~A.
Therefore, the value of the increasing rate of the thickness t is smaller than the above equations.
However, the conditions for forming an inwardly curved sectional shape do not change. This is confirmed by numerical calculation, for example by the finite element method.
The above theory is also applied to the tapered portion of the plate 18.
Fig. 11 shows a distribution of the magnetic flux in the magnetic circuit of Fig. 9. The same references as Fig. 5a are used. From the figure, it will be understood that a high density of magnetic flux is obtained in the gap G.
Fig. 12 shows magnetic flux densities and weight of prior arts 1 and 2 and the present invention. In the table, Bg represents the averaged magnetic flux density in the gap G, ~g is the magnetic flux in the gap, and ~m is a total magnetic flux in the magnet. It will be seen that the magnetic flux density of the present invention is higher than the prior arts 1 and 2 ,-.
. : :
11 2~3~185 and the magnetic circuit of the present invention islighter than the prior arts in weight.
The magnetic circuit of Fig. 13 has a recess 16a on the underside of the pole 16 in order to reduce the weight thereof.
In the seventh embodiment shown in Fig. 14, an additional recess 16b is formed on the upperside of the pole 16 so as to further reduce the weight. Since each the recesses 16a and 16b has a curved inner surface, leakage of magnetic flux therefrom can be reduced.
The magnetic circuit of Fig. 15 has a perforation 16c in the pole 16.
The magnet 19 of the magnetic circuit shown in Fig. 16 has an outwardly curved sectional shape similar to the first embodiment of Fig. l.
Figs. 17 to 19 show various sectional shapes of the magnet circuit.
While the presently preferred embodiments of the present invention have been shown and described, it is to be understood that this disclosure is for the purpose of illustration and that various changes and modifications may be made without departing from the scope of the invention as set forth in the appended claims.
'` ,.
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: '
An object of the present invention is to provide a magnetic circuit for a speaker which may increase magnetic efficiency, thereby enabling improvement of the tonal quality of the speaker.
Another object of the present invention is to provide a magnetic circuit which can be light in weight and may be manufactured at a low cost.
According to the present invention, there is provided a magnetic circuit for a speaker having a yoke base, a pole formed on the yoke base, an annular magnet mounted on the yoke base, and a top plate mounted on the magnet so as to form a gap between an inside wall thereof and an outer wall of the pole. At least one of the yoke base, pole and top plate has a periphery having a non-linear sectional shape.
The non-linear sectional shape is an outwardly curved sectional shape or an inwardly curved sectional shape.
In one aspect of the invention, the magnet has a periphery having an outwardly curved sectional shape.
- 203~185 The magnet, yoke base and top plate may have peripheries having respectively outwardly curved sectional shapes.
In another aspect, at least one of the yoke base and the top plate has an inwardly curved sectional shape.
The magnet may have a periphery having a sectional shape combining straight lines.
The other objects and features of this invention will become understood from the following description with reference to the accompanying drawings, in which ~ Fig. 1 is a sectional view showing a magnetic ;~ circuit according to a first embodiment of the present invention;
Fig. 2 is a sectional view of a second embodiment;
15Figs. 3 and 4 are sectional views showing third and fourth embodiments;
Fig. 5a is an illustration showing lines of magnetic force generated in the first embodiment;
Fig. 5b is an illustration showing lines of magnetic force generated in the conventional magnetic circuit;
Figs. 6, 7a and 7b are sectional views showing modifications of the sectional shape;
Fig. 8 is a sectional view of a fifth embodiment;
- ~ :
203818~
Fig. 9 is a sectional view showing a modification of the fifth embodiment;
Fig. 10 is a sectional view explaining the effects of tapered portions;
Fig. 11 is an illustration showing lines of magnetic force generated in the magnetic circuit of Fig. 9;
Fig. 12 is a table comparing performance and weight of the magnetic circuit of Fig. 8 with conventional magnetic circuits;
Figs. 13 to 19 are sectional views showing sixth to twelfth embodiments of the present invention;
Fig. 20 is a sectional view showing a conventional cone speaker; and Figs. 21 and 22 are sectional views showing lS sectional shapes of prior art magnetic circuits.
Reference will first be made to Figures 20 - 22, illustrating prior art speakers.
Fig. 20 shows a widely used cone speaker. The speaker comprises a yoke 51 having a yoke base 53 and a cylindrical pole 52 formed on the yoke base 53, an annular top plate 54, and a magnet 55 disposed between the yoke base 53 and the top plate 54. A voice coil 56 is supported by a damper 60 and disposed in a magnetic gap G between the pole 52 and the top plate 54 so as to be moved in the direction shown by arrows a and b. A frame 57 is secured , , ~ , .
;
.
203~18~
to the plate 54, and a diaphragm 59 is provided between an edge 58 of the frame 57 and the voice coil 56. Reference numeral 61 designates a terminal and 62 is a lead.
Referring to Fig. 21, the magnetic circuit is formed by the yoke 51, magnet 55 and plate 54, each of which has a rectangular cross section. Consequently, the magnetic flux ~D in the gap G is reduced by magnetic flux leakages ~A, ~B and ~C.
Furthermore, no effective measures are taken to prevent the leakage of magnetic flux. Although the periphery of the magnet 55 serves as a magnetic guard against the magnetic flux leakage ~A, the upper and lower corners of the magnet have but a small guarding effect.
Japanese Utility Model Publication 46-8272 discloses a magnetic circuit for a speaker intended to prevent the reduction of the magnetic efficiency. Fig. 22 shows the magnetic circuit disclosed in that publication. The yoke base 53 has a tapered underside 64 which serves to reduce the leakage of the magnetic flux ~A and ~B. However, the tapered yoke base has little effect in increasing the magnetic efficiency at the gap G.
Referring to Fig. 1, the magnetic circuit according to the present invention comprises a yoke 1 having a yoke base 2 and a cylindrical pole 3 having an aperture 3a, an annular magnet 4 mounted on the yoke base 2, and an annular top plate 5. The magnet 4 is secured to the yoke base 2 with adhesive, and the top plate 5 is also secured to the magnet with adhesive.
The magnetic circuit has a compressed spherical periphery. Namely, the yoke base 2 has a convex periphery 2a and the top plate 5 also has a convex periphery 5a, and the periphery 4a of the magnet 4 has an outwardly curved sectional shape.
In the magnetic circuit shown is Fig. 2, a solid pole 6 is formed on the yoke base 2. The yoke base 2 of the third embodiment shown in Fig. 3 has an annular recess 7 on the inside wall thereof, for allowing large axial movement of the voice coil, which is designed to be used for the woofer. A pole piece 8 is mounted on the pole 3.
As shown in Fig. 4, the periphery 4a of the magnet 4 may have a sectional shape defined by straight lines.
Namely, a periphery lla has a triangle sectional shape, and peripheries llb and llc have trapezoidal sectional shapes, respectively. Although the yoke base 2 and the top plate 5 have rectangular sectional shapes, they may have curved sectional shapes as shown in Fig. 1.
" . . ., : ..
, , , ;, ,: , -, :
6 20381~5 Referring to Fig. 5a showing lines of magnetic force generated in the magnetic cir~uit of Fig. 1, most of magnetic lines gl of force generated from the north pole of the magnet 4 enter in the plate 5 and are led to the gap G as magnetic flux g2. Magnetic flux g3 in the gap G is induced in the pole 3 and the yoke base 2 as magnetic flux g4 and led to the south pole of the magnet 4.
Since the periphery of the magnet has an outwardly curved sectional shape, the magnetic flux gl in the magnet 4 is led to the plate 5 along the periphery.
Consequently, magnetic flux density is high in the gap G as indicated by the equal magnetic flux density contours Ll~ L4. On the other hand, leakages ~1 and ~2 of magnetic flux outside the magnet 4, plate 5 and yoke 2 is in low density.
To the contrary, the conventional magnetic circuit has a low magnetic flux density in the gap G and a large leakage ~1 and ~2 of magnetic flux as shown in Fig. 5b.
In a magnetic circuit according to the first embodiment having a magnet radius of 65 mm, a maximum magnetic flux density in the gap G is 1.312 tesla. In the conventional magnetic circuit of Fig. 21 having the same magnetic radius as the first embodiment, a maximum magnetic flux density in the gap G is 1.309 tesla, ,,~
--because of a large amount of the leakage ~A and the leakage ~C of the magnetic flux from the plate 54 to the pole 52.
In addition, the weight of the magnetic circuit of the present invention is reduced by 20 ~ of the weight of the conventional magnetic circuit, since edges of the yoke base 2, magnet 4 and plate 5 are rounded.
Accordingly, expensive magnetic material is reduced in quantity to lower the manufacturing cost thereof.
Furthermore, the magnetic f lux density in the magnet 4 is more equalized, so that reduction of magnetization at low temperature is prevented.
Although each of the periphery of the magnetic circuits of Figs. 1 to 3 has a continuously curved sectional shape, a discontinuous periphery may be employed as shown in Figs. 6, 7a and 7b.
Each of the magnetic circuit of Figs. 1 to 4 is a solid of revolution about a center line ~. However, another magnetic circuit having a square shape or ellipse shape in plan view may be used in embodying the present invention.
Referring to Fig. 8 showing the fifth embodiment, the periphery of a yoke base 17 of yoke 15 has a tapered surface 17a, and a top plate 18 has a tapered surface 18a. A solid pole 16 is formed on the yoke 15.
~ . ~ , , ~ ,.......... . .
~ . ; : : :
.. :
:
8 203~85 Each of the tapered surfaces 17a and 18a is inwardly curved.
Since the outer periphery of the tapered surface 17a (18a), which has a circular shape in section, has a thin thickness, leakage ~B from the circular periphery can be prevented or reduced to a very small amount.
Fig. 9 shows a most preferable tapered surface.
The periphery of each of the yoke base 17 and the top plate has no circular sectional shape. Namely, the inwardly curved surface converges on the surface of a magnet 19.
The magnetic f lux and dimension of the magnetic circuit of Fig. 9 will be described with reference to Fig. 10. In the figure, X1 designates the outer radius of the magnet 19, X2 represents the inner radius, X3 the radius of the pole 16. Thickness t of the yoke base 17 at which inner magnetic flux density Bi becomes constant will be obtained as described hereinafter.
Here it is assumed that all of the magnetic flux in the magnet 19 flows in the yoke 15, hence there is no leakages ~A and ~B.
1. When X2_X_X1, magnetic flux between X and Xl is ~m(X)=ll(X12-X2)Bm Magnetic flux in the tapered portion of the yoke base 17 is 203818~
~i(X)=2lt~X.t.Bi Since ~m=~i, X(X12-X2)Bm=2~-X-t~Bi Therefore t~X)=(X12-X2)Bm/(2X-Bi) When X3<X_X2, magnetic flux between X and Xl is ~m(X)=T~(X12-X22)Bm Magnetic flux in the tapered portion of the yoke base 17 is ~i(X)=2~X.t~Bi Therefore t(X)=(X12-X22)Bm/(2X-Bi) When X=X1, dt(X)/dX=Bm/(2Bi)-(-xl2/X2-1) dt(X)/dt(X=X1)=-Bm/Bi These are the conditions which define the dimensions of the yoke base.
The following is the analysis of these conditions.
When X2~X<X1, t(X)=(cl/X)-c2~X
(cl and c2 are constants) Consequently, the tapered portion of the yoke base becomes an inwardly curved sectional shape.
; When X3SX_X2, t(X)=c3/X (c3 is a constant) `-.
/::
;' ~ :: . : : : . .~ . ` '::
- . .
. .
A
2038~8~
Therefore, in this case also, the tapered portion becomes inwardly curved.
The above values are obtained on the assumption that the leakage of the magnetic flux ~A does not exist. Actually a part of the flux does not pass through the pole 16 because of the leakage ~A.
Therefore, the value of the increasing rate of the thickness t is smaller than the above equations.
However, the conditions for forming an inwardly curved sectional shape do not change. This is confirmed by numerical calculation, for example by the finite element method.
The above theory is also applied to the tapered portion of the plate 18.
Fig. 11 shows a distribution of the magnetic flux in the magnetic circuit of Fig. 9. The same references as Fig. 5a are used. From the figure, it will be understood that a high density of magnetic flux is obtained in the gap G.
Fig. 12 shows magnetic flux densities and weight of prior arts 1 and 2 and the present invention. In the table, Bg represents the averaged magnetic flux density in the gap G, ~g is the magnetic flux in the gap, and ~m is a total magnetic flux in the magnet. It will be seen that the magnetic flux density of the present invention is higher than the prior arts 1 and 2 ,-.
. : :
11 2~3~185 and the magnetic circuit of the present invention islighter than the prior arts in weight.
The magnetic circuit of Fig. 13 has a recess 16a on the underside of the pole 16 in order to reduce the weight thereof.
In the seventh embodiment shown in Fig. 14, an additional recess 16b is formed on the upperside of the pole 16 so as to further reduce the weight. Since each the recesses 16a and 16b has a curved inner surface, leakage of magnetic flux therefrom can be reduced.
The magnetic circuit of Fig. 15 has a perforation 16c in the pole 16.
The magnet 19 of the magnetic circuit shown in Fig. 16 has an outwardly curved sectional shape similar to the first embodiment of Fig. l.
Figs. 17 to 19 show various sectional shapes of the magnet circuit.
While the presently preferred embodiments of the present invention have been shown and described, it is to be understood that this disclosure is for the purpose of illustration and that various changes and modifications may be made without departing from the scope of the invention as set forth in the appended claims.
'` ,.
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: '
Claims (12)
1. A magnetic circuit for a speaker having a yoke base, a pole formed on the yoke base, an annular magnet mounted on the yoke base, and a top plate mounted on the magnet so as to form a gap between an inside wall thereof and an outer wall of the magnet, characterized in that;
at least one of the yoke base, magnet and top plate has a periphery having a non-linear sectional shape.
at least one of the yoke base, magnet and top plate has a periphery having a non-linear sectional shape.
2. The magnetic circuit according to claim 1 wherein the non-linear sectional shape is an outwardly curved sectional shape.
3. The magnetic circuit according to claim 1 wherein the non-linear sectional shape is an inwardly curved sectional shape.
4. The magnetic circuit according to claim 1 wherein the non-linear sectional shape is a sectional shape combining straight lines.
5. The magnetic circuit according to claim 2 wherein the magnet has a periphery having an outwardly curved sectional shape.
6. The magnetic circuit according to claim 2 wherein the magnet and one of the yoke base and top plate have peripheries having outwardly curved sectional shapes respectively.
7. The magnetic circuit according to claim 2 wherein the magnet, yoke base and top plate respectively have peripheries having outwardly curved sectional shapes.
8. The magnetic circuit according to claim 3 wherein at least one of the yoke base and the top plate has an inwardly curved sectional shape.
9. The magnetic circuit according to claim 8 wherein a periphery of one of the yoke base and the top plate has a circular sectional shape.
10. The magnetic circuit according to claim 8 wherein the inwardly curved surface converges on a surface of the magnet.
11. The magnetic circuit according to claim 8 wherein the magnet has periphery having an outwardly curved sectional shape.
12. The magnetic circuit according to claim 8 wherein the magnet has a periphery having a sectional shape combining straight lines so as to project outwardly.
Applications Claiming Priority (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19327790A JPH0479700A (en) | 1990-07-20 | 1990-07-20 | Magnetic circuit for loudspeaker |
| JP2-193277 | 1990-07-20 | ||
| JP2280773A JP2987188B2 (en) | 1990-10-19 | 1990-10-19 | Magnetic circuit for speaker |
| JP2-280773 | 1990-10-19 |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA2038185A1 true CA2038185A1 (en) | 1992-01-21 |
Family
ID=26507782
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA002038185A Abandoned CA2038185A1 (en) | 1990-07-20 | 1991-03-13 | Magnetic circuit for a speaker |
Country Status (4)
| Country | Link |
|---|---|
| EP (1) | EP0467016B1 (en) |
| KR (1) | KR920003800A (en) |
| CA (1) | CA2038185A1 (en) |
| DE (1) | DE69127862T2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR20020046897A (en) * | 2000-12-09 | 2002-06-21 | 이형도 | A Magnetic circuit of micro speaker |
| CN109714696A (en) * | 2018-12-07 | 2019-05-03 | 歌尔股份有限公司 | A kind of assembly method of magnetic circuit component |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0224313Y2 (en) * | 1980-08-01 | 1990-07-03 | ||
| JPS6248246A (en) * | 1985-08-27 | 1987-03-02 | Moriyama Kogyo Kk | Rotary machine of permanent magnet |
-
1991
- 1991-03-13 CA CA002038185A patent/CA2038185A1/en not_active Abandoned
- 1991-03-15 DE DE69127862T patent/DE69127862T2/en not_active Revoked
- 1991-03-15 EP EP91104052A patent/EP0467016B1/en not_active Revoked
- 1991-05-16 KR KR1019910007931A patent/KR920003800A/en not_active Application Discontinuation
Also Published As
| Publication number | Publication date |
|---|---|
| KR920003800A (en) | 1992-02-29 |
| EP0467016A3 (en) | 1992-06-17 |
| EP0467016A2 (en) | 1992-01-22 |
| EP0467016B1 (en) | 1997-10-08 |
| DE69127862T2 (en) | 1998-05-28 |
| DE69127862D1 (en) | 1997-11-13 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EEER | Examination request | ||
| FZDE | Dead |