AU486552B2 - Loudspeaker - Google Patents
LoudspeakerInfo
- Publication number
- AU486552B2 AU486552B2 AU70575/74A AU7057574A AU486552B2 AU 486552 B2 AU486552 B2 AU 486552B2 AU 70575/74 A AU70575/74 A AU 70575/74A AU 7057574 A AU7057574 A AU 7057574A AU 486552 B2 AU486552 B2 AU 486552B2
- Authority
- AU
- Australia
- Prior art keywords
- suspension means
- diaphragm
- loudspeaker
- elastic material
- frame
- 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.)
- Expired
Links
Description
70.575 /74 BACKGROUND OF THE INVENTION
Field of the Invention:
This invention relates to a dynamic, cone type loud-
speaker, and more particularly to a loudspeaker with
suspension means for supporting the cone from a frame.
Description of the Prior Art:
In a typical conventional dynamic loudspeaker, there
is found a circular yoke, an annular yoke, an annular
magnet and a central pole fixed on the circular yoke.
The vibration system comprises a cylindrical bobbin, a
voice coil wound around the cylindrical bobbin, a sus-
pension means or a damper suspending the bobbin from a
cone-shaped frame and a cone-shaped diaphragm fixed
adhesively on the upper end of the bobbin. An annular suspension means has its outer edge bonded to the upper
end of the frame with a suitable binder and has its inner
edge bonded to the upper end of the diaphragm by a suitable
binder.
Generally, the suspension means provides an edge for
the cone which has a curved portion with a nearly semi-
circular cross section projecting upward at its center,
which is elastically deformable due to its own elasticity,
whereby the diaphragm can be linearly vibrated in the
vertical direction. The stiffness of the edge has an important effect on the lower frequency characteristic.
The stiffness should be reduced for the lowering of the
lower threshold frequency. For such a purpose, the edge is generally formed of urethane sponge or cotton cloth
impregnated with phenol resin, or of a mixture of nitryl
butadiene rubber, styrene butadien rubber or isobutyl-
2 486. 552
70,575 /74 isoprene rubber with carbonic fine grains.
For satisfactory vibration of the diaphragm, it is
required that the edge be deformable both radially and
peripherally. Moreover, it is necessary that the peri-
pheral deformation be larger than the radial deformation.
An edge formed of cotton cloth has the following dis-
advantages: When the diaphragm is strongly vibrated, the
edge is wrinkled and its internal loss is increased, since
it is little deformed in the peripheral direction. More-
over, sounds are generated from the edge.
An edge formed of the vulcanized mixture of the above-
mentioned rubber with carbonic fine grains has the follow-
ing disadvantages: The thickness of the edge should be
relatively large for the required stiffness. Therefore,
the sound conversion efficiency is lowered with the in-
crease of the weight of the edge.
Generally, the damper is annular and undulated in
shape, and deformable in a radial direction. This prevents
the voice coil from contacting the yoke during vibration.
It supports the diaphragm and the voice coil.
Also, the stiffness of the damper has an important effect on the lower threshold frequency f With a
damper having a large degree of stiffness, sounds cannot
be reproduced with high fidelity, since the damper does
not vibrate accompanied with the diaphragm. For that
reason, the damper is manufactured in such a manner that
the cotton cloth impregnated with phenol resin is formed
under heat into undulation so as to obtain a lower stiff-
ness.
However, the conventional damper cannot be deformed
486.5 52
575/74 in a peripheral direction when the vibration system is operated. Accordingly,the linearity of the deformability
is unsatisfactory under large vibrations. The size and the thickness of the damper are increased for the required stiffness and so the weight of the damper is increased. Accordingly, the internal loss of the damper is decreased. Therefore, the mechanical impedance of the loudspeaker is increased in the lower frequency range. As the result, the sharpnesses of the mechanical resonance and the elec- trical resonance are increased and so.the quality of the reproduced sounds is worsened.
4 486.552
70.57 5/74
The present invention provides a loudspeaker
comprising a diaphragm with a voice coil, a frame surround-
ing said diaphragm, and a suspension means for suspending
said diaphragm from said frame, which is characterized
in that said suspension means is formed of a mixture of'
elastic materi alImpregatded wxh carbo fibers/-ACM
The above, and oth r preferred features and advan-
tages of the invention will be apparent in the following
detailed description of illustrative embodiments thereof
which is to be read in connection with the accompanying
drawings.
Figure 1 is a schematic cross-sectional view of a
4 86,5 52
70,575 /74 loudspeaker of one preferred embodiment of this invention;
Figure 2 is a plan view of a first suspension means in Figure 1;
Figure 3 is an enlarged plan view of a part of the first suspension means shown in Figure 2;
Figure 4 is a cross-sectional view taken along the line IV-IV of Figure 31
Figure 5 is a cross-sectional view of a metal mold employed for the manufacture of the first suspension
means shown on Figure 2;
Figure 6 is a rio view of a second suspension means in Figure 1;
Figure 7 is an enlarged plan view of a part of the second suspension means shown in Figure 6; Figure 8 is a cross-sectional view taken along the line VIII-VIII of Figure 7;
Figure 9 is a'graph showing a frequency-response characteristic; and
Figure 10 is a graph showing a frequency-impedance characteristic.
DESCRIPTION OF THE PREFERRED EMBODIMENTS Referring to Figure 1, the magnetic portion of a loudspeaker 1, according to one embodiment of this invention, comprises a circular yoke 2a, an annular yoke 2b, an annular magnet 3 disposed between the circular yoke 2a and the annular yoke 2b, and a central pole 4 which extends upwardly from the center of the circular yokel:2a and is fixed with respect thereto. A vibration system comprises a bobbin 5 for a voice coil, a voice coil 6 wound around the bobbin 5 and a cone-shaped
6 486, 552
575 /74 diaphragm 9 fixed on the upper end of the bobbin 5. The
first annular suspension means 20 is bonded to the upper
end of a frame 7 and to the upper end of the diaphragm 9,
with a suitable binder. A second annular suspension means,
namely a damper 28 is bonded to the lower end of the dia-
phragm 9 to suspend the diaphragm 9 elastically from the
frame 7. A sound absorber 11 is fixed on the upper face
of the bobbin 5. A cap 12 covers the surface of the
sound absorber 11. A clamping ring 13 is fixed on the
upper end of the edge 20 to prevent the edge 20 from
peeling from the upper end of the frame 7.
The edge or first suspension means 20 will now be
described in detail with reference to Figures 2 to 4.
The first suspension means 20 defines a curved or
ridge-like portion 20a with a nearly semicircular cross
section projecting upward, an inclining portion 20b and
an outer horizontal circumferential portion 20c. The
first suspension means 20 is manufactured in such a
manner that carbon fibers 21 with lengths of 0.3 to 0.8 mm
are mixed into an elastic material such as synthetic
rubber, (for example, nitryl butadiene rubber, styrene
butadiene rubber and isobutyl-isoprene rubber), natural
rubber or synthetic resin (for example, soft foamed-
urethane). The carbon fibers 21 are aligned radially
as diagrammatically shown in Figure 3.
The upper end of the diaphragm 9 is fixed on the
inclined portion 20b of the first suspension means
and the upper end of the frame 7 is fixed to the horizon-
tal circumferential portion 20c of the first suspension
means
7 486.552
70.575 /74 The method for manufacturing the edge 20 will be
described with reference to Figure
1 to 40 aron fibers, with Young's modulus 2 20000 kg/mm diameter 8-C and length 3 to 6 mm, and a
different material, such for example, stearic acid, sulpher,
carbon black, etc., are mixed into solid styrene butadiene
rubber by a mixing mill, where the carbon fibers are cut
needle-like into 0.3 to 0.8 mm. A resulting mixture 22
is put on the center of a metal mold 23, heated up to a
required temperature, for example 150 0 which defines an
annular groove 24 having the same cross section as the
first suspension means 20. Another metal mold 26 is
provided having a mating annular projection 25 of the same
cross section as the annular groove 24. The metal mold
26 is brought over therone metal mold 23, heated up to the
said required temperature. The mixture 22 is put between
the metal molds 23 bnd 26. Accordingly, as the metal
mold 26 is pressed down, the mixture 22 is radially
spread out from the center of the metal mold 23 in the
direction shown by the arrows 27 in Figure 5 and then led
into the annular groove 24, between the metal molds 23
and 26. When the annular projection 25 is fitted into
the annular groove 24, the mixture 22 is vulcanized at 0 a temperature over 140 between the metal molds 23 and 26. Thereafter, the metal molds 23 and 26 are cooled
to solidify the mixture 22. The formed mixture 22 is
drawn out from the metal mold 23. As the result, the
first suspension means 20 is obtained, as shown on Figure
2 and Figure 4.
In the manufacturing process, since the mixture 22
8 4 86.5 52
70575 /74 is spread out directionally, the carbon fibers 21 con- tained in the mixture 22 are displaced directionally.
Therefore, the carbon fibers 21 with the lengths of 0.3
to 0.8 mm are radially dispersed in the direction of the
diameter of the first suspension means 20 (Figure 3).
With such a dispersion of the carbon fibers 21, the
deformability of the first suspension means 20 is im-
proved on the peripheral direction. There is no possibility that the first suspension means 20 will be wrinkled. The specific .weight of the first suspension means 20 is small
and the stiffness of the first suspension means 20 is
large, since it is manufactured in a vulcanizing process
of the mixture containing carbon fibers. Consequently,
the thickness of the curved portion 20a of the first
suspension means 20 can be reduced to the minimum for the
required stiffness and so the total weight of the first
suspension means 26 can be reduced.
According tbXie ivention, the second suspension
means 28 is also formed of the mixture of elastic
material with the carbonfibers.
Referring to Figure 6 to Figure 8, a second sus-
pension means 28 has a plurality of concentric curved
portions 28a with a semicircular cross section projecting
upward. It also has concentric curved portions 28b with
a semicircular cross section projecting downward, an
inner edge portion.28c with a U-shaped cross section
projecting downward, and a horizontal circumferential
portion 28d. The second suspension means 28 is formed of a mixture of the same elastic material as the first sus-
pension means 20 with the carbon fibers. As shown in
9 486,5 52
70,575 /74 .Figure 7, carbon fibers 31 with lengths of 0.3 to 0.8 mm
are radially aligned in the direction of the diameter of
the second suspension means 28. It is preferable that the Young's modulus of the carbon fiber 31 be more than
20000 kg/mm 22 and that the diameter of the carbon fiber 31
is smaller than the Jength of the carbon fiber, for example,
about 1 to 40c, aron fibers 31 are contained in the second suspension means 28.
In the loudspeaker 1, the inner end portion 28c is
bonded to the bobbin 5 and the horizontal circumferential
portion 28d is bonded to the frame 7. The second sus- pension means 28 can be manufactured in the same manner
as the first suspension means The deformability of the second suspension means 28 is higher in the peripheral direction than in the radial
direction, since the carbon fibers 31 are radially dis-
persed in the second suspension means 28. When a mixture of styrene butadiene rubber with the carbon fibers is
vulcanized for the manufacture of the second suspension
means 28, a small specific weight and a large stiffness
can be obtained for the second suspension means 28.
Consequently, the thickness of the second suspension
means 28 can be reduced to a minimum for the required
stiffness and hence the total weight of the second sus- pension means 28 can be reduced.
Figure 9 shows the frequency-response characteristics
of cone-type dynamic speakers using the first suspension
means 20 according to this invention and the conventional
first suspension means formed of cotton cloth.
In a curve for a speaker using cotton cloth, the
10 48 6,5 52
70.575 /74 response fluctuates in frequencies above 500.-Hz, where
peaks or dips occur. Therefore, the quality of tone is
deteriorated. 4w In aqlj for a speaker using the
first suspension means according to this invention, no
peak or dip occurs in the higher frequencies. The re-
sponse lowers abruptly in the frequencies above a higher threshold frequency 1500 Hz. Therefore, high quality of
tone can be obtained. The reasons are that the suspension
means according to this invention is not wrinkled in the
vibration and no sound is generated from the suspension,
means, and that the sound conversion efficiency is im-
proved due to the reduction of the weight.
Figure 10 shows frequency-impedance characteristics.
Curve is for a conventional loudspeaker using a damper
formed of cotton cloth impregnated with phenol resin,
where the resonant frequency f is 78 Hz, the maximum
impedance Z o 100f and the minimum impedance RE 6Jl. The
sharpness QM of the mechanical resonance is represented fo by an equation f2- 0M where fl and f 2 are Q r2 1 Z 1 frequencies for an impedance Z From a.curve
fl 67 Hz and f2 88 Hz are apparent. Therefore,
3.71 for the curve The sharpness 88-67 Q of the electrical resonance is represented by an RE 6 equation Qo QM x Qo 3.71 x 0.223 0o for the curve b.
The values of.Q M and Qo are large for the conventional is damper, as above described and so the damping effect low for the lower frequency range. Therefore, it will be
understood that the tone quality is inferior. The frequency characteristic is remarkably improved
11 486,552
70,575 /74 by using the second suspension means 28 according to this
invention, as shown by a curve on Figure 10, where the
resonant frequency.f is 84 Hz, the maximum impedance
Zo 242 and the minimum impedance RE 6AI. The frequencies 84 f and f2 are 50 Hz and 143 Hz for an impedance Z
Therefore, the sharpness QM of the mechanical resonance
is 84 0.9. And the sharpness Q of the 143-50 6 electrical resonance is 0.9 x 0.18. 24 +6 It will be understood that QM and Qo can be remark-
ably lowered by the second suspension means according to
this invention, compared with the conventional suspension
means.
Although an illustrative embodiment of this invention
has been described in detail herein with reference to the
accompanying drawings, it is to be understood that the invention is not limited to that precise embodiment, and
that various changes and modifications may be effected
therein by one skilled in the art without departing from
the scope or spirit of this invention, as defined in the
appended claims. For example, the shape and the size of
the first and the second suspension means may be varied.
Moreover, this invention can be applied to a double cone-
type loudspeaker or a dome-type loudspeaker, too.
486,552
Claims (1)
- 70.575 /74 THE CLAIMS DEFINING THE INVENTION ARE AS FOLLOWS:1. A loudspeaker comprising a diaphragm with a voicecoil, a frame surrounding said diaphragm, and a suspensionmeans for suspending said diaphragm from said frame, whichis characterized in that said suspension means is formedof a mixture of elastic material impregnated with carbonfibers,, a ;1 dU1 A 2. A loudspeaker according to claim 1, wherein saidelastic material is rubber.3. A loudspeaker according to claim 2, wherein saidsuspension means is disposed between the upper portion ofsaid diaphragm and said frame and it defines an intermedi-ate portion having an arcuate cross section.4. A loudspeaker according to claim 2, wherein saidsuspension means is disposed between the lower portionof said diaphragm and said frame and it defines an inter-mediate portion having a wave-like cross section. A loudspeaker according to claim 1, whereinsaid ela tic material is ak6. A loudspeaker comprising a cone-shaped diaphragmwith a voice coil, a frame surrounding said cone-shapeddiaphragm, a first suspension means for suspending the upper part of said diaphragm from said frame, and asecond suspension.means for suspending the lower part ofsaid diaphragm from said frame, which is characterized inthat at least one of said suspension is being formed ofa mixture of elastic material impregnated with carbonam fiber a dad2m,4 0113 4 86.5 5270.575/74 7. A loudspeaker according to claim 6, wherein' saidelastic material is rubber.8. A loudspeaker according to claim 6, wherein theother suspension means is also formed of a mixture of elasticmaterial with carbon fibers.9. A loudspeaker according to claim 8, wherein saidelastic material is rubber and said carbon fibers are needle-like and are radially aligned in the material of said firstand said second suspension means.A loudspeaker according to any one of claims 1to 5 wherein said mixture of elastic material impregnatedwith carbon fibers is 1 to 40% by weight carbon fibers.11. A loudspeaker according to any one of claims6 to 9 wherein said mixture of elastic material impregnatedwith carbon fiber is 1 to 40% by weight carbon fibers.12. Loudspeaker substantially as hereinbeforedescribed with reference' to the accompanying drawings.DATED this 4th day of July, 1977.SONY CORPORATIONBy its Patent Attorneys:CLEMENT HACK CO.Fellows Institute of Patent Attorneys of Australia.14 48 6,.552
Applications Claiming Priority (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1973078632U JPS5351154Y2 (en) | 1973-07-02 | 1973-07-02 | |
| JPJP78632/73 | 1973-07-02 | ||
| JPJP135591/7 | 1973-11-24 | ||
| JP13559173U JPS5432905Y2 (en) | 1973-11-24 | 1973-11-24 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| AU7057574A AU7057574A (en) | 1976-01-08 |
| AU486552B2 true AU486552B2 (en) | 1976-01-08 |
Family
ID=
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| AU631866B2 (en) * | 1989-06-01 | 1992-12-10 | Odyl Group Limited | Loudspeaker |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| AU631866B2 (en) * | 1989-06-01 | 1992-12-10 | Odyl Group Limited | Loudspeaker |
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