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(11) | EP 0 456 416 A2 |
| (12) | EUROPEAN PATENT APPLICATION |
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| (54) | Loudspeaker system |
| (57) A dip-free plane flat pressure level-frequency characteristic is realized by a cascade
bass-reflex loudspeaker system provided with a port-containing partition or partitions
in a speaker cabinet to divide a space inside thereof into two internal acoustically
connected spaces by establishing in either internal space a Helmholtz resonator possessing
the same resonant frequency as a second antiresonant frequency to absorb a negative-phase
sound radiated from the port to the outside of the cabinet, thereby eliminating a
dip in the sound pressure-level frequency characteristic due to the second antiresonance
unique to a cascade bass-reflex loudspeaker system. |
[0001] This invention relates to a loudspeaker system which is small but can reproduce a powerful sound of deep-low tone.
[0002] One of the conventional small loudspeaker systems which can reproduce a sound of deep-low tone has been a cascade bass-reflex system (as disclosed in the Japanese Patent Publication No. 1-254097). Fig. 6 shows a cross section of this conventional cascade bass-reflex loudspeaker system. In Fig. 6, 1 is a cabinet of a loudspeaker system, 2 is a speaker unit, 3 is a partition which divides the internal space of the aforesaid cabinet 1 into two spaces, 4 is the first space divided by the aforesaid partition 3, 5 is a second space, 6 is a first port installed on the aforesaid partition 3, and 7 is a second port installed on the back of the aforesaid cabinet 1.
[0003] Fig. 7 is an equivalent circuit of the loud speaker system shown in Fig. 6. In Fig. 7, Z represents an impedance comprising a mass attributable to the speaker unit 2, a compliance, and a resistance, C1 does a compliance at the first space 4, P1 does a mass at the first port 6, C2 does a compliance at the second space 5, and P2 does a mass at the second port 7.
[0004] In the loudspeaker system constructed as above, the first space 4 and port 6 and the second space 5 and port 7, namely, two compliances and two masses additionally provide a system of two degrees of freedom possessing two antiresonant frequencies f1 and f2. Fig. 8 shows that this gives a favorable sound pressure level-frequency characteristic in the frequency ranges around f1 and from f1 to f2 by equalizing the phases of the sound radiated from the diaphragm of the speaker unit and the sound radiated from the second port 7 as in the case with a simple bass-reflex-type loudspeaker system.
[0005] A problem is, however, that, around the second antiresonant frequency f2, the phase of the sound radiated from the second port 7 is inverted again with increasing level of sound to cause a large dip in the frequency response around f2 due to the interference with the sound radiated from the aforesaid diaphragm. This type of system can, therefore, be used as a super woofer system dedicated for the reproduction of deep-low tone, but is hardly applicable as a loudspeaker system to reproduce the entire frequency range.
[0006] An object of this invention is to realize a small and deep-low tone-reproducible loudspeaker system for the reproduction of the entire frequency range by eliminating the above-mentioned dip in the sound pressure level-frequency characteristic.
[0007] To attain the above object, a loudspeaker system of this invention is a cascade bass-reflex loudspeaker system which is additionally provided with a second partition on which at least one hole or port is further installed to construct a third space.
[0008] The sizes of the aforesaid third space and hole or port are adjusted so that the resonant frequency of a Helmholtz resonator composed of the aforesaid third space and a hole or port installed on the aforesaid second partition may coincide with the above-mentioned frequency f2. This allows the aforesaid Helmholtz resonator to absorb the second antiresonance at the frequency around f2 attributable to the cascade bass-reflex system, thereby substantially improving the large dip in the sound pressure level-frequency characteristic around f2.
[0009] Fig. 1 shows a cross section of a loudspeaker system in the first embodiment of this invention.
[0012] Fig. 4 shows a cross section of a loudspeaker system in the second embodiment of this invention.
[0013] Fig. 5 shows a cross section of a loudspeaker system in the third embodiment of this invention.
[0017] A loudspeaker system in the first embodiment of this invention is explained below with reference to the drawings.
[0018] Fig. 1 shows a cross section of a loudspeaker system in the first embodiment of this invention, Fig. 2 does an equivalent circuit of the system, and Fig. 3 does a specific example of the sound pressure level-frequency characteristic.
[0019] In Fig. 1, a cabinet 1, a speaker unit 2, a partition 3, a first space 4, a second space 5, a first port 6, and a second port 7 are the same as each of those in Fig. 6. 8 is a second partition provided within the second space 5, 9 is a third space constructed by the second partition 8, and 10 is a hole installed on the second partition to compose a Helmholtz resonator with the third space.
[0020] In Fig. 2, Z represents an impedance comprising a mass attributable to the speaker unit 2, a compliance, and a resistance, C1 does a compliance at the first space 4, P1 does a mass at the first port 6, C2 does a compliance at the second space 5, P2 does a mass at the second port 7, C3 does a compliance at the third space 9, and P3 does a mass at the hole 10.
[0021] The function of the loudspeaker system constructed as above is explained below with reference to Fig. 1, Fig. 2, and Fig. 3.
[0022] As mentioned in an example of a conventional system, a simple cascade bass-reflex loudspeaker system is additionally provided with a system of two degrees of freedom possessing two antiresonant frequencies f1 and f2 by the first space 4 and port 6 and the second space 5 and port 7 in Fig. 1, namely, two compliances C1 & C2 and two masses P1 and P2 in Fig. 2. As a result, around the second antiresonant frequency f2, the phase of the sound radiated from the second port 7 is inverted again with increasing level of sound to cause a large dip in the frequency response around f2 due to the interference with the sound radiated from the aforesaid diaphragm. Here, if the volume of the aforesaid third space 9 and/or the size of the hole 10 is adjusted so that the resonant frequency of a Helmholtz resonator composed of the third space 9 and the hole 10 may be almost the same as the aforesaid second antiresonant frequency f2, the second antiresonance is absorbed by the resonance of a Helmholtz resonator composed of P3 and C3 in Fig. 2. This reduces the vibration of air within the second port, thereby substantially improving the dip in the sound pressure level-frequency characteristic around f2 as shown in Fig. 3.
[0023] According to the above embodiment, a dip in the sound pressure level-frequency characteristic around the second antiresonant frequency can be substantially improved for better reproduction quality by providing a cascade bass-reflex-type loudspeaker system with a third space and a third hole and, then, adjusting the volume of the aforesaid third space and the size of the third hole so that the resonant frequency of a Helmholtz resonator composed of the above space and hole provided may be almost the same as the second antiresonant frequency f2.
[0025] Fig. 4 shows a cross section of a loudspeaker system in the second embodiment of this invention.
[0026] Fig. 4 is different from Fig. 1 in that a third port 11 in place of the hole 10 is installed on the second partition 8. Even such a structure allows a Helmholtz resonator composed of the third space 9 and the third port 11 to function in a similar manner to that in the first embodiment, thereby improving the dip in the sound pressure level-frequency characteristic around the second antiresonant frequency f2. Moreover, the resonant frequency of a Helmholtz resonator can be easily established around f2 simply by adjusting the length of the third port 11.
[0028] Fig. 5 shows a cross section of a loudspeaker system in the third embodiment of this invention.
[0029] Fig. 5 is different from Fig. 4 in that a port wall 12 composing a second port 7 is so structured that the cross-sectional area of the aforesaid port may increase gradually toward outside the cabinet 1. Such a structure allows the flow of air to be kept smooth within the port at the time of resonance in a lower range of frequency in particular, thereby reducing an acoustic noise due to the wind hissing through the port.
[0030] More than one holes or ports may be installed on the second partition in the above first, second, and third embodiments. More than one third spaces may also be constructed by providing more than one second partitions. Furthermore, the second partition may be provided in other manners than that to divide the space within the cabinet sideways such as by dividing it vertically.
1. A phase reversing loudspeaker system comprising a cabinet, a speaker unit attached
to the cabinet, and a port installed on a side of the cabinet, wherein at least one
partition is provided within said cabinet to divide a space therein into a space containing
said port and a space not containing said port, a second port is installed on said
partition, a second partition is further provided to construct a tightly closed space
in either the space containing said port or the space not containing said port, and
a hole is installecd on said scond partition.
2. A loudspeaker system according to Claim 1, wherein a third port is installed in place
of said hole.
3. A loudspeaker system according to Claim 1, wherein a cross-sectional area of said
port gradually increases from a central part thereof to an opening end of the port.