Electroacoustic driving circuit

Abstract: A driving apparatus for electrically driving a vibrator constituting an acoustic apparatus, wherein the output impedance of the driving apparatus is negative at at least one frequency associated with the output sound pressure of the acoustic apparatus among resonance frequencies when the acoustic apparatus is viewed from a terminal for driving the vibrator, and the ratio of the output impedance to the internal impedance inherent in the vibrator never becomes constant over all the acoustic reproduction range of the acoustic apparatus. Then, it is possible to eliminate mutual dependency between resonance systems having the resonance frequencies, design of the resonance systems become easy, and improved performance of sound radiation can be expected.

Description: Driving Apparatus BACKGROUND OF THE INVENTION : The present invention relates to a system comprising a driving apparatus and a vibrator a set forth in the preamble of claim 1. (Description of the Prior Art) Various speaker systems are known as a conventional acoustic apparatus. As a driving apparatus for driving a speaker unit constituting such a speaker system, a power amplifier whose output impedance is essentially 0 is used. Figs. 41A and 41B are respectively a perspective view and a sectional view showing an arrangement of a bass-reflex type speaker system as one of conventional speaker systems. In the speaker system shown in Figs. 41A and 41B, a hole is formed in the front surface of a cabinet 1, and a vibrator (speaker unit) 4 consisting of a diaphragm 2 and a dynamic electro-acoustic transducer 3 is mounted in the hole. A resonance port 8 having an opening 6 and a sound path 7 is arranged below the vibrator 4. The cabinet 1 and the port 8 constitute a Helmholtz resonator. Fig. 42 shows a simplified electrically equivalent circuit when the bass-reflex speaker system shown in Figs. 41A and 41B is driven at a constant voltage by a power amplifier whose output impedance is 0. In Fig. 42, reference symbol E VC denotes an output voltage of a constant voltage source as a power amplifier; R VC , a voice coil resistance of the speaker unit 4; L O and C O , an equivalent capacitance (or an equivalent mass) and an equivalent inductance (or a reciprocal number of an equivalent stiffness) of a motional impedance generated when a voice coil of the speaker unit 4 is moved; L C , an equivalent inductance (or a reciprocal number of an equivalent stiffness) of the cabinet 1; and C P , an equivalent capacitance (or an equivalent mass) of the port 8. Fig. 43 shows electrical impedance-frequency characteristics of the circuit shown in Fig. 42. In Fig. 43, reference symbol f₁ denotes a resonance frequency of a first resonance system (to be referred to as a unit resonance system hereinafter) essentially formed by the motional impedances L O and C O of the speaker unit 4 and the equivalent stiffness 1/L C of the cabinet 1; f₂, a resonance frequency of a second resonance system (to be referred to as a port resonance system hereinafter) formed by the equivalent mass C P of the port 8 and the equivalent stiffness 1/L C of the cabinet 1; and f₃, a resonance frequency of a third resonance system essentially formed by the motional impedances L O and C O of the speaker unit 4 and the equivalent mass C P of the port 8. Of these resonance frequencies, the frequency f₃ is not associated with a sound pressure. However, the resonance frequencies f₁ and f₂ directly influence a sound pressure. A Q value Q₁ of the unit resonance system at the resonance frequency f₁ and a Q value Q₂ of the port resonance system at the resonance frequency f₂ largely influence frequency characteristics and sound quality of an output sound pressure. When the bass-reflex speaker system is driven at a constant voltage, if the resonance frequency f₂ of the port resonance system is decreased, the Q value Q₁ of the unit resonance system is increased, and the Q value Q₂ of the port resonance system is decreased. In this manner, the resonance frequencies and Q values have mutual dependencies. For this reason, in order to obtain flat frequency characteristics of an output sound pressure, the unit and port resonance systems must be accurately matched with each other, such that the Q value Q₁ of the unit resonance system is set to be Q₁ = √3, the resonance frequency f₂ of the port resonance system is set to be f₂ = f₁/ √2, and so on, thus restricting a design margin. If the cabinet is rendered compact, the equivalent stiffness 1/L C of the cabinet is increased, and the equivalent inductance L C is decreased. As a result, the Q value Q₁ is increased, and the Q value Q₂ is decreased. For this reason, if a conventional constant voltage driving method is employed without any modification, a normal operation of the bass-reflex speaker system is difficult to achieve. Therefore, it is difficult to make the cabinet of the bass-reflex speaker system compact without impairing frequency characteristics of an output sound pressure and sound quality. Fig. 44 shows a negative impedance generating circuit for which an application is filed as U.S.P. No. 07/286,869 by the present applicant. When the negative impedance generating circuit in Fig. 44 is used as a driving apparatus for the equivalent circuit shown in Fig. 42 and an output impedance is caused to include a negative resistance -R O , the voice coil resistance R VC is reduced or invalidated. Thus, the value Q₁ can be decreased and the value Q₂ can be increased as compared to a case wherein the speaker system is driven at a constant voltage by the power amplifier whose output impedance is 0. Thus, the bass-reflex speaker system can be effectively rendered compact. However, in this case, if the negative resistance -R O is constant, since the values Q₁ and Q₂ cannot be independently set, the speaker unit or the cabinet suffers from a certain limitation when the values Q₁ and Q₂ are set to be desired values. Fig. 45 shows a second example of a conventional speaker system. This acoustic apparatus is the same as a speaker system with a port disclosed in Japanese Patent Laid-Open (Kokai) Sho No. 60-98793. An internal space of a known cabinet 21 having a rectangular section is divided into two chambers 21a and 21b by a partition wall 22. Opening ports 23a and 23b are respectively provided to the outer walls of the chambers 21a and 21b. The chamber 21a and the opening port 23a, and the chamber 21b and the opening port 23b respectively form two Helmholtz resonators. The resonance frequencies of the respective Helmholtz resonators are set to be f₄ and f₂ (f₄ < f₂). An opening 22a is formed in the partition wall 22. A vibrator (dynamic speaker unit) 25 is mounted in the opening 22a. A diaphragm 26 of the vibrator 25 is mounted to close the opening 22a, the front surface of the diaphragm 26 faces the chamber 21a, and its rear surface faces the chamber 21b. Fig. 46 shows an electrically equivalent circuit when the vibrator 25 of the apparatus shown in Fig. 45 is driven at a constant voltage. In Fig. 46, a parallel resonance circuit Z₁ is formed by the equivalent motional impedance of the vibrator 25. In this circuit, reference symbol r O denotes an equivalent resistance of a vibration system; L O , an equivalent inductance (or a reciprocal number of an equivalent stiffness) of the vibration system; and C O , an equivalent capacitance (or an equivalent mass) of the vibration system. A series resonance circuit Z₄ is formed by the equivalent motional impedance of the first Helmholtz resonator constituted by the chamber 21a and the opening port 23a. In this circuit, reference symbol r 1a denotes an equivalent resistance of the chamber 21a as a cavity of the resonator; L 1a , an equivalent inductance (or a reciprocal number of an equivalent stiffness) of this cavity; r 1p , an equivalent resistance of the opening port 23a; and C 1p , an equivalent capacitance (or an equivalent mass) of the opening port 23a. A series resonance circuit Z₂ is formed by the equivalent motional impedance of the second Helmholtz resonator constituted by the chamber 21b and the opening port 23b. In this circuit, reference symbol r 2a denotes an equivalent resistance of the chamber 21b as a cavity of the resonator; L 2a , an equivalent inductance (or a reciprocal number of an equivalent stiffness) of this cavity; r 2p , an equivalent resistance of the opening port 23b; and C 2p , an equivalent capacitance (or an equivalent mass) of the opening port 23b. In Fig. 46, reference symbol Z VC denotes an internal impedance of the vibrator 25. When the vibrator 25 is a dynamic direct radiation speaker, the internal impedance mainly serves as the resistance R VC of the voice coil, and includes a slight inductance. Reference symbol E VC denotes a constant voltage source as a driving source whose output impedance is 0. Note that the equivalent resistances r 1a , r 1p , r 2a , and r 2p have small values which can be ignored as compared to the resistance R VC of the voice coil. Fig. 47 shows electrical impedance characteristics of the system shown in Fig. 45. In the system shown in Fig. 45, five resonance points f₁ to f₅ are generated by one parallel resonance circuit Z₁ and two series resonance circuits Z₂ and Z₄. Of these resonance points f₁ to f₅, the resonance frequency f₂ by the series resonance circuit Z₂ and the resonance frequency f₄ by the series resonance circuit Z₄ are mainly associated with the output sound pressure. In the speaker system shown in Fig. 45, it is ideal that the output sound pressures from the opening ports 23a and 23b become equal to each other at the frequencies f₂ and f₄, as indicated by solid curves in Fig. 48, and are mixed to generate a flat total sound pressure between the frequencies f₂ and f₄, as indicated by a dotted line in Fig. 48. However, in order to achieve this, Q values must be set to be appropriate values. For example, a Q value Q₄ at the frequency f₄ must be set to be higher than a Q value Q₂ at the frequency f₂. In the conventional constant voltage driving method, a damping resistance determining Q values at the frequencies f₂ and f₄ is commonly R VC . Therefore, in order to adjust these Q values to appropriate values, the volumes (L 1a and L 2a ) of the chambers 21a and 21b and the masses (C 1p and C 2p ) in the ports can only be adjusted. The speaker system with the arrangement shown in Fig. 45 (to be referred to as a double bass-reflex system hereinafter) is originally adopted to efficiently reproduce a narrow band as compared to normal speaker systems, and achieves this by utilizing two resonance states. Note that f₂ = 80 Hz and f₄ = 40 HZ, and a sub-woofer having flat characteristics in a frequency range of 40 Hz to 80 Hz is assumed. An average energy spectrum of a music is attenuated at two sides to have 200 Hz as the center, as shown in Fig. 49. Thus, in the energy spectrum of a music signal applied to this sub-woofer, a component E(f₂) of the frequency f₂ is generally larger than a component E(f₄) of the frequency f₄. In order to achieve high efficiency, a resonance at the frequency f₂ or higher must be valid. An acoustic resonance tends to have a high Q value at a high frequency rather than a low frequency if a volume remains the same, and a sound pressure is proportional to an acceleration of an air vibration. Therefore, since E(f₂) > E(f₄), the output sound pressure at the frequency f₂ becomes higher than that at the frequency f₄ if the resonance Q value is left unchanged. Therefore, it is easier to validate a resonance at the frequency f₂ than at the frequency f₄, and is preferable in terms of efficiency. However, the fact that the sound pressure at the frequency f₄ and the output sound pressure at the frequency f₂ are almost equal to each other and a band from f₂ to f₄ is almost flat is an original condition for the speaker system. Therefore, if the resonance at only the frequency f₂ is valid, the original condition for the speaker system cannot be satisfied, and flat frequency characteristics cannot be obtained. In order to obtain flat frequency characteristics, unless a resonance at the frequency f₄ is performed under a more effective condition than that at the frequency f₂, the sound pressure at the frequency f₄ which tends to be low is decreased. For these reasons, in an actual double bass-reflex system, the sound pressure at the frequency f₄ is increased by establishing (the volume of the cavity 21a) >> (the volume of the cavity 21b). The volume of the cavity 21a and the dimensions of the opening port 23a are designed to have a relatively small Q value at the frequency f₂ so that the sound pressure at the frequency f₂ matches with that at the frequency f₄. This is to satisfy a frequency characteristic condition which is the prime importance as the performance of the speaker system by all means. Of course, such a speaker system can have improved efficiency as compared to a speaker system with no port. However, since the sound pressure by the resonance at the frequency f₂ is caused to match with that at the frequency f₄, efficiency at the frequency f₂ is inevitably decreased. The dimensions of the speaker system are almost determined by a design not for the frequency f₂ but for the frequency f₄. Therefore, in view of energy, the dimensions of the system are determined on the basis of the frequency f₄ at which an energy less than that at the frequency f₂ is applied, and the efficiency at the frequency f₂ must be suppressed to match with the sound pressure at the frequency f₄. In the acoustic apparatus shown in Fig. 45 for driving the double bass-reflex speaker system at a constant voltage, since the dimensions of the cabinet are related to the Q values at the resonance frequencies f₂ and f₄, a design margin is small, and it is difficult to make the cabinet compact. Fig. 50 shows an electrically equivalent circuit when a dynamic speaker unit is mounted on an infinite baffle and is driven at a constant voltage by a power amplifier whose output impedance is 0. In Fig. 50, reference symbol E VC denotes a constant voltage source as the power amplifier and its output voltage; and R VC and L VC , a resistance and an inductance of a voice coil of the speaker unit, respectively. Reference symbols L O and C O denote an equivalent capacitance and inductance of a motional impedance generated when the voice coil of the speaker unit is moved; and R O , a mechanical damping resistance. In general, R O >> R VC . R VC and L VC are an electrical resistance and inductance of the voice coil itself, and are non-motional impedances. The non-motional impedance Z VC is given by: Z VC = R VC + jωL VC A motional impedance Z M is given by: Z M = jωL O R O 1 - ω 2 L O C O R O + jωL O where ω is the angular frequency. If the frequency is represented by f , ω = 2πf. Fig. 51 shows electrical impedance-frequency characteristics of the circuit shown in Fig. 50. In Fig. 50, an increase in impedance in a high-frequency range is caused by the inductance L VC of the voice coil. As described above, the inductance L VC is an electrical inductance of the voice coil itself, and is not a motional impedance. Therefore, when the voice coil is placed in a magnetic circuit formed by a magnetic member and is moved therein in response to a signal, the inductance is modulated by this signal. In particular, when a high-frequency signal is input simultaneously with a low-frequency signal having a large amplitude, the inductance L VC is largely varied by the low-frequency signal, and a current of the high-frequency signal is modulated to generate a so-called IM distortion (intermodulation distortion). A frequency f O is a resonance frequency caused by the motional impedance Z M , and is given by: f O = 1 2π L O C O When the negative impedance generating circuit shown in Fig. 44 is used as the driving apparatus E VC in the equivalent circuit shown in Fig. 50 and the circuit is driven while the output impedance is caused to include the negative resistance -R O (to be referred to as negative-resistance driving hereinafter), the voice coil resistance R VC is equivalently reduced by the negative resistance -R O . In the dynamic speaker unit as shown in the equivalent circuit of Fig. 50, the motional impedance Z M in a low-frequency range near the resonance frequency f O is very large, and the impedance jωL VC of the inductance L VC is very small. For this reason, the impedance jωL VC can be ignored with respect to the motional impedance Z M . If R VC - R O = 0, the output voltage of the constant voltage source E VC is substantially directly applied to the vibration system (motional impedance Z M ). Therefore, the Q value of the parallel resonance circuit of L O and C O constituting the vibration system becomes 0, and the operation of the vibration system becomes a constant-speed operation, thereby increasing a driving force and a damping force. Note that if R VC - R O > 0, since the resistance R VC is equivalently decreased, an intermediate state between a case wherein the speaker unit is driven at a constant voltage and a case wherein the vibration system is operated at a constant speed while R VC - R O = 0 can be established. The driving force and damping force of the vibration system can be increased as compared to constant-voltage driving. However, at a frequency in a high-frequency range separated from the resonance frequency f O , the impedance jωL VC of the inductance L VC is increased, and the impedance 1/jωC O of the equivalent capacitance C O is decreased so that the motional impedance Z M is decreased. Thus, the driving current is determined by the non-motional impedance Z VC consisting of the resistance R VC of the voice coil and the inductance L VC . For this reason, when the voice coil resistance R VC is decreased by the negative resistance driving, a driving current in a high-frequency range tends to be influenced by the voice coil inductance L VC . Therefore, an adverse influence on distortion characteristics of the speaker unit due to the inductance L VC is enhanced as compared to the normal constant-voltage driving method. In practice, the above-mentioned infinite baffle is not used, and the speaker unit is generally mounted on a cabinet. When the speaker unit is mounted on a closed baffle (cabinet), the motional impedance Z M is equivalently connected in parallel with an equivalent inductance L C of the closed cabinet. A resonance frequency f OC and a motional impedance Z MC in such a practical use state are respectively given by: f OC = 1 2π · L O + L C C O L O L C Z MC = 1 1/Z M + 1/L C When such a closed baffle is used, if the above-mentioned f O is replaced with f OC and Z M is replaced with Z MC , the above description made for a case wherein the infinite baffle is used can be applied. The bass-reflex speaker system shown in Fig. 41 in which the speaker unit is mounted on the cabinet having the resonance port, causes three resonance frequencies, i.e., the first resonance frequency f₁ by a parallel resonance of the equivalent inductance L C of the cabinet and the motional impedance Z M (L O and C O ), the second resonance frequency f₂ by a series resonance of the equivalent capacitance C P of the resonance port and the equivalent inductance L C of the cabinet, and the third resonance frequency f₃ by a parallel resonance of the motional impedance Z M and the equivalent capacitance C P of the resonance port, as described above. Of these resonance frequencies, the resonance frequency f₁ directly influences a sound pressure, and Q values at the resonance frequencies f₁ and f₂ largely influence frequency characteristics of the output sound pressure and sound quality. In this bass-reflex speaker system, when negative resistance driving is performed, the Q value at the frequency f₁ is decreased and the Q value at the frequency f₂ is increased as compared to those in the constant-voltage driving. Thus, the damping force and driving force at the frequency f₁ are increased, and a matching state between the speaker unit and the cabinet can be adjusted by the negative resistance -R O , thus increasing a design margin and allowing lower bass sound reproduction. However, at a frequency in a high-frequency range separated from these resonance frequencies f₁ and f₂, a driving current tends to be influenced by the inductance L VC . Therefore, an adverse influence on acoustic characteristics, e.g., distortion characteristics caused by the inductance L VC is promoted as compared to the normal constant-voltage driving method. In Journal of the Audio Engineering, Vol. 19, Nos. 5 and 6, "Loudspeakers in Vented Boxes, Part I and II" discloses a speaker system of the vented box type wherein a negative impedance driving is excerted in a speaker unit without driving the speaker unit by the amplifier with negative impedance in lower and positive impedance in higher frequency ranges. US-A-4 493 389 discloses a speaker assembly and deals with the design of the housing of such an assembly without any reference how to electrically drive the loudspeaker. From EP-A-0 125 625 a bass-reflex type speaker system is known having a housing with a separation wall in order to form two sub-cavities. This reference does not disclose any hints how to electrically drive the loudspeaker. SUMMARY OF THE INVENTION: The present invention has been made in consideration of the conventional problems, and has as its first object to provide a driving apparatus for driving a vibrator of an acoustic apparatus in which the vibrator is disposed on a resonator having a closed cavity (e.g., a cabinet) and acoustic mass means (e.g., a resonance opening) for causing the cavity to acoustically communicate with an external area, wherein Q values at a first frequency by the vibrator and a stiffness of the cavity and at a second frequency by the stiffness of the cavity and the mass means can be independently set, and a size of a system including the acoustic apparatus and the driving apparatus of the present invention can be reduced and performance of the system can be improved, in such a manner that the acoustic apparatus can be rendered compact, and a damping force can be increased. It is a second object of the present invention to provide a driving apparatus for driving an acoustic apparatus which drives a plurality of resonators having different resonance frequencies by one vibrator, wherein the acoustic apparatus can be made compact and a design margin can be increased. It is a third object of the present invention to provide a driving apparatus which can eliminate an adverse influence on sound quality caused by a non-motional impedance of an electro-acoustic transducer (vibrator) to a level equivalent to or lower than that achieved by a normal constant-voltage driving method while improving a driving force (sound pressure) and a damping force near a resonance frequency associated with a sound pressure of the transducer. In order to achieve the above objects, according to a first aspect of the present invention, there is provided a driving apparatus for driving a vibrator of an acoustic apparatus in which the vibrator is disposed in a cavity having acoustic mass means, characterized in that at least one of output impedances at a first resonance frequency by the vibrator and a stiffness of the cavity and at a second resonance frequency by the stiffness of the cavity and the mass means becomes a negative impedance, and the output impedances have different values. The equivalent circuit shown in Fig. 42 will be again exemplified below. When the output impedance of the driving apparatus is a negative impedance -Z O and can completely invalidate an impedance Z V (e.g., R VC in Fig. 42) inherent in the vibrator, i.e., when Z V - Z O = 0 (R VC - R O = 0 in Fig. 42), the parallel resonance circuit as a unit resonance system constituted by the equivalent inductance L O and the equivalent capacitance C O of the speaker unit is short-circuited through the constant voltage source E VC as the driving apparatus. Therefore, the value Q₁ becomes 0, and this circuit is essentially not resonated. In other words, the unit resonance system resonance circuit is driven by the driving apparatus E VC in a perfectly damped state. The series resonance circuit (port resonance system) at the resonance side constituted by the equivalent stiffness 1/L C of the cavity and the equivalent mass C P of the mass means is short-circuited through the driving apparatus E VC . However, since this resonance system is a series resonance circuit, a theoretical value Q₂ is ∞ if the acoustically equivalent resistance of the cavity and the mass means is ignored. In this case, the unit resonance system and the port resonance system are independently driven by the driving apparatus E VC , and have no mutual dependency therebetween. Therefore, the resonance frequencies f₁ and f₂ and the Q values Q₁ and Q₂ can be set independently of each other. When R VC - R O > 0 or when the acoustically equivalent resistance of the cabinet and the resonance port (or a resonance opening) cannot be ignored, the values Q₁ and Q₂ take intermediate values between the 0 and ∞ mentioned above and those by the conventional driving method in which the output impedance of the driving apparatus is 0. When the output impedance of the driving apparatus is a positive value, the value Q₁ is increased and the value Q₂ is decreased as the output impedance value is increased. Assuming a bass-reflex speaker system in which a resonance frequency by a cabinet and a port is set to be low while using a compact cabinet, it has a larger value Q₁ and a smaller value Q₂ than those of a bass-reflex speaker system according to a standard design. When this speaker system is driven by the negative resistance -R O (R VC - R O ≧ 0), the value Q₁ is decreased and the value Q₂ is increased as the absolute value of the negative resistance -R O is increased. Fig. 1 shows the relationship among the negative resistance -R O , Q₁, and Q₂. In Fig. 1, when R O = 0, a conventional, general constant-voltage drive state is established. When -R O is decreased to be smaller than 0 and to be approximate to -R VC , the value Q₁ is almost linearly decreased toward 0. On the contrary, the value Q₂ is increased but does not reach ∞, and approaches a value determined by the acoustic resistance of the cabinet and the port. Therefore, the values Q₁ and Q₂ may become desired values at a given -R O . However, as shown in Fig. 1, the -R O value (-R O = -R A ) yielding a desired Q₁ (= A) may often be different from the -R O value (-R O = -R B ) yielding a desired Q₂ (= B). According to the first aspect of the present invention, in this case, the output impedance of the driving apparatus (to be referred to as a driving impedance hereinafter) at the frequency f₁ is set to be -R A , and the driving impedance at the frequency f₂ is set to be -R B , thereby obtaining the desired values Q₁ and Q₂. In some cabinet designs, both the values Q₁ and Q₂ are increased, and must be decreased. In this case, according to the present invention, as shown in Fig. 2, the driving impedance Z₁ at the frequency f₁ is set to be negative (-R A ), and the driving impedance Z₂ at the frequency f₂ is set to be positive (R B ). In contrast to this, when both the values Q₁ and Q₂ are to be increased, according to the present invention, the driving impedance Z₁ at the frequency f₁ is set to be positive (R A ), and the driving impedance Z₂ at the frequency f₂ is set to be negative (-R B ). Note that since another resonance frequency f₃ is not associated with an output sound pressure, the driving impedance value at this frequency f₃ is not particularly limited. The driving impedance Z₃ at the frequency f₃ is preferably set to satisfy Z₃ < 0 so as to suppress a wasteful movement of the diaphragm of the vibrator. As described above, according to the first aspect of the present invention, when the vibrator of the acoustic apparatus in which the vibrator is disposed in the resonator constituted by the cavity and the acoustic mass means, the driving impedance Z₁ at the first resonance frequency f₁ determined by the vibrator and the cavity and the driving impedance Z₂ at the second resonance frequency f₂ determined by the cavity and the mass means are set to be negative values and to satisfy Z₁ ≠ Z₂, or one of the Z₁ and Z₂ is set to be positive or 0 and the other is set to be negative, so that the values Q₁ and Q₂ can be independently set. Thus, the acoustic apparatus having the resonator, e.g., a speaker system can be designed regardless of limitations on a conventional bass-reflex type system. For example, the cabinet can be rendered compact so as to achieve a compact system without impairing the sound pressure and sound quality. Since appropriate Q values can be obtained at the resonance frequencies f₁ and f₂, a design margin can be increased compared to a system having a constant negative output impedance (-Z O ). Depending on conditions, improved performance can be expected compared to a system having a constant -Z O . When the driving impedance Z₁ at the first resonance frequency f₁ is set to be a negative value so as to decrease the value Q₁, the speaker system can be driven while the unit resonance system is damped. According to a second aspect of the present invention, there is provided a driving apparatus for driving a vibrator of an acoustic apparatus in which a plurality of resonators having different resonance frequencies are driven by the vibrator and sound pressure outputs of the resonators are mixed to be radiated as an acoustic wave, characterized in that the vibrator is driven by the driving apparatus which includes a negative impedance in an output impedance at least at one of resonance frequencies associated with a sound pressure among a plurality of resonance frequencies formed by a combination of motional impedance elements of the vibrator and the resonators. The driving apparatus according to the second aspect of the present invention negative-impedance drives the vibrator at least at one frequency of resonance frequencies associated with a sound pressure of those formed by the plurality of motional impedances. Therefore, a non-motional impedance of the vibrator at that resonance frequency is eliminated or invalidated. For example, when the output impedance of the driving apparatus is the negative resistance -R O (R VC - R O = 0) in the entire reproduction range of the acoustic apparatus shown in Fig. 45, i.e., when the resistance R VC is short-circuited in the equivalent circuit shown in Fig. 46, the resonance circuits Z₁, Z₂, and Z₄ are equivalently directly connected to the constant voltage source E VC having an AC impedance 0, and their two ends are short-circuited in an AC manner. Thus, the parallel resonance circuit Z₁ has a resonance Q value of 0, and the series resonance circuits Z₂ and Z₄ theoretically have Q values of ∞ if the acoustically equivalent resistances r 1a , r 1p , r 2a , and r 2p are ignored. In this case, the resonance circuits Z₂ and Z₄ are connected through the zero impedance, and have no mutual dependency. Therefore, the resonance frequencies f₄ and f₂ and the Q values Q₄ and Q₂ can be independently set. Note that when R VC - R O > 0, or when the acoustically equivalent resistances r 1a , r 1P , r 2a , and r 2p of the cavities and the resonance opening ports cannot be ignored, the values Q₄ and Q₂ take intermediate values between ∞ and those in a case of the conventional constant-voltage driving method in which the output impedance of the driving apparatus is 0, as in the first aspect. When the output impedance of the driving apparatus is a positive value, the values Q₂ and Q₄ are decreased as the output impedance value is increased. In this manner, according to the second aspect of the present invention, the output impedance of the driving apparatus is appropriately set at least at a resonance frequency associated with a sound pressure, so that Q values at the corresponding resonance frequencies can be appropriately set to obtain appropriate sound pressure characteristics. Therefore, the dimensions of the cavity (cabinet) of the acoustic apparatus can be relatively freely designed, thus increasing a design margin and making the cavity compact. When a driving apparatus according to a third aspect of the present invention drives an electro-acoustic transducer (vibrator), it drives, by a negative impedance, this transducer near at least a resonance frequency associated with a sound pressure of those in an actual use state of this transducer, and drives, by a zero positive impedance, the transducer in a range wherein the influence of a non-motional impedance of the transducer on sound quality cannot be ignored. According to the driving apparatus of the third aspect, since the electro-acoustic transducer is driven by the negative impedance near at least a resonance frequency associated with a sound pressure of those in an actual use state of the transducer, the non-motional impedance of the transducer is eliminated or invalidated. Therefore, a Q value at a resonance frequency f C , f OC , or f₁ of a vibration system of the transducer equivalently constituting a parallel resonance system is decreased, and a driving force and damping force near the resonance frequency can be improved. More specifically, the vibration system is operated at a constant speed by the negative impedance driving, and the driving force and damping force of the speaker unit are improved. Note that the Q value is increased and an output sound pressure from the resonance port is increased near the resonance frequency f₂ by the resonance port and the cabinet of the bass-reflex speaker system equivalently constituting a series resonance system. Since the transducer is driven by the zero or positive impedance at a frequency separated from these resonance frequencies, the transducer is driven at a constant voltage or current. More specifically, the driving current is determined by the output impedance and a linear component of the non-motional impedance of the speaker unit. An acoustic distortion caused by the influence of a non-linear component of the non-motional impedance which remains when the non-motional impedance is eliminated or invalidated by the negative impedance driving is suppressed by the zero-impedance driving to a level equivalent to that by the conventional constant-voltage driving, and can be decreased by the positive-impedance driving to a level lower than that by the constant-voltage driving. In this manner, according to the third aspect of the present invention, the electro-acoustic transducer is driven by the negative impedance near at least a resonance frequency associated with a sound pressure of those in an actual use state of the transducer, so that advantages of the negative-impedance driving, such as improvement of the damping force, driving force, and a design margin, can be enhanced. At the same time, the transducer is driven by the zero or positive impedance in a range wherein the influence of the non-motional impedance of the transducer given to sound quality cannot be ignored, so that the adverse influence of the non-motional impedance can be prevented or eliminated. BRIEF DESCRIPTION OF THE DRAWINGS: The present invention in shown in Figures 29-51 and the corresponding parts in the description. Figs. 1 and 2 are graphs showing the relationship between an output impedance and a Q value for explaining the principle of the present invention; Fig. 3 is a circuit diagram for explaining a basic arrangement of a driving apparatus; Fig. 4 is a circuit diagram showing a modification of Fig. 3; Fig. 5 is a circuit diagram showing an example of the circuit shown in Fig. 4; Fig. 6 is a circuit diagram; Fig. 7 is a graph showing frequency characteristics of an output impedance of the circuit shown in Fig. 6; Fig. 8 is a circuit diagram; Fig. 9 is a graph showing frequency characteristics of an output impedance of the circuit shown in Fig. 8; Fig. 10 is a circuit diagram; Figs. 11 to 14 are graphs showing frequency characteristics of an output impedance in accordance with various setting states of constants in the circuit shown in Fig. 10; Fig. 15 is a circuit diagram, which is operated in the same manner as the circuit shown in Fig. 10; Fig. 16 is a circuit diagram; Figs. 17 to 19 are graphs showing frequency characteristics of an output impedance according to various setting states of constants in the circuit shown in Fig. 16; Fig. 20 is a circuit diagram; Fig. 21 is a graph showing frequency characteristics of an output impedance of the circuit shown in Fig. 20; Fig. 22 is a circuit diagram; Fig. 23 is a diagram showing a basic arrangement of an acoustic apparatus; Figs. 24 and 25 are electrically equivalent circuit diagrams of the apparatus shown in Fig. 23; Fig. 26 is a graph showing the relationship between an output impedance of a driving apparatus and a Q value of a resonator; Fig. 27 is a graph showing frequency characteristics of an output impedance when the circuit with the arrangement shown in Fig. 8 is used as the driving apparatus in Fig. 23; Fig. 28 is a graph showing frequency characteristics of an impedance of the acoustic apparatus shown in Fig. 23 and an output impedance of the driving apparatus when the circuit with the arrangement shown in Fig. 22 is used as the driving apparatus in Fig. 23; Fig. 29 is a circuit diagram showing a basic arrangement according to the present invention; Fig. 30 is a graph showing frequency characteristics of an output impedance for explaining the principle of the invention; Fig. 31 is a circuit diagram showing a first example of the invention; Fig. 32 is a graph showing frequency characteristics of an output impedance of the circuit shown in Fig. 31; Fig. 33 is a circuit diagram showing a second example of the invention; Fig. 34 is a graph showing frequency characteristics of an output impedance of the circuit shown in Fig. 33; Fig. 35 is a graph showing characteristics of filters (LPF and HPF) for explaining a modification of Fig. 33; Fig. 36 is a graph showing frequency characteristics of an output impedance of the circuit using the filters shown in Fig. 35; Fig. 37 is a graph showing frequency characteristics of an output impedance of the circuit using the filters shown in Fig. 35 in comparison with an impedance of a dynamic speaker unit; Fig. 38 is a graph showing frequency characteristics of a woofer; Fig. 39 is a circuit diagram showing a third example of the invention; Fig. 40 is a graph showing frequency characteristics of a feedback filter in the circuit shown in Fig. 39; Figs. 41A and 41B are respectively a perspective view and a sectional view showing an arrangement of a conventional bass-reflex speaker system; Fig. 42 is an electrical equivalent circuit diagram when the bass-reflex speaker system shown in Fig. 41 is-driven at a constant voltage; Fig. 43 is a graph showing electrical impedance-frequency characteristics of the equivalent circuit shown in Fig. 42; Fig. 44 is a circuit diagram showing a negative impedance generating circuit according to a prior application; Fig. 45 is a sectional view showing an arrangement of a double bass-reflex speaker system; Fig. 46 is an electrically equivalent circuit diagram when the speaker system shown in Fig. 45 is driven at a constant voltage; Fig. 47 is a graph showing electrical impedance-frequency characteristics of the speaker system shown in Fig. 45; Fig. 48 is a graph showing an acoustic output of the speaker system shown in Fig. 45; Fig. 49 is a graph showing an average energy spectrum of a music piece; Fig. 50 is an electrically equivalent circuit diagram when a dynamic speaker is mounted on an infinite baffle and is driven at a constant voltage; and Fig. 51 is a graph showing electrical impedance-frequency characteristics of the equivalent circuit shown in Fig. 50. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS: Preferred embodiments of the present invention will now be described with reference to the accompanying drawings. Fig. 3 shows a basic circuit arrangement of a driving apparatus. In the driving apparatus in Fig. 3, an output from an amplifier 31 having a gain A is supplied to a load Z L of a speaker 32. A current I L flowing through the load Z L is detected, and is positively fed back to the amplifier 31 through a feedback circuit 33 having a transmission gain β. With this arrangement, an output impedance Z O of the driving apparatus is given by Z O = Z S (1 - Aβ) where Z S is the impedance of a sensor for detecting the current I L . From this equation, if Aβ > 1, Z O becomes an open-stable negative impedance. An application example corresponding to this circuit is disclosed in Japanese Patent Publication Sho No. 59-51771. Current detection can be performed at a non-ground side of the speaker 32. An application example of this circuit is disclosed in, e.g., Japanese Patent Publication Sho No. 54-33704. Fig. 4 shows a BTL connection, and can be easily applied to the circuit shown in Fig. 3. In Fig. 4, reference numeral 34 denotes an inverter. Fig. 5 shows a detailed circuit of an amplifier including a negative resistance component in an output impedance. The output impedance Z O in the amplifier shown in Fig. 5 is given by: Z O = R S (1 - R b /R a ) = 0.22(1 - 30/1.6) = -3.9 (Ω) In the circuit shown in Fig. 3, if one of A, β, and Z S is caused to have characteristics in which its a value changes according to a frequency (to be referred to as frequency dependency hereinafter), the output impedance Z O can have the frequency dependency. Fig. 6 shows a circuit arrangement when output impedances Z₁ and Z₂ at frequencies f₁ and f₂ are negative impedances and can be close to each other. The circuit shown in Fig. 6 employs a current detection resistor R S as a sensor for detecting the current I L , and employs as the negative feedback circuit 33, a CR circuit 33a which consists of a capacitor C₁ and resistors R₁ and R₂ and whose transmission gain has frequency dependency (frequency characteristics in a predetermined range are not flat), and an amplifier 33b whose transmission gain does not have frequency dependency (transmission gain is constant in the predetermined range), so that the transmission gain β has frequency dependency in the negative feedback circuit 33 as a whole. Note that if the CR circuit 33a is included in the current detection sensor Z S , the sensor Z S can be regarded to have frequency dependency. Fig. 7 shows frequency characteristics of the circuit shown in Fig. 6. In Fig. 7, Z 1 = R S 1 - A· R 2 R 1 + R 2 ·β O Z 2 = R S (1 - Aβ O ) A frequency f P at an inflection point P where an output impedance falls from Z₁ toward Z₂ when an output impedance curve is line approximated in accordance with the Nyquist method is almost 1/2πC₁R₂. Fig. 8 shows a circuit when Z₁ < Z₂ < 0, and Fig. 9 shows frequency dependency of the circuit shown in Fig. 8. In Fig. 9, Z 1 = R S (1 - Aβ O ) Z 2 = R S 1 - A· R 2 R 1 + R 2 ·β O The inflection point frequency f P is almost 1/2πC₁R₁. Fig. 10 shows a circuit when Z₁ < Z₂ and Z₂ is largely changed with respect to Z₁. In the circuit shown in Fig. 10, a signal having a dip at a frequency f₂ is fed back to an amplifier 31 by a twin T circuit 35 whose dip frequency is set at f₂. For this reason, an output impedance only near the frequency f₂ can be increased, as shown in Fig. 11. In the circuit shown in Fig. 10, output impedances Z₁ and Z₃ at frequencies f₁ and f₃ are given by: Z 1 = Z 3 = R S (1 - Aβ O ) and can be set to be arbitrary values by selecting β O . The shape of the curve in Fig. 11 can be varied by a variable resistor VR₁ in the circuit shown in Fig. 10, as shown in Fig. 12, and can be varied by a variable resistor VR₂, as shown in Fig. 13. In the circuit shown in Fig. 10, if the dip frequency of the twin T circuit 35 is set at f₁, Z₁ > Z₂ and Z₃ can be established, as shown in Fig. 14. A resonance at the frequency f₃ is not associated with a sound pressure. In the circuits in Figs. 6, 8, and 10, the output impedance Z₃ at the frequency f₃ is set to be a negative impedance to decrease a Q value Q₃ at the frequency f₃. Thus, the speaker 32 is sufficiently damped so as not to be wastefully moved. Fig. 15 shows a modification of the circuit shown in Fig. 10, in which an LC resonance circuit 36 is used in place of the twin T circuit 35. In this manner, when the LC resonance circuit 36 is used, the same operation as in the circuit shown in Fig. 10 can be achieved. Fig. 16 shows a circuit wherein an LC resonance circuit 37 is connected in series with a feedback system. In the circuit shown in Fig. 16, a feedback amount (transmission gain β) is maximized at a resonance frequency of this LC resonance circuit 37, which is given by: f = 1 2π L 1 C 1 Therefore, as shown in Fig. 17, the output impedance at the frequency f can be minimized. When the frequency f is set at f₁ or f₂, the output impedances Z₁ and Z₂ can be set considerably different from each other, as shown in Fig. 18 or 19. Fig. 20 shows a circuit wherein a second LC resonance circuit 38 which is resonated at the frequency f₃ is added to the circuit shown in Fig. 17. As shown in Fig. 21, when the output impedance at the frequency f₃ is decreased, the Q value Q₃ is decreased. With this arrangement, a wasteful movement of the speaker 32 can be effectively prevented. In Fig. 21, f 1 = 1 2π L 1 C 1 f 3 = 1 2π L 2 C 2 In the above circuit, the output impedance Z O is Z O = R S (1 - Aβ), and when β ≧ 0, the maximum value of Z O is R S . When the feedback circuit 33 is used for both positive and negative feedback operations, one of Z₁ and Z₂ can be set to be a negative value, while the other can be set to be a positive value larger than R S . Fig. 22 shows a circuit whose transmission gain is given by: β = β O {F(X) - F(Y)} and which has both positive and negative components. As shown in Fig. 22, when the feedback circuit 33 is caused to have given transmission characteristics F(X) and -F(Y), β > 0 is established in a range wherein the gain of F(X) exceeds F(Y). Since Z O = R S (1 - Aβ), the output impedance is equal to or smaller than R S , and a negative impedance can be realized when Aβ > 1. Contrary to this, since β < 0 is established in a range where the gain of F(Y) exceeds F(X), the output impedance becomes a positive impedance equal to or larger than R S . In this manner, the speaker system having a bass-reflex structure is driven by a negative impedance at least at one of resonance points f₁ and f₂ associated with its sound pressure, and output impedance values Z₁ and Z₂ at the resonance points f₁ and f₂ are set to yield Z₁ ≠ Z₂. Thus, the Q values Q₁ and Q₂ at the corresponding resonance points f₁ and f₂ can be independently set, and a damping force, performance, and sound quality can be improved. In the above embodiment, the resistor R S is used as a current detection sensor. As the sensor, however, a current probe such as a current transformer (C.T.) or a Hall element may be used. As the sensor, a reactance element such as a capacitor or inductance may be used. In this case, the sensor itself can have frequency dependency. When the output from the sensor is differentiated or integrated, frequency dependency or flat frequency characteristics can be provided. For example, the current I L is detected by a terminal voltage of the resistor R S , and is differentiated or integrated by the feedback circuit 33, so that the transmission gain β can have frequency dependency. Alternatively, the current I L is detected by a terminal voltage of the capacitor and is differentiated by the feedback circuit 33, so that the frequency dependency of the transmission gain β becomes flat. In order to provide frequency dependency to the feedback circuit 33, current or voltage feedback may be performed in the feedback amplifier (33b in Fig. 6) itself. Fig. 23 shows a basic arrangement of an acoustic apparatus. In the acoustic apparatus shown in Fig. 45, a cabinet 21 is made compact as compared to the conventional apparatus shown in Fig. 45, and opening ports (resonance ports) 23a and 23b which are difficult to be housed in the cabinet 21 accordingly are arranged to extend outwardly from the cabinet 21. As a driving apparatus for driving a vibrator (speaker unit) 25 mounted on a partition plate 22, a driving apparatus 30 which includes a negative impedance in an output impedance at least at one frequency of resonance frequencies f₂ and f₄ associated with a sound pressure output of five resonance frequencies f₁, f₂, f₃, f₄ and f₅ shown in Fig. 47, is used. Fig. 24 shows an electrically equivalent circuit of Fig. 23. Fig. 25 shows an electrically equivalent circuit when Z V - Z O = 0 in Fig. 24, i.e., an internal impedance inherent in the vibrator 25 is equivalently completely invalidated. In the state shown in Fig. 25, two ends of each of series resonance circuits Z₄ and Z₂ by equivalent motional impedances of Helmholtz resonators formed by chambers 21a and 21b and the opening ports 23a and 23b are short-circuited in an AC manner. Therefore, equivalent resistors equivalently connected in series with these series resonance circuits Z₄ and Z₂ are only r 1a , r 1p , r 2a , and r 2p . The Q values of these series resonance circuits Z₄ and Z₂ respectively become R VC /(r 1a + r 1p ) times and R VC /(r 2a + r 2p ) times those obtained when the system is driven at a constant voltage. Since the resistances of these equivalent resistors r 1a , r 1p , r 2a , and r 2p are negligibly small as compared to the voice coil resistor R VC , as described above, the Q values of the series resonance circuits Z₄ and Z₂ can be greatly increased as compared to a case wherein the system is driven at a constant voltage. Fig. 26 shows the relationship between the output impedance and the Q value of the driving apparatus 30. This relationship is represented by the same curve as that of the relationship between the output impedance and Q₂ of the driving apparatus shown in Figs. 1 and 2. As can be seen from Fig. 26, the Q value of the series resonance circuit can be increased by the negative-impedance driving, and can be set to be equal to or smaller than that by the conventional constant-voltage driving by zero- or positive-impedance driving. The Q value at the frequency f₄ is decreased upon making the cavity 21a compact in the conventional constant-voltage driving. However, in the acoustic apparatus shown in Fig. 23, the driving apparatus 30 has a negative impedance at the frequency f₄ and therefore the Q value can be sufficiently increased compensating for an amount which would be decreased by the constant-voltage driving. More specifically, in the structure shown in Fig. 23, a Q value which is to be highest is the Q value Q₄ at the resonance frequency f₄. In the constant-voltage driving, when the cavity 21a is decreased in volume, the value Q₄ is decreased. However, in the acoustic apparatus shown in Fig. 23, even if the volume of the cavity 21a is decreased, the resonance Q value Q₄ at the resonance frequency f₄ can be set to be sufficiently large by setting an appropriate negative impedance as the output impedance of the driving apparatus 30. For this reason, the cabinet can be rendered compact, thus realizing a compact system. If the output impedances of the driving apparatus 30 are the same at the frequencies f₄ and f₂, the Q value can be easily set to be higher at the frequency f₂ (higher than the frequency f₄) than at the frequency f₄, and an output sound pressure level is also high, as described above. Therefore, flat sound pressure output characteristics cannot be obtained between the frequencies f₄ and f₂. This can be solved as follows. That is, the output impedance of the driving apparatus 30 is set to have frequency dependency so that the output impedance becomes negative at the frequency f₄ and the output impedance at the frequency f₂ becomes higher than that at the frequency f₄. As a negative impedance generating circuit for driving the vibrator by the negative impedance as described above, the same circuit as that described in the first embodiment represented by the basic arrangement shown in Fig. 3 can be used. In this case, the circuit and constants must be selected taking into consideration the fact that resonance frequencies of interest are series resonance frequencies f₂ and f₄, and to allow use of a smaller cabinet, the output impedance Z₄ at the frequency f₄ must be set to be negative and the output impedance Z₂ at the frequency f₄ must be set to be higher (or larger) than Z₄. For example, as the driving apparatus 30, the circuit shown in Fig. 6 can be used. Fig. 27 shows frequency characteristics in this case. In Fig. 27, Z 2 = R S 1 - A· R 2 R 1 + R 2 ·β O Z 4 = R S (1 - Aβ O ) The frequency f p at the inflection point P is almost 1/2πC₁R₂. In the description of the first embodiment, the same circuit as in Fig. 22 can be used as the driving apparatus 30 of the second embodiment. Since the transmission gain β of the circuit shown in Fig. 22 has both positive and negative components as expressed by: β = β O {F(X) - F(Y)} this circuit can realize frequency characteristics in which the output impedance changes between the positive and negative levels, as shown in Fig. 28. When the vibrator 25 of the double bass-reflex speaker system shown in Fig. 23 is driven by the driving apparatus 30 having output impedance characteristics as shown in Fig. 27, both a compact system and high efficiency can be achieved. For example, in the conventional system shown in Fig. 45, the cavity 21a is reduced in size, and the output impedance of the driving apparatus at the resonance frequency f₄ is set to be negative so as to increase the Q value. Meanwhile, the cavity 21b is designed to be relatively larger than a conventional one to improve efficiency, and the system is driven by the positive impedance, thereby decreasing the Q value. Fig. 27 shows the relationship between the resonance frequency of the resonator and the output impedance of the driving apparatus 30 when the system is driven as described above. In the above embodiment, the opening port is used as an acoustic mass means constituting the resonator. However, the acoustic mass means may be a simple opening or may be a passive vibrating body such as a drone cone. Fig. 29 shows a basic circuit arrangement of a driving apparatus according to the present invention. The basic arrangement in Fig. 29 is completely the same as that shown in Fig. 3, and its output impedance Z O is represented by Z O = Z S (1 - Aβ). When Aβ > 1, the output impedance becomes an open-stable negative impedance, and when Aβ ≦ 1, it becomes 0 or a positive impedance. For example, if a speaker 32 is a dynamic speaker unit whose equivalent circuit is shown in Fig. 50, when Aβ > 1 is set in Fig. 29 and the detection resistor R S like in the prior application apparatus shown in Fig: 43 is used as the current detection impedance Z S in Fig. 29, the output impedance becomes Z O = R S (1 - Aβ) = -R O , i.e., a negative resistance. The negative-resistance driving in which the speaker unit is driven while a negative resistance is used as the output impedance can effectively, equivalently reduce the value of the voice coil resistor R VC . Thus, the vibration system can be operated At a constant speed, thereby increasing a driving force and a damping force. When the negative-resistance driving is also performed in a high-frequency range, the impedance of the equivalent capacitance C O is decreased in the high-frequency range and the high-frequency range driving current is determined by the resistor R VC and the impedance of the inductor L VC . Therefore, when the resistance of the resistor R VC is decreased by the negative-resistance driving, the high-frequency driving current tends to be influenced by L VC . Therefore, in the high-frequency range, the driving impedance is preferably high to reduce the influence of L VC . A constant-speed operation is difficult to achieve at a frequency separated from the resonance frequency f O , and the high-frequency region is originally a mass control region, and it is less significant even if the constant-speed operation is achieved in this region. In the third embodiment, the output impedance of the driving apparatus is set to be Aβ > 1, i.e., a negative impedance at a low frequency near the resonance frequency f O , as shown Fig. 30, and is set to be Aβ < 1, i.e., a positive impedance at a high frequency at which the electrical inductance L VC of the voice coil begins to function. In order to vary or switch the output impedance between negative and positive levels in accordance with a frequency, A or β can be varied or switched in accordance with the frequency. In this embodiment, the way of a change in output impedance in an intermediate frequency range between the high- and low-frequency ranges is not particularly limited. Fig. 31A shows a circuit arrangement of a driving apparatus in which the feedback circuit 33 is arranged to have a large positive feedback amount β in a low-frequency range and a small feedback amount in a high-frequency range. The circuit shown in Fig. 31A uses the current detection resistor R S as a sensor for detecting the current I L , and the feedback circuit 33 is constituted by an amplifier 33b having a gain β C and an LPF (low-pass filter) 33a for allowing only a low-frequency component of an AC voltage signal generated at the current detection resistor R S to pass therethrough and to inputting it into the amplifier 33b. As the LPF 33a, a circuit shown in Fig. 31B may be used. A gain G of this circuit is G ≒ 1 for a low-frequency signal, and is G ≒ 0 for a high-frequency signal. Therefore, in Fig. 31A, when the circuit shown in Fig. 31B is used as the LPF 33a and the gain A of the amplifier 31 and the gain β O of the amplifier 33 are set to satisfy Aβ O > 1, since Aβ = A(β O G) ≒ Aβ O > 1 for the low-frequency signal, the output impedance Z O is given by: Z O = R S (1 - Aβ O ) = -R O < 0 and becomes the negative resistance -R O , as described above with reference to Fig. 29. Since Aβ = A(β O G) ≒ 0 for the high-frequency signal, the output impedance is given by: Z O = R S (1 - Aβ) ≒ R S Therefore, the output impedance becomes a positive impedance almost equal to the value of R S itself. More specifically, the circuit shown in Fig. 31A has a negative output impedance in a low-frequency range and a positive output impedance in a high-frequency range, as shown in Fig. 32. Fig. 33 shows a circuit arrangement of a driving apparatus in which the feedback circuit 33 is used for both positive and negative feedback operations. The circuit shown in Fig. 33 uses the current detection resistor R S as a sensor for detecting the current I L , and the feedback circuit 33 is constituted by an amplifier 33b of a gain β O having positive (non-inverting) and negative (inverting) input terminals, an LPF 33a for allowing only a low-frequency component of an AC voltage signal generated at the current detection resistor R S to pass therethrough to input it to the positive input terminal of the amplifier 33b, and an HPF (high-pass filter) 33c for allowing only a high-frequency component of the AC voltage signal generated at the current detection resistor R S to pass therethrough to supply it to the negative input terminal of the amplifier 33b. Therefore, in the circuit shown in Fig. 33, for a low-frequency signal, β > 0 is established and the output impedance is: Z O = R S (1 - Aβ O ) Therefore, the output impedance becomes smaller than R S , and when Aβ O > 1, a negative impedance can be realized. On the other hand, for a high-frequency signal, since β < 0, Z O = R S (1 + Aβ O ) Therefore, the output impedance becomes a positive impedance larger than R S . A similar circuit has already been illustrated in Fig. 22. The circuits shown in Figs. 33 and 22 have different setting standards of cutoff frequencies of filters and gains of pass-bands (passage gain). Fig. 34 shows frequency dependency of the output impedance of the circuit shown in Fig. 33. Note that in the circuit shown in Fig. 33, when the LPF 33a and the HPF 33c have different gains, the absolute value of the positive impedance can be different from that of the negative impedance. For example, when the gain of the HPF 33c is set to be larger than that of the LPF 33a, as shown in Fig. 35, the absolute value of the positive impedance can be set to be larger than that of the negative impedance, as shown in Fig. 36. In this manner, the gain of the HPF 33c is set to be larger than that of the LPF 33a, so that the output impedance Z O is set to be a negative impedance of |Z O | < R VC in a low-frequency range, and to be a positive impedance of Z LVC << |Z O | with respect to an impedance Z LVC of the inductance L VC of the voice coil, as shown in Fig. 37. As a result, a damping force for the speaker 32 is increased near the resonance frequency f O of the speaker 32, and the influence of the inductance L VC of the voice coil, i.e., an acoustic distortion can be eliminated in a high-frequency range. Note that when the frequency dependency of the output sound pressure is changed upon a change in driving impedance, the change can be corrected at an input V i side as needed. The driving apparatus has both an effect of improving high-frequency characteristics (in particular, distortion characteristics) and an effect of increasing a damping force in a low-frequency range near the resonance frequency f O . Therefore, the driving apparatus can be effectively applied to, particularly, a full-range speaker, or a mid-range speaker or tweeter in a multi-amplifier system. In the tweeter or the like, the resonance frequency f O is separated from the frequency f LVC at which the inductance L VC of the voice coil begins to function. However, in many woofers or the like, as shown in Fig. 38, f O is approximate to f LVC . In this case, the object may not be achieved with the output impedance characteristics shown in Fig. 32, 34, 36, or 37. Fig. 39 shows a circuit arrangement of a driving apparatus which can be suitably used in a woofer or the like in which the resonance frequency f O is approximate to the frequency f LVC at which the inductance L VC of the voice coil begins to function. The circuit shown in Fig. 39 uses a circuit constituted by an all-pass filter 33d and an amplifier 33b as the feedback circuit 33 in the circuit shown in Fig. 29. In Fig. 39, the all-pass filter 33d has a transmission gain of 1 in the entire region in a predetermined frequency range, and phase characteristics in which a phase is inverted through 180° at a predetermined frequency f  or higher. Therefore, in the circuit shown in Fig. 39, for a low-frequency signal lower than the frequency f  , since β > 0, Z O = R S (1 - Aβ O ) Therefore, the output impedance becomes smaller than R S , and when Aβ O > 1, a negative impedance can be realized. For a high-frequency signal higher than the frequency f  , since β < 0, Z O = R S (1 + Aβ O ) Therefore, the output impedance becomes a positive impedance larger than R S . Therefore, the phase inverting frequency f  is set at a frequency as shown in, e.g., Fig. 38, increases in damping force and driving force of the speaker unit and reduction of an acoustic distortion can be achieved at the same time. (Application Range of Third Embodiment) In the third embodiment, the case has been exemplified wherein the dynamic speaker unit is driven by the driving apparatus of the present invention. This embodiment can be applied to a speaker unit which can improve a damping force and driving force, or a design margin by eliminating or invalidating a non-motional impedance at its resonance frequency, and in which the adverse influence, e.g., an acoustic distortion by eliminating or invalidating the non-motional impedance is enhanced at a frequency other than the resonance frequency, e.g., an electromagnetic speaker unit, in addition to the dynamic speaker unit.

Claims: A system comprising a driving apparatus and a vibrator (4), the driving apparatus comprising a drive circuit for providing a drive signal to the vibrator (4), the drive circuit having an output impedance (Z o ) which varies with frequency; the vibrator (4) being arranged in a resonator (1, 8) constituted by a closed cavity (1) and an acoustic mass means (8) for causing said cavity (1) to acoustically communicate with an external region so as to directly radiate an acoustic wave to the outside, the vibrator (4) being driven by the driving apparatus to cause the resonator (1, 8) to radiate a resonant acoustic wave through said acoustic mass means (8) to the outside, characterized in that the output impedance (Z o ) of the drive circuit is negative in the low frequency range and is positive in the high frequency range wherein the low frequency range includes a first resonance frequency which is determined by the motional frequency of said vibrator (4) and the equivalent stiffness of said cavity (1) and a second resonance frequency which is the resonance frequency of said resonator (1, 8). A driving apparatus according to claim 1, characterized in that said resonator (1, 8) is a Helmholtz resonator which comprises a cabinet having an outer wall defining said cavity (1) and an opening or opening port (6) formed on the outer wall of said cabinet as said acoustic mass means (8), and wherein said vibrator (4) is mounted on the outer wall of said cabinet, a first surface of the vibrating body (2, 3) of said vibrator (4) facing said external region, and a second surface thereof facing said cavity (1). A driving apparatus according to claim 1 or 2, characterized in that said vibrator (4) is arranged to drive a plurality of resonators (1, 8) in parallel wherein each resonator (1, 8) is constituted by a closed cavity (1) and an acoustic mass means (8) for causing the respective cavity (1) to acoustically communicate with an external region and wherein the resonators (1, 8) have different resonance frequencies. A driving apparatus according to claim 3, characterized by further including a cabinet having a partition plate (22) therein which divides the cabinet into two chambers (21a, 21b), the partition plate (22) having an opening, wherein each of the two chambers (21a, 21b) defines the cavity of a respective resonator, and said acoustic mass means (23a, 23b) of each resonator comprising one of an opening, an opening port or a passive vibrating body located on the outer wall of said cabinet, and wherein said vibrator (4) is mounted on the partition plate (22), said vibrator (4) closing the opening formed in said partition plate (22), a first surface of said vibrating body facing one of the cavities, and a second surface thereof facing the other cavity. A driving apparatus according to any of the preceding claims, characterized in that the output impedance (Z o ) of the driving apparatus near at least a resonance frequency associated with a sound pressure among resonance frequencies in the state of actual use of said vibrator (4) is negative, and the output impedance (Z o ) of the driving apparatus is positive in a frequency range in which the influence of non-motional impedance of said vibrator (4) on sound quality is not negligible. A driving apparatus according to any of the preceding claims, characterized in that said vibrator (4) is a dynamic electro-acoustic transducer.

Inventors: NORO MASAO, NORO, MASAO
Applicants: YAMAHA CORP, YAMAHA CORPORATION
Application year: 1989
Main classification: H04R3
IPC codes: H04R3