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Loudspeaker having a two-part diaphragm for use as a car loudspeaker
| Details |
Inventors: Nieuwendijk, Joris A. M.; Bax, Johannes W. T.; Kamphues, Johannes J. M.; de Haas, Franciscus C. M.;
Assignee: U.S. Philips Corp. (New York, NY)
Primary Examiner: Hix; L. T.
Assistant Examiner: Brown; Brian W.
Attorney, Agent or Firm: Franzblau; Bernard
An electrodynamic loudspeaker (1) has a diaphragm comprising a central part (2) and a peripheral part (3), and a voice-coil device (9, 10) coupled to the central part (2). The surface ratio S.sub.2 /S.sub.1 complies with the relationship 0.5.ltoreq.S.sub.2 /S.sub.1 .ltoreq.6, where S.sub.1 and S.sub.2 are the surface areas of the central part (2) and the peripheral part (3) respectively. The mass ratio m.sub.2 /m.sub.1 complies with the relationship 0.5.ltoreq.m.sub.2 /m.sub.1 .ltoreq.8 where m.sub.1 and m.sub.2 are the mass of the central part (2) and the voice-coil device (9, 10) and the mass of the peripheral part (3) respectively. Further, the stiffness imposed on the diaphragm by the space (6, 6') defined by the diaphragm (2, 3) and the chassis (4) and/or the magnet system (7) is smaller than the stiffness of the diaphragm itself. Thus it is possible to derive a car loudspeaker which has a specific dip in its frequency response characteristic P (FIG. 2a), measured in an anechoic room. |
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DETAILED DESCRIPTION In order to obtain a frequency response characteristic with a broadened dip, the loudspeaker in accordance with the invention should be characterized in that the first value and the second value are equal to 0. 5 and 6 respectively, the third value and the fourth value are equal to 0. 5 and 8 respectively, and in that the stiffness imposed on the diaphragm by the space formed by the diaphragm and the magnet system and/or the chassis is smaller than the stifness of the diaphragm. In fact, the requirement that the stifness imposed on the diaphragm by the space formed by the diaphragm and the magnet system and/or the chassis be smaller than the stiffness of the diaphragm itself, means that the motion of the diaphragm should not be impeded by the air volume at the rear of the diaphragm. In other words: the air volume at the rear diaphragm should not or not significantly affect the frequency response characteristic of the loudspeaker. The stiffness of the diaphragm is defined as the force [in N], exerted on the voice-coil former in the direction of its excursion divided by the excursion of the voice-coil former [in m]. The above requirement can be met by making the air volume behind the diaphragm large enough, provided that it is a fully enclosed volume. However, this renders the loudspeaker rather bulky, which may be a disadvantage when it is to be used as a car loudspeaker. Another possibility is to provide the magnet system and/or the chassis with at least one aperture in order to provide an acoustic path through the magnet system and/or the chassis of the transducer. The invention is based on the recognition of the fact that during use of a loudspeaker having a two-part diaphragm, when the mechanical damping of the peripheral part is chosen correctly, the frequency response versus input impedance characteristic of the loudspeaker substantially exhibits only two maxima which correspond to the two resonant frequencies f. sub. 1 and f. sub. 2 for which the central part and the peripheral part vibrate in phase and in phase opposition relative to each other
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