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WO2011111968A2 - Speaker - Google Patents

Speaker Download PDF

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Publication number
WO2011111968A2
WO2011111968A2 PCT/KR2011/001573 KR2011001573W WO2011111968A2 WO 2011111968 A2 WO2011111968 A2 WO 2011111968A2 KR 2011001573 W KR2011001573 W KR 2011001573W WO 2011111968 A2 WO2011111968 A2 WO 2011111968A2
Authority
WO
WIPO (PCT)
Prior art keywords
speaker
magnet
magnetic
magnetic circuit
voice coil
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.)
Ceased
Application number
PCT/KR2011/001573
Other languages
French (fr)
Korean (ko)
Other versions
WO2011111968A9 (en
WO2011111968A3 (en
Inventor
김석주
허동철
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Individual
Original Assignee
Individual
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Priority claimed from KR1020110019102A external-priority patent/KR101184537B1/en
Application filed by Individual filed Critical Individual
Priority to JP2012556969A priority Critical patent/JP2013522946A/en
Priority to CN2011800230474A priority patent/CN102948171A/en
Priority to US13/582,605 priority patent/US20120328147A1/en
Publication of WO2011111968A2 publication Critical patent/WO2011111968A2/en
Publication of WO2011111968A9 publication Critical patent/WO2011111968A9/en
Publication of WO2011111968A3 publication Critical patent/WO2011111968A3/en
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R9/00Transducers of moving-coil, moving-strip, or moving-wire type
    • H04R9/02Details
    • H04R9/025Magnetic circuit

Definitions

  • the present invention relates to a speaker, and more particularly, to a speaker having excellent performance while having a significantly low height.
  • speakers are devices that convert electrical signals into sounds that we can hear.
  • the micro speaker refers to a speaker suitable for mounting in a small electronic device or a mobile communication terminal.
  • FIG. 1 and 2 are cross-sectional views showing a single magnet speaker according to the prior art.
  • the frame 111 forms the outer shape of the speaker 120.
  • a yoke 104 is provided inside the frame 111 to provide a passage path for the magnetic flux generated by the magnet 101.
  • the yoke 104 is composed of a cylindrical bottom plate 102 and a disc shaped top plate 103 with a closed bottom.
  • a disc shaped magnet 101 is placed between the bottom plate 102 and the top plate 103.
  • the magnetic flux generated by the magnet 101 is guided to the yoke 104 and meets the discontinuous point of the yoke 104, which is called a magnetic gap.
  • Magnetic circuits are devices that provide the magnetic fields needed by speakers to convert electrical signals into sound.
  • a voice coil 105 is located in the magnetic gap.
  • the voice coil 105 is connected to a diaphragm 106.
  • the voice coil 105 moves up and down in accordance with the electrical signal applied to the voice coil 105, this movement is transmitted to the diaphragm 106, and the diaphragm 106 vibrates, whereby the electrical signal is converted into sound.
  • the diaphragm 106 has a central dome and an edge rib shape, and a voice coil 105 is connected to a boundary between two domes. The reason why the diaphragm 106 has a double dome shape is to control the vibration range while smoothing the vibration of the diaphragm 106.
  • a lead wire 107 is connected to the voice coil 105 to apply an electrical signal.
  • the leadwire 107 is generally bonded along the surface of the diaphragm 106 and is connected to the terminal PCB 108 through a hole formed in the frame 111.
  • the diaphragm 106 and the voice coil 105 form a vibrometer 132.
  • the through cap 109 is covered above the diaphragm 106.
  • the through cap 109 is for protecting devices inside the speaker, including the diaphragm 106.
  • the through cap 109 is formed with a plurality of through holes 110. Meanwhile, a plurality of heat dissipation openings 112 are formed in the frame 111 so that heat generated inside the speaker is discharged outward.
  • the speaker according to the prior art operates as follows.
  • an electrical signal is applied to the voice coil 105 via the terminal PCB 108 and the lead wire 107
  • the voice coil 105 located in the magnetic gap moves in a direction perpendicular to the magnetic field by the Fleming law.
  • This movement is transmitted to the diaphragm 106.
  • the motion transmitted to the diaphragm 106 vibrates the diaphragm 106, whereby the electrical signal is converted into sound.
  • the speaker of the prior art according to FIGS. 1 and 2 has the following problems.
  • the thickness of the magnet 101 has to be reduced.
  • the magnetic flux density of the magnetic gap is reduced, resulting in a lower sound pressure of the speaker.
  • the separate assembly in the electronic module (PCB) PCB board not only reduces the efficiency of the manufacturing process, but also increases the assembly time due to many components, which eventually has a problem that the manufacturing cost increases. .
  • FIG. 3 is a cross-sectional view showing a double magnet speaker according to the prior art.
  • the speaker shown in FIG. 3 has a disk shaped first magnet 141 and a ring-shaped second magnet 142 sharing a center with the first magnet.
  • the first magnet 141 and the second magnet 142 are provided on one bottom plate 143. Meanwhile, the first magnet is covered with the first top plate 144, and the second magnet is covered with the second top plate 145. A magnetic gap is formed between the first top plate 144 and the second top plate 145.
  • the bottom plate 143, the first top plate 144, and the second top plate 145 form a yoke 146 that provides a passage path for the magnetic flux.
  • the double magnet speaker according to FIG. 3 also has a magnetic circuit and a vibrometer, the thickness of the first magnet 141 and the second magnet 142 can be reduced to reduce the thickness of the entire speaker. Therefore, as with a single magnet speaker, not only the sound pressure is lowered, but also the manufacturing cost increases due to the complicated structure.
  • FIG. 4 is a cross-sectional view showing a speaker according to the prior art applied to a navigation and a portable game machine.
  • the speaker shown in FIG. 4 is also a speaker of the same method as FIG. 1.
  • the bottom plate 151 was used as a frame.
  • the speaker illustrated in FIG. 4 has a thin vibration system.
  • the voice coil 152 deviates much from the magnetic field, causing loss of frequency band. That is, there is a problem in that the lowest reproduction limit frequency f0 becomes high.
  • a thick voice coil 152 should be used to produce a high output, and the outer diameter of the voice coil 152 is small, so that the winding width is increased, and the X-MAX value when the voice coil 152 is reciprocated up and down (at rated output). Due to the vertical movement width of the coil (mm), the height of the magnetic circuit is increased. In addition, there is a problem of lack of clarity, resolution and sound pressure of the voice tone due to the weakening of the magnetic force of the magnetic circuit.
  • 5 is a cross-sectional view showing a magnetic and magnetic magnetic circuits according to the prior art.
  • 5 (a) is a cross-sectional view showing a conventional magnetic magnetic circuit configuration
  • (b) is a cross-sectional view showing a conventional magnetic magnetic circuit configuration.
  • the magnet 161 since the magnet 161 is inside the yoke 164, this is called a magnetic magnetic circuit.
  • the yoke 164 includes a bottom plate 162 and a top plate 163, and the arrow direction indicates a passage path of the magnetic flux formed by the magnet 161.
  • 5B is referred to as an external magnetic circuit because the magnet 171 has a structure outside the pole piece 175 connected to the bottom plate 172.
  • the arrow direction shown in (b) of FIG. 5 indicates a passage path of the magnetic flux formed by the magnet 171.
  • the speaker according to the prior art has a problem in that the height of the speaker is increased by stacking a bottom plate, a magnet, and a top plate to form a magnetic circuit, and by constructing a vibrometer thereon.
  • the present invention is to solve the problems of the prior art as described above, it is an object of the present invention to provide a speaker that improves the acoustic characteristics while significantly reducing the height of the speaker.
  • the present invention in the configuration of the magnetic circuit of the speaker, unlike the polarity arrangement in the vertical direction of the prior art, the magnetic circuit formed in the horizontal direction, forming the polarity of the magnet in the horizontal direction A vibrometer is formed inside.
  • the micro speaker according to the present invention has the following effects.
  • the voice coil diameter is large, a wire thicker than the conventional voice coil thickness can be used, and thus a high input and high output speaker can be manufactured.
  • the number of speaker parts can be reduced to simplify the assembly work of the micro-speakers, and the production cost can be reduced by automating the production.
  • the sound pressure can be increased, but the strong diaphragm can be used to lower f0.
  • 1 and 2 are cross-sectional views showing a single magnet speaker according to the prior art.
  • FIG. 3 is a cross-sectional view showing a double magnet speaker according to the prior art.
  • FIG. 4 is a cross-sectional view showing a speaker according to the prior art applied to a navigation and a portable game machine.
  • FIG. 5 is a cross-sectional view showing a magnetic and magnetic magnetic circuits according to the prior art.
  • FIG. 6 is a cross-sectional view of an embodiment of a magnetic circuit of a speaker according to the present invention.
  • FIG. 7 is a sectional view showing a first embodiment of a speaker according to the present invention.
  • FIG. 8 is a sectional view showing a second embodiment of a speaker according to the present invention.
  • FIG. 9 is a sectional view showing a third embodiment of a speaker according to the present invention.
  • FIG. 10 is an exploded perspective view showing a first embodiment of a speaker according to the present invention.
  • FIG. 11 is an exploded perspective view showing a third embodiment of a speaker according to the present invention.
  • FIG. 12 is a graph comparing the performance of the speaker according to the first embodiment of the present invention with the performance of the speaker according to the prior art.
  • FIG. 13 is a graph comparing the performance of the speaker according to the third embodiment of the present invention with the performance of the speaker according to the prior art.
  • the speaker according to the present invention includes a magnetic circuit and a vibrometer, wherein the magnetic circuit has a ring shape, based on the center of the ring, has a first polarity on the outer surface, and the first surface on the inner surface.
  • FIG. 6 is a cross-sectional view of an embodiment of a magnetic circuit of a speaker according to the present invention.
  • the N pole and the S pole of the magnet are formed horizontally.
  • the magnet is formed with the N pole and the S pole vertically, the magnetic flux is formed horizontally only in the magnetic gap.
  • the N pole and the S pole are formed horizontally, and the magnetic flux is formed horizontally even in the magnetic gap.
  • Figure 6 (a) shows an embodiment having two plates in the magnetic circuit of the speaker according to the present invention.
  • the magnet 501 according to the present embodiment has a ring shape and has a step from the outside to the inside.
  • the polarity of the magnet 501 is formed as the S pole on the inside and the N pole on the outside. That is, the N pole and the S pole are formed horizontally.
  • the N pole is located on the inner side, it may be formed horizontally so that the S pole on the outside.
  • the magnetic circuit may be configured such that the magnet 501 is in close contact with the first plate 501.
  • the magnetic circuit may be configured such that the magnet 501 is spaced apart from the first plate 501 by a predetermined distance.
  • Figure 6 (b) shows an embodiment having one plate in the magnetic circuit of the speaker according to the present invention.
  • the magnet 601 according to the present embodiment has a ring shape and has a step from the outside to the inside.
  • the polarity of the magnet 601 is formed as the S pole on the inside and the N pole on the outside. That is, the N pole and the S pole are formed horizontally.
  • the N pole is located on the inner side, it may be formed horizontally so that the S pole on the outside.
  • the magnetic circuit may be configured such that the magnet 601 is in close contact with the yoke 602, or may be configured to be spaced apart from the yoke 602 by a predetermined distance. .
  • FIG. 7 is a sectional view showing a first embodiment of a speaker according to the present invention.
  • This embodiment relates to a speaker to which a magnetic circuit of the type described in Fig. 6A is applied.
  • the magnetic circuit of the speaker according to the present embodiment includes a magnet 701 having horizontally formed N poles and S poles, a first plate 702, a second plate 703, and a first plate 702 and a second plate ( And a magnetic gap 705 formed between 703.
  • the magnet 701 is preferably a ring shape having a step from the outside to the inside.
  • the ring shape includes not only a circular ring but also a ring shape having a square or ellipse shape.
  • the magnetic flux generated in the magnet 701 passes through the first plate 702 and passes through the magnetic gap 705 and the second plate 703. It leads to the S pole formed inside the magnet 701.
  • the first plate 702 and the second plate 703 perform the function of a yoke 704 to provide a passage path for the magnetic flux.
  • the vibration system of the speaker is composed of a voice coil 706 and a diaphragm 707 located in the magnetic gap 705.
  • the voice coil 706 is connected to the diaphragm 707 and the edge part 708, the diaphragm 707 is preferably a double dome shape having a dome shape at the center and a lip shape at the edge.
  • the edge portion 708 not only supports the voice coil 706, but also facilitates the movement of the diaphragm 707 and performs a function of controlling the vibration of the diaphragm not to exceed a predetermined range.
  • the voice coil 706 is connected to the lead wire 709 to receive an electrical signal, the lead wire 709 is connected to the terminal PCB 710.
  • the external amplifier signal is delivered to the speaker via the terminal PCB 710.
  • the through cap 711 is covered above the diaphragm 707.
  • the through cap 711 is for protecting devices inside the speaker, including the diaphragm 707.
  • the through cap 711 forms a plurality of through holes.
  • the bottom portion 712 is attached to the bottom of the first plate 702, and serves to filter foreign matter from entering the speaker, as well as to release heat inside the speaker to the outside.
  • the speaker according to the present invention since the height of the ring-shaped magnet (or the height of the magnetic circuit) determines the height of the speaker, provides a speaker that is significantly reduced in thickness compared to the prior art. That is, according to the speaker of the prior art, since the vibration system is formed above the magnetic circuit, the thickness of the speaker is the sum of the height of the magnetic circuit and the height of the vibration system. However, according to the present invention, since the vibrometer is surrounded by the magnetic circuit, the thickness of the speaker is determined by the height of the magnetic circuit. Therefore, the thickness of the speaker is reduced by the height of the vibration system.
  • the strength of the magnetic field of the magnetic circuit is dependent on the volume of the magnet
  • the speaker according to the present invention can maintain the volume while reducing the thickness of the magnet, since the magnet is made of the outer diameter of the speaker, reducing the height of the magnetic circuit It becomes possible.
  • the yoke functions as a frame forming the outer shape of the speaker, a separate frame is omitted, thereby increasing the size of the magnetic circuit.
  • Table 1 compares the magnetic flux density formed in the yoke in the magnetic circuit of the prior art with the magnetic flux density formed in the yoke of the speaker according to the first embodiment of the present invention.
  • the magnetic circuit according to the first embodiment of the present invention has twice the magnetic flux density as compared to the magnetic circuit according to the prior art.
  • the speaker magnetic circuit section when the mass of the vibration system (weight of the voice coil + weight of the diaphragm) is constant, it can be seen that the speaker according to the present invention can further improve the sound pressure based on the strength of a very large magnetic field. .
  • Table 2 compares the performance of the speaker according to the prior art and the speaker according to the first embodiment of the present invention.
  • the thickness of the diaphragm of the speaker according to the prior art and the thickness of the diaphragm according to the first embodiment of the present invention are different from each other by 10 microns, but there is a significant difference in sound pressure. .
  • the voice coil according to the prior art has a wire diameter of ⁇ 40 microns, it is generally not able to produce a high output, but in the first embodiment of the present invention, it is possible to further increase the sound pressure by using a thicker coil wire. It is shown.
  • the size of the magnetic gap is 0.23 mm in the gap between the N pole (or S pole) and the inner diameter coil.
  • the gap between the S pole (or N pole) and the outer diameter coil is also preferably set to 0.23 mm.
  • FIG. 8 is a sectional view showing a second embodiment of a speaker according to the present invention.
  • This embodiment relates to a speaker to which a magnetic circuit of the type described in FIG. 6 (b) is applied.
  • the magnetic circuit of the speaker according to the present embodiment includes a magnet 801, a yoke 804, and a magnetic gap 805 formed between the yoke 804 and the magnet 801 in which the N pole and the S pole are horizontally formed. Is done.
  • the magnet 801 is preferably a ring shape having a step from the outside to the inside. In this case, the ring shape includes not only a circular ring but also a ring shape having a square or ellipse shape.
  • the magnetic flux generated in the magnet 801 passes through the yoke 804, passes through the magnetic gap 805, and is formed inside the magnet 801. It leads to the pole.
  • yoke 804 provides a path for passage of magnetic flux.
  • the vibration system of the speaker is composed of a voice coil 806 and a diaphragm 807 located in the magnetic gap 805.
  • the voice coil 806 is connected to the diaphragm 807 and the edge portion 808, the diaphragm 807 is preferably a double dome shape having a dome shape at the center and a lip shape at the edge.
  • the edge portion 808 not only supports the voice coil 806, but also facilitates the movement of the diaphragm 807, and performs a function of controlling the vibration of the diaphragm not to exceed a predetermined range.
  • the voice coil 806 is connected to the lead wire 809 to receive an electrical signal, the lead wire 809 is connected to the terminal PCB 810.
  • the external amplifier signal is transmitted to the speaker through the terminal PCB (810).
  • the through cap 811 is covered above the diaphragm 807.
  • the through cap 811 is for protecting devices inside the speaker, including the diaphragm 807.
  • the bottom portion 812 together with the yoke 804 forms the bottom surface of the speaker.
  • the bottom portion 812 not only serves to filter foreign matter from entering the speaker, but also discharges heat inside the speaker to the outside.
  • FIG. 9 is a sectional view showing a third embodiment of a speaker according to the present invention. This embodiment relates to a speaker to which the magnetic circuit in which the form described in Fig. 6A is modified is applied.
  • the magnetic circuit of the speaker according to the present embodiment includes a magnet 901 in which N poles and S poles are formed horizontally, a first plate 902, a second plate 903, and a first plate 902 and a second plate ( And a magnetic gap 905 formed between 903.
  • the magnet 901 is preferably ring-shaped.
  • the ring shape includes not only a circular ring but also a ring shape having a square or ellipse shape.
  • the magnetic flux generated in the magnet 901 passes through the first plate 902 and passes through the magnetic gap 905 and the second plate 903. It leads to the S pole formed inside the magnet 901.
  • the first plate 902 and the second plate 903 perform the function of a yoke 904 to provide a passage path for the magnetic flux.
  • the vibration system of the speaker is composed of a voice coil 906, a bobbin 911 and a diaphragm 907 located in the magnetic gap 905.
  • the voice coil 906 is wound around the bobbin 911, which is connected to the diaphragm 907 and the edge portion 908.
  • the diaphragm 907 preferably has a triple rib shape.
  • the edge portion 908 not only supports the voice coil 906, but also facilitates the movement of the diaphragm 907 and performs a function of controlling the vibration of the diaphragm not to exceed a predetermined range.
  • the voice coil 906 is connected to the lead wire 909 to receive an electrical signal, the lead wire 909 is connected to the terminal PCB 910.
  • the external amplifier signal is transmitted to the speaker through the terminal PCB (910).
  • the bottom portion 912 is attached to the bottom surface of the first plate 902.
  • the speaker according to the present embodiment has omitted the through-cap so as to be mounted in the plastic injection molding of the small electronic device. According to this embodiment, since the strength of the magnetic field of the magnetic circuit is enhanced, it is preferable to lower the f0 by making the thickness of the diaphragm 40 microns. According to the configuration as described above, the speaker according to the present embodiment has the advantage that can extend the middle voice band of the audio frequency.
  • FIG. 10 is an exploded perspective view showing a first embodiment of a speaker according to the present invention.
  • the speaker shown in FIG. 10 corresponds to a case where the magnet 701 has a substantially rectangular ring shape.
  • the magnet 701 is bound inside the first plate 702, and the second plate 703 having a rectangular ring shape is bound inside the magnet 701.
  • the voice coil 706 is located in a magnetic gap, which is a gap between the first plate 702 and the second plate 703, and the inside of the voice coil 706 is connected to the diaphragm 707 having a double dome shape.
  • the outer side of the voice coil 706 is connected to an edge portion constituting the outer side of the diaphragm.
  • a terminal PCB 710 for applying an electrical signal is located inside the first plate 702, and upper and lower ends of the speaker are covered with the through cap 711 and the bottom 712.
  • Speakers according to embodiments of the present invention can be applied to a speaker of various uses, it is particularly preferable to apply to a micro speaker.
  • FIG. 11 is an exploded perspective view showing a third embodiment of a speaker according to the present invention.
  • the speaker shown in FIG. 11 corresponds to the case where the magnet 901 has a circular ring shape.
  • the magnet 901 is bound inside the first plate 902, and the second plate 903 having a circular ring shape is bound inside the magnet 901.
  • the voice coil 906 is wound around the bobbin 911, and the bobbin 911 on which the voice coil 906 is wound is located in a magnetic gap, which is a gap between the first plate 902 and the second plate 903.
  • the bobbin 911 is connected to the diaphragm 907 having a lip shape on the inside, and is connected to the edge portion forming the outside of the diaphragm 907 on the outside.
  • the terminal PCB 910 for applying an electrical signal is located inside the first plate 902, the lower end of the speaker is covered with a bottom portion 912.
  • FIG. 12 is a graph comparing the performance of the speaker according to the first embodiment of the present invention with the performance of the speaker according to the prior art. This graph shows the sound pressure and frequency according to the 3cc rear open type using ARTA measuring instruments and measuring microphones.
  • the speaker according to the first embodiment of the present invention has a flatter characteristic at a wider frequency than the speaker according to the prior art.
  • the sound pressure is remarkably high. Therefore, when the present invention is applied to a mobile communication terminal or the like, it can be seen that the call sound can be provided with high sound quality such as earphone sound.
  • FIG. 13 is a graph comparing the performance of the speaker according to the third embodiment of the present invention with the performance of the speaker according to the prior art. This graph shows the sound pressure and frequency at 1m / 1w / 2.83v on an 8 kHz basis using an LMS measuring instrument and a measuring microphone.
  • the speaker according to the third embodiment of the present invention has superior f0 to 200 to 300 Hz and a sound pressure of 4 dB or more as compared with the speaker of the related art.
  • the present invention can be applied to various speakers.

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Acoustics & Sound (AREA)
  • Signal Processing (AREA)
  • Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)

Abstract

The present invention relates to a speaker wherein, in configuring the magnetic circuit of the speaker, the vertically-oriented polarity arrangement of the prior art is not adhered to in that the polarity of the magnet is formed with a horizontal orientation, and a vibration system is formed inside the magnetic circuit formed with the horizontal orientation. Consequently, because the magnetic circuit surrounds the vibration system, it is possible to produce a speaker that has only the height of the magnetic circuit, which contrasts with speakers of the prior art which have been formed to a height comprising the sum of the thicknesses of the magnetic circuit and the vibration system. Also, the acoustic characteristics of the speaker can be improved because the height of the speaker can be reduced even if the volume of the magnet is large.

Description

스피커speaker

본 발명은 스피커에 관한 것으로서, 보다 상세하게는, 높이가 현저히 낮으면서도 우수한 성능을 가지는 스피커에 관한 것이다.TECHNICAL FIELD The present invention relates to a speaker, and more particularly, to a speaker having excellent performance while having a significantly low height.

일반적으로, 스피커는 전기 신호를 우리가 들을 수 있는 소리로 변환해 주는 장치를 말한다. 한편, 스피커 중에서 마이크로 스피커는 소형 전자기기나 이동통신 단말기 등에 장착하기 적합한 스피커를 말한다.In general, speakers are devices that convert electrical signals into sounds that we can hear. Meanwhile, among the speakers, the micro speaker refers to a speaker suitable for mounting in a small electronic device or a mobile communication terminal.

현재 전자기기는 점점 더 작고 가벼워 지는 추세이다. 따라서, 전자기기에 적용되는 스피커 역시 더 작고 가벼우면서도 우수한 성능을 필요로 하게 되었다. At present, electronic devices are becoming smaller and lighter. Therefore, the speakers applied to electronic devices also need to be smaller, lighter and better performance.

도 1 및 도 2 는 종래 기술에 따른 단일 마그네트(magnet) 스피커를 나타낸 단면도이다. 도 1 에 도시된 바와 같이, 종래 기술에 따른 스피커는, 프레임(111)이 스피커(120)의 외형을 형성한다. 프레임(111) 안쪽으로는 마그네트(101)에 의해 발생한 자속의 통과 경로를 제공하는 요크(yoke)(104)가 구비된다. 요크(104)는 아래쪽이 막힌 원통 형상의 바텀 플레이트(bottom plate)(102)와 원반 형상의 탑 플레이트(top plate)(103)로 이루어진다. 바텀 플레이트(102)와 탑 플레이트(103)의 사이에는 원반형의 마그네트(101)가 놓인다. 한편, 마그네트(101)에 의해 발생한 자속이 요크(104)에 유도되다가 요크(104)의 불연속점을 만나게 되는데, 이를 자기 갭(magnetic gap)이라고 한다. 1 and 2 are cross-sectional views showing a single magnet speaker according to the prior art. As shown in FIG. 1, in the speaker according to the related art, the frame 111 forms the outer shape of the speaker 120. A yoke 104 is provided inside the frame 111 to provide a passage path for the magnetic flux generated by the magnet 101. The yoke 104 is composed of a cylindrical bottom plate 102 and a disc shaped top plate 103 with a closed bottom. A disc shaped magnet 101 is placed between the bottom plate 102 and the top plate 103. On the other hand, the magnetic flux generated by the magnet 101 is guided to the yoke 104 and meets the discontinuous point of the yoke 104, which is called a magnetic gap.

도 2 에 도시된 바와 같이, 마그네트(101), 요크(104) 및 자기 갭이 자기회로를 형성한다. 자기회로란 스피커가 전기신호를 소리로 변환하기 위해 필요한 자기장(magnetic field)을 제공하는 장치를 말한다. As shown in FIG. 2, the magnet 101, the yoke 104 and the magnetic gap form a magnetic circuit. Magnetic circuits are devices that provide the magnetic fields needed by speakers to convert electrical signals into sound.

한편, 자기 갭에는 보이스 코일(voice coil)(105)이 위치한다. 보이스 코일(105)은 다이어프램(diaphragm)(106)에 연결되어 있다. 보이스 코일(105)에 인가된 전기 신호에 따라 보이스 코일(105)이 상하 운동을 하면, 이러한 운동은 다이어프램(106)에 전달되고, 다이어프램(106)이 진동함으로써, 전기신호가 소리로 변환된다. 도 1 에 도시된 바와 같이, 다이어프램(106)은 중앙부의 돔과 가장 자리의 립(Rib) 형상으로 이루어지며, 두개의 돔 사이의 경계에 보이스 코일(105)이 연결되어 있다. 다이어프램(106)을 이중 돔 형상으로 하는 이유는, 다이어프램(106)의 진동을 원활하게 하면서도 진동 범위를 제어하기 위함이다. On the other hand, a voice coil 105 is located in the magnetic gap. The voice coil 105 is connected to a diaphragm 106. When the voice coil 105 moves up and down in accordance with the electrical signal applied to the voice coil 105, this movement is transmitted to the diaphragm 106, and the diaphragm 106 vibrates, whereby the electrical signal is converted into sound. As shown in FIG. 1, the diaphragm 106 has a central dome and an edge rib shape, and a voice coil 105 is connected to a boundary between two domes. The reason why the diaphragm 106 has a double dome shape is to control the vibration range while smoothing the vibration of the diaphragm 106.

리드 와이어(lead wire)(107)는 보이스 코일(105)에 연결되어 전기 신호를 인가한다. 리드와이어(107)는 일반적으로 다이어프램(106)의 표면을 따라 접착되어 있으며, 프레임(111)에 형성된 홀(hole)을 통과하여 터미널 PCB(108)에 연결된다. A lead wire 107 is connected to the voice coil 105 to apply an electrical signal. The leadwire 107 is generally bonded along the surface of the diaphragm 106 and is connected to the terminal PCB 108 through a hole formed in the frame 111.

도 2 에 도시된 바와 같이, 다이어프램(106)과 보이스 코일(105)은 진동계(132)를 형성한다. As shown in FIG. 2, the diaphragm 106 and the voice coil 105 form a vibrometer 132.

다이어프램(106) 위쪽으로는 통공 캡(109)을 덮는다. 통공 캡(109)은 다이어프램(106)을 비롯한 스피커 내부 장치들을 보호하기 위한 것이다. 그리고, 다이어프램(106)에 의해 발생된 소리가 스피커 밖으로 잘 전달되도록 하기 위해, 통공 캡(109)에는 다수의 통공(110)을 형성한다. 한편, 스피커 안쪽에 발생하는 열기가 밖으로 배출되도록, 프레임(111)에 열 방출구(112)를 다수 형성한다.The through cap 109 is covered above the diaphragm 106. The through cap 109 is for protecting devices inside the speaker, including the diaphragm 106. In addition, in order for the sound generated by the diaphragm 106 to be well transmitted to the outside of the speaker, the through cap 109 is formed with a plurality of through holes 110. Meanwhile, a plurality of heat dissipation openings 112 are formed in the frame 111 so that heat generated inside the speaker is discharged outward.

종래 기술에 의한 스피커는 다음과 같이 동작한다. 터미널 PCB(108) 및 리드 와이어(107)를 통해 보이스 코일(105)에 전기 신호가 인가되면, 자기 갭(magnetic gap) 안에 위치한 보이스 코일(105)이 플레밍 법칙에 의해 자기장과 수직한 방향으로 운동을 하고, 이러한 운동이 다이어프램(106)에 전달된다. 다이어프램(106)에 전달된 운동은 다이어프램(106)을 진동시킴으로써, 전기 신호가 소리로 변환된다. The speaker according to the prior art operates as follows. When an electrical signal is applied to the voice coil 105 via the terminal PCB 108 and the lead wire 107, the voice coil 105 located in the magnetic gap moves in a direction perpendicular to the magnetic field by the Fleming law. This movement is transmitted to the diaphragm 106. The motion transmitted to the diaphragm 106 vibrates the diaphragm 106, whereby the electrical signal is converted into sound.

도 1 및 도 2 에 따른 종래기술의 스피커에는 다음과 같은 문제점들이 있다. 먼저, 종래 기술에 따른 스피커는 자기회로(131)와 진동계(132)가 수직으로 층을 이루고 있으므로, 스피커의 전체 높이가 높아지는 문제점 있었다. 즉, 스피커의 전체 높이는 자기회로의 두께와 진동계의 두께를 더한 값으로 결정되었다.The speaker of the prior art according to FIGS. 1 and 2 has the following problems. First, in the speaker according to the prior art, since the magnetic circuit 131 and the vibrometer 132 are vertically layered, there is a problem that the overall height of the speaker increases. That is, the overall height of the speaker was determined by adding the thickness of the magnetic circuit and the thickness of the vibration system.

따라서, 스피커의 두께를 보다 얇게 하기 위해는 마그네트(101)의 두께를 줄일 수 밖에 없었다. 그러나, 마그네트(101)의 두께를 줄이게 되면, 자기 갭의 자속밀도(magnetic flux density)가 줄어들게 됨으로써, 결국 스피커의 음압이 낮아지는 문제점이 발생하였다. Therefore, in order to make the thickness of the speaker thinner, the thickness of the magnet 101 has to be reduced. However, when the thickness of the magnet 101 is reduced, the magnetic flux density of the magnetic gap is reduced, resulting in a lower sound pressure of the speaker.

또한, 스피커(120) 두께로 인해, 전자 모듈(module) PCB 기판 에서 분리 조립을 하고 있어 제조 과정의 효율이 떨어질 뿐 아니라, 많은 부품으로 인해 조립 시간의 늘어나고, 결국 이는 제조 원가가 높아지는 문제점이 있었다. In addition, due to the thickness of the speaker 120, the separate assembly in the electronic module (PCB) PCB board not only reduces the efficiency of the manufacturing process, but also increases the assembly time due to many components, which eventually has a problem that the manufacturing cost increases. .

도 3 은 종래 기술에 따른 더블 마그네트 스피커를 나타낸 단면도이다. 도 3 에 나타낸 스피커는 중앙에 원반 형상의 제 1 마그네트(141)와, 제 1 마그네트와 중심을 공유하는 링 형상의 제 2 마그네트(142)를 구비한다. 3 is a cross-sectional view showing a double magnet speaker according to the prior art. The speaker shown in FIG. 3 has a disk shaped first magnet 141 and a ring-shaped second magnet 142 sharing a center with the first magnet.

제 1 마그네트(141)와 제 2 마그네트(142)는 하나의 바텀 플레이트(143)위에 구비된다. 한편, 제 1 마그네트는 제 1 탑 플레이트(144)로 덮혀있고, 제 2 마그네트는 제 2 탑 플레이트(145)로 덮혀 있다. 제 1 탑플레이트(144)와 제 2 탑 플레이트(145) 사이에는 자기 갭(magnetic gap)이 형성된다. 또한, 바텀 플레이트(143)와 제 1 탑플레이트(144) 및 제 2 탑 플레이트(145)는 자속의 통과 경로를 제공하는 요크(146)를 형성한다. The first magnet 141 and the second magnet 142 are provided on one bottom plate 143. Meanwhile, the first magnet is covered with the first top plate 144, and the second magnet is covered with the second top plate 145. A magnetic gap is formed between the first top plate 144 and the second top plate 145. In addition, the bottom plate 143, the first top plate 144, and the second top plate 145 form a yoke 146 that provides a passage path for the magnetic flux.

도 3 에 따른 더블 마그네트 스피커 역시 자기회로와 진동계가 층을 이루고 있으므로, 스피커 전체의 두께를 줄이기 위해서는 제 1 마그네트(141)와 제 2 마그네트(142)의 두께를 줄일 수 밖에 없다. 따라서, 단일 마그네트 스피커와 같이, 음압이 낮아지는 문제가 발생할 뿐 아니라, 복잡한 구조로 인해 제조 비용이 상승하는 문제점이 있었다. Since the double magnet speaker according to FIG. 3 also has a magnetic circuit and a vibrometer, the thickness of the first magnet 141 and the second magnet 142 can be reduced to reduce the thickness of the entire speaker. Therefore, as with a single magnet speaker, not only the sound pressure is lowered, but also the manufacturing cost increases due to the complicated structure.

도 4 는 네비게이션 및 휴대용 게임기에 적용되는 종래 기술에 따른 스피커를 나타낸 단면도이다. 도 4 에 나타낸 스피커 역시 도 1 과 같은 방식의 스피커이다. 다만, 생산성 향상을 위해, 바텀 플레이트(151)를 프레임으로 사용하였다. 또한, 도 4 에 도시된 스피커는 스피커 자체의 두께를 줄이기 위해, 진동계를 얇게 형성하였다. 4 is a cross-sectional view showing a speaker according to the prior art applied to a navigation and a portable game machine. The speaker shown in FIG. 4 is also a speaker of the same method as FIG. 1. However, in order to improve productivity, the bottom plate 151 was used as a frame. In addition, in order to reduce the thickness of the speaker itself, the speaker illustrated in FIG. 4 has a thin vibration system.

그러나, 도 4 에 도시된 스피커는 보이스 코일(152)가 자계에서 많이 벗어나 있어서 주파수 대역의 손실을 발생시킨다. 즉, 최저 재생 한계 주파수(f0)가 높아지는 문제점이 있다. However, in the speaker shown in FIG. 4, the voice coil 152 deviates much from the magnetic field, causing loss of frequency band. That is, there is a problem in that the lowest reproduction limit frequency f0 becomes high.

또한, 고출력을 내기 위해서는 굵은 보이스 코일(152)을 사용해야 하는데, 보이스 코일(152)의 외경이 적어, 권폭이 증가하게 되고, 보이스 코일 (152)이 상하 왕복 운동 시 X - MAX 값(정격 출력 시 코일의 상하 운동폭 : mm) 때문에 자기회로의 높이가 높아지는 문제점 있다. 또한, 자기회로의 자기력 약화로 보이스음색의 명료도 및 해상력 부족과 음압이 떨어지는 문제점이 있다. In addition, a thick voice coil 152 should be used to produce a high output, and the outer diameter of the voice coil 152 is small, so that the winding width is increased, and the X-MAX value when the voice coil 152 is reciprocated up and down (at rated output). Due to the vertical movement width of the coil (mm), the height of the magnetic circuit is increased. In addition, there is a problem of lack of clarity, resolution and sound pressure of the voice tone due to the weakening of the magnetic force of the magnetic circuit.

도 5 는 종래 기술에 따른 내자형 및 외자형 자기회로를 나타낸 단면도이다. 도 5 의 (가)는 종래의 내자형 자기회로 구성을 보여주는 단면도 이며, (나)는 종래의 외자형 자기회로 구성을 보여주는 단면도 이다. 5 is a cross-sectional view showing a magnetic and magnetic magnetic circuits according to the prior art. 5 (a) is a cross-sectional view showing a conventional magnetic magnetic circuit configuration, (b) is a cross-sectional view showing a conventional magnetic magnetic circuit configuration.

도 5 의 (가)는 마그네트(161)가 요크(164)의 내측에 있으므로, 이를 내자형 자기회로라고 한다. 여기서, 요크(164)는 바텀 플레이트(162)와 탑 플레이트(163)로 이루어지고, 상기 화살표 방향은 마그네트(161)에 의해 형성된 자속의 통과 경로를 나타낸다. In FIG. 5A, since the magnet 161 is inside the yoke 164, this is called a magnetic magnetic circuit. Here, the yoke 164 includes a bottom plate 162 and a top plate 163, and the arrow direction indicates a passage path of the magnetic flux formed by the magnet 161.

도 5 의 (나)는 마그네트(171)가 바텀 플레이트(172)에 연결된 폴피스(pole piece)(175) 외측에 있는 구조를 가지므로 외자형 자기회로라고 한다. 도 5 의 (나)에 표시된 화살표 방향은 마그네트(171)에 의해 형성된 자속의 통과 경로를 나타낸다.5B is referred to as an external magnetic circuit because the magnet 171 has a structure outside the pole piece 175 connected to the bottom plate 172. The arrow direction shown in (b) of FIG. 5 indicates a passage path of the magnetic flux formed by the magnet 171.

상기한 바와 같이, 종래 기술에 따른 스피커는 바텀 플레이트, 마그네트, 탑 플레이트를 적층하여 자기 회로를 구성하고, 그 위에 진동계를 구성함으로써, 스피커의 높이가 높아지는 문제점이 있었다.As described above, the speaker according to the prior art has a problem in that the height of the speaker is increased by stacking a bottom plate, a magnet, and a top plate to form a magnetic circuit, and by constructing a vibrometer thereon.

본 발명은 상기한 바와 같이 종래 기술의 문제점을 해결하기 위한 것으로, 스피커의 높이를 현저히 줄이면서도 음향특성을 향상시킨 스피커를 제공하는데 그 목적이 있다. The present invention is to solve the problems of the prior art as described above, it is an object of the present invention to provide a speaker that improves the acoustic characteristics while significantly reducing the height of the speaker.

상기와 같은 목적을 달성하기 위해, 본 발명은, 스피커의 자기회로를 구성함에 있어서, 종래 기술의 수직방향의 극성 배열과는 달리, 마그네트의 극성을 수평 방향으로 형성하고, 수평 방향으로 형성된 자기회로 내측에 진동계를 형성한다.In order to achieve the above object, the present invention, in the configuration of the magnetic circuit of the speaker, unlike the polarity arrangement in the vertical direction of the prior art, the magnetic circuit formed in the horizontal direction, forming the polarity of the magnet in the horizontal direction A vibrometer is formed inside.

본 발명에 따른 마이크로 스피커는 다음과 같은 효과를 가진다.The micro speaker according to the present invention has the following effects.

첫째, 자기력을 증대시켜 높은 출력 음압을 제공할 수 있다.First, it can increase the magnetic force to provide high output sound pressure.

둘째, 스피커의 높이를 최대한 줄임으로써, 스피커를 장착한 전자기기의 크기를 줄일 수 있다. Second, by reducing the height of the speaker as much as possible, it is possible to reduce the size of the electronic device equipped with the speaker.

셋째, 보이스 코일 구경이 커서 종래의 보이스 코일 굵기 보다 더 굵은 와이어 사용할 수 있게 되므로, 고입력, 고출력 스피커를 제조할 수 있다.Third, since the voice coil diameter is large, a wire thicker than the conventional voice coil thickness can be used, and thus a high input and high output speaker can be manufactured.

넷째, 스피커 부품의 수가 감소되어 마이크로 스피커의 조립 작업을 단순화 할 수 있고, 생산을 자동화하여 생산 비용을 절감할 수 있는 효과가 있다. Fourth, the number of speaker parts can be reduced to simplify the assembly work of the micro-speakers, and the production cost can be reduced by automating the production.

다섯째, 저면부측에 통공부가 형성되어 있기 때문에, 보이스 코일 에서 발생하는 열이 바로 방출될 수 있고, 내구성을 향상시킬 수 있다.Fifth, since the through portion is formed on the bottom surface side, heat generated in the voice coil can be immediately released, and durability can be improved.

일곱째, 음압은 높이면서도 강한 다이어프램을 사용해 f0 를 낮출 수 있다.Seventh, the sound pressure can be increased, but the strong diaphragm can be used to lower f0.

여덟째, 소형 휴대기기 제조업체의 전자 PCB 모듈과 조립을 같이 할 수 있어 생산성이 향상되는 효과가 있다.Eighth, it is possible to assemble together with the electronic PCB module of a small portable device manufacturer has the effect of improving productivity.

도 1 및 도 2 는 종래 기술에 따른 단일 마그네트 스피커를 나타낸 단면도이다.1 and 2 are cross-sectional views showing a single magnet speaker according to the prior art.

도 3 은 종래 기술에 따른 더블 마그네트 스피커를 나타낸 단면도이다.3 is a cross-sectional view showing a double magnet speaker according to the prior art.

도 4 는 네비게이션 및 휴대용 게임기에 적용되는 종래 기술에 따른 스피커를 나타낸 단면도이다.4 is a cross-sectional view showing a speaker according to the prior art applied to a navigation and a portable game machine.

도 5 는 종래 기술에 따른 내자형 및 외자형 자기회로를 나타낸 단면도이다. 5 is a cross-sectional view showing a magnetic and magnetic magnetic circuits according to the prior art.

도 6 은 본 발명에 따른 스피커의 자기회로를 나타낸 일실시예 단면도이다. 6 is a cross-sectional view of an embodiment of a magnetic circuit of a speaker according to the present invention.

도 7 은 본 발명에 따른 스피커의 제 1 실시예를 나타낸 단면도이다.7 is a sectional view showing a first embodiment of a speaker according to the present invention.

도 8 은 본 발명에 따른 스피커의 제 2 실시예를 나타낸 단면도이다.8 is a sectional view showing a second embodiment of a speaker according to the present invention.

도 9 는 본 발명에 따른 스피커의 제 3 실시예를 나타낸 단면도이다.9 is a sectional view showing a third embodiment of a speaker according to the present invention.

도 10 은 본 발명에 따른 스피커의 제 1 실시예를 나타낸 분해사시도이다. 10 is an exploded perspective view showing a first embodiment of a speaker according to the present invention.

도 11 은 본 발명에 따른 스피커의 제 3 실시예를 나타낸 분해사시도이다. 11 is an exploded perspective view showing a third embodiment of a speaker according to the present invention.

도 12 는 본 발명의 제 1 실시예에 따른 스피커의 성능을 종래 기술에 따른 스피커의 성능과 비교한 그래프이다.12 is a graph comparing the performance of the speaker according to the first embodiment of the present invention with the performance of the speaker according to the prior art.

도 13 은 본 발명의 제 3 실시예에 따른 스피커의 성능을 종래 기술에 따른 스피커의 성능과 비교한 그래프이다.13 is a graph comparing the performance of the speaker according to the third embodiment of the present invention with the performance of the speaker according to the prior art.

본 발명에 따른 스피커는, 자기회로와 진동계를 포함하여 이루어지되, 상기 자기회로는, 링 형상을 가지며, 상기 링의 중심을 기준으로, 외측면에는 제 1 극성을 가지고, 내측면에는 상기 제 1 극성과 반대되는 제 2 극성을 가지는 마그네트 및 상기 마그네트로부터 발생하는 자속의 통과 경로를 제공하는 요크를 포함하여 이루어진다.The speaker according to the present invention includes a magnetic circuit and a vibrometer, wherein the magnetic circuit has a ring shape, based on the center of the ring, has a first polarity on the outer surface, and the first surface on the inner surface. A magnet having a second polarity opposite to the polarity and a yoke that provides a passage path for the magnetic flux generated from the magnet.

상술한 목적, 특징들 및 장점은 첨부된 도면과 관련한 다음의 상세한 설명을 통하여 보다 분명해 질 것이다. 이하 첨부된 도면을 참조하여 본 발명에 따른 바람직한 실시예를 상세히 설명한다. The above objects, features and advantages will become more apparent from the following detailed description taken in conjunction with the accompanying drawings. Hereinafter, exemplary embodiments of the present invention will be described in detail with reference to the accompanying drawings.

도 6 은 본 발명에 따른 스피커의 자기회로를 나타낸 일실시예 단면도이다. 도 6 에 따른 자기회로는 마그네트의 N 극과 S 극이 수평하게 형성된다. 종래기술에 따른 스피커의 자기회로에 있어서는, 도 5 에 도시된 바와 같이, 마그네트는 N 극과 S 극이 수직으로 형성되고, 자기 갭에서만 자속이 수평하게 형성된다. 그러나, 본 발명에 따른 자기회로는 N 극과 S 극이 수평으로 형성되고, 자기 갭에서도 자속이 수평하게 형성된다. 6 is a cross-sectional view of an embodiment of a magnetic circuit of a speaker according to the present invention. In the magnetic circuit of FIG. 6, the N pole and the S pole of the magnet are formed horizontally. In the magnetic circuit of the speaker according to the prior art, as shown in Fig. 5, the magnet is formed with the N pole and the S pole vertically, the magnetic flux is formed horizontally only in the magnetic gap. However, in the magnetic circuit according to the present invention, the N pole and the S pole are formed horizontally, and the magnetic flux is formed horizontally even in the magnetic gap.

도 6 (a) 는 본 발명에 따른 스피커의 자기회로에 있어서, 두개의 플레이트를 가지는 실시예를 나타낸 것이다. 도 6 (a)를 참조하면, 본 실시예에 따른 마그네트(501)는 링 형상으로서, 외측에서 내측으로 단차를 가진다. 또한, 마그네트(501)의 극성은 내측이 S 극이고 외측이 N 극으로 형성된다. 즉, N 극과 S 극이 수평하게 형성된다. 한편, 내측에 N 극이 위치하고, 외측에 S 극이 위치하도록 수평하게 형성될 수도 있음은 자명하다. Figure 6 (a) shows an embodiment having two plates in the magnetic circuit of the speaker according to the present invention. Referring to FIG. 6 (a), the magnet 501 according to the present embodiment has a ring shape and has a step from the outside to the inside. In addition, the polarity of the magnet 501 is formed as the S pole on the inside and the N pole on the outside. That is, the N pole and the S pole are formed horizontally. On the other hand, it is obvious that the N pole is located on the inner side, it may be formed horizontally so that the S pole on the outside.

도 6 (a) 와 같이, 마그네(501)트의 외측에 N 극이 위치한 경우, 자속(magnetic flux)은 N 극에서 시작하여 제 1 플레이트(502)와 자기 갭(505) 및 제 2 플레이트(503)를 통과하여 마그네트(501)의 S 극으로 향한다. 제 1 플레이트(502) 및 제 2 플레이트(503)는 자속의 통과 경로를 제공하는 요크(504)의 역할을 한다. 이때, 마그네트(501)가 제 1 플레이트(501)에 밀착되도록 자기회로를 구성할 수도 있다. 그러나, 도 6 (a) 에 도시된 바와 같이, 마그네트(501)가 제 1 플레이트(501)와 일정한 거리만큼 이격되도록 자기회로를 구성할 수도 있다. As shown in FIG. 6A, when the N pole is located outside the magnet 501, the magnetic flux starts at the N pole, and the first plate 502, the magnetic gap 505, and the second plate ( Pass 503 to the S pole of the magnet 501. The first plate 502 and the second plate 503 serve as yokes 504 that provide a passage path for the magnetic flux. In this case, the magnetic circuit may be configured such that the magnet 501 is in close contact with the first plate 501. However, as shown in FIG. 6A, the magnetic circuit may be configured such that the magnet 501 is spaced apart from the first plate 501 by a predetermined distance.

도 6 (b) 는 본 발명에 따른 스피커의 자기회로에 있어서, 하나의 플레이트를 가지는 실시예를 나타낸 것이다. 도 6 (b)를 참조하면, 본 실시예에 따른 마그네트(601)는 링 형상으로서, 외측에서 내측으로 단차를 가진다. 또한, 마그네트(601)의 극성은 내측이 S 극이고 외측이 N 극으로 형성된다. 즉, N 극과 S 극이 수평하게 형성된다. 한편, 내측에 N 극이 위치하고, 외측에 S 극이 위치하도록 수평하게 형성될 수도 있음은 자명하다. Figure 6 (b) shows an embodiment having one plate in the magnetic circuit of the speaker according to the present invention. Referring to FIG. 6 (b), the magnet 601 according to the present embodiment has a ring shape and has a step from the outside to the inside. In addition, the polarity of the magnet 601 is formed as the S pole on the inside and the N pole on the outside. That is, the N pole and the S pole are formed horizontally. On the other hand, it is obvious that the N pole is located on the inner side, it may be formed horizontally so that the S pole on the outside.

도 6 (b) 와 같이, 마그네트(601)의 외측에 N 극이 위치한 경우, 자속(magnetic flux)은 N 극에서 시작하여 요크(602)와 자기 갭(605)을 통과하여 마그네트(601)의 S 극으로 향한다. 요크(602)는 자속의 통과 경로를 제공한다. 이때, 도 6 (b) 에 도시된 바와 같이, 마그네트(601)가 요크(602)에 밀착되도록 자기회로를 구성할 수도 있고, 요크(602)와 일정한 거리만큼 이격되도록 자기회로를 구성할 수도 있다. As shown in FIG. 6 (b), when the N pole is located outside the magnet 601, the magnetic flux starts at the N pole and passes through the yoke 602 and the magnetic gap 605 to the magnet 601. Head to the S pole. Yoke 602 provides a path for passage of magnetic flux. At this time, as shown in Figure 6 (b), the magnetic circuit may be configured such that the magnet 601 is in close contact with the yoke 602, or may be configured to be spaced apart from the yoke 602 by a predetermined distance. .

도 7 은 본 발명에 따른 스피커의 제 1 실시예를 나타낸 단면도이다. 본 실시예는 도 6 (a) 에서 설명한 형태의 자기회로를 적용한 스피커에 관한 것이다. 본 실시예에 따른 스피커의 자기회로는 수평하게 N 극과 S 극이 형성된 마그네트(701)와, 제 1 플레이트(702), 제 2 플레이트(703) 및 제 1 플레이트(702)와 제 2 플레이트(703) 사이에 형성된 자기 갭(705)을 포함하여 이루어진다. 7 is a sectional view showing a first embodiment of a speaker according to the present invention. This embodiment relates to a speaker to which a magnetic circuit of the type described in Fig. 6A is applied. The magnetic circuit of the speaker according to the present embodiment includes a magnet 701 having horizontally formed N poles and S poles, a first plate 702, a second plate 703, and a first plate 702 and a second plate ( And a magnetic gap 705 formed between 703.

마그네트(701)는 외측에서 내측으로 단차를 가지는 링 형상인 것이 바람직하다. 이때, 링 형상은 원형의 링 뿐 아니라, 사각이나 타원 형태의 링 형상을 포함한다. The magnet 701 is preferably a ring shape having a step from the outside to the inside. In this case, the ring shape includes not only a circular ring but also a ring shape having a square or ellipse shape.

마그네트(701)의 외측이 N 극을 형성하는 경우의 예를 들면, 마그네트(701)에서 발생하는 자속은 제 1 플레이트(702)를 통과하여 자기 갭(705)와 제 2 플레이트(703)를 거쳐 마그네트(701)의 내측에 형성된 S 극으로 이어진다. 따라서, 제 1 플레이트(702) 및 제 2 플레이트(703)는 자속의 통과 경로를 제공하는 요크(yoke)(704)의 기능을 수행한다. For example, in the case where the outside of the magnet 701 forms the N pole, the magnetic flux generated in the magnet 701 passes through the first plate 702 and passes through the magnetic gap 705 and the second plate 703. It leads to the S pole formed inside the magnet 701. Thus, the first plate 702 and the second plate 703 perform the function of a yoke 704 to provide a passage path for the magnetic flux.

한편, 본 실시예에 따른 스피커의 진동계는 자기 갭(705)에 위치한 보이스 코일(706)과 다이어프램(707)으로 이루어진다. 보이스 코일(706)은 다이어프램(707) 및 에지부(edge part)(708)에 연결되며, 다이어프램(707)은 중앙부에 돔 형상을 가지고 가장자리에는 립 형상을 가지는 이중 돔 형상인 것이 바람직하다. 에지부(708)는 보이스 코일(706)을 지지할 뿐 아니라, 다이어프램(707)의 움직임을 원할하게 하고, 다이어프램의 진동이 일정한 범위를 넘지 않도록 제어하는 기능을 수행한다. 보이스 코일(706)은 전기 신호를 입력 받기 위해 리드 와이어(709)에 연결되며, 리드 와이어(709)는 터미털 PCB(710)에 연결된다. 외부의 앰프 신호는 터미널 PCB(710)을 통해 스피커로 전달된다.On the other hand, the vibration system of the speaker according to the present embodiment is composed of a voice coil 706 and a diaphragm 707 located in the magnetic gap 705. The voice coil 706 is connected to the diaphragm 707 and the edge part 708, the diaphragm 707 is preferably a double dome shape having a dome shape at the center and a lip shape at the edge. The edge portion 708 not only supports the voice coil 706, but also facilitates the movement of the diaphragm 707 and performs a function of controlling the vibration of the diaphragm not to exceed a predetermined range. The voice coil 706 is connected to the lead wire 709 to receive an electrical signal, the lead wire 709 is connected to the terminal PCB 710. The external amplifier signal is delivered to the speaker via the terminal PCB 710.

다이어프램(707) 위쪽으로는 통공 캡(711)을 덮는다. 통공 캡(711)은 다이어프램(707)을 비롯한 스피커 내부 장치들을 보호하기 위한 것이다. 그리고, 다이어프램(707)에 의해 발생된 소리가 스피커 밖으로 잘 전달되도록 하기 위해, 통공 캡(711)에는 다수의 통공을 형성한다. 저면부(712)는 제 1 플레이트(702) 저면에 부착되는데, 이물질이 스피커 내부로 유입되지 않도록 필터링 하는 역할을 할 뿐 아니라, 스피커 내부의 열을 외부로 방출시키는 역할을 한다. The through cap 711 is covered above the diaphragm 707. The through cap 711 is for protecting devices inside the speaker, including the diaphragm 707. In addition, in order for the sound generated by the diaphragm 707 to be transmitted to the outside of the speaker, the through cap 711 forms a plurality of through holes. The bottom portion 712 is attached to the bottom of the first plate 702, and serves to filter foreign matter from entering the speaker, as well as to release heat inside the speaker to the outside.

상기와 같이, 본 발명에 따른 스피커는, 링 형상의 마그네트의 높이(또는 자기회로의 높이)가 스피커의 높이를 결정하게 되므로, 종래 기술에 비해 두께가 현저히 줄어든 스피커를 제공한다. 즉, 종래 기술의 스피커에 따르면, 자기회로 위쪽에 진동계가 형성되므로, 스피커의 두께는 자기회로의 높이와 진동계의 높이를 합한 것이 된다. 그러나, 본 발명에 따르면, 진동계는 자기회로에 둘러싸여 있게 되므로, 자기회로의 높이로 스피커의 두께가 결정된다. 따라서, 진동계의 높이만큼 스피커의 두께가 줄어들게 된다. 나아가, 자기회로의 자기장의 세기는 마그네트의 부피에 의존하는데, 본 발명에 따른 스피커는 마그네트가 스피커의 외경을 이루게 되므로, 마그네트의 두께를 줄이면서도 부피를 유지할 수 있게 되어, 자기회로의 높이마저 줄일 수 있게 된다. As described above, the speaker according to the present invention, since the height of the ring-shaped magnet (or the height of the magnetic circuit) determines the height of the speaker, provides a speaker that is significantly reduced in thickness compared to the prior art. That is, according to the speaker of the prior art, since the vibration system is formed above the magnetic circuit, the thickness of the speaker is the sum of the height of the magnetic circuit and the height of the vibration system. However, according to the present invention, since the vibrometer is surrounded by the magnetic circuit, the thickness of the speaker is determined by the height of the magnetic circuit. Therefore, the thickness of the speaker is reduced by the height of the vibration system. Furthermore, the strength of the magnetic field of the magnetic circuit is dependent on the volume of the magnet, the speaker according to the present invention can maintain the volume while reducing the thickness of the magnet, since the magnet is made of the outer diameter of the speaker, reducing the height of the magnetic circuit It becomes possible.

또한, 요크가 스피커의 외형을 형성하는 프레임의 기능을 하게 됨에 따라, 별도의 프레임이 생략되므로 그만큼 자기회로의 크기를 크게 할 수 있게 된다.In addition, as the yoke functions as a frame forming the outer shape of the speaker, a separate frame is omitted, thereby increasing the size of the magnetic circuit.

표 1 은 종래 기술의 자기 회로에 있어서 요크에 형성되는 자속밀도(magnetic flux density)와 본 발명의 제 1 실시예에 따른 스피커의 요크에 형성되는 자속밀도를 비교한 것이다. Table 1 compares the magnetic flux density formed in the yoke in the magnetic circuit of the prior art with the magnetic flux density formed in the yoke of the speaker according to the first embodiment of the present invention.

표 1 극성 최대가우스 종래기술 N 극 500 S 극 1000 본 발명 N 극 2200 S 극 2500 Table 1 polarity Gaussian maximum Prior art N pole 500 S pole 1000 The present invention N pole 2200 S pole 2500

표 1 을 참조하면, 본 발명의 제 1 실시예에 따른 자기회로는 종래 기술에 따른 자기회로에 비해 2 배 이상의 자속밀도를 가진다는 것을 알 수 있다. Referring to Table 1, it can be seen that the magnetic circuit according to the first embodiment of the present invention has twice the magnetic flux density as compared to the magnetic circuit according to the prior art.

스피커 자기회로부에 있어서, 진동계의 질량(보이스 코일의 무게 + 다이어프램의 무게)이 일정하다고 할 때, 본 발명에 따른 스피커는 매우 큰 자기장의 세기를 바탕으로 음압을 한층 향상시킬 수 있다는 것을 알 수 있다. In the speaker magnetic circuit section, when the mass of the vibration system (weight of the voice coil + weight of the diaphragm) is constant, it can be seen that the speaker according to the present invention can further improve the sound pressure based on the strength of a very large magnetic field. .

표 2 는 종래 기술에 따른 스피커와 본 발명의 제 1 실시예에 따른 스피커의 성능을 비교한 것이다. Table 2 compares the performance of the speaker according to the prior art and the speaker according to the first embodiment of the present invention.

표 2 다이어프램 두께 코일 굵기 임피던스(Ω) 음압(db) 종래기술 10 micron φ40 micron 7.4 90 본발명 20 micron φ60 micron 6.8 96 TABLE 2 Diaphragm thickness Coil thickness Impedance (Ω) Sound pressure (db) Prior art 10 micron φ40 micron 7.4 90 Invention 20 micron φ60 micron 6.8 96

표 2 를 참조하면, 종래 기술에 따른 스피커의 다이어프램의 두께와 본 발명의 제 1 실시예에 따른 다이어프램의 두께는 10 미크론(micron)의 차이가 나지만 음압에 있어서는 상당한 차이를 보인다는 것을 알 수 있다. Referring to Table 2, it can be seen that the thickness of the diaphragm of the speaker according to the prior art and the thickness of the diaphragm according to the first embodiment of the present invention are different from each other by 10 microns, but there is a significant difference in sound pressure. .

또한, 종래 기술에 따른 보이스 코일은 φ 40 미크론(micron)의 선경을 가지므로 일반적으로 고출력을 낼 수 없으나, 본 발명의 제 1 실시예에서는 더 굵은 코일 와이어를 사용함으로써 음압을 더 높일 수 있다는 것을 나타내고 있다. In addition, since the voice coil according to the prior art has a wire diameter of φ 40 microns, it is generally not able to produce a high output, but in the first embodiment of the present invention, it is possible to further increase the sound pressure by using a thicker coil wire. It is shown.

이때, 자기갭의 크기는 N 극(또는 S극)과 내경 코일과의 갭은 0.23 mm 로 하는 것이 바람직하다. 또한, S 극(또는 N극)과 외경 코일과의 갭 또한 0.23 mm 로 하는 것이 바람직하다. At this time, it is preferable that the size of the magnetic gap is 0.23 mm in the gap between the N pole (or S pole) and the inner diameter coil. In addition, the gap between the S pole (or N pole) and the outer diameter coil is also preferably set to 0.23 mm.

도 8 은 본 발명에 따른 스피커의 제 2 실시예를 나타낸 단면도이다. 본 실시예는 도 6 (b) 에서 설명한 형태의 자기회로를 적용한 스피커에 관한 것이다. 본 실시예에 따른 스피커의 자기회로는 수평하게 N 극과 S 극이 형성된 마그네트(801), 요크(804), 및 요크(804)와 마그네트(801) 사이에 형성된 자기 갭(805)을 포함하여 이루어진다. 마그네트(801)는 외측에서 내측으로 단차를 가지는 링 형상인 것이 바람직하다. 이때, 링 형상은 원형의 링 뿐 아니라, 사각이나 타원 형태의 링 형상을 포함한다. 8 is a sectional view showing a second embodiment of a speaker according to the present invention. This embodiment relates to a speaker to which a magnetic circuit of the type described in FIG. 6 (b) is applied. The magnetic circuit of the speaker according to the present embodiment includes a magnet 801, a yoke 804, and a magnetic gap 805 formed between the yoke 804 and the magnet 801 in which the N pole and the S pole are horizontally formed. Is done. The magnet 801 is preferably a ring shape having a step from the outside to the inside. In this case, the ring shape includes not only a circular ring but also a ring shape having a square or ellipse shape.

마그네트(801)의 외측이 N 극을 형성하는 경우의 예를 들면, 마그네트(801)에서 발생하는 자속은 요크(804)를 통과하여 자기 갭(805)을 거쳐 마그네트(801)의 내측에 형성된 S 극으로 이어진다. 따라서, 요크(804)는 자속의 통과 경로를 제공한다. For example, in the case where the outside of the magnet 801 forms the N pole, the magnetic flux generated in the magnet 801 passes through the yoke 804, passes through the magnetic gap 805, and is formed inside the magnet 801. It leads to the pole. Thus, yoke 804 provides a path for passage of magnetic flux.

한편, 본 실시예에 따른 스피커의 진동계는 자기 갭(805)에 위치한 보이스 코일(806)과 다이어프램(807)으로 이루어진다. 보이스 코일(806)은 다이어프램(807) 및 에지부(808)에 연결되며, 다이어프램(807)은 중앙부에 돔 형상을 가지고 가장자리에는 립 형상을 가지는 이중 돔 형상인 것이 바람직하다. 에지부(808)는 보이스 코일(806)을 지지할 뿐 아니라, 다이어프램(807)의 움직임을 원할하게 하고, 다이어프램의 진동이 일정한 범위를 넘지 않도록 제어하는 기능을 수행한다. 보이스 코일(806)은 전기 신호를 입력 받기 위해 리드 와이어(809)에 연결되며, 리드 와이어(809)는 터미털 PCB(810)에 연결된다. 외부의 앰프 신호는 터미널 PCB(810)을 통해 스피커로 전달된다.On the other hand, the vibration system of the speaker according to the present embodiment is composed of a voice coil 806 and a diaphragm 807 located in the magnetic gap 805. The voice coil 806 is connected to the diaphragm 807 and the edge portion 808, the diaphragm 807 is preferably a double dome shape having a dome shape at the center and a lip shape at the edge. The edge portion 808 not only supports the voice coil 806, but also facilitates the movement of the diaphragm 807, and performs a function of controlling the vibration of the diaphragm not to exceed a predetermined range. The voice coil 806 is connected to the lead wire 809 to receive an electrical signal, the lead wire 809 is connected to the terminal PCB 810. The external amplifier signal is transmitted to the speaker through the terminal PCB (810).

다이어프램(807) 위쪽으로는 통공 캡(811)을 덮는다. 통공 캡(811)은 다이어프램(807)을 비롯한 스피커 내부 장치들을 보호하기 위한 것이다. 그리고, 다이어프램(807)에 의해 발생된 소리가 스피커 밖으로 잘 전달되도록 하기 위해, 통공 캡(811)에는 다수의 통공을 형성하는 것이 바람직하다. 저면부(812)는 요크(804)와 함께 스피커의 바닥면을 형성한다. 저면부(812)는 이물질이 스피커 내부로 유입되지 않도록 필터링 하는 역할을 할 뿐 아니라, 스피커 내부의 열을 외부로 방출시키는 역할을 한다. The through cap 811 is covered above the diaphragm 807. The through cap 811 is for protecting devices inside the speaker, including the diaphragm 807. In addition, in order for the sound generated by the diaphragm 807 to be well transmitted to the outside of the speaker, it is preferable to form a plurality of through holes in the through cap 811. The bottom portion 812 together with the yoke 804 forms the bottom surface of the speaker. The bottom portion 812 not only serves to filter foreign matter from entering the speaker, but also discharges heat inside the speaker to the outside.

도 9 는 본 발명에 따른 스피커의 제 3 실시예를 나타낸 단면도이다. 본 실시예는 도 6 (a) 에서 설명한 형태를 변형한 자기회로를 적용한 스피커에 관한 것이다. 9 is a sectional view showing a third embodiment of a speaker according to the present invention. This embodiment relates to a speaker to which the magnetic circuit in which the form described in Fig. 6A is modified is applied.

본 실시예에 따른 스피커의 자기회로는 수평하게 N 극과 S 극이 형성된 마그네트(901)와, 제 1 플레이트(902), 제 2 플레이트(903) 및 제 1 플레이트(902)와 제 2 플레이트(903) 사이에 형성된 자기 갭(905)을 포함하여 이루어진다. 마그네트(901)는 링 형상인 것이 바람직하다. 이때, 링 형상은 원형의 링 뿐 아니라, 사각이나 타원 형태의 링 형상을 포함한다. The magnetic circuit of the speaker according to the present embodiment includes a magnet 901 in which N poles and S poles are formed horizontally, a first plate 902, a second plate 903, and a first plate 902 and a second plate ( And a magnetic gap 905 formed between 903. The magnet 901 is preferably ring-shaped. In this case, the ring shape includes not only a circular ring but also a ring shape having a square or ellipse shape.

마그네트(901)의 외측이 N 극을 형성하는 경우의 예를 들면, 마그네트(901)에서 발생하는 자속은 제 1 플레이트(902)를 통과하여 자기 갭(905)와 제 2 플레이트(903)를 거쳐 마그네트(901)의 내측에 형성된 S 극으로 이어진다. 따라서, 제 1 플레이트(902) 및 제 2 플레이트(903)는 자속의 통과 경로를 제공하는 요크(yoke)(904)의 기능을 수행한다. For example, when the outside of the magnet 901 forms an N pole, the magnetic flux generated in the magnet 901 passes through the first plate 902 and passes through the magnetic gap 905 and the second plate 903. It leads to the S pole formed inside the magnet 901. Thus, the first plate 902 and the second plate 903 perform the function of a yoke 904 to provide a passage path for the magnetic flux.

한편, 본 실시예에 따른 스피커의 진동계는 자기 갭(905)에 위치한 보이스 코일(906), 보빈(911) 및 다이어프램(907)으로 이루어진다. 보이스 코일(906)은 보빈(911)에 권선되며, 보빈(911)은 다이어프램(907) 및 에지부(908)에 연결된다. 다이어프램(907)은 대략 3 중의 립(rib) 형상을 가지는 것이 바람직하다. 에지부(908)는 보이스 코일(906)을 지지할 뿐 아니라, 다이어프램(907)의 움직임을 원할하게 하고, 다이어프램의 진동이 일정한 범위를 넘지 않도록 제어하는 기능을 수행한다. 보이스 코일(906)은 전기 신호를 입력 받기 위해 리드 와이어(909)에 연결되며, 리드 와이어(909)는 터미털 PCB(910)에 연결된다. 외부의 앰프 신호는 터미널 PCB(910)을 통해 스피커로 전달된다. 한편, 저면부(912)는 제 1 플레이트(902) 저면에 부착된다.On the other hand, the vibration system of the speaker according to the present embodiment is composed of a voice coil 906, a bobbin 911 and a diaphragm 907 located in the magnetic gap 905. The voice coil 906 is wound around the bobbin 911, which is connected to the diaphragm 907 and the edge portion 908. The diaphragm 907 preferably has a triple rib shape. The edge portion 908 not only supports the voice coil 906, but also facilitates the movement of the diaphragm 907 and performs a function of controlling the vibration of the diaphragm not to exceed a predetermined range. The voice coil 906 is connected to the lead wire 909 to receive an electrical signal, the lead wire 909 is connected to the terminal PCB 910. The external amplifier signal is transmitted to the speaker through the terminal PCB (910). Meanwhile, the bottom portion 912 is attached to the bottom surface of the first plate 902.

본 실시예에 따른 스피커는 소형 전자기기의 프라스틱 사출물 내에 장착될 수 있도록 통공캡이 생략되었다. 본 실시예에 따르면, 자기회로의 자기장의 세기가 강화되므로, 진동판의 두께를 40 미크론으로 하여 f0 를 낮추는 것이 바람직하다. 상기와 같은 구성에 따라, 본 실시예에 따른 스피커는 가청 주파수 중 중음 목소리 대역을 확장할 수 있는 장점이 있다. The speaker according to the present embodiment has omitted the through-cap so as to be mounted in the plastic injection molding of the small electronic device. According to this embodiment, since the strength of the magnetic field of the magnetic circuit is enhanced, it is preferable to lower the f0 by making the thickness of the diaphragm 40 microns. According to the configuration as described above, the speaker according to the present embodiment has the advantage that can extend the middle voice band of the audio frequency.

도 10 은 본 발명에 따른 스피커의 제 1 실시예를 나타낸 분해사시도이다. 도 10 에 나타낸 스피커는 마그네트(701)가 대략 사각의 링 형태를 가지는 경우에 해당한다. 10 is an exploded perspective view showing a first embodiment of a speaker according to the present invention. The speaker shown in FIG. 10 corresponds to a case where the magnet 701 has a substantially rectangular ring shape.

도 10 에 도시된 바와 같이, 마그네트(701)는 제 1 플레이트(702) 내측에 결착되고, 마그네트(701)의 내측에는 사각의 링 형상을 가지는 제 2 플레이트(703)가 결착된다. 한편 보이스 코일(706)은 제 1 플레이트(702)와 제 2 플레이트(703)의 간극인 자기 갭에 위치하며, 보이스 코일(706)의 내측은 이중의 돔 형상을 가지는 다이어프램(707)에 연결되고, 보이스 코일(706)의 외측은 다이어프램의 외측을 구성하는 에지부에 연결된다. As shown in FIG. 10, the magnet 701 is bound inside the first plate 702, and the second plate 703 having a rectangular ring shape is bound inside the magnet 701. Meanwhile, the voice coil 706 is located in a magnetic gap, which is a gap between the first plate 702 and the second plate 703, and the inside of the voice coil 706 is connected to the diaphragm 707 having a double dome shape. The outer side of the voice coil 706 is connected to an edge portion constituting the outer side of the diaphragm.

한편, 제 1 플레이트(702) 내측으로 전기신호를 인가하기 위한 터미널 PCB(710)이 위치하며, 스피커의 상단 및 하단은 통공 캡(711)과 저면부(712)로 덮히게 된다. Meanwhile, a terminal PCB 710 for applying an electrical signal is located inside the first plate 702, and upper and lower ends of the speaker are covered with the through cap 711 and the bottom 712.

본 발명의 각 실시예에 따른 스피커들은 다양한 용도의 스피커에 적용이 가능하나, 특별히 마이크로 스피커에 적용하는 것이 바람직하다. Speakers according to embodiments of the present invention can be applied to a speaker of various uses, it is particularly preferable to apply to a micro speaker.

도 11 은 본 발명에 따른 스피커의 제 3 실시예를 나타낸 분해사시도이다. 도 11 에 나타낸 스피커는 마그네트(901)가 원형의 링 형태를 가지는 경우에 해당한다. 11 is an exploded perspective view showing a third embodiment of a speaker according to the present invention. The speaker shown in FIG. 11 corresponds to the case where the magnet 901 has a circular ring shape.

도 11 에 도시된 바와 같이, 마그네트(901)는 제 1 플레이트(902) 내측에 결착되고, 마그네트(901)의 내측에는 원형의 링 형상을 가지는 제 2 플레이트(903)가 결착된다. 한편 보이스 코일(906)은 보빈(911)에 권선되며, 보이스 코일(906)이 권선된 보빈(911)은 제 1 플레이트(902)와 제 2 플레이트(903)의 간극인 자기 갭에 위치한다. 한편, 보빈(911)은 내측으로는 립 형상을 가지는 다이어프램(907)에 연결되고, 외측으로는 다이어프램(907)의 외측을 구성하는 에지부에 연결된다. As shown in FIG. 11, the magnet 901 is bound inside the first plate 902, and the second plate 903 having a circular ring shape is bound inside the magnet 901. The voice coil 906 is wound around the bobbin 911, and the bobbin 911 on which the voice coil 906 is wound is located in a magnetic gap, which is a gap between the first plate 902 and the second plate 903. On the other hand, the bobbin 911 is connected to the diaphragm 907 having a lip shape on the inside, and is connected to the edge portion forming the outside of the diaphragm 907 on the outside.

한편, 제 1 플레이트(902) 내측으로 전기신호를 인가하기 위한 터미널 PCB(910)가 위치하며, 스피커의 하단은 저면부(912)로 덮히게 된다. On the other hand, the terminal PCB 910 for applying an electrical signal is located inside the first plate 902, the lower end of the speaker is covered with a bottom portion 912.

도 12 는 본 발명의 제 1 실시예에 따른 스피커의 성능을 종래 기술에 따른 스피커의 성능과 비교한 그래프이다. 본 그래프는 ARTA 측정장비 및 측정 마이크를 이용하여 3cc 후면 개방형에 따른 음압과 주파수를 나타낸 것이다. 12 is a graph comparing the performance of the speaker according to the first embodiment of the present invention with the performance of the speaker according to the prior art. This graph shows the sound pressure and frequency according to the 3cc rear open type using ARTA measuring instruments and measuring microphones.

도 12 를 참조하면, 본 발명의 제 1 실시예에 따른 스피커는 종래 기술에 따른 스피커에 비해 넓은 대역의 주파수에서 보다 평탄한 특성을 가진다는 것을 알 수 있다. 또한, 사람의 목소리 대역인 중음과 저음 주파수의 경우에 있어서, 현저하게 높은 음압을 가진다는 것을 알 수 있다. 따라서, 이동통신 단말기 등에 본 발명을 적용한 경우, 통화음을 이어폰 음과 같은 고음질로 제공할 수 있다는 것을 알 수 있다. 12, it can be seen that the speaker according to the first embodiment of the present invention has a flatter characteristic at a wider frequency than the speaker according to the prior art. In addition, it can be seen that in the case of the mid and low frequencies, which are human voice bands, the sound pressure is remarkably high. Therefore, when the present invention is applied to a mobile communication terminal or the like, it can be seen that the call sound can be provided with high sound quality such as earphone sound.

도 13 은 본 발명의 제 3 실시예에 따른 스피커의 성능을 종래 기술에 따른 스피커의 성능과 비교한 그래프이다. 본 그래프는 LMS 측정장비 및 측정 마이크를 이용하여 8Ω 기준으로, 1m/1w/2.83v 에 있어서 음압과 주파수 나타낸 것이다. 13 is a graph comparing the performance of the speaker according to the third embodiment of the present invention with the performance of the speaker according to the prior art. This graph shows the sound pressure and frequency at 1m / 1w / 2.83v on an 8 kHz basis using an LMS measuring instrument and a measuring microphone.

도 13 을 참조하면, 본 발명의 제 3 실시예에 따른 스피커는, 종래 기술에 따른 스피커에 비해 f0 가 200 ~ 300 Hz 우수하며, 음압 또한 4dB 이상 높다는 것을 알 수 있다. Referring to FIG. 13, it can be seen that the speaker according to the third embodiment of the present invention has superior f0 to 200 to 300 Hz and a sound pressure of 4 dB or more as compared with the speaker of the related art.

이상에서 설명한 본 발명은, 본 발명이 속하는 기술분야에서 통상의 지식을 가진 자에 있어 본 발명의 기술적 사상을 벗어나지 않는 범위 내에서 여러 가지 치환, 변형 및 변경이 가능하므로 전술한 실시예 및 첨부된 도면에 의해 한정되는 것이 아니다.The present invention described above is capable of various substitutions, modifications, and changes without departing from the spirit of the present invention for those of ordinary skill in the art to which the present invention pertains, as described above and the accompanying examples. It is not limited by the drawings.

본 발명은 다양한 스피커에 적용할 수 있다.The present invention can be applied to various speakers.

Claims (12)

자기회로와 진동계를 포함하여 이루어지되, Including magnetic circuits and vibrometers, 상기 자기회로는,The magnetic circuit, 링 형상을 가지며, 상기 링의 중심을 기준으로, 외측면에는 제 1 극성을 가지고, 내측면에는 상기 제 1 극성과 반대되는 제 2 극성을 가지는 마그네트; 및A magnet having a ring shape and having a first polarity on an outer side surface and a second polarity opposite to the first polarity on an inner side surface based on the center of the ring; And 상기 마그네트로부터 발생하는 자속의 통과 경로를 제공하는 요크Yoke to provide a passage path for the magnetic flux generated from the magnet 를 포함하여 이루어지는 스피커.Speaker comprising a. 제 1 항에 있어서,The method of claim 1, 상기 요크는,The yoke, 상기 제 1 극성에 상응하여 자속의 통과 경로를 제공하는 제 1 플레이트; 및A first plate providing a passage path for magnetic flux corresponding to the first polarity; And 상기 제 2 극성에 상응하여 자속의 통과 경로를 제공하는 제 2 플레이트A second plate providing a passage path for the magnetic flux corresponding to the second polarity 를 포함하여 이루어지는 스피커.Speaker comprising a. 제 2 항에 있어서,The method of claim 2, 상기 제 1 플레이트와 상기 제 2 플레이트는 상호 이격되어 자기 갭을 형성하는 것을 특징으로 하는 스피커.And the first plate and the second plate are spaced apart from each other to form a magnetic gap. 제 1 항에 있어서,The method of claim 1, 상기 요크는, The yoke, 상기 제 1 극성에 상응하여 자속의 통과 경로를 제공하는 것을 특징으로 하는 스피커.And a passage path for magnetic flux corresponding to the first polarity. 제 4 항에 있어서,The method of claim 4, wherein 상기 요크는 상기 마그네트와 상호 이격되어 자기 갭을 형성하는 것을 특징으로 하는 스피커.The yoke is spaced apart from the magnet to form a magnetic gap. 제 1 항에 있어서,The method of claim 1, 상기 진동계는, 상기 링의 중심을 기준으로, 자기회로 안쪽에 형성되는 것을 특징으로 하는 스피커. The vibration system is a speaker, characterized in that formed on the inside of the magnetic circuit, based on the center of the ring. 제 6 항에 있어서,The method of claim 6, 상기 진동계의 높이는 상기 마그네트의 높이보다 낮은 것을 특징으로 하는 스피커. The height of the vibration system is a speaker, characterized in that lower than the height of the magnet. 제 1 항에 있어서,The method of claim 1, 상기 진동계는,The vibrometer, 전기 신호가 인가되는 도선으로서, 상기 자기회로에 따라 형성되는 자기장 내에 위치하여, 상기 전기 신호 및 상기 자기장에 따라 기계적인 운동을 수행하는 보이스 코일; 및A conductive wire to which an electric signal is applied, the voice coil being located in a magnetic field formed according to the magnetic circuit and performing mechanical movement according to the electric signal and the magnetic field; And 상기 보이스 코일에 연결되어, 상기 보이스 코일의 기계적인 운동을 소리로 변환하는 다이어프램;A diaphragm connected to the voice coil and converting mechanical movement of the voice coil into sound; 을 포함하여 이루어지는 스피커.Speaker comprising a. 제 8 항에 있어서,The method of claim 8, 상기 마그네트는, 상기 링의 중심을 기준으로 내측면에 단차를 가지는 것을 특징으로 하는 스피커.The magnet, characterized in that having a step on the inner side with respect to the center of the ring. 제 9 항에 있어서,The method of claim 9, 상기 진동계는,The vibrometer, 일측은 상기 마그네트의 단차와 연결되고, 타측은 상기 보이스 코일에 연결되는 에지부를 더 포함하는 것을 특징으로 하는 스피커. One side is connected to the step of the magnet, the other side speaker further comprises an edge portion connected to the voice coil. 제 1 항에 있어서,The method of claim 1, 상기 링 형상은,The ring shape is, 원형의 링 형상인 것을 특징으로 하는 스피커.A speaker comprising a circular ring shape. 제 1 항에 있어서,The method of claim 1, 상기 링 형상은,The ring shape is, 사각의 링 형상인 것을 특징으로 하는 스피커.A speaker comprising a rectangular ring shape.
PCT/KR2011/001573 2010-03-09 2011-03-08 Speaker Ceased WO2011111968A2 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP2012556969A JP2013522946A (en) 2010-03-09 2011-03-08 speaker
CN2011800230474A CN102948171A (en) 2010-03-09 2011-03-08 Speaker
US13/582,605 US20120328147A1 (en) 2010-03-09 2011-03-08 Speaker

Applications Claiming Priority (4)

Application Number Priority Date Filing Date Title
KR20100020889 2010-03-09
KR10-2010-0020889 2010-03-09
KR10-2011-0019102 2011-03-03
KR1020110019102A KR101184537B1 (en) 2010-03-09 2011-03-03 Speaker

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WO2011111968A2 true WO2011111968A2 (en) 2011-09-15
WO2011111968A9 WO2011111968A9 (en) 2011-11-10
WO2011111968A3 WO2011111968A3 (en) 2011-12-22

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002186080A (en) * 2000-12-19 2002-06-28 Citizen Electronics Co Ltd Multifunctional acoustic unit
KR20040078705A (en) * 2003-03-04 2004-09-13 (주) 모토조이 Light Weight Speaker
KR20090003687A (en) * 2007-07-03 2009-01-12 김영안 Microspeakers Using Radial Magnetized Outer Ring Magnets

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