TWI353584B - Acoustic device - Google Patents

Acoustic device Download PDF

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TWI353584B
TWI353584B TW97124112A TW97124112A TWI353584B TW I353584 B TWI353584 B TW I353584B TW 97124112 A TW97124112 A TW 97124112A TW 97124112 A TW97124112 A TW 97124112A TW I353584 B TWI353584 B TW I353584B
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Taiwan
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sounding
electromagnetic wave
carbon nanotube
sound
wave signal
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TW97124112A
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Chinese (zh)
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TW201002099A (en
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Kai-Li Jiang
Lin Xiao
Zhuo Chen
Shou-Shan Fan
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Hon Hai Prec Ind Co Ltd
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  • Electrostatic, Electromagnetic, Magneto- Strictive, And Variable-Resistance Transducers (AREA)
  • Diaphragms For Electromechanical Transducers (AREA)

Description

1353584 九、發明說明: 【發明所屬之技術領域】 本發明涉及一種發聲裝置,尤其涉及-種基於夺米碳 管的發聲裝置。 【先前技術】 上發聲裝置一般由信號輸入裝置和發聲元件組成。通 過#號輸入裝置輸入電信號給發聲元件,進而發出聲 音。先前技術中的發聲元件一般爲一揚聲器。該揚聲器 ,種把電仏號轉換成聲音信號的電聲器件。具體地, 揚聲器可將—^範圍内的音頻電功率信號通過換能方式 轉變爲失真小並具有足够聲壓級的可聽聲音。揚聲器的 種類很多,雖然、它們的工作方式不同,但—般均爲通過 産生機械振動推動周圍的空氣,使空氣介質產生波動從 而實現“電·力-聲,,之轉換。 請參閱圖1’先前的電動式揚聲器1〇〇通常由三部分 組成:音圈102、磁鐵104以及振膜1〇6。音圈1〇2通^ :用-導體,當音目繼中輸入一個音頻電流信號時, 曰圈m相當於-個載流導體。若將其放在固定磁場裏, 根據載流導體在磁場中會受到洛倫茲力作用,音圈 二二到個大小與曰頻電流成正比、方向隨音頻電流方 =化而變化的力m〇2就會在磁場作用下産 ^動’並帶動振膜應振動,振膜_前後的空“ ^之振動,將電信號轉換成聲波向四周輕射。秋而,該 電動式揚聲器的結構較爲複雜’且其必須在有磁: 1353584 條件下工作。 進-步地,先前技術中的發聲裝置的發聲原理 力·聲”之轉換原理,即發聲 ’、二 入。在極端環境,“電d:件爲電信號的輸 震置進行發聲。".、^境下’則無法應用上述發聲 時,if!指當物質受到周期性强度調製的光照射 ㈤s生生聲仏唬的現象。當物質受到光照射時 因::光能而受激發’並通過非輻射使吸部 ::變爲熱。如果照射的光束經過周期性的强度』 在物質内産生周期性的溫度變化’使這部分物質 及』近的媒質熱脹冷縮而產生應力(或壓力)的周期 性變化’因而産生聲信號,此種信號稱光聲信號。光聲 #號的頻率與光調製頻率相同,其强度和相位則决定於 物質的光學、熱學、彈性和幾何的特性。目前,利用光 聲效應製造的光聲譜儀及光聲顯微鏡已經被廣;乏應用於 物質組分分析檢測領域。例如’先前技術中的光聲譜儀 般包括一光源、一樣品室及一信號檢測器。該光源一 般爲-調製的脉衝雷射源或連續雷射源。該信號檢測器 一般爲一麥克風。該樣品室中放置有待測的樣品,該樣 品材料不限,可以爲氣體、液體或固體材料,如一固體 粉末或一生物樣品等。該雷射源發射雷射照射到樣品室 t的樣品上,由於光聲效應中産生的聲能直接正比於物 質吸收的光能,而不同成分的物質在不同光波的波長處 出現吸收峰值,故當具有多譜線或連續光譜的光源以不 1353584 同波長的光束相繼照射樣品時,樣品内不同成分的物質 將在與各自的吸收峰相對應的光波波長處產生光聲信號 極大值。該信號檢測器通過檢測該光聲信號的極大值, 從而判斷待測樣品的材料種類。 ^然而,一般材料受到光吸收能力的限制,産生的光 聲信號强度較弱’且頻率範圍在兆赫兹以上只能通過 麥克風或壓電傳感器等換能裝置接收,&,先前技術中 還沒有利用光聲效應製造的發聲裝置使其產生的聲音信 號月匕直接被人耳感知。另外,先前技術中也沒有將廣義 的電磁波應用光聲效應製造的發聲裝置。 自九十年代初以來,以奈米碳管(請參見 microtubules of graphitic carbon, Nature, Sumio Iijima, v〇l 354, P56(1991))爲代表的奈米材料以其獨特的結構和 性質引起了人們極大的關注。近幾年來,隨著奈米礙管 及奈米材料研究的不斷深人,其廣闊的應用前景不斷顯 現出來。例如,由於奈米碳管所具有的獨特的電磁學、 =、。力學、化學等性能,大量有關其在場發射電子源、 名器、新型光學材料、軟鐵磁材料等領域的應用研究 :::報:。然而’先前技術中却尚未發現奈米碳管作 爲發聲70件用於聲學領域。 有鑒於此,提供一種結構簡單,可在無磁、益電的 =下直接發出能够被人耳感知的聲音的發聲I置實為 【發明内容】 1353584 一種發聲裝置,其包括一電磁波信號輸入裝置以及一 發聲元件。該發聲元件與該電磁波信號輸入裝置間隔設 置。其中’該發聲元件包括一奈米碳管結構,該電磁波信 •號輸入裝置傳遞電磁波信號至該奈米碳管結構,使該奈米 碳管結構通過吸收該電磁波信號發熱,從而加熱氣體介質 發出聲波。 相較于先前技術’所述發聲裝置具有以下優點:其一, 鲁由於所述發聲裝置中的發聲元件僅由奈米碳管結構組成, 無需磁鐵等其它複雜結構,故該發聲裝置的結構較爲簡 單’有利於降低該發聲裝置的成本。其二,該發聲裴置利 用輸入k號造成該奈米碳管結構溫度變化,從而使其周圍 氣體介質迅速膨脹和收縮,進而發出聲波,故該奈米碳管 結構組成的發聲裝置可在無磁的條件下工作。其三,由於 該奈米碳官結構具有較小的熱容和大的比表面積,故該奈 米碳$結構具有升溫迅速、熱滯後小、熱交換速度快的特 _點故該奈米峡官結構組成的發聲裝置可以發出很寬頻譜 範圍内的聲音(1Hz_1GGkHz),且具有較好的發聲效果。 其四,由於奈米碳管具有較好的機械强度和韌性,故由奈 米碳管組成的奈米碳管結構具有較好的機械强度和韌性 耐用性較好,從而有利於製備由奈米碳管結構組成的各種 开/狀尺寸的發聲裝置,進而方便地應用於各種領域。 【實施方式】 以下將結合附圖詳細說明本技術方案實施例的發聲裝 1353584 請參閱圖2,本技術方案第一實施例提供一種發聲裝 置10’該發聲裝置1〇包括一電磁波信號輸入装置112,一 .發聲几件114’ 一支撑結構116及一調製裝置118。該發聲 元件114 s又置於該支撑結構上。該電磁波信號輸入裝 置112與該發聲元件114對應且間隔設置。該調製裝置ιΐ8 设置於該電磁波信號輸入裝置112與發聲元件114之間。 從該電磁波信號輸入裝置112發出的電磁波信號12〇通過 該調製裝置118進行强度和頻率的調製後傳遞至該發聲元 件114表面。 所述發聲元件114包括一奈米碳管結構。該奈米碳管 結構y以爲一自支撑的奈米碳管結構,或一非自支撑的奈 米碳管結構。該奈米碳管結構爲層狀或其它形狀,且具有 t的比表面積。所述奈米碳管結構包括均勻分佈的ς来 碳管。該奈米碳管結構中的奈米碳管爲無序或有序排列。1353584 IX. Description of the Invention: [Technical Field] The present invention relates to a sound emitting device, and more particularly to a sound generating device based on a carbon nanotube. [Prior Art] The upper sounding device is generally composed of a signal input device and a sounding element. The electric signal is input to the sounding element through the # input device, and then the sound is emitted. The sounding element of the prior art is typically a speaker. The speaker is an electroacoustic device that converts an electric nickname into a sound signal. Specifically, the speaker can convert the audio electric power signal within the range of -^ into a audible sound having a small distortion and having a sufficient sound pressure level. There are many types of speakers. Although they work in different ways, they generally push the surrounding air by generating mechanical vibrations to cause fluctuations in the air medium to achieve "electricity, force, and sound." See Figure 1 The previous electric speaker 1〇〇 usually consists of three parts: the voice coil 102, the magnet 104, and the diaphragm 1〇6. The voice coil 1〇2 passes ^: with a conductor, when the audio input is followed by an audio current signal , the ring m is equivalent to a current-carrying conductor. If it is placed in a fixed magnetic field, according to the current-carrying conductor in the magnetic field will be subjected to Lorentz force, the voice coil 22 to a size is proportional to the 曰 frequency current, The force m〇2 whose direction changes with the audio current = will produce under the action of the magnetic field and drive the diaphragm to vibrate, and the vibration of the diaphragm _ before and after the vibration will convert the electrical signal into sound waves to the periphery. Light shot. In the autumn, the structure of the electric speaker is more complicated' and it must work under the condition of magnetic: 1353584. In the advanced way, the principle of the sounding of the sounding device of the prior art is the principle of the conversion of the sound and the sound, that is, the sounding, and the second input. In the extreme environment, "electricity d: the sound of the electrical signal is sounded." When "., ^下下' can not apply the above vocalization, if! refers to the phenomenon that the substance is subjected to periodic intensity modulation of light (5) sshengshengsheng. When the substance is exposed to light, it is excited by light energy: and the suction part :: becomes hot by non-radiation. If the illuminating beam undergoes periodic intensity changes in the material, causing periodic changes in the material and the near medium, causing periodic changes in stress (or pressure), thus producing an acoustic signal, This type of signal is called a photoacoustic signal. The frequency of the photoacoustic # is the same as the frequency of the optical modulation, and its intensity and phase are determined by the optical, thermal, elastic and geometric properties of the material. At present, photoacoustic spectroscopy and photoacoustic microscopy using photoacoustic effects have been widely used; they are used in the field of material composition analysis and detection. For example, the prior art photoacoustic spectrometer includes a light source, a sample chamber, and a signal detector. The source is typically a modulated pulsed laser source or a continuous source of laser light. The signal detector is typically a microphone. The sample to be tested is placed in the sample chamber, and the sample material is not limited and may be a gas, a liquid or a solid material such as a solid powder or a biological sample. The laser source emits a laser to the sample of the sample chamber t. Since the sound energy generated by the photoacoustic effect is directly proportional to the light energy absorbed by the substance, the substances of different compositions have absorption peaks at different wavelengths of the light wave, so When a source having a multi-spectral or continuous spectrum sequentially illuminates a sample with a beam of the same wavelength of 1353584, substances of different compositions within the sample will produce photoacoustic signal maxima at the wavelength of the light wave corresponding to the respective absorption peak. The signal detector determines the material type of the sample to be tested by detecting the maximum value of the photoacoustic signal. ^ However, the general material is limited by the light absorbing ability, and the generated photoacoustic signal intensity is weak' and the frequency range is above megahertz and can only be received by a transducer such as a microphone or a piezoelectric sensor. & The sound signal produced by the photoacoustic effect causes the sound signal generated by the sound to be directly perceived by the human ear. Further, in the prior art, there is no sound generating device which is manufactured by applying a photoacoustic effect to a generalized electromagnetic wave. Since the early 1990s, nanomaterials represented by carbon nanotubes (see microtubules of graphitic carbon, Nature, Sumio Iijima, v〇l 354, P56 (1991)) have been caused by their unique structure and properties. People are greatly concerned. In recent years, with the deepening of research on nano-barriers and nanomaterials, its broad application prospects have been continuously revealed. For example, due to the unique electromagnetic properties of carbon nanotubes, =. Mechanics, chemistry and other properties, a large number of applications related to its field emission electron source, name, new optical materials, soft ferromagnetic materials, etc. ::: reported:. However, in the prior art, no carbon nanotubes have been found as a sounding 70 for the field of acoustics. In view of the above, the present invention provides a sound emitting device that can directly emit a sound that can be perceived by the human ear under the non-magnetic and power-saving = [Abstract] 1353584 A sounding device including an electromagnetic wave signal input device And a sounding component. The sound emitting element is spaced apart from the electromagnetic wave signal input device. Wherein the sounding element comprises a carbon nanotube structure, and the electromagnetic wave signal input device transmits an electromagnetic wave signal to the carbon nanotube structure, so that the carbon nanotube structure generates heat by absorbing the electromagnetic wave signal, thereby heating the gas medium to emit Sound waves. Compared with the prior art, the sounding device has the following advantages: First, since the sounding element in the sounding device is composed only of a carbon nanotube structure, and no other complicated structure such as a magnet is needed, the structure of the sounding device is relatively Simple 'helps reduce the cost of the sounding device. Secondly, the sounding device uses the input k number to cause the temperature change of the carbon nanotube structure, so that the surrounding gas medium rapidly expands and contracts, and then emits sound waves, so the sound generating device composed of the carbon nanotube structure can be Working under magnetic conditions. Third, since the carbon carbon structure has a small heat capacity and a large specific surface area, the nano carbon structure has a rapid temperature rise, a small thermal hysteresis, and a fast heat exchange rate. The sounding device composed of the official structure can emit sound in a wide spectral range (1 Hz_1 GGkHz) and has a good sounding effect. Fourth, because the carbon nanotubes have good mechanical strength and toughness, the carbon nanotube structure composed of carbon nanotubes has good mechanical strength and toughness and durability, which is favorable for the preparation of carbon nanotubes. A variety of open/small-sized sounding devices of structural composition are conveniently used in various fields. Embodiments of the present invention will be described in detail with reference to the accompanying drawings. Referring to FIG. 2, a first embodiment of the present invention provides a sounding device 10' that includes an electromagnetic wave signal input device 112. A sounding piece 114' a support structure 116 and a modulation device 118. The sounding element 114s is again placed on the support structure. The electromagnetic wave signal input device 112 corresponds to the sounding element 114 and is spaced apart. The modulation device ι 8 is disposed between the electromagnetic wave signal input device 112 and the sounding element 114. The electromagnetic wave signal 12 发出 emitted from the electromagnetic wave signal input device 112 is modulated by the modulation device 118 to the intensity and frequency, and then transmitted to the surface of the sounding element 114. The sounding element 114 includes a carbon nanotube structure. The carbon nanotube structure y is a self-supporting carbon nanotube structure or a non-self-supporting carbon nanotube structure. The carbon nanotube structure is layered or otherwise shaped and has a specific surface area of t. The carbon nanotube structure includes a uniformly distributed carbon nanotube. The carbon nanotubes in the carbon nanotube structure are disordered or ordered.

2地,該奈米碳管結構包括奈米碳管薄膜、多個奈米碳 &長線結構或其任意組合。該奈米碳管薄臈爲 2,膜或無序的奈米碳管薄臈。該奈米碳管長線結構包 夕固百尾相連的奈米碳管束組成的束狀結構或由多個首 =的奈米好束㈣的料結構。該奈米碳管 奈米碳管長線結構長度方向的扭轉過程獲 1 管長線結構可以相互平行排列或者相互 2構=Γ—層狀的奈米碳管結構。另外,該奈米碳 二:構上述奈米碳管薄膜與奈米碳管長線結構組合 〜、體地,所述奈米碳管長線可以平行或交又的役置 1353584 於所述奈米碳管薄膜的表面,從而起到一支撑的作用,在 不减小奈米碳管結構的比表面積的條件下增强奈米碳管結 構的勒性。 該奈米碳管結構的厚度爲0.5奈米〜1毫米。該奈米碳 管結構中的奈米碳管包括單壁奈米碳管、雙壁奈米碳管及 多壁奈米碳管中的一種或多種。所述單壁奈米碳管的直徑 爲0.5奈米〜50奈米,所述雙壁奈米碳管的直徑爲1〇奈米 籲〜50奈米,所述多壁奈米碳管的直徑爲1 5奈米〜%奈米。 總之,所述奈米碳管結構的具體結構不限,只需滿足 以下二個條件,即:該奈米碳管結構具有較大的比表面積; 包括均勻分佈的奈米碳管;以及厚度爲〇 5奈米〜1毫米。 一由於該奈米碳管結構具有較大的比表面積,故當該奈 米碳管結構吸收光能或其它形式的電磁波的能量産生熱量 後可以迅速的與周圍氣體介質進行熱交換,從而使周圍空 氣加熱,造成空氣的膨脹和收縮並發出聲音。另外,由於 #奈米碳管結構具有較大的比表面積,在凡德瓦爾力的作用 下,該奈米碳管結構本身有很好的粘附性,故採用該奈米 碳管結構作發聲元件114時,該發聲元件114可以直接粘 附固定於所述支撑結構116上。另夕卜該發聲元件也 可以通過一粘結劑與所述支撑結構116結合。所述粘結劑 可以爲一耐高溫的石夕膠。 …由於該奈米碳管結構包括均勾分佈的奈米碳管,該奈 米碳管結構能够均勻的加熱空氣發出聲音,從而使該發聲 元件114具有均勻的發聲效果。 11 (S ) 1353584 * p由於該奈米碳管結構應具有較大的比表面積,故該夺 .米碳官結構的厚度不能太厚,太厚則影響奈米碳管盘周圍 .氣體介質進行熱交換。另外,該奈米碳管結構的厚度不能 •太薄,太薄則該奈米碳管結構强度較在發聲過程” 易損壞。可以理解’當該奈求碳管結構的厚度相對較小時, 例如小於1〇微米’該奈米碳管結構具有較高的透明度,故 採用該奈米碳管結構的發聲元件114爲透明發聲元件 籲m,此時,可以將該發聲元件m直接設置在各種顯示農 置、手機顯示屏的顯示表面或油晝的表面,從而達到節省 空間的目的。 所述支撑結構116主要起支撑作用,其形狀不限,任 何具有確定形狀的物體,如一墙壁或桌面,均可作爲本技 術方案第一實施例中的支撑結構116。具體地,該支撑結 構116可以爲一平面或曲面結構,並具有一表面。此時, 該發聲兀件114直接設置並貼合於該支撑結構116的表面 籲上。由於該發聲元件114整體通過支撑結構116支撑,故 該發聲元件114可以承受强度較高的電磁波信號12〇輸 入,從而具有較高的發聲强度。另外,該支撑結構116也 可以爲一框架結構、杆狀結構或不規則形狀結構。此時, 該發聲元件114部分與該支撑結構116相接觸,其餘部分 懸空设置。此種設置方式可以使該發聲元件114與空氣或 周圍介質更好地進行熱交換。該發聲元件114與空氣或周 圍介質接觸面積更大’熱交換速度更快’故具有更好的發 聲效率。In the second place, the carbon nanotube structure comprises a carbon nanotube film, a plurality of nanocarbon & long-line structures or any combination thereof. The carbon nanotubes are thin, 2, membrane or disordered carbon nanotubes. The nano-carbon tube long-line structure consists of a beam-like structure composed of a bundle of nano carbon nanotubes connected to each other or a material structure composed of a plurality of first = nanometer bundles (four). The twisting process of the long-length structure of the carbon nanotubes of the carbon nanotubes is obtained by a long-line structure in which the long-line structures can be arranged in parallel or in a mutually structured structure. In addition, the nano carbon two: the above-mentioned carbon nanotube film and the nano carbon tube long-line structure combination ~, the body, the nano carbon tube long line can be parallel or cross-serving 1353584 in the nano carbon The surface of the tube film serves as a support for enhancing the linearity of the carbon nanotube structure without reducing the specific surface area of the carbon nanotube structure. The carbon nanotube structure has a thickness of 0.5 nm to 1 mm. The carbon nanotubes in the carbon nanotube structure include one or more of a single-walled carbon nanotube, a double-walled carbon nanotube, and a multi-walled carbon nanotube. The single-walled carbon nanotube has a diameter of 0.5 nm to 50 nm, and the double-walled carbon nanotube has a diameter of 1 nm to 50 nm, and the diameter of the multi-walled carbon nanotube For 1 5 nm ~% nano. In short, the specific structure of the carbon nanotube structure is not limited, and only needs to satisfy the following two conditions: the carbon nanotube structure has a large specific surface area; includes a uniformly distributed carbon nanotube; and the thickness is 〇 5 nm ~ 1 mm. Since the carbon nanotube structure has a large specific surface area, when the carbon nanotube structure absorbs energy of light energy or other forms of electromagnetic waves to generate heat, it can quickly exchange heat with the surrounding gaseous medium, thereby making the surrounding The air heats up, causing the air to expand and contract and make a sound. In addition, since the #nano carbon nanotube structure has a large specific surface area, the carbon nanotube structure itself has good adhesion under the action of van der Waals force, so the carbon nanotube structure is used for sounding. When the component 114 is in use, the sounding component 114 can be directly adhered to the support structure 116. In addition, the sounding element can also be coupled to the support structure 116 by an adhesive. The binder may be a high temperature resistant stone. ... Since the carbon nanotube structure includes a carbon nanotube having a uniform hook distribution, the carbon nanotube structure can uniformly heat the air to emit sound, so that the sound emitting element 114 has a uniform sounding effect. 11 (S ) 1353584 * p Since the carbon nanotube structure should have a large specific surface area, the thickness of the carbon-weighted structure should not be too thick, too thick to affect the surrounding of the carbon nanotube disk. Heat exchange. In addition, the thickness of the carbon nanotube structure cannot be too thin, and if the thickness is too thin, the structural strength of the carbon nanotube is more susceptible to damage during the vocal process. It can be understood that when the thickness of the carbon tube structure is relatively small, For example, if the carbon nanotube structure has a high transparency, the sound emitting element 114 of the carbon nanotube structure is used for the transparent sounding element. In this case, the sounding element m can be directly disposed in various types. Displaying the display surface of the farm display, the display screen of the mobile phone or the surface of the oil raft to achieve the purpose of saving space. The support structure 116 mainly serves as a support, and its shape is not limited, any object having a certain shape, such as a wall or a table top, The support structure 116 can be a planar or curved structure and has a surface. In this case, the sounding element 114 is directly disposed and attached to the support structure 116. The surface of the support structure 116 is appealed. Since the sounding element 114 is entirely supported by the support structure 116, the sounding element 114 can withstand high-intensity electromagnetic wave signals 12 〇 input, so as to have a higher vocal intensity. In addition, the support structure 116 can also be a frame structure, a rod-like structure or an irregular shape structure. At this time, the sound-emitting element 114 is partially in contact with the support structure 116, and the rest Partially suspended setting. This arrangement allows for better heat exchange between the sounding element 114 and the air or surrounding medium. The sounding element 114 has a larger contact area with air or surrounding medium 'faster heat exchange rate' and therefore better Sound efficiency.

12 該支撑結構116的材料不限,可以爲一硬性材料,如 ^石、木質材料 '玻璃或石英。另外,所述支撑結構Μ •遊可爲一柔性材料,如紙質材料、塑料或樹脂。優選地, •該支撑結構116的材料應具有較好的絕熱性能,從而防止 k發聲元件114産生的熱量過度的被該支撑結構吸 收,無法達到加熱空氣發聲的目的。另外,該支撑結構ιΐ6 優選爲具有一較爲粗糙的表面,從而可以使設置於上述支 ⑩撑結構116表面的發聲元件114與空氣或其他外界介質具 有更大的接觸面積。 ^可以理解,由於上述發聲元件114中的奈米碳管結構 爲一自支撑結構,故該支撑結構116爲一可選擇結構。 所述電磁波信號輸入裝置112包括一電磁波信號源, 該電磁波信號源可以發出强度或頻率可變的電磁波,形成 一電磁波信號120。該電磁波信號12〇的强度或頻率可不 斷變化,從而能够使作爲發聲元件114的奈米碳管結構吸 鲁枚該電磁波信號120間歇加熱空氣,使空氣不斷膨脹收 縮’進而持續發出聲音。該電磁波信號12〇的頻率範圍包 括無線電波、紅外線、可見光、紫外線、微波、X射線及 γ射線等。優選的,該電磁波信號源爲一光信號源,所發 出的電磁波信號120可以爲一光信號,該光信號的波長包 括從紫外至遠紅外波長的各種光波。該電磁波信號12〇的 平均功率密度在1 y w/mm2〜20W/mm2範圍内。可以理解, 該電磁波信號120的强度不能太弱,太弱則無法使奈米碳 管結構充分加熱周圍空氣發出聲音,並且,該電磁波信號 13 1353584 .120的强度不能太强,太强使奈米碳管結構與空氣中的氧 .發生反應’從而破壞該奈米碳管結構。優選地,該電磁波 .信號源爲一脉衝雷射發生器。 該電磁波信號輸入裝置112發出的電磁波信號120在 發聲元件114上的入射角度與位置不限。另外,該電磁波 信號輸入裝置112與發聲元件114之間的距離不限,但應 確保從該電磁波信號輸入裝置112發出的電磁波能够傳遞 籲至該發聲元件114表面。優選地,當該電磁波信號爲一光 仏號,且該電磁波信號輸入裝置112與該發聲元件114距 離較遠時’該電磁波信號輸入裝置112可以進一步包括一 光纖,該光纖一端與所述光信號源連接,另一端延伸至所 述奈米碳管薄膜附近,從而使通過上述雷射發生器發出的 電磁波信號120通過光纖遠距離傳遞至發聲元件114表面。 所述調製裝置118爲一可選擇結構,設置於該電磁波 信號120的傳輸路徑上,包括强度調製器、頻率調製器或 鲁兩者的結合。所述發聲裝置1〇通過調製裝置118對電磁波 #號120的强度及頻率進行調製,從而實現使發聲元件 所發出的聲音的强度及頻率的改變。具體地,可以通過以 不同頻率開關電磁波信號120調製電磁波信號12〇的强 弱,或者以不同頻率變化電磁波信號12〇的强度調製電磁 波信號120的强弱。電磁波信號12〇强弱的變化影響發聲 7G件114發聲頻率的變化。通過對該電磁波信號12〇進行 調製,可以使該發聲元件114發出不同頻率的聲音。可以 理解,該調製裝置118可以與所述電磁波信號輸入裝置112 14 (S ) 1353584 .集成或間隔設置。當所述電磁波信號輪入裝置112包括一 •光纖時,該調製裝置118可設置於光纖的起始端或結束端 -上。本實施例令,該調製裝置118爲一電光晶體。 本技術方案實施例發聲裝置中採用奈米碳管結構作爲 發聲元件,由於奈米碳管對電磁波的吸收接近絕對黑體, 從而使發聲裝置對於各種波長的電磁波具有均一的吸收特 f生另外,奈米碳管具有較小的熱容和較大的散熱面積。 鲁故,备發聲元件114中的奈米碳管受到如雷射等電磁波的 照射時,奈米碳管因吸收光能而受激發,並通過非輻射使 吸收的光能全部或部分轉變爲熱。奈米碳管溫度迅速升 円,並和周圍的空氣或其他介質進行迅速的熱交換。如果 照射的電磁波經過周期性的强度調製,則在奈米碳管内産 生周期性的溫度變化,從而使其周圍的氣體介質也産生周 期性的溫度變化,造成周圍空氣或其他介質迅速的膨脹和 收縮,從而發出聲音。進一步地,本實施例令,所述發聲 φ 7L件114包括由大量奈米碳管組成的奈米碳管結構,故當 電磁波信號輸入裝置118發出的電磁波信號12〇的頻率合 適’且發聲元件114周圍介質爲空氣時,發聲元件114發 出的聲音可以直接被人耳感知。可以理解,當電磁波信號 120的頻率增高時’該發聲元件114可以發出超聲波。 請參閱圖3’本技術方案第二實施例提供一種發聲裝 置20’該發聲裝置20包括一信號輸入裝置212、一發聲元 件214、一支撑結構216及一調製裝置218。 該支撑結構216爲一框架結構、杆狀結構或不規則形 15 1353584 .狀結構。該發聲元件214部分與該支撑結構216相接觸, 其餘部分懸空設置,從而使聲音能够透過該發聲元件214 傳遞。該電磁波信號輸入裝置212與該發聲元件214對應 且間隔设置。該調製裝置218設置於該電磁波信號輸入裝 置212與發聲元件214之間。 該發聲裝置20與第一實施例中的發聲裝置1〇的結構 基本相似,與第一實施例中的發聲裝置1〇的區別在於該 鲁發聲裝置20進一步包括一攏音結構222,該攏音結構222 間隔設置在所述發聲元件214遠離電磁波信號22〇輸入的 一側I。該攏音結構222與該發聲元件214相隔設置,從而 使發聲元件214發出的聲波通過攏音結構222反射,增强 該發聲裝置20的發聲效果。根據發聲元件214的大小,該 距離可以爲1厘米〜1求。可以理解,該攏音結構222可以 爲具有一較大表面的各種結構,如一平面結構或一曲面結 構。本實施财,該攏音結構222爲一平板。該搬音結構 # 222可以通過支架與該發聲元件214間隔。另外,該攏音 結構222與該支撑結構216也可爲一集成設置的整體如 一具有狹窄開口的腔體,該發聲元件214平鋪於該腔體的 開口上’從而形成一亥姆霍兹共振腔。該攏音結構⑵的 材料爲木質、塑料、金屬或玻璃等。 <本技術方案實施例中,所述發聲元件發聲的頻率範圍 2 1赫兹至H)萬赫兹。當發聲元件中的奈米碳管結射的 不、未碳管有序排列且奈米碳管結構的厚度較薄時,發聲强 度就可以達到70分貝聲壓級_飢)。當該奈米碳管結構12 The material of the support structure 116 is not limited and may be a hard material such as stone, wood material 'glass or quartz. Additionally, the support structure can be a flexible material such as paper material, plastic or resin. Preferably, the material of the support structure 116 should have better thermal insulation properties, so that the heat generated by the k sounding element 114 is prevented from being excessively absorbed by the support structure, and the purpose of heating the air is not achieved. Further, the support structure ι 6 preferably has a relatively rough surface so that the sound-emitting element 114 provided on the surface of the support structure 116 can have a larger contact area with air or other external medium. It can be understood that since the carbon nanotube structure in the sound generating element 114 is a self-supporting structure, the support structure 116 is an optional structure. The electromagnetic wave signal input device 112 includes an electromagnetic wave signal source that emits an electromagnetic wave of variable intensity or frequency to form an electromagnetic wave signal 120. The intensity or frequency of the electromagnetic wave signal 12〇 can be constantly changed, so that the carbon nanotube structure as the sounding element 114 can absorb the electromagnetic wave signal 120 to intermittently heat the air, and the air is continuously expanded and contracted to continuously emit sound. The frequency range of the electromagnetic wave signal 12 包 includes radio waves, infrared rays, visible rays, ultraviolet rays, microwaves, X rays, and gamma rays. Preferably, the electromagnetic wave signal source is an optical signal source, and the emitted electromagnetic wave signal 120 can be an optical signal, and the wavelength of the optical signal includes various light waves from ultraviolet to far infrared wavelengths. The electromagnetic wave signal 12 has an average power density in the range of 1 y w/mm 2 to 20 W/mm 2 . It can be understood that the intensity of the electromagnetic wave signal 120 cannot be too weak, and if it is too weak, the carbon nanotube structure cannot sufficiently heat the surrounding air to emit sound, and the intensity of the electromagnetic wave signal 13 1353584 .120 cannot be too strong, so that the nanometer is too strong. The carbon tube structure reacts with oxygen in the air to destroy the carbon nanotube structure. Preferably, the electromagnetic wave signal source is a pulsed laser generator. The incident angle and position of the electromagnetic wave signal 120 emitted from the electromagnetic wave signal input device 112 on the sound emitting element 114 are not limited. Further, the distance between the electromagnetic wave signal input device 112 and the sound emitting element 114 is not limited, but it should be ensured that electromagnetic waves emitted from the electromagnetic wave signal input device 112 can be transmitted to the surface of the sound emitting element 114. Preferably, when the electromagnetic wave signal is an optical signal, and the electromagnetic wave signal input device 112 is far away from the sound emitting element 114, the electromagnetic wave signal input device 112 may further include an optical fiber, one end of the optical fiber and the optical signal. The source is connected, and the other end extends to the vicinity of the carbon nanotube film, so that the electromagnetic wave signal 120 emitted by the above-mentioned laser generator is transmitted to the surface of the sound emitting element 114 through the optical fiber. The modulating device 118 is an optional structure disposed on the transmission path of the electromagnetic wave signal 120, including a combination of an intensity modulator, a frequency modulator, or a dual. The sounding device 1A modulates the intensity and frequency of the electromagnetic wave #120 by the modulation device 118, thereby realizing the change in the intensity and frequency of the sound emitted by the sounding element. Specifically, the intensity of the electromagnetic wave signal 120 can be modulated by switching the electromagnetic wave signal 120 at a different frequency, or the intensity of the electromagnetic wave signal 120 can be modulated by varying the intensity of the electromagnetic wave signal 12〇 at a different frequency. The change in the intensity of the electromagnetic wave signal 12 affects the change in the sounding frequency of the 7G piece 114. By modulating the electromagnetic wave signal 12A, the sound producing element 114 can be made to emit sound of different frequencies. It can be understood that the modulating device 118 can be integrated or spaced apart from the electromagnetic wave signal input device 112 14 (S ) 1353584 . When the electromagnetic wave signal wheeling device 112 includes an optical fiber, the modulation device 118 can be disposed at the beginning or end of the optical fiber. In this embodiment, the modulation device 118 is an electro-optic crystal. In the sounding device of the embodiment of the present invention, a carbon nanotube structure is used as the sounding element, and since the absorption of the electromagnetic wave by the carbon nanotube is close to the absolute black body, the sounding device has a uniform absorption for the electromagnetic waves of various wavelengths. The carbon nanotube has a small heat capacity and a large heat dissipation area. In the case where the carbon nanotubes in the acoustic generating element 114 are irradiated by electromagnetic waves such as lasers, the carbon nanotubes are excited by the absorption of light energy, and the absorbed light energy is completely or partially converted into heat by non-radiation. . The carbon nanotubes rapidly rise in temperature and undergo rapid heat exchange with the surrounding air or other medium. If the irradiated electromagnetic wave is periodically intensity modulated, a periodic temperature change is generated in the carbon nanotube, so that the surrounding gas medium also undergoes periodic temperature changes, causing rapid expansion and contraction of the surrounding air or other medium. , thus making a sound. Further, in this embodiment, the sounding φ 7L member 114 includes a carbon nanotube structure composed of a large number of carbon nanotubes, so that the frequency of the electromagnetic wave signal 12 发出 emitted by the electromagnetic wave signal input device 118 is appropriate 'and the sounding element When the surrounding medium is air, the sound emitted by the sounding element 114 can be directly perceived by the human ear. It will be understood that the sounding element 114 can emit ultrasonic waves when the frequency of the electromagnetic wave signal 120 is increased. Referring to FIG. 3', a second embodiment of the present invention provides a sounding device 20'. The sounding device 20 includes a signal input device 212, a sounding element 214, a support structure 216, and a modulation device 218. The support structure 216 is a frame structure, a rod-shaped structure or an irregular shape 15 1353584. The sounding element 214 is partially in contact with the support structure 216, and the remaining portion is suspended so that sound can be transmitted through the sounding element 214. The electromagnetic wave signal input device 212 is corresponding to and spaced apart from the sound emitting element 214. The modulation device 218 is disposed between the electromagnetic wave signal input device 212 and the sound emitting element 214. The sounding device 20 is substantially similar in structure to the sounding device 1A in the first embodiment, and is different from the sounding device 1A in the first embodiment in that the sounding device 20 further includes a sounding structure 222. The structure 222 is spaced apart from the side I of the sounding element 214 that is remote from the electromagnetic wave signal 22〇. The sound-sounding structure 222 is disposed apart from the sound-emitting element 214 such that the sound waves emitted by the sound-emitting element 214 are reflected by the sound-sounding structure 222, enhancing the sounding effect of the sound-emitting device 20. Depending on the size of the sounding element 214, the distance can be 1 cm~1. It can be understood that the sound structure 222 can be various structures having a large surface, such as a planar structure or a curved structure. In the implementation, the sound structure 222 is a flat plate. The sound transmitting structure #222 can be spaced from the sounding element 214 by a bracket. In addition, the sound absorbing structure 222 and the supporting structure 216 can also be an integrated whole body such as a cavity having a narrow opening, and the sounding element 214 is laid on the opening of the cavity to form a Helmholtz resonance. Cavity. The material of the sound-absorbing structure (2) is wood, plastic, metal or glass. < In the embodiment of the present invention, the sounding element emits sound in a frequency range of 2 Hz to H) 10,000 Hz. When the carbon nanotubes in the sounding element are not aligned, the carbon tubes are arranged in an order, and the thickness of the carbon nanotube structure is thin, the sound intensity can reach 70 dB sound pressure level _ hunger. When the carbon nanotube structure

16 比 3584 的厚度增加時,發聲强度可以進一步增强。另外,本技術 案實知例中的奈米碳管結構具有較好的勒性和機械强 度’利用所述奈米碳管結構可方便地製成各種形狀和尺寸 的發聲裝置’該發聲裝置可方便地應用於各種音樂設備 中,如音響、手機、聰、MP4、電視、計算機等電子領 域及其匕發聲裝置中。另外,由於電磁波,尤其雷射,可 乂在真二中遠距離傳播,該發聲裝置可以用於遠距離信號 馨傳輸湏域如將聲音信號通過電磁波的形式遠距離傳輸。 進步地,由於上述發聲元件通過電磁波照射即可發聲, 故,當該電磁波爲紅外線、可見光、紫外線微波、χ射 線及Y射線時,該發聲元件可以在-無電、無磁的極端環 境下工作。 本技術方案實施例提供的發聲裝置具有以下優點:其 、由於所述發聲裝置中的發聲元件僅由奈米碳管結構組 f無需磁鐵等其它複雜結構,故該發聲裝置的結構較爲 鲁簡單,有利於降低該發聲裝置的成本。其二,由於所述由 奈米石反管結構組成的發聲元件可以通過輸入 發聲:故,該發聲元件可以在一無電環境下工作。其^ 該發聲裝置利用輸入信號造成該奈米碳管結構溫度變化, 從而使其周圍氣體介質迅速膨脹和收縮,進而發出聲波, 故該奈求碳管結構組成的發聲裝置可在無磁的條件下工 作。其四’由於該奈米碳管結構具有較小的熱容和大的比 表面積ii:該不米石反官結構具有升溫迅速、熱滞後小、敎 交換速度快的特點,故該奈米碳管結構組成的發聲裝置ΐ 17 (S ) 1353584 以發出很寬頻譜範圍内的聲音Γ 好的菸Π里甘 叼耷曰dHz-lOOkHz),且具有較 .." ’、五’由於奈米碳管具有較好的機械强度 =二由奈米碳管組成的奈米碳管結構具有較好的機 ^ 奸從而有利於製備由奈米碳管 j組成的各種形狀、尺寸的發聲I置,進而方便地應用 於各種領域。其六,當該奈米碳管結構厚度比較小時,例 如小於1G微米’該奈米碳管結構具有較高的透明度,故採When the thickness of 16 is increased by 3584, the vocal intensity can be further enhanced. In addition, the carbon nanotube structure in the embodiment of the present technology has better linearity and mechanical strength. The sound generating device can be conveniently fabricated into various shapes and sizes by using the carbon nanotube structure. Conveniently used in a variety of music equipment, such as audio, mobile phones, Cong, MP4, television, computers and other electronic fields and their sounding devices. In addition, since electromagnetic waves, especially lasers, can be transmitted over long distances in the true two, the sounding device can be used for long-distance signal transmission, such as transmitting sound signals over long distances in the form of electromagnetic waves. Progressively, since the sound emitting element can be sounded by electromagnetic wave irradiation, when the electromagnetic wave is infrared light, visible light, ultraviolet microwave, ray line, and ray, the sound generating element can operate in an extreme environment of no electricity or magnetism. The sounding device provided by the embodiment of the present technical solution has the following advantages: since the sound emitting element in the sounding device only requires no complicated structure such as a magnet by the carbon nanotube structure group f, the structure of the sounding device is relatively simple and simple. It is beneficial to reduce the cost of the sounding device. Second, since the sounding element composed of the nano stone back tube structure can be audible through the input: the sound generating element can operate in an electroless environment. The sound generating device uses the input signal to cause the temperature change of the carbon nanotube structure, thereby rapidly expanding and contracting the surrounding gas medium, thereby generating sound waves, so that the sound generating device composed of the carbon tube structure can be in a non-magnetic condition. Work under. The fourth 'because of the carbon nanotube structure has a small heat capacity and a large specific surface area ii: the non-meterite reverse structure has the characteristics of rapid temperature rise, small thermal hysteresis, and fast exchange rate of cesium, so the nanometer The carbon tube structure consists of a sounding device ΐ 17 (S ) 1353584 to emit sound in a wide spectral range, good soot, 叼耷曰 Π 叼耷曰 叼耷曰 d - l - , , , , , , , , , , , , , , , , , , The carbon nanotubes have better mechanical strength = two carbon nanotube structures composed of carbon nanotubes have better mechanical properties, which facilitates the preparation of various shapes and sizes of sounding I composed of carbon nanotubes j. Conveniently used in a variety of fields. Sixth, when the thickness of the carbon nanotube structure is relatively small, for example, less than 1G micron, the carbon nanotube structure has high transparency, so

用該奈米碳管结構的發聲元件爲透明發聲元件,可直接設 置於-顯示裝置或油晝的上表面’從而達到節省空間的目 ^其七,所述發聲裝置可進—步包括―攏音結構,該搬 日結構可以反射發聲元件發出的聲波,冑强所述發聲裝置 的發聲效果。 a綜上所述,本發明確已符合發明專利之要件,遂依法 提出專利申請。惟,以上所述者僅為本發明之較佳實施例, 自不能以此限制本案之申請專利範圍。舉凡習知本案技藝 人士援依本發明之精神所作之等效修飾或變化,皆應涵 蓋於以下申請專利範圍内。 【圖式簡單說明】 圖1係先前技術中揚聲器的結構示意圖。 圖2係本技術方案第一實施例發聲裝置的結構示意 圖。 圖3係本技術方案第二實施例發聲裝置的結構示意 圖0 【主要元件符號說明】The sound emitting element of the carbon nanotube structure is a transparent sounding element, which can be directly disposed on the upper surface of the display device or the oil raft to achieve space saving. The sound generating device can further include The sound structure, the moving structure can reflect the sound waves emitted by the sounding element, and the sounding effect of the sounding device is reluctant. a In summary, the present invention has indeed met the requirements of the invention patent, and has filed a patent application according to law. However, the above description is only a preferred embodiment of the present invention, and it is not possible to limit the scope of the patent application in this case. Equivalent modifications or variations made by those skilled in the art in light of the spirit of the present invention are intended to be included in the scope of the following claims. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic structural view of a speaker in the prior art. Fig. 2 is a schematic view showing the structure of a sound generating device of a first embodiment of the present technical solution. Figure 3 is a schematic structural view of a sounding device according to a second embodiment of the present technical solution. Figure 0 [Description of main component symbols]

(S 18 1353584 揚聲器 音圈 磁鐵 振膜 發聲裝置 電磁波信號輸入裝置 發聲元件 支撑結構 •調製裝置 電磁波信號 攏音結構 100 102 104 106 10, 20 112, 212 114, 214 116, 216 118, 218 120, 220 222(S 18 1353584 Speaker voice coil magnet diaphragm sounding device electromagnetic wave signal input device sounding element support structure • Modulation device electromagnetic wave signal sound structure 100 102 104 106 10, 20 112, 212 114, 214 116, 216 118, 218 120, 220 222

1919

Claims (1)

1353584 十、申請專利範圍 1. 一種發聲裝置,其包括·· 一電磁波信號輸入裝置;以及 一發聲元件’該發聲元件與該電磁波信號輸入裝置對應 且間隔設置, 其改良在於,該發聲元件包括一奈米碳管結構,該電磁 波k號輸入裝置傳遞電磁波信號至該奈米碳管結構使 該奈米碳管結構通過吸收該電磁波信號發熱,從而加熱 • 氣體介質發出聲波。 所述 2.如申請專利範圍第丄項所述的發聲裝置,其中 奈米碳管結構爲層狀結構。 3·如申請,利範圍第2項所述的發聲裝置,其中,所述 结構包括奈米碳管薄膜、多個奈米碳管長線 構或其任意組合形成的複合結構。 其中,所述 4. 如申請專利範圍第i項所述的發聲裝置 奈米碳管結構的厚度爲0.5奈米〜i毫米, 其中,所域 5. 如申請專利範圍第1項所述的發聲襄置 奈^碳管結構包括均勻分佈的奈米碳管。 所iil 6. 如申請專利範圍笛ς 太乎碏圍第 述的發聲裝置,其中 7 V申:米碳管爲無序或有序排列 奈米石炭管結構中的夺的發聲裝置’其中’❹ 米碳管及多壁奈米碳管單壁奈米碳管、雙壁: 米碳管的直徑爲〇5夺、一種或多種,所述單壁^ 的直徑爲以奈米,太、奈米’所述雙壁奈米碳‘ ,丁、木’所述多壁奈米碳管的直」 20 9 爲1.5奈米〜50奈米。 =申請專㈣項所述 聲裝置進-步包括-支撑^聲裝置,其中,該發 支撑結構固定設置。構’所述發聲元件通過該 所述 所述 所述 如申請專利範圍第8項所述 支撐結構爲一平面或曲面心發^,其中 菸蓉-从士 1 田、,口構’並具有一表面 Π)如申料置並貼合於該支撑結構的表面· •支撑結構爲一框架結構其中’所述 n L 聲凡件通過該支撑結構部分懸空設置。 .申睛專利範圍第10項所述& | # 發聲裝置進-步包括ιΛΙ發衫置,其中,所述 於發聲元件遠離電磁波“:述攏音結構設置 發聲元件相對並間隔設置 裝置的一侧,與所述 圍第8項所述的發聲裝置,其中,所述 支撑、.,。構的材料爲硬性材料或柔性材料。 .如申晴專利範圍第8項所 支撑結構的材料爲金剛石玻的璃發聲石裝 木質材料或紙質材料。麵石央、塑料、樹脂、 發聲裝置,其中,所述 _J 步匕括搋曰結構’所述攏音結構包括 霍㈣振腔,所述發聲元件通過該攏音結構固 15^磁申f專利範圍第1項所述的發聲裝置,其令,所述 皮㈣爲無線電波、紅外線、可見光、紫外線、1353584 X. Patent application scope 1. A sounding device comprising: an electromagnetic wave signal input device; and a sounding element 'the sounding element corresponding to the electromagnetic wave signal input device and spaced apart, the improvement is that the sounding element comprises a The carbon nanotube structure, the electromagnetic wave k input device transmits an electromagnetic wave signal to the carbon nanotube structure, so that the carbon nanotube structure generates heat by absorbing the electromagnetic wave signal, thereby heating the gas medium to emit sound waves. 2. The sounding device of claim 2, wherein the carbon nanotube structure is a layered structure. 3. The sounding device of claim 2, wherein the structure comprises a composite structure of a carbon nanotube film, a plurality of carbon nanotube long wires, or any combination thereof. Wherein, the thickness of the carbon nanotube structure of the sounding device as described in claim i is 0.5 nm to i mm, wherein the field is as described in claim 1 The carbon nanotube structure includes a uniformly distributed carbon nanotube. Iil 6. If the patent application scope flute is too far from the first sounding device, 7 V Shen: the carbon nanotubes are disordered or orderedly arranged in the nano-carboniferous structure of the sounding device 'where '❹ Carbon nanotubes and multi-walled carbon nanotubes, single-walled carbon nanotubes, double-walled: The diameter of the carbon nanotubes is 〇5, one or more, and the diameter of the single-walled ^ is nanometer, too, and nanometer. 'The double-walled nanocarbon', Ding, Mu's multi-walled carbon nanotubes have a straightness of 20 9 to 1.5 nm to 50 nm. = The application of the sound device step-by-step includes a support device, wherein the hair support structure is fixedly set. The sound-emitting element is a planar or curved surface of the support structure according to the eighth aspect of the patent application, wherein the cigarette---------------------- The surface Π is placed on the surface of the support structure as claimed. • The support structure is a frame structure in which the n L acoustic member is partially suspended by the support structure. The sounding device step-by-step includes the ιΛΙ hairpin set, wherein the sounding element is away from the electromagnetic wave ": the sounding structure is arranged to set the sounding element relative to the interval setting device The sounding device according to the above aspect, wherein the material of the support structure is a hard material or a flexible material. The material supported by the structure of the eighth item of the Shenqing patent scope is diamond. The glass horn is made of wood material or paper material, the surface stone, the plastic, the resin, the sounding device, wherein the _J step 匕 搋曰 structure, the sound structure comprises a Huo (four) vibration chamber, the sounding The sound generating device according to the first aspect of the invention, wherein the skin (four) is radio waves, infrared rays, visible light, ultraviolet rays, 21 1353584 微波、X射線及γ射線中的一種或多種。 16. 如申請專利範圍第1項所述的發聲裝置,其中,所述 電磁波信號輸入裝置進一步包括一光信號源,所述電 磁波彳§號輸入裝置通過該光信號源發出光信號,該光 k號的波長耗圍爲從紫外區至遠紅外區之間。 17. 如申請專利範圍第16項所述的發聲裝置,其中,所述 光信號源爲一腺衝雷射發生器。 18. 如申請專利範圍第16項所述的發聲裝置,其中,所述 電磁波信號輸入裝置進一步包括一光纖,該光纖一端 與所述光k號源連接,另一端延伸至所述奈米碳管薄 膜附近,所述光信號通過光纖傳遞至所述奈米碳管結 構。 19. 如申請專利範㈣i項所述的發聲裝置,纟中,該發 聲裝置進-步包括一調製裝置,該調製裝置設置於所 述電磁波信號輸入裝置與發聲元件之間,且位於所述 電磁波信號的傳輸路徑上,該調製裝置包括强度調势 • 裝置、頻率調製裝置或兩者的結合。 、 2〇·如申請f利範圍第1項所述的發聲裝置,其中,所迷 電磁波信號的平均功率密度冑1/zW/mm2〜2〇w/mm2。21 1353584 One or more of microwave, X-ray and gamma rays. 16. The sounding device of claim 1, wherein the electromagnetic wave signal input device further comprises an optical signal source, and the electromagnetic wave signal input device emits an optical signal through the optical signal source, the light k The wavelength of the number is between the ultraviolet region and the far infrared region. 17. The sounding device of claim 16, wherein the optical signal source is a gland laser generator. 18. The sounding device of claim 16, wherein the electromagnetic wave signal input device further comprises an optical fiber, one end of the optical fiber is connected to the light source k, and the other end is extended to the carbon nanotube Near the film, the optical signal is transmitted through the optical fiber to the carbon nanotube structure. 19. The sounding device of claim 4, wherein the sounding device further comprises a modulation device disposed between the electromagnetic wave signal input device and the sounding element and located at the electromagnetic wave The modulation means includes a strength adjustment device, a frequency modulation device, or a combination of both on the transmission path of the signal. The sounding device according to the first aspect of the invention, wherein the electromagnetic wave signal has an average power density of 胄1/zW/mm2 to 2〇w/mm2. 22twenty two
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