TWI225333B - Class D amplifier - Google Patents
Class D amplifier Download PDFInfo
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- TWI225333B TWI225333B TW092104653A TW92104653A TWI225333B TW I225333 B TWI225333 B TW I225333B TW 092104653 A TW092104653 A TW 092104653A TW 92104653 A TW92104653 A TW 92104653A TW I225333 B TWI225333 B TW I225333B
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- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03F—AMPLIFIERS
- H03F3/00—Amplifiers with only discharge tubes or only semiconductor devices as amplifying elements
- H03F3/20—Power amplifiers, e.g. Class B amplifiers, Class C amplifiers
- H03F3/21—Power amplifiers, e.g. Class B amplifiers, Class C amplifiers with semiconductor devices only
- H03F3/217—Class D power amplifiers; Switching amplifiers
- H03F3/2171—Class D power amplifiers; Switching amplifiers with field-effect devices
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- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03F—AMPLIFIERS
- H03F2200/00—Indexing scheme relating to amplifiers
- H03F2200/03—Indexing scheme relating to amplifiers the amplifier being designed for audio applications
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Description
1225333 玖、發明說明: 【發明所屬之技術領域】 本發明係有關於變換音樂信號等的類比信號成為脈衝信 號而施以電力放大之D級放大器(數位放大)之相關技術,特 別疋有關於用以驅動控制輸出用功率M〇s電晶體之電路技 術。 【先前技術】 白知上,已知有以音樂信號等的類比信號作為輸入信 號’並將其變換成脈衝信號而施以電力放大之D級放大器, 在该輸出端子係中介低域濾波器而連接著放音器的輸入端 子。依據該D級放大器,其輸入信號的振幅(資料成份)係反 映於脈衝寬幅而輸出經電力放大的脈衝信號。而且,該脈 衝#號係經通過低域濾波器,而抽出經電力放大的類比量 的音樂信號,而該音樂信號即驅動放音器。D級放大器係因 為能形成於矽晶片上,故能實現小型且價廉之設計,多被 使用於要求低消耗電力的攜帶型終端機或個人電腦等。 圖12係表示D級放大器900之構成的使用例。 居圖中’仏號源SIG係以接地電位(〇 v)作為振幅中點的類 比量的音樂信號VIN的產生源,其係中介將包含於該音樂信 號的直流成份予以遮斷的輸入電容器(未圖示),而連接於D 級放大器900的輸入端子TI。D級放大器9〇〇係所謂的PWM 放大器(PWM: Pulse Width Modulation),其係由輸入段 901 、調變電路902、驅動電路903、η型功率MOS電晶體904、 905所構成。 輸入段901係使音樂信號VIN的中點產生移動,而變換音 80426 樂信號VIN成適合於電源VDD (例如10 V)所作動的調變電 路902的輸入特性之波形。調變電路902係將輸入段901所輸 出的音樂信號予以變換成脈衝信號,且反映音樂信號的資 訊成份於脈衝寬幅而進行PWM調變。驅動電路903係依據調 變電路902所調變的脈衝信號,而互補地驅動控制輸出用功 率MOS電晶體904、905。 功率MOS電晶體904係在正電源VPP+ (例如+50 V)與輸出 端子TO之間連接有電流路徑,且用以輸出高準位。此外, 功率MOS電晶體905係在負電源VPP-(例如_50 V)與輸出端 子TO之間連接有電流路徑,且用以輸出低準位。輸出端子 TO係中介由電感L和電容器C所組成的低域滤波器而連接 於放音器SPK的輸入端子。 根據該D級放大器900,則自信號源SIG所輸入的音樂信 號VIN係經由輸入段901及調變電路902而變換成脈衝信 號。此時,調變電路902係配合於音樂信號VIN而對載波信 號施以脈衝寬幅調變。驅動電路903係依據經調變的脈衝信 號而互補地導通控制功率MOS電晶體904、905,並輸出經 電力放大的脈衝信號至輸出端子TO。該電力放大的脈衝信 號係藉由電感L和電容器C所組成的低域濾波器而除去載波 頻率成份,並形成電力放大的類比量的音樂信號而供應至 放音器SPK。 然而,上述之調變電路902因係以單一的電源VDD (例如 10V)來作動之一種構成,故其輸出信號的脈衝信號的低準 位係形成接地電位(〇 V),而高準位則為供應著電源VDD的 80426 1225333 電壓(10 V)。因此,依樣地使用具有如此信號準位的脈衝信 號,則在MOS電晶體的特性上,係無法將連接汲極於正電 源VPP+ (+50 V)的功率MOS電晶體904充分地控制於ON狀 態,而且無法將連接源極於負電源VPP- (-50V)的功率MOS 電晶體905控制於OFF狀態。因此,在驅動電路903中係有 必要作成依據調變電路902所調變的脈衝信號而用以控制 上述功率MOS電晶體904、905之用的機能。 以下說明驅動電路903。 為了控制輸出具有從正電源VPP+變化至負電源VPP-的 信號之功率MOS電晶體的導通狀態,雖只要自驅動電路903 供應能平衡於正電源VPP+與負電源VPP-的脈衝信號,至功 率MOS電晶體904、905的閘極即可,但卻必須使用高耐壓 電晶體所構成的驅動電路903 ’而導致成本的上昇。是故’ 藉由將分別驅動功率MOS電晶體904與功率MOS電晶體905 的電路的電源系統予以分離(絕緣)之措施,而使用能緩和施 加於各電路的實效電源電壓之方法而構成驅動電路903。 圖12所示之例示中,功率MOS電晶體904、905的雙方均 為η型,故驅動電路903係分離成功率MOS電晶體904的源極 電壓,亦即以顯現於輸出端子TO的輸出信號為基準的電源 系統、及功率MOS電晶體905的源極電壓,亦即以供應負電 源VPP-的電壓為基準的電源系統。是故,驅動功率MOS電 晶體904的電路的電源系統,係追隨於顯現於輸出端子TO 的輸出信號的電壓變化而產生變動。然而,當驅動電路903 的電源系統如此追隨於顯現於輸出端子TO的輸出信號時, 80426 2相對於前段側的調變電路902所輸出的脈衝信號的信號 準位,驅動電路903的輸入臨界值即形成變動之狀態,而產 生所1鴿法正確地從調變電路9〇2傳送信號至驅動電路9〇3 的不適切情形。 心而用以解決如此不適切情形的第丨習知技術,係使用自益 ^^l(b〇otstrap clrcu⑴之技術,而將調變電路所輸出的 脈衝仏號昇壓至適合於驅動電路9〇3側的信號準位。 兩此外作為第2習知技術,係使用絕緣變壓器,而將調變 私各902所輸出的脈衝信號電壓變換至適合於驅動電路 側的信號準位。 甚至作為第3習知技術,係使用光耦合器而調變調變電 各902口的幸則出#號成光信號,而傳送至驅動電路9〇3侧。 是根據上述之第1習知技術,由於為了變換調變電路 所輸出的信號的準位而使用自益電路,故有信號頻率變高 而形成動作不安定之問題。 ,外’根據上述之第2、第3習知技術,由於絕緣變壓器 或先耦合器等的電子元件其價格較高而使成本上昇。而 且’必須確❹以構裝此類電子元件的空間,而使裝置大 知構成中’係作成調變電路術為以 =統的電源·作動之構成,但假定輸入段9〇ι、調變 私路902、驅動電路9〇3的全 ^ vpp , ^ E塊為以南電壓系統的正電 ’原VPP+、負電源vppj 淮户 力則撕須如上述般地變換信號 卞位’而旎使電路構成簡略化。 …、而,在此情形下,對於 80426 1225333 全部區塊則因為必須使用耐高壓製程的製造技術,縱使假 定分別將各區塊施以IC化’亦必然使個個⑽之製造成本 上昇。 本發明係有鑑於上述情形而創作,以提供一種不使用特 殊私路技術或電子元件而能驅動控制輸出用功率電晶 體、且能抑@高耐壓製程的必要使用於最小限度之〇級放大 器。 【發明内容】 為解決上述之問題,本發明具有以下之構成。 亦即,申请專利範圍第丨項所記載之本發明之〇級放大 為,其係具有·第1輸出用電晶體,其係在正電源與輸出端 :《間連接電流路a ;第2輸出用電晶體,其係在負電源與 前述輸出端子之間連接電流路徑;並將包含於中介輸入端 子而自外#所輸人的信號之資訊成份,予以反映於脈衝寬 幅而調變該信號成脈衝信號,且依據該脈衝信號而互補地 導通前述第1及第2輸出用電晶體而構成,其特徵在於:具 備:互補信號產生電$,其係產生由#述脈衝信號的同相 信號和反相信號所組成的第丨互補信號並予以輸出;信號變 換電路,其係在維持前述同相信號的信號準位和前述反相 信號的信號準位之間的大小關係於原狀之狀態下,將前述 第1互補信號予以準位變換成第2互補信號,而該第^互補信 號為追隨於以前述第1或第2輸出用電晶體的源極電壓為基 準的既定電壓;驅動電路,其係以前述源極電壓為基準的 内部電源而作動,且輸入前述第2互補信號並依據包含於該 80426 -10- 1225333 第2互補信號的前述同相信號的信號成份和前述反相信號 的信號成份,而驅動前述第1或第2輸出用電晶體。 根據該構成,即可因應於調變電路所輸出的脈衝信號的 信號準位,而決定構成第1互補信號的同相信號和反相信號 的各信號準位。例如,脈衝信號為高準位時,同相信號係 形成高準位而反相信號係形成低準位。反之,若脈衝信號 為低準位時,同相信號係形成低準位而反相信號係形成高 準位。亦即,由調變電路所輸出的脈衝信號的信號準位, 係變換成構成第1互補信號的同相信號和反相信號的各信 號準位的組合,且重新呈現此類同相信號和反相信號的大 小關係。是故’在維持該大小關係於原狀下,同相信號和 反相信號的各信號成份即作為第2互補信號而呈現。驅動電 路係依據構成第2互補信號的同相信號和反相信號的差份 而控制第1或第2輸出用電晶體。 於是,第2互補信號即使係追隨於以前述第丨或第2輸出用 電晶體的源極電壓為基準的既定電壓而變化,因包含於兮 第2互補信號的同相信號和反相信號的各成份的大小關係 係被維持,故由該大小關係而能掌握由調變電路所輸出的 脈衝信號的信號準位。因此,根據本發明,即無須使用特 殊之製造製程或電子元件,即能傳送脈衝信號於電源系統 為分離的驅動電路,而能驅動控制輸出用電晶體。 、 申請專利範圍第2項所記載之本發明,其係如記載於申二太 專利範圍第i項之D級放大器,其特徵在於:前述變換電2 係具備:一對的第1電阻,其係連接於呈現前述第丨互^传 -11 - 80426 號的前述信號變換電路的一對的輸出部、和呈現前述第2互 補信號的前述驅動電路的一對的輸入部之間;一對的第2電 阻,其係一端側為連接於前述驅動電路的一對的輸入部; 偏壓電路’其係將前述一對的第2電阻的他端側偏壓成前述 既定電壓。 申叫專利庫巳圍第3項所記載之本發明,其係如記載於申請 專利範圍第2項之D級放大器,其特徵在於··更具備:電容 /、係用以修JL寄生於自别述信號變換電路的一對的輸 =部而達於前述驅動電路的—對的輸人部之信號路徑上的 電容量成份的非平衡狀態。 申請專利第4項所記載之本發明,纟係如記載於中請 專利範圍第2項或第3項之D級放大器,其特徵在於:更具 備·電流注人電路,其係注人電流於前述—對的第i電阻, 以消除流通於該一對的第丨電阻的同相電流。 申請專利範㈣5項所記載之本發明,其係如記載於申請 =範圍第4項之D級放大器,其特徵在於:前述電流注入 =係由如下所組成:電流監视電路,其係監視流通於前 的第!電阻的同相電流。電流反射鏡電路,其係輸入 則逑電流監視電路所監顽乏兩、、云,*击人, 哈、六、k 1皿視《私,瓜,並輸出和該電流等值的 电 於前述一對的第J電阻。 專Sit圍第6項所記載之本發明’其係如記載於中請 3 之D級放大器,其特徵在於:前述偏 ^路係由雙輸出型的運算放大器所構成,該運算放大器 ,、有.反相輸入部,其係連接於前述第2電阻的他端側;非 80426 -12- 1225333 反相輸入部,其係輸入著前述既定電壓;一對的輸出部, 其係連接著前述一對的第2電阻的一端侧。 【實施方式】 以下,參閱圖面而說明本發明之實施形態。 (實施形態1) 圖1係表示該實施形態1之D級放大器DAMP之構成及使 用例。該圖中,信號源SIG係具有以接地電位(Ο V)作為振幅 中點的類比量的音樂信號(類比量)的產生源,輸入電容器 CIN係用以遮斷直流成份者,來信號源SIG所供應的信號係 中介電容器CIN,而作為音樂信號VIN並供應於D級放大器 DAMP的輸入端子TI 〇 D級放大器DAMP係所謂的PWM放大器,由輸入段100、 調變電路200、驅動控制電路300、η型功率MOS電晶體401、 402所構成。 此處,輸入段100係相當於前述習知技術之輸入段901, 其係由輸入電阻R1和回授電阻R2 (=R1)和反相回授型的運 算放大器OP所構成。輸入電阻R1的一端係連接於運算放大 器OP的反相輸入部(-),而其另一端係連接於輸入端子TI。 回授電阻R2係連接於運算放大器OP的反相輸入部和輸出 部之間。在運算放大器OP的非反相輸入部係施加有基準電 壓VREF。因基準電壓VREF係由未圖示之電壓產生部所產 生,故以電阻分割例如供應著標準電源VDD的電壓而產 生,並設定成電源VDD的2分之1。 如此構成之輸入段100,係以放大率「1」的反相放大器 -13 -1225333 发明 Description of the invention: [Technical field to which the invention belongs] The present invention relates to a technology related to a class D amplifier (digital amplification) that converts an analog signal such as a music signal into a pulse signal and applies power amplification, and particularly relates to the use of Circuit technology to drive and control the power Mos transistor. [Prior art] It is known that there is a D-class amplifier that uses an analog signal such as a music signal as an input signal and converts it into a pulse signal to apply power amplification. The output terminal is a low-domain filter. Connected to the input terminal of the amplifier. According to this class D amplifier, the amplitude (data component) of the input signal is reflected by the pulse width and the pulse signal amplified by power is output. Moreover, the pulse ## is passed through a low-domain filter to extract an analogue amount of music signal amplified by electric power, and the music signal drives the player. Because the D-class amplifier can be formed on a silicon chip, it can realize a small and inexpensive design. It is often used in portable terminals or personal computers that require low power consumption. FIG. 12 shows an example of use of the configuration of the D-class amplifier 900. In the figure, the “仏” source SIG is a generation source of a music signal VIN using the ground potential (0v) as an analog of the amplitude midpoint, and it is an input capacitor that the DC component of the music signal is blocked by the intermediary ( (Not shown), and is connected to the input terminal TI of the D-class amplifier 900. The Class D amplifier 900 is a so-called PWM amplifier (PWM: Pulse Width Modulation), which is composed of an input section 901, a modulation circuit 902, a driving circuit 903, and n-type power MOS transistors 904 and 905. The input section 901 shifts the midpoint of the music signal VIN, and changes the audio signal 80426 into a waveform of the input characteristics of the modulation circuit 902 suitable for the operation of the power supply VDD (for example, 10 V). The modulation circuit 902 converts the music signal output from the input section 901 into a pulse signal, and reflects the information component of the music signal in a pulse width to perform PWM modulation. The driving circuit 903 drives the control output power MOS transistors 904 and 905 complementarily based on the pulse signal modulated by the modulation circuit 902. The power MOS transistor 904 is connected with a current path between the positive power source VPP + (for example, +50 V) and the output terminal TO, and is used to output a high level. In addition, the power MOS transistor 905 is connected with a current path between the negative power supply VPP- (for example, _50 V) and the output terminal TO, and is used to output a low level. The output terminal TO is connected to the input terminal of the SPK via a low-domain filter composed of an inductor L and a capacitor C. According to the class D amplifier 900, the music signal VIN input from the signal source SIG is converted into a pulse signal through the input section 901 and the modulation circuit 902. At this time, the modulation circuit 902 performs pulse width modulation on the carrier signal in accordance with the music signal VIN. The driving circuit 903 is based on the modulated pulse signal to complementarily turn on and control the power MOS transistors 904 and 905, and outputs a pulse signal amplified by electric power to the output terminal TO. The power-amplified pulse signal is supplied to the amplifier SPK by removing a carrier frequency component by a low-domain filter composed of an inductor L and a capacitor C, and forming an analog signal of a power amplification. However, the above-mentioned modulation circuit 902 operates with a single power source VDD (for example, 10V). Therefore, the low level of the pulse signal of the output signal forms the ground potential (0V) and the high level It is the 80426 1225333 voltage (10 V) supplied with the power supply VDD. Therefore, if a pulse signal with such a signal level is used as it is, the characteristics of the MOS transistor cannot fully control the power MOS transistor 904 connected to the positive power supply VPP + (+50 V) to ON. State, and the power MOS transistor 905 connected to the negative power source VPP- (-50V) cannot be controlled to the OFF state. Therefore, in the driving circuit 903, it is necessary to create a function for controlling the power MOS transistors 904 and 905 according to the pulse signal modulated by the modulation circuit 902. The driving circuit 903 will be described below. In order to control the conduction state of the power MOS transistor that outputs a signal that changes from the positive power supply VPP + to the negative power supply VPP-, although the self-driving circuit 903 supplies a pulse signal that can balance the positive power supply VPP + and the negative power supply VPP- to the power MOS The gates of the transistors 904 and 905 are sufficient, but a driving circuit 903 ′ composed of a high-withstand piezoelectric crystal must be used, resulting in an increase in cost. That's why. By separating (insulating) the power supply system that drives the circuits of the power MOS transistor 904 and the power MOS transistor 905 separately, the driving circuit is constructed by using a method that reduces the effective power supply voltage applied to each circuit. 903. In the example shown in FIG. 12, both of the power MOS transistors 904 and 905 are n-type, so the driving circuit 903 is a source voltage of the MOS transistor 904 with a success rate of separation, that is, the output signal appearing at the output terminal TO. The reference power supply system and the source voltage of the power MOS transistor 905, that is, the power supply system based on the voltage of the negative power supply VPP-. Therefore, the power supply system for driving the circuit of the power MOS transistor 904 changes in accordance with the voltage change of the output signal appearing at the output terminal TO. However, when the power supply system of the driving circuit 903 follows the output signal appearing at the output terminal TO in this way, the input level of the driving circuit 903 is critical relative to the signal level of the pulse signal output from the modulation circuit 902 on the front side. The value is in a fluctuating state, and the unsuitable situation in which the first pigeonhole method correctly transmits a signal from the modulation circuit 902 to the driving circuit 903 is generated. The first known technique to solve such uncomfortable situations is to use the technique of self-help ^^ l (b〇otstrap clrcu⑴) to boost the pulse number 仏 output by the modulation circuit to be suitable for the driving circuit. The signal level on the 903 side. In addition, as a second conventional technique, an insulated transformer is used to convert the pulse signal voltage output from the modulation unit 902 to a signal level suitable for the drive circuit side. Even as The third conventional technique is to use an optical coupler to modulate each of the 902 ports of the modulation circuit. The # signal is converted into an optical signal and transmitted to the 903 side of the drive circuit. It is based on the first conventional technique described above. The self-benefit circuit is used to change the level of the signal output from the modulation circuit, so there is a problem that the signal frequency becomes high and the operation is unstable. According to the above-mentioned second and third conventional techniques, the insulation transformer Electronic components such as or couplers have higher prices and increase costs. Moreover, 'the space for the installation of such electronic components must be determined, and the device must be constructed in the system'. Traditional power supply and operating structure It is assumed that the input section 90m, the modulation private circuit 902, and the drive circuit 903 are all ^ vpp, ^ E blocks are the positive electricity of the south voltage system, the original VPP +, and the negative power supply vppj. The signal structure is changed as described above to simplify the circuit configuration .... In this case, for all blocks of 80426 1225333, it is necessary to use a manufacturing technology capable of withstanding high voltages. Even if each block is assumed to be separate, The implementation of IC technology will also inevitably increase the manufacturing cost of each individual. The present invention was created in view of the above circumstances, in order to provide a power transistor that can drive and control output without using special private circuit technology or electronic components. In order to solve the above problems, the present invention has the following structure. That is, the invention described in item 丨 of the application scope The stage amplification is as follows: it has a first output transistor, which is connected between the positive power source and the output terminal: "between the current path a; a second output transistor, which is between the negative power source and the aforementioned output terminal. Connect the current path; reflect the information component of the signal input from the external input terminal and from outside # to the pulse width and modulate the signal into a pulse signal, and turn on the aforementioned first part complementaryly according to the pulse signal The first and second outputs are composed of transistors, and are characterized in that they include: a complementary signal generating electric $, which generates and outputs a complementary signal composed of an in-phase signal and an in-phase signal of the pulse signal; The signal conversion circuit transforms the first complementary signal into a second complementary signal while maintaining the magnitude relationship between the signal level of the in-phase signal and the signal level of the inverted signal. And the third complementary signal is a predetermined voltage that follows the source voltage of the first or second output transistor as a reference; the driving circuit is operated by an internal power source based on the source voltage, And input the second complementary signal and drive according to the signal component of the in-phase signal and the signal component of the inverting signal included in the 80426 -10- 1225333 second complementary signal. Operate the first or second output transistor. According to this configuration, the signal levels of the in-phase signal and the reverse-phase signal constituting the first complementary signal can be determined according to the signal level of the pulse signal output from the modulation circuit. For example, when the pulse signal is at a high level, the in-phase signal is at a high level and the inverting signal is at a low level. Conversely, if the pulse signal is at a low level, the in-phase signal is formed at a low level and the inverted signal is formed at a high level. That is, the signal level of the pulse signal output by the modulation circuit is converted into a combination of the signal levels of the in-phase signal and the inverse signal constituting the first complementary signal, and such in-phase signals are re-presented. And the magnitude of the inverted signal. Therefore, while maintaining this magnitude relationship as it is, each signal component of the in-phase signal and the reverse-phase signal is presented as a second complementary signal. The driving circuit controls the first or second output transistor based on the difference between the in-phase signal and the inverting signal constituting the second complementary signal. Therefore, even if the second complementary signal follows a predetermined voltage based on the source voltage of the first or second output transistor as a reference, the second complementary signal is included in the in-phase signal and the inverting signal included in the second complementary signal. The magnitude relationship of each component is maintained, so the signal level of the pulse signal output by the modulation circuit can be grasped from the magnitude relationship. Therefore, according to the present invention, it is not necessary to use a special manufacturing process or electronic components, that is, the pulse signal can be transmitted to the power supply system as a separate driving circuit, and the output transistor can be driven. The invention described in item 2 of the scope of patent application is the D-class amplifier described in item i of the scope of Shen Ertai's patent, which is characterized in that the conversion circuit 2 is provided with: a pair of first resistors, It is connected between a pair of output sections of the aforementioned signal conversion circuit which presents the aforementioned No. 11-80426 and a pair of input sections of the aforementioned drive circuit which presents the aforementioned second complementary signal; The second resistor has one input side connected to a pair of input portions of the driving circuit, and the bias circuit 'bias the other terminal side of the second resistor of the pair to the predetermined voltage. The application is called the invention described in item 3 of the patent library, which is a class D amplifier as described in item 2 of the scope of the patent application, and is characterized by: more: a capacitor /, which is used to repair JL parasitic The unbalanced state of the capacitance component on the signal path of the input pair of the driving circuit of the pair of input circuits of the aforementioned driving circuit is not mentioned separately. The invention described in item 4 of the application for patent is not a class D amplifier as described in item 2 or item 3 of the patent scope, which is further equipped with a current injection circuit which injects current into the circuit. The i-th resistor of the pair is used to eliminate the in-phase current flowing through the i-th resistor of the pair. The invention described in item 5 of the patent application is the D-class amplifier described in the fourth item of the scope of the application. The current injection is composed of the following: a current monitoring circuit that monitors the flow of electricity. The in-phase current of the first! Resistor. The current mirror circuit, its input is the current monitoring circuit monitored by the two monitors, the cloud, the shock, the ha, six, and k 1 dishes as "private, melon, and output the current equivalent to the current The Jth resistance of a pair. The present invention described in item 6 of Sit 'is a class D amplifier as described in Zhongyou 3, characterized in that the aforementioned bias circuit is composed of a dual output type operational amplifier, and the operational amplifier has, Inverting input section, which is connected to the other end of the second resistor; not 80426 -12-1225333 Inverting input section, which inputs the predetermined voltage; a pair of output sections, which are connected to the first One end of the second resistor pair. [Embodiment] Hereinafter, an embodiment of the present invention will be described with reference to the drawings. (Embodiment 1) Fig. 1 shows a configuration and a use example of a D-class amplifier DAMP according to the first embodiment. In the figure, the signal source SIG is a source of generating a music signal (analog quantity) with an analog quantity using the ground potential (0 V) as the midpoint of the amplitude. The input capacitor CIN is used to block the DC component. The supplied signal is an intermediate capacitor CIN, and is supplied as a music signal VIN to the input terminal TI of the D-class amplifier DAMP. The D-class amplifier DAMP is a so-called PWM amplifier. The input section 100, the modulation circuit 200, and the drive control circuit 300, n-type power MOS transistors 401, 402. Here, the input section 100 is equivalent to the input section 901 of the conventional technology, which is composed of an input resistor R1 and a feedback resistor R2 (= R1) and an inverting feedback type operational amplifier OP. One end of the input resistance R1 is connected to the inverting input section (-) of the operational amplifier OP, and the other end is connected to the input terminal TI. The feedback resistor R2 is connected between the inverting input section and the output section of the operational amplifier OP. A reference voltage VREF is applied to a non-inverting input section of the operational amplifier OP. Since the reference voltage VREF is generated by a voltage generating unit (not shown), it is generated by dividing the voltage with a standard power supply VDD, for example, and is set to 1/2 of the power supply VDD. The input section 100 thus constituted is an inverting amplifier with an amplification factor "1" -13-
80426 1225333 而作動,並以基準信號VREF為中點而輸出使音樂信號VIN 的相位反相的信號。據此,而將來自信號源SIG所輸入的音 樂信號VIN變換成適合於後段側的調變電路200的信號。 又,該實施形態係將電源VDD電壓作成「+10 V」,以作 為該技術領域之標準電源電壓。 調變電路200係和前述習知技術之調變電路902相同構 成,其係將來自前段的輸入段100所輸出的音樂信號變換成 脈衝信號,而將該音樂信號的資訊成份反應於脈衝寬幅而 進行PWM調變。以下之說明,係將PWM調變而自調變電路 200所輸出之脈衝信號稱為「PWM信號」。 驅動控制電路300係本發明者,其係依據來自調變電路 200所輸出之PWM信號,而互補地驅動控制輸出用之功率 MOS電晶體401和功率MOS電晶體402。該驅動控制電路300 雖係對應於前述習知技術之驅動電路903,但其構成上之特 徵,則係自調變電路200所輸出之PWM信號產生互補信號 (同相信號及反相信號),並依據構成該互補信號的同相信號 及反相信號,而能互補地驅動控制一對的功率MOS電晶體 401、402而構成之。有關該驅動控制電路300之詳細容於後 述0 功率MOS電晶體401係用以輸出高準位於輸出端子TO 者,其汲極及源極為分別連接於正電源VPP+及輸出端子 TO。另一方的功率MOS電晶體402係用以輸出低準位於輸 出端子TO者,其汲極及源極為分別連接於負電源VPP-及輸 出端子TO。本實施形態1係將正電源VPP+的電壓作成 -14-80426 1225333 operates and outputs a signal that inverts the phase of the music signal VIN with the reference signal VREF as the midpoint. Accordingly, the music signal VIN input from the signal source SIG is converted into a signal suitable for the modulation circuit 200 on the rear stage side. In this embodiment, the power supply VDD voltage is made "+10 V" as a standard power supply voltage in the technical field. The modulation circuit 200 has the same structure as the modulation circuit 902 of the above-mentioned conventional technology. It converts the music signal output from the input section 100 of the previous stage into a pulse signal, and reflects the information component of the music signal to the pulse. Wide PWM modulation. In the following description, the PWM signal and the pulse signal output from the self-modulation circuit 200 are referred to as "PWM signals". The drive control circuit 300 is the inventor of the present invention. It drives the power MOS transistor 401 and the power MOS transistor 402 for control output in a complementary manner based on the PWM signal output from the modulation circuit 200. Although the driving control circuit 300 corresponds to the driving circuit 903 of the aforementioned conventional technology, its structural feature is that the PWM signals output by the self-modulation circuit 200 generate complementary signals (in-phase signals and inverted signals). According to the in-phase signal and the inverting signal constituting the complementary signal, the pair of power MOS transistors 401 and 402 can be driven and controlled complementarily. The details of the drive control circuit 300 are described later. The 0 power MOS transistor 401 is used to output Micro Motion at the output terminal TO, and its drain and source are connected to the positive power supply VPP + and the output terminal TO, respectively. The other power MOS transistor 402 is used for outputting a person who is located at the output terminal TO, whose drain and source are connected to the negative power supply VPP- and the output terminal TO, respectively. In the first embodiment, the voltage of the positive power source VPP + is made -14-
80426 1225333 「+50 V」、負電源VPP-的電壓作成「-50 V」。 輸出端子TO係中介由電感L和電容器C所組成的低域濾 波器而連接於放音器SPK的一方的輸入端子,該放音器SPK 的另一方的輸入端子係接地。由電感L和電容器C所組成的 低域滤波器的常數,係設定成能去除中介輸出端子TO而來 自D級放大器DAMP所輸出之脈衝信號之載波頻率成份,且 能通過音樂信號成分之狀態。 如上述,該D級放大器DAMP係以標準電源VDD、正電源 VPP+、負電源VPP-的3個電源而作動。 繼之,詳細說明驅動控制電路300之構成。 圖2為表示驅動控制電路300之構成。該圖中,和圖1所示 之構成要素相共通之要素係賦予相同符號。 圖2所示之驅動控制電路300之構成,係備有互補信號產 生電路301H、信號變換電路302H、及驅動電路303H,以作 為用以驅動一方的功率MOS電晶體401之電路系統(以下稱 高側驅動),且備有互補信號產生電路301L、信號變換電路 302L、及驅動電路303L,以作為用以驅動另一方的功率MOS 電晶體402之電路系統(以下稱低側驅動)。呈現於功率MOS 電晶體401和功率MOS電晶體402的汲極的連接點的信號, 係作為該D級放大器DAMP的輸出信號OUT,並中介上述之 輸出端子TO而輸出至外部。 首先,詳細說明高側驅動之構成。 互補信號產生電路301H係產生一種來自上述之調變電路 200所輸出之PWM信號的同相信號H1及反相信號H2,係由 -15-80426 1225333 The voltage of "+50 V" and negative power supply VPP- is made "-50 V". The output terminal TO is a low-domain filter composed of an inductor L and a capacitor C, and is connected to one input terminal of the sounder SPK, and the other input terminal of the sounder SPK is grounded. The constants of the low-domain filter composed of the inductor L and the capacitor C are set so that the carrier frequency component of the pulse signal output from the D-level amplifier DAMP can be removed from the intermediate output terminal TO, and can pass through the state of the music signal component. As described above, the D-class amplifier DAMP operates with three power sources: a standard power source VDD, a positive power source VPP +, and a negative power source VPP-. Next, the configuration of the drive control circuit 300 will be described in detail. FIG. 2 shows a configuration of the drive control circuit 300. In this figure, the same elements as those shown in FIG. 1 are assigned the same reference numerals. The structure of the drive control circuit 300 shown in FIG. 2 is provided with a complementary signal generating circuit 301H, a signal conversion circuit 302H, and a drive circuit 303H as a circuit system for driving one power MOS transistor 401 (hereinafter referred to as high Side drive), and a complementary signal generating circuit 301L, a signal conversion circuit 302L, and a drive circuit 303L are provided as a circuit system for driving the other power MOS transistor 402 (hereinafter referred to as low-side drive). The signal presented at the connection point of the drain terminals of the power MOS transistor 401 and the power MOS transistor 402 is output as the output signal OUT of the class D amplifier DAMP, and is output to the outside via the output terminal TO described above. First, the configuration of the high-side drive will be described in detail. The complementary signal generating circuit 301H generates an in-phase signal H1 and an inverting signal H2 from the PWM signal output by the above-mentioned modulation circuit 200.
80426 1225333 CMOS (Complementary Metal Oxide Semiconductot)構成的 緩衝器Bll、B12及反相輸入型的緩衝器(反相器)B13所構 成。此處,在緩衝器B11的輸入部係供應來自調變電路200 所輸出之PWM信號,其輸_部係共通地連接於緩衝器 B12、B13的輸入部。此類之緩衝器Bll、B12、B13係供應 電源VDD而作動,並自緩衝器B12、B13分別輸出PWM信號 的同相信號H1及反相信號H2。此類之同相信號H1及反相信 號H2係作為互補信號(HI、H2)而輸出至信號變換電路 302H。 信號變換電路302H,係將同相信號H1及反相信號H2,予 以準位變換成追隨於以功率MOS電晶體401的源極電壓VS (亦即輸出信號OUT的信號準位)為基準的既定電壓vr 1之 同相信號H3及反相信號H4者,係由一對的電阻ri卜Ri2 (一 對的第1電阻)、一對的電阻R13、R14 (一對的第2電阻)、以 及偏壓電路P11所構成。同相信號H3及反相信號H4,係供 應至構成後段側的驅動電路3〇3H的比較器CM1的一對的輸 入邵(非反相輸入部及反相輸入部)。 此處,在呈現同相信號H1及反相信號H2的緩衝器Bl2、 B13的。一對的輸出部,和呈現同相信號H3及反相信號 比較器CM1的—對的輸人部之間,係連接著—對的電阻 R^、R12。亦即,電阻Ru的一端係連接於緩衝器Μ的輸 出邯,其另—端係連接於比較器〇]^1的非反相輸入部。此 =’電阻R12的—端係連接於緩衝器Bn的輸出部,其另一 端係連接於比較器CM1的反相輸入部。此類之電阻r^、ri2 80426 -16- 係形成一自互補信號產生電路301H用以傳送同相信號HI 及反相信號H2至驅動電路303H之線路。 此外,在比較器CM1的一對的輸入部係分別連接著一對 的電阻R13、R14的一端,該電阻R13、R14的另一端係藉由 偏壓電路P11,而偏壓成以功率MOS電晶體401的源極電壓VS 為基準的既定電壓VR1。本實施形態中,既定電壓VR1係設 定成加上電源VDD的2分之1於源極電壓VS之值(=VS + VDD/2) 。此時,因電源VDD係10 V,故加算其一半的5 V於源極電 壓VS的電壓即形成既定電壓VR1。 圖3係表示偏壓電路P11的構成例。如該圖所示,偏壓電 路P11係在正電源VPP+和呈現上述之源極電壓VS的節點 (亦即功率MOS電晶體401的源極)之間,串接著電阻PR及蕭 特基二極體PD,且蕭特基二極體PD和安定化之電容器PC 作並列連接而構成,並將呈現於電阻PR和蕭特基二極體PD 的連接點的電壓作成既定電壓VR1。該實施形態1中,蕭特 基二極體PD的屏障電壓係設定成相當於電源VDD (10 V)的 2分之1的5 V,據此,上述之既定電壓VR1即產生加上電源 VDD的2分之1於源極電壓VS之值(=VS + VDD / 2)者。 繼之,回至圖2說明驅動電路303H之構成。 驅動電路303H係一驅動控制功率MOS電晶體401者,由比 較器CM1、緩衝器B14、及内部電源P12所構成。此處,比 較器CM1的非反相輸入部係中介電阻Rl 1而連接於緩衝器 B 12的輸出部,而反相輸入部係中介電阻R12而連接於緩衝 器B 13的輸入部。此外,比較器CM1的輸出部係連接於緩衝 80426 -17- 1225333 态B14的輸入部,該緩衝器B14的輸0部係連接於上述功率 MOS電晶體4〇1的閘極。 内部電源P12係以功率MOS電晶體401的源極電壓又8為 基準’而產生相當於電源VDD的電壓VD1者,基本上係和上 述圖2所示之偏壓電路相同之構成。其中,此時之蕭特基二 極fa PD的屏障電壓係設定成相當於電源vdd的電壓之丨〇 v 。該内部電源P12係以源極電壓vs為基準而產生相當於電 · 源VDD的電壓VD1,並作為電源電壓而供應於上述之比較 < 姦CM1和緩衝器B14。因此,驅動電路3〇3H的電源系統,係._ 在追ik於功率MOS電晶體401的源極電壓vs而產生變化的 同時,亦作為等值於比較器(^乂丨與緩衝器B14相關的限制電 源VDD之電源而作動。以上係說明用以驅動功率M〇s電晶 體40 1的高側驅動之構成。 繼之,說明用以驅動功率M0S電晶體4〇2的低側驅動之構 成。 構成低側驅動之互補信號產生電路3〇1L、信號變換電路 302L、及驅動電路3〇3L係分別和構成上述高側驅動之互㉟馨 信號產生電路301H、信號變換電路3〇2H、及驅動電路3〇3H 、 為相同之構成。亦即,互補信號產生電路3 〇丨L係產生一種 、 來自上述之調變電路2〇〇所輸出之PWM信號的反相信號以 及同相仏號L2者,由緩衝器B21、B22、B23所構成,且此 類之緩衝器係分別對應於構成上述互補信號產纟電路3〇m 分別為正邏輯輸入型及負邏輯輸入型之構成,而緩衝器 80426 -18 - B22、B23則分別為負邏輯輸入型及正邏輯輸入型之構成。 此外,信號變換電路302L係由電阻R21、R22、R23、R24、 及偏壓電路P21所構成,且此類係分別對應於構成上述信號 變換電路302H之電阻R1卜R12、R13、R14、及偏壓電路P11。 其中,偏壓電路P21係以負電源VPP-為基準而產生相當於電 源VDD的2分之1之電壓VR2。 而且,驅動電路303L係由比較器CM2、緩衝器B24、及内 部電源P22所構成,且此類係分別對應於構成上述驅動電路 303H之比較器CM1、緩衝器B14、内部電源P12。其中,内 部電源P22係以功率MOS電晶體402的源極電壓(亦即負電 源VPP-)為基準而產生相當於電源VDD的電壓VD2,並作為 電源電壓而供應於比較器CM2和緩衝器B24。 以下,參閱圖4所示之波形圖及圖2所示之驅動控制電路 300說明本實施形態的動作。 又,圖4中,自調變電路200所輸出之PWM信號,因係和 同相信號H1相同之相位,故借用同相信號H1的波形而呈 現。 首先,說明高側驅動的動作。信號產生電路301H,係響 應於前述調變電路200所輸出之PWM信號,而產生具有和該 PWM信號相同相位的同相信號H1、以及具有相反相位的反 相信號H2。具體而言,若PWM信號為低準位,則輸出低準 位而作為同相信號H1,並輸出高準位而作為反相信號H2。 反之,若PWM信號為高準位,則輸出高準位而作為同相信 號H1,並輸出低準位而作為反相信號H2。亦即,互補信號 80426 -19- 1225333 產生電路301H,係將PWM信號的信號準位變換成同相信號 H1和反相信號H2之信號準位的組合,並重新呈現此類之信 號準位的大小關係。 圖4所示之波形圖中,其在初期狀態,調變電路2〇〇所輸80426 1225333 CMOS (Complementary Metal Oxide Semiconductot) buffers B11, B12 and inverting input type buffer (inverter) B13. Here, the input section of the buffer B11 is supplied with the PWM signal output from the modulation circuit 200, and its input section is connected in common to the input sections of the buffers B12 and B13. These buffers B11, B12, and B13 are operated by supplying power VDD, and output the in-phase signal H1 and the inverted signal H2 of the PWM signal from the buffers B12 and B13, respectively. These in-phase signals H1 and anti-trust signals H2 are output to the signal conversion circuit 302H as complementary signals (HI, H2). The signal conversion circuit 302H converts the in-phase signal H1 and the inverted signal H2 to a predetermined level and follows the source voltage VS of the power MOS transistor 401 (that is, the signal level of the output signal OUT) as a reference. The in-phase signal H3 and the inverting signal H4 of the voltage vr 1 are a pair of resistors ri2 (a pair of first resistors), a pair of resistors R13, R14 (a pair of second resistors), and The bias circuit P11 is configured. The non-inverting signal H3 and the inverting signal H4 are input to a pair of the comparator CM1 (the non-inverting input section and the inverting input section) which are supplied to the comparator CM1 constituting the driving circuit 303H on the rear side. Here, the buffers B12 and B13 presenting the in-phase signal H1 and the inverted signal H2. The pair of output sections and the pair of input sections of the comparator CM1 presenting the in-phase signal H3 and the inverting signal are connected to the pair of resistors R ^, R12. That is, one end of the resistor Ru is connected to the output of the buffer M, and the other end thereof is connected to the non-inverting input portion of the comparator 0] ^ 1. The-terminal of this = 'resistor R12 is connected to the output portion of the buffer Bn, and the other terminal thereof is connected to the inverting input portion of the comparator CM1. These resistors r ^, ri2 80426-16 form a line that generates a self-complementary signal generating circuit 301H for transmitting the in-phase signal HI and the inverted signal H2 to the driving circuit 303H. In addition, one pair of inputs of the comparator CM1 is connected to one end of a pair of resistors R13 and R14, and the other ends of the resistors R13 and R14 are biased to a power MOS by a bias circuit P11. The source voltage VS of the transistor 401 is a predetermined voltage VR1 based on the reference voltage. In the present embodiment, the predetermined voltage VR1 is set to a value (= VS + VDD / 2) in which one-half of the power source VDD is added to the source voltage VS. At this time, since the power source VDD is 10 V, the voltage of half of 5 V is added to the source voltage VS to form the predetermined voltage VR1. FIG. 3 shows a configuration example of the bias circuit P11. As shown in the figure, the bias circuit P11 is connected between the positive power supply VPP + and the node showing the above-mentioned source voltage VS (that is, the source of the power MOS transistor 401), followed by a resistor PR and Schottky II. The polar body PD is formed by connecting the Schottky diode PD and the stabilizing capacitor PC in parallel, and the voltage appearing at the connection point between the resistor PR and the Schottky diode PD is set to a predetermined voltage VR1. In the first embodiment, the barrier voltage of the Schottky diode PD is set to 5 V corresponding to one-half of the power source VDD (10 V). Based on this, the predetermined voltage VR1 described above is generated plus the power source VDD. 1/2 is the value of the source voltage VS (= VS + VDD / 2). Next, the structure of the driving circuit 303H will be described referring back to FIG. 2. The driving circuit 303H is a driver MOS transistor 401, which is composed of a comparator CM1, a buffer B14, and an internal power source P12. Here, the non-inverting input section of the comparator CM1 is connected to the output section of the buffer B 12 through the intermediate resistor R11, and the inverting input section is connected to the input section of the buffer B 13 through the intermediate resistor R12. In addition, the output part of the comparator CM1 is connected to the input part of the buffer 80426 -17-1225333 state B14, and the output part 0 of the buffer B14 is connected to the gate of the power MOS transistor 401. The internal power source P12 generates a voltage VD1 corresponding to the power source VDD based on the source voltage of the power MOS transistor 401 and 8 ', and basically has the same configuration as the bias circuit shown in FIG. 2 described above. Among them, the barrier voltage of the Schottky diode fa PD at this time is set to be equal to the voltage of the power supply vdd. This internal power source P12 generates a voltage VD1 corresponding to the power source VDD based on the source voltage vs. and supplies it to the above comparison < CM1 and the buffer B14 as the power source voltage. Therefore, the power supply system of the drive circuit 303H is the same as the source voltage vs. of the power MOS transistor 401 and changes as well as being equivalent to the comparator (^ 乂 丨 related to the buffer B14). The above is a description of the configuration of the high-side drive for driving the power transistor 401. Next, the configuration of the low-side drive for driving the power transistor 402 is described. The complementary signal generating circuit 301L, the signal conversion circuit 302L, and the driving circuit 303L constituting the low-side drive are respectively the mutual signal generating circuit 301H, the signal conversion circuit 302H, and the signal converting circuit 302H constituting the above-mentioned high-side drive. The driving circuit 303H has the same structure. That is, the complementary signal generating circuit 3〇 丨 L generates an inverted signal of the PWM signal output from the modulation circuit 2000 described above and the in-phase signal L2. Or, it is composed of buffers B21, B22, and B23, and such buffers correspond to the configurations of the complementary signal generating circuit 30m, which are respectively a positive logic input type and a negative logic input type, and the buffers are 80426 -18-B22 B23 and B23 are respectively a negative logic input type and a positive logic input type. In addition, the signal conversion circuit 302L is composed of resistors R21, R22, R23, R24, and a bias circuit P21, and these types correspond to The resistors R1, R12, R13, R14, and bias circuit P11 constituting the above-mentioned signal conversion circuit 302H. Among them, the bias circuit P21 generates one-half of the power supply VDD based on the negative power supply VPP- as a reference. Voltage VR2. The driving circuit 303L is composed of a comparator CM2, a buffer B24, and an internal power supply P22, and these types correspond to the comparator CM1, the buffer B14, and the internal power supply P12, respectively, which constitute the driving circuit 303H. Among them, the internal power source P22 generates a voltage VD2 corresponding to the power source VDD based on the source voltage of the power MOS transistor 402 (ie, the negative power source VPP-), and supplies it to the comparator CM2 and the buffer B24 as the power source voltage. Hereinafter, the operation of this embodiment will be described with reference to the waveform diagram shown in Fig. 4 and the drive control circuit 300 shown in Fig. 2. In Fig. 4, the PWM signal output by the self-modulation circuit 200 is the same as Phase signal H1 is the same phase It is presented using the waveform of the in-phase signal H1. First, the operation of the high-side drive will be described. The signal generating circuit 301H generates the same signal as the PWM signal in response to the PWM signal output from the aforementioned modulation circuit 200. Phase in-phase signal H1 and phase-inverted signal H2. Specifically, if the PWM signal is at a low level, a low level is output as an in-phase signal H1, and a high level is output as an inversion Signal H2. Conversely, if the PWM signal is at a high level, the high level is output as the in-phase signal H1, and the low level is output as the inverted signal H2. That is, the complementary signal 80426 -19-1225333 generating circuit 301H transforms the signal level of the PWM signal into a combination of the signal level of the in-phase signal H1 and the inverted signal H2, and re-presents the signal level of this type. Size relationship. In the waveform diagram shown in FIG. 4, in the initial state, the output of the modulation circuit 2000 is
出之PWM信號係高準位,將其輸入的互補信號產生電路 3 01H,係輸出高準位而作為同相信號111,並輸出低準位而 作為反相信號H2。因此,初期狀態中,在同相信號m和反 相信號H2之間,係存在相當於電源VDD的準位差,同相信 號H1為較反相信號H2高出相當於電源VDD的電壓份。 自互補信號產生電路3〇1H所輸出的同相信號m及反相 信號H2,係中介構成信號變換電路3〇2H的電阻rii、ri2, 而以同相信號H3及反相信號H4供應至驅動電路3〇311側。此 時,構成該驅動電路303H的比較器CM1的輸入部,因係中The output PWM signal is a high level, and the complementary signal generating circuit 3 01H inputted thereto outputs a high level as an in-phase signal 111 and a low level as an inverted signal H2. Therefore, in the initial state, there is a level difference corresponding to the power supply VDD between the in-phase signal m and the reverse-phase signal H2, and the same confidence signal H1 is higher than the reverse-phase signal H2 by a voltage equivalent to the power supply VDD. The in-phase signal m and the inverting signal H2 output from the self-complementary signal generating circuit 3101H are the resistors rii and ri2 that constitute the signal conversion circuit 302H, and are supplied to the drive by the in-phase signal H3 and the inverting signal H4. Circuit 3031 side. At this time, the input part of the comparator CM1 constituting the driving circuit 303H is
介電阻R13、R14而連接於偏壓電路pu,故同相信號出的 #唬準位,係呈現出藉由電阻Ru、R13將偏壓電路ριι所產 生的電壓VR1和同相信號H1之間的電位差予以分壓而得的 電壓,且反相仏號H4係呈現出藉由電阻R12、Ri4將電壓 和反相信號H2之間的電位差予以分壓而得的電壓。因此, 同相信號H3及反相信號H4 #以給社甘丄, 你以維持其大小關係之狀態而 追隨於電壓VR1而產生變化。 驅動電路303H的比較器CM1從击入山 m — 平乂杂LM1係輸出一因應於同相信號 H3及反相信號H4的大小關係的彳士臃、、佳 、 剛你的t唬率位。初期狀態中,因 同相信號H3較反相信號H4其俨鲈淮户^ | ^ 1口就卞位較大,故比較器CM1 係輸出咼準位’而將其輸入的緩衝The dielectric resistors R13 and R14 are connected to the bias circuit pu. Therefore, the #blaze level of the in-phase signal shows the voltage VR1 and the in-phase signal H1 generated by the bias circuit ρι through the resistors Ru and R13. The voltage obtained by dividing the potential difference between the voltages, and the reverse phase H4 represents a voltage obtained by dividing the potential difference between the voltage and the reverse phase signal H2 by the resistors R12 and Ri4. Therefore, the in-phase signal H3 and the inverting signal H4 # are given to the company, and you follow the voltage VR1 in a state of maintaining the magnitude relationship, and change. The comparator CM1 of the driving circuit 303H outputs a signal from the knock-in mountain m — the flat hybrid LM1 system according to the magnitude relationship between the in-phase signal H3 and the inverting signal H4. In the initial state, since the in-phase signal H3 is larger than the inverting signal H4, the bass bit is larger. Therefore, the comparator CM1 outputs the “level” and buffers its input.
J、友衡姦B14,係以功率m〇S 80426 -20- 1225333 電晶體401的源極為基準而將具有相當於電源VDD的信號 準位之信號H5輸出至其閘極。據此,功率MOS電晶體401 係形成導通狀態。如後所述,功率MOS電晶體401、402係 控制成互補性的導通狀態,故當功率MOS電晶體401為導通 狀態時,功率MOS電晶體402即形成不導通狀態,而輸出信 號OUT的信號準位(亦即源極電壓VS)即上昇至正電源VPP+ 的電源電壓。 tJ. Youhengpu B14 is based on the source of power MOS 80426 -20-1225333 transistor 401 and outputs a signal H5 with a signal level equivalent to the power supply VDD to its gate. Accordingly, the power MOS transistor 401 is turned on. As described later, the power MOS transistors 401 and 402 are controlled to be in a complementary conducting state. Therefore, when the power MOS transistor 401 is in the conducting state, the power MOS transistor 402 is in a non-conducting state, and the signal of the output signal OUT is output. The level (ie, the source voltage VS) rises to the power supply voltage of the positive power supply VPP +. t
此時,驅動電路303H因係自内部電源P12供應以源極電壓 VS為基準的電壓VD1,故該驅動電路303H的電源系統係追 隨功率MOS電晶體401的源極電壓VS而上昇。因此,比較器 CM1的輸入臨界值亦和源極電壓VS同時上昇,但因偏壓電 路P11所產生的電壓VR1亦追隨源極電壓VS而上昇,故同相 信號H3及反相信號H4的各信號準位,係維持適合於構成驅 動電路303H的比較器CM1的輸入特性之狀態,且功率MOS 電晶體401係維持於導通狀態。該狀態中,信號H5的信號準 位係形成較正電源VPP+高出電壓VD1份(=VDD)之狀態。 亦即,内部電源P12因係和圖3所示之内部電源P11相同之 構成,故當輸出信號OUT的信號準位上昇至正電源VPP+ 時,中介相當於安定化電容器PC的電容器而昇壓電壓 VD1,並承受該電壓而信號H5的信號準位即形成較正電源 VPP+高出電壓VD1份(=VDD)之狀態。此狀態中,電壓VD1 雖因相當於圖3所示之電阻PR之電阻的存在而低於正電源 VPP +之電壓,但此種放大器因輸出信號OUT的頻率較高, 故藉由相當於安定化電容器PC的電容器,電壓VD1維持於 80426 -21 - 1225333 昇壓之狀態,而信號H5的信號準位維持於較正電源VPP+為 高之狀態。 一方的低側驅動中,初期狀態中輸入高準位的PWM信號 的互補信號產生電路301L,係輸出低準位而作為反相信號 L1,並輸出高準位而作為同相信號L2。因此,初期狀態中, 在反相信號L1和同相信號L2之間,係因應於該大小關係而 存在著相當於電源VDD的準位差,且反相信號L1係較同相 信號L2低下相當於電源VDD的電壓份。 自互補信號產生電路301L所輸出的反相信號L1和同相信 號L2,係中介構成信號變換電路302L的電阻R21、R22而以 反相信號L3和同相信號L4而供應至驅動電路303L側。此 時,反相信號L3的信號準位係呈現出藉由電阻R21、R23將 偏壓電路P21所產生的電壓VR2和反相信號L1之間的電位 差予以分壓而得的電壓,且同相信號L4的信號準位係呈現 出藉由電阻R22、R24將電壓VR2和同相信號L2之間的電位 差予以分壓而得的電壓。因此,反相信號L3及同相信號L4 係以維持其大小關係之狀態而追隨於電壓VR2而下降。 初期狀態中,驅動電路303L的比較器CM2,係因反相信 號L3較同相信號L4其信號準位較小,故輸出低準位,而將 其輸入的緩衝器B24,係將具有相等於功率MOS電晶體402 的源極電壓(VPP-)的信號準位的信號L5輸出至其閘極。因 此,功率MOS電晶體402係形成不導通狀態。此時,内部電 源P22因係產生以負電源VPP-為基準之電壓VD2,故驅動電 路303L的電源系統係位於低態,且該驅動電路303L的輸入 -22-At this time, the drive circuit 303H is supplied with the voltage VD1 based on the source voltage VS from the internal power supply P12, so the power supply system of the drive circuit 303H rises in accordance with the source voltage VS of the power MOS transistor 401. Therefore, the input threshold value of the comparator CM1 also rises at the same time as the source voltage VS, but the voltage VR1 generated by the bias circuit P11 also rises following the source voltage VS, so the in-phase signal H3 and the inverted signal H4 Each signal level is maintained in a state suitable for the input characteristics of the comparator CM1 constituting the driving circuit 303H, and the power MOS transistor 401 is maintained in an on state. In this state, the signal level of the signal H5 is in a state that is 1 part higher than the positive power supply VPP + voltage VD (= VDD). That is, the internal power supply P12 has the same structure as the internal power supply P11 shown in FIG. 3, so when the signal level of the output signal OUT rises to the positive power supply VPP +, the intermediary is equivalent to the capacitor of the stabilization capacitor PC and boosts the voltage. VD1, and bears the voltage, and the signal level of the signal H5 forms a state higher than the positive power supply VPP + by a voltage VD1 (= VDD). In this state, although the voltage VD1 is lower than the voltage of the positive power supply VPP + due to the presence of a resistance equivalent to the resistance PR shown in FIG. 3, because this amplifier has a higher frequency of the output signal OUT, The capacitor V of the capacitor PC is maintained at a voltage of 80426 -21-1225333, and the signal level of the signal H5 is maintained at a state higher than the positive power supply VPP +. In one low-side drive, a complementary signal generating circuit 301L that inputs a high-level PWM signal in an initial state outputs a low-level as an inverted signal L1 and outputs a high-level as an in-phase signal L2. Therefore, in the initial state, there is a level difference corresponding to the power supply VDD between the inverted signal L1 and the in-phase signal L2 due to the magnitude relationship, and the inverted signal L1 is substantially lower than the in-phase signal L2. The voltage portion of the power supply VDD. The inverted signal L1 and the same signal L2 outputted from the complementary signal generating circuit 301L are supplied to the drive circuit 303L side with the inverted signal L3 and the in-phase signal L4 via the resistors R21 and R22 constituting the signal conversion circuit 302L. At this time, the signal level of the inverted signal L3 is a voltage obtained by dividing the potential difference between the voltage VR2 generated by the bias circuit P21 and the inverted signal L1 through the resistors R21 and R23, and the same The signal level of the phase signal L4 is a voltage obtained by dividing the potential difference between the voltage VR2 and the in-phase signal L2 by the resistors R22 and R24. Therefore, the inverted signal L3 and the in-phase signal L4 follow the voltage VR2 and fall in a state of maintaining the magnitude relationship. In the initial state, the comparator CM2 of the driving circuit 303L outputs a low level because the inverted signal L3 has a lower signal level than the in-phase signal L4, and the buffer B24 inputted thereto has an equivalent The signal L5 of the signal level of the source voltage (VPP-) of the power MOS transistor 402 is output to its gate. Therefore, the power MOS transistor 402 is in a non-conducting state. At this time, the internal power supply P22 generates a voltage VD2 based on the negative power supply VPP-, so the power supply system of the driving circuit 303L is in a low state, and the input of the driving circuit 303L is -22-
80426 5s界值即位於降低狀態。但是,因偏壓電路p2丨所產生的電 壓VR2亦追隨功率MOS電晶體4〇1的源極電壓而位於降低 狀態,故反相信號L3和同相信號L4的各信號準位,係形成 合適於構成驅動電路3 03L的比較器CM 1的輸入特性的信號 準位,且功率MOS電晶體402係維持於不導通狀態。故在初 期狀怨’功率MOS電晶體401成導通狀態,而功率m〇S電晶 骨豆402形成不導通狀態,則形成能輸出相當於正電源vpp+ 的電壓的高準位之狀態,而作成輸出信號out。 自如此之初期狀態,在圖4所示之時間ti中,當pwM信號 遷移至低準位,響應於此而同相信號扪形成低準位且反相 k號H2形成高準位。是故,同相信號H1和反相信號η]的大 小關係即反過來,在時間t2中,同相信號H3和反相信號H4 的大小關係亦相反。因此,輸入同相信號H3和反相信號H4 的比較器CM 1的輸出信號即自高準位(較正電源vpp+高出 電壓VD1份的高電壓狀態)變化至低準位(相當於正電源 VPP+的電壓狀態),而將其輸入的緩衝器b14的輸出信號H5 亦變化至低準位(相當於正電源VPP+的電壓狀態)。其結 果’功率MOS電晶體401的閘極電壓即等於源極電壓vs (=正 電源VPP + ),而該功率電晶體4〇1即形成不導通狀態。 另一方面,在之時間tl中,當PWM信號遷移至低準位, 響應於此而反相信號L1形成高準位且同相信號L2形成低準 位。因此,反相信號L1和同相信號L2的大小關係即反轉, 響應於此而反相信號L3和同相信號L4的大小關係亦反轉。 疋故,比較益CM2的輸出信號即自低準位(相當於負電源 80426 -23- 1225333 VPP-的電壓狀態)變化至高準位(較負電源VPP-高出電壓 VD2份的高電壓狀態),而將其輸入的緩衝器B24的輸出信 號L5亦變化至高準位,其結果,功率MOS電晶體402的閘極 電壓即對源極電壓高出電壓VD2份,而該功率MOS電晶體 402即形成導通狀態。 當功率MOS電晶體402形成導通狀態時,功率MOS電晶體 401的源極電壓VS係隨著輸出信號OUT而降低,以此為基準 而内部電源P12所產生的電壓VD1亦下降。此時,偏壓電路 P11所產生的電壓VR1亦隨著功率MOS電晶體401的源極電 壓VS的變化而下降,故同相信號H1和反相信號H2的大小關 係維持原狀而此類之信號準位即和驅動電路303H的電源系 統一起下降。因此,比較器CM1所輸出的信號準位係維持 低準位(源極電壓VS)。據此,在輸出信號OUT遷移於低準 位(負電源VPP-)的過程中,功率MOS電晶體401係維持不導 通狀態。 因上述情形,自初期狀態在時間tl中,當PWM信號遷移 至低準位時,一方的功率MOS電晶體401係形成不導通狀 態,而另一方的功率MOS電晶體402即形成導通狀態,且輸 出信號OUT即自正電源VPP +遷移至負電源VPP-,並輸出低 準位。 繼之,在時間t3中,當PWM信號回復至高準位時,響應 於此而在時間t4中,高側驅動側的同相信號H3形成高準位 而反相信號H4形成低準位。因此,輸入此類同相信號H3和 反相信號H4的比較器CM1係輸出高準位,且功率MOS電晶 -24- aThe 80426 5s threshold is in a reduced state. However, because the voltage VR2 generated by the bias circuit p2 丨 also follows the source voltage of the power MOS transistor 401 and is in a reduced state, the respective levels of the inverted signal L3 and the in-phase signal L4 are formed. The signal level of the input characteristic of the comparator CM 1 suitable for constituting the driving circuit 303L is maintained, and the power MOS transistor 402 is maintained in a non-conducting state. Therefore, in the initial state, the power MOS transistor 401 is turned on, and the power transistor 402 is turned off, and a high level state capable of outputting a voltage equivalent to the positive power supply vpp + is formed. Output signal out. From such an initial state, at time ti shown in FIG. 4, when the pwM signal shifts to a low level, the in-phase signal 扪 forms a low level in response to this and the inverse k number H2 forms a high level. Therefore, the magnitude relationship between the in-phase signal H1 and the inverted signal η] is reversed. At time t2, the magnitude relationship between the in-phase signal H3 and the inverted signal H4 is also reversed. Therefore, the output signal of the comparator CM 1 that inputs the in-phase signal H3 and the inverting signal H4 is changed from a high level (higher voltage state than the positive power supply vpp + higher than the voltage VD) to a low level (equivalent to the positive power supply VPP + Voltage state), and the output signal H5 of the buffer b14 to which it is input also changes to a low level (equivalent to the voltage state of the positive power supply VPP +). As a result, the gate voltage of the power MOS transistor 401 is equal to the source voltage vs (= positive power supply VPP +), and the power transistor 401 is in a non-conducting state. On the other hand, at time t1, when the PWM signal shifts to a low level, the inversion signal L1 forms a high level and the in-phase signal L2 forms a low level in response to this. Therefore, the magnitude relationship between the inverted signal L1 and the in-phase signal L2 is reversed, and the magnitude relationship between the inverted signal L3 and the in-phase signal L4 is reversed in response thereto. For this reason, the output signal of the comparative CM2 is changed from a low level (equivalent to the voltage state of the negative power supply 80426 -23-1225333 VPP-) to a high level (higher voltage state than the negative power supply VPP- higher than the voltage VD2) The output signal L5 of the input buffer B24 is also changed to a high level. As a result, the gate voltage of the power MOS transistor 402 is higher than the source voltage by VD2, and the power MOS transistor 402 is A conduction state is formed. When the power MOS transistor 402 is turned on, the source voltage VS of the power MOS transistor 401 decreases with the output signal OUT. Based on this, the voltage VD1 generated by the internal power source P12 also decreases. At this time, the voltage VR1 generated by the bias circuit P11 also decreases with the change of the source voltage VS of the power MOS transistor 401, so the magnitude relationship between the in-phase signal H1 and the inverting signal H2 remains the same, and so on The signal level drops with the power supply system of the driving circuit 303H. Therefore, the level of the signal output from the comparator CM1 is maintained at a low level (source voltage VS). Accordingly, the power MOS transistor 401 remains in a non-conductive state while the output signal OUT is shifted to a low level (negative power supply VPP-). Due to the above situation, when the PWM signal transitions to a low level from the initial state at time t1, one power MOS transistor 401 is in a non-conducting state, and the other power MOS transistor 402 is in a conducting state, and The output signal OUT is migrated from the positive power supply VPP + to the negative power supply VPP- and outputs a low level. Next, at time t3, when the PWM signal returns to the high level, in response to this, at time t4, the in-phase signal H3 on the high-side drive side forms a high level and the inverting signal H4 forms a low level. Therefore, the comparator CM1 that inputs such in-phase signal H3 and inverted signal H4 outputs a high level, and the power MOS transistor -24- a
80426 1225333 體401係形成導通狀態。一方的低側驅動側則反相信號 形成低準位,且同相信號L4形成高準位。因此,輸入此類 反相信號L3和同相信號L4的比較器CM2係輸出低準位,且 功率MOS電晶體4〇2係形成不導通狀態。 於是,當功率MOS電晶體401形成導通狀態,則其源極電 壓vs即隨輸出信號ουτ上昇,以此為基準而内部電源pi2 所產生的電壓VD1亦上昇。但,偏壓電路pii所產生的電壓 VR1亦追隨源極電壓vS而上昇,且維持同相信號η 1和反相 信號Η2的大小關係,故比較點器CM1所輸出的輸出信號的 信號準位係保持高準位(對源極電壓VS高出電壓VD1份的 電壓狀態)。因此,在輸出信號OUT遷移至高準位的過程 中,功率MOS電晶體401係維持導通狀態。 是故,在時間t3中當P WM信號形成高準位,則功率M0S 電晶體401形成導通狀態,且功率m〇s電晶體402形成不導 通狀態,並輸出相當於正電源VPP+的高準位而作為輸出信 號 OUT 〇 因此’高側驅動側的同相信號H3和反相信號H4的各信號 準位係可如下式而求得。 (同相信號H3的高準位) =[Rll{(VPP+)+ VRl} + R13 X VDD] /(Rll + R13) (同相信號H3的低準位) =[R1 {(VPP+) + yR1} + R13 X 0 ] / (R11 + R13) (反相信號H4的高準位) =[R12{(VPP+)+ VRi} + R14X VDD] /(R12+ R14) -25-80426 1225333 The body 401 is in a conducting state. On the low-side drive side, the inverted signal forms a low level and the in-phase signal L4 forms a high level. Therefore, the comparator CM2, which inputs such an inverted signal L3 and an in-phase signal L4, outputs a low level, and the power MOS transistor 402 is in a non-conducting state. Therefore, when the power MOS transistor 401 is turned on, its source voltage vs. rises with the output signal οτ, and based on this, the voltage VD1 generated by the internal power supply pi2 also rises. However, the voltage VR1 generated by the bias circuit pii also increases following the source voltage vS and maintains the magnitude relationship between the in-phase signal η 1 and the inverting signal Η2. Therefore, the signal accuracy of the output signal output by the comparator CM1 The bit system maintains a high level (a voltage state where the source voltage VS is higher than the voltage VD by 1). Therefore, during the transition of the output signal OUT to a high level, the power MOS transistor 401 maintains an on state. Therefore, when the P WM signal forms a high level at time t3, the power M0S transistor 401 forms a conducting state, and the power m0s transistor 402 forms a non-conducting state, and outputs a high level equivalent to the positive power source VPP + As the output signal OUT, the respective signal levels of the in-phase signal H3 and the inverting signal H4 on the high-side drive side can be obtained by the following formula. (High level of in-phase signal H3) = [Rll {(VPP +) + VRl} + R13 X VDD] / (Rll + R13) (Low level of in-phase signal H3) = [R1 {(VPP +) + yR1 } + R13 X 0] / (R11 + R13) (high level of the inverted signal H4) = [R12 {(VPP +) + VRi} + R14X VDD] / (R12 + R14) -25-
80426 (反相信號H4的低準位) =[R12{(VPP+)+ VR1} + R14 X 0] /(R12+ R14) 相同地,低側驅動側的反相信號L3、同相信號L4的各信 號準位亦可如下式而求得。 (反相信號L3的高準位) =[R21 {(VPP-)+ VR2} + R23 X VDD] /(R21 + R23) (反相信號L3的低準位) =[R21 {(VPP-)+ VR2} + R23 X 0] /(R21 + R23) (同相信號L4的高準位) =[R22{(VPP-)+ VR2} + R23 X VDD] / (R22 + R24) (同相信號L4的低準位) =[R22{(VPP-)+ VR2} + R23 X 0] /(R22+ R24) 如上述,說明該實施形態1。 根據該實施形態,則無須使用特殊電路技術或電子元 件’而能將調變電路200的輸出信號變換成適合於功率M〇s 電晶體之信號準位。因此,能以電源VDD來作動輸入段1 〇〇 或碉變電路200而構成電路,且能抑制高耐壓製程的使用於 所須的最小限度。 而且,因使用電阻而進行信號準位的變換,故能抑制電 路構成的複雜化於所須的最小限度,且能有效地抑制成本。 (實施形態2) 繼之,說明本發明之實施形態2。 上述之實施形態1中,並未考量寄生於傳送互補信號產生 兒路301H、301L所產生的同相信號和反相信號的信號路徑 80426 -26- 1225333 上的電容量,但實際上係存在著各種電容量。當該寄生電 容f對同相信號和反相信號形成非平衡狀態時,同相信號 和反相信號的振幅即變小,且有產生此類之信號準位的大 小關係導致相反等的問題。此外,當該寄生電容量過大時, 例如輸入至驅動電路3〇3H的同相信號H3和反相信號H4,即 交ί于較相當於該驅動電路的接地的源極電壓vs較低,而有 比較器CM 1變得無法動作等的問題。 圖6(a)係表示信號路徑上不存在有寄生電容量的非平衡 狀態時的同相信號H3和反相信號H4之波形例。此外,圖6(b) 係表示在各信號路徑和呈現源極電壓VS的節點之間存在有 非平衡狀態時的波形例。該波形例係寄生於同相信號H3的 信號路徑和呈現源極電壓VS的節點之間的電容量,為較反 相信號H4的信號路徑更大者。此外,圖6(c)係表示各信號 路徑和接地等的固定節點之間的寄生電容量過大時之波形 例。此類之波形例係在前述之圖4中,對應於放大輸出信號 OUT為自低準位上昇至高準位之際的波形。 寄生於同相信號H3和反相信號H4的信號路徑上的電容 量為不存在有非平衡狀態時,如圖6(a)所示,同相信號H3 和反相信號H4,當在時間η確立信號準位時,即維持其大 小關係並追隨輸出信號OUT而上昇。因此,將其輸入的比 車父咨CM 1係無誤動作,而維持因應於時間t4所確定的同相 信號H3和反相信號H4的大小關係之信號準位。 相對於此,存在有並接於電阻R11、R12的寄生電容量之 非平衡狀態時,如圖6(b)所示,在信號HI、H2的變化過程 80426 -27- 中,受到寄生電容量的非孚偷 .非千衡的衫響,而有同相信號H3和 反相k唬H4的大小關係即 ^ τ 1倒得的b形。當同相信號Η3和反 1:號的大小關係倒轉時’比較器㈤即產生誤動作, :有,率刪電晶體4G1暫時形成不導通狀態之情形。相同 予在有寄生於低側驅動侧的電阻R2i m的電容量 非平衡狀態時,亦有導致比較器⑽的誤動作之情形。 H3此1:=生電容量過大時,係如圖6⑷所示,同相信號 ==的信號準位無法追隨於輸时號㈣(亦即源極電 土 )的逢化’且有較輸出信號〇υτ為低的情形。因此,無 法滿足以源極電壓VS Α其ί佳AA + ra: b為基率的電壓VD1作為電源電壓的比 M1的輸入特性’且有比較器cM1誤動作的情形。於 是,在該實料態2,則在上述實施㈣m構成中,備有 :以1U正自L號變換電路的一對輸出節點達於驅動電路的 節點的信號路徑上所寄生的電容量成份的非平衡 之電容器。 圖5係表示在高側驅動侧設置修正用的電容器⑶、⑴ <例,。如該騎示,在.連接於同相信肋3的信號路徑的 車乂 CM1的非反相輸入_、和呈現源極電壓π的節點之 間’連接有修正用的電容器⑶。此外,在連接於反相信號 H4的信號路徑的比較器CM1的反相輸人部,和呈現源極電 £ VS的節點之間,連接有修正用的電容器c 14。電容器 C14的值,係設足成略等於連接於同相信號和反相 ^號H4的各信號路徑的電容量。據此,因輸出信號贿的 又化而產生於各信號路徑的電壓變動量即變得略為相等, 80426 -28- 且能維持同相信號H3和反相信號H4的大小關係。 而且,相對於寄生於各信號路徑和接地等的固定節點之 間的電容量,若設定充分大的電容器C13、C14,則在輸出 信號OUT的信號準位變化之際,輸出信號out即中介電容 器C13、C14而拉高同相信號H3和反相信號H4使其較輸出信 號OUT更高。據此,同相信號H3和反相信號H4係滿足比較 器CM1的輸入特性,且能避免該比較器cmi的不產生動作 之情形。 此外,圖5之例示中,係對電阻r1]L、R12分別連接電容器 C 11、C12,據此,來自緩衝器b 12、B 13所輸出的同相信號 H1和反相信號H2的信號準位的變化即快速地傳達至比較 器CM1側,且能改善因電阻R11、r12所導致的信號延遲。 繼之,說明圖5所示之電容器和電阻之各設定值之一例。 又,圖5中,為了方便說明,係作成符合各電容器的電容量 值及符合各電阻的電阻值。 在寄生電容量為無非平衡狀態時,若令R1丨:R13 = C13 :C11 、R12:R14=C14:C12,則對於DC特性(靜態動作特性)及 AC特性(動悲動作特性)其匹配阻抗即完備,而能獲得無過 調節(over shoot)的波形。其中,ci4:C12=C13 :C11。例 如在作成R11 = R12= 1〇〇1^Ω、Rl3 = R14=5k^時,則作成 C11 = C12=1PF' Cl3=C14=2〇pF。該狀態中,當高側驅 動的源極電壓VS (亦即輸出信號ουτ)產生變化,則同相信 號Η3和反相信號Η4即追隨源極電壓^^而變化,且滿足比較 器CM1的輸入特性。 80426 -29- 1225333 相對於此纟寄生屯各里為存在有非平衡狀態時,如上 述之同相信號和反相信號的大小關係即倒轉,而造成誤動 作之原因。故而為消除寄生電容量的非平衡,而將高側驅 動侧的電容量C13、C14作成非平衡。例如,在作成纽= R12= 100 kQ、R13=R14=5 扣、cu = ci2=】pF時則 作成C=18pF、C14=12pF。據此,而能獲得動作界限, 即使是存在有寄生電容量的非平衡,亦能防止因該非平衡80426 (Low level of inverted signal H4) = [R12 {(VPP +) + VR1} + R14 X 0] / (R12 + R14) Similarly, each of the inverted signal L3 and the in-phase signal L4 on the low-side drive side The signal level can also be obtained by the following formula. (High level of inverted signal L3) = [R21 {(VPP-) + VR2} + R23 X VDD] / (R21 + R23) (Low level of inverted signal L3) = [R21 {(VPP-) + VR2} + R23 X 0] / (R21 + R23) (high level of in-phase signal L4) = [R22 {(VPP-) + VR2} + R23 X VDD] / (R22 + R24) (in-phase signal Low level of L4) = [R22 {(VPP-) + VR2} + R23 X 0] / (R22 + R24) As described above, the first embodiment will be described. According to this embodiment, the output signal of the modulation circuit 200 can be converted into a signal level suitable for a power Mos transistor without using special circuit technology or electronic components'. Therefore, the power supply VDD can be used to operate the input stage 100 or the conversion circuit 200 to form a circuit, and the use of a high withstand voltage process can be suppressed to the minimum required. In addition, since the signal level is converted using a resistor, the complexity of the circuit configuration can be suppressed to the minimum required, and the cost can be effectively suppressed. (Embodiment 2) Next, Embodiment 2 of the present invention will be described. In the first embodiment described above, no consideration is given to the capacitance on the signal path 80426 -26-1225333 which is parasitic on the in-phase signal and the inverting signal generated by the complementary signal generating channels 301H and 301L, but actually exists. Various electric capacity. When the parasitic capacitance f forms an unbalanced state with respect to the in-phase signal and the reverse-phase signal, the amplitudes of the in-phase signal and the reverse-phase signal become smaller, and there is a problem that the relationship between the levels of such signal levels causes the opposite. In addition, when the parasitic capacitance is too large, for example, the in-phase signal H3 and the inverting signal H4 input to the driving circuit 30H, that is, the source voltage vs. which is equivalent to the ground of the driving circuit is lower, and There is a problem that the comparator CM 1 becomes inoperable. Fig. 6 (a) shows waveform examples of the in-phase signal H3 and the reverse-phase signal H4 when there is no unbalanced state of parasitic capacitance on the signal path. Fig. 6 (b) shows an example of a waveform when an unbalanced state exists between each signal path and a node exhibiting the source voltage VS. This waveform example is the capacitance between the signal path of the in-phase signal H3 and the node showing the source voltage VS, which is larger than the signal path of the reverse-phase signal H4. Fig. 6 (c) shows an example of a waveform when the parasitic capacitance between each signal path and a fixed node such as a ground is too large. This type of waveform example corresponds to the waveform when the amplified output signal OUT rises from a low level to a high level in FIG. 4 described above. When the capacitance parasitic on the signal path of the in-phase signal H3 and the inverting signal H4 is not in an unbalanced state, as shown in FIG. 6 (a), the in-phase signal H3 and the inverting signal H4, when at time η When the signal level is established, the magnitude relationship is maintained and it rises following the output signal OUT. Therefore, the input car driver CM1 has no error operation, and maintains the signal level corresponding to the magnitude relationship between the in-phase signal H3 and the anti-phase signal H4 determined at time t4. In contrast, when there is an unbalanced state of the parasitic capacitances connected in parallel to the resistors R11 and R12, as shown in FIG. 6 (b), the parasitic capacitances are received during the change process of the signals HI and H2 80426 -27- The non-fu stealing and non-weighing shirt sounds, but there is a magnitude relationship between the in-phase signal H3 and the inverse k1 H4, that is, ^ τ 1 inverted b-shape. When the magnitude relationship between the in-phase signal Η3 and the inverse 1: is reversed, the 'comparator' will malfunction. Yes, there is a case where the transistor 4G1 is temporarily turned off. Similarly, when the capacitance of the resistor R2im parasitic on the low-side driving side is unbalanced, the comparator ⑽ may malfunction. H3: 1: When the generating capacity is too large, as shown in Figure 6⑷, the signal level of the in-phase signal == cannot follow the output of the time signal 输 (that is, the source electrode) and has a relatively high output. When the signal υτ is low. Therefore, it is impossible to satisfy the input characteristic of the ratio M1 based on the voltage VD1 with the source voltage VS A and its best AA + ra: b as the base voltage, and the comparator cM1 malfunctions. Therefore, in this actual state 2, in the above-mentioned implementation ㈣m configuration, a pair of output nodes that are 1U positive from the L-number conversion circuit reach the capacitance component parasitic on the signal path of the node of the drive circuit. Unbalanced capacitor. Fig. 5 shows an example in which correction capacitors CU, ⑴ < are provided on the high-side drive side. As shown in this riding example, a correction capacitor CU is connected between the non-inverting input_ of the car CM1 connected to the signal path of the rib 3 and the node showing the source voltage π '. Further, a capacitor c 14 for correction is connected between the inverting input section of the comparator CM1 connected to the signal path of the inverting signal H4 and a node showing the source voltage £ VS. The value of capacitor C14 is set to be substantially equal to the capacitance of each signal path connected to the in-phase signal and the inverting signal H4. Accordingly, the amount of voltage variation in each signal path due to the reversion of the output signal becomes slightly equal, 80426 -28-, and the magnitude relationship between the in-phase signal H3 and the inverting signal H4 can be maintained. In addition, if the capacitors C13 and C14 are set sufficiently large with respect to the capacitance parasitic between each signal path and a fixed node such as ground, the output signal out is an intermediate capacitor when the signal level of the output signal OUT changes. C13 and C14 pull up the in-phase signal H3 and the inverting signal H4 to make it higher than the output signal OUT. Accordingly, the in-phase signal H3 and the inverting signal H4 satisfy the input characteristics of the comparator CM1, and the situation in which the comparator cmi does not operate can be avoided. In addition, in the example shown in FIG. 5, the resistors r1] L and R12 are connected to the capacitors C 11 and C 12 respectively, and accordingly, the in-phase signal H1 and the inverted signal H2 output from the buffers b 12 and B 13 The bit change is quickly transmitted to the comparator CM1 side, and the signal delay caused by the resistors R11 and r12 can be improved. Next, an example of each setting value of the capacitor and the resistance shown in FIG. 5 will be described. In addition, in FIG. 5, for convenience of explanation, the capacitance values corresponding to the respective capacitors and the resistance values corresponding to the respective resistors are prepared. When the parasitic capacitance is in an unbalanced state, if R1 丨: R13 = C13: C11, R12: R14 = C14: C12, the matching impedance for DC characteristics (static operation characteristics) and AC characteristics (dynamic motion characteristics) That is complete, and a waveform without over shoot can be obtained. Among them, ci4: C12 = C13: C11. For example, when R11 = R12 = 1001 ^ Ω and Rl3 = R14 = 5k ^, C11 = C12 = 1PF 'Cl3 = C14 = 2 pF. In this state, when the source voltage VS (ie, the output signal ουτ) of the high-side drive changes, the in-phase signal Η3 and the inverting signal Η4 follow the source voltage ^^ and satisfy the input of the comparator CM1 characteristic. 80426 -29- 1225333 In contrast, when there is an unbalanced state in the parasites, the magnitude relationship between the in-phase signal and the anti-phase signal is reversed as described above, which causes the malfunction. Therefore, in order to eliminate the unbalance of the parasitic capacitance, the capacitances C13 and C14 of the high-side driving side are made unbalanced. For example, when creating a button = R12 = 100 kQ, R13 = R14 = 5 buckle, cu = ci2 =] pF, then C = 18 pF, C14 = 12 pF. According to this, the operating limit can be obtained, and even if there is an imbalance in the parasitic capacitance, it can be prevented from being caused by the imbalance.
而導致的誤動作。圖6⑷係表示在高側驅動側的電容量 C13、C14設置非平衡並修正該電容量值時的波形例。該圖 例係在輸出信號OUT的遷移過程中,放大同相信號H3和反 相信號H4的信號準位之差值部份。因此,同相信號H3和反 相信號H4的信號準位即無倒轉情形,且輸入此類信號的比 較器CM1亦無誤動作的情形。 如上述說明實施形態2。 (實施形態3) 着 以下說明本發明之實施形態3。 孩實施形態3係在上述實施形態卜2中,藉由將流通於高 側驅動側的電阻R11、R12及低側驅動側的電阻R21、R22的 同相電流予以消除的措施而達成高速化。 此處,參閱圖7,以電阻Rii、R12為例,說明同相電流的 產生機構和因同相電流所產生的問題點。圖7係在前述的圖 2中’表示自互補信號產生電路3〇111的緩衝器bi2、B13至 驅動電路303H的比較器CM1的信號路徑者,其和圖2所示之 相同元件則賦予相同符號。 80426 -30- 圖7中,當源極電壓vs追隨於輸出信號而上昇時,則以此 為基準而偏壓電路P11所產生的電壓VR1亦上昇。因此,偏 壓電路pii的輸出節點的電壓即較緩衝器B12、B13所輸出 的#號準位較高,且自偏壓電路P11朝向緩衝器b12、bi3 而分別泥通同相電流11、12於電阻ri 1、R12。是故,同相 信號H3和反相信號H4的信號準位係較偏壓電路ρι丨所產生 的電壓VR1多少更低。反之,當源極電壓vs追隨於輸出信 號out而下降時,則以此為基準而偏壓電路P11所產生的電 壓VR1亦下降。此情形時,自緩衝器b 12、b 13朝向偏壓電 路P11流通反方向之同相電流Π、12於電阻R11、R12。因此, 同相信號H3和反相信號H4的信號準位係較偏壓電路P11所 產生的電壓VR1多少更高。 於疋’务設定R11 /R13比為較小,則能加大同相信號H3 和反相信號H4的差值部份,且能高速化。但是,如上述, 同相信號H3和反相信號H4的信號準位因係依據輸出信號 OUT的變化而對電壓VR1產生上下變動,故為了不使同相信 號H3和反相信號H4能不超過比較器CM1的同相輸入範 圍,而必須設定R11/R13、R12/R14的各比值。因此,無法 任意地縮小R11 /R13比,也因此而無法充份地取得輸入於比 較器CM1的同相信號H3和反相信號H4的差值部份,故而影 響到將其輸入的比較器CM1的響應速度。 本實施形態3係藉由消除上述同相電流II、12之措施,而 僅將流通於電阻R13、R14的電流作成反相電流(依據同相信 號和反相信號的差值部份的電流成份),而抑制比較器CM1 80426 -31- 的輸入變動。據此,即能縮小R11/R13比,且能改善比較器 的響應速度。 以下,具體說明本實施形態3的構成。 圖8係表示本實施形態3的D級放大器之構成上的特徵。於 該圖中,和前述實施形態1之圖2所示之構成元件的相同元 件係賦予相同符號。圖8係表示高側驅動側的構成,於圖8 所示之構成中,更具備有緩衝器BD12、BD13、電阻RD11、 RD12、NMOS電晶體Nil〜N14、PMOS電晶體P11〜P14,此 類係構成用以注入將上述同相電流II、12予以消除之用的電 流於電阻R11、R12之電流注入電路。 此處,緩衝器BD12、BD13係類比緩衝器,為對應於上述 緩衝器B12、B13者,誠如後述,係在呈現相當於電壓VR1 的電壓於NMOS電晶體N14和PMOS電晶體P14之範圍下驅 動電阻RD11、RD12者,而在此類之輸入部,係共通地施加 相當於電源VDD的2分之1的電壓之電壓VREFC。電阻RD11 、RD12係具有和上述電阻Rll、R12相等的電阻值,電阻 RD11係連接於緩衝器BD12的輸出節點和NMOS電晶體N14 的節點之間,電阻RD12係連接於緩衝器BD13的輸出節點和 PMOS電晶體P14之間。 NMOS電晶體N14係設定流通於電阻RD 11的電流,並設定 其閘極電壓VRP1,以使其源極電壓能相等於上述之電壓 VR1。PMOS電晶體P14係設定流通於電阻RD12的電流,並 設定其閘極電壓VRN1,以使其源極電壓能相等於上述之電 壓 VR1。 80426 -32- 此夕卜,在PMOS電晶體P11的源極係供應著電壓VD1,且 其汲極係和閘極均連接於NMOS電晶體N14的汲極。在 PMOS電晶體P12、P13的源極係供應著電壓VD1,且此類的 沒極係分別連接於比較器CM 1的反相輸入部和非反相輸入 部。此類PMOS電晶體Pll、P12、P13係構成一監視流通於 電阻RD11的電流而用以注入電流於電阻R11、R12的電流反 射鏡。又,於圖8中,電壓VR1係和圖2的電壓VR1相同,係 以源極電壓VS為基準的電壓,電壓VD1亦同。因此,閘極 電壓VRP1、VRN1的電位亦以源極電壓VS為基準而被供應。 相同地,在NMOS電晶體Nil的源極係供應著電壓VS,其 沒極係和閘極均連接於PMOS電晶體P14的汲極。在NMOS 電晶體N12、N13的源極係供應著電壓VS,此類的汲極係分 別連接於比較器CM1的反相輸入部和非反相輸入部。此類 NMOS電晶體Nil、N12、N13係構成一監視流通於電阻RD12 而用以注入電流於電阻R11、R12的電流反射鏡。 以下,著手於上述之電流注入電路而說明本實施形態3。 根據上述之構成,相當於電阻R11的電阻RD11與NMOS 電晶體N14的源極相連接的電壓HD3、以及呈現於相當於電 阻R12的電阻RD12與PMOS電晶體P14的源極的連接點的信 號HD4的電壓,係概略等於電壓VR1,且輸出信號OUT係往 復於正電源VPP +和負電源VPP-之間。 是故,輸出信號OUT為正電源VPP+時,流通於PMOS電 晶體P11的電流IP11表示如下式。 IP11 = {(VPP+)+ VR1 — VREFC} /RD11 80426 -33 - 1225333 此外,輸出信號OUT為VPP-時,流通於NMOS電晶體Nil 的電流IN11表示如下式。 IN11 = {VREFC —(VPP-) - VR1} /RD12 此類之電流IP11、IN11係概略等於流通於電阻Rll、R12 的同相電流II、12,而形成監視此類同相電流的電流。其中, 相當於電流IP11的電流,係和PMOS電晶體P11均自構成電 流反射鏡的PMOS電晶體P12、P13而注入於電阻Rll、R12。 此外,相當於電流INI 1的電流,係和NMOS電晶體Nl 1均自 構成電流反射鏡的NMOS電晶體N12、N13而注入電阻R11、 R12。此結果,即能消除流通於電阻R1卜R12的同相電流II、 12,巨觀上,在電阻R13、R14係不存在同相電流II、12, 只形成反相電流。因此,因基於該反相電流之電壓的下降, 同相信號H3和反相信號H4即以電壓VR1為中心而呈現,且 縮小驅動電路3 0 3 Η的比車父益C1的同相輸入範圍。 根據本實施形態3,即能消除流通於電阻R13、R14的同 相電流,且流通於此類之電阻的電流變小,故能設定電阻 R13、R14的值於更大。據此,因能加大比較器CM1的輸入 信號的差份(差動電位差),而可高速化,而且能使電路動作 安定化,且能提昇信賴性。 此外,因在同相輸入範圍小的狀態下,能加大比較器CM1 的輸入信號的差份,故能更進一步提高正電源VPP +和負電 源VPP-,且能對應於D級放大器的大輸出化。 (實施形態4) 以下,說明本實施形態4。 -34- 80426 1225333 上述之實施形態3,係監視流通於電阻RDll、RD12的電 流而注入電流,並藉由偏壓電路P11而將電阻R13、R14偏 壓成電阻VR1者,但本實施形態4則使用運算放大器而在進 行電流注入的同時,亦將電阻R13、R14偏壓成電阻VR1。 圖9係表示本實施形態4之D級放大器之構成上的特徵。 本實施形態4係在前述之圖2所示之實施形態1的構成 中,係將具有一對的輸出部01、02的2輸出型運算放大器 OP60作成偏壓電路。此處,其反相輸入部係連接於共通連 接端,而其非反相輸入部係施加著電壓VR1,其一對的輸 出部係分別連接於一對的電阻R13、R14的另一端側。 圖10係表示運算放大器OP60的構成。 該圖中,定電流源SI1、PMOS電晶體P20、P21、NMOS 電晶體N20、N21係構成差動放大器,其輸出部係連接於 NMOS電晶體N22、N23的閘極。在此類的NMOS電晶體 N22、N23的汲極係中介定電流源SI2、SI3而供應著電壓 VD1,而在此類電晶體的源極係供應著源極電壓VS。此類 NM0S電晶體N22、N23的汲極係作成一對的輸出部。根據 該運算放大器OP60的構成,則因應於施加於PM0S電晶體 P20、P21的閘極的差動電位差而輸出電流於一對的輸出部 01、02。 此處,回歸圖9的說明,並說明本實施形態4的動作。 圖2所示之輸出信號OUT係相當於電源VPP+的電壓之電 壓狀態,在高側驅動側的驅動電路303H為電源VPP+側時, 圖9所示之同相信號H3和反相信號H4的電位,係因同相電 -35- 80426 1225333 流II、12而降低,但因施加於運算放大器OP60的反相輸入 部的基準電壓為電壓VR1,故運算放大器OP60即自一對的 輸出部注入同相電流於電阻R11、R12,而使節點Q的電壓 相等於電壓VR1,而在節點Q的電壓等於電壓VR1的時點, 運算放大器OP60的輸出電流即安定。 輸出信號OUT為VPP-侧時,同相信號H3及反相信號H4的 電壓係因同相電流而上昇,但運算放大器OP60係注入同相 電流於電阻Rll、R12而使節點Q的電壓相等於電壓VR1。據 此’在電阻R13、R14係形成只流通反相電流之狀悲’同相 信號H3和反相信號H4則因基於反相電流的電位功效,而以 電壓VR1為中心而差動輸入於比較器CM1。且同相輸入亦以 電壓VR1為中心而作動。 根據本實施形態4,則即使加大電阻R13、R14,亦能擴 大比較器CM1的差動電位差。因此,能抑制消費電流,且 能改善動作速度。 而且,因同相輸入範圍較小,故能提高正電源VPP+及負 電源VPP-。 以上,雖說明本發明之一實施形態,但並不自限於上述 之實施形態,即使在不脫離本發明之要義的範圍而作的設 計變更亦包含於本發明中。例如,上述之實施形態1中,互 補信號產生電路301H、301L雖係作成輸出高準位或低準位 的2值者,但亦可作成輸出類比信號者。 該構成例示於圖11。於該圖中,放大器B52、B53係對應 於圖2所示之緩衝器B12、B13,且輸出因應於PWM信號的 -36- 80426 I225333 類比信號。運算放大器0P51、電阻R52、r53係構成差動放 大器,且中介電阻R11、R12而將放大器B52、B53所輸入的 類比信號的差份丁以放大。電阻R54、R55、運算放大哭〇p 5 2 係構成放大器’該放大器係用以變換將追隨於功率電晶體 501的射極電壓的基準電壓VREF作為振幅中心的波形。功 率電晶體501係用以驅動未圖示之輸出端子。藉由如此之構 -成而亦能適用於線性放大器。 如以上之說明,根據本發明,則產生由調變的脈衝信號 籲 的同相信號和反相信號所構成的第丨互補信號,並在維持前 述同相信號的信號準位和前述反相信號的信號準位之間的 大小關係之狀怨下,而將前述第丨互補信號予以準位變換成 追隨於既定電壓的第2互補信號,並基於包含於前述第2互 補L號的别述同相抬號的信號成份和前述反相信號的信號 成份的大小關係,而得以驅動輸出用電晶體,故無須使用 特殊之製造製程或電子元件,而能驅動控制輸出用的功率 MOS電晶體。 【圖式簡單說明】 每 、圖1係表7^本發明之實施形態1之D級放大器之全體構成 之圖式。 ·, 圖係表不本發明之實施形態1之信號變換電路之構成> 電路圖。 圖3係表 - 士 式。“不本發明之實施形態1之偏壓電路之構成之圖 圖4係用以命 ,兄明本發明之實施形態1之D級放大器之動作 80426 •37· 之波形圖。 圖5係表示本發明 > ^ 、 特欲部份之 圖式',實施形態2之D級放大器之構成上之 圖6(a)〜(d)係用以 夕a、 成明本發明之實施形態2之D級放大器 <動作 < 波形圖。 圖7係用以說明太菰M、_ 椹、兩 赞月 < 貫施形態3之同相電流的產生機 傅之電路圖。 圖8係表不本發明士 g她形態3之D級放大器之構成上之 特徵邵份之圖式。 圖9係表不本發明之實施形態4之D級放大器之構成上之 特徵部份之圖式。 圖係表示本發明之實施形態3之輸出型運算放大器之 構成之圖式。 圖11係表示本發明之變形例之D級放大器之構成上之特 徵部份之圖式。 圖12係用以說明習知技術之D級放大器之構成之圖式。 【圖式代表符號說明】 SIG 信號源 CIN 電容器 DAMP D級放大器 100 輸入段 200 調變電路 300 驅動控制電路 301H、301L 信號產生電路 80426 -38 - 302H、302L 信號變換電路 303H、303L 驅動電路 401 、 402 輸出用MOS電晶體 L 電感(線圈) C 電容(電容器) SPK 放音器 Bn、B12、B13 、B14、B2卜 B22、B23、B24、BD12、BD13 緩衝器 1225333And cause malfunction. Fig. 6 shows an example of a waveform when the capacitances C13 and C14 on the high-side driving side are set to be unbalanced and the capacitance value is corrected. This example shows that during the transition of the output signal OUT, the difference between the signal levels of the in-phase signal H3 and the in-phase signal H4 is amplified. Therefore, the signal levels of the in-phase signal H3 and the in-phase signal H4 are not reversed, and the comparator CM1 inputting such signals does not malfunction. As described above, the second embodiment is described. (Embodiment 3) Hereinafter, Embodiment 3 of the present invention will be described. In the third embodiment, in the second embodiment, the high-speed is achieved by eliminating the in-phase current flowing through the resistors R11 and R12 on the high-side drive side and the resistors R21 and R22 on the low-side drive side. Here, referring to FIG. 7, the resistors Rii and R12 are taken as examples to explain the in-phase current generating mechanism and the problems caused by the in-phase current. FIG. 7 shows the signal paths from the buffers bi2 and B13 of the complementary signal generating circuit 3111 to the comparator CM1 of the driving circuit 303H in FIG. 2 described above, and the same components as those shown in FIG. 2 are given the same symbol. 80426 -30- In Fig. 7, when the source voltage vs. increases following the output signal, the voltage VR1 generated by the bias circuit P11 also increases based on this. Therefore, the voltage of the output node of the bias circuit pii is higher than the # mark output by the buffers B12 and B13, and the self-bias circuit P11 faces the buffers b12 and bi3 to pass through the same-phase current 11, respectively. 12 in resistance ri 1, R12. Therefore, the signal levels of the in-phase signal H3 and the inverted signal H4 are somewhat lower than the voltage VR1 generated by the bias circuit ρι. On the other hand, when the source voltage vs decreases following the output signal out, the voltage VR1 generated by the bias circuit P11 also decreases based on this. In this case, in-phase currents Π, 12 flowing in the opposite direction from the buffers b 12, b 13 toward the bias circuit P11 are in the resistors R11, R12. Therefore, the signal levels of the in-phase signal H3 and the inverted signal H4 are somewhat higher than the voltage VR1 generated by the bias circuit P11. If the R11 / R13 ratio is set to be small, the difference between the in-phase signal H3 and the inverting signal H4 can be increased, and the speed can be increased. However, as described above, the signal levels of the in-phase signal H3 and the inverting signal H4 change the voltage VR1 up and down according to the change of the output signal OUT, so that the in-phase signal H3 and the inverting signal H4 can not exceed The non-inverting input range of the comparator CM1 must set the ratios of R11 / R13, R12 / R14. Therefore, the R11 / R13 ratio cannot be arbitrarily reduced, and the difference between the in-phase signal H3 and the inverting signal H4 input to the comparator CM1 cannot be fully obtained, which affects the comparator CM1 which is input thereto. Response speed. In the third embodiment, by eliminating the above-mentioned in-phase currents II and 12, only the current flowing through the resistors R13 and R14 is made into an inverted current (based on the current component of the difference between the in-phase signal and the inverted signal). , And suppress the input change of comparator CM1 80426 -31-. According to this, the R11 / R13 ratio can be reduced, and the response speed of the comparator can be improved. Hereinafter, the configuration of the third embodiment will be described in detail. Fig. 8 is a diagram showing a characteristic of the structure of a class D amplifier according to the third embodiment. In this figure, the same components as those shown in Fig. 2 of the first embodiment are given the same reference numerals. FIG. 8 shows the structure of the high-side drive side. In the structure shown in FIG. 8, it further includes buffers BD12, BD13, resistors RD11, RD12, NMOS transistors Nil ~ N14, PMOS transistors P11 ~ P14, and so on. It is a current injection circuit for injecting a current for eliminating the above-mentioned in-phase currents II and 12 into the resistors R11 and R12. Here, the buffers BD12 and BD13 are analog buffers corresponding to the above-mentioned buffers B12 and B13. As described later, the voltages corresponding to the voltage VR1 are in the range of the NMOS transistor N14 and the PMOS transistor P14. Those driving the resistors RD11 and RD12, and a voltage VREFC corresponding to a voltage equal to one-half of the power source VDD is commonly applied to the input portion of this type. The resistors RD11 and RD12 have the same resistance value as the resistors R11 and R12. The resistor RD11 is connected between the output node of the buffer BD12 and the node of the NMOS transistor N14. The resistor RD12 is connected to the output node of the buffer BD13 and PMOS transistor P14. The NMOS transistor N14 sets the current flowing through the resistor RD 11 and sets its gate voltage VRP1 so that its source voltage can be equal to the above-mentioned voltage VR1. The PMOS transistor P14 sets the current flowing through the resistor RD12 and sets its gate voltage VRN1 so that its source voltage can be equal to the above-mentioned voltage VR1. 80426 -32- In addition, the source of PMOS transistor P11 is supplied with voltage VD1, and its drain and gate are connected to the drain of NMOS transistor N14. The source of the PMOS transistors P12 and P13 is supplied with a voltage VD1, and such an anode is connected to the inverting input section and the non-inverting input section of the comparator CM1, respectively. These PMOS transistors P11, P12, and P13 constitute a current mirror that monitors the current flowing through the resistor RD11 and injects current into the resistors R11 and R12. In FIG. 8, the voltage VR1 is the same as the voltage VR1 in FIG. 2, and is the voltage based on the source voltage VS, and the voltage VD1 is also the same. Therefore, the potentials of the gate voltages VRP1 and VRN1 are also supplied based on the source voltage VS. Similarly, the source of the NMOS transistor Nil is supplied with a voltage VS, and its anode and gate are connected to the drain of the PMOS transistor P14. The source of the NMOS transistors N12 and N13 is supplied with a voltage VS, and such a drain is connected to the inverting input section and the non-inverting input section of the comparator CM1, respectively. These NMOS transistors Nil, N12, and N13 form a current mirror that monitors and flows through the resistor RD12 and injects current into the resistors R11 and R12. Hereinafter, the third embodiment will be described starting with the above-mentioned current injection circuit. According to the above configuration, the voltage HD3 between the resistor RD11 corresponding to the resistor R11 and the source of the NMOS transistor N14, and the signal HD4 appearing at the connection point between the resistor RD12 corresponding to the resistor R12 and the source of the PMOS transistor P14. The voltage is roughly equal to the voltage VR1, and the output signal OUT is reciprocated between the positive power source VPP + and the negative power source VPP-. Therefore, when the output signal OUT is the positive power supply VPP +, the current IP11 flowing through the PMOS transistor P11 is expressed by the following formula. IP11 = {(VPP +) + VR1 — VREFC} / RD11 80426 -33-1225333 In addition, when the output signal OUT is VPP-, the current IN11 flowing through the NMOS transistor Nil is expressed as follows. IN11 = {VREFC — (VPP-)-VR1} / RD12 This type of current IP11, IN11 is roughly equal to the in-phase currents II, 12 flowing through the resistors Rll, R12, and forms a current that monitors this type of in-phase current. Among them, the current corresponding to the current IP11, and the PMOS transistor P11 are injected into the resistors R11 and R12 from the PMOS transistors P12 and P13 constituting the current mirror. In addition, a current corresponding to the current INI 1 and the NMOS transistor N11 are injected into the resistors R11 and R12 from the NMOS transistors N12 and N13 constituting a current mirror. As a result, the in-phase currents II and 12 flowing through the resistors R1 and R12 can be eliminated. On a large scale, the in-phase currents II and 12 do not exist in the resistors R13 and R14, and only the reverse-phase current is formed. Therefore, due to the decrease of the voltage based on the inversion current, the in-phase signal H3 and the inversion signal H4 are centered on the voltage VR1, and the in-phase input range of the driving circuit 3 0 3 比 is lower than that of the driver ’s benefit C1. According to the third embodiment, the in-phase current flowing through the resistors R13 and R14 can be eliminated, and the current flowing through such a resistor becomes smaller, so that the values of the resistors R13 and R14 can be set larger. As a result, the difference (differential potential difference) in the input signal of the comparator CM1 can be increased, which can increase the speed, stabilize the circuit operation, and improve reliability. In addition, because the input signal of the comparator CM1 can be increased in the state where the in-phase input range is small, the positive power supply VPP + and the negative power supply VPP- can be further increased, and it can correspond to the large output of the class D amplifier. Into. (Embodiment 4) Hereinafter, Embodiment 4 will be described. -34- 80426 1225333 The third embodiment described above is the one that monitors the current flowing through the resistors RD11 and RD12 to inject current, and biases the resistors R13 and R14 to the resistor VR1 by the bias circuit P11, but this embodiment 4 uses an operational amplifier to simultaneously bias the resistors R13 and R14 into a resistor VR1 while performing current injection. FIG. 9 is a diagram showing the configuration of a class D amplifier according to the fourth embodiment. In the fourth embodiment, in the configuration of the first embodiment shown in Fig. 2 described above, a two-output type operational amplifier OP60 having a pair of output sections 01 and 02 is used as a bias circuit. Here, its inverting input section is connected to a common connection terminal, and its non-inverting input section is applied with a voltage VR1, and its pair of output sections are respectively connected to the other ends of a pair of resistors R13 and R14. FIG. 10 shows the configuration of the operational amplifier OP60. In this figure, the constant current sources SI1, PMOS transistors P20, P21, and NMOS transistors N20 and N21 form a differential amplifier, and the output is connected to the gates of NMOS transistors N22 and N23. In the NMOS transistors N22 and N23, the drains of the NMOS transistors N22 and N23 are supplied with a voltage VD1, and the source of the transistors is supplied with a source voltage VS. The drains of these NM0S transistors N22 and N23 form a pair of output sections. According to the configuration of the operational amplifier OP60, a current is output to a pair of output sections 01 and 02 in response to a differential potential difference applied to the gates of the PM0S transistors P20 and P21. Here, returning to the description of FIG. 9 and describing the operation of the fourth embodiment. The output signal OUT shown in FIG. 2 is a voltage state corresponding to the voltage of the power supply VPP +. When the drive circuit 303H on the high-side drive side is the power supply VPP + side, the potentials of the in-phase signal H3 and the reverse-phase signal H4 shown in FIG. 9 It is reduced by in-phase electricity -35- 80426 1225333 currents II and 12, but because the reference voltage applied to the inverting input section of the operational amplifier OP60 is voltage VR1, the operational amplifier OP60 injects in-phase current from a pair of output sections. With the resistors R11 and R12, the voltage of the node Q is equal to the voltage VR1, and when the voltage of the node Q is equal to the voltage VR1, the output current of the operational amplifier OP60 is stable. When the output signal OUT is on the VPP- side, the voltages of the in-phase signal H3 and the inverting signal H4 rise due to the in-phase current, but the OP60 system injects the in-phase current into the resistors Rll and R12 to make the voltage at the node Q equal to the voltage VR1. . Based on this, the resistors R13 and R14 are formed like a reverse-phase current. The in-phase signal H3 and the reverse-phase signal H4 are differentially input for comparison based on the potential effect of the reverse-phase current and centered on the voltage VR1.器 CM1. The non-inverting input also operates around the voltage VR1. According to the fourth embodiment, even if the resistors R13 and R14 are increased, the differential potential difference of the comparator CM1 can be increased. Therefore, the consumption current can be suppressed, and the operation speed can be improved. In addition, since the non-inverting input range is small, the positive power supply VPP + and the negative power supply VPP- can be increased. Although one embodiment of the present invention has been described above, it is not limited to the above embodiment, and design changes made without departing from the scope of the present invention are included in the present invention. For example, in the first embodiment described above, although the complementary signal generating circuits 301H and 301L are designed to output a high value or a low level binary value, they can also be used to output an analog signal. An example of this configuration is shown in FIG. 11. In the figure, the amplifiers B52 and B53 correspond to the buffers B12 and B13 shown in Fig. 2 and output -36- 80426 I225333 analog signals corresponding to the PWM signals. The operational amplifiers OP51, resistors R52, and r53 constitute a differential amplifier, and the resistors R11 and R12 are used to amplify the difference of the analog signals input by the amplifiers B52 and B53. The resistors R54, R55, and operational amplifiers are configured as amplifiers. The amplifiers are used to convert the waveform having the reference voltage VREF following the emitter voltage of the power transistor 501 as the center of the amplitude. The power transistor 501 is used to drive an output terminal (not shown). With this structure, it is also applicable to linear amplifiers. As described above, according to the present invention, a first complementary signal composed of an in-phase signal and an inverted signal modulated by a modulated pulse signal is generated, and the signal level of the in-phase signal and the inverted signal are maintained. The magnitude of the relationship between the signal levels of the signal is complained about, and the aforementioned complementary signal is transformed into the second complementary signal following the predetermined voltage, and based on the other in-phase in the second complementary L number The magnitude of the signal component and the signal component of the inverted signal can drive the output transistor, so there is no need to use special manufacturing processes or electronic components to drive the power MOS transistor for output control. [Brief description of the drawings] Each and FIG. 1 is a diagram showing the overall structure of a class D amplifier according to Embodiment 1 of the present invention. · The diagram is a circuit diagram showing the configuration of a signal conversion circuit according to the first embodiment of the present invention. Figure 3 is a table-taxi style. "The structure of the bias circuit according to the first embodiment of the present invention. Fig. 4 is a waveform diagram for explaining the operation of the D-class amplifier according to the first embodiment of the present invention. The present invention > ^, Schematic diagram of the special desire part, Fig. 6 (a) ~ (d) on the structure of the Class D amplifier of the second embodiment are used to form a second embodiment of the present invention. D-level amplifier < action < waveform diagram. Fig. 7 is a circuit diagram for explaining the generation mechanism of the in-phase current of 菰 M, 椹 椹, two Zanyue < implementation mode 3. Fig. 8 shows the present invention Fig. 9 is a diagram showing the characteristics of the structure of the D-class amplifier in Form 3. Fig. 9 is a diagram showing the features of the structure of the D-class amplifier in Embodiment 4 of the present invention. The structure of the output-type operational amplifier according to the third embodiment of the invention. Fig. 11 is a diagram showing a characteristic part of the structure of a class D amplifier according to a modification of the present invention. Fig. 12 is a diagram for explaining a conventional technique. Structure of Class D amplifier. [Description of Symbols in Drawing] SIG signal source CIN capacitor DAMP D Stage amplifier 100 input section 200 modulation circuit 300 drive control circuit 301H, 301L signal generation circuit 80426 -38-302H, 302L signal conversion circuit 303H, 303L drive circuit 401, 402 output MOS transistor L inductor (coil) C capacitor (Capacitor) SPK Bn, B12, B13, B14, B2, B22, B23, B24, BD12, BD13 buffer 1225333
Rll、R12、R13、R14、R2卜 R22、R23、R24、R52、R53、R54、R55 電阻 Cll、C12、C13、C14 電容器Rll, R12, R13, R14, R2, R22, R23, R24, R52, R53, R54, R55 Resistors Cll, C12, C13, C14 Capacitors
Pll 、 P12 偏壓電路 CM1、CM2 比較器 P12 、 P22 内部電源 P11、P12、P13、P14 PMOS電晶體 N11、N12、N13、N14 NMOS電晶體 OP60、OP52 運算放大器 B52、B53 放大器 501 電晶體(npn型) 80426 -39-Pll, P12 Bias circuit CM1, CM2 Comparator P12, P22 Internal power supply P11, P12, P13, P14 PMOS transistor N11, N12, N13, N14 NMOS transistor OP60, OP52 Operational amplifier B52, B53 amplifier 501 transistor ( npn type) 80426 -39-
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JP2002061107A JP3941549B2 (en) | 2002-03-06 | 2002-03-06 | Class D amplifier |
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TW200402189A TW200402189A (en) | 2004-02-01 |
TWI225333B true TWI225333B (en) | 2004-12-11 |
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TW092104653A TWI225333B (en) | 2002-03-06 | 2003-03-05 | Class D amplifier |
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KR (1) | KR100582172B1 (en) |
TW (1) | TWI225333B (en) |
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JP4561459B2 (en) * | 2004-04-30 | 2010-10-13 | ヤマハ株式会社 | Class D amplifier |
KR100716527B1 (en) * | 2006-03-06 | 2007-05-09 | 주식회사 쓰리에스테크놀로지 | Sigma-delta modulation type 3-level d class audio amplifier controlling bandwidth of output frequency |
JP2009118447A (en) * | 2007-10-18 | 2009-05-28 | Onkyo Corp | Switching amplifier |
JP5597300B2 (en) * | 2013-12-25 | 2014-10-01 | 株式会社日立製作所 | Semiconductor measuring equipment |
JP6728173B2 (en) * | 2014-12-09 | 2020-07-22 | インフィネオン テクノロジーズ オーストリア アクチエンゲゼルシャフト | Regulated high-side gate drive circuit for power transistor |
US9503028B2 (en) * | 2015-01-30 | 2016-11-22 | Mitsubishi Electric Research Laboratories, Inc. | Three-way sequential power amplifier system for wideband RF signal |
JP6651835B2 (en) * | 2015-03-13 | 2020-02-19 | ヤマハ株式会社 | Power amplifier |
JP7411411B2 (en) * | 2019-12-27 | 2024-01-11 | ローランド株式会社 | Musical signal amplifier |
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2002
- 2002-03-06 JP JP2002061107A patent/JP3941549B2/en not_active Expired - Fee Related
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2003
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KR100582172B1 (en) | 2006-05-23 |
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