5秒后页面跳转
AN1042 PDF预览

AN1042

更新时间: 2024-10-29 03:18:47
品牌 Logo 应用领域
安森美 - ONSEMI 开关音频放大器
页数 文件大小 规格书
12页 96K
描述
High Fidelity Switching Audio Amplifiers Using TMOS Power MOSFETs

AN1042 数据手册

 浏览型号AN1042的Datasheet PDF文件第2页浏览型号AN1042的Datasheet PDF文件第3页浏览型号AN1042的Datasheet PDF文件第4页浏览型号AN1042的Datasheet PDF文件第5页浏览型号AN1042的Datasheet PDF文件第6页浏览型号AN1042的Datasheet PDF文件第7页 
AN1042/D  
High Fidelity Switching  
Audio Amplifiers Using  
TMOS Power MOSFETs  
Prepared by: Donald E. Pauly  
ON Semiconductor  
http://onsemi.com  
Special Consultant  
APPLICATION NOTE  
Almost all switching amplifiers operate by generating a  
high frequency square wave of variable duty cycle. This  
square wave can be generated much more efficiently than  
an analog waveform. By varying the duty cycle from 0 to  
100%, a net dc component is created that ranges between  
the negative and positive supply voltages. A low pass filter  
delivers this dc component to the speaker. The square wave  
must be generated at a frequency well above the range of  
hearing in order to be able to cover the full audio spectrum  
from dc to 20 kHz. Figure 1 shows a square wave  
generating a sine wave of one–ninth its frequency as its  
duty cycle is varied.  
With the introduction of complementary bipolar power  
transistors in the late 1960s, switching amplifiers became  
theoretically practical. At low frequencies, bipolar transistors  
have switching efficiencies of 99% and will directly drive  
a low impedance speaker filter. The requirement for  
switching frequencies above 100 kHz resulted in excessive  
losses however. Bipolar drive circuitry was also complex  
because of its large base current requirement.  
With the advent of complementary (voltage/current  
ratings) TMOS power MOSFETs, gate drive circuitry has  
been simplified. These MOS devices are very efficient as  
switches and they can operate at higher frequencies.  
A block diagram of the amplifier is shown in Figure 2.  
An output switch connects either +44 or –44 volts to the  
input of the low pass filter. This switch operates at a carrier  
frequency of 120 kHz. Its duty cycle can vary from 5% to  
95% which allows the speaker voltage to reach 90% of  
either the positive or negative supplies. The filter has a  
response in the audio frequency range that is as flat as  
possible, with high attenuation of the carrier frequency and  
its harmonics. A 0.05 ohm current sense resistor (R27) is  
used in the ground return of the filter and speaker to provide  
short circuit protection.  
The negative feedback loop is closed before the filter to  
prevent instabilities. Feedback cannot be taken from the  
speaker because of the phase shift of the output filter, which  
varies from 0° at dc to nearly 360° at 120 kHz. Since the  
filter is linear, feedback may be taken from the filter input,  
which has no phase shift. Unfortunately, this point is a high  
frequency square wave which must be integrated to  
determine its average voltage. The input is mixed with the  
square wave output by resistors R4 and R5 shown in Figure  
2. The resultant signal is integrated, which accurately  
simulates the effect of the output filter. The output of the  
integrator will be zero only if the filter input is an accurate  
inverted reproduction of the amplifier input. If the output  
is higher or lower than desired, the integrator will generate  
a negative or positive error voltage. This error voltage is  
applied to the input of the switch controller, which makes  
the required correction. The integrator introduces a 90°  
phase shift at high frequencies which leaves a phase margin  
of nearly 90°.  
Input  
1.0  
Switching Frequency =  
9X Modulation Frequency  
0.75  
0.5  
Output  
+1  
0
0.25  
0
–1  
–0.25  
–0.5  
–0.75  
–1.0  
0°  
90°  
180°  
270°  
360° 420°  
Figure 1. Switching Amplifier Basic Waveforms  
The concept of switching amplifiers has been around for  
about 50 years but they were impractical before the advent  
of complementary TMOS power MOSFETs. Vacuum tubes  
were fast enough but they were rather poor switches. A  
totem pole circuit with supply voltages of±250 volts would  
drop about 50 volts when switching a current of 200  
milliamps. The efficiency of a tube switching amp could  
therefore not exceed 80%. The transformer needed to  
match the high plate impedance to the low impedance  
speaker filter was impractical as well.  
This document may contain references to devices which are no  
longer offered. Please contact your ON Semiconductor represen-  
tative for information on possible replacement devices.  
Semiconductor Components Industries, LLC, 2002  
1
Publication Order Number:  
August, 2002 – Rev. 3  
AN1042/D  

与AN1042相关器件

型号 品牌 获取价格 描述 数据表
AN-1042 CYMBET

获取价格

EnerChip CC Backup Power for Epson RX-8564 Real-Time Clock
AN1042D ONSEMI

获取价格

High Fidelity Switching Audio Amplifiers Using TMOS Power MOSFETs
AN1043 MICROCHIP

获取价格

Unique Features of the MCP23X08/17 GPIO Expanders
AN-1043 CYMBET

获取价格

EnerChip CC as Backup Power for a DS1390 Real-Time Clock
AN10436 NXP

获取价格

TDA8932B/33(B) Class-D audio amplifier
AN1045 STMICROELECTRONICS

获取价格

ST7 S/W IMPLEMENTATION OF I2C BUS MASTER
AN-1045 CYMBET

获取价格

EnerChip CC Backup Power for Micro Crystal RV-2123 RTC
AN-1046 CYMBET

获取价格

EnerChip CC as Backup Power for a Microchip MCP79410 RTC
AN-1047 CYMBET

获取价格

EnerChip CC Real-Time Clock Backup for K60 Microcontroller
AN-1048 CYMBET

获取价格

EnerChip CC as Backup Power for a DS1340 Real-Time Clock