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TPA152DR 参数 Datasheet PDF下载

TPA152DR图片预览
型号: TPA152DR
PDF下载: 下载PDF文件 查看货源
内容描述: 双路音频放大器\n [Dual Audio Amplifier ]
分类和应用: 消费电路商用集成电路音频放大器视频放大器光电二极管PC
文件页数/大小: 16 页 / 271 K
品牌: TI [ TEXAS INSTRUMENTS ]
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TPA152  
75-mW STEREO AUDIO POWER AMPLIFIER  
SLOS210A – JUNE 1998 – REVISED MARCH 2000  
APPLICATION INFORMATION  
gain setting resistors, R and R  
F
I
The gain for the TPA152 is set by resistors R and R according to equation 1.  
F
I
R
F
Gain  
(1)  
R
I
Given that the TPA152 is a MOS amplifier, the input impedance is very high, consequently input leakage  
currents are not generally a concern although noise in the circuit increases as the value of R increases. In  
F
addition, a certain range of R values are required for proper start-up operation of the amplifier. Taken together  
F
it is recommended that the effective impedance seen by the inverting node of the amplifier be set between 5  
kand 20 k. The effective impedance is calculated in equation 2.  
R R  
F I  
Effective Impedance  
(2)  
R
R
F
I
As an example, consider an input resistance of 20 kand a feedback resistor of 20 k. The gain of the amplifier  
would be 1 and the effective impedance at the inverting terminal would be 10 k, which is within the  
recommended range.  
For high performance applications, metal film resistors are recommended because they tend to have lower  
noise levels than carbon resistors. For values of R above 50 k, the amplifier tends to become unstable due  
F
to a pole formed from R and the inherent input capacitance of the MOS input structure. For this reason, a small  
F
compensation capacitor of approximately 5 pF should be placed in parallel with R . This, in effect, creates a  
F
low-pass filter network with the cutoff frequency defined in equation 3.  
1
2 R C  
f
(3)  
c(lowpass)  
F
F
For example if R is 100 kand C is 5 pF then f is 318 kHz, which is well outside the audio range.  
co(lowpass)  
F
F
input capacitor, C  
I
In the typical application, an input capacitor, C , is required to allow the amplifier to bias the input signal to the  
I
proper dc level for optimum operation. In this case, C and R form a high-pass filter with the corner frequency  
I
I
determined in equation 4.  
1
f
(4)  
c(highpass)  
2 R C  
I
I
The value of C is important to consider as it directly affects the bass (low frequency) performance of the circuit.  
I
Consider the example where R is 20 kand the specification calls for a flat bass response down to 20 Hz.  
I
Equation 4 is reconfigured as equation 5.  
1
C
(5)  
I
2 R f  
c(highpass)  
I
In this example, C is 0.40 µF, so one would likely choose a value in the range of 0.47 µF to 1 µF. A further  
I
consideration for this capacitor is the leakage path from the input source through the input network (R , C ) and  
I
I
thefeedbackresistor(R )totheload. Thisleakagecurrentcreatesadcoffsetvoltageattheinputtotheamplifier  
F
that reduces useful headroom, especially in high-gain applications (> 10). For this reason a low-leakage  
tantalum or ceramic capacitor is the best choice. When polarized capacitors are used, the positive side of the  
capacitor should face the amplifier input in most applications, as the dc level there is held at V /2, which is  
DD  
likely higher that the source dc level. Please note that it is important to confirm the capacitor polarity in the  
application.  
12  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
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