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TS4890ID 数据表(PDF) 29 Page - STMicroelectronics |
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TS4890ID 数据表(HTML) 29 Page - STMicroelectronics |
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29 / 32 page ![]() TS4890 29/32 s Note on how to use the PSRR curves (page 8) We have finished a design and we have chosen for the components : • Rin=Rfeed=22k Ω • Cin=100nF • Cb=1µF Now, on fig. 16, we can see the PSRR (input grounded) vs frequency curves. At 217Hz, we have a PSRR value of -36dB. In reality we want a value about -70dB. So, we need a gain of 34dB ! Now, on fig. 15 we can see the effect of Cb on the PSRR (input grounded) vs. frequency. With Cb=100µF, we can reach the -70dB value. The process to obtain the final curve (Cb=100µF, Cin=100nF, Rin=Rfeed=22k Ω) is a simple transfer point by point on each frequency of the curve on fig. 16 to the curve on fig. 15. The measurement result is shown on the next figure. Fig. 107 : PSRR changes with Cb s Note on PSRR measurement What is the PSRR ? The PSRR is the Power Supply Rejection Ratio. It's a kind of SVR in a determined frequency range. The PSRR of a device, is the ratio between a power supply disturbance and the result on the output. We can say that the PSRR is the ability of a device to minimize the impact of power supply disturbances to the output. How do we measure the PSRR ? Fig. 108 : PSRR measurement schematic s Principle of operation • We fixed the DC voltage supply (Vcc) • We fixed the AC sinusoidal ripple voltage (Vripple) • No bypass capacitor Cs is used The PSRR value for each frequency is : Remark : The measure of the Rms voltage is not a Rms selective measure but a full range (2 Hz to 125 kHz) Rms measure. It means that we measure the effective Rms signal + the noise. 10 100 1000 10000 100000 -70 -60 -50 -40 -30 Cin=100nF Cb=100 µF Cin=100nF Cb=1 µF Vcc = 5 & 2.2V Rfeed = 22k, Rin = 22k Rg = 100 Ω, RL = 8Ω Tamb = 25 °C Frequency (Hz) Vripple Vcc Rin Cin Rg 100 Ohms Cb Rfeed 4 3 2 1 5 8 Vin- Vin+ - + - + Bypass Standby Bias 6 Vout1 Vout2 Av=-1 TS4890 Vs- Vs+ RL 7 − × = − + ) Vs Vs ( Rms ) V ( Rms Log 20 ) dB ( PSRR ripple 10 |
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