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TS421-2 数据表(PDF) 27 Page - STMicroelectronics |
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TS421-2 数据表(HTML) 27 Page - STMicroelectronics |
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27 / 32 page ![]() TS419-TS421 27/32 APPLICATION INFORMATION s BTL Configuration Principle The TS419 & TS420 are monolithic power amplifiers with a BTL output type. BTL (Bridge Tied Load) means that each end of the load is connected to two single-ended output amplifiers. Thus, we have: Single ended output 1 = Vout1 = Vout (V) Single ended output 2 = Vout2 = -Vout (V) And Vout1 - Vout2 = 2Vout (V) The output power is : For the same power supply voltage, the output power in BTL configuration is four times higher than the output power in single ended configuration. s Gain In Typical Application Schematic (cf. page 3 of TS419-TS421 datasheet) In the flat region (no CIN effect), the output voltage of the first stage is: For the second stage : Vout2 = -Vout1 (V) The differential output voltage is The differential gain named gain (Gv) for more convenient usage is : Remark : Vout2 is in phase with Vin and Vout1 is phased 180 ° with Vin. This means that the positive terminal of the loudspeaker should be connected to Vout2 and the negative to Vout1. s Low and high frequency response In the low frequency region, CIN starts to have an effect. CIN forms with RIN a high-pass filter with a -3dB cut off frequency . In the high frequency region, you can limit the bandwidth by adding a capacitor (Cfeed) in parallel with Rfeed. It forms a low-pass filter with a -3dB cut off frequency . s Power dissipation and efficiency Hypothesis: • Load voltage and current are sinusoidal (Vout and Iout) • Supply voltage is a pure DC source (Vcc) Regarding the load we have: and and Then, the average current delivered by the supply voltage is: The power delivered by the supply voltage is: Psupply = Vcc IccAVG (W) Then, the power dissipated by the amplifier is: Pdiss = Psupply - Pout (W) and the maximum value is obtained when: and its value is: Remark : This maximum value is only dependent upon power supply voltage and load values. ) W ( R ) Vout 2 ( Pout L 2 RMS = ) V ( Rin Rfeed Vin 1 Vout − = ) V ( Rin Rfeed Vin 2 1 Vout 2 Vout = − Rin Rfeed 2 Vin 1 Vout 2 Vout Gv = − = (Hz) RinCin 2 1 FCL π = ) Hz ( Cfeed Rfeed 2 1 FCH π = ) V ( t sin V V PEAK OUT ω = ) A ( R V I L OUT OUT = ) W ( R 2 V P L 2 PEAK OUT = ) A ( R V 2 Icc L PEAK AVG π = ) W ( P P R Vcc 2 2 Pdiss OUT OUT L − π = 0 P Pdiss OUT = ∂ ∂ ) W ( R Vcc 2 max Pdiss L 2 2 π = |
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