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MIPSZ2012D2R2 Datasheet(PDF) 38 Page - STMicroelectronics |
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MIPSZ2012D2R2 Datasheet(HTML) 38 Page - STMicroelectronics |
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38 / 48 page ![]() Application information TS4621B 38/48 Doc ID 022194 Rev 2 The gain range in these configurations remains unchanged and is given by: With reference to Figure 80., note that the absolute phase in the audio band is 180°. 4.5.1 Layout recommendations for single-ended operation The connection location of each input that has to be set to ground is extremely important. Incorrect connection location Figure 81. Incorrect ground connection for single-ended option If these inputs are connected to AGnd (the ground of the TS4621B class-G), the output voltage can be expressed by the following simplified equation from an AC point of view. Vout = Av x (Vaudio + Vmc + Vgndnoise) + Vbatnoise x PSRR (1) As shown in Equation (1), any ground noise and any parasitic AC voltage on Vmc is directly multiplied by the gain of the amplifier. If Vmc can be totally controlled by the design of the audio source device (no parasitic AC voltage), it is not necessarily the case for Vgndnoise. This noise can be significantly reduced by an adequate low impedance ground plane, but not totally eliminated. In practice, only ten millivolts in the right frequency range are enough to produce an audible parasitic sound in the headphone with a volume level as low as -20 dB. VoutLR VinLR Gain × = Rout 12 ohms min. Rout 12 ohms min. Cout 0.8 nF min. Cout 0.8 nF min. Cin 1 µF Cin 1 µF Cin 1 µF Cin 1 µF 1 2 3 J1 C12 2.2 µF Cs 2.2 µF Css 2.2 µF Ct 10 µF L1 3.3 µH Vbat I²C bus + - + - I2C Negative supply Positive supply AGnd C1 C2 SDA SCL AVdd InL- InL+ InR+ InR- VoutL VoutR CMS Level detector Level detector Sw HpVdd PVss Audio driver Left output Right output Vgndnoise VaudioL VaudioR Vmc AM06154 |
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