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TS4994 Folha de dados(PDF) 21 Page - STMicroelectronics

Nome de Peças TS4994
Descrição Electrónicos  1W Differential Input/Output Audio Power Amplifier with Selectable Standby
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Fabricante Electrônico  STMICROELECTRONICS [STMicroelectronics]
Página de início  http://www.st.com
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TS4994 Folha de dados(HTML) 21 Page - STMicroelectronics

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Application Information
TS4994
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4.5 Calculating the influence of mismatching
On PSRR performance:
For this calculation, we consider that Cin and Cfeed have no influence.
We use the same kind of resistor (same tolerance) and
∆R is the tolerance value in %.
The following equation is valid for frequencies ranging from DC to about 1kHz. Above this frequency,
parasitic effects start to be significant and a literal equation is not possible to write.
The PSRR equation is (
∆R in %):
This equation doesn’t include the additional performance provided by bypass capacitor filtering. If a
bypass capacitor is added, it acts, together with the internal high output impedance bias, as a low-pass
filter, and the result is a quite important PSRR improvement with a relatively small bypass capacitor.
The complete PSRR equation (
∆R in %, Cb in microFarad and F in Hz) is:
Example: With
∆R=0.1% and Cb=0, the minimum PSRR would be -60dB. With a 100nF bypass
capacitor, at 100Hz the new PSRR would be -93dB.
This example is a worst case scenario, where each resistor has extreme tolerance and illustrates the fact
that with only a small bypass capacitor, the TS4994 produce high PSRR performance.
In addition, it’s important to note that this is a theoretical formula. As the TS4994 has self-generated
noise, you should consider that the highest practical PSRR reachable is about -110dB. It is therefore
unreasonable to target a -120dB PSRR.
The three following graphs show PSRR versus frequency and versus bypass capacitor Cb in worst-case
condition (
∆R=0.1%).
Figure 70. PSRR vs. frequency worst case
condition
Figure 71. PSRR vs. frequency worst case
condition
)
dB
(
)
R
10000
(
100
R
Log
20
PSRR
2
×
×
PSRR
20
∆R 100
×
10000
∆R
2
()
1F
2
+
C
b
2
22.2
×
×
×
-----------------------------------------------------------------------------------------------------
log
×
(dB)
100
1000
10000
-140
-130
-120
-110
-100
-90
-80
-70
-60
-50
-40
-30
-20
-10
0
Cb=0.1
µF
Cb=1
µF
Cb=0
20k
20
Cb=0.47
µF
Vcc = 5V, Vripple = 200mVpp
Av = 1, Cin = 4.7
µF
∆R/R = 0.1%, RL ≥ 8Ω
Tamb = 25
°C, Inputs = Grounded
Frequency (Hz)
100
1000
10000
-140
-130
-120
-110
-100
-90
-80
-70
-60
-50
-40
-30
-20
-10
0
Cb=0.1
µF
Cb=1
µF
Cb=0
20k
20
Cb=0.47
µF
Vcc = 3.3V, Vripple = 200mVpp
Av = 1, Cin = 4.7
µF
∆R/R = 0.1%, RL ≥ 8Ω
Tamb = 25
°C, Inputs = Grounded
Frequency (Hz)


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