Datasheet
TS488-TS489 Application information
Doc ID 11971 Rev 5 25/32
4.5 Gain setting
In the flat frequency response region (with no effect from C
in
, C
out
, C
feed
), the output voltage
is:
The gain A
V
is:
4.6 Decoupling of the circuit
Two capacitors are needed to properly bypass the TS488 (TS489), a power supply capacitor
C
s
and a bias voltage bypass capacitor C
b
.
C
s
has a strong influence on the THD+N in the high frequency range (above 7kHz) and
indirectly on the power supply disturbances. With 1 µF, you can expect THD+N performance
to be similar to the one shown in the datasheet. If C
s
is lower than 1 µF, the THD+N
increases in the higher frequencies and disturbances on the power supply rail are less
filtered. On the contrary, if C
s
is higher than 1 µF, the disturbances on the power supply rail
are more filtered.
C
b
has an influence on the THD+N in the low frequency range. Its value is critical on the
PSRR with grounded inputs in the lower frequencies:
■ If C
b
is lower than 1 µF, the THD+N improves and the PSRR worsens.
■ If C
b
is higher than 1 µF, the benefit on the THD+N and PSRR is small.
Note: The input capacitor C
in
also has a significant effect on the PSRR at lower frequencies. The
lower the value of C
in
, the higher the PSRR.
4.7 Standby mode
When the standby mode is activated an internal circuit of the TS488 (TS489) is charged
(see Figure 82). A time required to change the internal circuit is a few microseconds.
Figure 82. Internal equivalent schematic of the TS488 (TS489) in standby mode
V
OUT
V
IN
R
feed
R
in
--------------–
⎝⎠
⎛⎞
⋅ V
IN
A
V
⋅==
A
V
R
feed
R
in
--------------–=
25K
25K
600K
600K
Vin1
BYPASS
Vin2
Vout1
Vout2
GND
TS488/9