MAX9778ETI+T Maxim Integrated Products, MAX9778ETI+T Datasheet - Page 19
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MAX9778ETI+T
Manufacturer Part Number
MAX9778ETI+T
Description
IC AMP AUDIO PWR 2.6W AB 28TQFN
Manufacturer
Maxim Integrated Products
Type
Class ABr
Datasheet
1.MAX9777ETIT.pdf
(27 pages)
Specifications of MAX9778ETI+T
Output Type
2-Channel (Stereo) with Stereo Headphones
Max Output Power X Channels @ Load
2.6W x 2 @ 4 Ohm; 200mW x 2 @ 16 Ohm
Voltage - Supply
4.5 V ~ 5.5 V
Features
Depop, Input Multiplexer, Mute, Shutdown, Thermal Protection,
Mounting Type
Surface Mount
Package / Case
28-TQFN Exposed Pad
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
External feedback components set the gain of the
MAX9777/MAX9778. Resistor R
input amplifier (A
the second stage amplifier (A
Combining A
ended gain of the device as follows:
As shown, the two-stage amplifier architecture results
in a noninverting gain configuration, preserving
absolute phase through the MAX9777/MAX9778. The
gain of the device in BTL mode is twice that of the sin-
gle-ended mode. Choose R
and R
The input capacitor (C
a highpass filter that removes the DC bias from an
incoming signal. The AC-coupling capacitor allows the
amplifier to bias the signal to an optimum DC level.
Assuming zero-source impedance, the -3dB point of
the highpass filter is given by:
Choose R
tion. Choose the C
lowest frequency of interest. Setting f
the amplifier’s low-frequency response. Use capacitors
whose dielectrics have low-voltage coefficients, such as
tantalum or aluminum electrolytic. Capacitors with high-
voltage coefficients, such as ceramics, may result in an
increased distortion at low frequencies.
Other considerations when designing the input filter
include the constraints of the overall system,
the actual frequency band of interest, and click-and-
pop suppression.
The MAX9777/MAX9778 require output-coupling
capacitors to operate in single-ended (headphone)
mode. The output-coupling capacitor blocks the DC
component of the amplifier output, preventing DC cur-
rent from flowing to the load. The output capacitor and
A
V
=
F
A
between 15kΩ and 100kΩ.
VIN
A
IN
VIN
×
according to the Gain-Setting Resistors sec-
VIN
A
= −
VOUT
and A
VIN
_ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _
⎛
⎜
⎝
f
IN
10
−
R
), and resistor R
Stereo 3W Audio Power Amplifiers with
3
= −
IN
dB
k
IN
such that f
VOUT
Ω
), in conjunction with R
⎛
⎜
⎝
⎞
⎟
⎠
=
10
,
Output-Coupling Capacitor
R
2π
Component Selection
IN
A
IN
, R
k
VOUT
Ω
R C
VOUT
between 10kΩ and 15kΩ
IN IN
IN
1
⎞
⎟ × −
⎠
Gain-Setting Resistors
IN
-3dB
and R
):
sets the gain of the
= −
-3dB
⎛
⎜
⎝
F
is well below the
10
Headphone Drive and Input Mux
⎛
⎜
⎝
sets the gain of
F
R
10
too high affects
k
R
F
set the single-
Ω
k
F
Ω
Input Filter
⎞
⎟ = +
⎠
⎞
⎟
⎠
IN
⎛
⎜
⎝
, forms
R
R
IN
F
⎞
⎟
⎠
the load impedance form a highpass filter with a -3dB
point determined by:
As with the input capacitor, choose C
f
Setting f
quency response.
Load impedance is a concern when choosing C
Load impedance can vary, changing the -3dB point of
the output filter. A lower impedance increases the cor-
ner frequency, degrading low-frequency response.
Select C
bination yields an adequate response. Select capaci-
tors with low ESR to minimize resistive losses and
optimize power transfer to the load.
If layout constraints require a physically smaller output-
coupling capacitor, decrease the value of C
series resistance to the output of the MAX9777/MAX9778
(see Figure 9). With the added series resistance at the
output, the cutoff frequency of the highpass filter is:
Since the cutoff frequency of the output highpass filter
is inversely proportional to the product of the total load
resistance seen by the outputs (R
C
MAX9777/MAX9778 outputs by the same amount C
is decreased to maintain low-frequency performance.
Since the added series resistance forms a voltage-
divider with the headphone speaker resistance for fre-
quencies within the passband of the highpass filter,
there is a loss in voltage gain. To compensate for this
loss, increase the voltage gain setting by an amount
equal to the attenuation due to the added series resis-
tance. Use the following equation to approximate the
required voltage gain compensation:
Figure 9. Reducing C
-3dB
OUT
is well below the lowest frequency of interest.
, increase the total resistance seen by the
OUT_+
OUT
-3dB
A
V COMP
f
such that the worst-case load/C
−
_
too high affects the amplifier‘s low-fre-
3
dB
=
f
OUT
−
C
3
OUT
2π
dB
=
by Adding R
(
20
R
=
L
log
2π
+
R
R C
⎛
⎜
⎝
SERIES
L OUT
R
1
1
L
R
SERIES
+
SERIES
R
R
SERIES
L
)
L
C
+ R
OUT
OUT
OUT
SERIES
⎞
⎟
⎠
such that
OUT
and add
R
L
) and
com-
OUT
OUT
19
.