MAX9724C/MAX9724D
the MAX9724 addresses the problem of the RF suscep-
tibility by rejecting RF noise and preventing it from cou-
pling into the audio band.
The RF susceptibility of an amplifier can be measured
by placing the amplifier in an isolated chamber and sub-
jecting it to an electric field of known strength. If the
electric field is modulated with an audio band signal, a
percentage of the modulated signal is demodulated and
amplified by the device in the chamber. Figure 2 shows
the signal level at the outputs of an unoptimized amplifi-
er and the MAX9724. The test conditions are shown in
Table 1.
Click-and-Pop Suppression
In conventional single-supply audio amplifiers, the out-
put-coupling capacitor contributes significantly to audi-
ble clicks and pops. Upon startup, the amplifier charges
the coupling capacitor to its bias voltage, typically half
the supply. Likewise, on shutdown, the capacitor is dis-
charged. This results in a DC shift across the capacitor,
which appears as an audible transient at the speaker.
Since the MAX9724C/MAX9724D do not require output-
coupling capacitors, this problem does not arise.
Additionally, the MAX9724C/MAX9724D feature exten-
sive click-and-pop suppression that eliminates any audi-
ble transient sources internal to the device.
Typically, the output of the device driving the
MAX9724C/MAX9724D has a DC bias of half the supply
voltage. At startup, the input-coupling capacitor, C
IN
, is
charged to the preamplifier’s DC bias voltage through
the MAX9724C/MAX9724D input resistor, R
IN
, and a
series 15kΩ resistor. This DC shift across the capacitor
results in an audible click-and-pop. Delay the rise of
SHDN 4 to 5 time constants based on R
IN
x 15kΩ x C
IN
to eliminate clicks-and-pops caused by the input filter.
Shutdown
The MAX9724C/MAX9724D feature a < 0.1µA, low-
power shutdown mode that reduces quiescent current
consumption and extends battery life for portable appli-
cations. Drive SHDN low to disable the amplifiers and
the charge pump. In shutdown mode, the amplifier out-
put impedance is set to 14kΩ||R
F
(R
F
is 30kΩ for the
MAX9724D). The amplifiers and charge pump are
enabled once SHDN is driven high.
Applications Information
Power Dissipation
Under normal operating conditions, linear power ampli-
fiers can dissipate a significant amount of power. The
maximum power dissipation for each package is given
in the
Absolute Maximum Ratings
section under
Continuous Power Dissipation or can be calculated by
the following equation:
where T
J(MAX)
is +150°C, T
A
is the ambient tempera-
ture, and θ
JA
is the reciprocal of the derating factor in
P
TT
DISSPKG MAX
J MAX A
JA
()
()
=
θ
Low RF Susceptibility DirectDrive Stereo Head-
phone Amplifier with 1.8V Compatible Shutdown
10 ______________________________________________________________________________________
TEST PARAMETER SETTING
RF Field Strength 50V/m
RF Modulation Type Sine wave
RF Modulation Index 100%
RF Modulation Frequency 1kHz
Table 1. RF Susceptibility Test Conditions
MAX9724 fig02
RF CARRIER FREQUENCY (MHz)
AMPLIFIER OUTPUT AMPLITUDE (dBV)
1600 21001100
600
-80
-60
-40
-20
0
20
40
RF SUSCEPTIBLE
AMPLIFIER
MAX9724
62dB IMPROVEMENT
AT 850MHz
39dB IMPROVEMENT
AT 900MHz
67dB IMPROVEMENT
AT 1800MHz
49dB IMPROVEMENT
AT 1900MHz
-100
100
2600
Figure 2. RF Susceptibility of the MAX9724 and a Typical Headphone Amplifier
MAX9724C/MAX9724D
Low RF Susceptibility DirectDrive Stereo Head-
phone Amplifier with 1.8V Compatible Shutdown
______________________________________________________________________________________ 11
°C/W as specified in the
Absolute Maximum Ratings
section. For example, θ
JA
of the thin QFN package is
+68°C/W, and 154.2°C/W for the UCSP package.
The MAX9724C/MAX9724D have two power dissipation
sources; a charge pump and the two output amplifiers.
If power dissipation for a given application exceeds the
maximum allowed for a particular package, reduce
V
DD
, increase load impedance, decrease the ambient
temperature, or add heatsinking to the device. Large
output, supply, and ground traces decrease θ
JA
, allow-
ing more heat to be transferred from the package to the
surrounding air.
Thermal-overload protection limits total power dissipa-
tion in the MAX9724C/MAX9724D. When the junction
temperature exceeds +150°C, the thermal protection
circuitry disables the amplifier output stage. The ampli-
fiers are enabled once the junction temperature cools
by approximately 12°C. This results in a pulsing output
under continuous thermal-overload conditions.
Output Dynamic Range
Dynamic range is the difference between the noise floor
of the system and the output level at 1% THD+N.
Determine the system’s dynamic range before setting the
maximum output gain. Output clipping occurs if the out-
put signal is greater than the dynamic range of the sys-
tem. The DirectDrive architecture of the MAX9724C/
MAX9724D has increased the dynamic range compared
to other single-supply amplifiers.
Maximum Output Swing
V
DD
< 4.35V
If the output load impedance is greater than 1kΩ, the
MAX9724C/MAX9724D can swing within a few millivolts
of their supply rail. For example, with a 3.3V supply, the
output swing is 2V
RMS
, or 2.83V peak while maintaining
a low 0.003% THD+N. If the supply voltage drops to
3V, the same 2.83V peak has only 0.05% THD+N.
V
DD
> 4.35V
Internal device structures limit the maximum voltage
swing of the MAX9724C/MAX9724D when operated at
supply voltages greater than 4.35V. The output must not
be driven such that the peak output voltage exceeds the
opposite supply voltage by 9V. For example, if V
DD
=
5V, the charge pump sets PVSS = -5V. Therefore, the
peak output swing must be less than ±4V to prevent
exceeding the absolute maximum ratings.
UVLO
The MAX9724C/MAX9724D feature an undervoltage
lockout (UVLO) function that prevents the device from
operating if the supply voltage is less than 2.5V. This fea-
ture ensures proper operation during brownout condi-
tions and prevents deep battery discharge. Once the
supply voltage exceeds the UVLO threshold, the
MAX9724C/MAX9724D charge pump is turned on and
the amplifiers are powered, provided that SHDN is high.
Component Selection
Input-Coupling Capacitor
The input capacitor (C
IN
), in conjunction with the input
resistor (R
IN
), forms a highpass filter that removes the
DC bias from an incoming signal (see the
Functional
Diagram/Typical Operating Circuits
). The AC-coupling
capacitor allows the device to bias the signal to an opti-
mum DC level. Assuming zero-source impedance, the
-3dB point of the highpass filter is given by:
Choose the C
IN
such that f
-3dB
is well below the lowest
frequency of interest. Setting f
-3dB
too high affects the
device’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, can result
in increased distortion at low frequencies.
Charge-Pump Capacitor Selection
Use ceramic capacitors with a low ESR for optimum
performance. For optimal performance over the extend-
ed temperature range, select capacitors with an X7R
dielectric. Table 2 lists suggested manufacturers.
Flying Capacitor (C1)
The value of the flying capacitor (see the
Functional
Diagram/Typical Operating Circuits
) affects the charge
f
RC
dB
IN IN
=
3
1
2π
SUPPLIER PHONE FAX
WEBSITE
Taiyo Yuden 800-348-2496 847-925-0899 www.t-yuden.com
TDK 847-803-6100 847-390-4405
www.component.tdk.com
Murata 770-436-1300 770-436-3030
www.murata.com
Table 2. Suggested Capacitor Manufacturers
MAX9724C/MAX9724D
pump’s load regulation and output resistance. A C1
value that is too small degrades the device’s ability to
provide sufficient current drive, which leads to a loss of
output voltage. Increasing the value of C1 improves load
regulation and reduces the charge-pump output resis-
tance to an extent. See the Output Power vs. Load
Resistance and Charge-Pump Capacitor Size graph in
the
Typical Operating Characteristics
. Above 1µF, the
on-resistance of the switches and the ESR of C1 and C2
dominate.
Hold Capacitor (C2)
The hold capacitor value (see the
Functional
Diagram/Typical Operating Circuits
) and ESR directly
affect the ripple at PVSS. Increasing the value of C2
reduces output ripple. Likewise, decreasing the ESR of
C2 reduces both ripple and output resistance. Lower
capacitance values can be used in systems with low
maximum output power levels. See the Output Power
vs. Load Resistance and Charge-Pump Capacitor Size
graph in the
Typical Operating Characteristics
.
Power-Supply Bypass Capacitor (C3)
The power-supply bypass capacitor (see the
Functional
Diagram/Typical Operating Circuits
) lowers the output
impedance of the power supply and reduces the
impact of the MAX9724C/MAX9724D’s charge-pump
switching transients. Bypass V
DD
with C3, the same
value as C1, and place it physically close to the V
DD
and PGND pins.
Amplifier Gain
The gain of the MAX9724D amplifier is internally set to
-1.5V/V. All gain-setting resistors are integrated into the
device, reducing external component count. The inter-
nally set gain, in combination with DirectDrive, results in
a headphone amplifier that requires only five small
capacitors to complete the amplifier circuit: two for the
charge pump, two for audio input coupling, and one for
power-supply bypassing (see the
Functional
Diagram/Typical Operating Circuits
).
The gain of the MAX9724C amplifier is set externally as
shown in Figure 3, the gain is:
A
V
= -R
F
/R
IN
(V/V)
Choose feedback resistor values in the tens of kΩ
range. Lower values may cause excessive power dissi-
pation and require impractically small values of R
IN
for
large gain settings. The high-impedance state of the
outputs can also be degraded during shutdown mode
if an inadequate feedback resistor is used since the
equivalent output impedance during shutdown is
14kΩ||R
f
(R
F
is equal to 30kΩ for the MAX9724D). The
source resistance of the input device may also need to
be taken into consideration. Since the effective value of
R
IN
is equal to the sum of the source resistance of the
input device and the value of the input resistor connect-
ed to the inverting terminal of the headphone amplifier
(20kΩ for the MAX9724D), the overall closed-loop gain
of the headphone amplifier can be reduced if the input
resistor is not significantly larger than the source resis-
tance of the input device.
Low RF Susceptibility DirectDrive Stereo Head-
phone Amplifier with 1.8V Compatible Shutdown
12 ______________________________________________________________________________________
LEFT
AUDIO
INPUT
RIGHT
AUDIO
INPUT
OUTL
INL
INR
OUTR
MAX9724C
R
IN
R
IN
R
F
R
F
Figure 3. Gain Setting for the MAX9724C

MAX9724DETC+

Mfr. #:
Manufacturer:
Maxim Integrated
Description:
Audio Amplifiers Low RF Susceptible Headphone Amplifier
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