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Component selection – Rainbow Electronics MAX13331 User Manual

Page 11

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MAX13330/MAX13331

Automotive DirectDrive Headphone Amplifiers

with Output Protection and Diagnostics

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11

Thermal-overload protection limits total power dissipa-
tion in the MAX13330/MAX13331. When the junction
temperature exceeds +145°C (typ), the thermal-protec-
tion circuitry disables the amplifier output stage. The
amplifiers are enabled once the junction temperature
cools by 5°C. This results in a pulsing output under
continuous thermal-overload conditions.

Output Power

The device has been specified for the worst-case sce-
nario, when both inputs are in-phase. Under this condi-
tion, the amplifiers simultaneously draw current from the
charge pump, leading to a proportional reduction in
V

SS

headroom. In typical stereo audio applications, the

left and right signals have differences in both magni-
tude and phase, subsequently leading to an increase in
the maximum attainable output power. Figure 4 shows
the two extreme cases for in- and out-of-phase. In reali-
ty, the available power lies between these extremes.

UVLO

The MAX13330/MAX13331 feature a UVLO function that
prevents the device from operating if the supply voltage
is less than 3.6V (typ). This feature ensures proper
operation during brownout conditions and prevents
deep battery discharge. Once the supply voltage
reaches the UVLO threshold, the charge-pump is
turned on and the amplifiers are powered.

Component Selection

Gain-Setting Resistors (MAX13331 Only)

The gain of the MAX13330 is internally set at -1.5V/V.
All gain-setting resistors are integrated into the device,
reducing external component count. The internally set
gain, in combination with DirectDrive, results in a head-
phone amplifier that requires only five tiny 1µF capaci-
tors to complete the amplifier circuit: two for the
charge-pump, two for audio input coupling, and one for
power-supply bypassing (see the

Typical Application

Circuits

). The gain of the MAX13331 amplifier is set

externally as shown in the

Typical Application Circuits

,

the gain is:

Choose feedback resistor values of 10kΩ. Values other
than 10kΩ increase output offset voltage due to the
input bias current, which in turn, increases the amount
of DC current flow to the load.

Input Filtering

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

Typical

Application Circuits

). The AC-coupling capacitor allows

the device to bias the signal to an optimum DC level.
Assuming zero source impedance, the -3dB point of
the highpass filter is given by:

Choose C

IN

so f

-3dB

is well below the lowest frequency

of interest. For the MAX13330, use the value of R

IN

as

given in the

Electrical Characteristics

table. 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 capacitors with an ESR less than 100mΩ for opti-
mum performance. Low-ESR ceramic capacitors mini-
mize the output resistance of the charge pump. For
best performance over the extended temperature
range, select capacitors with an X7R dielectric.

f

R

C

Hz

dB

IN

IN

=

Ч

Ч

3

1

2

π

(

)

A

R

R

V V

V

F

IN

= −

( / )

OUTPUT POWER vs. SUPPLY VOLTAGE

SUPPLY VOLTAGE (V)

OUTPUT POWER (mW)

4.25

5.00

5.25

4.75

4.50

50

100

150

200

250

0

4.00

5.50

f

IN

= 1kHz

R

L

= 32

Ω

THD+N = 10%

INPUTS

IN PHASE

INPUTS 180

°

OUT OF PHASE

Figure 4. Output Power vs. Supply Voltage