The TDA8932B is a high efficiency class-D amplifier with low power dissipation.
The continuous time output power is 2 × 15 W in stereo half-bridge application (RL=4Ω)
or 1 × 30 W in mono full-bridge application (RL=8Ω). Due to the low power dissipation
the device can be used without any external heat sink when playing music. Due to the
implementation of thermal foldback, even for high supply voltages and/or lower load
impedances, the device remains operating with considerable music output power without
the need for an external heat sink.
The device has two full-differential inputs driving two independent outputs. It can be used
as mono full-bridge configuration (BTL) or as stereo half-bridge configuration (SE).
2.Features
n Operating voltage from 10 V to 36 V asymmetrical or ±5 V to ±18 V symmetrical
n Mono-bridged tied load (full-bridge) or stereo single-ended (half-bridge) application
n Application without heatsink using thermally enhanced small outline package
n High efficiency and low-power dissipation
n Thermally protected and thermal foldback
n Current limiting to avoid audio holes
n Full short-circuit proof across load and to supply lines (using advanced current
n Switchable internal or external oscillator (master-slave setting)
n No pop noise
n Full-differential inputs
3.Applications
n Flat panel television sets
n Flat panel monitor sets
n Multimedia systems
n Wireless speakers
n Mini and micro systems
n Home sound sets
protection)
NXP Semiconductors
4.Quick reference data
Table 1.Quick reference data
VP= 22 V; f
Symbol ParameterConditionsMinTypMaxUnit
Supplies
V
P
I
P
I
q(tot)
Stereo SE channel; R
P
o(RMS)
Mono BTL; R
P
o(RMS)
osc
supply voltageasymmetrical supply102236V
supply currentSleep mode-0.61.0mA
total quiescent
current
RMS output powercontinuous time output power
RMS output powercontinuous time output power;
= 320 kHz; T
< 0.1 Ω
s
[1]
< 0.1 Ω
s
TDA8932B
Class-D audio amplifier
=25°C; unless otherwise specified.
amb
Operating mode; no load, no
snubbers and no filter
connected
[1]
per channel;
THD+N = 10 %; f
=4Ω; VP= 22 V13.815.3-W
R
L
=8Ω; VP= 30 V14.015.5-W
R
L
= 1 kHz
i
short time output power per
channel; THD+N = 10 %;
f
= 1 kHz
i
RL=4Ω; VP= 29 V23.826.5-W
THD+N = 10 %; f
=4Ω; VP= 12 V15.517.2-W
R
L
=8Ω; VP= 22 V28.932.1-W
R
L
= 1 kHz
i
short time output power;
THD+N = 10 %; f
= 1 kHz
i
RL=8Ω; VP= 29 V49.555.0-W
- 4050mA
[2]
[2]
[1] Output power is measured indirectly; based on R
[2] Two layer application board (55 mm × 45 mm), 35 µm copper, FR4 base material in free air with natural
convection.
measurement.
DSon
5.Ordering information
Table 2.Ordering information
Type number Package
NameDescriptionVersion
TDA8932BTSO32plastic small outline package; 32 leads;
body width 7.5 mm
TDA8932BTW HTSSOP32 plastic thermal enhanced thin shrink small outline
IN1P2positive audio input for channel 1
IN1N3negative audio input for channel 1
DIAG4diagnostic output; open-drain
ENGAGE5engage input to switch between Mute mode and Operating mode
POWERUP6power-up input to switch between Sleep mode and Mute mode
CGND7control ground; reference for POWERUP, ENGAGE and DIAG
V
DDA
V
SSA
OSCREF10input internal oscillator setting (only master setting)
HVPREF11decoupling of internal half supply voltage reference
INREF12decoupling for input reference voltage
TEST13test signal input; for testing purpose only
IN2N14negative audio input for channel 2
IN2P15positive audio input for channel 2
V
SSD(HW)
V
SSD(HW)
DREF18decoupling of internal (reference) 5 V regulator for logic supply
1negative digital supply voltage and handle wafer connection
8positive analog supply voltage
9negative analog supply voltage
16negative digital supply voltage and handle wafer connection
17negative digital supply voltage and handle wafer connection
HVP219half supply output voltage 2 for charging single-ended capacitor for
V
DDP2
BOOT221bootstrap high-side driver channel 2
OUT222PWM output channel 2
V
SSP2
STAB224decoupling of internal 11 V regulator for channel 2 drivers
STAB125decoupling of internal 11 V regulator for channel 1 drivers
V
SSP1
OUT127PWM output channel 1
BOOT128bootstrap high-side driver channel 1
V
DDP1
HVP130half supply output voltage 1 for charging single-ended capacitor for
OSCIO31oscillator input in slave configuration or oscillator output in master
V
SSD(HW)
Exposed die
pad
TDA8932B
Class-D audio amplifier
channel 2
20positive power supply voltage for channel 2
23negative power supply voltage for channel 2
26negative power supply voltage for channel 1
29positive power supply voltage for channel 1
channel 1
configuration
32negative digital supply voltage and handle wafer connection
-HTSSOP32 package only
[1]
[1] The exposed die pad has to be connected to V
8.Functional description
8.1General
The TDA8932B is a mono full-bridge or stereo half-bridge audio power amplifier using
class-D technology. The audio input signal is converted into a Pulse Width Modulated
(PWM) signal via an analog input stage and PWM modulator. To enable the output power
Diffusion Metal Oxide Semiconductor (DMOS) transistors to be driven, this digital PWM
signal is applied to a control and handshake block and driver circuits forboth the high side
and low side. A 2nd-order low-pass filter converts the PWM signal to an analog audio
signal across the loudspeakers.
The TDA8932B contains two independent half-bridges with full differential input stages.
The loudspeakers can be connected in the following configurations:
• Mono full-bridge: Bridge Tied Load (BTL)
• Stereo half-bridge: Single-Ended (SE)
The TDA8932B contains common circuits to both channels such as the oscillator, all
reference sources, the mode functionality and a digital timing manager. The following
protections are built-in: thermal foldback, temperature, current and voltage protections.
The TDA8932B can be switched in three operating modes using pins POWERUP and
ENGAGE:
• Sleep mode: with low supply current.
• Mutemode: the amplifiers are switching idle (50 % duty cycle), but the audio signal at
• Operating mode: the amplifiers are fully operational with output signal.
• Fault mode.
Both pins POWERUP and ENGAGE refer to pin CGND.
Table 4 shows the different modes as a function of the voltages on the POWERUP and
ENGAGE pins.
Table 4.Mode selection
ModePin
Sleep< 0.8 V< 0.8 Vdon’t care
Mute2 V to 6.0 V
Operating2 V to 6.0 V
Fault2 V to 6.0 V
TDA8932B
Class-D audio amplifier
the output is suppressed bydisabling the Vl-converter input stages. The capacitors on
pins HVP1 and HVP2 have been charged to half the supply voltage (asymmetrical
supply only).
POWERUPENGAGEDIAG
[1]
[1]
[1]
[1]
< 0.8 V
2.4 V to 6.0 V
don’t care< 0.8 V
[1]
> 2 V
>2V
[1] In case of symmetrical supply conditions the voltage applied to pins POWERUP and ENGAGE must never
exceed the supply voltage (V
DDA
, V
DDP1
or V
DDP2
).
If the transition between Mute mode and Operatingmode is controlled via a time constant,
the start-up will be pop free since the DC output offset voltage is applied gradually to the
output between Mute mode and Operating mode. The bias current setting of the
VI-converters is related to the voltage on pin ENGAGE:
• Mute mode: the bias current setting of the VI-converters is zero (VI-converters
disabled)
• Operating mode: the bias current is at maximum
The time constant required to apply the DC output offset voltage gradually between Mute
mode and Operating mode can be generated by applying a decoupling capacitor on pin
ENGAGE. The value of the capacitor on pin ENGAGE should be 470 nF.
The output signal of the amplifier is a PWM signal with a carrier frequency of
approximately 320 kHz. Using a 2nd-order low-pass filter in the application results in an
analog audio signal across the loudspeaker. The PWM switching frequency can be set by
an external resistor Rosc connected between pins OSCREF and V
frequency can be set between 300 kHz and 500 kHz. Using an external resistor of 39 kΩ,
the carrier frequency is set to an optimized value of 320 kHz (see Figure 5).
If two or more TDA8932B devices are used in the same audio application, it is
recommended to synchronize the switching frequency of all devices. This can be realized
by connecting all pins OSCIO together and configure one of the TDA8932B in the
application as clock master, while the other TDA8932B devices are configured in slave
mode.
AUDIOAUDIOAUDIO
PWMPWM
operatingoperating
001aaf885
SSD(HW)
sleepmuteoperatingfault
. The carrier
Pin OSCIO is a 3-state input or output buffer.Pin OSCIO is configured in master mode as
oscillator output and in slave modeas oscillator input. Master mode is enabled byapplying
a resistor while slave mode is entered by connecting pin OSCREF directly to pin V
SSD(HW)
(without any resistor).
The value of the resistor also sets the frequency of the carrier which can be estimated by
If the junction temperature of the TDA8932B exceeds the threshold level (Tj> 140 °C) the
gain of the amplifier is decreased graduallyto a level where the combination of dissipation
(P) and the thermal resistance from junction to ambient [R
temperature around the threshold level.
This means that the device will not completely switch off, but remains operational at lower
output power levels. Especially with music output signals this feature enables high peak
output power while still operating without any external heat sink other than the
printed-circuit board area.
If the junction temperature still increases due to external causes, the OTP shuts down the
amplifier completely.
8.4.2OverTemperature Protection (OTP)
If the junction temperature Tj> 155 °C, then the power stage will shut down immediately.
8.4.3OverCurrent Protection (OCP)
When the loudspeaker terminals are short-circuited or if one of the demodulated outputs
of the amplifier is short-circuited to one of the supply lines, this will be detected by the
OCP.
TDA8932B
Class-D audio amplifier
] results in a junction
th(j-a)
If the output current exceeds the maximum output current (I
be limitedby the amplifier to 4 A while the amplifier outputs remain switching (the amplifier
is NOT shutdown completely). This is called current limiting.
The amplifier can distinguish between an impedance drop of the loudspeaker and a
low-ohmic short-circuit across the load or to one of the supply lines. This impedance
threshold depends on the supply voltage used:
• Incase of a short-circuit across the load, the audio amplifier is switchedoff completely
and after approximately 100 ms it will try to restart again. If the short-circuit condition
is still present after this time, this cycle will be repeated. The average dissipation will
be low because of this low duty cycle.
• In case of a short to one of the supply lines, this will trigger the OCP and the amplifier
will be shut down. During restart the window protection will be activated. As a result
the amplifier will not start until 100 ms after the short to the supply lines is removed.
• In case of impedance drop (e.g. due to dynamic behavior of the loudspeaker) the
same protection will be activated. The maximum output current is again limited to 4 A,
but the amplifier will NOT switch off completely (thus preventing audio holes from
occurring). The result will be a clipping output signal without any artifacts.
8.4.4Window Protection (WP)
The WP checks the PWM output voltage before switchingfrom Sleep mode to Mute mode
(outputs switching) and is activated:
> 4 A), this current will
O(ocp)
• During the start-up sequence, when pin POWERUP is switched from Sleep mode to
Mute mode. In the event of a short-circuit at one of the output terminals to V
V
, V
SSP1
for open-circuit outputs. Because the check is done before enablingthe power stages,
no large currents will flow in the event of a short-circuit.
the start-up procedure is interrupted and the TDA8932B waits
SSP2
DDP1
,
NXP Semiconductors
• When the amplifier is completely shut down due to activation of the OCP because a
8.4.5Supply voltage protection
If the supply voltage drops below 10 V, the UnderVoltage Protection (UVP) circuit is
activated and the system will shut down directly. This switch-off will be silent and without
pop noise. When the supply voltage rises above the threshold level, the system is
restarted again after 100 ms.
If the supply voltage exceeds 36 V the OverVoltage Protection (OVP) circuit is activated
and the power stages will shut down. It is re-enabled as soon as the supply voltage drops
below the threshold level. The system is restarted again after 100 ms.
It should be noted that supply voltages > 40 V may damage the TDA8932B. Two
conditions should be distinguished:
1. If the supply voltage is pumped to higher values by the TDA8932B application itself
2. If a supply voltage > 40 V is caused by other or external causes, then the TDA8932B
TDA8932B
Class-D audio amplifier
short-circuit to one of the supply lines is made, then during restart (after 100 ms) the
window protection will be activated. As a result the amplifier will not start until the
short-circuit to the supply lines is removed.
(see also Section 14.3), the OVP is triggered and the TDA8932B is shut down. The
supply voltage will decrease and the TDA8932B is protected against any overstress.
will shut down, but the device can still be damaged since the supply voltage will
remain > 40 V in this case. The OVP protection is not a supply voltage clamp.
An additional UnBalance Protection (UBP) circuit compares the positive analog supply
voltage (V
) and the negative analog supply voltage (V
DDA
) and is triggered if the
SSA
voltage difference between them exceeds a certain level. This level depends on the sum
of both supply voltages. The unbalance threshold levels can be defined as follows:
• LOW-level threshold: V
• HIGH-level threshold: V
P(th)(ubp)l
P(th)(ubp)h
<8⁄5× V
>8⁄3× V
HVPREF
HVPREF
In a symmetrical supply the UBP is released when the unbalance of the supply voltage is
within 6 % of its starting value.
Table 6 shows an overview of all protection and the effect on the output signal.
Whenevera protection is triggered, except for TF, pin DIAG is activated to LOWlevel (see
Table 6). An internal reference supply will pull-up the open-drain DIAG output to
approximately 2.4 V. This internal reference supply can deliver approximately 50 µA.
Pin DIAG refers to pin CGND. The diagnostic output signal during different short
conditions is illustrated in Figure 6. Using pin DIAG as input, a voltage < 0.8 V will put the
device into Fault mode.
TDA8932B
Class-D audio amplifier
V
2.4 V
0 V
o
amplifier
restartno restart
≈ 50 ms
≈ 50 ms
shorted load
2.4 V
0 V
V
o
short to
supply line
001aad759
Fig 6. Diagnostic output for different short-circuit conditions
8.6Differential inputs
For a high common-mode rejection ratio and a maximum of flexibility in the application,
the audio inputs are fully differential. By connecting the inputs anti-parallel, the phase of
one of the two channels can be inverted, so that the amplifier can operate as a mono BTL
amplifier. The input configuration for a mono BTL application is illustrated in Figure 7.
In SE configuration it is also recommended to connect the two differential inputs in
anti-phase. This has advantages forthe current handling of the power supply at low signal
frequencies and minimizes supply pumping (see also Section 14.8).
IN1P
IN1N
OUT1
audio
input
IN2P
IN2N
OUT2
001aad760
Fig 7. Input configuration for mono BTL application
8.7Output voltage buffers
When pin POWERUP is set HIGH, the half supply output voltage buffers are switched on
in asymmetrical supply configuration. The start-up will be pop free since the device starts
switching when the capacitor on pin HVPREF and the SE capacitors are completely
charged.
In accordance with the Absolute Maximum Rating System (IEC 60134).
Symbol ParameterConditionsMinMaxUnit
V
P
V
x
I
ORM
T
j
T
stg
T
amb
Ppower dissipation-5W
V
esd
TDA8932B
Class-D audio amplifier
supply voltageasymmetrical supply
voltage on pin x
IN1P, IN1N, IN2P, IN2N
OSCREF, OSCIO, TEST
POWERUP, ENGAGE,
DIAG
all other pins
repetitive peak output
current
maximum output
current limiting
junction temperature-150°C
storage temperature−55+150°C
ambient temperature−40+85°C
electrostatic discharge
voltage
HBM
MM
[1]
−0.3+40V
[2]
−5+5V
[3]
V
SSD(HW)
[4]
V
CGND
[5]
VSS− 0.3VDD + 0.3 V
[6]
4-A
[7]
−2000+2000V
[8]
−200+200V
− 0.3 5V
− 0.36V
[1] VP = V
[2] Measured with respect to pin INREF; Vx < VDD + 0.3 V.
[3] Measured with respect to pin V
[4] Measured with respect to pin CGND; Vx < VDD + 0.3 V.
[5] VSS = V
[6] Current limiting concept.
[7] Human Body Model (HBM); Rs= 1500 Ω; C = 100 pF
For pins 2, 3, 11, 14 and 15 V
[8] Machine Model (MM); Rs=0Ω; C = 200 pF; L = 0.75 µH.
DDP1
SSP1
− V
= V
SSP1
SSP2
= V
DDP2
; VDD = V
− V
SSD(HW)
DDP1
esd
SSP2
.
; Vx < VDD + 0.3 V.
= V
= ±1800 V.
DDP2
.
11. Thermal characteristics
Table 9.Thermal characteristics
SymbolParameterConditionsMinTypMaxUnit
SO32 package
R
Ψ
Ψ
th(j-a)
j-lead
j-top
thermal resistance from junction
to ambient
thermal characterization
parameter from junction to lead
thermal characterization
parameter from junction to top
thermal characterization
parameter from junction to lead
Ψ
j-top
thermal characterization
parameter from junction to top
R
th(j-c)
thermal resistance from junction
to case
[1] Measured on a JEDEC high K-factor test board (standard EIA/JESD 51-7) in free air with natural convection.
[2] Two layer application board (55 mm × 45 mm), 35 µm copper, FR4 base material in free air with natural convection.
[3] Strongly depends on where the measurement is taken on the package.
[4] Two layer application board (55 mm × 40 mm), 35 µm copper, FR4 base material in free air with natural convection.
free air natural convection
[1]
JEDEC test board
2 layer application board
-4750K/W
[4]
-48-K/W
--30K/W
[3]
--2K/W
free air natural convection-4.0-K/W
12. Static characteristics
Table 10.Static characteristics
VP= 22 V; f
SymbolParameterConditionsMinTypMaxUnit
Supply
V
P
I
P
I
q(tot)
Series resistance output power switches
R
DSon
Power-up input: pin POWERUP
V
I
I
I
V
IL
V
IH
Engage input: pin ENGAGE
V
O
V
I
I
O
V
IL
V
IH
= 320 kHz; T
osc
=25°C; unless otherwise specified.
amb
supply voltageasymmetrical supply102236V
symmetrical supply±5±11±18V
supply currentSleep mode; no load-0.61.0mA
total quiescent currentOperating mode; no load, no
[1] Measured with respect to pin CGND.
[2] Measured with respect to pin V
HIGH-level input voltage4.0-5V
LOW-level input voltage0-0.8V
HIGH-level output voltage4.0-5V
LOW-level output voltage0-0.8V
maximum number of slavesdriven by one master12---
[2]
SSD(HW)
.
13. Dynamic characteristics
Table 11.Switching characteristics
VP= 22 V; T
SymbolParameterConditionsMinTypMaxUnit
Internal oscillator
f
osc
Timing PWM output: pins OUT1 and OUT2
t
r
t
f
t
w(min)
=25°C; unless otherwise specified.
amb
oscillator frequencyRosc = 39 kΩ-320-kHz
range300-500kHz
rise timeIO=0A-10-ns
fall timeIO=0A-10-ns
minimum pulse widthIO=0A-80-ns
Table 12.SE characteristics
VP= 22 V; RL=2×4Ω; fi= 1 kHz; f
= 320 kHz; Rs< 0.1
osc
[1]
Ω
; T
=25°C; unless otherwise specified.
amb
SymbolParameterConditionsMinTypMaxUnit
THD+Ntotal harmonic
distortion-plus-noise
G
|∆G
α
cs
v(cl)
v
closed-loop voltage gainVi= 100 mV; no load293031dB
THD+N = 0.5 %; f
THD+N = 0.5 %; f
THD+N = 10 %; f
THD+N = 10 %; f
=8Ω; VP=30V
R
L
THD+N = 0.5 %; f
THD+N = 0.5 %; f
THD+N = 10 %; f
THD+N = 10 %; f
short time output power per channel
= 1 kHz10.912.1-W
i
= 100 Hz-12.1-W
i
= 1 kHz13.815.3-W
i
= 100 Hz-15.3-W
i
= 1 kHz11.112.3-W
i
= 100 Hz-12.3-W
i
= 1 kHz14.015.5-W
i
= 100 Hz-15.5-W
i
[5]
RL=4Ω; VP=29V
THD+N = 0.5 %19.021.1-W
THD+N = 10 %23.826.5-W
[1] Rs is the series resistance of inductor and capacitor of low-pass LC filter in the application.
[2] THD+N is measured in a bandwidth of 20 Hz to 20 kHz, AES17 brick wall.
[3] Maximum V
[4] B = 20 Hz to 20 kHz, AES17 brick wall.
[5] Output power is measured indirectly; based on R
Two layer application board (55 mm × 45 mm), 35 µm copper, FR4 base material in free air with natural convection.
output power efficiencyPo= 15 W; VP= 12 V and RL=4Ω8890-%
= 30 W; VP= 22 V and RL=8Ω9092-%
P
o
RMS output powercontinuous time output power
[5]
RL=4Ω; VP=12V
THD+N = 0.5 %; f
THD+N = 0.5 %; f
THD+N = 10 %; f
THD+N = 10 %; f
=8Ω; VP=22V
R
L
THD+N = 0.5 %; f
THD+N = 0.5 %; f
THD+N = 10 %; f
THD+N = 10 %; f
short time output power
= 1 kHz11.813.2-W
i
= 100 Hz-13.2-W
i
= 1 kHz15.517.2-W
i
= 100 Hz-17.2-W
i
= 1 kHz23.125.7-W
i
= 100 Hz-25.7-W
i
= 1 kHz28.932.1-W
i
= 100 Hz-32.1-W
i
[5]
RL=4Ω; VP=15V
THD+N = 0.5 %18.520.6-W
THD+N = 10 %23.926.6-W
=8Ω; VP=29V
R
L
THD+N = 0.5 %36.040.0-W
THD+N = 10 %49.555.0-W
[1] Rs is the series resistance of inductor and capacitor of low-pass LC filter in the application.
[2] THD+N is measured in a bandwidth of 20 Hz to 20 kHz, AES17 brick wall.
[3] Maximum V
[4] B = 20 Hz to 20 kHz, AES17 brick wall.
[5] Output power is measured indirectly; based on R
Two layer application board (55 mm × 45 mm), 35 µm copper, FR4 base material in free air with natural convection.
= oscillator frequency (Hz); 320 kHz typical with Rosc = 39 kΩ
osc
The output power Po at THD+N = 10 % can be estimated by:
2
(2)
2
(3)
P
o10%()
1.25P
×=
o 0.5%()
(4)
Figure 8 and Figure 9 show the estimated output power at THD+N = 0.5 % and
THD+N = 10 % as a function of the supply voltage for SE and BTL configurations at
different load impedances. The output power is calculated with: R
Tj=25°C), Rs= 0.05 Ω, R
is internally limited above a level of 4 A (minimum). During
O(max)
normal operation the output current should not exceed this threshold level of 4 A
otherwise the output signal is distorted. The peak output current in SE or BTL
configurations can be estimated using Equation 5 and Equation 6.
A4Ω speaker in the BTL configuration can be used up to a supply voltage of 18 V without
running into current limiting. Current limiting (clipping) will avoid audio holes but it causes
a comparable distortion like voltage clipping.
14.3Speaker configuration and impedance
For a flat frequency response (second-order Butterworth filter) it is necessary to change
the low-pass filter components Llc and Clc according to the speaker configuration and
impedance. Table 14 shows the practical required values.
Table 14.Filter component values
ConfigurationRL (Ω)Llc (µH)Clc (nF)
SE422680
633470
847330
BTL4101500
6151000
822680
14.4Single-ended capacitor
The SE capacitor forms a high-pass filter with the speaker impedance. So the frequency
response will roll-off with 20 dB per decade below f
Table 15 shows an overview of the required SE capacitor values in case of 60 Hz, 40 Hz
or 20 Hz 3 dB cut-off frequency.
Table 15.SE capacitor values
Impedance (Ω)Cse (µF)
468010002200
64706801500
83304701000
14.5Gain reduction
The gain of the TDA8932B is internally fixed at 30 dB for SE (or 36 dB for BTL). The gain
can be reduced by a resistive voltage divider at the input (see Figure 10).
f
=60Hzf
-3dB
=40Hzf
-3dB
-3dB
(7)
=20Hz
470 nF
R1
audio in
Fig 10. Input configuration for reducing gain
R2
R3
470 nF
100
kΩ
001aad762
When applying a resistive divider, the total closed-loop gain G
Equation 8 and Equation 9:
R
G
vtot()Gvcl()
20
log+=
----------------------------------------- -
R
EQ
EQ
R1R2+()+
Where:
G
= total closed-loop voltage gain (dB)
v(tot)
G
= closed-loop voltage gain, fixed at 30 dB for SE (dB)
v(cl)
REQ= equivalent resistance, R3 and Zi (Ω)
R1 = series resistor (Ω)
R2 = series resistor (Ω)
Substituting R1 = R2 = 4.7 kΩ,Zi= 100 kΩ andR3=22kΩ in Equation 8 and Equation 9
results in a gain of G
v(tot)
= 26.3 dB.
14.6Device synchronization
If two or more TDA8932B devices are used in one application it is recommended that all
devices are synchronized running at the same switching frequency to avoid beat tones.
Synchronization canbe realized byconnecting all OSCIO pins together andconfigure one
of the TDA8932B devicesas master,while the other TDA8932B devices are configured as
slaves (see Figure 11).
A device is configured as master when connecting a resistor between pins OSCREF and
V
SSD(HW)
oscillator output for synchronization. The OSCREF pins of the slave devices should be
shorted to V
setting the carrier frequency. Pin OSCIO of the master is then configured as an
SSD(HW)
configuring pin OSCIO as an input.
(9)
masterslave
C
osc
100 nF
TDA8932B
OSCREF V
R
osc
39 kΩ
IC1
SSD(HW)
OSCIO
OSCIOOSCREF
IC2
TDA8932B
V
SSD(HW)
001aaf600
Fig 11. Master slave concept in two chip application
The TDA8932B is available in two different thermally enhanced packages:
TDA8932BT in a SO32 (SOT287-1) package for reflow and wave solder process
TDA8932BTW in an HTSSOP32 (SOT549-1) package for reflow solder process only
The SO32 package has special thermal corner-leads, increasing the power capability
(reducing the overall R
and 32) should be attached to a copper plane. The SO package is very suitable for
applications with limited space for a thermal plane (in a single layer PCB design).
The HTSSOP32 package has an exposed die-pad that reduces significantly the overall
R
th(j-a)
plane forcooling. The HTSSOP package will havea low thermal resistance when used on
a multi-layer PCB with sufficient space for one or two thermal planes.
Increasing the area of the thermal plane, the number of planes or the copper thickness
can reduce further the thermal resistance R
. Therefore it is required to solder the exposed die-pad (at V
of both packages.
th(j-a)
TDA8932B
Class-D audio amplifier
level) to a copper
SSD
Typical thermal resistance R
application board (55 mm × 45 mm), 35 µm copper, FR4 base material is 44 K/W.
Typical thermal resistance R
application board (55 mm × 40 mm), 35 µm copper, FR4 base material is 48 K/W.
Equation 10 shows the relation between the maximum allowable power dissipation P and
the thermal resistance from junction to ambient.
R
th j a–()
T
=
------------------------------------
–
j max()Tamb
P
Where:
R
= thermal resistance from junction to ambient
th(j-a)
T
= maximum junction temperature
j(max)
T
= ambient temperature
amb
P = power dissipation which is determined by the efficiency of the TDA8932B
The power dissipation is shown in Figure 22 (SE) and Figure 34 (BTL).
The thermal foldback will limit the maximum junction temperature to 140 °C.
14.8Pumping effects
of the SO32 package soldered at a small 2-layer
th(j-a)
of the HTSSOP32 package soldered at a small 2-layer
th(j-a)
(10)
When the amplifier is used in a SE configuration, a so-called 'pumping effect' can occur.
During one switching interval, energy is taken from one supply (e.g. V
that energy is delivered back to the other supply line (e.g. V
) and visa versa. When
SSP1
), whilea part of
DDP1
the power supply cannot sink energy, the voltage across the output capacitors of that
power supply will increase.
The voltage increase caused by the pumping effect depends on:
• Speaker impedance
• Supply voltage
• Audio signal frequency
• Value of decoupling capacitors on supply lines
• Source and sink currents of other channels
The pumping effect should not cause a malfunction of either the audio amplifier and/or the
power supply. For instance, this malfunction can be caused by triggering of the
undervoltage or overvoltage protection of the amplifier.
Pumping effects in a SE configuration can be minimized by connecting audio inputs in
anti-phase and change the polarity of one speaker. This is illustrated in Figure 12.
This text provides a very brief insight into a complex technology. A more in-depth account
of soldering ICs can be found in Application Note
soldering description”
17.1Introduction to soldering
Soldering is one of the most common methods through which packages are attached to
Printed Circuit Boards (PCBs), to form electrical circuits. The soldered joint provides both
the mechanical and the electrical connection. There is no single soldering method that is
ideal for all IC packages. Wave soldering is often preferred when through-hole and
Surface Mount Devices (SMDs) are mixed on one printed wiring board; however, it is not
suitable for fine pitch SMDs. Reflow soldering is ideal for the small pitches and high
densities that come with increased miniaturization.
17.2Wave and reflow soldering
Wave soldering is a joining technology in which the joints are made by solder coming from
a standing wave of liquid solder. The wave soldering process is suitable for the following:
TDA8932B
Class-D audio amplifier
AN10365 “Surface mount reflow
.
• Through-hole components
• Leaded or leadless SMDs, which are glued to the surface of the printed circuit board
Not all SMDs can be wave soldered. Packages with solder balls, and some leadless
packages which have solder lands underneath the body, cannot be wave soldered. Also,
leaded SMDs with leads having a pitch smaller than ~0.6 mm cannot be wave soldered,
due to an increased probability of bridging.
The reflow soldering process involves applying solder paste to a board, followed by
component placement and exposure to a temperature profile. Leaded packages,
packages with solder balls, and leadless packages are all reflow solderable.
Key characteristics in both wave and reflow soldering are:
• Board specifications, including the board finish, solder masks and vias
• Package footprints, including solder thieves and orientation
• The moisture sensitivity level of the packages
• Package placement
• Inspection and repair
• Lead-free soldering versus PbSn soldering
17.3Wave soldering
Key characteristics in wave soldering are:
• Process issues, such as application of adhesive and flux, clinching of leads, board
transport, the solder wave parameters, and the time during which components are
exposed to the wave
• Solder bath specifications, including temperature and impurities
• Lead-free versus SnPb soldering; note thata lead-free reflowprocess usually leads to
• Solder paste printing issues including smearing, release, and adjusting the process
• Reflow temperature profile; this profile includes preheat, reflow (in which the board is
Table 16.SnPb eutectic process (from J-STD-020C)
Package thickness (mm)Package reflow temperature (°C)
< 2.5235220
≥ 2.5220220
TDA8932B
Class-D audio amplifier
higher minimum peak temperatures (see Figure 42) than a PbSn process, thus
reducing the process window
window for a mix of large and small components on one board
heated to the peak temperature) and cooling down. It is imperative that the peak
temperature is high enough for the solder to makereliable solder joints (a solder paste
characteristic). In addition, the peak temperature must be low enough that the
packages and/or boards are not damaged. The peak temperature of the package
depends on package thickness and volume and is classified in accordance with
Table 16 and 17
Volume (mm3)
< 350≥ 350
Table 17.Lead-free process (from J-STD-020C)
Package thickness (mm)Package reflow temperature (°C)
Volume (mm3)
< 350350 to 2000> 2000
< 1.6260260260
1.6 to 2.5260250245
> 2.5250245245
Moisture sensitivity precautions, as indicated on the packing, must be respected at all
times.
Studies have shown that small packages reach higher temperatures during reflow
soldering, see Figure 42.
TDA8932B_320070621Product data sheet-TDA8932B_2
Modifications:
TDA8932B_220070329Preliminary data sheet-TDA8932B_1
TDA8932B_120070214Objective data sheet--
Objective [short] data sheetDevelopmentThis document contains data from the objective specification for product development.
Preliminary [short] data sheet QualificationThis document contains data from the preliminary specification.
Product [short] data sheetProductionThis document contains the product specification.
[1] Please consult the most recently issued document before initiating or completing a design.
[2] The term ‘short data sheet’ is explained in section “Definitions”.
[3] The product status of device(s) described in this documentmay have changed since this document was published and may differin case of multiple devices. The latest product status
information is available on the Internet at URL
[1][2]
Product status
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