The TPA032D01 is a monolithic power IC mono
audio amplifier that operates in extremely efficient
Class-D operation, using the high switching speed
of power DMOS transistors to replicate the analog
input signal through high-frequency switching of
the output stage. This allows the TPA032D01 to
be configured as a bridge-tied load (BTL) amplifier
capable of delivering up to 10 W of continuous
average power into a 4-Ω load at 0.5% THD+N
from a 12-V power supply in the high-fidelity audio
frequency range (20 Hz to 20 kHz). A BTL
configuration eliminates the need for external
coupling capacitors on the output. A chip-level
shutdown control is provided to limit total supply
current to 20 µA, making the device ideal for
battery-powered applications.
The output stage is compatible with a range of power supplies from 8 V to 14 V . Protection circuitry is included
to increase device reliability: thermal and under-voltage shutdown, with a status feedback terminal for use when
any error condition is encountered.
The high switching frequency of the TP A032D01 allows the output filter to consist of three small capacitors and
two small inductors per channel. The high switching frequency also allows for good THD+N performance.
The TPA032D01 is offered in the thermally enhanced 48-pin PowerPAD TSSOP surface-mount package
(designator DCA).
Please be aware that an important notice concerning availability, standard warranty, and use in critical applications of
Texas Instruments semiconductor products and disclaimers thereto appears at the end of this data sheet.
PowerPAD is a trademark of Texas Instruments Incorporated.
PRODUCTION DATA information is current as of publication date.
Products conform to specifications per the terms of Texas Instruments
standard warranty. Production processing does not necessarily include
testing of all parameters.
Copyright 2000, Texas Instruments Incorporated
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
1
T
l
R
l
D
7
11
94
2
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
•
PV
DD
INP
INN
COMP
V
DD
COSC
PV
DD
+
_
10 kΩ10 kΩ
1.5 V
V
DD
RAMP
GENERATOR
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
schematic
FAULT0
OUTN
OUTP
PV
DD
VCP PV
VCP PV
+
_
GATE
DRIVE
GATE
DRIVE
DD
DD
PV
DD
THERMAL
DETECT
VCP-UVLO
DETECT
CONTROL and
PV
DD
5-V
REGULATOR
and BIASES
FAULT1
STARTUP
LOGIC
SHUTDOWN
MUTE
V
VCCREG
CC
V2P5
emp
ate
e
ease
ate:
–
–
AGND
PGND
NOTE A: VDD and PVDD are externally connected. AGND and PGND are externally connected.
PV
DD
DOUBLER
CHARGE PUMP
VCP
CP2
CP1
DESCRIPTION
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
Terminal Functions
TERMINAL
NAMENO.
AGND3, 7, 20,
COSC48Connect a capacitor from analog ground to this terminal to set the frequency of the ramp reference signal.
CP124First diode node for charge pump
CP225First inverter switching node for charge pump
FAULT042Logic level fault0 output signal. Lower order bit of the two fault signals with open drain output.
FAULT141Logic level fault1 output signal. Higher order bit of the two fault signals with open drain output.
COMP6Compensation capacitor terminal for Class-D amplifier
INN4Class-D negative input
INP5Class-D positive input
OUTN14, 15Class-D amplifier negative output of H-bridge
OUTP10, 11Class-D amplifier positive output of H-bridge
PV
DD
MUTE
NC18, 19, 23,
PGND12, 13Power ground for H–bridge only
PGND27Power ground for charge pump only
PGND36, 37Power ground for right-channel H-bridge only
PV
DD
43, 44, 45,
46, 47
9, 16Class-D amplifier power supply
2
26, 30, 31,
34, 35, 38,
39
21, 28, 33,40VDD supply for charge-pump and gate drive circuitry
Analog ground for headphone and Class-D analog circuitry
Active-low TTL logic-level mute input signal. When MUTE is held low, the selected amplifier is muted. When
MUTE
is held > high, the device operates normally. When the Class-D amplifier is muted, the low-side output
transistors are turned on, shorting the load to ground.
Not connected
SHUTDOWN
V2P5292.5V internal reference bypass. This terminal requires a capacitor to ground.
V
CC
VCCREG175-V regulator output. This terminal requires a 1-µF capacitor to ground for stability reasons.
VCP22Connect a capacitor from this terminal to power ground to provide storage for the charge pump output voltage.
V
DD
1
325V supply to circuitry. This terminal is typically connected to VCCREG.
8VDD bias supply for analog circuitry. This terminal needs to be well filtered to prevent degrading the device
Active-low TTL logic-level shutdown input signal. When SHUTDOWN is held low, the device goes into shutdown
mode. When SHUTDOWN
performance.
is held high, the device operates normally.
Class-D amplifier faults
Table 1. Class-D Amplifier Fault Table
FAULT 0FAULT 1DESCRIPTION
11No fault. The device is operating normally.
01Charge pump under-voltage lock-out (VCP-UV) fault. All low-side transistors are turned on, shorting the load to
00Thermal fault. All the low-side transistors are turned on, shorting the load to ground. Once the junction temperature
ground. Once the charge pump voltage is restored, normal operation resumes, but FAUL T1 is still active. This is not
a latched fault, however. FAULT1 is cleared by cycling MUTE
drops 20°C, normal operation resumes (not a latched fault). But the FAULTx terminals are still set and are cleared
by cycling MUTE
, SHUTDOWN, or the power supply.
, SHUTDOWN, or the power supply.
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
3
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
AVAILABLE OPTIONS
T
A
–40°C to 125°CTPA032D01DCA
†
The DCA package is available in left-ended tape and reel. T o order
a taped and reeled part, add the suffix R to the part number (e.g.,
TPA032D01DCAR).
PACKAGED DEVICES
†
TSSOP
(DCA)
absolute maximum ratings over operating free-air temperature range, TC = 25°C (unless otherwise
noted)
Lead temperature 1,6 mm (1/16 inch) from case for 10 seconds 260°C. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
Stresses beyond those listed under “absolute maximum ratings” may cause permanent damage to the device. These are stress ratings only, and
functional operation of the device at these or any other conditions beyond those indicated under “recommended operating conditions” is not
implied. Exposure to absolute-maximum-rated conditions for extended periods may affect device reliability.
DISSIPATION RATING TABLE
PACKAGE
DCA5.6 W44.8 mW/°C3.6 W2.9 W
‡
Please see the Texas Instruments document,
Report
(literature number SLMA002), for more information on the PowerPAD package. The thermal data
was measured on a PCB layout based on the information in the section entitled
Recommended Board for PowerPAD
TA ≤ 25°C
POWER RATING
‡
DERATING FACTOR
ABOVE TA = 25°C
PowerPAD Thermally Enhanced Package Application
on page 33 of the before mentioned document.
TA = 70°C
POWER RATING
TA = 85°C
POWER RATING
Texas Instruments
recommended operating conditions
MINNOMMAXUNIT
Supply voltage, VDD, PVDD, LPVDD, RPV
Logic supply voltage, V
High-level input voltage, VIH (MUTE, SHUTDOWN)2VDD + 0.3 VV
Low-level input voltage, VIL (MUTE, SHUTDOWN)–0.30.8V
Audio inputs, LINN, LINP, RINN, RINP, differential input voltage1 V
PWM frequency100250500kHZ
4
CC
DD
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
814V
4.55.5V
RMS
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
electrical characteristics Class-D amplifier, VDD = PVDD = 12 V, RL = 4 Ω to 8 Ω, TA = 25°C,
See Figure 1 (unless otherwise noted)
PARAMETERTEST CONDITIONSMINTYPMAXUNIT
Power supply rejection ratioVDD = PVDD = xPVDD = 11 V to 13 V–40dB
In the typical application an input capacitor, CI, is required to allow the amplifier to bias the input signal to the
proper dc level for optimum operation. In this case, CI and ZI, the TPA032D01’s input resistance forms a
high-pass filter with the corner frequency determined in equation 8.
–3 dB
f
c(highpass)
+
1
2pZIC
I
ZI is nominally 10 kΩ
f
c
The value of CI is important to consider as it directly affects the bass (low frequency) performance of the circuit.
Consider the example where the specification calls for a flat bass response down to 40 Hz. Equation 8 is
reconfigured as equation 9.
+
1
2pZIf
c
C
I
In this example, CI is 0.40 µF so one would likely choose a value in the range of 0.47 µF to 1 µF . A low-leakage
tantalum or ceramic capacitor is the best choice for the input capacitors. When polarized capacitors are used,
the positive side of the capacitor should face the amplifier input, as the dc level there is held at 1.5 V, which is
likely higher than the source dc level. Please note that it is important to confirm the capacitor polarity in the
application.
(8)
(9)
differential input
The TP A032D01 has differential inputs to minimize distortion at the input to the IC. Since these inputs nominally
sit at 1.5 V, dc-blocking capacitors are required on each of the four input terminals. If the signal source is
single-ended, optimal performance is achieved by treating the signal ground as a signal. In other words,
reference the signal ground at the signal source, and run a trace to the dc-blocking capacitor, which should be
located physically close to the TP A032D01. If this is not feasible, it is still necessary to locally ground the unused
input terminal through a dc-blocking capacitor.
power supply decoupling, C
S
The TPA032D01 is a high-performance Class-D CMOS audio amplifier that requires adequate power supply
decoupling to ensure the output total harmonic distortion (THD) is as low as possible. Power supply decoupling
also prevents oscillations for long lead lengths between the amplifier and the speaker. The optimum decoupling
is achieved by using two capacitors of different types that target different types of noise on the power supply
leads. For higher frequency transients, spikes, or digital hash on the line, a good low equivalent-seriesresistance (ESR) ceramic capacitor, typically 0.1 µF placed as close as possible to the device’s various V
leads, works best. For filtering lower-frequency noise signals, a larger aluminum electrolytic capacitor of 10 µF
or greater placed near the audio power amplifier is recommended.
The TP A032D01 has several different power supply terminals. This was done to isolate the noise resulting from
high-current switching from the sensitive analog circuitry inside the IC.
DD
10
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
APPLICATION INFORMATION
mute and shutdown modes
The TP A032D01 employs both a mute and a shutdown mode of operation designed to reduce supply current,
IDD, to the absolute minimum level during periods of non-use for battery-power conservation. The SHUTDOWN
input terminal should be held high during normal operation when the amplifier is in use. Pulling SHUTDOWN
low causes the outputs to mute and the amplifier to enter a low-current state, IDD = 20 µA. Mute mode alone
reduces I
using low-ESR capacitors
Low-ESR capacitors are recommended throughout this applications section. A real (as opposed to ideal)
capacitor can be modeled simply as a resistor in series with an ideal capacitor. The voltage drop across this
resistor minimizes the beneficial effects of the capacitor in the circuit. The lower the equivalent value of this
resistance the more the real capacitor behaves like an ideal capacitor.
output filter components
The output inductors are key elements in the performance of the class-D audio amplifier system. It is important
that these inductors have a high enough current rating and a relatively constant inductance over frequency and
temperature. The current rating should be higher than the expected maximum current to avoid magnetically
saturating the inductor. When saturation occurs, the inductor loses its functionality and looks like a short circuit
to the PWM signal, which increases the harmonic distortion considerably.
to 10 mA.
DD
A shielded inductor may be required if the class-D amplifier is placed in an EMI sensitive system; however, the
switching frequency is low for EMI considerations and should not be an issue in most systems. The dc series
resistance of the inductor should be low to minimize losses due to power dissipation in the inductor, which
reduces the efficiency of the circuit.
Capacitors are important in attenuating the switching frequency and high frequency noise, and in supplying
some of the current to the load. It is best to use capacitors with low equivalent-series-resistance (ESR). A low
ESR means that less power is dissipated in the capacitor as it shunts the high-frequency signals. Placing these
capacitors in parallel also parallels their ESR, effectively reducing the overall ESR value. The voltage rating is
also important, and, as a rule of thumb, should be 2 to 3 times the maximum rms voltage expected to allow for
high peak voltages and transient spikes. These output filter capacitors should be stable over temperature since
large currents flow through them.
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
11
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
APPLICATION INFORMATION
efficiency of class-D vs linear operation
Amplifier efficiency is defined as the ratio of output power delivered to the load to power drawn from the supply .
In the efficiency equation below, PL is power across the load and P
P
Efficiency+h
+
P
L
SUP
A high-efficiency amplifier has a number of advantages over one with lower efficiency . One of these advantages
is a lower power requirement for a given output, which translates into less waste heat that must be removed
from the device, smaller power supply required, and increased battery life.
Audio power amplifier systems have traditionally used linear amplifiers, which are well known for being
inefficient. Class-D amplifiers were developed as a means to increase the efficiency of audio power amplifier
systems.
A linear amplifier is designed to act as a variable resistor network between the power supply and the load. The
transistors operate in their linear region and voltage that is dropped across the transistors (in their role as
variable resistors) is lost as heat, particularly in the output transistors.
is the supply power.
SUP
The output transistors of a class-D amplifier switch from full OFF to full ON (saturated) and then back again,
spending very little time in the linear region in between. As a result, very little power is lost to heat because the
transistors are not operated in their linear region. If the transistors have a low on-resistance, little voltage is
dropped across them, further reducing losses. The ideal class-D amplifier is 100% efficient, which assumes that
both the on-resistance (r
) and the switching times of the output transistors are zero.
DS(on)
the ideal class-D amplifier
T o illustrate how the output transistors of a class-D amplifier operate, a half-bridge application is examined first
(see Figure 4).
V
DD
M1
V
A
M2
I
L
L
I
OUT
+
V
R
C
L
C
OUT
L
–
Figure 4. Half-Bridge Class-D Output Stage
Figures 5 and 6 show the currents and voltages of the half-bridge circuit. When transistor M1 is on and M2 is
off, the inductor current is approximately equal to the supply current. When M2 switches on and M1 switches
off, the supply current drops to zero, but the inductor keeps the inductor current from dropping. The additional
inductor current is flowing through M2 from ground. This means that V
(the voltage at the drain of M2, as shown
A
in Figure 4) transitions between the supply voltage and slightly below ground. The inductor and capacitor form
a low-pass filter, which makes the output current equal to the average of the inductor current. The low pass filter
averages V
, which makes V
A
equal to the supply voltage multiplied by the duty cycle.
OUT
12
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
APPLICATION INFORMATION
the ideal class-D amplifier (continued)
Control logic is used to adjust the output power, and both transistors are never on at the same time. If the output
voltage is rising, M1 is on for a longer period of time than M2.
Inductor Current
Output Current
Supply Current
Current
0
Voltage
0
M1 on
M2 off
M1 on
M2 off
M1 off
M2 on
M1 off
M2 on
M1 on
M2 off
Time
Figure 5. Class-D Currents
M1 on
M2 off
Time
Figure 6. Class-D Voltages
V
DD
V
A
V
OUT
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
13
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
APPLICATION INFORMATION
the ideal class-D amplifier (continued)
Given these plots, the efficiency of the class-D device can be calculated and compared to an ideal linear
amplifier device. In the derivation below, a sine wave of peak voltage (VP) is the output from an ideal class-D
and linear amplifier and the efficiency is calculated.
CLASS-DLINEAR
V
V
L(rms)
AverageǒI
PL+
P
SUP
P
SUP
Efficiency+h
+
VL
+
VDD
V
+
Ǹ
DD
I
DD
P
2
L
I
Ǔ
+
AverageǒI
I
L(rms)
+
P
L(rms)
V
DD
P
L
SUP
V
DD
V
DD
V
L(rms)
L(rms)
Ǔ
V
L(rms)
PL+
AverageǒI
P
SUP
Efficiency+h
Efficiency+h+VDD
Efficiency+h+1Efficiency
+
V
L(rms)
R
+
VDD
V
P
Ǹ
2
2
+
L
Ǔ
+
DD
+h+
2
V
P
2R
L
V
2
p
R
AverageǒI
P
L
+
P
SUP
p
4
V
P
L
V
DD
DD
2
p
P
Ǔ
V
2R
+
2
P
L
V
R
VDDV
R
P
L
P
L
2
p
In the ideal efficiency equations, assume that VP = VDD, which is the maximum sine wave magnitude without
clipping. Then, the highest efficiency that a linear amplifier can have without clipping is 78.5%. A class-D
amplifier, however, can ideally have an efficiency of 100% at all power levels.
The derivation above applies to an H-bridge as well as a half-bridge. An H-bridge requires approximately twice
the supply current but only requires half the supply voltage to achieve the same output power—factors that
cancel in the efficiency calculation. The H-bridge circuit is shown in Figure 7.
V
DD
M1
V
A
M2
I
I
L
OUT
L
C
L
V
+
OUT
R
L
–
L
C
L
M4
M3
V
DD
Figure 7. H-Bridge Class-D Output Stage
14
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
APPLICATION INFORMATION
losses in a real-world class-D amplifier
Losses make class-D amplifiers nonideal, and reduce the efficiency below 100%. These losses are due to the
output transistors having a nonzero r
The loss due to a nonzero r
is called conduction loss, and is the power lost in the output transistors at
DS(on)
nonswitching times, when the transistor is on (saturated). Any r
Figure 8 shows an H-bridge output circuit simplified for conduction loss analysis and can be used to determine
new efficiencies with conduction losses included.
, and rise and fall times that are greater than zero.
DS(on)
above 0 Ω causes conduction loss.
DS(on)
VDD = 12 V
r
DS(on)
r
DS(off)
0.36 Ω
R
4 Ω
5 MΩ
Figure 8. Output Transistor Simplification for Conduction Loss Calculation
The power supplied, P
, is determined to be the power output to the load plus the power lost in the transistors,
SUP
assuming that there are always two transistors on.
P
Efficiency+h
Efficiency+h
Efficiency+h
+
+
+
L
P
SUP
I22r
2r
DS(on)
I2R
DS(on)
R
L
)
L
)
I2R
L
R
L
Efficiency+h+95%ǒat all output levels r
L
0.36 Ω
5 MΩ
r
r
DS(on)
DS(off)
DS(on)
+
0.1 Ω,RL+
4 Ω
Ǔ
Efficiency+h+85%ǒat all output levels r
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
DS(on)
+
0.36 Ω,RL+
4 Ω
Ǔ
15
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
APPLICATION INFORMATION
losses in a real-world class-D amplifier (continued)
Losses due to rise and fall times are called switching losses. A diagram of the output, showing switching losses,
is shown in Figure 9.
1
f
SW
t
SWon
t
+
SWoff
=
t
SW
Figure 9. Output Switching Losses
Rise and fall times are greater than zero for several reasons. One is that the output transistors cannot switch
instantaneously because (assuming a MOSFET) the channel from drain to source requires a specific period
of time to form. Another is that transistor gate-source capacitance and parasitic resistance in traces form RC
time constants that also increase rise and fall times.
Switching losses are constant at all output power levels, which means that switching losses can be ignored at
high power levels in most cases. At low power levels, however, switching losses must be taken into account
when calculating efficiency. Switching losses are dominated by conduction losses at the high output powers,
but should be considered at low powers. The switching losses are automatically taken into account if you
consider the quiescent current with the output filter and load.
class-D effect on power supply
Efficiency calculations are an important factor for proper power supply design in amplifier systems. Table 2
shows Class-D efficiency at a range of output power levels (per channel) with a 1-kHz sine wave input. The
maximum power supply draw from a stereo 10-W per channel audio system with 4-Ω loads and a 12-V supply
is almost 26 W. A similar linear amplifier such as the TPA032D01 has a maximum draw of greater than 50 W
under the same circumstances.
Table 2. Efficiency vs Output Power in 12-V 4-Ω H-Bridge Systems
Output Power (W)Efficiency (%)Peak Voltage (V)Internal Dissipation (W)
0.541.720.35
266.740.5
575.16.320.83
87881.13
1077.98.94
†
High peak voltages cause the THD to increase
†
1.42
16
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
APPLICATION INFORMATION
class-D effect on power supply (continued)
There is a minor power supply savings with a class-D amplifier versus a linear amplifier when amplifying sine
waves. The difference is much larger when the amplifier is used strictly for music. This is because music has
much lower RMS output power levels, given the same peak output power (see Figure 10); and although linear
devices are relatively efficient at high RMS output levels, they are very inefficient at mid-to-low RMS power
levels. The standard method of comparing the peak power to RMS power for a given signal is crest factor, whose
equation is shown below. The lower RMS power for a set peak power results in a higher crest factor
P
PK
P
rms
Power
Crest Factor
+
10 log
P
P
PK
RMS
Time
Figure 10. Audio Signal Showing Peak and RMS Power
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
17
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
APPLICATION INFORMATION
crest factor and thermal considerations
A typical music CD requires 12 dB to 15 dB of dynamic headroom to pass the loudest portions without distortion
as compared with the average power output. From the TPA032D01 data sheet, one can see that when the
TP A032D01 is operating from a 12-V supply into a 4-Ω speaker that 20-W peaks are available. Converting watts
to dB:
P
W
ǒ
PdB+
Subtracting the crest factor restriction to obtain the average listening level without distortion yields:
6.0 dB*18 dB
6.0 dB*15 dB
6.0 dB*12 dB
6.0 dB*9dB
6.0 dB*6dB
6.0 dB*3dB+3dB(3 dB crest factor
Converting dB back into watts:
PW+
10Log
PdBń10
10
+
315 mW (18 dB crest factor)
+
630 mW (15 dB crest factor)
+
1.25 W (12 dB crest factor)
+
2.5 W (9 dB crest factor)
+
5 W (6 dB crest factor)
+
10 W (3 dB crest factor)
Ǔ
+
P
ref
+*+*
+*+*+*
10Log
12 dB(15 dB crest factor
9dB(15 dB crest factor
6dB(12 dB crest factor
3dB(9 dB crest factor
0dB(6 dB crest factor
P
ref
20
ǒ
Ǔ
+
6dB
1
)
)
)
)
)
)
(17)
(18)
This is valuable information to consider when attempting to estimate the heat dissipation requirements for the
amplifier system. Comparing the absolute worst case, which is 10 W of continuous power output with a 3 dB
crest factor, against 12 dB and 15 dB applications drastically af fects maximum ambient temperature ratings for
the system. Using the power dissipation curves for a 12-V, 4-Ω system, the internal dissipation in the
TPA032D01 and maximum ambient temperatures are shown in Table 3.
18
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
AVERAGE OUTPUT POWER
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
APPLICATION INFORMATION
crest factor and thermal considerations (continued)
Table 3. TPA032D01 Power Rating, 12-V, 4-Ω, Stereo
TPA032D01
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
PEAK OUTPUT POWER
(W)
2010 W (3 dB)2.8487°C
205 W (6 dB)1.66113°C
202.5 W (9 dB)1.12125°C
201.25 W (12 dB)0.87125°C
20630 mW (15 dB)0.7125°C
20315 mW (18 dB)0.6125°C
POWER DISSIPATIONMAXIMUM AMBIENT
(W/Channel)TEMPERATURE
The maximum ambient temperature depends on the heatsinking ability of the PCB system. Using the 0 CFM
data from the dissipation rating table, the derating factor for the DCA package with 6.9 in2 of copper area on
a multilayer PCB is 44.8 mW/°C. Converting this to ΘJA:
+
Derating
+
0.0448
+
22.3°CńW
1
(19)
1
Θ
JA
To calculate maximum ambient temperatures, first consider that the numbers from the dissipation graphs are
per channel so the dissipated heat needs to be doubled for two channel operation. Given ΘJA, the maximum
allowable junction temperature, and the total internal dissipation, the maximum ambient temperature can be
calculated with the following equation. The maximum recommended junction temperature for the TP A032D01
is 150 °C. The internal dissipation figures are taken from the Efficiency vs Output Power graphs.
TAMax
+
TJMax
+
150*22.3(0.35)+
+
150*22.3(1.42)+
*
Θ
JAPD
125°C(15 dB crest factor
118°C(3dB crest factor
)
(20)
)
(Maximum recommended case temperature is 125°C)
NOTE:
Internal dissipation of 0.7 W is estimated for a 10-W system with a 15 dB crest factor per channel.
The TPA032D01 is designed with thermal protection that turns the device off when the junction temperature
surpasses 150°C to prevent damage to the IC. Table 3 was calculated for maximum listening volume without
distortion. When the output level is reduced the numbers in the table change significantly. Also, using 8-Ω
speakers dramatically increases the thermal performance by increasing amplifier efficiency.
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
19
TPA032D01
10-W MONO CLASS-D AUDIO POWER AMPLIFIER
SLOS282A – DECEMBER 1999 – REVISED MARCH 2000
THERMAL INFORMATION
The thermally enhanced DCA package is based on the 56-pin TSSOP, but includes a thermal pad (see Figure 11)
to provide an effective thermal contact between the IC and the PWB.
Traditionally, surface-mount and power have been mutually exclusive terms. A variety of scaled-down TO-220-type
packages have leads formed as gull wings to make them applicable for surface-mount applications. These packages,
however, have only two shortcomings: they do not address the very low profile requirements (<2 mm) of many of
today’s advanced systems, and they do not offer a terminal-count high enough to accommodate increasing
integration. On the other hand, traditional low-power surface-mount packages require power-dissipation derating that
severely limits the usable range of many high-performance analog circuits.
The PowerP AD package (thermally enhanced TSSOP) combines fine-pitch surface-mount technology with thermal
performance comparable to much larger power packages.
The PowerPAD package is designed to optimize the heat transfer to the PWB. Because of the very small size and
limited mass of a TSSOP package, thermal enhancement is achieved by improving the thermal conduction paths that
remove heat from the component. The thermal pad is formed using a patented lead-frame design and manufacturing
technique to provide a direct connection to the heat-generating IC. When this pad is soldered or otherwise thermally
coupled to an external heat dissipator, high power dissipation in the ultra-thin, fine-pitch, surface-mount package can
be reliably achieved.
DIE
Side View (a)
DIE
End View (b)
Thermal
Pad
Bottom View (c)
20
Figure 11. Views of Thermally Enhanced DCA Package
NOTES: A. All linear dimensions are in millimeters.
B. This drawing is subject to change without notice.
C. Body dimensions do not include mold flash or protrusion not to exceed 0,15.
D. The package thermal performance may be enhanced by bonding the thermal pad to an external thermal plane.
This pad is electrically and thermally connected to the backside of the die and possibly selected leads.
E. Falls within JEDEC MO-153
PowerPAD is a trademark of Texas Instruments.
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
PINS **
48
12,60
12,40
56
14,10
64
17,10
16,9013,90
4073259/A 01/98
21
IMPORTANT NOTICE
T exas Instruments and its subsidiaries (TI) reserve the right to make changes to their products or to discontinue
any product or service without notice, and advise customers to obtain the latest version of relevant information
to verify, before placing orders, that information being relied on is current and complete. All products are sold
subject to the terms and conditions of sale supplied at the time of order acknowledgment, including those
pertaining to warranty, patent infringement, and limitation of liability.
TI warrants performance of its semiconductor products to the specifications applicable at the time of sale in
accordance with TI’s standard warranty. Testing and other quality control techniques are utilized to the extent
TI deems necessary to support this warranty . Specific testing of all parameters of each device is not necessarily
performed, except those mandated by government requirements.
Customers are responsible for their applications using TI components.
In order to minimize risks associated with the customer’s applications, adequate design and operating
safeguards must be provided by the customer to minimize inherent or procedural hazards.
TI assumes no liability for applications assistance or customer product design. TI does not warrant or represent
that any license, either express or implied, is granted under any patent right, copyright, mask work right, or other
intellectual property right of TI covering or relating to any combination, machine, or process in which such
semiconductor products or services might be or are used. TI’s publication of information regarding any third
party’s products or services does not constitute TI’s approval, warranty or endorsement thereof.
Copyright 2000, Texas Instruments Incorporated
Loading...
+ hidden pages
You need points to download manuals.
1 point = 1 manual.
You can buy points or you can get point for every manual you upload.