TI TPA005D02DCA

TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
DCA PACKAGE
(TOP VIEW)
NOT RECOMMENDED FOR NEW DESIGNS
D
D
D
D
D
D
D
D
D
D
Choose TPA2000D2 For Upgrade
Extremely Efficient Class-D Stereo
Operation
Drives L and R Channels
2-W BTL Output into 4 Ω
5-W Peak Music Power
Fully Specified for 5-V Operation
Low Quiescent Current
Shutdown Control
Thermally-Enhanced PowerPAD SurfaceMount Packaging
Thermal and Under-Voltage Protection
description
The TPA005D02 is a monolithic power IC stereo
audio amplifier. It operates in extremely efficient
Class-D operation, using the high switching speed
of power DMOS transistors. These transistors
replicate the analog signal through high-frequency switching of the output stage. This allows the
TPA005D02 to be configured as a bridge-tied load
(BTL) amplifier.
When configured as a BTL amplifier, the
TPA005D02 is capable of delivering up to 2 W of
continuous average power into a 4-Ω load at 0.5%
THD+N from a 5-V power supply in the high fidelity
range (20 Hz to 20 kHz).
SHUTDOWN
MUTE
AGND
LINN
LINP
LCOMP
AGND
VDD
LPVDD
LOUTP
LOUTP
PGND
PGND
LOUTN
LOUTN
LPVDD
NC
NC
NC
AGND
PVDD
VCP
CP3
CP2
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
48
47
46
45
44
43
42
41
40
39
38
37
36
35
34
33
32
31
30
29
28
27
26
25
COSC
AGND
AGND
RINN
RINP
RCOMP
FAULT0
FAULT1
RPVDD
ROUTP
ROUTP
PGND
PGND
ROUTN
ROUTN
RPVDD
PVDD
NC
NC
V2P5
LSBIAS
PGND
CP4
CP1
NC – No internal connection
A BTL configuration eliminates the need for external coupling capacitors on the output. A chip-level shutdown
control limits total supply current to 400 µA. This makes the device ideal for battery-powered applications.
Protection circuitry increases device reliability: thermal and under-voltage shutdown, with two status feedback
terminals for use when any error condition is encountered.
The high switching frequency of the TPA005D02 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 TPA005D02 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.
Copyright  2000, 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.
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1
LPVDD
POST OFFICE BOX 655303 • DALLAS, TEXAS 75265
PVDD
GATE
DRIVE
VDD
BIAS
GENERATOR
HPVCC
V2P5
COSC
VCP LSBIAS
RAMP
GENERATOR
_
RCOMP
VCP-UVLO
DETECT
GATE
DRIVE
+
PVDD
+
_
RINP
RINN
10 kΩ
10 kΩ
1.5 V
RPVDD
AGND
RPVDD
RPVDD
RPVDD
TRIPLER
CHARGE PUMP
GATE
DRIVE
CP1
CP2
NOTE A: LPVDD, RPVDD, VDD, and PVDD are externally connected. AGND and PGND are externally connected.
CP3
CP4
VCP
PVDD
ROUTN
ROUTP
PGND
VCP LSBIAS
Template Release Date: 7–11–94
+
_
LCOMP
MUTE
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
VCP LSBIAS
SHUTDOWN
CONTROL and
STARTUP
LOGIC
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
LINN
FAULT1
THERMAL
DETECT
+
_
LINP
VDD
LSBIAS
GATE
DRIVE
10 kΩ
FAULT0
LPVDD
1.5 V
10 kΩ
LSBIAS
VCP LSBIAS
LPVDD
LOUTN
LOUTP
2
LPVDD
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
Terminal Functions
TERMINAL
NAME
DESCRIPTION
NO.
AGND
3, 7, 20,
46, 47
COSC
48
Capacitor I/O for ramp generator. Adjust the capacitor size to change the switching frequency.
CP1
25
First diode node for charge pump
CP2
24
First inverter switching node for charge pump
CP3
23
Second diode node for charge pump
CP4
26
Second inverter switching node for charge pump
FAULT0
42
Logic level fault0 output signal. Lower order bit of the two fault signals with open drain output.
FAULT1
41
Logic level fault1 output signal. Higher order bit of the two fault signals with open drain output.
LCOMP
6
Compensation capacitor terminal for left-channel Class-D amplifier
LINN
4
Class-D left-channel negative input
5
Class-D left-channel positive input
LINP
Analog ground for analog sections
LOUTN
14, 15
Class-D amplifier left-channel negative output of H-bridge
LOUTP
10, 11
Class-D amplifier left-channel positive output of H-bridge
LPVDD
LSBIAS
9, 16
Class-D amplifier left-channel power supply
28
Level-shifter power supply, to be tied to VCP
2
Active-low 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.
MUTE
NC
PGND
17, 18, 19,
30, 31
12, 13
No internal connection
Power ground for left-channel H–bridge only
PGND
27
PGND
36, 37
Power ground for right-channel H-bridge only
PVDD
RCOMP
21, 32
43
VDD supply for charge-pump and internal logic circuitry
Compensation capacitor terminal for right-channel Class-D amplifier
45
Class-D right-channel negative input
44
Class-D right-channel positive input
RINN
RINP
Power ground for charge pump only
RPVDD
ROUTN
33, 40
Class-D amplifier right-channel power supply
34, 35
Class-D amplifier right-channel negative output of H-bridge
ROUTP
38, 39
Class-D amplifier right-channel positive output of H-bridge
SHUTDOWN
1
Active-low logic-level shutdown input signal. When SHUTDOWN is held low, the device goes into shutdown
mode. When SHUTDOWN is held at logic high, the device operates normally.
V2P5
29
2.5-V internal reference bypass
VCP
22
Storage capacitor terminal for charge pump
VDD
8
VDD bias supply for analog circuitry. This terminal needs to be well filtered to prevent degrading the device
performance.
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3
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
Class-D amplifier faults
Table 1. Amplifier Fault Table
FAULT 0†
FAULT 1†
1
1
No fault—The device is operating normally.
1
0
Charge pump under-voltage lock-out (VCP-UV) fault—All low-side transistors are turned on, shorting the load to
ground. Once the charge pump voltage is restored, normal operation resumes, but FAULT1 is still active. FAULT1 is
cleared by cycling MUTE, SHUTDOWN, or the power supply.
0
0
Thermal fault—All the low-side transistors are turned on, shorting the load to ground. Once the junction temperature
drops 20°C, normal operation resumes. But the FAULTx terminals are still set and are cleared by cycling MUTE,
SHUTDOWN, or the power supply.
DESCRIPTION
† These logic levels assume a pull up to PVDD from the open-drain outputs.
AVAILABLE OPTIONS
TA
PACKAGED DEVICES
TSSOP†
(DCA)
– 40°C to 125°C
TPA005D02DCA
† The DCA package is available in left-ended tape and reel. To order
a taped and reeled part, add the suffix R to the part number (e.g.,
TPA005D02DCAR).
absolute maximum ratings over operating free-air temperature range, TC = 25°C (unless otherwise
noted)‡
Supply voltage, VDD (PVDD, LPVDD, RPVDD, VDD) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5.5 V
Bias voltage (LSBIAS) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 12 V to 20 V
Input voltage, VI (SHUTDOWN, MUTE, MODE) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 0.3 V to 5.8 V
Output current, IO (FAULT0, FAULT1), open drain terminated . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1 mA
Charge pump voltage, VCP . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . PVDD + 20 V
Continuous H-bridge output current . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2 A
Pulsed H-Bridge output current, each output, Imax (see Note 1) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5 A
Continuous total power dissipation, TC = 25°C . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4.5 W§
Operating virtual junction temperature range, TJ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 40°C to 150°C
Operating case temperature range, TC . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 40°C to 125°C
Storage temperature range, Tstg . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . – 65°C to 150°C
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.
§ Thermal shutdown activates when TJ = 125°C.
NOTE 1: Pulse duration = 10 ms, duty cycle
2%
v
DISSIPATION RATING TABLE
PACKAGE
TA ≤ 25°C¶
POWER RATING
DERATING FACTOR
ABOVE TA = 25°C
TA = 70°C
POWER RATING
TA = 85°C
POWER RATING
TA = 125°C
POWER RATING
DCA
5.6 W
44.8 mW/°C
3.6 W
2.9 W
1.1 W
¶ Please see the Texas Instruments document, PowerPAD Thermally Enhanced Package Application 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 Texas Instruments Recommended Board for PowerPAD on page 33 of the before mentioned
document.
4
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TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
recommended operating conditions
MIN
Supply voltage, PVDD, LPVDD, RPVDD, VDD
NOM
4.5
High-level input voltage, VIH
MAX
5.5
4.25
V
V
Low-level input voltage, VIL
0.75
Audio inputs, LINN, LINP, RINN, RINP, HPLIN, HPRIN, differential input voltage
1
PWM frequency
UNIT
100
500
V
VRMS
kHZ
electrical characteristics, VDD = PVDD = LPVDD = RPVDD = 5 V, RL = 4 Ω, TC = 25°C, See Figure 1
(resistive load) (unless otherwise noted)
PARAMETER
TEST CONDITIONS
PSRR
Power supply rejection ratio
IDD
IDD(MUTE)
Supply current
VDD = PVDD = LPVDD = RPVDD = 4.9 V to 5.1 V
No load or output filter
Supply current, mute mode
MUTE = 0 V
IDD(SD)
IIH
Supply current, shutdown mode
SHUTDOWN = 0 V
High-level input current
IIL
Low-level input current
VIH = 5.3 V
VIL = – 0.3 V
rDS(on)
Total static drain-to-source
on-state resistance
(low-side plus high-side FETs)
rDS(on)
Matching
MIN
TYP
MAX
40
25
ID = 0.5 A
dB
40
mA
10
15
mA
400
2000
µA
620
95%
UNIT
10
µA
–10
µA
750
mΩ
99.5%
operating characteristics, VDD = PVDD = LPVDD = RPVDD = 5 V, RL = 4 Ω, TC = 25°C, See Figure 1
(unless otherwise noted)
PARAMETER
PO
THD+N
TEST CONDITIONS
Total harmonic distortion plus noise
MAX
UNIT
W
0.2%
80%
Gain
24
Left/right channel gain matching
dB
95%
Noise floor
Dynamic range
Crosstalk
f = 1 kHz
Frequency response bandwidth, post output filter, – 3 dB
BOM
TYP
2
PO = 1 W, f = 1 kHz
RL = 8 Ω
Efficiency
AV
MIN
RMS output power, THD = 0.5%, per channel
60
dB
70
dB
55
dB
20
Maximum output power bandwidth
20,000
Hz
20
kHz
thermal resistance
PARAMETER
RθJP
TEST CONDITIONS
Thermal resistance, junction-to-pad
MIN
TYP
MAX
UNIT
10
°C/W
RθJA Thermal resistance, junction-to-pad†
22.3
°C/W
† Please see the Texas Instruments document, PowerPAD Thermally Enhanced Package Application 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
Texas Instruments Recommended Board for PowerPAD on page 33 of the before mentioned document.
POST OFFICE BOX 655303
• DALLAS, TEXAS 75265
5
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
PARAMETER MEASUREMENT INFORMATION
FAULT0
VCP
PVDD
PVDD
28
1
2
FAULT1
LSBIAS
SHUTDOWN
LOUTN
MUTE
42
41
14,15
15 µH
0.22 µF
5V
9,16
LOUTP
1 µF
5
Balanced
Differential
Input Signal
4
1 µF
43
470 pF
LINN
1 µF
4Ω
10,11
15 µH
29
LCOMP
1 µF
RCOMP
470 pF
VDD
48
4Ω
LINP
V2P5
6
1 µF
0.22 µF
LPVDD
8
COSC
470 pF
CP1
1 µF
44
Balanced
Differential
Input Signal
45
47 nF
CP2
RINP
CP3
RINN
12,13,27,36,37
5V
21, 32
24
23
47 nF
1 µF
33,40
5V
2, 3, 7,20,46,47
25
CP4
RPVDD
AGND (see Note A)
VCP
26
22
2.2 µF
PGND (see Note A)
PVDD
ROUTN
34,35
15 µH
0.22 µF
0.22 µF
ROUTP
Figure 1. 5-V, 4-Ω Test Circuit
6
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38,39
15 µH
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
TYPICAL CHARACTERISTICS
Table of Graphs
FIGURE
IDD
vs Switching frequency
Supply current
THD+N
2
vs Free-air temperature
Total harmonic distortion plus noise
3
vs Frequency
4, 5
vs Output power
6, 7
Voltage amplification and phase shift
vs Frequency
8
Crosstalk
vs Frequency
9
Efficiency
vs Output power
10
SUPPLY CURRENT
vs
FREE–AIR TEMPERATURE
SUPPLY CURRENT
vs
SWITCHING FREQUENCY
50
100
Open Load
80
IDD – Supply Current – mA
IDD – Supply Current – mA
Open Load
60
With Output Filter
40
40
With Output Filter
30
20
Without Output Filter
10
20
Without Output Filter
0
0
100
200
300
400
500
0
–40
0
40
80
120
125
TA – Free–Air Temperature – °C
f – Switching Frequency – Hz
Figure 3
Figure 2
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• DALLAS, TEXAS 75265
7
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
TYPICAL CHARACTERISTICS
1
RL = 4 Ω
0.5
PO = 2W
0.2
0.1
PO = 100 mW
PO = 1W
0.05
0.02
0.01
20
100 200
50
500 1k
2k
TOTAL HARMONIC DISTORTION PLUS NOISE
vs
FREQUENCY
THD+N – Total Harmonic Distortion Plus Noise – %
THD+N – Total Harmonic Distortion Plus Noise – %
TOTAL HARMONIC DISTORTION PLUS NOISE
vs
FREQUENCY
5k 10k 20k
1
RL = 8 Ω
0.5
PO = 100 mW
0.2
0.1
PO = 1W
0.05
0.02
0.01
20
50
100 200
f – Frequency – Hz
THD+N – Total Harmonic Distortion Plus Noise – %
THD+N – Total Harmonic Distortion Plus Noise – %
RL = 4 Ω
2
1
0.5
f = 1 kHz
0.2
0.1
f = 20 kHz
f = 20 Hz
0.05
f = 20 kHz
f = 20 Hz
0.02
0.01
0.01 0.02
0.05 0.1 0.2
5k 10k 20k
0.5
1
2
5
10
10
5
TOTAL HARMONIC DISTORTION PLUS NOISE
vs
OUTPUT POWER
RL = 8 Ω
2
1
0.5
0.2
f = 1 kHz
f = 20 Hz
0.1
0.05
f = 20 kHz
0.02
0.01
10m 20m 50m 100m 200m 500m 1
PO – Output Power – W
Figure 7
POST OFFICE BOX 655303
2
PO – Output Power – W
Figure 6
8
2k
Figure 5
TOTAL HARMONIC DISTORTION PLUS NOISE
vs
OUTPUT POWER
5
500 1k
f – Frequency – Hz
Figure 4
10
PO = 500 mW
• DALLAS, TEXAS 75265
5
10
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
TYPICAL CHARACTERISTICS
GAIN AND PHASE
vs
FREQUENCY
28
Voltage Amplification
26
24
22
20
Gain – dB
18
Phase Shift
16
14
12
10
8
6
4
2
0
10 20
50 100 200 500 1k 2k
45°
40°
35°
30°
25°
20°
15°
10°
5°
0°
– 5°
– 10°
– 15°
– 20°
– 25°
– 30°
– 35°
– 40°
– 45°
5k 10k 20k 50k 100k
Po = 2W
RL = 4Ω
Phase
30
f – Frequency – Hz
Figure 8
CROSSTALK
vs
FREQUENCY
EFFICIENCY
vs
OUTPUT POWER
0
90
PO = 2W
RL = 4Ω
–10
–20
RL = 8Ω
–30
80
–50
–60
–70
Efficiency – %
Crosstalk – dB
–40
Left-to-Right
–80
–90
–100
–110
RL = 4Ω
70
60
Right-to-Left
–120
–130
50
–140
–150
20
50 100 200
500 1k
2k
5k 10k 20k
40
0
0.4
0.8
1.2
1.6
2.0
PO – Output Power – W
f – Frequency – Hz
Figure 10
Figure 9
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• DALLAS, TEXAS 75265
9
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – 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 PowerPAD 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)
Thermal
Pad
DIE
End View (b)
Bottom View (c)
Figure 11. Views of Thermally Enhanced DCA Package
selection of components
Figure 12 is a schematic diagram of a typical notebook computer application circuit.
10
POST OFFICE BOX 655303
• DALLAS, TEXAS 75265
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
APPLICATION INFORMATION
FAULT0
VCP
PVDD
PVDD
28
1
2
FAULT1
LSBIAS
SHUTDOWN
LOUTN
MUTE
42
41
14,15
15 µH
0.22 µF
5V
9,16
LOUTP
1 µF
5
Balanced
Differential
Input Signal
4
1 µF
43
470 pF
LINN
1 µF
4Ω
10,11
15 µH
29
LCOMP
1 µF
RCOMP
470 pF
VDD
48
4Ω
LINP
V2P5
6
1 µF
0.22 µF
LPVDD
8
COSC
470 pF
CP1
1 µF
44
Balanced
Differential
Input Signal
45
47 nF
CP2
RINP
CP3
RINN
12,13,27,36,37
5V
21, 32
24
23
47 nF
1 µF
33,40
5V
2, 3, 7,20,46,47
25
CP4
RPVDD
AGND (see Note A)
VCP
26
22
2.2 µF
PGND (see Note A)
PVDD
ROUTN
34,35
15 µH
0.22 µF
0.22 µF
ROUTP
38,39
15 µH
NOTE A: A 0.1 µF ceramic capacitor should be placed as close as possible to the IC. For filtering lower-frequency noise signals, a larger aluminum
electrolytic capacitor of 10 µF or greater should be placed near the audio power amplifier.
Figure 12. TPA005D02 Typical Configuration Application Circuit
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• DALLAS, TEXAS 75265
11
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
APPLICATION INFORMATION
input capacitor, CI
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 RIN, the TPA005D002’s input resistance forms a
high-pass filter with the corner frequency determined in equation 8.
–3 dB
f
c(highpass)
+ 2 p R1
(8)
C
IN I
RIN is nominally 10 kΩ
fc
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.
CI
+ 2 p R1
(9)
f
IN c
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.
differential input
The TPA005D02 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 TPA005D02. If this is not feasible, it is still necessary to locally ground the unused
input terminal through a dc-blocking capacitor.
power supply decoupling, CS
The TPA005D02 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 VDD
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 TPA005D02 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.
12
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TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
APPLICATION INFORMATION
mute and shutdown modes
The TPA005D02 employs both a mute and a shutdown mode of operation designed to reduce supply current,
IDD, to the absolute minimum level during periods of nonuse 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 = 400 µA. Mute mode alone
reduces IDD to 10 mA.
Table 2. Shutdown and Mute Mode Functions
INPUTS†
OUTPUT
SE/BTL
HP/LINE
MUTE IN
Low
Low
X
X
X
X
Low
High
High
High
AMPLIFIER STATE
SHUTDOWN
MUTE OUT
INPUT
Low
Low
Low
L/R Line
BTL
—
High
—
X
Mute
High
—
High
X
Mute
Low
Low
Low
L/R HP
BTL
Low
Low
Low
Low
L/R Line
SE
High
Low
Low
Low
L/R HP
SE
OUTPUT
† Inputs should never be left unconnected.
X = do not care
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.
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
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13
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – 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 PSUP is the supply power.
Efficiency
+ h + PP 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.
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 (RDS(ON)) and the switching times of the output transistors are zero.
the ideal class D amplifier
To illustrate how the output transistors of a class D amplifier operate, a half-bridge application is examined first
(Figure 13).
VDD
M1
VA
IL
IOUT
+
L
M2
RL
CL
C
VOUT
–
Figure 13. Half-Bridge Class D Output Stage
Figures 14 and 15 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 VA (the voltage at the drain of M2, as shown
in Figure 13) 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 VA, which makes VOUT equal to the supply voltage multiplied by the duty cycle.
14
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TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – 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
Current
Supply Current
0
M1 on M1 off M1 on
M2 off M2 on M2 off
Time
Figure 14. Class D Currents
VDD
Voltage
VA
VOUT
0
M1 on M1 off M1 on
M2 off M2 on M2 off
Time
Figure 15. Class D Voltages
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15
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – 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 D
V L(rms)
+ Ǹ2
V L(rms)
ǒ Ǔ+
Average I DD
PL
LINEAR
VP
+ VL
+ VDD
P SUP
+
V DD
V L(rms)
PL
V DD
IL
P SUP
Efficiency
I L(rms)
V L(rms)2
RL
+2 R
ǒ Ǔ+p
ǒ Ǔ
P SUP
V L(rms)
Efficiency
V DD
L
VP
2
+ VDD
RL
ǒ Ǔ+
Average I DD
V DD V P
RL
2
p
+ h + PP L
SUP
+ h + PP L
Efficiency
SUP
Efficiency
V P2
Average I DD
Average I DD
I L(rms)
+
+ Ǹ2
VP
V P2
2R L
+ h + VDD
V
2
p
+ h +1
Efficiency
+ h + p4
V
V
P
RL
P
DD
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 16.
VDD
M1
VA
VDD
IL
IOUT
M4
+ VOUT –
L
M2
L
RL
CL
CL
Figure 16. H-Bridge Class D Output Stage
16
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M3
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – 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 RDS(on), and rise and fall times that are greater than zero.
The loss due to a nonzero RDS(on) is called conduction loss, and is the power lost in the output transistors at
nonswitching times, when the transistor is ON (saturated). Any RDS(on) above 0 Ω causes conduction loss.
Figure 17 shows an H-bridge output circuit simplified for conduction loss analysis and can be used to determine
new efficiencies with conduction losses included.
VDD = 5 V
RDS(on)
0.31 Ω
5 MΩ
RDS(off)
0.31 Ω
RDS(on)
RL
4Ω
RDS(off)
5 MΩ
Figure 17. Output Transistor Simplification for Conduction Loss Calculation
The power supplied, PSUP, is determined to be the power output to the load plus the power lost in the transistors,
assuming that there are always two transistors on.
Efficiency
+ h + PP L
SUP
Efficiency
Efficiency
+ h + I2 2R
+ h + 2R
DS(on)
RL
ǒ
ǒ
DS(on)
+ h + 95%
Efficiency + h + 87%
Efficiency
I 2R L
) I2RL
) RL
Ǔ
+ 0.1, RL + 4
at all output levels R DS(on) + 0.31, R L + 4
at all output levels R DS(on)
POST OFFICE BOX 655303
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Ǔ
17
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – 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 plot of the output, showing switching losses, is
shown in Figure 18.
1
f
tSWon
SW
tSWoff
+
=
tSW
Figure 18. 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 1-W per channel audio system with 8-Ω loads and a 5-V supply is
almost 2.7 W. A similar linear amplifier such as the TPA005D02 has a maximum draw of 3.25 W under the same
circumstances.
Table 3. Efficiency vs Output Power in 5-V 8-Ω H-Bridge Systems
Output Power (W)
Efficiency (%)
Peak Voltage (V)
Internal Dissipation (W)
0.25
63.4
2
0.145
0.5
73
2.83
0.183
0.75
77.1
3.46
0.222
1
79.3
80.6
4
4.47†
0.314
1.25
† High peak voltages cause the THD to increase
18
POST OFFICE BOX 655303
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0.3
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – 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 (Figure 19); 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
Crest Factor
+ 10 log PP
PK
rms
Power
PPK
PRMS
Time
Figure 19. Audio Signal Showing Peak and RMS Power
Figure 20 is a comparison of a 5-V class D amplifier to a similar linear amplifier playing music that has a 13.76-dB
crest factor. From the plot, the power supply draw from a stereo amplifier that is playing music with a 13.76 dB
crest factor is 1.02 W, while a class D amplifier draws 420 mW under the same conditions. This means that just
under 2.5 times the power supply is required for a linear amplifier over a class D amplifier.
POWER SUPPLIED
vs
PEAK OUTPUT VOLTAGE AND PEAK OUTPUT POWER
600
Power Supplied (mW)
500
400
TPA0202
300
TPA005D02
200
100
0
1
0.25
1.5
0.56
2
1
2.5
1.56
3
2.25
3.5
3.06
4
4
4.5
5.06
Peak Output Voltage (V)
Peak Output Power (W)
Figure 20. Audio Signal Showing Peak and RMS Power (with Music Applied)
POST OFFICE BOX 655303
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19
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
APPLICATION INFORMATION
class D effect on battery life
Battery operations for class D amplifiers versus linear amplifiers have similar power supply savings results. The
essential contributing factor to longer battery life is lower RMS supply current. Figure 21 compares the
TPA005D02 supply current to the supply current of the TPA0202, a 2-W linear device, while playing music at
different peak voltage levels.
SUPPLY CURRENTS
vs
PEAK OUTPUT VOLTAGE AND PEAK OUTPUT POWER
400
Supply Current (mA rms)
350
300
250
TPA0202
200
150
100
TPA005D02
50
0
1
0.25
1.5
0.56
2
1
2.5
1.56
3
2.25
3.5
3.06
4
4
Peak Output Voltage (V)
Peak Output Power (W)
Figure 21. Supply Current vs Peak Output Voltage of TPA005D02 vs TPA0202 With Music Input
This plot shows that a linear amplifier has approximately three times more current draw at normal listening levels
than a class D amplifier. Thus, a class D amplifier has approximately three times longer battery life at normal
listening levels. If there is other circuitry in the system drawing supply current, that must also be taken into
account when estimating battery life savings.
20
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TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – 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 TPA005D02 data sheet, one can see that when the
TPA005D02 is operating from a 5-V supply into a 4-Ω speaker that 4 W peaks are available. Converting Watts
to dB:
P dB
+ 10 Log
ǒǓ
PW
P ref
+ 10Log
ǒ Ǔ+
4
1
6 dB
(17)
Subtracting the crest factor restriction to obtain the average listening level without distortion yields:
* 18 dB + * 12 dB (15 dB crest factor)
6.0 dB * 15 dB + * 9 dB (15 dB crest factor)
6.0 dB * 12 dB + * 6 dB (12 dB crest factor)
6.0 dB * 9 dB + * 3 dB (9 dB crest factor)
6.0 dB * 6 dB + * 0 dB (6 dB crest factor)
6.0 dB * 3 dB + 3 dB (3 dB crest factor)
6.0 dB
Converting dB back into watts:
PW
+ 10PdBń10 Pref
+ 63 mW (18 dB crest factor)
+ 125 mW (15 dB crest factor)
+ 250 mW (12 dB crest factor)
+ 500 mW (9 dB crest factor)
+ 1000 mW (6 dB crest factor)
+ 2000 mW (3 dB crest factor)
(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 2 W of continuous power output with a 3 dB crest
factor, against 12 dB and 15 dB applications drastically affects maximum ambient temperature ratings for the
system. Using the power dissipation curves for a 5-V, 4-Ω system, the internal dissipation in the TPA005D02
and maximum ambient temperatures is shown in Table 4.
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21
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
APPLICATION INFORMATION
crest factor and thermal considerations (continued)
Table 4. TPA005D02 Power Rating, 5-V, 4-Ω, Stereo
PEAK OUTPUT POWER
(W)
AVERAGE OUTPUT POWER
POWER DISSIPATION
(W/Channel)
MAXIMUM AMBIENT
TEMPERATURE
4
2 W (3 dB)
0.56
125°C
4
1000 mW (6 dB)
0.30
136°C
4
500 mW (9 dB)
0.23
139°C
4
250 mW (12 dB)
0.20
141°C
4
120 mW (15 dB)
0.14
143°C
4
63 mW (18 dB)
0.09
146°C
ÁÁÁÁÁÁÁ
ÁÁÁÁÁÁ
ÁÁÁÁÁÁÁ
ÁÁÁÁÁ
ÁÁÁÁÁ
ÁÁÁÁÁÁÁ
ÁÁÁÁÁÁ
ÁÁÁÁÁÁÁ
ÁÁÁÁÁ
ÁÁÁÁÁ
DISSIPATION RATING TABLE
PACKAGE
DCA
TA ≤ 25°C
5.6 W
DERATING FACTOR
44.8 mW/°C
TA = 70°C
3.5 W
TA = 85°C
2.9 W
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:
Θ JA
1
+ Derating
1
+ 0.0448
+ 22.3°CńW
(19)
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 TPA005D02
is 150 °C. The internal dissipation figures are taken from the Efficiency vs Output Power graphs.
T A Max
+ TJ Max * ΘJA PD
+ 150 * 22.3 (0.14 2) + 143°C (15 dB crest factor)
+ 150 * 22.3 (0.56 2) + 125°C (3dB crest factor)
(20)
NOTE:
Internal dissipation of 0.6 W is estimated for a 2-W system with a 15 dB crest factor per channel.
Table 4 shows that for some applications no airflow is required to keep junction temperatures in the specified
range. The TPA005D02 is designed with thermal protection that turns the device off when the junction
temperature surpasses 150°C to prevent damage to the IC. Table 4 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.
22
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TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
THERMAL INFORMATION
The thermally enhanced DCA package is based on the 56-pin TSSOP, but includes a thermal pad (see Figure 59)
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 PowerPAD 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.
Thermal
Pad
DIE
Side View (a)
DIE
End View (b)
Bottom View (c)
Figure 22. Views of Thermally Enhanced DCA Package
POST OFFICE BOX 655303
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23
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
MECHANICAL DATA
DCA (R-PDSO-G**)
PowerPAD PLASTIC SMALL-OUTLINE PACKAGE
48 PINS SHOWN
0,27
0,17
0,50
48
0,08 M
25
Thermal Pad
(See Note D)
6,20
6,00
8,30
7,90
0,15 NOM
Gage Plane
1
24
0,25
A
0°– 8°
0,75
0,50
Seating Plane
0,15
0,05
1,20 MAX
PINS **
0,10
48
56
64
A MAX
12,60
14,10
17,10
A MIN
12,40
13,90
16,90
DIM
4073259/A 01/98
NOTES: A.
B.
C.
D.
All linear dimensions are in millimeters.
This drawing is subject to change without notice.
Body dimensions do not include mold flash or protrusion not to exceed 0,15.
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.
24
POST OFFICE BOX 655303
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IMPORTANT NOTICE
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TI warrants performance of its semiconductor products to the specifications applicable at the time of sale in
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Customers are responsible for their applications using TI components.
In order to minimize risks associated with the customer’s applications, adequate design and operating
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TI assumes no liability for applications assistance or customer product design. TI does not warrant or represent
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Copyright  2000, Texas Instruments Incorporated