Texas Instruments TPA005D02EVM, TPA005D02DCA, TPA005D02DCAR Datasheet

TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
1
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
NOT RECOMMENDED FOR NEW DESIGNS
D
D
Extremely Efficient Class-D Stereo Operation
D
Drives L and R Channels
D
2-W BTL Output into 4
D
5-W Peak Music Power
D
Fully Specified for 5-V Operation
D
Low Quiescent Current
D
Shutdown Control
D
Thermally-Enhanced PowerP AD Surface­Mount Packaging
D
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 TP A005D02 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- load at 0.5% THD+N from a 5-V power supply in the high fidelity range (20 Hz to 20 kHz).
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 TP A005D02 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).
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.
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.
SHUTDOWN
MUTE AGND
LINN LINP
LCOMP
AGND
V
DD
LPV
DD
LOUTP LOUTP
PGND
PGND LOUTN LOUTN
LPV
DD
NC NC NC
AGND
PV
DD
VCP
CP3 CP2
COSC AGND AGND RINN RINP RCOMP FAULT0 FAULT1 RPV
DD
ROUTP ROUTP PGND PGND ROUTN ROUTN RPV
DD
PV
DD
NC NC V2P5 LSBIAS PGND CP4 CP1
NC – No internal connection
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
DCA PACKAGE
(TOP VIEW)
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
Template Release Date: 7–11–94
2
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
10 k10 k
_
+
_
+
LINP
RAMP
GENERATOR
_
+
_
+
GATE
DRIVE
LPV
DD
GATE
DRIVE
LPV
DD
GATE
DRIVE
RPV
DD
GATE
DRIVE
RPV
DD
THERMAL
DETECT
VCP-UVLO
DETECT
TRIPLER
CHARGE PUMP
CONTROL and
STARTUP
LOGIC
BIAS
GENERATOR
HPV
CC
PV
DD
LINN
LCOMP
COSC
RCOMP
RINP RINN
RPV
DD
AGND
LPV
DD
ROUTP
ROUTN
PV
DD
VCP
CP4
CP3
CP2
CP1
LOUTP
LOUTN
LSBIAS
FAULT0
FAULT1
SHUTDOWN
MUTE
V2P5
LPV
DD
RPV
DD
PGND
VCP LSBIAS
VCP LSBIAS
VCP LSBIAS
VCP LSBIAS
LSBIAS
V
DD
V
DD
PV
DD
1.5 V
10 k10 k
1.5 V
NOTE A: LPVDD, RPVDD, VDD, and PVDD are externally connected. AGND and PGND are externally connected.
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
3
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
Terminal Functions
TERMINAL
NAME NO.
DESCRIPTION
AGND 3, 7, 20,
46, 47
Analog ground for analog sections
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 LINP 5 Class-D left-channel positive input 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 LPV
DD
9, 16 Class-D amplifier left-channel power supply
LSBIAS 28 Level-shifter power supply, to be tied to VCP MUTE
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.
NC 17, 18, 19,
30, 31
No internal connection
PGND 12, 13 Power ground for left-channel H–bridge only PGND 27 Power ground for charge pump only PGND 36, 37 Power ground for right-channel H-bridge only PV
DD
21, 32 VDD supply for charge-pump and internal logic circuitry RCOMP 43 Compensation capacitor terminal for right-channel Class-D amplifier RINN 45 Class-D right-channel negative input RINP 44 Class-D right-channel positive input RPV
DD
33, 40 Class-D amplifier right-channel power supply ROUTN 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 V
DD
8 VDD bias supply for analog circuitry. This terminal needs to be well filtered to prevent degrading the device
performance.
TPA005D02 2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
4
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
Class-D amplifier faults
Table 1. Amplifier Fault Table
FAULT 0†FAULT 1
DESCRIPTION
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.
These logic levels assume a pull up to PVDD from the open-drain outputs.
AVAILABLE OPTIONS
PACKAGED DEVICES
T
A
TSSOP
(DCA)
–40°C to 125°C TPA005D02DCA
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., TPA005D02DCAR).
absolute maximum ratings over operating free-air temperature range, TC = 25°C (unless otherwise noted)
Supply voltage, V
DD
(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, V
CP
PVDD + 20 V. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
Continuous H-bridge output current 2 A. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
Pulsed H-Bridge output current, each output, I
max
(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, T
C
–40°C to 125°C. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
Storage temperature range, T
stg
–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 v 2%
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 T exas Instruments document,
PowerPAD Thermally Enhanced Package Application Report
(literature number SLMA002), for more information on the PowerP AD package. The thermal data was measured on a PCB layout based on the information in the section entitled
T exas Instruments Recommended Board for PowerP AD
on page 33 of the before mentioned
document.
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
5
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
recommended operating conditions
MIN NOM MAX UNIT
Supply voltage, PVDD, LPVDD, RPVDD, V
DD
4.5 5.5 V
High-level input voltage, V
IH
4.25 V
Low-level input voltage, V
IL
0.75 V
Audio inputs, LINN, LINP, RINN, RINP, HPLIN, HPRIN, differential input voltage 1 V
RMS
PWM frequency 100 500 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 MIN TYP MAX UNIT
PSRR Power supply rejection ratio VDD = PVDD = LPVDD = RPVDD = 4.9 V to 5.1 V 40 dB I
DD
Supply current No load or output filter 25 40 mA
I
DD(MUTE)
Supply current, mute mode MUTE = 0 V 10 15 mA
I
DD(SD)
Supply current, shutdown mode SHUTDOWN = 0 V 400 2000 µA
I
IH
High-level input current VIH = 5.3 V 10 µA
I
IL
Low-level input current VIL = –0.3 V –10 µA
r
DS(on)
Total static drain-to-source on-state resistance (low-side plus high-side FETs)
ID = 0.5 A 620 750 m
r
DS(on)
Matching 95% 99.5%
operating characteristics, VDD = PVDD = LPVDD = RPVDD = 5 V, RL = 4 , TC = 25°C, See Figure 1 (unless otherwise noted)
PARAMETER TEST CONDITIONS MIN TYP MAX UNIT
P
O
RMS output power, THD = 0.5%, per channel 2 W
THD+N Total harmonic distortion plus noise PO = 1 W, f = 1 kHz 0.2%
Efficiency RL = 8 80%
A
V
Gain 24 dB Left/right channel gain matching 95% Noise floor 60 dB Dynamic range 70 dB Crosstalk f = 1 kHz 55 dB Frequency response bandwidth, post output filter, –3 dB 20 20,000 Hz
B
OM
Maximum output power bandwidth 20 kHz
thermal resistance
PARAMETER TEST CONDITIONS MIN TYP MAX UNIT
R
θJP
Thermal resistance, junction-to-pad 10 °C/W
R
θJA
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
T exas Instruments Recommended Board for PowerPAD
on page 33 of the before mentioned document.
TPA005D02 2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
6
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
PARAMETER MEASUREMENT INFORMATION
LINP
LINN
LCOMP
V
DD
COSC
RCOMP
RINP
RINN
RPV
DD
AGND (see Note A)
LPV
DD
PV
DD
LSBIAS
SHUTDOWN
V2P5
PGND (see Note A)
15 µH
15 µH
0.22 µF
0.22 µF 1 µF
4
VCP
5 V
5 V
1 µF
1 µF
Balanced
Differential
Input Signal
470 pF
470 pF
470 pF
1 µF
1 µF
Balanced
Differential
Input Signal
5 V
CP1
CP2 CP3
CP4
VCP
FAULT0 FAULT1
MUTE
PV
DD
PV
DD
1 µF
LOUTP
LOUTN
15 µH
15 µH
0.22 µF
0.22 µF 1 µF
4
ROUTP
ROUTN
47 nF
47 nF
2.2 µF
28
42
1 2
9,16
5
4
6
43
48
44
45
33,40
2, 3, 7,20,46,47
12,13,27,36,37
21, 32
41
14,15
10,11
29
8
25
24 23
26 22
34,35
38,39
Figure 1. 5-V, 4- Test Circuit
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
7
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
TYPICAL CHARACTERISTICS
Table of Graphs
FIGURE
pp
vs Switching frequency 2
IDDSupply current
vs Free-air temperature 3
p
vs Frequency 4, 5
THD+N
Total harmonic distortion plus noise
vs Output power 6, 7 Voltage amplification and phase shift vs Frequency 8 Crosstalk vs Frequency 9 Efficiency vs Output power 10
Figure 2
SUPPLY CURRENT
vs
SWITCHING FREQUENCY
0 100 200 300
400 500
Open Load
f – Switching Frequency – Hz
40
20
I
80
100
0
60
With Output Filter
Without Output Filter
DD
– Supply Current – mA
Figure 3
SUPPLY CURRENT
vs
FREE–AIR TEMPERATURE
–40 0 40 80
120 125
Open Load
TA – Free–Air Temperature – °C
20
10
40
50
0
30
With Output Filter
Without Output Filter
I
DD
– Supply Current – mA
TPA005D02 2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
8
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
TYPICAL CHARACTERISTICS
Figure 4
TOTAL HARMONIC DISTORTION PLUS NOISE
vs
FREQUENCY
0.05
0.02
0.2
20 100 500 2k
1
0.01
THD+N – Total Harmonic Distortion Plus Noise – %
f – Frequency – Hz
50 200 1k 5k
0.5
0.1
10k 20k
PO = 100 mW
PO = 1W
PO = 2W
RL = 4
Figure 5
TOTAL HARMONIC DISTORTION PLUS NOISE
vs
FREQUENCY
0.05
0.02
0.2
20 100 500 2k
1
0.01
THD+N – Total Harmonic Distortion Plus Noise – %
f – Frequency – Hz
50 200 1k 5k
0.5
0.1
10k 20k
RL = 8
PO = 100 mW
PO = 1W
PO = 500 mW
Figure 6
TOTAL HARMONIC DISTORTION PLUS NOISE
vs
OUTPUT POWER
0.05
0.02
0.2
0.01 0.05 0.2 1
1
0.01
THD+N – Total Harmonic Distortion Plus Noise – %
PO – Output Power – W
0.02 0.1 0.5 2
0.5
0.1
510
f = 1 kHz
f = 20 kHz
f = 20 kHz
f = 20 Hz
f = 20 Hz
10
RL = 4
2
5
Figure 7
TOTAL HARMONIC DISTORTION PLUS NOISE
vs
OUTPUT POWER
0.05
0.02
0.2
10m 50m 200m 1
1
0.01
THD+N – Total Harmonic Distortion Plus Noise – %
PO – Output Power – W
20m 100m 500m 2
0.5
0.1
510
f = 1 kHz
f = 20 kHz
f = 20 Hz
10
2
5
RL = 8
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
9
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
TYPICAL CHARACTERISTICS
GAIN AND PHASE
vs
FREQUENCY
16
4
20
10 50 200 1k
24
0
Gain – dB
f – Frequency – Hz
20 100 500 2k
22
18
5k 100k
30
26
28
2
6
10
8
12
14
Phase
10k 20k 50k
Po = 2W RL = 4
–45°
–40°
–35°
–30°
–25°
–20°
–15°
–10°
–5°
0°
5°
10°
15°
20°
25°
30°
35°
40°
45°
Phase Shift
Voltage Amplification
Figure 8
Figure 9
CROSSTALK
vs
FREQUENCY
–70
–130
–50
50 200 1k
–30
–150
Crosstalk – dB
f – Frequency – Hz
20 100 500 2k
–40
–60
5k 20k
0
–20
–10
–140
–120
–100
–110
–90
–80
PO = 2W RL = 4
Left-to-Right
Right-to-Left
10k
Figure 10
EFFICIENCY
vs
OUTPUT POWER
0 0.4 0.8 1.2
1.6 2.0
RL = 8
PO – Output Power – W
60
50
Efficiency – %
80
90
40
70
RL = 4
TPA005D02 2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
10
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
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)
End View (b)
Bottom View (c)
DIE
Thermal
Pad
Figure 11. Views of Thermally Enhanced DCA Package
selection of components
Figure 12 is a schematic diagram of a typical notebook computer application circuit.
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
11
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
APPLICATION INFORMATION
LINP
LINN
LCOMP
V
DD
COSC
RCOMP
RINP
RINN
RPV
DD
AGND (see Note A)
LPV
DD
PV
DD
LSBIAS
SHUTDOWN
V2P5
PGND (see Note A)
15 µH
15 µH
0.22 µF
0.22 µF 1 µF
4
VCP
5 V
5 V
1 µF
1 µF
Balanced
Differential
Input Signal
470 pF
470 pF
470 pF
1 µF
1 µF
Balanced
Differential
Input Signal
5 V
CP1
CP2 CP3
CP4
VCP
FAULT0 FAULT1
MUTE
PV
DD
PV
DD
1 µF
LOUTP
LOUTN
15 µH
15 µH
0.22 µF
0.22 µF 1 µF
4
ROUTP
ROUTN
47 nF
47 nF
2.2 µF
28
42
1 2
9,16
5
4
6
43
48
44
45
33,40
2, 3, 7,20,46,47
12,13,27,36,37
21, 32
41
14,15
10,11
29
8
25
24 23
26 22
34,35
38,39
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
TPA005D02 2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
12
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
APPLICATION INFORMATION
input capacitor, C
I
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.
(8)
f
c(highpass)
+
1
2pRINC
I
–3 dB
f
c
RIN is nominally 10 k
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.
(9)
C
I
+
1
2pRINf
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 TP A005D02 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 A005D02. 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 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 V
DD
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 A005D02 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.
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
SLOS227C – AUGUST 1998 – REVISED MARCH 2000
13
POST OFFICE BOX 655303 DALLAS, TEXAS 75265
APPLICATION INFORMATION
mute and shutdown modes
The TP A005D02 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 I
DD
to 10 mA.
Table 2. Shutdown and Mute Mode Functions
INPUTS
OUTPUT
AMPLIFIER STATE
SE/BTL
HP/LINE
MUTE IN
SHUTDOWN
MUTE OUT
INPUT OUTPUT
Low Low Low Low Low L/R Line BTL
X X High X Mute X X High High X Mute
Low High Low Low Low L/R HP BTL
High Low Low Low Low L/R Line SE High High Low Low Low L/R HP SE
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.
TPA005D02 2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
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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
SUP
is the supply power.
Efficiency+h
+
P
L
P
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 (R
DS(ON)
) and the switching times of the output transistors are zero.
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 (Figure 13).
V
DD
V
OUT
L
C
L
R
L
I
L
I
OUT
+
V
A
M2
M1
C
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 V
A
(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 V
A
, which makes V
OUT
equal to the supply voltage multiplied by the duty cycle.
TPA005D02
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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.
Supply Current
Time
M1 on M2 off
M1 off M2 on
M1 on M2 off
Output Current
Inductor Current
0
Current
Figure 14. Class D Currents
V
DD
V
A
V
OUT
0
Voltage
Time
M1 on M2 off
M1 off M2 on
M1 on M2 off
Figure 15. Class D Voltages
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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.
V
L(rms)
+
V
P
2
Ǹ
CLASS D LINEAR
V
L(rms)
+
V
P
2
Ǹ
PL+
VL
I
L
AverageǒI
DD
Ǔ
+
I
L(rms)
V
L(rms)
V
DD
PL+
V
L(rms)
2
R
L
+
V
P
2
2R
L
AverageǒI
DD
Ǔ
+
2
p
V
P
R
L
P
SUP
+
VDD
AverageǒI
DD
Ǔ
P
SUP
+
VDD
AverageǒI
DD
Ǔ
+
VDDV
P
R
L
2
p
P
SUP
+
V
DD
I
L(rms)
V
L(rms)
V
DD
Efficiency+h
+
P
L
P
SUP
Efficiency+h
+
P
L
P
SUP
Efficiency+h+VDD
V
P
2
2R
L
2
p
V
P
R
L
Efficiency+h+1 Efficiency+h
+
p
4
V
P
V
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.
V
DD
V
OUT
L
C
L
R
L
I
L
I
OUT
+
V
A
M2
M1
V
DD
L
C
L
M4
M3
Figure 16. H-Bridge Class D Output Stage
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
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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
DS(on)
, and rise and fall times that are greater than zero.
The loss due to a nonzero R
DS(on)
is called conduction loss, and is the power lost in the output transistors at
nonswitching times, when the transistor is ON (saturated). Any R
DS(on)
above 0 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
R
L
4
0.31
0.31
R
DS(on)
R
DS(off)
R
DS(off)
R
DS(on)
5 M
5 M
Figure 17. Output Transistor Simplification for Conduction Loss Calculation
The power supplied, P
SUP
, 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
+
I2R
L
I22R
DS(on)
)
I2R
L
Efficiency+h
+
P
L
P
SUP
Efficiency+h
+
R
L
2R
DS(on)
)
R
L
Efficiency+h+95%ǒat all output levels R
DS(on)
+
0.1, RL+
4
Ǔ
Efficiency+h+87%ǒat all output levels R
DS(on)
+
0.31, RL+
4
Ǔ
TPA005D02 2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
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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.
t
SWon
+
t
SWoff
=
t
SW
1
f
SW
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- loads and a 5-V supply is almost 2.7 W. A similar linear amplifier such as the TP A005D02 has a maximum draw of 3.25 W under the same circumstances.
Table 3. Efficiency vs Output Power in 5-V 8- 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 4 0.314
1.25 80.6 4.47
0.3
High peak voltages cause the THD to increase
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
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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
P
PK
P
rms
Time
P
PK
Power
P
RMS
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.
600
500
300
200
100
0
400
1 1.5 2 2.5
Power Supplied (mW)
POWER SUPPLIED
vs
PEAK OUTPUT VOLTAGE AND PEAK OUTPUT POWER
4 4.53
3.5
0.25 0.56 1 1.56 4 5.062.25
3.06
Peak Output Voltage (V)
Peak Output Power (W)
TPA0202
TPA005D02
Figure 20. Audio Signal Showing Peak and RMS Power (with Music Applied)
TPA005D02 2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
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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.
400
350
250
200
150
0
300
1 1.5 2 2.5
Supply Current (mA rms)
SUPPLY CURRENTS
vs
PEAK OUTPUT VOLTAGE AND PEAK OUTPUT POWER
43
3.5
100
50
0.25 0.56 1 1.56 42.25
3.06
Peak Output Voltage (V)
Peak Output Power (W)
TPA0202
TPA005D02
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.
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
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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 TP A005D02 is operating from a 5-V supply into a 4- speaker that 4 W peaks are available. Converting W atts to dB:
PdB+
10Log
ǒ
P
W
P
ref
Ǔ
+
10Log
ǒ
4 1
Ǔ
+
6dB
(17)
Subtracting the crest factor restriction to obtain the average listening level without distortion yields:
6.0 dB*15 dB
+*
9dB(15 dB crest factor
)
6.0 dB*12 dB
+*
6dB(12 dB crest factor
)
6.0 dB*9dB
+*
3dB(9 dB crest factor
)
6.0 dB*6dB
+*
0dB(6 dB crest factor
)
6.0 dB*3dB+3dB(3 dB crest factor
)
6.0 dB*18 dB
+*
12 dB(15 dB crest factor
)
Converting dB back into watts:
PW+
10
PdBń10
P
ref
+
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)
+
63 mW (18 dB crest factor)
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 af fects maximum ambient temperature ratings for the system. Using the power dissipation curves for a 5-V, 4- system, the internal dissipation in the TPA005D02 and maximum ambient temperatures is shown in Table 4.
TPA005D02 2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
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APPLICATION INFORMATION
crest factor and thermal considerations (continued)
Table 4. TPA005D02 Power Rating, 5-V, 4-, Stereo
PEAK OUTPUT POWER
POWER DISSIPATION MAXIMUM AMBIENT
(W)
AVERAGE OUTPUT POWER
(W/Channel) 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
DISSIPATION RATING TABLE
PACKAGE
TA 25°C
DERATING FACTOR TA = 70°C TA = 85°C
DCA
5.6 W
44.8 mW/°C
БББББ
3.5 W
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 TP A005D02 is 150 °C. The internal dissipation figures are taken from the Efficiency vs Output Power graphs.
T
A
Max+TJMax
*
Θ
JA
P
D
+
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.
TPA005D02
2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
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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 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)
End View (b)
Bottom View (c)
DIE
Thermal
Pad
Figure 22. Views of Thermally Enhanced DCA Package
TPA005D02 2-W STEREO CLASS-D AUDIO POWER AMPLIFIER
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MECHANICAL DATA
DCA (R-PDSO-G**) PowerPAD PLASTIC SMALL-OUTLINE PACKAGE
0,25
0,50
0,75
0,15 NOM
Gage Plane
6,00
6,20
8,30 7,90
Thermal Pad (See Note D)
64
17,10
56
14,10
Seating Plane
16,9013,90
4073259/A 01/98
0,27
25
24
A
0,17
48 PINS SHOWN
48
1
48
DIM
PINS **
A MAX
A MIN
1,20 MAX
12,40
12,60
0,50
0,10
M
0,08
0°–8°
0,05
0,15
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.
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
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