TEXAS INSTRUMENTS TPA6120A2 Technical data

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Filter and
I/V Gain Stage
Stereo Hi−Fi
TPA6120A2
DYR > 120 dB
for Whole
System!
OUT A
OUT B
OUT C
OUT D
C
F
2.7 nF
R
F
LIN− LIN+
R
F
RIN−
RIN+
R
I
1 k
1 k
LOUT
ROUT
1 k
R
F
R
O
10
R
O
10
1 k
R
F
R
F
1 k
R
I
1 k
R
I
1 k
R
I
1 k
C
F
2.7 nF
R
F
1 k
1 k
C
F
2.7 nF
R
F
C
F
2.7 nF
R
F
1 k
1 k
1/2 OPA4134
1/2 OPA4134
−IN A
−IN B
+IN B
+IN A
−IN C
−IN D
+IN D
+IN C
PCM
Audio
Data
Source
Controller
PCM1792
or
DSD1792
LRCK BCK
DATA
RST
SCK
MDO
MC
MDI
MS
ZEROL
ZEROR
I
OUT
L−
I
OUT
L+
I
OUT
R−
I
OUT
R+
AUDIO DAC
HIGH FIDELITY HEADPHONE AMPLIFIER

FEATURES DESCRIPTION

80 mW into 600 From a ±12-V Supply at
0.00014% THD + N
Current-Feedback Architecture
Greater than 120 dB of Dynamic Range
SNR of 120 dB
Output Voltage Noise of 5 µVrms at
Gain = 2 V/V
Power Supply Range: ±5 V to ±15 V
1300 V/µs Slew Rate
Differential Inputs
Independent Power Supplies for Low
Crosstalk
Short Circuit and Thermal Protection

APPLICATIONS

Professional Audio Equipment
Mixing Boards
Headphone Distribution Amplifiers
Headphone Drivers
Microphone Preamplifiers
TPA6120A2
SLOS431 – MARCH 2004
The TPA6120A2 is a high fidelity audio amplifier built on a current-feedback architecture. This high bandwidth, extremely low noise device is ideal for high performance equipment. The better than 120 dB of dynamic range exceeds the capabilities of the human ear, ensuring that nothing audible is lost due to the amplifier. The solid design and performance of the TPA6120A2 ensures that music, not the amplifier, is heard.
Three key features make current-feedback amplifiers outstanding for audio. The first feature is the high slew rate that prevents odd order distortion anomalies. The second feature is current-on-demand at the output that enables the amplifier to respond quickly and linearly when necessary without risk of output distortion. When large amounts of output power are suddenly needed, the amplifier can re­spond extremely quickly without raising the noise floor of the system and degrading the signal-to-noise ratio. The third feature is the gain-independent fre­quency response that allows the full bandwidth of the amplifier to be used over a wide range of gain settings. The excess loop gain does not deteriorate at a rate of 20 dB/decade.
PowerPAD is a trademark of Texas Instruments.
PRODUCTION DATA information is current as of publication date. Products conform to specifications per the terms of the 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.
Copyright © 2004, Texas Instruments Incorporated
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TPA6120A2
SLOS431 – MARCH 2004
These devices have limited built-in ESD protection. The leads should be shorted together or the device placed in conductive foam during storage or handling to prevent electrostatic damage.

ABSOLUTE MAXIMUM RATINGS

over operating free-air temperature range (unless otherwise noted)
Supply voltage, V Input voltage, V Differential input voltage, V Minimum load impedance 8 Continuous total power dissipation See Dissipation Rating Table Operating free–air temperature range, T Operating junction temperature range, T Storage temperature range, T Lead temperature 1,6 mm (1/16 inch) from case for 10 seconds 235°C
(1) 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. (2) When the TPA6120A2 is powered down, the input source voltage must be kept below 600-mV peak. (3) The TPA6120A2 incorporates an exposed PowerPAD on the underside of the chip. This acts as a heatsink and must be connected to a
thermally dissipating plane for proper power dissipation. Failure to do so may result in exceeding the maximum junction temperature that
could permanently damage the device. See TI Technical Brief SLMA002 for more information about utilizing the PowerPAD thermally
enhanced package.
to V
CC+
(2)
I
CC-
ID
A
(3)
J
stg
(1)
TPA6120A2
33 V
± V
CC
6 V
- 40°C to 85°C
- 40°C to 150°C
- 40°C to 125°C

DISSIPATION RATING TABLE

(1)
θ
PACKAGE
JA
(°C/W) (°C/W) POWER RATING
DWP 44.4 33.8 2.8 W
θ
JC
TA= 25°C
(1) The PowerPAD must be soldered to a thermal land on the printed-circuit board. See the PowerPAD
Thermally Enhanced Package application note (SLMA002)

AVAILABLE OPTIONS

T
A
-40°C to 85°C DWP
(1) The DWP package is available taped and reeled. To order a taped and reeled part, add the suffix R
to the part number (e.g., TPA6120A2DWPR).
PACKAGE PART NUMBER SYMBOL
(1)

RECOMMENDED OPERATING CONDITIONS

Supply voltage, V
Load impedance V Operating free–air temperature, T
and V
CC+
CC-
A
TPA6120A2DWP 6120A2
MIN MAX UNIT
Split Supply ±5 ±15
Single Supply 10 30
= ±5 V or ±15 V 16
CC
-40 85 °C
V
2
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ELECTRICAL CHARACTERISTICS

over operating free-air temperature range (unless otherwise noted)
PARAMETER TEST CONDITIONS MIN TYP MAX UNIT
|V
| Input offset voltage (measured differentially) V
IO
PSRR Power supply rejection ratio V
V
IC
I
CC
I
O
r
i
r
o
V
O
Common mode input voltage V
Supply current (each channel) mA
Output current (per channel) VCC= ±5 V to ±15 V 700 mA Input offset voltage drift V Input resistance 300 k Output resistance Open Loop 13
Output voltage swing V
TPA6120A2
SLOS431 – MARCH 2004
= ±5 V or ±15 V 2 5 mV
CC
= 2.5 V to 5.5 V 75 dB
CC
V
= ±5 V ±3.6 ±3.7
CC
V
= ±15 V ±13.4 ±13.5
CC
V
= ±5 V 11.5 13
CC
VCC= ±15 V 15
= ±5 V or ±15 V 20 µV/°C
CC
= ±15 V, RL= 25 V
CC
11.8 to 12.5 to
-11.5 -12.2
3
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TPA6120A2
SLOS431 – MARCH 2004

OPERATING CHARACTERISTICS

TA= 25°C, RL= 25 , Gain = 2 V/V (unless otherwise noted)
PARAMETER TEST CONDITIONS MIN TYP MAX UNIT
IMD
THD+N
k
SVR
CMRR V
SR Slew rate V/µs
V
n
SNR Signal-to-noise ratio RL= 32 to 64 dB
(1) For IMD, THD+N, k
Intermodulation distortion Gain = 2 V/V, (SMPTE) IM frequency = 60 Hz
Total harmonic distortion plus noise
Supply voltage rejection ratio
Common mode rejection ratio (differential)
Output noise voltage RL= 32 to 64 µVrms
Dynamic range dB
Crosstalk RL= 32 to 64 -90 dB
, and crosstalk, the bandwidth of the measurement instruments was set to 80 kHz.
SVR
(1)
V
= ±12 V to ±15 V,
CC
SMTPE ratio = 4:1,
High frequency = 7 kHz
PO= 100 mW, RL= 32 f = 1 kHz
PO= 100 mW, RL= 64 f = 1 kHz
V
= ±12 V, Gain = 3 V/V
CC
RL= 600 , f = 1 kHz V
= ±15 V, Gain = 3 V/V
CC
RL= 600 , f = 1 kHz
V
= ±12 V,
CC
Gain = 3 V/V
V
= ±15 V,
CC
Gain = 3 V/V
RL= 32 , 0.00014% VI= 1 V
PP
V
= ±12 V to ±15 V,
CC
RL= 64 , 0.000095% VI= 1 V
PP
V
= ±12 V 0.00055%
CC
V
= ±15 V 0.00060%
CC
V
= ±12 V 0.00038%
CC
V
= ±15 V 0.00029%
CC
PO= 80 mW 0.00014% PO= 40 mW 0.000065% PO= 125 mW 0.00012% PO= 62.5 mW 0.000061% VO= 15 VPP,
RL= 10 k 0.000024% f = 1 kHz
VO= 15 VPP, RL= 10 k 0.000021% f = 1 kHz
RL= 32 VCC= ±12 V -80 f = 10 Hz to 22 kHz V
= 1 V
(RIPPLE)
PP
VCC= ±15 V -83
RL= 64 VCC= ±12 V -76 f = 10 Hz to 22 kHz V
V V V
= 1 V
(RIPPLE)
= ±5 V or ±15 V 100 dB
CC
= ±15 V, Gain = 5 V/V, VO= 20 V
CC
= ±5 V, Gain = 2 V/V, VO= 5 V
CC
= ±12 V to ±15 V Gain = 2 V/V 5
CC
PP
f = 1 kHz V
= ±12 V to ±15 V Gain = 2 V/V 125
CC
f = 1 kHz
RL= 32 , f = 1 kHz
RL= 64 , f = 1 kHz
V
= ±12 V to ±15 V
CC
f = 1 kHz
VCC= ±15 V -79
PP
PP
Gain = 100 V/V 50
Gain = 100 V/V 104 V
= ±12 V 123
CC
V
= ±15 V 125
CC
V
= ±12 V 124
CC
V
= ±15 V 126
CC
VI= 1 V
RMS
RF= 1 k
1300
900
dB
4
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DEVICE INFORMATION

1 2 3 4 5 6 7 8 9 10
20 19 18 17 16 15 14 13 12
11
LVCC−
LOUT
LVCC+
LIN+ LIN−
NC NC NC NC NC
RVCC− ROUT RVCC+ RIN+ RIN− NC NC NC NC NC
NC − No internal connection
Thermally Enhansed SOIC (DWP)
PowerPAD™ Package
Top View
TERMINAL FUNCTIONS
PIN NAME PIN NUMBER I/O DESCRIPTION
LVCC- 1 I LOUT 2 O Left channel output
LVCC+ 3 I Left channel positive power supply LIN+ 4 I Left channel positive input LIN- 5 I Left channel negative input NC 6,7,8,9,10,11,12,13,14,15 - Not internally connected RIN- 16 I Right channel negative input RIN+ 17 I Right channel positive input RVCC+ 18 I Right channel positive power supply ROUT 19 O Right channel output
RVCC- 20 I
Thermal Pad - -
Left channel negative power supply must be kept at the same potential as RVCC-.
Right channel negative power supply - must be kept at the same potential as LVCC-.
Connect to ground. The thermal pad must be soldered down in all applications to properly secure device on the PCB.
TPA6120A2
SLOS431 – MARCH 2004
5
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0.001
0.01
10 100 1 k 10 k 50 k
THD+N −Total Harmonic Distortion + Noise − %
f − Frequency − Hz
RL = 10 k, Gain = 3 V/V , RF = 2 k, RI = 1 k, BW = 80 kHz
VCC =15 VO = 15 V
PP
VCC =12 VO = 15 V
PP
VCC =12 VO = 12 V
PP
VCC =15 VO = 23 V
PP
0.0001
0.00001
0.0001
0.001
0.01
10 100 1 k 10 k 50 k
RL = 600 , Gain = 3 V/V , RF = 2 k, RI = 1 k, BW = 80 kHz
THD+N −Total Harmonic Distortion + Noise − %
f − Frequency − Hz
VCC =12 V ,
PO = 80 mW
VCC =15 V ,
PO = 125 mW
TPA6120A2
SLOS431 – MARCH 2004

TYPICAL CHARACTERISTICS

Table of Graphs

vs Frequency 1, 2, 3, 4
Total harmonic distortion + noise vs Output voltage 5
vs Output power 6, 7, 8 Power dissipation vs Output power 9 Supply voltage rejection ratio vs Frequency 10, 11
Intermodulation distortion
Crosstalk vs Frequency 14 Signal-to-noise ratio vs Gain 15, 16 Slew rate vs Output step 17, 18 Small and large signal frequency response 19, 20 400-mV step response 21 10-V step response 22 20-V step response 23
vs High frequency 12
vs IM Amplitude 13
FIGURE
TOTAL HARMONIC DISTORTION + NOISE TOTAL HARMONIC DISTORTION + NOISE
vs vs
FREQUENCY FREQUENCY
Figure 1. Figure 2.
6
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0.0001
0.01
0.1
1 k 10 k 50 k
THD+N −Total Harmonic Distortion + Noise − %
f − Frequency − Hz
RL = 64 , Gain = 2 V/V , RF = 1 k, RI = 1 k, BW = 80 kHz
VCC =15 V , PO = 700 mW
VCC =15 V , PO = 1.35 W
10
100
VCC =12 V , PO = 500 mW
VCC =12 V , PO = 425 mW
0.001
THD+N −Total Harmonic Distortion + Noise − %
f − Frequency − Hz
0.001
1
10 100 1 k 10 k 50 k
0.01
0.1
RL = 32 , Gain = 2 V/V , RF = 1 k, RI = 1 k, BW = 80 kHz
0.0001
VCC =15 V , PO = 1.5 W
VCC =12 V , PO = 800 mW
VCC =12 V , PO = 950 mW
VCC =15 V , PO = 1.25 W
0.001
0.01
0.1
1
10
3 5 10 15 20 25 30 35
THD+N −Total Harmonic Distortion + Noise − %
VO − Output Voltage − V
PP
RL = 10 k, Gain = 3 V/V , f = 1 kHz, RF = 2 k, RI = 1 k, BW = 80 kHz
VCC =12 V
VCC =15 V
0.0001
0.00001
THD+N −Total Harmonic Distortion + Noise − %
PO − Output Power − W
0.00001
0.01
1
10
0.01 0.1 0.2
0.0001
0.001
0.1
VCC = 15 V
VCC = 12 V
RL = 600 , Gain = 3 V/V , f = 1 kHz, RF = 2 k, RI = 1 k, BW = 80 kHz
TYPICAL CHARACTERISTICS (continued)
TPA6120A2
SLOS431 – MARCH 2004
TOTAL HARMONIC DISTORTION + NOISE TOTAL HARMONIC DISTORTION + NOISE
vs vs
FREQUENCY FREQUENCY
Figure 3. Figure 4.
TOTAL HARMONIC DISTORTION + NOISE TOTAL HARMONIC DISTORTION + NOISE
vs vs
OUTPUT VOLTAGE OUTPUT POWER
Figure 5. Figure 6.
7
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THD+N −Total Harmonic Distortion + Noise − %
0.01
1
10
0.01 0.1 2
0.0001
0.001
0.1
PO − Output Power − W
VCC = 15 V
VCC = 12 V
1
RL = 64 , Gain = 2 V/V , f = 1 kHz, RF = 1 k, RI = 1 k, BW = 80 kHz
THD+N −Total Harmonic Distortion + Noise − %
0.01
1
10
0.01 3
0.0001
0.001
0.1
PO − Output Power − W
VCC = 15 V
VCC = 12 V
0.1 1 2 4
RL = 32 , Gain = 2 V/V , f = 1 kHz, RF = 1 k, RI = 1 k, BW = 80 kHz
−90
−80
−70
−60
−50
−40
−30
−20
0
10 100 1 k 10 k 50 k
32
k
SVR
− Supply Voltage Rejection Ratio − dB
f − Frequency − Hz
64
−10
VCC = 12 V , V
(ripple)
= 1 VPP, Gain = 2 V/V BW = 80 kHz
Representative of both positive and negative supplies.
− Power Dissipation − W P
D
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
0 0.5 1 1.5 2 2.5 3 3.5
VCC =15 V , RL = 32
VCC =15 V ,
RL = 64
VCC =12 V ,
RL = 64
VCC =12 V , RL = 32
PO − Output Power − W
Mono Operation
TPA6120A2
SLOS431 – MARCH 2004
TYPICAL CHARACTERISTICS (continued)
TOTAL HARMONIC DISTORTION + NOISE TOTAL HARMONIC DISTORTION + NOISE
vs vs
OUTPUT POWER OUTPUT POWER
Figure 7. Figure 8.
POWER DISSIPATION SUPPLY VOLTAGE REJECTION RATIO
vs vs
OUTPUT POWER FREQUENCY
8
Figure 9. Figure 10.
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0.0001
0.001
0.01
0.1
2 k 10 k 50 k
Intermodulation Distortion − %
f − High Frequency − Hz
4:1 SMPTE Ratio VI = 1 VPP, Gain = 2 V/V , IM Frequency = 60 Hz
VCC =12 V ,
RL = 32
VCC =12 V ,
RL = 64
VCC =15 V ,
RL = 64
0.00001
VCC =15 V ,
RL = 32
−90
−80
−70
−60
−50
−40
−30
−20
−0
10 100 1 k 10 k 50 k
32
k
SVR
− Supply Voltage Rejection Ratio − dB
f − Frequency − Hz
−10
VCC = 15 V , V
(ripple)
= 1 VPP, Gain = 2 V/V BW = 80 kHz
64
Representative of both positive and negative supplies.
−120
−110
−100
−90
−80
−70
−60
10
100
1 k 10 k 50 k
RF = 1 k, Gain = 2 V/V , BW = 80 kHz
Crosstalk − dB
f − Frequency − Hz
VCC =12 V , RL = 32
VCC =15 V , RL = 64
VCC =12 V , RL = 64
VCC =15 V , RL = 32
IM Amplitude (At Input) − V
PP
0.00001
0.01
1
10
0 1 10
0.0001
0.001
0.1
VCC =15 V , RL = 32
VCC =12 V , RL = 64
VCC =12 V , RL = 32
4:1 SMPTE Ratio Gain = 3 V/V , High Frequency = 7 kHz IM Frequency = 60 Hz
2 3 4 5 6 7 8 9
VCC =15 V , RL = 64
Intermodulation Distortion − %
TYPICAL CHARACTERISTICS (continued)
TPA6120A2
SLOS431 – MARCH 2004
SUPPLY VOLTAGE REJECTION RATIO INTERMODULATION DISTORTION
vs vs
FREQUENCY HIGH FREQUENCY
Figure 11. Figure 12.
INTERMODULATION DISTORTION CROSSTALK
vs vs
IM AMPLITUDE (AT INPUT) FREQUENCY
Figure 13. Figure 14.
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Signal−To−Noise Ratio − dB
100
120
110
130
1 10 20 30 40 50 60 70
Gain − V/V
80 90 100
VCC =12 V
RI = 64
RI = 32
105
115
125
Signal−To−Noise Ratio − dB
100
105
110
115
120
125
130
1 10 20 30 40 50 60 70
Gain − V/V
80 90 100
VCC =15 V
THD+N, RI = 64
THD+N, RI = 32
0
Output Step (Peak−To−Peak) − V
1500
100
20
900
5
1100
700
10
1300
500
300
VCC = ± 15 V Gain = 5 V/V RF = 1 k RL = 25
15
+SR
−SR
Slew Rate − V/
sµ
0
Output Step (Peak−To−Peak) − V
1000
100
5
700
1
800
600
2 3
900
Slew Rate − V/
sµ
500
300
4
VCC = ± 5 V Gain = 2 V/V RF = 1 k RL = 25
400
200
+SR
−SR
TPA6120A2
SLOS431 – MARCH 2004
TYPICAL CHARACTERISTICS (continued)
SIGNAL-TO-NOISE RATIO SIGNAL-TO-NOISE RATIO
vs vs
GAIN GAIN
Figure 15. Figure 16.
SLEW RATE SLEW RATE
vs vs
OUTPUT STEP OUTPUT STEP
10
Figure 17. Figure 18.
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10M100k 500M1M 100M10k1k10010
f − Frequency − Hz
−27
−30
−18
−15
Output Level − dBV
−12
−3
−9
−6
VI = 500 mV
−24
−21
Gain = 1 V/V VCC = ± 15 V RF = 820 RL = 25
VI = 250 mV
VI = 125 mV
VI = 62.5 mV
10M100k 500M1M 100M10k1k10010
f − Frequency − Hz
−21
−24
−12
−9
Output Level − dBV
−6
3
−3
0
VI = 500 mV
−18
−15
Gain = 2 V/V VCC = ± 15 V RF = 680 RL = 25
VI = 250 mV
VI = 125 mV
VI = 62.5 mV
t − Time − ns
VCC = ±15 V Gain = 2 V/V RL = 25 RF = 1 k tr/tf= 300 ps See Figure 3
100
−100
0
−200
V
O
− Output Voltage − mV
300
200
0 15010050 200 250 350300 400 450 500
400
−300
−400
t − Time − ns
2
−2
0
−4
V
O
− Output Voltage − V
6
4
0 15010050 200 250 350300 400 450 500
8
−6
−8
VCC = ±15 V Gain = 2 V/V RL = 25 RF = 1 k tr/tf= 5 ns See Figure 3
TYPICAL CHARACTERISTICS (continued)
SMALL AND LARGE SIGNAL SMALL AND LARGE SIGNAL
FREQUENCY RESPONSE FREQUENCY RESPONSE
TPA6120A2
SLOS431 – MARCH 2004
400-mV STEP RESPONSE 10-V STEP RESPONSE
Figure 19. Figure 20.
Figure 21. Figure 22.
11
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t − Time − ns
VCC = ±15 V Gain = 5 V/V RL = 25 RF = 2 k tr/tf= 5 ns See Figure 3
4
−4
0
−8
V
O
− Output Voltage − V
12
8
0 15010050 200 250 350300 400 450 500
16
−12
−16
TPA6120A2
SLOS431 – MARCH 2004
TYPICAL CHARACTERISTICS (continued)
20-V STEP RESPONSE
Figure 23.
12
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+
R
F
= 1 k
V
CC+
R
I
= 1 k
R
S
= 50
R
O
= 10
R
L
V
I
V
CC−
TPA6120A2
SLOS431 – MARCH 2004

APPLICATION INFORMATION

Current-Feedback Amplifiers

The TPA6120A2 is a current-feedback amplifier with differential inputs and single-ended outputs. Current-feedback results in low voltage noise, high open-loop gain throughout a large frequency range, and low distortion. It can be used in a similar fashion as voltage-feedback amplifiers. The low distortion of the TPA6120A2 results in a signal-to-noise ratio of 120 dB as well as a dynamic range of 120 dB.

Independent Power Supplies

The TPA6120A2 consists of two independent high-fidelity amplifiers. Each amplifier has its own voltage supply. This allows the user to leave one of the amplifiers off, saving power, and reducing the heat generated. It also reduces crosstalk.
Although the power supplies are independent, there are some limitations. When both amplifiers are used, the same voltage must be applied to each amplifier. For example, if the left channel amplifier is connected to a ±12-V supply, the right channel amplifier must also be connected to a ±12-V supply. If it is connected to a different supply voltage, the device may not operate properly and consistently.
When the use of only one amplifier is preferred, it must be the left amplifier. The voltage supply to the left amplifier is also responsible for internal start-up and bias circuitry of the device. Regardless of whether one or both amplifiers are used, the V
To power down the right channel amplifier, disconnect the V The two independent power supplies can be tied together on the board to receive their power from the same
source.
pins of both amplifiers must always be at the same potential.
CC-
pin from the power source.
CC+

Power Supply Decoupling

As with any design, proper power supply decoupling is essential. It prevents noise from entering the device via the power traces and provides the extra power the device can sometimes require in a rapid fashion. This prevents the device from being momentarily current starved. Both of these functions serve to reduce distortion, leaving a clean, uninterrupted signal at the output.
Bulk decoupling capacitors should be used where the main power is brought to the board. Smaller capacitors should be placed as close as possible to the actual power pins of the device. Because the TPA6120A2 has four power pins, use four surface mount capacitors. Both types of capacitors should be low ESR.

Resistor Values

Figure 24. Single-Ended Input With a Noninverting Gain of 2 V/V
In the most basic configuration (see Figure 24 ), four resistors must be considered, not including the load impedance. The feedback and input resistors, R amplifier. R
is a series output resistor designed to protect the amplifier from any capacitance on the output path,
O
including board and load capacitance. R
and RI, respectively, determine the closed-loop gain of the
F
is a series input resistor. Because the TPA6120A2 is a
S
current-feedback amplifier, take care when choosing the feedback resistor.
13
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+
R
F
= 1 k
V
CC+
R
I
= 1 k
R
O
= 10
R
L
V
I
V
CC−
+
R
F
= 1 k
V
CC+
RI= 1 k
R
O
= 10
R
L
V
I−
V
CC−
V
I+
R
I
= 1 k
R
F
= 1 k
TPA6120A2
SLOS431 – MARCH 2004
APPLICATION INFORMATION (continued)
The value of the feedback resistor should be chosen by using Figure 27 through Figure 32 as guidelines. The gain can then be set by adjusting the input resistor. The smaller the feedback resistor, the less noise is introduced into the system. However, smaller values move the dominant pole to higher and higher frequencies, making the device more susceptible to oscillations. Higher feedback resistor values add more noise to the system, but pull the dominant pole down to lower frequencies, making the device more stable. Higher impedance loads tend to make the device more unstable. One way to combat this problem is to increase the value of the feedback resistor. It is not recommended that the feedback resistor exceed a value of 10 k. The typical value for the feedback resistor for the TPA6120A2 is 1 k. In some cases, where a high-impedance load is used along with a relatively large gain and a capacitive load, it may be necessary to increase the value of the feedback resistor from 1 k to 2 k, thus adding more stability to the system. Another method to deal with oscillations is to increase the size of RO.
CAUTION:
Do not place a capacitor in the feedback path. Doing so can cause oscillations.
Capacitance at the outputs can cause oscillations. Capacitance from some sources, such as layout, can be minimized. Other sources, such as those from the load (e.g., the inherent capacitance in a pair of headphones), cannot be easily minimized. In this case, adjustments to R
The series output resistor should be kept at a minimum of 10 . It is small enough so that the effect on the load is minimal, but large enough to provide the protection necessary such that the output of the amplifier sees little capacitance. The value can be increased to provide further isolation, up to 100 .
The series resistor, RS, should be used for two reasons:
1. It prevents the positive input pin from being exposed to capacitance from the line and source.
2. It prevents the source from seeing the input capacitance of the TPA6120A2.
The 50- resistor was chosen because it provides ample protection without interfering in any noticeable way with the signal. Not shown is another 50- resistor that can be placed on the source side of R capacity, it serves as an impedance match to any 50- source.
O
and/or R
may be necessary.
F
to ground. In that
S
Figure 25. Single-Ended Input With a Noninverting Gain of -1 V/V
Figure 26. Differential Input With a Noninverting Gain of 2 V/V
Figure 26 shows the TPA6120A2 connected with differential inputs. Differential inputs are useful because they take the greatest advantage of the device's high CMRR. The two feedback resistor values must be kept the same, as do the input resistor values.
14
www.ti.com
10M100k 500M1M 100M10k1k10010
f − Frequency − Hz
Normalized Output Response − dB
VCC = ±15 V RL = 100 Gain = 1 V/V VI = 200 mV
−1
−3
−5
−7
−2
−4
−6
1
2
0
3
RF = 1 k
RF = 620
RF = 820
10M100k 500M1M 100M10k1k10010
f − Frequency − Hz
Normalized Output Response − dB
VCC = ±15 V RL = 100 Gain = 2 V/V VI = 200 mV
−1
−3
−5
−2
−4
−6
1
2
0
3
RF = 430
RF = 1 k
RF = 620
TPA6120A2
SLOS431 – MARCH 2004
APPLICATION INFORMATION (continued)
Special note regarding mono operation:
If both amplifiers are powered on, but only one channel is to be used, the unused amplifier MUST have a feedback resistor from the output to the negative input. Additionally, the positive input should be grounded as close to the pin as possible. Terminate the output as close to the output pin as possible with a 25- load to ground.
These measures should be followed to prevent the unused amplifier from oscillating. If it oscillates, and the power pins of both amplifiers are tied together, the performance of the amplifier could be seriously degraded.

Checking for Oscillations and Instability

Checking the stability of the amplifier setup is recommended. High frequency oscillations in the megahertz region can cause undesirable effects in the audio band.
Sometimes, the oscillations can be quite clear. An unexpectedly large draw from the power supply may be an indication of oscillations. These oscillations can be seen with an oscilloscope. However, if the oscillations are not obvious, or there is a chance that the system is stable but close to the edge, placing a scope probe with 10 pF of capacitance can make the oscillations worse, or actually cause them to start.
A network analyzer can be used to determine the inherent stability of a system. An output vs frequency curve generated by a network analyzer can be a good indicator of stability. At high frequencies, the curve shows whether a system is oscillating, close to oscillation, or stable. Looking at Figure 27 through Figure 32 , several different phenomena occur. In one scenario, the system is stable because the high frequency rolloff is smooth and has no peaking. Increasing R section). Another scenario shows some peaking at high frequency. If the peaking is 2 dB, the amplifier is stable as there is still 45 degrees of phase margin. As the peaking increases, the phase margin shrinks, the amplifier and the system, move closer to instability. The same system that has a 2-dB peak has an increased peak when a capacitor is added to the output. This indicates the system is either on the verge of oscillation or is oscillating, and corrective action is required.
decreases the frequency at which this rolloff occurs (see the Resistor Values
F
Figure 27. Normalized Output Response vs Frequency Figure 28. Normalized Output Response vs Frequency
15
www.ti.com
10M100k 500M1M 100M10k1k10010
f − Frequency − Hz
Normalized Output Response − dB
−3
−5
−7
−9
−4
−6
−8
−1
0
−2
1
RL = 100
RL = 25
VCC = ±15 V RF = 1 k Gain = 1 V/V VI = 200 mV
RL = 50
RL = 200
10M100k 500M1M 100M10k1k10010
f − Frequency − Hz
Normalized Output Response − dB
VCC = ±15 V RF = 1 k Gain = 2 V/V VI = 200 mV
−3
−5
−7
−9
−4
−6
−8
−1
0
−2
1
RL = 100
RL = 25
RL = 200
RL = 50
10M100k 500M1M 100M10k1k10010
f − Frequency − Hz
−5
−6
−2
−1
Output Amplitude − dB
0
3
1
2
−4
−3
VCC = ± 5 V Gain = 1 V/V RL = 25 VI = 200 mV
RF = 1 k
RF = 1.5 k
RF = 620
10M100k 500M1M 100M10k1k10010
f − Frequency − Hz
1
0
4
5
Output Amplitude − dB
6
9
7
8
2
3
VCC = ± 5 V Gain = 2 V/V RL = 25 VI = 200 mV
RF = 820
RF = 1.2 k
RF = 510
TPA6120A2
SLOS431 – MARCH 2004
APPLICATION INFORMATION (continued)
Figure 29. Normalized Output Response vs Frequency Figure 30. Normalized Output Response vs Frequency
Figure 31. Output Amplitude vs Frequency Figure 32. Output Amplitude vs Frequency

PCB Layout

Proper board layout is crucial to getting the maximum performance out of the TPA6120A2. A ground plane should be used on the board to provide a low inductive ground connection. Having a ground
plane underneath traces adds capacitance, so care must be taken when laying out the ground plane on the underside of the board (assuming a 2-layer board). The ground plane is necessary on the bottom for thermal reasons. However, certain areas of the ground plane should be left unfilled. The area underneath the device where the PowerPAD is soldered down should remain, but there should be no ground plane underneath any of the input and output pins. This places capacitance directly on those pins and leads to oscillation problems. The underside ground plane should remain unfilled until it crosses the device side of the input resistors and the output series resistor. Thermal reliefs should be avoided if possible because of the inductance they introduce.
16
www.ti.com
+
R
I
R
O
R
L
V
I
Too Long
Too Long
Too Long
Too Long
TPA6120A2
R
F
+
R
I
R
O
R
L
V
I
TPA6120A2
Ground as Close to the Pin as Possible
Short Trace Before Resistors
R
F
Minimized Length of the Trace Between Output Node and R
O
Minimized Length of Feedback Path
Efficiency of an amplifier
P
L
P
SUP
P
L
V
LRMS
2
R
L
, andV
LRMS
V
P
2
, therefore, P
L
V
P
2
2R
L
per channel
P
SUP
VCCICCavg VCCI
CC(q)
I
CC
avg
1
2
0
V
P
R
L
sin(t) dt  
V
P
R
L
[cos(t)]
2 0
V
P
R
L
TPA6120A2
SLOS431 – MARCH 2004
APPLICATION INFORMATION (continued)
Despite the removal of the ground plane in critical areas, stray capacitance can still make its way onto the sensitive outputs and inputs. Place components as close as possible to the pins and reduce trace lengths. See Figure 33 and Figure 34 . It is important for the feedback resistor to be extremely close to the pins, as well as the series output resistor. The input resistor should also be placed close to the pin. If the amplifier is to be driven in a noninverting configuration, ground the input close to the device so the current has a short, straight path to the PowerPAD (gnd).
Figure 33. Layout That Can Cause Oscillation

Thermal Considerations

Amplifiers can generate quite a bit of heat. Linear amplifiers, as opposed to Class-D amplifiers, are extremely inefficient, and heat dissipation can be a problem. There is no one to one relationship between output power and heat dissipation, so the following equations must be used:
Where
Where
Figure 34. Layout Designed To Reduce Capacitance On Critical Nodes
(1)
(2) (3)
(4)
17
www.ti.com
VP 2 PLR
L
P
SUP
VCCV
P
R
L
VCCI
CC(q)
P
DISS
(1) P
SUP
TAMax TJMax ΘJAP
Diss
− Power Dissipation − W P
D
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
0 0.5 1 1.5 2 2.5 3 3.5
VCC =15 V , RL = 32
VCC =15 V ,
RL = 64
VCC =12 V ,
RL = 64
VCC =12 V , RL = 32
PO − Output Power − W
Mono Operation
TPA6120A2
SLOS431 – MARCH 2004
APPLICATION INFORMATION (continued)
Therefore,
PL= Power delivered to load (per channel) P
= Power drawn from power supply
SUP
V
= RMS voltage on the load
LRMS
RL= Load resistance VP= Peak voltage on the load ICCavg = Average current drawn from the power supply ICC(q) = Quiescent current (per channel) VCC= Power supply voltage (total supply voltage = 30 V if running on a ±15-V power supply η = Efficiency of a SE amplifier
(5)
(6)
For stereo operation, the efficiency does not change because both P
and P
L
are doubled. This effects the
SUP
amount of power dissipated by the package in the form of heat. A simple formula for calculating the power dissipated, P
In stereo operation, P
is twice the quantity that is present in mono operation.
SUP
, is shown in Equation 7 :
DISS
The maximum ambient temperature, TA, depends on the heat-sinking ability of the system. θ whose thermal pad is properly soldered down, is shown in the dissipation rating table.
for a 20-pin DWP,
JA
(7)
(8)
18
Figure 35. Power Dissipation vs Output Power
www.ti.com

Application Circuit

DATA
24 23 22 21 20 19 18 17 16 15
5 6 7 8 9
10
11 12 13 14
PCM1792
BCK SCK DGND V
DD
MS MDI MC MDO RST
AGND2
I
OUT
R−
VCC1
V
COM
L
V
COM
R
I
REF
I
OUT
R+
AGND3R
AGND1
ZEROL
1 2 3 4
ZEROR MSEL LRCK
28 27 26 25
VCC2L
AGND3L
I
OUT
L−
I
OUT
L+
5 V
VCC2R
0.1 µF
Controller
10 µF
3.3 V
PCM
Audio
Data
Source
0.1 µF 10 µF
+
+
47 µF
47 µF
5 V
10 µF
10 k
+
CF 2.7 nF
R
F
1 k
0.1 µF
10 µF
5 V
+
+
+
+
V−
V+
4
12
13
14
−IND OUTD
+
CF 2.7 nF
R
F
1 k
V−
V+
4
10
9
8
−INC
+
CF 2.7 nF
R
F
1 k
V−
V+
4
3
2
1
+
CF 2.7 nF
R
F
1 k
V−
V+
4
5
6
7
11
11
11
11
−INB
−INA
OUTA
OUTB
OUTC
+
1 k
V
CC−
3
4
5
2
LOUT
0.1 F
V
CC+
LIN− LIN+
0.1 F
R
O
10
4
+
R
F
V
CC−
18
17
16
19
ROUT
0.1 F
V
CC+
RIN− RIN+
0.1 F
20
1 k
1 k
R
I
R
F
1 k
R
I
1 k
1 k
1 k
R
I
R
F
1 k
R
I
R
F
+
10 µF
0.1 µF
5 V
V+
+
10 µF0.1 µF
−5 V
V−
OPA4134
+
100 µF
10 µF
12 V
V
CC+
+
100 µF10 µF
−12 V
V
CC−
TPA6120A2
+
+
R
O
10
TPA6120A2
SLOS431 – MARCH 2004
In many applications, the audio source is digital. It must go through a digital-to-analog converter (DAC) so that traditional analog amplifiers can drive the speakers or headphones.
Figure 36 shows a complete circuit schematic for such a system. The digital audio is fed into a high performance DAC. The PCM1792, a Burr-Brown product from TI, is a 24-bit, stereo DAC.
The output of the PCM1792 is current, not voltage, so the OPA4134 is used to convert the current input to a voltage output. The OPA4134, a Burr-Brown product from TI, is a low-noise, high-speed, high-performance operational amplifier. C Figure 36 has a cutoff frequency of 59 kHz. All four amplifiers of the OPA4134 are used so the TPA6120A2 can be driven differentially.
and R
F
Figure 36. Typical Application Circuit
are used to set the cutoff frequency of the filter. The RC combination in
F
19
www.ti.com
TPA6120A2
SLOS431 – MARCH 2004
The output of the OPA4134 goes into the TPA6120A2. The TPA6120A2 is configured for use with differential inputs, stereo use, and a gain of 2V/V. Note that the 0.1-uF capacitors are placed at every supply pin of the TPA6120A2, as well as the 10- series output resistor.
Each output goes to one channel of a pair of stereo headphones, where the listener enjoys crisp, clean, virtually noise free music with a dynamic range greater than the human ear is capable of detecting.
20
PACKAGE OPTION ADDENDUM
www.ti.com
5-Oct-2007
PACKAGING INFORMATION
Orderable Device Status
TPA6120A2DWP ACTIVE SO
(1)
Package
Type
Power
Package
Drawing
Pins Package
Qty
Eco Plan
DWP 20 25 Green (RoHS &
no Sb/Br)
PAD
TPA6120A2DWPG4 ACTIVE SO
Power
DWP 20 25 Green (RoHS &
no Sb/Br)
PAD
TPA6120A2DWPR ACTIVE SO
Power
DWP 20 2000 Green (RoHS &
no Sb/Br)
PAD
TPA6120A2DWPRG4 ACTIVE SO
Power
DWP 20 2000 Green (RoHS &
no Sb/Br)
PAD
(1)
The marketing status values are defined as follows:
ACTIVE: Product device recommended for new designs. LIFEBUY: TI has announced that the device will be discontinued, and a lifetime-buy period is in effect. NRND: Not recommended for new designs. Device is in production to support existing customers, but TI does not recommend using this part in
a new design.
PREVIEW: Device has been announced but is not in production. Samples may or may not be available. OBSOLETE: TI has discontinued the production of the device.
(2)
Eco Plan - The planned eco-friendly classification: Pb-Free (RoHS), Pb-Free (RoHS Exempt), or Green (RoHS & no Sb/Br) - please check
http://www.ti.com/productcontent for the latest availability information and additional product content details.
TBD: The Pb-Free/Green conversion plan has not been defined. Pb-Free (RoHS): TI's terms "Lead-Free" or "Pb-Free" mean semiconductor products that are compatible with the current RoHS requirements
for all 6 substances, including the requirement that lead not exceed 0.1% by weight in homogeneous materials. Where designed to be soldered at high temperatures, TI Pb-Free products are suitable for use in specified lead-free processes. Pb-Free (RoHS Exempt): This component has a RoHS exemption for either 1) lead-based flip-chip solder bumps used between the die and package, or 2) lead-based die adhesive used between the die and leadframe. The component is otherwise considered Pb-Free (RoHS compatible) as defined above. Green (RoHS & no Sb/Br): TI defines "Green" to mean Pb-Free (RoHS compatible), and free of Bromine (Br) and Antimony (Sb) based flame retardants (Br or Sb do not exceed 0.1% by weight in homogeneous material)
(2)
Lead/Ball Finish MSL Peak Temp
CU NIPDAU Level-2-260C-1 YEAR
CU NIPDAU Level-2-260C-1 YEAR
CU NIPDAU Level-2-260C-1 YEAR
CU NIPDAU Level-2-260C-1 YEAR
(3)
(3)
MSL, Peak Temp. -- The Moisture Sensitivity Level rating according to the JEDEC industry standard classifications, and peak solder
temperature.
Important Information and Disclaimer:The information provided on this page represents TI's knowledge and belief as of the date that it is provided. TI bases its knowledge and belief on information provided by third parties, and makes no representation or warranty as to the accuracy of such information. Efforts are underway to better integrate information from third parties. TI has taken and continues to take reasonable steps to provide representative and accurate information but may not have conducted destructive testing or chemical analysis on incoming materials and chemicals. TI and TI suppliers consider certain information to be proprietary, and thus CAS numbers and other limited information may not be available for release.
In no event shall TI's liability arising out of such information exceed the total purchase price of the TI part(s) at issue in this document sold by TI to Customer on an annual basis.
Addendum-Page 1
PACKAGE MATERIALS INFORMATION
www.ti.com
TAPE AND REEL INFORMATION
19-Mar-2008
*All dimensions are nominal
Device Package
TPA6120A2DWPR SO
Type
Power
PAD
Package Drawing
DWP 20 2000 330.0 24.4 10.8 13.0 2.7 12.0 24.0 Q1
Pins SPQ Reel
Diameter
(mm)
Reel
Width
W1 (mm)
A0 (mm) B0 (mm) K0 (mm) P1
(mm)W(mm)
Quadrant
Pin1
Pack Materials-Page 1
PACKAGE MATERIALS INFORMATION
www.ti.com
19-Mar-2008
*All dimensions are nominal
Device Package Type Package Drawing Pins SPQ Length (mm) Width (mm) Height (mm)
TPA6120A2DWPR SO PowerPAD DWP 20 2000 346.0 346.0 41.0
Pack Materials-Page 2
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