KINGBOR KB4863MTE

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KB4863
KB4863
Dual 2.2W Audio Amplifier Plus Stereo Headphone
Function
General Description
Key Specifications
The KB4863 is a dual bridge-connected audio power amplifier which, when connected to a 5V supply, will deliver 2.2W
to a 4Ω load (Note 1) or 2.5W to a 3Ω load (Note 2) with less
than 1.0% THD+N. In addition, the headphone input pin
allows the amplifiers to operate in single-ended mode when
driving stereo headphones.
n PO at 1% THD+N
n
KB4863LQ, 3Ω, 4Ω loads
2.5W(typ), 2.2W(typ)
n
KB4863MTE, 3Ω, 4Ω loads
2.5W(typ), 2.2W(typ)
n
KB4863MTE, 8Ω load
1.1W(typ)
n
KB4863, 8Ω
1.1W(typ)
n Single-ended mode THD+N at 75mW into
32Ω
0.5%(max)
n Shutdown current
0.7µA(typ)
n Supply voltage range
2.0V to 5.5V
Boomer audio power amplifiers were designed specifically to
provide high quality output power from a surface mount
package while requiring few external components. To simplify audio system design, the KB4863 combines dual bridge
speaker amplifiers and stereo headphone amplifiers on one
chip.
The KB4863 features an externally controlled, low-power
consumption shutdown mode, a stereo headphone amplifier
mode, and thermal shutdown protection. It also utilizes circuitry to reduce “clicks and pops” during device turn-on.
Note 1: An KB4863MTE or KB4863LQ that has been properly mounted to
a circuit board will deliver 2.2W into 4Ω. The other package options for the
KB4863 will deliver 1.1W into 8Ω. See the Application Information sections
for further information concerning the KB4863MTE and KB4863LQ.
Note 2: An KB4863MTE or KB4863LQ that has been properly mounted to a
circuit board and forced-air cooled will deliver 2.5W into 3Ω.
Features
n
n
n
n
n
Stereo headphone amplifier mode
“Click and pop” suppression circuitry
Unity-gain stable
Thermal shutdown protection circuitry
SOIC, DIP, TSSOP and exposed-DAP TSSOP and LLP
packages
Applications
n Multimedia monitors
n Portable and desktop computers
n Portable televisions
Typical Application
Note: Pin out shown for DIP and SO packages. Refer to the Connection Diagrams for the pinout of the TSSOP, Exposed-DAP TSSOP, and Exposed-DAP
LLP packages.
Rev: 1.1
1/19
2005-12-05
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KB4863
Connection Diagrams
Top View
Order Number KB4863M, KB4863N
N16E for DIP
M16B for SO
Top View
Order Number KB4863MT
MTC20 for TSSOP
Top View
Order Number KB4863MTE
MXA20A for Exposed-DAP
TSSOP
Rev: 1.1
Top View
Order Number KB4863LQ
LQA24A for Exposed-DAP LLP
2/19
2005-12-05
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KB4863
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Absolute Maximum Ratings
(Note 3)
If Military/Aerospace specified devices are required,
please contact the Kingbor Semiconductor Sales Office/
Distributors for availability and specifications.
Supply Voltage
6.0V
Storage Temperature
Input Voltage
−65˚C to +150˚C
θJC (typ) — M16B
20˚C/W
θJA (typ) — M16B
80˚C/W
θJC (typ) — N16A
20˚C/W
θJA (typ) — N16A
63˚C/W
θJC (typ) — MTC20
20˚C/W
θJA (typ) — MTC20
80˚C/W
−0.3V to VDD
+0.3V
θJC (typ) — MXA20A
2˚C/W
θJA (typ) — MXA20A
41˚C/W (Note 7)
Power Dissipation (Note 4)
Internally limited
θJA (typ) — MXA20A
51˚C/W (Note 8)
ESD Susceptibility(Note 5)
2000V
θJA (typ) — MXA20A
90˚C/W(Note 9)
ESD Susceptibility (Note 6)
200V
θJC (typ) — LQ24A
3.0˚C/W
150˚C
θJA (typ) — LQ24A
42˚C/W (Note 10)
Junction Temperature
Solder Information
Small Outline Package
Vapor Phase (60 sec.)
215˚C
Infrared (15 sec.)
220˚C
Operating Ratings
Temperature Range
TMIN ≤ TA ≤ TMAX
See AN-450 “Surface Mounting and their Effects on
Product Reliablilty” for other methods of soldering
surface mount devices.
−40˚C ≤ TA ≤ 85˚C
2.0V ≤ VDD ≤ 5.5V
Supply Voltage
Thermal Resistance
Electrical Characteristics for Bridged-Mode Operation (Notes 3, 11)
The following specifications apply for VDD = 5V unless otherwise specified. Limits apply for TA = 25˚C.
Symbol
Parameter
Conditions
VOS
Output Offset Voltage
VIN = 0V
PO
Output Power (Note 15)
THD+N = 1%, f = 1kHz (Note 16)
KB4863MTE, R L = 3Ω
KB4863LQ, R L = 3Ω
KB4863
Typical
(Note 12)
Limit
(Note 13)
5
50
Units
(Limits)
mV (max)
2.5
2.5
W
W
KB4863MTE, R L = 4Ω
KB4863LQ, R L = 4Ω
2.2
2.2
W
W
KB4863, R L = 8Ω
1.1
1.0
W (min)
THD+N = 10%, f = 1kHz (Note 16)
KB4863MTE, R L = 3Ω
KB4863LQ, R L = 3Ω
Rev: 1.1
3/19
3.2
3.2
W
W
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Electrical Characteristics for Bridged-Mode Operation (Notes 3, 11)
(Continued)
The following specifications apply for VDD = 5V unless otherwise specified. Limits apply for TA = 25˚C.
Symbol
Parameter
Conditions
KB4863
Typical
(Note 12)
Limit
(Note 13)
2.7
2.7
KB4863MTE, R L = 4Ω
KB4863LQ, R L = 4Ω
KB4863, R L = 8Ω
THD+N = 1%, f = 1kHz, RL = 32Ω
Units
(Limits)
W
W
1.5
W
0.34
W
%
THD+N
Total Harmonic Distortion+Noise
20Hz ≤ f ≤ 20kHz, AVD = 2
KB4863MTE, R L = 4Ω, PO = 2W
KB4863LQ, R L = 4Ω, PO = 2W
0.3 0.3
KB4863, R L = 8Ω, PO = 1W
0.3
%
PSRR
Power Supply Rejection Ratio
VDD = 5V, VRIPPLE = 200mVRMS, RL = 8Ω,
CB = 1.0µF
67
dB
XTALK
Channel Separation
f = 1kHz, CB = 1.0µF
90
dB
SNR
Signal To Noise Ratio
VDD = 5V, PO = 1.1W, RL = 8Ω
98
dB
Electrical Characteristics for Single-Ended Operation (Notes 3, 4)
The following specifications apply for VDD = 5V unless otherwise specified. Limits apply for TA = 25˚C.
Symbol
Parameter
Conditions
KB4863
Typical
(Note 12)
Limit
(Note 13)
Units
(Limits)
VOS
Output Offset Voltage
VIN = 0V
5
50
mV (max)
PO
Output Power
THD+N = 0.5%, f = 1kHz, RL = 32Ω
85
75
mW (min)
THD+N = 1%, f = 1kHz, RL = 8Ω
340
mW
THD+N = 10%, f = 1kHz, RL = 8Ω
440
mW
THD+N
Total Harmonic Distortion+Noise
AV = −1, PO = 75mW, 20Hz ≤ f ≤ 20kHz,
RL = 32Ω
0.2
%
PSRR
Power Supply Rejection Ratio
CB = 1.0µF, VRIPPLE = 200mV
f = 1kHz
52
dB
RMS,
XTALK
Channel Separation
f = 1kHz, CB = 1.0µF
60
dB
SNR
Signal To Noise Ratio
VDD = 5V, PO = 340mW, RL = 8Ω
95
dB
Note 3: Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is
functional, but do not guarantee specific performance limits. Electrical Characteristics state DC and AC electrical specifications under particular test conditions which
guarantee specific performance limits. This assumes that the device is within the Operating Ratings. Specifications are not guaranteed for parameters where no limit
is given, however, the typical value is a good indication of device performance.
Note 4: The maximum power dissipation is dictated by TJMAX, θ JA, and the ambient temperature TA and must be derated at elevated temperatures. The maximum
allowable power dissipation is PDMAX = (TJMAX − T A)/θJA. For the KB4863, T JMAX = 150˚C. For the θJAs for different packages, please see the Application
Information section or the Absolute Maximum Ratings section.
Note 5: Human body model, 100 pF discharged through a 1.5 kΩ resistor.
Note 6: Machine model, 220 pF–240 pF discharged through all pins.
Note 7: The given θJA is for an KB4863 packaged in an MXA20A with the exposed−DAP soldered to an exposed 2in 2 area of 1oz printed circuit board copper.
Note 8: The given θJA is for an KB4863 packaged in an MXA20A with the exposed−DAP soldered to an exposed 1in 2 area of 1oz printed circuit board copper.
Note 9: The given θJA is for an KB4863 packaged in an MXA20A with the exposed-DAP not soldered to printed circuit board copper.
Note 10: The given θJA is for an KB4863 packaged in an LQA24A with the exposed−DAP soldered to an exposed 2in 2 area of 1oz printed circuit board copper.
Note 11: All voltages are measured with respect to the ground (GND) pins unless otherwise specified.
Note 12: Typicals are measured at 25˚C and represent the parametric norm.
Note 13: Limits are guaranteed to Kingbor’s AOQL (Average Outgoing Quality Level).
Note 14: The quiescent power supply current depends on the offset voltage when a practical load is connected to the amplifier.
Note 15: Output power is measured at the device terminals.
Note 16: When driving 3Ω or 4Ω and operating on a 5V supply, the KB4863LQ and KB4863MTE must be mounted to the circuit board that has a minimum of 2.5in 2
of exposed, uninterrupted copper area connected to the LLP package’s exposed DAP.
Rev: 1.1
4/19
2005-12-05
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KB4863
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Typical Performance Characteristics
MTE Specific Characteristics
Rev: 1.1
KB4863MTE
THD+N vs Output Power
KB4863MTE
THD+N vs Frequency
KB4863MTE
THD+N vs Output Power
KB4863MTE
THD+N vs Frequency
KB4863MTE
Power Dissipation vs Power Output
KB4863MTE
Power Derating Curve
5/19
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Typical Performance Characteristics
MTE Specific Characteristics (Continued)
KB4863MTE (Note 17)
Power Derating Curve
Note 17: This curve shows the KB4863MTE’s thermal dissipation ability at different ambient temperatures given these conditions:
500LFPM + JEDEC board: The part is soldered to a 1S2P 20-lead exposed-DAP TSSOP test board with 500 linear feet per minute of forced-air flow across it.
Board information - copper dimensions: 74x74mm, copper coverage: 100% (buried layer) and 12% (top/bottom layers), 16 vias under the exposed-DAP.
500LFPM + 2.5in2: The part is soldered to a 2.5in2, 1 oz. copper plane with 500 linear feet per minute of forced-air flow across it.
2.5in2: The part is soldered to a 2.5in2, 1oz. copper plane.
Not Attached: The part is not soldered down and is not forced-air cooled.
Non-MTE Specific Characteristics
Rev: 1.1
THD+N vs Frequency
THD+N vs Frequency
THD+N vs Frequency
THD+N vs Output Power
6/19
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Non-MTE Specific Characteristics
Rev: 1.1
(Continued)
THD+N vs Output Power
THD+N vs Output Power
THD+N vs Output Power
THD+N vs Frequency
THD+N vs Output Power
THD+N vs Frequency
7/19
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Non-MTE Specific Characteristics
Rev: 1.1
KB4863
(Continued)
Output Power vs
Load Resistance
Power Dissipation vs
Supply Voltage
Output Power vs
Supply Voltage
Output Power vs
Supply Voltage
Output Power vs
Supply Voltage
Output Power vs
Load Resistance
8/19
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Non-MTE Specific Characteristics
Rev: 1.1
(Continued)
Output Power vs
Load Resistance
Power Dissipation vs
Output Power
Dropout Voltage vs
Supply Voltage
Power Derating Curve
Power Dissipation vs
Output Power
Noise Floor
9/19
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Non-MTE Specific Characteristics
KB4863
(Continued)
Channel Separation
Channel Separation
Power Supply
Rejection Ratio
Open Loop
Frequency Response
Supply Current vs
Supply Voltage
Rev: 1.1
10/19
2005-12-05
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External Components Description
(Refer to Figure 1.)
Components
Functional Description
1.
Ri
The Inverting input resistance, along with Rf, set the closed-loop gain. Ri, along with Ci, form a high pass
filter with fc = 1/(2πRiCi).
2.
Ci
The input coupling capacitor blocks DC voltage at the amplifier’s input terminals. Ci, along with Ri, create a
highpass filter with fc = 1/(2πRiCi). Refer to the section, SELECTING PROPER EXTERNAL
COMPONENTS, for an explanation of determining the value of Ci.
3.
Rf
The feedback resistance, along with Ri, set the closed-loop gain.
4.
Cs
The supply bypass capacitor. Refer to the POWER SUPPLY BYPASSING section for information about
properly placing, and selecting the value of, this capacitor.
5.
CB
The capacitor, CB, filters the half-supply voltage present on the BYPASS pin. Refer to the SELECTING
PROPER EXTERNAL COMPONENTS section for information concerning proper placement and selecting
CB’s value.
Application Information
EXPOSED-DAP PACKAGE PCB MOUNTING
CONSIDERATIONS
The KB4863’s exposed-DAP (die attach paddle) packages
(MTE and LQ) provide a low thermal resistance between the
die and the PCB to which the part is mounted and soldered.
This allows rapid heat transfer from the die to the surrounding PCB copper traces, ground plane and, finally, surrounding air. The result is a low voltage audio power amplifier that
produces 2.2W at ≤ 1% THD with a 4Ω load. This high power
is achieved through careful consideration of necessary thermal design. Failing to optimize thermal design may compromise the KB4863’s high power performance and activate
unwanted, though necessary, thermal shutdown protection.
The MTE and LQ packages must have their DAPs soldered
to a copper pad on the PCB. The DAP’s PCB copper pad is
connected to a large plane of continuous unbroken copper.
This plane forms a thermal mass and heat sink and radiation
area. Place the heat sink area on either outside plane in the
case of a two-sided PCB, or on an inner layer of a board with
more than two layers. Connect the DAP copper pad to the
inner layer or backside copper heat sink area with 32(4x8)
(MTE) or 6(3x2) (LQ) vias. The via diameter should be
0.012in - 0.013in with a 1.27mm pitch. Ensure efficient thermal conductivity by plating-through and solder-filling the
vias.
Best thermal performance is achieved with the largest practical copper heat sink area. If the heatsink and amplifier
share the same PCB layer, a nominal 2.5in2 (min) area is
necessary for 5V operation with a 4Ω load. Heatsink areas
not placed on the same PCB layer as the KB4863 should be
5in2 (min) for the same supply voltage and load resistance.
The last two area recommendations apply for 25˚c ambient
temperature. Increase the area to compensate for ambient
temperatures above 25˚c. In systems using cooling fans, the
KB4863MTE can take advantage of forced air cooling. With
an air flow rate of 450 linear-feet per minute and a 2.5in2
exposed copper or 5.0in2 inner layer copper plane heatsink,
the KB4863MTE can continuously drive a 3Ω load to full
power. The KB4863LQ achieves the same output power
Rev: 1.1
11/19
level without forced air cooling. In all circumstances and
conditions, the junction temperature must be held below
150˚C to prevent activating the KB4863’s thermal shutdown
protection. The KB4863’s power de-rating curve in the Typical Performance Characteristics shows the maximum
power dissipation versus temperature. Example PCB layouts
for the exposed-DAP TSSOP and LLP packages are shown
in the Demonstration Board Layout section. Further detailed and specific information concerning PCB layout, fabrication, and mounting an LLP package is available from
Kingbor Semiconductor’s package Engineering Group.
When contacting them, ask for ’Preliminary Application Note
for the Assembly of the LLP Package on a Printed Circuit
Board, Revision A dated 11/24/05.’
PCB LAYOUT AND SUPPLY REGULATION
CONSIDERATIONS FOR DRIVING 3Ω AND 4Ω LOADS
Power dissipated by a load is a function of the voltage swing
across the load and the load’s impedance. As load impedance decreases, load dissipation becomes increasingly dependent on the interconnect (PCB trace and wire) resistance
between the amplifier output pins and the load’s connections. Residual trace resistance causes a voltage drop,
which results in power dissipated in the trace and not in the
load as desired. For example, 0.1Ω trace resistance reduces
the output power dissipated by a 4Ω load from 2.1W to 2.0W.
This problem of decreased load dissipation is exacerbated
as load impedance decreases. Therefore, to maintain the
highest load dissipation and widest output voltage swing,
PCB traces that connect the output pins to a load must be as
wide as possible.
Poor power supply regulation adversely affects maximum
output power. A poorly regulated supply’s output voltage
decreases with increasing load current. Reduced supply
voltage causes decreased headroom, output signal clipping,
and reduced output power. Even with tightly regulated supplies, trace resistance creates the same effects as poor
supply regulation. Therefore, making the power supply
traces as wide as possible helps maintain full output voltage
swing.
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Application Information
(Continued)
* Refer to the section Proper Selection of External Components, for a detailed discussion of CB size.
FIGURE 1. Typical Audio Amplifier Application Circuit
Pin out shown for DIP and SO packages. Refer to the Connection Diagrams for the pinout of the TSSOP,
Exposed-DAP TSSOP, and Exposed-DAP LLP packages.
BRIDGE CONFIGURATION EXPLANATION
As shown in Figure 1, the KB4863 consists of two pairs of
operational amplifiers, forming a two-channel (channel A and
channel B) stereo amplifier. (Though the following discusses
channel A, it applies equally to channel B.) External resistors
Rf and Ri set the closed-loop gain of Amp1A, whereas two
internal 20kΩ resistors set Amp2A’s gain at -1. The KB4863
drives a load, such as a speaker, connected between the two
amplifier outputs, -OUTA and +OUTA.
Figure 1 shows that Amp1A’s output serves as Amp2A’s
input. This results in both amplifiers producing signals identical in magnitude, but 180˚ out of phase. Taking advantage
of this phase difference, a load is placed between -OUTA
and +OUTA and driven differentially (commonly referred to
as ’bridge mode’). This results in a differential gain of
(1)
AVD = 2 x (Rf / Ri)
Bridge mode amplifiers are different from single-ended amplifiers that drive loads connected between a single amplifier’s output and ground. For a given supply voltage, bridge
mode has a distinct advantage over the single-ended configuration: its differential output doubles the voltage swing
across the load. This produces four times the output power
when compared to a single-ended amplifier under the same
conditions. This increase in attainable output power assumes that the amplifier is not current limited or that the
output signal is not clipped. To ensure minimum output signal clipping when choosing an amplifier’s closed-loop gain,
refer to the Audio Power Amplifier Design section.
Rev: 1.1
12/19
Another advantage of the differential bridge output is no net
DC voltage across the load. This is accomplished by biasing
channel A’s and channel B’s outputs at half-supply. This
eliminates the coupling capacitor that single supply,
single-ended amplifiers require. Eliminating an output coupling capacitor in a single-ended configuration forces a
single-supply amplifier’s half-supply bias voltage across the
load. This increases internal IC power dissipation and may
permanently damage loads such as speakers.
POWER DISSIPATION
Power dissipation is a major concern when designing a
successful single-ended or bridged amplifier. Equation (2)
states the maximum power dissipation point for a singleended amplifier operating at a given supply voltage and
driving a specified output load
(2)
PDMAX = (VDD)2 / (2π2 RL) Single-Ended
However, a direct consequence of the increased power delivered to the load by a bridge amplifier is higher internal
power dissipation for the same conditions.
The KB4863 has two operational amplifiers per channel. The
maximum internal power dissipation per channel operating in
the bridge mode is four times that of a single-ended amplifier. From Equation (3), assuming a 5V power supply and an
4Ω load, the maximum single channel power dissipation is
1.27W or 2.54W for stereo operation.
(3)
PDMAX = 4 x (VDD)2 / (2π2 RL) Bridge Mode
The LM4973’s power dissipation is twice that given by Equation (2) or Equation (3) when operating in the single-ended
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Application Information
(Continued)
mode or bridge mode, respectively. Twice the maximum
power dissipation point given by Equation (3) must not exceed the power dissipation given by Equation (4):
(4)
PDMAX’ = (TJMAX − TA) / θJA
The KB4863’s T JMAX = 150˚C. In the LQ (LLP) package
soldered to a DAP pad that expands to a copper area of 5in2
on a PCB, the KB4863’s θJA is 20˚C/W. In the MTE package
soldered to a DAP pad that expands to a copper area of 2in2
on a PCB , the KB4863’s θJA is 41˚C/W. At any given
ambient temperature TJ\A, use Equation (4) to find the maximum internal power dissipation supported by the IC packaging. Rearranging Equation (4) and substituting PDMAX for
PDMAX’ results in Equation (5). This equation gives the
maximum ambient temperature that still allows maximum
stereo power dissipation without violating the KB4863’s
maximum junction temperature.
(5)
TA = TJMAX − 2 x PDMAX θJA
For a typical application with a 5V power supply and an 4Ω
load, the maximum ambient temperature that allows maximum stereo power dissipation without exceeding the maximum junction temperature is approximately 99˚C for the LLP
package and 45˚C for the MTE package.
(6)
TJMAX = PDMAX θJA + TA
Equation (6) gives the maximum junction temperature TJMAX. If the result violates the KB4863’s 150˚C, reduce the
maximum junction temperature by reducing the power supply voltage or increasing the load resistance. Further allowance should be made for increased ambient temperatures.
The above examples assume that a device is a surface
mount part operating around the maximum power dissipation
point. Since internal power dissipation is a function of output
power, higher ambient temperatures are allowed as output
power or duty cycle decreases.
If the result of Equation (2) is greater than that of Equation
(3), then decrease the supply voltage, increase the load
impedance, or reduce the ambient temperature. If these
measures are insufficient, a heat sink can be added to
reduce θJA. The heat sink can be created using additional
copper area around the package, with connections to the
ground pin(s), supply pin and amplifier output pins. External,
solder attached SMT heatsinks such as the Thermalloy
7106D can also improve power dissipation. When adding a
heat sink, the θJA is the sum of θJC, θCS, and θSA. (θJC is the
junction−to−case thermal impedance, CS is the case−to−sink
thermal impedance, and θSAis the sink−to−ambient thermal
impedance.) Refer to the Typical Performance Characteristics curves for power dissipation information at lower output
power levels.
POWER SUPPLY BYPASSING
As with any power amplifier, proper supply bypassing is
critical for low noise performance and high power supply
rejection. Applications that employ a 5V regulator typically
use a 10µF in parallel with a 0.1µF filter capacitors to stabilize the regulator’s output, reduce noise on the supply line,
and improve the supply’s transient response. However, their
presence does not eliminate the need for a local 1.0µF
tantalum bypass capacitance connected between the
KB4863’s supply pins and ground. Do not substitute a ceramic capacitor for the tantalum. Doing so may cause oscillation in the output signal. Keep the length of leads and
traces that connect capacitors between the KB4863’s power
supply pin and ground as short as possible. Connecting a
Rev: 1.1
13/19
1µF capacitor, CB, between the BYPASS pin and ground
improves the internal bias voltage’s stability and improves
the amplifier’s PSRR. The PSRR improvements increase as
the bypass pin capacitor value increases. Too large, however, increases turn-on time and can compromise amplifier’s
click and pop performance. The selection of bypass capacitor values, especially CB, depends on desired PSRR requirements, click and pop performance (as explained in the section, Proper Selection of External Components), system
cost, and size constraints.
MICRO-POWER SHUTDOWN
The voltage applied to the SHUTDOWN pin controls the
KB4863’s shutdown function. Activate micro-power shutdown by applying VDD to the SHUTDOWN pin. When active,
the KB4863’s micro-power shutdown feature turns off the
amplifier’s bias circuitry, reducing the supply current. The
logic threshold is typically VDD/2. The low 0.7µA typical
shutdown current is achieved by applying a voltage that is as
near as VDD as possible to the SHUTDOWN pin. A voltage
thrat is less than VDD may increase the shutdown current.
There are a few ways to control the micro-power shutdown.
These include using a single-pole, single-throw switch, a
microprocessor, or a microcontroller. When using a switch,
connect an external 10kΩ pull-up resistor between the
SHUTDOWN pin and VDD. Connect the switch between the
SHUTDOWN pin and ground. Select normal amplifier operation by closing the switch. Opening the switch connects the
SHUTDOWN pin to VDD through the pull-up resistor, activating micro-power shutdown. The switch and resistor guarantee that the SHUTDOWN pin will not float. This prevents
unwanted state changes. In a system with a microprocessor
or a microcontroller, use a digital output to apply the control
voltage to the SHUTDOWN pin. Driving the SHUTDOWN pin
with active circuitry eliminates the pull up resistor.
TABLE 1. Logic level truth table for SHUTDOWN and
HP-IN Operation
SHUTDOWN
HP-IN PIN
OPERATIONAL MODE
Low
logic Low
Bridged amplifiers
Low
logic High
Single-Ended amplifiers
High
logic Low
Micro-power Shutdown
High
logic High
Micro-power Shutdown
HP-IN FUNCTION
Applying a voltage between 4V and VDD to the KB4863’s
HP-IN headphone control pin turns off Amp2A and Amp2B,
muting a bridged-connected load. Quiescent current consumption is reduced when the IC is in this single-ended
mode.
Figure 2 shows the implementation of the KB4863’s headphone control function. With no headphones connected to
the headphone jack, the R1-R2 voltage divider sets the
voltage applied to the HP-IN pin (pin 16) at approximately
50mV. This 50mV enables Amp1B and Amp2B, placing the
KB4863’s in bridged mode operation. The output coupling
capacitor blocks the amplifier’s half-supply DC voltage, protecting the headphones.
While the KB4863 operates in bridged mode, the DC potential across the load is essentially 0V. The HP-IN threshold is
set at 4V. Therefore, even in an ideal situation, the output
swing cannot cause a false single-ended trigger. Connecting
headphones to the headphone jack disconnects the head2005-12-05
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Application Information
(Continued)
phone jack contact pin from -OUTA and allows R1 to pull the
HP Sense pin up to VDD. This enables the headphone function, turns off Amp2A and Amp2B, and mutes the bridged
speaker. The amplifier then drives the headphones, whose
impedance is in parallel with resistor R2 and R3. These
resistors have negligible effect on the KB4863’s output drive
capability since the typical impedance of headphones is
32Ω.
FIGURE 2. Headphone Circuit
Figure 2 also shows the suggested headphone jack electrical connections. The jack is designed to mate with a
three-wire plug. The plug’s tip and ring should each carry
one of the two stereo output signals, whereas the sleeve
should carry the ground return. A headphone jack with one
control pin contact is sufficient to drive the HP-IN pin when
connecting headphones.
A microprocessor or a switch can replace the headphone
jack contact pin. When a microprocessor or switch applies a
voltage greater than 4V to the HP-IN pin, a bridge-connected
speaker is muted and Amp1A and Amp2A drive a pair of
headphones.
SELECTING PROPER EXTERNAL COMPONENTS
Optimizing the KB4863’s performance requires properly selecting external components. Though the KB4863 operates
well when using external components with wide tolerances,
best performance is achieved by optimizing component values.
The KB4863 is unity-gain stable, giving a designer maximum
design flexibility. The gain should be set to no more than a
given application requires. This allows the amplifier to
achieve minimum THD+N and maximum signal-to-noise ratio. These parameters are compromised as the closed-loop
gain increases. However, low gain demands input signals
with greater voltage swings to achieve maximum output
power. Fortunately, many signal sources such as audio CODECs have outputs of 1VRMS (2.83VP-P). Please refer to the
Audio Power Amplifier Design section for more information on selecting the proper gain.
Rev: 1.1
14/19
KB4863
Input Capacitor Value Selection
Amplifying the lowest audio frequencies requires high value
input coupling capacitor (Ci in Figure 1). A high value capacitor can be expensive and may compromise space efficiency
in portable designs. In many cases, however, the speakers
used in portable systems, whether internal or external, have
little ability to reproduce signals below 150Hz. Applications
using speakers with this limited frequency response reap
little improvement by using large input capacitor.
Besides effecting system cost and size, Ci has an affect on
the KB4863’s click and pop performance. When the supply
voltage is first applied, a transient (pop) is created as the
charge on the input capacitor changes from zero to a quiescent state. The magnitude of the pop is directly proportional
to the input capacitor’s size. Higher value capacitors need
more time to reach a quiescent DC voltage (usually VDD/2)
when charged with a fixed current. The amplifier’s output
charges the input capacitor through the feedback resistor,
Rf. Thus, pops can be minimized by selecting an input
capacitor value that is no higher than necessary to meet the
desired -3dB frequency.
A shown in Figure 1, the input resistor (RI) and the input
capacitor, CI produce a −3dB high pass filter cutoff frequency
that is found using Equation (7).
(7)
As an example when using a speaker with a low frequency
limit of 150Hz, CI, using Equation (4), is 0.063µF. The 1.0µF
CI shown in Figure 1 allows the KB4863 to drive high efficiency, full range speaker whose response extends below
30Hz.
Bypass Capacitor Value Selection
Besides minimizing the input capacitor size, careful consideration should be paid to value of CB, the capacitor connected to the BYPASS pin. Since CB determines how fast
the KB4863 settles to quiescent operation, its value is critical
when minimizing turn−on pops. The slower the KB4863’s
outputs ramp to their quiescent DC voltage (nominally 1/2
VDD), the smaller the turn−on pop. Choosing CB equal to
1.0µF along with a small value of Ci (in the range of 0.1µF to
0.39µF), produces a click-less and pop-less shutdown function. As discussed above, choosing Ci no larger than necessary for the desired bandwidth helps minimize clicks and
pops.
OPTIMIZING CLICK AND POP REDUCTION
PERFORMANCE
The KB4863 contains circuitry to minimize turn-on and shutdown transients or ’clicks and pop’. For this discussion,
turn-on refers to either applying the power supply voltage or
when the shutdown mode is deactivated. While the power
supply is ramping to its final value, the KB4863’s internal
amplifiers are configured as unity gain buffers. An internal
current source changes the voltage of the BYPASS pin in a
controlled, linear manner. Ideally, the input and outputs track
the voltage applied to the BYPASS pin. The gain of the
internal amplifiers remains unity until the voltage on the
bypass pin reaches 1/2 VDD. As soon as the voltage on the
BYPASS pin is stable, the device becomes fully operational.
Although the bypass pin current cannot be modified, changing the size of CB alters the device’s turn-on time and the
magnitude of ’clicks and pops’. Increasing the value of CB
reduces the magnitude of turn-on pops. However, this pre2005-12-05
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(Continued)
sents a tradeoff: as the size of CB increases, the turn-on time
increases. There is a linear relationship between the size of
CB and the turn-on time. Here are some typical turn-on times
for various values of CB:
CB
TON
0.01µF
20 ms
0.1µF
200 ms
0.22µF
440 ms
0.47µF
940 ms
1.0µF
2 Sec
NO LOAD STABILITY
The KB4863 may exhibit low level oscillation when the load
resistance is greater than 10kΩ. This oscillation only occurs
as the output signal swings near the supply voltages. Prevent this oscillation by connecting a 5kΩ between the output
pins and ground.
AUDIO POWER AMPLIFIER DESIGN
Audio Amplifier Design: Driving 1W into an 8Ω Load
The following are the desired operational parameters:
Load Impedance:
Input Level:
Input Impedance:
Bandwidth:
Thus, a minimum gain of 2.83 allows the KB4863’s to reach
full output swing and maintain low noise and THD+N performance. For this example, let AVD = 3.
The amplifier’s overall gain is set using the input (Ri) and
feedback (Rf) resistors. With the desired input impedance
set at 20kΩ, the feedback resistor is found using Equation
(11).
(11)
Rf/Ri = AVD/2
The value of Rf is 30kΩ.
The last step in this design example is setting the amplifier’s
−3dB frequency bandwidth. To achieve the desired ± 0.25dB
pass band magnitude variation limit, the low frequency response must extend to at least one−fifth the lower bandwidth
limit and the high frequency response must extend to at least
five times the upper bandwidth limit. The gain variation for
both response limits is 0.17dB, well within the ± 0.25dB
desired limit. The results are an
(12)
fL = 100Hz/5 = 20Hz
and an
(13)
FH = 20kHzx5 = 100kHz
As mentioned in the External Components section, Ri
and Ci create a highpass filter that sets the amplifier’s lower
bandpass frequency limit. Find the coupling capacitor’s
value using Equation (12).
1Wrms
8Ω
1Vrms
20kΩ
100Hz−20 kHz ± 0.25 dB
The design begins by specifying the minimum supply voltage
necessary to obtain the specified output power. One way to
find the minimum supply voltage is to use the Output Power
vs Supply Voltage curve in the Typical Performance Characteristics section. Another way, using Equation (4), is to
calculate the peak output voltage necessary to achieve the
desired output power for a given load impedance. To account for the amplifier’s dropout voltage, two additional voltages, based on the Dropout Voltage vs Supply Voltage in the
Typical Performance Characteristics curves, must be
added to the result obtained by Equation (8). The result in
Equation (9).
(8)
VDD ≥ (VOUTPEAK + (VODTOP + VODBOT))
(9)
The Output Power vs Supply Voltage graph for an 8Ω load
indicates a minimum supply voltage of 4.6V. This is easily
met by the commonly used 5V supply voltage. The additional
voltage creates the benefit of headroom, allowing the
KB4863 to produce peak output power in excess of 1W
Rev: 1.1
After satisfying the KB4863’s power dissipation requirements, the minimum differential gain is found using Equation
(10).
(10)
In order eliminate ’clicks and pops’, all capacitors must be
discharged before turn-on. Rapidly switching VDD may not
allow the capacitors to fully discharge, which may cause
’clicks and pops’. In a single-ended configuration, the output
is coupled to the load by COUT. This capacitor usually has a
high value. COUT discharges through internal 20kΩ resistors.
Depending on the size of COUT, the discharge time constant
can be relatively large. To reduce transients in single-ended
mode, an external 1kΩ - 5kΩ resistor can be placed in
parallel with the internal 20kΩ resistor. The tradeoff for using
this resistor is increased quiescent current.
Power Output:
without clipping or other audible distortion. The choice of
supply voltage must also not create a situation that violates
maximum power dissipation as explained above in the
Power Dissipation section.
15/19
the result is
(14)
1/(2π*20kΩ*20Hz) = 0.398µF
Use a 0.39µF capacitor, the closest standard value.
The product of the desired high frequency cutoff (100kHz in
this example) and the differential gain, AVD, determines the
upper passband response limit. With AVD = 3 and fH =
100kHz, the closed-loop gain bandwidth product (GBWP) is
300kHz. This is less than the KB4863’s 3.5MHz GBWP. With
this margin, the amplifier can be used in designs that require
more differential gain while avoiding performance-lrestricting
bandwidth limitations.
RECOMMENDED PRINTED CIRCUIT BOARD LAYOUT
Figures 3 through 6 show the recommended two-layer PC
board layout that is optimized for the 20-pin MTE-packaged
KB4863 and associated external components. Figures 7
through 11 show the recommended four-layer PC board
layout that is optimized for the 24-pin LQ-packaged KB4863
and associated external components. These circuits are designed for use with an external 5V supply and 4Ω speakers.
These circuit boards are easy to use. Apply 5V and ground to
the board’s VDD and GND pads, respectively. Connect 4Ω
speakers between the board’s -OUTA and +OUTA and
OUTB and +OUTB pads.
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Physical Dimensions
KB4863
inches (millimeters) unless otherwise noted
16-Lead (0.300" Wide) Molded Small Outline Package, JEDEC
Order Number KB4863M
Package Number M16B
16-Lead (0.300" Wide) Molded Dual-In-Line Package
Order Number KB4863N
Package Number N16E
Rev: 1.1
16/19
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Physical Dimensions
KB4863
inches (millimeters) unless otherwise noted (Continued)
20-Lead Molded PKG, TSSOP, JEDEC, 4.4mm BODY WIDTH
Order Number KB4863MT
Package Number MTC20
Rev: 1.1
17/19
2005-12-05
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Physical Dimensions
KB4863
inches (millimeters) unless otherwise noted (Continued)
20-Lead Molded TSSOP, Exposed Pad, 6.5x4.4x0.9mm
Order Number KB4863MTE
Package Number MXA20A
Rev: 1.1
18/19
2005-12-05
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Physical Dimensions
KB4863
inches (millimeters) unless otherwise noted (Continued)
24-Lead Molded pkg, Leadframe Package LLP
Order Number KB4863LQ
NS Package Number LQA24A
Rev: 1.1
19/19
2005-12-05