LM4702B [NSC]

LM4702 Overture Audio Power Amplifier Series Stereo High Fidelity 200 Volt* Driver with Mute; LM4702序曲音频功率放大器系列立体声高保真200伏*驱动器与静音
LM4702B
型号: LM4702B
厂家: National Semiconductor    National Semiconductor
描述:

LM4702 Overture Audio Power Amplifier Series Stereo High Fidelity 200 Volt* Driver with Mute
LM4702序曲音频功率放大器系列立体声高保真200伏*驱动器与静音

驱动器 放大器 功率放大器
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中文:  中文翻译
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September 2005  
LM4702 Overture® Audio Power Amplifier Series  
Stereo High Fidelity 200 Volt* Driver with Mute  
General Description  
Key Specifications  
The LM4702 is a high fidelity audio power amplifier driver  
designed for demanding consumer and pro-audio applica-  
tions. Amplifier output power may be scaled by changing the  
supply voltage and number of output devices. The LM4702  
is capable of delivering in excess of 300 watts per channel  
single ended into an 8 ohm load in the presence of 10% high  
line headroom and 20% supply regulation.  
j
Wide operating voltage range  
LM4702A (in development)  
LM4702B (in development)  
LM4702C  
20V to 85V  
20V to 80V  
20V to 75V  
3µV  
j
j
j
Equivalent Noise  
PSRR  
110dB (typ)  
0.001%  
The LM4702 includes thermal shut down circuitry that acti-  
vates when the die temperature exceeds 150˚C. The  
LM4702’s mute function, when activated, mutes the input  
drive signal and forces the amplifier output to a quiescent  
state.  
THD  
Features  
n Very high voltage operation  
n Scalable output power  
n Minimum external components  
n External compensation  
n Thermal Shutdown and Mute  
The LM4702 is available in 3 grades that span a wide range  
of applications and performance levels. The LM4702C is  
targeted at high volume applications. The LM4702B (in de-  
velopment) includes a higher voltage rating along with the  
tighter specifications. The LM4702A (in development) is the  
premium part with the highest voltage rating, fully specified  
with limits over voltage and temperature, and is offered in a  
military 883 compliant TO-3 package.  
Applications  
n AV receivers  
n Audiophile power amps  
n Pro Audio  
n High voltage industrial applications  
*
Tentative Max Operating voltage for the LM4702A,  
LM4702B (in development)  
Typical Application and Connection Diagrams  
20158302  
Plastic Package — 15 Lead TO-220  
(for LM4702; LM4702B, in development)  
20158320  
Metal Can — 15 Lead TO-3  
(for LM4702A, in development)  
20158319  
FIGURE 1. Typical Audio Amplifier Application Circuit  
SPiKe Protection and Overture are trademarks of National Semiconductor Corporation.  
© 2005 National Semiconductor Corporation  
DS201583  
www.national.com  
Typical Application and Connection Diagrams (Continued)  
20158319  
FIGURE 1. Typical Audio Amplifier Application Circuit  
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2
Connection Diagram  
Plastic Package (For B and C) (Note 13)  
20158301  
Top View  
Order Number LM4702T(B & C)  
See NS Package Number TA15A  
3
www.national.com  
Absolute Maximum Ratings (Notes 1,  
2)  
Storage Temperature  
-40˚C to +150˚C  
Thermal Resistance  
θJA  
θJC  
30˚C/W  
1˚C/W  
If Military/Aerospace specified devices are required,  
please contact the National Semiconductor Sales Office/  
Distributors for availability and specifications.  
Supply Voltage |V+| + |V-|  
Differential Input Voltage  
200V  
Operating Ratings (Notes 1, 2)  
Temperature Range  
+/-6V  
Common Mode Input Range  
Power Dissipation (Note 3)  
ESD Susceptibility (Note 4)  
ESD Susceptibility (Note 5)  
Junction Temperature (TJMAX) (Note 9)  
Soldering Information  
0.4 Vee to 0.4 Vcc  
TMIN TA TMAX  
Supply Voltage |V+| + |V-|  
LM4702A (in development)  
LM4702B (in development)  
LM4702C  
−20˚C TA +75˚C  
4W  
1.5kV  
200V  
+/-20V VTOTAL +/-85V  
+/-20V VTOTAL +/-80V  
+/-20V VTOTAL +/-75V  
150˚C  
T Package (10 seconds)  
260˚C  
Electrical Characteristics (LM4702C) Vcc = +75V, Vee = –75V (Notes 1, 2)  
The following specifications apply for IMUTE = 1.5mA, unless otherwise specified. Limits apply for TA = 25˚C.  
Symbol  
Parameter  
Conditions  
LM4702  
Typical Limit  
(Note 6) (Notes 7, 8)  
Units  
(Limits)  
ICC  
Total Quiescent Power Supply VCM = 0V, VO = 0V, IO = 0A  
Current  
25  
0.005  
50  
30  
mA (max)  
%
THD+N  
Total Harmonic Distortion +  
Noise  
No load, AV = 30dB  
@
VOUT = 14VRMS 1kHz  
RS  
Input Bias Resistor  
Closed Loop Voltage Gain  
Open Loop Gain  
100  
26  
k(max)  
dB (min)  
dB  
Av  
Av open  
Vom  
Vin = 1mVrms, f = 1KHz, C = 30pF  
THD = 0.05%, Freq = 20Hz to 20KHz  
93  
51  
Output Voltage Swing  
Vrms (min)  
µV (max)  
µV  
150  
90  
300  
Rs = 10k, LPF = 30kHz, Av = 30dB  
A-weighted  
Vnoise  
IOUT  
Output Noise  
Output Current  
Current from Source to Sink Pins  
To put part in “play” mode  
5.5  
3
10  
1
mA(min)  
mA (max)  
mA(min)  
mA (max)  
dB  
Imute  
Current into Mute Pin  
1.5  
2
@
XTALK  
SR  
Channel Separation (Note 11) f = 1kHz Av = 30dB  
85  
15  
Slew Rate  
VIN = 1.2VP-P, f = 10kHz square Wave,  
V/µs  
Outputs shorted  
VOS  
IB  
Input Offset Voltage  
Input Bias Current  
VCM = 0V, IO = 0mA  
VCM = 0V, IO = 0mA  
10  
35  
95  
mV (max)  
nA  
500  
110  
PSRR  
Power Supply Rejection Ratio Rs = 1k, f = 100Hz,  
Vripple = 1Vrms, Input Referred  
dB (min)  
Electrical Characteristics (LM4702C) Vcc = +50V, Vee = –50V (Notes 1, 2)  
The following specifications apply for IMUTE = 1.5mA, unless otherwise specified. Limits apply for TA = 25˚C.  
Symbol  
Parameter  
Conditions  
LM4702  
Typical Limit  
(Note 6) (Notes 7, 8)  
Units  
(Limits)  
ICC  
Total Quiescent Power Supply VCM = 0V, VO = 0V, IO = 0A  
Current  
22  
0.005  
50  
30  
mA (max)  
%
THD+N  
RS  
Total Harmonic Distortion +  
Noise  
No load, AV = 30dB  
@
VOUT = 10VRMS 1kHz  
Input Bias Resistor  
100  
k(max)  
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4
Electrical Characteristics (LM4702C) Vcc = +50V, Vee = –50V (Notes 1,  
2) (Continued)  
The following specifications apply for IMUTE = 1.5mA, unless otherwise specified. Limits apply for TA = 25˚C.  
Symbol  
Parameter  
Conditions  
LM4702  
Typical Limit  
Units  
(Limits)  
(Note 6) (Notes 7, 8)  
Av  
Closed Loop Voltage Gain  
Open Loop Gain  
26  
dB (min)  
dB  
Av open  
Vom  
Vin = 1mVrms, f = 1KHz, C = 30pF  
THD = 0.05%, Freq = 20Hz to 20KHz  
93  
33  
Output Voltage Swing  
Vrms (min)  
µV (max)  
µV  
150  
90  
300  
Rs = 10k, LPF = 30kHz, Av = 30dB  
A-weighted  
Vnoise  
Output Noise  
3
10  
1
mA(min)  
mA (max)  
mA(min)  
mA (max)  
dB  
IOUT  
Imute  
Output Current  
Outputs Shorted  
5.2  
1.5  
Current into Mute Pin  
To put part in “play” mode  
2
XTALK  
SR  
Channel Separation (Note 11) f = 1kHz at Av = 30dB  
85  
15  
Slew Rate  
VIN = 1.2VP-P, f = 10kHz square Wave,  
V/µs  
Outputs shorted  
VOS  
IB  
Input Offset Voltage  
Input Bias Current  
VCM = 0V, IO = 0mA  
VCM = 0V, IO = 0mA  
10  
35  
95  
mV (max)  
nA  
500  
110  
PSRR  
Power Supply Rejection Ratio Rs = 1k, f = 100Hz,  
Vripple = 1Vrms, Input Referred  
dB (min)  
Electrical Characteristics (LM4702B) Vcc = +80V, Vee = –80V (Pre-release  
information) (Notes 1, 2)  
The following specifications apply for IMUTE = 1.5mA, unless otherwise specified. Limits apply for TA = 25˚C.  
Symbol  
Parameter  
Conditions  
LM4702  
Typical Limit  
(Note 6) (Notes 7, 8)  
Units  
(Limits)  
ICC  
Total Quiescent Power Supply VCM = 0V, VO = 0V, IO = 0A  
Current  
27  
0.003  
50  
TBD  
mA (max)  
% (max)  
THD+N  
Total Harmonic Distortion +  
Noise  
No load, AV = 30dB  
TBD  
@
VOUT = 20VRMS 1kHz  
RS  
Input Bias Resistor  
Closed Loop Voltage Gain  
Open Loop Gain  
TBD  
TBD  
k(max)  
dB (min)  
dB  
Av  
Av open  
Vom  
Vnoise  
Vin = 1mVrms, f = 1KHz, C = 30pF  
THD = 0.05%, Freq = 20Hz to 20KHz  
Rs = 10k, LPF = 30kHz, Av = 30dB  
A-weighted  
93  
54  
Output Voltage Swing  
Output Noise  
TBD  
TBD  
TBD  
TBD  
TBD  
TBD  
TBD  
TBD  
TBD  
Vrms (min)  
150  
90  
µV (max)  
mA(min)  
mA (max)  
mA(min)  
IOUT  
Imute  
Output Current  
Outputs Shorted  
5.5  
1.5  
Current into Mute Pin  
To put part in “play” mode  
mA (max)  
dB (min)  
V/µs (min)  
XTALK  
SR  
Channel Separation (Note 11) f = 1kHz at Av = 30dB  
85  
17  
Slew Rate  
VIN = 1.2VP-P, f = 10kHz square Wave,  
Outputs shorted  
VOS  
IB  
Input Offset Voltage  
Input Bias Current  
VCM = 0V, IO = 0mA  
VCM = 0V, IO = 0mA  
7
TBD  
TBD  
TBD  
mV (max)  
nA (max)  
dB (min)  
350  
110  
PSRR  
Power Supply Rejection Ratio Rs = 1k, f = 100Hz,  
Vripple = 1Vrms, Input Referred  
5
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Electrical Characteristics (LM4702A) Vcc = +85V, Vee = –85V (Pre-release  
information) (Notes 1, 2)  
The following specifications apply for IMUTE = 1.5mA, unless otherwise specified. Limits apply for TA = 25˚C.  
Symbol  
Parameter  
Conditions  
LM4702  
Typical Limit  
(Note 6) (Notes 7, 8)  
Units  
(Limits)  
ICC  
Total Quiescent Power Supply VCM = 0V, VO = 0V, IO = 0A  
Current  
27  
0.001  
50  
TBD  
mA (max)  
% (max)  
THD+N  
Total Harmonic Distortion +  
Noise  
No load, AV = 30dB  
TBD  
@
VOUT = 20VRMS 1kHz  
RS  
Input Bias Resistor  
Closed Loop Voltage Gain  
Open Loop Gain  
TBD  
TBD  
k(max)  
dB (min)  
dB  
Av  
Av open  
Vom  
Vnoise  
Vin = 1mVrms, f = 1KHz, C = 30pF  
THD = 0.05%, Freq = 20Hz to 20KHz  
Rs = 10k, LPF = 30kHz, Av = 30dB  
A-weighted  
93  
57  
Output Voltage Swing  
Output Noise  
TBD  
TBD  
TBD  
TBD  
TBD  
TBD  
TBD  
TBD  
TBD  
Vrms (min)  
100  
80  
µV (max)  
mA(min)  
mA (max)  
mA(min)  
IOUT  
Imute  
Output Current  
Outputs Shorted  
5.5  
1.5  
Current into Mute Pin  
To put part in “play” mode  
mA (max)  
dB (min)  
V/µs (min)  
XTALK  
SR  
Channel Separation (Note 11) f = 1kHz at Av = 30dB  
90  
Slew Rate  
VIN = 1.2VP-P, f = 10kHz square Wave,  
TBD  
Outputs shorted  
VOS  
IB  
Input Offset Voltage  
Input Bias Current  
VCM = 0V, IO = 0mA  
VCM = 0V, IO = 0mA  
5
TBD  
TBD  
TBD  
mV (max)  
nA (max)  
dB (min)  
150  
110  
PSRR  
Power Supply Rejection Ratio Rs = 1k, f = 100Hz,  
Vripple = 1Vrms, Input Referred  
Note 1: All voltages are measured with respect to the ground pins, unless otherwise specified.  
Note 2: 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 condition 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’s performance.  
Note 3: The maximum power dissipation must be de-rated at elevated temperatures and is dictated by T  
, θ , and the ambient temperature T . The maximum  
A
JMAX JC  
allowable power dissipation is P  
= (T  
-T )/θ or the number given in the Absolute Maximum Ratings, whichever is lower. For the LM4702, T  
= 150˚C  
DMAX  
JMAX  
A
JC  
JMAX  
and the typical θ is 1˚C/W. Refer to the Thermal Considerations section for more information.  
JC  
Note 4: Human body model, 100pF discharged through a 1.5kresistor.  
Note 5: Machine Model: a 220pF - 240pF discharged through all pins.  
Note 6: Typical specifications are measured at 25˚C and represent the parametric norm.  
Note 7: Tested limits are guaranteed to National’s AOQL (Average Outgoing Quality Level).  
Note 8: Datasheet min/max specification limits are guaranteed by design, test, or statistical analysis.  
Note 9: The maximum operating junction temperature is 150˚C.  
Note 10: PCB layout will affect cross talk. It is recommended that input and output traces be separated by as much distance as possible. Return ground traces from  
outputs should be independent back to a single ground point and use as wide of traces as possible.  
Note 11: The TA15A is a non-isolated package. The package’s metal back and any heat sink to which it is mounted are connected to the Vee potential when using  
only thermal compound. If a mica washer is used in addition to thermal compound, θ (case to sink) is increased, but the heat sink will be electrically isolated from  
CS  
Vee.  
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6
Typical Performance Characteristics for LM4702C  
THD+N vs Output Voltage  
THD+N vs Output Voltage  
VDD  
=
50V, f = 1kHz, outputs shorted  
VDD  
=
75V, f = 1kHz, outputs shorted  
20158308  
20158338  
THD+N vs Frequency  
THD+N vs Frequency  
VDD  
=
50V, VOUT = 10Vrms, outputs shorted  
VDD  
=
75V, VOUT = 14Vrms, outputs shorted  
20158310  
20158339  
Crosstalk vs Frequency  
Crosstalk vs Frequency  
VDD  
=
50V  
VDD  
=
75V  
20158335  
20158336  
7
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Typical Performance Characteristics for LM4702C (Continued)  
+PSRR vs Frequency  
50V, RS = 1k, Ripple on VCC  
−PSRR vs Frequency  
VDD = 50V, RS = 1k, Ripple on Vee  
VDD  
=
20158331  
20158333  
+PSRR vs Frequency  
−PSRR vs Frequency  
VDD  
=
75V, RS = 1k, Ripple on VCC  
VDD  
=
75V, RS = 1k, Ripple on Vee  
20158332  
20158334  
Open Loop and Phase  
Upper-Phase, Lower-Gain  
20158337  
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8
Test Circuit  
20158303  
FIGURE 1.  
9
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Application Information  
MUTE FUNCTION  
The thermal resistance from the die to the outside air, θJA  
(junction to ambient), is a combination of three thermal re-  
sistances, θJC (junction to case), θCS (case to sink), and θSA  
(sink to ambient). The thermal resistance, θJC (junction to  
case), of the LM4702T is 0.8˚C/W. Using Thermalloy Ther-  
macote thermal compound, the thermal resistance, θCS  
(case to sink), is about 0.2˚C/W. Since convection heat flow  
(power dissipation) is analogous to current flow, thermal  
resistance is analogous to electrical resistance, and tem-  
perature drops are analogous to voltage drops, the power  
dissipation out of the LM4702 is equal to the following:  
The mute function of the LM4702 is controlled by the amount  
of current that flows into the mute pin. If there is less than  
1mA of current flowing into the mute pin, the part will be in  
mute. This can be achieved by shorting the mute pin to  
ground or by floating the mute pin. If there is between 1mA  
and 2mA of current flowing into the mute pin, the part will be  
in “play” mode. This can be done by connecting a power  
supply (Vmute) to the mute pin through a resistor (Rm). The  
current into the mute pin can be determined by the equation  
Imute = (Vmute – 2.9) / Rm. For example, if a 5V power  
supply is connected through a 1.4k resistor to the mute pin,  
then the mute current will be 1.5mA, at the center of the  
specified range. It is also possible to use Vcc as the power  
supply for the mute pin, though Rm will have to be recalcu-  
lated accordingly. It is not recommended to flow more than  
2mA of current into the mute pin because damage to the  
LM4702 may occur.  
PDMAX = (TJMAX−TAMB) / θJA  
(1)  
where TJMAX = 150˚C, TAMB is the system ambient tempera-  
ture and θJA = θJC + θCS + θSA  
.
It is highly recommended to switch between mute and “play”  
modes rapidly. This is accomplished most easily through  
using a toggle switch that alternatively connects the mute pin  
through a resistor to either ground or the mute pin power  
supply. Slowly increasing the mute current may result in  
undesired voltages on the outputs of the LM4702, which can  
damage an attached speaker.  
20158355  
Once the maximum package power dissipation has been  
calculated using equation 2, the maximum thermal resis-  
tance, θSA, (heat sink to ambient) in ˚C/W for a heat sink can  
be calculated. This calculation is made using equation 4  
which is derived by solving for θSA in equation 3.  
THERMAL PROTECTION  
The LM4702 has a sophisticated thermal protection scheme  
to prevent long-term thermal stress of the device. When the  
temperature on the die exceeds 150˚C, the LM4702 shuts  
down. It starts operating again when the die temperature  
drops to about 145˚C, but if the temperature again begins to  
rise, shutdown will occur again above 150˚C. Therefore, the  
device is allowed to heat up to a relatively high temperature  
if the fault condition is temporary, but a sustained fault will  
cause the device to cycle in a Schmitt Trigger fashion be-  
tween the thermal shutdown temperature limits of 150˚C and  
145˚C. This greatly reduces the stress imposed on the IC by  
thermal cycling, which in turn improves its reliability under  
sustained fault conditions.  
θSA = [(TJMAX−TAMB)−PDMAX(θJC +θCS)] / PDMAX (2)  
Again it must be noted that the value of θSA is dependent  
upon the system designer’s amplifier requirements. If the  
ambient temperature that the audio amplifier is to be working  
under is higher than 25˚C, then the thermal resistance for the  
heat sink, given all other things are equal, will need to be  
smaller.  
PROPER SELECTION OF EXTERNAL COMPONENTS  
Proper selection of external components is required to meet  
the design targets of an application. The choice of external  
component values that will affect gain and low frequency  
response are discussed below.  
Since the die temperature is directly dependent upon the  
heat sink used, the heat sink should be chosen so that  
thermal shutdown is not activated during normal operation.  
Using the best heat sink possible within the cost and space  
constraints of the system will improve the long-term reliability  
of any power semiconductor device, as discussed in the  
Determining the Correct Heat Sink section.  
The gain of each amplifier is set by resistors Rf and Ri for the  
non-inverting configuration shown in Figure 1. The gain is  
found by Equation (3) below:  
AV = 1 + Rf / Ri (V/V)  
(3)  
POWER DISSIPATION AND HEAT SINKING  
For best noise performance, lower values of resistors are  
used. A value of 1kis commonly used for Ri and then  
setting the value of Rf for the desired gain. For the LM4702  
the gain should be set no lower than 26dB. Gain settings  
below 26dB may experience instability.  
When in “play” mode, the LM4702 draws a constant amount  
of current, regardless of the input signal amplitude. Conse-  
quently, the power dissipation is constant for a given supply  
voltage and can be computed with the equation PDMAX = Icc  
* (Vcc – Vee). For a quick calculation of PDMAX, approximate  
the current to be 25mA and multiply it by the total supply  
voltage (the current varies slightly from this value over the  
operating range).  
The combination of Ri with Ci (see Figure 1) creates a high  
pass filter. The low frequency response is determined by  
these two components. The -3dB point can be found from  
Equation (4) shown below:  
fi = 1 / (2πRiCi) (Hz)  
(4)  
DETERMINING THE CORRECT HEAT SINK  
If an input coupling capacitor is used to block DC from the  
inputs as shown in Figure 5, there will be another high pass  
filter created with the combination of CIN and RIN. When  
using a input coupling capacitor RIN is needed to set the DC  
The choice of a heat sink for a high-power audio amplifier is  
made entirely to keep the die temperature at a level such  
that the thermal protection circuitry is not activated under  
normal circumstances.  
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10  
One of the recommended methods of preventing thermal  
runaway is to use a heat sink on the bipolar output transis-  
tors. This will keep the temperature of the transistors lower.  
A second recommended method is to use emitter degenera-  
tion resistors (see Re1, Re2, Re3, Re4 in Figure 1). As  
current increases, the voltage across the emitter degenera-  
tion resistor also increases, which decreases the voltage  
across the base and emitter. This mechanism helps to limit  
the current and counteracts thermal runaway.  
Application Information (Continued)  
bias point on the amplifier’s input terminal. The resulting  
-3dB frequency response due to the combination of CIN and  
RIN can be found from Equation (5) shown below:  
fIN = 1 / (2πRINCIN) (Hz)  
(5)  
With large values of RIN oscillations may be observed on the  
outputs when the inputs are left floating. Decreasing the  
value of RIN or not letting the inputs float will remove the  
oscillations. If the value of RIN is decreased then the value of  
CIN will need to increase in order to maintain the same -3dB  
frequency response.  
A third recommended method is to use a “Vbe multiplier” to  
bias the bipolar output stage (see Figure 1). The Vbe multi-  
plier consists of a bipolar transistor (Qmult, see Figure 1)  
and two resistors, one from the base to the collector (Rb2,  
Rb4, see Figure 1) and one from the base to the emitter  
(Rb1, Rb3, see Figure 1). The voltage from the collector to  
the emitter (also the bias voltage of the output stage) is  
Vbias = Vbe(1+Rb2/Rb1), which is why this circuit is called  
the Vbe multiplier. When Vbe multiplier transistor (Qmult,  
see Figure 1) is mounted to the same heat sink as the bipolar  
output transistors, its temperature will track that of the output  
transistors. Its Vbe is dependent upon temperature as well,  
and so it will draw more current as the output transistors heat  
it up. This will limit the base current into the output transis-  
tors, which counteracts thermal runaway.  
AVOIDING THERMAL RUNAWAY WHEN USING  
BIPOLAR OUTPUT STAGES  
When using a bipolar output stage with the LM4702 (as in  
Figure 1), the designer must beware of thermal runaway.  
Thermal runaway is a result of the temperature dependence  
of Vbe (an inherent property of the transistor). As tempera-  
ture increases, Vbe decreases. In practice, current flowing  
through a bipolar transistor heats up the transistor, which  
lowers the Vbe. This in turn increases the current again, and  
the cycle repeats. If the system is not designed properly, this  
positive feedback mechanism can destroy the bipolar tran-  
sistors used in the output stage.  
11  
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LM4702 Demo Board Artwork  
Top Overlay  
20158330  
Top Layer  
20158329  
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12  
LM4702 Demo Board Artwork (Continued)  
Bottom Layer  
20158328  
13  
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Revision History  
Rev  
Date  
Description  
1.0  
8/18/05  
Input corrected data under the Typical  
and Limit columns on all the 4 EC tables  
(per Kevin H.).  
1.1  
8/22/05  
Changed limits back on LM4702A/B/C to  
85V/80V/75V respectively (under Key  
Spec...)  
1.2  
1.3  
8/31/05  
9/2/05  
First WEB released of the datasheet.  
Due to miscommunication with the ASSY  
plant (EM), the datasheet needs to be  
taken off the WEB for now (per Robin  
Simpson).  
1.4  
9/09/05  
Taken out Limits on Vom (under the  
+75V and +50V.. LM4702C EC tables),  
then released D/S to the WEB (per Robin  
Simpson).  
1.5  
1.6  
9/14/05  
9/15/05  
Changed TM to R ( Overture R) in the  
doc title (per Kevin C), Naomi Mitchell  
called Kevin about it.  
Re-released D/S to the WEB with  
Overture “R”.  
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14  
Physical Dimensions inches (millimeters) unless otherwise noted  
Non-Isolated TO-220 15-Lead Package  
Order Number LM4702T(B&C)  
NS Package Number TA15A  
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