NSC LM390N

LM390 1W Battery Operated Audio Power Amplifier
General Description
The LM390 Power Audio Amplifier is optimized for 6V, 7.5V,
9V operation into low impedance loads. The gain is internally set at 20 to keep the external part count low, but the
addition of an external resistor and capacitor between pins
2 and 6 wil increase the gain to any value up to 200. The
inputs are ground referenced while the output is automatically biased to one half the supply voltage.
Y
Y
Y
Y
Applications
Y
Y
Y
Features
Y
Y
Y
Y
Y
Y
Battery operation
1W output power
Minimum external parts
Excellent supply rejection
Ground referenced input
Self-centering output quiescent voltage
Variable voltage gain
Low distortion
Fourteen pin dual-in-line package
Y
Y
Y
Y
Y
AM-FM radio amplifiers
Portable tape player amplifiers
Intercoms
TV sound systems
Lamp drivers
Line drivers
Ultrasonic drivers
Small servo drivers
Power converters
Equivalent Schematic and Connection Diagrams
Dual-In-Line Package
TL/H/7848 – 2
Order Number LM390N
See NS Package Number N14A
TL/H/7848 – 1
C1995 National Semiconductor Corporation
TL/H/7848
RRD-B30M115/Printed in U. S. A.
LM390 1W Battery Operated Audio Power Amplifier
April 1995
Absolute Maximum Ratings
Operating Temperature
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales
Office/Distributors for availability and specifications.
Supply Voltage
Package Dissipation 14-Pin DIP (Note 1)
Input Voltage
Storage Temperature
10V
8.3W
g 0.4V
0§ C to a 70§ C
Junction Temperature
150§ C
Lead Temperature (Soldering, 10 sec.)
Thermal Resistance
iJC
iJA
260§ C
30§ C/W
79§ C/W
b 65§ C to a 150§ C
Electrical Characteristics TA e 25§ C, (Figure 1)
Symbol
VS
Parameter
Conditions
Operating Supply Voltage
Min
Typ
4
Units
9
V
20
mA
30
dB
dB
IQ
Quiescent Current
VS e 6V, VIN e 0
POUT
Output Power
VS e 6V, RL e 4X, THD e 10%
0.8
1.0
AV
Voltage Gain
VS e 6V, f e 1 kHz
10 mF from Pin 2 to 6
23
26
46
BW
Bandwidth
VS e 6V, Pins 2 and 6 Open
300
THD
Total Harmonic Distortion
VS e 6V, RL e 4X, POUT e 500 mW
f e 1 kHz, Pins 2 and 6 Open
0.2
PSRR
Power Supply Rejection Ratio
VS e 6V, f e 1 kHz, CBYPASS e 10 mF,
Pins 2 and 6 Open, Referred to Output
(Note 2)
50
dB
50
kX
250
nA
RIN
Input Resistance
IBIAS
Input Bias Current
10
Max
10
VS e 6V, Pins 7 and 8 Open
W
kHz
1
%
Note 1: Pins 3, 4, 5, 10, 11, 12 at 25§ C. Above 25§ C case, derate at 15§ C/W junction to case, or 85§ C/W junction to ambient.
Note 2: If load and bypass capacitor are returned to VS (Figure 2) , rather than ground (Figure 1) , PSRR is typically 30 dB.
Typical Performance Characteristics
Maximum Device Dissipation
vs Ambient Temperature
Quiescent Supply Current vs
Supply Voltage
Power Supply Rejection Ratio
(Referred to the Output) vs
Frequency
Peak-to-Peak Output Voltage
Swing vs Supply Voltage
Voltage Gain vs Frequency
Distortion vs Frequency
TL/H/7848 – 5
2
Typical Performance Characteristics
Distortion vs Output Power
(Continued)
Device Dissipation vs
Output Power 4X Load
Device Dissipation vs
Output Power 8X Load
TL/H/7848 – 6
Application Hints
bypass the unused input, preventing degradation of gain
and possible instabilities. This is done with a 0.1 mF capacitor or a short to ground depending on the dc source resistance on the driven input.
Gain Control
To make the LM390 a more versatile amplifier, two pins (2
and 6) are provided for gain control. With pins 2 and 6 open,
the 1.35 kX resistor sets the gain at 20 (26 dB). If a capacitor is put from pin 2 to 6, bypassing the 1.35 kX resistor, the
gain will go up to 200 (46 dB). If a resistor is placed in series
with the capacitor, the gain can be set to any value from 20
to 200. A low frequency pole in the gain response is caused
by the capacitor working against the external resistor in series with the 150X internal resistor. If the capacitor is eliminated and a resistor connects pin 2 to 6 then the output dc
level may shift due to the additional dc gain. Gain control
can also be done by capacitively coupling a resistor (or
FET) from pin 6 to ground, as in Figure 7 .
Additional external components can be placed in parallel
with the internal feedback resistors to tailor the gain and
frequency response for individual applications. For example,
we can compensate poor speaker bass response by frequency shaping the feedback path. This is done with a series RC from pin 6 to 13 (paralleling the internal 15 kX resistor). For 6 dB effective bass boost: R j 15 kX, the lowest
value for good stable operation is R e 10 kX if pin 2 is
open. If pins 2 and 6 are bypassed then R as low as 2 kX
can be used. This restriction is because the amplifier is only
compensated for closed-loop gains greater than 9 V/V.
Bootstrapping
The base of the output transistor of the LM390 is brought
out to pin 9 for Bootstrapping. The output stage of the amplifier during positive swing is shown in Figure 3 with its
external circuitry.
R1 a R2 set the amount of base current available to the
output transistor. The maximum output current divided by
beta is the value required for the current in R1 and R2:
(R1 a R2) e bO
(VS/2) b VBE
IO MAX
Good design values are VBE e 0.7V and bO e 100.
Example 0.8 watt into 4X load with VS e 6V.
2 PO
e 632 mA
IO MAX e
RL
(6/2) b 0.7
e 364X
(R1 a R2) e 100
0.632
0
#
J
To keep the current in R2 constant during positive swing
capacitor CB is added. As the output swings positive CB lifts
R1 and R2 above the supply, maintaining a constant voltage
across R2. To minimize the value of CB, R1 e R2. The pole
due to CB and R1 and R2 is usually set equal to the pole
due to the output coupling capacitor and the load. This
gives:
Input Biasing
The schematic shows that both inputs are biased to ground
with a 50 kX resistor. The base current of the input transistors is about 250 nA, so the inputs are at about 12.5 mV
when left open. If the dc source resistance driving the
LM390 is higher than 250 kX it will contribute very little
additional offset (about 2.5 mV at the input, 50 mV at the
output). If the dc source resistance is less than 10 kX, then
shorting the unused input to ground will keep the offset low
(about 2.5 mV at the input 50 mV at the output). For dc
source resistances between these values we can eliminate
excess offset by putting a resistor from the unused input to
ground, equal in value to the dc source resistance. Of
course all offset problems are eliminated if the input is capacitively coupled.
When using the LM390 with higher gains (bypassing the
1.35 kX resistor between pins 2 and 6) it is necessary to
4Cc
C
j c
bO
25
Example: for 100 Hz pole and RL e 4X; Cc e 400 mF and
CB e 16 mF, if R1 is made a diode and R2 increased to give
the same current, CB can be decreased by about a factor of
4, as in Figure 4 .
For reduced component count the load can replace R1. The
value of (R1 a R2) is the same, so R2 is increased. Now CB
is both the coupling and the bootstrapping capacitor (see
Figure 2 ).
CB j
3
Typical Applications
TL/H/7848 – 4
TL/H/7848 – 3
FIGURE 2. Load Returned to Supply
(Amplifier with Gain e 20)
FIGURE 1. Load Returned to Ground
(Amplifier with Gain e 20)
TL/H/7848 – 7
FIGURE 3
TL/H/7848 – 8
FIGURE 4. Amplifier with Gain e 200 and Minimum CB
FIGURE 5. 2.5W Bridge Amplifier
4
TL/H/7848 – 9
Typical Applications (Continued)
TL/H/7848 – 11
TL/H/7848 – 10
FIGURE 6(b). Frequency Response
with Bass Boost
FIGURE 6(a). Amplifier with Bass Boost
FIGURE 7. Intercom
TL/H/7848 – 12
TL/H/7848 – 13
FIGURE 8. AM Radio Power Amplifier
Note 1: Twist supply lead and supply ground very tightly.
Note 4: R1C1 band limits input signals.
Note 2: Twist speaker lead and ground very tightly.
Note 5: All components must be spaced very close to IC.
Note 3: Ferrite bead is Ferroxcube K5-001-001/3B with 3 turns of wire.
5
LM390 1W Battery Operated Audio Power Amplifier
Physical Dimensions inches (millimeters)
Molded Dual-In-Line Package (N)
Order Number LM390N
See NS Package Number N14A
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