ETC TDA2030A

TDA2030A
LINEAR INTEGRATED CIRCUIT
14W HI-FI AUDIO AMPLIFIER
DESCRIPTION
The Contek TDA2030A is a monolithic audio power amplifier
integrated circuit.
1
FEATURES
*Very low external component required.
*High current output and high operating voltage.
*Low harmonic and crossover distortion.
*Built-in Over temperature protection.
*Short circuit protection between all pins.
*Safety Operating Area for output transistors.
TO-220B
PIN CONFIGURATIONS
1
2
3
4
5
Non inverting input
Inverting input
-VS
Output
+VS
ABSOLUTE MAXIMUM RATINGS (Ta=25
C)
PARAMETER
SYMBOL
VALUE
UNIT
Supply Voltage
Input Voltage
Differential Input Voltage
Peak Output Current(internally limited)
Total Power Dissipation at Tcase=90 C
Storage Temperature
Junction Temperature
Vs
Vi
Vdi
Io
Ptot
Tstg
Tj
+-12
Vs
+-15
3.5
20
-40~+150
-40~+150
V
V
V
A
W
C
C
ELECTRICAL CHARACTERISTICS(Refer to the test circuit, Vs =+-16V,Ta=25
PARAMETER
SYMBOL
Supply Voltage
Quiescent Drain
Current
Input Bias Current
Input Offset Voltage
Input Offset Current
Vs
Id
Ib
Vos
Ios
TEST CONDITIONS
MIN
MAX
UNIT
50
+-22
80
V
mA
0.2
+-2
+-20
2
+-20
+-200
mA
mV
nA
+-6
Vs=+-18v
C)
TYP
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1
TDA2030A
(Continued)
Output Power
Power Bandwidth
Open loop voltage
Gain
Closed Loop
Voltage Gain
Total harmonic
distortion
Total harmonic
Distortion
Second Order CCIF
Intermodulation
distortion
Third Order CCIF
Intermodulation
Distortion
Input Noise Voltage
Input Noise Voltage
Input Noise Current
Input
Resistance(pin 1)
Supply Voltage
Rejection
Thermal ShutDown Junction
Temperature
LINEAR INTEGRATED CIRCUIT
Po
BW
Gvo
d=0.5%,Gv=26dB,f=40 to 5kHz
RL=8W
RL=4W
Vs=+-19V, RL=4W
Po=15W,RL=4W
f=1kHz
Gvc
THD
15
10
13
18
12
16
100
80
25.5
26
W
W
W
KHz
dB
26.5
Po=0.1 to 14W,RL=4W
f=1kHz
Po=0.1 to 14W,RL=4W
f=1kHz
Po=0.1 to 9W,RL=8W
f=40 to 15 kHz
Po=4W ,RL=8W
f2-f1=1 kHz
0.08
%
0.03
%
0.05
%
0.03
%
d3
f2=14 kHz,f1=15kHz
0.08
%
eN
iN
Ri
B=curve A
B= 22Hz to 22kHz
B= 22Hz to 22kHz
Open loop,f=1kHz
THD
d2
RL=4W,Gv=26dB
Rg=22kW,f=1kHz
Tj
0.5
2
3
80
5
10
200
mA
mV
pA
MW
54
dB
145
C
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dB
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2
TDA2030A
LINEAR INTEGRATED CIRCUIT
TEST CIRCUIT
+Vs
Vi
C5
220 m F
C1
1 mF
C3
100nF
D1
1N4001
1
R3
22k W
2
5
Contek
TDA2030A
4
3
R3
680 W
R4
1W
R1
13k W
RL
D1
1N4001
C2
22 m F
C4
100nF
C6
100 m F
C7
220nF
-Vs
APPLICATION CIRCUIT
+Vs
Vi
C5
220 m F
C1
1 mF
C3
100nF
D1
1N4001
1
R3
22k W
2
5
Contek
TDA2030A
4
3
R3
680 W
C2
22 m F
R1
13k W
R4
1W
RL
D1
1N4001
C6
100 m F
C4
100nF
C7
220nF
-Vs
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3
TDA2030A
LINEAR INTEGRATED CIRCUIT
+Vs
22 mF
1
5
Contek
100k W
TDA2030A
2
3
100k W
220 mF
1N4001
4
100k W
R4
1W
4.7k W
2.2 mF
1N4001
C7
220nF
2200 mF
Vi
0.1 mF
RL=4W
100k W
2.2 mF
Fig.1 Single supply amplifier
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4
TDA2030A
LINEAR INTEGRATED CIRCUIT
TYPICAL PERFORMANCE CHARACTERISTICS
Gv
(dB)
Fig.3 Output power vs. Supply
voltage
140
180
Phase
100
90
Phase
Fig.2 Open loop frequency
response
Po
(W)
24
Gv=26dB
d=0.5%
f=40 to 15kHz
20
RL=4 W
0
60
16
RL=8 W
Gain
20
12
-20
8
-60
1
10
2
10
3
10
4
10
5
10
6
10
4
7
10
24
Frequency (Hz)
Fig.4 Total harmonic distortion
vs. output power
d
(%)
d
(%)
f=15kHz
-2
10
-1
10
Order (2f1-f2)
-1
10
0
10
1
10
Po (W)
Order (2f2-f1)
2
10
-2
10
1
10
30
Vs=+-15V
RL=8 W
25
3
10
4
10
5
10
Frequency (Hz)
Ptot
(W)
30
25
20
15
15
10
10
1
10
2
10
3
10
Frequency (kHz)
4
10
5
he
a
Rt tsin
h= k
4 ha
X vin
he
C/ g
at
W
Rth sink
=8 hav
ing
X
C/
W
-50
0
50
ink
ats
he
e
init
g
inf
vin
ha /W
ink X C
ats
he ty=25
R
Vs=+-15V
RL=4 W
20
5
2
10
Fig.7 Maximum allowable power
dissipation vs. ambient
temperture
Fig.6 Large signal frequency
response
Vo
(Vp-p)
44
Vs=32V
Po=4W
RL=4 W
Gv=26dB
Vs=32V
RL=4 W
f=1kHz
-2
10
40
Vs (V)
Po (W)
2
10
0
10
Vs=38V
RL=8 W
-1
10
36
1
10
Gv=26dB
0
10
32
Fig.5 Two tone CCIF
intermodulation distortion
2
10
1
10
28
100
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150
200
Tamb ( X C)
5
TDA2030A
LINEAR INTEGRATED CIRCUIT
2
5
4
TDA2030A
R4
3.3kW
C4
10 mF
C8
2200 mF
3
R5
30kW
BD907
R8
1W
RL=4W
C2
22 mF
R3 Contek
56kW
BD908
1N4001
1
R2
56kW
C5
220 mF
/40V
R6
1.5W
1N4001
R1
56kW
C6
0.22 mF
Vi
C1
2.2 mF
C3
0.22 mF
+Vs
R7
1.5W
C7
0.22 mF
Fig. 8 Single supply high power amplifier( Contek TDA2030+BD908/BD907)
TYPICAL PERFORMANCE OF THE CIRCUIT OF FIG. 8
PARAMETER
Supply Voltage
Quiescent Drain
Current
Output Power
SYMBOL
Vs
Id
Po
Voltage Gain
Slew Rate
Total Harmonic
Distortion
Input Sensitivity
Gv
SR
d
Signal to Noise
Ratio
S/N
Vi
TEST CONDITIONS
MIN
Vs=36V
d=0.5%,RL=4W
f=40Hz to 15kHz,Vs=39V
d=0.5%,RL=4W
f=40Hz to 15kHz,Vs=36V
d=0.5%,f=1kHz,
RL=4W Vs=39V
d=0.5%,RL=4W
f=1kHz,Vs=36V
f=1kHz
Po=20W,f=1kHz
Po=20W,f=40Hz to 15kHz
Gv=20dB,Po=20W,
f=1kHz,RL=4W
RL=4W,Rg=10kW
B=curve A,Po=25W
RL=4W,Rg=10kW
B=curve A,Po=25W
TYP
MAX
UNIT
36
50
44
V
mA
35
28
W
44
35
19.5
20
8
0.02
0.05
890
20.5
108
100
Contek Microelectronics Co.,Ltd.
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dB
V/msec
%
%
mV
dB
6
TDA2030A
LINEAR INTEGRATED CIRCUIT
TYPICAL PERFORMANCE CHARACTERISTICS
Fig. 10 Output power vs. supply
voltage
Fig. 11 Total harmonic distortion
vs. output power
Po
(W)
d
(%)
Vs=36V
RL=4 W
Gv=20dB
45
0
10
35
25
-1
10
f=15kHz
15
f=1kHz
5
24
28
32
34
36
Vs
(V)
40
-2
10
-1
10
Fig. 12 Output power vs.
Input level
0
10
1
10
Po
(W)
Fig. 13 Power dissipation vs.
output power
Ptot
(W)
Po
(W)
20
20
Complete
Amplifier
Gv=26dB
15
15
Gv=20dB
10
10
5
5
0
100
250
400
550
700
Vi
(mV)
BD908/
BD907
Contek
TDA2030
0
0
8
16
24
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32
Po
(W)
7
TDA2030A
LINEAR INTEGRATED CIRCUIT
+Vs
Vi
C5
100 mF
C1
1 mF
C3
100nF
D1
1N4001
1
R3
22kW
2
Contek
TDA2030A
5
4
3
C8
R5
R4
1W
RL
D2
R1
22kW 1N4001
R3
680W
C2
22 mF
C6
100 mF
C4
C7
100nF 220nF
-Vs
Fig. 14 Typical amplifier with split power supply
Vs+
100
1
R1
22k W
2
m F
5
Contek
TDA2030A
4
3
C8
IN
m F
C7
100nF
R3
22k
W
22
C4
R8
1 W
0.22 mF
220
C1
C6
m F
RL
8 W
R4
W
680
R7
W
22k
4
3
R5
22k
W
Vs22
100
C2
m F
C3
100nF
C5
C9
2
5
Contek
TDA2030A
0.22 mF
1
R2
22k
W
R9
1 W
m F
R6
680
W
Fig. 16 Bridge amplifier with split power supply(Po=34W,Vs+=16V,Vs-=16V)
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8
TDA2030A
LINEAR INTEGRATED CIRCUIT
MULTIWAY SPEAKER SYSTEMS AND ACTIVE BOXES
Multiway loudspeaker systems provide the best possible acoustic performance since each loudspeaker is
specially designed and optimized to handle a limited range of frequencies. Commonly, these loudspeaker systems
divide the audio spectrum two or three bands.
To maintain a flat frequency response over the Hi-Fi audio range the bands cobered by each loudspeaker must
overlap slightly. Imbalance between the loudspeakers produces unacceptable results therefore it is important to
ensure that each unit generates the correct amount of acoustic energy for its segments of the audio spectrum. In this
respect it is also important to know the energy distribution of the music spectrum to determine the cutoff frequencies
of the crossover filters(see Fig. 18).As an example,1 100W three-way system with crossover frequencies of 400Hz
and 3khz would require 50W for the woofer,35W for the midrange unit and 15W for the tweeter.
Both active and passive filters can be used for crossovers but active filters cost significantly less than a good
passive filter using aircored inductors and non-electrolytic capacitors. In addition active filters do not suffer from the
typical defects of passive filters:
--Power less;
--Increased impedance seen by the loudspeaker(lower damping)
--Difficulty of precise design due to variable loudspeaker impedance.
Obviously, active crossovers can only be used if a power amplifier is
provide for each drive unit. This makes it
particularly interesting and economically sound to use monolithic power amplifiers.
In some applications complex filters are not relay necessary and simple RC low-pass and high-pass
networks(6dB/octave) can be recommended.
The result obtained are excellent because this is the best type of audio filter and the only one free from phase and
transient distortion.
The rather poor out of band attenuation of single RC filters means that the loudspeaker must operate linearly well
beyond the crossover frequency to avoid distortion.
A more effective solution, named "Active power Filter" by SGS is shown in Fig. 19.
The proposed circuit can realize combined power amplifiers and 12dB/octave or 18dB octave high-pass or lowpass filters.
In proactive, at the input pins amplifier two
equal and in-phase voltages are available, as required for the active
filter operations.
The impedance at the Pin(-) is of the order of 100 W,while that of the Pin (+) is very high, which is also what was
wanted.
Fig. 18 Power distribution vs.
frequency
Fig. 19 Active power filter
100
C1 C2 C3
IEC/DIN NOISE
SPECTRUM
FOR SPEAKER
TESTING
80
Morden
Music
Spectrum
RL
60
R1 R2
R3
3.3kW
Vs-
40
100W
20
0
Vs+
1
10
2
10
3
10
4
10
5
10
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9
TDA2030A
LINEAR INTEGRATED CIRCUIT
The components values calculated for fc=900Hz using a Bessel 3rd Sallen and Key structure are:
C1=C2=C3=22nF,R1=8.2K
W,R2=5.6KW,R3=33KW.
Using this type of crossover filter, a complete 3-way 60W active loudspeaker system is shown in Fig. 20.
It employs 2nd order Buttherworth filter with the crossover frequencies equal to 300Hz and 3kHz.
The midrange section consistors of two filters a high pass circuit followed by a low pass network. With Vs=36V
the
output power delivered to the woofer is 25W at d=0.06%( 30W at d=0.5%).The power delivered to the midrange and
the tweeter can be optimized in the design phase taking in account the loudspeaker efficiency and impedance(RL=4 W
to 8W).
It is quite common that midrange and tweeter speakers have an efficiency 3dB higher than woofers.
22k W
2
22kW
33nF
680W
18nF
1
1N4001
5
BD908
4
Contek
TDA2030A
3
100 mF
2200 mF
0.22 mF
1N4001
1.5W
3.3kW
100W
BD907
4W
22k W
1W
1 mF
0.22 mF
IN
1.5W
Low-pass
300Hz
0.22 mF
2200 mF
Vs+
Woofer
Vs+
Band-pass
300Hz to 3kHz
0.22 mF
1N4001
3
1N4001
100 mF
100W
Vs+
0.22 mF
1N4001
100W
2.2k W
High-pass
3kHz
8W
3
1N4001
47 mF
100 mF
4
1W
2
5
Contek
TDA2030A
0.22 mF
1
22kW
12kW
0.1 mF
22kW
100 mF
22kW
0.1 mF
Midrange
2.2k W
High-pass
3kHz
Vs+
220 mF
4
1W
3.3nF
2
5
Contek
TDA2030A
8W
1
0.22 mF
22k W
18nF
22k W
6.8kW
0.1 mF
3.3kW
0.1 mF
Tweeter
Contek Microelectronics Co.,Ltd.
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10
TDA2030A
LINEAR INTEGRATED CIRCUIT
MUSICAL INSTRUMENTS AMPLIFIERS
Another important field of application for active system is music.
In this area the use of several medium power amplifiers is more convenient than a single high power amplifier, and it
is also more reliable. A typical
example(see Fig. 21) consist of four amplifiers each driving a low-cost, 12 inch
loudspeaker. This application can supply 80 to 160W rms.
TRANSIENT INTER-MODULATION DISTORTION(TIM)
Transient inter-modulation distortion is an unfortunate phenomena associated with negative-feedback amplifiers.
When a feedback amplifier receives an input signal which rises very steeply, i.e. contains high-frequency components,
the feedback can arrive too late so that the amplifiers overloads and a burst of inter-modulation
distortion will be produced as in Fig.22.Since transients occur frequently in music this obviously a problem for the
designed of audio amplifiers. Unfortunately, heavy negative feedback is frequency used to reduce the total harmonic
distortion of an amplifier, which tends to aggravate the transient inter- modulation(TIM situation.)The best known
Fig.21 High power active box for musical
instrument
Fig.22 Overshoot phenomenon in
feedback amplifiers
FEEDBACK
PATH
20 to 40W
Amplifier
V4
INPUT
V1
20 to 40W
Amplifier
PRE
AMPLIFIER
V2
V3
POWER
AMPLIFIER
OUTPUT
V4
V1
20 to 40W
Amplifier
V2
20 to 40W
Amplifier
V3
V4
method for the measurement of TIM consists of feeding sine waves superimposed onto square wavers, into the
amplifier under test. The output spectrum is then examined using a spectrum analyzer and compared to the input.
This method suffers from serious disadvantages: the accuracy is limited, the measurement is a tatter delicate
operation and an expensive spectrum analyzer is essential. A new approach (see Technical Note 143(Applied by
SGS to monolithic amplifiers measurement is fast cheap, it requires nothing more sophisticated than an
oscilloscope-and sensitive-and it can be used down to the values as low as 0.002% in high power amplifiers.
The "inverting- sawtooth" method of measurement is based on the response of an amplifier to a 20KHz saw-tooth
wave-form. The amplifier has no difficulty following the slow ramp but it cannot follow the fast edge. The output will
follow the upper line in Fig.23 cutting of the shade area and thus increasing the mean level. If this output signal is
filtered to remove the saw-tooth, direct voltage remains which indicates the amount of TIM distortion, although it is
difficult to measure because it is indistinguishable from the DC offset of the amplifier. This problem is neatly avoided
in the IS-TIM method by periodically inverting the saw-tooth wave-form at a low audio frequency as shown in
Fig.24.Inthe case of the saw-tooth in Fig. 25 the means level was increased by the TIM distortion, for a saw-tooth in
the other direction the opposite is true.
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11
TDA2030A
LINEAR INTEGRATED CIRCUIT
Input
Signal
SR(V/ms)
m2
m1
Filtered
Output
Siganal
Fig.23 20kHz sawtooth waveform
Fig.24 Inverting
sawtooth waveform
The result is an AC signal at the output whole peak-to-peak value is the TIM voltage, which can be measured
easily with an oscilloscope. If the peak- topeak value of the signal and the peak-to-peak of the inverting sawtooth are
measured, the TIM can be found very simply from:
TIM =
-1
10
2
10
SR(V/
TDA2030A
BD908/907
Gv=26dB
Vs=36V
RL=4W
-1
10
0
10
s)
Fig. 26 TIM design
diagram(fc=30kHz)
RC Filter fc=30kHz
1
10
RC Filter fc=30kHz
-2
10
* 100
0
10
1
10
Po(W)
2
10
-1
10
-1
10
TI
M
=0
.0
TI
1%
M
=0
.1
TI
%
M
=1
%
0
10
Vsawtooth
Fig. 25 TIM distortion Vs.
Output Power
1
10
TIM(%)
VOUT
0
10
1
10
Vo(Vp-p)
2
10
In Fig.25 The experimental results are shown for the 30W amplifier using the TDA2030A as a driver and a low-cost
complementary pair. A simple RC filter on the input of the amplifier to limit the maximum signal
slope(SS) is an
effective way to reduce TIM.
The Diagram of Fig.26 originated by SGS can be used to find the Slew- Rate(SR) required for a given output power
or voltage and a TIM design target.
For example if an anti-TIM filter with a cutoff at 30kHz is used and the max. Peak to peak output voltage is 20V then,
referring to the diagram, a Slew-Rate of 6V/ ms is necessary for 0.1% TIM.
As shown Slew-Rates of above 10V/ ms do not contribute to a further reduction in TIM.
Slew-Rates of 100V/ms are not only useless but also a disadvantage in hi-fi audio amplifiers because they tend to turn
the amplifier into a radio receiver.
POWER SUPPLY
Using monolithic audio amplifier with non regulated supply correctly. In any working case it must provide a supply
voltage less than the maximum value fixed by the IC breakdown voltage.
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12
TDA2030A
LINEAR INTEGRATED CIRCUIT
It is essential to take into account all the working conditions, in particular mains fluctuations and supply voltage
variations with and without load. The TDA2030(Vsmax=44V) is particularly suitable for substitution of the standard IC
power amplifiers(with Vsmax=36V) for more reliable applications.
An example, using a simple full-wave rectifier followed by a capacitor filter, is shown in the table and in the diagram of
Fig.27.
A regulated supply is not usually used for the power output stages because of its dimensioning must be done taking
into account the power to supply in signal peaks. They are not only a small percentage of the total music signal, with
consequently large overdimensioning of the circuit.
Even if with a regulated supply higher output power can be
obtained(Vs is constant in all working conditions),the
additional cost and power dissipation do not usually justify its use.
using non-regulated supplies, there are fewer
designee restriction. In fact, when signal peaks are present, the capacitor filter acts as a flywheel supplying the
required energy.
In average conditions, the continuous power supplied is lower. The music power/continuous power ratio is greater
in case than for the case of regulated supplied, with space saving and cost reduction.
Fig.27 DC characteristics of
50W non-regulated supply
Ripple
(Vp-p)
Vo(V)
36
34
Ripple
4
32
220V
2
3300 mF
30
Vout
Vo
0
28
0
Mains(220V)
+20%
+15%
+10%
-10%
-15%
-20%
0.4
0.8
1.2
1.6
2.0
Io(A)
Secondary Voltage
28.8V
27.6V
26.4V
24V
21.6V
20.4V
19.2V
DC Output Voltage(Vo)
Io=0
43.2V
41.4V
39.6V
36.2V
32.4V
30.6V
28.8V
Io=0.1A
42V
40.3V
38.5V
35V
31.5V
29.8V
28V
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Io=1A
37.5V
35.8V
34.2V
31V
27.8V
26V
24.3
13
TDA2030A
LINEAR INTEGRATED CIRCUIT
SHORT CIRCUIT PROTECTION
The Contek TDA2030 has an original circuit which limits the current of the output transistors. This function can be
considered as being peak power limiting rather than simple current limiting. It reduces the possibility that the device
gets damaged during an accidental short circuit from AC output to Ground.
THERMAL SHUT-DOWN
The presence of a thermal limiting circuit offers the following advantages:
1).An overload on the output (even if it is permanent),or an above limit ambient temperature can be easily supported
since the Tj can not be higher than 150 C
2).The heatsink can have a smaller factor of safety compared with that of a congenital circuit, There is no possibility of
device damage due to high junction temperature increase up to 150, the thermal shut-down simply reduces the power
dissipation and the current consumption.
APPLICATION SUGGESTION
The recommended values of the components are those shown on application circuit of Fig.14. Different values can be
used. The following table can help the designer.
COMPONENT
RECOMMENDED
VALUE
PURPOSE
LARGE THAN
RECOMMENDED
VALUE
LARGE THAN
RECOMMENDED
VALUE
R1
22KW
Increase of Gain
Decrease of Gain
R2
680W
Decrease of Gain
Increase of Gain
R3
22KW
1W
R5
3R2
Increase of input
impedance
Danger of oscillation
at high frequencies
with inductive loads.
Poor high frequencies
attenuation
Decrease of input
impedance
R4
Closed loop gaon
setting.
Closed loop gaon
setting.
Non inverting input
biasing
Frequency stacility
C1
1mF
C2
22mF
C3,C4
0.1mF
C5,C6
100mF
C7
C8
0.22mF
1/(2p*B*R1)
D1,D2
1N4001
Upper frequency
cutoff
Input DC decoupling
Inverting DC
decoupling
Supply voltage
bypass
Supply voltage
bypass
Frequency stability
Upper frequency
cutoff
To protect the device
against output voltage
spikes.
Dange of oscillation
Increase of low
frequencies cutoff
Increase of low
frequencies cutoff
Dange of oscillation
Dange of oscillation
smaller bandwidth
Contek Microelectronics Co.,Ltd.
CONTEK
http://www.contek-ic.com E-mail:[email protected]
Larger bandwidth
Larger bandwidth
14