TDA2030-TA5-T [UTC]

14W HI-FI AUDIO AMPLIFIER; 14W HI- FI音频放大器
TDA2030-TA5-T
型号: TDA2030-TA5-T
厂家: Unisonic Technologies    Unisonic Technologies
描述:

14W HI-FI AUDIO AMPLIFIER
14W HI- FI音频放大器

音频放大器
文件: 总13页 (文件大小:209K)
中文:  中文翻译
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UNISONIC TECHNOLOGIES CO., LTD  
TDA2030  
LINEAR INTEGRATED CIRCUIT  
14W HI-FI AUDIO AMPLIFIER  
„
DESCRIPTION  
The UTC TDA2030 is a monolithic audio power amplifier  
integrated circuit.  
„
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.  
*Pb-free plating product number: TDA2030L  
„ ORDERING INFORMATION  
Ordering Number  
Package  
Packing  
Normal  
Lead Free Plating  
TDA2030L-TA5-T  
TDA2030L-TB5-T  
TDA2030-TA5-T  
TDA2030-TB5-T  
TO-220-5  
TO-220B  
Tube  
Tube  
„ PIN CONFIGURATION  
PIN NO.  
PIN NAME  
Non inverting input  
1
2
3
4
5
Inverting input  
-VS  
Output  
+VS  
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Copyright © 2007 Unisonic Technologies Co., Ltd  
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TDA2030  
LINEAR INTEGRATED CIRCUIT  
„
ABSOLUTE MAXIMUM RATINGS (Ta=25°C)  
PARAMETER  
SYMBOL  
Vs  
RATINGS  
UNIT  
V
±18  
Supply Voltage  
Input Voltage  
VIN  
Vs  
V
±15  
Differential Input Voltage  
VI(DIFF)  
IOUT  
V
Peak Output Current(internally limited)  
Total Power Dissipation at Tc=90°C  
Junction Temperature  
3.5  
A
PD  
20  
W
°C  
°C  
TJ  
-40~+150  
-40~+150  
Storage Temperature  
TSTG  
Note: Absolute maximum ratings are those values beyond which the device could be permanently damaged.  
Absolute maximum ratings are stress ratings only and functional device operation is not implied.  
„
ELECTRICAL CHARACTERISTICS (Refer to the test circuit, Vs =±16V,Ta=25°C)  
PARAMETER  
SYMBOL  
Vs  
TEST CONDITIONS  
MIN  
±6  
TYP  
MAX  
±18  
UNIT  
V
Supply Voltage  
Quiescent Drain Current  
Input Bias Current  
Input Offset Voltage  
Input Offset Current  
Power Bandwidth  
IQ  
40  
0.2  
±2  
60  
2
±20  
±200  
mA  
µA  
MV  
NA  
Hz  
W
II(BIAS)  
VI(OFF)  
II(OFF)  
BW  
Vs=±18v  
POUT=12W, RL=4, Gv=30dB  
±20  
10~140,000  
d=0.5%, Gv=30dB  
f=40Hz to 15KHz  
RL=4Ω  
12  
8
14  
9
RL=8Ω  
RL=4Ω  
RL=8Ω  
W
Output Power  
POUT  
d=10%, Gv=30dB  
f=1KHz  
18  
11  
90  
30  
W
W
Open Loop Voltage Gain  
Closed Loop Voltage Gain  
Gvo  
Gvc  
dB  
dB  
f=1kHz  
29.5  
30 .5  
0.5  
POUT=0.1 to 12W, RL=4Ω  
f=40Hz to 15KHz, Gv=30dB  
0.2  
0.1  
%
%
Distortion  
THD  
POUT=0.1 to 8W, RL=8Ω  
0.5  
f=40Hz to 15KHz, Gv=30dB  
B= 22Hz to 22kHz  
Input Noise Voltage  
Input Noise Current  
Input Resistance(pin 1)  
eN  
iN  
3
80  
5
10  
µV  
pA  
B= 22Hz to 22kHz  
200  
RIN  
0.5  
40  
MΩ  
RL=4, Gv=30dB  
Rg=22k, fripple=100Hz,  
Vripple=0.5Veff  
Supply Voltage Rejection  
SVR  
TJ  
50  
dB  
Thermal Shut-Down Junction  
Temperature  
145  
°C  
UNISONIC TECHNOLOGIES CO., LTD  
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QW-R107-004,D  
www.unisonic.com.tw  
TDA2030  
LINEAR INTEGRATED CIRCUIT  
„
TEST CIRCUIT  
„
APPLICATION CIRCUIT  
+Vs  
C5  
C3  
220 F  
100nF  
C1  
1 F  
D1  
Vi  
1N4001  
4
1
2
5
3
R3  
22k  
UTC  
TDA 2030  
R4  
1
R1  
13k  
RL  
R3  
D1  
680  
1N4001  
C2  
C6  
C4 C7  
22 F  
100 F  
100nF 220nF  
-Vs  
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TDA2030  
LINEAR INTEGRATED CIRCUIT  
„
TYPICAL CHARACTERISTICS  
Fig.2 Open loop frequency response  
Fig.3 Output power vs. Supply voltage  
140  
100  
24  
20  
180  
90  
Gv=26dB  
d=0.5%  
f=40 to 15kHz  
Phase  
RL=4  
60  
20  
0
16  
12  
RL=8  
Gain  
-20  
-60  
8
4
1
2
3
4
5
6
7
24  
28  
32  
36  
40  
44  
10  
10  
10  
10  
10  
10  
10  
Frequency (Hz)  
Vs (V)  
Fig.4 Total harmonic distortion  
vs. output power  
Fig.5 Two tone CCIF intermodulation  
distortion  
2
2
10  
10  
1
1
10  
10  
Gv=26dB  
Vs=32V  
PoUT=4W  
RL=4  
0
0
10  
10  
Vs=38V  
RL=8  
Gv=26dB  
Order (2f1-f2)  
Order (2f2-f1)  
f=15kHz  
-1  
10  
-1  
10  
Vs=32V  
RL=4  
f=1kHz  
-2  
10  
-2  
10  
-2  
10  
-1  
10  
0
1
2
1
2
3
4
5
10  
10  
10  
10  
10  
10  
10  
10  
Po (W)  
Frequency (Hz)  
Fig.7 Maximum allowable power  
dissipation vs. ambient temperture  
Fig.6 Large signal frequency response  
30  
30  
Vs=+-15V  
RL=8  
25  
25  
Vs=+-15V  
RL=4  
20  
15  
20  
15  
10  
5
10  
5
1
2
3
4
-50  
0
50  
100  
150  
200  
10  
10  
10  
10  
Ta (°C)  
Frequency (kHz)  
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TDA2030  
LINEAR INTEGRATED CIRCUIT  
+Vs  
C5  
220 F  
/40V  
R1  
56k  
R6  
1.5  
C1  
2.2 F  
Vi  
1
2
C8  
2200 F  
5
3
R3  
56k  
UTC  
TDA2030  
4
R2  
R8  
1
56k  
R5  
30k  
R4  
3.3k  
R7  
1.5  
C4  
10 F  
C7  
0.22 F  
Fig. 1 Single supply high power amplifier  
„
TYPICAL PERFORMANCE OF THE CIRCUIT OF FIG. 1  
PARAMETER  
SYMBOL TEST CONDITIONS  
Vs  
MIN  
TYP  
36  
MAX  
44  
UNIT  
V
Supply Voltage  
Quiescent Drain Current  
IQ  
Vs=36V  
50  
mA  
d=0.5%,RL=4Ω  
f=40Hz to 15kHz,Vs=39V  
d=0.5%,RL=4Ω  
f=40Hz to 15kHz,Vs=36V  
d=10%,f=1kHz,  
RL=4,Vs=39V  
d=10%,RL=4Ω  
f=1kHz,Vs=36V  
f=1kHz  
35  
28  
44  
35  
Output Power  
POUT  
W
Voltage Gain  
Slew Rate  
Gv  
SR  
19.5  
20  
8
20.5  
dB  
V/µsec  
%
POUT=20W,f=1kHz  
0.02  
0.05  
Total Harmonic Distortion  
Input Sensitivity  
d
POUT=20W,f=40Hz to 15kHz  
%
Gv=20dB,POUT=20W,  
f=1kHz,RL=4Ω  
RL=4,Rg=10kΩ  
VIN  
890  
mV  
dB  
B=curve A,POUT=25W  
108  
100  
Signal to Noise Ratio  
S/N  
RL=4,Rg=10kΩ  
B=curve A,POUT=4W  
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TDA2030  
LINEAR INTEGRATED CIRCUIT  
„
TYPICAL PERFORMANCE CHARACTERISTICS  
Total Harmonic Distortion vs. Output Power  
Output Power vs. Supply Voltage  
Vs=36V  
RL=4  
45  
Gv=20dB  
0
-1  
-2  
10  
0  
10  
35  
25  
15  
5
f=15kHz  
f=1kHz  
40  
24  
28  
32  
34  
Vs (V)  
36  
-1  
0
1
10  
10  
10  
PoUT (W)  
Output Power vs. Input Level  
Power Dissipation vs. Output Power  
20  
20  
Complete  
Amplifier  
Gv=26dB  
15  
10  
15  
10  
Gv=20dB  
UTC  
TDA2030  
5
0
5
0
100  
250  
400  
550  
700  
0
8
16  
24  
32  
VIN (mV)  
PoUT (W)  
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TDA2030  
LINEAR INTEGRATED CIRCUIT  
TYPICAL AMPLIFIER WITH SPLIT POWER SUPPLY  
+Vs  
C5  
C3  
100 F  
100nF  
C1  
1 F  
D1  
Vi  
1N4001  
1
5
3
R3  
22k  
4
2
R4  
1
C8  
R5  
R1  
RL  
R3  
D2  
680  
22k 1N4001  
C2  
C6  
C4 C7  
22 F  
100 F  
100nF 220nF  
-Vs  
BRIDGE AMPLIFIER WITH SPLIT POWER SUPPLY(POUT=34W,VS=16V, VS=-16V)  
Vs+  
C6  
100 F  
C7  
100nF  
C1  
2.2  
F
1
2
5
UTC TDA2030  
3
IN  
4
R1  
22k  
C8  
0.22  
F
R3  
R8  
1
22k  
C4  
22 F  
RL  
8
R4  
680  
R7  
22k  
1
2
5
R2  
22k  
4
UTC TDA2030  
C9  
0. 2 2  
F
3
R5  
22k  
R9  
1
Vs-  
C5  
22 F  
R6  
680  
C2  
100 F  
C3  
100nF  
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TDA2030  
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. 2).As an example, a 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 is shown in Fig. 3.  
The proposed circuit can realize combined power amplifiers and 12dB/octave or high-pass or low-pass 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,while that of the Pin (+) is very high, which is also what was  
wanted.  
The components values calculated for fc=900Hz using a Bessel 3rd Sallen and Key structure are:  
C1=C2=C3=22nF,R1=8.2K,R2=5.6K,R3=33K.  
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=4to 8).  
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TDA2030  
LINEAR INTEGRATED CIRCUIT  
It is quite common that midrange and tweeter speakers have an efficiency 3dB higher than woofers.  
Vs+  
Low-pass  
300Hz  
2200  
F
0.22 F  
1N4001  
1.5  
1
F
IN  
22k  
22k  
BD908  
1
5
UTC  
TDA2030  
4
18nF  
680  
2200  
F
2
0.22  
F
33nF  
3
100  
F
22k  
1
BD907  
4
1.5  
100  
1N4001  
0.22  
F
3.3k  
Woofer  
Vs+  
Band-pass  
300Hz to 3KHz  
0.22  
F
1N4001  
0.1  
F
0.1 F  
22k  
22k  
1
2
5
220  
F
UTC  
4
18nF  
TDA2030  
3.3k  
6.8k  
1
3
8
3.3nF  
0.22  
F
1N4001  
100  
F
2.2k  
Midrange  
Vs+  
100  
0.22  
F
High-pass  
3KHz  
1N4001  
Vs+  
3.3 nF  
3.3 nF  
1
2
5
100  
F
UTC  
4
22k  
TDA2030  
22k  
12k  
1
3
8
1N4001  
0.22  
F
22k  
100  
F
47  
F
2.2k  
Tweeter  
High-pass  
3KHz  
100  
„
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. 4) consist of four amplifiers each driving a low-cost, 12 inch  
loudspeaker. This application can supply 80 to 160W rms.  
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TDA2030  
LINEAR INTEGRATED CIRCUIT  
„
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.5. 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.)  
Fig.4 High power active box for musical instrument  
Fig.5 Overshoot phenomenon in feedback amplifiers  
FEEDBACK  
PATH  
20 to 40W  
Amplifier  
¦ÂV4  
INPUT  
V1  
OUTPUT  
POWER  
PRE AMPLIFIER  
AMPLIFIER  
V2  
V3  
V4  
20 to 40W  
Amplifier  
V1  
V2  
20 to 40W  
Amplifier  
20 to 40W  
Amplifier  
V3  
V4  
The best known 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.  
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.6 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.7. In the case of the saw-tooth in Fig. 8 the mean level was increased by the TIM distortion, for a saw-tooth in the  
other direction the opposite is true.  
Input  
SR(V/ s)  
Signal  
m2  
m1  
Filtered  
Output  
Siganal  
Fig.6 20kHz sawtooth waveform  
Fig.7 Inverting sawtooth waveform  
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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:  
VOUT  
TIM =  
* 100  
Vsawtooth  
In Fig.8 The experimental results are shown for the 30W amplifier using the UTC TDA2030 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.9 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/µs is necessary for 0.1% TIM.  
As shown Slew-Rates of above 10V/µs do not contribute to a further reduction in TIM.  
Slew-Rates of 100V/µs are not only useless but also a disadvantage in hi-fi audio amplifiers because they tend to  
turn the amplifier into a radio receiver.  
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LINEAR INTEGRATED CIRCUIT  
„
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.  
It is essential to take into account all the working conditions, in particular mains fluctuations and supply voltage  
variations with and without load. The UTC 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.10.  
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.10 DC characteristics of 50W non-regulated supply  
36  
34  
Ripple  
4
2
0
220V  
32  
30  
Vo  
3300  
F
Vout  
28  
0
0.4  
0.8  
1.2  
1.6  
2.0  
IOUT(A)  
DC Output Voltage(VOUT  
)
Mains(220V)  
Secondary Voltage  
IOUT =0  
43.2V  
41.4V  
39.6V  
36.2V  
32.4V  
30.6V  
28.8V  
IOUT =0.1A  
42V  
IOUT =1A  
37.5V  
35.8V  
34.2V  
31V  
+20%  
+15%  
+10%  
28.8V  
27.6V  
26.4V  
24V  
40.3V  
38.5V  
35V  
-10%  
-15%  
-20%  
21.6V  
20.4V  
19.2V  
31.5V  
29.8V  
28V  
27.8V  
26V  
24.3V  
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TDA2030  
LINEAR INTEGRATED CIRCUIT  
„
SHORT CIRCUIT PROTECTION  
The UTC 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°C, 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.  
SMALLER THAN  
RECOMMENDED  
VALUE  
LARGER THAN  
RECOMMENDED VALUE  
COMPONENT  
PURPOSE  
RECOMMENDED  
VALUE  
Closed loop gaon  
setting.  
R1  
R2  
R3  
22KΩ  
680Ω  
22KΩ  
Increase of Gain  
Decrease of Gain  
Increase of Gain  
Closed loop gaon  
setting.  
Decrease of Gain  
Non inverting input  
biasing  
Decrease of input  
impedance  
Increase of input impedance  
Danger of oscillation at high  
frequencies with inductive  
loads.  
R4  
1Ω  
Frequency stability  
Poor high frequencies  
attenuation  
R5  
C1  
C2  
3R2  
1µF  
Upper frequency cutoff  
Input DC decoupling  
Danger of oscillation  
Increase of low  
frequencies cutoff  
Increase of low  
frequencies cutoff  
Danger of oscillation  
Danger of oscillation  
Larger bandwidth  
Larger bandwidth  
Inverting DC  
decoupling  
22µF  
C3,C4  
C5,C6  
C7  
0.1µF  
100µF  
0.22µF  
Supply voltage bypass  
Supply voltage bypass  
Frequency stability  
C8  
1/(2π*B*R1)  
Upper frequency cutoff smaller bandwidth  
To protect the device  
against output voltage  
spikes.  
D1,D2  
1N4001  
UTC assumes no responsibility for equipment failures that result from using products at values that  
exceed, even momentarily, rated values (such as maximum ratings, operating condition ranges, or  
other parameters) listed in products specifications of any and all UTC products described or contained  
herein. UTC products are not designed for use in life support appliances, devices or systems where  
malfunction of these products can be reasonably expected to result in personal injury. Reproduction in  
whole or in part is prohibited without the prior written consent of the copyright owner. The information  
presented in this document does not form part of any quotation or contract, is believed to be accurate  
and reliable and may be changed without notice.  
UNISONIC TECHNOLOGIES CO., LTD  
13 of 13  
QW-R107-004,D  
www.unisonic.com.tw  

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