THS4082ID [TI]

175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS; 175 - MHz的低功耗高速放大器
THS4082ID
型号: THS4082ID
厂家: TEXAS INSTRUMENTS    TEXAS INSTRUMENTS
描述:

175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS
175 - MHz的低功耗高速放大器

消费电路 商用集成电路 音频放大器 视频放大器 光电二极管
文件: 总24页 (文件大小:384K)
中文:  中文翻译
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THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
THS4081  
D OR DGN PACKAGE  
(TOP VIEW)  
Ultralow 3.4 mA Per Channel Quiescent  
Current  
High Speed  
– 175 MHz Bandwidth (–3 dB, G = 1)  
– 230 V/µs Slew Rate  
– 43 ns Settling Time (0.1%)  
NC  
IN–  
IN+  
NC  
1
2
3
4
8
7
6
5
V
+
CC  
OUT  
NC  
High Output Drive, I = 85 mA (typ)  
O
V
CC–  
Excellent Video Performance  
– 35 MHz Bandwidth (0.1 dB, G = 1)  
– 0.01% Differential Gain  
NC – No internal connection  
THS4082  
D OR DGN PACKAGE  
(TOP VIEW)  
– 0.05° Differential Phase  
Very Low Distortion  
– THD = –64 dBc (f = 1 MHz, R = 150 )  
– THD = –79 dBc (f = 1 MHz, R = 1 k)  
1OUT  
1IN–  
1IN+  
V
+
CC  
1
2
3
4
8
7
6
5
L
L
2OUT  
2IN–  
2IN+  
Wide Range of Power Supplies  
V
CC–  
– V  
= ±5 V to ±15 V  
CC  
Available in Standard SOIC or MSOP  
PowerPAD Package  
Evaluation Module Available  
Cross Section View Showing  
PowerPAD Option (DGN)  
description  
The THS4081 and THS4082 are ultralow-power,  
high-speed voltage feedback amplifiers that are  
ideal for communication and video applications.  
These amplifiers operate off of a very low 3.4-mA  
quiescent current per channel and have a high  
outputdrivecapabilityof85 mA. Thesignal-ampli-  
fier THS4081 and the dual-amplifier THS4082  
offer very good ac performance with 175-MHz  
bandwidth, 230-V/µs slew rate, and 43-ns settling  
time (0.1%). With total harmonic distortion (THD)  
of –64 dBc at f = 1 MHz, the THS4081 and  
THS4082 are ideally suited for applications  
requiring low distortion.  
SUPPLY CURRENT  
vs  
SUPPLY VOLTAGE  
3.8  
3.6  
3.4  
3.2  
3.0  
2.8  
2.6  
2.4  
2.2  
T
=85°C  
A
T
=25°C  
A
T
=–40°C  
A
5
7
9
11  
13  
15  
RELATED DEVICES  
± V  
- Supply Voltage - V  
CC  
DEVICE  
DESCRIPTION  
THS4011/2 290-MHz Low Distortion High-Speed Amplifiers  
THS4031/2 100-MHz Low Noise High Speed-Amplifiers  
THS4051/2  
70-MHz High-Speed Amplifiers  
CAUTION: The THS4081 and THS4082 provide ESD protection circuitry. However, permanent damage can still occur if this device  
is subjected to high-energy electrostatic discharges. Proper ESD precautions are recommended to avoid any performance  
degradation or loss of functionality.  
Please be aware that an important notice concerning availability, standard warranty, and use in critical applications of  
Texas Instruments semiconductor products and disclaimers thereto appears at the end of this data sheet.  
PowerPAD is a trademark of Texas Instruments.  
Copyright 2000, Texas Instruments Incorporated  
PRODUCTION DATA information is current as of publication date.  
Products conform to specifications per the terms of Texas Instruments  
standard warranty. Production processing does not necessarily include  
testing of all parameters.  
1
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
AVAILABLE OPTIONS  
PACKAGED DEVICES  
PLASTIC PLASTIC  
NUMBER OF  
CHANNELS  
MSOP  
SYMBOL  
EVALUATION  
MODULE  
T
A
SMALL OUTLINE  
(D)  
MSOP  
(DGN)  
1
2
1
2
THS4081CD  
THS4082CD  
THS4081ID  
THS4082ID  
THS4081CDGN  
THS4082CDGN  
THS4081IDGN  
THS4082IDGN  
AEO  
AER  
AEQ  
AEP  
THS4081EVM  
0°C to 70°C  
THS4082EVM  
40°C to 85°C  
The D and DGN packages are available taped and reeled. Add an R suffix to the device type (i.e., THS4081CDGN).  
functional block diagram  
2
3
IN–  
IN+  
6
OUT  
Figure 1. THS4081 – Single Channel  
V
CC  
1IN–  
1IN+  
1OUT  
2OUT  
2IN–  
2IN+  
–V  
CC  
Figure 2. THS4082 – Dual Channel  
2
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
absolute maximum ratings over operating free-air temperature (unless otherwise noted)  
Supply voltage, V  
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±16.5 V  
CC  
Input voltage, V . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±V  
I
CC  
Output current, I . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 150 mA  
O
Differential input voltage, V  
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±4 V  
IO  
Continuous total power dissipation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . See Dissipation Rating Table  
Maximum junction temperature, T . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 150°C  
J
Operating free-air temperature, T : C-suffix . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0°C to 70°C  
A
I-suffix . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 40°C to 85°C  
Storage temperature, T  
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 65°C to 150°C  
stg  
Lead temperature 1,6 mm (1/16 inch) from case for 10 seconds . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 300°C  
Stresses beyond those listed under “absolute maximum ratings” may cause permanent damage to the device. These are stress ratings only and  
functional operation of the device at these or any other conditions beyond those indicated under “recommended operating conditions” is not  
implied. Exposure to absolute-maximum-rated conditions for extended periods may affect device reliability.  
DISSIPATION RATING TABLE  
θ
θ
T = 25°C  
A
JA  
(°C/W)  
JC  
PACKAGE  
(°C/W)  
38.3  
4.7  
POWER RATING  
D
167  
740 mW  
§
DGN  
58.4  
2.14 W  
§
This data was taken using the JEDEC standard Low-K test PCB. For the JEDEC Proposed  
High-K test PCB, the θ is 95°C/W with a power rating at T = 25°C of 1.32 W.  
This data was taken using 2 oz. trace and copper pad that is soldered directly to a 3 in. × 3 in.  
JA  
A
PC. For further information, refer to Application Information section of this data sheet.  
recommended operating conditions  
MIN NOM  
MAX  
±15  
30  
UNIT  
Dual supply  
Single supply  
C-suffix  
±5  
10  
Supply voltage, V  
and V  
CC–  
V
CC+  
0
70  
Operating free-air temperature, T  
°C  
A
I-suffix  
40  
85  
3
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
electrical characteristics at T = 25°C, V  
= ±15 V, R = 150 (unless otherwise noted)  
L
A
CC  
dynamic performance  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
175  
160  
70  
MAX  
UNIT  
V
V
V
V
V
V
V
V
V
V
V
V
V
V
= ±15 V  
CC  
Gain = 1  
Gain = –1  
Gain = 1  
MHz  
= ±5 V  
= ±15 V  
= ±5 V  
= ±15 V  
= ±5 V  
CC  
Small-signal bandwidth (–3 dB)  
Bandwidth for 0.1 dB flatness  
CC  
MHz  
MHz  
MHz  
V/µs  
ns  
65  
CC  
BW  
SR  
35  
CC  
35  
CC  
= 20 V,  
= 5 V,  
V
V
= ±15 V  
= ±5 V  
2.7  
7.1  
230  
170  
43  
O(pp)  
O(pp)  
CC  
Full power bandwidth  
CC  
= ±15 V,  
= ±5 V,  
= ±15 V,  
= ±5 V,  
= ±15 V,  
= ±5 V,  
20-V step,  
5-V step  
5-V step  
2-V step  
5-V step  
2-V step  
Gain = 5  
Gain = 1  
CC  
CC  
CC  
CC  
CC  
CC  
Slew rate  
Settling time to 0.1%  
Gain = –1  
Gain = –1  
30  
t
s
233  
280  
Settling time to 0.01%  
ns  
Slew rate is measured from an output level range of 25% to 75%.  
Full power bandwidth = slew rate/2π V  
.
O(Peak)  
noise/distortion performance  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
–64  
–79  
–64  
–77  
10  
MAX  
UNIT  
R
R
R
R
= 150 Ω  
= 1 kΩ  
L
L
L
L
V
= ±15 V  
= ±5 V  
CC  
CC  
V
= 2 V,  
O(pp)  
f = 1 MHz, Gain = 2  
THD  
Total harmonic distortion  
dBc  
= 150 Ω  
= 1 kΩ  
V
V
n
Input voltage noise  
Input current noise  
V
V
= ±5 V or ±15 V, f = 10 kHz  
= ±5 V or ±15 V, f = 10 kHz  
nV/Hz  
pA/Hz  
CC  
I
n
0.7  
CC  
V
CC  
V
CC  
V
CC  
V
CC  
= ±15 V  
= ±5 V  
= ±15 V  
= ±5 V  
0.01%  
0.01%  
0.05°  
Gain = 2,  
40 IRE modulation,  
NTSC,  
±100 IRE ramp  
Differential gain error  
Differential phase error  
Gain = 2,  
40 IRE modulation,  
NTSC,  
±100 IRE ramp  
0.05°  
Channel-to-channel crosstalk  
(THS4082 only)  
X
T
V
CC  
= ±5 V or ±15 V, f = 1 MHz  
–75  
dB  
4
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
electrical characteristics at T = 25°C, V = ±15 V, R = 150 (unless otherwise noted) (continued)  
A
CC  
L
dc performance  
PARAMETER  
TEST CONDITIONS  
MIN  
10  
9
TYP  
MAX  
UNIT  
T
= 25°C  
19  
A
V
= ±15 V,  
= ±5 V,  
V
= ±10 V,  
= ±2.5 V,  
R
= 1 kΩ  
V/mV  
CC  
O
L
L
T
A
= full range  
= 25°C  
Open loop gain  
T
A
8
16  
1
V
CC  
V
R
= 250 Ω  
V/mV  
O
T
A
= full range  
= 25°C  
7
T
A
7
8
V
OS  
Input offset voltage  
Offset voltage drift  
Input bias current  
mV  
µV/°C  
µA  
T
= full range  
= full range  
= 25°C  
A
A
T
A
15  
V
CC  
= ±5 V or ±15 V  
T
1.2  
6
8
I
I
IB  
T
A
= full range  
= 25°C  
T
A
20  
250  
400  
Input offset current  
Offset current drift  
nA  
OS  
T
A
= full range  
T
A
= full range  
0.3  
nA/°C  
Full range = 0°C to 70°C for C suffix and 40°C to 85°C for I suffix  
input characteristics  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
MAX  
UNIT  
V
CC  
V
CC  
V
CC  
V
CC  
= ±15 V  
= ±5 V  
±13.8 ±14.1  
V
Common mode input voltage range  
V
ICR  
±3.8  
84  
±3.9  
93  
= ±15 V,  
= ±5 V,  
V
V
= ±12 V,  
= ±2 V,  
T
= full range  
dB  
dB  
ICR  
ICR  
A
CMRR Common mode rejection ratio  
T
A
= full range  
78  
90  
R
C
Input resistance  
1
MΩ  
pF  
I
I
Input capacitance  
1.5  
Full range = 0°C to 70°C for C suffix and 40°C to 85°C for I suffix  
output characteristics  
PARAMETER  
TEST CONDITIONS  
MIN  
TYP  
MAX  
UNIT  
V
V
V
V
V
V
V
= ±15 V  
= ±5 V  
R
R
= 250 Ω  
±12 ±13.6  
±3.4 ±3.8  
±13.5 ±13.8  
CC  
CC  
CC  
CC  
CC  
CC  
CC  
L
L
V
= 150 Ω  
V
I
Output voltage swing  
O
= ±15 V  
= ±5 V  
R
R
= 1 kΩ  
V
L
L
±3.5  
65  
±3.9  
85  
= ±15 V  
= ±5 V  
= 20 Ω  
mA  
Output current  
O
50  
70  
I
Short-circuit current  
Output resistance  
= ±15 V  
100  
mA  
SC  
R
Open loop  
13  
O
Observe power dissipation ratings to keep the junction temperature below the absolute maximum rating when the output is heavily loaded or  
shorted. See the absolute maximum ratings section of this data sheet for more information.  
5
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
electrical characteristics at T = 25°C, V = ±15 V, R = 150 (unless otherwise noted) (continued)  
A
CC  
L
power supply  
PARAMETER  
TEST CONDITIONS  
MIN  
±4.5  
9
TYP  
MAX  
±16.5  
33  
UNIT  
Dual supply  
Single supply  
V
Supply voltage operating range  
Supply current (per amplifier)  
V
CC  
T
= 25°C  
3.4  
2.9  
90  
4.2  
A
V
= ±15 V  
CC  
T
A
= full range  
5
I
mA  
dB  
CC  
T
= 25°C  
3.7  
A
V
V
= ±5 V  
CC  
T
A
= full range  
4.5  
PSRR Power supply rejection ratio  
= ±5 V or ±15 V  
T
A
= full range  
79  
CC  
Full range = 0°C to 70°C for C suffix and 40°C to 85°C for I suffix  
6
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
TYPICAL CHARACTERISTICS  
OPEN LOOP GAIN  
& PHASE RESPONSE  
vs  
CROSSTALK  
vs  
FREQUENCY  
FREQUENCY  
100.00  
80.00  
60.00  
40.00  
20.00  
0.00  
45°  
0°  
20  
0
V
= ±15 V  
CC  
Gain = 1  
R
R
= 0 Ω  
= 150 Ω  
F
L
Gain  
–45°  
90°  
–20  
–40  
–60  
–80  
Phase  
135°  
180°  
V
= ±5 V and ±15 V  
CC  
1k  
–225°  
–20.00  
100  
10k 100k 1M 10M 100M 1G  
100k  
1M  
10M  
100M  
1G  
f – Frequency – Hz  
f – Frequency – Hz  
Figure 3  
Figure 4  
SETTLING  
TOTAL HARMONIC DISTORTION  
TOTAL HARMONIC DISTORTION  
vs  
vs  
vs  
OUTPUT STEP  
FREQUENCY  
FREQUENCY  
–40  
–50  
–60  
–70  
–80  
–90  
–100  
–40  
–50  
–60  
–70  
–80  
–90  
–100  
330  
290  
250  
210  
170  
130  
90  
V
= ± 15 V  
V
= ± 5 V  
CC  
Gain = 2  
CC  
Gain = 2  
V
= 2 V  
V
= 2 V  
O(PP)  
O(PP)  
R
= 150 Ω  
R
= 150 Ω  
V
= ±5 V(0.01%)  
CC  
L
L
V
= ±15 V(0.01%)  
CC  
R
= 1 kΩ  
L
V
= ±5 V(0.1%)  
CC  
R
= 1 kΩ  
L
V
= ±15 V(0.1%)  
CC  
50  
10  
2
3
4
5
100k  
1M  
10M  
100k  
1M  
10M  
f - Frequency - Hz  
f - Frequency - Hz  
V
– Output Step Voltage – V  
O
Figure 5  
Figure 6  
Figure 7  
POWER SUPPLY REJECTION  
DISTORTION  
vs  
OUTPUT VOLTAGE  
DISTORTION  
vs  
OUTPUT VOLTAGE  
RATIO  
vs  
FREQUENCY  
–50  
–50  
–60  
0
–20  
2nd Harmonic  
V
= ± 15 V & ± 5 V  
CC  
2nd Harmonic  
–60  
–70  
–V  
3rd Harmonic  
3rd Harmonic  
CC  
–70  
–40  
+V  
CC  
–80  
–80  
–60  
V
R
= ± 15 V  
V
= ± 15 V  
R = 150 Ω  
L
CC  
= 1 kΩ  
CC  
–90  
–90  
–80  
L
Gain = 5  
Gain = 5  
f = 1 MHz  
f = 1 MHz  
–100  
–100  
–100  
0
5
10  
15  
20  
0
5
10  
15  
20  
100k  
1M  
10M  
100M  
f - Frequency - Hz  
V
– Output Voltage – V  
V
– Output Voltage – V  
O
O
Figure 8  
Figure 9  
Figure 10  
7
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
TYPICAL CHARACTERISTICS  
DISTORTION  
vs  
DISTORTION  
DISTORTION  
vs  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
–50  
–60  
–50  
–60  
–50  
–60  
V
R
= ± 15 V  
V
R
= ± 5 V  
V
= ± 15 V  
CC  
= 1 kΩ  
CC  
= 1 kΩ  
CC  
R = 150 Ω  
L
L
L
Gain = 2  
= 2 V  
Gain = 2  
= 2 V  
Gain = 2  
V = 2 V  
V
V
O(PP)  
O(PP)  
O(PP)  
3rd Harmonic  
–70  
–70  
–70  
2nd Harmonic  
2nd Harmonic  
2nd Harmonic  
–80  
–80  
–80  
3rd Harmonic  
–90  
–90  
–90  
3rd Harmonic  
–100  
–100  
–100  
100k  
1M  
10M  
100k  
1M  
10M  
100k  
1M  
10M  
f – Frequency – Hz  
f – Frequency – Hz  
Figure 12  
f – Frequency – Hz  
Figure 11  
Figure 13  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
DISTORTION  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
–50  
–60  
4
4
V
R
= ± 5 V  
CC  
= 150 Ω  
Gain = 2  
= 2 V  
L
R
= 130 Ω  
F
R
= 51 Ω  
= 0 Ω  
F
2
0
2
0
V
O(PP)  
R
= 51 Ω  
R
= 130 Ω  
F
F
3rd Harmonic  
–70  
R
R
= 0 Ω  
F
F
2nd Harmonic  
–80  
–2  
–4  
–6  
–2  
–4  
–6  
V
= ± 15 V  
V
= ± 5 V  
CC  
Gain = 1  
= 150 Ω  
CC  
Gain = 1  
–90  
R
V
R
= 150 Ω  
L
L
= 63 mV  
V
= 63 mV  
O(PP)  
O(PP)  
–100  
100k  
1M  
10M  
100k  
1M  
10M 100M 1G  
100k  
1M  
10M 100M 1G  
f – Frequency – Hz  
f - Frequency - Hz  
f - Frequency - Hz  
Figure 14  
Figure 15  
Figure 16  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
2
2
2
R
= 51 Ω  
F
R = 1.3 kΩ  
F
R
= 51 Ω  
F
R
= 2 kΩ  
F
0
–2  
–4  
–6  
–8  
0
–2  
–4  
–6  
–8  
0
–2  
–4  
–6  
–8  
R
= 0 Ω  
F
R
= 1 kΩ  
F
R
= 0 Ω  
F
V
= ± 15 V  
V
= ± 5 V  
V
= ± 15 V  
CC  
Gain = 1  
CC  
Gain = 1  
= 1 kΩ  
CC  
Gain = –1  
R = 150 Ω  
L
R
V
= 1 kΩ  
R
V
L
L
= 63 mV  
= 63 mV  
V
= 63 mV  
O(PP)  
O(PP)  
O(PP)  
100k  
1M  
10M 100M 1G  
100k  
1M  
10M 100M 1G  
100k  
1M  
10M 100M 1G  
f - Frequency - Hz  
f - Frequency - Hz  
f - Frequency - Hz  
Figure 17  
Figure 18  
Figure 19  
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SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
TYPICAL CHARACTERISTICS  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
2
0
2
0
2
0
R
= 1.3 kΩ  
R = 1.5 kΩ  
F
F
R
= 1.5 kΩ  
F
R
= 2 kΩ  
R
= 2 kΩ  
F
F
R
= 1.3 kΩ  
R = 1.3 kΩ  
F
F
R
= 1 kΩ  
F
–2  
–4  
–6  
–8  
–2  
–4  
–6  
–8  
–2  
–4  
–6  
–8  
V
= ± 5 V  
V
= ± 15 V  
V
= ± 5 V  
CC  
CC  
Gain = –1  
= 1 kΩ  
CC  
Gain = –1  
R = 1 kΩ  
L
Gain = –1  
R
V
= 150 Ω  
R
V
L
L
= 63 mV  
= 63 mV  
V
= 63 mV  
O(PP)  
O(PP)  
O(PP)  
100k  
1M  
10M 100M 1G  
100k  
1M  
10M 100M 1G  
100k  
1M  
10M 100M 1G  
f - Frequency - Hz  
f - Frequency - Hz  
f - Frequency - Hz  
Figure 20  
Figure 21  
Figure 22  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
OUTPUT AMPLITUDE  
vs  
FREQUENCY  
FREQUENCY  
FREQUENCY  
8
8
8
R = 1.2 kΩ  
F
R
= 1.2 kΩ  
R
= 1.5 kΩ  
F
F
R = 1.5 kΩ  
F
R
= 1.5 kΩ  
F
6
4
6
4
6
4
R
= 1.2 kΩ  
F
R
= 750 Ω  
F
R
= 750 Ω  
F
2
2
2
V
= ± 15 V  
V
= ± 5 V  
V
= ± 15 V  
CC  
Gain = 2  
= 150 Ω  
CC  
CC  
Gain = 2  
R = 1 kΩ  
L
0
0
0
Gain = 2  
R
R
= 150 Ω  
L
L
V
= 126 mV  
V
= 126 mV  
V
= 126 mV  
O(PP)  
O(PP)  
O(PP)  
–2  
–2  
–2  
100k  
1M  
10M 100M 1G  
100k  
1M  
100k  
1M  
10M 100M 1G  
10M  
100M  
1G  
f - Frequency - Hz  
f - Frequency - Hz  
f - Frequency - Hz  
Figure 23  
Figure 24  
Figure 25  
OUTPUT AMPLITUDE  
vs  
FREQUENCY  
2-V STEP RESPONSE  
5-V STEP RESPONSE  
8
1.2  
3
V
= ± 5 V  
CC  
Gain = 2  
R
= 1.2 kΩ  
F
0.8  
0.4  
2
1
R
R
= 1.2 kΩ  
= 150 Ω  
6
4
F
L
R
= 1.5 kΩ  
F
0.0  
0
2
–0.4  
–0.8  
–1.2  
–1  
–2  
–3  
V
= ± 5 V  
CC  
Gain = –1  
V
= ± 5 V  
CC  
Gain = 2  
0
R
R
= 1.3 kΩ  
= 150 Ω  
F
L
R
V
= 1 kΩ  
L
= 126 mV  
O(PP)  
–2  
100k  
1M  
10M 100M 1G  
0
200  
400  
600  
800  
1000  
0
200  
400  
600  
800  
1000  
f - Frequency - Hz  
t - Time - ns  
t - Time - ns  
Figure 26  
Figure 27  
Figure 28  
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TYPICAL CHARACTERISTICS  
INPUT OFFSET VOLTAGE  
vs  
FREE-AIR TEMPERATURE  
2-V STEP RESPONSE  
20-V STEP RESPONSE  
1.2  
1.0  
12  
10  
8
1.5  
1.3  
1.1  
0.9  
0.7  
0.5  
0.3  
V
= ± 15 V  
V
= ± 15 V  
CC  
Gain = 2  
CC  
Gain = 5  
0.8  
R
R
= 1.2 kΩ  
= 150 Ω  
R
R
= 1.2 kΩ  
= 150 Ω  
F
L
F
L
V
= ± 15 V  
0.6  
6
CC  
0.4  
4
0.2  
2
–0.0  
–0.2  
–0.4  
–0.6  
–0.8  
–1.0  
–1.2  
0
–2  
–4  
–6  
–8  
–10  
–12  
V
= ± 5 V  
CC  
0
200  
400  
600  
800  
1000  
0
200  
400  
600  
800  
1000  
–40 –20  
0
20  
40  
60  
80 100  
t - Time - ns  
t - Time - ns  
T
- Free-Air Temperature - °C  
A
Figure 29  
Figure 30  
Figure 31  
OUTPUT VOLTAGE  
vs  
INPUT BIAS CURRENT  
vs  
COMMON-MODE INPUT VOLTAGE  
vs  
SUPPLY VOLTAGE  
FREE-AIR TEMPERATURE  
SUPPLY VOLTAGE  
2.0  
1.9  
1.8  
1.7  
1.6  
1.5  
1.4  
1.3  
15  
13  
11  
9
15  
13  
11  
9
T
=25°C  
T
=25°C  
A
A
R
= 1 kΩ  
V
= ±15 V  
L
CC  
R
= 150 Ω  
L
7
7
V
= ± 5 V  
CC  
5
5
3
3
–40 –20  
0
20  
40  
60  
80 100  
5
7
9
11  
13  
15  
5
7
9
11  
13  
15  
T
- Free-Air Temperature - °C  
±V  
- Supply Voltage - V  
±V  
CC  
- Supply Voltage - V  
A
CC  
Figure 32  
Figure 33  
Figure 34  
SUPPLY CURRENT  
vs  
VOLTAGE & CURRENT NOISE  
OUTPUT VOLTAGE  
vs  
vs  
FREE-AIR TEMPERATURE  
SUPPLY VOLTAGE  
FREQUENCY  
15  
13  
11  
9
3.8  
3.6  
3.4  
3.2  
3.0  
2.8  
2.6  
2.4  
2.2  
100  
10  
V
T
A
= ± 15 V and ± 5 V  
CC  
= 25°C  
V
R
= ± 15 V  
= 150 Ω  
CC  
L
T
=85°C  
A
V
N
V
R
= ± 15 V  
CC  
= 1 kΩ  
L
T
=25°C  
A
7
V
R
= ± 5 V  
CC  
= 1 kΩ  
I
N
1
5
L
T
=–40°C  
A
3
V
= ± 5 V  
CC  
R
= 150 Ω  
L
1
0.1  
–40 –20  
0
20  
40  
60  
80 100  
5
7
9
11  
- Supply Voltage - V  
CC  
13  
15  
10  
100  
1k  
10k  
100k  
T
– Free-Air Temperature –  
C
± V  
f - Frequency - Hz  
A
Figure 35  
Figure 36  
Figure 37  
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APPLICATION INFORMATION  
theory of operation  
The THS408x is a high-speed, operational amplifier configured in a voltage feedback architecture. It is built  
using a 30-V, dielectrically isolated, complementary bipolar process with NPN and PNP transistors possessing  
f s of several GHz. This results in an exceptionally high performance amplifier that has a wide bandwidth, high  
T
slew rate, fast settling time, and low distortion. A simplified schematic is shown in Figure 38.  
(7) V  
+
CC  
(6) OUT  
IN(2)  
IN+ (3)  
(4) V  
CC  
Figure 38. THS4081 Simplified Schematic  
noise calculations and noise figure  
Noise can cause errors on very small signals. This is especially true when amplifying small signals, where  
signal-to-noise ratio (SNR) is very important. The noise model for the THS408x is shown in Figure 39. This  
model includes all of the noise sources as follows:  
e = Amplifier internal voltage noise (nV/Hz)  
n
IN+ = Noninverting current noise (pA/Hz)  
IN– = Inverting current noise (pA/Hz)  
e
= Thermal voltage noise associated with each resistor (e = 4 kTR )  
Rx x  
Rx  
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APPLICATION INFORMATION  
noise calculations and noise figure (continued)  
e
Rs  
e
n
R
Noiseless  
S
+
_
e
ni  
e
no  
IN+  
IN–  
e
Rf  
R
F
e
Rg  
R
G
Figure 39. Noise Model  
The total equivalent input noise density (e ) is calculated by using the following equation:  
ni  
2
2
2
e
e
IN  
R
IN–  
R
R
4 kTR  
4 kT R  
R
n
s
ni  
S
F
G
F
G
Where:  
–23  
k = Boltzmann’s constant = 1.380658 × 10  
T = Temperature in degrees Kelvin (273 +°C)  
R || R = Parallel resistance of R and R  
F
G
F
G
To get the equivalent output noise of the amplifier, just multiply the equivalent input noise density (e ) by the  
ni  
overall amplifier gain (A ).  
V
R
R
F
e
e
A
e
1
(noninverting case)  
no  
ni  
ni  
V
G
As the previous equations show, to keep noise at a minimum, small value resistors should be used. As the  
closed-loop gain is increased (by reducing R ), the input noise is reduced considerably because of the parallel  
G
resistance term. This leads to the general conclusion that the most dominant noise sources are the source  
resistor (R ) and the internal amplifier noise voltage (e ). Because noise is summed in a root-mean-squares  
S
n
method, noise sources smaller than 25% of the largest noise source can be effectively ignored. This can greatly  
simplify the formula and make noise calculations much easier to calculate.  
For more information on noise analysis, please refer to the Noise Analysis section in Operational Amplifier  
Circuits Applications Report (literature number SLVA043).  
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APPLICATION INFORMATION  
noise calculations and noise figure (continued)  
This brings up another noise measurement usually preferred in RF applications, the noise figure (NF). Noise  
figure is a measure of noise degradation caused by the amplifier. The value of the source resistance must be  
defined and is typically 50 in RF applications.  
2
e
ni  
NF  
10log  
2
e
Rs  
Because the dominant noise components are generally the source resistance and the internal amplifier noise  
voltage, we can approximate noise figure as:  
2
2
e
IN  
R
n
S
NF  
10log 1  
4 kTR  
S
Figure 40 shows the noise figure graph for the THS408x.  
NOISE FIGURE  
vs  
SOURCE RESISTANCE  
40.00  
f = 10 kHz  
35.00  
T
A
= 25°C  
30.00  
25.00  
20.00  
15.00  
10.00  
5.00  
0.00  
10  
100  
1k  
10k  
100k  
Source Resistance – R ()  
S
Figure 40. Noise Figure vs Source Resistance  
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APPLICATION INFORMATION  
driving a capacitive load  
Driving capacitive loads with high performance amplifiers is not a problem as long as certain precautions are  
taken. The first is to realize that the THS408x has been internally compensated to maximize its bandwidth and  
slew rate performance. When the amplifier is compensated in this manner, capacitive loading directly on the  
output will decrease the device’s phase margin leading to high frequency ringing or oscillations. Therefore, for  
capacitive loads of greater than 10 pF, it is recommended that a resistor be placed in series with the output of  
the amplifier, as shown in Figure 41. A minimum value of 20 should work well for most applications. For  
example, in 75-transmission systems, setting the series resistor value to 75 both isolates any capacitance  
loading and provides the proper line impedance matching at the source end.  
1.3 kΩ  
1.3 kΩ  
_
Input  
20 Ω  
Output  
LOAD  
THS408x  
+
C
Figure 41. Driving a Capacitive Load  
offset voltage  
Theoutputoffsetvoltage,(V )isthesumoftheinputoffsetvoltage(V )andbothinputbiascurrents(I )times  
OO  
IO  
IB  
the corresponding gains. The following schematic and formula can be used to calculate the output offset  
voltage:  
R
F
I
IB–  
R
G
+
+
V
I
V
O
R
S
I
IB+  
R
R
R
R
F
F
V
V
1
I
R
1
I
R
OO  
IO  
IB  
S
IB–  
F
G
G
Figure 42. Output Offset Voltage Model  
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APPLICATION INFORMATION  
general configurations  
When receiving low-level signals, limiting the bandwidth of the incoming signals is often required. The simplest  
way to accomplish this is to place an RC filter at the noninverting terminal of the amplifier (see Figure 43).  
R
R
F
G
V
1
O
+
V
I
R1  
V
C1  
f
–3dB  
2 R1C1  
R
O
F
1
1
V
R
1
sR1C1  
I
G
Figure 43. Single-Pole Low-Pass Filter  
circuit layout considerations  
To achieve the levels of high frequency performance of the THS408x, follow proper printed-circuit board high  
frequency design techniques. A general set of guidelines is given below. In addition, a THS408x evaluation  
board is available to use as a guide for layout or for evaluating the device performance.  
Ground planes – It is highly recommended that a ground plane be used on the board to provide all  
components with a low inductive ground connection. However, in the areas of the amplifier inputs and  
output, the ground plane can be removed to minimize the stray capacitance.  
Proper power supply decoupling – Use a 6.8-µF tantalum capacitor in parallel with a 0.1-µF ceramic  
capacitor on each supply terminal. It may be possible to share the tantalum among several amplifiers  
depending on the application, but a 0.1-µF ceramic capacitor should always be used on the supply terminal  
of every amplifier. In addition, the 0.1-µF capacitor should be placed as close as possible to the supply  
terminal. As this distance increases, the inductance in the connecting trace makes the capacitor less  
effective. The designer should strive for distances of less than 0.1 inches between the device power  
terminals and the ceramic capacitors.  
Sockets – Sockets are not recommended for high-speed operational amplifiers. The additional lead  
inductancein the socket pins will often lead to stability problems. Surface-mount packages soldered directly  
to the printed-circuit board is the best implementation.  
Short trace runs/compact part placements – Optimum high frequency performance is achieved when stray  
series inductance has been minimized. To realize this, the circuit layout should be made as compact as  
possible, thereby minimizing the length of all trace runs. Particular attention should be paid to the inverting  
input of the amplifier. Its length should be kept as short as possible. This will help to minimize stray  
capacitance at the input of the amplifier.  
Surface-mount passive components – Using surface-mount passive components is recommended for high  
frequency amplifier circuits for several reasons. First, because of the extremely low lead inductance of  
surface-mountcomponents, theproblemwithstrayseriesinductanceisgreatlyreduced. Second, thesmall  
size of surface-mount components naturally leads to a more compact layout, thereby minimizing both stray  
inductance and capacitance. If leaded components are used, it is recommended that the lead lengths be  
kept as short as possible.  
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general PowerPAD design considerations  
The THS408x is available packaged in a thermally-enhanced DGN package, which is a member of the  
PowerPAD family of packages. This package is constructed using a downset leadframe upon which the die  
is mounted [see Figure 44(a) and Figure 44(b)]. This arrangement results in the lead frame being exposed as  
a thermal pad on the underside of the package [see Figure 44(c)]. Because this thermal pad has direct thermal  
contact with the die, excellent thermal performance can be achieved by providing a good thermal path away  
from the thermal pad.  
The PowerPAD package allows for both assembly and thermal management in one manufacturing operation.  
During the surface-mount solder operation (when the leads are being soldered), the thermal pad can also be  
soldered to a copper area underneath the package. Through the use of thermal paths within this copper area,  
heat can be conducted away from the package into either a ground plane or other heat dissipating device.  
The PowerPAD package represents a breakthrough in combining the small area and ease of assembly of the  
surface mount with the, heretofore, awkward mechanical methods of heatsinking.  
DIE  
Side View (a)  
Thermal  
Pad  
DIE  
End View (b)  
Bottom View (c)  
NOTE A: The thermal pad is electrically isolated from all terminals in the package.  
Figure 44. Views of Thermally Enhanced DGN Package  
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APPLICATION INFORMATION  
general PowerPAD design considerations (continued)  
Although there are many ways to properly heatsink this device, the following steps illustrate the recommended  
approach.  
Thermal pad area (68 mils x 70 mils) with 5 vias  
(Via diameter = 13 mils)  
Figure 45. PowerPAD PCB Etch and Via Pattern  
1. Prepare the PCB with a top side etch pattern as shown in Figure 45. There should be etch for the leads as  
well as etch for the thermal pad.  
2. Place five holes in the area of the thermal pad. These holes should be 13 mils in diameter. Keep them small  
so that solder wicking through the holes is not a problem during reflow.  
3. Additionalvias may be placed anywhere along the thermal plane outside of the thermal pad area. This helps  
dissipate the heat generated by the THS408xDGN IC. These additional vias may be larger than the 13-mil  
diameter vias directly under the thermal pad. They can be larger because they are not in the thermal pad  
area to be soldered, so wicking is not a problem.  
4. Connect all holes to the internal ground plane.  
5. When connecting these holes to the ground plane, do not use the typical web or spoke via connection  
methodology. Webconnectionshaveahighthermalresistanceconnectionthatisusefulforslowingtheheat  
transfer during soldering operations. This makes the soldering of vias that have plane connections easier.  
In this application, however, low thermal resistance is desired for the most efficient heat transfer. Therefore,  
the holes under the THS408xDGN package should make their connection to the internal ground plane with  
a complete connection around the entire circumference of the plated-through hole.  
6. The top-side solder mask should leave the terminals of the package and the thermal pad area with its five  
holes exposed. The bottom-side solder mask should cover the five holes of the thermal pad area. This  
prevents solder from being pulled away from the thermal pad area during the reflow process.  
7. Apply solder paste to the exposed thermal pad area and all of the IC terminals.  
8. With these preparatory steps in place, the THS408xDGN IC is simply placed in position and run through  
the solder reflow operation as any standard surface-mount component. This results in a part that is properly  
installed.  
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APPLICATION INFORMATION  
general PowerPAD design considerations (continued)  
The actual thermal performance achieved with the THS408xDGN in its PowerPAD package depends on the  
application. In the example above, if the size of the internal ground plane is approximately 3 inches × 3 inches,  
then the expected thermal coefficient, θ , is about 58.4 C/W. For comparison, the non-PowerPAD version  
JA  
of the THS408x IC (SOIC) is shown. For a given θ , the maximum power dissipation is shown in Figure 46 and  
JA  
is calculated by the following formula:  
T
–T  
MAX  
A
P
D
JA  
Where:  
P
= Maximum power dissipation of THS408x IC (watts)  
= Absolute maximum junction temperature (150°C)  
= Free-ambient air temperature (°C)  
D
T
MAX  
T
A
θ
= θ + θ  
JA  
JC CA  
θ
θ
= Thermal coefficient from junction to case  
JC  
= Thermal coefficient from case to ambient air (°C/W)  
CA  
MAXIMUM POWER DISSIPATION  
vs  
FREE-AIR TEMPERATURE  
3.5  
DGN Package  
= 58.4°C/W  
T
= 150°C  
J
θ
JA  
2 oz. Trace And Copper Pad  
With Solder  
3
DGN Package  
= 158°C/W  
2 oz. Trace And  
Copper Pad  
2.5  
2
θ
JA  
SOIC Package  
High-K Test PCB  
θ
= 98°C/W  
JA  
Without Solder  
1.5  
1
SOIC Package  
Low-K Test PCB  
0.5  
0
θ
= 167°C/W  
JA  
–40  
–20  
0
20  
40  
60  
80  
100  
T
A
– Free-Air Temperature – °C  
NOTE A: Results are with no air flow and PCB size = 3”× 3”  
Figure 46. Maximum Power Dissipation vs Free-Air Temperature  
More complete details of the PowerPAD installation process and thermal management techniques can be found  
in the Texas Instruments Technical Brief, PowerPAD Thermally Enhanced Package. This document can be  
found at the TI web site (www.ti.com) by searching on the key word PowerPAD. The document can also be  
ordered through your local TI sales office. Refer to literature number SLMA002 when ordering.  
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175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
APPLICATION INFORMATION  
general PowerPAD design considerations (continued)  
The next consideration is the package constraints. The two sources of heat within an amplifier are quiescent  
power and output power. The designer should never forget about the quiescent heat generated within the  
device, especially multiamplifier devices. Because these devices have linear output stages (Class A-B), most  
of the heat dissipation is at low output voltages with high output currents. Figure 47 to Figure 50 show this effect,  
along with the quiescent heat, with an ambient air temperature of 50°C. Obviously, as the ambient temperature  
increases, the limit lines shown will drop accordingly. The area under each respective limit line is considered  
the safe operating area. Any condition above this line will exceed the amplifier’s limits and failure may result.  
When using V  
= ±5 V, there is generally not a heat problem, even with SOIC packages. But, when using V  
CC  
CC  
= ±15 V, the SOIC package is severely limited in the amount of heat it can dissipate. The other key factor when  
looking at these graphs is how the devices are mounted on the PCB. The PowerPAD devices are extremely  
useful for heat dissipation. But, the device should always be soldered to a copper plane to fully use the heat  
dissipation properties of the PowerPAD . The SOIC package, on the other hand, is highly dependent on how  
it is mounted on the PCB. As more trace and copper area is placed around the device, θ decreases and the  
JA  
heatdissipationcapabilityincreases. Thecurrentsandvoltagesshowninthesegraphsareforthetotalpackage.  
For the dual amplifier package (THS4082), the sum of the RMS output currents and voltages should be used  
to choose the proper package. The graphs shown assume that both amplifier’s outputs are identical.  
THS4081  
MAXIMUM RMS OUTPUT CURRENT  
vs  
THS4081  
MAXIMUM RMS OUTPUT CURRENT  
vs  
RMS OUTPUT VOLTAGE DUE TO THERMAL LIMITS  
RMS OUTPUT VOLTAGE DUE TO THERMAL LIMITS  
200  
1000  
100  
10  
T
T
= 150°C  
= 50°C  
Maximum Output  
Current Limit Line  
V
= ± 5 V  
= 150°C  
= 50°C  
J
A
CC  
V
= ± 15 V  
CC  
T
T
A
180  
160  
140  
120  
100  
J
Maximum Output  
Current Limit Line  
DGN Package  
= 58.4°C/W  
θ
JA  
Package With  
θ
< = 127°C/W  
JA  
SO-8 Package  
= 167°C/W  
θ
JA  
Low-K Test PCB  
80  
60  
40  
SO-8 Package  
= 98°C/W  
θ
JA  
High-K Test PCB  
SO-8 Package  
= 167°C/W  
θ
JA  
Low-K Test PCB  
Safe Operating  
Area  
Safe Operating  
Area  
20  
0
0
1
2
3
4
5
0
3
6
9
12  
15  
| V | – RMS Output Voltage – V  
O
| V | – RMS Output Voltage – V  
O
Figure 47  
Figure 48  
19  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
APPLICATION INFORMATION  
general PowerPAD design considerations (continued)  
THS4082  
THS4082  
MAXIMUM RMS OUTPUT CURRENT  
vs  
MAXIMUM RMS OUTPUT CURRENT  
vs  
RMS OUTPUT VOLTAGE DUE TO THERMAL LIMITS  
RMS OUTPUT VOLTAGE DUE TO THERMAL LIMITS  
1000  
100  
200  
Maximum Output  
Current Limit Line  
Package With  
64°C/W  
V
T
= ± 15 V  
Maximum Output  
Current Limit Line  
CC  
= 150°C  
θ
JA  
180  
160  
140  
120  
100  
J
T
= 50°C  
A
Both Channels  
SO-8 Package  
= 167°C/W  
SO-8 Package  
= 98°C/W  
θ
80  
60  
40  
JA  
Low-K Test PCB  
θ
10  
JA  
High-K Test PCB  
Safe Operating Area  
= ± 5 V  
DGN Package  
= 58.4°C/W  
V
CC  
= 150°C  
SO-8 Package  
SO-8 Package  
= 98°C/W  
θ
JA  
T
J
θ
= 167°C/W  
θ
JA  
Low-K Test PCB  
JA  
High-K Test PCB  
20  
0
T = 50°C  
A
Safe Operating Area  
Both Channels  
4
1
0
3
6
9
12  
15  
0
1
2
3
5
| V | – RMS Output Voltage – V  
O
| V | – RMS Output Voltage – V  
O
Figure 49  
Figure 50  
20  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
APPLICATION INFORMATION  
evaluation board  
AnevaluationboardisavailablefortheTHS4081(literaturenumberSLOP242)andTHS4082(literaturenumber  
SLOP239). This board has been configured for very low parasitic capacitance in order to realize the full  
performance of the amplifier. A schematic of the evaluation board is shown in Figure 51. The circuitry has been  
designed so that the amplifier may be used in either an inverting or noninverting configuration. For more  
information, please refer to the THS4081 EVM User’s Guide or the THS4082 EVM User’s Guide. To order the  
evaluation board, contact your local TI sales office or distributor.  
V
CC  
+
+
C2  
C3  
6.8 µF  
0.1 µF  
R4  
1.3 kΩ  
R5  
49.9 Ω  
IN+  
+
_
R3  
49.9 Ω  
OUT  
THS4081  
R2  
C1  
1.3 kΩ  
6.8 µF  
+
C4  
0.1 µF  
IN–  
V
CC  
R1  
49.9 Ω  
Figure 51. THS4081 Evaluation Board  
21  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
MECHANICAL INFORMATION  
D (R-PDSO-G**)  
PLASTIC SMALL-OUTLINE PACKAGE  
14 PIN SHOWN  
PINS **  
0.050 (1,27)  
8
14  
16  
DIM  
0.020 (0,51)  
0.014 (0,35)  
0.010 (0,25)  
0.197  
(5,00)  
0.344  
(8,75)  
0.394  
(10,00)  
M
A MAX  
14  
8
0.189  
(4,80)  
0.337  
(8,55)  
0.386  
(9,80)  
A MIN  
0.244 (6,20)  
0.228 (5,80)  
0.008 (0,20) NOM  
0.157 (4,00)  
0.150 (3,81)  
Gage Plane  
1
7
A
0.010 (0,25)  
0°8°  
0.044 (1,12)  
0.016 (0,40)  
Seating Plane  
0.004 (0,10)  
0.010 (0,25)  
0.004 (0,10)  
0.069 (1,75) MAX  
4040047/D 10/96  
NOTES: A. All linear dimensions are in inches (millimeters).  
B. This drawing is subject to change without notice.  
C. Body dimensions do not include mold flash or protrusion, not to exceed 0.006 (0,15).  
D. Falls within JEDEC MS-012  
22  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
THS4081, THS4082  
175-MHz LOW-POWER HIGH-SPEED AMPLIFIERS  
SLOS274C – DECEMBER 1999 – REVISED MAY 2000  
MECHANICAL INFORMATION  
DGN (S-PDSO-G8)  
PowerPAD PLASTIC SMALL-OUTLINE PACKAGE  
0,38  
0,25  
0,65  
M
0,25  
8
5
Thermal Pad  
(See Note D)  
0,15 NOM  
3,05  
2,95  
4,98  
4,78  
Gage Plane  
0,25  
0°6°  
1
4
0,69  
0,41  
3,05  
2,95  
Seating Plane  
0,10  
0,15  
0,05  
1,07 MAX  
4073271/A 01/98  
NOTES: A. All linear dimensions are in millimeters.  
B. This drawing is subject to change without notice.  
C. Body dimensions include mold flash or protrusions.  
D. The package thermal performance may be enhanced by attaching an external heat sink to the thermal pad. This pad is electrically  
and thermally connected to the backside of the die and possibly selected leads.  
E. Falls within JEDEC MO-187  
PowerPAD is a trademark of Texas Instruments.  
23  
POST OFFICE BOX 655303 DALLAS, TEXAS 75265  
IMPORTANT NOTICE  
Texas Instruments and its subsidiaries (TI) reserve the right to make changes to their products or to discontinue  
any product or service without notice, and advise customers to obtain the latest version of relevant information  
to verify, before placing orders, that information being relied on is current and complete. All products are sold  
subject to the terms and conditions of sale supplied at the time of order acknowledgment, including those  
pertaining to warranty, patent infringement, and limitation of liability.  
TI warrants performance of its semiconductor products to the specifications applicable at the time of sale in  
accordance with TI’s standard warranty. Testing and other quality control techniques are utilized to the extent  
TI deems necessary to support this warranty. Specific testing of all parameters of each device is not necessarily  
performed, except those mandated by government requirements.  
Customers are responsible for their applications using TI components.  
In order to minimize risks associated with the customer’s applications, adequate design and operating  
safeguards must be provided by the customer to minimize inherent or procedural hazards.  
TI assumes no liability for applications assistance or customer product design. TI does not warrant or represent  
that any license, either express or implied, is granted under any patent right, copyright, mask work right, or other  
intellectual property right of TI covering or relating to any combination, machine, or process in which such  
semiconductor products or services might be or are used. TI’s publication of information regarding any third  
party’s products or services does not constitute TI’s approval, warranty or endorsement thereof.  
Copyright 2000, Texas Instruments Incorporated  

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