AD8330ACPZ-R7 [ADI]

Low Cost DC to 150 MHz Variable Gain Amplifier; 低成本DC至150 MHz可变增益放大器
AD8330ACPZ-R7
型号: AD8330ACPZ-R7
厂家: ADI    ADI
描述:

Low Cost DC to 150 MHz Variable Gain Amplifier
低成本DC至150 MHz可变增益放大器

消费电路 商用集成电路 放大器 PC
文件: 总32页 (文件大小:751K)
中文:  中文翻译
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Low Cost DC to 150 MHz  
Variable Gain Amplifier  
AD8330  
FEATURES  
Fully differential signal path and also used  
with single-sided signals  
FUNCTIONAL BLOCK DIAGRAM  
16  
15  
14  
13  
ENBL  
OFST  
VPOS  
CNTR  
Inputs from 0.3 mV to 1 V rms, rail-to-rail outputs  
Differential RIN = 1 kΩ; ROUT (each output) 75 Ω  
Automatic offset compensation (optional)  
Linear-in-dB and linear-in-magnitude gain modes  
0 dB to 50 dB, for 0 V < VDBS < 1.5 V (30 mV/dB)  
Inverted gain mode: 50 dB to 0 dB at −30 mV/dB  
×0.03 to ×10 nominal gain for 15 mV < VMAG < 5 V  
Constant bandwidth: 150 MHz at all gains  
Low noise: 5 nV/√Hz typical at maximum gain  
Low distortion: ≤−62 dBc typical  
Low power: 20 mA typical at VS of 2.7 V to 6 V  
Available in a space-saving, 3 mm × 3 mm LFCSP package  
1
2
3
4
VPSI  
VPSO 12  
CM AND  
OFFSET  
BIAS AND V  
REF  
CONTROL  
OPHI  
11  
INHI  
OUTPUT  
STAGES  
VGA CORE  
OPLO  
10  
INLO  
MODE  
VDBS  
CMOP  
VMAG  
9
OUTPUT  
CONTROL  
GAIN INTERFACE  
CMGN  
COMM  
5
6
7
8
Figure 1.  
APPLICATIONS  
Pre-ADC signal conditioning  
75 Ω cable driving adjust  
AGC amplifiers  
Using VMAG, the basic 0 dB to 50 dB range can be repositioned  
to any value from ±0 dB higher (that is, ±0 dB to 70 dB) to at least  
30 dB lower (that is, –30 dB to +±0 dB) to suit the application,  
thereby providing an unprecedented gain range of over 100 dB.  
A unique aspect of the AD8330 is that its bandwidth and pulse  
response are essentially constant for all gains, over both the basic  
50 dB linear-in-dB range, but also when using the linear-in-  
magnitude function. The exceptional stability of the HF response  
over the gain range is of particular value in those VGA applications  
where it is essential to maintain accurate gain law-conformance at  
high frequencies.  
GENERAL DESCRIPTION  
The AD83301 is a wideband variable gain amplifier for applications  
requiring a fully differential signal path, low noise, well-defined  
gain, and moderately low distortion, from dc to 150 MHz. The  
input pins can also be driven from a single-ended source. The  
peak differential input is ±± V, allowing sine wave operation at  
1 V rms with generous headroom. The output pins can drive  
single-sided loads essentially rail-to-rail. The differential output  
resistance is 150 Ω. The output swing is a linear function of the  
voltage applied to the VMAG pin that internally defaults to 0.5 V  
providing a peak output of ±± V. This can be raised to 10 V p-p,  
limited by the supply voltage.  
An external capacitor at Pin OFST sets the high-pass corner of  
an offset reduction loop, whose frequency can be as low as 5 Hz.  
When this pin is grounded, the signal path becomes dc-coupled.  
When used to drive an ADC, an external common-mode control  
voltage at Pin CNTR can be driven to within 0.5 V of either ground  
or VS to accommodate a wide variety of requirements. By default,  
the two outputs are positioned at the midpoint of the supply, VS/±.  
Other features, such as two levels of power-down (fully off and a  
hibernate mode), further extend the practical value of this excep-  
tionally versatile VGA.  
The basic gain function is linear-in-dB, controlled by the voltage  
applied to Pin VDBS. The gain ranges from 0 dB to 50 dB for  
control voltages between 0 V and 1.5 V—a slope of 30 mV dB.  
The gain linearity is typically within ±0.1 dB. By changing the  
logic level on Pin MODE, the gain decreases over the same range,  
with an opposite slope. A second gain control port is provided at  
the VMAG pin and allows the user to vary the numeric gain from  
a factor of 0.03 to 10. All the parameters of the AD8330 have low  
sensitivities to temperature and supply voltages.  
The AD8330 is available in 16-lead LFCSP and 16-lead QSOP  
packages and is specified for operation from −40°C to +85°C.  
1
Protected by U.S. Patent No. 5,969,657; other patents pending.  
Rev. C  
Information furnished by Analog Devices is believed to be accurate and reliable. However, no  
responsibility is assumed by Analog Devices for its use, nor for any infringements of patents or other  
rights of third parties that may result from its use. Specifications subject to change without notice. No  
license is granted by implication or otherwise under any patent or patent rights of Analog Devices.  
Trademarks and registeredtrademarks arethe property of their respective owners.  
One Technology Way, P.O. Box 9106, Norwood, MA 02062-9106, U.S.A.  
Tel: 781.329.4700  
Fax: 781.461.3113  
www.analog.com  
©2006 Analog Devices, Inc. All rights reserved.  
 
 
AD8330  
TABLE OF CONTENTS  
Features .............................................................................................. 1  
Theory of Operation ...................................................................... 14  
Circuit Description .................................................................... 14  
Using the AD8330...................................................................... 20  
Applications..................................................................................... 25  
ADC Driving............................................................................... 25  
Simple AGC Amplifier .............................................................. 25  
Wide Range True RMS Voltmeter............................................ 26  
Outline Dimensions....................................................................... 28  
Ordering Guide .......................................................................... 29  
Applications....................................................................................... 1  
General Description......................................................................... 1  
Functional Block Diagram .............................................................. 1  
Revision History ............................................................................... 2  
Specifications..................................................................................... 3  
Absolute Maximum Ratings............................................................ 5  
ESD Caution.................................................................................. 5  
Pin Configurations and Function Descriptions ........................... 6  
Typical Performance Characteristics ............................................. 7  
REVISION HISTORY  
6/06—Rev. B to Rev. C  
10/04—Rev. A to Rev. B  
Changes to Absolute Maximum Ratings........................................4  
Changes to Ordering Guide.............................................................4  
Change to TPC 14 .............................................................................8  
Note added to CP-16 Package....................................................... 26  
Updated Format..................................................................Universal  
Changes to Figure 1.......................................................................... 1  
Deleted Figure 2................................................................................ 1  
Changes to Specifications Section.................................................. 3  
Change to Absolute Maximum Ratings......................................... 5  
Changes to Typical Performance Characteristics  
Summary Statement ......................................................................... 7  
Changes to Figure 14 and Figure 15............................................... 8  
Changes to Figure 31 and Figure 32............................................. 11  
Updated Outline Dimensions....................................................... 28  
4/03—Rev. 0 to Rev. A  
Updated Outline Dimensions....................................................... 26  
Rev. C | Page 2 of 32  
 
AD8330  
SPECIFICATIONS  
VS = 5 V, TA = ±5°C, CL = 1± pF on OPHI and OPLO, RL = ∞, VDBS = 0.75 V, VMODE = high, VMAG = O/C (0.5 V), VOFST = 0 V, differential  
operation, unless otherwise noted.  
Table 1.  
Parameter  
Conditions  
Min  
Typ  
Max  
Unit  
INPUT INTERFACE  
Full-Scale Input  
Pin INHI, Pin INLO  
VDBS = 0 V, differential drive  
VDBS = ±.5 V  
Pin-to-pin  
Either pin to COMM  
f = ± MHz, VDBS = ±.5 V; inputs ac-shorted  
±±.ꢀ  
±ꢀ.5  
800  
±2  
±6.3  
± k  
5
3.0  
±
V
mV  
Ω
pF  
nV/√Hz  
V
mV rms  
μV/°C  
V
Input Resistance  
Input Capacitance  
Voltage Noise Spectral Density  
Common-Mode Voltage Level  
Input Offset  
±.2 k  
Pin OFST connected to Pin COMM  
Drift  
2
Permissible CM Range±  
0
VS  
Common-Mode AC Rejection  
f = ± MHz, 0.± V rms  
f = 50 MHz  
−60  
−55  
dB  
dB  
OUTPUT INTERFACE  
Small Signal –3 dB Bandwidth  
Peak Slew Rate  
Pin OPHI, Pin OPLO  
0 V < VDBS < ±.5 V  
VDBS = 0  
±50  
±500  
±2  
±ꢀ.5  
2.5  
MHz  
V/μs  
V
V
V
nV/√Hz  
Ω
dBc  
dBc  
Peak-to-Peak Output Swing  
±±.8  
±ꢀ  
2.ꢀ  
±2.2  
2.6  
VMAG ≥ 2 V (peaks are supply limited)  
Pin CNTR O/C  
f = ± MHz, VDBS = 0  
Common-Mode Voltage  
Voltage Noise Spectral Density  
Differential Output Impedance  
HD22  
62  
Pin-to-pin  
±20  
±50  
−62  
−53  
±80  
VOUT = ± V p-p, f = ±0 MHz, RL = ± kΩ  
VOUT = ± V p-p, f = ±0 MHz, RL = ± kΩ  
Pin OFST  
CHPF on Pin OFST (0 V < VDBS < ±.5 V)  
CHPF = 3.3 nF, from OFST to CNTR (scales as ±/CHPF  
Pin CNTR  
HD32  
OUTPUT OFFSET CONTROL  
AC-Coupled Offset  
High-Pass Corner Frequency  
COMMON-MODE CONTROL  
Usable Voltage Range  
Input Resistance  
±0  
±00  
mV rms  
kHz  
)
0.5  
27  
ꢀ.5  
V
kΩ  
From Pin CNTR to VS/2  
VDBS, CMGN, and MODE pins  
CMGN connected to COMM  
CMGN O/C (VCMGN rises to 0.2 V)  
Mode high or low  
0.3 V ≤ VDBS ≤ ±.2 V  
VDBS = 0  
Flows out of Pin VDBS  
DECIBEL GAIN CONTROL  
Normal Voltage Range  
Elevated Range  
Gain Scaling  
Gain Linearity Error  
Absolute Gain Error  
Bias Current  
Incremental Resistance  
Gain Settling Time to 0.5 dB Error  
Mode Up/Down  
0 to ±.5  
0.2 to ±.7  
30  
V
V
33  
+0.35  
+2  
mV/dB  
dB  
dB  
nA  
MΩ  
ns  
−0.35 ±0.±  
−2  
±0.5  
±00  
±00  
250  
VDBS stepped from 0.05 V to ±.ꢀ5 V or ±.ꢀ5 V to 0.05 V  
Pin MODE  
Mode Up Logic Level  
Mode Down Logic Level  
LINEAR GAIN INTERFACE  
Peak Output Scaling, Gain vs. VMAG  
Gain Multiplication Factor vs. VMAG  
Usable Input Range  
Default Voltage  
Gain increases with VDBS, MODE = O/C  
Gain decreases with VDBS  
±.5  
3.8  
V
V
0.5  
ꢀ.2  
Pin VMAG, Pin CMGN  
See Circuit Description section  
Gain is nominal when VMAG = 0.5 V  
ꢀ.0  
×2  
V/V  
0
0.ꢀ8  
5
0.52  
V
V
kΩ  
MHz  
VMAG O/C  
0.5  
±50  
Incremental Resistance  
Bandwidth  
For VMAG ≥ 0.± V  
Rev. C | Page 3 of 32  
 
 
AD8330  
Parameter  
Conditions  
Min  
Typ  
Max  
Unit  
CHIP ENABLE  
Pin ENBL  
Logic Voltage for Full Shutdown  
Logic Voltage for Hibernate Mode  
Logic Voltage for Full Operation  
Current in Full Shutdown  
Current in Hibernate Mode  
Minimum Time Delay3  
POWER SUPPLY  
0.5  
±.7  
V
V
V
μA  
mA  
μs  
Output pins remain at CNTR  
±.3  
2.3  
±.5  
20  
±.5  
±.7  
±00  
VPSI, VPOS, VPSO, COMM, and CMOP pins  
VDBS = 0.75 V  
Supply Voltage  
Quiescent Current  
2.7  
6
27  
V
mA  
20  
± The use of an input common-mode voltage significantly different than the internally set value is not recommended due to its effect on noise performance.  
See Figure 56.  
2 See Typical Performance Characteristics for more detailed information on distortion in a variety of operating conditions.  
3 For minimum sized coupling capacitors.  
Rev. C | Page ꢀ of 32  
 
AD8330  
ABSOLUTE MAXIMUM RATINGS  
Table 2.  
Stresses above those listed under Absolute Maximum Ratings  
may cause permanent damage to the device. This is a stress  
rating only; functional operation of the device at these or any  
other conditions above those indicated in the operational  
section of this specification is not implied. Exposure to absolute  
maximum rating conditions for extended periods may affect  
device reliability.  
Parameter  
Rating  
Supply Voltage  
6 V  
Power Dissipation  
RQ Package±  
0.62 W  
CP Package  
±.67 W  
Input Voltage at Any Pin  
Storage Temperature Range  
θJA  
VS + 200 mV  
−65°C to +±50°C  
RQ-±6 Package  
CP-±6 Package  
±05.ꢀ°C/W  
60°C/W  
θJC  
RQ-±6 Package  
39°C/W  
Operating Temperature Range  
Lead Temperature (Soldering 60 sec)  
−ꢀ0°C to +85°C  
300°C  
±
Four-Layer JEDEC Board (252P).  
ESD CAUTION  
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as ꢀ000 V readily accumulate on  
the human body and test equipment and can discharge without detection. Although this product features  
proprietary ESD protection circuitry, permanent damage may occur on devices subjected to high energy  
electrostatic discharges. Therefore, proper ESD precautions are recommended to avoid performance  
degradation or loss of functionality.  
Rev. C | Page 5 of 32  
 
 
AD8330  
PIN CONFIGURATIONS AND FUNCTION DESCRIPTIONS  
16  
15  
14  
13  
OFST  
ENBL  
VPSI  
1
2
3
4
5
6
7
8
16 VPOS  
15 CNTR  
VSPI  
INHI  
1
2
3
4
12 VPSO  
11 OPHI  
10 OPLO  
AD8330 14 VPSO  
TOP VIEW 13 OPHI  
AD8330  
INHI  
TOP VIEW  
(Not to Scale)  
(Not to Scale)  
INLO  
MODE  
INLO  
12 OPLO  
MODE  
VDBS  
CMGN  
11 CMOP  
10 VMAG  
9
CMOP  
9
COMM  
5
6
7
8
Figure 2. 16-Lead LFCSP Pin Configuration  
Figure 3. 16-Lead QSOP Pin Configuration  
Table 3. 16-Lead LFCSP Pin Function Descriptions  
Table 4. 16-Lead QSOP Pin Function Descriptions  
Pin  
No.  
Pin  
No.  
Mnemonic Description  
Mnemonic Description  
±
2
VPSI  
INHI  
Positive Supply for Input Stages.  
Differential Signal Input, Positive Polarity.  
Differential Signal Input, Negative  
Polarity.  
Logic Input: Selects Gain Slope. High =  
±
2
3
OFST  
ENBL  
VPSI  
INHI  
Used in Offset Control Modes.  
Power Enable, Active High.  
Positive Supply for Input Stages.  
Differential Signal Input, Positive Polarity.  
Differential Signal Input, Negative  
Polarity.  
3
INLO  
MODE  
5
INLO  
gain up vs. VDBS  
Input for Linear-in-dB Gain Control  
Voltage, VDBS  
.
5
VDBS  
6
7
8
9
MODE  
VDBS  
Logic Input: Selects Gain Slope. High =  
.
gain up vs. VDBS  
Input for linear-in-dB Gain Control  
Voltage, VDBS  
.
Common Baseline for Gain Control  
Interfaces.  
Ground for Input and Gain Control Bias  
Circuitry.  
Input for Gain/Amplitude Control, VMAG  
Ground for Output Stages.  
6
7
CMGN  
COMM  
.
CMGN  
COMM  
Common Baseline for Gain Control  
Interfaces.  
Ground for Input and Gain Control Bias  
Circuitry.  
8
9
VMAG  
CMOP  
.
Differential Signal Output, Negative  
Polarity.  
Differential Signal Output, Positive  
Polarity.  
±0  
±±  
±2  
VMAG  
CMOP  
OPLO  
Input for Gain/Amplitude Control, VMAG  
Ground for Output Stages.  
Differential Signal Output, Negative  
Polarity.  
.
±0  
±±  
OPLO  
OPHI  
±2  
±3  
±ꢀ  
±5  
±6  
VPSO  
CNTR  
VPOS  
OFST  
ENBL  
Positive Supply for Output Stages.  
Common-Mode Output Voltage Control.  
Positive Supply for Inner Stages.  
Used in Offset Control Modes.  
Power Enable, Active High.  
±3  
±ꢀ  
±5  
±6  
OPHI  
VPSO  
CNTR  
VPOS  
Differential Signal Output, Positive Polarity.  
Positive Supply for Output Stages.  
Common-Mode Output Voltage Control.  
Positive Supply for Inner Stages.  
Rev. C | Page 6 of 32  
 
AD8330  
TYPICAL PERFORMANCE CHARACTERISTICS  
VS = 5 V, TA = ±5°C, CL = 1± pF, VDBS = 0.75 V, VMODE = high (or O/C) VMAG = O/C (0.5 V), RL = ∞, VOFST = 0, differential operation, unless  
otherwise noted.  
50  
45  
40  
35  
30  
25  
20  
15  
10  
5
2.0  
NORMALIZED @V  
= 0.75V  
DBS  
1.5  
LO MODE  
HI MODE  
1.0  
50MHz  
100MHz  
0.5  
10MHz, 50MHz  
0
–0.5  
–1.0  
–1.5  
–2.0  
1MHz  
1MHz  
10MHz  
100MHz  
0
0
0.25  
0.50  
0.75  
(V)  
1.00  
1.25  
1.50  
0
0.2  
0.4  
0.6  
0.8  
1.0  
1.2  
1.4  
1.6  
V
V
(V)  
DBS  
DBS  
Figure 4. Gain vs. VDBS  
Figure 7. Gain Error vs. VDBS at Various Frequencies  
10  
9
8
7
6
5
4
3
2
1
0
20  
15  
10  
5
2340 UNITS  
MODE = LO  
0
–30.630.530.430.330.230.130.029.929.829.729.629.529.429.329.229.129.0  
20  
MODE = HI  
15  
10  
5
0
29.1 29.2 29.3 29.4 29.5 29.6 29.7 29.8 29.9 30.0 30.1 30.2 30.3 30.4 30.5 30.6  
0
1
2
3
4
5
GAIN SCALING (mV/dB)  
V
(V)  
MAG  
Figure 5. Linear Gain Multiplication Factor vs. VMAG  
Figure 8. Gain Slope Histogram  
1.0  
0.8  
0.6  
0.4  
0.2  
60  
V
= 1.5V  
DBS  
50  
40  
1.2V  
0.9V  
0.6V  
30  
20  
0.3V  
0V  
T = –40°C  
10  
0
–0.2  
–0.4  
–0.6  
–0.8  
–1.0  
0
–10  
–20  
–30  
–40  
–50  
T = +85°C  
T = +25°C  
0
0.2  
0.4  
0.6  
0.8  
1.0  
1.2  
1.4  
1.6  
100k  
1M  
10M  
FREQUENCY (Hz)  
100M  
500M  
V
(V)  
DBS  
Figure 9. Frequency Response in 10 dB Steps for Various Values of VDBS  
Figure 6. Gain Linearity Error Normalized at 25°C vs. VDBS  
at Three Temperatures, f = 1 MHz  
,
Rev. C | Page 7 of 32  
 
 
 
AD8330  
50  
25  
20  
15  
10  
5
V
= 4.8V  
1.52V  
MAG  
1048 UNITS  
ENABLE MODE  
40  
30  
0.48V  
0.15V  
20  
10  
0.048V  
0.015V  
0
–10  
–20  
–30  
–40  
100k  
0
1M  
10M  
FREQUENCY (Hz)  
100M  
500M  
DIFFERENTIAL OFFSET (mV)  
Figure 10. Frequency Response for Various Values of VMAG  
VDBS = 0.75 V  
,
Figure 13. Differential Input Offset Histogram  
10  
8
10  
0
V
= 0.1V  
DBS  
–10  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
–90  
6
4
2
0
100k  
1M  
10M  
100M  
300M  
100k  
1M  
10M  
FREQUENCY (Hz)  
100M  
FREQUENCY (Hz)  
Figure 11. Group Delay vs. Frequency  
Figure 14. Output Balance Error vs. Frequency for a Representative Part  
0
200  
190  
180  
170  
160  
150  
140  
130  
120  
110  
100  
–1  
–2  
–3  
–4  
–5  
–6  
–7  
T = –40°C  
T = +25°C  
T = +85°C  
1.2 1.4  
0
0.2  
0.4  
0.6  
0.8  
1.0  
1.6  
100k  
1M  
10M  
100M  
300M  
V
(V)  
FREQUENCY (Hz)  
DBS  
Figure 12. Differential Output Offset vs. VDBS for Three Temperatures,  
for a Representative Part  
Figure 15. Output Impedance vs. Frequency  
Rev. C | Page 8 of 32  
AD8330  
6000  
5000  
4000  
3000  
2000  
1000  
0
90  
80  
70  
60  
50  
40  
30  
20  
10  
0
V
V
= 1.5V  
DBS = 1.5V  
OFST: ENABLED  
DISABLED  
DBS  
f = 1MHz  
V
= 0.75V  
DBS  
V
= 0V  
DBS  
–10  
50k 100k  
0
0.5  
1.0  
1.5  
2.0  
2.5  
1M  
FREQUENCY (Hz)  
10M  
100M  
V
(V)  
MAG  
Figure 16. CMRR vs. Frequency  
Figure 19. Output Referred Noise vs. VMAG  
80  
70  
60  
50  
40  
30  
20  
10  
0
1500  
V
= 0.5V  
MAG  
T = +85°C  
T = +25°C  
f = 1MHz  
= 0.5V  
f = 1MHz  
V
MAG  
1200  
900  
600  
300  
0
T = +85°C  
T = +25°C  
T = –40°C  
T = –40°C  
0
0.2  
0.4  
0.6  
0.8  
1.0  
1.2  
1.4  
1.6  
0
0.2  
0.4  
0.6  
0.8  
1.0  
1.2  
1.4  
1.6  
V
(V)  
V
(V)  
DBS  
DBS  
Figure 17. Output Referred Noise vs. VDBS for Three Temperatures  
Figure 20. Input Referred Noise vs. VDBS for Three Temperatures  
700  
180  
f = 1MHz  
160  
f = 1MHz  
600  
140  
500  
400  
300  
200  
100  
0
V
= 0.125V  
MAG  
120  
100  
80  
60  
40  
20  
0
V
= 0.5V  
MAG  
V
= 2V  
MAG  
0
0.5  
1.0  
1.5  
2.0  
2.5  
0
0.2  
0.4  
0.6  
0.8  
1.0  
1.2  
1.4  
1.6  
V
(V)  
V
(V)  
MAG  
DBS  
Figure 18. Output Referred Noise vs. VMAG,  
VDBS = 0.75 V  
Figure 21. Input Referred Noise vs. VDBS for Three Values of VMAG  
Rev. C | Page 9 of 32  
 
AD8330  
7
0
–10  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
V
= 1.5V  
DBS  
f = 10MHz  
6
5
4
3
2
1
0
HD3, R = 1kΩ  
L
HD2, R = 1kΩ  
L
0
0.3  
0.6  
0.9  
(V p-p)  
1.2  
1.5  
100k  
1M  
10M  
FREQUENCY (Hz)  
100M  
100M  
50  
V
OUT  
Figure 25. Harmonic Distortion vs. VOUT , VMAG = 0.5 V  
Figure 22. Input Referred Noise vs. Frequency  
0
–10  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
0
V
= 0.75V  
DBS  
f = 10MHz  
V
R
= 1V p-p  
= 1kΩ  
OUT  
–10  
L
–20  
–30  
–40  
–50  
–60  
–70  
–80  
1
HD2 AND HD3, R = 150Ω  
L
HD3  
HD3, R = 1kΩ  
L
HD2  
HD2, R = 1kΩ  
L
1
OUTPUT AMPLITUDE HARD LIMITED  
0
1
2
3
4
5
100k  
1M  
10M  
FREQUENCY (Hz)  
V
(V p-p)  
OUT  
Figure 26. Harmonic Distortion vs. VOUT , VMAG = 2.0 V  
Figure 23. Harmonic Distortion vs. Frequency  
0
–10  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
0
–10  
–20  
–30  
–40  
–50  
–60  
–70  
V
= 0.75V  
= 1V p-p  
= 1k  
f = 10MHz  
DBS  
V
R
= 1V p-p  
V
OUT  
= 1kΩ  
OUT  
R
L
L
HD3  
HD2  
HD3  
HD2  
30  
0
10  
20  
40  
0
0.2  
0.4  
0.6  
0.8  
1.0  
1.2  
1.4  
1.6  
C
(pF)  
V
(V)  
LOAD  
DBS  
Figure 24. Harmonic Distortion vs. CLOAD  
Figure 27. Harmonic Distortion vs. VDBS  
Rev. C | Page ±0 of 32  
AD8330  
30  
25  
20  
15  
10  
5
33  
28  
23  
18  
13  
8
10  
0
23  
f = 10MHz  
f = 10MHz  
13  
–10  
–20  
–30  
–40  
–50  
3
f = 50MHz  
–7  
–17  
–27  
–37  
0
3
0
0.4  
0.6  
0.8  
1.0  
1.2  
1.4  
1.6  
0
0.2  
0.4  
0.6  
0.8  
1.0  
1.2  
1.4  
1.6  
0.2  
V
(V)  
DBS  
V
(V)  
DBS  
Figure 31. OIP3 vs. VDBS  
Figure 28. Input Voltage 1 dBV vs. VDBS  
40  
35  
30  
25  
20  
15  
10  
5
43  
38  
33  
28  
23  
18  
13  
8
20  
10  
0
33  
23  
13  
3
f = 10MHz  
f = 10MHz  
–10  
f = 50MHz  
–20  
–30  
–40  
–7  
–17  
–27  
3
1.6  
0
0
1
2
3
4
5
6
0
0.4  
0.6  
0.8  
1.0  
1.2  
1.4  
0.2  
V
(V)  
V
(V)  
MAG  
MAG  
Figure 29. Output Voltage 1 dB vs. VMAG  
Figure 32. OIP3 vs. VMAG  
0
1.5  
1.0  
V
= 0.75V  
= 1V p-p  
DBS  
V
–10  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
–90  
OUT  
0.5  
V
= 0V  
DBS  
0
–0.5  
–1.0  
–1.5  
1M  
10M  
100M  
–50  
–25  
0
25  
50  
75  
100  
FREQUENCY (Hz)  
TIME (ns)  
Figure 30. IM3 Distortion vs. Frequency  
Figure 33. Full-Scale Transient Response, VDBS = 0 V  
Rev. C | Page ±± of 32  
AD8330  
1.5  
1.0  
0.5  
0
1V  
V
= 0.75V  
DBS  
–0.5  
–1.0  
1V  
400ns  
–1.5  
–50  
–25  
0
25  
50  
75  
100  
TIME (ns)  
Figure 37. VDBS Interface Response, Top: VDBS, Bottom: VOUT  
Figure 34. Full-Scale Transient Response, VDBS = 0.75 V,  
f = 1 MHz, VOUT = 2 V p-p  
1.5  
1.0  
2V  
0.5  
V
= 1.5V  
DBS  
0
–0.5  
–1.0  
–1.5  
1mV  
400ns  
–50  
–25  
0
25  
50  
75  
100  
TIME (ns)  
Figure 35. Full-Scale Transient Response, VDBS = 1.5 V,  
f = 1 MHz, VOUT = 2 V p-p  
Figure 38. VMAG Interface Response, Top: VMAG, Bottom: VOUT  
500mV  
1V  
V
= 5V  
MAG  
C
= 12pF  
L
V
= 0.5V  
MAG  
C
= 54pF  
L
C
= 24pF  
L
V
= 0.05V  
MAG  
12.5ns  
100mV  
12.5ns  
Figure 36. Transient Response vs. Various Load Capacitances, G = 25 dB  
Figure 39. Transient Response vs. VMAG  
Rev. C | Page ±2 of 32  
AD8330  
26  
24  
22  
20  
18  
16  
14  
4.00V  
OUTPUT  
+85°C  
+25°C  
–40°C  
INPUT  
50mV  
25ns  
0
0.2  
0.4  
0.6  
0.8  
1.0  
1.2  
1.4  
1.6  
V
(V)  
DBS  
Figure 40. Overdrive Response, VDBS = 1.5 V, VMAG = 0.5 V, 18.5 dB Overdrive  
Figure 43. Supply Current vs. VDBS at Three Temperatures  
2V  
3.125V  
2.5V  
1.875V  
3.125V  
2.5V  
1.875V  
1V  
400ns  
100ns  
Figure 41. ENBL Interface Response. Top: VENBL; Bottom: VOUT, f = 10 MHz  
Figure 44. CNTR Transient Response, Top: Input to CNTR,  
Bottom: VOUT Single-Ended  
–10  
V
= 0.75V  
DBS  
–20  
–30  
V
–40  
PSI  
–50  
–60  
V
PSO  
V
POS  
–70  
–80  
–90  
–100  
–110  
1M  
10M  
FREQUENCY (Hz)  
100M  
200M  
Figure 42. PSRR vs. Frequency  
Rev. C | Page ±3 of 32  
AD8330  
OUTPUT IS xl  
INPUT IS xl  
G = I /I  
N
N
D
D
LOOP  
AMPLIFIER  
THEORY OF OPERATION  
CIRCUIT DESCRIPTION  
(1–x) I  
2
(1–x) I  
2
(1–x) I  
2
(1+x) I  
2
D
D
N
N
+
Many monolithic variable gain amplifiers use techniques that  
share common principles that are broadly classified as trans-  
linear. This term refers to circuit cells whose functions depend  
directly on the very predictable properties of bipolar junction  
transistors, notably the linear dependence of their transcon-  
ductance on collector current. Since the discovery of these  
cells in 1967, and their commercial exploitation in products  
developed during the early 1970s, accurate wide bandwidth  
analog multipliers, dividers, and variable gain amplifiers have  
invariably employed translinear principles.  
Q1  
Q4  
Q2  
Q3  
I
DENOMINATOR  
BIAS CURRENT BIAS CURRENT  
NUMERATOR  
I
N
D
Figure 45. Basic Core  
ENBL  
VPSI  
OFST  
BIAS AND  
VPOS  
CNTR  
VPSO  
CM MODE AND  
Although these techniques are well understood, the realization  
of a high performance variable gain amplifier (VGA) requires  
special technologies and attention to many subtle details in  
its design. The AD8330 is fabricated on a proprietary silicon-  
on-insulator, complementary bipolar IC process and draws  
on decades of experience in developing many leading edge  
products using translinear principles to provide an unprecedented  
level of versatility.  
V
OFFSET CONTROL  
REF  
INHI  
OPHI  
AD8330  
OUTPUT  
STAGES  
INLO  
VGA CORE  
OPLO  
CMOP  
OUTPUT  
Figure 45 shows a basic representative cell comprising just four  
transistors. This, or a very closely related form, is at the heart  
of most translinear multipliers, dividers, and VGAs. The key  
concepts are as follows: First, the ratio of the currents in the  
left-hand and right-hand pairs of transistors is identical, rep-  
resented by the modulation factor, x, with values between −1  
and +1. Second, the input signal is arranged to modulate the  
fixed tail current, ID, to cause the variable value of x, introduced  
in the left-hand pair, to be replicated in the right-hand pair,  
and, thus, generate the output by modulating its nominally  
fixed tail current, IN. Third, the current gain of this cell is  
exactly G = IN/ID over many decades of variable bias current.  
MODE  
GAIN INTERFACE  
CMGN  
CONTROL  
VDBS  
COMM  
VMAG  
Figure 46. Block Schematic  
Overall Structure  
Figure 46 shows a block schematic of the AD8330 locating the  
key sections. More detailed descriptions of its structure and  
features are provided throughout the Theory of Operation  
section; however, Figure 46 provides a general overview of its  
capabilities.  
The VGA core contains a more elaborate version of the cell  
shown in Figure 45. The current, ID, is controlled exponentially  
(linear-in-decibels) through the decibel gain interface at  
Pin VDBS and its local common, Pin CMGN. The gain span  
(that is, the decibel difference between maximum and  
minimum values) provided by this control function is slightly  
more than 50 dB. The absolute gain from input to output is a  
function of source and load impedance, and also depends on  
the voltage on a second gain control pin (VMAG), explained in  
the Normal Operating Conditions section.  
In practice, the realization of the full potential of this circuit  
involves many other factors, but these three elementary ideas  
remain essential.  
By varying IN, the overall function is that of a two-quadrant  
analog multiplier, exhibiting a linear relationship to both the  
signal modulation factor (x) and this numerator current. On the  
other hand, by varying ID, a two-quadrant analog divider is  
realized, having a hyperbolic gain function with respect to the  
input factor, x, controlled by this denominator current. The  
AD8330 exploits both modes of operation. However, since a  
hyperbolic gain function is generally of less value than one in  
which the decibel gain is a linear function of a control input, a  
special interface is included to provide either increasing or  
decreasing exponential control of ID.  
Normal Operating Conditions  
To minimize confusion, normal operating conditions are  
defined as follows:  
The input pins are voltage driven (the source impedance is  
assumed to be zero);  
The output pins are open circuited (the load impedance is  
assumed to be infinite);  
Rev. C | Page ±ꢀ of 32  
 
 
 
 
 
 
AD8330  
output interface, rather than an op amp style voltage-mode  
Pin VMAG is unconnected setting up the output bias  
current (IN in the four-transistor gain cell) to its nominal  
value;  
output, is preferable in high speed applications because the  
effects of complex reactive loads on the gain and phase can be  
better controlled. The top end of the AD8330 ac response is  
optimally flat for a 12 pF load on each pin, but this is not critical  
and the system remains stable for any value of load capacitance  
including zero.  
Pin CMGN is grounded; and  
MODE is either tied to a logic high or left unconnected, to  
set the up gain mode.  
The effects of other operating conditions are considered  
separately.  
Another useful feature of this VGA in connection with the  
driving of an ADC is that the peak output magnitude can be  
precisely controlled by the voltage on Pin VMAG. Usually, this  
voltage is internally preset to 500 mV, and the peak differential,  
unloaded output swing is 2 V 3ꢀ. However, any voltage  
from zero to at least 5 V can be applied to this pin to alter the  
peak output in an exactly proportional way. Because either  
output pin can swing rail-to-rail, which in practice means down  
to at least 0.35 V and to within the same voltage below the  
supply, the peak-to-peak output between these pins can be as  
high as 10 V using VS = 6 V.  
Throughout this data sheet, the end-to-end voltage gain for  
the normal operating conditions are referred to as the basic  
gain. Under these conditions, it runs from 0 dB when VDBS = 0  
(where this voltage is more exactly measured with reference to  
Pin CMGN, which is not necessarily tied to ground) up to  
50 dB for VDBS = 1.5 V. The gain does not fold over when the  
VDBS pin is driven below ground or above its nominal full-  
scale value.  
The input is accepted at the Differential Port INHI/INLO.  
These pins are internally biased to roughly the midpoint of the  
supply, VS (it is actually ~2.75 V for VS = 5 V, VDBS = 0, and  
1.5 V for VS = 3 V), but the AD8330 is able to accept a forced  
common-mode value, from zero to VS, with certain limitations.  
This interface provides good common-mode rejection up to  
high frequencies (see Figure 16) and, thus, can be driven in  
either a single-sided or differential manner. However, operation  
using a differential drive is preferable, and this is assumed in the  
specifications, unless otherwise stated.  
CM MODE  
FEEDBACK  
VPSI  
VPSO  
TRANSIMPEDANCE  
OUTPUT STAGE  
500  
500Ω  
INHI  
OPHI  
R
=
150Ω  
OPLO  
ΔV = 0  
ΔV = 0  
OUT  
INLO  
O/P CM-MODE  
NORMALLY  
AT V /2  
P
CNTR  
LINEAR-IN-dB  
INTERFACE  
MAGNITUDE  
INTERFACE  
The pin-to-pin input resistance is specified as 950 Ω 20ꢀ. The  
driving-point impedance of the signal source can range from  
zero up to values considerably in excess of this resistance, with a  
corresponding variation in noise figure (see Figure 53). In most  
cases, the input is coupled via two capacitors, chosen to provide  
adequate low frequency transmission. This results in the  
minimum input noise that increases when some other  
common-mode voltage is forced onto these pins. The short-  
circuit, input referred noise at maximum gain is approximately  
5 nV/√Hz.  
100µA  
VMAG  
MODE  
VDBS  
V
MAG  
V
DBS  
12.65µA–4mA OR  
4mA–12.65µA  
5kΩ  
COMM  
COMM  
Figure 47. Schematic of Key Components  
Linear-in-dB Gain Control (VDBS  
)
All Analog Devices, Inc. VGAs featuring a linear-in-dB gain  
law, such as the X-AMP® family, provide exact, constant gain  
scaling over the fully specified gain range, and the deviation  
from the ideal response is within a small fraction of a dB. For  
the AD8330, the scaling of both of its gain interfaces is  
substantially independent of process, supply voltage, or  
temperature. The basic gain, GB, is simply  
Output Pin OPHI and Output Pin OPLO operate at a common-  
mode voltage at the midpoint of the supply, VS/2, within a few  
millivolts. This ensures that an analog-to-digital converter  
(ADC) attached to these outputs operates within the often  
narrow range permitted by their design. When a common-  
mode voltage other than VS/2 is required at this interface, it can  
easily be forced by applying an externally provided voltage to  
the output centering pin, CNTR. This voltage can run from zero  
to the full supply, though the use of such extreme values leaves  
only a small range for the differential output signal swing.  
VDBS  
30 mV  
GB  
(dB  
)
=
(1)  
(2)  
where VDBS is in volts. Alternatively, this can be expressed as a  
numerical gain magnitude  
V
The differential impedance measured between OPHI and  
OPLO is 150 Ω 20ꢀ. It follows that both the gain and the  
full-scale voltage swing depend on the load impedance; both are  
nominally halved when this is also 150 Ω. A fixed impedance  
DBS  
GBN = 100.6V  
Rev. C | Page 15 of 32  
 
AD8330  
The gain can be increased or decreased by changing the voltage,  
VMAG, applied to the VMAG pin. The internally set default value  
of 500 mV is derived from the same band gap reference that  
determines the decibel scaling. The tolerance on this voltage,  
and mismatches in certain on-chip resistors, cause small gain  
errors (see the Specifications section). Though not all appli-  
cations of VGAs demand accurate gain calibration, it is a  
valuable asset in many situations, for example, in reducing  
design tolerances.  
VMAG  
0.5 V  
(3)  
(4)  
GT = GBN  
Using this to calculate the output voltage  
OUT = ± × GIN × VIN × VMAG  
V
from which it is apparent that the AD8330 implements a linear,  
two-quadrant multiplier with a bipolar VIN and a unipolar VMAG  
Because the AD8330 is a dc-coupled system, it can be used in  
many applications where a wideband two-quadrant multiplier  
function is required, from dc up to about 100 MHz from either  
input (VIN or VMAG).  
.
Figure 47 shows the core circuit in more detail. The range and  
scaling of VDBS is independent of the supply voltage, and the  
Gain Control Pin VDBS presents a high incremental input re-  
sistance (~100 Mꢀ) with a low bias current (~100 nA), making  
the AD8330 easy to drive from a variety of gain control sources.  
As VMAG is varied, so also is the peak output magnitude, up to a  
point where this is limited by the absolute output limit imposed  
by the supply voltage. In the absence of the latter effect, the  
peak output into an open circuited load is just  
Inversion of the Gain Slope  
The AD8330 supports many features that further extend the  
versatility of this VGA in wide bandwidth, gain control systems.  
For example, the Logic Pin MODE allows the slope of the gain  
function to be inverted, so that the basic gain starts at +50 dB  
for a gain voltage, VDBS, of zero and runs down to 0 dB when  
this voltage is at its maximum specified value of 1.5 V. The basic  
forms of these two gain control modes are shown in Figure 48.  
V
OUT_PK = ±4 VMAG  
(5)  
(6)  
whereas for a load resistance of RL directly across OPHI and  
OPLO, it is  
±± VMAGRL  
VOUT _ PK  
=
(RL +150  
)
50  
These capabilities are illustrated in Figure 49, where VS = 6 V,  
MODE PIN  
LOW, GAIN  
DECREASES  
MODE PIN  
HIGH, GAIN  
INCREASES  
RL = O/C, VDBS = 0 V, VIN is swept from −±.5 V dc to +±.5 V dc, and  
MAG is set to 0.±5 V, 0.5 V, 1 V, and ± V. Except for the last value  
V
WITH V  
WITH V  
40  
30  
20  
10  
0
DBS  
DBS  
of VMAG, the peak output follows Equation 5. This exceeds the  
supply-limited value when VMAG = ± V and the peak output is  
±5.65 V, that is, ±6 V − 0.35 V. Figure 50 demonstrates the high  
speed multiplication capability. The signal input is a 100 MHz,  
0.1 V sine wave, VDBS is set to 0.6 V, and VMAG is a square wave at  
5 MHz alternating from 0.±5 V to 1 V. The output is ideally a  
sine wave switching in amplitude between 0.5 V and ± V.  
8
V
= 2V  
1V  
MAG  
6
4
0
0.25  
0.50  
0.75  
1.0  
1.25  
1.50  
V
(V)  
DBS  
Figure 48. The Two Gain Directions of the AD8330  
0.5V  
2
Gain Magnitude Control (VMAG  
)
0.25V  
0
In addition to the basic linear-in-dB control, two more gain  
control features are provided. The voltage applied to Pin VMAG  
provides accurate linear-in-magnitude gain control with a very  
rapid response. The bandwidth of this interface is >100 MHz.  
When this pin is unconnected, VMAG assumes its default value of  
500 mV (see Figure 47) to set up the basic 0 dB to 50 dB range.  
However, any voltage from ~15 mV to 5 V can be applied to  
either lower the gain by up to 30 dB or to raise it by ±0 dB. The  
combined gain span is thus 100 dB, that is, the 50 dB basic gain  
span provided by VDBS plus a 60 dB linear-in-magnitude span  
provided by VMAG. The latter modifies the basic numerical gain  
–2  
–4  
–6  
–8  
–3  
–2  
–1  
0
1
2
3
V
( V)  
IN  
Figure 49. Effect of VMAG on Gain and Peak Output  
G
BN to generate a total gain, expressed here in magnitude terms  
Rev. C | Page ±6 of 32  
 
 
 
AD8330  
VIN  
0.10  
0.05  
0
Amplitude/Phase Response  
The ac response of the AD8330 is remarkably consistent not  
only over the full 50 dB of its basic gain range, but also with  
changes of gain due to alteration of VMAG, as demonstrated in  
Figure 51. This is an overlay of two sets of results: first with a  
very low VMAG of 16 mV that reduces the overall gain by 30 dB  
[±0 × log10(500 mV/16 mV)]; second, with VMAG = 5 V that  
increases the gain by ±0 dB = ±0 × log10(5 V/0.5 V).  
–0.05  
–0.10  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0
VMAG  
VOUT  
90  
70  
2.5  
2.0  
1.5  
1.0  
50  
0.5  
0
30  
–0.5  
–1.0  
–1.5  
–2.0  
10  
–10  
–30  
–50  
100k  
0
–400  
–300  
–200  
–100  
0
100  
200  
300  
TIME (ns)  
1M  
10M  
100M  
300M  
Figure 50. Using VMAG in Modulation Mode  
G = +70dB  
–50  
Another gain related feature allows both gain control ranges  
to be accurately raised by ±00 mV. To enable this offset, open  
circuit Pin 6 (CMGN) and add a 0.1 μF capacitor to ground.  
In use, the nominal range for VDBS extends from 0.± V to 1.7 V  
and VMAG from 0.± V to 5.± V. These specifications apply for any  
supply voltage. This allows the use of DACs whose output range  
does not include ground as sources for the gain control function(s).  
–100  
–150  
–200  
–250  
–300  
–350  
G = –20dB  
100M 300M  
10k  
100k  
1M  
10M  
FREQUENCY (Hz)  
Figure 51. AC Performance over a 100 dB Gain Range Obtained by  
Using Two Values of VMAG  
Note that the ±00 mV that appears on this pin affects the  
response to an externally applied VMAG, but when Pin VMAG is  
unconnected, the internally set default value of 0.5 V still applies.  
Furthermore, Pin CMGN can, if desired, be driven by a user  
supplied voltage to reposition the baseline for VDBS (or for an  
externally applied VMAG) to any other voltage up to 500 mV. In  
all cases, the gain scaling, its law conformance, and temperature  
stability are unaffected.  
This 50 dB step change in gain produces two sets of gain curves,  
having a total gain span of 100 dB. It is apparent that the ampli-  
tude and phase response are essentially independent of the gain  
over this wide range, an aspect of the AD8330 performance  
potential unprecedented in any prior VGA.  
It is unusual for an application to require such a wide range of  
gains, of course; and as a practical matter, the peak output  
voltage for VMAG = 16 mV is reduced by the factor 16/500,  
compared to its nominal value of ±± V, to only ±64 mV. As  
already noted, most applications of VGAs require that they  
operate in a mode that is predominantly of either an IVGA or  
OVGA style, rather than mixed modes.  
Two Classes of Variable Gain Amplifiers  
Note that there are two broad classes of VGAs. The first type is  
designed to cope with a very wide range of input amplitudes  
and, by virtue of its gain control function, compress this range  
down to an essentially constant output. This is the function  
needed in an AGC system. Such a VGA is called an IVGA,  
referring to a structure optimized to address a wide range of  
input amplitudes. By contrast, an OVGA is optimized to deliver  
a wide range of output values while operating with an essentially  
constant input amplitude. This function might be needed, for  
example, in providing a variable drive to a power amplifier.  
With this limitation in mind, and simply in order to illustrate  
the unusual possibilities afforded by the AD8330, it is noted  
that with appropriate drive to VDBS and VMAG in tandem, the  
gain span is a remarkable 1±0 dB, extending from −50 dB to  
+70 dB, as shown in Figure 5± for operation at 1 MHz and  
100 MHz. In this case, VDBS and VMAG are driven from a common  
control voltage, VGAIN, that varies from 1.± mV to 5 V, with 30%  
It is apparent from the foregoing sections that the AD8330 is  
both an IVGA and an OVGA in one package. This is an unusual  
and possibly confusing degree of versatility for a VGA; therefore,  
these two distinct control functions are described at separate  
points throughout this data sheet to explain the operation and  
applications of this product. It is, nevertheless, useful to briefly  
describe the capabilities of these features when used together.  
(1.5/5) of VGAIN applied to VDBS, and 100% applied to VMAG  
.
The gain varies in a linear-in-dB manner with VDBS, although  
the response from VMAG is linear-in-magnitude. Consequently, the  
overall numerical gain as the product of these two functions is  
V
GAIN  
0.6 V  
GAIN = VGAIN /0.5 V×0.3 ×10  
(7)  
Rev. C | Page ±7 of 32  
 
 
AD8330  
In rare cases where such a wide gain range is of value, the  
calibration is still accurate and the temperature is stable.  
When a source of impedance (RS) is terminated using a resistor  
of RS (a condition that is not to be confused with matching),  
only one of these components is used, either the current (as in  
the AD8330) or the voltage. Then, even if the amplifier is  
perfect, the noise figure cannot be better than 3 dB. The 1 kΩ  
internal termination resistance would result in a minimum  
noise figure of 3 dB for an RS of 1 kΩ if the amplifier were  
noise-free. However, this is not the case, and the minimum  
noise figure occurs at a slightly different value of RS (for an  
example, see Figure 53 and Using the AD8330 section).  
80  
60  
40  
20  
0
–20  
–40  
–60  
100k  
10k  
1k  
100  
10  
1
15  
14  
13  
12  
11  
10  
0.001  
0.01  
0.1  
1
10  
V
(V)  
GAIN  
Figure 52. Gain Control Function and Input Referred Noise Spectral Density  
over a 120 dB Range  
9
8
7
Noise, Input Capacity, and Dynamic Range  
The design of variable gain amplifiers invariably incurs some  
compromises in noise performance. However, the structure of  
the AD8330 is such that this penalty is minimal. Examination  
of the simplified schematic (Figure 47) shows that the input  
voltage is converted to current-mode form by the two 500 Ω  
resistors at Pin INHI and Pin INLO, whose combined Johnson  
noise contributes 4.08 nV/√Hz. The total input noise at full  
gain, when driven from a low impedance source, is typically  
5 nV/√Hz after accounting for the voltage and current noise  
contributions of the loop amplifier. For a ±00 kHz channel  
bandwidth, this amounts to ±.±4 μV rms. The peak input at full  
gain is ±6.4 mV, or +4.5 mV rms for a sine wave signal. The  
signal-to-noise ratio at full input, that is, the dynamic range, for  
these conditions is, thus, ±0 log10(4.5 mV/±.±4 μV), or 66 dB.  
The value of VMAG has essentially no effect on the input referred  
noise, but it is assumed to be 0.5 V.  
6
5
10  
100  
1k  
10k  
R
()  
S
Figure 53. Noise Figure for Source Resistance of 50 Ω to 5 kΩ, at f = 10 MHz  
(Lower) and 100 MHz (Simulation)  
144  
140  
CONSTANT 1V rms  
OUTPUT, BOTH CASES  
136  
X-AMP WITH 40dB  
132  
OF GAIN AND AN  
INPUT NSD  
OF nV/Hz  
128  
124  
120  
116  
Below midgain (±5 dB, VDBS = 0.75 V), noise in the output  
section dominates, and the total input noise is 11 nV/√Hz, or  
4.9 ꢁV rms in a ±00 kHz bandwidth, and the peak input is  
78 mV rms. Thus, the dynamic range increases to 84 dB.  
At minimum gain, the input noise is up to 1±0 nV/√Hz, or  
53.7 mV rms in the assumed ±00 kHz bandwidth, while the  
input capacity is ±± V, or +1.414 V rms (sine), a dynamic range  
of 88.4 dB. In calculating the dynamic range for other channel  
bandwidths, Δf, subtract 10 log10(Δf/±00 kHz) from these  
illustrative values. A system operating with a ± MHz bandwidth,  
for example, exhibits dynamic range values that are uniformly  
10 dB lower; used in an audio application with a ±0 kHz band-  
width, they are 10 dB higher.  
0
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1 1.2 1.3 1.4 1.5  
V
(V)  
DBS  
Figure 54. Dynamic Range in dB/√Hz vs. VDBS (VMAG = 0.5 V, 1 V rms Output)  
Compared with a Representative X-AMP (Simulation)  
Dynamic Range  
The ratio of peak output swing, expressed in rms terms, to the  
output-referred noise spectral density provides a measure of  
dynamic range, in dB/√Hz. For a certain class of variable gain  
amplifiers, exemplified by the Analog Devices X-AMP family,  
the dynamic range is essentially independent of the gain setting  
because the peak output swing and noise are both constant. The  
AD8330 provides a different dynamic range profile since there  
is no longer a constant relationship between these two parameters.  
Figure 54 compares the dynamic range of the AD8330 to a  
representative X-AMP.  
Noise figure is a misleading metric for amplifiers that are not  
impedance matched at their input, which is the special condi-  
tion resulting only when both the voltage and current components  
of a signal, that is, the signal power, are used at the input port.  
Rev. C | Page ±8 of 32  
 
 
 
AD8330  
Input Common-Mode Range and Rejection Ratio  
The scaling for VDBS = 0 is as follows:  
Input Pin INHI and Pin INLO should be ac-coupled in most  
applications to achieve the stated noise performance. When  
direct coupling is used, care must be taken in setting the dc  
voltage level at these inputs, in general, and particularly when  
minimizing noise is critical. This objective is complicated by the  
fact that the common-mode level varies with the basic gain  
voltage, VDBS. Figure 55 shows this relationship for a supply  
voltage of 5 V, for temperatures of −40°C, +±5°C, and +85°C.  
Figure 56 shows the input noise spectral density (RS = 0) vs. the  
input common-mode voltage, for VDBS = 0.5 V, 0.6 V, 0.75 V, and  
1.5 V. It is apparent that there is a broad range over which the  
noise is unaffected by this dc level. The input CMRR is excellent  
(see Figure 16).  
V
V
OUT_PK = ±4 VMAG  
(8)  
(9)  
NOISE_OUT = (85 + 70 VMAG) nV/√Hz  
For example, using a reduced value of VMAG = 0.±5 V that lowers  
all gain values by 6 dB, the peak output swing is ±1 V (differ  
entially) and the output noise spectral density evaluates to  
10±.5 nV/√Hz. The peak output swing is no different at full  
gain, but the noise becomes  
VNOISE_OUT = (0.1 + 0.3± VMAG) ꢁV/√Hz  
(10)  
for RS = 0 and VDBS = 1.5 V, assuming an input noise of 5 nV/√Hz.  
The output noise for very small values of VMAG (at or below 15 mV)  
is not precise, partly because the small input offset associated  
with this interface has a large effect on the gain.  
3.2  
T = +85°C  
Offset Compensation  
T = +25°C  
T = –40°C  
3.1  
3.0  
2.9  
2.8  
2.7  
2.6  
The AD8330 includes an offset compensation feature that is  
operational in the default condition (no connection to Pin OFST).  
This loop introduces a high-pass filter function into the signal  
path, whose −3 dB corner frequency is at  
1
fHPF  
=
(11)  
(
±πRINTCHP  
)
where CHP is the external capacitance added from OFST to  
CNTR, and RINT is an internal resistance of approximately  
480 ꢀ, having a maximum uncertainty of about ±±0%. This  
evaluates to  
0
0.2  
0.4  
0.6  
0.8  
1.0  
1.2  
1.4  
1.6  
V
(V)  
DBS  
Figure 55. Common-Mode Voltage at Input Pins vs. VDBS, for VS = 5 V,  
T = −40°C, + 25°C, and + 85°C  
330 μ  
CHP  
fHPF  
=
(CHP in μF)  
(1±)  
26  
24  
A small amount of peaking at this corner when using small  
capacitor values can be avoided by adding a series resistor.  
Useful combinations are CHP = 3 nF, RHP = 180 ꢀ , f = 100 kHz;  
CHP = 33 nF, RHP = 10 ꢀ, f = 10 kHz; CHP = 0.33 μF, RHP = 0 ꢀ,  
f = 1 kHz; CHP = 3.3 μF, RHP = 0 ꢀ, f = 100 Hz.  
V
= 0.5V  
DBS  
22  
20  
18  
16  
14  
12  
10  
V
= 0.6V  
DBS  
The offset compensation feature can be disabled simply by  
grounding the OFST pin. This provides a dc-coupled signal  
path, with no other effects on the overall ac response. Input  
offsets must be externally nulled in this mode of operation, as  
shown in Figure 58.  
V
= 0.75V  
DBS  
8
6
4
SIMULATION  
V
= 1.5V  
DBS  
0
0.4 0.8 1.2 1.6 2.0 2.4 2.8 3.2 3.6 4.0 4.4 4.8  
COMMON-MODEVOLTAGE AT INHI, INLO (V)  
Effects of Loading on Gain and AC Response  
The differential output impedance (RO) is 150 ꢀ, and the  
frequency response of the output stage is optimized for  
operation with a certain load capacitance on each output pin  
(OPHI and OPLO) to ground, in combination with a load  
resistance (RL) directly across these pins. In the absence of these  
capacitances, there is a small amount of peaking at the top  
extremity of the ac response. Suitable combinations are: RL = ∞,  
CL = 1± pF; RL = 150 ꢀ, CL = ±5 pF; RL = 75 ꢀ, CL = 40 pF;  
RL = 50 ꢀ, CL = 50 pF.  
Figure 56. Input Noise vs. Common-Mode Input Voltage for  
VDBS = 0.5 V, 0.6 V, 0.75 V, and 1.5 V  
Output Noise and Peak Swing  
The output noise of the AD8330 is the input noise multiplied by  
the overall gain, including any optional change to the voltage,  
MAG, applied to Pin VMAG. The peak output swing is also  
proportional to this voltage, which, at low gains and high values  
of VMAG, affects the output noise.  
V
Rev. C | Page ±9 of 32  
 
 
 
AD8330  
The gain calibration is specified for an open-circuited load,  
such as the high input resistance of an ADC. When resistively  
loaded, all gain values are nominally lowered as follows:  
As in all high frequency circuits, careful observation of the  
ground nodes associated with each function is important. Three  
positive supply pins are provided: VPSI supports the input cir-  
cuitry that often operates at a relatively high sensitivity; VPOS  
supports general bias sources and needs no decoupling; and  
VPSO biases the output stage where decoupling can be useful in  
maintaining a glitch-free output. Figure 57 shows the general  
case, where VPSI and VPSO are each provided with their own  
decoupling network, but this is not needed in all cases.  
GUNLOADED RL  
(13)  
GLOADED  
=
(
150 Ω + RL  
)
Thus, when RL = 150 ꢀ, the gain is reduced by 6 dB; for  
RL = 75 Ω, the reduction is 9.5 dB; and for RL = 50 ꢀ, it is 1± dB.  
Gain Errors Due to On-Chip Resistor Tolerances  
V
2.7V TO 6V  
CD2  
S
In all cases where external resistors are used, keep in mind that  
all on-chip resistances, including the RO and the input resistance  
(RI), are subject to variances of up to ±±0%.  
RD1  
CHPF  
RD2  
ENBL  
VPSI  
OFST  
BIAS AND  
VPOS  
CM MODE AND  
CNTR  
VPSO  
CD1  
CD3  
These variances need to be accounted for when calculating the  
gain with input and output loading. This sensitivity can be avoided  
by adjusting the source and load resistances to bear an inverse  
relationship as follows:  
V-REF  
OFFSET CONTROL  
INHI  
OPHI  
If RS = αRI, then make RL = RO; or,  
if RL = αRO, then make RS = RI/α  
OUTPUT,  
±2V MAX  
INPUT,  
0V TO ±2V MAX  
OUTPUT  
STAGES  
VGA CORE  
OPLO  
INLO  
The simplest case is when RS = 1 kΩ and RL = 150 ꢀ, therefore,  
the gain is 1± dB lower than the basic value. The reduction of  
peak swing at the load can be corrected by using VMAG = 1 V,  
thereby restoring 6 dB of gain; using VMAG = ± V restores the full  
basic gain and doubles the peak available output swing.  
OUTPUT  
CONTROL  
MODE  
GAIN INTERFACE  
CMGN  
NC  
CMOP  
VDBS  
COMM  
VMAG  
NC  
Output (Input) Common-Mode Control  
BASIC GAIN BIAS  
0V TO 1.5V  
V
:
GROUND  
DBS  
The output voltages are nominally positioned at the midpoint of  
the supply, VS/±, over the range ±.7 V < VS < 6 V, and this voltage  
appears at Pin CNTR, which is not normally expected to be  
loaded (the source resistance is ~4 kꢀ). However, some circum-  
stances require a small change in this voltage, and a resistor  
from CNTR to ground can lower this voltage, whereas a resistor  
to the supply raises it. On the other hand, this pin can be driven  
by an external voltage source to set the common-mode level to  
satisfy, for example, the needs of a following ADC. Any value  
from 0.5 V above ground to 0.5 V below the supply is permissible.  
Of course, when using an extreme common-mode level, the  
available output swing is limited, and it is recommended that  
a value equal or close to the default of VCNTR = VS/± be used.  
There may be a few millivolts of offset between the applied  
voltage and the actual common-mode level at the output pins.  
Figure 57. Power Supply Decoupling and Basic Connections  
Because of the differential nature of the signal path, power  
supply decoupling is, in general, much less critical than in a  
single-sided amplifier; and where the minimization of board-  
level components is especially crucial, it is possible that these  
pins need no decoupling at all. On the other hand, when the  
signal source is single-sided, giving extra attention to the  
decoupling on Pin VPSI is sometimes required. Likewise,  
care is required in decoupling the VPSO pin if the output is  
loaded on only one of its two output pins. The general common  
(COMM) and the output stage common (CMOP) are usually  
grounded as shown in the Figure 57; however, the Applications  
section shows how a negative supply can optionally be used.  
The input common-mode voltage, VCMI, at Pin INHI and  
Pin INLO is slaved to the output, but with a shifted value of  
The AD8330 is enabled by taking the ENBL pin to a logical high  
(or, in all cases, the supply). The UP gain mode is enabled either  
by leaving the MODE pin unconnected or taking it to a logical  
high. When the opposite gain direction is needed, the MODE  
pin should be grounded or driven to a logical low. The low-pass  
corner of the offset loop is determined by Capacitor CHPF; this  
is preferably tied to the CNTR pin, that in turn, should be  
decoupled to ground. The gain interface common pin (CMGN)  
is grounded, and the output magnitude control pin (VMAG) is  
left unconnected, or can optionally be connected to a 500 mV  
source for basic gain calibration.  
V
CMI = 0.757 VCNTR + 1.1± V  
(14)  
for VDBS = 0.75 and T = ±5°C. Thus, the default value for VCMI  
when VS = 5 V is 3.01 V (see Figure 55).  
USING THE AD8330  
This section describes a few general aspects of using the  
AD8330. Applying the AD8330 to a wide variety of circum-  
stances requires very few precautions.  
Rev. C | Page 20 of 32  
 
 
 
AD8330  
Connections to the input and output pins are not shown in  
Figure 57 because of the many options that are available. When  
the AD8330 is used to drive an ADC, connect the OPHI and  
OPLO pins directly to the differential inputs of a suitable converter,  
such as an AD9214. If an adjustment is needed to this common-  
mode level, it can be introduced by applying that voltage to the  
CNTR pin, or, more simply, by using a resistor from this pin to  
either ground or the supply (see the Applications section). The  
CNTR pin can also supply the common-mode voltage to an  
ADC that supports such a feature.  
Occasionally, it is possible to avoid the use of coupling  
capacitors when the dc level of the driving source is within a  
certain range, as shown in Figure 56. This range extends from  
3.5 V to 4.5 V when using a 5 V supply, and at high basic gains,  
where the effect of an incorrect dc level degrades the noise level  
due to internal aspects of the input stage. For example, suppose  
the driver, IC, is an LNA having an output topology in which its  
load resistors are taken to the supply, and the output is buffered  
by emitter followers. This presents a source for the AD8330 that  
can readily be directly coupled.  
DC-Coupled Signal Path  
When the loads to be driven introduce a dc resistive path to  
ground, coupling capacitors must be used. These should be of  
sufficient value to pass the lowest frequency components of the  
signal without excessive attenuation. Keep in mind that the  
voltage swing on such loads alternate both above and below  
ground, requiring that the subsequent component must be able  
to cope with negative signal excursions.  
In many cases, where the VGA is not required to provide its  
lowest noise, the full common-mode input range of zero to VS  
can be used without problems, avoiding the need for any ac  
coupling means. However, such direct coupling at both the input  
and output does not automatically result in a fully dc-coupled  
signal path. The internal offset compensation loop must also be  
disengaged by connecting the OFST pin to ground. Keep in  
mind that at the maximum basic gain of 50 dB (×316), every  
millivolt of offset at the input, arising from whatever source,  
causes an output offset of 316 mV, which is an appreciable  
fraction of the peak output swing.  
Gain and Swing Adjustments When Loaded  
The output can also be coupled to a load via a transformer to  
achieve a higher load power by impedance transformation. For  
example, using a 2:1 turns ratio, a 50 Ω final load presents a  
200 Ω load on the output. The gain loss (relative to the basic  
value with no termination) is 20 log10{(200+150)/200} or  
4.86 dB, which can be restored by raising the voltage on the  
VMAG pin by a factor of 104.86/20 or × 1.75, from its basic value  
of 0.5 V to 0.875 V. This also restores the peak swing at the 200 Ω  
level to 2 V, or 1 V into the 50 Ω final load.  
Since the offset correction loop is placed after the front-end  
variable gain sections of the AD8330, the most effective way  
of dealing with such offsets is at the input pins, as shown in  
Figure 58. For example, assume, for illustrative purposes, that  
the resistances associated with each side of the source in a cer-  
tain application are 50 Ω. If this source has a very low (op amp)  
output impedance, the extra resistors should be inserted, with a  
negligible noise penalty and an attenuation of only 0.83 dB. The  
resistor values shown provide a trim range of about 2 mV.  
Whenever a stable supply voltage is available, additional voltage  
swing can be provided by adding a resistor from the VMAG pin  
to the supply. The calculation is based on knowing that the in-  
ternal bias is delivered via a 5 kΩ source; because an additional  
0.375 V is needed, the current in this external resistor must be  
0.375 V/5 kΩ = 75 μA. Thus, using a 5 V supply, a resistor of  
5 V − 0.875 V/75 μA = 55 kΩ is used. Based on this example,  
the corrections for other load conditions are easy to calculate.  
If the effects on gain and peak output swing due to supply  
variations cannot be tolerated, VMAG must be driven by an  
accurate voltage.  
V
2.7V TO 6V  
CD2  
S
RD1  
RD2  
ENBL  
VPSI  
OFST  
BIAS AND  
VPOS  
CM MODE AND  
CNTR  
VPSO  
CD1  
CD3  
V-REF  
OFFSET CONTROL  
INHI  
OPHI  
Input Coupling  
R
ASSUMED  
S
50k  
TO BE 50Ω  
ON EACH  
SIDE  
OUTPUT,  
±2V MAX  
OUTPUT  
STAGES  
The dc common-mode voltage at the input pins varies with  
the supply, the basic gain bias, and temperature (see Figure 55);  
for this reason, many applications need to use coupling capaci-  
tors from the source that are large enough to support the lowest  
frequencies to be transmitted. Using one capacitor at each input  
pin, their minimum values can be readily found from the expression  
VGA CORE  
INLO  
OPLO  
75kΩ  
OUTPUT  
CONTROL  
MODE  
GAIN INTERFACE  
CMGN  
CMOP  
VDBS  
COMM  
VMAG  
320 μF  
fHPF  
CIN_CPL  
=
(15)  
NC  
BASIC GAIN BIAS  
0V TO 1.5V  
V
:
GROUND  
DBS  
where fHPF is the –3dB frequency expressed in hertz. Thus, for  
an fHPF of 10 kHz, 33 nF capacitors are used.  
Figure 58. Input Offset Nulling in a DC-Coupled System  
Rev. C | Page 21 of 32  
 
AD8330  
90  
80  
70  
60  
50  
40  
30  
20  
10  
0
common-mode control loop appear in both the magnitude and  
phase response.  
V
= 1.5V  
OFST: ENABLED  
DISABLED  
DBS  
V
= 0.75V  
DBS  
Adding a dummy 75 Ω to OPLO results in Line 3: the gain is a  
further 2.5 dB lower, at about 14 dB. The CM artifacts are no  
longer present but a small amount of peaking occurs. If objec-  
tionable, this can be eliminated by raising both of the capacitors  
on the output pins to 25 pF, as shown in Line 4 of Figure 60.  
V
= 0V  
DBS  
The gain reduction incurred both by using only one output and  
by the additional effect of loading can be overcome by taking  
advantage of the VMAG feature, provided primarily for just such  
circumstances. Thus, to restore the basic gain in the first case  
(Line 1), a 1 V source should be applied to this pin; to restore the  
gain in the second case, this voltage should be raised by a factor  
of ×1.5 to 1.5 V. In Case 3 and Case 4, a further factor of ×1.33  
is needed to make up the 2.5 dB loss, that is, VMAG should be  
raised to 2 V. With the restoration of gain, the peak output  
swing at the load is, likewise restored to 2 V.  
–10  
50k 100k  
1M  
FREQUENCY (Hz)  
10M  
100M  
Figure 59. Input CMRR vs. Frequency for Various Values of VDBS  
Using Single-Sided Sources and Loads  
Where the source provides a single-sided output, either INHI or  
INLO can be used for the input, with of course a polarity change  
when using INLO. The unused pin must be connected either  
through a capacitor to ground, or a dc bias point that corresponds  
closely to the dc level on the active signal pin. The input CMRR  
over the full frequency range is illustrated in Figure 59. In some  
cases, an additional element such as a SAW filter (having a  
single-sided balanced configuration) or a flux-coupled trans-  
former can be interposed. Where this element must be terminated  
in the correct impedance, other than 1 kΩ, it is necessary to add  
either shunt or series resistors at this interface.  
Pulse Operation  
When using the AD8330 in applications where its transient  
response is of greater interest and the outputs are conveyed to  
their loads via coaxial cables, the added capacitances can slightly  
differ in value, and can be placed either at the sending or load  
end of the cables, or divided between these nodes. Figure 61  
shows an illustrative example where dual, 1 meter, 75 Ω cables  
are driven through dc-blocking capacitors and are independently  
terminated at ground level.  
30  
LINE 1  
LINE 3  
Because of the considerable variation between applications,  
only general recommendations can be made with regard to  
minimizing pulse overshoot and droop. The former can be  
optimized by adding small load capacitances, if necessary;  
the latter requires the use of sufficiently large capacitors (C1).  
20  
10  
0
LINE 4  
LINE 2  
–10  
–20  
–30  
V
2.7V–6V  
0
S
LINE 2  
RD2  
CD2  
–100  
LINE 3  
–200  
LINE 4  
–300  
ENBL  
VPSI  
OFST  
VPOS  
CNTR  
CD3  
–400  
LINE 1  
VPSO  
BIAS AND  
V-REF  
CM MODE AND  
OFFSET CONTROL  
–500  
–600  
RL1  
1M  
10M  
FREQUENCY (Hz)  
100M  
500M  
C1  
C1  
INHI  
OPHI  
Figure 60. AC Gain and Phase for Various Loading Conditions  
CL1  
OUTPUT  
STAGES  
VGA CORE  
When driving a single-sided load, either OPHI or OPLO can be  
used. These outputs are very symmetric, so the only effect of  
this choice is to select the desired polarity. However, when the  
frequency range of interest extends to the upper limits of the  
AD8330, a dummy resistor of the same value should be attached  
to the unused output. Figure 60 illustrates the ac gain and phase  
response for various loads and VDBS = 0.75 V. Line 1 shows the  
unloaded (CL = 12 pF) case for reference; the gain is 6 dB lower  
(20 dB) using only the single-sided output. Adding a 75 Ω load  
from OPHI to an ac ground results in Line 2. The gain becomes  
a factor of ×1.5 V or 3.54 dB lower, but artifacts of the output  
INLO  
OPLO  
CL2  
RL2  
OUTPUT  
MODE  
GAIN INTERFACE  
CMGN  
CMOP  
VMAG  
CONTROL  
VDBS  
COMM  
NC  
Figure 61. Driving Dual Cables with Grounded Loads  
Rev. C | Page 22 of 32  
 
 
 
AD8330  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0
–0.2  
0.2  
that is not dependent on sample-to-sample variations in on chip  
resistances. Furthermore, this fixed and predictable loss can be  
corrected by an adjustment to VMAG , as indicated in Table 5.  
0
Table 5. Preserving Absolute Gain  
–0.2  
–0.4  
–0.6  
–0.8  
–1.0  
–1.2  
1.2  
1.0  
0.8  
0.6  
0.4  
Uncorrected Loss  
VMAG Required to  
Correct Loss  
0.5±0  
0.5±5  
0.520  
0.530  
0.55±  
0.578  
0.605  
0.66±  
0.720  
0.8ꢀ5  
±.±25  
±.53±  
2.000  
3.±25  
ꢀ.500  
RS (Ω)  
±0  
±5  
20  
30  
RL (Ω)  
±5 k  
±0 k  
7.5 k  
5.0 k  
3.0 k  
2.0 k  
±.5 k  
±.0 k  
750  
500  
300  
200  
±50  
±00  
75  
Factor  
0.980  
0.97±  
0.96±  
0.9ꢀ3  
0.907  
0.865  
0.826  
0.756  
0.69ꢀ  
0.592  
0.ꢀꢀꢀ  
0.327  
0.250  
0.±60  
0.±±±  
dB  
0.±7  
0.26  
0.3ꢀ  
0.5±  
0.85  
±.26  
±.66  
2.ꢀ3  
3.±7  
ꢀ.56  
7.0ꢀ  
9.72  
±2.0  
±5.9  
±9.±  
0.2  
0
–0.2  
0.2  
0
–0.2  
–0.4  
–0.6  
–0.8  
–1.0  
–1.2  
50  
75  
0
5ns  
10ns  
15ns  
20ns  
25ns  
±00  
±50  
200  
300  
500  
750  
± k  
Figure 62. Typical Pulse Response for Figure 61  
Figure 6± shows typical results for VDBS = 0.±4 V, a square wave  
input amplitude of 450 mV (the actual combination is not  
important), a rise time of ± ns, and VMAG raised to ±.0 V. In the  
upper waveforms, the load capacitors are both zero, and a small  
amount of overshoot is visible; with 40 pF the response is cleaner.  
A shunt capacitance of ±0 pF from OPHI to OPLO has a similar  
effect. Coupling capacitors for this demonstration are suffi-  
ciently large to prevent any visible droop over this time scale.  
The outputs at the load side eventually assume a mean value of  
zero, with negative and positive excursions depending on the  
duty cycle.  
±.5 k  
2 k  
Calculation of Noise Figure  
The AD8330 noise is a consequence of its intrinsic voltage noise  
spectral density (ENSD) and the current noise spectral density  
(INSD). Their combined effect generates a net input noise,  
The bandwidth from Pin VMAG to these outputs is somewhat  
higher than from the normal input pins. Thus, when this pin is  
used to rapidly modulate the primary signal, some further  
experimentation with response optimization may be required.  
In general, the AD8330 is very tolerant of a wide range of  
loading conditions.  
V
NOISE_IN, that is a function of the input resistance of the device  
(RI), nominally 1 kꢀ, and the differential source resistance (RS)  
as follows:  
±
±
VNOISE _ IN  
=
E
{
± + INSD R + R  
(16)  
(
) }  
NSD  
I
S
Note that we assume purely resistive source and input impedances  
as a concession to simplicity. A more thorough treatment of  
noise mechanisms, for the case where the source is reactive, is  
beyond the scope of these brief notes. Also note that VNOISE_IN is  
the voltage noise spectral density appearing across INHI and  
INLO, the differential input pins. In preparing for the  
calculation of the noise figure, VSIG is defined as the open-  
circuit signal voltage across the source, and VIN is defined as the  
differential input to the AD8330. The relationship is simply  
Preserving Absolute Gain  
Although the AD8330 is not laser trimmed, its absolute gain  
calibration, based mainly on ratios, is very good. Full details are  
found in the Specifications section and in the typical performance  
curves (see the Typical Performance Characteristics section).  
Nevertheless, having finite input and output impedances, the  
gain is necessarily dependent on the source and load conditions.  
The loss that is incurred when either of these is finite causes an  
error in the absolute gain. The absolute gain can also be  
uncertain due to the approximately ±±0% tolerance in the  
absolute value of the input and output impedances.  
V
SIGRI  
(17)  
VIN  
=
R + R  
(
)
I
S
At maximum gain, ENSD is 4.1 nV/√Hz, and INSD is 3 pA/√Hz.  
Thus, the short-circuit voltage noise is  
Often, such losses and uncertainties can be tolerated and  
accommodated by a correction to the gain control bias. On the  
other hand, the error in the loss can be essentially nulled by  
using appropriate modifications to either the source impedance  
(RS) or the load impedance (RL), or both (in some cases by  
padding them with series or shunt components).  
±
±
±
VNOISE _ IN  
=
{
(  
4.1 nV/ Hz  
)
+
(
3pA / Hz  
)
(
1 kΩ + 0  
)
}
=
5.08 nV/√Hz  
(18)  
The formulation for this correction technique was previously  
described. However, to simplify its use, Table 5 shows spot  
values for combinations of RS and RL resulting in an overall loss  
Next, examine the net noise when RS = RI = 1 kꢀ, often  
incorrectly called the matching condition, rather than source  
Rev. C | Page 23 of 32  
 
 
 
AD8330  
impedance termination, which is the actual situation in this  
case. Repeating the procedure  
theory, yield extremely low distortion, a result of the funda-  
mental linearization technique that is an inherent aspect of  
these circuits.  
2
2
2
V
=
(
ꢀ.±nV/ Hz  
)
+
(
3 pA/ Hz  
)
(
± kΩ +±kΩ  
)
NOISE _IN  
In practice, however, the effect of device mismatches and  
junction resistances in the core cell, and other mechanisms in  
its supporting circuitry inevitably cause distortion, further  
aggravated by other effects in the later output stages. Some of  
these effects are very consistent from one sample to the next,  
while those due to mismatches (causing predominantly even-  
order distortion components) are quite variable. Where the  
highest linearity (and also lowest noise) is demanded, consider  
using one of the X-AMP products such as the AD603 (single-  
channel), AD604 (dual-channel), or AD833± (wideband dual-  
channel with ultralow noise LNAs).  
= 7.3 nV/√Hz  
(19)  
The noise figure is the decibel representation of the noise factor,  
FAC, commonly defined as follows:  
N
SNR at input  
SNRatoutput  
NFAC  
=
(±0)  
(±1)  
However, this is equivalent to  
SNRatthe source  
NFAC  
=
SNRattheinput pins  
P1 dB and V1 dB  
In addition to the nonlinearities that arise within the core of the  
AD8330, at moderate output levels, another metric that is more  
commonly stated for RF components that deliver appreciable  
power to a load is the 1 dB compression point. This is defined  
in a very specific manner: it is that point at which, with increasing  
output level, the power delivered to the load eventually falls to a  
value that is 1 dB lower than it would be for a perfectly linear  
system. (Although this metric is sometimes called the 1 dB gain  
compression point, it is important to note that this is not the  
output level at which the incremental gain has fallen by 1 dB).  
Let VNSD be the voltage noise spectral density √kTRS due to the  
source resistance. Using Equation 17, gives  
VSIG  
{
RI /  
(
RI + RS
)
}
/VNSD  
NFAC  
=
VIN  
{
/ VNOISE _ IN RS /  
(
RI + RS  
)
}
RIVNOISE _ IN  
RS VNSD  
=
(±±)  
Then, using the result from Equation 19 for a source resistance  
of 1 kꢀ, having a noise-spectral density of 4.08 nV/√Hz,  
produces  
As was shown in Figure 49, the output of the AD8330 limits  
quite abruptly, and the gain drops sharply above the clipping  
level. The output power, on the other hand, using an external  
resistive load, RL, continues to increase. In the most extreme  
case, the waveform changes from the sinusoidal form of the test  
signal, with an amplitude just below the clipping level, VCLIP, to  
a squarewave of precisely the same amplitude. The change in  
power over this range is from (VCLIP/√±)±/RL to (VCLIP)±/RL, that  
is, a factor of ±, or 3 dB in power terms. It can be shown that for  
an ideal limiting amplifier, the 1 dB compression point occurs  
for an overdrive factor of ± dB.  
1 kꢀ 7.3 nV/ Hz  
(
)
(
)
NFAC  
=
= 1.79  
(±3)  
1 kꢀ 4.08 nV/ Hz  
(
)
(
)
Finally, converting this to decibels using  
FIG = 10 log10(NFAC  
Thus, the resultant noise figure in this example is 5.06 dB,  
N
)
(±4)  
which is somewhat lower than the value shown in Figure 53 for  
this operating condition.  
Noise as a Function of VDBS  
For example, if the AD8330 is driving a 150 ꢀ load and VMAG  
has been set to ± V, the peak output is nominally ±4 V (as  
noted above, the actual value when loaded can differ because  
of a mismatch between on chip and external resistors), or  
±.83 V rms for a sine wave output that corresponds to a power  
of 53.3 mW, that is, 17.3 dBm in 150 ꢀ. Thus, the P1dB level, at  
± dB above clipping, is 19.3 dBm.  
The chief consequence of lowering the basic gain using VDBS is  
that the current noise spectral density INSD increases with the  
square root of the basic gain magnitude, GBN such that  
INSD = (3 pA/√Hz)(√GBN)  
(±5)  
Therefore, at the minimum basic gain of ×0, INSD rises to  
53.3 pA/√Hz. However, the noise figure rises to 17.± db if it  
is recalculated using the procedures in Equation16 through  
Equation ±4.  
Though not involving power transfer, it is sometimes useful to  
state the V1dB, which is the output voltage (unloaded or  
loaded) that is ± dB above clipping for a sine waveform. In the  
above example, this voltage is still ±.83 V rms that can be  
expressed as 9.04 dBV (0 dBV corresponds to a 1 V sine wave).  
Thus, the V1dB is at 11.04 dBV.  
Distortion Considerations  
Continuously variable gain amplifiers invariably employ  
nonlinear circuit elements; consequently, it is common for their  
distortion to be higher than well-designed fixed gain amplifiers.  
The translinear multiplier principles used in the AD8330, in  
Rev. C | Page 2ꢀ of 32  
 
 
AD8330  
APPLICATIONS  
The AD8330s versatility, very constant ac response over a wide  
range of gains, large signal dynamic range, output swing, single  
supply operation, and low power consumption commend this  
VGA to a diverse variety of applications. Only a few can be de-  
scribed here, including the most basic uses and some unusual ones.  
from VMAG to ground. An overrange condition is signaled by  
a high state on pin OR of the AD9214. DFS/GAIN is  
unconnected in this example producing an offset-binary output.  
To provide a twos complement output, it should be connected  
to the REF pin.  
ADC DRIVING  
For ADCs running at sampling rates substantially below the  
bandwidth of the AD8330, an intervening noise filter is  
recommended to limit the noise bandwidth. A one-pole filter  
can easily be created with a single differential capacitor between  
OPHI and OPLO outputs. For a corner frequency of fC, the  
capacitor should have a value of  
The AD8330 is well-suited to drive a high speed converter.  
There are many high speed converters available, but to illus-  
trate the general features, the example in this data sheet uses  
one of the least expensive, the AD9214. This is available in three  
grades for operation at 65 MHz, 80 MHz, and 105 MHz; the  
AD9214BRS-80 is a good complement to the general capabili-  
ties of this VGA.  
CFILT = 1/942 fC  
(26)  
For example, a 10 MHz corner requires about 100 pF.  
Figure 63 shows the connections to drive an ADC. A 3.3 V  
supply is used for both parts. The ADC requires that its input  
pins be positioned at one third of the supply, or 1.1 V. Given  
that the default output level of the VGA is one half the supply  
or 1.65 V, a small correction is introduced by the 8 kΩ resistor  
from CNTR to ground. The ADC specifications require that the  
common-mode input be within ±0.2 V of the nominal 1.1 V;  
variations of up to ±20ꢀ in the AD8330 on chip resistors change  
this voltage by only ±±0 mV. With the connections shown, the  
AD9214 is able to receive an input of 2 V p-p; the peak output  
of the AD8330 can be reduced if desired by adding a resistor  
SIMPLE AGC AMPLIFIER  
Figure 64 illustrates the use of the inverted gain mode and the  
offset gain range (0.2 V < VDBS < 1.± V) in supporting a low cost  
AGC loop. Q1 is used as a detector. When OPHI is sufficiently  
higher than CNTR, due to the signal swing, it conducts and  
charges C1. This raises VDBS and rapidly lowers the gain. Note  
that MODE is grounded (see Figure 48). The minimum voltage  
needed across R1 to set up the full gain is 0.2 V because CMGN  
is dc open-circuited (this does not alter VMAG) and the  
maximum voltage is 1.± V.  
V , 3.3V  
S
3.3  
3.3Ω  
0.1µF  
0.1µF  
OVER-  
RANGE  
8kΩ  
CHPF  
0.1µF  
10Ω  
ENBL  
VPSI  
OFST  
VPOS  
CNTR  
VPSO  
OR  
AV  
DrV  
DD  
DD  
BIAS AND  
V-REF  
CM MODE AND  
OFFSET CONTROL  
D9  
D8  
D7  
D6  
D5  
D4  
D3  
D2  
D1  
D0  
PWRDN  
DFS/GAIN  
0.1µF  
A
IN  
INHI  
OPHI  
INPUT,  
±2V MAX  
OUTPUT  
STAGES  
AD9214BRS-80  
VGA CORE  
A
IN  
OPLO  
INLO  
REFSENSE  
REF  
OUTPUT  
CONTROL  
MODE  
GAIN INTERFACE  
CMGN  
NC  
CMOP  
VMAG  
AGND  
DGND  
CLK  
COMM  
VDBS  
0.1µF  
NC  
GAIN BIAS,  
, 0V–1.5V  
CLOCK  
V
DBS  
ANALOG GROUND  
DIGITAL  
GROUND  
Figure 63. Driving an Analog-to-Digital Converter (Preliminary)  
Rev. C | Page 25 of 32  
 
 
 
 
 
AD8330  
V
, 2.7V–6V  
This simple detector exhibits a temperature variation in the  
differential output amplitude of about 4 mV/°C. It provides a  
fast attack time (an increase in the input is quickly leveled to the  
nominal output, due to the high peak currents in Q1) and a  
slow release time (a decrease in the input is not restored as  
quickly). The voltage at the VDBS pin can be used as an RSSI  
output, scaled 30 mV/dB. Note that the attack time can be  
halved by adding a second transistor, labeled Q2 in Figure 64.  
For operation at lower frequencies, the AGC hold capacitor  
must be increased.  
S
33nF  
10  
4.7Ω  
ENBL  
VPSI  
OFST  
VPOS  
CNTR  
VPSO  
CM MODE AND  
OFFSET CONTROL  
BIAS AND  
V-REF  
0.1µF  
0.1µF  
INHI  
OPHI  
OUTPUT,  
~1V rms  
INPUT,  
5mV TO 1V rms  
OUTPUT  
STAGES  
SEE  
TEXT  
VGA CORE  
INLO  
OPLO  
CMOP  
WIDE RANGE TRUE RMS VOLTMETER  
Q2  
Q1  
OUTPUT  
MODE  
GAIN INTERFACE  
CMGN  
CONTROL  
The AD8362 is an rms responding detector providing a  
dynamic range of 60 dB from low frequencies to 2.7 GHz.  
This can increase to 110 dB using an AD8330 as a precondi-  
tioner, provided the noise bandwidth is limited by an interstage  
low-pass or band-pass filter.  
COMM  
VDBS  
VMAG  
NC  
0.1µF  
R1  
10kΩ  
C1  
0.1µF  
0.1µF  
Figure 64. Simple AGC Amplifier (Preliminary)  
The VGA also provides an input port that is easier to drive than  
the 200 Ω input of the AD8362. Figure 67 shows the general  
scheme.  
When the loop is settled, the average current in Q1 is VDBS/R1,  
which varies from 2 μA at maximum gain (VDBS = 0.2 V) to  
17 μA at minimum gain (VDBS = 1.7 V). This change in the Q1  
current causes an increase of ~0.25 dB over the full gain range  
in the differential output of nominally 0.75 dBV at midrange  
(3.08 V p-p), corresponding to a 200:1 compression ratio. This  
is plotted in Figure 65 for a representative 100 kHz input.  
Both the AD8330 and AD8362 provide linear-in-decibel control  
interfaces. Thus, when the output of the AD8362 is used to  
control the gain of the AD8330, the functional form is  
unaffected. The overall scaling is 33 mV/dB. Figure 68 shows  
the time domain response using a loop filter capacitor of 10 nF,  
for inputs ranging from 10 μV to 1 V rms, that is, a 100 dB  
measurement range.  
1.0  
0.9  
0.8  
0.7  
0.6  
0.5  
1.75  
1.50  
V
DBS  
1.25  
1.00  
0.75  
0.50  
0.25  
0
3
2
1
0
–50  
–40  
–30  
–20  
–10  
0
–1  
–2  
–3  
–4  
INPUT TO AD8330 (dBV)  
OUTPUT  
Figure 65. AGC Output vs. Input Amplitude (Simulation)  
0
10 20 30 40 50 60 70 80 90 100 110 120 130 140 150  
TIME (µs)  
The upper panel in Figure 66 shows time-domain output for  
fourteen 3 dB steps in input amplitude from 5.4 mV to 1.7 V.  
The waveforms in Figure 65 show the AGC voltage (VDBS).  
Figure 66. Time Domain Waveforms (Simulation)  
Rev. C | Page 26 of 32  
 
 
 
 
AD8330  
5V  
3.3  
3.3Ω  
3.3Ω  
AD8362  
0.1µF  
0.1µF  
VPOS  
0.1µF  
3.6V  
0.1µF  
1
2
3
4
5
6
7
8
16  
15  
14  
13  
12  
11  
10  
9
COMM  
CHPF  
DECL  
INHI  
ACOM  
VREF  
VTGT  
VPOS  
VOUT  
VSET  
ACOM  
CLPF  
10µF  
ENBL  
VPS1  
OFST  
CNTR  
VPSO  
INHI  
OPHI  
OPLO  
CMOP  
C
FLT  
18nF  
3.6V  
INPUT  
AD8330  
INLO  
MODE  
VOUT  
INLO  
DECL  
PWDN  
COMM  
0.1µF  
VDBS CMGN COMM VMAG  
10µF  
6.04kΩ  
4.02kΩ  
Figure 67. Wide Range True RMS Voltmeter (Preliminary)  
4
3
2
1
0
0
0.4 0.8 1.2 1.6 2.0 2.4 2.8 3.2 3.6 4.0 4.4 4.8  
TIME (ms)  
Figure 68. Time Domain Response of RMS Voltmeter (Simulation)  
Rev. C | Page 27 of 32  
 
 
AD8330  
OUTLINE DIMENSIONS  
0.50  
0.40  
0.30  
0.60 MAX  
3.00  
BSC SQ  
PIN 1  
INDICATOR  
BOTTOM VIEW  
*
1.65  
1.50 SQ  
1.35  
13  
12  
16  
1
0.45  
PIN 1  
INDICATOR  
2.75  
BSC SQ  
TOP  
VIEW  
EXPOSED  
PAD  
4
9
8
0.50  
BSC  
5
0.25 MIN  
1.50 REF  
0.80 MAX  
12° MAX  
THE EXPOSED PAD IS NOT CONNECTED  
INTERNALLY. FOR INCREASED RELIABILITY  
OF THE SOLDER JOINTS AND MAXIMUM  
THERMAL CAPABILITY, IT IS RECOMMENDED  
THAT THE PADDLE BE SOLDERED TO THE  
GROUND PLANE.  
0.65 TYP  
0.90  
0.85  
0.80  
0.05 MAX  
0.02 NOM  
SEATING  
PLANE  
0.30  
0.23  
0.18  
0.20 REF  
*
COMPLIANT TO JEDEC STANDARDS MO-220-VEED-2  
EXCEPT FOR EXPOSED PAD DIMENSION.  
Figure 69. 16-Lead Lead Frame Chip Scale Package [LFCSP_VQ]  
3 mm × 3 mm Body, Very Thin Quad  
(CP-16-3)  
Dimensions shown in millimeters  
0.197  
0.193  
0.189  
16  
1
9
8
0.158  
0.154  
0.150  
0.244  
0.236  
0.228  
PIN 1  
0.069  
0.053  
0.065  
0.049  
8°  
0°  
0.010  
0.004  
0.025  
BSC  
0.012  
0.008  
0.050  
0.016  
SEATING  
PLANE  
0.010  
0.006  
COPLANARITY  
0.004  
COMPLIANT TO JEDEC STANDARDS MO-137-AB  
Figure 70. 16-Lead Shrink Small Outline Package [QSOP]  
(RQ-16)  
Dimensions shown in inches  
Rev. C | Page 28 of 32  
 
AD8330  
ORDERING GUIDE  
Model  
Temperature Range  
Package Description  
Package Option  
Branding  
AD8330ACP-R2  
AD8330ACP-REEL  
AD8330ACP-REEL7  
AD8330ACPZ-R2±  
AD8330ACPZ-RL±  
AD8330ACPZ-R7±  
AD8330ARQ  
AD8330ARQ-REEL  
AD8330ARQ-REEL7  
AD8330ARQZ±  
−ꢀ0°C to +85°C  
−ꢀ0°C to +85°C  
−ꢀ0°C to +85°C  
−ꢀ0°C to +85°C  
−ꢀ0°C to +85°C  
−ꢀ0°C to +85°C  
−ꢀ0°C to +85°C  
−ꢀ0°C to +85°C  
−ꢀ0°C to +85°C  
−ꢀ0°C to +85°C  
−ꢀ0°C to +85°C  
−ꢀ0°C to +85°C  
±6-Lead LFCSP_VQ  
±6-Lead LFCSP_VQ  
±6-Lead LFCSP_VQ  
±6-Lead LFCSP_VQ  
±6-Lead LFCSP_VQ  
±6-Lead LFCSP_VQ  
±6-Lead QSOP  
±6-Lead QSOP  
±6-Lead QSOP  
±6-Lead QSOP  
±6-Lead QSOP  
CP-±6-3  
CP-±6-3  
CP-±6-3  
CP-±6-3  
CP-±6-3  
CP-±6-3  
RQ-±6  
RQ-±6  
RQ-±6  
RQ-±6  
RQ-±6  
JFA  
JFA  
JFA  
JFZ  
JFZ  
JFZ  
AD8330ARQZ-RL±  
AD8330ARQZ-R7±  
AD8330-EVAL  
±6-Lead QSOP  
Evaluation Board  
RQ-±6  
± Z = Pb-free part.  
Rev. C | Page 29 of 32  
 
 
AD8330  
NOTES  
Rev. C | Page 30 of 32  
AD8330  
NOTES  
Rev. C | Page 3± of 32  
AD8330  
NOTES  
©2006 Analog Devices, Inc. All rights reserved. Trademarks and  
registered trademarks are the property of their respective owners.  
C03217-0-6/06(C)  
Rev. C | Page 32 of 32  

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Low Cost DC to 150 MHz Variable Gain Amplifier
ADI

AD8330_06

Low Cost DC to 150 MHz Variable Gain Amplifier
ADI