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FEATURES "Linear in dB" Gain Control Pin Programmable Gain Ranges -11 dB to +31 dB with 90 MHz Bandwidth +9 dB to +51 dB with 9 MHz Bandwidth Any Intermediate Range, e.g., -1 dB to +41 dB with 30 MHz Bandwidth Bandwidth Independent of Variable Gain 1.3 nV/Hz Input Noise Spectral Density 0.5 dB Typical Gain Accuracy MIL-STD-883 Compliant and DESC Versions Available APPLICATIONS RF/IF AGC Amplifier Video Gain Control A/D Range Extension Signal Measurement PRODUCT DESCRIPTION
Low Noise, 90 MHz Variable-Gain Amplifier AD603*
1 V to span the central 40 dB of the gain range. An over- and under-range of 1 dB is provided whatever the selected range. The gain-control response time is less than 1 s for a 40 dB change. The differential gain-control interface allows the use of either differential or single-ended positive or negative control voltages. Several of these amplifiers may be cascaded and their gain-control gains offset to optimize the system S/N ratio. The AD603 can drive a load impedance as low as 100 with low distortion. For a 500 load in shunt with 5 pF, the total harmonic distortion for a 1 V sinusoidal output at 10 MHz is typically -60 dBc. The peak specified output is 2.5 V minimum into a 500 load, or 1 V into a 100 load. The AD603 uses a proprietary circuit topology--the X-AMPTM. The X-AMP comprises a variable attenuator of 0 dB to -42.14 dB followed by a fixed-gain amplifier. Because of the attenuator, the amplifier never has to cope with large inputs and can use negative feedback to define its (fixed) gain and dynamic performance. The attenuator has an input resistance of 100 , laser trimmed to 3%, and comprises a seven-stage R-2R ladder network, resulting in an attenuation between tap points of 6.021 dB. A proprietary interpolation technique provides a continuous gain-control function which is linear in dB. The AD603A is specified for operation from -40C to +85C and is available in both 8-lead SOIC (R) and 8-lead ceramic DIP (Q). The AD603S is specified for operation from -55C to +125C and is available in an 8-lead ceramic DIP (Q). The AD603 is also available under DESC SMD 5962-94572.
The AD603 is a low noise, voltage-controlled amplifier for use in RF and IF AGC systems. It provides accurate, pin selectable gains of -11 dB to +31 dB with a bandwidth of 90 MHz or +9 dB to +51 dB with a bandwidth of 9 MHz. Any intermediate gain range may be arranged using one external resistor. The input referred noise spectral density is only 1.3 nV/Hz and power consumption is 125 mW at the recommended 5 V supplies. The decibel gain is "linear in dB," accurately calibrated, and stable over temperature and supply. The gain is controlled at a high impedance (50 M), low bias (200 nA) differential input; the scaling is 25 mV/dB, requiring a gain-control voltage of only
FUNCTIONAL BLOCK DIAGRAM
VPOS VNEG GPOS
SCALING REFERENCE
PRECISION PASSIVE INPUT ATTENUATOR
FIXED GAIN AMPLIFIER VOUT
VG GNEG GAIN CONTROL INTERFACE
AD603
6.44k * FDBK 694 *
0dB VINP
-6.02dB -12.04dB -18.06dB -24.08dB -30.1dB -36.12dB -42.14dB R 2R R 2R R 2R R 2R R 2R R 2R R R *NORMAL VALUES 20 *
COMM R = 2R LADDER NETWORK
*Patented. X-AMP is a trademark of Analog Devices, Inc.
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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 which may result from its use. No license is granted by implication or otherwise under any patent or patent rights of Analog Devices. One Technology Way, P.O. Box 9106, Norwood, MA 02062-9106, U.S.A. Tel: 781/329-4700 World Wide Web Site: http://www.analog.com Fax: 781/326-8703 (c) Analog Devices, Inc., 2000
C, 5 mV V +500 mV, GNEG AD603-SPECIFICATIONS (@ T = R+25 500V =, and V, -500pF, unlessotherwise noted.)= 0 V, -10 dB to +30 dB Gain Range, = C =5
A S G L L
Model Parameter INPUT CHARACTERISTICS Input Resistance Input Capacitance Input Noise Spectral Density1 Noise Figure 1 dB Compression Point Peak Input Voltage OUTPUT CHARACTERISTICS -3 dB Bandwidth Slew Rate Peak Output2 Output Impedance Output Short-Circuit Current Group Delay Change vs. Gain Group Delay Change vs. Frequency Differential Gain Differential Phase Total Harmonic Distortion 3rd Order Intercept ACCURACY Gain Accuracy TMIN to TMAX Output Offset Voltage3 TMIN to TMAX Output Offset Variation vs. VG TMIN to TMAX GAIN CONTROL INTERFACE Gain Scaling Factor TMIN to TMAX GNEG, GPOS Voltage Range4 Input Bias Current Input Offset Current Differential Input Resistance Response Rate POWER SUPPLY Specified Operating Range Quiescent Current TMIN to TMAX
Conditions Pins 3 to 4 Input Short Circuited f = 10 MHz, Gain = max, RS = 10 f = 10 MHz, Gain = max, RS = 10
Min 97
AD603 Typ Max 100 2 1.3 8.8 -11 1.4 90 275 3.0 2 50 2 2 0.2 0.2 -60 15 0.5 1 1.5 20 30 20 30 40.6 42 +2.0 103
Unit pF nV/Hz dB dBm V MHz V/s V mA ns ns % Degree dBc dBm dB dB mV mV mV mV dB/V dB/V V nA nA M dB/s V mA mA
2
VOUT = 100 mV rms RL 500 RL 500 f 10 MHz f = 3 MHz; Full Gain Range VG = 0 V; f = 1 MHz to 10 MHz f = 10 MHz, VOUT = 1 V rms f = 40 MHz, Gain = max, RS = 50 -500 mV VG +500 mV VG = 0 V -500 mV VG +500 mV
2.5
39.4 38 -1.2
40
Pins 1 to 2 Full 40 dB Gain Change 4.75
200 10 50 40 6.3 17 20
12.5
NOTES 1 Typical open or short-circuited input; noise is lower when system is set to maximum gain and input is short-circuited. This figure includes the effects of both voltage and current noise sources. 2 Using resistive loads of 500 or greater, or with the addition of a 1 k pull-down resistor when driving lower loads. 3 The dc gain of the main amplifier in the AD603 is x35.7; thus, an input offset of 100 V becomes a 3.57 mV output offset. 4 GNEG and GPOS, gain control, voltage range is guaranteed to be within the range of - VS + 4.2 V to +VS - 3.4 V over the full temperature range of -40C to +85C. Specifications shown in boldface are tested on all production units at final electrical test. Results from those tests are used to calculate outgoing quality levels. All min and max specifications are guaranteed, although only those shown in boldface are tested on all production units. Specifications subject to change without notice.
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AD603
ABSOLUTE MAXIMUM RATINGS 1
Supply Voltage VS . . . . . . . . . . . . . . . . . . . . . . . . . . . . 7.5 V Internal Voltage VINP (Pin 3) . . . . . . . . . . . 2 V Continuous . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . VS for 10 ms GPOS, GNEG (Pins 1, 2) . . . . . . . . . . . . . . . . . . . . . . . VS Internal Power Dissipation2 . . . . . . . . . . . . . . . . . . . . 400 mW Operating Temperature Range AD603A . . . . . . . . . . . . . . . . . . . . . . . . . . . - 40C to +85C AD603S . . . . . . . . . . . . . . . . . . . . . . . . . . - 55C to +125C Storage Temperature Range . . . . . . . . . . . . -65C to +150C Lead Temperature Range (Soldering 60 sec) . . . . . . . . +300C
NOTES 1 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. 2 Thermal Characteristics: 8-Lead SOIC Package: JA = 155C/W, JC = 33C/W 8-Lead Ceramic Package: JA = 140C/W, JC = 15C/W
PIN FUNCTION DESCRIPTIONS
Pin Pin 1 Pin 2 Pin 3 Pin 4 Pin 5 Pin 6 Pin 7 Pin 8
Mnemonic GPOS GNEG VINP COMM FDBK VNEG VOUT VPOS
Description Gain-Control Input "HI" (Positive Voltage Increases Gain) Gain-Control Input "LO" (Negative Voltage Increases Gain) Amplifier Input Amplifier Ground Connection to Feedback Network Negative Supply Input Amplifier Output Positive Supply Input
CONNECTION DIAGRAMS 8-Lead Plastic SOIC (R) Package 8-Lead Ceramic DIP (Q) Package
GPOS 1 GNEG 2
8
VPOS
VOUT TOP VIEW VINP 3 (Not to Scale) 6 VNEG
7 5
AD603
COMM 4
FDBK
ORDERING GUIDE Part Number AD603AR AD603AQ AD603SQ/883B* AD603-EB AD603ACHIPS AD603AR-REEL AD603AR-REEL7 Temperature Range -40C to +85C -40C to +85C -55C to +125C -40C to +85C -40C to +85C -40C to +85C Package Description 8-Lead SOIC 8-Lead Ceramic DIP 8-Lead Ceramic DIP Evaluation Board Die 13" Reel 7" Reel Package Option SO-8 Q-8 Q-8
SO-8 SO-8
*Refer to AD603 Military data sheet. Also available as 5962-9457203MPA.
CAUTION ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily accumulate on the human body and test equipment and can discharge without detection. Although the AD603 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.
WARNING!
ESD SENSITIVE DEVICE
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AD603
THEORY OF OPERATION
The AD603 comprises a fixed-gain amplifier, preceded by a broadband passive attenuator of 0 dB to 42.14 dB, having a gain-control scaling factor of 40 dB per volt. The fixed gain is laser-trimmed in two ranges, to either 31.07 dB (x35.8) or 50 dB (x358), or may be set to any range in between using one external resistor between Pins 5 and 7. Somewhat higher gain can be obtained by connecting the resistor from Pin 5 to common, but the increase in output offset voltage limits the maximum gain to about 60 dB. For any given range, the bandwidth is independent of the voltage-controlled gain. This system provides an under- and overrange of 1.07 dB in all cases; for example, the overall gain is -11.07 dB to 31.07 dB in the maximum-bandwidth mode (Pin 5 and Pin 7 strapped). This X-AMP structure has many advantages over former methods of gain-control based on nonlinear elements. Most importantly, the fixed-gain amplifier can use negative feedback to increase its accuracy. Since large inputs are first attenuated, the amplifier input is always small. For example, to deliver a 1 V output in the -1 dB/+41 dB mode (that is, using a fixed amplifier gain of 41.07 dB) its input is only 8.84 mV; thus the distortion can be very low. Equally important, the small-signal gain and phase response, and thus the pulse response, are essentially independent of gain. Figure 1 is a simplified schematic. The input attenuator is a seven-section R-2R ladder network, using untrimmed resistors of nominally R = 62.5 , which results in a characteristic resistance of 125 20%. A shunt resistor is included at the input and laser trimmed to establish a more exact input resistance of 100 3%, which ensures accurate operation (gain and HP corner frequency) when used in conjunction with external resistors or capacitors. The nominal maximum signal at input VINP is 1 V rms ( 1.4 V peak) when using the recommended 5 V supplies, although operation to 2 V peak is permissible with some increase in HF distortion and feedthrough. Pin 4 (SIGNAL COMMON) must be connected directly to the input ground; significant impedance in this connection will reduce the gain accuracy. The signal applied at the input of the ladder network is attenuated by 6.02 dB by each section; thus, the attenuation to each of the taps is progressively 0 dB, 6.02 dB, 12.04 dB, 18.06 dB, 24.08 dB, 30.1 dB, 36.12 dB and 42.14 dB. A unique circuit technique is employed to interpolate between these tap-points,
indicated by the "slider" in Figure 1, thus providing continuous attenuation from 0 dB to 42.14 dB. It will help, in understanding the AD603, to think in terms of a mechanical means for moving this slider from left to right; in fact, its "position" is controlled by the voltage between Pins 1 and 2. The details of the gaincontrol interface are discussed later. The gain is at all times very exactly determined, and a linear-indB relationship is automatically guaranteed by the exponential nature of the attenuation in the ladder network (the X-AMP principle). In practice, the gain deviates slightly from the ideal law, by about 0.2 dB peak (see, for example, Figure 16).
Noise Performance
An important advantage of the X-AMP is its superior noise performance. The nominal resistance seen at inner tap points is 41.7 (one third of 125 ), which exhibits a Johnson noisespectral density (NSD) of 0.83 nV/Hz (that is, 4kTR) at 27C, which is a large fraction of the total input noise. The first stage of the amplifier contributes a further 1 nV/Hz, for a total input noise of 1.3 nV/Hz. It will be apparent that it is essential to use a low resistance in the ladder network to achieve the very low specified noise level. The signal's source impedance forms a voltage divider with the AD603's 100 input resistance. In some applications, the resulting attenuation may be unacceptable, requiring the use of an external buffer or preamplifier to match a high impedance source to the low impedance AD603. The noise at maximum gain (that is, at the 0 dB tap) depends on whether the input is short-circuited or open-circuited: when shorted, the minimum NSD of slightly over 1 nV/Hz is achieved; when open, the resistance of 100 looking into the first tap generates 1.29 nV/Hz, so the noise increases to a total of 1.63 nV/Hz. (This last calculation would be important if the AD603 were preceded by, for example, a 900 resistor to allow operation from inputs up to 10 V rms.) As the selected tap moves away from the input, the dependence of the noise on source impedance quickly diminishes. Apart from the small variations just discussed, the signal-tonoise (S/N) ratio at the output is essentially independent of the attenuator setting. For example, on the -11 dB/+31 dB range the fixed gain of x35.8 raises the output NSD to 46.5 nV/Hz. Thus, for the maximum undistorted output of 1 V rms and a 1 MHz bandwidth, the output S/N ratio would be 86.6 dB, that is, 20 log (1 V/46.5 V).
VPOS VNEG GPOS
SCALING REFERENCE
PRECISION PASSIVE INPUT ATTENUATOR
FIXED GAIN AMPLIFIER VOUT
VG GNEG GAIN CONTROL INTERFACE
AD603
6.44k * FDBK 694 *
0dB VINP
-6.02dB -12.04dB -18.06dB -24.08dB -30.1dB -36.12dB -42.14dB R 2R R 2R R 2R R 2R R 2R R 2R R R *NORMAL VALUES 20 *
COMM R = 2R LADDER NETWORK
Figure 1. Simplified Block Diagram of the AD603
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REV. C
AD603
The Gain-Control Interface
The attenuation is controlled through a differential, highimpedance (50 M) input, with a scaling factor which is laser-trimmed to 40 dB per volt, that is, 25 mV/dB. An internal bandgap reference ensures stability of the scaling with respect to supply and temperature variations. When the differential input voltage VG = 0 V, the attenuator "slider" is centered, providing an attenuation of 21.07 dB. For the maximum bandwidth range, this results in an overall gain of 10 dB (= -21.07 dB + 31.07 dB). When the control input is -500 mV, the gain is lowered by 20 dB (= 0.500 V x 40 dB/V), to -10 dB; when set to +500 mV, the gain is increased by 20 dB, to 30 dB. When this interface is overdriven in either direction, the gain approaches either -11.07 dB (= - 42.14 dB + 31.07 dB) or 31.07 dB (= 0 + 31.07 dB), respectively. The only constraint on the gain-control voltage is that it be kept within the common-mode range (-1.2 V to +2.0 V assuming +5 V supplies) of the gain control interface. The basic gain of the AD603 can thus be calculated using the following simple expression: Gain (dB) = 40 VG + 10 (1) where VG is in volts. When Pins 5 and 7 are strapped (see next section) the gain becomes Gain (dB) = 40 VG + 20 for 0 to +40 dB and Gain (dB) = 40 VG + 30 for +10 to +50 dB (2) The high impedance gain-control input ensures minimal loading when driving many amplifiers in multiple channel or cascaded applications. The differential capability provides flexibility in choosing the appropriate signal levels and polarities for various control schemes. For example, if the gain is to be controlled by a DAC providing a positive only ground-referenced output, the "Gain Control LO" (GNEG) pin should be biased to a fixed offset of +500 mV, to set the gain to -10 dB when "Gain Control HI" (GPOS) is at zero, and to 30 dB when at +1.00 V. It is a simple matter to include a voltage divider to achieve other scaling factors. When using an 8-bit DAC having an FS output of +2.55 V (10 mV/bit), a divider ratio of 2 (generating 5 mV/bit) would result in a gain-setting resolution of 0.2 dB/bit. The use of such offsets is valuable when two AD603s are cascaded, when various options exist for optimizing the S/N profile, as will be shown later.
Programming the Fixed-Gain Amplifier Using Pin Strapping
DECIBELS
VC1
GPOS
VPOS
VPOS
AD603
VC2 GNEG VOUT VNEG VNEG VOUT
VIN
VINP
COMM
FDBK
a. -10 dB to +30 dB; 90 MHz Bandwidth
VC1 GPOS VPOS VPOS
AD603
VC2 GNEG VOUT VNEG VNEG 2.15k COMM FDBK 5.6pF VOUT
VIN
VINP
b. 0 dB to +40 dB; 30 MHz Bandwidth
VC1 GPOS VPOS VPOS
AD603
VC2 GNEG VOUT VNEG VNEG VOUT
VIN
VINP
COMM
FDBK 18pF
c. +10 dB to +50 dB; 9 MHz Bandwidth Figure 2. Pin Strapping to Set Gain
52 50 48 46 44 42 40 38 36 34 32 30 10 100 1k REXT 10k 100k 1M -2:VdB (OUT) VdB (OUT) -1:VdB (OUT)
Access to the feedback network is provided at Pin 5 (FDBK). The user may program the gain of the AD603's output amplifier using this pin, as shown in Figure 2. There are three modes: in the default mode, FDBK is unconnected, providing the range +9 dB/+51 dB; when VOUT and FDBK are shorted, the gain is lowered to -11 dB/+31 dB; when an external resistor is placed between VOUT and FDBK any intermediate gain can be achieved, for example, -1 dB/+41 dB. Figure 3 shows the nominal maximum gain versus external resistor for this mode.
Figure 3. Gain vs. REXT, Showing Worst-Case Limits Assuming Internal Resistors Have a Maximum Tolerance of 20%
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-5-
AD603
Optionally, when a resistor is placed from FDBK to COMM, higher gains can be achieved. This fourth mode is of limited value because of the low bandwidth and the elevated output offsets; it is thus not included in Figure 2. The gain of this amplifier in the first two modes is set by the ratio of on-chip laser-trimmed resistors. While the ratio of these resistors is very accurate, the absolute value of these resistors can vary by as much as 20%. Thus, when an external resistor is connected in parallel with the nominal 6.44 k 20% internal resistor, the overall gain accuracy is somewhat poorer. The worst-case error occurs at about 2 k (see Figure 4).
1.2 1.0 0.8 0.6 DECIBELS 0.4 0.2 0.0 -0.2 -0.4 -0.6 -0.8 80 -1.0 10 100 1k REXT 10k 100k 1M 90 85 VdB (OUT) - VdB (OREF) -1:VdB (OUT) - (-1):VdB (OREF)
There are several ways of connecting the gain-control inputs in cascaded operation. The choice depends on whether it is important to achieve the highest possible Instantaneous Signal-to-Noise Ratio (ISNR), or, alternatively, to minimize the ripple in the gain error. The following examples feature the AD603 programmed for maximum bandwidth; the explanations apply to other gain/ bandwidth combinations with appropriate changes to the arrangements for setting the maximum gain. Sequential Mode (Optimal S/N Ratio) In the sequential mode of operation, the ISNR is maintained at its highest level for as much of the gain control range possible. Figure 5 shows the SNR over a gain range of -22 dB to +62 dB, assuming an output of 1 V rms and a 1 MHz bandwidth; Figure 6 shows the general connections to accomplish this. Here, both the positive gain-control inputs (GPOS) are driven in parallel by a positive-only, ground-referenced source with a range of 0 V to +2 V, while the negative gain-control inputs (GNEG) arc biased by stable voltages to provide the needed gain-offsets. These voltages may be provided by resistive dividers operating from a common voltage reference.
S/N RATIO - dB
75 70 65 60 55 50 -0.2
Figure 4. Worst-Case Gain Error, Assuming Internal Resistors Have a Maximum Tolerance of -20% (Top Curve) or +20% (Bottom Curve)
While the gain-bandwidth product of the fixed-gain amplifier is about 4 GHz, the actual bandwidth is not exactly related to the maximum gain. This is because there is a slight enhancing of the ac response magnitude on the maximum bandwidth range, due to higher order poles in the open-loop gain function; this mild peaking is not present on the higher gain ranges. Figure 2 shows how optional capacitors may be added to extend the frequency response in high gain modes.
CASCADING TWO AD603S
0.2
0.6
1.0 VC
1.4
1.8
2.2
Figure 5. SNR vs. Control Voltage--Sequential Control (1 MHz Bandwidth)
Two or more AD603s can be connected in series to achieve higher gain. Invariably, ac coupling must be used to prevent the dc offset voltage at the output of each amplifier from overloading the following amplifier at maximum gain. The required high pass coupling network will usually be just a capacitor, chosen to set the desired corner frequency in conjunction with the welldefined 100 input resistance of the following amplifier. For two AD603s, the total gain-control range becomes 84 dB (two times 42.14 dB); the overall -3 dB bandwidth of cascaded stages will be somewhat reduced. Depending on the pin-strapping, the gain and bandwidth for two cascaded amplifiers can range from -22 dB to +62 dB (with a bandwidth of about 70 MHz) to +22 dB to +102 dB (with a bandwidth of about 6 MHz).
The gains are offset (Figure 7) such that A2's gain is increased only after A1's gain has reached its maximum value. Note that for a differential input of -600 mV or less, the gain of a single amplifier (A1 or A2) will be at its minimum value of -11.07 dB; for a differential input of +600 mV or more, the gain will be at its maximum value of 31.07 dB. Control inputs beyond these limits will not affect the gain and can be tolerated without damage or foldover in the response. This is an important aspect of the AD603's gain-control response. (See the Specifications section of this data sheet for more details on the allowable voltage range) The gain is now Gain (dB) = 40 VG + GO (3) where VG is the applied control voltage and GO is determined by the gain range chosen. In the explanatory notes that follow, we assume the maximum-bandwidth connections are used, for which GO is -20 dB.
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AD603
A1 -40.00dB -42.14dB GPOS VG1 VC = 0V GNEG 31.07dB A2 -51.07dB -8.93dB -42.14dB GPOS VG2 GNEG 31.07dB OUTPUT -20dB
INPUT 0dB
VO1 = 0.473V
VO2 = 1.526V
a.
0dB 0dB GPOS VG1 VC = 1.0V GNEG 31.07dB -11.07dB 31.07dB -42.14dB GPOS VG2 GNEG 31.07dB OUTPUT 20dB
INPUT 0dB
VO1 = 0.473V
VO2 = 1.526V
b.
0dB 0dB GPOS VG1 VC = 2.0V GNEG 31.07dB -2.14dB GPOS VG2 GNEG 31.07dB OUTPUT 60dB -28.93dB 31.07dB
INPUT 0dB
VO1 = 0.473V
VO2 = 1.526V
c. Figure 6. AD603 Gain Control Input Calculations for Sequential Control Operation
+31.07dB +31.07dB +10dB +28.96dB
A1
* *
-11.07dB
A2
-8.93dB 0.473 GAIN (dB) -22.14 0 -20 0.5 0
-11.07dB 1.526 1.0 20 1.50 40 2.0 60 VC (V) 62.14
When VG = +2.0 V, the gain of A1 is pinned at 31.07 dB and that of A2 is near its maximum value of 28.93 dB, resulting in an overall gain of 60 dB (see Figure 6c). This mode of operation is further clarified by Figure 8, which is a plot of the separate gains of A1 and A2 and the overall gain versus the control voltage. Figure 9 is a plot of the gain error of the cascaded amplifiers versus the control voltage. Figure 10 is a plot of the gain error of the cascaded stages versus the control voltages.
70 60 COMBINED 50
*GAIN OFFSET OF 1.07dB, OR 26.75mV
Figure 7. Explanation of Offset Calibration for Sequential Control
With reference to Figure 6, note that VG1 refers to the differential gain-control input to A1 and VG2 refers to the differential gain-control input to A2. When VG is zero, VG1 = -473 mV and thus the gain of A1 is -8.93 dB (recall that the gain of each individual amplifier in the maximum-bandwidth mode is -10 dB for VG = -500 mV and 10 dB for VG = 0 V); meanwhile, VG2 = -1.908 V so the gain of A2 is "pinned" at -11.07 dB. The overall gain is thus -20 dB. This situation is shown in Figure 6a. When VG = +1.00 V, VG1 = 1.00 V - 0.473 V = +0.526 V, which sets the gain of A1 to at nearly its maximum value of 31.07 dB, while VG2 = 1.00 V - 1.526 V = 0.526 V, which sets A2's gain at nearly its minimum value -11.07 dB. Close analysis shows that the degree to which neither AD603 is completely pushed to its maximum or minimum gain exactly cancels in the overall gain, which is now +20 dB. This is depicted in Figure 6b.
OVERALL GAIN - dB
40 A1 30 20 10 0 -10 -20 -30 -0.2 0.2 0.6 0.1 VC 1.4 1.8 2.2 A2
Figure 8. Plot of Separate and Overall Gains in Sequential Control
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AD603
90 80 70
GAIN ERROR - dB
2.0 1.5 1.0 0.5 0.0 -0.5 -1.0 -1.5 -2.0 -0.2 0.0 0.2
S/N RATIO - dB
60 50 40 30 20 10 -0.2
0.2
0.6
1.0 VC
1.4
1.8
2.2
0.4 0.6
0.8
1.0 VC
1.2 1.4
1.6 1.8
2.0 2.2
Figure 9. SNR for Cascaded Stages--Sequential Control
Figure 11. Gain Error for Cascaded Stages-Parallel Control
90 85 80
2.0 1.5 1.0
GAIN ERROR - dB
0.5 0.0 -0.5 -1.0 -1.5 -2.0 -0.2 0.0 0.2
IS/N RATIO - dB
75 70 65 60 55 50 -0.2
0.4 0.6
0.8
1.0 VC
1.2 1.4
1.6 1.8
2.0 2.2
0
0.2
0.4 VC
0.6
0.8
1.0
1.2
Figure 10. Gain Error for Cascaded Stages--Sequential Control
Figure 12. ISNR for Cascaded Stages-Parallel Control
Parallel Mode (Simplest Gain-Control Interface) In this mode, the gain-control of voltage is applied to both inputs in parallel--the GPOS pins of both A1 and A2 are connected to the control voltage and the GNEW inputs are grounded. The gain scaling is then doubled to 80 dB/V, requiring only a 1.00 V change for an 80 dB change of gain: Gain (dB) = 80 VG + GO (4) where, as before GO depends on the range selected; for example, in the maximum-bandwidth mode, GO is +20 dB. Alternatively, the GNEG pins may be connected to an offset voltage of +0.500 V, in which case, GO is -20 dB. The amplitude of the gain ripple in this case is also doubled, as shown in Figure 11, while the instantaneous signal-to-noise ratio at the output of A2 now decreases linearly as the gain increased (Figure 12).
Low Gain Ripple Mode (Minimum Gain Error) As can be seen from Figures 9 and 10, the error in the gain is periodic, that is, it shows a small ripple. (Note that there is also a variation in the output offset voltage, which is due to the gain interpolation, but this is not exact in amplitude.) By offsetting the gains of A1 and A2 by half the period of the ripple, that is, by 3 dB, the residual gain errors of the two amplifiers can be made to cancel. Figure 13 shows that much lower gain ripple when configured in this manner. Figure 14 plots the ISNR as a function of gain; it is very similar to that in the "Parallel Mode."
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AD603
3.0 2.5 2.0 1.5
GAIN ERROR - dB
THEORY OF THE AD603 A Low Noise AGC Amplifier
1.0 0.5 0.0 -0.5 -1.0 -1.5 -2.0 -2.5 -3.0 -0.1 0.0 0.1 0.2 0.3 0.4 0.5 VC 0.6 0.7 0.8 0.9 1.0 1.1
Figure 15 shows the ease with which the AD603 can be connected as an AGC amplifier. The circuit illustrates many of the points previously discussed: It uses few parts, has linear-in-dB gain, operates from a single supply, uses two cascaded amplifiers in sequential gain mode for maximum S/N ratio, and an external resistor programs each amplifier's gain. It also uses a simple temperature-compensated detector. The circuit operates from a single 10 V supply. Resistors R1, R2, R3, and R4 bias the common pins of A1 and A2 at 5 V. This pin is a low impedance point and must have a low impedance path to ground, here provided by the 100 F tantalum capacitors and the 0.1 F ceramic capacitors. The cascaded amplifiers operate in sequential gain. Here, the offset voltage between the pins 2 (GNEG) of A1 and A2 is 1.05 V (42.14 dB x 25 mV/dB), provided by a voltage divider consisting of resistors R5, R6, and R7. Using standard values, the offset is not exact, but it is not critical for this application. The gain of both A1 and A2 is programmed by resistors R13 and R14, respectively, to be about 42 dB; thus the maximum gain of the circuit is twice that, or 84 dB. The gain-control range can be shifted up by as much as 20 dB by appropriate choices of R13 and R14. The circuit operates as follows. A1 and A2 are cascaded. Capacitor C1 and the 100 of resistance at the input of A1 form a time-constant of 10 s. C2 blocks the small dc offset voltage at the output of A1 (which might otherwise saturate A2 at its maximum gain) and introduces a high-pass corner at about 16 kHz, eliminating low frequency noise.
0 0.2 0.4 VC 0.6 0.8 1.0 1.2
Figure 13. Gain Error for Cascaded Stages-Low Ripple Mode
90 85 80
IS/N RATIO - dB
75 70 65 60 55 50 -0.2
Figure 14. ISNR vs. Control Voltage-Low Ripple Mode
A half-wave detector is used, based on Q1 and R8. The current into capacitor CAV is just the difference between the collector current of Q2 (biased to be 300 A at 300 K, 27C) and the collector current of Q1, which increases with the amplitude of the
10V
THIS CAPACITOR SETS AGC TIME CONSTANT VAGC
C7 0.1 F C1 0.1 F J1 RT 100 1 10V R1 2.49k + C3 100 F2 C4 0.1 F R2 2.49k 10V R13 2.49k C8 0.1 F C2 0.1 F 10V R3 2.49k + C5 100 F2 C6 0.1 F R4 2.49k 10V R14 2.49k CAV 0.1 F
R9 1.54k Q2 2N3906
R10 1.24k
C11 0.1 F
R11 3.83k Q1 2N3904 R8 806 5V R12 4.99k C9 0.1 F
A1 AD603
A2 AD603
J2 C10 0.1 F
AGC LINE
R5 5.49k 5.5V NOTES 1R PROVIDES A 50 INPUT IMPEDANCE T 2C3 AND C5 ARE TANTALUM
1V OFFSET FOR SEQUENTIAL GAIN
R6 1.05k 6.5V
R7 3.48k
10V
Figure 15. A Low Noise AGC Amplifier
REV. C
-9-
AD603
output signal. The automatic gain control voltage, VAGC, is the time-integral of this error current. In order for VAGC (and thus the gain) to remain insensitive to short-term amplitude fluctuations in the output signal, the rectified current in Q1 must, on average, exactly balance the current in Q2. If the output of A2 is too small to do this, VAGC will increase, causing the gain to increase, until Q1 conducts sufficiently. Consider the case where R8 is zero and the output voltage VOUT is a square wave at, say, 455 kHz, which is well above the corner frequency of the control loop. During the time VOUT is negative with respect to the base voltage of Q1, Q1 conducts; when VOUT is positive, it is cut off. Since the average collector current of Q1 is forced to be 300 A, and the square wave has a duty-cycle of 1:1, Q1's collector current when conducting must be 600 A. With R8 omitted, the peak amplitude of VOUT is forced to be just the VBE of Q1 at 600 A, typically about 700 mV, or 2 VBE peak-to-peak. This voltage, hence the amplitude at which the output stabilizes, has a strong negative temperature coefficient (TC), typically -1.7 mV/C. Although this may not be troublesome in some applications, the correct value of R8 will render the output stable with temperature. To understand this, first note that the current in Q2 is made to be proportional to absolute temperature (PTAT). For the moment, continue to assume that the signal is a square wave. When Q1 is conducting, VOUT is now the sum of VBE and a voltage that is PTAT and which can be chosen to have an equal but opposite TC to that of the VBE. This is actually nothing more than an application of the "bandgap voltage reference" principle. When R8 is chosen such that the sum of the voltage across it and the VBE of Q1 is close to the bandgap voltage of about 1.2 V, VOUT will be stable over a wide range of temperatures, provided, of course, that Q1 and Q2 share the same thermal environment. Since the average emitter current is 600 A during each halfcycle of the square wave a resistor of 833 would add a PTAT voltage of 500 mV at 300 K, increasing by 1.66 mV/C. In practice, the optimum value will depend on the type of transistor used and, to a lesser extent, on the waveform for which the temperature stability is to be optimized; for the inexpensive 2N3904/2N306 pair and sine wave signals, the recommended value is 806 . This resistor also serves to lower the peak current in Q1 when more typical signals (usually, sinusoidal) are involved, and the 1.8 kHz LP filter it forms with CAV helps to minimize distortion due to ripple in VAGC. Note that the output amplitude under sine wave conditions will be higher than for a square wave, since the average value of the current for an ideal rectifier would be 0.637 times as large, causing the output amplitude to be 1.88 (=1.2/0.637) V, or 1.33 V rms. In practice, the somewhat nonideal rectifier results in the sine wave output being regulated to about 1.4 V rms, or 3.6 V p-p. The bandwidth of the circuit exceeds 40 MHz. At 10.7 MHz, the AGC threshold is 100 V (-67 dBm) and its maximum gain is 83 dB (20 log 1.4 V/100 V). The circuit holds its output at 1.4 V rms for inputs as low as -67 dBm to +15 dBm (82 dB), where the input signal exceeds the AD603's maximum input rating. For a 30 dBm input at 10.7 MHz, the second harmonic is 34 dB down from the fundamental and the third harmonic is 35 dB down.
CAUTION
Careful component selection, circuit layout, power-supply decoupling, and shielding are needed to minimize the AD603's susceptibility to interference from radio and TV stations, etc. In bench evaluation, we recommend placing all of the components in a shielded box and using feedthrough decoupling networks for the supply voltage. Circuit layout and construction are also critical, since stray capacitances and lead inductances can form resonant circuits and are a potential source of circuit peaking, oscillation, or both.
-10-
REV. C
AD603
2.50 2.00 1.50
GAIN ERROR - dB
45MHz
10.7MHz 0.50 0.00 -0.50 70MHz -1.00 -1.50 -0.5 -0.4 -0.3 -0.2 -0.1 0.0 0.2 0.3 0.4 0.5 0.6 GAIN VOLTAGE - Volts 455kHz
GAIN - dB
100k
1M 10M FREQUENCY - Hz
100M
GAIN - dB
1.00
70MHz
100k
1M 10M FREQUENCY - Hz
100M
Figure 16. Gain Error vs. Gain Control Voltage at 455 kHz, 10.7 MHz, 45 MHz, 70 MHz
Figure 17. Frequency and Phase Response vs. Gain (Gain = -10 dB, PIN = -30 dBm, Pin 5 Connected to Pin 7)
Figure 18. Frequency and Phase Response vs. Gain (Gain = +10 dB, PIN = -30 dBm, Pin 5 Connected to Pin 7)
7.60
+5V
7.40
0.1 F
GROUP DELAY - ns
7.20
GAIN - dB
HP3326A DUAL CHANNEL SYNTHESIZER 100
AD603
7.00
HP3585A 10 PROBE SPECTRUM ANALYZER
0.1 F
511
6.80
-5V
6.60
DATEL DVC 8500
100k
1M 10M FREQUENCY - Hz
100M
6.40 -0.6
-0.4 -0.2 0 0.2 0.4 GAIN CONTROL VOLTAGE - Volts
0.6
Figure 19. Frequency and Phase Response vs. Gain (Gain = +30 dB, PIN = -30 dBm, Pin 5 Connected to Pin 7)
Figure 20. Group Delay vs. Gain Control Voltage
Figure 21. Third Order Intermodulation Distortion Test Setup
10dB/DIV
10dB/DIV
NEGATIVE OUTPUT VOLTAGE LIMIT - Volts
-1.0 -1.2 -1.4 -1.6 -1.8 -2.0 -2.2 -2.4 -2.6 -2.8 -3.0 -3.2 -3.4 0 50 100 200 500 1000 2000 LOAD RESISTANCE -
Figure 22. Third Order Intermodulation Distortion at 455 kHz (10x Probe Used to HP3585A Spectrum Analyzer, Gain = 0 dB, PIN = 0 dBm, Pin 5 Connected to Pin 7)
Figure 23. Third Order Intermodulation Distortion at 10.7 MHz (10x Probe Used to HP3585A Spectrum Analyzer, Gain = 0 dB, PIN = 0 dBm, Pin 5 Connected to Pin 7)
Figure 24. Typical Output Voltage Swing vs. Load Resistance (Negative Output Swing Limits First)
REV. C
-11-
AD603
102 102 102
INPUT IMPEDANCE -
INPUT IMPEDANCE -
100
100
INPUT IMPEDANCE -
1M 10M FREQUENCY - Hz 100M
100
98
98
98
96
96
96
94 100k 1M 10M FREQUENCY - Hz 100M
94 100k
94 100k 1M 10M FREQUENCY - Hz 100M
Figure 25. Input Impedance vs. Frequency (Gain = -10 dB)
Figure 26. Input Impedance vs. Frequency (Gain = +10 dB)
Figure 27. Input Impedance vs. Frequency (Gain = +30 dB)
4.5V
8V
1V
100 90
INPUT GND 1V/DIV
INPUT GND 100mV/DIV
500mV
1V OUTPUT GND 1V/DIV
10 0%
1V
200ns
-500mV -49ns
OUTPUT GND 500mV/DIV
50ns
451ns
-2V -49ns
50ns
451ns
Figure 28. Gain-Control Channel Response Time
Figure 29. Input Stage Overload Recovery Time, Pin 5 Connected to Pin 7 (Input Is 500 ns Period, 50% Duty-Cycle Square Wave, Output Is Captured Using Tektronix 11402 Digitizing Oscilloscope)
Figure 30. Output Stage Overload Recovery Time, Pin 5 Connected to Pin 7 (Input Is 500 ns Period, 50% Duty-Cycle Square Wave, Output Is Captured Using Tektronix 11402 Digitizing Oscilloscope)
3.5V
3.5V
0 -10
INPUT 500mV/DIV
GND
INPUT GND 100mV/DIV
PSRR - dB
-20 -30 -40 -50 -60
500mV
500mV
OUTPUT 500mV/DIV
GND
OUTPUT GND 500mV/DIV
-1.5V -44ns
50ns
456ns
-1.5V -44ns
50ns
456ns
100k
1M 10M FREQUENCY - Hz
100M
Figure 31. Transient Response, G = 0 dB, Pin 5 Connected to Pin 7 (Input is 500 ns Period, 50% DutyCycle Square Wave, Output Is Captured Using Tektronix 11402 Digitizing Oscilloscope)
Figure 32. Transient Response, G = +20 dB, Pin 5 Connected to Pin 7 (Input is 500 ns Period, 50% DutyCycle Square Wave, Output Is Captured Using Tektronix 11402 Digitizing Oscilloscope)
Figure 33. PSRR vs. Frequency (Worst Case Is Negative Supply PSRR, Shown Here)
-12-
REV. C
AD603
23
+5V
0.1 F
21
30MHz 70MHz TA = 25 C RS = 50 TEST SETUP FIGURE 34
21 19
19
10MHz
NOISE FIGURE - dB
HP3326A DUAL CHANNEL SYNTHESIZER 100 0.1 F
17 15 13 11
10MHz 50MHz
NOISE FIGURE - dB
17 15 13 11 9 7
20MHz
TA = 25 C RS = 50 TEST SETUP FIGURE 34
AD603
50
HP3585A SPECTRUM ANALYZER
-5V
DATEL DVC 8500
9 7 5 20 21 22 23 24 25 26 27 28 29 30 GAIN - dB
Figure 34. Test Setup Used for: Noise Figure, 3rd Order Intercept and 1 dB Compression Point Measurements
5 30 31 32 33 34 35 36 37 38 39 40 GAIN - dB
Figure 35. Noise Figure in -10 dB/ +30 dB Mode
Figure 36. Noise Figure in 0 dB/+40 dB Mode
0
TA = 25 C TEST SETUP FIGURE 34
20
TA = 25 C TEST SETUP FIGURE 34
20
TA = 25 C RS = 50 RIN = 50 RL = 100 TEST SETUP FIGURE 34
-5
18
18
OUTPUT LEVEL - dBm
16
40MHz
OUTPUT LEVEL - dBm
30MHz
INPUT LEVEL - dBm
30MHz
16
40MHz
-10
14
14
-15
12
70MHz
12
70MHz
-20
10
10
-25 10
30 50 INPUT FREQUENCY - MHz
70
8 -20
-10 INPUT LEVEL - dBm
0
8 -40
-30 INPUT LEVEL - dBm
-20
Figure 37. 1 dB Compression Point, -10 dB/+30 dB Mode, Gain = 30 dB
Figure 38. 3rd Order Intercept -10 dB/ +30 dB Mode, Gain = 10 dB
Figure 39. 3rd Order Intercept, -10 dB/ +30 dB Mode, Gain = 30 dB
REV. C
-13-
AD603
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
8-Lead Cerdip (Q-8)
0.005 (0.13) MIN
8
0.055 (1.4) MAX
5
0.310 (7.87) 0.220 (5.59)
1 4
PIN 1 0.405 (10.29) MAX 0.200 (5.08) MAX 0.060 (1.52) 0.015 (0.38) 0.150 (3.81) MIN SEATING PLANE
0.320 (8.13) 0.290 (7.37)
0.200 (5.08) 0.125 (3.18) 0.023 (0.58) 0.100 0.070 (1.78) 0.014 (0.36) (2.54) 0.030 (0.76) BSC
15 0
0.015 (0.38) 0.008 (0.20)
8-Lead SOIC (SO-8)
0.1968 (5.00) 0.1890 (4.80)
8 5 4
0.1574 (4.00) 0.1497 (3.80) PIN 1
1
0.2440 (6.20) 0.2284 (5.80)
0.0500 (1.27) BSC 0.0098 (0.25) 0.0040 (0.10) SEATING PLANE 0.0688 (1.75) 0.0532 (1.35) 0.0192 (0.49) 0.0138 (0.35) 8 0.0098 (0.25) 0 0.0075 (0.19)
0.0196 (0.50) 0.0099 (0.25)
45
0.0500 (1.27) 0.0160 (0.41)
-14-
REV. C
PRINTED IN U.S.A.
C1851a-0-1/00 (rev. C)


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