Datasheet AD8307AR-REEL7, AD8307AR-REEL, AD8307AR, AD8307AN, AD8307-EB Datasheet (Analog Devices)
Page 1
Low Cost DC-500 MHz, 92 dB
a
FEATURES
Complete Multistage Logarithmic Amplifier
92 dB Dynamic Range: –75 dBm to +17 dBm
to –90 dBm Using Matching Network
Single Supply of 2.7 V Min at 7.5 mA Typical
DC-500 MHz Operation, ⴞ1 dB Linearity
Slope of 25 mV/dB, Intercept of –84 dBm
Highly Stable Scaling Over Temperature
Fully Differential DC-Coupled Signal Path
100 ns Power-Up Time, 150 A Sleep Current
APPLICATIONS
Conversion of Signal Level to Decibel Form
Transmitter Antenna Power Measurement
Receiver Signal Strength Indication (RSSI)
Low Cost Radar and Sonar Signal Processing
Network and Spectrum Analyzers (to 120 dB)
Signal Level Determination Down to 20 Hz
True Decibel AC Mode for Multimeters
Logarithmic Amplifier
AD8307
FUNCTIONAL BLOCK DIAGRAM
SUPPLY ENABLE
+INPUT
–INPUT
COMMON
VPS
INP
1.15kV
INM
COM
BANDGAP REFERENCE
7.5mA
SIX 14.3dB 900MHz
AMPLIFIER STAGES
3
NINE DETECTOR CELLS
SPACED 14.3dB
INPUT-OFFSET
COMPENSATION LOOP
AD8307
AND BIASING
MIRROR
2mA
/dB
2
COM
ENB
INT
OUT
12.5kV
OFS
INT. ADJ
OUTPUT
OFS. ADJ.
PRODUCT DESCRIPTION
The AD8307 is the first logarithmic amplifier in an 8-lead (SO-8)
package. It is a complete 500 MHz monolithic demodulating
logarithmic amplifier based on the progressive compression
(successive detection) technique, providing a dynamic range of
92 dB to ±3 dB law-conformance and 88 dB to a tight ±1 dB
error bound at all frequencies up to 100 MHz. It is extremely
stable and easy to use, requiring no significant external components. A single supply voltage of 2.7 V to 5.5 V at 7.5 mA is
needed, corresponding to an unprecedented power consumption
of only 22.5 mW at 3 V. A fast-acting CMOS-compatible control pin can disable the AD8307 to a standby current of under
150 µA.
Each of the cascaded amplifier/limiter cells has a small-signal
gain of 14.3 dB, with a –3 dB bandwidth of 900 MHz. The
input is fully differential and at a moderately high impedance
(1.1 kΩ in parallel with about 1.4 pF). The AD8307 provides a
basic dynamic range extending from approximately –75 dBm
(where dBm refers to a 50 Ω source, that is, a sine amplitude of
about ±56 µV) up to +17 dBm (a sine amplitude of ±2.2 V).
A simple input-matching network can lower this range to –88dBm
to +3 dBm. The logarithmic linearity is typically within ±0.3 dB
up to 100 MHz over the central portion of this range, and is
degraded only slightly at 500 MHz. There is no minimum
frequency limit; the AD8307 may be used at audio frequencies
(20 Hz) or even lower.
The output is a voltage scaled 25 mV/dB, generated by a current
of nominally 2 µA/dB through an internal 12.5 kΩ resistor. This
voltage varies from 0.25 V at an input of –74 dBm (that is, the
ac intercept is at –84 dBm, a 20 µV rms sine input), up to 2.5 V
for an input of +16 dBm. This slope and intercept can be trimmed
using external adjustments. Using a 2.7 V supply, the output
scaling may be lowered, for example to 15 mV/dB, to permit
utilization of the full dynamic range.
The AD8307 exhibits excellent supply insensitivity and temperature stability of the scaling parameters. The unique combination of low cost, small size, low power consumption, high
accuracy and stability, very high dynamic range, and a frequency
range encompassing audio through IF to UHF, make this product useful in numerous applications requiring the reduction of a
signal to its decibel equivalent.
The AD8307 is available in the industrial temperature range of
–40°C to +85°C, and in 8-lead SOIC and PDIP packages.
REV. A
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 © Analog Devices, Inc., 1999
Page 2
AD8307–SPECIFICA TIONS
(VS = +5 V, TA = 25ⴗC, RL ≥ 1M⍀, unless otherwise noted)
Parameter Conditions Min Typ Max Units
GENERAL CHARACTERISTICS
Input Range (±1 dB Error) Expressed in dBm re 50 Ω –72 16 dBm
Logarithmic Conformance f ≤ 100 MHz, Central 80 dB ±0.3 ±1dB
f = 500 MHz, Central 75 dB ±0.5 dB
Logarithmic Slope Unadjusted
vs. Temperature 23 27 mV/dB
Logarithmic Intercept Sine Amplitude; Unadjusted
1
2
23 25 27 mV/dB
20 µV
Equivalent Sine Power in 50 Ω –87 –84 –77 dBm
vs. Temperature –88 –76 dBm
Input Noise Spectral Density Inputs Shorted 1.5 nV/√Hz
Operating Noise Floor R
= 50 Ω/2 –78 dBm
SOURCE
Output Resistance Pin 4 to Ground 10 12.5 15 kΩ
Internal Load Capacitance 3.5 pF
Response Time Small Signal, 10%-90%, 400 ns
0 mV–100 mV, C
= 2 pF
L
Large Signal, 10%-90%, 500 ns
= 2 pF
L
500 MHz
Upper Usable Frequency
3
0 V–2.4 V, C
Lower Usable Frequency Input AC-Coupled 10 Hz
AMPLIFIER CELL CHARACTERISTICS
Cell Bandwidth –3 dB 900 MHz
Cell Gain 14.3 dB
INPUT CHARACTERISTICS
DC Common-Mode Voltage Inputs AC-Coupled 3.2 V
Common-Mode Range Either Input (Small Signal) –0.3 1.6 VS – 1 V
DC Input Offset Voltage
4
R
SOURCE
≤ 50 Ω 50 500 µV
Drift 0.8 µV/°C
Incremental Input Resistance Differential 1.1 kΩ
Input Capacitance Either Pin to Ground 1.4 pF
Bias Current Either Input 10 25 µA
POWER INTERFACES
Supply Voltage 2.7 5.5 V
Supply Current V
Disabled V
NOTES
1
This may be adjusted downward by adding a shunt resistor from the Output to Ground. A 50 kΩ resistor will reduce the nominal slope to 20 mV/dB.
2
This may be adjusted in either direction by a voltage applied to Pin 5, with a scale factor of 8 dB/V.
3
See Application on 900 MHz operation.
4
Normally nulled automatically by internal offset correction loop. May be manually nulled by a voltage applied between Pin 3 and Ground; see APPLICATIONS.
Specifications subject to change without notice.
≥ 2 V 8 10 mA
ENB
≤ 1 V 150 750 µA
ENB
–2–
REV. A
Page 3
AD8307
ABSOLUTE MAXIMUM RATINGS*
Supply Voltage . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . +7.5 V
Input Voltage (Pins 1, 8) . . . . . . . . . . . . . . . . . . . . . . V
SUPPLY
Storage Temperature Range, N, R . . . . . . . . –65°C to +125°C
*Stresses above those listed under Absolute Maximum Ratings may cause perma-
nent 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 effect device reliability.
Ambient Temperature Range, Rated Performance Industrial,
AD8307AN, AD8307AR . . . . . . . . . . . . . –40°C to +85°C
Lead Temperature Range (Soldering 10 sec) . . . . . . . +300°C
ORDERING GUIDE
Model Temperature Range Package Descriptions Package Options
AD8307AR –40°C to +85°C SOIC SO-8
AD8307AN –40°C to +85°C Plastic DIP N-8
AD8307AR-REEL 13" REEL
AD8307AR-REEL7 7" REEL
AD8307-EB Evaluation Board
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
WARNING!
the AD8307 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.
ESD SENSITIVE DEVICE
PIN CONFIGURATION
INM
COM
OFS
OUT
1
2
AD8307
TOP VIEW
3
(Not to Scale)
4
8
INP
7
VPS
6
ENB
5
INT
PIN FUNCTION DESCRIPTIONS
Pin Name Function
1 INM Signal Input, Minus Polarity; Normally at
V
/2.
POS
2 COM Common Pin (Usually Grounded).
3 OFS Offset Adjustment; External Capacitor
Connection.
4 OUT Logarithmic (RSSI) Output Voltage; R
OUT
=
12.5 kΩ.
5 INT Intercept Adjustment; ±6 dB (See Text).
6 ENB CMOS-compatible Chip Enable; Active when
“HI.”
7 VPS Positive Supply, 2.7 V–5.5 V.
8 INP Signal Input, Plus Polarity; Normally at V
POS
/
2. Note: Due to the symmetrical nature of the
response, there is no special significance to the
sign of the two input pins. DC resistance from
INP to INM = 1.1 kΩ.
–3–REV. A
Page 4
AD8307–T ypical Performance Characteristics
8
7
6
5
4
3
SUPPLY CURRENT – mA
2
1
0
1.0
1.1
1.2
1.3
1.4
1.5
ENB
1.6
– Volts
V
Figure 1. Supply Current vs. V
8
7
6
5
4
3
SUPPLY CURRENT – mA
2
1
1.7
1.8
Voltage (5 V)
ENB
1.9
2.0
3
2
1
0
ERROR – dB
–1
–2
–3
–80
TEMPERATURE ERROR @ +858C
TEMPERATURE ERROR @ +258C
TEMPERATURE ERROR @ –408C
–40 –20 0
INPUT LEVEL – dBm
20–60
Figure 4. Log Conformance vs. Input Level (dBm) at 25°C,
°
C, –40°C
85
3
INPUT FREQUENCY 10MHz
2
INPUT FREQUENCY 100MHz
– Volts
OUT
V
1
INPUT FREQUENCY 300MHz
INPUT FREQUENCY 500MHz
0
1.0
1.1
1.2
1.3
1.4
1.5
V
– Volts
ENB
Figure 2. Supply Current vs. V
3
2
1
0
ERROR – dB
–1
–2
–3
FREQUENCY INPUT = 300MHz
FREQUENCY INPUT = 100MHz
–80 20–60
INPUT LEVEL – dBm
–40 –20 0
1.7
1.6
Voltage (3 V)
ENB
1.8
1.9
2.0
Figure 3. Log Conformance vs. Input Level (dBm) @
100 MHz, 300 MHz
0
–80
Figure 5. V
1.5
1.0
0.5
0
ERROR – dB
–0.5
–1.0
– 1.5
vs. Input Level (dBm) at Various Frequencies
OUT
CFO VALUE = 0.01mF
CFO VALUE = 0.1mF
– 80 20– 60
–40 –20 0
INPUT LEVEL – dBm
CFO VALUE = 1mF
– 40 – 20 0
INPUT LEVEL – dBm
20–60
Figure 6. Log Conformance vs. CFO Values at 1 kHz Input
Frequency
–4–
REV. A
Page 5
3.0
INPUT LEVEL – dBm
3
2
–3
–80 20–60
ERROR – dB
–40 –20 0
1
0
–1
–2
– INPUT
+ INPUT
100MHz
INPUT LEVEL – dBm
3
2
–3
–70 10–60
ERROR – dB
–50 –40 –30
1
0
–1
–2
100MHz
500MHz
20–20 –10 0
10MHz
AD8307
2.5
2.0
INT PIN = 4.0V
10MHz, INT = –87.71dBm
1.5
– Volts
OUT
V
1.0
0.5
0
–80
Figure 7. V
–70 –50 –30 –10 10
OUT
10MHz, INT = –96.52dBm
vs. Input Level at 5 V Supply; Showing
Intercept Adjustment
3.0
2.5
2.0
INT VOLTAGE
INT NO CONNECT, INT = –71dBm
1.5
– Volts
OUT
V
1.0
INT PIN = 3.0V
NO CONNECT ON INT
10MHz, INT = –82.90dBm
INPUT LEVEL – dBm
–20 0
INT = 1.0V, INT = –86dBm
INT VOLTAGE
20–60 –40
Figure 10. Log Conformance vs. Input Level at 100 MHz;
Showing Response to Alternative Inputs
3
2
1
0
ERROR – dB
–1
100MHz
500MHz
0.5
0
–80 –70 –60 –50 –40 –30 –20 –10
Figure 8. V
vs. Input Level at 3 V Supply Using AD820
OUT
INT VOLTAGE
INT = 2.0V, INT = –78dBm
INPUT LEVEL – dBm
010
as Buffer, Gain = +2; Showing Intercept Adjustment
2.5
2.0
1.5
100MHz @ –408C
– Volts
OUT
1.0
100MHz @ +258C
V
0.5
100MHz @ +858C
0
–80 20–60
Figure 9. V
(–40
°
C, +25°C, +85°C)
OUT
–40 –20 0
INPUT LEVEL – dBm
vs. Input Level at Three Temperatures
–2
–3
–90 10–70
–50 –30 –10
INPUT LEVEL – dBm
Figure 11. Log Conformance vs. Input at 100 MHz, 500 MHz;
Input Driven Differentially Using Transformer
Figure 12. Log Conformance vs. Input Level at 3 V Supply
Using AD820 as Buffer, Gain = +2
–5–REV. A
Page 6
AD8307
Ch1 200mV
GND
500nsCh2 2.00V
Figure 13. Power-Up Response Time
Ch1 200mV
V
OUT
CH 1
V
ENB
CH 2
GND
500nsCh2 2.00V
V
OUT
CH 1
V
ENB
CH 2
CH 1 GND
INPUT SIGNAL
CH 2
2.5V
INPUT SIGNAL
CH 2
CH 1 GND
2V
Ch1 500mV
Figure 16. V
Ch1 500mV
Rise Time
OUT
V
OUT
CH 1
CH 2 GND
200nsCh2 1.00V
CH 2 GND
V
OUT
CH 1
200nsCh2 1.00V
Figure 14. Power-Down Response Time
HP8648B
SIGNAL
GENERATOR
RF OUT
52.3V
VPS = +5.0V
0.1mF
1nF
INP VPS ENB INT
AD8307
INM COM OFS OUT
1nF
NC = NO CONNECT
NC
HP8112A
GENERATOR
NC
TEK P6139A
10x PROBE
PULSE
OUT
SYNCH OUT
TEK744A
SCOPE
TRIG
Figure 15. Test Setup For Power-Up/Power-Down
Response Time
Figure 17. Large Signal Response Time
HP8648B
SIGNAL
GENERATOR
PULSE
MODULATION
MODE
RF OUT
10MHz REF CLK
PULSE MODE IN
VPS = +5.0V
1nF
INP VSP ENB INT
52.3V
INM COM OFS OUT
1nF
NC = NO CONNECT
Figure 18. Test Setup For V
0.1mF
AD8307
NC
EXT TRIG
OUT
NC
TEK P6204
FET PROBE
Pulse Response
OUT
HP8112A
PULSE
GENERATOR
TEK744A
SCOPE
TRIG
OUT
TRIG
–6–
REV. A
Page 7
AD8307
LOG AMP THEORY
Logarithmic amplifiers perform a more complex operation than
that of classical linear amplifiers, and their circuitry is significantly different. A good grasp of what log amps do, and how
they do it, will avoid many pitfalls in their application. The
essential purpose of a log amp is not to amplify, though amplification is utilized to achieve the function. Rather, it is to compress a signal of wide dynamic range to its decibel equivalent. It
is thus a measurement device. A better term might be logarithmic converter, since its basic function is the conversion of a
signal from one domain of representation to another, via a precise
nonlinear transformation.
Logarithmic compression leads to situations that may be confusing or paradoxical. For example, a voltage offset added to
the output of a log amp is equivalent to a gain increase ahead of
its input. In the usual case where all the variables are voltages,
and regardless of the particular structure, the relationship between
the variables can be expressed as:
V
= VY log (V
OUT
) (1)
IN /VX
where:
V
is the output voltage,
OUT
V
is called the slope voltage; the logarithm is usually taken
Y
to base-ten (in which case V
V
is the input voltage,
IN
is also the volts-per-decade),
Y
and
V
is called the intercept voltage.
X
All log amps implicitly require two references, here V
and VY,
X
which determine the scaling of the circuit. The absolute accuracy of a log amp cannot be any better than the accuracy of its
scaling references. Equation 1 is mathematically incomplete in
representing the behavior of a demodulating log amp such as
the AD8307, where V
has an alternating sign. However, the
IN
basic principles are unaffected, and we can safely use this as our
starting point in the analyses of log amp scaling which follow.
V
OUT
5V
Y
4V
V
OUT
Y
3V
Y
2V
Y
V
Y
= 0
VIN = 10–2V
–40dBc
–2V
Y
LOWER INTERCEPT
VIN = V
X
0dBc
X
V
V
IN
+40dBc
SHIFT
= 102V
LOG V
IN
= 104V
V
X
IN
X
+80dBc
Figure 19. Ideal Log Amp Function
Figure 19 shows the input/output relationship of an ideal log
amp, conforming to Equation 1. The horizontal scale is logarithmic and spans a wide dynamic range, shown here as over
120 dB, or six decades. The output passes through zero (the
log-intercept) at the unique value V
= VX and would ideally
IN
become negative for inputs below the intercept. In the ideal
case, the straight line describing V
for all values of VIN would
OUT
continue indefinitely in both directions. The dotted line shows
that the effect of adding an offset voltage V
to lower the effective intercept voltage V
X
to the output is
SHIFT
. Exactly the same
alteration could be achieved raising the gain (or signal level)
ahead of the log amp by the factor V
V
is 500 mV per decade (that is, 25 mV/dB, as for the AD8307),
Y
SHIFT/VY
. For example, if
an offset of +150 mV added to the output will appear to lower
the intercept by two tenths of a decade, or 6 dB. Adding an
offset to the output is thus indistinguishable from applying an
input level that is 6 dB higher.
The log amp function described by Equation 1 differs from that
of a linear amplifier in that the incremental gain ∂V
very strong function of the instantaneous value of V
/∂VIN is a
OUT
IN
, as is
apparent by calculating the derivative. For the case where the
logarithmic base is e, we have:
∂V
∂V
OUT
V
Y
=
V
IN
IN
(2)
That is, the incremental gain is inversely proportional to the
instantaneous value of the input voltage. This remains true for
any logarithmic base, which is chosen as 10 for all decibelrelated purposes. It follows that a perfect log amp would be
required to have infinite gain under classical small-signal (zeroamplitude) conditions. Less ideally, this result indicates that,
whatever means are used to implement a log amp, accurate
response under small-signal conditions (that is, at the lower end
of the dynamic range) demands the provision of a very high
gain-bandwidth product. A further consequence of this high
gain is that, in the absence of an input signal, even very small
amounts of thermal noise at the input of a log amp will cause a
finite output for zero input, resulting in the response line curving
away from the ideal shown in Figure 19 toward a finite baseline,
which can be either above or below the intercept. Note that the
value given for this intercept may be an extrapolated value, in
which case the output may not cross zero, or even reach it, as is
the case for the AD8307.
While Equation 1 is fundamentally correct, a simpler formula is
appropriate for specifying the calibration attributes of a log amp
like the AD8307, which demodulates a sine wave input:
V
OUT
= V
SLOPE (PIN
– P0) (3)
where:
V
is the demodulated and filtered baseband (video or
OUT
RSSI) output,
V
is the logarithmic slope, now expressed in volts/dB
SLOPE
(typically between 15 and 30 mV/dB),
P
is the input power, expressed in decibels relative to some
IN
reference power level,
and
P
is the logarithmic intercept, expressed in decibels relative
0
to the same reference level.
The most widely used reference in RF systems is decibels above
1 mW in 50 Ω, written dBm. Note that the quantity (P
– P0) is
IN
just dB. The logarithmic function disappears from the formula
because the conversion has already been implicitly performed in
stating the input in decibels. This is strictly a concession to popular convention: log amps manifestly do not respond to power
(tacitly, power absorbed at the input), but, rather, to input
–7–REV. A
Page 8
AD8307
voltage. The use of dBV (decibels with respect to 1 V rms) would
be more precise, though still incomplete, since waveform is
involved, too. Since most users think about and specify RF
signals in terms of power—even more specifically, in dBm re 50 Ω
—we will use this convention in specifying the performance of
the AD8307.
Progressive Compression
Most high speed high dynamic range log amps use a cascade of
nonlinear amplifier cells (Figure 20) to generate the logarithmic
function from a series of contiguous segments, a type of piecewise-linear technique. This basic topology immediately opens
up the possibility of enormous gain-bandwidth products. For
example, the AD8307 employs six cells in its main signal path,
each having a small-signal gain of 14.3 dB (×5.2) and a –3 dB
bandwidth of about 900 MHz; the overall gain is about 20,000
(86 dB) and the overall bandwidth of the chain is some 500MHz,
resulting in the incredible gain-bandwidth product (GBW) of
10,000 GHz, about a million times that of a typical op amp.
This very high GBW is an essential prerequisite to accurate
operation under small-signal conditions and at high frequencies.
Equation 2 reminds us, however, that the incremental gain will
decrease rapidly as V
increases. The AD8307 continues to
IN
exhibit an essentially logarithmic response down to inputs as
small as 50 µV at 500 MHz.
STAGE 1 STAGE 2 STAGE N –1 STAGE N
V
A
X
A A A
V
W
in the case of the AD8307, VY is traceable to an on-chip bandgap reference, while V
is derived from the thermal voltage kT/q
X
and later temperature-corrected.
Let the input of an N-cell cascade be V
. For small signals, the overall gain is simply AN. A six-
V
OUT
, and the final output
IN
stage system in which A = 5 (14 dB) has an overall gain of
15,625 (84 dB). The importance of a very high small-signal gain
in implementing the logarithmic function has been noted; however, this parameter is of only incidental interest in the design of
log amps.
From here onward, rather than considering gain, we will analyze
the overall nonlinear behavior of the cascade in response to a
simple dc input, corresponding to the V
very small inputs, the output from the first cell is V
from the second, V
a certain value of V
equal to the knee voltage E
are N–1 cells of gain A ahead of this node, we can calculate that
V
IN
= EK /A
N–1
= A2 VIN, and so on, up to VN = AN VIN. At
2
, the input to the Nth cell, V
IN
. Thus, V
K
. This unique situation corresponds to the lin-log
of Equation 1. For
IN
= AEK and since there
OUT
= AVIN;
1
, is exactly
N–1
transition, labeled 1 on Figure 22. Below this input, the cascade
of gain cells is acting as a simple linear amplifier, while for higher
values of V
, it enters into a series of segments which lie on a
IN
logarithmic approximation (dotted line).
V
OUT
(4A-3) E
K
Figure 20. Cascade of Nonlinear Gain Cells
To develop the theory, we will first consider a slightly different
scheme to that employed in the AD8307, but which is simpler
to explain and mathematically more straightforward to analyze.
This approach is based on a nonlinear amplifier unit, which we
may call an A/1 cell, having the transfer characteristic shown in
Figure 21. The local small-signal gain ∂V
tained for all inputs up to the knee voltage E
/∂VIN is A, main-
OUT
, above which the
K
incremental gain drops to unity. The function is symmetrical: the
same drop in gain occurs for instantaneous values of V
than –E
range –E
. The large-signal gain has a value of A for inputs in the
K
≤ +EK, but falls asymptotically toward unity for
K ≤ VIN
IN
less
very large inputs. In logarithmic amplifiers based on this amplifier function, both the slope voltage and the intercept voltage
must be traceable to the one reference voltage, E
. Therefore, in
K
this fundamental analysis, the calibration accuracy of the log amp
is dependent solely on this voltage. In practice, it is possible to
separate the basic references used to determine V
AE
A/1
K
OUTPUT
0
E
SLOPE = 1
SLOPE = A
K
and VX and
Y
INPUT
Figure 21. The A/1 Amplifier Function
(3A-2) E
(2A-1) E
AE
K
K
K
0
(A-1) E
K
RATIO
OF A
N–1
/A
E
K
EK/A
N–2
EK/A
N–3
EK/A
N–4
LOG V
IN
Figure 22. The First Three Transitions
Continuing this analysis, we find that the next transition occurs
when the input to the (N–1) stage just reaches E
V
= EK /A
IN
N–2
. The output of this stage is then exactly AEK,
; that is, when
K
and it is easily demonstrated (from the function shown in Figure
21) that the output of the final stage is (2A–1) E
Figure 22). Thus, the output has changed by an amount (A–1)E
for a change in VIN from EK /A
N–1
to EK /A
(labeled ➁ on
K
N–2
, that is, a ratio
K
change of A. At the next critical point, labeled ➂, we find the
input is again A times larger and V
that is, by another linear increment of (A–1)E
has increased to (3A–2)EK,
OUT
. Further analysis
K
shows that right up to the point where the input to the first cell
is above the knee voltage, V
change of A in V
. This can be expressed as a certain fraction
IN
of a decade, which is simply log
changes by (A–1)EK for a ratio
OUT
(A). For example, when A = 5
10
a transition in the piecewise linear output function occurs at
regular intervals of 0.7 decade (that is, log
(A), or 14 dB divided
10
by 20 dB). This insight allows us to immediately write the Volts
per Decade scaling parameter, which is also the Scaling Voltage
, when using base-10 logarithms, as:
V
Y
E
A−1
Linear Change in V
VY=
Decades Change in V
()
OUT
=
log10A
IN
K
()
(4)
–8–
REV. A
Page 9
AD8307
I
OUT
V
IN
A4V
IN
V
LIM
A/0
g
m
A/0
g
m
A3V
IN
A/0
g
m
A2V
IN
A/0
g
m
AV
IN
g
m
Note that only two design parameters are involved in determining V
, namely, the cell gain A and the knee voltage EK, while
Y
N, the number of stages, is unimportant in setting the slope of
the overall function. For A = 5 and E
= 100 mV, the slope
K
would be a rather awkward 572.3 mV per decade (28.6 mV/dB).
A well designed log amp will have rational scaling parameters.
The intercept voltage can be determined by using two pairs of
transition points on the output function (consider Figure 22).
The result is:
E
VX=
K
N+1/ A−1
()
()
A
(5)
For the case under consideration, using N = 6, we calculate
= 4.28 µV. However, we need to be careful about the inter-
V
Z
pretation of this parameter, since it was earlier defined as the
input voltage at which the output passes through zero (see Figure 19). But clearly, in the absence of noise and offsets, the
output of the amplifier chain shown in Figure 21 can be zero
when, and only when, V
= 0. This anomaly is due to the finite
IN
gain of the cascaded amplifier, which results in a failure to maintain
the logarithmic approximation below the lin-log transition (point ➀
in Figure 22). Closer analysis shows that the voltage given by
Equation 5 represents the extrapolated, rather than actual,
intercept.
Demodulating Log Amps
Log amps based on a cascade of A/1 cells are useful in baseband
VY=
Preference for the A/0 style of log amp, over one using A/1 cells,
stems from several considerations. The first is that an A/0 cell
can be very simple. In the AD8307 it is based on a bipolartransistor differential pair, having resistive loads R
emitter current source, I
voltage of E
The large signal transfer function is the hyperbolic tangent (see
dotted line in Figure 23). This function is very precise, and the
deviation from an ideal A/0 form is not detrimental. In fact, the
rounded shoulders of the tanh function beneficially result in a
lower ripple in the logarithmic conformance than that obtained
using an ideal A/0 function.
An amplifier built of these cells is entirely differential in structure and can thus be rendered very insensitive to disturbances
on the supply lines and, with careful design, to temperature
variations. The output of each gain cell has an associated
transconductance (g
put voltage of the cell to a pair of differential currents, which are
summed simply by connecting the outputs of all the g
tor) stages in parallel. The total current is then converted back
to a voltage by a transresistance stage, to generate the logarithmic output. This scheme is depicted, in single-sided form, in
Figure 24.
AE
K
log10A
()
and an
. This will exhibit an equivalent knee-
= 2 kT/q and a small signal gain of A = IERL /EK.
K
E
) cell, which converts the differential out-
m
L
(detec-
m
(6)
applications, because they do not demodulate their input signal.
However, baseband and demodulating log amps alike can be
made using a different type of amplifier stage, which we will call
an A/0 cell. Its function differs from that of the A/1 cell in that
the gain above the knee voltage E
falls to zero, as shown by the
K
solid line in Figure 23. This is also known as the limiter function, and a chain of N such cells is often used to generate a
hard-limited output, in recovering the signal in FM and PM
modes.
Figure 24. Log Amp Using A/0 Stages and Auxiliary Summing Cells
The chief advantage of this approach is that the slope voltage
SLOPE = 0
AE
K
E
K
TANH
SLOPE = A
INPUT
A/0
OUTPUT
0
Figure 23. A/0 Amplifier Functions (Ideal and Tanh)
The AD640, AD606, AD608, AD8307 and various other Analog
Devices communications products incorporating a logarithmic
IF amplifier all use this technique. It will be apparent that the
output of the last stage can no longer provide the logarithmic
output, since this remains unchanged for all inputs above the
limiting threshold, which occurs at V
= EK /A
IN
N–1
. Instead, the
logarithmic output is now generated by summing the outputs of
all the stages. The full analysis for this type of log amp is only
slightly more complicated than that of the previous case. It is
may now be decoupled from the knee-voltage E
which is inherently PTAT. By contrast, the simple summation
of the cell outputs would result in a very high temperature coefficient of the slope voltage given by Equation 6. To do this, the
detector stages are biased with currents (not shown in the Figure) which are rendered stable with temperature. These are
derived either from the supply voltage (as in the AD606 and
AD608) or from an internal bandgap reference (as in the AD640
and AD8307). This topology affords complete control over the
magnitude and temperature behavior of the logarithmic slope,
decoupling it completely from E
.
K
A further step is yet needed to achieve the demodulation response,
required when the log amp is to convert an alternating input
into a quasi-dc baseband output. This is achieved by altering the
g
cells used for summation purposes to also implement the
m
rectification function. Early discrete log amps based on the
progressive compression technique used half-wave rectifiers.
This made post-detection filtering difficult. The AD640 was the
first commercial monolithic log amp to use a full-wave rectifier,
a practice followed in all subsequent Analog Devices types.
= 2 kT/q,
K
readily shown that, for practical purpose, the intercept voltage
is identical to that given in Equation 5, while the slope
V
X
voltage is:
–9–REV. A
Page 10
AD8307
We can model these detectors as being essentially linear gm cells,
but producing an output current independent of the sign of the
voltage applied to the input of each cell. That is, they implement the absolute-value function. Since the output from the
later A/0 stages closely approximates an amplitude-symmetric
square wave for even moderate input levels (most stages of the
amplifier chain operate in a limiting mode), the current output
from each detector is almost constant over each period of the
input. Somewhat earlier detectors stages produce a waveform
having only very brief dropouts, while the detectors nearest the
input produce a low level almost-sinusoidal waveform at twice
the input frequency. These aspects of the detector system result
in a signal that is easily filtered, resulting in low residual ripple
on the output.
Intercept Calibration
All monolithic log amps from Analog Devices include accurate
means to position the intercept voltage V
(or equivalent power
X
for a demodulating log amp). Using the scheme shown in Figure
24, the basic value of the intercept level departs considerably
from that predicted by the simpler analyses given earlier. However, the intrinsic intercept voltage is still proportional to E
,
K
which is PTAT (Equation 5). Recalling that the addition of an
offset to the output produces an effect which is indistinguishable
from a change in the position of the intercept, we can cancel the
left-right motion of V
by adding an offset having the required temperature behavior.
E
K
resulting from the temperature variation of
X
The precise temperature-shaping of the intercept-positioning
offset results in a log amp having stable scaling parameters,
making it a true measurement device, for example, as a calibrated Received Signal Strength Indicator (RSSI). In this application, one is more interested in the value of the output for an
input waveform which is invariably sinusoidal. The input level
may alternatively be stated as an equivalent power, in dBm, but
here we must step carefully. It is essential to know the load
impedance in which this power is presumed to be measured.
In RF practice, it is generally safe to assume a reference impedance of 50 Ω, in which 0 dBm (1 mW) corresponds to a sinusoidal amplitude of 316.2 mV (223.6 mV rms). The intercept may
likewise be specified in dBm. For the AD8307, it is positioned
at –84 dBm, corresponding to a sine amplitude of 20 µV. It is
important to bear in mind that log amps do not respond to
power, but to the voltage applied to their input.
The AD8307 presents a nominal input impedance much higher
than 50 Ω (typically 1.1 kΩ at low frequencies). A simple input
matching network can considerably improve the sensitivity of
this type of log amp. This will increase the voltage applied to the
input and thus alter the intercept. For a 50 Ω match, the voltage
gain is 4.8 and the whole dynamic range moves down by 13.6 dB
(see Figure 33). Note that the effective intercept is a function of
waveform. For example, a square-wave input will read 6 dB
higher than a sine wave of the same amplitude, and a Gaussian
noise input 0.5 dB higher than a sine wave of the same rms
value.
Offset Control
In a monolithic log amp, direct-coupling between the stages is
used for several reasons. First, this avoids the use of coupling
capacitors, which may typically have a chip area equal to that of
a basic gain cell, thus considerably increasing die size. Second,
the capacitor values predetermine the lowest frequency at which
the log amp can operate; for moderate values, this may be as
high as 30 MHz, limiting the application range. Third, the parasitic (back-plate) capacitance lowers the bandwidth of the cell,
further limiting the applications.
But the very high dc gain of a direct-coupled amplifier raises a
practical issue. An offset voltage in the early stages of the chain
is indistinguishable from a ‘real’ signal. If it were as high as, say,
400 µV, it would be 18 dB larger than the smallest ac signal
(50 µV), potentially reducing the dynamic range by this amount.
This problem is averted by using a global feedback path from
the last stage to the first, which corrects this offset in a similar
fashion to the dc negative feedback applied around an op amp.
The high frequency components of the signal must, of course,
be removed, to prevent a reduction of the HF gain in the forward path.
In the AD8307, this is achieved by an on-chip filter, providing
sufficient suppression of HF feedback to allow operation above
1 MHz. To extend the range below this frequency, an external
capacitor may be added. This permits the high pass corner to be
lowered to audio frequencies using a capacitor of modest value.
Note that this capacitor has no effect on the minimum signal
frequency for input levels above the offset voltage: this extends
down to dc (for a signal applied directly to the input pins). The
offset voltage will vary from part to part; some will exhibit essentially stable offsets of under 100 µV, without the benefit of an
offset adjustment.
Extension of Range
The theoretical dynamic range for the basic log amp shown in
Figure 24 is A
N
. For A = 5.2 (14.3 dB) and N = 6, it is 20,000
or 86 dB. The actual lower end of the dynamic range is largely
determined by the thermal noise floor, measured at the input of
the chain of amplifiers. The upper end of the range is extended
upward by the addition of top-end detectors. The input signal is
applied to a tapped attenuator, and progressively smaller signals
are applied to three passive rectifying g
cells whose outputs are
m
summed with those of the main detectors. With care in design,
the extension to the dynamic range can be seamless over the full
frequency range. For the AD8307 it amounts to a further 27 dB.
The total dynamic range is thus theoretically 113 dB. The specified range of 90 dB (–74 dBm to +16 dBm) is that for high
accuracy, calibrated operation, and includes the low end degradation due to thermal noise, and the top end reduction due to
voltage limitations. The additional stages are not, however,
redundant, but are needed to maintain accurate logarithmic
conformance over the central region of the dynamic range, and
in extending the usable range considerably beyond the specified
range. In applications where log-conformance is less demanding, the AD8307 can provide over 95 dB of range.
–10–
REV. A
Page 11
AD8307
PRODUCT OVERVIEW
The AD8307 comprises six main amplifier/limiter stages, each
having a gain of 14.3 dB and small signal bandwidth of 900 MHz;
the overall gain is 86 dB with a –3 dB bandwidth of 500 MHz.
These six cells, and their associated g
-styled full-wave detec-
m
tors, handle the lower two-thirds of the dynamic range. Three
top-end detectors, placed at 14.3 dB taps on a passive attenuator, handle the upper third of the 90 dB range. Biasing for these
cells is provided by two references: one determines their gain;
the other is a bandgap circuit that determines the logarithmic
slope and stabilizes it against supply- and temperature-variations.
The AD8307 may be enabled/disabled by a CMOS-compatible
level at ENB (Pin 6). The first amplifier stage provides a low
voltage noise spectral density (1.5 nV/√Hz).
The differential current-mode outputs of the nine detectors are
summed and then converted to single-sided form in the output
stage, nominally scaled 2 µA/dB. The logarithmic output voltage
is developed by applying this current to an on-chip 12.5 kΩ
resistor, resulting in a logarithmic slope of 25 mV/dB (i.e.,
500 mV/decade) at OUT. This voltage is not buffered, allowing
the use of a variety of special output interfaces, including the
addition of post-demodulation filtering. The last detector stage
includes a modification to temperature-stabilize the log intercept,
which is accurately positioned to make optimal use of the full
output voltage range available. The intercept may be adjusted
using the pin INT, which adds or subtracts a small current to
the signal current.
SUPPLY ENABLE
+INPUT
–INPUT
COMMON
VPS
INP
1.1kV
INM
COM
BAND GAP REFERENCE
7.5mA
SIX 14.3dB 900MHz
AMPLIFIER STAGES
3
NINE DETECTOR CELLS
SPACED 14.3dB
INPUT– OFFSET
COMPENSATION LOOP
AD8307
AND BIASING
MIRROR
2mA
/dB
2
COM
ENB
OUT
12.5kV
OFS
COM
INT
INT. ADJ
OUTPUT
OFS. ADJ.
Figure 25. Main Features of the AD8307
The last gain stage also includes an offset-sensing cell. This
generates a bipolarity output current when the main signal path
has an imbalance due to accumulated dc offsets. This current is
integrated by an on-chip capacitor (which may be increased in
value by an off-chip component, at OFS). The resulting voltage
is used to null the offset at the output of the first stage. Since it
does not involve the signal input connections, whose ac coupling
capacitors otherwise introduce a second pole in the feedback
path, the stability of the offset correction loop is assured.
The AD8307 is built on an advanced dielectrically-isolated
complementary bipolar process. Most resistors are thin-film
types having a low temperature coefficient of resistance (TCR)
and high linearity under large signal conditions. Their absolute
tolerance will typically be within ±20%. Similarly, the capacitors
have a typical tolerance of ±15% and essentially zero temperature or voltage sensitivity. Most interfaces have additional small
junction capacitances associated with them, due to active
devices or ESD protection; these may be neither accurate nor
stable. Component numbering in each of these interface diagrams is local.
Enable Interface
The chip-enable interface is shown in Figure 26. The currents
in the diode-connected transistors control the turn-on and turnoff states of the bandgap reference and the bias generator, and
are a maximum of 100 µA when Pin 6 is taken to 5 V, under
worst case conditions. Left unconnected, or at a voltage below
1 V, the AD8307 will be disabled and consume a sleep current
of under 50 µA; tied to the supply, or a voltage above 2 V, it will
be fully enabled. The internal bias circuitry is very fast (typically
<100 ns for either OFF or ON), and in practice the latency
period before the log amp exhibits its full dynamic range is more
likely to be limited by factors relating to the use of ac coupling
at the input or the settling of the offset-control loop (see following sections).
AD8307
TO BIAS
STAGES
ENB
40kV
COM
Figure 26. Enable Interface
VPS
S
125V
COM
6kV
6kV
~3kV
S
Q1
Q2
I
E
2.4mA
INP
INM
COM
COM
4kV
2kV
TOP-END
DETECTORS
TYP +2.2V FOR
+3V SUPPLY,
+3.2V AT +5V
C
P
C
D
C
M
Figure 27. Signal Input Interface
Input Interface
Figure 27 shows the essentials of the signal input interface. C
P
and CM are the parasitic capacitances to ground; CD is the differential input capacitance, mostly due to Q1 and Q2. In most
applications both input pins are ac-coupled. The switches S
close when Enable is asserted. When disabled, the inputs float,
bias current I
is shut off, and the coupling capacitors remain
E
charged. If the log amp is disabled for long periods, small leakage currents will discharge these capacitors. If they are poorly
matched, charging currents at power-up can generate a transient
input voltage which may block the lower reaches of the dynamic
range until it has become much less than the signal.
–11–REV. A
Page 12
AD8307
In most applications, the signal will be single-sided, and may be
applied to either Pin 1 or Pin 8, with the other pin ac-coupled to
ground. Under these conditions, the largest input signal that can
be handled by the AD8307 is +10 dBm (sine amplitude of ±1V)
when operating from a 3 V supply; a +16 dBm may be handled
using a 5 V supply. The full 16 dBm may be achieved for supplies down to 2.7 V, using a fully balanced drive. For frequencies
above about 10 MHz, this is most easily achieved using a matching
network (see below). Using such a network, having an inductor
at the input, the input transient noted above is eliminated. Occasionally, it may be desirable to use the dc-coupled potential of
the AD8307. The main challenge here is to present signals to
the log amp at the elevated common-mode input level, requiring
the use of low noise, low offset buffer amplifiers. Using dual
supplies of ±3 V, the input pins may operate at ground potential.
Offset Interface
The input-referred dc offsets in the signal path are nulled via the
interface associated with Pin 3, shown in Figure 28. Q1 and Q2
are the first stage input transistors, with their corresponding
load resistors (125 Ω). Q3 and Q4 generate small currents,
which can introduce a dc offset into the signal path. When the
voltage on OFS is at about 1.5 V, these currents are equal, and
nominally 16 µA. When OFS is taken to ground, Q4 is off and
the effect of the current in Q3 is to generate an offset voltage of
16 µA × 125 Ω = 2 mV. Since the first stage gain is ×5, this is
equivalent to a input offset (INP to INM) of 400 µV. When
OFS is taken to its most positive value, the input-referred offset
is reversed, to –400 µV. If true dc-coupling is needed, down to
very small inputs, this automatic loop must be disabled, and the
residual offset eliminated using a manual adjustment, as explained
in the next section.
In normal operation, however, using an ac-coupled input signal,
the OFS pin should be left open. Any residual input-offset voltage is then automatically nulled by the action of the feedback
loop. The g
cell, which is gated off when the chip is disabled,
m
converts any output offset (sensed at a point near the end of the
cascade of amplifiers) to a current. This is integrated by the onchip capacitor C
, plus any added external capacitance C
HP
OFS
,
so as to generate an error voltage, which is applied back to the
input stage in the polarity needed to null the output offset. From
a small-signal perspective, this feedback alters the response of
the amplifier, which, rather than behaving as a fully dc-coupled
system, now exhibits a zero in its ac transfer function, resulting
in a closed-loop high-pass corner at about 700 kHz.
VPS
1.2V
Q1
125V
Q2
16mA AT
BALANCE
Q3
36kV
Q4
MAIN GAIN
48kV
STAGES
OFS
TO LAST
DETECTOR
S
g
m
AVERAGE
ERROR
CURRENT
C
OFS
C
HP
COM
INPUT
STAGE
BIAS,
Figure 28. Offset Interface and Offset-Nulling Path
The offset feedback is limited to a range ±400 µV; signals larger
than this override the offset control loop, which only impacts
performance for very small inputs. An external capacitor reduces the high pass corner to arbitrarily low frequencies; using
1 µF this corner is below 10 Hz. All ADI log amps use an offsetnulling loop; the AD8307 differs in using this single-sided form.
Output Interface
The outputs from the nine detectors are differential currents,
having an average value that is dependent on the signal input
level, plus a fluctuation at twice the input frequency. The currents are summed at nodes LGP and LGN in Figure 29. Further currents are added at these nodes, to position the intercept,
by slightly raising the output for zero input, and to provide
temperature compensation. Since the AD8307 is not lasertrimmed, there is a small uncertainty in both the log slope and
the log intercept. These scaling parameters may be adjusted (see
below).
For zero-signal conditions, all the detector output currents are
equal. For a finite input, of either polarity, their difference is
converted by the output interface to a single-sided unipolar
current nominally scaled 2 µA/dB (40 µA/decade), at the output
pin OUT. An on-chip 12.5 kΩ resistor, R1, converts this current to a voltage of 25 mV/dB. C1 and C2 are effectively in
shunt with R1 and form a low-pass filter pole, with a corner
frequency of about 5 MHz. The pulse response settles to within
1% of the final value within 300 ns. This integral low-pass filter
provides adequate smoothing in many IF applications. At
10.7 MHz, the 2f ripple is 12.5 mV in amplitude, equivalent to
±0.5 dB, and only 0.5 mV (±0.02 dB) at f = 50 MHz. A filter
capacitor C
added from OUT to ground will lower this cor-
FLT
ner frequency. Using 1 µF, the ripple is maintained to less than
±0.5 dB down to input frequencies of 100 Hz. Note that C
OFS
(above) should also be increased in low frequency applications,
and will typically be made equal to C
FLT
.
It may be desirable to increase the speed of the output response,
with the penalty of increased ripple. One way to do this is simply by connecting a shunt load resistor from OUT to ground,
which raises the low pass corner frequency. This also alters the
logarithmic slope, for example to 7.5 mV/dB using a 5.36 kΩ
resistor, while reducing the 10%-90% rise time to 25 ns. The
ripple amplitude for 50 MHz input remains 0.5 mV, but this is
now equivalent to ±0.07 dB. If a negative supply is available,
the output pin may be connected directly to the summing
node of an external op amp connected as an inverting-mode
transresistance stage.
LGP
LGM
25mV/dB
OUT
FROM ALL
DETECTORS
C
FLT
3pF
2mA/dB
0-220mA
C1
2.5pF
1.25kV
1.25kV
C2
1pF
R1
12.5kV
1.25kV
400mV
1.25kV
8.25kV
60kV
BIAS
60mA
VPS
INT
COM
–12–
Figure 29. Simplified Output Interface
REV. A
Page 13
AD8307
INPUT LEVEL – dBm
3
2.5
0
–80 20–60
OUTPUT VOLTAGE – Volts
–40 –20 0
2
1.5
1
0.5
500MHz
–70 –50 –30 –10 10
100MHz
10MHz
INPUT LEVEL – dBm
5
4
–5
–80
20
–60
ERROR – dB
–40 –20
0
3
2
1
–4
500MHz
–70 –50 –30 –10 10
100MHz
10MHz
–3
–2
–1
0
USING THE AD8307
The AD8307 has very high gain and a bandwidth from dc to
over 1 GHz, at which frequency the gain of the main path is still
over 60 dB. Consequently, it is susceptible to all signals within
this very broad frequency range that find their way to the input
terminals. It is important to remember that these are quite indistinguishable from the “wanted” signal, and will have the effect
of raising the apparent noise floor (that is, lowering the useful
dynamic range). For example, while the signal of interest may
be an IF of 50 MHz, any of the following could easily be larger
than the IF signal at the lower extremities of its dynamic range:
60 Hz hum, picked up due to poor grounding techniques; spurious coupling from a digital clock source on the same PC board;
local radio stations; etc.
Careful shielding is essential. A ground plane should be used to
provide a low impedance connection to the common pin COM,
for the decoupling capacitor(s) used at VPS, and as the output
ground. It is inadvisable to assume that the ground plane is an
equipotential, however, and neither of the inputs should be accoupled directly to the ground plane, but kept separate from it,
being returned instead to the low associated with the source.
This may mean isolating the low side of an input connector with
a small resistance to the ground plane.
Basic Connections
Figure 30 shows the simple connections suitable for many applications. The inputs are ac-coupled by C1 and C2, which should
have the same value, say, C
. The coupling time-constant is R
C
IN
CC/2, thus forming a high pass corner with a 3 dB attenuation at
f
= 1/(p R
HP
). In high frequency applications, fHP should
IN CC
be as large as possible, in order to minimize the coupling of
unwanted low frequency signals. Conversely, in low frequency
applications, a simple RC network forming a low-pass filter
should be added at the input for the same reason. For the case
where the generator is not terminated, the signal range should
be expressed in terms of the voltage response, and extends from
–85 dBV to +6 dBV.
Figure 31 shows the output versus the input level, in dBm when
driven from a terminated 50 Ω generator, for sine inputs at
10 MHz, 100 MHz and 500 MHz; Figure 32 shows the typical
logarithmic conformance under the same conditions. Note that
+10 dBm corresponds to a sine amplitude of 1 V, equivalent to
an rms power of 10 mW in a 50 Ω termination. But if the termination resistor is omitted, the input power is negligible. The use
of dBm to define input level therefore needs to be considered
carefully in connection with the AD8307.
Figure 31. Log Response at 10 MHz, 100 MHz and 500 MHz
INPUT
–75dBm TO
+16dBm
Figure 30. Basic Connections
Where it is necessary to terminate the source at a low impedance, the resistor R
shunting effect of the basic 1.1 kΩ input resistance (R
AD8307. For example, to terminate a 50 Ω source a 52.3 Ω 1%
tolerance resistor should be used. This may be placed on the
input side or the log-amp side of the coupling capacitors; in the
former case, smaller capacitors can be used for a given frequency range; in the latter case, the effective R
directly at the log-amp inputs.
0.1mF
C1 = C
C
INP VPS ENB INT
R
<
IN
R
T
1.1kV
INM COM OFS OUT
C2 = C
C
NC = NO CONNECT
should be added, with allowance for the
T
AD8307
NC
4.7V
NC
VP, 2.7V – 5.5V
8mA
AT
OUTPUT
25mV/dB
IN
is lowered
IN
) of the
Figure 32. Logarithmic Law Conformance at 10 MHz,
100 MHz and 500 MHz
Input Matching
Where higher sensitivity is required, an input matching network
is valuable. Using a transformer to achieve the impedance transformation also eliminates the need for coupling capacitors,
lowers the offset voltage generated directly at the input, and
balances the drives to INP and INM. The choice of turns ratio
will depend somewhat on the frequency. At frequencies below
50 MHz, the reactance of the input capacitance is much higher
than the real part of the input impedance. In this frequency
range, a turns ratio of about 1:4.8 will lower the input impedance to 50 Ω while raising the input voltage, and thus lowering
the effect of the short circuit noise voltage by the same factor.
There will be a small contribution from the input noise current,
so the total noise will be reduced by a somewhat smaller factor.
The intercept will also be lowered by the turns ratio; for a
50 Ω match, it will be reduced by 20 log
(4.8) or 13.6 dB.
10
–13–REV. A
Page 14
AD8307
Narrow-Band Matching
Transformer coupling is useful in broadband applications. However, a magnetically-coupled transformer may not be convenient
in some situations. At high frequencies, it is often preferable to
use a narrow-band matching network, as shown in Figure 33.
This has several advantages. The same voltage gain is achieved,
providing increased sensitivity, but now a measure of selectively
is also introduced. The component count is low: two capacitors
and an inexpensive chip inductor. Further, by making these
capacitors unequal the amplitudes at INP and INM may be
equalized when driving from a single-sided source; that is, the
network also serves as a balun. Figure 34 shows the response for
a center frequency of 100 MHz; note the very high attenuation
at low frequencies. The high-frequency attenuation is due to the
input capacitance of the log amp.
50V INPUT
–88dBm TO
+3dBm
C1
ZIN = 50V
C2
0.1mF
L
M
NC = NO CONNECT
INP VPS ENB INT
INM COM OFS OUT
AD8307
NC
4.7V
NC
VP, 2.7V – 5.5V
AT
8mA
OUTPUT
25mV/dB
Figure 33. High Frequency Input Matching Network
14
13
12
11
10
9
8
7
6
DECIIBELS
5
4
3
2
1
0
–1
60 15080
70 90 120 140
100 110 130
FREQUENCY – MHz
GAIN
INPUT
Figure 34. Response of 100 MHz Matching Network
Table I provides solutions for a variety of center frequencies F
C
and matching impedances ZIN of nominally 50 Ω and 100 Ω.
The unequal capacitor values were chosen to provide a wellbalanced differential drive, and also to allow better centering of
the frequency response peak when using standard value components; this generally results in a Z
that is not exact. The full
IN
AD8307 HF input impedance and the inductor losses were
included in the modeling.
Table I. Narrow-Band Matching Values
F
C
Z
IN
C1 C2 L
M
Voltage
MHz Ω pF pF nH Gain (dB)
10 45 160 150 3300 13.3
20 44 82 75 1600 13.4
50 46 30 27 680 13.4
100 50 15 13 330 13.4
150 57 10 8.2 220 13.2
200 57 7.5 6.8 150 12.8
250 50 6.2 5.6 100 12.3
500 54 3.9 3.3 39 10.9
10 103 100 91 5600 10.4
20 102 51 43 2700 10.4
50 99 22 18 1000 10.6
100 98 11 9.1 430 10.5
150 101 7.5 6.2 260 10.3
200 95 5.6 4.7 180 10.3
250 92 4.3 3.9 130 9.9
500 114 2.2 2.0 47 6.8
Slope and Intercept Adjustments
Where higher calibration accuracy is needed, the adjustments
shown in Figure 35 can be used, either singly or in combination.
The log slope is lowered to 20 mV/dB by shunting the nominally
12.5 kΩ on-chip load resistor (see Figure 29) with 50 kΩ,
adjusted by VR1. The calibration range is ±10% (18 mV/dB to
22 mV/dB), including full allowance for the variability in the
value of the internal load. The adjustment may be made by
alternately applying two input levels, provided by an accurate
signal generator, spaced over the central portion of the log amp’s
dynamic range, for example –60 dBm and 0 dBm. An AMmodulated signal, at the center of the dynamic range, can also
be used. For a modulation depth M, expressed as a fraction, the
decibel range between the peaks and troughs over one cycle of
the modulation period is given by:
∆ dB = 20 log
10
1+ M
1− M
(7)
For example, using an rms signal level of –40 dBm with a 70%
modulation depth (M = 0.7), the decibel range is 15 dB, as the
signal varies from –47.5 dBm to –32.5 dBm.
The log intercept is adjustable over a ±3 dB range, which is
sufficient to absorb the worst-case intercept error in the AD8307
plus some system-level errors. For greater range, set R
to zero.
S
VR2 is adjusted while applying an accurately known CW signal
near the lower end of the dynamic range, in order to minimize
the effect of any residual uncertainty in the slope. For example,
to position the intercept to –80 dBm, a test level of –65 dBm
may be applied and VR2 adjusted to produce a dc output of
15 dB above zero at 25 mV/dB, which is +0.3 V.
INPUT
–75dBm TO
+16dBm
NC = NO CONNECT
C1 = C
C2 = C
0.1mF
C
INP VPS ENB INT
AD8307
INM COM OFS OUT
C
NC
32.4kV
4.7V
VR2
R
50kV
63dB
FOR VP = 3V, RS = 20kV
VR1
50kV
S
V
= 5V, RS = 51kV
P
VP, 2.7V – 5.5V
8mA
AT
20mV/dB
610%
–14–
Figure 35. Slope and Intercept Adjustments
REV. A
Page 15
AD8307
APPLICATIONS
The AD8307 is a highly versatile and easily applied log amp
requiring very few external components. Most applications of
this product can be accommodated using the simple connections shown in the preceding section. A few examples of more
specialized applications are provided here.
Buffered Output
The output may be buffered, and the slope optionally increased,
using an op amp. If the single-supply capability is to be preserved, a suitable component is the AD8031. Like the AD8307,
it is capable of operating from a 2.7 V supply and features a railto-rail output capability; it is available in a 5-pin version and in
dual form as the 8-pin AD8032. Figure 36 shows how the slope
may be increased to 50 mV/dB (1 V per decade), requiring a 5 V
supply (90 dB times 50 mV is a 4.5 V swing). VR1 provides a
±10% slope adjustment; VR2 provides a ±3 dB intercept range.
With R2 = 4.99 kΩ, the slope is adjustable to 25 mV/dB, allowing the use of a 2.7 V supply. Setting R2 to 80.6 kΩ, it is raised
to 100 mV/dB, providing direct reading in decibels on a digital
voltmeter. Since a 90 dB range now corresponds to a 9 V swing,
a supply of at least this amount is needed for the op amp.
INPUT
–75dBm TO
+16dBm
0.1mF
INP VPS ENB INT
AD8307
INM COM OFS OUT
4.7V
VR2
63dB
VR1
50kV
R
AD8031
20mV/dB
50kV
NC
32.4kV
NC = NO CONNECT
S
C1
VP, 2.7V – 5.5V
= 3V, RS = 20kV
FOR V
P
V
= 5V, RS = 51kV
P
R2
30.1kV
R1
20kV
OUTPUT
50mV/dB
610%
COM
Figure 36. Log Amp with Buffered Output
C1 is optional; it lowers the corner frequency of the low-pass
output filter. A value of 0.1 µF should be used for applications
in which the output is measured on a voltmeter or other low
speed device. On the other hand, when C1 is omitted the 10%90% response time is under 200 ns, and is typically 300 ns to
99% of final value. To achieve faster response times, it is necessary to lower the load resistance at the output of the AD8307,
then restore the scale using a higher gain in the op amp. Using
8.33 kΩ, the basic slope is 10 mV/dB; this can be restored to
25 mV/dB using a buffer gain of 2.5. The overall 10%-90%
response time is under 100 ns. Figure 37 shows how the output
current capability can be augmented to drive a 50 Ω load; R
T
optionally provides reverse termination, which halves the slope
to 12.5 mV/dB.
Four-Pole Filter
In low frequency applications, for example, audio down to 20 Hz,
it is useful to employ the buffer amplifier as a multipole low-pass
filter, in order to achieve low output ripple while maintaining a
rapid response time to changes in signal level.
INPUT
–75dBm TO
+16dBm
0.1mF
INP VPS ENB INT
AD8307
INM COM OFS OUT
4.7V
VR2
50kV
63dB
10mV/dB 618%
NC
VR1
5kV
6.34kV
NC = NO CONNECT
(SEE FIGURE 36)
R
S
AD8031
R1
2kV
2N3904
25mV/dB
R2
3.01kV
V
, 2.7–5.5V
P
R
T
(OPTIONAL)
OUTPUT
50V
MIN
COM
Figure 37. Cable-Driving Log Amp
In Figure 38, the capacitor values were chosen for operation in
the audio field, providing a corner frequency of 10 Hz, an attenuation of 80 dB/decade above this frequency, and a 1% settling
time of 150 ms (0.1% in 175 ms). The residual ripple is 4 mV
(±0.02 dB) when the input to the AD8307 is at 20 Hz. This
filter may easily be adapted to other frequencies, by proportional
scaling of C5–C7 (e.g., for 100 kHz use 100 pF). Placed ahead
of a digital multimeter, the convenient slope scaling of 100 mV/dB
requires only a repositioning of the decimal point to read directly
in decibels. The supply voltage for the filter must be large enough
to support the dynamic range; a minimum of 9 V is needed for
most applications; 12 V is recommended.
INPUT
5mV TO
160V rms
C3
2.5nF
0.1mF
R1
50kV
C1
10mF
INP VPS ENB INT
AD8307
INM COM OFS OUT
C2
10mF
VR1
2kV
INT 64dB
C4
1mF
NC
4.7V
422V
VR2
50kV
SLOPE
32.4kV
V
OP AMP IS AD8032
P
SCALE C1 – C8 AS NEEDED
(SEE TEXT). NOTE POLARITIES
IF TANTALUM CAPACITORS
ARE USED.
7.32kV
C5
1mF
34kV
1mF
C6
100kV
34kV
80.6kV
C8
1mF
C7
1mF
OUTPUT
100mV/dB
93kV
75kV
COM
Figure 38. Log Amp with Four-Pole Low-Pass Filter
Figure 38 also shows the use of an input attenuator which may
optionally be employed here, or in any other of these applications, to produce a useful wide-range ac voltmeter with directdecibel scaling. The basic range of –73 dBm to +17 dBm (that
is, 50 µV rms to 1.6 V rms, for sine excitations) is shifted, for
illustrative purposes, to 5 mV to 160 V rms (at which point the
power in R1 is 512 mW). Because the basic input resistance of
the AD8307 is not precise, VR1 is used to center the signal
range at its input, doubling as a ±4 dB intercept adjustment.
The low frequency response extends to 15 Hz; a higher corner
frequency can be selected as needed, by scaling C1 and C2. The
shunt capacitor C3 is used to lower the high frequency bandwidth to about 100 kHz, and thus lower the susceptibility to
spurious signals. Other values should be chosen as needed for
the coupling and filter capacitors.
–15–REV. A
Page 16
AD8307
1 W to 1 kW 50 ⍀ Power Meter
The front-end adaptation shown in Figure 39 provides the measurement of power being delivered from a transmitter final amplifier to an antenna. The range has been set to cover the power
range –30 dBm (7.07 mV rms, or 1 µW) to +60 dBm (223 V rms,
or 1 kW). A nominal voltage attenuation ratio of 158:1 (44 dB) is
used; thus the intercept is moved from –84 dBm to –40 dBm and
the AD8307, scaled 0.25 V/decade of power, will now read 1.5 V
for a power level of 100 mW, 2.0 V at 10 W and 2.5 V at 1 kW.
The general expression is:
P (dBm) = 40 (V
OUT
– 1)
The required attenuation could be implemented using a capacitive divider, providing a very low input capacitance, but it is
difficult to ensure accurate values of small capacitors. A better
approach is to use a resistive divider, taking the required precautions to minimize spurious coupling into the AD8307 by placing
it in a shielded box, with the input resistor passing through a
hole in this box, as indicated in the figure. The coupling capacitors shown here are suitable for f ≥ 10 MHz. A capacitor may be
added across the input pins of the AD8307 to reduce the response to spurious HF signals which, as already noted, extends
to over 1 GHz.
The mismatch caused by the loading of this resistor will be
trivial; only 0.05% of the power delivered to the load will be
absorbed by the measurement system, a maximum of 500 mW
at 1 kW. The post-demodulation filtering and slope-calibration
arrangements should be chosen from other applications described
here, to meet the particular system requirements. The 1 nF
capacitor lowers the risk of HF signals entering the AD8307 via
the load.
TO
ANTENNA
50V INPUT
FROM P.A.
1mW TO
1kW
100kV
1/2W
51pF
VR1
2kV
INT 63dB
604V
51pF
NC = NO CONNECT
0.1mF
NC
INP VPS ENB INT
AD8307
INM COM OFS OUT
NC
1nF
22V
LEAD-
THROUGH
CAPACITORS,
2kV
1nF
OUTPUT
V
P
+5V
V
OUT
Figure 39. 1 µW to 1 kW 50-Ω Power Meter
Measurement System with 120 dB Dynamic Range
The dynamic range of the AD8307 can be extended further—
from 90 dB to over 120 dB—by the addition of an X-AMP™
such as the AD603. This type of variable gain amplifier exhibits
a very exact exponential gain control characteristic, which is
another way of stating that the gain varies by a constant number
of decibels for a given change in the control voltage. For the
AD603, this scaling factor is 40 dB/V, or 25 mV/dB. It will be
apparent that this property of a linear-in-dB response is characteristic of log amps; indeed, the AD8307 exhibits the same
scaling factor.
The AD603 has a very low input referred noise: 1.3 nV/√Hz at
its 100-Ω input, or 0.9 nV/√Hz when matched to 50 Ω, equivalent
to 0.4 µV rms, or –115 dBm, in a 200 kHz bandwidth. It is also
capable of handling inputs in excess of 1.4 V rms, or +16 dBm.
It is thus able to cope with a dynamic range of over 130 dB in
this particular bandwidth.
Now, if the gain control voltage for the X-AMP is derived from
the output of the AD8307, the effect will be to raise the gain of
this front-end stage when the signal is small and lower it when it
is large, but without altering the fundamental logarithmic nature
of the response. This gain range is 40 dB, which, combined with
the 90 dB range of the AD8307, again corresponds to a 130 dB
range.
NC
80.6k
0.1mF
R7
V
VP , +5V
NC
OUTPUT
10mV/dB
0.3V
TO
2.3V
50
INPUT
–105dBm
TO
+15dBm
750nH
150pF
V
L1
C1
28k
0.65V
R5
100k
R2
GPOS
GNEG
VINP
COMM
R1
187k
V
VPOS
VOUT
AD603
VNEG
FDBK
V
* E.G., MURATA SFE10.7MS2G-A
NC = NO CONNECT
BANDPASS
V
, –5V
V
N
0.15V TO 1.15V
FILTER*
R3
V
330
464
VR1
V
5k
INT
6
8dB
4.7
INP VPS ENB INT
R4
V
INM COM OFS OUT
1nF
R6
20k
V
AD8307
V
Figure 40. 120 dB Measurement System
Figure 40 shows how these two parts can work together to provide state-of-the-art IF measurements in applications such as
spectrum/ network analyzers and other high dynamic range
instrumentation. To understand the operation, note first that
the AD8307 is used to generate an output of about 0.3 V to
2.3 V. This 2 V span is divided by 2 in R5/R6/R7 to provide the
1 V span needed by the AD603 to vary its gain by 40 dB. Note
that an increase in the positive voltage applied at GNEG (Pin 2)
lowers the gain. This feedback network is tapped to provide a
convenient 10 mV/dB scaling at the output node, which may be
buffered if necessary.
The center of the voltage range fed back to the AD603 is 650 mV
and the ±20 dB gain range is centered by R1/R2. Note that the
intercept calibration of this system benefits from the use of a
well regulated 5 V supply. To absorb the insertion loss of the
filter and center the full dynamic range, the intercept is adjusted
by varying the maximum gain of the AD603, using VR1.
Figure 41 shows the AD8307 output over the range –120 dBm
to +20 dBm and the deviation from an ideal logarithmic response. The dotted line shows the increase in the noise floor
that results when the filter is omitted; the decibel difference is
about 10log10(50/0.2) or 24 dB, assuming a 50 MHz bandwidth from the AD603. An L-C filter may be used in place of
the ceramic filter used in this example.
X-AMP is a trademark of Analog Devices, Inc.
–16–
REV. A
Page 17
AD8307
2.50
2.25
2.00
1.75
1.50
1.25
– Volts
1.00
OUT
V
0.75
0.50
0.25
0
–100
WITH FILTER
–80
WITHOUT
FILTER
ERROR
(WITH FILTER)
–60 –40
INPUT LEVEL – dBm
–20 0
2
1
0
–1
–2
20
ERROR – dB
Figure 41. Results for 120 dB Measurement System
Operation at Low Frequencies
The AD8307 provides excellent logarithmic conformance at
signal frequencies that may be arbitrarily low, depending only
on the values used for the input coupling capacitors. It may also
be desirable to add a low-pass input filter in order to desensitize
the log amp to HF signals. Figure 42 shows a simple arrangement, providing coupling with an attenuation of 20 dB; the
intercept is shifted up by this attenuation, from –84 dBm to
–64 dBm, and the input range is now 0.5 mV to 20 V (sine
amplitude).
A high pass 3 dB corner frequency of nominally 3 Hz is set by
the 10 µF coupling capacitors C1 and C2, which are preferably
tantalum electrolytics (note the polarity) and a low pass 3 dB
corner frequency of 200 kHz (set by C3 and the effective resistance at the input of 1 kΩ). The –1% amplitude error points
occur at 20 Hz and 30 kHz. These are readily altered to suit
other applications by simple scaling. When C3 is zero, the low
pass corner is at 200 MHz. Note that the lower end of the dynamic range is improved by this capacitor, which provides essentially an HF short circuit at the input, thus significantly
lowering the wideband noise; the noise reduction is about 2 dB
compared to the case when the AD8307 is driven from a 50 Ω
source.
To ensure that the output is free of post-demodulation ripple, it
is necessary to lower the low-pass filter time-constant. This is
provided by C5; with the value shown, the output time-constant
is 125 ms. (See also Figure 38 for a more elaborate filter). Finally,
to improve the law-conformance at very low signal levels and at
low frequencies, C4 has been added to the offset compensation
loop.
+5V
V
4.7
0.1mF
R1
V
C3
R2
V
INP
VPS
AD8307
INM COM OFS OUT
1mF
C4
NC
ENB INT
FOR SLOPE AND
INTERCEPT ADJUSTMENTS
SEE FIGURE 35
V
OUT
25mV/dB
C5
1mF
NC = NO CONNECT
V
IN
0.5mV
TO 20V
SINE
AMPLITUDE
C1
10mF
C2
10mF
5k
750pF
5k
Figure 42. Connections for Low Frequency Operation
DC-Coupled Applications
It may occasionally be necessary to provide response to dc inputs. Since the AD8307 is internally dc-coupled, there is no
fundamental reason why this is precluded. However, there is a
practical constraint, which is that its inputs must be positioned
about 2 V above the COM potential for proper biasing of the
first stage. If it happens that the source is a differential signal at
this level, it may be directly connected to the input. For example, a microwave detector can be ac-coupled at its RF input
and its baseband load then automatically provided by the “floating” R
and CIN of the AD8307, at about VP/2.
IN
Usually, the source will be a single-sided ground-referenced
signal, and it will thus be necessary to provide a negative supply
for the AD8307. This can be achieved as shown in Figure 43.
The output is now referenced to this negative supply, and it is
necessary to provide an output interface that performs a differential-to-single-sided conversion. This is the purpose of the
AD830. The slope may be arranged to be 20 mV/dB, when the
output ideally runs from zero, for a dc input of 10 µV, to +2.2 V
for an input of 4 V. The AD8307 is fundamentally insensitive to
the sign of the input signal, but with this biasing scheme, the
maximum negative input is constrained to about –1.5 V. The
transfer function after trimming and with R7 = 0, is
V
= (0.4 V) log10 (VIN/10µV)
OUT
V
IN
AD589
+5V
TEMP
R3
1kV
R1
4.7V
3.3kV
1mF
R2
C2
0.1mF
Q1
2N3904
C1
INP
ENB INT
VPS
AD8307
INM COM OFS OUT
–2V
VR1
2kV
* 51kV FOR
100mV/dB
C3
0.1mF
VR2
50kV
R5
*
20mV/dB
5k FOR
20mV/dB
VP
INT
X1 X2 Y1 Y2
R6
32.4kV
VR3
50kV
+5V FOR 20mV/dB
+10V FOR 50mV/dB
+15V FOR 100mV/dB
AD830
Figure 43. Connections for DC-Coupled Applications
–17–REV. A
NC VN
R9
250V
–5V
–5V
V
R7
R7,R8:
SEE TEXT
R8
NC = NO CONNECT
OUT
Page 18
AD8307
The intercept can be raised, for example, to 100 µV, with the
rationale that the dc precision does not warrant operation in the
first decade (from 10 µV–100 µV). Likewise, the slope can be
raised to 50 mV/dB, using R7 = 3 kΩ, R8 = 2 kΩ, or to 100 mV/
dB, to simplify decibel measurements on a DVM, using R7 =
8kΩ, R8 = 2 kΩ, which raises the maximum output to +11 V,
thus requiring a +15 V supply for the AD830. The output may
be made to swing in a negative direction by simply reversing
Pins 1 and 2. Low-pass filtering capacitor C3 sets the output
rise time to about 1 ms.
6.0
5.5
5.0
4.5
10
1.0
0.5
0
–0.5
–1.0
ERROR – dB
– V
OUT
V
4.0
3.5
3.0
2.5
2.0
1.5
1.0
0.5
0
10m
100m
1m 10m 100m
V
IN
1
Figure 44. Ideal Output and Law-Conformance Error for
the DC-Coupled AD8307 at 50 mV/dB
Figure 44 shows the output and the law-conformance error in
the absence of noise and input offset, for the 50 mV/dB option.
Note in passing that the error ripple for dc excitation is about
twice that for the more usual sinusoidal excitation. In practice,
both the noise and the internal offset voltage will degrade the
accuracy in the first decade of the dynamic range. The latter is
now manually nulled, by VR1, using a simple method that ensures very low residual offsets.
A temporary ac signal, typically a sine wave of 100 mV in amplitude at a frequency of about 100 Hz, is applied via the capacitor
at node TEMP; this has the effect of disturbing the offset-nulling
voltage. The output voltage is then viewed on an oscilloscope
and VR1 is adjusted until the peaks of the (frequency-doubled)
waveform are exactly equal in amplitude. This procedure can
provide an input null down to about 10 µV; the temperature
drift is very low, though not specified since the AD8307 is not
principally designed to operate as a baseband log amp, and in ac
modes this offset is continuously and automatically nulled.
Next, it is necessary to set the intercept. This is the purpose of
VR2, which should be adjusted after VR1. The simplest method
is to short the input and adjust VR2 for an output of 0.3 V,
corresponding to the noise floor. For more exacting applications, a temporary sinusoidal test voltage of 1 mV in amplitude,
at about 1 MHz, should be applied, which may require the use
of a temporary onboard input attenuator. For 20 mV/dB scaling,
a 10 µV dc intercept (which is 6 dB below the ac intercept)
requires adjusting the output to 0.68 V; for the 100 mV/dB
scaling, this becomes 3.4 V. If a 100 µV intercept is preferred
(usefully lowering the maximum output voltage), these become
0.28 V and 1.4 V respectively.
Finally, the slope must be adjusted. This can be performed by
applying a low frequency square wave to the main input, having
precisely determined upper and lower voltage levels, provided
by a programmable waveform generator. A suitable choice is a
100 Hz square wave with levels of 10 mV and 1 V. The output
will be a low-pass filtered square wave, and its amplitude should
be 0.8 V, for 20 mV/dB scaling, or 4 V for 100 mV/dB scaling.
Operation Above 500 MHz
The AD8307 is not intended for use above 500 MHz. However,
it does provide useful performance at higher frequencies.
Figure 45 shows a plot of the logarithmic output of the AD8307
for an input frequency of 900 MHz. The device shows good
logarithmic conformance from –50 dBm to –10 dBm. There is a
“bump” in the transfer function at –5 dBm, but if this is acceptable, the device is usable over a 60 dB dynamic range (–50 dBm
to +10 dBm).
2
1.8
1.6
1.4
1.2
1
– Volts
OUT
0.8
V
0.6
0.4
0.2
0
–50 –30 –10 10
–60
–40 –20 0
PIN – dBm
Figure 45. Output vs. Input Level for a 900 MHz Input Signal
Evaluation Board
An evaluation board, carefully laid out and tested to demonstrate the specified high speed performance of the AD8307 is
available. Figure 46 shows the schematic of the evaluation board.
For ordering information, please refer to the Ordering Guide.
Figures 47 and 49 show the component-side and solder-side
silkscreens of the evaluation board. The component-side and
solder-side layouts are shown in Figures 48 and 50.
For connection to external instruments, side-launched SMA
type connectors are provided. Space is also provided on the
board for the installation of SMB or SMC type connectors.
When using the top-mount SMA connector, it is recommended
that the stripline on the outside 1/8" of the board edge be removed (i.e., scraped using a blade) as this unused stripline acts
as an open stub, which could degrade the overall performance of
the evaluation board/device combination at high frequencies.
–18–
REV. A
Page 19
AD8307
+V
S
C3
10mF
C4
0.1mF
A
B
INPUT
LK1
R1
52.3V
C2
0.1mF
INP VPS ENB INT
INM COM OFS OUT
C1
0.1mF
AD8307
C6
1nF
LK5
LK2
LK4 LK3
C5
0.1mF
Figure 46. Evaluation Board Schematic
R2
50kV
R3
12.5kV
LOG
OUTPUT
Figure 49. Solder Side Silkscreen
Figure 47. Component Side Silkscreen
Figure 48. Board Layout (Component Side)
Figure 50. Board Layout (Solder Side)
Link and Trim Options
There are a number of link options and trim potentiometers on
the evaluation board which should be set for the required operating setup before using the board. The functions of these link
options and trim potentiometers are described in detail in
Table II.
–19–REV. A
Page 20
AD8307
Table II. Evaluation Board Link Options
Link No. Default Position Function
LK1 A Power Up/Power Down. When this link is in position B, the ENB pin is connected to ground,
putting the AD8307 in power-down mode. Placing this link in position A connects the ENB
pin to the positive supply, thereby putting the AD8307 in normal operating mode.
LK2 Open Intercept Adjust. When Pin LK2 is left open, the AD8307 has a nominal logarithmic
intercept of –84 dBm. Putting LK2 in place connects the wiper of potentiometer R2 to Pin 5
(INT). By varying the voltage on INT, the position of the intercept can be adjusted. The intercept varies by about 8 dB/V.
LK3 Open Slope Adjust. When this link is open, the nominal slope of the output is 25 mV/dB. Putting this
link in place connects a ground referenced 12.5 kΩ load resistor (R3) to the logarithmic output. The parallel combination of this resistor and an internal 12.5 kΩ resistor reduces the
logarithmic slope to 12.5 mV/dB. R3 may be adjusted for other scaling factors.
LK4 Open Corner Frequency of Low-Pass Demodulating Filter. When this link is open, the corner fre-
quency of the low pass post demodulation filter has a nominal value of 4 MHz. This is set by
an on-chip load impedance of 12.5 kΩ and an on-chip load capacitance of 3.5 pF. The load
capacitance (e.g., of an oscilloscope probe) must be added to this capacitance, and will lower
the internal video bandwidth, to a nominal 1 MHz for a total of 13.5 pF. Putting LK4 in place
connects an external load capacitance (C5) of 0.1 µF to the output, reducing the corner fre-
quency of the low-pass filter to about 125 Hz. For large values of C5, the corner frequency can
be calculated using the equation, f ≈ 12.7 Hz/C5 (
LK5 Open Offset Control Loop. When this link is open, the internal offset control loop gives the circuit an
overall high pass corner frequency of about 1 MHz. With LK5 link in place, a 1 nF capacitor
(C6) is connected to the OFS pin, reducing the high pass corner frequency to allow accurate
operation down to 10 kHz. To reduce the minimum operational frequency even further, a
larger capacitor can replace C6 (e.g., a 1 µF capacitor allows operation down to 10 Hz). Note
that that external capacitor C6 has no effect on the minimum signal frequency for input levels
that exceed the offset voltage (typically 400 µV). The range for such signals extends down to dc
(for signals applied directly to the input pins).
µ
F).
C3065a–0–3/99
0.210 (5.33)
MAX
0.160 (4.06)
0.115 (2.93)
0.022 (0.558)
0.014 (0.356)
8-Lead Plastic DIP
(N-8)
0.430 (10.92)
0.348 (8.84)
8
14
PIN 1
0.100
(2.54)
BSC
5
0.280 (7.11)
0.240 (6.10)
0.060 (1.52)
0.015 (0.38)
0.070 (1.77)
0.045 (1.15)
0.130
(3.30)
MIN
SEATING
PLANE
0.325 (8.25)
0.300 (7.62)
0.015 (0.381)
0.008 (0.204)
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
0.1574 (4.00)
0.1497 (3.80)
0.195 (4.95)
0.115 (2.93)
PIN 1
0.0098 (0.25)
0.0040 (0.10)
SEATING
PLANE
0.1968 (5.00)
0.1890 (4.80)
8
0.0688 (1.75)
0.0532 (1.35)
0.0500
0.0192 (0.49)
(1.27)
0.0138 (0.35)
BSC
8-Lead SOIC
(SO-8)
5
0.2440 (6.20)
41
0.2284 (5.80)
0.0098 (0.25)
0.0075 (0.19)
0.0196 (0.50)
0.0099 (0.25)
88
08
0.0500 (1.27)
0.0160 (0.41)
3 458
PRINTED IN U.S.A.
–20–
REV. A
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