AD8314
Rev. B | Page 9 of 20
2.3
1.7
2.7 3.5
V
S
(V)
V
DN
(V)
2.2
2.1
2.0
1.9
1.8
2.8 2.9 3.0 3.1 3.2 3.3 3.4
0mA
2mA
4mA
6mA
01086-022
Figure 22. Maximum V
DN
Voltage vs. V
S
by Load Current
V
UP
GND
V
DN
GND
VPOS AND ENABLE
2V PER
VERTICAL
DIVISION
V
UP
AVERAGE: 128 SAMPLES
GND
V
UP
500mV/VERTICAL
DIVISION
V
UP
500mV/VERTICAL
DIVISION
1µs PER
HORIZONTAL
DIVISION
01086-023
Figure 23. Power-On and Power-Off Response, Measurement Mode
1
2
3
4
ENBL
RFIN
AD8314
RF OUT
TEK
TDS784C
SCOPE
TRIG
OUT
HP8116A
PULSE
GENERATOR
10MHz REF OUTPUT
NC = NO CONNECT
NC
8
7
6
5
VSET
FLTR
V_DN
VPOS
COMM
V_UP
TEK P6204
FET PROBE
TEK P6204
FET PROBE
PULSE
OUT
TRIG
52.3
33dB
V
HP8648B
SIGNAL
GENERATOR
EXT TRIG
49.9
732
AD811
01086-024
Figure 24. Test Setup for Power-On and Power-Off Response
2.3
1.7
2.7 3.5
V
S
(V)
V
DN
(V)
2.2
2.1
2.0
1.9
1.8
2.8 2.9 3.0 3.1 3.2 3.3 3.4
SHADING INDICATES
±3 SIGMA
01086-025
Figure 25. Maximum V
DN
Voltage vs. V
S
with 3 mA Load
100ns PER
HORIZONTAL
DIVISION
200mV PER
VERTICAL
DIVISION
V
DN
AVERAGE: 128 SAMPLES
2V PER
VERTICAL
DIVISION
VPOS AND ENABLE
V
DN
GND
GND
01086-026
Figure 26. Power-On Response, V
DN
, Controller Mode with VSET Held Low
1
2
3
4
ENBL
RFIN
AD8314
RF OUT
TEK
TDS784C
SCOPE
TRIG
OUT
HP8112A
PULSE
GENERATOR
10MHz REF OUTPUT
NC = NO CONNECT
NC
NC
8
7
6
5
VSET
FLTR
V_DN
VPOS
COMM
V_UP
TEK P6204
FET PROBE
PULSE
OUT
TRIG
HP8648B
SIGNAL
GENERATOR
EXT TRIG
49.9
732
AD811
52.3
0.2
01086-027
Figure 27. Test Setup for Power-On Response at V_DN Output,
Controller Mode with VSET Pin Held Low
AD8314
Rev. B | Page 10 of 20
THEORY OF OPERATION
The AD8314 is a logarithmic amplifier (log amp) similar in
design to the AD8313; further details about the structure and
function can be found in the
AD8313 data sheet and other log
amps produced by ADI.
Figure 28 shows the main features of
the AD8314 in block schematic form.
The AD8314 combines two key functions needed for the
measurement of signal level over a moderately wide dynamic
range. First, it provides the amplification needed to respond to
small signals, in a chain of four amplifier/limiter cells, each
having a small signal gain of 10 dB and a bandwidth of
approximately 3.5 GHz. At the output of each of these amplifier
stages is a full-wave rectifier, essentially a square-law detector
cell, that converts the RF signal voltages to a fluctuating current
having an average value that increases with signal level. A
further passive detector stage is added prior to the first stage.
Therefore, there are five detectors, each separated by 10 dB,
spanning some 50 dB of dynamic range. The overall accuracy at
the extremes of this total range, viewed as the deviation from an
ideal logarithmic response, that is, the law-conformance error,
can be judged by reference to
Figure 7, which shows that errors
across the central 40 dB are moderate.
Figure 5, Figure 6, Figure 8
through
Figure 11, Figure 13, and Figure 14 show how the
conformance to an ideal logarithmic function varies with
supply voltage, temperature, and frequency.
The output of these detector cells is in the form of a differential
current, making their summation a simple matter. It can easily
be shown that such summation closely approximates a logarithmic
function. This result is then converted to a voltage, at Pin V_UP,
through a high-gain stage. In measurement modes, this output
is connected back to a voltage-to-current (V-I) stage, in such a
manner that V_UP is a logarithmic measure of the RF input
voltage, with a slope and intercept controlled by the design. For
a fixed termination resistance at the input of the AD8314, a
given voltage corresponds to a certain power level.
However, in using this part, it must be understood that log
amps do not fundamentally respond to power. It is for this
reason the dBV is used (decibels above 1 V rms) rather than the
commonly used metric of dBm. While the dBV scaling is fixed,
independent of termination impedance, the corresponding
power level is not. For example, 224 mV rms is always −13 dBV
(with one further condition of an assumed sinusoidal waveform;
see the
Applications section for more information on the effect
of waveform on logarithmic intercept), and it corresponds to a
power of 0 dBm when the net impedance at the input is 50 Ω.
When this impedance is altered to 200 Ω, the same voltage
clearly represents a power level that is four times smaller
(P = V
2
/R), that is, −6 dBm. Note that dBV can be converted to
dBm for the special case of a 50 Ω system by simply adding
13 dB (0 dBV is equivalent to +13 dBm).
Therefore, the external termination added prior to the AD8314
determines the effective power scaling. This often takes the
form of a simple resistor (52.3 Ω provides a net 50 Ω input),
but more elaborate matching networks can be used. This
impedance determines the logarithmic intercept, the input
power for which the output would cross the baseline (V_UP =
zero) if the function were continuous for all values of input.
Because this is never the case for a practical log amp, the
intercept refers to the value obtained by the minimum-error
straight-line fit to the actual graph of V_UP vs. PIN (more
generally, V
IN
). Again, keep in mind that the quoted values
assume a sinusoidal (CW) signal. Where there is complex
modulation, as in CDMA, the calibration of the power response
needs to be adjusted accordingly. Where a true power (waveform-
independent) response is needed, the use of an rms-responding
detector, such as the
AD8361, should be considered.
10dB
OFFSET
COMPENSATION
V-I
I-V
RFIN
COMM
(
PADDLE)
VPOS
X2
ENBL
V_DN
V_UP
VSET
FLTR
AD8314
10dB10dB 10dB
BAND GAP
REFERENCE
DETDET
+
+
DETDETDET
01086-028
Figure 28. Block Schematic
AD8314
Rev. B | Page 11 of 20
Table 4. Typical Specifications at Selected Frequencies at 25°C (Mean and Σ)
±1 dB Dynamic Range
1
(dBV)
Slope (mV/dB) Intercept (dBV)
High Point Low Point
Frequency (GHz)
μ σ μ σ μ σ μ σ
0.1 21.3 0.4 −62.2 0.4 –11.8 0.3 −59 0.5
0.9 20.7 0.4 −63.6 0.4 –13.8 0.3 −61.4 0.4
1.9 19.7 0.4 −66.3 0.4 –19 0.7 −64 0.6
2.5 19.2 0.4 −62.1 0.7 –16.4 1.7 −61 1.3
1
Refer to Figure 32.
However, the logarithmic slope, the amount by which the
output V_UP changes for each decibel of input change (voltage
or power) is, in principle, independent of waveform or termination
impedance. In practice, it usually falls off somewhat at higher
frequencies, due to the declining gain of the amplifier stages
and other effects in the detector cells. For the AD8314, the slope
at low frequencies is nominally 21.3 mV/dB, falling almost
linearly with frequency to about 19.2 mV/dB at 2.5 GHz. These
values are sensibly independent of temperature (see
Figure 10)
and almost totally unaffected by the supply voltage from 2.7 V
to 5.5 V (see
Figure 11).
INVERTED OUTPUT
The second provision is the inclusion of an inverting amplifier
to the output, for use in controller applications. Most power
amplifiers require a gain-control bias that must decrease from a
large positive value toward ground level as the power output is
required to decrease. This control voltage, which appears at
Pin V_DN, is not only of the opposite polarity to V_UP, but also
needs to have an offset added to determine its most positive value
when the power level (assumed to be monitored through a
directional coupler at the output of the PA) is minimal.
The starting value of V_DN is nominally 2.25 V, and it falls on a
slope of twice that of V_UP; in other words,−43 mV/dB.
Figure 29
shows how this is achieved: the reference voltage that determines
the maximum output is derived from the on-chip voltage
reference and is substantially independent of the supply voltage
or temperature. However, the full output cannot be attained for
supply voltages under 3.3 V;
Figure 22 shows this dependency.
The relationship between V_UP and V_DN is shown in
Figure 30.
V-I
BAND GAP
REFERENCE
+2
VSET
+
FLTR
I-V
1.125V
V
DN
= 2.25V – 2.0 × V_UP
CURRENTS FROM
DETECTORS
AD8314
V_UP
V_DN
01086-029
Figure 29. Output Interfaces
2.5
0
–60 0
INPUT AMPLITUDE (dBV)
VOLTS
2.0
1.5
1.0
0.5
–50 –40 –30 –20 –10
OUTPUT FOR
MEASUREMENT
OUTPUT FOR
PA CONTROL
V_UP
V_DN
01086-030
Figure 30. Showing V_UP and V_DN Relationship

AD8314ARM-REEL7

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
RF Detector RF Detector/Cntlr 100MHz-2.7GHz 45dB
Lifecycle:
New from this manufacturer.
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