AD8310
Rev. F | Page 15 of 24
INPUT LEVEL (dBV)
–5
–120 20–100
(–87dBm)
–80 –60 –40 –20 0
(+13dBm)
5
ERROR (dB)
4
–1
–2
–3
–4
2
0
3
1
10MHz
50MHz
100MHz
±3dB DYNAMIC RANGE
±1dB DYNAMIC RANGE
01084-030
Figure 30. Log Conformance Error vs. Input Level at 10 MHz,
50 MHz, and 100 MHz
TRANSFER FUNCTION IN TERMS OF SLOPE AND
INTERCEPT
The transfer function of the AD8310 is characterized in terms
of its slope and intercept. The logarithmic slope is defined as the
change in the RSSI output voltage for a 1 dB change at the input.
For the AD8310, slope is nominally 24 mV/dB. Therefore, a
10 dB change at the input results in a change at the output of
approximately 240 mV. The plot of log conformance shows the
range over which the device maintains its constant slope. The
dynamic range of the log amp is defined as the range over
which the slope remains within a certain error band, usually
±1 dB or ±3 dB. In Figure 30, for example, the ±1 dB dynamic
range is approximately 95 dB (from +4 dBV to −91 dBV).
The intercept is the point at which the extrapolated linear
response would intersect the horizontal axis (see Figure 29).
For the AD8310, the intercept is calibrated to be −108 dBV
(−95 dBm). Using the slope and intercept, the output voltage
can be calculated for any input level within the specified input
range using the following equation:
V
OUT
= V
SLOPE
× (P
IN
P
O
) (3)
where:
V
OUT
is the demodulated and filtered RSSI output.
V
SLOPE
is the logarithmic slope expressed in V/dB.
P
IN
is the input signal expressed in dB relative to some reference
level (either dBm or dBV in this case).
P
O
is the logarithmic intercept expressed in dB relative to the
same reference level.
For example, for an input level of −33 dBV (−20 dBm), the
output voltage is
V
OUT
= 0.024 V/dB × (−33 dBV − (−108 dBV)) = 1.8 V (4)
dBV vs. dBm
The most widely used convention in RF systems is to specify
power in dBm, decibels above 1 mW in 50 Ω. Specification of
the log amp input level in terms of power is strictly a concession
to popular convention. As mentioned previously, log amps do
not respond to power (power absorbed at the input), but to the
input voltage. The use of dBV, defined as decibels with respect
to a 1 V rms sine wave, is more precise. However, this is still
ambiguous, because waveform is also involved in the response
of a log amp, which, for a complex input such as a CDMA
signal, does not follow the rms value exactly. Because most
users specify RF signals in terms of power (more specifically, in
dBm/50 Ω) both dBV and dBm are used to specify the perform-
ance of the AD8310, showing equivalent dBm levels for the
special case of a 50 Ω environment. Values in dBV are
converted to dBm re 50 Ω by adding 13 dB.
Table 4. Correction for Signals with Differing Crest Factors
Signal Type Correction Factor
1
(dB)
Sine wave 0
Square wave or dc −3.01
Triangular wave 0.9
GSM channel (all time slots on) 0.55
CDMA channel (forward link, nine
channels on)
3.55
CDMA channel (reverse link) 0.5
PDC channel (all time slots on) 0.58
1
Add to the measured input level.
INPUT MATCHING
Where higher sensitivity is required, an input matching network
is useful. Using a transformer to achieve the impedance trans-
formation also eliminates the need for coupling capacitors,
lowers the offset voltage generated directly at the input, and
balances the drive amplitude to INLO and INHI.
The choice of turns ratio depends 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
lowers the input impedance to 50 Ω, while raising the input
voltage lowers the effect of the short-circuit noise voltage by the
same factor. The intercept is also lowered by the turns ratio; for
a 50 Ω match, it is reduced by 20 log
10
(4.8) or 13.6 dB. The total
noise is reduced by a somewhat smaller factor, because there is a
small contribution from the input noise current.
AD8310
Rev. F | Page 16 of 24
FREQUENCY (MHz)
14
4
–1
60 15080
DECIBELS
100 110 130
3
2
1
0
70 90 120 140
NARROW-BAND MATCHING
Transformer coupling is useful in broadband applications.
However, a magnetically coupled transformer might not be
convenient in some situations. Table 5 lists narrow-band
matching values.
GAIN
Table 5. Narrow-Band Matching Values
f
C
(MHz)
Z
IN
(Ω)
C1
(pF)
C2
(pF)
L
M
(nH)
Voltage 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 13 270 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
INPUT
9
8
7
6
5
13
12
11
10
01084-032
At high frequencies, it is often preferable to use a narrow-band
matching network, as shown in Figure 31. This has several advan-
tages. The same voltage gain is achieved, providing increased
sensitivity, but a measure of selectivity is also introduced. The
component count is low: two capacitors and an inexpensive chip
inductor. Additionally, by making these capacitors unequal, the
amplitudes at INP and INM can be equalized when driving from
a single-sided source; that is, the network also serves as a balun.
Figure 32 shows the response for a center frequency of 100 MHz;
note the very high attenuation at low frequencies. The high fre-
quency attenuation is due to the input capacitance of the log amp.
C1
C2
INLO
INHI
AD8310
SIGNAL
INPUT
L
M
8
01084-031
1
Figure 31. Reactive Matching Network
Figure 32. Response of 100 MHz Matching Network
GENERAL MATCHING PROCEDURE
For other center frequencies and source impedances, the
following steps can be used to calculate the basic matching
parameters.
Step 1: Tune Out C
IN
At a center frequency, f
C
, the shunt impedance of the input
capacitance, C
IN
, can be made to disappear by resonating with
a temporary inductor, L
IN
, whose value is given by
IN
IN
C
L
2
1
ω
= (5)
where C
IN
= 1.4 pF. For example, at f
C
= 100 MHz, L
IN
= 1.8 μH.
Step 2: Calculate C
O
and L
O
Now, having a purely resistive input impedance, calculate the
nominal coupling elements, C
O
and L
O
, using
()
C
MIN
O
MIN
C
O
f
RR
L
RRf
C
π
=
π
=
2
;
2
1
(6)
For the AD8310, R
IN
is 1 kΩ. Therefore, if a match to 50 Ω is
needed, at f
C
= 100 MHz, C
O
must be 7.12 pF and L
O
must be
356 nH.
Step 3: Split C
O
into Two Parts
To provide the desired fully balanced form of the network
shown in Figure 31, two capacitors C1 and C2, each of
nominally twice C
O
, can be used. This requires a value of
14.24 pF in this example. Under these conditions, the voltage
amplitudes at INHI and INLO are similar. A somewhat better
balance in the two drives can be achieved when C1 is made
slightly larger than C2, which also allows a wider range of
choices in selecting from standard values.
For example, capacitors of C1 = 15 pF and C2 = 13 pF can be
used, making C
O
= 6.96 pF.
AD8310
Rev. F | Page 17 of 24
()
+V
S
(2.7V–5.5V)
Step 4: Calculate L
M
The matching inductor required to provide both L
IN
and L
O
is
the parallel combination of these.
O
IN
O
IN
M
LL
LL
L
+
=
(7)
With L
IN
= 1.8 μH and L
O
= 356 nH, the value of L
M
to complete
this example of a match of 50 Ω at 100 MHz is 297.2 nH.
The nearest standard value of 270 nH can be used with only a
slight loss of matching accuracy. The voltage gain at resonance
depends only on the ratio of impedances, as given by
=
=
S
IN
S
IN
R
R
R
R
GAIN log10log20 (8)
SLOPE AND INTERCEPT ADJUSTMENTS
Where system (that is, software) calibration is not available, the
adjustments shown in Figure 33 can be used, either singly or in
combination, to trim the absolute accuracy of the AD8310.
The log slope can be raised or lowered by VR1; the values
shown provide a calibration range of ±10% (22.6 mV/dB to
27.4 mV/dB), which includes full allowance for the variability in
the value of the internal resistances. The adjustment can be
made by alternately applying two fixed input levels, provided by
an accurate signal generator, spaced over the central portion of
the dynamic range, for example, −60 dBV and −20 dBV.
Alternatively, an AM-modulated signal at about the center of
the dynamic range can 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
M
M
+
+
=Δ
1
1
log20dB
10
(9)
For example, using a generator output of −40 dBm with a 70%
modulation depth (M = 0.7), the decibel range is 15 dB, because
the signal varies from −47.5 dBm to −32.5 dBm.
The log intercept is adjustable by VR2 over a −3 dB range with
the component values shown. VR2 is adjusted while applying
an accurately known CW signal, preferably near the lower end
of the dynamic range, 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 can be applied, and VR2
can be adjusted to produce a dc output of 15 dB above 0 at
24 mV/dB, which is 360 mV.
0.01μF
4.7Ω
52.3Ω
NC = NO CONNECT
C1
0.01μF
NC
INHI ENBL BFIN VPOS
INLO COMM OFLT VOUT
AD8310
V
OUT
(RSSI)
SIGNAL
INPUT
10kΩ
C2
0.01μF
25kΩ
VR1
10kΩ
R
S
VR2
100kΩ
FOR V
POS
= 3V, R
S
= 500kΩ
FOR V
POS
= 5V, R
S
= 850kΩ
24mV/dB ±10%
1234
8765
01084-033
Figure 33. Slope and Intercept Adjustments
INCREASING THE SLOPE TO A FIXED VALUE
It is also possible to increase the slope to a new fixed value and,
therefore, to increase the change in output for each decibel of
input change. A common example of this is the need to map the
output swing of the AD8310 into the input range of an analog-
to-digital converter (ADC) with a rail-to-rail input swing.
Alternatively, a situation might arise when only a part of the
total dynamic range is required (for example, just 20 dB) in an
application where the nominal input level is more tightly
constrained, and a higher sensitivity to a change in this level is
required. Of course, the maximum output is limited by either
the load resistance and the maximum output current rating of
25 mA or by the supply voltage (see the Specifications section).
The slope can easily be raised by adding a resistor from VOUT
to BFIN, as shown in Figure 34. This alters the gain of the
output buffer, by means of stable positive feedback, from its
normal value of 4 to an effective value that can be as high as 16,
corresponding to a slope of 100 mV/dB.
V
S
(2.7V–5.5V)
0.01μF
4.7Ω
52.3Ω
NC = NO CONNECT
C1
0.01μF
NC
INHI ENBL BFIN VPOS
INLO COMM OFLT VOUT
AD8310
V
OUT
100mV/dB
SIGNAL
INPUT
C2
0.01μF
8765
R
SLOPE
12.1kΩ
1234
01084-034
Figure 34. Raising the Slope to 100 mV/dB
The resistor, R
SLOPE
, is set according to the equation
Slope
R
SLOPE
mV/dB24
1
k22.9 Ω
= (10)

AD8310ARMZ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Logarithmic Amplifiers V-Out DC to 440 MHz 95dB
Lifecycle:
New from this manufacturer.
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