ADL5303 Data Sheet
Rev. A | Page 12 of 24
USING THE ADL5303
The default configuration (see Figure 25) includes a 2.5:1 atten-
uator in the feedback path around the buffer. This increases the
slope of 10 mV/dB at the VLOG pin to 25 mV/dB at VOUT.
For the full dynamic range of 160 dB (80 dB optical), the output
swing is 4.0 V, which can be accommodated by the rail-to-rail
output stage when using the recommended 5 V supply.
The capacitor from VLOG to ground forms an optional
single-pole low-pass filter. Because the resistance at this pin
is trimmed to 5 kΩ, an accurate time constant can be realized.
For example, with C
FLT
= 10 nF, the 3 dB corner frequency is
3.2 kHz. Such filtering is useful in minimizing the output noise,
particularly when I
PD
is small. Multipole filters are even more
effective in reducing noise. A capacitor between VSUM and
ground is essential for minimizing the noise on this node.
When the bias voltage at either VPDB or VREF is not needed,
these pins should be left unconnected.
SLOPE AND INTERCEPT ADJUSTMENTS
The choice of slope and intercept depends on the application.
The versatility of the ADL5303 permits optimal choices to
be made in two common situations. First, it allows an input
current range of less than the full 160 dB to use the available
voltage span at the output. Second, it allows this output voltage
range to be optimally positioned to fit the input capacity of a
subsequent ADC. In special applications, very high slopes, such
as 1 V/decade, allow small subranges of I
PD
to be covered at high
sensitivity.
The slope can be lowered without limit by the addition of a
shunt resistor, R
S
, from VLOG to ground. Because the resistance
at this pin is trimmed to 5 kΩ, the accuracy of the modified
slope depends on the external resistor. It is calculated by,
5
+
=
S
S
Y
Y
R
R
V
V
(8)
For example, using R
S
= 3 k, the slope is lowered to 75 mV per
decade or 3.75 mV/dB. Table 4 provides a selection of suitable
values for R
S
and the resulting slopes.
Table 4. Examples of Lowering the Slope
R
S
(kΩ) V
Y
(mV/decade)
3 75
5 100
15 150
In addition to uses in filter and comparator functions, the
buffer amplifier provides the means to adjust both the slope
and intercept, which require a minimal number of external
components. The high input impedance at BFIN, low input
offset voltage, large output swing, and wide bandwidth of this
amplifier permit numerous transformations of the basic V
LOG
signal, using standard op amp circuit practices. For example, it
has been noted that to raise the gain of the buffer, and therefore
the slope, a feedback attenuator, R
A
and R
B
in Figure 25, should
be inserted between VLOG and the inverting input BFNG pin.
NC
V
OUT
500mV/DEC
200mV/DEC
R18 (R
B
)
10k
~10k
R15 (R
A
)
15kΩ
5k
C7 (C
FILT
)
NC
NC = NO CONNECT
V
P
100nF
R1
750
C1
1nF
I
PD
C3
PDB BIAS
VREF
VPDB
VSUM
INPT
VSUM
ACOM
VPS2
PWDN VPS1
VREF
VLOG
BFIN
BFNG
VOUT
0.5V
ADL5303
5
2
3
4
15 14
GND
GND
7 11
10
16
12
6
8
9
13
TEMPERATURE
COMPENSA
TION
10661-025
Figure 25. Basic Connections (R15, R18, C7 are Optional; R1 and C1 are the Default Values)
Data Sheet ADL5303
Rev. A | Page 13 of 24
A wide range of gains may be used and the resistor magnitudes
are not critical; their parallel sum should be about equal to
the net source resistance at the noninverting input. When
high gains are used, the output dynamic range is reduced; for
a maximum swing of 4.8 V, it amounts to 4.8 V/V
Y
decades.
Thus, using a ratio of 3×, to set up a slope 30 mV/dB (600 mV/
decade), eight decades can be handled, whereas with a ratio
of 5×, which sets up a slope of 50 mV/dB (1 V/decade), the
dynamic range is 4.8 decades, or 96 dB. When using a lower
supply voltage, the calculation proceeds in the same way,
remembering to first subtract 0.2 V to allow for 0.1 V upper
and lower headroom in the output swing.
Alteration of the logarithmic intercept is only slightly more
tricky. First, note that it is rarely necessary to lower the intercept
below a value of 100 pA, because this merely raises all output
voltages further above ground. However, where this is required,
the first step is to raise the voltage, V
LOG
, by connecting a
resistor, R
Z
, from VLOG to VREF (2 V) as shown in Figure 26.
This has the effect of elevating, V
LOG
, for small inputs while
lowering the slope to some extent because of the shunt effect
of R
Z
on the 5 kΩ output resistance. If necessary, the slope may
be increased as before, using a feedback attenuator around the
buffer. Table 5 lists some examples of lowering the intercept
combined with several slope variations.
Table 5. Examples of Lowering the Intercept
V
Y
(mV/decade) I
Z
(pA) R
A
(kΩ) R
B
(kΩ) R
Z
(kΩ)
200 1 20.0 100 25
200 10 10.0 100 50
200 50 3.01 100 165
300 1 10.0 12.4 25
300 10 8.06 12.4 50
300 50 6.65 12.4 165
400 1 11.5 8.2 25
400 10 9.76 8.2 50
400
50
8.66
8.2
165
500 1 16.5 8.2 25
500 10 14.3 8.2 50
500 50 13.0 8.2 165
Use the following equation with Table 5:
+
×+
×
+
×=
Z
LOG
LOG
REF
Z
PD
LOG
Z
Z
Y
OUT
RR
R
V
I
I
RR
R
VGV
10
log
(9)
where G = 1 + R
A
/R
B
and R
LOG
= 5 kΩ.
NC
V
OUT
500mV/DEC
R18 (R
B
)
R14 (R
Z
)
R15 (R
A
)
NC = NO CONNECT
V
P
100nF
R1
750
C1
1nF
I
PD
C3
PDB BIAS
VREF
VPDB
VSUM
INPT
VSUM
ACOM
VPS2
PWDN VPS1
VREF
VLOG
BFIN
BFNG
VOUT
0.5V
ADL5303
~10k
5k
5
2
3
4
15 14
GNDGND
7 11
10
16
12
6
8
9
13
TEMPERATURE
COMPENSATION
10661-026
Figure 26. Method for Lowering the Intercept
ADL5303 Data Sheet
Rev. A | Page 14 of 24
Generally, it is useful to raise the intercept. Keep in mind that
this moves the V
LOG
line in Figure 26 to the right, lowering all
output values. Figure 27 shows how raising the intercept is
achieved. The feedback resistors, R
A
and R
B
, around the buffer
are now augmented with a third resistor, R
Z
, placed between the
BFNG and VREF pins. Adding a third resistor raises the zero-
signal voltage on BFNG, which has the effect of pushing V
OUT
lower. Note that the addition of the R
Z
resistor also alters the
feedback ratio. However, this change in feedback ratio is readily
compensated in the design of the network. Table 6 lists the
resistor values for representative intercepts.
Table 6. Examples of Raising the Intercept
V
Y
(mV/decade) I
Z
(nA) R
A
(kΩ) R
B
(kΩ) R
C
(kΩ)
300 10 7.5 37.4 24.9
300 100 8.25 130 18.2
400 10 10 16.5 25.5
400 100 9.76 25.5 16.2
400 500 9.76 36.5 13.3
500 10 12.4 12.4 24.9
500 100 12.4 16.5 16.5
500 500 11.5 20.0 12.4
Use the following equation with Table 6:
+
×
×
=
C
B
A
B
A
REF
Z
PD
Y
OUT
R
R
R
R
R
V
I
I
V
GV
10
log
(10)
where
.and1
B
A
B
A
B
A
C
B
A
RR
RR
RR
RR
R
G
+
×
=+=
NC
V
OUT
500mV/DEC
R15
(R
A
)
R18
(R
B
)
NC = NO CONNECT
V
P
100nF
R1
750
C1
1nF
I
PD
C3
PDB BIAS VREF
VPDB
VSUM
INPT
VSUM
ACOM
VPS2
PWDN VPS1
VREF
VLOG
BFIN
BFNG
VOUT
0.5V
ADL5303
~10k
5k
5
2
3
4
15 14
GNDGND
7 11
10
16
12
6
8
9
13
TEMPERATURE
COMPENSATION
R13
(R
C
)
10661-027
Figure 27. Method for Raising the Intercept

ADL5303ACPZ-RL

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Logarithmic Amplifiers Log Amp
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
T/T Paypal Visa MoneyGram Western Union

Products related to this Datasheet