AD8304ARU Analog Devices Inc, AD8304ARU Datasheet - Page 12

Logarithmic Amplifier IC

AD8304ARU

Manufacturer Part Number
AD8304ARU
Description
Logarithmic Amplifier IC
Manufacturer
Analog Devices Inc
Type
Logarithmic Converterr
Datasheet

Specifications of AD8304ARU

No. Of Amplifiers
1
No. Of Pins
14
Operating Temperature Range
-40°C To +85°C
Slew Rate
15V/µs
Peak Reflow Compatible (260 C)
No
Input Bias Current
400nA
Supply Voltage
5.5V
Bandwidth
10MHz
Rohs Status
RoHS non-compliant
Design Resources
Interfacing ADL5315 to Translinear Logarithmic Amplifier (CN0056) Interfacing ADL5317 High Side Current Mirror to a Translinear Logarithmic Amplifier in an Avalanche Photodiode Power Detector
Applications
Fiber Optics
Mounting Type
Surface Mount
Package / Case
14-TSSOP
Lead Free Status / RoHS Status
Contains lead / RoHS non-compliant

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AD8304
Low Supply Slope and Intercept Adjustment
When using the device with a positive supply less than 4 V, it is
necessary to reduce the slope and intercept at the VLOG Pin in
order to preserve good log conformance over the entire 160 dB
operating range. The voltage at the VLOG Pin is generated by
an internal current source with an output current of 40 µA/decade
feeding the internal laser-trimmed output resistance of 5 kΩ. When
the voltage at the VLOG Pin exceeds V
source ceases to respond linearly to logarithmic increases in current.
This headroom issue can be avoided by reducing the logarithmic
slope and intercept at the VLOG Pin. This is accomplished by
connecting an external resistor R
in combination with an intercept lowering resistor R
shown in Figure 6 illustrate a good solution for a 3.0 V positive
supply. The resulting logarithmic slope measured at VLOG is
62.5 mV/decade with a new intercept of 57 fA. The original
logarithmic slope of 200 mV/decade can be recovered using voltage
gain on the internal buffer amplifier.
NC = NO CONNECT
Figure 6. Recommended Low Supply Application Circuit
NC = NO CONNECT
R1
750
C1
1nF
10nF
R1
750
C1
1nF
I
10nF
PD
I
PD
NC
NC
Figure 5. Method for Raising the Intercept
6
3
4
5
6
3
4
5
VPDB
VSUM
VSUM
INPT
VPDB
VSUM
VSUM
INPT
VNEG
VNEG
VPS2
VPS2
1
1
PDB
PDB
10
10
PWDN
~10k
PWDN
~10k
ACOM
COMPENSATION
TEMPERATURE
BIAS
ACOM
COMPENSATION
BIAS
TEMPERATURE
2
2
S
14
from the VLOG Pin to ground
14
VPS1
0.5V
VPS1
0.5V
P
– 2.3 V, the current
VREF
VOUT
VREF
VOUT
12
5k
12
5k
11
11
BFNG
VLOG
VREF
BFNG
BFIN
BFIN
Z
. The values
13
7
8
9
V
13
7
8
9
V
P
62.5mV/DEC
VREF
P
VLOG
RA
4.98k
RZ
15.4k
2.67k
RA
RS
V
V
OUT
OUT
RC
RB
RB
2.26k
–12–
Using the Adaptive Bias
For most photodiode applications, the placement of the anode
somewhat above ground is acceptable, as long as the positive
bias on the cathode is adequate to support the peak current for a
particular diode, limited mainly by its series resistance. To address
this matter, the AD8304 provides for the diode a bias that varies
linearly with the current. This voltage appears at Pin VPDB, and
varies from 0.6 V (reverse-biasing the diode by 0.1 V) for I
100 pA and rises to 2.6 V (for a diode bias of 1 V) at I
This results in a constant internal junction bias of 0.1 V when the
series resistance of the photodiode is 200 Ω. For optical power
measurements over a wide dynamic range the adaptive biasing
function will be valuable in minimizing dark current while pre-
venting the loss of photodiode bias at high currents. Use of the
adaptive bias feature is shown in Figure 7.
Capacitor CPB, between the photodiode cathode at Pin VPDB
and ground, is included to lower the impedance at this node and
thereby improve the high frequency accuracy at those current
levels where the AD8304 bandwidth is high. It also ensures an
HF path for any high frequency modulation on the optical signal
which might not otherwise be accurately averaged. It will not be
necessary in all cases, and experimentation may be required to find
an optimum value.
Changing the Voltage at the Summing Node
The default value of VSUM is determined by using a quarter of
VREF (2 V). This may be altered by applying an independent volt-
age source to VSUM, or by adding an external resistive divider
from VREF to VSUM. This network will operate in parallel with
the internal divider (40 kΩ and 13.3 kΩ), and the choice of external
resistors should take this into account. In practice, the total
resistance of the added string may be as low as 10 kΩ (consuming
400 µA from VREF). Low values of VSUM and thus V
Figure 13) are not advised when large values of I
Implementing Low-Pass Filters
Noise, leading to uncertainty in an observed value, is inherent to
all measurement systems. Translinear log amps exhibit significant
amounts of noise for reasons stated above, and are more trouble-
some at low current levels. The standard way of addressing this
problem is to average the measurement over an appropriate time
interval. This can be achieved in the digital domain, in post-ADC
DSP, or in analog form using a variety of low-pass structures.
R1
750
C1
1nF
CPB
10nF
I
PD
VPDB
6
3
4
5
VSUM
VSUM
INPT
Figure 7. Using the Adaptive Biasing
VNEG
VPS2
1
PDB
10
PWDN
~10k
ACOM
COMPENSATION
TEMPERATURE
BIAS
2
14
0.5V
VPS1
VREF
VOUT
12
5k
11
PD
VLOG
BFNG
BFIN
are expected.
PD
13
9
7
8
V
= 10 mA.
P
VREF
CE
REV. A
RA
(see
CFILT
PD
RB
V
OUT
=

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