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ADA4350ARUZ-R7 Scheda tecnica(PDF) 28 Page - Analog Devices

Il numero della parte ADA4350ARUZ-R7
Spiegazioni elettronici  FET Input Analog Front End with ADC Driver
PDF  38 Pages
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Produttore elettronici  AD [Analog Devices]
Homepage  http://www.analog.com
Logo AD - Analog Devices

ADA4350ARUZ-R7 Scheda tecnica(HTML) 28 Page - Analog Devices

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Data Sheet
ADA4350
Rev. B | Page 27 of 37
THEORY OF OPERATION
KELVIN SWITCHING TECHNIQUES
Traditional gain selectable amplifiers use analog switches in a
feedback loop to connect discrete external resistors and capacitors
to the inverting input by selecting the appropriate feedback
path. This approach introduces several errors due to the nonideal
nature of the analog switches in the loop. For example, the
on-resistance of the analog switch causes voltage and temperature
dependent gain errors, while the leakage current causes offset
errors, especially at high temperature. The Kelvin switching
technique solves this problem by introducing two switches in
each gain selection loop, one to connect the transimpedance/
op amp output to the feedback network, and the other to connect
the feedback network output to the downstream components.
Figure 54 shows a programmable gain transimpedance amplifier
with Kelvin switching.
VOUT
V1
V2
S2B
HIGH IMPEDANCE LOAD
EXAMPLE
S1B
S2A
S1A
CF1
RF1
RL
CF2
RF2
IPHOTO
NOTES
1. S1A, S1B, S2A, AND S2B ARE THE ANALOG SWITCHES.
RFx ARE THE FEEDBACK RESISTORS SPECIFIC TO EACH
TRANSIMPEDANCE PATH. CFx ARE THE FEEDBACK CAPACITORS
SPECIFIC TO EACH TRANSIMPEDANCE PATH.
Figure 54. Programmable Gain Transimpedance Amplifier with Kelvin
Switching
Although this technique requires using twice as many switches,
the voltage (Vx) in the center node is no longer switch dependent;
it is only dependent on the current across the selected resistor
(see Equation 1 through Equation 3).
VOUT = −IPHOTO × (RF2 + RS1B)
(1)
V1 = VOUT × (RF2/(RF2 + RS1B))
(2)
Substituting Equation 1 into Equation 2,
V1 = −IPHOTO × RF2
(3)
where:
VOUT is the output of the first amplifier.
IPHOTO is the current from the photodiode.
RF2 is the feedback resistor of Transimpedance Path 2.
RS1B is the switch resistance of the S1B switch.
The switches shown on the right (S2A and S2B) in Figure 54
only have a small output impedance and contribute negligible
error if the amplifier drives a high impedance load. In the case
of the ADA4350, the high impedance load is the integrated
ADC driver.



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