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MCP6V06T データシート(PDF) 27 Page - Microchip Technology

部品番号 MCP6V06T
部品情報  300 關A, Auto-Zeroed Op Amps
PDF  44 Pages
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メーカー  MICROCHIP [Microchip Technology]
ホームページ  http://www.microchip.com
Logo MICROCHIP - Microchip Technology

MCP6V06T データシート(HTML) 27 Page - Microchip Technology

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© 2008 Microchip Technology Inc.
DS22093B-page 27
MCP6V06/7/8
4.3.9.3
Difference Amplifier Layout for
Thermo-junctions
Figure 4-12 shows the recommended difference ampli-
fier circuit. Usually, we choose R1 =R2 and R3 =R4.
The guard traces (with ground vias at the ends) help
minimize the thermal gradients. The resistor layout
cancels the resistor thermal voltages, assuming the
temperature gradient is constant near the resistors:
EQUATION 4-3:
FIGURE 4-12:
PCB Layout and Schematic
for Single Difference Amplifier.
4.3.9.4
Dual Non-inverting Amplifier Layout
for Thermo-junctions
The dual op amp amplifiers shown in Figure 4-16 and
Figure 4-17 produce a non-inverting difference gain
greater than 1, and a common mode gain of 1 .They
can use the layout shown in Figure 4-13. The gain set-
ting resistors (R2) between the two sides are not com-
bined so that the thermal voltages can be canceled.
The guard traces (with ground vias at the ends) help
minimize the thermal gradients. The resistor layout
cancels the resistor thermal voltages, assuming the
temperature gradient is constant near the resistors:
EQUATION 4-4:
FIGURE 4-13:
PCB Layout and Schematic
for Dual Non-inverting Amplifier.
Note:
Changing the orientation of the resistors
will usually cause a significant decrease in
the cancellation of the thermal voltages.
VOUT ≈ VREF +(VP –VM)GDM
Where:
Thermal voltages are approximately equal
GDM
=R3/R1 =R4/R2, difference gain
VOS is neglected
VOUT ≈ VREF +(VP –VM)GDM
R4
VOUT
R2
VM
U1
MCP6V06
VP
R1
R3
VREF
U1
VM
VOUT
VP
R4
R2
R1
R3
VREF
Note:
Changing the orientation of the resistors
will usually cause a significant decrease in
the cancellation of the thermal voltages.
(VOA –VOB) ≈ (VIA –VIB)GDM
(VOA +VOB)/2 ≈ (VIA +VIB)/2
Where:
Thermal voltages are approximately equal
GDM =1 + R3/R2, differential mode gain
GCM = 1, common mode gain
VOS is neglected
U1
VIB
VOA
VOB
VIA
R1
R2
R3
R1
R2
R3
VIB
VOB
R1
U1
½MCP6V07
VIA
R3
VOA
R1
R2
U1
½MCP6V07
R3
R2



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