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MPY100B Datasheet(PDF) 7 Page - Burr-Brown (TI)

[Old version datasheet] Texas Instruments acquired Burr-Brown Corporation.
Part # MPY100B
Description  MULTIPLIER-DIVIDER
Download  12 Pages
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Manufacturer  BURR-BROWN [Burr-Brown (TI)]
Direct Link  http://www.burr-brown.com
Logo BURR-BROWN - Burr-Brown (TI)

MPY100B Datasheet(HTML) 7 Page - Burr-Brown (TI)

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®
MPY100
7
FIGURE 1. MPY100 Functional Block Diagram.
(X
1 – X2)(Y1 – Y2)
10
Attenuator
Z
2
Z
1
Multiplier
Core
Y
2
Y
1
X
2
X
1
V-I
V-I
V-I
A
Out
High Gain
Output Amplifier
Stable
Reference
and Bias
+V
S
–V
S
V
O = A
– (Z
1 – Z2)
Transfer Function
and is modulated by the voltage, V2, to give
gm ≈ V2/VTRE
Substituting this into the original equation yields the overall
transfer function
VO = gmRLV1 = V1V2 (RL/VTRE)
which shows the output voltage to be the product of the two
input voltages, V1 and V2.
Variations in IE due to V2 cause a large common-mode
voltage swing in the circuit. The errors associated with this
common-mode voltage can be eliminated by using two
differential stages in parallel and cross-coupling their out-
puts as shown in Figure 3.
FIGURE 3. Cross-Coupled Differential Stages as a Variable-
Transconductance Multiplier.
FIGURE 2. Basic Differential Stage as a Transconductance
Multiplier.
–+
V
O
+V
CC
R
L
R
L
I
1
I
2
R
E
I
E
+
V
2
Q
3
Q
2
Q
1
+
V
1
THEORY OF OPERATION
The MPY100 is a variable transconductance multiplier con-
sisting of three differential voltage-to-current converters, a
multiplier core and an output differential amplifier as illus-
trated in Figure 1.
The basic principle of the transconductance multiplier can
be demonstrated by the differential stage in Figure 2.
For small values of the input voltage, V1, that are much
smaller than VT, the transistor’s thermal voltage, the differ-
ential output voltage, VO, is:
VO = gm RLV1
The transconductance gm of the stage is given by:
gm = IE/VT
An analysis of the circuit in Figure 3 shows it to have the
same overall transfer function as before:
VO = V1V2 (RL/VTRE).
For input voltages larger than VT, the voltage-to-current
transfer characteristics of the differential pair Q1, Q2 or Q3
and Q4 are no longer linear. Instead, their collector currents
are related to the applied voltage V1
=
= e
The resultant nonlinearity can be overcome by developing
V1 logarithmically to exactly cancel the exponential rela-
tionship just derived. This is done by diodes D1 and D2 in
Figure 4.
The emitter degeneration resistors, RX and RY, in Figure 4,
provide a linear conversion of the input voltages to differen-
tial current, IX and IY, where:
I
3
I
4
I
1
I
2
V
T
V
1
+
V
O
+V
S
R
L
+
V
2
Q
5
Q
2
Q
1
+
V
1
Q
4
Q
3
I
3
I
1
I
2
I
4
R
E
R
E
Q
6
I
T
–V
CC
R
L


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