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MPY100B Datasheet(PDF) 7 Page - Burr-Brown (TI) |
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MPY100B Datasheet(HTML) 7 Page - Burr-Brown (TI) |
7 / 12 page ® 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 |
Similar Part No. - MPY100B |
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Similar Description - MPY100B |
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