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AD5280 Datasheet(PDF) 23 Page - Analog Devices |
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AD5280 Datasheet(HTML) 23 Page - Analog Devices |
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23 / 28 page ![]() AD5280/AD5282 Rev. C | Page 23 of 28 PROGRAMMABLE LOW-PASS FILTER At resonance, setting the following balances the bridge: In analog-to-digital conversion applications, it is common to include an antialiasing filter to band-limit the sampling signal. Dual-channel digital potentiometers can be used to construct a second-order Sallen key low-pass filter (see Figure 63). The design equations are 2 2 O O V ω = 2 O O i S Q S V ω + ω + (11) R1R2C1C2 O 1 = ω (12) R2C2 R1C1 Q 1 1 + = (13) Users can first select some convenient values for the capacitors. To achieve maximally flat bandwidth where Q = 0.707, let C1 be twice the size of C2 and let R1 = R2. As a result, R1 and R2 can be adjusted to the same settings to achieve the desirable bandwidth. VI U1 VO R1 A R W B R2 A R W B C2 C C1 C +2.5V V+ V– –2.5V AD8601 ADJUSTED TO SAME SETTING Figure 63. Sallen Key Low-Pass Filter PROGRAMMABLE OSCILLATOR In a classic Wien-bridge oscillator (Figure 64), the Wien network (R, R', C, C') provides positive feedback, while R1 and R2 provide negative feedback. At the resonant frequency, fO, the overall phase shift is 0, and the positive feedback causes the circuit to oscillate. With R = R', C = C', and R2 = R2A//(R2B + Rdiode), the oscillation frequency is RC f or RC o O π ω 1 1 = = 2 (14) where R is equal to RWA such that AB R D R 256 256 = − (15) 2 = R1 R2 (16) In practice, R2/R1 should be set slightly larger than 2 to ensure that oscillation can start. On the other hand, the alternate turn- on of Diode D1 and Diode D2 ensures that R2/R1 are smaller than 2 momentarily and, therefore, stabilizes the oscillation. Once the frequency is set, the oscillation amplitude can be tuned by R2B because D B D O V R2 I V + = 3 2 (17) VO, ID, and VD are interdependent variables. With proper selection of R2B, an equilibrium is reached such that VO converges. R2B can be in series with a discrete resistor to increase the amplitude, but the total resistance cannot be too large to prevent saturation of the output. FREQUENCY ADJUSTMENT C 2.2nF CI 2.2nF RI 10kΩ R 10kΩ BA A W V+ V– B B W W D1 D2 VO U1 VP A VN –2.5V +2.5V R1 1kΩ R2B 10kΩ R2A 2.1kΩ R1 = R1I = R2B = AD5282 D1 = D2 = 1N4148 AMPLITUDE ADJUSTMENT OP1177 Figure 64. Programmable Oscillator with Amplitude Control |
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