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AD8137YCP-R2 数据表(PDF) 19 Page - Analog Devices |
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AD8137YCP-R2 数据表(HTML) 19 Page - Analog Devices |
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19 / 24 page ![]() AD8137 Rev. B | Page 19 of 24 The differential output voltage noise contains contributions from the AD8137’s input voltage noise and input current noise as well as those from the external feedback networks. The contribution from the input voltage noise spectral density is computed as ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ + = G F n R R v Vo_n 1 1 , or equivalently, vn/β (7) where vn is defined as the input-referred differential voltage noise. This equation is the same as that of traditional op amps. The contribution from the input current noise of each input is computed as ( ) F n R i Vo_n = 2 (8) where in is defined as the input noise current of one input. Each input needs to be treated separately since the two input currents are statistically independent processes. The contribution from each RG is computed as ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ = G F G R R TR Vo_n k 4 3 (9) This result can be intuitively viewed as the thermal noise of each RG multiplied by the magnitude of the differential gain. The contribution from each RF is computed as F TR Vo_n k 4 4 = (10) Voltage Gain The behavior of the node voltages of the single-ended-to- differential output topology can be deduced from the signal definitions and Figure 63. Referring to Figure 63, (CF = 0) and setting VIN = 0 one can write: F ON AP G AP IP R V V R V V − = − (11) ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + = = G F G OP AP AN R R R V V V (12) Solving the above two equations and setting VIP to Vi gives the gain relationship for VO, dm/Vi. i G F dm O, ON OP V R R V V V = = − (13) An inverting configuration with the same gain magnitude can be implemented by simply applying the input signal to VIN and setting VIP = 0. For a balanced differential input, the gain from VIN, dm to VO, dm is also equal to RF/RG, where VIN, dm = VIP − VIN. Feedback Factor Notation When working with differential drivers, it is convenient to introduce the feedback factor β, which is defined as G F G R R R + ≡ β (14) This notation is consistent with conventional feedback analysis and is very useful, particularly when the two feedback loops are not matched. Input Common-Mode Voltage The linear range of the VAN and VAP terminals extends to within approximately 1 V of either supply rail. Since VAN and VAP are essentially equal to each other, they are both equal to the amplifier’s input common-mode voltage. Their range is indicated in the specifications tables as input common-mode range. The voltage at VAN and VAP for the connection diagram in Figure 63 can be expressed as = = = ACM AP AN V V V ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ × + + ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ + × + OCM G F G IN IP G F F V R R R V V R R R 2 ) ( (15) where VACM is the common-mode voltage present at the amplifier input terminals. Using the β notation, Equation (15) can be written as ( ) ICM OCM ACM V V V β − + β = 1 (16) or equivalently, ( ) ICM OCM ICM ACM V V V V − β + = (17) where VICM is the common-mode voltage of the input signal, that is 2 IN IP ICM V V V + ≡ For proper operation, the voltages at VAN and VAP must stay within their respective linear ranges. Calculating Input Impedance The input impedance of the circuit in Figure 63 depends on whether the amplifier is being driven by a single-ended or a differential signal source. For balanced differential input signals, the differential input impedance (RIN, dm) is simply G dm IN, R R 2 = (18) For a single-ended signal (for example, when VIN is grounded, and the input signal drives VIP), the input impedance becomes ) ( 2 1 F G F G IN R R R R R + − = (19) |
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