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AD8307 データシート(PDF) 9 Page - Analog Devices |
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AD8307 データシート(HTML) 9 Page - Analog Devices |
9 / 24 page AD8307 Rev. D | Page 9 of 24 LOG AMP THEORY Logarithmic amplifiers perform a more complex operation than that of classical linear amplifiers, and their circuitry is significantly different. A good grasp of what log amps do and how they work can prevent many pitfalls in their application. The essential purpose of a log amp is not to amplify, though amplification is utilized to achieve the function. Rather, it is to compress a signal of wide dynamic range to its decibel equivalent. It is thus a measurement device. A better term may be logarithmic converter, because its basic function is the conversion of a signal from one domain of representation to another via a precise nonlinear transformation. Logarithmic compression leads to situations that can be confusing or paradoxical. For example, a voltage offset added to the output of a log amp is equivalent to a gain increase ahead of its input. In the usual case where all the variables are voltages, and regardless of the particular structure, the relationship between the variables can be expressed as ) / ( log X IN Y OUT V V V V = (1) where: VOUT is the output voltage. VY is the slope voltage; the logarithm is usually taken to base 10 (in which case VY is also the volts per decade). VIN is the input voltage. VX is the intercept voltage. All log amps implicitly require two references, in this example, VX and VY, which determine the scaling of the circuit. The abso- lute accuracy of a log amp cannot be any better than the accuracy of its scaling references. Equation 1 is mathematically incomplete in representing the behavior of a demodulating log amp, such as the AD8307, where VIN has an alternating sign. However, the basic principles are unaffected, and this can be safely used as the starting point in the analyses of log amp scaling. VOUT 5VY 4VY 3VY 2VY –2VY VY VOUT = 0 VSHIFT LOWER INTERCEPT VIN = VX 0dBc VIN = 102VX +40dBc VIN = 104VX +80dBc LOG VIN VIN = 10–2VX –40dBc Figure 21. Ideal Log Amp Function Figure 21 shows the input/output relationship of an ideal log amp, conforming to Equation 1. The horizontal scale is logarithmic and spans a wide dynamic range, shown in Figure 21 as over 120 dB, or six decades. The output passes through zero (the log intercept) at the unique value VIN = VX and ideally becomes negative for inputs below the intercept. In the ideal case, the straight line describing VOUT for all values of VIN continues indefinitely in both directions. The dotted line shows that the effect of adding an offset voltage, VSHIFT, to the output is to lower the effective intercept voltage, VX. Exactly the same alteration can be achieved by raising the gain (or signal level) ahead of the log amp by the factor, VSHIFT/VY. For example, if VY is 500 mV per decade (25 mV/dB), an offset of 150 mV added to the output appears to lower the intercept by two-tenths of a decade, or 6 dB. Adding an offset to the output is thus indistinguishable from applying an input level that is 6 dB higher. The log amp function described by Equation 1 differs from that of a linear amplifier in that the incremental gain δVOUT/δVIN is a very strong function of the instantaneous value of VIN, as is apparent by calculating the derivative. For the case where the logarithmic base is δ, IN Y IN OUT V V V V = δ δ (2) That is, the incremental gain is inversely proportional to the instantaneous value of the input voltage. This remains true for any logarithmic base, which is chosen as 10 for all decibel related purposes. It follows that a perfect log amp is required to have infinite gain under classical small signal (zero amplitude) conditions. Less ideally, this result indicates that whatever means are used to implement a log amp, accurate response under small signal conditions (that is, at the lower end of the dynamic range) demands the provision of a very high gain bandwidth product. A further consequence of this high gain is that in the absence of an input signal, even very small amounts of thermal noise at the input of a log amp cause a finite output for zero input. This results in the response line curving away from the ideal shown in Figure 21 toward a finite baseline, which can be either above or below the intercept. Note that the value given for this intercept can be an extrapolated value, in which case the output cannot cross zero, or even reach it, as is the case for the AD8307. While Equation 1 is fundamentally correct, a simpler formula is appropriate for specifying the calibration attributes of a log amp like the AD8307, which demodulates a sine wave input. VOUT = VSLOPE (PIN – P0) (3) where: VOUT is the demodulated and filtered baseband (video or RSSI) output. VSLOPE is the logarithmic slope, now expressed in V/dB (typically between 15 mV/dB and 30 mV/dB). PIN is the input power, expressed in decibels relative to some reference power level. P0 is the logarithmic intercept, expressed in decibels relative to the same reference level. The most widely used reference in RF systems is decibels above 1 mW in 50 Ω, written dBm. Note that the quantity (PIN – P0) is |
同様の部品番号 - AD8307_15 |
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同様の説明 - AD8307_15 |
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