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EVALAD5933EB Datasheet(PDF) 23 Page - Analog Devices |
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EVALAD5933EB Datasheet(HTML) 23 Page - Analog Devices |
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23 / 32 page ![]() Preliminary Technical Data EVAL-AD5933EB Rev. PrC | Page 23 of 32 effect on the AD5933 calibration (that is, the gain factor calculation) and subsequent impedance readings in comparison with those obtained by connecting the small impedance directly to the VOUT pin (and directly in series with ROUT). The external amplifier buffers the unknown impedance from the effects of the output series resistance of the AD5933 (ROUT) and introduces a smaller output impedance in series with the impedance being tested (ZUNKNOWN). I-V PGA VDD/2 DDS ROUT VOUT R2 VIN RFB RFB VDD VDD/2 1µF 20kΩ 20kΩ ZUNKNOWN AD8531 AD820 AD8641 AD8627 R1 2V p-p TRANSMIT SIDE OUTPUT AMPLIFIER Figure 28. Additional External Amplifier Circuit for Measuring Small Impedances For example, a user might want to measure an impedance, ZUNKNOWN, that is known to have a value within the range of 90 Ω to 110 Ω (that is, a small impedance) over the frequency range of 30 kHz to 32 kHz. In this case, the user may not be able to characterize the output series resistance (ROUT) directly in the factory/lab. Therefore, the user may choose to add an extra amplifier circuit as shown in Figure 28 to the signal path of the AD5933. The user must ensure that the chosen external amplifier has a sufficiently low output series resistance over the bandwidth of interest in comparison with the impedance range being tested (visit www.analog.com/opamps for an op amp selection guide). The data sheets of most Analog Devices amplifiers show the closed loop output impedance vs. frequency at different amplifier gains to provide an idea of the effect on output series impedance. The system settings are as follows: VDD = 3.3 V VOUT = 2 V p-p R2 = 20 kΩ R1 = 4 kΩ Gain setting resistor = 500 Ω ZUNKNOWN = 100 Ω PGA setting = ×1 Choose a ratio of R1/R2 to attenuate the excitation voltage at VOUT. With the values of R1 = 4 kΩ and R2 = 20 kΩ, the signal is attenu- ated by 1⁄5 (1/5 of 2 V p-p = 400 mV). The maximum current flowing through the impedance will be 400 mV/90 Ω = 4.4 mA. The system is subsequently calibrated at a midpoint frequency in the sweep using the usual method with a midpoint impedance value of 100 Ω for the calibration resistor and feedback resistor. Increasing the value of the I-V gain resistor at the RFB pin improves the dynamic range of the input signal to the receive side of the AD5933. For example, by increasing the I-V gain setting resistor at the RFB pin, the peak-to-peak signal presented to the ADC input increases from 400 mV (Rfb = 100 Ω) to 2 V p-p (Rfb = 500 Ω). The gain factor calculated is for a 100 Ω resistor connected between VOUT and VIN, assuming the output series resistance of the external amplifier is small enough to be ignored. One final important point to note about the biasing of the circuit shown in Figure 28 is that the receive side of the AD5933 is hard biased about VDD/2 by design. Therefore, to prevent the output of the external amplifier (attenuated AD5933 range 1 excitation signal) from saturating the receive side amplifiers of the AD5933, a voltage equal to VDD/2 must be applied to the noninverting terminal of the external amplifier. Measuring Lower Excitation Frequencies The AD5933 has a flexible internal direct digital synthesizer (DDS) core and DAC, which together generate the excitation signal used to measure the impedance (ZUNKNOWN). The DDS core has a 27-bit phase accumulator, allowing subhertz (<0.1 Hz) frequency resolution. The output of the phase accumulator is connected to the input of a read only memory (ROM). The digital output of the phase accumulator is used to address individual memory locations in the ROM. The digital contents of the ROM represent amplitude samples of a single cycle of a sinusoidal excitation waveform. The content of each address within the ROM look-up table are in turn passed to the input of a digital-to-analog converter (DAC) that produces the analog excitation waveform made available at the VOUT pin. The DDS core (that is, the phase accumulator and the ROM look-up table) and the DAC are referenced from a single system clock. The function of the phase accumulator is to act as a system clock divider. The system clock for the AD5933 DDS engine can be provided in one of two ways. • Use a highly accurate and stable clock (crystal oscillator) at the external clock pin (MCLK, Pin 8). • Use the AD5933 internal clock oscillator with a typical frequency of 16.776 MHz. (The internal oscillator is not available in the AD5934; therefore, the user must apply a clock to the external clock pin (MCLK).) Select the preferred system clock by programming Bit D3 in the CONTROL register (Address 81 hex; see AD5933 data sheet). The system clock is also used by the internal ADC to digitize the response signal. The ADC requires 16 clock periods to perform a single conversion. Therefore, with a maximum |
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