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ADL5903SCPZN-R7 数据表(PDF) 15 Page - Analog Devices |
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ADL5903SCPZN-R7 数据表(HTML) 15 Page - Analog Devices |
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15 / 20 page ![]() Data Sheet ADL5903 Rev. B | Page 15 of 20 THEORY OF OPERATION The ADL5903 is a true rms detector with a 35 dB measurement range at 2.14 GHz with useable range up to 6 GHz. It features no error ripple over its range, low temperature drift, and very low power consumption. Temperature stability of the rms output measurements provides ≤±0.5 dB error typical over the temperature range of −40°C to +85°C up to 3.5 GHz. The measurement output voltage scales linearly in decibels with a slope of approximately 36 mV/dB. The ADL5903 operates from a nominal supply voltage of 3.0 V to 5.0 V. The rms core is internally regulated to 3.6 V, that is, the full measurement range is available for supply voltages between 3.8 V and 5.0 V. Below 3.8 V, the high end of the measurement range degrades gradually whereas the low end shows no noticeable change in error characteristics or calibration requirements. At 2.14 GHz, the measurement range extends to 14 dBm for 3.8 V and above, and to 12 dBm at a supply voltage of 3.0 V. The low end of the ADL5903 measurement range is limited by internal device offsets that vary from device to device but tracks well over temperature. See the Device Calibration and Error Calculation section for more information. The core rms processing of the ADL5903 uses a proprietary technique that provides accuracy for complex modulation signals irrespective of the crest factor of the input signal. An integrating filter capacitor at Pin CRMS performs the square domain averaging. An RF input matching network allows the device to be driven with a 50 Ω source with reasonable input return loss. The measurement intercept varies with frequency, as shown in Table 1 and the Typical Performance Characteristics section. Figure 39. Simplified Architecture RF INPUT INTERFACE A single-ended input at the RFIN pin drives the ADL5903, and a 50 Ω source can drive it directly without any external components. Figure 40 shows the simplified RF input interface. An on-chip matching network presents 133 Ω of shunt resistance to ground and ac coupling to the rms core. The ESD protection circuitry is designed to allow voltage swings as high as ±2 V at the input. As shown in Figure 12 (input return loss, S11), the device offers excellent input return loss over most of the operating range but rises to around −9 dB near its minimum operating frequency of 200 MHz. Add an external shunt resistance of 127 Ω, if desired, when operating at low frequencies to improve input return loss over the range of 200 MHz to 1.7 GHz. Figure 41 shows a comparison of the input return loss, with and without the external shunt resistor. Figure 40. Simplified RF Input Interface Figure 41. Return Loss with and Without External Shunt Termination BASIC CONNECTIONS The ADL5903 requires a single supply of 3.0 V to 5.0 V. The supply is connected to the VPOS supply pin. This pin is decoupled using two capacitors with values equal or similar to those shown in Figure 44. Place these capacitors as near the VPOS pin as possible. The CREG pin provides a bypass capacitor connection for an on-chip regulator. The CREG pin is connected to ground with a 4.02 Ω resistor and a 0.1 μF capacitor. The CRMS pin provides an averaging function for the rms computation and is referenced to Pin 4 (CREG). A filter capacitor can be placed between the CRMS and CREG pins. More information on choosing the CRMS capacitor is provided in the Choosing a Value for CRMS section. Using smaller values for CRMS allows quicker response times to a pulsed waveform. Higher values of CRMS are required for correct rms computation as the peak to average ratio of modulated signals increases and the bandwidth of the modulated signals decreases. 5 1 6 ADL5903 RFIN ENBL RMS CORE INTERNAL FILTERING BUFFER 630pF 1kΩ 100Ω 4pF VPOS 2 GND 8 NIC EP 4 CREG 3 CRMS 7 VRMS VPOS MATCHING NETWORK GND 133Ω 4pF OPTIONAL 127Ω –25 –20 –15 –10 –5 0 012 345 6 FREQUENCY (GHz) EXTERNAL 127Ω SHUNT TERM NO SHUNT TERM |
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