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AD8362 Datasheet(PDF) 19 Page - Analog Devices |
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AD8362 Datasheet(HTML) 19 Page - Analog Devices |
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19 / 32 page ![]() AD8362 Rev. D | Page 19 of 32 OPERATION IN RF MEASUREMENT MODE BASIC CONNECTIONS Basic connections for operating the AD8362 in measurement mode are shown in Figure 47. While the AD8362 requires a single supply of nominally 5 V, its performance is essentially unaffected by variations of up to ±10%. The supply is connected to the VPOS pin using the decoupling network also displayed in Figure 47. The capacitors used in this network must provide a low impedance over the full frequency range of the input and should be placed as close as possible to the VPOS pin. Two different capacitors are used in parallel to reduce the overall impedance because these have different reso- nant frequencies. The measurement accuracy is not critically dependent on supply decoupling because the high frequency signal path is confined to the relevant input pins. Lead lengths from both DECL pins to ground and from INHI/INLO to the input coupling capacitors should be as short as possible. All COMM pins should also connect directly to the ground plane. To place the device in measurement mode, connect VOUT to VSET and connect VTGT directly to VREF. DEVICE DISABLE The AD8362 is disabled by a logic high on the PWDN pin, which can be directly grounded for continuous operation. When enabled, the supply current is nominally 20 mA and essentially independent of supply voltage and input signal strength. When powered down by a logic low on PWDN, the supply current is reduced to 230 μA. RECOMMENDED INPUT COUPLING The full dynamic range of the AD8362, particularly at very high frequencies (above 500 MHz), is realized only when the input is presented to it in differential (balanced) form. In Figure 47, a transmission line balun is used at the input. Having a 1:4 impedance ratio (1:2 turns ratio), the 200 Ω differential input resistance of the AD8362 becomes 50 Ω at the input to the balun. 1 16 2 15 3 14 4 13 5 12 6 11 7 10 8 9 COMM CHPF DECL INHI INLO DECL PWDN COMM ACOM VREF VTGT VPOS VOUT VSET ACOM CLPF AD8362 C4 1nF C8 1000pF C7 1nF T1 ETC1.6-4-2-3 C10 1000pF SIGNAL INPUT Z = 50Ω C6 100pF C5 100pF C3 0.1µF VOUT C2 1nF C1 0.1µF VS 5V @ 24mA 1:4 Z-RATIO Figure 47. Basic Connections for RF Power Measurement The balun outputs must be ac-coupled to the input of the AD8362. The balun used in this example (M/A-COM ETC 1.6-4-2-3) is specified for operation from 0.5 GHz to 2.5 GHz. If a center-tapped, flux-coupled transformer is used, connect the center tap to the DECL pins, which are biased to the same potential as the inputs (~3.6 V). At lower frequencies where impedance matching is not neces- sary, the AD8362 can be driven from a low impedance differential source, remembering the inputs must be ac-coupled. Choosing Input Coupling Capacitors As noted, the inputs must be ac-coupled. The input coupling capacitors combine with the 200 Ω input impedance to create an input high pass corner frequency equal to fHP = 1/(200 × π × CC) (12) Typically, fHP should be set to at least one tenth the lowest input frequency of interest. Single-Ended Input Drive As previously noted, the input stages of the AD8362 are optimally driven from a fully balanced source, which should be provided wherever possible. In many cases, unbalanced sources can be applied directly to one or the other of the two input pins. The chief disadvantage of this driving method is a 10 dB to 15 dB reduction in dynamic range at frequencies above 500 MHz. Figure 48 illustrates one of many ways of coupling the signal source to the AD8362. Because the input pins are biased to about 3.6 V (for VS = 5 V), dc-blocking capacitors are required when driving from a grounded source. For signal frequencies >5 MHz, a value of 1 nF is adequate. While either INHI or INLO can be used, INHI is chosen here. 1 16 2 15 3 14 4 13 5 12 6 11 7 10 8 9 COMM CHPF DECL INHI INLO DECL PWDN COMM ACOM VREF VTGT VPOS VOUT VSET ACOM CLPF AD8362 1nF 1nF 1nF 0.01µF 1nF RF INPUT 100Ω Figure 48. Input Coupling from a Single-Ended 50 Ω Source |
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