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AD8311 bảng dữ liệu(PDF) 17 Page - Analog Devices

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AD8311
Rev. A | Page 17 of 24
tolerance of the external resistor. This method of matching is
most useful in wideband applications or in multiband systems
where there is more than one operating frequency.
A reactive match can also be implemented as shown in
Figure 34. This is not recommended at low frequencies because
device tolerances dramatically vary the quality of the match due
to the large input resistance. For low frequencies, Figure 33 or
Figure 35 is recommended.
In Figure 34, the matching components are drawn as generic
reactances. Depending on the frequency, the input impedance,
and the availability of standard value components either a
capacitor or an inductor is used. As in the previous case, the
input impedance at a particular frequency is plotted on a Smith
Chart and matching components are chosen (shunt or series L,
shunt or series C) to move the impedance to the center of the
chart.
RFIN
AD8311
RIN
CIN
CC
RSHUNT
52.3
Ω
Figure 33. Broadband Resistive Input Coupling Option
RFIN
AD8311
x2
RIN
CIN
CC
x1
Figure 34. Narrow Band Reactive Input Coupling Option
RFIN
AD8311
RIN
CIN
CC
RATTN
ANTENNA
STRIPLINE
PA
Figure 35. Series Attention Input Coupling Option
Figure 35 shows a third method for coupling the input signal
into the AD8311. A series resistor connected to the RF source
combines with the input impedance of the AD8311 to
resistively divide the input signal being applied to the input.
This has the advantage of very little power being tapped off in
RF power transmission applications.
TEMPERATURE DRIFT
Figure 36 shows the log slope and error over temperature for a
0.9 GHz input signal. Error due to drift over temperature
consistently remains within ±1 dB and only begins to exceed
this limit when the ambient temperature goes above +65 °C and
below −20 °C. For all frequencies using a reduced temperature
range, higher measurement accuracy is achievable.
10
–60
0.2
1.6
VSET (V)
0
–10
–20
–30
–40
–50
0.4
0.6
0.8
1.0
1.2
1.4
4
–3
2
1
0
–1
–2
3
–40°C
–20°C
0°C
+25°C
+45°C
+65°C
+85°C
Figure 36. Typical Drift at 900 GHz for Various Temperatures
DEVICE CALIBRATION AND ERROR CALCULATION
The measured transfer function of the AD8311 at 0.9 GHz is
shown in Figure 37. The figure shows plots of both input power
and calculated error vs. setpoint voltage.
The vertical axis represents the input power required at the RFIN
pin to null the control loop when a VSET voltage is applied. As
the setpoint voltage varies from about 0.2 V to 1.5 V, the
corresponding input power varies from −60 dBm to +10 dBm.
10
–60
0
1.6
VSET (V)
0
–10
–20
–30
–40
–50
4
–3
2
1
0
–1
–2
3
0.2
0.4
0.6
0.8
1.0
1.2
1.4
PIN2
PIN1
VSET1
INTERCEPT
VSET2
PINIDEAL = (VSET1/ SLOPE) + INTERCEPT
ERROR (dB) = (PINIDEAL – PIN)
SLOPE = (VSET2 – VSET1)/(PIN1 – PIN2)
INTERCEPT = PIN1 – (VSET1 / SLOPE)
+85°C
–40°C
+25°C
–40°C
+25°C
+85°C
Figure 37. Transfer Function of AD8311 at 0.9 GHz
Because slope and intercept vary from device to device, board-
level calibration must be performed to achieve high accuracy.



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