参数资料
型号: AD8318ACPZ-WP
厂商: ANALOG DEVICES INC
元件分类: 运动控制电子
英文描述: 1 MHz - 8 GHz, 60 dB Logarithmic Detector/Controller
中文描述: LOG OR ANTILOG AMPLIFIER, 600 MHz BAND WIDTH, QCC16
封装: 4 X 4 MM, MO-220-VGGC, LFCSP-16
文件页数: 15/24页
文件大小: 2127K
代理商: AD8318ACPZ-WP
AD8318
Rev. 0 | Page 15 of 24
V
OUT(MAX)
= (2.1 V ×
X
) when
X
< (
V
P
– 400 mV)/(2.1 V)
V
OUT(MAX)
= (
V
P
– 400 mV) when
X
(
V
P
– 400 mV)/(2.1 V)
When X = 1, the typical output voltage swing is 0.5 V to 2.1 V.
The output voltage swing can be modeled by using the equations
above and restricted by the following equation:
V
OUT(MIN)
<
V
OUT
<
V
OUT(MAX)
For the case when
X
= 4 and
V
P
= 5 V
(
X
×
V
OFFSET
) <
V
OUT
< (
V
P
– 400 mV)
(4 × 0.5 V) <
V
OUT
< (2.1 V × 4)
2 V <
V
OUT
< 4.6 V
For X = 4, Slope = 100 mV/dB; V
OUT
can swing 2.6 V, and
usable dynamic range will be reduced to 26 dB from 0 dBm to
–26 dBm.
The slope is very stable versus process and temperature
variation. When base-10 logarithms are used, V
SLOPE/DECADE
represents the “volts/decade.” A decade corresponds to 20 dB,
V
SLOPE/DECADE
/20 = V
SLOPE/dB
represents the slope in “volts/dB.”
As noted in the equations above, the V
OUT
voltage has a negative
slope. This is also the correct slope polarity to control the gain of
many power amplifiers and other VGAs in a negative feedback
configuration. Since both the slope and intercept vary slightly
with frequency, it is recommended to refer to the specification
pages for application specific values for slope and intercept.
Although demodulating log amps respond to input signal
voltage, not input signal power, it is customary to discuss the
amplitude of high frequency signals in terms of power. In this
case, the characteristic impedance of the system, Z
o
, must be
known to convert voltages to their corresponding power levels.
Starting with the definitions of dBm and dBV,
P(dBm) = 10 × log
10
(V
rms2
/(Z
O
× 1 mW)) (3)
V(dBV) = 20 × log
10
(V
rms
/1 V
rms
) (4)
Expanding Equation 3 gives us:
P(dBm) = 20 × log
10
(V
rms
) 10 × log
10
( Z
O
× 1 mW) (5)
and given Equation 4, we can rewrite Equation 5 as
P(dBm) = V(dBV) 10 × log
10
(Z
O
× 1 mW) (6)
For example, P
INTERCEPT
for a sinusoidal input signal
expressed in terms of dBm (decibels referred to 1 mW), in a
50 system is:
P
INTERCEPT
(dBm) = V
INTERCEPT
(dBV)
– 10 × log
10
(Zo × 1 mW) (7)
= +7 dBV 10 × log
10
(50 × 10
-3
) = +20 dBm
Further information on the intercept variation dependence
upon waveform can be found in the AD8313 and AD8307
data sheets.
AD8318 data sheet specifications for slope and intercept
have been calculated based on a best straight line fit using
measured data in the 10 dBm to 50 dBm range (see
Figure 29).
DEVICE CALIBRATION AND ERROR
CALCULATION
The measured transfer function of the AD8318 at
2.2 GHz is shown in
Figure 30
. The figure shows plots of
both output voltage versus input power and calculated
error versus input power.
As the input power varies from
65 dBm to 0 dBm, the
output voltage varies from 2 V to about 0.5 V.
2.2
2.0
1.8
1.6
1.4
1.2
1.0
0.8
0.6
0.4
0.2
2.5
2.0
1.5
1.0
0.5
0
–0.5
–1.0
–1.5
–2.0
–65 –60 –55
–45 –40 –35 –30 –25 –20 –15
P
IN
(dBm)
–5
0
5
INTERCEPT
0
PIN
1
PIN
2
V
O
E
V
OUT
+25
°
C
V
OUT
–40
°
C
V
+85
°
C
ERROR +25
°
C
ERROR –40
°
C
ERROR +85
°
C
VOUT
2
VOUT
1
VOUT
IDEAL
= SLOPE
×
(P
IN
– INTERCEPT)
SLOPE = (VOUT
1
– VOUT
2
)/(PIN
– PIN
2
)
INTERCEPT = PIN
– (VOUT
1
/SLOPE)
ERROR (dB) = (VOUT
×
VOUT
IDEAL
)/SLOPE
Figure 30. Transfer Function at 2.2 GHz
Because slope and intercept vary from device to device,
board-level calibration must be performed to achieve high
accuracy.
We can rewrite the equation for output voltage from the
previous section using an intercept expressed in dBm
V
OUT
=
Slope
× (
P
IN
Intercept
) (8)
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