AD8362
4.0
3.5
3.0
2.5
2.0
1.5
1.0
0.5
Accordingly, VTGT (and its fractional part VATG) determines the
output that must be provided by the VGA for the AGC loop to
settle. Since the scaling parameters of the two squarers are
accurately matched, it follows that Equation 3 is satisfied only
when
2
2
MEAN
(
VSIG
)
= VATG
(4)
In a formal solution, one would then extract the square root of
both sides to provide an explicit value for the root-mean-square
(rms) value. However, it is apparent that by forcing this identity,
through varying the VGA gain and extracting the mean value
by the filter provided by the capacitor(s), the system inherently
establishes the relationship
0
100µV
1mV
10mV
100mV
1V
10V
RMS INPUT VOLTAGE (100µV TO 3.2V)
Figure 43. Ideal Response of the AD8362
rms
VSIG
=VATG
(5)
EFFECT OF INPUT COUPLING ON THE INTERCEPT
VALUE
Substituting the value of VSIG from Equation 2, we have
Reductions of VIN due to coupling losses directly affect VZ. In
high frequency applications, several factors contribute to the
coupling of the source into the IC, including the board and
package resonances and attenuation. Any uncertainties in the
input impedance result in the intercept expressed in power
terms, which is nominally −57 dBm for a 50 Ω system, being
less accurately determined than when stated in dBV (that is, in
pure voltage) terms. On the other hand, the slope VSLP is
unaffected by all such impedance or coupling uncertainties.
rms
GOVIN exp
−VSET VGNS
=VATG
(6)
As a measurement device, VIN is the unknown quantity and all
other parameters can be fixed by design. Solving Equation 6:
rms
GOVIN VATG
= exp
VSET VGNS
(7)
so
VSET =VGNS log
rms
(VIN
)
VZ
(8)
OFFSET ELIMINATION
The quantity VZ = VATG/GO is defined as the intercept voltage
because VSET must be 0 when rms (VIN) = VZ.
To address the small dc offsets that arise in the variable gain
amplifier, an offset-nulling loop is used. The high-pass corner
frequency of this loop is internally preset to 1 MHz, sufficiently
low for most HF applications. When using the AD8362 in LF
applications, the corner frequency can be reduced as needed by
the addition of a capacitor from the CHPF pin to ground having
a nominal value of 200 µF/Hz. For example, to lower the high-
pass corner frequency to 150 Hz, a capacitance of 1.33 µF is
required. The offset voltage varies depending on the actual gain
at which the VGA is operating, and thus, on the input signal
amplitude.
When connected as a measurement device, the output of the
buffer is tied directly to VSET, which closes the AGC loop.
Making the substitution VOUT = VSET and changing the log
base to 10, as needed in a decibel conversion, we have
VOUT =VSLP log10
rms
(VIN
)
VZ
(9)
where VSLP is the slope voltage, that is, the change in output
voltage for each decade of change in the input amplitude.
(Note that VSLP = VGNS log (10) = 2.303 VGNS). In the AD8362,
V
SLP is laser trimmed to 1 V using a 100 MHz test signal.
Baseline variations of this sort are a common aspect of all
VGAs, although more evident in the AD8362 because of the
method of its implementation, which causes the offsets to
ripple along the gain axis with a period of 6.33 dB. When an
excessively large value of CHPF is used, the offset correction
process may lag the more rapid changes in the VGA’s gain,
which may increase the time required for the loop to fully settle
for a given steady input amplitude.
Because a decade corresponds to 20 dB, this slope may also be
stated as 50 mV/dB. It is later shown how the effective value of
VSLP may be altered by the user.
Likewise, the intercept VZ is also laser trimmed to 316 µV
(−70 dBV). In an ideal system, VOUT would cross zero for an
rms input of that value. In a single-supply realization of the
function, VOUT cannot run fully down to ground; here, VZ is
the extrapolated value. In measurement modes, the output
ranges from 0.5 V for VIN = 1 mV (input values are stated as
rms, outputs values as dc), up to a voltage 60 dB × 50 mV/dB =
3 V above this for VIN = 1 V, that is, to 3.5 V. Figure 43 shows the
ideal form of Equation 9 scaled as in the AD8362.
Rev. B | Page 16 of 36