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Analysis of this portion of the filter circuit yields the transfer
function:
F1(s) = Kl *
1
s
*
(s + z)
[s2 + (2ζω ) s + ω2 ]o2
o2
The gain constant is defined as:
where:
Al = op-amp gain constant for selected pole positions.
RA = integrator feedback resistor.
RlA = integrator input resistor.
Kl = Al *
RA
RlA
eqt. 5
The integrator circuit introduces a zero, a pole at the origin,
and a second order pole set as described by the two pole model
for an op-amp. As in the case of the differential summing
amplifier, we assume the op-amp pole pair occur as a complex
conjugate pair making an angle of 45° to the real axis of the
complex frequency plane; are positioned for near unity gain
operation; and are located beyond the crossover frequency.
Since both the summing and integrating op-amps are realized
by the same type of op-amp (MC34182D), the open loop pole
positions for both amplifiers will be the same.
Further, the loop transfer function contains two poles located
at the origin, one introduced by the integrator and the other by
the VCO; hence a zero is necessary to compensate for the phase
shift produced by these poles and ensure loop stability. The
op-amp will be stable if the crossover point occurs before the
transfer function phase angle becomes 180°. The zero should
be positioned much less than one decade before the unity gain
frequency.
As in the case of the filter input circuitry, the poles and zero
from this analysis will be used as open loop poles and a zero
when performing the root locus analysis for the complete
system.
Determination of Element Values
The location of the zero is used to determine the element
values for the augmenting integrator. The value of the
capacitor, CA, is selected to provide adequate charge storage
when the loop is not sampling data. A value of 0.1 μF is
sufficient for most applications; this value may be increased
when the RDCLK frequency is much lower than 4 MHz. The
value of RA is governed by:
⎥ z⎥ =
1
2πRACA
eqt. 6
For unity gain operation of the integrating op-amp the value of
RlA is selected such that:
RlA = RA
eqt. 7
It should be noted that although the zero can be tuned by
varying either RA or CA, caution must be exercised when
adjusting the zero by varying CA because the integrator gain is
also a function of CA. Further, the gain of the loop filter can be
adjusted by changing the integrator input resistor RlA.
Voltage Divider
The input range to the VCOIN input is from 1.3 V + VEE to
2.6 V + VEE; hence, the output from the augmenting amplifier
section must be attenuated to meet the VCOIN constraints. A
simple voltage divider network provides the necessary
attenuation (Figure 8).
VIN
RV
RO
DB
Cd
VO
Figure 8. Voltage Divider Subsection
In addition, a shunt filter capacitor connected between the
VCOIN input pin and VEE provides the voltage divider
subsection with a single time constant transfer function that adds
a pole to the overall loop filter. The transfer function for the
voltage divider network is:
Fd(s) = Kd *
1
(s + p2)
The gain constant, Kd, is defined as:
Kd =
1
Rv Cd
eqt. 9
he value of Kd is easily extracted by rearranging Equation 1:
Kd =
Kol
Kφ * Ko * K1 * Kl
eqt. 10
The gain constant Kd is set such that the output from the
integrator circuit is within the range 1.3 V +VEE to 2.6 V +VEE.
The pole for the voltage divider network should be positioned
an octave beyond that for the filter input.
Determination of Element Values
Once the pole location and the gain constant Kd are established
the resistor values for the voltage divider network are
determined using the design guidelines mentioned above and
from the following relationship:
Kd
2π⎥ p2
=
Ro
Ro + Rv
Having determined the resistor values, the filter capacitor is
calculated by rearranging Equation 9:
Cd =
1
Rv Kd
eqt. 9a
Finally, a bias diode is included in the voltage divider network
to provide temperature compensation. The finite resistance of
this diode is neglected for these calculations.


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