1.0 LMF40 Application Information (Continued)
1.2 POWER SUPPLY
The LMF40 can be powered from a single supply or split
supplies. The split supply mode shown in
Figure 2
is the
most flexible and easiest to implement. Supply voltages of
g5V to g7V enable the use of TTL or CMOS clock logic
levels.
Figure 3
shows AGND resistor-biased to Va/2 for
single supply operation. In this mode only CMOS clock logic
levels can be used, and input signals should be capacitor-
coupled or biased near mid-supply.
1.3 INPUT IMPEDANCE
The LMF40 low-pass filter input (FILTER IN) is not a high
impedance buffer input. This input is a switched-capacitor
resistor equivalent, and its effective impedance is inversely
proportional to the clock frequency. The equivalent circuit of
the filter’s input can be seen in
Figure 4
. The input capacitor
charges to VIN during the first half of the clock period; dur-
ing the second half the charge is transferred to the feed-
back capacitor. The total transfer of charge in one clock
cycle is therefore Q eCIN VIN, and since current is defined
as the flow of charge per unit time, the average input current
becomes
IIN eQ/T
(where T equals one clock period) or
IIN AVE eCIN VIN
TeCIN VIN fCLK
The equivalent input resistor (RIN) then can be expressed
as
RIN eVIN
IIN
e1
CIN fCLK
The input capacitor is 2 pF for the LMF40-50 and 1 pF for
the LMF40-100, so for the LMF40-100
RIN e1c1012
fCLK
e1c1012
fcc100 e1c1010
fc
and
RIN e5c1011
fCLK
e5c1011
fcc50 e1c1010
fc
for the LMF40-50. The above equation shows that for a
given cutoff frequency (fc), the input resistance of the
LMF40-50 is the same as that of the LMF40-100. The high-
er the clock-to-cutoff-frequency ratio, the greater equivalent
input resistance for a given clock frequency.
This input resistance will form a voltage divider with the
source impedance (RSource). Since RIN is inversely propor-
tional to the cutoff frequency, operation at higher cutoff fre-
quencies will be more likely to attenuate the input signal
which would appear as an overall decrease in gain to the
output of the filter. Since the filter’s ideal gain is unity, the
overall gain is given by:
AVeRIN
RIN aRSource
If the LMF40-50 or the LMF40-100 were set up for a cutoff
frequency of 10 kHz the input impedance would be:
RIN e1c1010
10 kHz e1MX
As an example, with a source impedance of 10 kXthe over-
all gain would be:
AVe1MX
10 kXa1MXe0.99009 or b0.086 dB
Since the maximum overall gain error for the LMF40 is
a0.05, b0.15 dB @25§C with RSs2kXthe actual gain
error for this case would be b0.04 dB to b0.24 dB.
1.4 CUTOFF FREQUENCY RANGE
The filter’s cutoff frequency (fc) has a lower limit due to
leakage currents through the internal switches draining the
charge stored on the capacitors. At lower clock frequencies
these leakage currents can cause millivolts of error. For ex-
ample:
fCLK e100 Hz, ILeakage e1 pA, C e1pF
Ve1pA
1 pF (100 Hz) e10 mV
The propagation delay in the logic and the settling time re-
quired to acquire a new voltage level on the capacitors limit
the filter’s accuracy at high clock frequencies. The ampli-
tude characteristic on g5V supplies will typically stay flat
until fCLK exceeds 1.5 MHz and then peak at about 0.1 dB
at the corner frequency with a 2 MHz clock. As supply volt-
age drops to g2.5V, a shift in the fCLK/fcratio occurs which
will become noticeable when the clock frequency exceeds
500 kHz. The response of the LMF40 is still a good approxi-
mation of the ideal Butterworth low-pass characteristic
shown in
Figure 5
.
2.0 Designing with the LMF40
Given any low-pass filter specification, two equations will
come in handy in trying to determine whether the LMF40 will
do the job. The first equation determines the order of the
low-pass filter required to meet a given response specifica-
tion:
nelog [(100.1Amin b1)/(100.1Amax b1)]
2 log (fs/fb)(2)
where n is the order of the filter, Amin is the minimum stop-
band attenuation (in dB) desired at frequency fs, and Amax is
the passband ripple or attenuation (in dB) at cutoff frequen-
cy fb(Note 15). If the result of this equation is greater than
4, more than one LMF40 will be required.
The attenuation at any frequency can be found by the fol-
lowing equation:
Attn (f) e10 log [1a(100.1Amax b1)(f/fb)2n]dB (3)
where n e4 for the LMF40.
2.1 A LOW-PASS DESIGN EXAMPLE
Suppose the amplitude response specification in
Figure 6
is
given. Can the LMF40 be used? The order of the Butter-
worth approximation will have to be determined using (1):
Amin e18 dB, Amax e1.0 dB, fse2 kHz, and fbe1 kHz
nelog[(101.8 b1)/(100.1 b1)]
2 log(2) e3.95
Since n can only take on integer values, n e4. Therefore
the LMF40 can be used. In general, if n is 4 or less a single
LMF40 can be utilized.
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