NSC LB-45

National Semiconductor
Linear Brief 45
April 1979
Most frequency-to-voltage (F-to-V) converters suffer from
the classical tradeoff of ripple versus speed of response.
For example, the basic F-to-V converter shown below has
13 mVp-p of ripple, and a rather slow 0.6 second settling
time, when CFILTER is 1 mF. If you want less ripple than that,
the response time will be even slower. If you want quicker
response, it is easy to decrease CFILTER, but the ripple will
increase by the same factor.
The improved circuit in Figure 2 makes an end-run around
these compromises. A low-cost sample-and-hold circuit
such as LF398 can sample the F-to-V’s output at the peak
of its ripple, and hold it until the next cycle. The LF398 has
fairly low output ripple (rms) but it does have some short
duration noise spikes and glitches which can be removed
easily with a simple output filter. The ripple at the output of
the active filter V6 is smaller than 1 mV peak, but the settling time for a step change of input frequency is only 60 ms,
or ten times quicker than the ‘‘basic’’ FVC with CFILTER e
1 mF.
VOUT e fIN c
# J
output
ripple
p-p
# R J (1.9V) (1.1R C )
1
(1.9V) (1.1R C )
R
#C J
RL
c
c
S
t t
c
e
t t
c
FILTER
S
TL/H/8494 – 1
FIGURE 1. Basic Frequency-to-Voltage Converter
C1995 National Semiconductor Corporation
TL/H/8494
RRD-B30M115/Printed in U. S. A.
LB-45
TL/H/8494 – 2
FIGURE 2. Improved F-to-V Converter Using Sample-and-Hold
Frequency-to-Voltage Converter uses Sample-and-Hold
to Improve Response and Ripple
Frequency-to-Voltage
Converter uses Sampleand-Hold to Improve
Response and Ripple
Frequency-to-Voltage Converter uses Sample-and-Hold
to Improve Response and Ripple
DETAILS OF OPERATION (Refer to Figure 3 , Waveforms)
When the input frequency waveform has a negative-going
transition, pin 6 of the LM331 is driven momentarily lower
than the 13V threshold voltage at pin 7. This initiates a timing cycle controlled by the Rt and Ct at pin 5, and also
causes a transition from a 5V to 0V at pin 3, (the normal
VFC logic output) which is usually left unused in F-to-V operation.
During the timing cycle (t e 1.1 c Rt c Ct e 75 ms, for the
example shown) a precision current source i e 1.9 V/RS
flows out of pin 1 of the LM331, and charges V1 up to a
value slightly higher than the average DC value of V1. At the
end of the timing cycle, V1 stops charging up, and also V2
rises. The 10 kX pull-up resistor is coupled (through the 200
pF capacitor) to V3, and causes the LF398 to sample for
about 5 ms. Then the LF398 goes back into hold . This entire
operation is repeated at the same frequency as fIN. The
average voltage at V1 will be the same 10V full scale, according to the same formula of Figure 1 . And the peak-topeak ripple can be computed as 65 mV peak, 130 mVp-p,
using the appropriate formula.
Now, the input to the sample-and-hold at pin 3 may have a
10.000V average DC value, but the output will be at
10.065V, because the sample occurs at the peak value of
V1. Thus, to get an output with low offset, a 15 MX resistor
is used to offset the V1 signal to a lower level. Trim the
offset adjust pot to get VOUT e 1V at 1 kHz, and trim the
gain adjust pot to get VOUT e 10V at 10 kHz (the interaction is minor), as measured at V4, V5, or V6. The rms value
of the ripple at V4 is rather small, but the peak-to-peak ripple (spikes and glitches) may be excessive. A simple R-C
filter can provide a filtered output at V5; or a simple active
filter using an inexpensive LF351, will give sub-millivolt
(peak) ripple at V6, with improved settling time and low output impedance.
This F-to-V converter will have a good linearity, better than
0.1%, but only from 10 kHz down to 500 Hz. Between
200 Hz and 20 Hz, VOUT is not very proportional to fIN. And
at 0 Hz, the output will be indeterminate, because the sample-and-hold will never sample! However, there are many Fto-V applications where a 20:1 frequency range is adequate.
TL/H/8494 – 3
FIGURE 3. Waveforms, Improved F-to-V Converter
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LB-45
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