# Accurate Analogue Frequency Meter Circuit

To measure frequency one does not  immediately have to ‘go digital’. The
analogue approach will invariably prove simpler and cheaper, in
hand. All that is needed is n a plug-in device, a ‘trans1ator’, that
will give the meter an input it can ‘under stand’.
This design is based upon an  integrated
frequency-to-voltage con verter, the Raytheon 4151. The device a is
actually described as a voltage-t0 frequency converter; but it becomes
clear from the application notes that  there is more to it than just
that. The  linearity of the converter IC is about 1%, so.that
areasonably good mul timeter will enable quite accurate b frequency
measurements to be made. ·Because the 4151 is a little fussy about tithe
waveform and amplitude of its input signal, the input stage of this
design is a limiter-amplifier (compara tor). This stage will process a
signal of any shape, that has an amplitude of at least 50 mV, into a
form suitable for  feeding to the 4151. The input of this stage is
protected (by diodes) against voltages up to 400 V p-p. The drive to the
multimeter is provided by a ·short circuit-proof unity-gain amplifier.

The circuit

Figure1 gives the complete circuit of I the frequency plug-in. The input
is safe for 400 V p-p AC inputs only when the DC blocking capacitor is
suitably rated. The diodes prevent excessive drive volt ages from
reaching the input of the comparator IC1. The inputs of this IC are
biased to half the supply voltage by the divider R3/R4. The bias current
flowing in R2 will cause the output of ICI to saturate in the negative
direction. An input signal of sufficient amplitude to overcome this
offset will cause the output to change state, the actual switchover
being speeded up by the positive feedback through C3. On the opposite
excursion of the inputsignal the comparator will switch back again, so
that a large rectangularwave will be fed to the 4151 input.  The 4151
will now deliver a DC output voltage corresponding to the frequency of
the input signal. The relationship  between voltage and frequency is
given by:

U/f = R9.R11.C5/0.486(R10+p1) V/Hz

The circuit values have been chosen to give 1V per kHz. This means that a
10 volt f.s.d. will correspond to 10 kHz. Meters with a different full
scale deflec tion, for example 6 volts, can, however,  also be used.
There are two possibilities:   either one uses the existing scale cali
brations to read off frequencies to 6 kHz, or one sets P1 to achieve a 6
volt  output (i.e. full scale in our example)  when the frequency is 10
kHz. The  latter choice of course implies that every reading will
require a little mental gymnastics! With some meters it may be necessary
to modify the values of P1 and/or R10; the value of R10 + P1 must
however always be greater than 500E · The output is buffered by another
3130  (IC3). The circuit is an accurate voltage follower, so that low
frequencies can be more easily read off (without loss of accuracy) by
setting the multimeter to a lower range (e.g. 1 V f.s.d.).·The out put
is protected against short-circuiting by R12. To eliminate the error
that would otherwise occur due to the volt age drop in this resistor,
the voltage follower feedback is taken from behind R12; To enable the
full 10 volt output to be obtained in spite of the drop in R12 (that has
to be compensated by the IC) the meter used should have an  internal.
resistance of at least 5 kohm). This implies a nominal sensitivity of
500 ohm/volt on the 10 volt range. There » surely cannot be many meters
with a sensitivity lower than that. If one has a separate moving coil
milliameter available, it can be fitted with a series resistor that
makes its intemal resistance up to the value required of a voltmeter
giving f.s.d. · at 10 volt input. This alternative makes the frequency
meter independent of the multimeter, so that it can bedused to monitor
the output of a generator that for some reason may  have a dubious
scale- or knob-cali bration.

Construction

No trouble is to be anticipated if the    circuit is built up using the
PC board layout given in figure 2. Bear in imind that the human body
will not necess arily survive contact with input voltages that may not
damage the adequately rated input blocking capacitor. If one
contemplates measuring the frequency of such high voltages the circuit
should be assembled in a well-insulated box! The power supply does not
need to be regulated, so it can be kept very simple. A transformator
secondary of 12 volts, a bridge rectifier and a 470 uF/25 V reservoir
electrolytic will do the job nicely. Although a circuit that draws 25 mA
is not too well suited to battery supply,one may need or wish to do
this. In this case the battery should be ‘bridged by a low-leakage (e.g.
tantalum) 10uF/25 V capacitor to provide a low AC source impedance.

Calibration

The calibration can really only be done with an accurate generator. 10
kHz signal is fed to the input and Pl is set to bring the multimeter to
full scale deflection (e.g. 10 V). That com n pletes the calibration
although it is vwise to check that the circuit is oper ating correctly
by using lower input frequencies and observing whether the meter reading
is also (proportionately) lower.

A few specifications:

frequency range: 10 Hz . . .10 kHz
input impedance: > 560 k
sensitivity: 50 mV p-p
max input voltage: 400 V peak
minimum load on output: 5 k (if 10 V out required)