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Simple capacitance meter bins surface-mount parts

This Design Idea describes a simple two-chip CMOS
circuit that can sort capacitors into 20 bins over a wide range
(100 pF to 1 ?F), using 10 LEDs to display the value range. The
circuit is power efficient and can be run using two CR2032 cells.
As such, it can be built into a handheld probe.
The heart of the circuit is the RS flip-flop using 4093 NAN D
gates along with transistors Q1 and Q2, which discharge the
reference and test capacitors respectively. The reference capacitor
(CREF) and the test capacitor (CX) are charged from zero
volts, followed by a reset pulse applied to the bases of Q1 and
Q2. Depending on the values of the capacitors and their respective
series resistors, either CX or CREF reaches the gates’ VT
before the other; accordingly the outputs of the RS flip-flop are
set/reset. The outputs are so wired such that when CREF reaches
VT before CX, a clock pulse is applied to the CD4017 counter,
whose outputs (Q0-Q9) charge CREF through one of 10 different
series resistor values (R0-R9).
The master clock that runs the circuit is derived using a single
4093 Schmitt NAN D gate.
This steps the 4017 decoded decade counter, the flip-flop
“comparing” the voltage ramps across CX and CREF
while charging CREF through the different values. When CX
reaches VT before CREF, then 4017 is not clocked, and the
appropriate LED starts flashing indefinitely. Depress the
reset switch to take another reading, which resets the
4017 and selects the minimum resistor value, R0. There
are two ranges, each divided into 10 sections, which cover
100 pF-10 nF and 10 nF-1 ?F. The range is selected by an
SPDT switch which connects a CREF of either 100 pF or 10
nF.
A particular flashing LED indicates that the value of the
test capacitor lies in the range between it and the next lower
LED. Q3 takes care of lighting the LED in the appropriate
phase of the master clock. The anodes of the 10 LEDs
are connected to the outputs (Q0-Q9) of the CD4017. It
seems that lower values of charging resistors can result in
more reliable readings due to smaller errors in the charging
current (contributed mainly by reverse conduction in all the
diodes). R0-R9 can be scaled appropriately, together with an
inverse scaling of the master clock frequency.
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