Jeremy Ahern, a former school science
teacher has a keen interest in early scientific manuscripts and texts. He also maintains an
impressive attic laboratory at his home in
Wales, where he conducts experimental researches in
electrostatics and other areas. One of his developments is an inexpensive
electronic instrument useful in demonstrating
electrostatic phenomena [ESA, 1999]. A description of this instrument is included in the
Industrial Electrostatics Demonstration web site for several reasons. First, Ahern's
instrument can be
employed as an inexpensive and effective substitute for
the tonal electrostatic voltmeter
. Second, the instrument provides
polarity-dependent information about electric charge
motion that other, more
conventional instruments do not provide. Third, this apparatus is a very easily built
electronic-based instrument for monitoring static charge.
To learn more about this
instrument, please contact Dr. Ahern directly by EMAIL.
What distinguishes Ahern's instrument from other charge detection and measurement apparatuses used in electrostatics demonstrations, such as the conventional leaf electroscope and the tonal electrostatic voltmeter, is that Ahern's device responds to the movement of positive (+) and negative (-) electric charge toward or away from a sensing electrode. As such, the instrument is probably most closely akin to some of the electrostatic charge monitors now commercially available and routinely installed in electronics assembly areas to detect conditions that might cause damage to sensitive electronics components during assembly.
The instrument is
small and portable, it operates on a 9 volt battery, and
the output is visual. Furthermore, its construction
requires only minimal skills with a soldering iron and
other simple tools, and it can be packaged very
conveniently in a small, shielded box. Refer to the
photo at the left. A short, telescoping cellular
telephone antenna mounted so that it retracts into the
box when not in use, serves as a sensing
electrode.
The instrument is sensitive primarily to
the movement of charge rather than to its
presence. Thus, when the approach of negative charge
is sensed, the green LED comes on, while the red LED
lights if positive charge is approaching. As negative
charge starts to recede from the sensing electrode, the
green changes to red, while red changes to green as
positive charge recedes. If a condition of balance can
be achieved between positive and negative, then both
LED's can be made to light up; this balance is
exquisitely delicate due to the very high input
impedance of the cmos gates. In the absence of any
charge, neither LED lights up.
charge movement | instrument response |
---|---|
+ charge approaching | RED |
+ charge receding | RED changing to GREEN |
- charge approaching | GREEN |
- charge receding | GREEN changing to RED |
+ & - charges present | RED and GREEN |
no charge present | no LEDs lighted |
The instrument is much more sensitive than most hand-held charge detectors. During demonstrations of electrostatic phenomena -- for example, triboelectrification -- the moving charge sensor can be used to sense the charge and to determine its sign. The circuit draws very little current, so the instrument can be operated for extended periods of time without draining the battery.
The heart of this inexpensive circuit, the schematic of which is shown below, is a quad cmos NAND gate integrated circuit (4011). Experienced circuit designers will smile when they recognize that this circuit beneficially exploits the notorious static sensitivity of cmos IC devices. Only three of the four NAND gates in the IC are actually used in the instrument; the input of the fourth gate should be grounded. The 3 MW series resistor protects the chip from ESD damage, while the capacitors serve the primary function of biasing the gates to a quiescent state. Resistors in the ~10 GW range may be used instead, but the capacitors -- Ahern specifies tubular ceramics -- with their very small but not negligible leakage current, work just as well and are definitely cheaper and more readily available. In addition, the charge storage feature of the capacitors introduces some incidental phase lag between the two detection circuits that permits both LEDs to remained lighted when both signs of charge are detected simultaneously.
A small,
inexpensive telescoping antenna -- of the type used in
cell phones and available at electronics supply stores
-- serves the function of the input charge-sensing
electrode. But an even cheaper solution for the sensing
electrode is a length of rigid wire formed into a loop
so as not to present a hazard. One must make sure to
remove the insulation from this wire. If the circuit
is packaged in a plastic box, shielding is crucial.
Aluminum or copper foil taped or glued to at least one side of the box
and connected to the circuit ground is essential. In addition, if the telescoping antenna
is used, it may be a good idea to shield it from the circuit on the inside of the box.
Electrostatics
Society of America, Electrostatics Newletter, Issue
#142, Jan/Feb., 1999. Reference
Tonal ESV