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"Static Electricity" means "High Voltage"

1999 William J. Beaty

"Static electricity" is not electricity which is static. The thing we call "static electricity" really is an imbalance in the amounts of positive and negative charges in the surface of an object. In addition, there is always a strong electric field surrounding these charges. What is an "electric field?" One way to say it: an Electric field is like a magnetic field, but it is electrical. Another simple answer: an electric field is a voltage without a current. Another way to say it: "STATIC ELECTRICITY" is not "static", it really means "HIGH VOLTAGE ELECTRICITY."

When you scuff your shoes upon a rug, your body typically charges up to a potential of several thousand volts with respect to ground. Touch a grounded object, and a spark will leap between the object and your fingertip. This kind of electric spark can only exist when a high voltage is present. The tiniest spark requires about 500 volts. Big, nasty, painful sparks require lots more voltage, up to several thousand volts. But even when no sparks are jumping, there is a high voltage between your body and the ground, and you body is surrounded with an invisible electric field.

During low-humidity weather, scuffing shoes upon rugs can put a huge voltage on your body. It is fairly easy to detect this voltage (try RIDICULOUSLY SENSTIVE CHARGE DETECTOR) However, this voltage is fairly difficult to actually measure. A normal voltmeter is no good. The electrical resistance of a normal voltmeter will discharge your body in a few thousandths of a second (it places a 10-megohm resistor across a 200pF body capacitance.)

Recently I discovered that some teachers DON'T BELIEVE that "Static Electricity" actually involves high voltage." OK, then we need a way to prove that it does. Below are various ways to measure the high voltages which arise because of "static electricity" upon your body. Don't take my word for it, go measure it for yourself.

MEASURING "STATIC" HIGH VOLTAGES

1. Obtain a professional electrometer or Electrostatic Voltmeter (expensive!) The input resistance of the meter needs to be around 10^11 ohms or greater. Ground one input lead, hold the other lead in your hand, scuff on the rug, and watch the voltage-reading on the meter as it climbs up to several kilovolts. (Humidity must be low, of course, or the rug-scuffing won't charge up your body.)

2. Fix two large and polished brass balls (2" dia. or larger) to an insulating plate so there is a 1mm gap between them. Verify the 3,000-volt breakdown voltage of this spark gap by producing sparks between the balls using an adjustable HV DC supply. Now disconnect the power supply, ground one brass ball, hold your finger against the other one, and start madly scuffing your shoes on the rug. Sparks leap across the gap. Your body charges up to 3 kilovolts, and causes a spark-gap breakdown, just like the power supply did. (I've done variations on this measurement technique many times, since it makes an expensive electrometer unnecessary. Sometimes, when humidity is extremely low, you can widen the gap spacing by quite a bit, which implies that human body voltage exceeds 3,000 volts by quite a bit.)

3. Use an adjustable, calibrated High Voltage DC power supply to charge your body to various voltages (EXTREME DANGER! Limit the current to below a few hundred uA by using a series resistor chain. If you don't know how to use DC high-volt power supplies safely, then don't mess with them. IF YOU DO THIS WRONG, IT CAN KILL YOU.) Use the power supply to charge yourself to 3KV, 5KV, 7KV, and touch a grounded knob each time. No electrometer is needed, yet you've just verified the length, sound, and pain-level of the fingertip spark which appear when your body had been forced to take on certain high voltages. This procedure is a great way to learn the types of sparks produced by various voltages on your body, so the next time you get zapped by a car-door, you can say "YOW!, the ouchiness-factor of that spark indicates a human body voltage on the order of seven kilovolts." :)

4. Crudely measure your body-voltage by using an oscilloscope to compare it to a high-voltage power supply. First, connect an oscilloscope's input to a metal plate. Scuff on a carpet (during a low-humidity day), wave your hand near the metal plate, and see how much the trace on the oscilloscope is deflected. Adjust the scope's vertical gain to give a fairly large deflection during your hand-waving. (Don't TOUCH the plate while your body is charged, or you might damage the scope!)

Next, use a DC high-voltage power supply with a large current-limiting series resistor to charge your body to 5,000 volts. (EXTREME DANGER! You MUST limit the current to below a few hundred microamps by using a series resistor chain. If you don't know how to handle high-volt DC power supplies safely, then don't mess with them. IF YOU DO THIS WRONG, IT CAN KILL YOU.) Wave your charged hand near the metal plate while seeing how far the oscilloscope trace deflects. Adjust the HV supply voltage until the deflection is about the same as when your body was charged by the rug-scuffing. Read the power-supply voltage setting, and you will know the approximate body-voltage produced by rug-scuffing.

5. A more precise version of no. 4 above... Build a crude "field-mill" e-field sensor by using a small DC motor to whirl a grounded wire, place an oscilloscope probe behind the whirling wire so it is alternately shielded and unshielded, mount the entire assembly an inch or so from a large, electrically floating brass ball, then observe the scope trace. The observed AC voltage will be proportional to any DC voltage on the isolated brass ball with respect to ground. Apply a known kilovoltage to the brass ball in order to calibrate it against the AC reading on the scope (for example, 1,000 volts applied to the brass ball will produce a certain AC voltage reading on the scope, and any other voltage applied to the brass ball will be proportional.) Now go scuff on a rug while keeping one finger on the brass ball, and see what voltage is detected by the system. (No oscilloscope? Try placing a small metal disk behind the whirling wire, then connect an AC voltmeter to the plate and to ground, then set the meter to a sensitive scale. Calibrate the voltage reading on the meter against a known DC high voltage applied to the brass ball.)

To measure REALLY high voltages (such as those produced by a VandeGraaff machine), you can use the above technique, but use the VDG sphere itself instead of the "brass ball", and place the field-mill and the oscilloscope several feet away from the VDG sphere. Calibrate it as before. If 1KV applied artificially to the VDG sphere produces a certain waveform voltage, then 100KV will produce exactly 100 times higher AC voltage.

6. Build 300 crude electrometers which drive individual LEDs. Use them to build a "visible e-field detector panel." When charged objects approach the panel, the glowing field of LEDs darkens in a pattern around the object. Scuff on the rug, hold a hand up, and observe the darkened field around your hand. What body voltage does this imply? To find out, go grab the old 7KV supply, hold the live terminal, then wave your hand around the sensor panel. Whoa! The darkened field is larger than before. Decide that the rug-scuffing body-voltage must have been maybe half of the body voltage created by the 7KV supply, maybe 3,500 volts.

OTHER WAYS TO VERIFY THAT "STATIC ELECTRICITY" INVOLVES HIGH VOLTAGE

Read books which say that common "static electric" sparks first appear when the voltage on your body rises above 500VDC. Use a HV DC power supply to test this, and find that their estimate is too low, that sparks cannot be seen at all until 750V, and they are very hard to notice until the voltage on your body is above 1KV.

Calculate what happens when a charged balloon is lifted from your arm. Obtain a value of 100KV. Sounds sensible. Ordinarily a VandeGraaff Generator would be needed to make arm-hair stand up so fiercely.
Read research papers from people who measure such things. Here's one from J. Chubb Inc:

The Control of Body Voltage Getting Out of a Car

Their measurements for different clothing and various car-seats give impressively high voltages, and this occurred at humidity levels above 50%. The voltages should be MUCH higher at, say 5% R.H.!

Here's a suggestion taken from the PHYS-L discussion group:

Touch the electrode of a foil-leaf electroscope, and simultaneously scuff on the carpet. Observe the deflection of the foils. Now connect the electroscope terminal to an adjustable HV DC power supply with the other HV supply terminal connected to ground, and adjust the voltage to duplicate the foil deflection from before. Read the voltage. The power-supply voltage is the same as your rug-scuffing body-voltage was.

RUBBED-BALLOON VOLTAGE CALCULATION


I rub a balloon upon my arm hair.  If I know the attraction force and the
capacitance between those flat, plate-like regions of opposite charge,
then I can calculate the voltage.  If the attraction force is 0.1Nt (like
a 10gram weight) and if it is independent of plate-separation (because the
plates are closely spaced,) and if the spacing of the "capacitor plates" 
is initially 1mm (0.001meter), then it took an amount of energy equalling
(Force*distance)  to pull the attractive plates apart to 1mm, and the
stored energy is .1Nt * .001meter = 1e-4 Joules.  For the given attractive
force between the plates, we see that 100 microjoules of electrical energy
is stored by this capacitor. 

OK so far?  Now, what is the capacitance of two capacitor plates spaced
1mm apart and having the size of that typical contact area between the
balloon and my forearm?  Let's say the area is 4cm by 15cm, or .04*.15 =
.006 square meters.  The equation for parallel plate capacitors (plates
spaced very close) is Capacitance = k*area/spacing, where k=8.9e-12 and
lengths are in meters, so the capacitance of the balloon/arm capacitor at
a 1mm gap is 53.4pf.

An actual 4cm x 15cm foil-plate capacitor with a  paper-stack dielectric
measures 95pf on my capacitor meter, which is in the ballpark.  We should
expect it to be higher than our 53.4pF above, since it has a paper
dielectric, not air. 

The energy stored was 100 microjoules, so the voltage can be had by
U=1/2CV^2, or V=sqrt(2*U/C) (U is the stored energy.)  I get an answer of
1920 volts.  At 1mm spacing, the voltage is already almost 2,000 volts!

I also get a total charge of each imbalanced region which calculates to be
about .1 microcoulomb:  Force * distance = 1/2Q^2/C, or Q = sqrt(2CFd) =
1e-7coulombs.  Capacitor voltage is always V = Q/C, and capacitance varies
inversely with plate-spacing, therefor voltage varies directly with plate
spacing.  Double the plate spacing, and we double the voltage. 

   plate spacing  V(capacitor)
     1mm             1920v
     5mm             9600v      V = (1e-7)*D/(.006)/(8.9e-12)
     1cm            19200v
     5cm            95800v

WHOA!  100,000 volts at a couple of inches spacing?!!  However, this is
reasonable, since it normally takes a VandeGraaff Generator to make
arm-hair stand up so painfully rigid.  In the gap between the balloon and
my arm-hair, we have electric field strength which is easily the same as
the field strength at the surface of the sphere of a VDG machine.  Also,
the capacitor equation stops working correctly as we exceed about 1cm,
when the plate spacing becomes large in comparison to the shortest side
of each plate.  Maybe the voltage at 5cm is really only 50,000
volts.  Only!!!!!!!

The capacitor voltage varies as the square-root of the attraction force,
so what would happen if theis force was smaller?  If the attraction
between my arm and the balloon was only 0.01Nt (1 gram weight), then the
voltage would start at 606V at 1mm, and to up to 6060V at 1cm.  Not as
huge, but still pretty impressive.

Created and maintained by Bill Beaty. Mail me at: billb@eskimo.com.
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