ELECTROSTATICS
NEWSLETTER
November/December 2000 No.153
PRESIDENT’S MESSAGE
For the last several years, I've worked in the field
of micro-electromechanical systems, or "MEMS". Many of these tiny silicon micro-devices
rely on electrostatic forces to initiate mechanical motion. I entered this field after having been asked
to join a Boston University MEMS team of mechanical, manufacturing, and systems
engineers as the "electrostatics expert." The experience of working with this multidisciplinary team has
confirmed one of my long-held suspicions: Issues from one person's field are
often left as "exercises to the reader" by individuals from an
another field. For example, as a
die-hard electrical engineer I sometimes find myself modeling a 32-part
mechanical structure as a simple mass and restoring spring. Conversely, my colleagues usually model a
complex electrode structure as two "parallel capacitor plates." Similarly, I've often been asked by
coworkers to "just build some circuit" that can produce 1 kV at 10 mA
from a 9-V battery.
One common misconception that I hear often from
mechanical engineers is the notion that applying "two" voltages of
"opposite" polarity to two conductors will cause them to attract one
another, while applying "two" voltages of the same polarity will
cause the conductors to repel. This
faulty conclusion, of course, results from watching too many science museum
demonstrations involving charged, insulated ping-pong balls. As our electrostatics fundamentals tell us,
when two conductors are held at different fixed potentials (i.e., separated by
a single voltage difference,) the force between them will vary as the square of
the applied voltage. The force will be
unrelated to the polarity either conductor relative to ground and will always
be attractive. I've spent many hours
trying to convince my non-EE colleagues (and even one EE who is a systems type)
that it's impossible to get two conductors held at fixed potentials to
repel. The counter argument that I
often hear cites the example of the traditional foil-leaf electrometer, in
which two pieces of conducting foil are suspended from a conducting rod inside
a
sealed jar.
Applying voltage or charge to the rod causes the two foils, which are
electrically connected, to repel.
Hopefully you saw this demonstration in some science class or museum
exhibit. If you think
about the problem, you quickly realize that,
although the two foils do indeed
separate when charge or voltage is applied to the rod, the force cannot be
repulsive. The two foils are at the
same potential, hence the electric field between them must be zero, because an
electric field can only extend from a region of higher potential to a region of
lower potential. The foils separate due
to the attractive forces exerted between the charged foils and the outside
world -- charges of opposite polarity induced on either the surface of the
glass or on other conductors outside of the jar. (We usually think of glass as
being an insulator, but glass actually has a small surface conductivity due to
adsorbed moisture.)
These debates on the topic of electrostatic
repulsion of conductors have been stimulating, and they have reminded me of a
fascinating dialog what went on among the aging alumni of the MIT EPSEL lab
(all
former students of Profs. James Melcher and Gerald Wilson.)
The topic concerned two parallel metal plates held at different potentials and
immersed in a dielectric liquid. As is
well known, applying a voltage between the plates will cause the liquid to rise
between them. If a hole were punched in
one plate above the liquid level, could the system be used as a pump? (The
final conclusion, still not accepted by all who participated, was that the
structure will not act as a pump. Perhaps we can publish the friendly but
heated e-mail exchanges at a future date.)
These two discussion threads are reminiscent of the
countless poignant discussions that have taken place during the breaks and
mealtimes of our annual ESA meetings.
Many of us find these informal exchanges to be just as valuable learning
experiences as the formal talks and papers.
In the spirit of these exchanges, I'd like to start (or restart) a
tradition of including "food for thought" questions in the bi-monthly
ESA Newsletter. If you are inclined to
offer input, send it to me at mnh@bu.edu
and I'll start a discussion thread.
We can publish some of the more interesting discussions in subsequent
issues of the Newsletter. Similarly, if
you have a food-for-thought question that you’d like to pose, send it along as
well.
Discussion Question of the Month:
As noted above, two conductors held at different
potentials will always experience an attractive force. When one of the conductors is held at
constant charge rather than constant potential, a repulsive force can be
obtained. Under what conditions, if
any, can two conductors under constrained voltages be made to repel one
another?
One possibility has been suggested: Ground conductor #1 through a resistor of
value R. If conductor #1 has
capacitance C relative to conductor #2, then its charging time constant will be
RC. If a voltage
having combined ac and dc components is applied to
conductor #2, the dc voltage component will induce a fixed charge on conductor
#1, causing an attractive force between the conductors. If the frequency of the ac voltage is much
higher than 1/RC, the ac voltage will not induce any additional charge on
conductor #1, hence the charge on conductor #1 will remain at the value induced
by the dc voltage. Will the force
component associated with the ac voltage be alternately attractive and
repulsive,
or will it be only attractive?
By the way, the entries from last month's
President's Message attributable to James Clerk Maxwell: A Treatise on
Electricity and Magnetism, 1873 were numbers (3) and (6).
For the Friendly Society,
Mark Horenstein
ESA President
ELECTRIC FENCES AND GRASSHOPPERS
The Associated Press recently reported on a forest
fire in Washington State which was blamed on a grasshopper landing on an
electric fence. Let’s think about this
in two ways. First, is it
electrostatics (in the sense most of us use)?
And, second, is this story really credible?
An electric fence puts out brief pulses of high
voltage. There is certainly a motion of
charge, and a small current exists. But
everything important relates to charges and the electric fence. Surely magnetic fields are unimportant in
the operation of electric fences. So --
I would answer, yes -- this is an example of electrostatics. Compare it in your mind with electrostatic
spray painting or flocking or xerography.
And second is it credible? A grasshopper could alight on a fence wire and feel nothing. But it could span the distance between wire
and a close weed, to be electrocuted.
Could that start a fire? Do any
of our readers use electric fences?
Have you ever seen anything ignited?
Does anyone have accurate information on the energies involved?
And a related postscript. Do copy machines occasionally ignite dust or a sheet of paper?
Glenn Schmieg
RECHARGEABLE BATTERIES
In the November issue of Popular Science, there is
an interesting article about a potential breakthrough in rechargeable
batteries. It reminded me of a
presentation I made at our ESA conference back in June '81, in which I presented
my thoughts on what I called "Electrostatics, the Subtle Force". One of the items I speculated on was the
remote possibility of using capacitors to store energy for driving our cars. I suggested that a tankful of gasoline
(enough to drive a car about 300 miles) stored 2.1 x 109 Joules of
energy. Since gasoline engines are only
about 25% as efficient as electric motors, we could drive the same 300 miles on
5.2 x l08 joules of stored electrical energy. I recall computing the size of a capacitor
capable of storing that much energy, and I showed an overhead sketch of a 1 ton
car carrying 16 tons of capacitors on its roof. . . . Hardly a practical
solution to give us clean, efficient automobiles. That led me to think about the plain old electrochemical battery
as an extremely compact capacitor, in which my 3 mil mylar film capacitors are
replaced by positive and negative charges separated by molecular distances,
instead. The one advantage of
conventional capacitors, however, is that they can be charged, discharged, and
recharged quickly and indefinitely.
Rechargeable batteries require up to 8 hours or more for recharging, and
can be recycled only several hundred times, at most.
The breakthrough the Popular Science article
describes is a 12 volt "proton polymer battery" that is being
developed by Japan's NEC Corporation.
In this battery, the current is carried by protons and electrons,
instead of complex molecules of conventional rechargeable batteries,
substantially increasing its speed of charging and discharging, and causing
less degradation of the electrodes than the electrochemical reactions of
conventional batteries. Reportedly, it
can be recharged in about 5 minutes and is projected to last for tens of
thousands of cycles. And it is capable
of delivering much more power in a shorter period of time. NEC is showing its battery to other
manufacturers, but no date nor any certainty of production was announced.
This would not only make battery driven automobiles
more attractive, but its ability to deliver power in short pulses would also
make it applicable to "Bluetooth" short range radio technology,
wirelessly linking of notebook PC's, mobile phones, and even wirelessly
"patchcording" our VCR's, TV's, and CD players and recorders
together.
If this proves viable, future batteries may be more
like electrostatic capacitors than we had imagined.
Bob
Gundlach
STATIC ELECTRIC FIELDS AND QUANTUM GRAVITY
To couple these terms together seems like quite a
stretch. And, like most of our members,
my interests
certainly lie on the side of electrostatics. But connections in research over many
decades offer surprises. Let’s follow a
trail from A. D. Moore up to the most modern abstract research in string
theory.
In the 1930’s and beyond, A. D. was working with
industrial people who needed solutions to complicated electric field
problems. These problems had complex
boundaries, not the simple ”plane and sphere” of textbooks. He worked hard on a mathematical method
called curvilinear squares and an analog method called fluid mapping. Both of these have disappeared with the
coming of fast numerical iterations of Laplace’s equation on a computer. But don’t forget fluid mapping yet.
Spreading water between two parallel sheets of glass
allows flow patterns, and if the sheets are close together, say one millimeter
separation, these patterns satisfy Laplace’s equation. When A. D. first told me about this, and showed
me some wonderful flow patterns in his laboratory, he said there was some early
work by H. Hele-Shaw.
Now just lately, Hele-Shaw flow has been connected
with a set of abstract integrals. And
these in turn connected with another set of equations in quantum gravity!
It sounds bizarre, but the next progress made in
electrostatics could affect progress in quantum gravity (or vice versa). Now that’s something to think about.
Glenn
Schmieg
THANKS TO PROFESSOR KAZUTOSHI ASANO
The following letter was sent to Professor Asano by
Mark Horenstein on September 25, 2000.
Dear
“Kazie”
On
behalf of the ESA I want to thank you for the wonderful hospitality extended to
us by the membership of IEJ at our recent Joint Symposium in
Kyoto. The technical sessions were well
organized,
the food was great, and, as always, we enjoyed renewing friendships with our colleagues
and acquaintances. Although attendance
from ESA this year was smaller than we had expected, those who were
fortunate to attend found the conference stimulating and very enjoyable. We all felt that the meeting was a great
success.
I
hope that we can continue the tradition of hosting a joint conference every
other year. We would like to
invite the IEJ to the USA in 2002 in a city still to be determined. As soon as we have made
plans for a specific site that is convenient for travel from Japan, I will let
you know. May the long
relationship between ESA and IEJ continue.
Sincerely
yours,
Mark
Horenstein
ESA WEB SITE
Apologies for the long delay in updating the ESA Web
site at www.electrostatics.org. The
work schedule of the Webmaster has been daunting for the past two months,
leaving little time for webmastering.
For those of you who have submitted requests for links or e-mail address
additions, rest assured that they should be added to the Web site by the time
you receive this newsletter in the mail.
Did you know that you now can apply for ESA
membership over the Web? In the future,
we also hope to arrange for a method to pay for ESA conferences and other items
via credit card over the Web using a third party carrier. Stay tuned for more details.
WELCOME NEW ESA MEMBERS
Kevin Haynes Ries
Van Twisk
Anthony Dalla Villa James R. Reppermund
Gabriel Laryea
JOURNAL OF ELECTROSTATICS
Are you having trouble with your subscription to the
Journal of Electrostatics paid for via the ESA? Several members have contacted me with problems over unreceived
issues despite the cashing of their
checks.
These difficulties can be attributed to start up transients. Rest assured that payments for any
unreceived issues will carry over to next year. No one's subscription fees will disappear into the ether.
If you are having difficulty with your subscription
(or if your issues are regularly appearing,) we'd like to know that. Send an
e-mail to mnh@bu.edu.
ESA 2001 ANNUAL CONFERENCE
Plans continue for our 2001 Annual Conference at
Michigan State University from June 27-30.
Many thanks to Marty Kashef of Delsys Pharmaceutical Corp. for
volunteering to be Local Host Chair. Volunteers are still needed for various
odd jobs, including on-site registration, tour organizing, and outreach
mailings. Contact ESA President Mark
Horenstein (mnh@bu.edu; 617-353-5437) if you'd like to volunteer. Remember, the ESA has no paid employees
(that's why are dues remain so unreasonably low) and runs solely by the efforts
of its members.
WOULD YOU CONSIDER HAWAII?
In thinking about sites for future Electrostatics
Society of America/Institute of Electrostatics Japan joint meetings, would you
consider going to a meeting in Hawaii?
Some discussion occurred at the recent
IEJ/ESA meeting in Kyoto about choosing a compromise
site as a way of increasing overall attendance from both sides. Would you go to Hawaii if our regular
meeting were held there? Would you go if a separate meeting, held in addition
to our usual June meeting, were to be held?
Please share your thoughts with any of the ESA officers or Executive
Council members.