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On Tue, 25 Dec 2001 22:47:06 -0500 Ludwik Kowalski <kowalskiL@MAIL.MONTCLAIR.EDU>
writes:
> The comments of this thread prompted me to sketch an > introduction to electricity. Is it acceptable? I plan to > distribute it as a handout to students, after performing > standard demonstrations with rods and pith balls. > Ludwik Kowalski ***Most of us will agree that it is VERY MUCH easier to
find errors in a written passage than to actually write
such a passage without any errors. But as long as you asked,
Ludwik, here are some possible errors that come to mind
after a quick reading of your passage....
> Mass m is the mechanical attribute of an object. *** Mass is not the mechanical attribute of an object.
There are other mechanical attributes such as size,
shape, and density.
>It determines how the object accelerates (F=m*a) and
*** It partially determines how an object accelerates
.....
> how it is attracted by another mass (F=G*m*M/d^2).
*** and how moves in an electric or gravitational field.
> The first electric phenomenon discovered was mutual > attraction and mutual repulsion of light objects under > the influence of something which was not mass or > magnet. *** How do you know that this was the "first"
> That something was named charge. A glass
> rod robbed with silk, for example, acquires a property > of repelling another glass rod robbed with silk. *** Whether or not the glass was robbed or purchased
is irrelevant here.
> That property, named charge, was initially modeled as a
fluid.
> An object containing that fluid was said to be electrified. *** What was the date and circumstance of the initial modelling
of the property called charge?
> Likewise, a plastic rod robbed with wool repels
> another plastic rod robbed with wool. But an > electrified glass and an electrified plastic attract, > rather than repel, each other. *** The attraction (or repulsion) of a charged piece of
glass and a charged plastic rod is very tricky. It depends
on the type of plastic, its temperature, and the amount of
rubbing that is done.
> This, and many other,
> observation, and lead to a realization that there are > two kinds of electric fluids, positive and negative. *** In addition to the obvious errors in punctuation and
sentence structure, I wonder if static charges should be called
"electric fluids" at this point.
> The term charge used to be interpreted as the "amount of
> electric fluids" or "amount of electricity" which an > object can acquire or lose. > > A modern interpretation is based on the realization > that submicroscopic particles, protons and electrons, > are permanently charged with positive and negative > electricity. A macroscopic object is charged when the > number of electrons and the number of protons are not > identical. An excess of protons results in a net positive > charge while an excess of electrons results in a net > negative charge. *** Doesn't the above statement conflict with the idea
that the quantity of protons remains fixed within an atom
of glass or rubber. Isn't a negative charge associated
with a surplus of electons surrounding the nucleus and
a positive charge associated with a deficiency of such
electrons?
> The net charge, like the total mass,
> becomes an attribute of an object. It is an attribute > responsible for forces between electrified objects. *** But isn't it true that the the total mass of an
object is much less likely to change than its net charge.
> Two similar charges (both positive or both negative)
> always repel but two dissimilar charges (positive and > negative) always attract. This was the first qualitative > observation about electric forces. *** Is it the "charges" that repel or attract or is it the
"charged objects" that do the repelling and attracting?
> > It turns out that the magnitude of an electric force > between two charges (q1 and q2) is proportional to > the product q1*q2 and inversely proportional to the > square of the distance (d^2) between their centers. This > observation, made by Coulomb, is known of Coulombs > law. It can be written as: > > F = k*q1*q2 / d^2 > > where k is the proportionality constant. The value of > that constant can be chosen arbitrarily in order to > define a unit of electric charge. For the purpose of this > introduction the unit of electric charge, one coulomb, C, > we will defined by declaring that k=1,000,000,000. *** Iszn't it important to state the units (newton-meters
squared over coulombs squared) in the definition of k
here?
> This is equivalent to saying that the electric charge is
one
> coulomb if it attracts or repels an identical charge with > a force of one billion newtons when the distance between > the centers of two charges is one meter. One coulomb is > a very large charge; charges produced on robbed rods > and plates are usually expressed in microcoulombs or in > nanocoulombs. Ignoring sign differences we can say > that the charge of one electron and the charge of one > proton are identical (1.6*10^-19 C). > > The so-called "official" SI definition of the unit of charge > is conceptually different from the one presented above. > But in practical terms it is not at all different. In SI the > ampere, A, is the first unit; *** It would be better to say that the ampere is a defined
in the SI system as a "fundamental" unit rather than
a "first" unit. The terms fundamental and first are not really
synonomous.
> all other electrical units are
> defined in terms of kg, m, s and A. The unit of charge, > coulomb, C, is defined as A*s. In our sequence C is the > first electric unit and A will be defined as C/s. Other > nuances associated with electrical and magnetic SI units > will be discussed later. Note that F in Coulombs law is > positive when two charges repel (q1 and q2 have the > same sign) and negative when they attract (signs of q1 > and q2 are different). I hope that my "***" comments are helpful for your purpose.
Herb Gottlieb from New York City
The home of the infamous ground zero
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