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Theory – PASCO ES-9070 COULOMB BALANCE User Manual

Page 6

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Coulomb Balance

012-03760E

2

Theory

Take one gram of protons and place them one meter away

from one gram of electrons. The resulting force is equal to

1.5 x 10

23

newtons—roughly the force it would take to

“lift” an object from the surface of the Earth that had a

mass about 1/5 that of the moon—not a small force.
So, if such small amounts of charge produce such

enormous forces, why does it take a very delicate torsion

balance to measure the force between charged objects in

the laboratory? In a way, the very magnitude of the forces

is half the problem. The other half is that the carriers of the

electrical force—the tiny proton and the even tinier

electron—are so small, and the electrons are so mobile.

Once you separate them, how do you keep them

separated? The negatively charged electrons are not only

drawn toward the positively charged protons; they also

repel each other. Moreover, if there are any free electrons

or ions between the separated charges, these free charges

will move very quickly to reduce the field caused by the

charge separation.
So, since electrons and protons stick together with such

tenacity, only relatively small charge differentials can be

sustained in the laboratory. This is so much the case that,

even though the electrostatic force is more than a billion-

billion-billion-billion times as strong as the gravitational

force, it takes a very delicate torsion balance to measure

the electrical force, whereas we can measure the

gravitational force by weighing an object with a spring

balance.

ä NOTE: The torsion balance gives a direct and

reasonably accurate measurement of the Coulomb

force. The most accurate determinations of

Coulomb's law, however, are indirect. It can be

shown mathematically that if the inverse square law

holds for the electrostatic force, the electric field

inside a uniformly charged sphere must be

everywhere zero. Measurements of the field inside a

charged sphere have shown this to be true with

remarkable accuracy. The Coulomb force can be

expressed by the formula:

F = kq

1

q

2

/R

2+n

.

Using this indirect method, it has been demonstrated

experimentally that n ­ 2 x 10

–16

.