History of the Atom
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Transcript History of the Atom
History of the Atom:
Physics Chapter 27
Early work in Electricity and
Magnetism
Oersted:
Current makes magnetic field
Faraday/Henry:
Magnetic fields moving make currents
Maxwell:
Electricity, magnetism and light are all parts of the
electromagnetic field
Hertz:
Experiments supported Maxwell’s work
James Clerk Maxwell
1831-1879
Showed that electricity and
magnetism were related, and
were related to atoms
Predicted that accelerating
charges would make waves
(electromagnetic radiation)
Cathode Ray Tube Experiments
Glass tube with wire at each end; as much air pumped out as
possible
Charge passed across tube makes fluorescent glow
William Crookes
Tube coated with fluorescent material can be made to glow in
one focused dot
Rays travel in straight lines
Ray carries negative charge
Joseph John Thomson
1856-1940
Used a study of the cathode
ray tube to determine the
presence of electrons 1897
Suggested the plum pudding
model of the atom and the
existance of isotopes
Won the Nobel Prize in
Physics in 1906
J. J. Thomson’s Experiment
Thomson used both a
magnetic field and electric
field to deflect the electrons
He measured the deflection
of the ray and calculated the
charge:mass ratio of
electrons
J. J. Thomson’s Experiment
Used magnetic field to show cathode rays had negative charge
Used electric field to show cathode rays were particles with
negative charge
Used varying electric currents to determine charge to mass
ratio
Force caused by electric field: qE
Force caused by magnetic field: Bqv
When these forces are equal Bqv=qE
Then v = E/B
When electric field removed, particles given centripetal force by
magnetic field Bqv = mv2/r
Solved for mass/charge ratio: m/q = Br/v
Thomson calculated m/q as 5.686 x 10-12 kg/C
Evidence suggested particles very small and came from atom
J. J. Thomson’s experiment
Thomson calculated m/q as 5.686 x 10-12 kg/C
Millikan calculated q = 1.602 x 10-19 C
Can be used to calculate m:
m=(5.686 x 10-12 kg/C) q
m calculated as 9.109 x 10-31 kg
Method can be used for any charged particle
Example
A beam of electrons travels an undeflected path in a cathode
ray tube. E is 7.0 x 103 N/C. B is 3.5 x 10-2 T. What is the
speed of the electrons as they travel through the tube?
What we know:
E = 7.0 x 103 N/C
B=3.5 x 10-2 T
Equation:
v = E/B
Substitute:
v = (7.0 x 103N/A s) / (3.5 x 10-2 N/A m)
Solve!
v = 2.0 x 105 m/s
Example
An electron of mass 9.11 x 10-31 kg moves with a speed of 2.0
x 105 m/s across a magnetic field. The magnetic induction is
8.0 x 10-4 T. What is the radius of the circular path followed by
the electrons while in the field?
What we know:
M = 9.11 x 10-31 kg
B=8.0 x 10-4 T
Equation:
Bqv = mv2/r so r = (mv) / (Bq)
Substitute:
R = (9.11x10-31kg)(2.0x105 m/s)
(8.0x10-4N/Am)(1.6x10-19As)
Solve! r = 1.4 x 10-3 m
v=2.0 x 105 m/s
Robert A. Millikan
1858-1953
Used the 'falling drop method'
to determine the charge of the
electron (-1.6022 x 10-19 C) and
mass of electron as 9.10 x 10-28
g
Investigated photoelectric effect
and spectroscopy of elements
Won the Nobel Prize in Physics
in 1923