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6.1.2.
Atomic Theory <CJ chap 30 >
6.1.2.1.
Discussion
6.1.2.1.1.
The
Thompson model of the atom held that positive charge was spread out like a
pudding.
6.1.2.1.2.
In
1911 Rutherford scattered a particles from gold foil and showed the nuclear size
was ~1E-15m
6.1.2.1.3.
This
raised the problem of why the electron did not spiral into the center with
infinite radiation
6.1.2.1.4.
Atomic
spectra was observed at discrete frequencies rather than continuous emissions
6.1.2.1.4.1.
This implied discrete orbits for the
electron but what equations would make this work
6.1.2.1.5.
In
1913 Bohr proposed his model of the atom with quantized orbits and discrete
transitions
6.1.2.1.6.
The
Bohr model assumes that angular momentum is quantized.
6.1.2.1.7.
The
Pauli exclusion principle prevents two electrons from being in the same shell
simultaneously
6.1.2.1.8.
Einstein
predicted that if an excited atom is hit with a photon of the decaying energy
then ..
6.1.2.1.8.1.
rather than being absorbed, the
photon will stimulate the emission of another photon in phase
6.1.2.1.8.2.
This principle is the basis for the
operation of a laser
6.1.2.1.8.3.
LASER means Light Amplification by
Stimulated Emission of Radiation
6.1.2.1.9.
X
Rays were discovered by Wilhelm Roentgen by hitting electrons on a metal target
6.1.2.2.
Mathematical
6.1.2.2.1.
Atomic
spectra was observed to obey: 1/l = R(1/n12 – 1/n22) with terminology of:
6.1.2.2.1.1.
n1 = 1 Lyman series , n1 = 2, Balmer series, n1 = 3 Paschen series …
6.1.2.2.1.2.
Bohr’s model of quantized orbits
assumed a quantized angular momentum of Ln=n
h/(2p), n= 1,2
6.1.2.2.1.2.1.
This
assumption in addition to the classical equations gave workable orbits:
6.1.2.2.1.2.2.
One
balances Coulomb force with centripetal force: mv2/r = kZe2/r where Z=# protons
6.1.2.2.1.2.3.
Using
these two equations, the radius must be rn =
h2 n2 / (4p2kme2Z) =5.29E-11 n2/Z
6.1.2.2.1.2.4.
The
electron’s energy is KE+PE = E = (1/2) mv2 –kZe2/r
6.1.2.2.1.2.5.
Thus En = 2p2mk2e4/h2)(Z2/n2) = -13.6 eV Z2/n2 = -2.18E-18 J Z2/n2
6.1.2.2.1.2.5.1.
Note that the factor 13.6 eV is the
ionization energy of hydrogen (Z=1 & n=1)
6.1.2.2.1.2.6.
Since
1/l = f/c = E/hc then 1/l = 2p2mk2e4/(ch3)
(Z2/n2)
6.1.2.2.1.3.
De Broglie: If the electron ‘wave’
had to meet constructively with itself then Cir. = 2pr = n l = n h/p
6.1.2.2.1.3.1.
Consequently
we get quantized angular momentum as r p = L = n (h/ 2p)
6.1.2.2.2.
The
Schrödinger equation solution to the hydrogen atom gives the following energy
levels:
6.1.2.2.2.1.
The principle quantum number, n = 1,
2, 3, …..
6.1.2.2.2.1.1.
The
principle quantum numbers 1, 2, 3,..are denoted by the shell names: K, L,
M
6.1.2.2.2.2.
The orbital angular momentum l has the values 0, 1, 2, 3, … (n-1) where L = ((l( l+1))1/2)h/2p
6.1.2.2.2.2.1.
The
orbital angular quantum numbers 0, 1, 2, ..are denoted by the letters s, p, d,
f, g, h,
6.1.2.2.2.3.
There is also a ‘magnetic quantum
number’ that has the values – l,
- l+1, … l-1, l
6.1.2.2.2.3.1.
The
magnetic quantum number was seen when levels were split with a magnetic field
6.1.2.2.2.3.2.
It
is known to correspond to the z component of the angular momentum Lz
6.1.2.2.2.4.
A final splitting of the energy
levels occurred due to the z component of the spin of the electron
6.1.2.2.2.5.
The associated counting of levels
now exactly counts for the number of electrons in each orbit
6.1.2.2.2.5.1.
The
maximum number of electrons in a shell are 2(2 l+1)
6.1.2.2.2.5.2.
The
denotation of electrons in a shell is say: 2p5 thus n=2, l =1, and with 5 electrons
6.1.2.2.2.5.3.
Thus
the configuration of Carbon (6 electrons) is 1s2 2s2 2p2
6.1.2.2.3.
Pauli
Exclusion Principle: No two identical fermions can occupy the same state at the
same time
6.1.2.2.3.1.
A Fermion is an elementary particle with
a spin of ½, 3/2, 5/2, 7/2, … times h/(2p)
6.1.2.2.3.1.1.
Electrons,
protons, neutrons, neutrinos, muons, … are all Fermions
6.1.2.2.3.2.
A Boson is an elementary particle
with a spin of 0, 1, 2, 3, … times
h/(2p) e.g. a photon, pion…
6.1.2.2.3.2.1.
Bosons
actually ‘prefer’ to be in the same state rather than being prevented
6.1.2.2.3.3.
Without the exclusion principle, all
electrons would go to the atoms lowest state & not fill shells
6.1.2.2.3.3.1.
Then
without a tendency to fill shells, there would be no chemical bonding, & no
biology
6.1.2.2.3.3.2.
6.1.2.3.
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