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Hydrogen Atom

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Title: Hydrogen Atom


1
Hydrogen Atom
  • We will examine the simplest atom and describe
    what the wave function tells us about the
    behavior
  • When we solve the Schrodinger Equation in three
    dimensions we find we can only get acceptable
    solutions if some measureable quantities take on
    a series of precise values
  • Other quantities are not precise and have
    undertainties

2
Hydrogen Atom
  • These precisely observable quantities are called
    eigenvalues (proper values)
  • An eigenstate is a set of particular values for
    these observable quantities
  • Each eigenstate is characterized by integer
    numbers quantifying the observable quantities

3
Principle Quantum Number
  • The principle quantum number defines the energy
    of the electron just as in the Bohr theory

4
Orbital Quantum Number
  • The orbital quantum number is related to the
    magnitude of the angular momentum of the
    electron.
  • Classically, Lmvr
  • In quantum mechanics the result is

5
Magnetic Quantum Number
  • It turns out that just as charge is quantized, so
    is space!!! Directions in space are not allowed
    to be in just any old direction
  • The direction of the angular momentum vector
    (think of an orbiting electron as going in a
    circle and the plane of the circle is at right
    angles to the angular momentum) can only take on
    particular values

6
Magnetic Quantum Number
  • These values are described by the magnetic
    quantum number, ml which takes on values from -l
    to l in integer steps

Heres an example for l2.
7
Magnetic Quantum Number
  • This quantum number has the name because when
    atoms are placed in an external magnetic field,
    the spectra shows that the energy levels are
    modified slightly and depend on this orientation
  • This is called the Zeeman Effect
  • Since an electron with angular momentum must have
    some circular component it will be a rotating
    current and will generate a magnetic field which
    interacts with the external field

8
Magnetic Quantum Number
In a magnetic field, the electrons energy
depends on the value of ml. The result is that a
single spectral line is now becomes many lines
depending on the value of the magnetic quantum
number!
9
Spin Quantum Number
  • The solution to the Schrodinger Equation doesnt
    make any predictions about spin
  • However, if you calculate the speed of the
    electron in the ground state (n0) you find that
    it is about 2 x 106 m/s and special relativity
    needs to be considered

10
Spin Quantum Number
  • P.A.M. Dirac had to rewrite the Schrodinger
    Equation (which cannot work for relativity) to
    make it agree with Einstein
  • Miraculously, the solutions turned out to predict
    some additional angular momentum for the electron
    which could take on only two values,

11
Spin Quantum Number
  • Careful examination of spectra indeed showed this
    fine structure splitting of spectral lines which
    exactly agreed with Diracs prediction
  • It is called electron spin, which implies a
    particle spinning on its axis
  • But we know that a particle picture is silly, so
    we just deal with the angular momentum
  • The quantum number is or - 1/2 (spin up or spin
    down)

12
The Whole Picture
  • So the electron in a hydrogen atom is described
    by four quantum numbers
  • These are n, l, ml, and ms
  • They are related in that some are limited by the
    size of others
  • Best displayed in a table

13
The Whole Picture
14
The Whole Picture
  • Energy determined by n
  • Orientation and angular momentum determined by
    the other three
  • In more complex atoms, some dependence of energy
    on the others due to magnetic interactions
    between the various magnetic fields

15
Spectra and Selection Rules
  • It turns out that a photon also has angular
    momentum of h-bar
  • That means that to conserve angular momentum,
    when an electron changes states, it must change
    its angular momentum by one unit of h-bar so
  • This is called a selection rule

16
Pauli Esclusion Principle
  • Look at more complex atoms with multiple
    electrons
  • The Bohr model failed badly
  • Solutions to the Schrodinger equation (must be
    done numerically) predict the correct energy
    levels for the same quantum numbers as for
    hydrogen
  • The electrons interact with each other which
    complicates things enormously

17
Pauli Exclusion Principle
  • It quickly became apparent that a new principle
    was needed to explain the states of electrons in
    multi-electron atoms
  • No two electrons ever had the same quantum
    numbers at the same time in any individual atom
  • This is the Pauli Exclusion Principle
  • It turns out to have a deeper meaning
  • This provides for the chemical properties which
    appear in the periodic table

18
Periodic Table
  • States are occupied by electrons in increasing
    order of energy
  • For He, n1, l0, ml0, ms or - 1/2
  • For Li, the next electron must have n2
  • Build the whole table this way
  • Explains why we have shells and subshells

19
Periodic Table
20
X-Ray Spectra
  • Visible, UV and IR spectra deal with transitions
    between outer electrons
  • If we take a complex atom and kick out an inner
    shell electron, lots of energy involved
  • If an electron goes from far away and falls into
    a vacant inner shell, high energy photon is
    released
  • This is an x-ray, so x-ray spectra ought to give
    information about inner energy levels

21
X-Ray Spectra
The lines depend on the element. The continuous
part is due to bremsstrahlung or braking
radiation due to decelerating electrons striking
the target. The left side cutoff is where all
the energy of the electron goes into a photon.
22
X-Ray Spectra
The lines depend on the element. The continuous
part is due to bremsstrahlung or braking
radiation due to decelerating electrons striking
the targe. The left side cutoff is where all the
energy of the electron goes into a photon.
23
Fluorescence
  • Excite an electron in an atom or molecule to a
    higher energy state
  • If there is an intermediate state between where
    the electron is and where it came from, it can
    lose energy by emitting a photon and going to
    that intermediate state
  • From there it can decay again into the starting
    state

24
Fluorescence
25
Phosphorescence
  • The intermediate state is metastable
  • This means it has a much longer lifetime which
    may extend to minutes or even hours
  • Long delay in emitting the second photon
  • Both fluorescence and phosphorescence can be used
    to identify atoms or molecules

26
Lasers
  • Give off coherent light
  • Means all the light rays have the same phase
  • Again, metastable states of atoms are involved

27
Lasers
Absorption of Light
Stimulated Emission of Light
28
Lasers
  • Need a population inversion

29
Lasers
30
Ruby Laser
Using Chromium Atoms in Ruby
31
He-Ne Laser
32
CD-ROM
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