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General Physics (PHY 2140)

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Title: General Physics (PHY 2140)


1
General Physics (PHY 2140)
Lecture 34
  • Modern Physics
  • Atomic Physics
  • De Broglie wavelength in the atom
  • Quantum mechanics

http//www.physics.wayne.edu/apetrov/PHY2140/
Chapter 28
2
Lightning Review
  • Last lecture
  • Atomic physics
  • Bohrs model of atom

Review Problem Suppose that the electron in the
hydrogen atom obeyed classical rather then
quantum mechanics. Why should such an atom emit
a continuous rather then discrete spectrum?
3
Recall Bohrs Assumptions
  • Only certain electron orbits are stable.
    Radiation is emitted by the atom when the
    electron jumps from a more energetic initial
    state to a lower state
  • The size of the allowed electron orbits is
    determined by a condition imposed on the
    electrons orbital angular momentum

Why is that?
4
Modifications of the Bohr Theory Elliptical
Orbits
  • Sommerfeld extended the results to include
    elliptical orbits
  • Retained the principle quantum number, n
  • Added the orbital quantum number, l
  • l ranges from 0 to n-1 in integer steps
  • All states with the same principle quantum number
    are said to form a shell
  • The states with given values of n and l are said
    to form a subshell

5
Modifications of the Bohr Theory Zeeman Effect
and fine structure
  • Another modification was needed to account for
    the Zeeman effect
  • The Zeeman effect is the splitting of spectral
    lines in a strong magnetic field
  • This indicates that the energy of an electron is
    slightly modified when the atom is immersed in a
    magnetic field
  • A new quantum number, m l, called the orbital
    magnetic quantum number, had to be introduced
  • m l can vary from - l to l in integer steps
  • High resolution spectrometers show that spectral
    lines are, in fact, two very closely spaced
    lines, even in the absence of a magnetic field
  • This splitting is called fine structure
  • Another quantum number, ms, called the spin
    magnetic quantum number, was introduced to
    explain the fine structure

6
28.5 de Broglie Waves
  • One of Bohrs postulates was the angular momentum
    of the electron is quantized, but there was no
    explanation why the restriction occurred
  • de Broglie assumed that the electron orbit would
    be stable only if it contained an integral number
    of electron wavelengths

7
de Broglie Waves in the Hydrogen Atom
  • In this example, three complete wavelengths are
    contained in the circumference of the orbit
  • In general, the circumference must equal some
    integer number of wavelengths
  • but , so

This was the first convincing argument that the
wave nature of matter was at the heart of the
behavior of atomic systems
8
In an analysis relating Bohr's theory to the de
Broglie wavelength of electrons, when an electron
moves from the n 1 level to the n 3 level,
the circumference of its orbit becomes 9 times
greater. This occurs because (a) there are 3
times as many wavelengths in the new orbit, (b)
there are 3 times as many wavelengths and each
wavelength is 3 times as long, (c) the wavelength
of the electron becomes 9 times as long, or (d)
the electron is moving 9 times as fast.
QUICK QUIZ 1
(b). The circumference of the orbit is n times
the de Broglie wavelength (2pr n?), so there
are three times as many wavelengths in the n 3
level as in the n 1 level.
9
28.6 Quantum Mechanics and the Hydrogen Atom
  • One of the first great achievements of quantum
    mechanics was the solution of the wave equation
    for the hydrogen atom
  • The significance of quantum mechanics is that the
    quantum numbers and the restrictions placed on
    their values arise directly from the mathematics
    and not from any assumptions made to make the
    theory agree with experiments

10
Problem wavelength of the electron
Determine the wavelength of an electron in the
third excited orbit of the hydrogen atom, with n
4.
11
Determine the wavelength of an electron in the
third excited orbit of the hydrogen atom, with n
4.
Recall that de Broglies wavelength of electron
depends on its momentum, l h/(mev). Let us find
it,
Given n 4 Find le ?
Recall that
Thus,
12
Quantum Number Summary
  • The values of n can increase from 1 in integer
    steps
  • The values of l can range from 0 to n-1 in
    integer steps
  • The values of m l can range from -l to l in
    integer steps

13
How many possible orbital states are there for
(a) the n 3 level of hydrogen? (b) the n 4
level?
QUICK QUIZ 2
The quantum numbers associated with orbital
states are n, ?, and m . For a specified value of
n, the allowed values of ? range from 0 to n 1.
For each value of ?, there are (2 ? 1) possible
values of m?. (a) If n 3, then ? 0, 1, or
2. The number of possible orbital states is then
2(0) 1 2(1) 1 2(2) 1 1 3 5
9. (b) If n 4, one additional value of ? is
allowed (? 3) so the number of possible orbital
states is now 9 2(3) 1 9 7 16
14
Spin Magnetic Quantum Number
  • It is convenient to think of the electron as
    spinning on its axis
  • The electron is not physically spinning
  • There are two directions for the spin
  • Spin up, ms ½
  • Spin down, ms -½
  • There is a slight energy difference between the
    two spins and this accounts for the Zeeman effect

15
Electron Clouds
  • The graph shows the solution to the wave equation
    for hydrogen in the ground state
  • The curve peaks at the Bohr radius
  • The electron is not confined to a particular
    orbital distance from the nucleus
  • The probability of finding the electron at the
    Bohr radius is a maximum

16
Electron Clouds
  • The wave function for hydrogen in the ground
    state is symmetric
  • The electron can be found in a spherical region
    surrounding the nucleus
  • The result is interpreted by viewing the electron
    as a cloud surrounding the nucleus
  • The densest regions of the cloud represent the
    highest probability for finding the electron

17
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