Title: Atomic Physics
1Atomic Physics
2Atomic Models
3Introduction
4- Our main focus will be on the hydrogen atom.
- It is the simplestatomic system.
5- Why is it important to study the hydrogen atom?
- Studying the quantum numbers for the allowed
states of hydrogen will help us to describe the
allowed states of more complex atoms. - The hydrogen atom is an ideal system for relating
theory to experimentation. - Much that we learn about hydrogen can be extended
to single electron ions like He and Li.
6Early Models Of The Atom
- The Greek model
- Tiny, hard, indestructible sphere
- 3
7- The J. J. Thomson model
- A volume of positive charge is embedded with
negative charges called electrons
8- The Rutherford model
- A positive nucleus orbited by electrons.
- The nucleus contains 99.9 of the atoms mass
9- The Rutherford model
- Which force holds the electrons in orbit?
- The Coulomb force
10Problems with the Rutherford Model
- There were two basic difficulties with the
Rutherford model. - It could not explain why atoms radiate discrete
frequencies. - Accelerating electrons should radiate
electromagnetic waves.
11Electron Transitions
- Using a high voltage to move electrons through a
gas causes the gas electrons to become excited
and to jump from lower energy levels to higher
energy levels. - Photons of various wavelengths are produced when
electrons fall from higher energy levels to lower
energy levels.
12Emission Spectra
- The emission spectrum of hydrogen
- Can be produced by applying a high voltage across
an evacuated glass tube filled with hydrogen - The observed wavelengths are characteristic only
of hydrogen - 279, 57
13The Balmer Series
- In the Balmer Series
- nf 2
- There are four prominent wavelengths
- 656.3 nm (red)
- 486.1 nm (green)
- 434.1 nm (purple)
- 410.2 nm (deep violet)
- 278, 28.7
14Balmer Wavelengths
15The Balmer Series Wavelength Equation
- RH is the Rydberg constant
-
- RH 1.0973732 x 107 m-1
16Two Other Important Series
- Lyman series (UV)
- nf 1
- Paschen series (IR)
- nf 3
- 70
17Spectral Lines
- How many different spectral lines could be
produced by an electron in the n 3 state? - Three
18- How many different spectral lines could be
produced by an electron in the n 4 state? - Six
19Photon Energy
- The equation for determining the energy of the
emitted photon in any series
20The Absorption Spectrum
- An element can absorb the same wavelengths that
it emits. - The spectrum consists of a series of dark lines.
21Identifying Elements
- The absorption spectrum was used to identify
elements in the solar atmosphere were identified
in this way. - Helium was discovered.
22Thermal vs. Atomic Spectra
- How could you tell if the light from a candle
flame is thermal or atomic in origin?
23- If the spectrum is continuous, the source must be
thermal.
24Auroras
- What is the origin of the colors in the aurora
borealis?
25- High speed particles from space interact with the
earths magnetic field.
26The Bohr Theory Of Hydrogen
- At the beginning of the 20th century, scientists
wondered why atoms only radiated certain
wavelengths. - Bohr provided an explanation.
27Four Assumptions of The Bohr Theory
- 1) The electron orbits the proton due to the
- Coulomb force which produces centripetal
- acceleration.
28- 2) Only certain electron orbits are stable
- and do not radiate energy.
29- 3) Radiation is only emitted when an
- electron drops from a more energetic
- state to a lower state.
30- 4) The radius of the electrons orbit is
- determined by the electrons orbital
- angular momentum.
- 28.6
31Total Energy of the Hydrogen Atom
- The total energy of the hydrogen atom can be
determined by using this equation.
32The Bohr Radius
- An electron can exist only in certain allowed
orbits determined by the integer n. - When n 1, we have what is known as the Bohr
radius (ao). - ao 0.0529 nm
33Orbital Radii
- A general equation for finding the radius of any
orbit
34Energy States
- The energy for various energy states can be found
by using - n 1 is the ground state
35Ionization Energy
- The minimum energy required to ionize the atom is
called the ionization energy. - An electron is completely removed from the atom.
36The Hydrogen Spectrum
- The general expression for determining
wavelengths of the various series in the hydrogen
spectrum
37Bohrs Correspondence Principle
- Quantum mechanics is in agreement with classical
physics when the energy differences between
quantized levels are very small.
38Successes of the Bohr Theory
- It accounted for the Balmer series and other
series.
39- It predicted a value for the Rydberg constant
that agreed strongly with the experimental value.
40- It gave an expression for the radius of the
hydrogen atom.
41- It predicted the energy levels of hydrogen.
42- It also works with hydrogen-like (one electron)
atoms. - Singly ionized helium
43- It also works with hydrogen-like (one electron)
atoms. - Doubly ionized lithium
44- It also works with hydrogen-like (one electron)
atoms. - Triply ionized beryllium
45Four Quantum Numbers
- The state of an electron is specified by four
quantum numbers. - These numbers describe all possible electron
states. - The total number of electrons in a particular
energy level is given by
46Principle Quantum Number
- The principal quantum number (n) where n 1, 2,
3, - Determines the energy of the allowed states of
hydrogen - States with the same principal quantum number are
said to form a shell - K, L, M, (n 1, 2, 3, )
47Orbital Quantum Number
- The orbital quantum number (l) where l ranges
from 0 to (n 1) in integral steps - Allows multiple orbits within the same energy
level - Determines the shape of the orbits
- States with given values of n and l are called
subshells - s (l 0), p (l 1), d (l 2), f (l 3), etc
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50Electron Subshells
51- Generally, the electrons in the s subshell are at
the lowest energy level and those in the f
subshell in the highest shell occupy the highest
energy level.
52- As the shell number (n) increases the energy
difference between the shells diminishes, as
shown by the decreasing distance between each
successive shell.
53Electron Subshells
54Magnetic Quantum Number
- The magnetic quantum number (ml) where ml ranges
from - l to l in integral steps - Explains why strong magnetic fields can cause
single spectral lines to split into several
closely spaced lines - Called the Zeeman effect
55Spin Magnetic Quantum Number
- The spin magnetic quantum number (ms) where ms
can only be 0.5 or 0.5 - Accounts for the fine structure of single
spectral lines in the absence of a magnetic field
56Hydrogen Like Atoms
- Two important equations for hydrogen-like atoms
- Orbital energy
- Orbital radius
57Angular Momentum
- Physicists agreed that angular momentum was
quantized but no one was able to explain why. - 28.10
58Electron Standing Waves
- de Broglie stated that an electron orbit would be
stable if it contained an integral number of
electron wavelengths. - Analogous to standing waves in a string
59Wave Properties
- It became generally agreed upon that wave
properties were involved in the behavior of
atomic systems.
60Quantum Mechanics And The Hydrogen Atom
- A review of the various quantum number ranges
which are used to determine allowable states - n can range from 1 to infinity in integral steps
- l can range from 0 to (n - 1) in integral steps
- ml can range from l to l in integral steps
- ms can only be ½ or ½
61The Spin Magnetic Quantum Number
- The spin magnetic quantum number explains the
splitting of each energy level into two (the
Zeeman Effect). - It explains how two very closely spaced lines may
be formed in the spectra of certain gases. - Electron spin (spin-up and spin-down)
62Questions
63Electron Clouds
- The electron may be found at various distances
from the nucleus but the probability of finding
it at a distance corresponding to the first Bohr
orbit is a maximum. - It can be found in a spherical region known as
the electron cloud. - 281, 282
64The State of an Electron
- The state of an electron is specified by four
quantum numbers. - These numbers describe all possible electron
states. - The total number of electrons in a particular
energy level is given by
65The Pauli Exclusion Principle
- Two electrons in an atom can never have the same
set of quantum numbers. - Because of this, the elements all have different
chemical properties. - The n 1 energy level is filled with electrons
first.
66The Pauli Exclusion Principle And The Periodic
Table
- Mendeleev arranged the elements in a periodic
table according to their atomic masses and
chemical similarities. - He left gaps which were filled in within the next
20 years. - Vertical columns have similar chemical
properties. - 15
67The Periodic Table
68Special Groups Within the Periodic Table
- Noble gases
- The outer shell is filled.
- Alkali metals
- The outer shell has only one electron.
- Halogens
- The outer shell needs one electron.
69The Dow Corning Periodic Table
70X-Rays
- X-rays are emitted when a metal target is
bombarded with high-energy electrons to produce - A broad continuous band
- Bremsstrahlung
- Characteristic x-rays
- K??and K?
- 284, 285
71X-Ray Photons
- What can the incoming electron from an electron
gun do to a K-shell electron in a tungsten target
atom? - It can knock a K-shell electron out of its energy
level. Then, an electron from a higher energy
level can fall into the K-shell (n 1). - The energy lost by the falling electron shows up
as an emitted x-ray photon.
72Characteristic X-Rays
- K-shell emission produces higher-intensity x-rays
than Bremsstrahlung. - The x-ray photon comes out at a single
(characteristic) wavelength. - K??or K?
73Ka X-Rays
- When an incoming electron forces an electron out
of the K shell an electron can drop down from the
n 2 level and a Ka x-ray photon is emitted.
74Kb X-Rays
- When an incoming electron forces an electron out
of the K shell an electron can drop down from the
n 3 level and aKb x-ray photon is emitted.
75- Which x-ray photon has the highest energy?
76Ka X-Ray Wavelengths
- The wavelength of the emitted Ka x-ray
photon is given by
77Electron Shielding
- One electron in the K shell partially shields the
other from the charge of the nucleus. - Because of this, we use Zeff (Z - 1) in the Ka
equation.
78K? X-Ray Wavelengths
- The wavelength of the emitted K? x-ray
photon is given by
79Electron Shielding
- One electron in the K shell and eight electrons
in the L shell partially shield the M-shell
electrons from the charge of the nucleus. - Because of this, we use Zeff (Z - 9) in the K?
equation.
80Atomic Transitions
- Atoms will only emit or absorb EM radiation at
certain frequencies corresponding to transitions
involving the various energy states.
81Stimulated Absorption
- In the stimulated absorption process, light may
be used to stimulate electrons to higher excited
states. - Only certain frequencies will do this.
- 28.17
82Spontaneous Emission
- When the electrons randomly fall back to their
original orbits we call this spontaneous
emission. - 286
83Spontaneous Emission
84Stimulated Emission
- In stimulated emission, all of the electrons can
be made to fall back at the same time and thus
produce bright, coherent light. - This is the basis for the operation of LASERS.
85Stimulated Emission
86Lasers
- LASER - Light Amplification by Stimulated
Emission of Radiation
87Population Inversion
- In a laser, electrons are stimulated so that
there are more electrons in the excited state
than in the ground state. - This is called a population inversion.
- 287
88Laser Requirements
- There are three conditions for laser action to
occur. - A population inversion
- The excited state must be a metastable (long
lifetime) state. - The photons must be confined long enough to
stimulate further emissions.
89He-Ne Lasers
- The operation of a He-Ne laser
- An oscillator is used to sweep electrons through
a thin glass tube containing a He-Ne mixture. - The neon atoms are raised to a metastable state
by collisions with excited helium atoms. - Electrons simultaneously returning to a lower
energy state emit coherent photons of a
particular wavelength. (632.8 nm) - 28.22a, 71, 288
90Laser Frequencies
- Frequency ranges of lasers
- Infrared (CO2)
- Visible (red, green, blue)
- Ultraviolet
91Laser Applications
- Medical
- Welding detached retinas
- Laser surgery
- Laser vision correction (Lasik)
92Lasik Surgery
- An ultra-thin flap is created on the eye's
surface during LASIK corrective eye surgery.
After laser energy is applied to reshape the eye,
the flap is replaced to serve as a type of
natural bandage.
93- Surveying and distance measurement
94- Cutting and drilling metals in industry
95- Fiber optic communications
96Holography
- Used in the production of three-dimensional
images - Interference patterns are placed on film.
- Used to protect credit cards
- 283, 284
97Making Holograms
98CDs and DVDs
- Information is stored in binary form.
- Pits and land areas (ones and zeros)
- The laser beam follows a spiral path.
- A diffraction grating is used to provide
tracking. - 40 second memory for music CDs
99Infrared Remote Control
- A different infrared wavelength is assigned to
each number or function. - TV and stereo remote controls use IR.
- Some computers and calculators use IR.
- My MAC PowerPoint remote uses RF.
- Dont confuse IR with RF controls.
- MAC Photo Booth Demo
100Semiconductor Devices
- Doping
- Donor atoms
- N-type semiconductor
- Acceptor atoms
- P-type semiconductors
101Semiconductor Devices
- P-N junctions
- Diodes
- Forward bias
- Reverse bias
- Half-wave rectifiers
- Full-wave rectifiers
- Transistors
102Transistors
- Junction transistors
- Types
- npn
- pnp
- Parts of a transistor
- Emitter
- Base
- Collector
- 227
103Semiconductor Devices
- Integrated circuits
- What are they?
- Where are they used?
- What are the advantages of integrated circuits?
104Computer Memory
105Questions