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EMR info

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Continuous spectrum: shows all colors ... the e-'-s are free to move around the nucleus ... red hot metal, or fireworks. Also...life after Einstein and ... – PowerPoint PPT presentation

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Title: EMR info


1
EMR info
0
Waves, light, and energy Where chemistry and
physics collide
http//imagers.gsfc.nasa.gov/ems/waves3.html
2
0
First things first Waves
a and b represent wavelength (?)- the distance of
a wave from crest to successive crest measured
in meters
http//www.lbl.gov/MicroWorlds/ALSTool/EMSpec/EMSp
ec.html
3
Waves amplitude
0
  • The height of a wave from crest to midline or
    trough to midline measured in meters

4
Terms you need to know
0
  • Wavelength (?)
  • Amplitude
  • Frequency (v I know some of you have used f,
    move on and get with chemistry!)
  • the number of cycles per second
  • measured in cycles per second (s-1) or Hz (Hertz)
  • Propagation of electromagnetic waves

5
0
http//www.lbl.gov/MicroWorlds/ALSTool/EMSpec/EMSp
ec2.html
6
0
http//micro.magnet.fsu.edu/primer/lightandcolor/i
mages/electromagneticfigure1.jpg
7
0
http//lepus.physics.ualr.edu/tahall/EXAM2/emspec
.jpg
8
0
http//www.arpansa.gov.au/images/emsline2.gif
9
Visible Light
0
  • color wavelength(Å) f(1014 Hz) Energy
    (10-19 J)
  • Violet 4000---4600 7.5--6.5 5.0--4.3
  • Indigo 4600---4750 6.5--6.3 4.3--4.2
  • Blue 4750---4900 6.3--6.1 4.2--4.1
  • Green 4900---5650 6.1--5.3 4.1--3.5
  • Yellow 5650---5750 5.3--5.2 3.5--3.45
  • Orange 5750---6000 5.2--5.0 3.45--3.3
  • Red 6000---8000 5.0--3.7 3.3--2.5

10
Some equations you need to know
0
  • ? c / v
  • and
  • E hv
  • So.
  • E hc / ?
  • And
  • ? h / mv
  • When
  • ? wavelength in m
  • c speed of light, 3.00E8 m/s
  • v frequency in Hz
  • (cycles/sec or s-1 or 1/s)
  • E energy in J
  • h Planks constant, 6.626E-34 Js
    Joule(seconds)
  • m mass of particle in kg

11
What the h? Plancks Constant
0
  • When metals are heated, they glow
  • 1800s- physicists were trying to determine the
    relationship between the color (wavelength) and
    intensity of the glow
  • Max Planck (1900)- energy can be released or
    absorbed only in little chunks (packets) of
    energy of some minimal size

12
Max Planck and the h
0
  • The chunks of energy were dubbed quantum
    (fixed amount), which is the smallest amount
    that can be emitted or absorbed as EMR.
  • Proposed E hv
  • The energy (E) of a single quantum is equal to
    its frequency (v) times a constant

13
Planck and the Nobel (Physics)
0
  • Planck determined that h 6.626E-34 J-s
  • Energy is always released in multiples of hv
    (1hv, 2hv, 3hv, etc)
  • h is so small that we cannot see the effects of
    this in our daily lives
  • Analogous to
  • Planck won the 1918 Nobel Prize in physics for
    his work

14
Einstein Bohr Perfect Together
0
Einstein (or Mr., Read, you decide), left Bohr,
above
15
EinsteinThe Photoelectric Effect
0
  • Einstein discovered that one could cause
    electrons to be ejected from the surface of a
    metal if the energy of the light wave was strong
    enough
  • He treated the light needed to do this as a piece
    of matter- a photon, if you will
  • This ejection of e- is the photoelectric effect

16
The Photoelectric Effect
0
  • Only light of a certain energy could knock off an
    electron from the metal
  • Intense light of a weaker wavelength would not
    work, but even a low intensity of the correct
    wavelength would work
  • (the energy of the light is transferred to the
    kinetic energy of the electron)
  • Hmmm light acting as a particle and as a wave..

17
The photoelectric effect
0
  • http//www.lewport.wnyric.org/mgagnon/Photoelectri
    c_Effect/photoelectriceffect1.htm
  • http//www.xmission.com/locutus/applets/Photoelec
    tric.html

18
Getting to Bohr.
0
  • Light of a given wavelength is monochromatic (one
    color)
  • Most common EMR sources are polychromatic, but we
    see only one color
  • These can be reduced to a spectrum when the
    different wavelengths are separated out

19
Spectral Emissions
0
  • Continuous spectrum shows all colors of the
    rainbow

20
0
  • Bright line spectrum only certain wavelengths
    are visible (the rest do not appear at all)
  • Different elements have different bright line
    spectrum when they are heated
  • Na is yellow
  • Ne is orange-red

21
Line spectrum
0
  • Ne
  • I2

22
0
http//www.cartage.org.lb/en/themes/Sciences/Astro
nomy/Modenastronomy/Interactionoflight/AtomicAbsor
ption/AtomicAbsorption.htm
23
Hydrogen Spectra
0
Emission Spectra
Absorption Spectra
http//www.mhhe.com/physsci/astronomy/applets/Bohr
/content_files/section1.html
24
0
http//www.cartage.org.lb/en/themes/Sciences/Astro
nomy/Modenastronomy/Interactionoflight/AtomicAbsor
ption/AtomicAbsorption.htm
25
0
26
0
  • Line spectra formation- go to..
  • http//www.mhhe.com/physsci/chemistry/essentialch
    emistry/flash/linesp16.swf

27
Bohr Model and Spectral Emissions
0
  • Bohr proposed that the emission of light energy
    from an (electrically or thermally) excited atom
    corresponds to the orbit of the electron around
    the nucleus of the atom
  • That energy can only be achieved by being a
    specific distance from the nucleus

28
What youve seen so far.
0
Model of a Nitrogen (z7) atom
29
Bohr Model and moving electrons
0
  • http//www.colorado.edu/physics/2000/quantumzone/b
    ohr.html

30
Energy levels- Bohr Model
0
  • Electrons travel within set energy levels that
    have a particular energy associated with each
    level
  • After all, the e-s are moving around the nucleus
  • think KE here
  • Each shell has a number
  • Closest to the nucleus is n1
  • For each successive level add 1 to n
  • n2, n3, ect.

31
Energy increases as the distance from the nucleus
increases
0
32
Bohr Model and moving electrons
0
  • http//www.colorado.edu/physics/2000/quantumzone/b
    ohr.html

33
Electron config in energy level
0
34
SO
0
  • We know that the e--s are free to move around
    the nucleus
  • They also can move from one energy level to the
    next (and fall) back when energy is added
  • Move from ground state (home level) to a higher
    level (the excited state)
  • Returning back to the ground state releases energy

35
0
  • This emission is how we see colors
  • the wavelengths of EMR released from an atom when
    it has been excited by
  • Heat energy
  • Electrical energy
  • Chemical energy
  • Think glowing red hot metal, or fireworks

36
Alsolife after Einstein and Bohr
0
  • We know that electrons have characteristics of
    both light (waves) and matter, so we say that
    they have a dual nature

37
De Broglie
0
  • De Broglie proposed that an electron moving about
    the nucleus had a wave-like behavior, so that
    they it has a particular wavelength associated
    with it. This wavelength depends upon the mass
    and velocity of the electron.
  • ? h / mv
  • mv the momentum of the particle

38
0
  • This matter-wave idea applies to all matter, not
    just to electrons
  • However, the mass is so large, and the wavelength
    so small, that we cannot see it in macroscale
    objects
  • This matter-wave theory led to applications like
    the electron microscope

39
De Broglie wavelength
0
40
HeisenbergThe Uncertainty Principle
0
  • We cant determine information about small scale
    objects the same way we can for large scale
    objects
  • Case in point a ball rolling down a ramp- we can
    get position, direction, and speed at the same
    time
  • We cant for electrons
  • Hence, the uncertainty principle

41
Heisenberg, contd
0
  • It is inherently impossible for us to
    simultaneously know both the exact momentum and
    exact location of an electron
  • This is because anything we do to determine the
    location or momentum of the electron moves it
    from its original path and location this cant
    be reduced past a certain minimal level
  • We can know only momentum or location- not both
  • We can talk probability of the location/ momentum
    of an electron

42
Which brings us to this question
0
  • What the heck does all of this have to do with
    electron configuration and how matter behaves?
  • On to electron configuration, courtesy of
    Schrödinger and company (enter math that well
    skip)
  • Quantum theory

43
EMR and the atom Part Deux
0
Electron Configurations
http//imagers.gsfc.nasa.gov/ems/waves3.html
44
What youve seen so far.
0
Model of a Nitrogen (z7) atom
45
Which is really not true- why?
  • Because orbitals- the electron cloud are
  • 3-D
  • are not round in all most cases
  • e- spread out as much as possible.

46
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47
The s orbital
http//www.sfu.ca/nbranda/28xweb/images/s_orbital
.gif
48
p orbitals
49
d orbitals
50
d orbitals
51
f orbitals
52
General tutorials for electron configuration stuff
  • some slides in this PowerPoint are from this site
    already
  • http//www.wwnorton.com/chemistry/overview/ch3.htm
  • See key equations and concepts (select from menu
    on the left), as well as the looking through the
    overview where to the tutorials are listed (links
    for just those are on the left, too)

53
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54
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55
Quantum numbers
56
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