Modern Chemistry Chapter 4 Arrangement of Electrons in Atoms Sections 1-3 The Development of a New...
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Transcript of Modern Chemistry Chapter 4 Arrangement of Electrons in Atoms Sections 1-3 The Development of a New...
![Page 1: Modern Chemistry Chapter 4 Arrangement of Electrons in Atoms Sections 1-3 The Development of a New Atomic Model The Quantum Model of the Atom Electron.](https://reader035.fdocuments.us/reader035/viewer/2022062305/5697bfec1a28abf838cb8381/html5/thumbnails/1.jpg)
Modern ChemistryChapter 4
Arrangement of Electrons
in AtomsSections 1-3
The Development of a New Atomic ModelThe Quantum Model of the Atom
Electron Configurations
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Section 1
The Development of a New Atomic
Model
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Sect
ion 1
Voca
bula
ry Electromagnetic radiationElectromagnetic spectrumWavelengthFrequencyPhotoelectric effectQuantumPhotonGround StateExcited stateLine-emission spectrumContinuous spectrum
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Properties of Light• Electromagnetic Radiation: a form
of energy that exhibits wavelike behavior as it travels through space.
• Wavelength: the distance between corresponding points on adjacent waves
• Frequency: the number of waves that pass a given point in a specific time.
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Properties of a Wave:Properties of a Wave:
• Amplitude – is the height of the wave Amplitude – is the height of the wave measured from the origin to its crest.measured from the origin to its crest.– The brightness or intensity of the light The brightness or intensity of the light
depends on the amplitude.depends on the amplitude.
– The greater the amplitude, the brighter the The greater the amplitude, the brighter the light.light.
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Wavele
ngth
an
d F
requ
en
cy Im
ag
e
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Electromagnetic Spectrum Image
p. 9
8
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Ele
ctro
mag
neti
c S
pect
rum
Im
ag
e
p. 9
8
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Properties of Light• wavelength x frequency = speed of light
• x = c• Visible Light = R O Y G B I V
Long
Low Low E
Short
High High E
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The Photoelectric Effect • Max Planck proposed that energy is
proportional to the frequency of the electromagnetic wave.
• Electromagnetic energy is emitted from objects in small packages called quanta.
• E = h •Planck’s constant
–h = 6.626 x 10-34 J•sec
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Light as ParticlesLight as Particles
• QuantizedQuantized ContinuousContinuous
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Quanit
izati
on o
f En
erg
y
Anim
ati
on
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The Photoelectric Effect • Albert Einstein expanded on
Planck’s idea.• Electromagnetic radiation has a
dual wave-particle nature.• A particle of light is a photon.• Photon: a particle of
electromagnetic radiation having zero mass and carrying a quantum of energy.
• Ephoton = h
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En
erg
y o
f a P
hoto
n A
nim
ati
on
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The Photoelectric Effect• The
photoelectric effect refers to the emission of electrons from a metal when light shines on the metal.
p. 9
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Photo
ele
ctri
c E
ffect
An
imait
on
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The Photoelectric Effect To knock an electron loose,it must be hit with a photon whichpossesses a minimum amount of energy.This energy corresponds to its frequency.Different metals hold electrons
more or less tightlySo different metals require
different frequencies to show the photoelectric effect.
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The H-Atom’s Line Emission Spectrum
• Electric current is passed through a vacuum tube with hydrogen in it.
• A glow is produced• When shined
through a prism a line emission spectrum is produced
p. 1
01
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Abso
rpti
on a
nd
Em
issi
on
S
pect
rum
An
imati
on
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Bohr Model of the Atom • Niels Bohr proposed orbits for the
electrons• Each orbit has a fixed energy• Lower energy orbits are closer to
the nucleus• Between orbits the
electron cannot exist
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Explaining the Line Emission Spectrum An electron absorbs a specific amount of
energy (absorption) and moves from its ground state to an excited state
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Explaining the Line Emission Spectrum The electron returns to its ground
state and emits a photon (emission).
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Explaining the Line Emission Spectrum This photon has an energy corresponding to
the difference between the two states.This photon has a specific E, , and color.
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Photo
n E
mis
sion
and
Ab
sorp
tion
Im
ag
e
p. 1
02
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Bohr Model of the Atom • Bohr’s calculated values for the
lines agreed with the values observed for the lines in each series.
• However, it did not explain the spectraof atoms with more thanone electron.
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Bohr
Mod
el of
the A
tom
A
nim
ati
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Bohr and Einstein