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2.2 1 Atomic Spectra

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Atomic Spectra
Evidence for electron arrangement

Types of spectra
The entire range of colours
or wavelengths/frequencies
are present.
Only specific colours/lines or
wavelengths/frequencies are
present.
Specific colours or
wavelengths/frequencies are
missing.
Flame tests
 Comment on the colours of the flames when different
substances are heated in a Bunsen flame.



Do different substances burn with different coloured
flames?
What is the species in the substances that is responsible
for the colours?
Are the flames characteristic of these species?
 What causes the flames to have these colours?
 What inference can you make regarding atomic structure
from the observations through the spectroscope?
 http://webmineral.com/help/FlameTest.shtml
Dalton’s atom
Thomson’s atom
Rutherford’s atom
Bohr’s atom
How did Bohr figure it out?
 Based on observations from atomic spectroscopy.
 White light consists of electromagnetic radiation of a
specific range of frequencies.
 When an atomic sample is vaporised and heated, it
emits light of a certain colour that can be analysed for
the frequencies it contains using an atomic
spectrometer.
 This emitted light contains only specific frequencies
which appear as bright lines in an emission line
spectrum.
What do we know about light?
 Light is a form of electromagnetic radiation.
 Electromagnetic radiation is energy travelling in
waves.
 A wave is described by its frequency (υ) and its
wavelength (λ).
 They are related by λ = c/υ where c is the speed of
light (3.00 x 108 m s-1).
Wavelength and frequency
C = λν problems….
Work out υ:
 If λ is 3.00 m
 If λ is 30.0 cm
 If λ is 3.00 mm
Work out λ:
 If ν is 2.1 s-1
c = 3.00x108 m s-1
Electromagnetic Spectrum
Energy of a wave
 We can consider light to be not just a wave, but also
a particle.
 Hence, light can be emitted or absorbed in packets
or quanta of energy (called photons).
 The energy of a light photon is given by E = hυ
where h is the Planck constant (6.63 x 10-34 J s).
From ground to excited state
Hydrogen atom spectra
decreasing energy
E = hυ = hc/λ
Bohr’s atomic model
 Niels Bohr, in 1913, proposed a model of an atom
that helped to explain the observations. As spectra
of large multi-electron atoms are very complex and
difficult to interpret, Bohr used the spectra of
hydrogen to develop his model. He stated that
 Electrons can only occupy fixed energy levels; each
energy level being assigned a principal quantum
number. The energy level closest to the nucleus
being n = 1 and of lowest energy.
 The energy of an electron is quantised; the electron
may only have certain energies.
Bohr’s atomic model
 Electrons can only absorb or emit energy of specific
frequencies.
 When the electron occupies the energy level of
lowest energy the atom is said to be in its ground
state. An atom can have only one ground state.
 If the electron occupies one of the higher energy
levels then the atom is in an excited state. An atom
has many excited states.
spectral lines get closer at higher
energies/higher frequencies/shorter
wavelengths because energy gaps between
successive higher energy levels get closer.
increasing frequency / energy
The Electronic Configuration of Atoms
 The structure of the atom is pictured as consisting
of a positively charged nucleus surrounded by
negatively charged electrons.
 The protons and neutrons are tightly packed
together in the tiny nucleus.
The Electronic Configuration of Atoms
 The electrons move rapidly and orbit round the
nucleus, held by electrostatic forces of attraction.
The strength of the attractive force of the nucleus
on the electrons is known as the nuclear charge
and depends on the number of protons in the
nucleus.
 The electrons are found at relatively great distances
away from the nucleus in clearly defined regions
called electron shells that have specific energies
(energy levels).
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