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Cards (1677)
Quantum number sets
n = 2; l =
1
; ml =
-1
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Maximum number of electrons that can fill a subshell
2l2
+
2
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Electron falls from n = 4 to n = 1
A
photon
is
emitted
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Electron moves from n = 2 to n = 6
Greatest
gain in
energy
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Electron configuration illustrating
Hund's
rule
Filling orbitals with
unpaired
electrons first
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Percent composition of hydrogen isotopes
99.2%
H,
0.8%
D
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Electron configuration
1s22s22p63s23p64s13d5
Represents
Cr
and
Mn+
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Isotopes
Atoms
of the same element with
varying
mass numbers
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Isotopes of hydrogen
Protium
(1 proton, 1 neutron)
Deuterium
(1 proton, 2 neutrons)
Tritium
(1 proton, 3 neutrons)
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Atomic
number (Z)
Number of
protons
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Mass number (A)
Number of
protons
+ number of
neutrons
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In a neutral atom, the number of
protons equals
the number of
electrons
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Electrons
are not included in mass calculations because they are much
smaller
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Atomic mass
Nearly equal to the mass number (sum of
protons
and
neutrons
)
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Atomic weight
Weighted average of naturally occurring
isotopes
of an element
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There are no
atoms
with a mass exactly equal to the
atomic weight
of an element
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Mole
A number of "things" (atoms,
ions
, molecules) equal to
Avogadro's
number (6.02 x 10^23)
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The atomic weight represents both the
mass
of the "average" atom of an
element
(in amu) and the mass of one mole of the element (in grams)
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Rutherford
provided experimental evidence that an atom has a dense, positively charged
nucleus
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Planck developed the first quantum theory, proposing that energy emitted as electromagnetic radiation comes in
discrete
bundles called
quanta
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Planck's relation
E = hf, where E is the
energy
of a quantum, h is Planck's constant, and f is the
frequency
of the radiation
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Bohr used the work of Rutherford and
Planck
to develop his model of the electronic structure of the
hydrogen
atom
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Bohr's postulate on Angular Momentum
L = mvr = nh/2π, where L is angular
momentum
, m is
mass
, v is velocity, r is radius, n is the principal quantum number, and h is Planck's constant
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Bohr's equation for Electron Energy
E = -RH/n^2, where E is the
energy
of the electron, RH is the Rydberg unit of
energy
, and n is the principal quantum number
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The
energy
of an electron
increases
(becomes less negative) the
farther
out from the nucleus it is located (increasing n)
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Ground
state
The state of
lowest
energy, in which all electrons are in the
lowest
energy levels
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Quantized energy
Similar to the change in
gravitational potential energy
when ascending or descending a flight of stairs
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Staircase
Only allows certain
discrete
(quantized) changes of
potential energy
, unlike a ramp which allows an infinite number of steps
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Bohr's model of the hydrogen atom
A nucleus with one
proton
forming a dense core, around which a single electron revolved in a defined pathway (orbit) at a
discrete
energy value
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Electron "jumping" from one orbit to a higher-energy one
Requires an amount of
energy
exactly
equal
to the difference between one orbit and another
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Ground state
(n =
1
)
The orbit with the
smallest
,
lowest-energy
radius
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Excited
state
When the
electron
is promoted to an orbit with a larger radius (
higher
energy)
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Bohr's Nobel Prize-winning model was reconsidered over the next two decades but remains an important
conceptualization
of
atomic
behavior
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We now know that electrons are not restricted to specific pathways, but tend to be
localized
in certain regions of space
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Atomic emission spectrum
Composed of
light
at specified frequencies, where each line corresponds to a specific
electron
transition
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Each element can have its
electrons
excited to a different set of distinct energy levels, and thus possesses a unique atomic emission spectrum, which can be used as a
fingerprint
for the element
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Emissions from electrons dropping from an excited state to a
ground
state give rise to
fluorescence
, and the color of the emitted light is what we see
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Hydrogen emission line series
Lyman
series (transitions from n ≥
2
to n = 1)
Balmer
series (transitions from n ≥
3
to n = 2)
Paschen
series (transitions from n ≥ 4 to n =
3
)
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E = hc/λ
The energy of the emitted photon corresponds to the difference in energy between the higher-energy initial state and the lower-energy final state
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The wavelengths of absorption correspond exactly to the wavelengths of emission because the difference in energy between levels remains
unchanged
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