1/105
Looks like no tags are added yet.
Name | Mastery | Learn | Test | Matching | Spaced | Call with Kai |
|---|
No study sessions yet.
protons
in the nucleus
+1
mass of 1 amu
atomic number (Z)
number of protons found in an atom of that element
identifier of each element (at top of each square in periodic table)
neutrons
no charge
mass is slightly larger than 1 amu
mass number (A)
sum of the protons and neutrons in the atom’s nucleus
isotopes
atoms that share an atomic number (same element) but have different mass numbers
same # of protons, different # of neutrons
bc they have the same number of protons and electrons, they generally exhibit similar chemical properties
atomic weight
weighted average of all naturally occurring isotopes (at bottom of each square in periodic table)
electrons
move through the space surrounding the nucleus
varying levels of energy
-1
negligible mass
which is greater?
the electrostatic force of attraction between the unlike charges of the proton or electron
OR
the gravitational force of attraction based on their respective masses?
the electrostatic force of attraction between the unlike charges of the proton or electron is far greater
because subatomic particles’ masses are so small
the electrons closer to the nucleus are at (higher/lower?) energy levels?
lower energy levels
the electrons further away from the nucleus (in higher shells) have (higher/lower?) energy
higher energy
valence electrons
electrons that are farthest from the nucleus
strongest interactions with the surrounding environment
weakest interactions with the nucleus
much more likely to become involved in bonds with other atoms
why are valence electrons much more likely to become involved in bonds with other atoms?
they experience the least electrostatic pull from their own nucleus
sharing or transferring of valence electrons in bonds allows elements to…
fill their highest energy level to increase stability
cation
positively charged atom
anion
negatively charged atom
atomic mass of an atom (in amu)
nearly equal to its mass number
the sum of protons and neutrons
isotopes of hydrogen
protium
deuterium
tritium
protium
isotope of hydrogen
1 proton
mass=1 amu
deuterium
isotope of hydrogen
1 proton
1 neutron
mass=2 amu
tritium
isotope of hydrogen
1 proton
2 neutrons
mass=3 amu
half life indicates what?
stability
helps determine relative proportions of different isotopes
when an element has two or more isotopes, what does that mean in terms of mass and atomic weight?
when an element has two or more isotopes, no one isotope will have a mass exactly equal to the element’s atomic weight
utility of atomic weight
represents mass of the “average” atom of that element in amu
represents the mass of one mole of the element in grams
Avogadro’s number
6.02×1023
mole
number of “things” (atoms, ions, molecules) equal to Avogadro’s number
Rutherford
in 1910, Ernest Rutherford provided experimental evidence that an atom has a dense, positively charged nucleus that accounts for only a small portion of the atom’s volume
Planck
in 1921 Max Planck developed the first quantum theory, proposing:
energy emitted as electromagnetic radiation from matter comes in distinct bundles called quanta
how is the energy of a quantum calculated?
Planck reaction:
E=hf
Planck reaction
E=hf
where:
h= Planck’s constant
f (sometimes written as v)= frequency of the radiation
Planck’s constant (h)
6.626×10-34 J*s
Bohr’s idea
hydrogen atom consists of a central proton around which an e- travels in a circular orbit
centripetal force acting on the e- as it revolves around the nucleus is created by electrostatic force between p+ and e-
Bohr angular momentum equation
L = nh/2π
where:
n=principal quantum number (any + integer)
h=Planck’s constant
angular momentum changes how?
angular momentum of an electron changes only in discrete amounts with respect to the principal quantum number
because the only variable is the principal quantum number
Bohr energy of electron equation
E = -(RH)/(n2)
Rydberg unit of energy (RH)
2.18×10-18 J/electron
how does the energy of the electron change?
the energy of the electron changes in discrete amounts with respect to the quantum number
Bohr’s description of the structure of a 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
ground state
state of lowest energy, in which all electrons are in the lowest possible orbitals
excited state
at least one electron has moved to a subshell of higher than normal energy
how is Bohr’s model incorrect?
electrons are not restricted to specific pathways, but tend to be localized in certain regions of space
mnemonic: as electrons go from a lower → higher energy level, they get AHED
Absorb light
Higher potential
Excited
Distant (from the nucleus)
electromagnetic energy of photons equation
E = hc/λ
h=Planck’s constant
c= speed of light in a vacuum (3.00×108 m/s)
λ= wavelength of radiation
line spectrum
spectrum is composed of light at specified frequencies
each line on the emission spectrum corresponds to a specific electron transition
atomic emission spectrum
because each element can have its electrons excited to a different set of distinct energy levels, each possesses a unique atomic emission spectrum, which can be used as a fingerprint for the element
Lyman series
the group of hydrogen emission lines corresponding to transitions from energy levels n≥2 → n=1
Balmer series
the group of hydrogen emission lines corresponding to transitions from energy levels n≥3 → n=2
includes 4 wavelengths in the visible spectrum
compare Lyman series and Balmer series
Lyman series (n≥2 → n=1) includes larger energy transitions than the Balmer series (n≥3 → n=2)
so Lyman series has shorter photon wavelengths in the UV region of the electromagnetic spectrum
Paschen series
corresponds to transitions from n≥2 → n=3
how does energy relate to wavelength?
energy is inversely proportional to wavelength
E = hf = hc/λ
which equation shows that:
the energy associated with a change in the principal quantum number from a higher initial value (ni) to a lower final value (nf)
=
the energy of the photon
E = hc/λ = -RH [(1/ni2) - (1/nf2)]
the energy of the emitted photon corresponds to the difference in energy between the higher-energy initial state and the lower-energy final state
positive E value corresponds to:
emission
negative E value corresponds to:
absorption
ΔE for absorption or emission between any two energy levels is:
ΔE for absorption or emission between any two energy levels is the same according to the conservation of energy
this is also the same as the energy of the photon of light absorbed or emitted
absorption spectrum
every element possesses a characteristic absorption spectrum
exciting the electrons of a particular element results in energy absorption at specific wavelengths
wavelengths of absorption correspond exactly to the wavelengths of emission bc the difference in energy levels is the same
orbitals
electrons move rapidly and are localized within regions of space around the nucleus called orbitals
Heisenberg uncertainty principle
it is impossible to simultaneously determine, with perfect accuracy, the momentum and the position of an electron
Pauli exclusion principle
no two electrons in a given atom can possess the same set of four quantum numbers
energy state
the position and energy of an electron described by its quantum numbers
principal quantum number: n
quantum number used in Bohr’s model that can theoretically take on any positive integer value
shell #
size and energy of atomic orbital
the larger the integer value of n, the higher the:
higher energy level
larger radius of e-’s shell
equation for max # of e-s within a shell
2n2
the difference in energy between two shells [increases/decreases?]
as the distance from the nucleus [increases/decreases?]
difference in energy between two shells decreases as the distance from the nucleus increases
because the energy difference is a function of [1/ni2 - 1/nf2]
azimuthal (angular momentum) quantum number: l
refers to the shape and number of subshells within a given principal energy level (shell)
how does the value of n limit the value of l
for any given value of n, the range of possible values for l is 0→(n-1)
if l=0
s
if l=1
p
if l=2
d
if l=3
f
spectroscopic notation
l=0 →s
l=1 →p
l=2 →d
l=3 →f
max # of e-s within a subshell equation
4l + 2
magnetic quantum number: ml
specifies the particular orbital within a subshell where an electron is most likely to be found at a given moment in time
possible values are integers between -l and +l, including 0
each orbital can hold a max of how many e-s?
2
the shape of the orbital is dependent on what?
the subshell in which they are found
shape of orbitals in the s subshell
spherical
shape of orbitals in the p subshell
dumbbell shaped
align along the x-, y-, and z- axes (px, py, pz)
probability density
the likelihood that an e- will be found in a particular region of space
the shapes of orbitals are defined in terms of probability density
the s block contains how many elements?
2 elements in each row of the periodic table
the p block contains how many elements?
6 groups of elements
the d block contains how many elements?
10
the f block contains how many elements?
14
spin quantum number: ms
electron has two spin orientations designated +1/2 and -1/2
paired electrons
whenever two e-s are in the same orbital, they must have opposite spins
in this case they are paired
parallel spins
electrons in different orbitals with the same ms values
electron configuration
for a given atom or ion, the pattern by which subshells are filled, as well as the number of e-s within each principal energy level and subshell are designated by its electron configuration
first number is principal energy level
letter is subshell
subscript gives number of e-s in that subshell
Aufbau principle
electrons fill from lower to higher energy subshells
each subshell will fill completely before electrons begin to enter the next one
n + l rule
the lower the sum of the values of the 1st and 2nd quantum #s, n+l, the lower the energy of the subshell
if two subshells have the same n+l value, the one with the lower n value has lower energy (and will fill with e-s first)
lower energy fill up first
lowest s subshell
1s
lowest p subshell
2p
lowest d subshell
3d
lowest f subshell
4f
Hund’s rule
within a given subshell, orbitals are filled such that there are a maximum number of half-filled orbitals with parallel spins
this is true in subshells that contain more than one orbital
the basis for this is electron repulsion
electron repulsion
electrons in the same orbital tend to be closer to each other and thus repel each other more than electrons placed in different orbitals
half-filled and fully filled orbitals have [higher/lower?] energies than other states
lower energies
meaning higher stability
important exceptions to electron configuration
chromium (and other elements in its group)
copper (and other elements in its group)
why is chromium (and other elements in its group) an exception to electron configuration?
chromium (Z=24) should be [Ar]4s23d4 according to the rules
BUT moving 1 e- from 4s→3d allows the 3d subshell to be half filled: [Ar]4s13d5
extra stability from making 3d half filled outweighs the cost of it being energetically unfavorable
why is copper (and other elements in its group) an exception to electron configuration?
copper (Z=29) has the electron configuration: [Ar]4s13d10 instead of [Ar]4s23d9
full d subshell outweighs the cost of moving an e- out of the 4s subshell
in which subshell does the extra stability of the shift NOT outweigh the cost?
p subshell
paramagnetic
materials composed of atoms with unpaired electrons will orient their spins in alignment with a magnetic field
the material will thus be attracted to the magnetic
paramagnetic = magnetic field will cause parallel spins in unpaired e-s and cause attraction
diamagnetic
materials consisting of atoms that have only paired electrons will be slightly repelled by a magnetic field
given sufficiently strong magnetic fields beneath an object, any diamagnetic substance can be made to levitate
allotrope
configuration