Maximum number of electrons that can fill a subshell
2l2 + 2
Electron falls from n = 4 to n = 1
A photon is emitted
Electron moves from n = 2 to n = 6
Greatest gain in energy
Electron configuration illustrating Hund's rule
Filling orbitals with unpaired electrons first
Percent composition of hydrogen isotopes
99.2% H, 0.8% D
Electron configuration 1s22s22p63s23p64s13d5
Represents Cr and Mn+
Isotopes
Atoms of the same element with varying mass numbers
Isotopes of hydrogen
Protium (1 proton, 1 neutron)
Deuterium (1 proton, 2 neutrons)
Tritium (1 proton, 3 neutrons)
Atomic number (Z)
Number of protons
Mass number (A)
Number of protons + number of neutrons
In a neutral atom, the number of protons equals the number of electrons
Electrons are not included in mass calculations because they are much smaller
Atomic mass
Nearly equal to the mass number (sum of protons and neutrons)
Atomic weight
Weighted average of naturally occurring isotopes of an element
There are no atoms with a mass exactly equal to the atomic weight of an element
Mole
A number of "things" (atoms, ions, molecules) equal to Avogadro's number (6.02 x 10^23)
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)
Rutherford provided experimental evidence that an atom has a dense, positively charged nucleus
Planck developed the first quantum theory, proposing that energy emitted as electromagnetic radiation comes in discrete bundles called quanta
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
Bohr used the work of Rutherford and Planck to develop his model of the electronic structure of the hydrogen atom
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
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
The energy of an electron increases (becomes less negative) the farther out from the nucleus it is located (increasing n)
Ground state
The state of lowest energy, in which all electrons are in the lowest energy levels
Quantized energy
Similar to the change in gravitational potential energy when ascending or descending a flight of stairs
Staircase
Only allows certain discrete (quantized) changes of potential energy, unlike a ramp which allows an infinite number of steps
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
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
Ground state (n = 1)
The orbit with the smallest, lowest-energy radius
Excited state
When the electron is promoted to an orbit with a larger radius (higher energy)
Bohr's Nobel Prize-winning model was reconsidered over the next two decades but remains an important conceptualization of atomicbehavior
We now know that electrons are not restricted to specific pathways, but tend to be localized in certain regions of space
Atomic emission spectrum
Composed of light at specified frequencies, where each line corresponds to a specific electron transition
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
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
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)
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
The wavelengths of absorption correspond exactly to the wavelengths of emission because the difference in energy between levels remains unchanged