The principal quantum number (n) determines the energy level of an orbital, while the azimuthal quantum number (l) determines the shape or angular momentum of the orbital.
The radiation's energy increases from the radio wave end of the spectrum to the gamma ray end.
Visible light is a very small part of the entire spectrum.
The speed of light, c, is constant.
The energy of a photon, E, is related to the frequency, v, and the wavelength, X, of the radiation as E = hv.
Kinetic energy, KE, is stored in the motion of an object.
Potential energy, PE, is the energy of an object based on its interaction with others, such as gravity or electrostatic interaction.
Gravity is a type of potential energy.
Electrostatic interaction is a type of potential energy.
The unit of energy is the Joule (J).
Different forms of energy can be converted into each other, for example, a calorie (cal) can be converted into 1 Kcal.
An electronvolt (eV) is equal to 1.6 x10-19J.
Total energy is always constant and is conserved in a closed system.
Some observations are inconsistent with the wave picture of light.
Blackbody radiation is the glow emitted by hot, macroscopic objects.
The observed spectrum of blackbody radiation is continuous with a peak who's position depends on temperature (higher temperature = lower wavelength)
The peak position of the observed spectrum depends on temperature, with a higher temperature resulting in a lower wavelength.
Classical theory, which assumes that light is a wave, predicts that there is an infinite amount of low-frequency light shining on metals, also known as "blacklight".
The photoelectic effect, which assumes that light is a particle, predicts that electrons will be emitted when shining light on metals.
Max Planck assumed that energy is quantized: the amount of energy at some higher frequency is always an integer multiple of the fundamental packet size.
Photons, which have energy v = frequency, are emitted when light is a stream of particles, n = planck's constant (6.62x10-3 Js).
Hydrogen gas emits light at specific wavelengths/frequencies/energy.
White light is transmitted through cold hydrogen gas.
Atoms emit light only at specific wavelengths/frequencies/energy.
Atoms absorb light only at the same wavelengths/frequencies/energies.
An atom in a high-energy state can transition to a lower-energy state, and the energy that the atom lost is carried away by an emitted photon.
An atom in a low-energy state can absorb a photon of transition to a higher-energy state if the photon energy matches the difference in atom energies exactly.
A double slit experiment can show a diffraction pattern caused by interference.
Matter also exhibits wave-particle duality.
An object of mass m moving with velocity v behaves like a wave with wavelength x = h/(m xv).
Bohr's Model describes the electron (of the Hydrogen atom and other single-electron atoms) as having charge -1.
In Bohr's Model, the electron moves in circular orbits around the nucleus.
These orbits are stable, because electrostatic and nucleus charge are in balance.
The wavelength of the electron must fit into orbit n times, where n is always an integer or whole number.
Certain orbits, aka certain values of the energy, are allowed.
The energy levels of single-electron atoms are represented by the formula n = 1, 2, 3, ...
Single-electron atoms are referred to as Rydberg atoms.
All energy levels of Rydberg atoms are negative.
The largest space between energy levels of Rydberg atoms is between n = 1 and n = 2.
A transition in Rydberg atoms is a change of state from an initial value ni to a final value ne.