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electromagnetic radiation
forms of energy
electromagnetic spectrum
range of the frequencies of electromagnetic radiation
Maxwell's theory of the properties of light
radiation can travel through space (or a transparent medium) on two perpendicular axes: the magnetic field and electric field
Wavelength (λ)
the distance between two wave crests
Frequency (∨)
the number of crests that pass by a stationary point per second
all forms of radiation
travel at the speed of light (c), 2.998 * 10⁸ m/s
the relationship between wavelength and frequency is
inverse, λ = c/v
atomic emission spectra
element spectra, each element emits a characteristic spectrum
atomic absorption spectra
narrow dark lines on a continuous spectrum. Dark lines are in the same position as the emission spectra colored lines
Blackbody radiators
something that perplexed physicist because of its ability to absorb all light at cold temperatures, as well as emitting radiation dependent on temperature alone (i.e. temp = frequency)
no radiant energy
is truly continuous
objects only emit electromagnetic radiation
in integral multiples of an elementary unit, called a quantum
energy =
hv
h= planck's constant 6.626 * 10 ^-34 j•s
v = frequency
relating energy of a quantum to the energy of a wavelength
Quantized
having values of a whole number of a base value
quantum theory
energy is released or absorbed in discrete packets, or quantums, of energy
photon
tiny packets of radiant energy
photoelectric effect
electrons are emitted by metals or semi conductor materials when illuminated by or absorb electromagnetic radiation
incident radiation
radiation acting on something
threshold frequency (v₀)
minimum frequency at which photoelectrons are emitted
photoelectrons
electrons released by light
work function (φ)
in regard to material, the minimum quantity of energy required to emit photoelectrons from a photoelectric material
work function (φ) =
hv₀, work function value measures the force of attraction between an atoms nuclei and the electrons surrounding it
the higher the frequency above the work function threshold
the greater the kinetic energy of the ejected electron
work function (φ) of target metal
hv- KE electron
Different electron "falls"
produce different wavelengths (when electrons are excited, they jump to a higher energy state. The fall is when they fall back to their ground state)
larger electron transitions
release greater amounts of energy
empirical equation
equation derived solely from experiments w/o a theory backing it
Balmer equation for 4 brightest hydrogen emissions
λ (nm) = (364.56m^2/ m^2 - n^2) where n=2 and m>2
The Rydberg equation
gave a more general empirical formula where n₁ doesn't have to = 2, which allowed scientist to predict other series of hydrogen emission lines
the equation is 1/λ = Rh (1.097 * 10 ^-2 nm) (1/n₁² -1/n₂²) where n₂ > n₁
wavenumber
the inverse of the wavelength, directly proportional to the energy of an electron
In the Rydberg equation, the n₁ and n₂ correspond to
energy levels inside a hydrogen atom. the energy an atom emits or absorbs is the same as the difference in energy between a pair of energy levels
The Bohr Model
Electrons revolve around the nucleus of an atom at available, discrete orbitals
Orbits represent discrete energy levels in the atom
assigned orbits go from n=1, with larger orbital values being higher (less electron) energy
Can find energy in an electron using:
-2.187 * 10 ^-18 J (1/n^2), as n approaches ∞ E approaches 0
Zero energy
it means that the electron approaching n=∞ no longer exists as a part of the hydrogen atom. The hydrogen atom now exists as two separate particles: the H+ ion and the free electron
Energy equation has negative constant
because we want to measure the additional energy input help to help pry a negative electron from its positively charged nucleus
Bohr's model provides
theoretical framework to explain past scientists, only good for atoms or ions with one electron stably orbiting the nucleus
An electron moving through two different energy levels
ninitial = the initial electron energy state
nfinal = the final energy state
∆E = -2.78 * 10 ^-18 (1/nfinal² - 1/ninitial²)
When electron moves farther from nucleus 1/nfinal < 1/ninitial, therefore, it is a negative times a negative, making the overall equation positive, representing an increase in energy level
1/nfinal > 1/ninitial, indicates a decrease in energy level, showing an electron moving from a higher orbital level to a lower one
Ground state
when electron is at lowest energy level
ex. Hydrogen at n = 1, can't get to a lower orbital
Excited State
when electron is at higher energy level
ex. Hydrogen electron in orbital > n=1
Electron absorbing a quantum of energy
jumps to a higher energy level, matching energy difference of states
Electron emitting a quantum of energy
falls to a lower energy level, matching energy difference of states
Electron transition
movement of electrons to any two different energy levels
ionization
absorption of enough energy to separate the electron from the atom
De Broglie observations
electrons can act as particles of matter as well as wave
wavelength is inversely proportional to energy
de Broglie equation for calculating waves in motion
λ = h/mu
where h = planck length (6.626 *10-³⁴ J s)
m = mass (kg)
u = speed (m/s)
product of mass and speed is the particle's momentum
more momentum
shorter wavelength
matter wave
particle with wave like properties, explain stability of electron levels
de Broglie said orbiting electrons behave
like circular waves oscillating around the electron
Stable pattern of circular waves only
achieved if the circumference is a whole number multiple of wavelength
Orbit circumference
nλ,
n = the number of matter wave wavelength in orbit's circumference
Erwin Schrodinger
Developed the Schrodinger wave equation to describe the behavior of matter waves and the atomic model of hydrogen
Schrodinger wave equation
the solutions to the equations are called wave functions
Wave Functions- φ
describes how matter waves of an electron in an atom vary in the size and location inside the atom
orbitals (φ)
clarified by max born, space within the atoms where the probability of finding an electron is higher,
Have distinctive shapes, orientations, and average distances from the nucleus,
helpful in calculating the probability of electron transitions between orbitals when absorbing or emitting quantum of energy
quantum numbers
unique combination of 3 numbers, all of which are solutions to the schrodinger equation
n, principle quantum number
a positive integer that represents a relative size or energy of an orbital or group of orbitals,
orbitals with the same n value are in the same shell