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Atomic Nucleus
Dense core of protons and neutrons surrounded by electron cloud
4 fundamental forces:
Gravitational
Electromagnetism
Strong nuclear forces
Weak nuclear forces
Strong Nuclear Force
Interactions between protons and neutrons that keep protons together (stronger than electromagnetic forces)
Nuclear Binding Energy
Potential energy found in every nucleus that holds protons together despite repulsions
E =
mc2
Mass-energy Equivalence
Proposed by Einstein, resulting in equation E = mc2
Mass defect
Difference between experimental and calculated atomic masses due to binding energy1
1 eV
Energy equivalent to work needed to move an electron through voltage of 1V
1 eV =
1.602 × 10-19 J
Bohr Model of the Atom
Obsolete theory that suggested electrons orbit nucleus in one of limited number of stable orbital levels
Unique Property of Electrons
Show wave and particle duality like light does
De Broglie Equation
λ = h/mv
Orbitals
The areas which a probability wave is dispersed for an electron
Pauli Exclusion Principle
No two electrons in an atom can have the same set of quantum numbers
Heisenberg Uncertainty Principle
We can establish the position of a particle and its momentum to a certain degree of uncertainty
Photoelectric Effect
Substance emits electrons in response to photons being shined onto it due to exciting the electrons
When electrons are ejected…
The electron becomes proportional to the intensity of light
Insights to Photoelectric Effect
Enough energy must be provided to eject electrons
Energy is dependent on the frequency of light
Ephoton =
hf = hc/λ
Work Function
Ework function = hfthreshold
What is work function?
The minimum amount of energy needed to eject an electron
What happens is photon carries more energy than needed?
The excess energy not going towards work function is kinetic energy
KEmax =
Eincident - Ework function = hfincident - hfwork function
Rydberg Equation
1/λ = RH(1/n12 - 1/n22) using RH = 1 × 10-7 m-1
E = RH(1/n12 - 1/n22) using RH = 2.18 × 10-18 J
Emission Spectra
Black background on which emitted wavelengths appear in color
Absorption Spectra
Colored background with black lines for wavelengths absorbed
On a graph, low absorbance means…
More light is being reflected back (and likely showing color)
Atomic Number
Number of protons that an atom has
Atomic Weight
Protons and neutrons added together
isotopes
Different forms of an element by varying the number of neutrons
2 types of nuclear reactions:
Nuclear fission
Nuclear fusion
Nuclear Fusion Example
Helium production by the sun via fission of deuterium and tritium
21H + 31H → 42He + 10n + energy
Nuclear Fission
Neutron collides with an atom, breaking the nucleus of the atom down into two other atoms
Radioactive Decay
Spontaneous breakdown of isotopes which eject mass as radiation
Types of Radioactive Decay
Alpha
Beta
Gamma
More massive particles…
Are more dangerous and more shielded against
Alpha Decay
Alpha particle (Helium nucleus) is emitted
Alpha particle
Helium nuclei with 2 protons, 2 neutrons, and 2+ charge
Very dangerous but easily shielded
Beta Decay
Beta particle is emitted, two main types (- and +)
Beta-minus Decay
Neutron is converted into a proton, causing an electron to eject
Beta-plus Decay
A neutron is converted into an electron, and a proton is ejected
Move left on periodic table
Beta particles
Less massive, so less dangerous but harder to shield
Gamma Decay
Gamma rays have no mass or charge, so c just represents energy lost
Gamma Rays
Very penetrable and can have health-risks but less than beta and alpha
Electron Capture
Not technically decay; nucleus grabs electron changing a proton into a neutron (charges cancel)
Move left on periodic table
Half Life
Time it takes for half of a radioactive sample to decay (t1/2)
t1/2 =
.693/λ
Graph of Radioactive Decay
` BUT can be displayed as semi-log which shows a linear relationship
Applications of Radioactive Decay
PET scans detect where radioactive particles are emitted to make images
Radiolabeling
Incorporating radioactive atom to trace flow of atoms