Topic 7 Atomic, nuclear and particle physics 7.1 – Discrete energy and radioactivity Essential idea: In the microscopic world energy is discrete. Quantum model of the atom With the discovery of elementary particles, the model of the atom had to change Previously unexplained phenomena began to clear up with greater understanding of the composition of atoms and the properties of subatomic particles Blackbody Radiation One phenomena was that hot object emitted a specific spectra of light This radiation is typified for an idealized blackbody As the temperature of a blackbody changes, so does the intensity of the frequencies and wavelengths of light it emits The wavelengths of light emitted by a blackbody is defined by Wien’s Law 2.90 × 10−3 m ∙ 𝐾 λ= 𝑇 Blackbody Spectrum Sample Estimate the temperature of the Sun given that it emits light at peak intensity in the viable spectrum at around 500 nm. Discrete Energy In 1900, Max Planck proposed that the energy of the oscillations of atoms is not continuous The energy is a multiple of a minimum value of energy, defined by the frequency of the oscillaion 𝐸 = ℎ𝑓 Planck’s constant and has a value of ℎ = 6.626 × 10−34 J ∙ s Since this energy is not continuous, it is considered quantized, or discrete Photon Theory of Light In 1905, Albert Einstein extended the idea of discrete energy by proposing that when an oscillating molecule emits light, its energy decreases by an integer multiple of hf By conservation of energy, the emitted light must be emitted in quanta of energy, called photons 𝐸 = ℎ𝑓 λ= ℎ𝑐 𝐸 Sample Problem Calculate the energy of a photon of blue light with a wavelength of 450 nm in both J and eV. Photoelectric Effect When light is incident on the surface of a metal, electrons are emitted from the surface Discrete energy levels Electrons only exist in very specific energy states, which differ for atoms of different elements The ground state is the lowest energy state of an atom An excited state is any state in which an atom has higher energy than the ground state Electrons can only move from the specific energy state by gaining or losing a quantum of energy Energy level transition Going to excited state Going to ground state Energy level transition When electrical current is passed through a sample of matter, the atoms become excited As the electrons cycle through going from an excited state to the ground state the photons emitted have the specific frequencies that correspond to the quantum of energy between states When the light emitted by excited atoms is separated through a prism, the specific frequencies of light the result make up the emission-line spectrum Emission Spectrums Hydrogen Spectra Bohr’s Model In 1913, Danish physicist Niels Bohr proposed that electrons can only exist in specific orbits around the nucleus of an atom While in a given orbit, an electron neither gains nor loses energy Emission is the process by which an electron falls to a lower energy state, and releases a photon Absorption is the process by which a photon adds energy to increase the energy state of an electron Hydrogen Spectra Homework! p. 782 #4, 6, 10, 12, 16 Fundamental Forces In addition to gravity and electromagnetic forces, there are two other fundamental forces that exist within atoms The strong nuclear force is an attractive force between all nucleons The weak nuclear force is responsible for the radioactive decay of certain subatomic particles The nuclear forces are considered short-range, while both electromagnetic and gravitational forces are considered long-range Radioactive Decay At the end of the 1800’s, chemist/physicists were examining that unidentified radiation given off by certain elements without an external stimulus Through thorough experimentation, it became clear that this radiation was a result of the disintegration of unstable nuclei Predominantly this is a result of unstable isotopes Radioactive Decay There are multiple ways in which isotopes can undergo radioactive decay Alpha decay Beta Decay Gamma Decay Each type of decay has different characteristics and products Alpha Decay Alpha decay occurs when an isotope emits an α particle ( 42He), resulting in a change in identity of the atom 226 88Ra 222 4 86Rn + 2He Alpha decay occurs when the strong force is unable to hold large nuclei together While alpha particles are massive compared to the other particles, they have the lowest energy, and are therefore the easiest to be absorbed Beta Decay Beta decay can be either positive or negative Beta negative decay occurs when a neutron turns into a proton, releasing a β- particle (electron) and an antineutrino (ν) 14 6C 14 7N + 𝑒− + ν Beta positive decay occurs when a proton turns into a neutron, releasing a β+ particle (positron) and a neutrino (ν) 19 19 + 10Ne 9F + 𝑒 + ν Beta Decay The weak force is the crucial force for beta decay The energy of beta decay is greater than alpha decay, making it slightly more capable of penetrating materials Gamma Decay Like electrons, the nucleus of an atom can exist at an excited state Gamma decay occurs when a nucleus goes from an excited state to a ground state and releases a photon This photon is incredibly energetic and is referred to as a gamma ray 𝐴 ∗ 𝑍𝑁 𝐴 𝑍𝑁 +𝛾 Gamma Decay Gamma decay is the most energetic of the types of radioactive decay Therefore, it is the least easily absorbed and is the most dangerous Half Life As a sample of a radioactive isotope decays, it does so at a certain rate Since the radioactive material no longer exists in its original state, it decays exponentially The half life of a material is the time it takes for half of the initial sample to decay Half Life Half-life of C-14 What is the half life of C-14? What percentage of C-14 is left after 4 half-lives? How much carbon is left after 10,000 years? Decay Series Many radioisotopes decay into daughter nuclei that are also radioisotopes The successive decay of radioisotopes is called the decay series Decay Series http://atom.kaeri.re.kr/nuchart/?zlv=1
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