Nuclear Physics atom – the smallest particle of an element that retains the chemical properties of that element Atom Basics The number of protons determines the element An atom is composed of… • Nucleons – Protons Subatomic – Neutrons Particles • Electrons Neutrons and protons are about the same weight A electron An l t is i about b t 1/2000 th the mass off a proton t A teaspoon of nuclei would weigh more than a battleship! The nucleus is held together by nuclear forces Nucleons – protons and electrons in the nucleus 1 2 Subatomic Particles Atom Basics Symbol Charge Mass(u) The electrons determine the size of the atom e- -1 ≈0 p+ +1 1 n0 0 1 Electron Electrons move so fast in such a tiny area they make the atom seem solid (Like a moving fan blade) Size: If the nucleus was a marble… then the entire atom would be the size of a football field. Sizes of atoms are measured in picometers 1,000,000,000,000 picometers = 1 meter Proton 1 1 Neutron 1 0 3 Basics of Atoms Reading a Periodic Table Atomic Number “Z Number” ((number of p protons)) Atomic Mass (weighted average) 1) A neutral atom has the same number of electrons as it has protons. 3 Li Lithium 6.941 4 Symbol 2) Atoms of the same element can have different masses due d tto different diff t numbers b off neutrons. t Name 3) Elements with different masses are called isotopes. Nuclide is a term for an isotope. 5 6 1 Nuclear Physics Designating Isotopes Designating Isotopes Mass Number = Protons + Neutrons There are two common ways to present isotopes Example: an isotope of uranium has a mass of 235 and an atomic number of 92. → Mass Number – Protons = Neutrons Example: an isotope of uranium has a mass of 235 and an atomic number of 92. How many neutrons? mass Z 235 – 92 = 143 mass Nuclear Symbol protons neutrons 235 92 U Hyphen Notation Uranium-235 7 How to remember Nuclear Symbol Correct 235 92 Isotopes of hydrogen Electron Incorrect 92 235 U U Proton The nuclear symbol should look like an easy subtraction problem to calculate neutrons. 235 92 143 8 Neutron Protium Deuterium Tritium mass = 1 mass = 2 mass = 3 H 2 1 0.015% 1 1 99.985% U H 9 H 3 1 Rare & radioactive 10 Relative Atomic Mass – a separate unit of measurement is used for mass of individual atoms. Heavy Water Water composed of deuterium hydrogen is often labeled D2O rather than H2O. Because each molecule is heavier but still the same size, D2O is more dense. amu – Atomic Mass Unit (u) I cubes Ice b off D2O in i liliquid id H2O will ill sink!! i k!! 1 amu = 1.660540 x 10-27 kg The amu is based off 1/12th the mass of Carbon-12 Regular ice Proton – 1.007276 u Neutron – 1.008665 u D2O ice $65 / 100g 11 12 2 Nuclear Physics Nuclear Force – force that acts between protons and neutrons. Binding Energy – The difference in energy between individual nucleons and an assembled nucleus (always negative) This is about 100 times stronger than the electromagnetic l t ti fforce that th t causes protons t to repel one another. Nuclear forces only act at a distance of about the radius of a proton. Binding Bi di energy iis ttypically i ll given i iin electron l t volts (eV) or million electron volts (MeV) 1 eV = 1.60217 x 10-19 J 13 Mass Defect - The difference in mass between the total of nucleons and the assembled nucleus. E mc Find the binding energy of 42 He in MeV The mass of a helium-4 nucleus is 4.002603 u. There are 2 neutrons and 2 protons. Einstein related the binding energy to the mass defect. 2 14 E = energy m = mass defect c = 3 x 108 m/s Find the nucleon masses Protons 2 x 1.007276 1 007276 u Neutron 2 x 1.008665 u 4.031882 u Find the Mass Defect 4 4.002603 002603 u - 4.031882 u - 0.029279 u Convert using the binding energy of 1 u E = (-0.029279 u)(931.49 MeV / u) = -27.273 MeV Binding Energy for 1 u = 931.49 MeV 15 16 Binding Energy and Stability The most tightly bound nucleus is iron-56. Nuclear reactions for elements lighter than 56 will tend to increase the mass. Stars will transform hydrogen into helium, helium carbon carbon, and other heavier elements. Nuclear reactions with for heavier elements will tend to decrease the mass. An atom of Uranium-238 will decay into thorium-232. 17 17 18 3 Nuclear Physics Three Types of Decay Penetration Power of Radiation Alpha Emission – A helium nucleus (positively charged) is emitted from a large atom. This will drop the mass by four and the atomic number by two. The extra electrons from the large atom are quickly absorbed into the environment. Beta Emission – There are three types of beta emission. This will not effect the mass number but will affect the number of protons or neutrons. Gamma emission – This will involve the release of energy to stabilize the atom. This often accompanies alpha or beta decay. 19 Band of Stability 20 Alpha Emission ( ) 21 Beta Emission ( ) Electron Emission 22 Beta Emission ( ) Positron Emission 23 24 4 Nuclear Physics Beta Emission ( ) Electron Capture Gamma Emission ( ) This often accompanies alpha and beta decay. This releases excess energy without affecting the mass or atomic number. Gamma Emission Beta Decay 25 26 27 28 Thorium – 232 Decay Series Half Life Half Life is the time it takes for half of the atoms of an isotope to decay. To find the amount of material remaining: t 1 t1 / 2 A Ao 2 29 A = amount Ao = initial amount t = time t1/2 = half life 30 5 Nuclear Physics Smoke Detectors Smoke detectors use Americium-241 as an alpha source to continually ionize the air between two charged plates. This allows current to flow between them. Smoke particles neutralize the air particles and stop the electric current current. This will set off the alarm alarm. 31 32 Nuclear Fission Nuclear Fission Large amounts of energy are produced by fission Fission is the process of splitting an atomic nucleus into fission fragments of smaller atomic nuclei and neutrons. 1 0 92 141 1 n 235 92 U 36 Kr 56 Ba 3 0 n 200 MeV An atom that can be split called fissionable. Fissile nuclei a special type of fission that can have a chain reaction. Not all fissionable nuclei are fissile. Fissile nuclei are generally heavy atoms with large numbers of nucleons. The nuclei are struck by neutrons initiating the fission process. 33 34 35 36 Nuclear Chain Reaction A classic example of a fission reaction is that of UU235 where stray neutron strikes an atom of UU-235. It absorbs the neutron and becomes an unstable atom of UU-236. 236 This undergoes fission. fission More neutrons are released in the reaction. These neutrons can strike other UU-235 atoms to initiate their fission. Uranium 238 on the other hand is not fissile 6 Nuclear Physics Natural Fission Nuclear Power Generation The fission process is an a natural one as a French researcher found a natural uranium reactor in Gabon, West Africa; it has been estimated to be over 2 billion years old. 37 Fuel Rods 38 Control Rods A fuel assembly consists of a square array of 179 to 264 fuel rods, and 121 to 193 fuel assemblies are loaded into an individual reactor. A reactor could have over 50,000 fuel rods storing 200 tons of uranium!! Control rods slide in and out between fuel rods. They are used to moderate the nuclear reaction by absorbing neutrons. When completely inserted, they can absorb enough neutrons to stop the chain reaction. Cadmium, Indium, Silver and a variety of rare earth metals are used for control rods. 39 40 Nuclear Fusion on the Sun: Proton-Proton Chain Fusion Fusion is a nuclear reaction where two light atomic nuclei fuse or combine to form a single heavier nucleus. Fusion reactions do not occur naturally on our planet but are the principal type of reaction found in stars The large masses, densities, and high temperatures of stars provide the initial energies needed to fuel fusion p forces of p protons,, fusion will only y Due to the repulsive take place when nuclei have extreme high thermal energy. The proton-proton chain of the Sun requires temperatures at about 20,000,000 K !!! Fusion on the Sun involves turning four protons into a helium nucleus. This process gives off 25 MeV. The fusion reaction generates a tremendous amount of energy due to protons losing mass to form larger nuclei. 41 By comparison, one dynamite molecule can give of about 20 eV, or less than one millionth the energy. 42 7 Nuclear Physics Nuclear Fusion on the Sun Proton-Proton Chain Attempting Nuclear Fusion Nuclear fusion has been made possible on Earth using a fission reaction for ignition. Because temperatures required for fusion are so great, confining and harnessing power has not been achieved. Currently the most powerful nuclear devices are hydrogen bombs, also called thermonuclear bombs. These use a fission reaction to start the fusion process. 43 44 Hiroshima Little Boy – Messed up Hiroshima 45 Little Boy Play Video 46 Little Boy 47 48 8 Nuclear Physics Fat Man Fat Man – Messed up Nagasaki 49 Fat Man 50 Mushroom Clouds Cooler, Denser Air 51 Natural Mushroom Clouds Mount Redoubt Eruption - Alaska Hot, Less Dense Air 52 Hydrogen Bomb (Thermonuclear) 53 54 9 Nuclear Physics Castle Bravo Cloud – Bikini Island 1954 Hydrogen Bomb Operation 55 Castle Bravo Cloud – Crater Play Video 56 Relative Bomb Strengths 1 Mile 57 58 Tsar Bomba – The Biggest Play Movie About 57 megatons – 14 miles high Fireball Size 59 60 10 Nuclear Physics Fission Process Fission Chain Reaction 61 62 Energy Released E = mc2 Energy Change in Mass 63 Speed of Light 3 x 108 m/s 64 Castle Bravo Cloud – Bikini Island 1954 65 11