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Atomic and Nuclear Physics 9th of January 2014 7.1 ATOMIC STRUCTURE Simple model of an atom • Electrons kept in orbit around the nucleus as a result of the electrostatic attraction between the electrons and the nucleus (small + dense) The Plum-Pudding Model • The atom was imagined to be a sphere of positive charge with negatively charged electrons dotted around inside • Rutherford designed an experiment to test the plum pudding model. It was carried out by his assistants Geiger and Marsden. Evidence that supports a nuclear model of the atom: Geiger and Marsden’s Experiment • A beam of alpha particles was aimed at very thin gold foil (only few atoms thick) and their passage through the foil detected. • Expected the alpha particles to pass straight through the foil but something else also happened. Rutherford’s Scattering Experiment 1. Most undeflected alpha particles show – atoms are mostly empty space; 2. Small deflections show – a repulsive force exists; 3. Deflections show - same charge as the alpha rays (positive); 4. Only SOME deflections: hence the nuclei are a small target; Rutherford’s Scattering Experiment 5. Large Deflections show: nuclei have enough mass of alphas to bounce back; 6. Mass of nucleus is more than the mass of an alpha particle; 7. High density as it has a large mass and a small size ; Why must it be done in a Vacuum? 1. To avoid/ reduce absorption of alpha particles 2. To avoid/ reduce chances of collisions between air molecules and alpha particles 3. Allow sufficient range for alpha particles (so it reaches the gold foil) (Limitations of )Rutherford’s Nuclear Model • Electrons orbit a central nucleus (small, dense) • HOWEVER: ^ does not explain the stability of an atom – the electron accelerate around the nucleus, they would therefore never lose energy causing them to don’t spiral into the nucleus but in reality they should spiral into the nucleus but they don’t as there is a force that opposes it • Electron accelerate and give off energy Existence of atomic energy levels – SEE CHEMISTRY • Students should be familiar with emission and absorption spectra, but the details of atomic models are not required. Students should understand that light is not a continuous wave but is emitted as “packets” or “photons” of energy, each of energy hf. 7.2 NUCLEAR STRUCTURE Nuclide, Isotopes and Nucleon • Nuclide: a specific combination of a distinct # of protons and # of neutrons that form a nucleus • Isotopes: nuclei with the same number of protons but different number of neutrons • Nucleon: particles of the nucleus (proton or neutron) Atomic Number and Mass Number • Nucleon Number A = Proton # + Neutron # = (mass of the atom) • Proton Number Z = Atomic Number • Neutron number N = Neutron # atom Interactions in a Nucleus • Coulomb repulsion (electromagnetic force) long range between protons splits the nucleus • Strong, short-range nuclear interaction between nucleons (p and n) binds the nucleons • Overall balance must be correct and more neutrons needed • Strong force is very strong, short range and the same for all nucleons (as nuclei all have the same density) • Adding more neutrons (compared to protons) contributes to binding and does not add to tendency to split the nucleus / a proton repels every other proton (in the nucleus) so extra neutrons are needed for binding 7.2 RADIOACTIVE DECAY RADIOATIVITY Natural Radioactive Decay • Unstable nuclei change spontaneously/rando mly/emit energy; • by the emission of alpha particles and electrons and gamma rays • The inclusion of the antineutrino in β− decay is required. Alpha Particle, α • Range depends: the charge of the alpha particle, the kinetic energy of the alpha particle, the density of the air 2 protons and 2 neutrons = Helium Nucleus Charge 2+ Energy 5 MeV Range in Air > 5cm Penetration Low, Stopped by air Ionising Ability Very High Detection GM tube, cloud chamber, photographic paper Alpha Energy • Alike an explosion: • Momentum conserved; • so different speeds as different masses; • opposite directions because momentum was zero initially; Alpha Decay • Original Atom loses 2 Protons and 2 Neutrons - loses 4 from its Atomic Mass, loses 2 from Atomic Number • Changes into a different element Beta Particle, βFast moving electron Charge - Energy ___ MeV Range in Air > 30cm Penetration Moderate, about 1mm Aluminium Ionising Ability Very High Detection GM tube, cloud chamber, photographic paper • Most deflected by a magnetic field Beta Minus Decay • One neutron splits into one electron and one proton – Atomic number goes up by one and Atomic Mass remains unchanged • Electron emitted from the nucleus; antineutrino also emitted – reason for beta particles with different energy values Beta Plus Decay • One neutron splits into one positron and one proton – Atomic number goes down by one and Atomic Mass remains unchanged • Positron (antielectron as an electron) emitted from the nucleus; neutrino also emitted – reason for beta particles with different energy values Gamma Ray, γ • • • • • • Light – high speed 300,000,000 m/s High Energy Electromagnetic Radiation No Charge Large Range, High Penetration Stopped by think block of lead Low ionizing ability – loses some energy • Gamma radiation is often released as surplus energy; the energy difference as a gamma photon Comparing range of Beta and Alpha Decay • Beta have smaller mass / smaller / have greate r speed than alpha; • beta have smaller charge than alpha; • therefore less likely to interact with air molecu les; Nuclear radiation and health • To ionise an atom, it requires about 10eV • Very high dose: affect central nervous system, leading to loss of coordination and death within 2-3 days • Medium dose: can damage the stomach and intestine, resulting in sickness and diarrhoea • Low dose: loss of hair, bleeding and diarrhoea • Safe dose: all ionising radiation is potentially harmful so there is no point below which it becomes totally safe – however at low levels the risk is small and outweighed by the benefits Long Term Biological Effects of Ionising Radiation • Increased probability of getting cancer or having a child with a genetic mutation • Mutations in living organisms • Damage to cell and tissue • Problems arising the disposal of radioactive waste – difficult to dispose hence ^^ • How associated risks can be reduced – using thick sheets of lead/ thick lead container Protection against radiation • Distance - as alpha and beta have very short range in air • Number of gamma decreases proportional to 1 - hence the further you are, the safer you 2 𝑟 will be • Shielding – thick lead shielding Detecting Ionising Radiation • G-M (Geiger Muller) Tube – amplified passed on to a scaler (shows the total number) or ratemeter (shows the rate in ‘counts per second’ with a loudspeaker clicks each time a ray from the source passes through the tube) • Photographic Film – blackened/ gets darker Sources of Background Radiation • Cosmic Rays – From Outer Space • Rocks – Radon Gas from the Ground • Food – Naturally from animals, plants who absorb radiation from the soil – passes up through the food chain • Medical – X-Rays, Equipment • Fallouts – Nuclear Waste Why some nuclei are stable and others unstable • An explanation in terms of relative numbers of protons and neutrons and the forces involved is all that is required. • Increase proton number = increase coulomb force, to counter that neutrons needed to increase strong force 7.2 RADIOACTIVE DECAY – HALFLIFE Radioactive Decay • Unstable nuclei change spontaneously/randomly/ emit energy by the emission of alpha particles and electrons and gamma rays • Rate of decay decreases exponentially with time • Any quantity that reduces to half its initial value in a constant time decays exponentially • The nature of the decay is independent of the initial amount. Radioactive Half-life • Radioactive Half-life: Time taken for half of the nuclei in a sample to decay OR time taken for activity of a radioactive sample to halve – each half life is equal • Most ‘stable’ isotopes are the ones with the LONGEST half-life as it takes longer for the unstable nuclei to emit Alpha, Beta and Gamma as it randomly decays Activity • This activity is measured in becquerels • 1 becquerel = 1 nucleus decaying per second • Bodies are slightly radioactive with an activity of 4000 Bq Half Life • REMEMBER TO TAKE ACCOUNT BACKGROUND RADIATION – TAKE IT AWAY! Minus it! It isn’t zero so you need to take it into account! 7.3 NUCLEAR REACTIONS Artificial induced transmutation • Change of an atom from one element to another – this can be artificially initiated bombarding a target material with highenergy particles • 1 amu = 931.5 Mev Unified Nuclear Mass • 1/12 of the mass of a Carbon-12 atom • students must be familiar with the units MeV c −2 and GeV c −2 for mass Binding Energy 𝐸 = 𝑚𝑣 2 • Mass Defect • Binding Energy = energy released when nuclides form constituent OR the energy required to separate nucleus into separate nucleons • Binding Energy per nucleon = • Atomic mass + mass defect/ binding energy = total mass of protons + total mass of neutrons Nucleon number of the binding energy per nucleon Graph Explaining increases in binding energy • energy is released in the decay of K40 / energy released is the • difference in binding energies / decay is spont aneous / A40 • is more stable than K40; 7.3 FISSION AND FUSION Nuclear Fission • Large nuclei are induced to break up into smaller nuclei and release energy in the process. • Used in nuclear reactors and atomic bombs • Single reaction - bombarding a Uranium nucleus with a neutron • Chain reaction as it results in production of 3 neutrons Nuclear Fusion • Main source of the sun’s energy – fuels all suns: fusion of 2 different isotopes of Hydrogen to produce Helium • Small nuclei are induced to join together into large nuclei and release energy in the process Fusion v. Fission • nuclear fusion waste much less active than fission waste; fusion fuel much more abundant than fission fuel; fusion fuel has higher energy density than fission; radiation/pollution from plant lower for fusion; 13.2 NUCLEAR PHYSICS 13.2 RADIOACTIVE DECAY Beta positive Decay • Students should know that β energy spectra are continuous, and that the neutrino was postulated to account for these spectra. Equations for Exponential Decay (given) • 𝑁 = 𝑁0 𝑒 −𝜆𝑡 - exponential decay equation • ^ activity can substitute here too • Rate of decay is proportional to the no. of undecayed nuclei 𝑑𝑁 • 𝐷𝑒𝑐𝑎𝑦 𝐶𝑜𝑛𝑠𝑡𝑎𝑛𝑡 = = 𝜆 – how quickly the material will decay 𝑑𝑡 (s¯¹) proportionality between the number of nuclei and the rate of decay • 𝐴 (𝐵𝑞 − 𝑑𝑒𝑐𝑎𝑦 𝑝𝑒𝑟 𝑠𝑒𝑐) = − • 𝑇1 = 2 ln 2 𝜆 Δ𝑁 Δ𝑡 = −𝜆𝑁= 𝜆 𝑁0 𝑒 −𝜆𝑡 Outline methods for measuring the long half-life of an isotope • If a large amount of radioactive substance is used then a significant number of decays will occur per unit time, the activity can be measured • GM tube before sample, count the no. of decays • Plot of decays against time will produce a nice exponential curve. • The half-life can be calculated from the decay curve. However a problem arises if the half-life is very short or very long. Outline methods for measuring the short half-life of an isotope • Some nuclei have such short half-lives that transporting the sample to a detector is virtually impossible, • i.e. the substance decays before you get it to the detector. In such cases the sample must be created (Artificial Transmutation) in or very near a detector. NEEDED? Uses of Radioactivity • Works by injecting a radioisotope, then detecting it with a G.M counter – chosen isotope must have a short half-life but remains long enough to be detected 1. Radioactive Tracers – finding leaks from a pipeline, Fertiliser, 2. Medical Radioactive Tracers – to find kidney blocks NEEDED? Uses of Radioactivity 3. Sterilising – kill bacteria, moulds and insects in food – prolongs shelf life; sterilizes medical equipment (eg. Plastic Syringes) 4. Radiotherapy – careful usage kills cancer cells 5. Radioactive dating – archaeological specimens and rocks; by finding out how much uranium has changed into lead – possible to calculate the age of the rock NEEDED? Uses of Radioactivity 6. Quality Control – measuring how much ionizing radiation passes through then adjusting the thickness accordingly 7. Smoke Detection – Weak source emits alpha particles which ionizes the air and conducts electricity and a small current flows; when there is smoke, it absorbs the alpha particles, current reduces and the alarm sounds Radioactive Potassium- Argon Dating • K-40 decays to Ar-40 with a half-life of 1.26 x 10⁹ • When rock containing K is molten, any Ar that is formed will bubble up to the surface and leave the rock, but when the rock solidifies the argon is trapped • If a rock sample is heated the Ar atoms are released and can be counted with a mass spectrometer – if you count the K nuclei you can calculate the age of the rock Radioactive Carbon-14 Dating • Only used for organic material up to about 60000 years old • (living things contain) carbon (14) • C14 is a radioactive isotope / beta emitter • (radio)activity decreases (over time) • (estimate) half-lives (since material was alive) • compare activity (of sample now with living tissue) / ratio of C14 to C 12 is fixed in living material % 𝑛𝑜𝑤 = % 𝑜𝑟𝑖𝑔𝑖𝑛𝑎𝑙 𝑥 𝑒 −𝜆𝑡 Original is 10^-10 % 7.8 NUCLEAR REACTIONS Problems with using fission as an energy source • initial activity is very high; • it is still highly radioactive after 70 years; • thereby posing a severe health risk / causing problems of disposal / OWTTE; Nuclear Fission (splitting) • Nucleus of Uranium-235 splits by collision with a neutron to produce 2 daughter nuclei and a small number of neutrons (3) • This process releases energy in the form of kinetic energy (= thermal energy) of the 2 nuclei (fission products) • The neutrons produced by one fission can strike other U-235 nuclei creating a chain reaction Nuclear Fission (splitting) Chain Reaction? • Neutrons (about 3) are emitted which can collide with/hit other uranium nuclei; • Start new fission processes which in turn will lead to more and so on; Nuclear Reactor Outer Shell - Lead • When fission process is used as an energy source to generate electricity – the chain reaction must be controlled: Fuel Rods – Uranium Control Rods – Boron Moderator – Graphite Control Rods • • • • Made of boron Placed between rods of nuclear fuel Absorbs some of the neutrons Moveable, adjustable – so there are just enough neutrons to keep the chain reaction going • Lowered = decreased rate of reaction • Raised = increased rate of reaction Moderator • Usually made out of water, Graphite or heavy water (water with heavier isotopes) • Reduces the speed of neutrons, so the Control Rods have enough time to absorb it – can sustain a chain reaction involving U-235