From Last Time… Radioactive decay • Nucleus is small, tightly bound system of protons & neutrons. • Said last time that some nuclei are more stable than others. • Unstable nuclei can decay by emitting some form of energy. • Three different types of decay observed: • Proton number determines the element. • Different isotopes have different # neutrons. • Some isotopes unstable, radioactively decay • Nucleus held together by the strong nuclear force Alpha decay Beta decay Gamma decay – Stronger than coulomb force, – But much shorter range than coulomb force. • Strong force actually between quarks, internal constituents of the neutron/proton. ‘Leaks’ out to appear as an attractive force. Mon. Nov 22 (First three letters of greek alphabet). Phy107 Lecture 32 Mon. Nov 22 Penetrating power of radiation • Alpha radiation very weak • Beta radiation penetrates farther • Gamma radiation hardest to stop Mon. Nov 22 Phy107 Lecture 32 Is the radiation charged? • Alpha radiation positively charged • Beta radiation negatively charged • Gamma radiation uncharged Phy107 Lecture 32 Mon. Nov 22 Alpha radiation Phy107 Lecture 32 A new element • Alpha radiation now known to be a helium nucleus (2 protons, 2 neutrons) • When a nucleus emits an alpha-particle, it loses two neutrons and two protons. • It becomes a different element. Alpha particle • Example: Heavy nucleus spontaneously emits alpha particle 238 92 92 protons 146 neutrons Mon. Nov 22 Phy107 Lecture 32 € Mon. Nov 22 U→42 He+ 23490Th 2 protons 2 neutrons 90 protons 144 neutrons Phy107 Lecture 32 1 A random process • This is a quantum-mechanical process – It has some probability for occurring. • For every second of time, there is a probability that the nucleus will decay by emitting an alpha-particle. • The alpha-particle quantum-mechanically tunnels out of the nucleus. Radioactive half-life • Example of random decay. • Start with 8 identical radioactive nuclei • Suppose probability of decaying in one second is 50%. Every second, half the atoms decay Undecayed nuclei The half-life is one second t=0 Mon. Nov 22 Phy107 Lecture 32 Mon. Nov 22 More physical half-life has a half-life of 14 billion years Phy107 Lecture 32 Why? – All nucleons (neutrons & protons) attracted by short-range strong force – Protons forced apart by long-range Coulomb force. – Smaller nuclei will be more stable • Sample initially contains 1 million 232Th atoms • Every 14 billion years, the number of 232Th nuclei goes down by a factor of two. • Why is the ejected piece an alpha-particle, and not something else? – Helium nucleus is much more stable than other light nuclei Phy107 Lecture 32 Mon. Nov 22 • Nucleus emits a helium nucleus 2 neutrons, 2 protons. • Only heavy nuclei will alpha-decay. • Decay is by quantum mechanical tunneling. Tunneling is sensitive to the nuclear barrier. Decay probability (and hence half-life) varies dramatically Can vary 20 orders of magnitude Phy107 Lecture 32 Phy107 Lecture 32 Decay sequence of Half-lives of alpha-decay Mon. Nov 22 t=3 sec • Why does a piece come out of the atom? 232Th Mon. Nov 22 t=2 sec 238 U Number of protons • t=1 sec Mon. Nov 22 Number of neutrons Phy107 Lecture 32 2 Radon • One of the daughters in the 238U decay series is radon. Detecting radiation • A Geiger counter • Radiation ionizes (removes electrons) atoms in the counter • Radon is an alpha emitter that presents an environmental hazard • Inhalation of radon and its daughters can ionize lung cells enough to increase the risk of lung cancer. Leaves negative electrons and positive ions. • Health risk depends radon concentration, which depends on concentration of uranium and other radioactive elements. These are attracted to the anode/cathode, current flow is measured Mon. Nov 22 Phy107 Lecture 32 Mon. Nov 22 Other radioactive decay • Beta decay – Now know to be an electron. – Radioactive nucleus emits an electron • How can this be? – There are no electrons in the nucleus! – Has only neutrons and protons. Phy107 Lecture 32 Beta decay • Nucleus emits an electron (negative charge) • Must be balanced by a positive charge appearing in the nucleus. • Particles are not forever! – Charge is forever, energy/mass is forever – But particles can appear and disappear Mon. Nov 22 Phy107 Lecture 32 This occurs as a neutron changing into a proton Mon. Nov 22 Quarks Not just neutrons & protons • Nucleons have an internal structure. • Made up of different types of quarks. • In this sense, neutrons and protons not so different. Mon. Nov 22 Phy107 Lecture 32 • Six quarks (also six antiquarks) • All have electrical charge, spin, • Also have other quantum nujmbers.. Phy107 Lecture 32 Mon. Nov 22 Phy107 Lecture 32 3 Quark structure of nucleons • Proton = up+up+down Neutron into proton • Think about this in terms of quarks. • Neutron becomes proton by changing 1 quark. • Charge = 2/3+2/3-1/3=+1 proton • Proton is a composite object, as are many other particles. • Neutron = up+down+down= 2/3-1/3-1/3=0 Mon. Nov 22 neutron Phy107 Lecture 32 Down quark changes to up quark by emitting W-, decays to electron Mon. Nov 22 Phy107 Lecture 32 Example of beta decay Neutron decay • radioactive form of carbon, decays by beta decay (electron emission). • Carbon has 6 electrons, so six protons. • 12C has (12-6)=6 neutrons. • 14C has (14-6)=8 neutrons. • Can be clearer to visualize this diagramatically. 14C, Beta decay: Now have a new element (changed # protons) Element with 7 protons in nucleus is Nitrogen 14 6 Mon. Nov 22 Phy107 Lecture 32 Mon. Nov 22 − C →14 7 N+ e Phy107 Lecture 32 € Carbon dating • This decay is used to time since biological substance has died. • 14C naturally present in the atmosphere as a result of transmutation of 14N. Cosmic ray proton shatters atmospheric gas nucleus, producing atmospheric neutrons. Neutron knocks proton out of 14N nucleus, becoming Mon. Nov 22 14 C Phy107 Lecture 32 14 C • to 12 C ratio 14C has a half-life of ~6,000 years, continually decaying back into 14N. • Steady-state achieved in atmosphere, with 14C:12C ratio of 1:1 trillion (1 part in 10 12) As long as biological material alive, atmospheric carbon mix ingested (as CO2), ratio stays fixed. Mon. Nov 22 After death, no exchange with atmosphere. Ratio starts to change as 14 C decays Phy107 Lecture 32 4 Other isotopes of carbon Antimatter • Every particle now known to have an antiparticle. • Even antimatter has been generated. • Lighter forms of carbon are observed to emit a particle that looks like an electron, but has a positive charge! • This is the antiparticle of the electron. • Called the positron. Mon. Nov 22 Phy107 Lecture 32 What is going on? • Photons are created so that energy is conserved. Mon. Nov 22 has more neutrons than the most stable form 12C. – So it decays by electron emission, changing neutron into a proton. Guessing the decay route Light elements: Excess neutrons-> change neutron to proton by electron emission • Other isotopes of carbon have fewer neutrons – Decays by emitting positron, changing proton into neutron. Too few neutrons>change proton to neutrons by positron emission Phy107 Lecture 32 Mon. Nov 22 Detecting radiation • A Geiger counter • Radiation ionizes (removes electrons) atoms in the counter Phy107 Lecture 32 60 Cobalt • Is radioactive by measurement, half-life 5.3 yr. • By what mechanism will this decay? • From the periodic table, Co has 27 electrons. – Stable form of Co is 59 Co, with 32 neutrons – 60Co has 33 neutrons, one more than most stable form Leaves negative electrons and positive ions. • Likely to decay by changing one of the neutrons into a proton These are attracted to the anode/cathode, current flow is measured Mon. Nov 22 Phy107 Lecture 32 • Can often make good guesses regarding decay route • Only heavy nuclei decay via alpha emission • Nuclei decay in a way that produces a more stable nucleus 14C Mon. Nov 22 Matter and antimatter annihilate when in close proximity. – Charge conservation says electron must be emitted – One more proton means it becomes Nickel ( 60 Ni) – 60Ni is a stable isotope, with 26% natural abundance. Phy107 Lecture 32 Mon. Nov 22 Phy107 Lecture 32 5 Turning lead into gold Radioactive decay changes one element into another by changing the number of protons in a nucleus. This can also be done artificially by neutron bombardment. Nuclear fission • In some cases, the effect of neutron bombardment is more dramatic. • Leads to nuclear fission, where a heavy nucleus is split apart into two smaller ones. • The transmutation of platinum into gold accomplished by a sequence of two nuclear reactions • first: 198Pt + neutron --> 199Pt • second: 199Pt --> 199Au + subatomic particle Mon. Nov 22 Phy107 Lecture 32 Mon. Nov 22 Fission chain reaction • Neutrons are released in this process, leading to more fission events • Chain reaction can result Mon. Nov 22 Phy107 Lecture 32 Phy107 Lecture 32 Nuclear Fusion • ‘Opposite’ process also occurs, where nuclei are fused to produce a heavier nucleus, but requires large initial energy input. • Called nuclear fusion. Mon. Nov 22 Phy107 Lecture 32 6
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