FYS 3520 Kjernefysikk, struktur og spektroskopi Midterm Exam 2014 Deadline to hand it in is friday 4th of April. It can be sent electronically to [email protected] or on paper to the expedition office at physics (closes at 3 o´clock). 1. Nuclear properties a) How big is the atomic nucleus? How big is an atom? b) What is the density (Mass/Volume) of the nucleus? c) Does it depend on the mass number A? d) What are isotopes, isotones and isobars? e) The neutron has no charge, but still it has a magnetic moment, why? f) What is parity and symmetry? g) Can a spherical nucleus rotate? h) What is the heaviest (largest Z and largest A) nucleus we have managed to produce so far (do not use the textbook) i) Which element Z has the highest number of stable isotopes? Why? j) Is it harder to steal a neutron from 208Pd or 11Li or 4He? k) Why was Rutherford amazed by the results of his famous experiment? l) Why doesn´t the electrons fall into the nucleus? m) What is the energy released by fission of a 235U nucleus? Compare this to the energy released per molecule when burning coal. n) How can we measure planck´s constant h? 2. Nuclear binding energy a) Estimate the energy needed to remove one neutron from 40Ca nucleus (which has N=Z=20). b) Using Appendix C in Krane: A nucleus has given mass 166.932046 nuclear mass units (u). Calculate the binding energy Which nucleus is it? Write the chemical name, Z and neutron number. c) Calculate the binding energy by means of the semi empirical mass formula (Weizsäcker). Use the standard values of the coefficients given above. How does the result fit with what you found in question b)? d) 3. Fermi Gas T=0 a) Write down the phase space of a Fermion, differential in p b) Calculate the relationship between density and Fermi energy. c) Estimate the depth of the nuclear potential (Hint: calculate the Fermi energy for neutrons, then add the neutron binding energy) d) Calculate the pressure of a Fermi system given it´s density (degeneracy pressure) 4. Fermi gas T > 0. For a classical gas, Ex = 3/2T a) What is the excitation energy/temperature dependence? b) Why the difference? c) can you calculate the entropy and the density of levels? 5. Compound nuclear decay a) How can an excited nucleus get rid of it´s energy? List the possible decay channels. b) Neutron and photon emission. How their decay rate is similar and different. What is the form of the neutron spectrum? And of the photon spectrum? c) Fission decay. Discuss why the fission decay problem differs from that of neutron and gamma decay. d) Fission to neutron competition. Why are 235U, 233U and 239Pu fissile when hit by thermal neutron, while 238U and 232Th are not? e) Draw by hand the dependence of the fission cross section vs energy for a nucleus like 208Pb (Bf=28MeV) and for 238U (Bf= 6MeV). 6. Direct reactions The nucleus has quantized energy levels, how can we o study these states experimentally? Give an example of a direct reaction which can be used to study shell model states a) below the fermi energy b) above the fermi energy 7. We can make nuclear reactions in the laboratory by bombarding the nuclei in a target with a beam of charged nucleons with high energy. If the beam consists of e.g. alpha-particles, the speed must be sufficient to overcome the Coulomb barrier. How can we calculate the Coulomb barrier? Which energy should the alpha-particles have in order to penetrate 197Au. Good Luck !

© Copyright 2019 ExploreDoc