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A05715 ANY CALCULATOR School of Physics and Astronomy MODULE OUTSIDE THE MAIN DISCIPLINE 03 00680 LC THE COSMIC CONNECTION SUMMER EXAMINATIONS 2015 Total Time Allowed: 1 hour 30 minutes Answer Section 1 and two questions from Section 2. Section 1 counts for 40% of the marks for the examination. Full marks for this Section may be obtained by correctly answering four questions. You may attempt more questions, but marks in excess of 40% will be disregarded. Section 2 consists of three questions and carries 60% of the marks. Answer two questions from this Section. If you answer more than two questions, credit will only be given for the best two answers. The approximate allocation of marks to each part of a question is shown in [ ]. All symbols have their usual meaning. Calculators may be used in this examination but must not be used to store text. Calculators with the ability to store text should have their memories deleted prior to the start of the examination. Two tables of constants which may be required to answer some of the questions are attached to the back of this question paper. Page 1 TURN OVER ANY CALCULATOR SECTION 1 Full marks may be obtained by correctly answering four questions. You may attempt as many questions as you wish, but any marks in excess of 40% will be disregarded. 1. Explain briefly why Sunspots are fainter than the surrounding photosphere. 2. [10] What is the Hertzsprung Russell diagram? Describe the position of a white dwarf star relative to the Main Sequence on such a diagram. At what stage of stellar evolution does a star become a [10] white dwarf? 3. Use Wien’s law to explain quantitatively in what way the spectrum of the light from the Sun, with a surface temperature of about 6000K, would differ from that of a B star. 4. Under what circumstances would the light from stars formed long ago now be observed at infrared wavelengths? 5. A05715 [10] [10] Compare and contrast images of the Sun taken in (i) visible radiation; and (ii) X-ray radiation. [10] Page 2 TURN OVER ANY CALCULATOR 6. Discuss the properties of Cepheid stars that make them cosmologically important. [10] SECTION 2 Answer two questions from this Section. If you answer more than two questions, credit will only be given for the best two answers. 7. (a) Kepler derived his three laws of planetary motion from a study of Tycho Brahe’s observations of Mars. State Kepler’s three laws and include a sketch that illustrates their key features. (b) [12] Derive the constant of proportionality in Kepler’s Third Law, by using expressions for the forces that keep a body in a circular orbit together with the relationship between the period of a circular orbit, its radius and the speed of the object. (c) [9] Halley’s comet was last seen from Earth in 1986. The orbit of Halley’s comet has a semi-major axis of 17.9AU, and a distance of closest approach to the Sun of 0.59 AU. Use Kepler’s Third Law to estimate when we can expect to see it again. [9] A05715 Page 3 TURN OVER ANY CALCULATOR Neutron stars are some of the most compact objects in the 8. Universe. (a) Discuss briefly the neutron star stage of stellar evolution. [12] (b) Describe the lighthouse model for a pulsar, and indicate how the model is consistent with observations. (c) [12] One particular neutron star is observed to have a temperature of 600,000K and a luminosity of 0.046L. Calculate the radius of the star in kilometres and comment on your answer. [6] Discuss each of the following key concepts in the context of 9. theories of the behaviour of the early Universe: (a) The expansion of the Universe; (b) The Cosmological Principle; (c) The Big Bang; (d) The Cosmic Microwave Background; and (e) Dark Energy. (Marks will be divided equally between a brief discussion of the concept and its relevance to theories of the early Universe.) [30] A05715 Page 4 TURN OVER ANY CALCULATOR Physical Constants and Units Acceleration due to gravity g 9.81 m s-2 Gravitational constant G 6.673 10-11 N m2 kg-2 Avogadro constant NA 6.022 1023 mol-1 Note: 1 mole = 1 gram molecular-weight Ice point Tice 273.15 K Gas constant R 8.314 J K-1 mol-1 Boltzmann constant k, kB 1.381 10-23 J K-1 =0.862 10-4 eVK-1 Stefan constant 5.670 10-8 W m-2 K-4 Rydberg constant R 1.097 107 m-1 Rhc 13.606 eV Planck constant h 6.626 10-34 J s = 4.136 10-15 eV s h/2 1.055 10-34 J s = 6.582 10-16 eV s Speed of light in vacuo c 2.998 108 m s-1 c 197.3 MeV fm Charge of proton e 1.602 10-19 C Mass of electron me 9.109 10-31 kg Rest energy of electron Mass of proton 0.511 MeV mp Rest energy of proton One atomic mass unit 1.673 10-27 kg 938.3 MeV 1.66 10-27 kg u Atomic mass unit energy equivalent 931.5 MeV Electric constant 0 8.854 10-12 F m-1 Magnetic constant 0 4 10-7 H m-1 A05715 Page 5 TURN OVER ANY CALCULATOR Bohr magneton B 9.274 10-24 A m2 (J T-1) Nuclear magneton N 5.051 10-27 A m2 (J T-1) Fine-structure constant = e2/40 c 7.297 10-3 = 1/137.0 Compton wavelength of electron c = h/mc 2.426 10-12 m Bohr radius ao 5.2918 10-11 m angstrom A 10-10 m torr (mm Hg, 0C) torr 133.32 Pa (N m-2) barn b 10-28 m2 A05715 Page 6 TURN OVER ANY CALCULATOR Astrophysical Constants Quantity Symbol Value Astronomical Unit AU 1.50 1011 m Parsec pc 3.1 1016 m Tropical year y 365.2422 mean solar days Lo∙ Solar luminosity Absolute bolometric 3.9 1026 W Mbol +4m75 BC 0m08 mv(o) 26m74 magnitude of the Sun Bolometric correction for the Sun Apparent visual magnitude of the Sun f Solar constant Mo∙ Solar mass 1.37 103 W m 2.0 1030 kg Wien constant b 2.89 10 m K Hubble constant HO 75 (km s) Mpc Solar radius Ro∙ 6.96 108 m Distance of the Sun from 8.7 kpc galactic centre A05715 Page 7 END OF PAPER