Astronomy 141 Life in the Universe Professor Gaudi Homework #4 Solutions

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Astronomy 141 Life in the Universe Autumn Quarter 008 Prof Gaudi Homework #4 Solutions These questions concern the concept of targets for searches for extrasolar planets specifically (a) the number of targets available for these searches for stars of various types (b) the suitability of stars of various types and (c) the sizes of the signals for Earthlike planets for stars of various types and using various methods Assume that the space density of all main-sequence stars in the solar neighborhood is 01 stars per cubic parsec When necessary use the typical values for the physical parameters of stars of various spectral types taken from your book or my notes Question 1 (10 points) Estimate the number of A stars within 10 parsecs of the Sun a) 4 b) 0 c) 4 d) 419 e) 4189 The total number N of stars (of all types) within 10 parsecs is just the volume V contained by a sphere of radius 10 parsecs times the space density of stars ρ The volume is V = 4π 3 d 3 = 41888 pc 3 and so the total number of stars is N = ρv = 01 pc -3 41888 pc 3 = 419 The fraction of all stars that are A-type is given in Table 111 of your book and is 1% Therefore the number of A stars within 10 parsecs of the Sun is 001 N =001 419 ~ 4 Answer a) 4

Question (10 points) Estimate the number of G stars within 10 parsecs of the Sun a) 93 b) 93 c) 1 d) 7 e) 9 The fraction of all stars that are G-type is 7% according to Table 111 of your book Therefore the number of G stars within 10 parsecs of the Sun is 007 N = 007 419 ~ 9 Answer e) 9 Question 3 (10 points) Estimate the number of stars within 5 parsecs of the Sun a) 1 b) 393 c) 39 d) 314 e) 5 The total number of stars within 5 parsecs of the Sun is N = ρv = 01 pc -3 4π 3 (5 pc)3 = 5 Roughly 75% of all stars are stars and therefore the number within 5 parsecs of the Sun is 075 5 ~ 39 Answer c) 39 Question 4 (5 points) Assume that it takes 15 Gyr for intelligent life to evolve Further assume that the Sun has a lifetime of 10 Gyr and the lifetime of a main sequence star is proportional to -3 where is the mass of the star What kinds of main sequence stars should not be targeted for searches for intelligent life? a) Stars with mass less than about 55 times the mass of the Sun b) Stars with mass less than about 19 times the mass of the Sun

c) Stars with mass greater than about 19 times the mass of the Sun d) Stars with mass greater than about 053 times the mass of the Sun e) Stars with mass less than about 67 times the mass of the Sun If the lifetime of main sequence stars is proportional to -3 then we can write the lifetime relative to the Sun: Lifetime Star = Lifetime Sun Sun We can use this to determine the main sequence mass for which the lifetime is 15 Gyr Solving this equation for the mass of the main-sequence star relative to the Sun: 1/3 1/3 Lifetime = Star 15Gyr Sun = Sun = (015) 1/3 Sun 19 Sun Lifetime Sun 10Gyr Since more massive stars have shorter lifetimes we conclude that stars more massive than about 19 times the mass of the Sun will have lifetimes that are too short to allow intelligent life to evolve Answer c) Stars with mass greater than about 19 times the mass of the Sun For the following three questions pick the answer that is correct to within an order-of-magnitude (in other words pick the closest power of ten) Question 5 (15 points) An Jupiter-sized planet transits in front of an A0 main-sequence star By how much will the star dim when the planet passes in front of it? a) about 0001% b) about 001% c) about 01% d) about 1% e) about 10% The amount that a star dims when a planet passes in front of it is just given by the ratio of the planet to stellar radius squared ie 3

Radius of Planet Dimming = Radius of Star The radius of an A0 star according to my notes is 3 times the radius of the Sun Therefore Radius of Jupiter 7149 km Dimming = = = 1997 10 3 ~ 10 3 3 Radius of Sun 3 695500km Answer c) about 01% Question 6 (15 points) An ars-sized planet transits in front of an G main-sequence star By how much will the star dim when the planet passes in front of it? a) about 0001% b) about 001% c) about 01% d) about 1% e) about 10% The radius of an G star is just the radius of the Sun (since the Sun is a G star) Therefore Radius of ars 3397 km Dimming = = = 386 10 5 ~ 10 5 Radius of Sun 695500km Answer a) about 0001% Question 7 (15 points) An ars-sized planet transits in front of an 8 main-sequence star By how much will the star dim when the planet passes in front of it? a) about 0001% b) about 001% c) about 01% d) about 1% e) about 10% The radius of an 8 star according to my notes is 015 times the radius of the Sun Therefore

Radius of ars Dimming = 015 Radius of Sun Answer c) about 01% Extra Credit Questions: 3397 km = 015 695500km = 1060 10 3 ~ 10 3 Question 8 (30 points) Assume that the tidal locking radius as a function of the mass of the primary star is given by d lock = 04AU 1/ Sun where is the mass of the star For what primary masses will any planets in the optimistic habitable zone be tidally locked? (Hint: Adopt the mass-luminosity relationship I showed in class to derive a relationship between the habitable zone distance and primary mass) a) 011 Sun and below b) 05 Sun and below c) 038 Sun and below d) 089 Sun and below For the Sun the optimistic habitable zone extends out to 17 AU We can derive how this scales with the mass of the star using the fact that at fixed equilibrium temperature the distance should scale with the star s luminosity as d outer = L Star d outersun L Sun and adopting the mass-luminosity relation from class We can write L Star L Sun = Sun 4 1/

d outer = L Star d outersun L Sun 1/ = Sun 4 1/ = Sun To find the largest stellar mass for which all planets in the habitable zone are tidally locked we can just equate d outer in the expression above with d lock in the expression for the tidal locking radius given in the question text For the left hand side of the equation above we get d outer d outersun = d lock = 04AU d outersun 17 AU Sun 1/ = 0353 which we can now equate to the right hand side of the equation 0353 Sun 1/ = Sun Sun All that remains is to solve for After a small amount of algebra we get = 0353 Sun which we can easily solve for = (0353) /3 Sun = 038 Sun Answer c) 038 Sun and below 3/ 1/ Question 9 (30 points) The solar-like star Alpha Centauri is one of the closest stars to the Sun If Alpha Centauri were orbited by an Earth-mass planet near the outer edge of the optimistic habitable zone by what angle would Alpha Centauri appear to move back-and-forth as the Earth-mass planet completes its orbit? a) about 1 arcsecond b) about 01 arcseconds c) about 10-5 arcseconds d) about 001 arcseconds e) about 10 arcseconds

As the Earth-mass planet orbits Alpha Centauri the star will orbit about the common center-of-mass of the star-planet system The center of mass is offset a distance from the center of the star given by d Co = a Planet Star Where a is the semimajor axis of the planet We can assume that Alpha Centauri and the Sun are identical (this is not quite true but close enough for our purposes) Then the outer edge of the optimistic habitable zone for Alpha Centauri is the same as that for the Sun namely 17 AU The semimajor axis of the planet s orbit is then 17AU Since the center-of-mass distance is equal to the radius of the orbit the star will move by twice this value namely d wobble ~ d Co = a Planet ~ 17AU 5974 104 kg Star 19884 10 30 kg ~ 10 5 AU Where we ve assumed the mass Alpha Centauri is the same as that of the Sun Alpha Centauri is located at the distance of about 134 parsecs At this distance the wobble of the star corresponds to an angle θ on the sky of d θ = wobble 134 parsecs = 10 5 AU 134 parsecs 10 5 arcseconds Recall our first homework assignment and that one parsec is defined to be the distance at which one AU subtends on arcsecond Answer c) about 10-5 arcseconds