{"id":1084,"date":"2018-05-24T18:29:23","date_gmt":"2018-05-24T22:29:23","guid":{"rendered":"https:\/\/pressbooks.bccampus.ca\/a3600\/chapter\/29-7-the-anthropic-principle\/"},"modified":"2018-05-31T16:14:21","modified_gmt":"2018-05-31T20:14:21","slug":"29-7-the-anthropic-principle","status":"publish","type":"chapter","link":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/chapter\/29-7-the-anthropic-principle\/","title":{"raw":"29.7 The Anthropic Principle","rendered":"29.7 The Anthropic Principle"},"content":{"raw":"\n<div class=\"bcc-box bcc-highlight\">\n<h3>Learning Objectives<\/h3>\n<p id=\"fs-id1168582932412\">By the end of this section, you will be able to:<\/p>\n<ul id=\"fs-id1163975668742\">\n<li>Name some properties of the universe that, if different, would have precluded the development of humans<\/li>\n<\/ul>\n<\/div>\n<p id=\"fs-id1163974431855\">Despite our uncertainties, we must admit that the picture we have developed about the evolution of our universe is a remarkable one. With new telescopes, we have begun to collect enough observational evidence that we can describe how the universe evolved from a mere fraction of a second after the expansion began. Although this is an impressive achievement, there are still some characteristics of the universe that we cannot explain. And yet, it turns out that if these characteristics were any different, we would not be here to ask about them. Let\u2019s look at some of these \u201clucky accidents,\u201d beginning with the observations of the cosmic microwave background (CMB).<\/p>\n<section id=\"fs-id1163974429808\">\n<h1>Lucky Accidents<\/h1>\n<p id=\"fs-id1163975826179\">As we described in this chapter, the CMB is radiation that was emitted when the universe was a few hundred thousand years old. Observations show that the temperature of the radiation varies from one region to another, typically by about 10 millionths of a degree, and these temperature differences signal small differences in density. But suppose the tiny, early fluctuations in density had been much smaller. Then calculations show that the pull of gravity near them would have been so small that no galaxies would ever have formed.<\/p>\n<p id=\"fs-id1163974418616\">What if the fluctuations in density had been much larger? Then it is possible that very dense regions would have condensed, and these would simply have collapsed directly to black holes without ever forming galaxies and stars. Even if galaxies had been able to form in such a universe, space would have been filled with intense X-rays and gamma rays, and it would have been difficult for life forms to develop and survive. The density of stars within galaxies would be so high that interactions and collisions among them would be frequent. In such a universe, any planetary systems could rarely survive long enough for life to develop.<\/p>\n<p>So for us to be here, the density fluctuations need to be \u201cjust right\u201d\u2014not too big and not too small.<\/p>\n<p id=\"fs-id1163975741080\">Another lucky accident is that the universe is finely balanced between expansion and contraction. It is expanding, but very slowly. If the expansion had been at a much higher rate, all of the matter would have thinned out before galaxies could form. If everything were expanding at a much slower rate, then gravity would have \u201cwon.\u201d The expansion would have reversed and all of the matter would have recollapsed, probably into a black hole\u2014again, no stars, no planets, no life.<\/p>\n<p id=\"fs-id1163975738091\">The development of life on Earth depends on still-luckier coincidences. Had matter and <span class=\"no-emphasis\">antimatter<\/span> been present initially in exactly equal proportions, then all matter would have been annihilated and turned into pure energy. We owe our existence to the fact that there was slightly more matter than antimatter. (After most of the matter made contact with an equal amount of antimatter, turning into energy, a small amount of additional matter must have been present. We are all descendants of that bit of \u201cunbalanced\u201d matter.)<\/p>\n<p id=\"fs-id1163974285116\">If nuclear fusion reactions occurred at a somewhat faster rate than they actually do, then at the time of the initial fireball, all of the matter would have been converted from hydrogen into helium into carbon and all the way into iron (the most stable nucleus). That would mean that no stars would have formed, since the existence of stars depends on there being light elements that can undergo fusion in the main-sequence stage and make the stars shine. In addition, the structure of atomic nuclei had to be just right to make it possible for three helium atoms to come together easily to fuse carbon, which is the basis of life. If the <em>triple-alpha process<\/em> we discussed in the chapter on <a href=\"https:\/\/cnx.org\/contents\/2e737be8-ea65-48c3-aa0a-9f35b4c6a966@13.1:46b88c58-3f68-469e-98f0-ed46bc80f5a1@3\" class=\"target-chapter\">Stars from Adolescence to Old Age<\/a> were too unlikely, not enough carbon would have formed to lead to biology as we know it. At the same time, it had to be hard enough to fuse carbon into oxygen that a large amount of carbon survived for billions of years.<\/p>\n<p id=\"fs-id1163975673729\">There are additional factors that have contributed to life like us being possible. Neutrinos have to interact with matter at just the right, albeit infrequent, rate. Supernova explosions occur when <span class=\"no-emphasis\">neutrino<\/span>s escape from the cores of collapsing stars, deposit some of their energy in the surrounding stellar envelope, and cause it to blow out and away into space. The heavy elements that are ejected in such explosions are essential ingredients of life here on Earth. If neutrinos did not interact with matter at all, they would escape from the cores of collapsing stars without causing the explosion. If neutrinos interacted strongly with matter, they would remain trapped in the stellar core. In either case, the heavy elements would remain locked up inside the collapsing star.<\/p>\n<p id=\"fs-id1163974245734\">If gravity were a much stronger force than it is, stars could form with much smaller masses, and their lifetimes would be measured in years rather than billions of years. Chemical processes, on the other hand, would not be sped up if gravity were a stronger force, and so there would be no time for life to develop while stars were so short-lived. Even if life did develop in a stronger-gravity universe, life forms would have to be tiny or they could not stand up or move around.<\/p>\n<\/section>\n<section id=\"fs-id1163974552028\">\n<h1>What Had to Be, Had to Be<\/h1>\n<p id=\"fs-id1163974447113\">In summary, we see that a specific set of rules and conditions in the universe has allowed complexity and life on Earth to develop. As yet, we have no theory to explain why this \u201cright\u201d set of conditions occurred. For this reason, many scientists are beginning to accept an idea we call the anthropic principle\u2014namely, that the physical laws we observe must be what they are precisely because these are the only laws that allow for the existence of humans.<\/p>\n<p id=\"fs-id1163974188097\">Some scientists speculate that our universe is but one of countless universes, each with a different set of physical laws\u2014an idea that is sometimes referred to as the multiverse. Some of those universes might be stillborn, collapsing before any structure forms. Others may expand so quickly that they remain essentially featureless with no stars and galaxies. In other words, there may be a much larger multiverse that contains our own universe and many others. This multiverse (existing perhaps in more dimensions that we can become aware of) is infinite and eternal; it generates many, many inflating regions, each of which evolves into a separate universe, which may be completely unlike any of the other separate universes. Our universe is then the way it is because it is the only way it could be and have humans like ourselves in it to discover its properties and ask such questions.<\/p>\n<div id=\"fs-id1163975769687\" class=\"note astronomy link-to-learning\">\n<section>\n<div class=\"textbox shaded\">View the <a href=\"https:\/\/openstax.org\/l\/30mulcosinfla\" rel=\"nofollow\">2011 introductory talk<\/a> on the Multiverse and Cosmic Inflation by Dr. Anthony Aguirre of the University of California, part of the Silicon Valley Astronomy Lecture Series.<\/div>\n<\/section>\n<\/div>\n<p id=\"fs-id1163971955630\">It is difficult to know how to test these ideas since we can never make contact with any other universe. For most scientists, our discussion in this section borders on the philosophical and metaphysical. Perhaps in the future our understanding of physics will develop to the point that we can know why the gravitational constant is as strong as it is, why the universe is expanding at exactly the rate it is, and why all of the other \u201clucky accidents\u201d happened\u2014why they were inevitable and could be no other way. Then this anthropic idea would no longer be necessary. No one knows, however, whether we will ever have an explanation for why this universe works the way it does.<\/p>\n<p id=\"fs-id1163974320726\">We have come a long way in our voyage through the universe. We have learned a remarkable amount about <em>how<\/em> and <em>when<\/em> the cosmos came to be, but the question of <em>why<\/em> the universe is the way it is remains as elusive as ever.<\/p>\n<\/section>\n<section id=\"fs-id1163974182080\" class=\"summary\">\n<h1>Key Concepts and Summary<\/h1>\n<p>Recently, many cosmologists have noted that the existence of humans depends on the fact that many properties of the universe\u2014the size of density fluctuations in the early universe, the strength of gravity, the structure of atoms\u2014were just right. The idea that physical laws must be the way they are because otherwise we could not be here to measure them is called the anthropic principle. Some scientists speculate that there may be a multiverse of universes, in which ours is just one.<\/p>\n<\/section>\n<section id=\"fs-id1163975767119\" class=\"further-exploration\">\n<h1>For Further Exploration<\/h1>\n<section id=\"fs-id1163974333780\">\n<h2>Articles<\/h2>\n<p id=\"fs-id1163975376076\">Kruesi, L. \u201cCosmology: 5 Things You Need to Know.\u201d <em>Astronomy<\/em> (May 2007): 28. Five questions students often ask, and how modern cosmologists answer them.<\/p>\n<p id=\"fs-id1163975446232\">Kruesi, L. \u201cHow Planck Has Redefined the Universe.\u201d <em>Astronomy<\/em> (October 2013): 28. Good review of what this space mission has told us about the CMB and the universe.<\/p>\n<p id=\"fs-id1163975665255\">Lineweaver, C. &amp; Davis, T. \u201cMisconceptions about the Big Bang.\u201d <em>Scientific American<\/em> (March 2005): 36. Some basic ideas about modern cosmology clarified, using general relativity.<\/p>\n<p>Nadis, S. \u201cSizing Up Inflation.\u201d <em>Sky &amp; Telescope<\/em> (November 2005): 32. Nice review of the origin and modern variants on the inflationary idea.<\/p>\n<p>Nadis, S. \u201cHow We Could See Another Universe.\u201d <em>Astronomy<\/em> (June 2009): 24. On modern ideas about multiverses and how such bubbles of space-time might collide.<\/p>\n<p>Nadis, S. \u201cDark Energy\u2019s New Face: How Exploding Stars Are Changing our View.\u201d <em>Astronomy<\/em> (July 2012): 45. About our improving understanding of the complexities of type Ia supernovae.<\/p>\n<p id=\"fs-id1163975286947\">Naze, Y. \u201cThe Priest, the Universe, and the Big Bang.\u201d <em>Astronomy<\/em> (November 2007): 40. On the life and work of Georges Lema\u00eetre.<\/p>\n<p id=\"fs-id1163975727502\">Panek, R. \u201cGoing Over to the Dark Side.\u201d <em>Sky &amp; Telescope<\/em> (February 2009): 22. A history of the observations and theories about dark energy.<\/p>\n<p id=\"fs-id1163974347487\">Pendrick, D. \u201cIs the Big Bang in Trouble?\u201d <em>Astronomy<\/em> (April 2009): 48. This sensationally titled article is really more of a quick review of how modern ideas and observations are fleshing out the Big Bang hypothesis (and raising questions.)<\/p>\n<p id=\"fs-id1163975574719\">Reddy, F. \u201cHow the Universe Will End.\u201d <em>Astronomy<\/em> (September 2014): 38. Brief discussion of local and general future scenarios.<\/p>\n<p>Riess, A. and Turner, M. \u201cThe Expanding Universe: From Slowdown to Speedup.\u201d <em>Scientific American<\/em> (September 2008): 62.<\/p>\n<p>Turner, M. \u201cThe Origin of the Universe.\u201d <em>Scientific American<\/em> (September 2009): 36. An introduction to modern cosmology.<\/p>\n<\/section>\n<section id=\"fs-id1163975569284\">\n<h2>Websites<\/h2>\n<p id=\"fs-id1163975579232\">Cosmology Primer: https:\/\/preposterousuniverse.com\/cosmologyprimer\/. Caltech Astrophysicist Sean Carroll offers a non-technical site with brief overviews of many key topics in modern cosmology.<\/p>\n<p id=\"fs-id1163975534127\">Everyday Cosmology: http:\/\/cosmology.carnegiescience.edu\/. An educational website from the Carnegie Observatories with a timeline of cosmological discovery, background materials, and activities.<\/p>\n<p id=\"fs-id1163975360392\">How Big Is the Universe?: http:\/\/www.pbs.org\/wgbh\/nova\/space\/how-big-universe.html. A clear essay by a noted astronomer Brent Tully summarizes some key ideas in cosmology and introduces the notion of the acceleration of the universe.<\/p>\n<p>Universe 101: WMAP Mission Introduction to the Universe: http:\/\/map.gsfc.nasa.gov\/universe\/. Concise NASA primer on cosmological ideas from the WMAP mission team.<\/p>\n<p id=\"fs-id1163975661237\">Cosmic Times Project: http:\/\/cosmictimes.gsfc.nasa.gov\/. James Lochner and Barbara Mattson have compiled a rich resource of twentieth-century cosmology history in the form of news reports on key events, from NASA\u2019s Goddard Space Flight Center.<\/p>\n<\/section>\n<section id=\"fs-id1163974597124\">\n<h2>Videos<\/h2>\n<p id=\"fs-id1163975465582\">The Day We Found the Universe: http:\/\/www.cfa.harvard.edu\/events\/mon_video_archive09.html. Distinguished science writer Marcia Bartusiak discusses Hubble\u2019s work and the discovery of the expansion of the cosmos\u2014one of the Observatory Night lectures at the Harvard-Smithsonian Center for Astrophysics (53:46).<\/p>\n<p id=\"fs-id1163974215086\">Images of the Infant Universe: https:\/\/www.youtube.com\/watch?v=x0AqCwElyUk. Lloyd Knox\u2019s public talk on the latest discoveries about the CMB and what they mean for cosmology (1:16:00).<\/p>\n<p>Runaway Universe: https:\/\/www.youtube.com\/watch?v=kNYVFrnmcOU. Roger Blandford (Stanford Linear Accelerator Center) public lecture on the discovery and meaning of cosmic acceleration and dark energy (1:08:08).<\/p>\n<p id=\"fs-id1163975389678\">From the Big Bang to the Nobel Prize and on to the James Webb Space Telescope and the Discovery of Alien Life: http:\/\/svs.gsfc.nasa.gov\/vis\/a010000\/a010300\/a010370\/index.html. John Mather, NASA Goddard (1:01:02). His Nobel Prize talk from Dec. 8, 2006 can be found at http:\/\/www.nobelprize.org\/mediaplayer\/index.php?id=74&amp;view=1.<\/p>\n<p id=\"fs-id1163974318479\">Dark Energy and the Fate of the Universe: https:\/\/webcast.stsci.edu\/webcast\/detail.xhtml?talkid=1961&amp;parent=1. Adam Reiss (STScI), at the Space Telescope Science Institute (1:00:00).<\/p>\n<\/section>\n<\/section>\n<section id=\"fs-id1163975491281\" class=\"group-activities\">\n<h1>Collaborative Group Activities<\/h1>\n<ol id=\"fs-id1163975708743\">\n<li>This chapter deals with some pretty big questions and ideas. Some belief systems teach us that there are questions to which \u201cwe were not meant to know\u201d the answers. Other people feel that if our minds and instruments are capable of exploring a question, then it becomes part of our birthright as thinking human beings. Have your group discuss your personal reactions to discussing questions like the beginning of time and space, and the ultimate fate of the universe. Does it make you nervous to hear about scientists discussing these issues? Or is it exciting to know that we can now gather scientific evidence about the origin and fate of the cosmos? (In discussing this, you may find that members of your group strongly disagree; try to be respectful of others\u2019 points of view.)<\/li>\n<li>A popular model of the universe in the 1950s and 1960s was the so-called steady-state cosmology. In this model, the universe was not only the same everywhere and in all directions (homogeneous and isotropic), but also the same <em>at all times<\/em>. We know the universe is expanding and the galaxies are thinning out, and so this model hypothesized that new matter was continually coming into existence to fill in the space between galaxies as they moved farther apart. If so, the infinite universe did not have to have a sudden beginning, but could simply exist forever in a steady state. Have your group discuss your reaction to this model. Do you find it more appealing philosophically than the Big Bang model? Can you cite some evidence that indicates that the universe was not the same billions of years ago as it is now\u2014that it is not in a steady state?<\/li>\n<li>One of the lucky accidents that characterizes our universe is the fact that the time scale for the development of intelligent life on Earth and the lifetime of the Sun are comparable. Have your group discuss what would happen if the two time scales were very different. Suppose, for example, that the time for intelligent life to evolve was 10 times greater than the main-sequence lifetime of the Sun. Would our civilization have ever developed? Now suppose the time for intelligent life to evolve is ten times shorter than the main-sequence lifetime of the Sun. Would we be around? (This latter discussion requires considerable thought, including such ideas as what the early stages in the Sun\u2019s life were like and how much the early Earth was bombarded by asteroids and comets.)<\/li>\n<li>The grand ideas discussed in this chapter have a powerful effect on the human imagination, not just for scientists, but also for artists, composers, dramatists, and writers. Here we list just a few of these responses to cosmology. Each member of your group can select one of these, learn more about it, and then report back, either to the group or to the whole class.\n<ul id=\"fs-id1163974217055\">\n<li>The California poet Robinson Jeffers was the brother of an astronomer who worked at the Lick Observatory. His poem \u201cMargrave\u201d is a meditation on cosmology and on the kidnap and murder of a child: http:\/\/www.poemhunter.com\/best-poems\/robinson-jeffers\/margrave\/.<\/li>\n<li>In the science fiction story \u201cThe Gravity Mine\u201d by Stephen Baxter, the energy of evaporating supermassive black holes is the last hope of living beings in the far future in an ever-expanding universe. The story has poetic description of the ultimate fate of matter and life and is available online at: http:\/\/www.infinityplus.co.uk\/stories\/gravitymine.htm.<\/li>\n<li>The musical piece <em>YLEM<\/em> by Karlheinz Stockhausen takes its title from the ancient Greek term for primeval material revived by George Gamow. It tries to portray the oscillating universe in musical terms. Players actually expand through the concert hall, just as the universe does, and then return and expand again. See: http:\/\/www.karlheinzstockhausen.org\/ylem_english.htm.<\/li>\n<li>The musical piece <em>Supernova Sonata<\/em> http:\/\/www.astro.uvic.ca\/~alexhp\/new\/supernova_sonata.html by Alex Parker and Melissa Graham is based on the characteristics of 241 type Ia supernova explosions, the ones that have helped astronomers discover the acceleration of the expanding universe.<\/li>\n<li>Gregory Benford\u2019s short story \u201cThe Final Now\u201d envisions the end of an accelerating open universe, and blends religious and scientific imagery in a very poetic way. Available free online at: http:\/\/www.tor.com\/stories\/2010\/03\/the-final-now.<\/li>\n<\/ul>\n<\/li>\n<li>When Einstein learned about Hubble\u2019s work showing that the universe of galaxies is expanding, he called his introduction of the cosmological constant into his general theory of relativity his \u201cbiggest blunder.\u201d Can your group think of other \u201cbig blunders\u201d from the history of astronomy, where the thinking of astronomers was too conservative and the universe turned out to be more complicated or required more \u201coutside-the-box\u201d thinking?<\/li>\n<\/ol>\n<\/section>\n<section id=\"fs-id1163974183185\" class=\"review-questions\">\n<h1>Review Questions<\/h1>\n<div class=\"exercise\">\n<section>\n<div class=\"problem\">\n<p id=\"fs-id1163974419414\"><strong>1:<\/strong> What are the basic observations about the universe that any theory of cosmology must explain?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975571214\">\n<section>\n<div class=\"problem\">\n<p id=\"fs-id1163974178048\"><strong>2:<\/strong> Describe some possible futures for the universe that scientists have come up with. What property of the universe determines which of these possibilities is the correct one?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975770309\">\n<p id=\"fs-id1163975493844\"><strong>3:<\/strong> What does the term Hubble time mean in cosmology, and what is the current best calculation for the Hubble time?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974335761\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974230227\">\n<p><strong>4:<\/strong> Which formed first: hydrogen nuclei or hydrogen atoms? Explain the sequence of events that led to each.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975660888\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975531667\">\n<p id=\"fs-id1163974219597\"><strong>5:<\/strong> Describe at least two characteristics of the universe that are explained by the standard Big Bang model.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974318299\">\n<p><strong>6:<\/strong> Describe two properties of the universe that are not explained by the standard Big Bang model (without inflation). How does inflation explain these two properties?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974188367\">\n<p id=\"fs-id1163974352585\"><strong>7:<\/strong> Why do astronomers believe there must be dark matter that is not in the form of atoms with protons and neutrons?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974318006\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975705585\">\n<p id=\"fs-id1163975536867\"><strong>8:<\/strong> What is dark energy and what evidence do astronomers have that it is an important component of the universe?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163976539387\">\n<section>\n<div class=\"problem\" id=\"fs-id1163976458316\">\n<p id=\"fs-id1163976766205\"><strong>9:<\/strong> Thinking about the ideas of space and time in Einstein\u2019s general theory of relativity, how do we explain the fact that all galaxies outside our Local Group show a redshift?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163976748132\">\n<section>\n<div class=\"problem\" id=\"fs-id1163976407982\">\n<p id=\"fs-id1163976808195\"><strong>10:<\/strong> Astronomers have found that there is more helium in the universe than stars could have made in the 13.8 billion years that the universe has been in existence. How does the Big Bang scenario solve this problem?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975708965\">\n<p><strong>11:<\/strong> Describe the anthropic principle. What are some properties of the universe that make it \u201cready\u201d to have life forms like you in it?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163976632102\">\n<section>\n<div class=\"problem\" id=\"fs-id1163976857420\">\n<p id=\"fs-id1163973141179\"><strong>12:<\/strong> Describe the evidence that the expansion of the universe is accelerating.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<\/section>\n<section id=\"fs-id1163974245207\" class=\"thought-questions\">\n<h1>Thought Questions<\/h1>\n<div class=\"exercise\" id=\"fs-id1163975473448\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974284314\">\n<p id=\"fs-id1163975572404\"><strong>13:<\/strong> What is the most useful probe of the early evolution of the universe: a giant elliptical galaxy or an irregular galaxy such as the Large Magellanic Cloud? Why?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975825548\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975413162\">\n<p id=\"fs-id1163975531705\"><strong>14:<\/strong> What are the advantages and disadvantages of using quasars to probe the early history of the universe?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974639103\">\n<section>\n<div class=\"problem\">\n<p id=\"fs-id1163975481424\"><strong>15:<\/strong> Would acceleration of the universe occur if it were composed entirely of matter (that is, if there were no dark energy)?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975590978\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974375113\">\n<p id=\"fs-id1163975441589\"><strong>16:<\/strong> Suppose the universe expands forever. Describe what will become of the radiation from the primeval fireball. What will the future evolution of galaxies be like? Could life as we know it survive forever in such a universe? Why?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974412327\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974188449\">\n<p id=\"fs-id1163975451006\"><strong>17:<\/strong> Some theorists expected that observations would show that the density of matter in the universe is just equal to the critical density. Do the current observations support this hypothesis?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974340636\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975837957\">\n<p id=\"fs-id1163974343925\"><strong>18:<\/strong> There are a variety of ways of estimating the ages of various objects in the universe. Describe two of these ways, and indicate how well they agree with one another and with the age of the universe itself as estimated by its expansion.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974411668\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974258533\">\n<p id=\"fs-id1163974194108\"><strong>19:<\/strong> Since the time of <span class=\"no-emphasis\">Copernicus<\/span>, each revolution in astronomy has moved humans farther from the center of the universe. Now it appears that we may not even be made of the most common form of matter. Trace the changes in scientific thought about the central nature of Earth, the Sun, and our Galaxy on a cosmic scale. Explain how the notion that most of the universe is made of dark matter continues this \u201cCopernican tradition.\u201d<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974393618\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974550087\">\n<p id=\"fs-id1163972000574\"><strong>20:<\/strong> The anthropic principle suggests that in some sense we are observing a special kind of universe; if the universe were different, we could never have come to exist. Comment on how this fits with the Copernican tradition described in <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163974411668\" class=\"autogenerated-content\">Exercise<\/a>.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975840606\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974431259\">\n<p id=\"fs-id1163974176647\"><strong>21:<\/strong> Penzias and Wilson\u2019s discovery of the Cosmic Microwave Background (CMB) is a nice example of scientific <em>serendipity<\/em>\u2014something that is found by chance but turns out to have a positive outcome. What were they looking for and what did they discover?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974541815\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974184170\">\n<p id=\"fs-id1163975741498\"><strong>22:<\/strong> Construct a timeline for the universe and indicate when various significant events occurred, from the beginning of the expansion to the formation of the Sun to the appearance of humans on Earth.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<\/section>\n<section id=\"fs-id1163974220018\" class=\"figuring-for-yourself\">\n<h1>Figuring for Yourself<\/h1>\n<div class=\"exercise\" id=\"fs-id1163974343982\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975472994\">\n<p id=\"fs-id1163975638730\"><strong>23:<\/strong> Suppose the Hubble constant were not 22 but 33 km\/s per million light-years. Then what would the critical density be?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975581676\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975575041\">\n<p id=\"fs-id1163974264853\"><strong>24:<\/strong> Assume that the average galaxy contains 10<sup>11<\/sup> <em>M<\/em><sub>Sun<\/sub> and that the average distance between galaxies is 10 million light-years. Calculate the average density of matter (mass per unit volume) in galaxies. What fraction is this of the critical density we calculated in the chapter?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974406483\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974273046\">\n<p id=\"fs-id1163974172674\"><strong>25:<\/strong> The CMB contains roughly 400 million photons per m<sup>3<\/sup>. The energy of each photon depends on its wavelength. Calculate the typical wavelength of a CMB photon. Hint: The CMB is blackbody radiation at a temperature of 2.73 K. According to Wien\u2019s law, the peak wave length in nanometers is given by <span class=\"MathJax_Preview\"><\/span><span class=\"MathJax\" id=\"MathJax-Element-1-Frame\" role=\"presentation\" style=\"font-style: normal;font-weight: normal;line-height: normal;font-size: 14px;text-indent: 0px;text-align: left;letter-spacing: normal;float: none;direction: ltr;max-width: none;max-height: none;min-width: 0px;min-height: 0px;border: 0px;padding: 0px;margin: 0px\"><span class=\"math\" id=\"MathJax-Span-1\" role=\"math\"><span class=\"mrow\" id=\"MathJax-Span-2\"><span class=\"semantics\" id=\"MathJax-Span-3\"><span class=\"mrow\" id=\"MathJax-Span-4\"><span class=\"mrow\" id=\"MathJax-Span-5\"><span class=\"msub\" id=\"MathJax-Span-6\"><span class=\"mtext\" id=\"MathJax-Span-7\">\u03bb<\/span><span class=\"mrow\" id=\"MathJax-Span-8\"><span class=\"mtext\" id=\"MathJax-Span-9\">max<\/span><\/span><\/span><span class=\"mo\" id=\"MathJax-Span-10\">=<\/span><span class=\"mfrac\" id=\"MathJax-Span-11\"><span class=\"mrow\" id=\"MathJax-Span-12\"><span class=\"mn\" id=\"MathJax-Span-13\">3<\/span><span class=\"mspace\" id=\"MathJax-Span-14\"><\/span><span class=\"mo\" id=\"MathJax-Span-15\">\u00d7<\/span><span class=\"mspace\" id=\"MathJax-Span-16\"><\/span><span class=\"msup\" id=\"MathJax-Span-17\"><span class=\"mrow\" id=\"MathJax-Span-18\"><span class=\"mn\" id=\"MathJax-Span-19\">10<\/span><\/span><span class=\"mn\" id=\"MathJax-Span-20\">6<\/span><\/span><\/span><span class=\"mrow\" id=\"MathJax-Span-21\"><span class=\"mi\" id=\"MathJax-Span-22\">T<\/span><\/span><\/span><span class=\"mo\" id=\"MathJax-Span-23\">.<\/span><\/span><\/span><\/span><\/span><\/span><\/span><span class=\"MJX_Assistive_MathML\" role=\"presentation\">\u03bbmax=3\u00d7106T.<\/span> Calculate the wavelength at which the CMB is a maximum and, to make the units consistent, convert this wavelength from nanometers to meters.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975655088\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975433445\">\n<p id=\"fs-id1163975741435\"><strong>26:<\/strong> Following up on <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163974369405\" class=\"autogenerated-content\">Exercise<\/a> calculate the energy of a typical photon. Assume for this approximate calculation that each photon has the wavelength calculated in <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163974406483\" class=\"autogenerated-content\">Exercise<\/a>. The energy of a photon is given by <span class=\"MathJax_Preview\"><\/span><span class=\"MathJax\" id=\"MathJax-Element-2-Frame\" role=\"presentation\" style=\"font-style: normal;font-weight: normal;line-height: normal;font-size: 14px;text-indent: 0px;text-align: left;letter-spacing: normal;float: none;direction: ltr;max-width: none;max-height: none;min-width: 0px;min-height: 0px;border: 0px;padding: 0px;margin: 0px\"><span class=\"math\" id=\"MathJax-Span-24\" role=\"math\"><span class=\"mrow\" id=\"MathJax-Span-25\"><span class=\"semantics\" id=\"MathJax-Span-26\"><span class=\"mrow\" id=\"MathJax-Span-27\"><span class=\"mrow\" id=\"MathJax-Span-28\"><span class=\"mi\" id=\"MathJax-Span-29\">E<\/span><span class=\"mo\" id=\"MathJax-Span-30\">=<\/span><span class=\"mfrac\" id=\"MathJax-Span-31\"><span class=\"mrow\" id=\"MathJax-Span-32\"><span class=\"mi\" id=\"MathJax-Span-33\">h<\/span><span class=\"mi\" id=\"MathJax-Span-34\">c<\/span><\/span><span class=\"mtext\" id=\"MathJax-Span-35\">\u03bb<\/span><\/span><span class=\"mo\" id=\"MathJax-Span-36\">,<\/span><\/span><\/span><\/span><\/span><\/span><\/span><span class=\"MJX_Assistive_MathML\" role=\"presentation\">E=hc\u03bb,<\/span>where <em>h<\/em> is Planck\u2019s constant and is equal to 6.626 \u00d7 10<sup>\u201334<\/sup> J \u00d7 s, <em>c<\/em> is the speed of light in m\/s, and \u03bb is the wavelength in m.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974369405\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974220870\">\n<p id=\"fs-id1163975544550\"><strong>27:<\/strong> Continuing the thinking in <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163974369405\" class=\"autogenerated-content\">Exercise<\/a> and <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163975364885\" class=\"autogenerated-content\">Exercise<\/a>, calculate the energy in a cubic meter of space, multiply the energy per photon calculated in <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163975655088\" class=\"autogenerated-content\">Exercise<\/a> by the number of photons per cubic meter given above.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975364885\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974361252\">\n<p id=\"fs-id1163975454003\"><strong>28:<\/strong> Continuing the thinking in the last three exercises, convert this energy to an equivalent in mass, use Einstein\u2019s equation <em>E<\/em> = <em>mc<\/em><sup>2<\/sup>. Hint: Divide the energy per m<sup>3<\/sup> calculated in <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163974369405\" class=\"autogenerated-content\">Exercise<\/a> by the speed of light squared. Check your units; you should have an answer in kg\/m<sup>3<\/sup>. Now compare this answer with the critical density. Your answer should be several powers of 10 smaller than the critical density. In other words, you have found for yourself that the contribution of the CMB photons to the overall density of the universe is much, much smaller than the contribution made by stars and galaxies.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975727734\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975361222\">\n<p id=\"fs-id1163974195725\"><strong>29:<\/strong> There is still some uncertainty in the Hubble constant. (a) Current estimates range from about 19.9 km\/s per million light-years to 23 km\/s per million light-years. Assume that the Hubble constant has been constant since the Big Bang. What is the possible range in the ages of the universe? Use the equation in the text, <span class=\"MathJax_Preview\"><\/span><span class=\"MathJax\" id=\"MathJax-Element-3-Frame\" role=\"presentation\" style=\"font-style: normal;font-weight: normal;line-height: normal;font-size: 14px;text-indent: 0px;text-align: left;letter-spacing: normal;float: none;direction: ltr;max-width: none;max-height: none;min-width: 0px;min-height: 0px;border: 0px;padding: 0px;margin: 0px\"><span class=\"math\" id=\"MathJax-Span-37\" role=\"math\"><span class=\"mrow\" id=\"MathJax-Span-38\"><span class=\"semantics\" id=\"MathJax-Span-39\"><span class=\"mrow\" id=\"MathJax-Span-40\"><span class=\"mrow\" id=\"MathJax-Span-41\"><span class=\"msub\" id=\"MathJax-Span-42\"><span class=\"mi\" id=\"MathJax-Span-43\">T<\/span><span class=\"mn\" id=\"MathJax-Span-44\">0<\/span><\/span><span class=\"mo\" id=\"MathJax-Span-45\">=<\/span><span class=\"mfrac\" id=\"MathJax-Span-46\"><span class=\"mn\" id=\"MathJax-Span-47\">1<\/span><span class=\"mi\" id=\"MathJax-Span-48\">H<\/span><\/span><span class=\"mo\" id=\"MathJax-Span-49\">,<\/span><\/span><\/span><\/span><\/span><\/span><\/span><span class=\"MJX_Assistive_MathML\" role=\"presentation\">T0=1H,<\/span> and make sure you use consistent units. (b) Twenty years ago, estimates for the Hubble constant ranged from 50 to 100 km\/s per Mps. What are the possible ages for the universe from those values? Can you rule out some of these possibilities on the basis of other evidence?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974171126\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975658340\">\n<p id=\"fs-id1163975465099\"><strong>30:<\/strong> It is possible to derive the age of the universe given the value of the Hubble constant and the distance to a galaxy, again with the assumption that the value of the Hubble constant has not changed since the Big Bang. Consider a galaxy at a distance of 400 million light-years receding from us at a velocity, <em>v<\/em>. If the Hubble constant is 20 km\/s per million light-years, what is its velocity? How long ago was that galaxy right next door to our own Galaxy if it has always been receding at its present rate? Express your answer in years. Since the universe began when all galaxies were very close together, this number is a rough estimate for the age of the universe.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<\/section>\n<div>\n<h2>Glossary<\/h2>\n<dl id=\"fs-id1163975635844\" class=\"definition\">\n<dt>anthropic principle<\/dt>\n<dd id=\"fs-id1163975577923\">idea that physical laws must be the way they are because otherwise we could not be here to measure them<\/dd>\n<\/dl>\n<dl id=\"fs-id1163975661940\" class=\"definition\">\n<dt>multiverse<\/dt>\n<dd id=\"fs-id1163974191028\">the speculative idea that our universe is just one of many universes, each with its own set of physical laws<\/dd>\n<\/dl>\n<\/div>\n\n","rendered":"<div class=\"bcc-box bcc-highlight\">\n<h3>Learning Objectives<\/h3>\n<p id=\"fs-id1168582932412\">By the end of this section, you will be able to:<\/p>\n<ul id=\"fs-id1163975668742\">\n<li>Name some properties of the universe that, if different, would have precluded the development of humans<\/li>\n<\/ul>\n<\/div>\n<p id=\"fs-id1163974431855\">Despite our uncertainties, we must admit that the picture we have developed about the evolution of our universe is a remarkable one. With new telescopes, we have begun to collect enough observational evidence that we can describe how the universe evolved from a mere fraction of a second after the expansion began. Although this is an impressive achievement, there are still some characteristics of the universe that we cannot explain. And yet, it turns out that if these characteristics were any different, we would not be here to ask about them. Let\u2019s look at some of these \u201clucky accidents,\u201d beginning with the observations of the cosmic microwave background (CMB).<\/p>\n<section id=\"fs-id1163974429808\">\n<h1>Lucky Accidents<\/h1>\n<p id=\"fs-id1163975826179\">As we described in this chapter, the CMB is radiation that was emitted when the universe was a few hundred thousand years old. Observations show that the temperature of the radiation varies from one region to another, typically by about 10 millionths of a degree, and these temperature differences signal small differences in density. But suppose the tiny, early fluctuations in density had been much smaller. Then calculations show that the pull of gravity near them would have been so small that no galaxies would ever have formed.<\/p>\n<p id=\"fs-id1163974418616\">What if the fluctuations in density had been much larger? Then it is possible that very dense regions would have condensed, and these would simply have collapsed directly to black holes without ever forming galaxies and stars. Even if galaxies had been able to form in such a universe, space would have been filled with intense X-rays and gamma rays, and it would have been difficult for life forms to develop and survive. The density of stars within galaxies would be so high that interactions and collisions among them would be frequent. In such a universe, any planetary systems could rarely survive long enough for life to develop.<\/p>\n<p>So for us to be here, the density fluctuations need to be \u201cjust right\u201d\u2014not too big and not too small.<\/p>\n<p id=\"fs-id1163975741080\">Another lucky accident is that the universe is finely balanced between expansion and contraction. It is expanding, but very slowly. If the expansion had been at a much higher rate, all of the matter would have thinned out before galaxies could form. If everything were expanding at a much slower rate, then gravity would have \u201cwon.\u201d The expansion would have reversed and all of the matter would have recollapsed, probably into a black hole\u2014again, no stars, no planets, no life.<\/p>\n<p id=\"fs-id1163975738091\">The development of life on Earth depends on still-luckier coincidences. Had matter and <span class=\"no-emphasis\">antimatter<\/span> been present initially in exactly equal proportions, then all matter would have been annihilated and turned into pure energy. We owe our existence to the fact that there was slightly more matter than antimatter. (After most of the matter made contact with an equal amount of antimatter, turning into energy, a small amount of additional matter must have been present. We are all descendants of that bit of \u201cunbalanced\u201d matter.)<\/p>\n<p id=\"fs-id1163974285116\">If nuclear fusion reactions occurred at a somewhat faster rate than they actually do, then at the time of the initial fireball, all of the matter would have been converted from hydrogen into helium into carbon and all the way into iron (the most stable nucleus). That would mean that no stars would have formed, since the existence of stars depends on there being light elements that can undergo fusion in the main-sequence stage and make the stars shine. In addition, the structure of atomic nuclei had to be just right to make it possible for three helium atoms to come together easily to fuse carbon, which is the basis of life. If the <em>triple-alpha process<\/em> we discussed in the chapter on <a href=\"https:\/\/cnx.org\/contents\/2e737be8-ea65-48c3-aa0a-9f35b4c6a966@13.1:46b88c58-3f68-469e-98f0-ed46bc80f5a1@3\" class=\"target-chapter\">Stars from Adolescence to Old Age<\/a> were too unlikely, not enough carbon would have formed to lead to biology as we know it. At the same time, it had to be hard enough to fuse carbon into oxygen that a large amount of carbon survived for billions of years.<\/p>\n<p id=\"fs-id1163975673729\">There are additional factors that have contributed to life like us being possible. Neutrinos have to interact with matter at just the right, albeit infrequent, rate. Supernova explosions occur when <span class=\"no-emphasis\">neutrino<\/span>s escape from the cores of collapsing stars, deposit some of their energy in the surrounding stellar envelope, and cause it to blow out and away into space. The heavy elements that are ejected in such explosions are essential ingredients of life here on Earth. If neutrinos did not interact with matter at all, they would escape from the cores of collapsing stars without causing the explosion. If neutrinos interacted strongly with matter, they would remain trapped in the stellar core. In either case, the heavy elements would remain locked up inside the collapsing star.<\/p>\n<p id=\"fs-id1163974245734\">If gravity were a much stronger force than it is, stars could form with much smaller masses, and their lifetimes would be measured in years rather than billions of years. Chemical processes, on the other hand, would not be sped up if gravity were a stronger force, and so there would be no time for life to develop while stars were so short-lived. Even if life did develop in a stronger-gravity universe, life forms would have to be tiny or they could not stand up or move around.<\/p>\n<\/section>\n<section id=\"fs-id1163974552028\">\n<h1>What Had to Be, Had to Be<\/h1>\n<p id=\"fs-id1163974447113\">In summary, we see that a specific set of rules and conditions in the universe has allowed complexity and life on Earth to develop. As yet, we have no theory to explain why this \u201cright\u201d set of conditions occurred. For this reason, many scientists are beginning to accept an idea we call the anthropic principle\u2014namely, that the physical laws we observe must be what they are precisely because these are the only laws that allow for the existence of humans.<\/p>\n<p id=\"fs-id1163974188097\">Some scientists speculate that our universe is but one of countless universes, each with a different set of physical laws\u2014an idea that is sometimes referred to as the multiverse. Some of those universes might be stillborn, collapsing before any structure forms. Others may expand so quickly that they remain essentially featureless with no stars and galaxies. In other words, there may be a much larger multiverse that contains our own universe and many others. This multiverse (existing perhaps in more dimensions that we can become aware of) is infinite and eternal; it generates many, many inflating regions, each of which evolves into a separate universe, which may be completely unlike any of the other separate universes. Our universe is then the way it is because it is the only way it could be and have humans like ourselves in it to discover its properties and ask such questions.<\/p>\n<div id=\"fs-id1163975769687\" class=\"note astronomy link-to-learning\">\n<section>\n<div class=\"textbox shaded\">View the <a href=\"https:\/\/openstax.org\/l\/30mulcosinfla\" rel=\"nofollow\">2011 introductory talk<\/a> on the Multiverse and Cosmic Inflation by Dr. Anthony Aguirre of the University of California, part of the Silicon Valley Astronomy Lecture Series.<\/div>\n<\/section>\n<\/div>\n<p id=\"fs-id1163971955630\">It is difficult to know how to test these ideas since we can never make contact with any other universe. For most scientists, our discussion in this section borders on the philosophical and metaphysical. Perhaps in the future our understanding of physics will develop to the point that we can know why the gravitational constant is as strong as it is, why the universe is expanding at exactly the rate it is, and why all of the other \u201clucky accidents\u201d happened\u2014why they were inevitable and could be no other way. Then this anthropic idea would no longer be necessary. No one knows, however, whether we will ever have an explanation for why this universe works the way it does.<\/p>\n<p id=\"fs-id1163974320726\">We have come a long way in our voyage through the universe. We have learned a remarkable amount about <em>how<\/em> and <em>when<\/em> the cosmos came to be, but the question of <em>why<\/em> the universe is the way it is remains as elusive as ever.<\/p>\n<\/section>\n<section id=\"fs-id1163974182080\" class=\"summary\">\n<h1>Key Concepts and Summary<\/h1>\n<p>Recently, many cosmologists have noted that the existence of humans depends on the fact that many properties of the universe\u2014the size of density fluctuations in the early universe, the strength of gravity, the structure of atoms\u2014were just right. The idea that physical laws must be the way they are because otherwise we could not be here to measure them is called the anthropic principle. Some scientists speculate that there may be a multiverse of universes, in which ours is just one.<\/p>\n<\/section>\n<section id=\"fs-id1163975767119\" class=\"further-exploration\">\n<h1>For Further Exploration<\/h1>\n<section id=\"fs-id1163974333780\">\n<h2>Articles<\/h2>\n<p id=\"fs-id1163975376076\">Kruesi, L. \u201cCosmology: 5 Things You Need to Know.\u201d <em>Astronomy<\/em> (May 2007): 28. Five questions students often ask, and how modern cosmologists answer them.<\/p>\n<p id=\"fs-id1163975446232\">Kruesi, L. \u201cHow Planck Has Redefined the Universe.\u201d <em>Astronomy<\/em> (October 2013): 28. Good review of what this space mission has told us about the CMB and the universe.<\/p>\n<p id=\"fs-id1163975665255\">Lineweaver, C. &amp; Davis, T. \u201cMisconceptions about the Big Bang.\u201d <em>Scientific American<\/em> (March 2005): 36. Some basic ideas about modern cosmology clarified, using general relativity.<\/p>\n<p>Nadis, S. \u201cSizing Up Inflation.\u201d <em>Sky &amp; Telescope<\/em> (November 2005): 32. Nice review of the origin and modern variants on the inflationary idea.<\/p>\n<p>Nadis, S. \u201cHow We Could See Another Universe.\u201d <em>Astronomy<\/em> (June 2009): 24. On modern ideas about multiverses and how such bubbles of space-time might collide.<\/p>\n<p>Nadis, S. \u201cDark Energy\u2019s New Face: How Exploding Stars Are Changing our View.\u201d <em>Astronomy<\/em> (July 2012): 45. About our improving understanding of the complexities of type Ia supernovae.<\/p>\n<p id=\"fs-id1163975286947\">Naze, Y. \u201cThe Priest, the Universe, and the Big Bang.\u201d <em>Astronomy<\/em> (November 2007): 40. On the life and work of Georges Lema\u00eetre.<\/p>\n<p id=\"fs-id1163975727502\">Panek, R. \u201cGoing Over to the Dark Side.\u201d <em>Sky &amp; Telescope<\/em> (February 2009): 22. A history of the observations and theories about dark energy.<\/p>\n<p id=\"fs-id1163974347487\">Pendrick, D. \u201cIs the Big Bang in Trouble?\u201d <em>Astronomy<\/em> (April 2009): 48. This sensationally titled article is really more of a quick review of how modern ideas and observations are fleshing out the Big Bang hypothesis (and raising questions.)<\/p>\n<p id=\"fs-id1163975574719\">Reddy, F. \u201cHow the Universe Will End.\u201d <em>Astronomy<\/em> (September 2014): 38. Brief discussion of local and general future scenarios.<\/p>\n<p>Riess, A. and Turner, M. \u201cThe Expanding Universe: From Slowdown to Speedup.\u201d <em>Scientific American<\/em> (September 2008): 62.<\/p>\n<p>Turner, M. \u201cThe Origin of the Universe.\u201d <em>Scientific American<\/em> (September 2009): 36. An introduction to modern cosmology.<\/p>\n<\/section>\n<section id=\"fs-id1163975569284\">\n<h2>Websites<\/h2>\n<p id=\"fs-id1163975579232\">Cosmology Primer: https:\/\/preposterousuniverse.com\/cosmologyprimer\/. Caltech Astrophysicist Sean Carroll offers a non-technical site with brief overviews of many key topics in modern cosmology.<\/p>\n<p id=\"fs-id1163975534127\">Everyday Cosmology: http:\/\/cosmology.carnegiescience.edu\/. An educational website from the Carnegie Observatories with a timeline of cosmological discovery, background materials, and activities.<\/p>\n<p id=\"fs-id1163975360392\">How Big Is the Universe?: http:\/\/www.pbs.org\/wgbh\/nova\/space\/how-big-universe.html. A clear essay by a noted astronomer Brent Tully summarizes some key ideas in cosmology and introduces the notion of the acceleration of the universe.<\/p>\n<p>Universe 101: WMAP Mission Introduction to the Universe: http:\/\/map.gsfc.nasa.gov\/universe\/. Concise NASA primer on cosmological ideas from the WMAP mission team.<\/p>\n<p id=\"fs-id1163975661237\">Cosmic Times Project: http:\/\/cosmictimes.gsfc.nasa.gov\/. James Lochner and Barbara Mattson have compiled a rich resource of twentieth-century cosmology history in the form of news reports on key events, from NASA\u2019s Goddard Space Flight Center.<\/p>\n<\/section>\n<section id=\"fs-id1163974597124\">\n<h2>Videos<\/h2>\n<p id=\"fs-id1163975465582\">The Day We Found the Universe: http:\/\/www.cfa.harvard.edu\/events\/mon_video_archive09.html. Distinguished science writer Marcia Bartusiak discusses Hubble\u2019s work and the discovery of the expansion of the cosmos\u2014one of the Observatory Night lectures at the Harvard-Smithsonian Center for Astrophysics (53:46).<\/p>\n<p id=\"fs-id1163974215086\">Images of the Infant Universe: https:\/\/www.youtube.com\/watch?v=x0AqCwElyUk. Lloyd Knox\u2019s public talk on the latest discoveries about the CMB and what they mean for cosmology (1:16:00).<\/p>\n<p>Runaway Universe: https:\/\/www.youtube.com\/watch?v=kNYVFrnmcOU. Roger Blandford (Stanford Linear Accelerator Center) public lecture on the discovery and meaning of cosmic acceleration and dark energy (1:08:08).<\/p>\n<p id=\"fs-id1163975389678\">From the Big Bang to the Nobel Prize and on to the James Webb Space Telescope and the Discovery of Alien Life: http:\/\/svs.gsfc.nasa.gov\/vis\/a010000\/a010300\/a010370\/index.html. John Mather, NASA Goddard (1:01:02). His Nobel Prize talk from Dec. 8, 2006 can be found at http:\/\/www.nobelprize.org\/mediaplayer\/index.php?id=74&amp;view=1.<\/p>\n<p id=\"fs-id1163974318479\">Dark Energy and the Fate of the Universe: https:\/\/webcast.stsci.edu\/webcast\/detail.xhtml?talkid=1961&amp;parent=1. Adam Reiss (STScI), at the Space Telescope Science Institute (1:00:00).<\/p>\n<\/section>\n<\/section>\n<section id=\"fs-id1163975491281\" class=\"group-activities\">\n<h1>Collaborative Group Activities<\/h1>\n<ol id=\"fs-id1163975708743\">\n<li>This chapter deals with some pretty big questions and ideas. Some belief systems teach us that there are questions to which \u201cwe were not meant to know\u201d the answers. Other people feel that if our minds and instruments are capable of exploring a question, then it becomes part of our birthright as thinking human beings. Have your group discuss your personal reactions to discussing questions like the beginning of time and space, and the ultimate fate of the universe. Does it make you nervous to hear about scientists discussing these issues? Or is it exciting to know that we can now gather scientific evidence about the origin and fate of the cosmos? (In discussing this, you may find that members of your group strongly disagree; try to be respectful of others\u2019 points of view.)<\/li>\n<li>A popular model of the universe in the 1950s and 1960s was the so-called steady-state cosmology. In this model, the universe was not only the same everywhere and in all directions (homogeneous and isotropic), but also the same <em>at all times<\/em>. We know the universe is expanding and the galaxies are thinning out, and so this model hypothesized that new matter was continually coming into existence to fill in the space between galaxies as they moved farther apart. If so, the infinite universe did not have to have a sudden beginning, but could simply exist forever in a steady state. Have your group discuss your reaction to this model. Do you find it more appealing philosophically than the Big Bang model? Can you cite some evidence that indicates that the universe was not the same billions of years ago as it is now\u2014that it is not in a steady state?<\/li>\n<li>One of the lucky accidents that characterizes our universe is the fact that the time scale for the development of intelligent life on Earth and the lifetime of the Sun are comparable. Have your group discuss what would happen if the two time scales were very different. Suppose, for example, that the time for intelligent life to evolve was 10 times greater than the main-sequence lifetime of the Sun. Would our civilization have ever developed? Now suppose the time for intelligent life to evolve is ten times shorter than the main-sequence lifetime of the Sun. Would we be around? (This latter discussion requires considerable thought, including such ideas as what the early stages in the Sun\u2019s life were like and how much the early Earth was bombarded by asteroids and comets.)<\/li>\n<li>The grand ideas discussed in this chapter have a powerful effect on the human imagination, not just for scientists, but also for artists, composers, dramatists, and writers. Here we list just a few of these responses to cosmology. Each member of your group can select one of these, learn more about it, and then report back, either to the group or to the whole class.\n<ul id=\"fs-id1163974217055\">\n<li>The California poet Robinson Jeffers was the brother of an astronomer who worked at the Lick Observatory. His poem \u201cMargrave\u201d is a meditation on cosmology and on the kidnap and murder of a child: http:\/\/www.poemhunter.com\/best-poems\/robinson-jeffers\/margrave\/.<\/li>\n<li>In the science fiction story \u201cThe Gravity Mine\u201d by Stephen Baxter, the energy of evaporating supermassive black holes is the last hope of living beings in the far future in an ever-expanding universe. The story has poetic description of the ultimate fate of matter and life and is available online at: http:\/\/www.infinityplus.co.uk\/stories\/gravitymine.htm.<\/li>\n<li>The musical piece <em>YLEM<\/em> by Karlheinz Stockhausen takes its title from the ancient Greek term for primeval material revived by George Gamow. It tries to portray the oscillating universe in musical terms. Players actually expand through the concert hall, just as the universe does, and then return and expand again. See: http:\/\/www.karlheinzstockhausen.org\/ylem_english.htm.<\/li>\n<li>The musical piece <em>Supernova Sonata<\/em> http:\/\/www.astro.uvic.ca\/~alexhp\/new\/supernova_sonata.html by Alex Parker and Melissa Graham is based on the characteristics of 241 type Ia supernova explosions, the ones that have helped astronomers discover the acceleration of the expanding universe.<\/li>\n<li>Gregory Benford\u2019s short story \u201cThe Final Now\u201d envisions the end of an accelerating open universe, and blends religious and scientific imagery in a very poetic way. Available free online at: http:\/\/www.tor.com\/stories\/2010\/03\/the-final-now.<\/li>\n<\/ul>\n<\/li>\n<li>When Einstein learned about Hubble\u2019s work showing that the universe of galaxies is expanding, he called his introduction of the cosmological constant into his general theory of relativity his \u201cbiggest blunder.\u201d Can your group think of other \u201cbig blunders\u201d from the history of astronomy, where the thinking of astronomers was too conservative and the universe turned out to be more complicated or required more \u201coutside-the-box\u201d thinking?<\/li>\n<\/ol>\n<\/section>\n<section id=\"fs-id1163974183185\" class=\"review-questions\">\n<h1>Review Questions<\/h1>\n<div class=\"exercise\">\n<section>\n<div class=\"problem\">\n<p id=\"fs-id1163974419414\"><strong>1:<\/strong> What are the basic observations about the universe that any theory of cosmology must explain?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975571214\">\n<section>\n<div class=\"problem\">\n<p id=\"fs-id1163974178048\"><strong>2:<\/strong> Describe some possible futures for the universe that scientists have come up with. What property of the universe determines which of these possibilities is the correct one?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975770309\">\n<p id=\"fs-id1163975493844\"><strong>3:<\/strong> What does the term Hubble time mean in cosmology, and what is the current best calculation for the Hubble time?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974335761\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974230227\">\n<p><strong>4:<\/strong> Which formed first: hydrogen nuclei or hydrogen atoms? Explain the sequence of events that led to each.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975660888\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975531667\">\n<p id=\"fs-id1163974219597\"><strong>5:<\/strong> Describe at least two characteristics of the universe that are explained by the standard Big Bang model.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974318299\">\n<p><strong>6:<\/strong> Describe two properties of the universe that are not explained by the standard Big Bang model (without inflation). How does inflation explain these two properties?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974188367\">\n<p id=\"fs-id1163974352585\"><strong>7:<\/strong> Why do astronomers believe there must be dark matter that is not in the form of atoms with protons and neutrons?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974318006\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975705585\">\n<p id=\"fs-id1163975536867\"><strong>8:<\/strong> What is dark energy and what evidence do astronomers have that it is an important component of the universe?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163976539387\">\n<section>\n<div class=\"problem\" id=\"fs-id1163976458316\">\n<p id=\"fs-id1163976766205\"><strong>9:<\/strong> Thinking about the ideas of space and time in Einstein\u2019s general theory of relativity, how do we explain the fact that all galaxies outside our Local Group show a redshift?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163976748132\">\n<section>\n<div class=\"problem\" id=\"fs-id1163976407982\">\n<p id=\"fs-id1163976808195\"><strong>10:<\/strong> Astronomers have found that there is more helium in the universe than stars could have made in the 13.8 billion years that the universe has been in existence. How does the Big Bang scenario solve this problem?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975708965\">\n<p><strong>11:<\/strong> Describe the anthropic principle. What are some properties of the universe that make it \u201cready\u201d to have life forms like you in it?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163976632102\">\n<section>\n<div class=\"problem\" id=\"fs-id1163976857420\">\n<p id=\"fs-id1163973141179\"><strong>12:<\/strong> Describe the evidence that the expansion of the universe is accelerating.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<\/section>\n<section id=\"fs-id1163974245207\" class=\"thought-questions\">\n<h1>Thought Questions<\/h1>\n<div class=\"exercise\" id=\"fs-id1163975473448\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974284314\">\n<p id=\"fs-id1163975572404\"><strong>13:<\/strong> What is the most useful probe of the early evolution of the universe: a giant elliptical galaxy or an irregular galaxy such as the Large Magellanic Cloud? Why?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975825548\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975413162\">\n<p id=\"fs-id1163975531705\"><strong>14:<\/strong> What are the advantages and disadvantages of using quasars to probe the early history of the universe?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974639103\">\n<section>\n<div class=\"problem\">\n<p id=\"fs-id1163975481424\"><strong>15:<\/strong> Would acceleration of the universe occur if it were composed entirely of matter (that is, if there were no dark energy)?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975590978\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974375113\">\n<p id=\"fs-id1163975441589\"><strong>16:<\/strong> Suppose the universe expands forever. Describe what will become of the radiation from the primeval fireball. What will the future evolution of galaxies be like? Could life as we know it survive forever in such a universe? Why?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974412327\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974188449\">\n<p id=\"fs-id1163975451006\"><strong>17:<\/strong> Some theorists expected that observations would show that the density of matter in the universe is just equal to the critical density. Do the current observations support this hypothesis?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974340636\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975837957\">\n<p id=\"fs-id1163974343925\"><strong>18:<\/strong> There are a variety of ways of estimating the ages of various objects in the universe. Describe two of these ways, and indicate how well they agree with one another and with the age of the universe itself as estimated by its expansion.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974411668\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974258533\">\n<p id=\"fs-id1163974194108\"><strong>19:<\/strong> Since the time of <span class=\"no-emphasis\">Copernicus<\/span>, each revolution in astronomy has moved humans farther from the center of the universe. Now it appears that we may not even be made of the most common form of matter. Trace the changes in scientific thought about the central nature of Earth, the Sun, and our Galaxy on a cosmic scale. Explain how the notion that most of the universe is made of dark matter continues this \u201cCopernican tradition.\u201d<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974393618\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974550087\">\n<p id=\"fs-id1163972000574\"><strong>20:<\/strong> The anthropic principle suggests that in some sense we are observing a special kind of universe; if the universe were different, we could never have come to exist. Comment on how this fits with the Copernican tradition described in <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163974411668\" class=\"autogenerated-content\">Exercise<\/a>.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975840606\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974431259\">\n<p id=\"fs-id1163974176647\"><strong>21:<\/strong> Penzias and Wilson\u2019s discovery of the Cosmic Microwave Background (CMB) is a nice example of scientific <em>serendipity<\/em>\u2014something that is found by chance but turns out to have a positive outcome. What were they looking for and what did they discover?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974541815\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974184170\">\n<p id=\"fs-id1163975741498\"><strong>22:<\/strong> Construct a timeline for the universe and indicate when various significant events occurred, from the beginning of the expansion to the formation of the Sun to the appearance of humans on Earth.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<\/section>\n<section id=\"fs-id1163974220018\" class=\"figuring-for-yourself\">\n<h1>Figuring for Yourself<\/h1>\n<div class=\"exercise\" id=\"fs-id1163974343982\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975472994\">\n<p id=\"fs-id1163975638730\"><strong>23:<\/strong> Suppose the Hubble constant were not 22 but 33 km\/s per million light-years. Then what would the critical density be?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975581676\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975575041\">\n<p id=\"fs-id1163974264853\"><strong>24:<\/strong> Assume that the average galaxy contains 10<sup>11<\/sup> <em>M<\/em><sub>Sun<\/sub> and that the average distance between galaxies is 10 million light-years. Calculate the average density of matter (mass per unit volume) in galaxies. What fraction is this of the critical density we calculated in the chapter?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974406483\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974273046\">\n<p id=\"fs-id1163974172674\"><strong>25:<\/strong> The CMB contains roughly 400 million photons per m<sup>3<\/sup>. The energy of each photon depends on its wavelength. Calculate the typical wavelength of a CMB photon. Hint: The CMB is blackbody radiation at a temperature of 2.73 K. According to Wien\u2019s law, the peak wave length in nanometers is given by <span class=\"MathJax_Preview\"><\/span><span class=\"MathJax\" id=\"MathJax-Element-1-Frame\" role=\"presentation\" style=\"font-style: normal;font-weight: normal;line-height: normal;font-size: 14px;text-indent: 0px;text-align: left;letter-spacing: normal;float: none;direction: ltr;max-width: none;max-height: none;min-width: 0px;min-height: 0px;border: 0px;padding: 0px;margin: 0px\"><span class=\"math\" id=\"MathJax-Span-1\" role=\"math\"><span class=\"mrow\" id=\"MathJax-Span-2\"><span class=\"semantics\" id=\"MathJax-Span-3\"><span class=\"mrow\" id=\"MathJax-Span-4\"><span class=\"mrow\" id=\"MathJax-Span-5\"><span class=\"msub\" id=\"MathJax-Span-6\"><span class=\"mtext\" id=\"MathJax-Span-7\">\u03bb<\/span><span class=\"mrow\" id=\"MathJax-Span-8\"><span class=\"mtext\" id=\"MathJax-Span-9\">max<\/span><\/span><\/span><span class=\"mo\" id=\"MathJax-Span-10\">=<\/span><span class=\"mfrac\" id=\"MathJax-Span-11\"><span class=\"mrow\" id=\"MathJax-Span-12\"><span class=\"mn\" id=\"MathJax-Span-13\">3<\/span><span class=\"mspace\" id=\"MathJax-Span-14\"><\/span><span class=\"mo\" id=\"MathJax-Span-15\">\u00d7<\/span><span class=\"mspace\" id=\"MathJax-Span-16\"><\/span><span class=\"msup\" id=\"MathJax-Span-17\"><span class=\"mrow\" id=\"MathJax-Span-18\"><span class=\"mn\" id=\"MathJax-Span-19\">10<\/span><\/span><span class=\"mn\" id=\"MathJax-Span-20\">6<\/span><\/span><\/span><span class=\"mrow\" id=\"MathJax-Span-21\"><span class=\"mi\" id=\"MathJax-Span-22\">T<\/span><\/span><\/span><span class=\"mo\" id=\"MathJax-Span-23\">.<\/span><\/span><\/span><\/span><\/span><\/span><\/span><span class=\"MJX_Assistive_MathML\" role=\"presentation\">\u03bbmax=3\u00d7106T.<\/span> Calculate the wavelength at which the CMB is a maximum and, to make the units consistent, convert this wavelength from nanometers to meters.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975655088\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975433445\">\n<p id=\"fs-id1163975741435\"><strong>26:<\/strong> Following up on <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163974369405\" class=\"autogenerated-content\">Exercise<\/a> calculate the energy of a typical photon. Assume for this approximate calculation that each photon has the wavelength calculated in <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163974406483\" class=\"autogenerated-content\">Exercise<\/a>. The energy of a photon is given by <span class=\"MathJax_Preview\"><\/span><span class=\"MathJax\" id=\"MathJax-Element-2-Frame\" role=\"presentation\" style=\"font-style: normal;font-weight: normal;line-height: normal;font-size: 14px;text-indent: 0px;text-align: left;letter-spacing: normal;float: none;direction: ltr;max-width: none;max-height: none;min-width: 0px;min-height: 0px;border: 0px;padding: 0px;margin: 0px\"><span class=\"math\" id=\"MathJax-Span-24\" role=\"math\"><span class=\"mrow\" id=\"MathJax-Span-25\"><span class=\"semantics\" id=\"MathJax-Span-26\"><span class=\"mrow\" id=\"MathJax-Span-27\"><span class=\"mrow\" id=\"MathJax-Span-28\"><span class=\"mi\" id=\"MathJax-Span-29\">E<\/span><span class=\"mo\" id=\"MathJax-Span-30\">=<\/span><span class=\"mfrac\" id=\"MathJax-Span-31\"><span class=\"mrow\" id=\"MathJax-Span-32\"><span class=\"mi\" id=\"MathJax-Span-33\">h<\/span><span class=\"mi\" id=\"MathJax-Span-34\">c<\/span><\/span><span class=\"mtext\" id=\"MathJax-Span-35\">\u03bb<\/span><\/span><span class=\"mo\" id=\"MathJax-Span-36\">,<\/span><\/span><\/span><\/span><\/span><\/span><\/span><span class=\"MJX_Assistive_MathML\" role=\"presentation\">E=hc\u03bb,<\/span>where <em>h<\/em> is Planck\u2019s constant and is equal to 6.626 \u00d7 10<sup>\u201334<\/sup> J \u00d7 s, <em>c<\/em> is the speed of light in m\/s, and \u03bb is the wavelength in m.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974369405\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974220870\">\n<p id=\"fs-id1163975544550\"><strong>27:<\/strong> Continuing the thinking in <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163974369405\" class=\"autogenerated-content\">Exercise<\/a> and <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163975364885\" class=\"autogenerated-content\">Exercise<\/a>, calculate the energy in a cubic meter of space, multiply the energy per photon calculated in <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163975655088\" class=\"autogenerated-content\">Exercise<\/a> by the number of photons per cubic meter given above.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975364885\">\n<section>\n<div class=\"problem\" id=\"fs-id1163974361252\">\n<p id=\"fs-id1163975454003\"><strong>28:<\/strong> Continuing the thinking in the last three exercises, convert this energy to an equivalent in mass, use Einstein\u2019s equation <em>E<\/em> = <em>mc<\/em><sup>2<\/sup>. Hint: Divide the energy per m<sup>3<\/sup> calculated in <a href=\"https:\/\/cnx.org\/contents\/LnN76Opl@13.1:DLXReh3_@3\/The-Anthropic-Principle#fs-id1163974369405\" class=\"autogenerated-content\">Exercise<\/a> by the speed of light squared. Check your units; you should have an answer in kg\/m<sup>3<\/sup>. Now compare this answer with the critical density. Your answer should be several powers of 10 smaller than the critical density. In other words, you have found for yourself that the contribution of the CMB photons to the overall density of the universe is much, much smaller than the contribution made by stars and galaxies.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163975727734\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975361222\">\n<p id=\"fs-id1163974195725\"><strong>29:<\/strong> There is still some uncertainty in the Hubble constant. (a) Current estimates range from about 19.9 km\/s per million light-years to 23 km\/s per million light-years. Assume that the Hubble constant has been constant since the Big Bang. What is the possible range in the ages of the universe? Use the equation in the text, <span class=\"MathJax_Preview\"><\/span><span class=\"MathJax\" id=\"MathJax-Element-3-Frame\" role=\"presentation\" style=\"font-style: normal;font-weight: normal;line-height: normal;font-size: 14px;text-indent: 0px;text-align: left;letter-spacing: normal;float: none;direction: ltr;max-width: none;max-height: none;min-width: 0px;min-height: 0px;border: 0px;padding: 0px;margin: 0px\"><span class=\"math\" id=\"MathJax-Span-37\" role=\"math\"><span class=\"mrow\" id=\"MathJax-Span-38\"><span class=\"semantics\" id=\"MathJax-Span-39\"><span class=\"mrow\" id=\"MathJax-Span-40\"><span class=\"mrow\" id=\"MathJax-Span-41\"><span class=\"msub\" id=\"MathJax-Span-42\"><span class=\"mi\" id=\"MathJax-Span-43\">T<\/span><span class=\"mn\" id=\"MathJax-Span-44\">0<\/span><\/span><span class=\"mo\" id=\"MathJax-Span-45\">=<\/span><span class=\"mfrac\" id=\"MathJax-Span-46\"><span class=\"mn\" id=\"MathJax-Span-47\">1<\/span><span class=\"mi\" id=\"MathJax-Span-48\">H<\/span><\/span><span class=\"mo\" id=\"MathJax-Span-49\">,<\/span><\/span><\/span><\/span><\/span><\/span><\/span><span class=\"MJX_Assistive_MathML\" role=\"presentation\">T0=1H,<\/span> and make sure you use consistent units. (b) Twenty years ago, estimates for the Hubble constant ranged from 50 to 100 km\/s per Mps. What are the possible ages for the universe from those values? Can you rule out some of these possibilities on the basis of other evidence?<\/p>\n<\/div>\n<\/section>\n<\/div>\n<div class=\"exercise\" id=\"fs-id1163974171126\">\n<section>\n<div class=\"problem\" id=\"fs-id1163975658340\">\n<p id=\"fs-id1163975465099\"><strong>30:<\/strong> It is possible to derive the age of the universe given the value of the Hubble constant and the distance to a galaxy, again with the assumption that the value of the Hubble constant has not changed since the Big Bang. Consider a galaxy at a distance of 400 million light-years receding from us at a velocity, <em>v<\/em>. If the Hubble constant is 20 km\/s per million light-years, what is its velocity? How long ago was that galaxy right next door to our own Galaxy if it has always been receding at its present rate? Express your answer in years. Since the universe began when all galaxies were very close together, this number is a rough estimate for the age of the universe.<\/p>\n<\/div>\n<\/section>\n<\/div>\n<\/section>\n<div>\n<h2>Glossary<\/h2>\n<dl id=\"fs-id1163975635844\" class=\"definition\">\n<dt>anthropic principle<\/dt>\n<dd id=\"fs-id1163975577923\">idea that physical laws must be the way they are because otherwise we could not be here to measure them<\/dd>\n<\/dl>\n<dl id=\"fs-id1163975661940\" class=\"definition\">\n<dt>multiverse<\/dt>\n<dd id=\"fs-id1163974191028\">the speculative idea that our universe is just one of many universes, each with its own set of physical laws<\/dd>\n<\/dl>\n<\/div>\n","protected":false},"author":395,"menu_order":8,"template":"","meta":{"pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"class_list":["post-1084","chapter","type-chapter","status-publish","hentry"],"part":1049,"_links":{"self":[{"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/pressbooks\/v2\/chapters\/1084","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/wp\/v2\/users\/395"}],"version-history":[{"count":1,"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/pressbooks\/v2\/chapters\/1084\/revisions"}],"predecessor-version":[{"id":1164,"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/pressbooks\/v2\/chapters\/1084\/revisions\/1164"}],"part":[{"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/pressbooks\/v2\/parts\/1049"}],"metadata":[{"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/pressbooks\/v2\/chapters\/1084\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/wp\/v2\/media?parent=1084"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/pressbooks\/v2\/chapter-type?post=1084"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/wp\/v2\/contributor?post=1084"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/pressbooks.bccampus.ca\/astrojbrewer\/wp-json\/wp\/v2\/license?post=1084"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}