Chapter 29 The Big Bang
29.10 Questions and Exercises
1: What are the basic observations about the universe that any theory of cosmology must explain?
2: 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?
3: What does the term Hubble time mean in cosmology, and what is the current best calculation for the Hubble time?
4: Which formed first: hydrogen nuclei or hydrogen atoms? Explain the sequence of events that led to each.
5: Describe at least two characteristics of the universe that are explained by the standard Big Bang model.
6: 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?
7: Why do astronomers believe there must be dark matter that is not in the form of atoms with protons and neutrons?
8: What is dark energy and what evidence do astronomers have that it is an important component of the universe?
9: Thinking about the ideas of space and time in Einstein’s general theory of relativity, how do we explain the fact that all galaxies outside our Local Group show a redshift?
10: 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?
11: Describe the anthropic principle. What are some properties of the universe that make it “ready” to have life forms like you in it?
12: Describe the evidence that the expansion of the universe is accelerating.
13: 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?
14: What are the advantages and disadvantages of using quasars to probe the early history of the universe?
15: Would acceleration of the universe occur if it were composed entirely of matter (that is, if there were no dark energy)?
16: 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?
17: 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?
18: 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.
19: Since the time of Copernicus, 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 “Copernican tradition.”
20: 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 the previous exercise.
21: Penzias and Wilson’s discovery of the Cosmic Microwave Background (CMB) is a nice example of scientific serendipity—something that is found by chance but turns out to have a positive outcome. What were they looking for and what did they discover?
22: 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.
Figuring for Yourself
23: Suppose the Hubble constant were not 22 but 33 km/s per million light-years. Then what would the critical density be?
24: Assume that the average galaxy contains 1011 MSun 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?
25: The CMB contains roughly 400 million photons per m3. 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’s law, the peak wave length in nanometers is given by λmax=3×106 T. Calculate the wavelength at which the CMB is a maximum and, to make the units consistent, convert this wavelength from nanometers to meters.
26: Following up on the previous exercise, calculate the energy of a typical photon. Assume for this approximate calculation that each photon has the wavelength calculated in the previous exercise where the temperature is 2.73 K . The energy of a photon is given by E=hcλ where h is Planck’s constant and is equal to 6.626 × 10–34 J × s, c is the speed of light is 3.00 x 108 m/s, and λ is the wavelength in m.
27: Continuing the thinking from the two previous exercises, calculate the energy in a cubic meter of space, multiply the energy per photon calculated in Exercise 26 by the number of photons per cubic meter given above.
28: Continuing the thinking in the last three exercises, convert this energy to an equivalent in mass, use Einstein’s equation E = mc2. Hint: Divide the energy per m3 calculated in Exercise 27 by the speed of light squared. Check your units; you should have an answer in kg/m3. 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.
29: There is still some uncertainty in the Hubble constant. (a) Current estimates for H range from about 68 km/s per megaparsecs to 74 km/s per megaparsecs. 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, T0=1 / H, and make sure you use consistent units. (b) Twenty years ago, estimates for the Hubble constant ranged from 50 to 100 km/s per megaparsecs. 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?
30: 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, v. 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.