Answers to True/False and Multiple Choice Questions of the Final Exam

Answers to the True/False Questions

Answers to the Multiple Choice Questions

Some Miscellaneous Answers

  • Open Question 1: This is explained on pages 553-554 of the text, regarding how a red giant first forms.

  • Open Question 2: Answer is 23 degrees altitude with direction in the south (23oS).

  • Open Problem 4: Many students gave Hubble's law, i.e., the expansion of space, as an example supporting the Big Bang. This is not correct. The cosmic microwave radiation, He abundance, and deuterium abundance are all consequences of a hot dense beginning that later cooled off, but the expansion of space itself says nothing about the thermal or physical properties of the early universe. In fact, until the cosmic background radiation and He abundance were measured, there was competing theory called the "steady state universe" which postulated that the universe had always been expanding, with matter spontaneously appearing to keep the density constant. This theory was attractive because it got rid of the question of a beginning and end for the universe, there was no beginning.

  • Open Question 6: Part (a), many students realized they needed to divide a distance, 200 ly, by a speed, 0.8c, but took the long path of converting everything to meters or seconds. Here you can see the answer quickly with a little thinking. At the speed of light c, it would take 200 years to go 200 light-years by definition of a light year. So if you are traveling a bit slower at 0.8c, it would (1/.8) times longer, or 200/.8 = 250 years.

  • Open Question 7: Answer to one significant digit is 2,000 K. The new temperature is way above the temperature of boiling water (373 K) so is bad news since all the oceans will turn to steam and Earth will become like Venus.

    The subtle part of this problem was to deduce the distance d of Earth to the Sun after the Sun has swelled to about Mercury's orbit. Some students incorrectly chose d to be the distance of Earth to the edge of the swollen Sun. You needed to recall that at large distances between masses, a big mass like the Sun acts like a point mass at the center of the Sun. Thus whether the Sun swells to be a red giant or gets squished to a 3 km diameter black hole, Earth continues to remain 1 AU from the center of the Sun and this is the distance to use in this problem.

  • Open Question 8: Most students sadly missed the elegant insight here, there was evidently not enough practice during the course with the equivalence principle. The first step was to imagine an isolated rocket (no gravity present!) that is accelerating in space, say in the upwards direction of this page. Someone is holding two objects (say an apple and a steel ball) and these two objects are accelerating with the person and rocket because of the force exerted by the person's hands on the objects.

    Now the person lets go of the two objects at exactly the same time and at exactly the same height above the floor. As soon as the person let's go, the objects no longer have any force acting on them and they move upward with identical constant speeds. (This is Newton's first law, if there is no force, you move at constant speed in a constant direction.) But the rocket is accelerating which means that the floor of the rocket is rising faster and faster and will catch up and hit the two objects, and it will hit the objects at exactly the same time provided the objects were dropped from the same height at the same time. You can see that the fact that the floor catches up with the two objects has absolutely nothing to do with the shape or chemical properties or masses of the objects: you have two points at the same height above the floor moving upward with a constant speed, and the floor as a plane catches up and touches both objects at the same time.

    Finally, here is where you apply the equivalence principle. According to Einstein's insight, what happens in an accelerating rocket in the absence of gravity is physically undistinguishable from the same events happening in a stationary room in the presence of a vertical gravity field pointing downwards. Thus we must expect two objects to fall at the same rate and hit the ground at exactly the same time when dropped at the same time and height in a vertical gravitational field, and this fact can not depend on any physical properties such as mass or chemical composition because it is essentially a geometrical argument.

    I should point out that this problem has everything backwards historically. Einstein used the experimental fact that objects fall with the same acceleration independently of mass to guess the equivalence principle which he then applied to other problems such as the slowing down of clocks or the bending of light. But this is a nice problem because it shows that you can go backwards, starting from the equivalence principle and then deduce that objects falling under the influence of gravity do so with an acceleration that is independent of any property of the object.

  • Open Questions 9 and 10   Many students unfortunately confused special relativity with general relativity and answered these questions as if I had asked about special relativity. General relativity deals with gravity and distortions of space and time. Laboratory tests of general relativity include the bending of light by a star's mass (verified in 1919), the precession of Mercury's orbit by 43'' per century, and gravitational time dilation (clocks at tops of towers tick more rapidly than identical clocks at the base of towers, also the gravitational red shift). General relativity is essential for cosmology when trying to understand how space itself can expand or contract during the Big Bang (Hubble's data), also essential for understanding black holes that power quasars, radio sources like Sag A*, and some X-ray binaries (where does all the energy come from in such compact regions of space?).

    Examples like lack of simultaneity, length contraction, time dilation, increase of mass, E=mc2, and the modified addition rule for velocities all belong to special relativity. They are important in day-to-day thinking about astronomy, but are not as essential as general relativity for trying to understand the current astronomical mysteries such black holes, dark matter, beginning of the Big Bang, far future of the universe.

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