* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Outline of Lecture on Copernican Revolution: 1. Source of word
International Ultraviolet Explorer wikipedia , lookup
Aquarius (constellation) wikipedia , lookup
Lunar theory wikipedia , lookup
Planets beyond Neptune wikipedia , lookup
IAU definition of planet wikipedia , lookup
De revolutionibus orbium coelestium wikipedia , lookup
Tropical year wikipedia , lookup
History of Mars observation wikipedia , lookup
History of astronomy wikipedia , lookup
Definition of planet wikipedia , lookup
Celestial spheres wikipedia , lookup
Solar System wikipedia , lookup
Rare Earth hypothesis wikipedia , lookup
Extraterrestrial skies wikipedia , lookup
Astronomy on Mars wikipedia , lookup
Satellite system (astronomy) wikipedia , lookup
Astrobiology wikipedia , lookup
Formation and evolution of the Solar System wikipedia , lookup
Late Heavy Bombardment wikipedia , lookup
Planetary habitability wikipedia , lookup
History of Solar System formation and evolution hypotheses wikipedia , lookup
Astronomical unit wikipedia , lookup
Planets in astrology wikipedia , lookup
Extraterrestrial life wikipedia , lookup
Comparative planetary science wikipedia , lookup
Dialogue Concerning the Two Chief World Systems wikipedia , lookup
Copernican heliocentrism wikipedia , lookup
Timeline of astronomy wikipedia , lookup
Outline of Lecture on Copernican Revolution: 1. Source of word “revolution” with its present meaning. 2. Why did people care where the planets were? a. Agriculture. b. Auguries. g c. Cyclic behavior suggests some law, difficult to divine. 3. Why the sun, stars, and planets all should revolve around us. a. We are the center of everything, of course. b. Most observed motions immediately explained. c. Seasons caused byy inclination and speed p of sun’s motion. d. Moon’s phases come out fine. e. But there are small, nagging problems. 1 Outline of Lecture on Copernican Revolution: 4. Problems with the geocentric model: a. Retrograde motion of the planets. Particularly, Mars, Jupiter, and Saturn occasionally slow down relative to the stars and actually go backwards for a time. b. Phases of Venus (an objection more notable after the invention of the telescope). Full cycle of phases, correlated with Venus’ apparent size. 5. Retrograde motion “explained.” a Explained by epicyclic motion. a. motion b. Imperfect, but still circles, just more of them. c. This idea came from the Greek, Hipparchus, and was elaborated by Ptolemy, who lived in Alexandria in the second century AD. The problem with the retrograde motion was: • Hard to see why a god would have established so complex a motion. • This going forward and then occasionally backward, and then forward again would seem to demand constant attention from a god, who should more properly have better things to be attending to. Ptolemy’s epicycles derived the back and forth motion of the planets from circles turning on circles. • This motion might seem possible for a god to set going and then have it run on forever, since uniform circular motion seemed like something that could go on forever without attention. People had been able to build devices (wheels) that acted this way, although our human imperfection resulted in the wheels eventually slowing down and coming to rest. However divine wheels would be perfect and keep on turning. 2 But Ptolemy’s epicyclic motions were actually not built out of uniform circular motions. • The motion of the planet around the epicycle was uniform. • But the motion of the guiding center of the epicycle about its orbit circle was non-uniform. • But it was only slightly non-uniform. • This imperfection of Ptolemy’s model no doubt bothered the experts who thought about it, but then there weren’t very many experts around. There was another problem with Ptolemy’s epicycles, they were uncomfortably large. large • This made the motions of the planets quite bizarre. • Ptolemy’s model might never have caught on had he used the epicycles for the outer planets that describe their actual motion about the sun. More on this in a moment. The epicycles in this diagram from your textbook are not drawn correctly. In Ptolemy’s model, for most of these planets the epicycles are much larger than these in relation to the radii of the planets’ orbits about the earth. For the curious: In fact, to get the motion of a planet correct, the ratio of the radius of its i l to epicycle that of its orbit must equal the ratio of the radius of its orbit about the sun to that of the earth, or the inverse of that ratio, whichever is smaller. 3 Through a telescope, Mars actually appears larger during its retrograde motion, because it is closer to the earth at that time. The line of dots in the b k background d are the distant planet Uranus. 4 With a telescope, we can measure the variation in size of the visible disk of Mars, and hence deduce the ratio of its orbital radius to that of the earth. The distance of Mars from the earth was arbitrary in Ptolemy’s model. Its value could not be determined by observation with the technology of Ptolemy’s time. It was not until the invention of the telescope and Galileo’s training of that new instrument upon the sun, moon, and planets that it became clear that Venus exhibits a complete cycle of phases, like the Moon. The pphases of the pplanet Venus. Note that the disk of Venus becomes smaller as it nears its “full” phase. Without a telescope, one could see that Venus must be closer to the earth than the sun is, at least some of the time, because it has a “new” phase when it is clearly between us and the sun. A “full” Venus is only geometrically possible if Venus is further away from us than the sun. 5 Outline of Lecture on Copernican Revolution: 6. Phases of Venus. a. Hard to see phases of Venus without a telescope. b. But variations in brightness large and obvious. c Phases possible if Venus orbits Earth closer than the sun, c. sun at a very different speed. d. But Venus is never very far from the sun, so: 1) it must orbit earth at same average speed as the sun 2) epicycle must make it go back and forth from one side to the other of the sun in the sky. e. In this case, Venus can never be “full.” Its disk can at most be only half illuminated (and actually less than this). The epicycles in this diagram from your textbook are not drawn correctly. If we take the orbit × of the guiding center of the epicycle off Venus V as shown, then this epicycle must have its center precisely on the line joining the earth and the sun, and its radius should be about as indicated. The correct ratio of the radius of a planet’s epicycle to that of its guiding center’s orbit is the ratio of the radius of the planet’s actual orbit about the sun to that of the earth’ss actual earth orbit. For an outer planet like Mars, it is the inverse of this ratio. 6 The size of Venus’ epicycle on this diagram is fixed by the requirement that the greatest × observed angle on the sky between V Venus and d th the sun come out correctly. Thus if we make Venus’ orbit twice as far from the earth, we must double the radius of its epicycle. With the correct size of Venus’ epicycle, we would be advised to make the radius of the sun’s orbit on this diagram a bit bigger, so th t no one that might conclude that Venus was orbiting the sun and not orbiting us. × The guiding center for the epicycle of Venus must lie precisely on the line joining the earth and the sun. sun This was known to be true, because over thousands of years, Venus had never been seen more than about 40° away from the sun. The epicycles for Jupiter and Saturn, when correctly drawn, are indeed quite small on this diagram but diagram, the epicycle for Mars must be 66% × of the radius of the orbit of its guiding center as shown. To get Mars out of the way of Venus, we can move it outward. 7 In the Ptolemaic system, Venus orbits the earth on a circle at a rate that keeps it close to the sun in the sky. The phases of Venus therefore must be restricted. In particular, Venus can never be “full.” At the very most, only half the disc of Venus could appear illuminated by the sun. In the Copernican system, where both the earth and Venus orbit the sun, a full range of phases of Venus should be visible from the earth if the radius of Venus’ orbit is smaller than that of the earth (i.e. the orbit of Venus is inside that of the earth). Galileo observed a full set of phases for Venus. 8 Role of Ptolemy: 7. Ptolemy built a geocentric model that: a) used centuries of observations in library at Alexandria, b) used circular orbits and epicycles, with non-uniform motion of the centers of the epicycles along their circular orbits (known as the “deferent circles”), c) was set out in 13-volume Almagest, d) fit all observations for hundreds of years. 8. If it works, why change it? 99. By the fifteenth century, century clear that was something wrong wrong. 10. Aristarchus, an ancient Greek astronomer, had suggested that if the earth orbited the sun with the other planets, retrograde motion of the other planets was a natural consequence. 9 Illustration of how parallax can result in apparent retrograde motion of an outer planet. Modern Explanation of Retrograde Motion: 11. The apparent retrograde motion of the planets is an especially obvious example of parallax. a. Parallax causes a nearby object to appear to move relative to distant objects when an observer moves. b You b. Yo see this effect eevery er da day. JJust st look ooutt the window indo of a moving car. c. Your brain uses parallax to construct a stereo view of the world. d. If planets appear to move “backwards” because of parallax, then stars should exhibit this same effect. e. Ancient A i t people l were able bl to t supportt their th i view i off the th earth th at the center of the universe by pointing out that stars showed no parallax. f. Of course, stars do show parallax, but stars are so distant that this effect was unmeasurable before the invention of the telescope (the nearest star is only about 1 parsec away). 10 This change g in the apparent position of the star relative to more distant stars is too small to see without a telescope. The largest such motion is by an amount equal to about 1/1800 of the angular diameter of the observed disk of the Moon. As educated, modern people, we know that in fact both the earth and Mars orbit the sun. Because we are stuck on the earth, it is useful to define a coordinate system with the earth fixed and at the center. These coordinates must describe our perception of reality. They may not, however, provide the most useful description of reality, since fate may not have placed us at a particularly good spot from which to observe reality. In the coordinates in which we stay in one central location and everything else may move, it is clear that the sun will appear to orbit us in a circle. Because Mars is in turn orbiting the sun in something pretty close to a circle, the orbit of Mars about us must therefore appear to be a circle riding on a circle – an epicyclic orbit, just as Ptolemy said it was in his model of the solar system. But just a minute, the radius of the epicycle for Mars is larger than the radius of the guiding center of the epicycle (the radius of the orbit of the sun). 11 Our modern knowledge of the motions of the planets therefore tells us that the “actual” epicyclic orbit that Mars appears to follow about us is quite weird. It is a big cicle riding along a little circle, which would have seemed very strange to a classically trained guy like Ptolemy. The idea of epicyclic motion is fine, but the idea of a big epicycle riding on a little guiding center circle is not fine at all. It is simply implausible. Who would build a solar system in such a bizarre fashion? The model is saved, however, by a trick of geometry. It is a fact, and those who do not believe it can come talk with me in my office hours, that precisely the same apparent motion for Mars is generated if we switch the guiding center circle radius and the epicycle radius. Now everything is just fine, and the epicycle looks more like a detail, although a big detail. Here I have fit two circles over the orbits in the diagram from your textbook, and I have put red and blue dots over the positions of the two planets marked in the diagram. 12 We obtain the same apparent motion by letting the small circle move along the large one as we do by letting the large circle move along the small one. Here the motion along each circle is by the same amount from dot to dot as in the original diagram from your textbook. In both cases, we move half way around the small circle in 6 equal steps, and about a quarter of the way around the large circle in 6 equal steps. The radius of the small circle is the radius of the orbit of the earth about the sun. The radius of the large circle is that of the orbit of Mars about the sun. In both diagrams, the epicycle moves counterclockwise along the deferent circle, and the planet moves counterclockwise around the epicycle. 13 We get precisely the same motion, because it does not matter whether, as on the left, we go first along the vector with length equal to the radius of Mars’ orbit and then along the one with length equal to the radius of Earth’s orbit, or if, as on the right, we travel along these vectors in the opposite order. For the case of perfectly circular orbits and perfectly uniform motion along the circles, the paths traced out by the planet’s motion relative to us are identical. The two constructions are different, but the resulting paths of the planet are the same. Kepler discovered that the orbits of the planets are actually ellipses, and this modification of the planetary motion was approximated in Ptolemy’s model by a nonuniform motion of the epicycle around the deferent circle. Copernicus made an identical correction in his model by using a very small epicycle, which was truly a detail. Here we see the same point once again, perhaps more clearly. 14 15 Here we see how the two different constructions do indeed produce the identical result. In Ptolemy’s model, on the left, the guiding center of Mars’ epicycle orbits the earth on the “deferent” circle. We need to specify the radii of the deferent and of the epicycle, which must have a special ratio but which can both be scaled together arbitrarily. arbitrarily We must also specify the orbital periods for both the deferent and the epicycle. In the Copernican model, we must specify only the ratio of the orbital radii of Mars and the earth as well as the ratio of their orbital periods. Two arbitrary constants are eliminated from Ptolemy’s model, the radius of the deferent for Mars and one period (which is replaced with the period of the earth’s orbit). An epicycle disappears in the process as well. 16 In Ptolemy’s model, on the left, the guiding center of Mars’ epicycle orbits the earth on the “deferent” circle precisely once every year. Surely experts noted this. It is very hard to believe that this fact is an accident. It results naturally if the earth in fact orbits the sun, but in Ptolemy’s model it emerges as a completely unmotivated result. In fact, in Ptolemy’s model the periods in which also Jupiter and Saturn go around their individual epicycles are also, astonishingly, precisely one year. One would imagine that this accidental result would have caught someone’s attention. Ptolemy offers absolutely no reason why this is so. We can use this same diagram to understand the motion of an inner planet like Venus as it appears from the point of view of the earth. If we now ride on Mars and observe the apparent motion of Earth, we see that the sun will orbit us (Mars), and the Earth will travel on this deferent circle executing an epicyclic motion with an epicycle radius equal to that of the Earth’s orbit about the sun. It will exhibit a brief retrograde motion between points 3 and 5 on its orbit. 17 These are the actual “orbits” of Venus and Mercury as observed regarding the Earth as fixed. Hopefully, you can see from these last few slides why the idea of epicyclic motion was quite fitting as a description of the observed motions of the planets. At the left is Kepler’s p rendering g of the orbit of Mars as seen from an imagined g point above the earth. At the right is a modern rendering. As Mars appears to come close to the earth, the loops caused by its apparent epicyclic motion are not all the same. This is caused by the nonuniform motion of the guiding center along the deferent circle in Ptolemy’s model. In Kepler’s model, this feature results because the orbit of Mars is an ellipse and not a circle. The apparent motion of Mercury on the previous slide shows a similar nonuniform character, but to a lesser degree. 18 Both Ptolemy and Copernicus had to explain the nonuniform motion of the planets in their orbits. Planets move faster when they are closer to the sun. Ptolemy “explained” this by a nonuniform motion of the guiding center of the epicycle about the guiding center circle. Copernicus, perhaps rediscovering something that muslim mathematicians had realized two centuries before him, used a small epicycle that executes precisely 2 revolutions for every single revolution of its guiding center. The two constructions yield exactly the same result. Hence Copernicus built a theory that produced precisely the same motions as that of Ptolemy. Its results were not better, but its construction was far less arbitrary, and it proved far more conducive to productive thought. This is one sign in science of being on the right track. The angular motion of the epicycle about the deferent circle is uniform only when viewed from the equant point in Ptolemy’s model. This makes the epicycle move faster when it is closer to the earth. This is turn gives rise to the narrower and broader loops in the apparent motion of Mars shown on the previous slide. 19 A series of 13th and 14th century Muslim astronomers in Persia and in Damascus had discovered that Ptolemy’s device of the equant could be replaced by either a circle with two small epicycles or a circle with a single eccentric (i.e. off-center) epicycle. Copernicus may have rediscovered this fact independently, or he may have heard about it somehow (no one knows how). This device has the advantage, for an Aristotelian, of replacing a non-uniform motion about a circle with uniform motion about multiple circles. Copernicus used two epicycles at first, and in his final model, laid out in his landmark book, he switched to the single, off-center epicycle. Copernicus’ model therefore exactly reproduces Ptolemy’s model, and therefore it was no more accurate. Nevertheless, Copernicus was able to eliminate the large (single) epicycles in Ptolemy’s model (although replacing them with much smaller ones) by using instead a single orbit for the earth about the sun to explain all of these in one fell swoop. Copernicus thus showed that the epicycles in Ptolemy’s model were not in fact arbitrary or the result of accidents, but were in fact related to one another by the single orbit of the earth. For one thing, g, this explained p whyy the epicycles p y for the inner planets moved along their guiding (or “deferent”) circles at precisely the same speed as the sun moved around the earth. These planets were known to be closer than the sun, because they were sometimes observed in the “new” (dark) phase. 20 Ignore Ptolemy’s “equant” on the left. It is too complicated and will not be on the test. This diagram, however, serves to show that the epicycles in Copernicus’ model really are very small and really make very little impact on the apparent motion of the planets. They simply serve to generate a faster motion when the planets are closer to the sun. Today we understand that this is necessary because the force of the sun’s gravity is more strongly felt along this portion of the orbit. But it is a small effect. We can be sure that Copernicus used only very small epicycles compared with the ones used by Ptolemy, because otherwise Copernicus would have created orbits that did not simply slow down a little when the planet was farthest from the sun but would have actually produced real, not just apparent, retrograde motion. To see this, we build orbits using Copernicus’ construction with different sizes for the epicycles. We MUST have the period of the epicyclic motion precisely half the period of the orbit of the guiding center. For too large an epicycle radius, radius we get real retrograde motion (shown on the next slide). For a smaller epicycle, the effect distorts the orbits shape considerably (second following slide). A still smaller orbit looks just right. 21 22 This is the kind of orbit we are after. The planet will orbit faster at the right i ht andd slower l att the th left, while the orbit remains roughly circular. To get the right motion, we need to place the sun nearer to the right than to the left portions of the orbit. 23 5a: So, what was wrong with Ptolemy’s model to a contemporary mind? First, everything was an accident. That is to say that each planet had its own special “deferent” circle (i.e. guiding center circle) and its own special epicycle radius and period. For each planet, you needed to come up with the following completely unrelated and arbitrary parameters: 1. The radius of its deferent circle, that is, of the orbit of its guiding center about the earth. 2. The displacement of the center of the deferent circle from the earth. 3. The period of its orbit about the deferent circle. 4. The radius of its epicycle. 5. The period of its orbit about the epicycle. Th was no way tto establish, There t bli h within ithi the th model, d l a necessary ordering d i off the sun, moon, and planets in terms of their distances from the earth. The same observed positions on the sky could be explained by multiplying both the radius of the deferent and the radius of the epicycle by a common factor. The distances from the earth cannot therefore be determined in this model and are hence arbitrary. The work of an arbitrary-minded god? 5b: So, what was wrong with Ptolemy’s model to a contemporary mind? One also had to explain the following amazing coincidences: 1. The guiding centers of the epicycles for both Mercury and Venus revolve about the earth at precisely the speed of the sun’s orbit. 2. These guiding centers are both always located on the line joining the earth and the sun. 3. The periods of the motions about the earth of ALL the guiding centers of the planets are identical to the period of the motion of the sun about the earth if we choose for the outer planets to generate their motion using big epicycles traveling on small deferent circles rather than the other way around. (That is, we must explain why it is possible to build a model like Tycho Brahe built, that produces the same motions but in which all the epicyclic guiding center periods are identical.) 4 If we generate 4. t motions ti ffor th the outer t planets l t using i small ll epicycles, i l as Ptolemy did, we need to explain why all the periods of the motions of the outer planets about their epicycles are identical and equal to the period of the sun’s motion about the earth. (That is, we need to explain why the sun’s period should be involved at all here, since the motions of the planets around the earth have nothing to do with the sun in Ptolemy’s model.) 24 Outline of Lecture on Copernican Revolution: 5b: So, what was wrong with Ptolemy’s model to a contemporary mind? In short, Ptolemy had an awful lot of explaining to do. Usually, when a scientist is looking for a mechanism that can explain a collection of observations, coming upon such an apparently accidental equality of seemingly unrelated numbers is an important clue to the solution to the problem. It is often a sign that these numbers come out to be the same for a reason that is fundamental to the mechanism that creates the observed phenomena. Modern scientists are now familiar with this, but in Ptolemy’s time the clue might have been more easily missed. But the fact that the Greek’s were aware that a heliocentric model could naturally produce the observations suggests that the coincidences had indeed caused people to question and to think. In Ptolemy’s model, on the left, the guiding center of Mars’ epicycle orbits the earth on the “deferent” circle. We need to specify the radii of the deferent and of the epicycle, which must have a special ratio but which can both be scaled together arbitrarily. arbitrarily We must also specify the orbital periods for both the deferent and the epicycle. In the Copernican model, we must specify only the ratio of the orbital radii of Mars and the earth as well as the ratio of their orbital periods. Two arbitrary constants are eliminated from Ptolemy’s model, the radius of the deferent for Mars and one period (which is replaced with the period of the earth’s orbit). An epicycle disappears in the process as well. 25 If we consider the motion of only a single planet, like Mars, which is shown here, Ptolemy’s model does not seem much more complicated than Copernicus’. However, when we take the motions of all the 5 other known pplanets at the time,, Copernicus p had a veryy much simpler p construction. He eliminated all of Ptolemy’s large epicycles and explained the equality of all their periods, for the outer planets, and the periods of their guiding centers, for the inner planets. Details remained in both models. These result because the actual planetary orbits are elliptical and not circular. Ptolemy dealt with this using uniform motion about the equant point for an eccentric (displaced) deferent circle, and Copernicus dealt with it by introducing a small epicycle for each planet. As a result result, the 2 models were equally inaccurate (since both were wrong), wrong) but Copernicus’ model was much more appealing. This appeal was not purely aesthetic; its improved construction led the way to revisions that later produced a correct model and suggested the mechanism of gravity. Thus Ptolemy’s model, in which so many things appeared arbitrary or accidental, led nowhere and proved a scientific dead end. But Copernicus’ model produced a framework for thought in which it was soon possible to correct the inaccuracies through a slight modification (circles became ellipses). The model also exposed tantalizing trends in the radii and periods of planetary orbits, and these helped to lead later scientists to uncover the underlying mechanism driving the motions, the force of gravity. Thus Copernicus started out along an extremely fertile path of discovery. 26