Lecture 7: Copernicus I (Copernican v. Ptolemaic Systems) © Darrin Durant 2004 Copernicus v. Ptolemy The Ptolemaic System (Claudius Ptolemy, 100-170) The Eccentric Model: The earth is displaced from the centre of the geometrical construction. One could also put C in motion, either around the earth or around another point, but in each case the deferent would have as its centre either a fixed or a movable central-point. E.g.: if the distance between C – E = 0.03 the radius of the eccentric, the displaced circle will account for the 6 extra days the sun spends between the vernal and the autumnal equinoxes. Fig. 1: eccentric model The Epicycle-Deferent Model: Accounts for the periodic appearance of retrograde motion as seen from the earth. In Fig. 2, the planet P is moving eastward with the deferent and is at its maximum speed. If P were on the inside of D (between D and E), then P would be moving westward, against its deferent, and would be at its slowest speed (and appearing to retrogress). Planetary motions accounted for by varying the speed and direction of the epicycle and the deferent. Fig. 2: epicycle-deferent model Fig. 3: equant model Fig. 4: equant & epicycle The Equant Model: The rate of rotation of a deferent (and so on) is required to be uniform, not with respect to its own geometric centre, but with respect to an equant point displaced from that centre. E.g.: in Fig. 3, P sweeps out equal angles in equal times as measured at Q. Uniformity of angular motion (though not about the centre) retained, but uniformity of linear motion about the circumference is given up. 1 Lecture 7: Copernicus I (Copernican v. Ptolemaic Systems) © Darrin Durant 2004 The geometrical equivalence of the Copernican and Ptolemaic systems Fig. 5: Explanations of the motion of the sun and the seasons Earth Geocentric System S3 S1 S2 Section of the Starry Vault * * 3 * * * * * 2 * * * * * 11 Sun Heliocentric System E1 E3 E2 Fig. 6: Explanations of the retrograde motion of the planets Earth Geocentric System P3 P2 P P4 P P5 * Starry Vault * * 5 * 2 3 4 * 1 * P5 Heliocentric System P1 * * P4 P3 P2 P3 P1 E3 E4 E5 E2 E E1 2 * * * * * 1 Lecture 7: Copernicus I (Copernican v. Ptolemaic Systems) © Darrin Durant 2004 How the sun ‘governs’ the planets in the Ptolemaic system Fig. 7: 1. The centre of the epicycles of Mercury and Venus are tied to the earth-sun vector, keeping them roughly aligned with the sun. 2. The lines joining the epicycles of Mars, Jupiter and Saturn are required to remain parallel to the earth-sun radius vector. This means whenever a superior planet is at its point of maximum retrograde motion, the sun will be opposite it in the heavens. Why the ordering? Ptolemy admits he cannot measure distances Mars, Jupiter, Saturn Sun (Earth), Moon, Mercury, Venus 3 Lecture 7: Copernicus I (Copernican v. Ptolemaic Systems) © Darrin Durant 2004 The Copernican System (1473-1543) Fig. 8: Copernicus’ Heliocentric System: is Fig. 8 accurate? ‘Mean Sun’ Epicycles Dimensions? The nature of the orbs? Fig. 9: The Copernican explanation of stellar parallax: The line between a terrestrial observer and a fixed star does not stay parallel to itself as the earth moves in its orbit. Thus, the star’s apparent position on the stellar sphere should shift by a given angle (that between the two lines, close to the intermediate star) during an interval of six months. Fig. 10: Copernicus’ explanation of the difficulty of detecting stellar parallax: note that the further away the sphere of the fixed stars, the smaller the angle of parallax. An object within the earth’s atmosphere would have a large parallax, such as that of a comet. If comets are objects out in the celestial realm, then they would have a smaller parallax. 4 Lecture 7: Copernicus I (Copernican v. Ptolemaic Systems) © Darrin Durant 2004 Copernicus and Planetary Distances Fig. 11: Fig. 12: SE2 P2=90 E2 Venus P2 SE=10 SVE = 90 Earth Sun Sun P1 E1 VES = 46 Fig.11: VS/SE = VS/10 = sin 46, but sin 46 = .72 Fig.12: obtain a right angle triangle by letting a planet move from opposition to 90 point. Using orbital times and times of motion (R), we get: cosE2SP2 = SE/SP = 10/R or R = 10/cosE2SP2 Copernicus and Ptolemy on ‘Bounded Elongation’ Fig. 13: Ptolemy the angle between S and P must be restricted (keep centre of epicycle on ES vector) Earth Sun Planet Fig. 14: Copernicus 28 Orbit of earth Orbit of Venus Earth Orbit of Mercury The earth’s orbit contains the orbits of the inferior planets 46 5 Lecture 7: Copernicus I (Copernican v. Ptolemaic Systems) © Darrin Durant 2004 Summary of the Copernican system 3 motions: 1. Diurnal axial rotation (west to east) 2. Annual motion around sun 3. Conical motion of earth’s axis Problems: Why don’t we all fly off the earth? Why doesn’t the earth disintegrate? If everything is going in a circle, why do bodies fall to earth? Why can’t we detect stellar parallax? Why does the moon orbit the earth? Shouldn’t we see Phases of Venus? If Copernicus and Ptolemy both use epicycles, then how do we choose between them? 8. Scripture declares the universe to be geocentric 1. 2. 3. 4. 5. 6. 7. Issues: 1. Are the Copernican orbs ‘real’ (solid, material) 2. Is the system ‘heliocentric’ if there is a ‘mean sun’ centre? 3. Is the Copernican system is ‘simpler’ or ‘more harmonious”? 4. Which system was more ‘accurate’? Accurate according to what criteria? “Whether these eccentrics really exist in the spheres of the planets no mortal knows, unless we are to declare them, and likewise epicycles, to have been disclosed by some revelation of spirits (as some claim).” Albertus de Brudzewo, 1495 “God the creator placed these bodies so far away from our senses that that we are unable to produce principles of demonstration for them (as we can in the [study] of other things) or to discover what is natural and familiar, by means of which we may afterwards set out the causes of particular appearances.” Nicodemus Frischlin, De astronomicae artis… (1586)1 See Nicholas Jardine, “Epistemology of the Sciences”, in Schmitt et al, The Cambridge History of Renaissance Philosophy (1988), 685-711. Albertus de Brudzewo taught mathematics at the University of Cracow when Copernicus studied there. 1 6