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The History of Astronomy

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Presentation on theme: "The History of Astronomy"— Presentation transcript:

1 The History of Astronomy

2 The Roots of Astronomy Already in the stone and bronze ages, human cultures realized the cyclic nature of motions in the sky. Monuments dating back to ~ 3000 B.C. show alignments with astronomical significance. Those monuments were probably used as calendars or even to predict eclipses.

3 Stonehenge

4 Stonehenge Constructed 3000 – 1800 B.C. in Great Britain
Constructed 3000 – 1800 B.C. in Great Britain Alignments with locations of sunset, sunrise, moonset and moonrise at summer and winter solstices Probably used as calendar.

5 Amazon Stonehenge Constructed around A.D. 100 in Brazil

6 Other Examples around the World
Caracol (Mexico); Maya culture, approx. A.D. 1000

7 Ancient Greek Astronomers
Models were based on unproven “first principles”, believed to be “obvious” and were not questioned: 1. Geocentric “Universe”: The Earth is at the Center of the “Universe”. 2. “Perfect Heavens”: The motions of all celestial bodies can be described by motions involving objects of “perfect” shape, i.e., spheres or circles.

8 Ptolemy: Geocentric model, including epicycles
Central guiding principles: 1. Imperfect, changeable Earth, 2. Perfect Heavens (described by spheres)

9 Introduced to explain retrograde (westward) motion of planets
Epicycles a small circle whose center moves around the circumference of a larger one. Introduced to explain retrograde (westward) motion of planets

10 The Copernican Revolution
Nicolaus Copernicus (1473 – 1543): Heliocentric Universe (Sun in the Center)

11 New (and correct) explanation for retrograde motion of the planets:
Retrograde (westward) motion of a planet occurs when the Earth passes the planet. This made Ptolemy’s epicycles unnecessary. Described in Copernicus’ famous book “De Revolutionibus Orbium Coelestium” (“About the revolutions of celestial objects”)

12 Found a consistent description by abandoning both
Johannes Kepler (1571 – 1630) Used the precise observational tables of Tycho Brahe (1546 – 1601) to study planetary motion mathematically. Found a consistent description by abandoning both Circular motion and Uniform motion. Planets move around the sun on elliptical paths, with non-uniform velocities.

13 Kepler’s Laws of Planetary Motion
The orbits of the planets are ellipses with the sun at one focus. c Eccentricity e = c/a

14 Eccentricities of Ellipses
1) 2) 3) e = 0.02 e = 0.1 e = 0.2 5) 4) e = 0.4 e = 0.6

15 Eccentricities of planetary orbits
Orbits of planets are virtually indistinguishable from circles: Most extreme example: Pluto: e = 0.248 Earth: e =

16 A line from a planet to the sun sweeps over equal areas in equal intervals of time. Fast Slow Animation

17 Autumnal Equinox (beg. of fall)
Summer solstice (beg. of summer) July Winter solstice (beg. of winter) Fall Summer Winter Spring January Vernal equinox (beg. of spring)

18 Astronomical Units (AU) 1AU = (about) 150 mil km

19 Kepler’s Third Law A planet’s orbital period (P) squared is proportional to its average distance from the sun (a) cubed: Py2 = aAU3 (Py = period in years; aAU = distance in AU) Orbital period P known → Calculate average distance to the sun, a: aAU = Py2/3 Average distance to the sun, a, known → Calculate orbital period P. Py = aAU3/2

20 It takes 29. 46 years for Saturn to orbit once around the sun
It takes years for Saturn to orbit once around the sun. What is its average distance from the sun? 9.54 AU 19.64 AU 29.46 AU 44.31 AU AU

21 Isaac Newton (1643 - 1727) Major achievements:
Adding physics interpretations to the mathematical descriptions of astronomy by Copernicus, Galileo and Kepler Major achievements: Invented Calculus as a necessary tool to solve mathematical problems related to motion Discovered the three laws of motion Discovered the universal law of mutual gravitation

22 Newton’s Laws of Motion (I)
Newton’s Laws of Motion (I) A body continues at rest or in uniform motion in a straight line unless acted upon by some net force. An astronaut floating in space will float forever in a straight line unless some external force is accelerating him/her.

23 Velocity and Acceleration
Acceleration (a) is the change of a body’s velocity (v) with time (t): a a = Dv/Dt Velocity and acceleration are directed quantities (vectors)! v

24 Newton’s Laws of Motion (II)
The acceleration a of a body is inversely proportional to its mass m, directly proportional to the net force F, and in the same direction as the net force. a = F/m  F = m a

25 Newton’s Laws of Motion (III)
Newton’s Laws of Motion (III) To every action, there is an equal and opposite reaction. The same force that is accelerating the boy forward, is accelerating the skateboard backward.

26 The Universal Law of Gravity
A particle attracts every other particle in the universe using a force that is directly proportional to the product of their masses and inversely proportional to the square of the distance between them. Mm F = - G r2 (G is the Universal constant of gravity.)


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