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© 2005 Pearson Education Inc., publishing as Addison-Wesley Correction in Exam 1 Date: Thursday Feb. 10 Updated Syllabus in website has the corrected date.

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Presentation on theme: "© 2005 Pearson Education Inc., publishing as Addison-Wesley Correction in Exam 1 Date: Thursday Feb. 10 Updated Syllabus in website has the corrected date."— Presentation transcript:

1 © 2005 Pearson Education Inc., publishing as Addison-Wesley Correction in Exam 1 Date: Thursday Feb. 10 Updated Syllabus in website has the corrected date Please tell your classmates who are not here

2 © 2005 Pearson Education Inc., publishing as Addison-Wesley 4.1 and 4.2 Describing Motion, Newton and Galileo Speed, velocity and acceleration (skip momentum) Galileo’s experiments with falling objects: g = 9.8 m/sec 2 Objects fall together Inertia (motion in absence of force) Newton’s Laws: 1.3 laws of motion: a. Inertia b. F=ma c. Action = Reaction 2.Gravitation: F= GM 1 M 2 /d 2 (Inverse-square law) 4.3 (Thermal Energy only) 4.4 The force of Gravity The Strength of Gravity ■ Newton and Kepler Orbits: 1. Closed: circles (circular velocity) & ellipses (v > v c ) 2. Open: parabolas and hyperbolas (escape velocity, v > v e ) Tides: Lunar and Solar Outline of Ch 4 Motion and Gravity (soap opera’s final episode)

3 © 2005 Pearson Education Inc., publishing as Addison-Wesley 4.2 Newton’s Laws of Motion Our goals for learning: How did Newton change our view of the universe? What are Newton’s three laws of motion? What is Newton’s laws of gravitation?

4 © 2005 Pearson Education Inc., publishing as Addison-Wesley Realized the same physical laws that operate on Earth also operate in the heavens  one universe Discovered 3 laws of motion and law of gravitation Much more: experiments with light; first reflecting telescope, calculus… How did Newton change our view of the Universe? Sir Isaac Newton (1642-1727)

5 © 2005 Pearson Education Inc., publishing as Addison-Wesley What are Newton’s three laws of motion? Newton’s first law of motion (law of inertia): An object moves at constant velocity unless a net force acts to change its speed or direction (this he adopted from Galileo).

6 © 2005 Pearson Education Inc., publishing as Addison-Wesley Newton’s second law of motion: Force = mass  acceleration (F= ma)

7 © 2005 Pearson Education Inc., publishing as Addison-Wesley Newton’s third law of motion: For every force, there is always an equal and opposite reaction force (action = reaction).

8 © 2005 Pearson Education Inc., publishing as Addison-Wesley The Universal Law of Gravitation 1.Every mass attracts every other mass. 2.Attraction is directly proportional to the product of their masses. 3.Attraction is inversely proportional to the square of the distance between their centers..

9 © 2005 Pearson Education Inc., publishing as Addison-Wesley Question: Is the force the Earth exerts on you larger, smaller, or the same as the force you exert on it? A.Earth exerts a larger force on you. B.I exert a larger force on Earth. C.Earth and I exert equal and opposite forces on each other. D.There is no force between Earth and any object

10 © 2005 Pearson Education Inc., publishing as Addison-Wesley Question: A compact car and a Mack truck have a head-on collision. Are the following true or false? 1.The force of the car on the truck is equal and opposite to the force of the truck on the car. 2.The change of velocity (acceleration) of the car is the same as the change of velocity of the truck.

11 © 2005 Pearson Education Inc., publishing as Addison-Wesley Question: A compact car and a Mack truck have a head-on collision. Are the following true or false? 1.The force of the car on the truck is equal and opposite to the force of the truck on the car. 2.The change of velocity of the car is the same as the change of velocity of the truck. (remember F = ma, if “F” is the same and the masses are very different then “a”, which is the change in velocity must also be very different)

12 © 2005 Pearson Education Inc., publishing as Addison-Wesley What have we learned? How did Newton change our view of the universe? He discovered laws of motion & gravitation. He realized these same laws of physics were identical in the universe and on Earth. What are Newton’s Three Laws of Motion? 1)Object moves at constant velocity if no net force is acting. 2)Force = mass  acceleration 3)For every force there is an equal and opposite reaction force.

13 © 2005 Pearson Education Inc., publishing as Addison-Wesley 4.3 Ignore all except Thermal Energy Relation temperature  motion of atoms : The higher the temperature the faster the atoms in a substance will be moving As atoms collide the electrons collide and their motion is disturbed When the motion of electrons gets disturbed they produce photons The higher the temperature, the more collisions, the more photons (more about this in Ch. 5)

14 © 2005 Pearson Education Inc., publishing as Addison-Wesley Temperature Scales

15 © 2005 Pearson Education Inc., publishing as Addison-Wesley 4.1 and 4.2 Describing Motion, Newton and Galileo Speed, velocity and acceleration (skip momentum) Galileo’s experiments with falling objects: g = 9.8 m/sec 2 Objects fall together Inertia (motion in absence of force) Newton’s Laws: 1.3 laws of motion: a. Inertia b. F=ma c. Action = Reaction 2.Gravitation: F= GM 1 M 2 /d 2 (Inverse-square law) 4.3 (Thermal Energy only) 4.4 The force of Gravity The Strength of Gravity ■ Newton and Kepler Orbits: 1. Closed: circles (circular velocity) & ellipses (v > v c ) 2. Open: parabolas and hyperbolas (escape velocity, v > v e ) Tides: Lunar and Solar Outline of Ch 4 Motion and Gravity (soap opera’s final episode)

16 © 2005 Pearson Education Inc., publishing as Addison-Wesley 4.4 The Force of Gravity Our goals for learning: What determines the strength of gravity? How does Newton’s law of gravity extend Kepler’s laws? How do gravity and energy together allow us to understand orbits? How does gravity cause tides?

17 © 2005 Pearson Education Inc., publishing as Addison-Wesley What determines the strength of gravity? The Universal Law of Gravitation 1.Every mass attracts every other mass. 2.Attraction is directly proportional to the product of their masses. 3.Attraction is inversely proportional to the square of the distance between their centers..

18 © 2005 Pearson Education Inc., publishing as Addison-Wesley How does Newton’s law of gravity extend Kepler’s laws? (some not in book) Ellipses are not the only orbital paths. Orbits can be: bound Circle (v = v c ) Ellipse (v > v c ) unbound Parabola (v = v e ) Hyperbola (v > v e ) Circular and Escape velocities ( v c and v e )  v c =  GM/R  v e =  2GM/R circular and

19 © 2005 Pearson Education Inc., publishing as Addison-Wesley

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21 Newton generalized Kepler’s Third Law: Newton’s version of Kepler’s Third Law : If a small object orbits a larger one and you measure the orbiting object’s orbital period AND average orbital distance THEN you can calculate the mass of the larger object. Examples: Calculate mass of Sun from Earth’s orbital period (1 year) and average distance (1 AU). Calculate mass of Earth from orbital period and distance of a satellite. Calculate mass of Jupiter from orbital period and distance of one of its moons. What about asteroids?

22 © 2005 Pearson Education Inc., publishing as Addison-Wesley Newton’s version of Kepler’s Third Law p = orbital period a=average orbital distance (between centers) (M 1 + M 2 ) = sum of object masses

23 © 2005 Pearson Education Inc., publishing as Addison-Wesley How do gravity and energy together explain orbits? Orbits cannot change spontaneously. An object’s orbit can only change if it somehow gains or loses orbital energy = kinetic energy + gravitational potential energy (due to orbit).

24 © 2005 Pearson Education Inc., publishing as Addison-Wesley  So what can make an object gain or lose orbital energy? Friction or atmospheric drag Rocket engine A gravitational encounter.

25 © 2005 Pearson Education Inc., publishing as Addison-Wesley If an object gains enough orbital energy, it may escape (change from a bound to unbound orbit) escape velocity from Earth ≈ 11 km/s from sea level (about 40,000 km/hr, 25,000 mph) What is Earth’s circular velocity at sea level?

26 © 2005 Pearson Education Inc., publishing as Addison-Wesley How does Newton’s law of gravity extend Kepler’s laws? (some not in book) Ellipses are not the only orbital paths. Orbits can be: bound Circle (v = v c ) Ellipse (v > v c ) unbound Parabola (v = v e ) Hyperbola (v > v e ) Circular and Escape velocities ( v c and v e )  v c =  GM/R  v e =  2GM/R circular and

27 © 2005 Pearson Education Inc., publishing as Addison-Wesley Mastering Astronomy: Study area: Ch 4 Interactive Fig. 4.18

28 © 2005 Pearson Education Inc., publishing as Addison-Wesley Escape and orbital velocities do NOT depend on the mass of the cannonball

29 © 2005 Pearson Education Inc., publishing as Addison-Wesley 4.1 and 4.2 Describing Motion, Newton and Galileo Speed, velocity and acceleration (skip momentum) Galileo’s experiments with falling objects: g = 9.8 m/sec2 Objects fall together Inertia (motion in absence of force) Newton’s Laws: 1.3 laws of motion: a. Inertia b. F=ma c. Action = Reaction 2.Gravitation: F= GM 1 M 2 /d 2 (Inverse-square law) 4.3 (Thermal Energy only) 4.4 The force of Gravity The Strength of Gravity ■ Newton and Kepler Orbits: 1. Closed: circles (circular velocity) & ellipses (v > v c ) 2. Open: parabolas and hyperbolas (escape velocity, v > v e ) Tides: Lunar and Solar Outline of Ch 4 Motion and Gravity (soap opera’s final episode)

30 © 2005 Pearson Education Inc., publishing as Addison-Wesley The tides due to the Moon affect: a) Only the Oceans b) The whole Earth c) Only the night side of Earth d) None of the other answers is correct Question

31 © 2005 Pearson Education Inc., publishing as Addison-Wesley Tides Gravitational force decreases with (distance) 2 –The Moon’s pull on Earth is strongest on the side facing the Moon, and weakest on the opposite side. The Earth gets stretched along the Earth-Moon line. The oceans rise relative to land at these points.

32 © 2005 Pearson Education Inc., publishing as Addison-Wesley Tides vary with the phase of the Moon:

33 © 2005 Pearson Education Inc., publishing as Addison-Wesley

34 Special Topic: Why does the Moon always show the same face to Earth? Moon rotates in the same amount of time that it orbits… But why?

35 © 2005 Pearson Education Inc., publishing as Addison-Wesley Tidal friction… Tidal friction gradually slows Earth rotation (and makes Moon get farther from Earth). Moon once orbited faster (or slower); tidal friction caused it to “lock” in synchronous rotation with its orbit around Earth.

36 © 2005 Pearson Education Inc., publishing as Addison-Wesley How does Newton’s law of gravity allow us to extend Kepler’s laws? Applies to other objects, not just planets. Includes unbound orbit shapes: parabola, hyperbola We can now measure the mass of other systems. What have we learned? What determines the strength of gravity? Directly proportional to the product of the masses (M x m) Inversely proportional to the square of the separation d

37 © 2005 Pearson Education Inc., publishing as Addison-Wesley What have we learned? How do gravity and energy together allow us to understand orbits? Gravity determines orbits Orbiting object cannot change orbit without energy transfer Enough energy -> escape velocity -> object leaves. How does gravity cause tides? Gravity stretches Earth along Earth-Moon line because the near side is pulled harder than the far side.


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