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© 2005 Pearson Education Inc., publishing as Addison-Wesley Chapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity “ If I have.

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Presentation on theme: "© 2005 Pearson Education Inc., publishing as Addison-Wesley Chapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity “ If I have."— Presentation transcript:

1 © 2005 Pearson Education Inc., publishing as Addison-Wesley Chapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity “ If I have seen farther than others, it is because I have stood on the shoulders of giants.” — Sir Isaac Newton (1642 – 1727)

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 /R 2 (Inverse-square law) 4.3 (Thermal Energy only ignore the rest of 4.3) 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 4.1 Describing Motion Our goals for learning: How do we describe motion? How is mass different from weight?

4 © 2005 Pearson Education Inc., publishing as Addison-Wesley How do we describe motion? Precise definitions to describe motion: speed: rate at which object moves example: speed of 10 m/s velocity: speed and direction example: 10 m/s, due east acceleration: any change in velocity units of speed/time (m/s 2 )

5 © 2005 Pearson Education Inc., publishing as Addison-Wesley The Acceleration of Gravity (some not in book) g = 9.8 m/sec2 Objects fall together Inertia (motion in absence of force) Galileo was one of the giants on who’s shoulders Newton stood. Galileo’s experiments with falling objects showed that: Objects fall together (not counting friction of air resistance). On Earth, g ≈ 10 m/s 2 : speed increases 10 m/s with each second of falling (g = 9.8 m/s 2 ). Inertia (motion in absence of force: uniform rectilinear or at rest)

6 © 2005 Pearson Education Inc., publishing as Addison-Wesley

7 The Acceleration of Gravity (g) Galileo showed that g is the same for all falling objects, regardless of their mass. Apollo 15 demonstration

8 © 2005 Pearson Education Inc., publishing as Addison-Wesley Question: Is there a net force? Y/N 1.A car coming to a stop. 2.A bus speeding up. 3.A bicycle going around a curve. 4.A moon orbiting Jupiter.

9 © 2005 Pearson Education Inc., publishing as Addison-Wesley Is there a net force? Y/N 1.A car coming to a stop. Y 2.A bus speeding up. Y 3.A bicycle going around a curve. Y 4.A moon orbiting Jupiter. Y

10 © 2005 Pearson Education Inc., publishing as Addison-Wesley How is mass different from weight? mass – the amount of matter in an object weight – the force that acts upon an object You are weightless in free-fall!

11 © 2005 Pearson Education Inc., publishing as Addison-Wesley Question On the Moon: A.My weight is the same, my mass is less. B.My weight is less, my mass is the same. C.My weight is more, my mass is the same. D.My weight is more, my mass is less.

12 © 2005 Pearson Education Inc., publishing as Addison-Wesley On the Moon… A.My weight is the same, my mass is less. B.My weight is less, my mass is the same. C.My weight is more, my mass is the same. D.My weight is more, my mass is less.

13 © 2005 Pearson Education Inc., publishing as Addison-Wesley Why are astronauts weightless in space? There IS gravity in space… weightlessness is due to a constant state of free-fall: Ask me about another way to explain this

14 © 2005 Pearson Education Inc., publishing as Addison-Wesley What have we learned? How do we describe motion? Speed = distance/time Speed + direction => velocity (v) Change in velocity => acceleration (a)

15 © 2005 Pearson Education Inc., publishing as Addison-Wesley What have we learned? How is mass different from weight? Mass = quantity of matter Weight = force acting on mass Objects are weightless when in free-fall

16 © 2005 Pearson Education Inc., publishing as Addison-Wesley What have we learned? Galileo’s experiments with falling objects: On Earth g = 9.8 m/sec 2 (m/sec/sec) Objects fall together Inertia (motion in absence of force)

17 © 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?

18 © 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)

19 © 2005 Pearson Education Inc., publishing as Addison-Wesley What are Newton’s three laws of motion? Newton’s first law of motion: An object moves at constant velocity unless a net force acts to change its speed or direction (this he adopted from Galileo).

20 © 2005 Pearson Education Inc., publishing as Addison-Wesley Newton’s second law of motion: Force = mass  acceleration (F= ma)

21 © 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).

22 © 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..

23 © 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

24 © 2005 Pearson Education Inc., publishing as Addison-Wesley 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

25 © 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.

26 © 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. T 2.The change of velocity of the car is the same as the change of velocity of the truck. F

27 © 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. True 2.The change of velocity of the car is the same as the change of velocity of the truck. False (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)

28 © 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.

29 © 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)

30 © 2005 Pearson Education Inc., publishing as Addison-Wesley Temperature Scales

31 © 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 /R 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)

32 © 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?

33 © 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..

34 © 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

35 © 2005 Pearson Education Inc., publishing as Addison-Wesley

36

37 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?

38 © 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

39 © 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).

40 © 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.

41 © 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?

42 © 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

43 © 2005 Pearson Education Inc., publishing as Addison-Wesley Mastering Astronomy: Study area: Ch 4 Interactive Fig. 4.18

44 © 2005 Pearson Education Inc., publishing as Addison-Wesley Escape and orbital velocities do NOT depend on the mass of the cannonball

45 © 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 /R 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)

46 © 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

47 © 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

48 © 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.

49 © 2005 Pearson Education Inc., publishing as Addison-Wesley Tides vary with the phase of the Moon:

50 © 2005 Pearson Education Inc., publishing as Addison-Wesley

51 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?

52 © 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.

53 © 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

54 © 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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