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Newton’s Laws of Motion

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Presentation on theme: "Newton’s Laws of Motion"— Presentation transcript:

1 Newton’s Laws of Motion
Chapter 4 Newton’s Laws of Motion

2 Stationary Earth Earth is heavy It looks like the sky is moving
Easier to imagine the sky can move It looks like the sky is moving We have no sensation of our motion Rotating Earth would make objects fly off of the surface Stellar Parallax

3 Stellar Parallax Hipparchus 150 BC June Sun January

4 Aristotelian Universe Terrestrial Realm
Composition predicts motion natural tendencies Fire and Air tend to rise Earth and Water tend to sink Overall tendency to seek rest Objects are corruptible (changing)

5 Aristotle attempted to understand motion by classification.
1. ARISTOTLE ON MOTION Aristotle attempted to understand motion by classification. Two Classes: Natural and Violent

6 Aristotelian Universe Celestial Realm
Celestial Objects composed of Aether Self luminous but does not consume Motion is constant, circular Objects are incorruptible (not changing) Meteors and comets were phenomena of the Earth’s atmosphere

7 The falling speed of an object was supposed to be proportional to its weight.
Galileo’s Experiment

8 Nicholas Copernicus (Niklas Koppernigk) Developed a mathematical model for a Sun-centered solar system

9 Galileo Galilei Among the first to turn a telescope to the sky Developed the Scientific Method Believed in the popularization of science Developed the Law of Inertia

10 He tested with planes. Demo - Ball and incline plane
The change in speed depended on the slope of the incline. Seemed that the ball was trying to achieve the same vertical height.

11

12 Isaac Newton

13 Newton’s Laws The 1st Law
A body continues to move as it has been moving unless acted upon by an external force.

14 Newton’s First Law No mention of chemical composition.
No mention of terrestrial or celestial realms Force required when object changes motion. Acceleration is the observable consequence of force acting.

15 Net Force Force is a vector
We must add all the forces acting on the body 5 N 10 N 5 N 5 N 5 N 0 N 5 N 10 N 5 N

16 Equilibrium When the net force is zero (SF = 0) Acceleration is zero
Velocity may not be zero

17 Mass and Inertia Inertia is a property of a body that resists changes in motion Mass is a measure of the amount of matter in a body Inertia and Mass are the same concept Units – Kg or slugs

18 Weight Force of gravity pulling on the mass of the body
Units – Newtons or Pounds A newton is about the weight of a small apple One kg weighs 2.2 lbs. W = mg g = acceleration due to gravity = 32 ft/s2 = 9.8 m/s2

19 Inertia Demonstrations
Demo - Table setting Demo - Bottle, hoop, and chalk

20 The 2nd Law Newton’s Laws
The Sum of the Forces acting on a body is proportional to the acceleration that the body experiences S F  a S F = (mass) a

21 2. NEWTON'S 2nd LAW OF MOTION

22 If the net force is perpendicular to the velocity, the direction of the velocity changes.
Acceleration is always in the direction of the net force.

23 When Acceleration Is Zero - Equilibrium
Static Equilibrium Velocity is zero Examples: Scales pushing up Normal up Weight down Computer setting on a table Weighing yourself on a set of scales Hanging from a tree Tree pulling up Weight down Car parked on an incline Normal Friction Weight down Weight down

24 Dynamic Equilibrium Velocity is nonzero and constant Examples:
Driving at constant velocity Normal up Friction Force from road Weight down

25 Newton’s Laws The 3rd Law
For every action force there is an equal and opposite reaction force (You cannot touch without being touched)

26 Oppose motion or the tendency of motion
Dissipative Forces Oppose motion or the tendency of motion Friction Air Resistance

27 Friction Depends upon... Static friction (no motion)
Materials that are in contact Forces that press surfaces together (Normal forces) Static friction (no motion) Proportional to force used until maximum is reached Kinetic friction (motion) Nearly constant for normal speeds

28 Friction Static F f Kinetic f F

29 Air Resistance Terminal Velocity! Depends on
Surface Area Velocity When weight = air resistance we have SF= 0 Þ a = 0 Weight Air Resistance Terminal Velocity!


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