newton’s laws of motion dynamic dynamics and unexpected returns chapter 3

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Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

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Page 1: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Newton’s Laws of Motion

Dynamic dynamics and unexpected returnsChapter 3

Page 2: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Sir Isaac Newton

• Determined many physical laws based on mathematics.

• His book, Principia, revolutionized the fields of both science and mathematics

Page 3: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Newton’s First Law of Motion

• Inertia• An object at rest will remain at rest, and

an object in motion will remain in motion unless acted upon by an outside force– Dependent on mass

Page 4: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Newton’s 1st Law of Motion

Page 5: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Which has more inertia?

1. An empty dump truck2. A full dump truck

Page 6: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Which has more inertia?

1. A quarter2. A dime

Page 7: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Which has more inertia?

1. A freight train2. A full dump truck

Page 8: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Which has more inertia?

1. A freight train2. A cargo plane

Page 9: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Which has more inertia?

1. An empty dump truck going 170 km/h

2. A cargo plane sitting on the runway

Page 10: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Newton’s Second Law of Motion

• Force equals mass multiplied by acceleration

• F = m•a– Force is any push or pull that can affect

motion– Mass in kg, acceleration in m/s2

– Newtons: 1N = 1kg•m/s2

Page 11: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Newton’s 2nd Law of Motion

Page 12: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What is the force applied by a mass of 2 kg with an acceleration of 6 m/s2?1. 6 N2. 3 kg●m/s3. 12 kg●m/s2

Page 13: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What is the acceleration of a mass of 6 kg applying a force of 24 N?1. 4 m/s2

2. 144 m/s2

3. 0.25 m/s2

Page 14: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What is the force applied by the acceleration of a 3.5 kg mass to 7 m/s2?1. 2 N2. 24.5 kg●m/s2

3. 0.5 kg ●m/s2

Page 15: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What mass is required to apply a force of 28 N after an acceleration of 7 m/s2?1. 196 kg2. 4 kg3. 0.25 kg

Page 16: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What acceleration would cause a 12 kg mass to produce a force of 90 kg●m/s2?1. 7.5 N2. 7.5 m/s3. 7.5 m/s2

Page 17: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Balanced v. Unbalanced Forces• Balanced forces are equal and

opposite on the same object– Balanced forces result in NO

acceleration• Equilibrium

– Unbalanced forces are added geometrically• The Resulting or Net Force always results

in an acceleration

Page 18: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Showing “Equal and Opposite”

• The observer determines the direction of motion

• Directions opposite that motion can be considered NEGATIVE

• Because the direction is considered negative, the forces can be considered negative

Page 19: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What would the net force be if you pushed against the wall with 122,616N?1. 122,616 N2. -122,616 N3. 0 N

Page 20: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What would the net force be if two players kick a soccer ball from opposite directions according to the diagram?

1. 60 N, to the left2. 60 N, to the right3. 0 N4. 180 N, upwards

Page 21: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What would the net force be if you pushed a hockey puck with 200 N?1. 0 N2. 200 N against the push3. 200 N in the direction of the push

Page 22: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Newton’s Third Law of Motion

• For every action, there is an equal and opposite reaction– These forces act on two different

objects, so they are not balanced forces

Page 23: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Newton’s 3rd Law of Motion

Page 24: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Good Examples

• Rocket engines• Firing a gun• Jumping off of a johnboat

Page 25: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Forces and Vectors

Page 26: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Gravity

• Gravity is a force of attraction between all objects of mass.

• Depends on:– the distance between the masses

• “inverse square” law– the size of the masses

• Often as a percentage of the whole

Page 27: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Weight

• Weight is the force of attraction caused by gravity acting on a mass.

Fw = m•g

• The g means local gravity– on Earth, g = 9.8m/s2

Page 28: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Gravity

Page 29: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Weight v. Mass

• We use weight and mass interchangeably because the only comparison we have is the Earth’s gravity.

• Weight will change based on local gravity; NASA has to take this into effect

Page 30: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

How much does a 25 kg object weigh in Newtons?

1. 245 N2. 2.6 N3. 0.392 N

Page 31: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

If an object weighs 397 N, what is its mass?

1. 0.02 kg2. 3890.6 kg3. 40.5 kg

Page 32: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

If an object weighs 1100 N but has a mass of 125 kg, which planet is it on?1. Venus, g = 8.8 m/s2

2. Mars, g = 3.7 m/s2

3. Jupiter, g = 24.8 m/s2

Page 33: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Friction

• Friction is the force that opposes all motion.

• A moving object will always lose energy to friction

Page 34: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Types of Friction

• Sliding Friction– When two surfaces slide along each

other– Most resistive friction– Can lead to buildup of heat

Page 35: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Types of Friction

• Rolling Friction– When an object or surface rolls along

another– Less resistive than sliding, more

resistive than fluid

Page 36: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Types of Friction

• Fluid Friction– When a surface slides along a fluid

(gas or liquid)– Least resistive friction

• Lubrication

– Air resistance

Page 37: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What type of friction is exhibited by your shoes on the ground?1. Sliding2. Rolling3. Fluid4. Air Resistance5. None of the

above

Page 38: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What type of friction is exhibited by a lubricant?1. Sliding2. Rolling3. Fluid4. Air Resistance5. None of the

above

Page 39: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What type of friction is exhibited by the wheels on a cart?1. Sliding2. Rolling3. Fluid4. Air Resistance5. None of the

above

Page 40: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What type of friction is exhibited by your fingerprints?1. Sliding2. Rolling3. Fluid4. Air Resistance5. None of the

above

Page 41: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

The Big “Mo”

• Momentum is the product of an object’s mass multiplied by its velocity.

• p = m • v• kg•m/s = kg • m/s

Page 42: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

What is the momentum of a 210 kg hog running at 12 m/s?

1. 17.5 kg●m/s2. 2520 kg●m/s3. 0.057 kg●m/s

Page 43: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Law of Conservation of Momentum

• Momentum can not be created or destroyed under normal circumstances

• Momentum can be changed from one form to another– Total momentum before a change must

equal total momentum after a change• Ex. truck of gravel coming to a stop,

pieces of a dropped light bulb

Page 44: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Law of Conservation of Momentum

• Formulam1v1+m2v1 = m1v2+m2v2

Page 45: Newton’s Laws of Motion Dynamic dynamics and unexpected returns Chapter 3

Conservation of Momentum and Newton’s Laws

• An untethered astronaut is stranded away from his spaceship while working on a satellite in space. The only equipment he has is all the tools he was using to repair the satellite.

• Write a short narrative of how you think he can get back to his spaceship.