Transcript

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Physics I95.141

LECTURE 69/22/10

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Exam Prep Problem

• A rock is launched with an initial speed vo=22m/s at an angle θo=65º from the origin. Ignore air resistance.– A)(10pts) Draw a coordinate system for this problem

and show the trajectory of the rock. Give the initial velocity vector of the rock in component form.

– B) (8pts) How high does the rock go and how long does it take the rock to get to that height?

– C) (7pts) How far, horizontally, will the rock travel before it lands?

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Exam Prep Problem

• A rock is launched with an initial speed vo=22m/s at an angle θo=65º from the origin. Ignore air resistance.– A)(10pts) Draw a coordinate system for this problem and show

the trajectory of the rock. Give the initial velocity vector of the rock in component form.

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Exam Prep Problem

• A rock is launched with an initial speed vo=22m/s at an angle θo=65º from the origin. Ignore air resistance.– B) (8pts) How high does the rock go and how long does it take

the rock to get to that height?

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Exam Prep Problem

• A rock is launched with an initial speed vo=22m/s at an angle θo=65º from the origin. Ignore air resistance.– B) (7pts) How far, horizontally, will the rock travel before it

lands?

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Administrative Notes

• HW review Session Tonight– 6:30 pm, OH 218

• Structure of HW Review Sessions– Why we do it this way

– Why it is important to try

• Structure of this course– Combination of your effort/our effort

• Lecture Notes

• Practice exams/prep problems

• Attendance Policy

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Outline

• Force• Newton’s 1st Law• Newton’s 2nd Law• Newton’s 3rd Law

• What do we know?– Units– Kinematic equations– Freely falling objects– Vectors– Kinematics + Vectors = Vector Kinematics– Relative motion– Projectile motion

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Force

• Intuitively, we understand a Force to be a push or pull on an object– This could be a racket hitting a ball, elevator cable

pulling on a car, a locomotive pulling a train…• These are all contact forces, where the force is exerted by

one object in contact with another

– Force can also be exerted by magnets, electric fields, or gravity

• Here, Force is exerted by a field, not an object, but this is still a force!

• Force has magnitude and direction: it is a VECTOR!

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Force

• In order for something at rest to start moving, a Force must be exerted on it.

• However, if something is already moving, you also need a Force acting on it to stop motion!

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Inertia

• Obviously, some things are harder to get moving than others…

• If you had to choose whether to carry an ice skater or an offensive lineman up to the Dean’s office on the 5th floor: which do you think would be easier?

• We quantify inertia with a measure we call mass• SI units: mass [kg]

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Newton’s 2nd Law

• If Newton’s first law tells us how an object behave with no Force, we also want to understand how an object behaves with a Force applied.

• The acceleration of an object is directly proportional to the net force applied to the object, and the constant of proportionality is mass.

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Units for Force

• Using Newton’s 2nd Law, we can figure out the units of Force.

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Redefine Force

• An action capable of accelerating an object

• Acceleration is a vector, as is Force. Net acceleration is in the same direction as net Force.

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Example Problem

• A 1500kg car traveling at 100km/h needs to stop in 55m. What force is required?

• Draw diagram

• Determine coordinate system

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Example Problem

• A 1500kg car traveling at 100km/h needs to stop in 55m. What force is required?

• Knowns/Unknowns (UNITS)

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Example Problem

• A 1500kg car traveling at 100km/h needs to stop in 55m. What force is required?

• Choose equations and solvemx

kgm

v

final

sm

o

55

1500

8.27

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Connection between Newton’s 1st, 2nd Laws

• If F=ma• And no Force is exerted on an object• How can we describe the object’s velocity?

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Newton’s 2nd Law

• Do Newton’s 1st and 2nd Law work every where?– Say you are in a pickup truck that is accelerating, and

you put a frictionless block in the back.– What do you see happening to the block?

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Newton’s 2nd Law

• Do Newton’s 1st and 2nd Law work every where?– Say you are in a pickup truck that is accelerating, and

you put a frictionless block in the back.– What is the Force causing this?

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Newton’s 2nd Law• Do Newton’s 1st and 2nd Law work every where?

– Say you are in a pickup truck that is accelerating, and you put a frictionless block in the back.

– What does someone on the ground see?

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Inertial Reference Frames

• Newton’s Laws only work in Inertial reference frames

• Inertial reference frame– One in which Newton’s Laws hold

– A Reference Frame that moves with a constant velocity

– A Reference Frame at rest

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Newton’s 3rd Law of Motion

• 1st Law: Law of Inertia, things want to keep on doing what they are already doing.

• 2nd Law: Forces cause objects to accelerate, with a=F/m.

• But where do forces come from?– Forces come from other objects

• Hammer exerts a force on the nail• The Earth exerts a force on a falling ball (gravity)• Elevator cable exerts force on car…

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Newton’s 3rd Law

• But when hammer hits nail, it stops very quickly.• This is deceleration, which means the nail must

also exert a Force on the hammer.• This is Newton’s 3rd Law

– Whenever one object exerts a Force on a second object, the second object exerts an equal Force in the opposite direction.

– Sometimes, you hear: “For every action, there is an equal and opposite reaction”

– Remember though, the action and reaction act on different objects!

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Action/Reaction

• They actually get the Physics right here!

• For every Force exerted on an object, there is an equal and opposite force exerted by that object

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Describing Forces

• When we talk about Forces, it is very important that we describe the Force as “exerted by” something and “acting on” another thing.– For instance, in the case of the ice skater, force is exerted on the

skater by the ice.– For the car, the Force making the car move is exerted by the

ground on the tires.• When we start solving problems, it is important to keep

this straight. If you are interested in the motion of an object, you only want to sum up the Forces acting on that object.

• For a person walking, the ground is what moves the person forward.

GPPG FF

Department of Physics and Applied Physics95.141, F2010, Lecture 6

The Motivator

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Draw Diagram

• Want F, need to figure out acceleration– Assume

• Tf=0.25s

• M=60kg• Δx=1.8m• Δy=-1m

1.8m

1m

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Projectile Motion Problem (I)

• What is initial launch velocity?

Department of Physics and Applied Physics95.141, F2010, Lecture 6

Acceleration

• If we know the initial launch velocity, then we know the final velocity after acceleration– Initial velocity of part II = final velocity of part I

Department of Physics and Applied Physics95.141, F2010, Lecture 6

What Did We Learn

• Newton’s Laws– Law of Inertia– F=ma– Action/Reaction

• Solving basic Force problems• How to describe motion of an object with Force

applied.


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