Newton’s Laws of Motion

Slides:



Advertisements
Similar presentations
Chapter 4 The Laws of Motion Force Newton’s Laws Applications Friction.
Advertisements

Chapter 5 – Force and Motion I
Forces and Newton’s Laws of Motion
Chapter 4 The Laws of Motion.
Forces and Newton’s Laws of Motion Chapter 4. All objects naturally tend to continue moving in the same direction at the same speed. All objects resist.
1 Chapter Four Newton's Laws. 2  In this chapter we will consider Newton's three laws of motion.  There is one consistent word in these three laws and.
Dr. Steve Peterson Physics 1025F Mechanics NEWTON’S LAWS Dr. Steve Peterson
Applications of Newton’s Laws
Applying Forces (Free body diagrams).
AP Physics Chapter 5 Force and Motion – I.
PHYS 218 sec Review Chap. 4 Newton’s laws of motion.
Kinematics – the study of how things move
Chapter 4 Forces and Mass. Classical Mechanics does not apply for very tiny objects (< atomic sizes) objects moving near the speed of light.
Chapter 4 Forces and Mass.
Chapter 4: Forces & Newton’s Laws of Motion Lecture Notes
Ballistic Cart Demo Discuss law of cosines for planeinwindb problem Other HW problems?
ISAAC NEWTON AND THE FORCE Dynamics. Kinematics vs Dynamics Kinematics – the study of how stuff move  Velocity, acceleration, displacement, vector analysis.
Chapter 5 Force and Motion
Newton’s Laws of Motion
Forces and Newton’s Laws of Motion
Chapter 4 The Laws of Motion. Classical Mechanics Describes the relationship between the motion of objects in our everyday world and the forces acting.
Classical Mechanics Describes the relationship between the motion of objects in our everyday world and the forces acting on them Conditions when Classical.
Kinematics – the study of how things move Dynamics – the study of why things move Forces (the push or pull on an object) cause things to move Aristotle.
Dynamics Chapter 4. Expectations After Chapter 4, students will:  understand the concepts of force and inertia.  use Newton’s laws of motion to analyze.
Chapter 4: The Laws of Motion Forces  There seem to be two kinds of forces in Nature: Contact forces and field forces.  A contact force is transferred.
EVERY-DAY FORCES Force of gravity Normal force Force of friction Universal force of gravity.
FORCES AND LAWS OF MOTION. FORCE (push) (pull) Examples of forces: ContactField Pulling the handle of the door Pushing a stroller Hitting a tennis ball.
Chapter 6 Force and Motion.
Forces Contact Forces - those resulting from physical contact between objects –Normal Force –Friction –Tension (spring/rope) –Compression Action at a Distance.
Forces and the Laws of Motion Chapter Changes in Motion Objectives  Describe how force affects the motion of an object  Interpret and construct.
Forces and Mass. Classical Mechanics does not apply for very tiny objects (< atomic sizes) objects moving near the speed of light.
Newton’s Laws of Motion Dynamics After studying Kinematics, we know how to describe motion in two and three dimensions. But what causes this motion?
Chapter 4 The Laws of Motion. Classical Mechanics Describes the relationship between the motion of objects in our everyday world and the forces acting.
FORCES AND LAWS OF MOTION. FORCE EXAMPLES OF FORCES: Close rangeLong Range Pulling the handle of the door Pushing a stroller Hitting a tennis ball with.
Chapter 4 -Day 7 The Laws of Motion. Hi Ho Silver!! Horse A (Appaloosa)leaves from point A and travels 30mph. Horse B (Arabian) leaves point A, 2 hours.
Forces and the Laws of Motion
Newton’s Laws Chapter 4 Physics chapter 4.
Chapter 4 Forces and Newton’s Laws of Motion. 4.1 The Concepts of Force and Mass A force is a push or a pull. Contact forces arise from physical contact.
Physics 111: Mechanics Lecture 4
Chapter 5 THE LAWS OF MOTION. Force, net force : Force as that which causes an object to accelerate. The net force acting on an object is defined as.
Remember!!!! Force Vocabulary is due tomorrow
Forces Today’s Goal: 1.Describe and give examples of the law of inertia and understand that inertia is a basic property of matter.
Chapter 4 The Laws of Motion. Classical Mechanics Describes the relationship between the motion of objects in our everyday world and the forces acting.
Honors Physics Chapter 4
Chapter 5 The Laws of Motion.
Chapters 5, 6 Force and Laws of Motion. Newtonian mechanics Describes motion and interaction of objects Applicable for speeds much slower than the speed.
Raymond A. Serway Chris Vuille Chapter Four The Laws of Motion.
Chapter 4 Dynamics: Aim: How can we describe Newton’s Laws of Motion? © 2014 Pearson Education, Inc.
FORCES Chapter 5. Mechanics The study of Motion Isaac Newton, 1600’s The father of mechanics.
Forces and Newton’s Laws of Motion. A force is a push or a pull. Arrows are used to represent forces. The length of the arrow is proportional to the magnitude.
Chapter 4 The Laws of Motion.
Forces and the Laws of MotionSection 1 Preview Section 1 Changes in MotionChanges in Motion Section 2 Newton's First LawNewton's First Law Section 3 Newton's.
Physics Chapter 4 Forces and the Laws of Motion. §A force is defined as a push or pull exerted on an object. §Forces can cause objects to speed up, slow.
Forces. What is a Force? A force is a push or pull acting on an object that changes the motion of the object.
Physics and Forces Dynamics Newton’s Laws of Motion  Newton's laws are only valid in inertial reference frames:  This excludes rotating and accelerating.
Raymond A. Serway Chris Vuille Chapter Four The Laws of Motion.
Ying Yi PhD Chapter 4 The Laws of Motion 1 PHYS HCC.
 A force is defined simply as a push or a pull on an object  A force is a VECTOR quantity  Units: lbs or Newtons (N)  1 lb = 4.45 Newtons  What is.
Chapter 4 Forces in One Dimension. Classical Mechanics Describes the relationship between the motion of objects in our everyday world and the forces acting.
PHYSICS 101 Lecture 04. Newton’s Laws First Physics.
Chapter 4 Forces and Newton’s Laws of Motion. Newtonian mechanics Describes motion and interaction of objects Applicable for speeds much slower than the.
The Laws of Motion. Classical Mechanics Describes the relationship between the motion of objects in our everyday world and the forces acting on them Describes.
The Dynamics of Newton’s Laws
Forces Chapter 5.
Chapter 4 Newton’s Laws.
Forces and Newton’s Laws of Motion
Ch 4 Forces in One Dimension
Force Problems.
The Laws of Motion (not including Atwood)
Presentation transcript:

Newton’s Laws of Motion

Review Equations for Motion Along One Dimension

Review Motion Equations for Constant Acceleration 1. 2. 3. 4.

Dynamics vs Kinematics So far we’ve been studying kinematics, we’ve been describing how things move. We were only concerned with a particles position, velocity or acceleration. But why do things move? What gives objects motion?

What is Force?

What is Force? Force is either a push or a pull. It is an interaction between two bodies. Force is a vector. It has both magnitude and direction. When force is a result of two objects touching, we call that a contact force. Aside from that there are also long-range forces or field forces

Examples of Contact Forces Normal Force Frictional Force Tension Force

Examples of Field Forces Gravitational Force Magnetic Force Electric Attraction

Fundamental Forces Gravitational Forces – weakest of the four forces Electromagnetic Forces – force between electrically charged particles. Weak Nuclear Forces – responsible for some nuclear phenomena like beta decay Strong Nuclear Forces – only holds inside an atomic nucleus.

Superposition of Forces Throwing a basketball into the hoop What are the forces involved?

Superposition of Forces Throwing a basketball into the hoop What are the forces involved? Force of your hand on the ball Force of gravity (i.e. weight)

Superposition of Forces If we can add forces, we can also separate a force into its components!

Examples Young and Freedman 4.4 A man is dragging a trunk up a loading the loading ramp of a mover’s truck. The ramp has a slope angle of 20.0o, and the man pulls upward with a force F, who’s direction makes an angle of 30o with the ramp. (a) How large a force F is necessary for the component Fx parallel to the ramp to be 60.0 N? (b) How large will the component Fy perpendicular to the ramp then be?

Isaac Newton Born January 4, 1643 (December 25, 1642 under old calendar) He was a physicist, mathematician, astronomer, natural philosopher, alchemist and theologian. Considered by many to be the “greatest scientist who ever lived”. He published the “Philosophiæ Naturalis Principia Mathematica” in 1687 which laid the foundations for classical mechanics.

He also invented calculus

Isaac Newton – lesser known facts Was a religious nut He published more papers on scripture than science. He poured over the bible looking for secret codes. He also poured a lot of effort into alchemy and the philosophers stone

Isaac Newton – questionable facts Invented the cat door (pet door) Apple hitting Newton on the head

Principia was written due to a bet Christopher Wren was with some astronomers when he bet 40 shillings (around 4,000 php now) that no one could explain elliptical orbits. It took Newton years to find the answer so he didn’t get any money. But he expanded his answers and published Principia. Included in Principia are the Three Laws of Motion

First Law of Motion Lets examine an object at rest If there are no forces acting on it the object what will happen to the object? If the sum of forces on an abject equal zero, what will happen to the object?

First Law of Motion Lets examine an object in motion If there are no forces acting on it the object what will happen to the object? If the sum of forces on an abject equal zero, what will happen to the object?

First Law of Motion Every object continues in its state of rest or of uniform velocity as long as no net force acts on it. Inertia – the tendency of an object to maintain its state of rest or uniform motion Law of inertia A body is in equilibrium if

But wait If you’re in a decelerating car, your body gets thrown forward, but there is no net force acting on you!!!

Inertial Frames of Reference Frames of reference where First Law of Motion holds Frames fixed on the Earth can be considered to be inertial frames of reference Frames of reference travelling at constant velocity relative to another inertial frame are also inertial frames (a=0).

Mass Mass is usually defined as quantity of matter an object has. We need to be a bit more specific here Mass is a measure of inertia of an object. Uses SI unit kg

Mass vs Weight Mass and weight are used interchangeably in everyday language In physics, mass and weight are different Mass is the measure of inertia. It is an intrinsic property of matter. No matter where you are, or where the observer is, your mass will be the same. Weight is the force of gravity on an object. Your weight will be different here than on the moon or in space.

Young and Freedman 4.20 An astronauts pack weighs 17.5N on earth and 3.24N on an asteroid. (a) what is the acceleration due to gravity on the asteroid? (b) what is the mass of the pack on the asteroid?

What happens then if net Force is not equal to 0

Newton’s Second Law of Motion The acceleration of an object is directly proportional to the net force acting on it and indirectly proportional to its mass. The direction of the acceleration is in the direction of the net force acting on the object.

Force We now define the Newton 1 Newton is the amount of force needed to accelerate a 1kg object by 1m/s2 1N=1kg m /s2 It is the SI unit for Force

Force We now define the Newton 1 Newton is the amount of force needed to accelerate a 1kg object by 1m/s2 1N=1kg m /s2 It is the SI unit for Force Pull of the earth is a force Weight has SI unit of N

Example What average force is required to stop an 1,100 kg car in 8.0 s if the car is travelling at 95 km/h

Example We have mass, we need acceleration

Example

Newton’s Third Law of Motion Force is an interaction between two objects It always comes in pairs

Newton’s Third Law of Motion Whenever one object exerts a force on a second object, the second exerts an equal force in the opposite direction on the first.

Newton’s Third Law of Motion To every action there is an equal but opposite reaction Remember the action and reaction forces are acting on different objects

Horse and Cart Paradox

Example Giancoli 4-19 A box weighing 77.0N is resting on a table. A rope tied to the box runs vertically upward over a pulley and a weight is hung from the other end. Determine the force the table exerts on the box if the weight on the other side of the pulley weighs (a) 30.0N (b) 60.0N (c) 90.0N 77N

Example Force table exerts on the box is just normal force Normal Force = Weight of box on table 77N

Application of Newton’s Laws Serway 5-18 A bag of cement weighs 325 N and hangs from three wires. Two of the wires make angles 60.0o and 25.0o with the horizontal. If the system is in equilibrium, find the tensions, T1, T2, T3 in the wires.

Young & Freedman 5.10 A 1130 kg car is held in place by a light cable on a very smooth (frictionless) ramp. The cable makes an angle of 31.0o above the surface of the ramp. The ramp itself rises 25.0o above the horizontal. (a) find the tension in the cable. (c) How hard does the surface of the ramp push on the car?

Giancoli 4-30 At the instant a race began a 65kg sprinter exerted a force of 720N on the starting block at an angle of 22o with respect to the ground. (a) What is the horizontal acceleration of the sprinter? (b) if the force was exerted for 0.32s with what speed did the sprinter leave the starting block?

Serway 5-24 A 5.00 kg object placed on a frictionless, horizontal table is connected to a string that passes over a pulley and then is fastened to a hanging 9.00-kg object. Find the acceleration of the two objects and the tension in the string.

Giancoli 4-34 Two masses each initially 1.80 m above the ground, and the massless fricitonless pulley is 4.8m above the ground. What maximum height does the lighter mass reach after the system is released? 4.80 m 2.2 3.2 1.80 m

Friction Results from contact between two surfaces. Parallel to the surface of contact. Always opposite to the relative motion of the two surfaces.

Kinetic Friction Frictional force can be approximated to be proportional to normal force Where µk is the coefficient of kinetic friction Note: friction is not dependent on surface area

Static Friction Force of friction that arises even when objects are not in relative motion. Where µs is the coefficient of Static friction

Friction Graph

Young & Freedman 5.30 A box of bananas weighs 40.0N and rests on a horizontal surface. µs=0.40 while µk =0.20. (a) if no horizontal force is being applied and the box is at rest, what is the friction force exerted on the box. (b) What is the magnitude of friction is a monkey exerts a force of 6.0 N on the box. (c) What is the minimum horizontal force the monkey needs to apply to start the box in motion? (d) What is the minimum horizontal force the monkey needs to keep the box in motion? (e) If the monkey applies a horizontal force of 18.0N what is the magnitude of friction force and the boxes acceleration.

Young & Freedman 5.30 FN=40.0N (a) = 0 (b) max fs=0.4*40=16N => fs=6N (c) 16N (d) fk=0.2*40=8N (e) Fnet=ma=F-fk ma=18-8=10N a=10/m=10*9.8/40=2.45m/s2

Serway 5-44 Three objects are connected as shown. Table has µk =0.350. (a) determine the acceleration of each object in the system (b) Determine the tensions in the two chords.

Serway 5-49 A block weighing 75.0N rests on a plane inclined at 25.0o to the horizontal. A force F is applied at 40.0o to the horizontal pushing it upward on the plane. If µs =0.363 and µk =0.156 (a) What is the minimum value of F to prevent the block from slipping down the plane. (b) what is the minimum value of F that will start the block up the plane. (c) What value of F will move the block up at constant velocity.

Apparent Weight Tension in an elevator cable Elevator has a total mass of 800 kg. its moving downwards at 10 m/s but slows to a stop at constant acceleration for 25.0m. Find the tension T while the elevator is being brought to rest.

Apparent Weight Elevator has a total mass of 800 kg. its moving downwards at 10 m/s but slows to a stop at constant acceleration for 25.0m. Find the tension T while the elevator is being brought to rest. A woman is on a scale while riding the elevator. Mass of the woman is 50.0 kg, what is the reading on the scale?

Common Movie Mistakes

Seat Work/Home Work (time dependent) A block with mass 15.0kg is placed on a frictionless inclined plane with slope 20.0o and is connected to a second block with mass 6.00kg hanging over a small, frictionless pulley. (a) Will the first block accelerate to the left or to the right? (b) What is the magnitude of the acceleration?

Seat Work/Home Work (time dependent) A block with mass 15.0kg is placed on an inclined plane with slope 20.0o and is connected to a second block with mass 6.00kg hanging over a small, frictionless pulley. If µs= 0.300 and µk= 0.150 (a) Will the system accelerate? Why or why not? (b) If yes, what is the magnitude of the acceleration?