Instructor: Dr. Tatiana Erukhimova

Slides:



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

Newton’s Laws of Motion and Free Body Analysis
Chapter 5 – Force and Motion I
Chapter 7. Newton’s Third Law
Chapter 4 The Laws of Motion.
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.
Section 4-7 Solving Problems with Newton’s Laws; Free Body Diagrams
Newton’s Laws The Study of Dynamics Isaac Newton Arguably the greatest physical genius ever. Came up with 3 Laws of Motion to explain the observations.
Motion and Force Dynamics
AP Physics Chapter 5 Force and Motion – I.
Applying Newton’s Laws. A systematic approach for 1 st or 2 nd Law Problems 1.Identify the system to be analyzed. This may be only a part of a more complicated.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 19.
The first exam will be held on Tuesday, September 23, in room 109 Heldenfels from 7 to 9:30 p.m. Section 807 and half of section 808 (students with last.
Instructor: Dr. Tatiana Erukhimova
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Sections 818, 819, 820, 821 Lecture 11.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures Hw: Chapter 13 problems and exercises Reading: Chapter 14.
Chapter 5: The laws of motion
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 13.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures
Instructor: Dr. Tatiana Erukhimova
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 14.
Instructor: Dr. Tatiana Erukhimova
The first exam will be on Tuesday, September 25, room 109 in Heldenfels building. Section 807 and half of the Section 808 (students with last name starting.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Sections 818, 819, 820, 821 Lecture 10.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 15.
Physics Instructor: Dr. Tatiana Erukhimova Lecture 6.
The first exam will be held next Tuesday, on September 29, in room 114 Richardson from 7 to 9:10 p.m. Section 807 and half of section 808 (students with.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Sections 807, 808, 809 Lecture 8.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 11.
Physics 218, Lecture VII1 Physics 218 Lecture 7 Dr. David Toback.
Exam 1 results Average : 72 Section 807: 67 Section 808: 73 Section 809: 75 No. of students
Newton’s Laws 1st Law: A body acted on by no net force moves with constant velocity (which may be zero) 2st Law: The acceleration of an object is directly.
Large Hadron Collider went online on Sept Counter propagating proton beams accelerated to 7x10 12 eV make 11,000 revolutions per second and collide.
Chapter 7. Newton’s Third Law
Physics 203 – College Physics I Department of Physics – The Citadel Physics 203 College Physics I Fall 2012 S. A. Yost Chapter 4 Newton’s Laws – Part 3.
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.
Physics 201: Lecture 9, Pg 1 Lecture 8 l Goals:  Solve 1D & 2D problems introducing forces with/without friction  Utilize Newton’s 1 st & 2 nd Laws 
Forces Contact Forces - those resulting from physical contact between objects –Normal Force –Friction –Tension (spring/rope) –Compression Action at a Distance.
Newton’s Laws The Study of Dynamics.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 13, 14, 15.
Lecture 8: Forces & The Laws of Motion. Questions of Yesterday 1) You must apply a force F 1 to begin pushing a crate from rest across the floor, you.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 10.
Newton’s Laws - continued Friction, Inclined Planes, N.T.L., Law of Gravitation.
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.
Mechanics 105 Kinematics – answers the question “how?” Statics and dynamics answer the question “why?” Force Newton’s 1 st law (object at rest/motion stays.
PHYS16 – Lecture 10 & 11 Force and Newton’s Laws September 29 and October 1, 2010
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 13, 14, 15.
Monday, Sept. 18, 2002PHYS , Fall 2002 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #5 Monday, Sept. 18, 2002 Dr. Jaehoon Yu 1.Newton’s Laws.
Frictional Forces  Two types: - static – applies to stationary objects - kinetic – applies to sliding (moving) objects  Like F N, the Frictional Force.
Applications & Examples of Newton’s Laws. Forces are VECTORS!! Newton’s 2 nd Law: ∑F = ma ∑F = VECTOR SUM of all forces on mass m  Need VECTOR addition.
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.
Lecture 9: Forces & Laws of Motion. Questions of Yesterday You must apply a force F to push your physics book across your desk at a constant velocity.
More Fun with Newton’s Laws Friction, Inclined Planes, N.T.L.
Ch. 5: Using Newton’s Laws: Friction, Circular Motion, Drag Forces
Instructor: Dr. Tatiana Erukhimova
Newton’s Laws.
Physics Instructor: Dr. Tatiana Erukhimova Lecture 6.
Physics 215 – Fall 2014Lecture Welcome back to Physics 215 Today’s agenda: More on free-body diagrams and force components Applying Newton’s laws.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 16, 17, 18.
Monday, Sept. 20, 2004PHYS , Fall 2004 Dr. Jaehoon Yu 1 1.Newton’s Laws of Motion Gravitational Force and Weight Newton’s third law of motion 2.Application.
Force Problems. A car is traveling at constant velocity with a frictional force of 2000 N acting opposite the motion of the car. The force acting on the.
Physics 218 Lecture 8: Dynamics Alexei Safonov.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures
NEWTON'S LAWS OF MOTION Philosophiae Naturalis Principia Mathematica (1686)
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Presentation transcript:

Instructor: Dr. Tatiana Erukhimova Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 13-15

Newton’s Laws 1st Law: A body acted on by no net force moves with constant velocity (which may be zero) and zero acceleration 2nd Law: The acceleration of an object is directly proportional to the net force acting on it and is inversely proportional to its mass. The direction of the acceleration is in the direction of the net force acting on the object. 3rd Law: For every action there is an equal, but opposite reaction

Reading quizzes (Chs 5,6)

Hockey Puck a) Which of these three best represents a hockey puck in the real world? b) c)

Newton’s 1st Law A body acted on by no net force moves with constant velocity (which may be zero) and zero acceleration

Aristotle: a natural state of an object is at rest; a force is necessary to keep an object in motion. It follows from common sense. 384-322 B.C. Galileo: was able to identify a hidden force of friction behind common-sense experiments 1564-1642

Galileo: If no force is applied to a moving object, it will continue to move with constant speed in a straight line Inertial reference frames Galilean principle of relativity: Laws of physics (and everything in the Universe) look the same for all observers who move with a constant velocity with respect to each other.

Newton’s second law The vector acceleration of an object is in the same direction as the vector force applied to the object and the magnitudes are related by a constant called the mass of the object.

A Recipe for Solving Problems Sketch Isolate the body (only external forces but not forces that one part of the object exert on another part) 2. Write down 2nd Newton’s law Choose a coordinate system Write 2nd Newton’s law in component form: 3. Solve for acceleration

Is it better to push or pull a sled? You can pull or push a sled with the same force magnitude, FP, and angle Q, as shown in the figures. Assuming the sled doesn’t leave the ground and has a constant coefficient of friction, m, which is better? FP FP

FFriction = mKineticN Kinetic Friction THIS IS NOT A VECTOR EQUATION! For kinetic friction, it turns out that the larger the Normal Force the larger the friction. We can write FFriction = mKineticN Here m is a constant Warning: THIS IS NOT A VECTOR EQUATION!

FFriction  mStaticN Static Friction This is more complicated For static friction, the friction force can vary FFriction  mStaticN Example of the refrigerator: If I don’t push, what is the static friction force? What if I push a little?

Coefficient of friction:  H What is the normal force? What is the velocity of the block when it reaches the bottom?

For every action there is an equal, but opposite, reaction Newton’s 3rd Law For every action there is an equal, but opposite, reaction

Skater Equal and opposite force Force provides an acceleration Skater pushes on a wall The wall pushes back Equal and opposite force The push from the wall is a force Force provides an acceleration She flies off with some non-zero speed

P m1 m1 m2 Free body diagram N2 N1 F12 P F21 m2 m1 m2g m1g F12=F21 No friction P m1 m1 m2 Free body diagram N2 N1 F12 P F21 m2 m1 m2g m1g F12=F21

A small block, mass 2kg, rests on top of a larger block, mass 20 kg A small block, mass 2kg, rests on top of a larger block, mass 20 kg. The coefficient of friction between the blocks is 0.25. If the larger block is on a frictionless table, what is the largest horizontal force that can be applied to it without the small block slipping?

Force of tension Massless, unstretchable string; frictionless pulley

A Problem With First Year Physics Strings and Pulleys m1, m2 are given m2>m1 m2 String is massless and unstretchable Find accelerations of m1 and m2 (assume no friction)

V0 A block of mass m is given an initial velocity V0 up an inclined plane with angle of incline θ. Find acceleration of the block if a)  = 0 b) non-zero 

A wedge with mass M rests on a frictionless horizontal tabletop A wedge with mass M rests on a frictionless horizontal tabletop. A block with mass m is placed on the wedge and a horizontal force F is applied to the wedge. What must the magnitude of F be if the block is to remain at a constant height above the tabletop?

Block 1, of mass m1, is placed at rest on an inclined plane Block 1, of mass m1, is placed at rest on an inclined plane. It is attached by a massless, unstretchable string to block 2, of mass m2. The pulley is massless and frictionless and just changes the direction of the tension in the string. The coefficient of friction between the plane and m1 is the constant . 1 2 Determine what range of values for mass m2 will keep the system at rest. Find acceleration if mass 2 goes down.

Friction everywhere. 2 F 1 Find F necessary to drag the box 1 at constant speed.

The advantage of a pulley What minimum force F is needed to lift the piano of mass M?

Quiz a) A crate of mass m is on the flat bed of a pick up truck. The coefficient of friction between the crate and the truck is . The truck is traveling at the constant velocity of magnitude V1. Draw the free body diagram for the crate. b) The truck starts to accelerate with an acceleration ac. Draw the free body diagram for the crate, if the crate does not slip.

The Elevator Problem

Have a great day! Reading: Chapter 7 Hw: Chapter 6 problems and exercises