Lecture 9 Serway and Jewett : 5.7, 5.8

Slides:



Advertisements
Similar presentations
Physics Subject Area Test
Advertisements

Newton’s Laws of Motion and Free Body Analysis
Chapter 7. Newton’s Third Law
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
Section 4-7 Solving Problems with Newton’s Laws; Free Body Diagrams
 Dynamics – Atwood Machines / SBA urses/honors/dynamics/Atwood.html.
Motion and Force Dynamics
Applications of Newton’s Laws (Examples)
Newton’s Laws (II) Free-body diagrams Normal Force
Newton’s Second Law The net force on a body is equal to the product of the body’s mass and its acceleration.
Follow the same procedure as other force problems, but keep in mind: 1) Draw a free body diagram for EACH object or for each junction in a rope.
When a car accelerates forward on a level roadway, which force is responsible for this acceleration? State clearly which.
Newton’s Laws of Motion (Applications)
AP Physics Chapter 5 Force and Motion – I.
Problem Block A of mass 12 kg and block B of mass 6 kg are connected by a cable that passes over pulley C which can rotate freely. Knowing that the.
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.
04-1 Physics I Class 04 Newton’s Second Law for More Complex Cases.
Physics 101: Lecture 9, Pg 1 Physics 101: Application of Newton's Laws l Review of the different types of forces discussed in Chapter 4: Gravitational,
Physics 101: Lecture 9, Pg 1 Physics 101: Application of Newton's Laws l Review of the different types of forces discussed in Chapter 4: Gravitational,
Physics Instructor: Dr. Tatiana Erukhimova Lecture 6.
Kinds of Forces Lecturer: Professor Stephen T. Thornton
Newton’s Laws of Motion Problems MC Questions
Newton’s 3 rd Law Action-reaction pairs Inclined coordinate system Massless ropes and massless, frictionless pulleys Coupled objects Lecture 6: Newton’s.
Chapter 7. Newton’s Third Law
Newton’s Laws - continued
Chapter 8: 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.
Physics 1D03 - Lecture 25 TEST – Thursday at 7pm The test will cover things we have done in class up to Lecture 9 (Chapter 1,2,4, , 5.6,
Applications & Examples of Newton’s 2nd Law
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 
Problems Chapter 4,5.
Physics 1D03 - Lecture 81 Newton’s Laws (IV) Blocks, ramps, pulleys and other problems.
Newton’s Laws (cont…) Blocks, ramps, pulleys and other problems
Solving Problems with Newton’s Laws
Newton’s Laws - continued Friction, Inclined Planes, N.T.L., Law of Gravitation.
SECOND LAW OF MOTION If there is a net force acting on an object, the object will have an acceleration and the object’s velocity will change. Newton's.
Newton’s Laws - continued Friction, Inclined Planes, N3L, Law of Gravitation.
PHYS16 – Lecture 10 & 11 Force and Newton’s Laws September 29 and October 1, 2010
Aim: How can we solve problems dealing with Atwood Machines using Newton’s Laws? HW #6 Do Now: An object is of mass M is hanging from a rope as shown.
Force Systems accelerate together Combination Systems – connected masses Horizontal Pulley Atwood’s Machine.
Physics 1D03 - Lecture 81 Clicker Registration Remember to register your clicker at:
1 Some application & Forces of Friction. 2 Example: When two objects of unequal mass are hung vertically over a frictionless pulley of negligible mass,
Physics 1D03 - Lecture 71 Newton’s Laws (II) Free-body diagrams Normal Force Friction.
Frictional Forces  Two types: - static – applies to stationary objects - kinetic – applies to sliding (moving) objects  Like F N, the Frictional Force.
Tension.
Newton 2nd Law problems - Atwood Machines -Incline Planes -Tension Problems -Other Object Connected problems.
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.
Aim: More Atwood Machines Answer Key HW 6 Do Now: Draw a free-body diagram for the following frictionless inclined plane: m2m2 m1m1 M θ Mg m2m2 m1m1 M.
Newton's Laws of Motion Slide 4-19 Newton 0th Law Objects are dumb - They have no memory of the past and cannot predict the future. Objects only know what.
More Fun with Newton’s Laws Friction, Inclined Planes, N.T.L.
AP Physics 1 – DYNAMICS OF FORCE AND MOTION NEWTON’S THIRD LAW & MORE FRICTION! (IT’S BACK!)
Physics 1D03 - Lecture 81 Newton’s Laws (III) Blocks on ramps, and other problems Serway and Jewett : 5.7, 5.8.
Multiple Object Systems 1. Analyze the system as one object. 2. Analyze each object individually. 3. Create multiple equations to solve for multiple unknowns.
Isaac Newton: 1600’s, England Force: A push or pull between pairs of objects Mass is a measure of resistance to acceleration.
1 Newton’s Third Law Readings: Chapter 8. 2 Newton’s Third Law When you have more than 1 system the Newton’s Third Law can provide an additional information.
Newton’s Third Law If two objects interact, the force exerted by object 1 on object 2 is equal in magnitude and opposite in direction to the force.
Inclined Plane Problems. Axes for Inclined Planes X axis is parallel to the inclined plane Y axis is perpendicular to the inclined plane Friction force.
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.
FRICTION and Newton’s second law. The “Normal” Force, N When an object is pressed against a surface, the surface pushes back. (That’s Newton’s 3 rd Law)
Homework (due Monday) Section 4.5, 4.6 (Examples!!!!) Problems (p.111) #20, 32, 35, 36, 40, 45 A block of mass m is projected with an initial speed v 0.
Unit is the NEWTON(N) Is by definition a push or a pull Can exist during physical contact(Tension, Friction, Applied Force) Can exist with NO physical.
Solving problems when  F = ma
 A system can consist of one or more objects that affect each other.  Often, these objects are connected or in contact.
Tension Problems.
Atwood Machines and Multiple Body Systems
Solving Problems with Newton’s Laws
Newton’s Laws: Practice Problems
Motion in 2D and Pulleys Constant acceleration in 2-D Free fall in 2-D
Newton’s Laws: Practice Problems
Presentation transcript:

Lecture 9 Serway and Jewett : 5.7, 5.8 Newton’s Laws applied to systems with two or more accelerated bodies. Serway and Jewett : 5.7, 5.8 Physics 1D03 - Lecture 9

Problems with several accelerated objects: Free-body diagram for each object. Relate forces by finding action-reaction pairs, etc. Look for constraints on the motion to relate accelerations. “F=ma” for each diagram, break into components. Count unknowns: do you have enough equations? Use algebra to solve. Physics 1D03 - Lecture 9

Two blocks connected by a rope are being pulled by a horizontal force FA. Given that F=60 N, m1=12kg and m2=18kg, and that μk=0.1, find the tension in the rope between them and the acceleration of the system. T m2 FA m1 Physics 1D03 - Lecture 9

Atwood’s Machine Assume : - no friction Calculate the acceleration of the blocks. Assume : - no friction - massless rope and pulley - rope doesn’t stretch Plan: • free-body diagram for each mass • relate tensions, accelerations • use Newton’s second Law m1 m2 Physics 1D03 - Lecture 9

Constraints on the motion: Why are the accelerations equal (in magnitude)? Because the cord doesn’t stretch! Any downward motion of m1 requires an equal upward motion of m2. This is a constraint on the motion, which comes from the geometry of the apparatus. Label directions of a consistently on both diagrams: if m1 accelerates up, m2 accelerates down. Physics 1D03 - Lecture 9

T1 T2 a2 a1 m2g m1g Forces on m1 Forces on m2 Tensions are equal (“ideal” pulley, light rope) Accelerations are equal in magnitude (why?), opposite in direction Physics 1D03 - Lecture 9

is proportional to g, but can be small (and easy to measure) m2g a m1g . Eliminate T to get  is proportional to g, but can be small (and easy to measure) Physics 1D03 - Lecture 9

m2 m1 a1 Concept Quiz Consider the more elaborate Atwood’s machine shown. Assuming the rope and pulleys are ideal, the relation between the accelerations will be: a2 Physics 1D03 - Lecture 9

A block of mass m1 on a rough horizontal surface is pulled with a force FA at an angle θ to the horizontal. A ball of mass m2 is connected to the other side, hanging over a lightweight frictionless pulley. The coefficient of friction is given by μk. Determine the acceleration of the system. FA θ m1 m2 Physics 1D03 - Lecture 9

Eg: Given no friction, determine the acceleration of the system and the tension in the strings. Physics 1D03 - Lecture 9

m FP M Example: How do you calculate the acceleration of each block: if the upper block doesn’t slide? if the upper block does slide? m = 1.0 kg M = 2.0 kg ms = 0.6 mk = 0.4 FP = 15 N m FP M Physics 1D03 - Lecture 9

Suggested Problems Chapter 5: Problems 17, 25, 29, 43, 44, 62, Questions 19, 21 Physics 1D03 - Lecture 9