For every action force there is an equal and opposite reaction force!!

Slides:



Advertisements
Similar presentations
Copyright © 2012 Pearson Education Inc. Application of Newton’s laws: free body diagram Physics 7C lecture 03 Thursday October 3, 8:00 AM – 9:20 AM Engineering.
Advertisements

 The force that act on the object are balanced in all direction.  The force cancel each other, so that the resultant force or net force is zero.  Newton’s.
Chapter 4 The Laws of Motion.
Table of Contents Chapter 4
Section 4-7 Solving Problems with Newton’s Laws; Free Body Diagrams
Newton’s Second Law The net force on a body is equal to the product of the body’s mass and its acceleration.
Make a sketch Problem: A 10.0 kg box is pulled along a horizontal surface by a rope that makes a 30.0 o angle with the horizontal. The tension in the rope.
Translational Equilibrium Physics Montwood High School R. Casao.
Forces applied at an Angle & Inclined Planes
Forces and the Laws of MotionSection 4 Click below to watch the Visual Concept. Visual Concept Everyday Forces.
Newton’s Laws.
Chapter 4: Forces Newton’s Third Law You cannot touch
Kinds of Forces Lecturer: Professor Stephen T. Thornton
Physics 151: Lecture 8, Pg 1 Physics 151: Lecture 8 l Reaminder: çHomework #3 : (Problems from Chapter 5) due Fri. (Sept. 22) by 5.00 PM l Today’s Topics.
Forces and The Laws of Motion
Chapter 7. NEWTON’S SECOND LAW
Chapter 4B. Friction and Equilibrium
Chapter 7. Newton’s Third Law
Examples from Chapter 4.
Chapter 4 Preview Objectives Force Force Diagrams
Chapter 4 Section 1 Changes in Motion Force.
Chapter 4 Preview Objectives Force Force Diagrams
Forces Contact Forces - those resulting from physical contact between objects –Normal Force –Friction –Tension (spring/rope) –Compression Action at a Distance.
Aim: More Law of Inertia
1 4 Topics force and net force inertia and 1 st law acceleration and 2 nd law g notation force pairs and 3 rd law force diagrams equilibrium friction.
© Houghton Mifflin Harcourt Publishing Company The student is expected to: Chapter 4 Section 1 Changes in Motion TEKS 4E develop and interpret free-body.
1 4 Newton’s Laws Force, net-force, mass & inertia Newton’s Laws of Motion Weight, Contact Forces Labeling & Diagramming Hk: 37, 49, 53, 57, 59, 61, 65,
What is the normal force for a 500 kg object resting on a horizontal surface if a massless rope with a tension of 150 N is acting at a 45 o angle to the.
Newton’s Laws - continued Friction, Inclined Planes, N.T.L., Law of Gravitation.
Chapter 4 The Laws of Motion. Classical Mechanics Describes the relationship between the motion of objects in our everyday world and the forces acting.
Force and Motion–I Chapter 5 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
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.
Lecture Newton’s first Law If there are no external forces, the object does not change its velocity and direction. LAW of INERTIA!!!
Newton’s Third Law Newton’s 3 rd Law 3 rd Law examples Example 4-12 – Two blocks on table Example 4-13 – Atwood’s Machine Block on Inclined Plane Canal.
Newton’s Laws of Motion We have studied “kinematics”, or the description of motion. Now, we look at “dynamics”, the causes of motion.
Forces and Newton’s Laws of Motion. 4.1 The Concepts of Force and Mass A force is a push or a pull. Arrows are used to represent forces. The length of.
Newton’s Laws of Motion What are forces? How can diagrams be used to depict and analyze the forces acting on an object? What are the effects of net force.
Chapter 4 Dynamics: Newton’s Laws of Motion
Chapter 4 Dynamics: Newton’s Laws of Motion. Units of Chapter 4 Force Newton’s First Law of Motion Mass Newton’s Second Law of Motion Newton’s Third Law.
Chapter 4A. Translational Equilibrium
Chapter 5B Rotational Equilibrium
Force & Newton’s Laws of Motion. FORCE Act of pulling or pushing Act of pulling or pushing Vector quantity that causes an acceleration when unbalanced.
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.
Objectives: After completing this module, you should be able to: Write Newton’s second law using appropriate units for mass, force, and acceleration.Write.
Dynamics: Newton’s Laws of Motion
Lecture 9 Serway and Jewett : 5.7, 5.8
Chapter 7. NEWTON’S SECOND LAW A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.
© Houghton Mifflin Harcourt Publishing Company Preview Objectives Force Force Diagrams Chapter 4 Section 1 Changes in Motion.
Dynamics: Newton’s Laws of Motion. Force A force is a push or pull. An object at rest needs a force to get it moving; a moving object needs a force to.
CP Physics Chapter 4 Newton’s Laws Force Force (F) is a push or a pull Measured in Newtons (N) for SI, pounds (lb) in US. (4.45 N = 1 lb) It has magnitude.
Chapter 4 Dynamics: Aim: How can we describe Newton’s Laws of Motion? © 2014 Pearson Education, Inc.
Chapter 4 Dynamics: Newton’s Laws of Motion. Units of Chapter 4 Force Newton’s First Law of Motion Mass Newton’s Second Law of Motion Newton’s Third Law.
Ch. 3 & 4 Motion & Forces VI. Action and Reaction  Newton’s Third Law  Momentum  Conservation of Momentum.
4-8 Applications Involving Friction, Inclines
Force, Friction and Equilibrium Equilibrium: Until motion begins, all forces on the mower are balanced. Friction in wheel bearings and on the ground.
Force and Motion–I Chapter 5. Newton's First and Second Laws A force: o Is a “push or pull” acting on an object o Causes acceleration We will focus on.
I. Newton’s Laws II. Forces III. Free-Body Diagrams Chapter 4: Newton’s Laws and Forces.
NEWTON'S LAWS OF MOTION Philosophiae Naturalis Principia Mathematica (1686)
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.
Chapter 5 Force and Motion I. Classical Mechanics Describes the relationship between the motion of objects in our everyday world and the forces acting.
Basic Info: balanced Forces Objects are balanced only if their net force is zero in both the vertical and horizontal directions Objects are balanced only.
Newton’s third law of motion 1 Force 2
Force is part of an interaction
Chapter 4 Preview Objectives Force Force Diagrams
Newton’s Third Law of Motion
Newton's 3rd Law!! For every action force there is an equal and opposite reaction force!! For every action force there is an equal and opposite reaction.
Chapter 7. NEWTON’S SECOND LAW
The space shuttle Endeavor lifts off for an 11-day mission in space
Newton’s Laws of Motion
Newton’s Laws - continued
Presentation transcript:

For every action force there is an equal and opposite reaction force!!

These Two forces are known as an action/reaction pair.These Two forces are known as an action/reaction pair. Gravity acts on an object and the object acts with equal force.Gravity acts on an object and the object acts with equal force.

Newton’s Third Law Action-Reaction Pairs Action-Reaction Pairs The hammer exerts a force on the nail to the right. The hammer exerts a force on the nail to the right. The nail exerts an equal but opposite force on the hammer to the left. The nail exerts an equal but opposite force on the hammer to the left.

Acting and Reacting Forces Use the words by and on to study action/reaction forces below as they relate to the hand and the bar:Use the words by and on to study action/reaction forces below as they relate to the hand and the bar: The action force is exerted by the _____ on the _____. The reaction force is exerted by the _____ on the _____. bar hands bar hands Action Reaction

A 60-kg athlete exerts a force on a 10-kg skateboard. If she receives an acceleration of 4 m/s 2, what is the acceleration of the skateboard? Force on runner = -(Force on board) m r a r = -m b a b (60 kg)(4 m/s 2 ) = -(10 kg) a b a = - 24 m/s 2 Force on Runner Force on Board

Applying Newton’s Law Read, draw, and label problem.Read, draw, and label problem. Draw free-body diagram for each body.Draw free-body diagram for each body. Choose x or y-axis along motion and choose direction of motion as positive.Choose x or y-axis along motion and choose direction of motion as positive. Write Newton’s law for both axes:Write Newton’s law for both axes:  F x = m x  F y = m y  F x = m a x  F y = m a y Solve for unknown quantities.Solve for unknown quantities. Read, draw, and label problem.Read, draw, and label problem. Draw free-body diagram for each body.Draw free-body diagram for each body. Choose x or y-axis along motion and choose direction of motion as positive.Choose x or y-axis along motion and choose direction of motion as positive. Write Newton’s law for both axes:Write Newton’s law for both axes:  F x = m x  F y = m y  F x = m a x  F y = m a y Solve for unknown quantities.Solve for unknown quantities.

What is the tension T in the rope below if the block accelerates upward at 4 m/s 2 ? (Draw sketch and free-body.) 10 kg a = +4 m/s 2 Ta Tmg +  F x = m a x = 0 (No Motion)  F y = m a y = m a T - mg = m a mg = (10 kg)(9.8 m/s) = 98 N m a = (10 kg)(4 m/s) = 40 N - 98 N = 40 N T - 98 N = 40 N T = 138 N

Two-Body Problem: Find tension in the connecting rope if there is no friction on the surfaces. 2 kg 4 kg 12 N Find acceleration of system and tension in connecting cord. First apply F = m a to entire system (both masses). 12 N n (m 2 + m 4 )g  F x = (m 2 + m 4 ) a 12 N = (6 kg) a a =a =a =a = 12 N 6 kg a = 2 m/s 2

The two-body problem. 2 kg4 kg 12 N Now find tension T in connecting cord. Apply F = m a to the 2 kg mass where a = 2 m/s 2. T n m2 gm2 gm2 gm2 g  F x = m 2 a T = (2 kg)(2 m/s 2 ) T = 4 N

The two-body problem. 2 kg 4 kg 12 N Same answer for T results from focusing on 4-kg by itself. Apply F = m a to the 4 kg mass where a = 2 m/s 2.  F x = m 4 a 12 N - T = (4 kg)(2 m/s 2 ) T = 4 N 12 N n m2 gm2 gm2 gm2 g T

Find acceleration of system and tension in cord for the arrangement shown. First apply F = m a to entire system along the line of motion.  F x = (m 2 + m 4 ) a a = 6.53 m/s 2 n m2 gm2 gm2 gm2 g T m4 gm4 gm4 gm4 g T + a Note m 2 g is balanced by n. m 4 g = (m 2 + m 4 ) a (4 kg)(9.8 m/s 2 ) 2 kg + 4 kg a = = m 4 g m 2 + m 4 2 kg 4 kg

Now find the tension T given that the acceleration is a = 6.53 m/s 2. To find T, apply F = m a to just the 2 kg mass, ignoring 4 kg. T = (2 kg)(6.53 m/s 2 ) T = 13.1 N Same answer if using 4 kg. m 4 g - T = m 4 a T = m 4 (g - a ) = 13.1 N n m2 gm2 gm2 gm2 g T m4 gm4 gm4 gm4 g T + a 2 kg 4 kg

Vector Components So we have a person pulling a sled 30 o with respect to the horizontal at a force of 50 N.So we have a person pulling a sled 30 o with respect to the horizontal at a force of 50 N. We need to think of it like the sled being pulled vertically and horizontally at the same time, giving it both components.We need to think of it like the sled being pulled vertically and horizontally at the same time, giving it both components. Θ=30 o F=50N FyFy FxFx

Vector Components To solve for F x, we will use cosine because it is the adjacent side and we have the hypotenuse.To solve for F x, we will use cosine because it is the adjacent side and we have the hypotenuse. To solve for F y, use the same process but with sine.To solve for F y, use the same process but with sine. Θ=30 o F=50m/s FyFy FxFx

Angled Free-body Diagram kgA A B B W = mg BxBx ByBy AxAx AyAy 1. Draw and label sketch. 2. Draw and label vector force diagram. 3. Dot in rectangles and label x and y compo- nents opposite and adjacent to angles.

In the absence of friction, what is the acceleration down the 30 0 incline? 30 0 mg n n W mg sin 30 0 mg cos  F x = m a x mg sin 30 0 = m a a = g sin 30 0 a = (9.8 m/s 2 ) sin 30 0 a = 4.9 m/s 2

Summary Newton’s Second Law: A resultant force produces an acceleration in the direction of the force that is directly proportional to the force and inversely proportional to the mass.