Chapter 5 – Force and Motion I

Slides:



Advertisements
Similar presentations
Chapter 5 – Force and Motion I
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.
Physics 111: Mechanics Lecture 5
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.
Dr. Steve Peterson Physics 1025F Mechanics NEWTON’S LAWS Dr. Steve Peterson
Applications of Newton’s Laws
Newton’s Second Law The net force on a body is equal to the product of the body’s mass and its acceleration.
Force and Motion Force Newton’s First Law Newton’s Second Law Newton’s Third Law Gravitational Force Weight Normal Force pps by C Gliniewicz.
AP Physics Chapter 5 Force and Motion – I.
PHYS 218 sec Review Chap. 4 Newton’s laws of motion.
Chapter 5 Force and Motion (I) Kinematics vs Dynamics.
CHAPTER-5 Force and Motion-1.
Chapter 5 Force and Motion
I.Newton’s first law. II.Newton’s second law. III.Particular forces: - Gravitational - Gravitational - Weight - Weight - Normal - Normal - Tension - Tension.
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.
Chapter 5 Force and Motion In Chapters 2 and 4 we have studied “kinematics,” i.e., we described the motion of objects using parameters such as the position.
Force and Motion–I Chapter 5 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
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.
2009 Physics 2111 Fundamentals of Physics Chapter 5 1 Fundamentals of Physics Chapter 4 Force & Motion 1.What Causes an Acceleration? 2.Newton’s First.
Force and Laws of Motion
University Physics: Mechanics
Chapter 4 The Laws of Motion. Classes of Forces Contact forces involve physical contact between two objects Field forces act through empty space No physical.
Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4.
Physics 111: Mechanics Lecture 4
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.
Physics 111 Practice Problem Statements 04 Force and Motion I: The Laws of Motion SJ 8th Ed.: Ch. 5.1 – 5.7 Contents: 5-2E, 5-7P, 5-9E, 5-29P*, 5-31P*,
Chapters 5, 6 Force and Motion. Newtonian mechanics Describes motion and interaction of objects Applicable for speeds much slower than the speed of light.
The tendency of objects to resist change in their state of motion is called inertia  Inertia is measured quantitatively by the object's mass.  Objects.
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.
I.Newton’s first law. II.Newton’s second law. III.Particular forces: - Gravitational - Gravitational - Weight - Weight - Normal - Normal - Friction - Friction.
Chapter 4 Dynamics: Aim: How can we describe Newton’s Laws of Motion? © 2014 Pearson Education, Inc.
University Physics: Mechanics
Forces and Motion Chapter 5 and 6. Focus  Force: a push or a pull  Acts on objects to change its velocity.
An 7.3-kg object rests on the floor of an elevator which is accelerating downward at a rate of 1.0 m/s 2. What is the magnitude of the force the object.
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.
1 Chapter 5 The Laws of Motion. 2 Force Forces are what cause any change in the velocity of an object A force is that which causes an acceleration The.
Solving problems when  F = ma
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.
Forces. Log into my website, click the Introduction to Forces Notes On a note card, define the following terms: Force Newton Unbalanced force Contact.
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.
Chapter 5 Force and Motion I. Classical Mechanics Describes the relationship between the motion of objects in our everyday world and the forces acting.
Dynamics: Newton’s Laws of Motion
Physics 1: Mechanics Đào Ngọc Hạnh Tâm
FORCE AND MOTION I Change in velocity acceleration
Physics 218 Lecture 6: Dynamics Alexei Safonov.
University Physics: Mechanics
University Physics: Mechanics
University Physics: Mechanics
Chapter 5 Force and Motion Friday, May 25, 2018 Chap 5.
M Friction.
University Physics: Mechanics
Force and Motion February 6, 2006.
Phys 270 Newton’s Laws.
Chapter 5 Force and Motion
Fundamentals of Physics School of Physical Science and Technology
Chapter 5 Force and Motion.
Chapter 5 Force and Motion
GPS: SP1. Students will analyze the relationship between force, mass, gravity, and the motion of objects.
Chapter 5 The Laws of Motion.
Chapter 5 – Force and Motion I
Lecture 4 Dynamics: Newtons Laws of Motion
Chapter 5 – Force and Motion I
Example Problems for Newton’s Second Law Answers
Force Problems.
Step 1: Get Organized Draw a picture.
Aim: How do we explain Newton’s first two laws of motion?
University Physics: Mechanics
Presentation transcript:

Chapter 5 – Force and Motion I Newton’s first law. Newton’s second law. Particular forces: - Gravitational - Weight - Normal - Tension IV. Newton’s third law.

- Inertial reference frame: where Newton’s laws hold. Newton mechanics laws cannot be applied when: 1) The speed of the interacting bodies are a fraction of the speed of light Einstein’s special theory of relativity. 2) The interacting bodies are on the scale of the atomic structure  Quantum mechanics I. Newton’s first law: If no net force acts on a body, then the body’s velocity cannot change; the body cannot accelerate  Principle of superposition: when two or more forces act on a body, the net force can be obtained by adding the individual forces vectorially. - Inertial reference frame: where Newton’s laws hold.

the body’s mass and its acceleration. II. Newton’s second law: The net force on a body is equal to the product of the body’s mass and its acceleration. The acceleration component along a given axis is caused only by the sum of the force components along the same axis, and not by force components along any other axis. - System: collection of bodies. - External force: any force on the bodies inside the system. III. Particular forces: Gravitational: pull directed towards a second body, normally the Earth 

- Weight: magnitude of the upward force needed to balance the gravitational force on the body due to an astronomical body  Normal force: perpendicular force on a body from a surface against which the body presses. - Frictional force: force on a body when the body attempts to slide along a surface. It is parallel to the surface and opposite to the motion. -Tension: pull on a body directed away from the body along a massless cord.

from each other are always equal in magnitude and IV. Newton’s third law: When two bodies interact, the forces on the bodies from each other are always equal in magnitude and opposite in direction. QUESTIONS Q. Two horizontal forces F1, F2 pull a banana split across a frictionless counter. Without using a calculator, determine which of the vectors in the free body diagram below best represent: a) F1, b)F2. What is the net force component along (c) the x-axis, (d) the y-axis? Into which quadrant do (e) the net-force vector and (f) the split’s acceleration vector point? Same quadrant, 4 F1 F2

(b) Decreasing speed: vf < v0 a<0  T> Fg Q. A body suspended by a rope has a weigh of 75N. Is T equal to, greater than, or less than 75N when the body is moving downward at (a) increasing speed and (b) decreasing speed? (a) Increasing speed: vf >v0 a>0  T< Fg Movement (b) Decreasing speed: vf < v0 a<0  T> Fg Q. The figure below shows a train of four blocks being pulled across a frictionless floor by force F. What total mass is accelerated to the right by (a) F, (b) cord 3 (c) cord 1? (d) Rank the blocks according to their accelerations, greatest first. (e) Rank the cords according to their tension, greatest first. Fg T1 T2 T3 (a) F pulls mtotal= (10+3+5+2)kg = 20kg (c) Cord 1  T1  m= 10kg (b) Cord 3  T3  m=(10+3+5)kg = 18kg (d) F=ma  All tie, same acceleration

(c) Ftoy from dog house: 1 (e) F-T3= 2a T3-T2= 5a T2-T1=3a T1=10a F-T3= 2a  F=18a+2a=20a T3-13a= 5a  T3=18a T2-10a=3a  T2=13a T1=10a Q. A toy box is on top of a heavier dog house, which sits on a wood floor. These objects are represented by dots at the corresponding heights, and six vertical vectors (not to scale) are shown. Which of the vectors best represents (a) the gravitational force on the dog house, (b) on the toy box, (c) the force on the toy box from the dog house, (d) the force on the dog house from the toy box, (e) force on the dog house from the floor, (f) the force on the floor from the dog house? (g) Which of the forces are equal in magnitude? Which are (h) greatest and (i) least in magnitude? (a) Fg on dog house: 4 or 5 (h) Greatest: 6,3 (b) Fg on toy box: 2 (i) Smallest: 1,2,5 (c) Ftoy from dog house: 1 (d) Fdog-house from toy box: 4 or 5 (e) Fdog-house from floor: 3 (f) Ffloor from dog house: 6 (g) Equal: 1=2, 1=5, 3=6

There are two forces on the 2 kg box in the overhead view of the figure below but only one is shown. The figure also shows the acceleration of the box. Find the second force (a) in unit-vector notation and as (b) magnitude and (c) direction. F2

There are two forces on the 2 kg box in the overhead view of the figure below but only one is shown. The figure also shows the acceleration of the box. Find the second force (a) in unit-vector notation and as (b) magnitude and (c) direction. F2

Rules to solve Dynamic problems Select a reference system. Make a drawing of the particle system. Isolate the particles within the system. Draw the forces that act on each of the isolated bodies. Find the components of the forces present. Apply Newton’s second law (F=ma) to each isolated particle.

**. (a) A 11kg salami is supported by a cord that runs to a spring scale, which is supported by another cord from the ceiling. What is the reading on the scale, which is marked in weigh units? (b) Here the salami is supported by a cord that runs around a pulley and to a scale. The opposite end of the scale is attached by a cord to a wall. What is the reading on the scale? (c) The wall has been replaced by a second salami on the left, and the assembly is stationary. What is the reading on the scale now? T T T T T T T Fg Fg

T T T Fg T Fg In all three cases the scale is not accelerating, which means that the two cords exert forces of equal magnitude on it. The scale reads the magnitude of either of these forces. In each case the tension force of the cord attached to the salami must be the same in magnitude as the weight of the salami because the salami is not accelerating.

magnitude of the Normal force? 1B. (a) What should be the magnitude of F in the figure below if the body of mass m=10kg is to slide up along a frictionless incline plane with constant acceleration a=1.98 m/s2? (b) What is the magnitude of the Normal force? y F N Fg 20º x 30º

In the figure below, mblock=8. 5kg and θ=30º. Find (a) Tension in *** In the figure below, mblock=8.5kg and θ=30º. Find (a) Tension in the cord. (b) Normal force acting on the block. (c) If the cord is cut, find the magnitude of the block’s acceleration. y x N T Fg