F = ma. F = mg. Forces. Forces. Free Body Diagrams. Find the unknown forces!! Ex. 1 Ex N. Newton s First Law. Newton s Second Law

Similar documents
v v ax v a x a v a v = = = Since F = ma, it follows that a = F/m. The mass of the arrow is unchanged, and ( )

Chapter 4. Forces and Newton s Laws of Motion. continued

Newton s Law of Motion

Steps to Solving Newtons Laws Problems.

University Physics 226N/231N Old Dominion University. Getting Loopy and Friction

Conceptual Questions: Forces and Newton s Laws

C B A T 3 T 2 T What is the magnitude of the force T 1? A) 37.5 N B) 75.0 N C) 113 N D) 157 N E) 192 N

5. Forces and Motion-I. Force is an interaction that causes the acceleration of a body. A vector quantity.

Physics 11 Assignment KEY Dynamics Chapters 4 & 5

Work Energy & Power. September 2000 Number Work If a force acts on a body and causes it to move, then the force is doing work.

Worksheet #1 Free Body or Force diagrams

Forces. When an object is pushed or pulled, we say that a force is exerted on it.

Objective: Equilibrium Applications of Newton s Laws of Motion I

PHY231 Section 2, Form A March 22, Which one of the following statements concerning kinetic energy is true?

Serway_ISM_V1 1 Chapter 4

Physics 111: Lecture 4: Chapter 4 - Forces and Newton s Laws of Motion. Physics is about forces and how the world around us reacts to these forces.

VELOCITY, ACCELERATION, FORCE

Force. Force as a Vector Real Forces versus Convenience The System Mass Newton s Second Law. Outline

Name: Partners: Period: Coaster Option: 1. In the space below, make a sketch of your roller coaster.

Physics: Principles and Applications, 6e Giancoli Chapter 4 Dynamics: Newton's Laws of Motion

while the force of kinetic friction is fk = µ

Chapter 6. Work and Energy

Physics 125 Practice Exam #3 Chapters 6-7 Professor Siegel

Resistance in the Mechanical System. Overview

Two-Body System: Two Hanging Masses

AP Physics Applying Forces

PHY231 Section 1, Form B March 22, 2012

AP1 Dynamics. Answer: (D) foot applies 200 newton force to nose; nose applies an equal force to the foot. Basic application of Newton s 3rd Law.

Chapter 6. Work and Energy

Forces. Definition Friction Falling Objects Projectiles Newton s Laws of Motion Momentum Universal Forces Fluid Pressure Hydraulics Buoyancy

What You ll Learn Why It s Important Rock Climbing Think About This physicspp.com 118

Lecture 6. Weight. Tension. Normal Force. Static Friction. Cutnell+Johnson: , second half of section 4.7

Acceleration due to Gravity

If you put the same book on a tilted surface the normal force will be less. The magnitude of the normal force will equal: N = W cos θ

Lecture 07: Work and Kinetic Energy. Physics 2210 Fall Semester 2014

Experiment: Static and Kinetic Friction

STATIC AND KINETIC FRICTION

STATICS. Introduction VECTOR MECHANICS FOR ENGINEERS: Eighth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.

Newton s Laws. Physics 1425 lecture 6. Michael Fowler, UVa.

Chapter 5 Using Newton s Laws: Friction, Circular Motion, Drag Forces. Copyright 2009 Pearson Education, Inc.

Physics. Lesson Plan #6 Forces David V. Fansler Beddingfield High School

Examples of Scalar and Vector Quantities 1. Candidates should be able to : QUANTITY VECTOR SCALAR

FRICTION, WORK, AND THE INCLINED PLANE

Ch 7 Kinetic Energy and Work. Question: 7 Problems: 3, 7, 11, 17, 23, 27, 35, 37, 41, 43

TEACHER ANSWER KEY November 12, Phys - Vectors

B Answer: neither of these. Mass A is accelerating, so the net force on A must be non-zero Likewise for mass B.

Chapter 11 Equilibrium

AP Physics - Chapter 8 Practice Test

Physical Science Chapter 2. Forces

Work, Energy and Power Practice Test 1

Physics 2A, Sec B00: Mechanics -- Winter 2011 Instructor: B. Grinstein Final Exam

Chapter 07 Test A. Name: Class: Date: Multiple Choice Identify the choice that best completes the statement or answers the question.

PHYSICS 111 HOMEWORK SOLUTION, week 4, chapter 5, sec 1-7. February 13, 2013

Chapter 6 Work and Energy

At the skate park on the ramp

Fundamental Mechanics: Supplementary Exercises

F f v 1 = c100(10 3 ) m h da 1h 3600 s b =

Physics 201 Homework 8

Solution Derivations for Capa #11

WORK DONE BY A CONSTANT FORCE

force (mass)(acceleration) or F ma The unbalanced force is called the net force, or resultant of all the forces acting on the system.

Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx Acceleration Velocity (v) Displacement x

Weight The weight of an object is defined as the gravitational force acting on the object. Unit: Newton (N)

LAB 6: GRAVITATIONAL AND PASSIVE FORCES

GRADE 11 SUBJECT Physical Sciences WEEK 1 TOPIC Resultant of perpendicular vectors Lesson 1

Physics 1A Lecture 10C

Slide Basic system Models

CHAPTER 6 WORK AND ENERGY

NEWTON S LAWS OF MOTION

LAB 6 - GRAVITATIONAL AND PASSIVE FORCES

Lecture 7 Force and Motion. Practice with Free-body Diagrams and Newton s Laws

Tennessee State University

PHYS 211 FINAL FALL 2004 Form A

BHS Freshman Physics Review. Chapter 2 Linear Motion Physics is the oldest science (astronomy) and the foundation for every other science.

Kinetic Friction. Experiment #13

AP1 Oscillations. 1. Which of the following statements about a spring-block oscillator in simple harmonic motion about its equilibrium point is false?

9. The kinetic energy of the moving object is (1) 5 J (3) 15 J (2) 10 J (4) 50 J

Problem Set #8 Solutions

Catapult Engineering Pilot Workshop. LA Tech STEP

Recitation Week 4 Chapter 5

Work, Energy and Power

4 Gravity: A Force of Attraction

EDUH SPORTS MECHANICS

Newton s Laws of Motion

1. Mass, Force and Gravity

COEFFICIENT OF KINETIC FRICTION

Physics Midterm Review Packet January 2010

F N A) 330 N 0.31 B) 310 N 0.33 C) 250 N 0.27 D) 290 N 0.30 E) 370 N 0.26

PHYSICS 111 HOMEWORK SOLUTION #10. April 8, 2013

PHY121 #8 Midterm I

Lecture 17. Last time we saw that the rotational analog of Newton s 2nd Law is

Universal Law of Gravitation

When showing forces on diagrams, it is important to show the directions in which they act as well as their magnitudes.

Physics 2048 Test 1 Solution (solutions to problems 2-5 are from student papers) Problem 1 (Short Answer: 20 points)

APPLIED MATHEMATICS ADVANCED LEVEL

Work, Energy, Conservation of Energy

Chapter 7 Homework solutions

Newton s Laws Force and Motion

AP Physics C. Oscillations/SHM Review Packet

Transcription:

Forces Free Body Diagrams Push or pull on an object Causes acceleration Measured in Newtons N = Kg m s Shows all forces as vectors acting on an object Vectors always point away from object Used to help find net force Contact Forces pplied Force Frictional Force Tensional Force Normal Force Spring Force Field Forces Gravitational Force Electrical Force Magnetic Force F f F N F g F pull Find the unknown forces!! Ex. Ex. 00 N F Newton s First Law Law of Inertia Resistance to change motion 75 N 50 N Objects in motion stay in motion Objects at rest stay at rest et =? et = 00N 75 N et = 5 N Upward et = 0 N Downward et = F 50 N = 0 N F = 40 N Equilibrium balanced forces, net force = 0 Net force sum of all forces 3 4 Newton s Second Law net force will cause acceleration friction force from a fluid (gases and liquids) force mass F = ma acceleration Terminal Velocity constant velocity of falling when F drag = F g Gravity force F = mg Mass and weight are not the same!!! 5 6

Newton s Third Law Each action has an opposite and equal reaction F on B = F B on Interaction Pair action / reaction forces Solving Tips. Draw the problem and choose coordinates. Determine known and unknown forces. 3. Create a free body diagram showing the net force. 4. Use Newton s laws to link acceleration and net force. 5. Solve equations for the unknowns 7 8 Combining Forces Normal Force +X F N = mg F N = mg + F hand F N = mg F string 9 0 Friction Factor lways against motion Two branches of friction (3 Types) Kinetic (Moving) Sliding Rolling Static (Stationary) Friction of fluids is called viscosity Kinetic Friction Friction Force F f = k = friction factor = Normal Force F f,static s

The force of static friction is not constant! Static friction is equal to pulling force until the object begins to move The maximum static friction is equal to s F f,static,max F applied stays still F f,static,max = F applied constant speed, a=0 F f,s F f F f,s,max F f = s, F f,k F f = k, Kinetic Friction F f,static,max F applied accelerates F pplied 3 4 Thrust from Friction and Motion What is the maximum acceleration a car can achieve if the tires/road friction coefficient is equal to 0.7? (ignore drag) et,x = F thrust F drag = ma F Drag The maximum thrust cannot exceed road friction F thrust = F f,s,max = s = s mg F g F thrust From et,x ma = s mg 5 a = s mg = (0.7)(9.8m/s ) = 6.9m/s 6 The most important rule: This means that: Static Equilibrium F = 0 F x = 0 and F y = 0 Static Equilibrium LWYS FOLLOW THESE STEPS:. Draw a labeled free body diagram. Break angled forces into components 3. Write net equations ( et,x = ) Only use the components of angled forces!! et,x = 0 and et,y = 0 4. Solve for unknowns one at a time 7 8 3

Vector Direction ( Common Ways) Labeled degrees north or south of x axis Degrees from east direction (0 ). 80 N of East Or 80 80 45 S of East Or 35 45 30 N of West 30 Or 50 Working with Forces at an ngle When a force is at an angle: break into x and y components Do not use the original force again!! dd x and y components separately Find the new resultant force and its angle F = F x +F y = Tan O Using the angle from the x axis: X Component y Component F x = F cos F y = F sin 9 0 Right Triangle Help You will typically want to work with the angle from the x axis. = Tan O = angle = H Cos θ djacent 90 O = H Sin θ 90 Opposi ite SOH Sin θ = O CH TO Cos θ = H Tan θ = H = Sin O = Cos = Tan H H O Opposite djacent Hypotenuse O = H Sin θ = H Cos θ H = O Sin θ O = Tan θ = O H = Tan θ Cos θ O = H = H O H = +O O Forces at an ngle Breaking into components Forces on a Ramp Breaking into components m Find F P Components F Px = F P Cos F Py = F P Sin Use components for net equations etx = F Px ety = F N + F Py F g F Py F N F P F Px F g = mg F N should not equal F g!! F N = F g F py if a y = 0 3 Find F g Components F gx = F g Cos (90 ) F gy = F g Sin (90 ) Or just use SOH CH TO F gx = F g Sin F gy = F g Cos Use components for net equations etx = F gx ety = F N F gy F g = mg F N should not equal F g!! Many cases, F N will equal F gy 4 4

Free Body Diagrams Tension Force Spring Force