LECTURE 12: Free body diagrams

Similar documents
LECTURE 30: Conservation of energy

LECTURE 16: Friction

LECTURE 19: Universal Law of Gravitation

LECTURE 26: Work- Kinetic Energy

LECTURE 28: Spring force and potential energy

LECTURE 18: Uniform Circular Motion (UCM)

SPH4U UNIVERSITY PHYSICS

LECTURE 27: Gravitational potential energy

Answers without work shown will not be given any credit.

LECTURE 20: Rotational kinematics

LECTURE 10: Newton's laws of motion

LECTURE 04: Position, Velocity, and Acceleration Graphs

LECTURE 23: Momentum-Impulse

(a) On the dots below that represent the students, draw and label free-body diagrams showing the forces on Student A and on Student B.

PHYSICS 220 Lecture 04 Forces and Motion in 1 D Textbook Sections

Physics 207 Lecture 9. Lecture 9

Physics 207 Lecture 9. Lecture 9

Lecture PowerPoints. Chapter 7 Physics for Scientists and Engineers, with Modern Physics, 4 th Edition Giancoli

Lecture 10. Example: Friction and Motion

Physics 201 Lecture 16

PHY 123 Lab 1 - Error and Uncertainty and the Simple Pendulum

Chapter 3, Problem 28. Agenda. Forces. Contact and Field Forces. Fundamental Forces. External and Internal Forces 2/6/14

3/10/2019. What Is a Force? What Is a Force? Tactics: Drawing Force Vectors

Physics Mechanics. Lecture 11 Newton s Laws - part 2

SDI LAB #7: NEWTON S LAWS REVISITED

AP PHYSICS 1 UNIT 4 / FINAL 1 PRACTICE TEST

What Is a Force? Slide Pearson Education, Inc.

Physics 207 Lecture 7. Lecture 7

4.4 Energy in multiple dimensions, dot product

Lecture PowerPoints. Chapter 5 Physics for Scientists & Engineers, with Modern Physics, 4 th edition. Giancoli

NII.3: Dynamics & Statics

Which, if any, of the velocity versus time graphs below represent the movement of the sliding box?

Pulling force $ % 6 Least

Free-Body Diagrams: Introduction

Acceleration and Force: I

PHYSICS. Chapter 5 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

Spring 2010 Physics 141 Practice Exam II Phy141_mt1b.pdf

PHYSICS. Chapter 8 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

Sara Rwentambo. PHYS 1007 AB

PHYSICS. Chapter 7 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

AP Physics Free Response Practice Oscillations

Newton s First Law. Newton s Second Law 9/29/11

Kinematics + Dynamics

CHAPTER 2. FORCE and Motion. CHAPTER s Objectives

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

Ch.8: Forces as Interactions

Newton s First Law and IRFs

Lecture 5. Dynamics. Forces: Newton s First and Second

Chapter 7 Work and Energy

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.01 Physics Fall Term = # v x. t " =0. are the values at t = 0.

Chapter 6: Work and Kinetic Energy

Ballistic Pendulum. Caution

PHYSICS. Chapter 5 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

(A) 0 (B) mv (C) 2mv (D) 2mv sin θ (E) 2mv cos θ

Kinematics Lab. 1 Introduction. 2 Equipment. 3 Procedures

Physics 1A, Week 2 Quiz Solutions

# x = v f + v & % ( t x = v

What is a Force? Free-Body diagrams. Contact vs. At-a-Distance 11/28/2016. Forces and Newton s Laws of Motion

= 1 2 kx2 dw =! F! d! r = Fdr cosθ. T.E. initial. = T.E. Final. = P.E. final. + K.E. initial. + P.E. initial. K.E. initial =

General strategy for using Newton's second law to solve problems:

Chapter 5: Applications of Newton's laws Tuesday, September 17, :00 PM. General strategy for using Newton's second law to solve problems:

Potential Energy & Conservation of Energy

physics Chapter 8 Lecture a strategic approach randall d. knight FOR SCIENTISTS AND ENGINEERS CHAPTER8_LECTURE8.1 THIRD EDITION

MITOCW free_body_diagrams

PHYSICS 1 Forces & Newton s Laws

Energy Whiteboard Problems

(f ) From the graph, obtain the height of the tube given the mass of the dart is 20 grams and the constant force applied in the tube is 2 newtons.

Engage I 1. What do you think about this design? If the car were to suddenly stop, what would happen to the child? Why?

AP Physics C: Work, Energy, and Power Practice

RECAP!! Paul is a safe driver who always drives the speed limit. Here is a record of his driving on a straight road. Time (s)

Section /07/2013. PHY131H1F University of Toronto Class 9 Preclass Video by Jason Harlow. Based on Knight 3 rd edition Ch. 5, pgs.

LAB: FORCE AND MOTION

Calculating Acceleration

LECTURE 19: Simple harmonic oscillators

Chapter 3 Kinematics in Two Dimensions; Vectors

Concepts in Physics. Friday, October 16th

If there is now a constant air resistance force of 35 N, what is the new maximum height the ball attains?

Frictional Force ( ): The force that occurs when two object rub against one another and always OPPOSES motion. It's not dependent on area of contact.

To study applications of Newton s Laws as they. To study conditions that establish equilibrium. To consider contact forces and the effects of

Lecture Outline Chapter 6. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Dynamics: Forces and Newton s Laws of Motion

Lecture PowerPoints. Chapter 2 Physics for Scientists and Engineers, with Modern Physics, 4 th Edition Giancoli

Q2. A book whose mass is 2 kg rests on a table. Find the magnitude of the force exerted by the table on the book.

Physics 2A Chapter 4: Forces and Newton s Laws of Motion

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

Forces and Newton s Second Law

Physics Mechanics. Lecture 18 Energy Conservation I

Physics 8 Monday, October 9, 2017

Chapter 3 Kinematics in Two Dimensions; Vectors

The world is charged with the grandeur of God.

Exam. Name. 1) For general projectile motion with no air resistance, the horizontal component of a projectile's velocity A) B) C) D)

PHYSICAL SCIENCES: PAPER I

Physics 380 Physics and Society. Lecture 2: Newton s Laws, Mass, Force and Motion

PHY321 Homework Set 2

Show all work in answering the following questions. Partial credit may be given for problems involving calculations.

Physics 121, Sections 1 and 2, Winter 2011 Instructor: Scott Bergeson Exam #3 April 16 April 21, 2011 RULES FOR THIS TEST:

PHYSICS 8A, Lecture 2 Spring 2017 Midterm 2, C. Bordel Thursday, April 6 th, 7pm-9pm

Isaac Newton ( ) 1687 Published Principia Invented Calculus 3 Laws of Motion Universal Law of Gravity

Newton s first and second laws

MITOCW MIT8_01F16_L12v01_360p

Transcription:

LECTURE 12: Free body diagrams Select LEARNING OBJECTIVES: i. ii. iii. iv. v. vi. Understand how to define a system for which to draw a FBD for. Demonstrate the ability to draw a properly scaled free body diagram from an image of a scenario or a written description of a scenario. Understand the importance of including a coordinate system along with a FBD. Be able to determine the relative direction of the acceleration of an object based off of a properly scaled FBD. Understand that the two forces constituting a force pair will never show up on the same FBD. Be able to identify any internal forces for a system if applicable. TEXTBOOK CHAPTERS: Giancoli (Physics Principles with Applications 7 th ) :: N/A Knight (College Physics : A strategic approach 3 rd ) :: 4.3, 4.6, 5.7 BoxSand :: Forces ( Free Body Diagrams ) WARM UP: After a baseball with mass m1 is hit, it flies through the air from the home plate (HP) to the outfield from left to right as represented by the trajectory drawn below. Ignoring air resistance, which of the following FBDs for the baseball at point P could be correct? To help us properly analyze the motion of a system, we need to consider all the interactions that the system has with its surroundings before we write down any equations. The number of interactions can become daunting, not to mention keeping track of the magnitudes and directions of all the forces that we use to mathematically describe these interactions. A free body diagram (FBD) is an invaluable tool to help us visualize all the forces acting on our system so that we may analyze the motion of the system much more efficiently. Until otherwise noted, we will still be working under the point particle approximation. Thus all forces we draw on objects can be represented as acting through the object's center of mass, which itself can be represented by a point particle. Do not concern yourself with the actual calculation of the center of mass statement just yet, we will introduce that math at a later time. For now it is sufficient to just understand that we are writing equations of motion for the center of mass of our system, wherever that may be located. Lectures Page 1

Defining a system The first step in analyzing any problem is deciding what object(s) we are interested in. This is known as defining our system. So the system is just another word for the collection of objects, or single object, that we plan on analyzing to determine motion. We restrict ourselves to only defining a system of multiple objects if all objects have the same acceleration. Consider the collection of objects below. Where mass 1 and 2 do not slide relative to one another (i.e. mass 2 will always be directly on top of mass 1), and mass 3 is connected by a massless string which does not stretch. Since mass 2 does not slide relative to mass 1, they both have the same acceleration to the right. Also, since mass 3 is connected to mass 1 via a string that does not stretch, mass 3 has the same acceleration as mass 1. Thus, as the person is pulling mass 3 to the right via a massless string, all objects have the same acceleration. With this image constructed, we now have options for how we can define our system. The options for our system are (m 1, m 2, m 3, m 1 + m 2, m 1 + m 3, m 2 + m 3, m 1 + m 2 + m 3 ). A few of these options are shown below. Drawing a FBD Now that you have defined your system, it is time to draw a FBD for that system. Our FBD will consist of a single dot, representing our system, from which we draw force vectors that represent all the interactions that the system has with its environment. FBD are not complete without a coordinate system defined. To illustrate what a FBD is, we will look at two examples. EXAMPLE: Draw a FBD for the defined system below. Assume no friction exists between m 1 and the surface, and also that m 2 is stuck on top of m 1. Lectures Page 2

Since this is not a video, I will show the important steps that I take when drawing a FBD. Showing all these steps are not necessary, they are only shown for pedagogical purposes. After this one example, I will only show the final free body diagram(s) without the steps. Step 1: Draw horizontal and vertical axes Step 2: Draw non-contact forces Step 3: Draw contact forces NOTE: I like to draw my non-contact forces first, just so I don't forget them (e.g. I think about all the non-contact forces that exist and see if any of them would be present on the FBD of interest). Then I go through the long list of contact forces in my head to make sure I don't forget any of them either. You do not need to draw them in this order, I just use it as a systematic way so that I hopefully don't forget to include any necessary forces. Lectures Page 3

Step 4: Draw/label coordinate system ** This is the final finished FBD with the forces scaled appropriately. EXAMPLE: Draw a FBD for the defined system below. Assume no friction exists between m 1 and the table, also no friction between m 3 and the table, and that m 2 is stuck on top of m 1. The steps shown in the first example before this one should be followed (i.e. draw horizontal and vertical axes, draw non-contact forces, draw contact forces, define coordinate system). PRACTICE: Draw a FBD for each mass separately and the combined (m 1 + m 2 ) system. Attempt to scale each force relative to each other. Lectures Page 4

PRACTICE: Draw a FBD for the person m 2, and the scale m 1. Attempt to scale each force relative to each other. What does a scale really measure? Scale PRACTICE: Draw a FBD for the box below. Attempt to scale each force relative to each other. Lectures Page 5

PRACTICE: Mass 1 and mass 2 are suspended by three separate wires of negligible mass. Draw a FBD for each separate mass. Attempt to scale the forces relative to each other. *Do you see another system we could construct?* Lectures Page 6

Conceptual questions for discussion 1) 2) Will a force-pair ever show up on the same FBD? Consider the image below. Is there a normal force from the person on mass 2? 3) Consider the image below. How many systems could you construct to draw FBDs? Lectures Page 7