introduction forces

29
Copyright © 2012 Pearson Education Inc. Introduction Forces Physics 7C lecture A Thursday September 26, 8:00 AM – 9:20 AM Engineering Hall 1200

Upload: allegra-hatfield

Post on 31-Dec-2015

27 views

Category:

Documents


0 download

DESCRIPTION

Physics 7C lecture A. Introduction Forces. Thursday September 26, 8:00 AM – 9:20 AM Engineering Hall 1200. Course information. Class website: you can find the link in eee.uci.edu http:// www.physics.uci.edu /~ xia /X-lab/ Teaching.html Textbook : - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Introduction

Forces

Physics 7C lecture A

Thursday September 26, 8:00 AM – 9:20 AMEngineering Hall 1200

Page 2: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Course information

Class website:

you can find the link in eee.uci.edu

http://www.physics.uci.edu/~xia/X-lab/Teaching.html

Textbook:

Young & Freedman, University Physics with Modern Physics (13th edition)

Page 3: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Course information

Instructor: Jing Xia210F Rowland Hall, email: [email protected]

Office Hours: 9:30 AM - 10:30 AM every Thursday in my office 210F Rowland Hall

Lectures:

Tuesday/Thursday, 8:00 AM – 9:20 AM in EH 1200Discussion sessions: Wednesday

Page 4: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Course information

7C Grade:

Page 5: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Course information

Midterm 1 (Chapters 4, 5, 6 and 7): Thursday 8-9:20 AM, October 24, EH 1200·

Midterm 2 (Chapters 8, 9 and 10): Thursday 8-9:20 AM, November 21, EH 1200.

Final Exam (Comprehensive, with emphasis on the chapter 8 onwards): Two-hour exam on December 11th or 13th.

Exams are closed-book, closed-note.

Page 6: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Course schedule

Page 7: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Course information

Detailed class information can be found @:

http://www.physics.uci.edu/~xia/X-lab/Teaching.html

there is a link in eee.uci.edu

Page 8: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Goals for this lecture

• Review Physics 2 concepts

• To understand the meaning of force in physics

• To view force as a vector and learn how to combine forces

Page 9: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Review physics 2

• Units and physical quantities

• Motion in 1D

• Motion in 2D and 3D

Page 10: Introduction Forces

Copyright © 2012 Pearson Education Inc.

The nature of physics

• Physics is an experimental science in which physicists seek patterns that relate the phenomena of nature.

• The patterns are called physical theories.

• A very well established or widely used theory is called a physical law or principle.

Page 11: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Unit prefixes

• Table 1.1 shows some larger and smaller units for the fundamental quantities.

Page 12: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Uncertainty and significant figures—Figure 1.7• The uncertainty of a measured quantity

is indicated by its number of significant figures.

• For multiplication and division, the answer can have no more significant figures than the smallest number of significant figures in the factors.

• For addition and subtraction, the number of significant figures is determined by the term having the fewest digits to the right of the decimal point.

• Refer to Table 1.2, Figure 1.8, and Example 1.3.

• As this train mishap illustrates, even a small percent error can have spectacular results!

Page 13: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Vectors and scalars

• A scalar quantity can be described by a single number.

• A vector quantity has both a magnitude and a direction in space.

• In this book, a vector quantity is represented in boldface italic type with an arrow over it: A.

• The magnitude of A is written as A or |A|.

Page 14: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Drawing vectors—Figure 1.10

• Draw a vector as a line with an arrowhead at its tip.

• The length of the line shows the vector’s magnitude.

• The direction of the line shows the vector’s direction.

• Figure 1.10 shows equal-magnitude vectors having the same direction and opposite directions.

Page 15: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Adding two vectors graphically—Figures 1.11–1.12

• Two vectors may be added graphically using either the parallelogram method or the head-to-tail method.

Page 16: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Displacement, time, and average velocity—Figure 2.1

• A particle moving along the x-axis has a coordinate x.

• The change in the particle’s coordinate is x = x2 x1.

• The average x-velocity of the particle is vav-x = x/t.

• Figure 2.1 illustrates how these quantities are related.

Page 17: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Position vector

• The position vector from the origin to point P has components x, y, and z.

Page 18: Introduction Forces

Copyright © 2012 Pearson Education Inc.

The x and y motion are separable—Figure 3.16

• The red ball is dropped at the same time that the yellow ball is fired horizontally.

• The strobe marks equal time intervals.

• We can analyze projectile motion as horizontal motion with constant velocity and vertical motion with constant acceleration: ax = 0 and ay = g.

Page 19: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Tranquilizing a falling monkey

• Where should the zookeeper aim?

• Follow Example 3.10.

Page 20: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Introduction to forces

• We’ve studied motion in one, two, and three dimensions… but what causes motion?

• This causality was first understood in the late 1600s by Sir Isaac Newton.

• Newton formulated three laws governing moving objects, which we call Newton’s laws of motion.

• Newton’s laws were deduced from huge amounts of experimental evidence.

• The laws are simple to state but intricate in their application.

Page 21: Introduction Forces

Copyright © 2012 Pearson Education Inc.

What are some properties of a force?

Page 22: Introduction Forces

Copyright © 2012 Pearson Education Inc.

There are four common types of forces

• The normal force: When an object pushes on a surface, the surface pushes back on the object perpendicular to the surface. This is a contact force.

• Friction force: This force occurs when a surface resists sliding of an object and is parallel to the surface. Friction is a contact force.

Page 23: Introduction Forces

Copyright © 2012 Pearson Education Inc.

There are four common types of forces II

• Tension force: A pulling force exerted on an object by a rope or cord. This is a contact force.

• Weight: The pull of gravity on an object. This is a long-range force.

Page 24: Introduction Forces

Copyright © 2012 Pearson Education Inc.

What are the magnitudes of common forces?

Page 25: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Drawing force vectors—Figure 4.3

• Use a vector arrow to indicate the magnitude and direction of the force.

Page 26: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Superposition of forces—Figure 4.4

• Several forces acting at a point on an object have the same effect as their vector sum acting at the same point.

Page 27: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Decomposing a force into its component vectors

• Choose perpendicular x and y axes.

• Fx and Fy are the components of a force along these axes.

• Use trigonometry to find these force components.

Page 28: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Notation for the vector sum—Figure 4.7

• The vector sum of all the forces on an object is called the resultant of the forces or the net forces.

1 2 3   

R=F +F +F + = F

Page 29: Introduction Forces

Copyright © 2012 Pearson Education Inc.

Superposition of forces—Example 4.1

• Force vectors are most easily added using components: Rx = F1x + F2x + F3x + … , Ry = F1y + F2y + F3y + … . See Example 4.1 (which has three forces).