CT1: When I whirl a ball in a vertical circle attached to a rubber band, which statement is true? A. The rubber band will contract to provide an outward.

Slides:



Advertisements
Similar presentations
Newton’s Laws + Circular Motion. Sect. 5-2: Uniform Circular Motion; Dynamics A particle moving in uniform circular motion at radius r, speed v = constant:
Advertisements

Uniform Circular Motion
Circular Motion and Gravitation
PHYS16 – Lecture 11 Ch. 6 Circular Motion
Chapter 6: Circular Motion & Other Applications of Newton’s Laws
Circular Motion; Gravitation
Announcements: -Midterm 1 coming up Monday Oct. 1, (two evening times, 5-6 pm or 6-7 pm). -Material: Chapter I’ll provide key equations (last page.
D. C. B. A. E. CT1. X X X X D. C. B. A. CT2 X X X.
UB, Phy101: Chapter 5, Pg 1 Physics 101: Chapter 5 Application of Newton's Laws l New Material: Textbook Chapter 5 è Circular Motion & Centripetal Acceleration.
Copyright © 2009 Pearson Education, Inc. Lecture 4 Circular Motion 1.
06-1 Physics I Class 06 Uniform Circular Motion Newton’s Second Law - Yet Another Review!
Circular Motion and Other Applications of Newton’s Laws
05-1 Physics I Class 05 Uniform Circular Motion Newton’s Second Law - Review.
Chapter 6: Force and Motion II. Newton’s Laws I.If no net force acts on a body, then the body’s velocity cannot change. II.The net force on a body is.
5.2 Uniform Circular motion 5.3 Dynamic of Uniform Circular Motion
5.4 highway curves 5.5 Non-uniform circular motion 5.6 Drag Velocity
Circular Motion and Other Applications of Newton’s Laws
Using Newton’s Laws: Friction, Circular Motion, Drag Forces
Announcements! Extra credit posted this coming Sunday--get your team together! Mon/Tue-Circular applications of Newton’s Laws Good examples in the book!
Chapter 7 Rotational Motion & Law of Gravity Section 7-3 Causes of Circular Motion.
Circular Motion and Other Applications of Newton’s Laws
Uniform Circular Motion
Chapter 5 Uniform Circular Motion. Chapter 5 Objectives (*vocab) 1. Centripetal Acceleration centripetal* uniform circular motion* period* formula for.
CIRCULAR MOTION.
Chapter 6 Circular Motion and Other Applications of Newton’s Laws.
1 5.2 Uniform Circular Motion A force,, is directed toward the center of the circle This force is associated with an acceleration, a c Applying Newton’s.
Centripetal Force and Acceleration Unit 6, Presentation 1.
CIRCULAR MOTION.
RQ8: A car is driving at a constant speed in a perfect circle on a flat parking lot. The centripetal force acting on the car is: A. Gravity. B. The normal.
In this chapter we will learn about the forces acting on particles when they move on a circular trajectory. Chapter 6: Circular Motion Reading assignment:
Important situations in circular motion. When accelerating, the feeling you have is opposite the acceleration This is why it feels like there is centrifugal.
Uniform Circular Motion. Motion in a Circle Revolution: If entire object is moving in a circle around an external point. The earth revolves around the.
CHAPTER 6 : CIRCULAR MOTION AND OTHER APPLICATIONS OF NEWTON’S LAWS
PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, & Dr. Derrick Boucher Assoc. Prof. of Physics Session 9, Chapter 8.
Motion, Forces and Energy Lecture 5: Circles and Resistance m FrFr FrFr m FrFr A particle moving with uniform speed v in a circular path of radius r experiences.
Vertical Circular Motion
 Extension of Circular Motion & Newton’s Laws Chapter 6 Mrs. Warren Kings High School.
Circular Motion. Uniform Circular Motion  An object that moves in a circle at a constant speed, v.  The magnitude of the velocity remains the same but.
Ch. 6: Circular Motion & Other Applications of Newton’s Laws
Centripetal Acceleration and Circular Motion. A B C Answer: B v Circular Motion A ball is going around in a circle attached to a string. If the string.
Copyright © 2009 Pearson Education, Inc. Chapter 5 Using Newton’s Laws: Friction, Circular Motion, Drag Forces.
9/21/2012PHY 113 A Fall Lecture 101 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 10: Chapter 6 -- Newton’s Laws continued.
Circular Motion Dynamics 8.01 W04D2. Today’s Reading Assignment: W04D2 Young and Freedman: 3.4;
Set 4 Circles and Newton February 3, Where Are We Today –Quick review of the examination – we finish one topic from the last chapter – circular.
Lecture 5 Chapter 5 Using Newton’s Laws Friction Circular motion Drag Forces Numerical integration Misconceptions.
Announcements: -Midterm exam coming up Wednesday Feb. 16, (two evening times, 5-6 pm or 6-7 pm). -Material: Chapter Key equations will be provided.
Dynamics of Uniform Circular Motion Uniform Circular Motion Centripetal Acceleration Centripetal Force Satellites in Circular Orbits Vertical Circular.
Circular Motion Chapter 9 in the Textbook Chapter 6 is PSE pg. 81.
Circular Motion: Gravitation Chapter Kinematics of Uniform Circular Motion  Uniform circular motion is when an object moves in a circle at constant.
Circular Motion: Centripetal force Chapter 8 Nov 5/6.
5.5 Non-uniform circular motion 5.6 Drag Velocity
Circular Motion Dynamics 8.01 W04D2. Today’s Reading Assignment: W04D2 Young and Freedman: 3.4; Experiment 2: Circular Motion 2.
Warm Up. Two blocks of mass m = 2 kg and M = 5 kg are hanging off a single pulley, as shown. Determine the acceleration of the blocks. Ignore the mass.
Circular Motion Chapter 7 Section 1. What are we discussing today? Circular motion Centripetal acceleration & Centripetal force Tangential Speed You will.
UNIFORM CIRCULAR MOTION Centripetal force. UNIFORM CIRCULAR MOTION  Motion at a constant speed around a circle with a constant radius. V Fc Ac.
Dynamics of Uniform Circular Motion  An object moving on a circular path of radius r at a constant speed, V  Motion is not on a straight line, the direction.
Newton’s Laws. Newton’s First Law: The Law of Inertia An object at rest will stay at rest unless acted upon by a force, and an object in motion will stay.
AL Physics Circular Motion Circular motion Revision Circular motion in horizontal Vertical circular motion Loop-the-loop.
Chapter 6 Force and Motion II. Forces of Friction When an object is in motion on a surface or through a viscous medium, there will be a resistance to.
M Friction.
Centripetal Acceleration and Circular Motion
Circular Motion and Other Applications of Newton’s Laws
Ch. 6: Circular Motion & Other Applications of Newton’s Laws
Chapter 7 Objectives Solve problems involving centripetal force.
Circular Motion and the Law of Gravity.
Uniform Circular Motion
Newton’s Second Law Force equals mass times acceleration. F = ma.
Chapter 7 Objective Solve problems involving centripetal acceleration.
Forces & Circular Motion
Fundamentals of Physics School of Physical Science and Technology
Presentation transcript:

CT1: When I whirl a ball in a vertical circle attached to a rubber band, which statement is true? A. The rubber band will contract to provide an outward force on the nurf ball. B. The rubber band will contract because of the inward force on the nurf ball. C. The rubber band will not change in length. D. The rubber band will stretch because of the outward force on the nurf ball. E. The rubber band will stretch to provide an inward force on the nurf ball.

A. B. C. D. CT2

Chapter 6 Circular Motion and Other Applications of Newton’s Laws 6.1 Newton’s Second Law for a Particle in Uniform Circular Motion a r = v t 2 /r F r = ma r = mv t 2 /r taking inward as positive Note: a r = a c = centripetal acceleration a t =0, but because it is  to a r, it has no bearing on the radial direction

P6.1 (p.155)

A.E.F.B.C.D. P6.55 (p.160) CT3

Chapter 6 Circular Motion and Other Applications of Newton’s Laws 6.1 Newton’s Second Law for a Particle in Uniform Circular Motion Comparison of Linear and Circular Motion

Chapter 6 Circular Motion and Other Applications of Newton’s Laws 6.2 Nonuniform Circular Motion F r = ma r = mv t 2 /r taking inward as positive F t = ma t Note: a t = tangential or  acceleration Because a t is  to a r, they have no bearing on each other’s motion. You can do two separate 1D problems (Ch.2). 

CT4: At the top of the path when I whirl a bucket of water over my head, the water in the bucket will A. stay in the bucket because it is forced outward and stopped by the bottom of the bucket. B. stay in the bucket because gravity is temporarily suspended. C. stay in the bucket only if I whirl the bucket with enough speed so that the bottom of the bucket must supply an inward force. D. stay in the bucket at any speed that I whirl the bucket. E. not stay in the bucket.

rsin  r P6.58 (p.161)

Chapter 6 Circular Motion and Other Applications of Newton’s Laws 6.4 Motion in the Presence of Resistive Forces A. Smaller objects, lower speed: R = bv B. Larger objects, higher speeds: R = DAv 2 /2 D = drag coefficient;  = fluid density; A = cross-sectional area Both forces oppose motion.

P6.27 (p.157)

Fig. P6.60, p.178  Bs =  Bk =  Ps =  Pk = 0.450