Chapter 9: Rotational Motion

Slides:



Advertisements
Similar presentations
Q9.1 The graph shows the angular velocity and angular acceleration versus time for a rotating body. At which of the following times is the rotation speeding.
Advertisements

Angular Momentum The vector angular momentum of the point mass m about the point P is given by: The position vector of the mass m relative to the point.
© 2012 Pearson Education, Inc. The graph shows the angular velocity and angular acceleration versus time for a rotating body. At which of the following.
Warm-up: Centripetal Acceleration Practice
Rotational Motion Chapter Opener. Caption: You too can experience rapid rotation—if your stomach can take the high angular velocity and centripetal acceleration.
Physics 207: Lecture 16, Pg 1 Lecture 16Goals: Chapter 12 Chapter 12  Extend the particle model to rigid-bodies  Understand the equilibrium of an extended.
Copyright © 2012 Pearson Education Inc. Rotational Kinematics, Inertia Physics 7C lecture 11 Tuesday November 5, 8:00 AM – 9:20 AM Engineering Hall 1200.
Rotational Motion Chapter 9: Rotational Motion Rigid body instead of a particle Rotational motion about a fixed axis Rolling motion (without slipping)
Chapter 10. Rotation What is Physics?
Physics 201: Lecture 18, Pg 1 Lecture 18 Goals: Define and analyze torque Introduce the cross product Relate rotational dynamics to torque Discuss work.
Chapter 10 Rotational Motion
Lecture 34, Page 1 Physics 2211 Spring 2005 © 2005 Dr. Bill Holm Physics 2211: Lecture 34 l Rotational Kinematics çAnalogy with one-dimensional kinematics.
Physics 151: Lecture 20, Pg 1 Physics 151: Lecture 20 Today’s Agenda l Topics (Chapter 10) : çRotational KinematicsCh çRotational Energy Ch
Chapter 8 Rotational Motion.
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Classical Mechanics Review 4: Units 1-19
Physics. Session Rotational Mechanics - 5 Session Objectives.
Rotation and angular momentum
Chapters 10, 11 Rotation and angular momentum. Rotation of a rigid body We consider rotational motion of a rigid body about a fixed axis Rigid body rotates.
Rotational Kinematics and Energy
Lecture 18 Rotational Motion
ROTATIONAL MOTION AND EQUILIBRIUM
Chapter 10 - Rotation Definitions: –Angular Displacement –Angular Speed and Velocity –Angular Acceleration –Relation to linear quantities Rolling Motion.
T071 Q17. A uniform ball, of mass M = kg and radius R = 0
Chapter 8 Rotational Motion.
Q9.1 The graph shows the angular velocity and angular acceleration versus time for a rotating body. At which of the following times is the rotation speeding.
Rotation of Rigid Bodies
Two-Dimensional Rotational Kinematics 8.01 W09D1 Young and Freedman: 1.10 (Vector Products) , 10.5.
2008 Physics 2111 Fundamentals of Physics Chapter 10 1 Fundamentals of Physics Chapter 10 Rotation 1.Translation & Rotation 2.Rotational Variables Angular.
Chapter 10 Rotational Motion.
9 rad/s2 7 rad/s2 13 rad/s2 14 rad/s2 16 rad/s2
Physics 111: Lecture 17, Pg 1 Physics 111: Lecture 17 Today’s Agenda l Rotational Kinematics çAnalogy with one-dimensional kinematics l Kinetic energy.
Rotational Motion. 6-1 Angular Position, Velocity, & Acceleration.
Physics 207: Lecture 16, Pg 1 Lecture 16Goals: Chapter 12 Chapter 12  Extend the particle model to rigid-bodies  Understand the equilibrium of an extended.
4.1 Rotational kinematics 4.2 Moment of inertia 4.3 Parallel axis theorem 4.4 Angular momentum and rotational energy CHAPTER 4: ROTATIONAL MOTION.
Chapter 9: Rotational Motion
Ch. 9 Rotational Kinematics
Rotation of a Rigid Object About a Fixed Axis 10.
Rotational Motion – Part I AP Physics C. The radian  There are 2 types of pure unmixed motion:  Translational - linear motion  Rotational - motion.
Short Version : 10. Rotational Motion Angular Velocity & Acceleration (Instantaneous) angular velocity Average angular velocity  = angular displacement.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 10 Physics, 4 th Edition James S. Walker.
Lecture Outline Chapter 10 Physics, 4th Edition James S. Walker
Rotational Motion & Equilibrium Rigid Bodies Rotational Dynamics
Classical Mechanics Review 4: Units 1-22
Which object will win? All moments of inertia in the previous table can be expressed as;
Rotational Motion I AP PHYSICS 1.
Rotational Inertia & Kinetic Energy
Rotational Motion and Equilibrium
Rotational Motion AP Physics.
Figure 10.16  A particle rotating in a circle under the influence of a tangential force Ft. A force Fr in the radial direction also must be present to.
Rotation As you come in, please set clicker to channel 44 and then answer the following question (before the lecture starts). Quiz – You are building.
PHYS 1443 – Section 003 Lecture #16
Rotational Kinematics and Energy
Physics 207, Lecture 17, Nov. 1 Work/Energy Theorem, Energy Transfer
C9 – Rotational Energy Get a spring General Physics.
Lecture Outline Chapter 10 Physics, 4th Edition James S. Walker
Chapter 10:Rotation of a rigid object about a fixed axis
Chapter 9: Rotational Motion
Lecture Outline Chapter 10 Physics, 4th Edition James S. Walker
Chapter 11 Angular Momentum
Two-Dimensional Rotational Kinematics 8.01 W09D1
Rotational Motion Let’s begin with Rotational Kinematics!!
Two-Dimensional Rotational Kinematics W09D1 Young and Freedman: 1
Rotational Kinetic Energy Ekr (J)
Rotational Kinetic Energy
Physics 3 – Aug 31, 2017 P3 Challenge –
Rigid Body: Rotational and Translational Motion; Rolling without Slipping 8.01 W11D1 Today’s Reading Assignment Young and Freedman: 10.3.
Rotational Kinetic Energy
CH10 Recitation.
Rigid Body: Rotational and Translational Motion; Rolling without Slipping 8.01 W11D1 Today’s Reading Assignment Young and Freedman:
Presentation transcript:

Chapter 9: Rotational Motion © 2016 Pearson Education, Inc.

Goals for Chapter 9 To study angular velocity and angular acceleration. To examine rotation with constant angular acceleration. To understand the relationship between linear and angular quantities. To determine the kinetic energy of rotation and the moment of inertia. To study rotation about a moving axis. © 2016 Pearson Education, Inc.

Rotational Motion Rigid body instead of a particle Rotational motion about a fixed axis Rolling motion (without slipping) Rotational Motion

A New Way to Measure Angular Quantities – Figure 9.2 The radian is dimensionless as a ratio of lengths © 2016 Pearson Education, Inc.

Concepts of rotational motion 3 word dictionary Distance d  angle θ Velocity 𝒗  angular velocity 𝒘 Acceleration 𝒂  angular acceleration ∝ Angle θ How many degrees are in one radian ? (rad is the unit of choice for rotational motion) 𝜽= 𝑺 𝒓  ratio of two lengths (dimensionless) 𝑺 𝒓 = 𝟐𝝅𝒓 𝒓 =𝟐𝝅 𝒓𝒂𝒅 ≅𝟑𝟔𝟎° 𝟏 𝒓𝒂𝒅≅ 𝟑𝟔𝟎° 𝟐𝝅 = 𝟑𝟔𝟎° 𝟔.𝟐𝟖 =𝟓𝟕° ∴ Factors of unity 𝟏 𝒓𝒂𝒅 𝟓𝟕° or 𝟓𝟕° 𝟏 𝒓𝒂𝒅 1 radian is the angle subtended at the center of a circle by an arc with length equal to the radius. Angular velocity 𝒘 𝒘 𝒂𝒗 = 𝜽 𝟐 − 𝜽 𝟏 𝒕 𝟐 − 𝒕 𝟏 = ∆𝜽 ∆𝒕 𝒓𝒂𝒅 𝒔 →𝒘= lim ∆𝒕→𝟎 ∆𝜽 ∆𝒕 𝒓𝒂𝒅 𝒔 Other units are; 𝟏 𝒓𝒆𝒗 𝒔 = 𝟐𝝅 𝒓𝒂𝒅 𝒔 ∴𝟏 𝒓𝒆𝒗 𝒎𝒊𝒏 =𝟏 𝒓𝒑𝒎= 𝟐𝝅 𝟔𝟎 𝒓𝒂𝒅 𝒔

We Have a Sign Convention – Figure 9.7 © 2016 Pearson Education, Inc.

Angular acceleration ∝ ∝ 𝒂𝒗 = 𝒘 𝟐 − 𝒘 𝟏 𝒕 𝟐 − 𝒕 𝟏 = ∆𝒘 ∆𝒕 𝒓𝒂𝒅 𝒔 𝟐 → ∝= lim ∆𝒕→𝟎 ∆𝒘 ∆𝒕 𝒓𝒂𝒅 𝒔 𝟐 Relationship between linear and angular quantities 𝐬=𝜽𝒓  𝒗 𝒂𝒗 = ∆𝒔 ∆𝒓 =𝒓 ∆𝜽 ∆𝒕 =𝒓 𝒘 𝒂𝒗 ∴∆𝒕→𝟎 𝒈𝒊𝒗𝒆𝒔 𝒗=𝒓𝒘

Tangential component of acceleration; ∆𝑣=𝑟∆𝑤 ( 𝑎 𝑡𝑎𝑛𝑔𝑒𝑛𝑡 ) 𝑎𝑣 = ∆𝑣 ∆𝑡 =𝑟 ∆𝑤 ∆𝑡 For; ∆𝒕→𝟎; 𝒂 𝒕𝒂𝒏𝒈𝒆𝒏𝒕 =𝒓∝ Radial component 𝒂 𝒓𝒂𝒅 = 𝒗 𝟐 𝒓 = 𝒘 𝟐 𝒓 Magnitude of 𝑎 𝒂 =𝒂= 𝒂 𝒓𝒂𝒅 𝟐 + 𝒂 𝒕𝒂𝒏 𝟐

Angular Quantities Kinematical variables to describe the rotational motion: Angular position, velocity and acceleration Rotational Motion

Angular Quantities: Vector Kinematical variables to describe the rotational motion: Angular position, velocity and acceleration Vector natures z R.-H. Rule y x Rotational Motion

“R” from the Axis (O) Solid Disk Solid Cylinder Rotational Motion

Kinematical Equations for constant angular acceleration Rotational Motion

Rotational Motion

Rotation of a Bicycle Wheel – Figure 9.8 θ at t=3.00 s? 𝜃= 𝜃 0 + 𝜔 0 𝑡+ 1 2 𝛼 𝑡 2 =0+ 4.00 rad s 3.00 𝑠 + 1 2 2.00 rad s 2 3.00 s 2 =21.0 rad=21.0 rad 1 rev 2𝜋 rad =3.34 rev. 3 complete revolutions with an additional 0.34 rev 0.34 rev 2π rad rev =2.14 rad=123º ω at t=3.00 s? 𝜔= 𝜔 0 +𝛼𝑡 =4.00 rad s + 2.00 rad s 2 3.00 s =𝟏𝟎.𝟎 𝐫𝐚𝐝 𝐬 OR using Δθ 𝜔 2 = 𝜔 0 2 +2𝛼 𝜃− 𝜃 0 = 4.00 rad s 2 +2 2.00 rad s 2 21.0 rad =100 ra d 2 s 2 , 𝜔= 100 =𝟏𝟎 𝒓𝒂𝒅 𝒔 See Example 9.2 in your text © 2016 Pearson Education, Inc.

Relationship between Linear and Angular Quantities atan arad Rotational Motion

Q9.2 Clicker question A DVD is initially at rest so that the line PQ on the disc’s surface is along the +x-axis. The disc begins to turn with a constant = 5.0 rad/s2. At t = 0.40 s, what is the angle between the line PQ and the +x-axis? A. 0.40 rad B. 0.80 rad C. 1.0 rad D. 1.6 rad E. 2.0 rad Answer: A

Clicker question On a merry-go-round, you decide to put your toddler on an animal that will have a small angular velocity. Which animal do you pick? Any animal; they all have the same angular velocity. One close to the hub. One close to the rim. Answer: a) Any animal; they all have the same angular velocity. © 2016 Pearson Education, Inc.

Tooth spacing is the same 2r1 N1 2r2 N2 = vtan= same = r11= r22 Tooth spacing is the same 2r1 N1 2r2 N2 = 2 1 N1 = N2 Rotational Motion

A. a faster linear speed and a faster angular speed. Q9.5 Clicker question Compared to a gear tooth on the rear sprocket (on the left, of small radius) of a bicycle, a gear tooth on the front sprocket (on the right, of large radius) has A. a faster linear speed and a faster angular speed. B. the same linear speed and a faster angular speed. C. a slower linear speed and the same angular speed. D. the same linear speed and a slower angular speed. E. none of the above. Answer: D

Energy in rotational motion and moment of inertia: 𝐾 𝑟 = 𝑖 1 2 𝑚 𝑖 𝑣 𝑖 2 = 𝑖 1 2 𝑚 𝑖 𝑟 𝑖 2 𝑤 2 = 1 2 𝑖 𝑚 𝑖 𝑟 𝑖 2 𝐼 𝑤 2 = 1 2 𝐼 𝑤 2 With moment of Inertia; For large 𝐾 𝑟 it is better faster and not so much heavier Example: fly wheel. 𝐾= 1 2 𝐼 𝑤 2 → 𝐼=𝑀 𝑅 2 = 𝑖 𝑚 𝑖 𝑟 𝑖 2 [kg m2] For general shapes; (c - factors) 𝐼=𝑐𝑀 𝑅 2 Hula hoop = all point on the circumference 𝑟 𝑖 =𝑅

Example 9-3 Given; 𝑤=10 𝑟𝑎𝑑 𝑠 ; ∝=50 𝑟𝑎𝑑 𝑠 ; 𝑟=0.8𝑚 𝑎 𝑡𝑎𝑛 =𝑟∝=0.8∗50=40 𝑚 𝑠 2 𝑎 𝑟𝑎𝑑 = 𝑣 2 𝑟 = 𝑤 2 𝑟= 10 2 ∗0.8=80 𝑚 𝑠 2 Now; a =a= a rad 2 + a tan 2 =89 m s 2 Energy in rotational motion and moment of inertia; 𝑖 1 2 𝑚 𝑖 𝑣 𝑖 2 = 𝑖 1 2 𝑚 𝑖 𝑟 𝑖 2 𝑤 2 = 1 2 𝑖 𝑚 𝑖 𝑟 𝑖 2 𝐼 𝑤 2 = 1 2 𝐼 𝑤 2 𝐾= 1 2 𝐼 𝑤 2 → 𝐼= 𝑖 𝑚 𝑖 𝑟 𝑖 2 𝐼=𝑐𝑀 𝑅 2 → 𝐼=𝑀 𝑅 2

Finding the moment of inertia for common shapes

A. four times its initial value. B. twice its initial value. Q9.6 Clicker question You want to double the radius of a rotating solid sphere while keeping its kinetic energy constant. (The mass does not change.) To do this, the final angular velocity of the sphere must be A. four times its initial value. B. twice its initial value. C. the same as its initial value. D. half of its initial value. E. one-quarter of its initial value. Answer: D

A. Object A is rotating fastest. B. Object B is rotating fastest. Q9.7 Clicker question The three objects shown here all have the same mass and the same outer radius. Each object is rotating about its axis of symmetry (shown in blue). All three objects have the same rotational kinetic energy. Which object is rotating fastest? A. Object A is rotating fastest. B. Object B is rotating fastest. C. Object C is rotating fastest. D. Two of these are tied for fastest. E. All three rotate at the same speed. Answer: B A. B. C.

Q-RT9.1 Clicker question Objects A, B, and C all have the same mass, all have the same outer dimension, and are all uniform. A. B. C. Rank these objects in order of their moment of inertia about an axis through its center (shown in blue), from largest to smallest. Answer: BCA

Q-RT9.2 Clicker question Objects A, B, and C all have the same mass, all have the same outer dimension, and are all uniform. Each object is rotating about an axis through its center (shown in blue). All three objects have the same rotational kinetic energy. A. B. C. Answer: ACB Rank these objects in order of their angular speed of rotation, from fastest to slowest.

Note: In rotational motion the moment of inertia depends on the axis of rotation. It is not like a mass a constant parameter of an object Example 9.6: An abstract sculpture 𝐼= 𝑚 𝐴 𝑟 𝐴 2 + 𝑚 𝐵 𝑟 𝐵 2 + 𝑚 𝐶 𝑟 𝐶 2 For axis BC, disks B and C are on axis; 𝑟 𝐵 = 𝑟 𝐶 =0 𝐼 𝐵𝐶 = 𝑚 𝐴 𝑟 𝐴 2 =0.3∗ 0.4 2 =0.048 𝑘𝑔 𝑚 2 For axis through A perpendicular to the plane; 𝑟 𝐴 =0 𝐼 𝐴 = 𝑚 𝐵 𝑟 𝐵 2 + 𝑚 𝐶 𝑟 𝐶 2 =0.1∗ 0.5 2 +0.2∗ 0.4 2 =0.057 𝑘𝑔 𝑚 2 c) If the object rotates with 𝑤=4 𝑟𝑎𝑑 𝑠 around the axis through A perpendicular to the plane, what is 𝐾 𝑟𝑜𝑡 ? 𝐾 𝑟𝑜𝑡 = 1 2 𝐼 𝐴 𝑤 2 = 1 2 ∗0.057∗ 0.4 2 =0.46 𝐽

Moments of Inertia & Rotational Energy – Example 9.7 © 2016 Pearson Education, Inc.

Q9.8 Clicker question A thin, very light wire is wrapped around a drum that is free to rotate. The free end of the wire is attached to a ball of mass m. The drum has the same mass m. Its radius is R and its moment of inertia is I = (1/2)mR2. As the ball falls, the drum spins. At an instant that the ball has translational kinetic energy K, what is the rotational kinetic energy of the drum? Answer: C A. K B. 2K C. K/2 D. K/4 E. none of these

Problem 9.31: Each mass is at a distance r= 2∗ (0.4) 2 2 = 0.4 2 from the axis. 𝐼= 𝑚 𝑟 2 =4∗0.2∗ 0.4 2 2 =0.064 𝑘𝑔 𝑚 2 (axis is through center) Each mass is r=0.2m from the axis. 𝐼=4∗0.2∗ 0.2 2 =0.032 𝑘𝑔 𝑚 2 ( 𝒂𝒙𝒊𝒔 𝒊𝒔 along the line AB) Two masses are on the axis and two are 0.4 2 from the axis. 𝐼=2∗0.2∗ 0.4 2 2 =0.032 𝑘𝑔 𝑚 2 (axis is alongCD) The value of I depends on the location of the axis.

𝐼 𝑜 = 𝑚 𝑟𝑖𝑚 𝑅 2 + 8 3 𝑚 𝑠𝑝𝑜𝑘𝑒 𝑅 2 =0.193 𝑘𝑔 𝑚 2 𝑚 𝑟𝑖𝑚 =1.4kg 𝑚 𝑠𝑝𝑜𝑘𝑒 =0.28 kg Problem 9.34: 𝐼 𝑜 = 𝑚 𝑟𝑖𝑚 𝑅 2 + 8 3 𝑚 𝑠𝑝𝑜𝑘𝑒 𝑅 2 =0.193 𝑘𝑔 𝑚 2 Rotational Motion

An Airplane Propeller – Example 9.4 Refer to Figure 9.13 and the worked problem on page 264. © 2016 Pearson Education, Inc.

Which object will win? All moments of inertia in the previous table can be expressed as; 𝐼 𝑐𝑚 =𝛽𝑀 𝑅 2 =𝑐𝑀 𝑅 2 (c - number) Compare; a) For a thin walled hollow cylinder 𝛽=1 For a solid cylinder 𝛽= 1 2 etc. Conservation of energy; 0+𝑀𝑔ℎ= 1 2 𝑀 𝑣 2 + 1 2 𝐼 𝑤 2 = 1 2 𝑀 𝑣 2 + 1 2 𝛽𝑀 𝑅 2 ( 𝑣 𝑅 ) 2 = 1 2 (1+𝛽)𝑀 𝑣 2 𝒗= 𝟐𝒈𝒉 𝟏+𝛽 Small 𝛽 bodies wins over large 𝛽 bodies.

On a horizontal surface , what fraction of the total kinetic energy is rotational? a) a uniform solid cylinder . b) a uniform sphere c)a thin walled hollow sphere d)a hollow cylinder with outer radius R an inner radius R/2On K= 1 2 𝑀 𝑣 2 + 1 2 𝐼 𝑤 2 Small 𝛽 bodies win over large 𝛽 bodies Rotational Motion

9.40 A light string is wrapped around the outer rim of a solid uniform cylinder of diameter 75 cm that can rotate about an axis through its center. A stone is tied to the free end of the string .When the string is released from rest the stone reaches a speed of 3.5m/sec after having fallen 2.5 m What is the mass of the cylinder?? Rotational Motion

Clicker question You are preparing your unpowered soapbox vehicle for a soapbox derby down a local hill. You're choosing between solid-rim wheels and wheels that have transparent hollow rims. Which kind will help you win the race? Answer: c) The hollow-rim wheels. Either kind; it doesn't matter. The solid-rim wheels. The hollow-rim wheels. solid hollow © 2016 Pearson Education, Inc.

Conservation of energy in a well Find the speed v of the bucket and the angular velocity w of the cylinder just as the bucket hits the water 𝐾 𝑓 = 1 2 𝑚 𝑣 2 + 1 2 𝐼 𝑤 2 𝐼= 1 2 𝑀 𝑅 2 →𝑣=𝑅𝑤 Energy conservation; 𝐾 𝑖 + 𝑈 𝑖 = 𝐾 𝑓 + 𝑈 𝑓 0+𝑚𝑔ℎ= 1 2 𝑚 𝑣 2 + 1 2 1 2 𝑀 𝑅 2 𝑣 𝑅 2 = 1 2 𝑚+ 1 2 𝑀 𝑣 2 𝒗= 𝟐𝒈𝒉 𝟏+ 𝑴 𝟐𝒎 Note: free fall velocity for M<<<m; all energy goes to kinetic and not rotation.

Calculate the angular momentum and kinetic energy of a solid uniform sphere with a radius of 0.12 m and a mass of 14.0 kg if it is rotating at 6.00 rad/s about an axis through its center 𝐼= 2 5 𝑀 𝑅 2 = 2 5 ∗ 14𝑘𝑔 0.12𝑚 2 =0.0806 𝑘𝑔 𝑚 2 𝐿=𝐼𝑤=0.0806 𝑘𝑔 𝑚 2 ∗6.0 rad=0.484 kg 𝑚 2 𝑠 𝐾= 1 2 𝐼 𝑤 2 = 1 2 𝐿𝑤= 1 2 0.484 kg 𝑚 2 𝑠 ∗6 rad=1.45 J

Q-RT9.3 Clicker question Two identical uniform solid spheres are attached by a solid uniform thin rod. The rod lies on a line connecting the centers of mass of the two spheres. Axes A, B, C, and D are in the same plane as the centers of mass of the spheres and of the rod. For the combined object of two spheres plus rod, rank the object’s moments of inertia about the four axes, from largest to smallest. A B Answer: CBAD C D