Remember Newton’s 2nd Law?

Slides:



Advertisements
Similar presentations
4. The answer depends on the rotational inertia of the dumbbell.
Advertisements

Review Problems From Chapter 10&11. 1) At t=0, a disk has an angular velocity of 360 rev/min, and constant angular acceleration of rad/s**2. How.
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.
Comparing rotational and linear motion
 Chapter 11: Rotational Dynamics and Static Equilibrium Ch11-1 Torque
MSTC Physics Chapter 8 Sections 3 & 4.
Physics 201: Lecture 18, Pg 1 Lecture 18 Goals: Define and analyze torque Introduce the cross product Relate rotational dynamics to torque Discuss work.
Torque Web Quest Helpful Hints Part I: Definition of Torque Torque is defined as the tendency to produce a change in rotational motion. Examples:
Dynamics of Rotational Motion
Chapter 11 Rolling, Torque, and Angular Momentum In this chapter we will cover the following topics: -Rolling of circular objects and its relationship.
You are trying to open a door that is stuck by pulling on the doorknob in a direction perpendicular to the door. If you instead tie a rope to the doorknob.
Angular Momentum of a Particle
Q10. Rotational Motion.
Rotational Dynamics Just as the description of rotary motion is analogous to translational motion, the causes of angular motion are analogous to the causes.
ROTATIONAL MOTION AND EQUILIBRIUM
Chapter 10 - Rotation Definitions: –Angular Displacement –Angular Speed and Velocity –Angular Acceleration –Relation to linear quantities Rolling Motion.
Torque Chap 8 Units: m N 2.
AP Rotational Dynamics Lessons 91 and 94.  Matter tends to resist changes in motion ◦ Resistance to a change in velocity is inertia ◦ Resistance to a.
T071 Q17. A uniform ball, of mass M = kg and radius R = 0
Physics 207: Lecture 14, Pg 1 Physics 207, Lecture 14, Oct. 23 Agenda: Chapter 10, Finish, Chapter 11, Just Start Assignment: For Wednesday reread Chapter.
Torqued An investigation of rotational motion. Think Linearly Linear motion: we interpret – position as a point on a number line – velocity as the rate.
Physics 111 Practice Problem Statements 10 Torque, Energy, Rolling SJ 8th Ed.: Chap 10.6 – 10.9 Contents 11-47, 11-49*, 11-55*, 11-56, 11-60*, 11-63,
Newton’s Second Law for Rotation Examples
Rotational Dynamics Chapter 8 Section 3.
9 rad/s2 7 rad/s2 13 rad/s2 14 rad/s2 16 rad/s2
Wednesday 6/10 PHYS 2010 Nathalie Hoffmann University of Utah.
Lecture 14: Rolling Objects l Rotational Dynamics l Rolling Objects and Conservation of Energy l Examples & Problem Solving.
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.
Exam is Wednesday at 7:00 pm Remember extra office hours
Definition of Torque Statics and Dynamics of a rigid object
Physics. Session Rotational Mechanics - 3 Session Objectives.
Moments of INERTIA. Review of Inertia Inertia – Objects with mass always resist a change in there motion (acceleration). From Newton’s second law we see.
T072 : Q13. Assume that a disk starts from rest and rotates with an angular acceleration of 2.00 rad/s 2. The time it takes to rotate through the first.
Short Version : 10. Rotational Motion Angular Velocity & Acceleration (Instantaneous) angular velocity Average angular velocity  = angular displacement.
Goal: To understand angular motions Objectives: 1)To learn about Rotational Inertia 2)To learn about Torque 3)To understand Angular Momentum 4)To understand.
Lecture 18: Angular Acceleration & Angular Momentum.
Today: (Ch. 8)  Rotational Motion.
Pgs Chapter 8 Rotational Equilibrium and Dynamics.
Rotational Dynamics.
UNIT 6 Rotational Motion & Angular Momentum Rotational Dynamics, Inertia and Newton’s 2 nd Law for Rotation.
ROTATIONAL DYNAMICS. ROTATIONAL DYNAMICS AND MOMENT OF INERTIA  A Force applied to an object can cause it to rotate.  Lets assume the F is applied at.
TORQUE A torque is an action that causes objects to rotate. Torque is not the same thing as force. For rotational motion, the torque is what is most directly.
Angular Momentum. Definition of Angular Momentum First – definition of torque: τ = Frsinθ the direction is either clockwise or counterclockwise a net.
F1 F2 If F1 = F2… …no change in motion (by Newton’s 1st Law)
Angular Mechanics - Rolling using dynamics Contents:
General Physics I Rotational Motion
It’s just a new notation.
Dynamics of Rotational Motion
Physics 101: Lecture 15 Rolling Objects
9/16/2018 Physics 253.
Aim: How do we apply Newton’s 2nd Law of Rotational Motion?
Rotational Inertia & Kinetic Energy
Chapter 10: Rotational Motional About a Fixed Axis
Aim: How do we explain the rolling motion of rigid bodies?
Rotational Motion AP Physics.
Newton’s 2nd Law for Rotation
10.8   Torque Torque is a turning or twisting action on a body about a rotation axis due to a force, . Magnitude of the torque is given by the product.
HW #8 due Thursday, Nov 4 at 11:59 p.m.
Remember Newton’s 2nd Law?
Rotational Dynamics.
Q11. Rotational Vectors, Angular Momentum
Aim: How do we explain torque?
Lecture 17 Goals: Chapter 12
ROTATIONAL INERTIA AND THE ROTATIONAL SECOND LAW
Rotational Motion.
Rotational Kinetic Energy Ekr (J)
A block of mass m resting on a horizontal
Rotational Kinematics
Remember Newton’s 2nd Law?
CH10 Recitation.
Presentation transcript:

Remember Newton’s 2nd Law? For linear motion : F=ma a m F For rotational motion : =I I  

Example Treat the spindle as a solid cylinder. m = a) What is the moment of Inertia of the spindle? b) If the tension in the rope is 10 N, what is the angular acceleration of the wheel? c) What is the acceleration of the bucket? d) What is the mass M, of the bucket? m = M

Solution a) What is the moment of Inertia of the spindle? Given: m = 5 kg, r = 0.6 m M = 0.9 kgm2

Solution b) If the tension in the rope is 10 N, what is a? Given: I = 0.9 kg m2, T = 10 N, r = 0.6 m c) What is the acceleration of the bucket? Given: r=0.6 m, a = 6.67 rad/s M

Solution d) What is the mass of the bucket? Given: T = 10 N, a = 4 m/s2 M

1) A 1 kg wheel with a fixed hub start from rest, and a force is applied as shown. Assume that the hub and spokes are massless, and that F = 1 N, and the momentum of inertia is I = MR2. What is the magnitude of the wheel’s angular acceleration? M = 1 kg |F| = 1N R = 0.5 m Q = 60o w/r to horizontal ¼ rad/sec2 ½ rad/sec2 1 rad/sec2 2 rad/sec2 4 rad/sec2

2) A wheel (mass of 1kg and with a radius of 1m) with a fixed hub starts from rest, and forces are applied as shown. Assume that the hub and spokes are massless, and that the wheel is a hoop, I = MR2. F1 = 1 N and acts at a distance of half of the radius of the wheel. What is the angular acceleration of the wheel? F1=1N 1m 0.5m 0.25 rad/s2 0.50 rad/s2 1 rad/s2 2 rad/s2 4 rad/s2

3) Two identical wheels (mass of 1kg and with a radius of 1m) with fixed hubs start from rest, and forces are applied as shown. Assume that the hub and spokes are massless, and that F1 = 1 N. In order to impart identical angular accelerations, how large must F2 be? I = MR2 F1 F2 M = 1 kg 0.25 N 0.50 N 1 N 2 N 4 N F1 1m 0.5m

4) Two 1 kg wheels with fixed hubs start from rest, and forces are applied as shown. Assume that the hub and spokes are massless, and that F1 = 1 N. In order to impart identical angular accelerations, how large must F2 be? I = MR2 F1 F2 M = 1 kg R1 = 0.5 m R2 = 1.0 m 0.25 N 0.50 N 1 N 2 N 4 N

m Ex: A rotation and translation incline example Assume frictionless T Pulley: a disk mpulley = ? r = 0.20 m a=2.0 m/s2 2.0 kg m 20 a) Find the tension in the string. b) Find mass m. Treat the pulley as a solid cylinder. c) Find the torque on the pulley. d) Find the angular acceleration of the pulley. e) Find the rotational inertia of the pulley. f) Find the mass of the pulley.