1 / 26

Physics 207, Lecture 16, Oct. 27

Physics 207, Lecture 16, Oct. 27. Chapter 12 Extend the particle model to rigid-bodies U nderstand the equilibrium of an extended object. Understand rotation about a fixed axis. Employ “conservation of angular momentum” concept. Goals:. Assignment: HW7 due Oct. 29

franciso
Download Presentation

Physics 207, Lecture 16, Oct. 27

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Physics 207, Lecture 16, Oct. 27 • Chapter 12 • Extend the particle model to rigid-bodies • Understand the equilibrium of an extended object. • Understand rotation about a fixed axis. • Employ “conservation of angular momentum” concept Goals: Assignment: • HW7 due Oct. 29 • Wednesday: Review session

  2. Connection with motion... • So for a solid object which rotates about its center of mass and whose CM is moving: VCM 

  3. Rotational Dynamics: What makes it spin? A force applied at a distance from the rotation axis gives a torque a FTangential NET = |r| |FTang| ≡|r||F| sin f F Fradial r • Only the tangential component of the force matters. With torque the position of the force matters • Torque is the rotational equivalent of force Torque has units of kg m2/s2 = (kg m/s2) m = N m • A constant torque gives constant angularacceleration iff the mass distribution and the axis of rotation remain constant.

  4. F cos(90°-q) = FTang. line of action r a 90°-q q F F r sin q F Fradial r r r Torque is a vector quantity • Magnitude is given by |r| |F| sin q or, equivalently, by the |Ftangential | |r| or by |F| |rperpendicular to line of action | • Direction is parallel to the axis of rotation with respect to the “right hand rule” • And for a rigid object= I a

  5. Exercise Torque Magnitude • Case 1 • Case 2 • Same • In which of the cases shown below is the torque provided by the applied force about the rotation axis biggest? In both cases the magnitude and direction of the applied force is the same. • Remember torque requires F, rand sin q or the tangential force component times perpendicular distance L F F L axis case 1 case 2

  6. a FTangential F Fradial r Rotational Dynamics: What makes it spin? A force applied at a distance from the rotation axis NET = |r| |FTang| ≡|r||F| sin f • Torque is the rotational equivalent of force Torque has units of kg m2/s2 = (kg m/s2) m = N m NET = r FTang = r m aTang = r m r a = (m r2) a For every little part of the wheel

  7. a FTangential F Frandial r For a point massNET = m r2a and inertia The further a mass is away from this axis the greater the inertia (resistance) to rotation • This is the rotational version of FNET = ma • Moment of inertia, I≡ m r2 , (here I is just a point on the wheel) is the rotational equivalent of mass. • If I is big, more torque is required to achieve a given angular acceleration.

  8. Calculating Moment of Inertia where r is the distance from the mass to the axis of rotation. Example:Calculate the moment of inertia of four point masses (m) on the corners of a square whose sides have length L, about a perpendicular axis through the center of the square: m m L m m

  9. Calculating Moment of Inertia... • For a single object, Idepends on the rotation axis! • Example:I1 = 4 m R2 = 4 m (21/2 L / 2)2 I1= 2mL2 I2= mL2 I= 2mL2 m m L m m

  10. dr r R L dm r Moments of Inertia • For a continuous solid object we have to add up the mr2contribution for every infinitesimal mass element dm. • An integral is required to find I: Solid disk or cylinder of mass M and radius R, about perpendicular axis through its center. I = ½ M R2 • Some examples of I for solid objects: Use the table…

  11. Rotation & Kinetic Energy • Consider the simple rotating system shown below. (Assume the masses are attached to the rotation axis by massless rigid rods). • The kinetic energy of this system will be the sum of the kinetic energy of each piece: • K = ½m1v12 + ½m2v22 + ½m3v32 + ½m4v42 m4 m1 r1  r4 r2 m3 r3 m2

  12. m4 m1 r1  r4 m3 r2 r3 m2 Rotation & Kinetic Energy • Notice that v1 = w r1 , v2 = w r2 , v3 = w r3 , v4 = w r4 • So we can rewrite the summation: • We recognize the quantity, moment of inertia orI, and write:

  13. Ball 1 Ball 2 Exercise Rotational Kinetic Energy • ¼ • ½ • 1 • 2 • 4 • We have two balls of the same mass. Ball 1 is attached to a 0.1 m long rope. It spins around at 2 revolutions per second. Ball 2 is on a 0.2 m long rope. It spins around at 2 revolutions per second. • What is the ratio of the kinetic energy of Ball 2 to that of Ball 1 ?

  14. Work & Kinetic Energy: • Recall the Work Kinetic-Energy Theorem: K = WNET • This applies to both rotational as well as linear motion. • So for an object that rotates about a fixed axis • For an object which is rotating and translating

  15. Angular Momentum: • We have shown that for a system of particles, momentum is conserved if • What is the rotational equivalent of this? angular momentum is conserved if

  16. v1 m2 j  m1 r2 r1 i v2 r3 v3 m3 Angular momentum of a rigid bodyabout a fixed axis: • Consider a rigid distribution of point particles rotating in the x-y plane around the z axis, as shown below. The total angular momentum around the origin Is the sum of the angular momentum of each particle: • Even if no connecting rod we can deduce an Lz ( ri and vi, are perpendicular) Using vi =  ri, we get

  17. z z F Example: Two Disks • A disk of mass M and radius R rotates around the z axis with angular velocity 0. A second identical disk, initially not rotating, is dropped on top of the first. There is friction between the disks, and eventually they rotate together with angular velocity F. 0

  18. z z 0 F Example: Two Disks • A disk of mass M and radius R rotates around the z axis with initial angular velocity 0. A second identical disk, at rest, is dropped on top of the first. There is friction between the disks, and eventually they rotate together with angular velocity F. No External Torque so Lz is constant Li = Lf I wii = I wf½ mR2w0 = ½ 2mR2wf

  19. Example: Throwing ball from stool • A student sits on a stool, initially at rest, but which is free to rotate. The moment of inertia of the student plus the stool is I. They throw a heavy ball of mass M with speed v such that its velocity vector moves a distance d from the axis of rotation. • What is the angular speed F of the student-stool system after they throw the ball ? M v F d I I Top view: before after

  20. Example: Throwing ball from stool • What is the angular speed F of the student-stool system after they throw the ball ? • Process: (1) Define system (2) Identify Conditions (1) System: student, stool and ball (No Ext. torque, L is constant) (2) Momentum is conserved Linit = 0 = Lfinal = -mvd + I wf M v F d I I Top view: before after

  21. Angular Momentum as a Fundamental Quantity • The concept of angular momentum is also valid on a submicroscopic scale • Angular momentum has been used in the development of modern theories of atomic, molecular and nuclear physics • In these systems, the angular momentum has been found to be a fundamental quantity • Fundamental here means that it is an intrinsic property of these objects

  22. Fundamental Angular Momentum • Angular momentum has discrete values • These discrete values are multiples of a fundamental unit of angular momentum • The fundamental unit of angular momentum is h-bar • Where h is called Planck’s constant

  23. Intrinsic Angular Momentum photon

  24. Angular Momentum of a Molecule • Consider the molecule as a rigid rotor, with the two atoms separated by a fixed distance • The rotation occurs about the center of mass in the plane of the page with a speed of

  25. Angular Momentum of a Molecule (It heats the water in a microwave over) E = h2/(8p2I) [ J (J+1) ] J = 0, 1, 2, ….

  26. Physics 207, Lecture 16, Oct. 27 Assignment: • HW7 due Oct. 29 • Wednesday: Review session

More Related