1 / 34

Lecture 16: Work, Conservative and Non-Conservative Forces, Rotational Inertia, Power

This lecture covers topics such as work, conservative and non-conservative forces, rotational inertia, potential energy, power, and rotational dynamics. It also includes examples and exercises to help understand these concepts.

dawnhamilton
Download Presentation

Lecture 16: Work, Conservative and Non-Conservative Forces, Rotational Inertia, Power

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. Lecture 16 • Chapter 11 (Work) • Employ conservative and non-conservative forces • Relate force to potential energy • Use the concept of power (i.e., energy per time) • Chapter 12 • Define rotational inertia (“mass”) • Define rotational kinetic energy • Define center of mass Goals: Assignment: • HW7 due Tuesday, Nov. 2nd • For Wednesday: Read Chapter 12, Sections 1-3, 5 & 6 Exam 2 7:15 PM Thursday, Nov. 4th

  2. “Scalar or Dot Product” Definition of Work, The basics Ingredients:Force (F ), displacement ( r) Work, W, of a constant force F acts through a displacement  r: W = F· r(Work is a scalar) F  r  displacement If we know the angle the force makes with the path, the dot product gives usF cos qandDr

  3. v ExerciseWork in the presence of friction and non-contact forces • A box is pulled up a rough (m > 0) incline by a rope-pulley-weight arrangement as shown below. • How many forces (including non-contact ones) are doing work on the box ? • Of these which are positive and which are negative? • State the system (here, just the box) • Use a Free Body Diagram • Compare force and path • 2 • 3 • 4 • 5

  4. Work with varying forces or curved paths If the path is curved or if the force varies with position then at each point and

  5. Work and Varying Forces (1D) Area = Fx Dx F is increasing Here W = F·r becomes dW = Fdx • Consider a varying force F(x) Fx x Dx

  6. Example: Spring-Mass energy transfer • How much will the spring compress (u = x – xequilibrium) to bring the box to a stop (i.e., v = 0 ) if the object is moving initially at a constant velocity (vo) on frictionless surface as shown below ? to vo m spring at an equilibrium position u F V=0 t m spring compressed

  7. mg h mg Relate work to potential energy • Consider the ball moving up to height h (from time 1 to time 2) • How does this relate to the potential energy? Work done by the Earth’s gravity on the ball) W = F Dx = -mg h DU = Uf – Ui = mg h - mg 0 = mg h DU = -W This is a general result for all conservative forces (also path independent)

  8. Uf rf ri Ui Conservative Forces & Potential Energy • For any conservative force F we can define a potential energy function U in the following way: The work done by a conservative force is equal and opposite to the change in the potential energy function. ò W=F·dr= - U

  9. Conservative Forces and Potential Energy • So we can also describe work and changes in potential energy (for conservative forces) DU = - W • but in 1D W = Fx Dx • Combining these two, DU = - Fx Dx • Letting small quantities go to infinitesimals, dU = - Fx dx • Or, Fx = -dU / dx

  10. Path 2 Path 1 A Non-Conservative Force, Friction • Looking down on an air-hockey table with no air flowing (m > 0). • Now compare two paths in which the puck starts out with the same speed (Ki path 1 = Ki path 2) .

  11. Path 2 Path 1 A Non-Conservative Force Since path2 distance >path1 distance the puck will be traveling slower at the end of path 2. Work done by a non-conservative force irreversibly removes energy out of the “system”. Here WNC = Efinal - Einitial < 0 and reflects Ethermal

  12. Work & Power: • Two cars go up a hill, a Corvette and a ordinary Chevy Malibu. Both cars have the same mass. • Assuming identical friction, both engines do the same amount of work to get up the hill. • Are the cars essentially the same ? • NO. The Corvette can get up the hill quicker • It has a more powerful engine.

  13. Work & Power: • Power is the rate at which work is done. Average Power: Instantaneous Power: Units (SI) are Watts (W): 1 W = 1 J / 1s Example: • A person of mass 200. kg walks up 10.0 m. If he/she climbs in 10.00 sec what is the average power used (g = 10 m/s2) • Pavg = F h / t = mgh / t = 200. x 10.0 x 10.0 / 10.00 Watts • P = 2000 W

  14. Work & Power: • Average Power: • Instantaneous Power: • Constant force

  15. Work & Power: Example 2 : Engine of a jet develops a trust of 15,000 N when plane is flying at 300 m/s. What is the horsepower of the engine ? P = F v P = (15,000 N) (300 m/s) = 4.5 x 106 W = (4.5 x 106 W) (1 hp / 746 W) ~ 6,000 hp !

  16. Power time Power Z3 time Power time Exercise Work & Power • Top • Middle • Bottom • Starting from rest, a car drives up a hill at constant acceleration and then suddenly stops at the top. • The instantaneous power delivered by the engine during this drive looks like which of the following,

  17. Chap. 12: Rotational Dynamics • Up until now rotation has been only in terms of circular motion with ac = v2 / R and | aT | = d| v | / dt • Rotation is common in the world around us. • Many ideas developed for translational motion are transferable.

  18. Rotational Dynamics: A child’s toy, a physics playground or a student’s nightmare • A merry-go-round is spinning and we run and jump on it. What does it do? • We are standing on the rim and our “friends” spin it faster. What happens to us? • We are standing on the rim a walk towards the center. Does anything change?

  19. System of Particles (Distributed Mass): • Until now, we have considered the behavior of very simple systems (one or two masses). • But real objects have distributed mass ! • For example, consider a simple rotating disk and 2 equal mass m plugs at distances r and 2r. • Compare the velocities and kinetic energies at these two points. w 1 2

  20. 1 K= ½ m v2 = ½ m (w r)2 w 2 K= ½ m (2v)2 = ½ m (w 2r)2 System of Particles (Distributed Mass): • The rotation axis matters too! • Twice the radius, four times the kinetic energy

  21. 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

  22. 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:

  23. 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

  24. Calculating Moment of Inertia... • For a discrete collection of point masses we found: • 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: dm r

  25. dr r R L Moments of Inertia 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:

  26. Lecture 16, Work & Energy • Strings are wrapped around the circumference of two solid disks and pulled with identical forces for the same linear distance. Disk 1 has a bigger radius, but both are identical material (i.e. their density r = M/V is the same). Both disks rotate freely around axes though their centers, and start at rest. • Which disk has the biggest angular velocity after the pull? W = F d = ½ I w2 (A)Disk 1 (B)Disk 2 (C)Same w2 w1 F F start d finish

  27. Rotation & Kinetic Energy... • The kinetic energy of a rotating system looks similar to that of a point particle: Point Particle Rotating System v is “linear” velocity m is the mass.  is angular velocity I is the moment of inertia about the rotation axis.

  28. Connection with CM motion • If an object of mass M is moving linearly at velocity VCMwithout rotating then its kinetic energy is • If an object of moment of inertia ICMis rotating in place about its center of mass at angular velocityw then its kinetic energy is • What if the object is both moving linearly and rotating?

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

  30. + + m2 m1 m1 m2 System of Particles: Center of Mass (CM) • If an object is not held then it will rotate about the center of mass. • Center of mass: Where the system is balanced ! • Building a mobile is an exercise in finding centers of mass. mobile

  31. System of Particles: Center of Mass • How do we describe the “position” of a system made up of many parts ? • Define the Center of Mass (average position): • For a collection of N individual point-like particles whose masses and positions we know: RCM m2 m1 r2 r1 y x (In this case, N = 2)

  32. RCM = (12,6) (12,12) 2m m m (0,0) (24,0) Sample calculation: • Consider the following mass distribution: XCM = (m x 0 + 2m x 12 + m x 24 )/4m meters YCM = (m x 0 + 2m x 12 + m x 0 )/4m meters XCM= 12 meters YCM= 6 meters

  33. System of Particles: Center of Mass • For a continuous solid, convert sums to an integral. dm r y where dmis an infinitesimal mass element. x

  34. Recap Assignment: • HW7 due Nov. 2nd • For Monday: Read Chapter 12, Sections 7-11

More Related