1 / 11

Circular Motion

This lecture covers topics such as uniform circular motion, centripetal acceleration, dynamics problems, angular acceleration, displacement, velocity, acceleration, and kinematics equations.

rsotomayor
Download Presentation

Circular Motion

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 08: Circular Motion • Uniform Circular Motion • Centripetal Acceleration • More Dynamics Problems • Circular Motion with Angular Acceleration • Displacement, Velocity, Acceleration • Kinematics Equations

  2. Uniform Circular Motion v An object moving in a circle with constant velocity.

  3. Acceleration in Uniform Circular Motion v R • Centripetal Acceleration • Due to change in DIRECTION (not speed) • Direction of Acceleration: INWARD • Magnitude of Acceleration:

  4. Uniform Circular Motion R v a • Instantaneous velocity is tangent to circle. • Instantaneous acceleration is radially inward. • There must be a net inward force to provide the acceleration.

  5. Driving Example • As you drive over the top of a hill (with radius of curvature of 36 m) in your minivan, at what speed will you begin to leave the road? • There are two forces on the car: • Normal • Gravity • Write F = ma: • FN – Fg = -m v2/R (note: acceleration is DOWN!) • FN – mg = -m v2/R • FN = 0 as you just barely leave the road… • -mg = -m v2/R • g = v2/R FN Fg v 18.8 m/s

  6. More Circular Motion(Non-Uniform) • Angular Displacement Dq = q2-q1 • How far (through what angle) it has rotated • Units: radians (2p radians = 1 revolution) • Angular Velocity w = Dq/Dt • How fast it is rotating • Units: radians/second • Angular Acceleration  = D/Dt • Change in angular velocity divided by time • Units: radians/second2 • Period = 1/frequency T = 1/f = 2p/w • Time to complete 1 revolution (or 2 radians) • Units: seconds

  7. Circular to Linear • Displacement Dx = R Dq(q in radians) • Velocity |v| = Dx/Dt = R Dq/Dt = Rw • Acceleration |a| = Dv/Dt = R Dw/Dt = R

  8. Kinematics for Circular Motion w/ constanta Linear Variables x,v,a (constant a). Angular Variables q,w,a (constant a).

  9. Gears Example • One of the gears in your car has a radius of 20 cm. Starting from rest it accelerates from 900 rpm to 2000 rpm in 0.5 s (rpm stands for revolutions per minute). Find the angular acceleration, the angular displacement during this time, and the final linear speed of a point on the outside of the gear. • Note that 0 = 94 rad/s and  = 209 rad/s • Find angular acceleration: • Find angular displacement: • Find final linear speed:  = 230 rad/s2  = 76 rad v = 42 m/s

  10. Summary of Concepts • Uniform Circular Motion • Speed is constant • Direction is changing • Acceleration toward center a = v2 / R • Newton’s Second Law F = ma • Circular Motion with Angular Acceleration • q = angular position: rad. • w = angular velocity: rad/s • a = angular acceleration: rad/s2 • Linear to Circular conversions (x = Rq, v = Rw, a = Ra) • Kinematics Equations

  11. v

More Related