Torque. Correlation between Linear Momentum and Angular Momentum Resistance to change in motion: Linear behavior: Inertia Units M (mass), in kg Angular

Embed Size (px)

Citation preview

  • Slide 1
  • Torque
  • Slide 2
  • Correlation between Linear Momentum and Angular Momentum Resistance to change in motion: Linear behavior: Inertia Units M (mass), in kg Angular Rotational Inerita, Symbol I aka Moment of Inertia Has to do with more than just mass, it includes the shape of the object. If x cm is far away, I is bigger. Based on mass and mass distribution.
  • Slide 3
  • Three Important equations for I : Thin Walled Cylinder I = MR 2 (also valid for an orbiting body) Solid Cylinder I = (1/2)MR 2 (easier because the mass is not so far away) Sphere I = (2/5)MR 2 (marble)
  • Slide 4
  • Slide 5
  • Cause of acceleration Linear Force (Newtons) Angular Torque ( Nm)
  • Slide 6
  • Momentum Linear p = mv ( units kgm/s) Angular L = I (units kgm 2 /s) Bigger mass = harder to stop Faster moving = harder to stop
  • Slide 7
  • Kinetic Energy Linear K = (1/2) mv 2 (Units Joules) Angular K R = (1/2) I 2 A rolling ball has translational and rotational Kinetic energy. Remember: ms become Is, vs become s
  • Slide 8
  • Pivoting Object Take a shape and a piece of paper. Label an x-y axis on the paper. Label pivot point on the shape. Place at origin. Label x cm on shape. Draw weight vector. Draw position vector r from pivot to x cm. Move position vector from origin to x cm.
  • Slide 9
  • Definition: torque Torque is the cause of angular acceleration in the same way that force is the cause of linear acceleration. Symbol (pronounced tao) is the cross product between r and F We say = r cross F = r x F
  • Slide 10
  • Relationship between torque and Newtons second law F = ma rF = rma a is tangential, so a =r rF = torque, = rmr = mr 2 = I ( I=m 1 r 1 2 = m 2 r 2 2 ) So = I ( must be in rad/s 2 )
  • Slide 11
  • Back to picture Draw the angle between the FIRST r vector that starts at the pivot point and the F vector. Then draw the angle between the moved r vector and F. The moved vector is 180-. The old r vector was at . = rF g sin(180-) Mathematically, sin(180-) = sin So = rF g sin() in magnitude. Use RHR for direction.
  • Slide 12
  • On picture, Split weight vector out into components mgcos points toward pivot, mgsin points perpendicular to make it rotate. mgcos gets cancelled out, thats why we use the sin component, = rFsin() That component in this case is spinning it cw, or in the negative direction.
  • Slide 13
  • Lever arm Draw a line from pivot point across to weight vector so that is crosses weight vector at 90 degrees. That line has a magnitude of rsin This is very important. It has a special definition. Its called a lever arm (symbol l ) We can say: = l F
  • Slide 14
  • Cross Product Guided Practice #1 P = 4i + 2j k Q = -3i + 6j -2k P x Q = Answer: 2i + 11j + 30k
  • Slide 15
  • Guided Practice #2 Cross Products P = 2.12i + 8.15j 4.28k N and Q = 2.29i -8.93j 10.5k m Find P x Q Answer: -124i +12.5j 37.6k
  • Slide 16
  • Slide 17
  • Solution 1) O = 0.17 rad/s (v/r) 2) I = (2/5)MR 2 = 0.0144 kgm 2 3) = 1735 rad/s 4) = use quadratic to find time 5) t = 4.25 s
  • Slide 18
  • Slide 19
  • Solution Find I I = MR 2 =.625 kgm 2 Find = 16 rad/s Find = = 800 rad = 127 rev
  • Slide 20
  • Slide 21
  • Slide 22
  • Slide 23
  • Slide 24
  • Slide 25
  • Slide 26
  • Slide 27
  • Slide 28
  • Slide 29
  • Slide 30
  • Slide 31
  • Slide 32
  • Slide 33
  • Slide 34
  • Slide 35
  • Slide 36
  • Slide 37
  • Slide 38
  • Slide 39
  • Slide 40
  • Slide 41
  • Slide 42
  • Slide 43
  • Slide 44
  • Slide 45
  • Slide 46
  • end https://www.youtube.com/watch?v=GLlpi- 0_lB0 https://www.youtube.com/watch?v=GLlpi- 0_lB0