Apply a force toan extendedobject at somedistance from arotation axis forthe object.Degreesandradiansraises yourcenter ofmass 6 to10 cmΔ𝛳/ΔtIf the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesAn object isstable if itscenter of massis locatedabove its basea twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)DirectlyproportionalThis pointcorresponds tothe location onan object wherethe objectbalancesnon-rotatingframes ofreferenceThe apparentforce thatseems todeflect movingobjects fromtheir pathsEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceto bring thatbicyclesafely to astop whenneededThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zeromoves adistancex, given x= rΘ"momentofinertia"the perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedthe resistanceto change inan object’sangularvelocityThe apparentforce thatseems topush objectsoutwardthe torquesmust alsobalance witheach other orthe bicycle willtip overIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxistheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.The magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twothe greater thewheel’s angularvelocity, thefaster thebicycle travels.angularvelocityremainsconstantApply a force toan extendedobject at somedistance from arotation axis forthe object.Degreesandradiansraises yourcenter ofmass 6 to10 cmΔ𝛳/ΔtIf the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesAn object isstable if itscenter of massis locatedabove its basea twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)DirectlyproportionalThis pointcorresponds tothe location onan object wherethe objectbalancesnon-rotatingframes ofreferenceThe apparentforce thatseems todeflect movingobjects fromtheir pathsEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceto bring thatbicyclesafely to astop whenneededThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zeromoves adistancex, given x= rΘ"momentofinertia"the perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedthe resistanceto change inan object’sangularvelocityThe apparentforce thatseems topush objectsoutwardthe torquesmust alsobalance witheach other orthe bicycle willtip overIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxistheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.The magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twothe greater thewheel’s angularvelocity, thefaster thebicycle travels.angularvelocityremainsconstant

Bingo - Chapter 8 Rotational Motion - Call List

(Print) Use this randomly generated list as your call list when playing the game. There is no need to say the BINGO column name. Place some kind of mark (like an X, a checkmark, a dot, tally mark, etc) on each cell as you announce it, to keep track. You can also cut out each item, place them in a bag and pull words from the bag.


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  1. Apply a force to an extended object at some distance from a rotation axis for the object.
  2. Degrees and radians
  3. raises your center of mass 6 to 10 cm
  4. Δ𝛳/Δt
  5. If the torque and angular velocity are in opposite directions, then the angular velocity decreases
  6. An object is stable if its center of mass is located above its base
  7. a twist that can change an object’s angular velocity, and it is measured in newton-meters (Nm)
  8. Directly proportional
  9. This point corresponds to the location on an object where the object balances
  10. non-rotating frames of reference
  11. The apparent force that seems to deflect moving objects from their paths
  12. Equilibrium is achieved when all the forces balance and all the torques balance
  13. to bring that bicycle safely to a stop when needed
  14. The net force exerted on the object must be zero, and the net torque exerted on the object around all points must be zero
  15. moves a distance x, given x = rΘ
  16. "moment of inertia"
  17. the perpendicular distance from the axis of rotation to the point where the force is exerted
  18. the resistance to change in an object’s angular velocity
  19. The apparent force that seems to push objects outward
  20. the torques must also balance with each other or the bicycle will tip over
  21. It equals the net torque on the object about that axis divided by the object’s rotational inertia about that axis
  22. theta, omega, and alpha equal the corresponding linear quantities x, v, and a divided by the radius of the rotating object.
  23. The magnitude of force F, the distance to the axis of rotation r, and the angle between these two
  24. the greater the wheel’s angular velocity, the faster the bicycle travels.
  25. angular velocity remains constant