non-rotatingframes ofreferencetheta, 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 twomoves adistancex, given x= rΘDirectlyproportionalThe apparentforce thatseems todeflect movingobjects fromtheir pathsraises yourcenter ofmass 6 to10 cmthe greater thewheel’s angularvelocity, thefaster thebicycle travels.the resistanceto change inan object’sangularvelocityangularvelocityremainsconstantDegreesandradiansThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zeroThe apparentforce thatseems topush objectsoutwardIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxis"momentofinertia"Δ𝛳/ΔtIf the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesThis pointcorresponds tothe location onan object wherethe objectbalancesthe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedApply a force toan extendedobject at somedistance from arotation axis forthe object.An object isstable if itscenter of massis locatedabove its basethe torquesmust alsobalance witheach other orthe bicycle willtip overa twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)Equilibrium isachieved whenall the forcesbalance and allthe torquesbalanceto bring thatbicyclesafely to astop whenneedednon-rotatingframes ofreferencetheta, 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 twomoves adistancex, given x= rΘDirectlyproportionalThe apparentforce thatseems todeflect movingobjects fromtheir pathsraises yourcenter ofmass 6 to10 cmthe greater thewheel’s angularvelocity, thefaster thebicycle travels.the resistanceto change inan object’sangularvelocityangularvelocityremainsconstantDegreesandradiansThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zeroThe apparentforce thatseems topush objectsoutwardIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxis"momentofinertia"Δ𝛳/ΔtIf the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesThis pointcorresponds tothe location onan object wherethe objectbalancesthe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedApply a force toan extendedobject at somedistance from arotation axis forthe object.An object isstable if itscenter of massis locatedabove its basethe torquesmust alsobalance witheach other orthe bicycle willtip overa twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)Equilibrium isachieved whenall the forcesbalance and allthe torquesbalanceto bring thatbicyclesafely to astop whenneeded

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