It equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisthe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedthe resistanceto change inan object’sangularvelocityAn object isstable if itscenter of massis locatedabove its baseDirectlyproportionalEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceApply a force toan extendedobject at somedistance from arotation axis forthe object.a twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)"momentofinertia"Δ𝛳/ΔtThis pointcorresponds tothe location onan object wherethe objectbalancesnon-rotatingframes ofreferenceangularvelocityremainsconstanttheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.moves adistancex, given x= rΘThe apparentforce thatseems topush objectsoutwardthe torquesmust alsobalance witheach other orthe bicycle willtip overThe magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these tworaises yourcenter ofmass 6 to10 cmDegreesandradiansto bring thatbicyclesafely to astop whenneededThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zeroIf the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesthe greater thewheel’s angularvelocity, thefaster thebicycle travels.The apparentforce thatseems todeflect movingobjects fromtheir pathsIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisthe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedthe resistanceto change inan object’sangularvelocityAn object isstable if itscenter of massis locatedabove its baseDirectlyproportionalEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceApply a force toan extendedobject at somedistance from arotation axis forthe object.a twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)"momentofinertia"Δ𝛳/ΔtThis pointcorresponds tothe location onan object wherethe objectbalancesnon-rotatingframes ofreferenceangularvelocityremainsconstanttheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.moves adistancex, given x= rΘThe apparentforce thatseems topush objectsoutwardthe torquesmust alsobalance witheach other orthe bicycle willtip overThe magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these tworaises yourcenter ofmass 6 to10 cmDegreesandradiansto bring thatbicyclesafely to astop whenneededThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zeroIf the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesthe greater thewheel’s angularvelocity, thefaster thebicycle travels.The apparentforce thatseems todeflect movingobjects fromtheir paths

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