It equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisAn object isstable if itscenter of massis locatedabove its baseDirectlyproportionalraises yourcenter ofmass 6 to10 cmtheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.to bring thatbicyclesafely to astop whenneededThe apparentforce thatseems todeflect movingobjects fromtheir pathsa twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)angularvelocityremainsconstantmoves adistancex, given x= rΘEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceIf 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 isexerted"momentofinertia"DegreesandradiansThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zeroApply a force toan extendedobject at somedistance from arotation axis forthe object.non-rotatingframes ofreferenceThe magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twothe greater thewheel’s angularvelocity, thefaster thebicycle travels.the resistanceto change inan object’sangularvelocityThe apparentforce thatseems topush objectsoutwardΔ𝛳/Δtthe torquesmust alsobalance witheach other orthe bicycle willtip overIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisAn object isstable if itscenter of massis locatedabove its baseDirectlyproportionalraises yourcenter ofmass 6 to10 cmtheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.to bring thatbicyclesafely to astop whenneededThe apparentforce thatseems todeflect movingobjects fromtheir pathsa twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)angularvelocityremainsconstantmoves adistancex, given x= rΘEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceIf 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 isexerted"momentofinertia"DegreesandradiansThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zeroApply a force toan extendedobject at somedistance from arotation axis forthe object.non-rotatingframes ofreferenceThe magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twothe greater thewheel’s angularvelocity, thefaster thebicycle travels.the resistanceto change inan object’sangularvelocityThe apparentforce thatseems topush objectsoutwardΔ𝛳/Δtthe torquesmust alsobalance witheach other orthe bicycle willtip over

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