moves adistancex, given x= rΘIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisthe greater thewheel’s angularvelocity, thefaster thebicycle travels.The magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twoThe apparentforce thatseems topush objectsoutwardEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceDegreesandradiansthe torquesmust alsobalance witheach other orthe bicycle willtip overIf the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesThis pointcorresponds tothe location onan object wherethe objectbalancesto bring thatbicyclesafely to astop whenneededthe resistanceto change inan object’sangularvelocityThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zerothe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedraises yourcenter ofmass 6 to10 cma twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)theta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.Δ𝛳/Δtnon-rotatingframes ofreferenceThe apparentforce thatseems todeflect movingobjects fromtheir pathsangularvelocityremainsconstantAn object isstable if itscenter of massis locatedabove its baseApply a force toan extendedobject at somedistance from arotation axis forthe object.Directlyproportional"momentofinertia"moves adistancex, given x= rΘIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisthe greater thewheel’s angularvelocity, thefaster thebicycle travels.The magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twoThe apparentforce thatseems topush objectsoutwardEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceDegreesandradiansthe torquesmust alsobalance witheach other orthe bicycle willtip overIf the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesThis pointcorresponds tothe location onan object wherethe objectbalancesto bring thatbicyclesafely to astop whenneededthe resistanceto change inan object’sangularvelocityThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zerothe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedraises yourcenter ofmass 6 to10 cma twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)theta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.Δ𝛳/Δtnon-rotatingframes ofreferenceThe apparentforce thatseems todeflect movingobjects fromtheir pathsangularvelocityremainsconstantAn object isstable if itscenter of massis locatedabove its baseApply a force toan extendedobject at somedistance from arotation axis forthe object.Directlyproportional"momentofinertia"

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