"momentofinertia"If the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesDegreesandradiansthe greater thewheel’s angularvelocity, thefaster thebicycle travels.The magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twoa twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)Δ𝛳/ΔtThe apparentforce thatseems todeflect movingobjects fromtheir pathsThe apparentforce thatseems topush objectsoutwardIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisraises yourcenter ofmass 6 to10 cmthe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zerothe torquesmust alsobalance witheach other orthe bicycle willtip overThis pointcorresponds tothe location onan object wherethe objectbalancesApply a force toan extendedobject at somedistance from arotation axis forthe object.the resistanceto change inan object’sangularvelocityAn object isstable if itscenter of massis locatedabove its baseEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceangularvelocityremainsconstantDirectlyproportionalnon-rotatingframes ofreferencemoves adistancex, given x= rΘtheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.to bring thatbicyclesafely to astop whenneeded"momentofinertia"If the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesDegreesandradiansthe greater thewheel’s angularvelocity, thefaster thebicycle travels.The magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twoa twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)Δ𝛳/ΔtThe apparentforce thatseems todeflect movingobjects fromtheir pathsThe apparentforce thatseems topush objectsoutwardIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisraises yourcenter ofmass 6 to10 cmthe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zerothe torquesmust alsobalance witheach other orthe bicycle willtip overThis pointcorresponds tothe location onan object wherethe objectbalancesApply a force toan extendedobject at somedistance from arotation axis forthe object.the resistanceto change inan object’sangularvelocityAn object isstable if itscenter of massis locatedabove its baseEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceangularvelocityremainsconstantDirectlyproportionalnon-rotatingframes ofreferencemoves adistancex, given x= rΘtheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.to 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. "moment of inertia"
  2. If the torque and angular velocity are in opposite directions, then the angular velocity decreases
  3. Degrees and radians
  4. the greater the wheel’s angular velocity, the faster the bicycle travels.
  5. The magnitude of force F, the distance to the axis of rotation r, and the angle between these two
  6. a twist that can change an object’s angular velocity, and it is measured in newton-meters (Nm)
  7. Δ𝛳/Δt
  8. The apparent force that seems to deflect moving objects from their paths
  9. The apparent force that seems to push objects outward
  10. It equals the net torque on the object about that axis divided by the object’s rotational inertia about that axis
  11. raises your center of mass 6 to 10 cm
  12. the perpendicular distance from the axis of rotation to the point where the force is exerted
  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 torques must also balance with each other or the bicycle will tip over
  15. This point corresponds to the location on an object where the object balances
  16. Apply a force to an extended object at some distance from a rotation axis for the object.
  17. the resistance to change in an object’s angular velocity
  18. An object is stable if its center of mass is located above its base
  19. Equilibrium is achieved when all the forces balance and all the torques balance
  20. angular velocity remains constant
  21. Directly proportional
  22. non-rotating frames of reference
  23. moves a distance x, given x = rΘ
  24. theta, omega, and alpha equal the corresponding linear quantities x, v, and a divided by the radius of the rotating object.
  25. to bring that bicycle safely to a stop when needed