non-rotatingframes ofreferencethe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedtheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.DirectlyproportionalEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisthe torquesmust alsobalance witheach other orthe bicycle willtip overa twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)The 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 magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twoThis pointcorresponds tothe location onan object wherethe objectbalancesThe apparentforce thatseems topush objectsoutwardApply a force toan extendedobject at somedistance from arotation axis forthe object.Degreesandradiansthe resistanceto change inan object’sangularvelocityto bring thatbicyclesafely to astop whenneededThe apparentforce thatseems todeflect movingobjects fromtheir pathsraises yourcenter ofmass 6 to10 cmΔ𝛳/Δt"momentofinertia"An object isstable if itscenter of massis locatedabove its baseangularvelocityremainsconstantmoves adistancex, given x= rΘthe greater thewheel’s angularvelocity, thefaster thebicycle travels.non-rotatingframes ofreferencethe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedtheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.DirectlyproportionalEquilibrium isachieved whenall the forcesbalance and allthe torquesbalanceIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisthe torquesmust alsobalance witheach other orthe bicycle willtip overa twist that canchange an object’sangular velocity,and it is measuredin newton-meters(Nm)The 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 magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twoThis pointcorresponds tothe location onan object wherethe objectbalancesThe apparentforce thatseems topush objectsoutwardApply a force toan extendedobject at somedistance from arotation axis forthe object.Degreesandradiansthe resistanceto change inan object’sangularvelocityto bring thatbicyclesafely to astop whenneededThe apparentforce thatseems todeflect movingobjects fromtheir pathsraises yourcenter ofmass 6 to10 cmΔ𝛳/Δt"momentofinertia"An object isstable if itscenter of massis locatedabove its baseangularvelocityremainsconstantmoves adistancex, given x= rΘthe greater thewheel’s angularvelocity, thefaster thebicycle travels.

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