to bring thatbicyclesafely to astop whenneededApply 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)raises yourcenter ofmass 6 to10 cmmoves adistancex, given x= rΘtheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.the greater thewheel’s angularvelocity, thefaster thebicycle travels.Equilibrium isachieved whenall the forcesbalance and allthe torquesbalance"momentofinertia"The net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zeroIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisthe torquesmust alsobalance witheach other orthe bicycle willtip overThis pointcorresponds tothe location onan object wherethe objectbalancesDirectlyproportionalangularvelocityremainsconstantΔ𝛳/ΔtAn object isstable if itscenter of massis locatedabove its basethe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedThe apparentforce thatseems topush objectsoutwardDegreesandradiansthe resistanceto change inan object’sangularvelocityThe apparentforce thatseems todeflect movingobjects fromtheir pathsnon-rotatingframes ofreferenceThe magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twoIf the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesto bring thatbicyclesafely to astop whenneededApply 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)raises yourcenter ofmass 6 to10 cmmoves adistancex, given x= rΘtheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.the greater thewheel’s angularvelocity, thefaster thebicycle travels.Equilibrium isachieved whenall the forcesbalance and allthe torquesbalance"momentofinertia"The net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zeroIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisthe torquesmust alsobalance witheach other orthe bicycle willtip overThis pointcorresponds tothe location onan object wherethe objectbalancesDirectlyproportionalangularvelocityremainsconstantΔ𝛳/ΔtAn object isstable if itscenter of massis locatedabove its basethe perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedThe apparentforce thatseems topush objectsoutwardDegreesandradiansthe resistanceto change inan object’sangularvelocityThe apparentforce thatseems todeflect movingobjects fromtheir pathsnon-rotatingframes ofreferenceThe magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twoIf the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreases

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