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