The apparentforce thatseems todeflect movingobjects fromtheir pathsAn object isstable if itscenter of massis locatedabove its baseDirectlyproportionalIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisThe apparentforce thatseems topush objectsoutwardThis pointcorresponds tothe location onan object wherethe objectbalances"momentofinertia"the perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedΔ𝛳/Δtthe greater thewheel’s angularvelocity, thefaster thebicycle travels.If the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesa 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.angularvelocityremainsconstantDegreesandradiansto bring thatbicyclesafely to astop whenneededmoves adistancex, given x= rΘnon-rotatingframes ofreferenceThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zerotheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.Equilibrium isachieved whenall the forcesbalance and allthe torquesbalanceraises yourcenter ofmass 6 to10 cmthe resistanceto change inan object’sangularvelocitythe torquesmust alsobalance witheach other orthe bicycle willtip overThe magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these twoThe apparentforce thatseems todeflect movingobjects fromtheir pathsAn object isstable if itscenter of massis locatedabove its baseDirectlyproportionalIt equals the nettorque on theobject about thataxis divided by theobject’s rotationalinertia about thataxisThe apparentforce thatseems topush objectsoutwardThis pointcorresponds tothe location onan object wherethe objectbalances"momentofinertia"the perpendiculardistance from theaxis of rotation tothe point wherethe force isexertedΔ𝛳/Δtthe greater thewheel’s angularvelocity, thefaster thebicycle travels.If the torque andangular velocityare in oppositedirections, thenthe angularvelocity decreasesa 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.angularvelocityremainsconstantDegreesandradiansto bring thatbicyclesafely to astop whenneededmoves adistancex, given x= rΘnon-rotatingframes ofreferenceThe net force exertedon the object must bezero, and the nettorque exerted on theobject around allpoints must be zerotheta, omega, andalpha equal thecorrespondinglinear quantities x,v, and a divided bythe radius of therotating object.Equilibrium isachieved whenall the forcesbalance and allthe torquesbalanceraises yourcenter ofmass 6 to10 cmthe resistanceto change inan object’sangularvelocitythe torquesmust alsobalance witheach other orthe bicycle willtip overThe magnitude offorce F, thedistance to theaxis of rotation r,and the anglebetween these two

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