Circular Motion
Circular Motion
Angular Velocity
Circular Motion
Angular Velocity   Let O be the centre of a circle, radius r units.



         O
    r
Circular Motion
Angular Velocity   Let O be the centre of a circle, radius r units.
                   If the point moves from A to P in time t , where
                   AOP   ,
         O
    r   
A

             P
Circular Motion
Angular Velocity   Let O be the centre of a circle, radius r units.
                   If the point moves from A to P in time t , where
                   AOP   , then the angular velocity,  , of the
         O          point is defined as the rate of change of  with
    r              respect to time.
A                             measured in radians/second
             P
Circular Motion
Angular Velocity   Let O be the centre of a circle, radius r units.
                   If the point moves from A to P in time t , where
                   AOP   , then the angular velocity,  , of the
         O          point is defined as the rate of change of  with
    r              respect to time.
A                             measured in radians/second
                                            d
             P                         
                                             dt
                                           
Circular Motion
Angular Velocity     Let O be the centre of a circle, radius r units.
                     If the point moves from A to P in time t , where
                     AOP   , then the angular velocity,  , of the
        O             point is defined as the rate of change of  with
    r                respect to time.
A                               measured in radians/second
                                              d
            P                            
                                               dt
                                             
Linear Velocity (Tangential Velocity)
Circular Motion
Angular Velocity        Let O be the centre of a circle, radius r units.
                         If the point moves from A to P in time t , where
                         AOP   , then the angular velocity,  , of the
         O                point is defined as the rate of change of  with
    r                    respect to time.
A                                   measured in radians/second
                                                  d
              P                              
                                                   dt
                                                 
Linear Velocity (Tangential Velocity)
The linear velocity, v, of the point at every position on its path is
tangential to the circle.
Circular Motion
Angular Velocity        Let O be the centre of a circle, radius r units.
                         If the point moves from A to P in time t , where
                         AOP   , then the angular velocity,  , of the
         O                point is defined as the rate of change of  with
    r                    respect to time.
A                                   measured in radians/second
                     v
                                                  d
              P                              
                                                   dt
                                                 
Linear Velocity (Tangential Velocity)
The linear velocity, v, of the point at every position on its path is
tangential to the circle.
Circular Motion
Angular Velocity        Let O be the centre of a circle, radius r units.
                         If the point moves from A to P in time t , where
                         AOP   , then the angular velocity,  , of the
         O                point is defined as the rate of change of  with
    r                    respect to time.
A                                   measured in radians/second
                     v
                                                  d
              P                              
                                                   dt
                                                 
Linear Velocity (Tangential Velocity)
The linear velocity, v, of the point at every position on its path is
tangential to the circle.
                       Let arc AP = x
x  r
x  r
dx    d
   r
dt     dt
    r
x  r     v  r
dx    d
   r         OR
dt     dt
    r     v  r
x  r     v  r
         dx    d
            r         OR
         dt     dt
             r     v  r

Period
x  r                      v  r
         dx    d
            r                          OR
         dt     dt
             r                      v  r

Period

                 2
            T        (time taken for one revolution)
                 
x  r                         v  r
         dx    d
            r                             OR
         dt     dt
             r                         v  r

Period

                 2
            T           (time taken for one revolution)
                 

e.g. A satellite moves in a circular orbit of 20 rev/day
a) Describe  in rad/s
x  r                         v  r
         dx    d
            r                             OR
         dt     dt
             r                         v  r

Period

                 2
            T           (time taken for one revolution)
                 

e.g. A satellite moves in a circular orbit of 20 rev/day
a) Describe  in rad/s
                           20  2 rad/day
x  r                              v  r
         dx    d
            r                                  OR
         dt     dt
             r                              v  r

Period

                 2
            T           (time taken for one revolution)
                 

e.g. A satellite moves in a circular orbit of 20 rev/day
a) Describe  in rad/s
                           20  2 rad/day
                               20  2
                                             rad/s
                               24  60  60
                                
                                     rad/s
                               2160
b) Find the satellite' s tangential velocity, given that its radius is 9000km,
   in km/h
b) Find the satellite' s tangential velocity, given that its radius is 9000km,
   in km/h
                     v  r
                                  
                       9000           km/s
                                 2160
b) Find the satellite' s tangential velocity, given that its radius is 9000km,
   in km/h
                     v  r
                                  
                       9000           km/s
                                 2160
                                  
                       9000            60  60km/h
                              2160
                       15000km/h
b) Find the satellite' s tangential velocity, given that its radius is 9000km,
   in km/h
                     v  r
                                  
                       9000           km/s
                                 2160
                                  
                       9000            60  60km/h
                              2160
                       15000km/h




                            Exercise 9A; odd

X2 t06 03 circular motion (2012)

  • 1.
  • 2.
  • 3.
    Circular Motion Angular Velocity Let O be the centre of a circle, radius r units. O r
  • 4.
    Circular Motion Angular Velocity Let O be the centre of a circle, radius r units. If the point moves from A to P in time t , where AOP   , O r  A P
  • 5.
    Circular Motion Angular Velocity Let O be the centre of a circle, radius r units. If the point moves from A to P in time t , where AOP   , then the angular velocity,  , of the O point is defined as the rate of change of  with r  respect to time. A measured in radians/second P
  • 6.
    Circular Motion Angular Velocity Let O be the centre of a circle, radius r units. If the point moves from A to P in time t , where AOP   , then the angular velocity,  , of the O point is defined as the rate of change of  with r  respect to time. A measured in radians/second d P  dt  
  • 7.
    Circular Motion Angular Velocity Let O be the centre of a circle, radius r units. If the point moves from A to P in time t , where AOP   , then the angular velocity,  , of the O point is defined as the rate of change of  with r  respect to time. A measured in radians/second d P  dt   Linear Velocity (Tangential Velocity)
  • 8.
    Circular Motion Angular Velocity Let O be the centre of a circle, radius r units. If the point moves from A to P in time t , where AOP   , then the angular velocity,  , of the O point is defined as the rate of change of  with r  respect to time. A measured in radians/second d P  dt   Linear Velocity (Tangential Velocity) The linear velocity, v, of the point at every position on its path is tangential to the circle.
  • 9.
    Circular Motion Angular Velocity Let O be the centre of a circle, radius r units. If the point moves from A to P in time t , where AOP   , then the angular velocity,  , of the O point is defined as the rate of change of  with r  respect to time. A measured in radians/second v d P  dt   Linear Velocity (Tangential Velocity) The linear velocity, v, of the point at every position on its path is tangential to the circle.
  • 10.
    Circular Motion Angular Velocity Let O be the centre of a circle, radius r units. If the point moves from A to P in time t , where AOP   , then the angular velocity,  , of the O point is defined as the rate of change of  with r  respect to time. A measured in radians/second v d P  dt   Linear Velocity (Tangential Velocity) The linear velocity, v, of the point at every position on its path is tangential to the circle. Let arc AP = x
  • 11.
  • 12.
    x  r dx d r dt dt  r
  • 13.
    x  r v  r dx d r OR dt dt  r v  r
  • 14.
    x  r v  r dx d r OR dt dt  r v  r Period
  • 15.
    x  r v  r dx d r OR dt dt  r v  r Period 2 T (time taken for one revolution) 
  • 16.
    x  r v  r dx d r OR dt dt  r v  r Period 2 T (time taken for one revolution)  e.g. A satellite moves in a circular orbit of 20 rev/day a) Describe  in rad/s
  • 17.
    x  r v  r dx d r OR dt dt  r v  r Period 2 T (time taken for one revolution)  e.g. A satellite moves in a circular orbit of 20 rev/day a) Describe  in rad/s   20  2 rad/day
  • 18.
    x  r v  r dx d r OR dt dt  r v  r Period 2 T (time taken for one revolution)  e.g. A satellite moves in a circular orbit of 20 rev/day a) Describe  in rad/s   20  2 rad/day 20  2  rad/s 24  60  60   rad/s 2160
  • 19.
    b) Find thesatellite' s tangential velocity, given that its radius is 9000km, in km/h
  • 20.
    b) Find thesatellite' s tangential velocity, given that its radius is 9000km, in km/h v  r   9000  km/s 2160
  • 21.
    b) Find thesatellite' s tangential velocity, given that its radius is 9000km, in km/h v  r   9000  km/s 2160   9000   60  60km/h 2160  15000km/h
  • 22.
    b) Find thesatellite' s tangential velocity, given that its radius is 9000km, in km/h v  r   9000  km/s 2160   9000   60  60km/h 2160  15000km/h Exercise 9A; odd