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Kinematics
flipperworks.com

Dynam deals with the motion of bodies with
       ics
reference to the forces that act on the system.
Kinem atics deals with the motion of bodies
without reference to the forces that act on the
system.


   Two types of motion will be studied:

      1.    One dimensional motion
              - rectilinear motion

      2.    Two dimensional motion
              - projectile motion
flipperworks.com



  1. Definition of terms

  [I]   Displacement s

        Displacem is the distance travelled
                  ent
        along a specified direction.
                                                           B

Body travels along
curved path from A
to B.              A

        It is a vector quantity.
        SI unit: m etre, m
flipperworks.com


[II]   Speed v
       Speed is the rate of change of
       distance.
       It is a scalar quantity.
       SI unit: m s-1
       average speed
       < v > = total distance covered
                   total time taken
A body that travels equal distances in equal
intervals of time is said to be moving with
c o ns ta nt or unifo rm speed.
flipperworks.com

Estimates of speeds (in m s-1)

 walking           1.5
 sprinter          10
 Speed limit       25 [ie. 90 km h-1]
 Jet plane         250
 Sound (in air)    330
 Light (in vacuum) 3.00 × 108
flipperworks.com


[III]   Velocity v

        Velocity is the rate of change of
        displacem  ent.

        It is a vector quantity.
        SI unit: m s-1                   ds
                                      v=
                                         dt
        average velocity
                                            rate of
               total displaceme nt          change
        <v > =
                 total time taken
flipperworks.com



A body which travels equal distances in
the same direction in equal intervals of
time is said to be moving with c o ns ta nt
or unifo rm velocity.




        < speed > may not always be
        equal to < velocity >
flipperworks.com


     Example 1:
  (a) total distance = 5.0 + 5.0 = 10.0 km

(b) displacement =         5.0 2 + 5.0 2
                              N
             = 7.1 km              5.0 km
                                   θ
             5 .0
     tan θ =      = 1 .0                            5.0 km
             5 .0
     ⇒    θ = 45o
     Displacement is 7.1 km at a bearing of 135 o
     or S45oE.
flipperworks.com




                  10.0
(c)   <speed>   =
                   1 .0
                = 10 km h-1

                     7 .1
(d)   <velocity> =
                     1.0

                =    7.1 km h-1
                at a bearing of 135o
flipperworks.com


[IV]    Acceleration a

        Acceleration is the rate of change of
        velocity.

        It is a vector q ua ntity .      dv
                                      a=
        SI unit: m s-2                   dt


       A change in velocity can be caused by:
       (i) a change in its magnitude only,
       (ii) a change in its direction only, or
       (iii) a change in both its magnitude and
             direction.
flipperworks.com



A body which travels with equal increase
in speed in the same direction in equal
intervals of time is said to be moving
with c o ns ta nt or unifo rm acceleration.


acceleration = 0 ⇒ constant velocity



But when velocity = 0 at one instant,
acceleration need not be zero. (Think
of a situation where this can happen.)
flipperworks.com


Retardation or deceleration
describes a situation when magnitude of
velocity decreases with time
i.e. body is slowing down.

This occurs when acceleration and velocity act
in opposite directions.


In the next slide, observe the directions of the
velocity and acceleration when a body travels
faster and when it slows down.
flipperworks.com

      Free fall
K    A body is said to be in fre e fa ll if the only
i    force acting on it is the gravitational force
e    due to the Earth.
m
    The downward acceleration of such a body
a
    is known as a c c e le ra tio n d ue to g ra vity .
t   g = 9.81 m s-2
c   (assumed to be constant near Earth’s surface)
s
      True free fall only occurs in vacuum.
      All bodies falling freely will have this constant
      acceleration regardless of their masses.
flipperworks.com

          2   Graphical Representation of Motion
K
           2.1 Displacement-time graph
i
n displacement , s            average velocity
                              between O and A = S1
e                                                   t1
      s1
m                      A
                              (gradient of the line
a                             passing through O & A)
t
s

                                  time, t
      O                 t1
flipperworks.com




displacement , s
                              slope at A =
    s1              A ds      instantaneous
                              velocity at A
                                       ds
                    dt               =
                                       dt

                           time, t
    O              t1
x constant ⇒            flipperworks.com


               body is stationary
x
               or velocity is zero
    A            B      x decreases at a constant
                        rate ⇒ body is moving
                        back towards O. Velocity
                        is negative, uniform and
                        greater in magnitude than
                            t
                        that of OA.
0   x increases at a constant rate
                     C
    ⇒ body is moving with uniform velocity
    x

O                        A
flipperworks.com


Examples of displacement-time graphs


(a)      s




                                   t

      uniform velocity (constant gradient)
flipperworks.com


Examples of displacement-time graphs


(b)      s
                             curve 1




                                  t
      Curve 1: increasing velocity
               (gradient increasing)
flipperworks.com


Examples of displacement-time graphs


(b)      s
                            curve 2




                                  t
      Curve 2: decreasing velocity
               (gradient decreasing)

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Kinematics 2011 part1

  • 2. flipperworks.com Dynam deals with the motion of bodies with ics reference to the forces that act on the system. Kinem atics deals with the motion of bodies without reference to the forces that act on the system. Two types of motion will be studied: 1. One dimensional motion - rectilinear motion 2. Two dimensional motion - projectile motion
  • 3. flipperworks.com 1. Definition of terms [I] Displacement s Displacem is the distance travelled ent along a specified direction. B Body travels along curved path from A to B. A It is a vector quantity. SI unit: m etre, m
  • 4. flipperworks.com [II] Speed v Speed is the rate of change of distance. It is a scalar quantity. SI unit: m s-1 average speed < v > = total distance covered total time taken A body that travels equal distances in equal intervals of time is said to be moving with c o ns ta nt or unifo rm speed.
  • 5. flipperworks.com Estimates of speeds (in m s-1) walking 1.5 sprinter 10 Speed limit 25 [ie. 90 km h-1] Jet plane 250 Sound (in air) 330 Light (in vacuum) 3.00 × 108
  • 6. flipperworks.com [III] Velocity v Velocity is the rate of change of displacem ent. It is a vector quantity. SI unit: m s-1 ds v= dt average velocity rate of total displaceme nt change <v > = total time taken
  • 7. flipperworks.com A body which travels equal distances in the same direction in equal intervals of time is said to be moving with c o ns ta nt or unifo rm velocity. < speed > may not always be equal to < velocity >
  • 8. flipperworks.com Example 1: (a) total distance = 5.0 + 5.0 = 10.0 km (b) displacement = 5.0 2 + 5.0 2 N = 7.1 km 5.0 km θ 5 .0 tan θ = = 1 .0 5.0 km 5 .0 ⇒ θ = 45o Displacement is 7.1 km at a bearing of 135 o or S45oE.
  • 9. flipperworks.com 10.0 (c) <speed> = 1 .0 = 10 km h-1 7 .1 (d) <velocity> = 1.0 = 7.1 km h-1 at a bearing of 135o
  • 10. flipperworks.com [IV] Acceleration a Acceleration is the rate of change of velocity. It is a vector q ua ntity . dv a= SI unit: m s-2 dt A change in velocity can be caused by: (i) a change in its magnitude only, (ii) a change in its direction only, or (iii) a change in both its magnitude and direction.
  • 11. flipperworks.com A body which travels with equal increase in speed in the same direction in equal intervals of time is said to be moving with c o ns ta nt or unifo rm acceleration. acceleration = 0 ⇒ constant velocity But when velocity = 0 at one instant, acceleration need not be zero. (Think of a situation where this can happen.)
  • 12. flipperworks.com Retardation or deceleration describes a situation when magnitude of velocity decreases with time i.e. body is slowing down. This occurs when acceleration and velocity act in opposite directions. In the next slide, observe the directions of the velocity and acceleration when a body travels faster and when it slows down.
  • 13. flipperworks.com Free fall K A body is said to be in fre e fa ll if the only i force acting on it is the gravitational force e due to the Earth. m The downward acceleration of such a body a is known as a c c e le ra tio n d ue to g ra vity . t g = 9.81 m s-2 c (assumed to be constant near Earth’s surface) s True free fall only occurs in vacuum. All bodies falling freely will have this constant acceleration regardless of their masses.
  • 14. flipperworks.com 2 Graphical Representation of Motion K 2.1 Displacement-time graph i n displacement , s average velocity between O and A = S1 e t1 s1 m A (gradient of the line a passing through O & A) t s time, t O t1
  • 15. flipperworks.com displacement , s slope at A = s1 A ds instantaneous velocity at A ds dt = dt time, t O t1
  • 16. x constant ⇒ flipperworks.com body is stationary x or velocity is zero A B x decreases at a constant rate ⇒ body is moving back towards O. Velocity is negative, uniform and greater in magnitude than t that of OA. 0 x increases at a constant rate C ⇒ body is moving with uniform velocity x O A
  • 17. flipperworks.com Examples of displacement-time graphs (a) s t uniform velocity (constant gradient)
  • 18. flipperworks.com Examples of displacement-time graphs (b) s curve 1 t Curve 1: increasing velocity (gradient increasing)
  • 19. flipperworks.com Examples of displacement-time graphs (b) s curve 2 t Curve 2: decreasing velocity (gradient decreasing)