SlideShare a Scribd company logo
1 of 84
Download to read offline
Integrating Functions of Time

x



    1 2 3 4   t
Integrating Functions of Time

x
                                           4
                  change in displacement   xdt
                                             
                                           0

    1 2 3 4   t
Integrating Functions of Time

x
                                               4
                    change in displacement   xdt
                                               
                                               0

    1 2 3 4   t                         1      3       4
                  change in distance   xdt   xdt   xdt
                                                       
                                        0      1       3
Integrating Functions of Time

x
                                                4
                     change in displacement   xdt
                                                
                                                0

     1 2 3 4   t                         1      3       4
                   change in distance   xdt   xdt   xdt
                                                        
                                         0      1       3





x



     1 2 3 4   t
Integrating Functions of Time

x
                                                 4
                     change in displacement   xdt
                                                
                                                 0

     1 2 3 4   t                         1       3      4
                   change in distance   xdt   xdt   xdt
                                                        
                                         0       1      3





x
                                             4
                      change in velocity   dt
                                             x
                                             0

     1 2 3 4   t
Integrating Functions of Time

x
                                                     4
                     change in displacement   xdt
                                                
                                                     0

     1 2 3 4   t                         1           3       4
                   change in distance   xdt   xdt   xdt
                                                        
                                         0           1       3





x
                                                 4
                      change in velocity   dt
                                             x
                                                 0

     1 2 3 4   t                             2           4
                     change in speed    dt   dt
                                           x        x
                                             0           2
Derivative Graphs
  Function     1st derivative   2nd derivative
displacement       velocity      acceleration
Derivative Graphs
   Function        1st derivative   2nd derivative
 displacement          velocity      acceleration
stationary point    x intercept
Derivative Graphs
   Function        1st derivative     2nd derivative
 displacement          velocity        acceleration
stationary point    x intercept
inflection point   stationary point     x intercept
Derivative Graphs
   Function        1st derivative     2nd derivative
 displacement          velocity        acceleration
stationary point    x intercept
inflection point   stationary point     x intercept
  increasing         positive
Derivative Graphs
   Function        1st derivative     2nd derivative
 displacement          velocity        acceleration
stationary point    x intercept
inflection point   stationary point     x intercept
  increasing         positive
  decreasing         negative
Derivative Graphs
   Function        1st derivative     2nd derivative
 displacement          velocity        acceleration
stationary point    x intercept
inflection point   stationary point     x intercept
  increasing         positive
  decreasing         negative
  concave up         increasing          positive
Derivative Graphs
   Function        1st derivative     2nd derivative
 displacement          velocity        acceleration
stationary point    x intercept
inflection point   stationary point     x intercept
  increasing         positive
  decreasing         negative
  concave up         increasing          positive
concave down         decreasing          negative
graph type   integrate   differentiate
graph type        integrate     differentiate
horizontal line   oblique line      x axis
graph type        integrate     differentiate
horizontal line   oblique line       x axis
oblique line       parabola      horizontal line
graph type            integrate           differentiate
horizontal line      oblique line              x axis
oblique line           parabola            horizontal line

  parabola              cubic               oblique line
                  inflects at turning pt
graph type             integrate           differentiate
horizontal line        oblique line             x axis
oblique line            parabola            horizontal line

  parabola               cubic               oblique line
                   inflects at turning pt
Remember:
• integration = area
graph type             integrate              differentiate
horizontal line        oblique line                x axis
oblique line            parabola               horizontal line

  parabola               cubic                  oblique line
                   inflects at turning pt
Remember:
• integration = area
• on a velocity graph, total area = distance
                       total integral = displacement
graph type               integrate               differentiate
horizontal line         oblique line                  x axis
oblique line              parabola               horizontal line

  parabola                 cubic                   oblique line
                    inflects at turning pt
Remember:
• integration = area
• on a velocity graph, total area = distance
                       total integral = displacement
• on an acceleration graph, total area = speed
                              total integral = velocity
(ii) 2003 HSC Question 7b)
    The velocity of a particle is given by v  2  4 cos t for 0  t  2 ,
    where v is measured in metres per second and t is measured in seconds
  (i) At what times during this period is the particle at rest?
(ii) 2003 HSC Question 7b)
    The velocity of a particle is given by v  2  4 cos t for 0  t  2 ,
    where v is measured in metres per second and t is measured in seconds
  (i) At what times during this period is the particle at rest?
             v0
     2  4cos t  0
                  1
          cos t 
                  2
(ii) 2003 HSC Question 7b)
    The velocity of a particle is given by v  2  4 cos t for 0  t  2 ,
    where v is measured in metres per second and t is measured in seconds
  (i) At what times during this period is the particle at rest?
             v0             Q1, 4
     2  4cos t  0                1
                  1        cos  
          cos t                   2
                  2                
                               
                                    3
(ii) 2003 HSC Question 7b)
    The velocity of a particle is given by v  2  4 cos t for 0  t  2 ,
    where v is measured in metres per second and t is measured in seconds
  (i) At what times during this period is the particle at rest?
             v0               Q1, 4             t   , 2  
     2  4cos t  0                  1                5
                  1          cos               t ,
          cos t                     2                3 3
                  2                  
                                 
                                     3
                                                          5
   particle is at rest after    seconds and again after       seconds
                              3                             3
(ii) 2003 HSC Question 7b)
    The velocity of a particle is given by v  2  4 cos t for 0  t  2 ,
    where v is measured in metres per second and t is measured in seconds
  (i) At what times during this period is the particle at rest?
             v0                Q1, 4             t   , 2  
     2  4cos t  0                   1                5
                  1           cos               t ,
          cos t                      2               3 3
                  2                   
                                  
                                      3
                                                          5
    particle is at rest after    seconds and again after      seconds
                               3                            3
  (ii) What is the maximum velocity of the particle during this period?
(ii) 2003 HSC Question 7b)
    The velocity of a particle is given by v  2  4 cos t for 0  t  2 ,
    where v is measured in metres per second and t is measured in seconds
  (i) At what times during this period is the particle at rest?
             v0                Q1, 4             t   , 2  
     2  4cos t  0                   1                5
                  1           cos               t ,
          cos t                      2               3 3
                  2                   
                                  
                                      3
                                                          5
    particle is at rest after    seconds and again after      seconds
                               3                            3
  (ii) What is the maximum velocity of the particle during this period?
                         4  4 cos t  4
                         2  2  4 cos t  6
                    maximum velocity is 6 m/s
(iii) Sketch the graph of v as a function of t for 0  t  2
(iii) Sketch the graph of v as a function of t for 0  t  2
                                         2                     2
       amplitude  4 units      period            divisions 
       shift  2 units                   1                      4
                                        2                     
       flip upside down                                       
                                                                2
(iii) Sketch the graph of v as a function of t for 0  t  2
                                         2                     2
       amplitude  4 units      period            divisions 
       shift  2 units                   1                      4
                                        2                     
       flip upside down                                       
                                                                2
                v
              6
              5
              4
               3
              2
              1


              -1
                                             3         2   t
              -2
                          2                     2
(iii) Sketch the graph of v as a function of t for 0  t  2
                                         2                     2
       amplitude  4 units      period            divisions 
       shift  2 units                   1                      4
                                        2                     
       flip upside down                                       
                                                                2
                v
              6
              5
              4
               3
              2
              1


              -1
                                             3         2   t
              -2
                          2                     2
(iii) Sketch the graph of v as a function of t for 0  t  2
                                         2                     2
       amplitude  4 units      period            divisions 
       shift  2 units                   1                      4
                                        2                     
       flip upside down                                       
                                                                2
                v
              6
              5
              4
               3
              2
              1


              -1
                                             3         2   t
              -2
                          2                     2
(iii) Sketch the graph of v as a function of t for 0  t  2
                                         2                     2
       amplitude  4 units      period            divisions 
       shift  2 units                   1                      4
                                        2                     
       flip upside down                                       
                                                                2
                v
              6
              5
              4
               3
              2
              1


              -1
                                             3         2   t
              -2
                          2                     2
(iii) Sketch the graph of v as a function of t for 0  t  2
                                         2                     2
       amplitude  4 units      period            divisions 
       shift  2 units                   1                      4
                                        2                     
       flip upside down                                       
                                                                2
                v
              6
              5                                v  2  4 cos t
              4
               3
              2
              1


              -1
                                             3         2     t
              -2
                          2                     2
(iv) Calculate the total distance travelled by the particle between t = 0
     and t = 
(iv) Calculate the total distance travelled by the particle between t = 0
     and t = 
             
               3                     
distance =    2  4 cos t  dt    2  4 cos t  dt
               0                     
                                     3
(iv) Calculate the total distance travelled by the particle between t = 0
     and t = 
             
               3                      
distance =    2  4 cos t  dt    2  4 cos t  dt
               0                      

           =  2t  4sin t    2t 3 4sin t 
                            0                  

                            3                   3
(iv) Calculate the total distance travelled by the particle between t = 0
     and t = 
             
               3                      
distance =    2  4 cos t  dt    2  4 cos t  dt
               0                      

           =  2t  4sin t    2t 3 4sin t 
                            0                  

                            3                   3

                                              2  4sin  
           =  0  0    2  4sin    2              
                                               3        3
                    2 4 3 
           =2  2        
                     3   2 

                  2
           =4 3     metres
                   3
(iii) 2004 HSC Question 9b)
      A particle moves along the x-axis. Initially it is at rest at the origin.
      The graph shows the acceleration, a, of the particle as a function of
      time t for 0  t  5




(i) Write down the time at which the velocity of the particle is a maximum
(iii) 2004 HSC Question 9b)
      A particle moves along the x-axis. Initially it is at rest at the origin.
      The graph shows the acceleration, a, of the particle as a function of
      time t for 0  t  5




(i) Write down the time at which the velocity of the particle is a maximum
   v   adt

        adt is a maximum when t  2
(iii) 2004 HSC Question 9b)
      A particle moves along the x-axis. Initially it is at rest at the origin.
      The graph shows the acceleration, a, of the particle as a function of
      time t for 0  t  5




(i) Write down the time at which the velocity of the particle is a maximum
                                                                     dv
    v   adt                        OR     v is a maximum when         0
                                                                     dt
         adt is a maximum when t  2
(iii) 2004 HSC Question 9b)
      A particle moves along the x-axis. Initially it is at rest at the origin.
      The graph shows the acceleration, a, of the particle as a function of
      time t for 0  t  5




(i) Write down the time at which the velocity of the particle is a maximum
                                                                     dv
    v   adt                        OR     v is a maximum when         0
                                                                     dt
         adt is a maximum when t  2
               velocity is a maximum when t  2 seconds
(ii) At what time during the interval 0  t  5 is the particle furthest
     from the origin? Give reasons for your answer.
(ii) At what time during the interval 0  t  5 is the particle furthest
     from the origin? Give reasons for your answer.




    Question is asking, “when is displacement a maximum?”
                                        dx
                 x is a maximum when       0
                                        dt
(ii) At what time during the interval 0  t  5 is the particle furthest
     from the origin? Give reasons for your answer.




    Question is asking, “when is displacement a maximum?”
                                        dx
                 x is a maximum when       0
                                        dt
                 But v   adt
                   We must solve  adt  0
(ii) At what time during the interval 0  t  5 is the particle furthest
     from the origin? Give reasons for your answer.




    Question is asking, “when is displacement a maximum?”
                                        dx
                 x is a maximum when       0
                                        dt
                 But v   adt
                  We must solve  adt  0
           i.e. when is area above the axis = area below
            By symmetry this would be at t = 4
        particle is furthest from the origin at t  4 seconds
(iv) 2007 HSC Question 10a)                                          dx
    An object is moving on the x-axis. The graph shows the velocity, ,
                                                                     dt
    of the object, as a function of t.
    The coordinates of the points shown on the graph are A(2,1), B(4,5),
    C(5,0) and D(6,–5). The velocity is constant for t  6




(i) Using Simpson’s rule, estimate the distance travelled between t = 0
    and t = 4
(iv) 2007 HSC Question 10a)                                          dx
    An object is moving on the x-axis. The graph shows the velocity, ,
                                                                     dt
    of the object, as a function of t.
    The coordinates of the points shown on the graph are A(2,1), B(4,5),
    C(5,0) and D(6,–5). The velocity is constant for t  6




(i) Using Simpson’s rule, estimate the distance travelled between t = 0
    and t = 4                              h
                                distance   y0  4 yodd  2 yeven  yn 
                                            3
(iv) 2007 HSC Question 10a)                                          dx
    An object is moving on the x-axis. The graph shows the velocity, ,
                                                                     dt
    of the object, as a function of t.
    The coordinates of the points shown on the graph are A(2,1), B(4,5),
    C(5,0) and D(6,–5). The velocity is constant for t  6




(i) Using Simpson’s rule, estimate the distance travelled between t = 0
    and t = 4                              h
                                distance   y0  4 yodd  2 yeven  yn 
                                            3
    t      0      2      4
    v      0      1      5
(iv) 2007 HSC Question 10a)                                          dx
    An object is moving on the x-axis. The graph shows the velocity, ,
                                                                     dt
    of the object, as a function of t.
    The coordinates of the points shown on the graph are A(2,1), B(4,5),
    C(5,0) and D(6,–5). The velocity is constant for t  6




(i) Using Simpson’s rule, estimate the distance travelled between t = 0
    and t = 4                              h
                                distance   y0  4 yodd  2 yeven  yn 
                                            3
            1   4      1
    t      0      2      4
    v      0      1      5
(iv) 2007 HSC Question 10a)                                          dx
    An object is moving on the x-axis. The graph shows the velocity, ,
                                                                     dt
    of the object, as a function of t.
    The coordinates of the points shown on the graph are A(2,1), B(4,5),
    C(5,0) and D(6,–5). The velocity is constant for t  6




(i) Using Simpson’s rule, estimate the distance travelled between t = 0
    and t = 4                              h
                                distance   y0  4 yodd  2 yeven  yn 
                                            3
            1   4      1                    2
                                          0  4 1  5
     t      0   2      4                    3
     v      0   1      5
                                          6 metres
(ii) The object is initially at the origin. During which time(s) is the
     displacement decreasing?
(ii) The object is initially at the origin. During which time(s) is the
     displacement decreasing?
                                               dx
                        x is decreasing when       0
                                                dt
             displacement is decreasing when t  5 seconds
(ii) The object is initially at the origin. During which time(s) is the
     displacement decreasing?
                                               dx
                        x is decreasing when       0
                                                dt
             displacement is decreasing when t  5 seconds
(iii) Estimate the time at which the object returns to the origin. Justify
      your answer.
(ii) The object is initially at the origin. During which time(s) is the
     displacement decreasing?
                                               dx
                        x is decreasing when       0
                                                dt
             displacement is decreasing when t  5 seconds
(iii) Estimate the time at which the object returns to the origin. Justify
      your answer.
      Question is asking, “when is displacement = 0?”
(ii) The object is initially at the origin. During which time(s) is the
     displacement decreasing?
                                               dx
                        x is decreasing when       0
                                                dt
             displacement is decreasing when t  5 seconds
(iii) Estimate the time at which the object returns to the origin. Justify
      your answer.
      Question is asking, “when is displacement = 0?”
                     But x   vdt
          We must solve  vdt  0
(ii) The object is initially at the origin. During which time(s) is the
     displacement decreasing?
                                               dx
                        x is decreasing when       0
                                                dt
             displacement is decreasing when t  5 seconds
(iii) Estimate the time at which the object returns to the origin. Justify
      your answer.
      Question is asking, “when is displacement = 0?”
                     But x   vdt
          We must solve  vdt  0

 i.e. when is area above the axis = area below
(ii) The object is initially at the origin. During which time(s) is the
     displacement decreasing?
                                               dx
                        x is decreasing when       0
                                                dt
             displacement is decreasing when t  5 seconds
(iii) Estimate the time at which the object returns to the origin. Justify
      your answer.
      Question is asking, “when is displacement = 0?”
                     But x   vdt
          We must solve  vdt  0

 i.e. when is area above the axis = area below
 By symmetry, area from t = 4 to 5 equals area
 from t = 5 to 6
(ii) The object is initially at the origin. During which time(s) is the
     displacement decreasing?
                                               dx
                        x is decreasing when       0
                                                dt
             displacement is decreasing when t  5 seconds
(iii) Estimate the time at which the object returns to the origin. Justify
      your answer.
      Question is asking, “when is displacement = 0?”
                     But x   vdt
          We must solve  vdt  0

 i.e. when is area above the axis = area below
 By symmetry, area from t = 4 to 5 equals area
 from t = 5 to 6
  In part (i) we estimated area from t = 0 to 4 to be 6,
(ii) The object is initially at the origin. During which time(s) is the
     displacement decreasing?
                                               dx
                        x is decreasing when       0
                                                dt
             displacement is decreasing when t  5 seconds
(iii) Estimate the time at which the object returns to the origin. Justify
      your answer.
      Question is asking, “when is displacement = 0?”
                     But x   vdt
          We must solve  vdt  0

 i.e. when is area above the axis = area below
 By symmetry, area from t = 4 to 5 equals area                        A4
 from t = 5 to 6
  In part (i) we estimated area from t = 0 to 4 to be 6,
   A4  6
(ii) The object is initially at the origin. During which time(s) is the
     displacement decreasing?
                                               dx
                        x is decreasing when       0
                                                dt
             displacement is decreasing when t  5 seconds
(iii) Estimate the time at which the object returns to the origin. Justify
      your answer.
      Question is asking, “when is displacement = 0?”
                     But x   vdt
          We must solve  vdt  0
                                                                          a
 i.e. when is area above the axis = area below
 By symmetry, area from t = 4 to 5 equals area                        A4      5

 from t = 5 to 6
  In part (i) we estimated area from t = 0 to 4 to be 6,
   A4  6          a  1.2
     5a  6
(ii) The object is initially at the origin. During which time(s) is the
     displacement decreasing?
                                               dx
                        x is decreasing when       0
                                                dt
             displacement is decreasing when t  5 seconds
(iii) Estimate the time at which the object returns to the origin. Justify
      your answer.
      Question is asking, “when is displacement = 0?”
                     But x   vdt
          We must solve  vdt  0
                                                                          a
 i.e. when is area above the axis = area below
 By symmetry, area from t = 4 to 5 equals area                       A4 5
 from t = 5 to 6
  In part (i) we estimated area from t = 0 to 4 to be 6,
   A4  6          a  1.2
     5a  6           particle returns to the origin when t  7.2 seconds
(iv) Sketch the displacement, x, as a function of time.
(iv) Sketch the displacement, x, as a function of time.




  x
8.5

 6




        2     4     6     8     t
(iv) Sketch the displacement, x, as a function of time.
                                           object is initially at the origin




  x
8.5

 6




        2     4     6     8     t
(iv) Sketch the displacement, x, as a function of time.
                                           object is initially at the origin
                                           when t = 4, x = 6




  x
8.5

 6




        2     4     6     8     t
(iv) Sketch the displacement, x, as a function of time.
                                           object is initially at the origin
                                           when t = 4, x = 6
                                         by symmetry of areas t = 6, x = 6




  x
8.5

 6




        2     4     6     8     t
(iv) Sketch the displacement, x, as a function of time.
                                           object is initially at the origin
                                           when t = 4, x = 6
                                         by symmetry of areas t = 6, x = 6
                                         Area of triangle = 2.5
                                           when t  5, x  8.5

  x
8.5

 6




        2     4     6     8     t
(iv) Sketch the displacement, x, as a function of time.
                                           object is initially at the origin
                                           when t = 4, x = 6
                                          by symmetry of areas t = 6, x = 6
                                         Area of triangle = 2.5
                                           when t  5, x  8.5
                                          returns to x = 0 when t = 7.2
  x
8.5

 6




        2     4     6 7.2 8     t
(iv) Sketch the displacement, x, as a function of time.
                                           object is initially at the origin
                                           when t = 4, x = 6
                                          by symmetry of areas t = 6, x = 6
                                         Area of triangle = 2.5
                                           when t  5, x  8.5
                                          returns to x = 0 when t = 7.2
  x
                                         v is steeper between t = 2 and 4
8.5
                                         than between t = 0 and 2
 6                                        particle covers more distance
                                           between t  2 and 4


        2     4     6 7.2 8     t
(iv) Sketch the displacement, x, as a function of time.
                                           object is initially at the origin
                                           when t = 4, x = 6
                                          by symmetry of areas t = 6, x = 6
                                         Area of triangle = 2.5
                                           when t  5, x  8.5
                                          returns to x = 0 when t = 7.2
  x
                                         v is steeper between t = 2 and 4
8.5
                                         than between t = 0 and 2
 6                                        particle covers more distance
                                           between t  2 and 4
                                           when t > 6, v is constant
                                t         when t  6, x is a straight line
        2     4     6 7.2 8
(iv) Sketch the displacement, x, as a function of time.
                                           object is initially at the origin
                                           when t = 4, x = 6
                                          by symmetry of areas t = 6, x = 6
                                         Area of triangle = 2.5
                                           when t  5, x  8.5
                                          returns to x = 0 when t = 7.2
  x
                                         v is steeper between t = 2 and 4
8.5
                                         than between t = 0 and 2
 6                                        particle covers more distance
                                           between t  2 and 4
                                           when t > 6, v is constant
                                t         when t  6, x is a straight line
        2     4     6 7.2 8
(v) 2005 HSC Question 7b)




                                     dx
 The graph shows the velocity, dt , of a particle as a function of time.
 Initially the particle is at the origin.
(i) At what time is the displacement, x, from the origin a maximum?
(v) 2005 HSC Question 7b)




                                     dx
 The graph shows the velocity, dt , of a particle as a function of time.
 Initially the particle is at the origin.
(i) At what time is the displacement, x, from the origin a maximum?

  Displacement is a maximum when area is most positive, also when
  velocity is zero
                         i.e. when t = 2
(ii) At what time does the particle return to the origin? Justify
     your answer
(ii) At what time does the particle return to the origin? Justify
     your answer




    Question is asking, “when is displacement = 0?”
     i.e. when is area above the axis = area below?
(ii) At what time does the particle return to the origin? Justify
     your answer


                         2 a       w

                               a   2


    Question is asking, “when is displacement = 0?”
     i.e. when is area above the axis = area below?
(ii) At what time does the particle return to the origin? Justify
     your answer


                         2 a        w

                                a   2


    Question is asking, “when is displacement = 0?”
     i.e. when is area above the axis = area below?
                               2w = 2
                                w=1
(ii) At what time does the particle return to the origin? Justify
     your answer


                         2 a        w

                                a   2


    Question is asking, “when is displacement = 0?”
     i.e. when is area above the axis = area below?
                               2w = 2
                                w=1
             Returns to the origin after 4 seconds
d 2x
 (iii) Draw a sketch of the acceleration, 2 , as afunction of
                                         dt
       time for 0  t  6




d 2x
dt 2




       1   2   3   5   6   t
d 2x
 (iii) Draw a sketch of the acceleration, 2 , as afunction of
                                         dt
       time for 0  t  6                     differentiate a horizontal line
                                              you get the xaxis




d 2x
dt 2




       1   2   3   5   6     t
d 2x
 (iii) Draw a sketch of the acceleration, 2 , as afunction of
                                         dt
       time for 0  t  6                     differentiate a horizontal line
                                              you get the xaxis

                                              from 1 to 3 we have a cubic,
                                              inflects at 2, and is decreasing
                                       differentiate, you get a parabola,
                                       stationary at 2, it is below the x axis
d 2x
dt 2




       1   2   3   5   6     t
d 2x
 (iii) Draw a sketch of the acceleration, 2 , as afunction of
                                         dt
       time for 0  t  6                     differentiate a horizontal line
                                              you get the xaxis

                                              from 1 to 3 we have a cubic,
                                              inflects at 2, and is decreasing
                                       differentiate, you get a parabola,
                                       stationary at 2, it is below the x axis
d 2x
dt 2
                                       from 5 to 6 is a cubic, inflects at 6
                                       and is increasing (using symmetry)

                                        differentiate, you get a parabola
       1   2   3   5   6     t
                                        stationary at 6, it is above the x axis
d 2x
 (iii) Draw a sketch of the acceleration, 2 , as afunction of
                                         dt
       time for 0  t  6                     differentiate a horizontal line
                                              you get the xaxis

                                              from 1 to 3 we have a cubic,
                                              inflects at 2, and is decreasing
                                       differentiate, you get a parabola,
                                       stationary at 2, it is below the x axis
d 2x
dt 2
                                       from 5 to 6 is a cubic, inflects at 6
                                       and is increasing (using symmetry)

                                        differentiate, you get a parabola
       1   2   3   5   6     t
                                        stationary at 6, it is above the x axis
Exercise 3C; 1 ace etc, 2 ace etc, 4a, 7ab(i), 8, 9a, 10, 13, 15, 16, 18

More Related Content

What's hot

MCQMC 2020 talk: Importance Sampling for a Robust and Efficient Multilevel Mo...
MCQMC 2020 talk: Importance Sampling for a Robust and Efficient Multilevel Mo...MCQMC 2020 talk: Importance Sampling for a Robust and Efficient Multilevel Mo...
MCQMC 2020 talk: Importance Sampling for a Robust and Efficient Multilevel Mo...Chiheb Ben Hammouda
 
On gradient Ricci solitons
On gradient Ricci solitonsOn gradient Ricci solitons
On gradient Ricci solitonsmnlfdzlpz
 
4831603 physics-formula-list-form-4
4831603 physics-formula-list-form-44831603 physics-formula-list-form-4
4831603 physics-formula-list-form-4hongtee82
 
On estimating the integrated co volatility using
On estimating the integrated co volatility usingOn estimating the integrated co volatility using
On estimating the integrated co volatility usingkkislas
 
FoG 3.3 angle addition postulate
FoG 3.3 angle addition postulateFoG 3.3 angle addition postulate
FoG 3.3 angle addition postulateejfischer
 
Avoidance of Microstructural Heterogeneities by Hot Rolling Design in Thin Sl...
Avoidance of Microstructural Heterogeneities by Hot Rolling Design in Thin Sl...Avoidance of Microstructural Heterogeneities by Hot Rolling Design in Thin Sl...
Avoidance of Microstructural Heterogeneities by Hot Rolling Design in Thin Sl...Pello Uranga
 
A current perspectives of corrected operator splitting (os) for systems
A current perspectives of corrected operator splitting (os) for systemsA current perspectives of corrected operator splitting (os) for systems
A current perspectives of corrected operator splitting (os) for systemsAlexander Decker
 
Discrete Fourier Transform
Discrete Fourier TransformDiscrete Fourier Transform
Discrete Fourier TransformShahryar Ali
 
Modern features-part-1-detectors
Modern features-part-1-detectorsModern features-part-1-detectors
Modern features-part-1-detectorszukun
 
Physics formula list
Physics formula listPhysics formula list
Physics formula listJSlinkyNY
 
WAVELET-PACKET-BASED ADAPTIVE ALGORITHM FOR SPARSE IMPULSE RESPONSE IDENTIFI...
WAVELET-PACKET-BASED ADAPTIVE ALGORITHM FOR  SPARSE IMPULSE RESPONSE IDENTIFI...WAVELET-PACKET-BASED ADAPTIVE ALGORITHM FOR  SPARSE IMPULSE RESPONSE IDENTIFI...
WAVELET-PACKET-BASED ADAPTIVE ALGORITHM FOR SPARSE IMPULSE RESPONSE IDENTIFI...bermudez_jcm
 
Insiders modeling london-2006
Insiders modeling london-2006Insiders modeling london-2006
Insiders modeling london-2006Victor Romanov
 
Summary of "A Universally-Truthful Approximation Scheme for Multi-unit Auction"
Summary of "A Universally-Truthful Approximation Scheme for Multi-unit Auction"Summary of "A Universally-Truthful Approximation Scheme for Multi-unit Auction"
Summary of "A Universally-Truthful Approximation Scheme for Multi-unit Auction"Thatchaphol Saranurak
 
Second Order Perturbations During Inflation Beyond Slow-roll
Second Order Perturbations During Inflation Beyond Slow-rollSecond Order Perturbations During Inflation Beyond Slow-roll
Second Order Perturbations During Inflation Beyond Slow-rollIan Huston
 
Hidden Markov Models
Hidden Markov ModelsHidden Markov Models
Hidden Markov ModelsVu Pham
 

What's hot (18)

Lec04
Lec04Lec04
Lec04
 
MCQMC 2020 talk: Importance Sampling for a Robust and Efficient Multilevel Mo...
MCQMC 2020 talk: Importance Sampling for a Robust and Efficient Multilevel Mo...MCQMC 2020 talk: Importance Sampling for a Robust and Efficient Multilevel Mo...
MCQMC 2020 talk: Importance Sampling for a Robust and Efficient Multilevel Mo...
 
On gradient Ricci solitons
On gradient Ricci solitonsOn gradient Ricci solitons
On gradient Ricci solitons
 
4831603 physics-formula-list-form-4
4831603 physics-formula-list-form-44831603 physics-formula-list-form-4
4831603 physics-formula-list-form-4
 
On estimating the integrated co volatility using
On estimating the integrated co volatility usingOn estimating the integrated co volatility using
On estimating the integrated co volatility using
 
FoG 3.3 angle addition postulate
FoG 3.3 angle addition postulateFoG 3.3 angle addition postulate
FoG 3.3 angle addition postulate
 
Avoidance of Microstructural Heterogeneities by Hot Rolling Design in Thin Sl...
Avoidance of Microstructural Heterogeneities by Hot Rolling Design in Thin Sl...Avoidance of Microstructural Heterogeneities by Hot Rolling Design in Thin Sl...
Avoidance of Microstructural Heterogeneities by Hot Rolling Design in Thin Sl...
 
A current perspectives of corrected operator splitting (os) for systems
A current perspectives of corrected operator splitting (os) for systemsA current perspectives of corrected operator splitting (os) for systems
A current perspectives of corrected operator splitting (os) for systems
 
Discrete Fourier Transform
Discrete Fourier TransformDiscrete Fourier Transform
Discrete Fourier Transform
 
Modern features-part-1-detectors
Modern features-part-1-detectorsModern features-part-1-detectors
Modern features-part-1-detectors
 
Physics formula list
Physics formula listPhysics formula list
Physics formula list
 
WAVELET-PACKET-BASED ADAPTIVE ALGORITHM FOR SPARSE IMPULSE RESPONSE IDENTIFI...
WAVELET-PACKET-BASED ADAPTIVE ALGORITHM FOR  SPARSE IMPULSE RESPONSE IDENTIFI...WAVELET-PACKET-BASED ADAPTIVE ALGORITHM FOR  SPARSE IMPULSE RESPONSE IDENTIFI...
WAVELET-PACKET-BASED ADAPTIVE ALGORITHM FOR SPARSE IMPULSE RESPONSE IDENTIFI...
 
Insiders modeling london-2006
Insiders modeling london-2006Insiders modeling london-2006
Insiders modeling london-2006
 
Summary of "A Universally-Truthful Approximation Scheme for Multi-unit Auction"
Summary of "A Universally-Truthful Approximation Scheme for Multi-unit Auction"Summary of "A Universally-Truthful Approximation Scheme for Multi-unit Auction"
Summary of "A Universally-Truthful Approximation Scheme for Multi-unit Auction"
 
Second Order Perturbations During Inflation Beyond Slow-roll
Second Order Perturbations During Inflation Beyond Slow-rollSecond Order Perturbations During Inflation Beyond Slow-roll
Second Order Perturbations During Inflation Beyond Slow-roll
 
International Journal of Engineering Inventions (IJEI),
International Journal of Engineering Inventions (IJEI), International Journal of Engineering Inventions (IJEI),
International Journal of Engineering Inventions (IJEI),
 
Hidden Markov Models
Hidden Markov ModelsHidden Markov Models
Hidden Markov Models
 
San diego pres
San diego presSan diego pres
San diego pres
 

Similar to 12 x1 t04 06 integrating functions of time (2013)

1D graphs, kinematics, and calculus
1D graphs, kinematics, and calculus1D graphs, kinematics, and calculus
1D graphs, kinematics, and calculuscpphysics
 
Application of differentiation
Application of differentiationApplication of differentiation
Application of differentiationLily Maryati
 
[shaderx5] 4.2 Multisampling Extension for Gradient Shadow Maps
[shaderx5] 4.2 Multisampling Extension for Gradient Shadow Maps[shaderx5] 4.2 Multisampling Extension for Gradient Shadow Maps
[shaderx5] 4.2 Multisampling Extension for Gradient Shadow Maps종빈 오
 
Two dimensional geometric transformations
Two dimensional geometric transformationsTwo dimensional geometric transformations
Two dimensional geometric transformationsMohammad Sadiq
 
Geometric transformation cg
Geometric transformation cgGeometric transformation cg
Geometric transformation cgharinipriya1994
 
Kenimatics vector
Kenimatics vectorKenimatics vector
Kenimatics vectorohmed
 
Condition Monitoring Of Unsteadily Operating Equipment
Condition Monitoring Of Unsteadily Operating EquipmentCondition Monitoring Of Unsteadily Operating Equipment
Condition Monitoring Of Unsteadily Operating EquipmentJordan McBain
 
Composition Of Functions & Difference Quotient
Composition Of Functions & Difference QuotientComposition Of Functions & Difference Quotient
Composition Of Functions & Difference Quotientcpirie0607
 
Composition Of Functions & Difference Quotient
Composition Of Functions & Difference QuotientComposition Of Functions & Difference Quotient
Composition Of Functions & Difference Quotientcpirie0607
 
12 x1 t04 05 displacement, velocity, acceleration (2012)
12 x1 t04 05 displacement, velocity, acceleration (2012)12 x1 t04 05 displacement, velocity, acceleration (2012)
12 x1 t04 05 displacement, velocity, acceleration (2012)Nigel Simmons
 
12 x1 t04 05 displacement, velocity, acceleration (2013)
12 x1 t04 05 displacement, velocity, acceleration (2013)12 x1 t04 05 displacement, velocity, acceleration (2013)
12 x1 t04 05 displacement, velocity, acceleration (2013)Nigel Simmons
 

Similar to 12 x1 t04 06 integrating functions of time (2013) (14)

1D graphs, kinematics, and calculus
1D graphs, kinematics, and calculus1D graphs, kinematics, and calculus
1D graphs, kinematics, and calculus
 
Application of differentiation
Application of differentiationApplication of differentiation
Application of differentiation
 
[shaderx5] 4.2 Multisampling Extension for Gradient Shadow Maps
[shaderx5] 4.2 Multisampling Extension for Gradient Shadow Maps[shaderx5] 4.2 Multisampling Extension for Gradient Shadow Maps
[shaderx5] 4.2 Multisampling Extension for Gradient Shadow Maps
 
Two dimensional geometric transformations
Two dimensional geometric transformationsTwo dimensional geometric transformations
Two dimensional geometric transformations
 
Lecture 07
Lecture 07Lecture 07
Lecture 07
 
Geometric transformation cg
Geometric transformation cgGeometric transformation cg
Geometric transformation cg
 
Kenimatics vector
Kenimatics vectorKenimatics vector
Kenimatics vector
 
CRMS Calculus 2010 May 17, 2010
CRMS Calculus 2010 May 17, 2010CRMS Calculus 2010 May 17, 2010
CRMS Calculus 2010 May 17, 2010
 
Condition Monitoring Of Unsteadily Operating Equipment
Condition Monitoring Of Unsteadily Operating EquipmentCondition Monitoring Of Unsteadily Operating Equipment
Condition Monitoring Of Unsteadily Operating Equipment
 
Composition Of Functions & Difference Quotient
Composition Of Functions & Difference QuotientComposition Of Functions & Difference Quotient
Composition Of Functions & Difference Quotient
 
Composition Of Functions & Difference Quotient
Composition Of Functions & Difference QuotientComposition Of Functions & Difference Quotient
Composition Of Functions & Difference Quotient
 
Fourier transform
Fourier transformFourier transform
Fourier transform
 
12 x1 t04 05 displacement, velocity, acceleration (2012)
12 x1 t04 05 displacement, velocity, acceleration (2012)12 x1 t04 05 displacement, velocity, acceleration (2012)
12 x1 t04 05 displacement, velocity, acceleration (2012)
 
12 x1 t04 05 displacement, velocity, acceleration (2013)
12 x1 t04 05 displacement, velocity, acceleration (2013)12 x1 t04 05 displacement, velocity, acceleration (2013)
12 x1 t04 05 displacement, velocity, acceleration (2013)
 

More from Nigel Simmons

Goodbye slideshare UPDATE
Goodbye slideshare UPDATEGoodbye slideshare UPDATE
Goodbye slideshare UPDATENigel Simmons
 
12 x1 t02 02 integrating exponentials (2014)
12 x1 t02 02 integrating exponentials (2014)12 x1 t02 02 integrating exponentials (2014)
12 x1 t02 02 integrating exponentials (2014)Nigel Simmons
 
11 x1 t01 03 factorising (2014)
11 x1 t01 03 factorising (2014)11 x1 t01 03 factorising (2014)
11 x1 t01 03 factorising (2014)Nigel Simmons
 
11 x1 t01 02 binomial products (2014)
11 x1 t01 02 binomial products (2014)11 x1 t01 02 binomial products (2014)
11 x1 t01 02 binomial products (2014)Nigel Simmons
 
12 x1 t02 01 differentiating exponentials (2014)
12 x1 t02 01 differentiating exponentials (2014)12 x1 t02 01 differentiating exponentials (2014)
12 x1 t02 01 differentiating exponentials (2014)Nigel Simmons
 
11 x1 t01 01 algebra & indices (2014)
11 x1 t01 01 algebra & indices (2014)11 x1 t01 01 algebra & indices (2014)
11 x1 t01 01 algebra & indices (2014)Nigel Simmons
 
12 x1 t01 03 integrating derivative on function (2013)
12 x1 t01 03 integrating derivative on function (2013)12 x1 t01 03 integrating derivative on function (2013)
12 x1 t01 03 integrating derivative on function (2013)Nigel Simmons
 
12 x1 t01 02 differentiating logs (2013)
12 x1 t01 02 differentiating logs (2013)12 x1 t01 02 differentiating logs (2013)
12 x1 t01 02 differentiating logs (2013)Nigel Simmons
 
12 x1 t01 01 log laws (2013)
12 x1 t01 01 log laws (2013)12 x1 t01 01 log laws (2013)
12 x1 t01 01 log laws (2013)Nigel Simmons
 
X2 t02 04 forming polynomials (2013)
X2 t02 04 forming polynomials (2013)X2 t02 04 forming polynomials (2013)
X2 t02 04 forming polynomials (2013)Nigel Simmons
 
X2 t02 03 roots & coefficients (2013)
X2 t02 03 roots & coefficients (2013)X2 t02 03 roots & coefficients (2013)
X2 t02 03 roots & coefficients (2013)Nigel Simmons
 
X2 t02 02 multiple roots (2013)
X2 t02 02 multiple roots (2013)X2 t02 02 multiple roots (2013)
X2 t02 02 multiple roots (2013)Nigel Simmons
 
X2 t02 01 factorising complex expressions (2013)
X2 t02 01 factorising complex expressions (2013)X2 t02 01 factorising complex expressions (2013)
X2 t02 01 factorising complex expressions (2013)Nigel Simmons
 
11 x1 t16 07 approximations (2013)
11 x1 t16 07 approximations (2013)11 x1 t16 07 approximations (2013)
11 x1 t16 07 approximations (2013)Nigel Simmons
 
11 x1 t16 06 derivative times function (2013)
11 x1 t16 06 derivative times function (2013)11 x1 t16 06 derivative times function (2013)
11 x1 t16 06 derivative times function (2013)Nigel Simmons
 
11 x1 t16 05 volumes (2013)
11 x1 t16 05 volumes (2013)11 x1 t16 05 volumes (2013)
11 x1 t16 05 volumes (2013)Nigel Simmons
 
11 x1 t16 04 areas (2013)
11 x1 t16 04 areas (2013)11 x1 t16 04 areas (2013)
11 x1 t16 04 areas (2013)Nigel Simmons
 
11 x1 t16 03 indefinite integral (2013)
11 x1 t16 03 indefinite integral (2013)11 x1 t16 03 indefinite integral (2013)
11 x1 t16 03 indefinite integral (2013)Nigel Simmons
 
11 x1 t16 02 definite integral (2013)
11 x1 t16 02 definite integral (2013)11 x1 t16 02 definite integral (2013)
11 x1 t16 02 definite integral (2013)Nigel Simmons
 

More from Nigel Simmons (20)

Goodbye slideshare UPDATE
Goodbye slideshare UPDATEGoodbye slideshare UPDATE
Goodbye slideshare UPDATE
 
Goodbye slideshare
Goodbye slideshareGoodbye slideshare
Goodbye slideshare
 
12 x1 t02 02 integrating exponentials (2014)
12 x1 t02 02 integrating exponentials (2014)12 x1 t02 02 integrating exponentials (2014)
12 x1 t02 02 integrating exponentials (2014)
 
11 x1 t01 03 factorising (2014)
11 x1 t01 03 factorising (2014)11 x1 t01 03 factorising (2014)
11 x1 t01 03 factorising (2014)
 
11 x1 t01 02 binomial products (2014)
11 x1 t01 02 binomial products (2014)11 x1 t01 02 binomial products (2014)
11 x1 t01 02 binomial products (2014)
 
12 x1 t02 01 differentiating exponentials (2014)
12 x1 t02 01 differentiating exponentials (2014)12 x1 t02 01 differentiating exponentials (2014)
12 x1 t02 01 differentiating exponentials (2014)
 
11 x1 t01 01 algebra & indices (2014)
11 x1 t01 01 algebra & indices (2014)11 x1 t01 01 algebra & indices (2014)
11 x1 t01 01 algebra & indices (2014)
 
12 x1 t01 03 integrating derivative on function (2013)
12 x1 t01 03 integrating derivative on function (2013)12 x1 t01 03 integrating derivative on function (2013)
12 x1 t01 03 integrating derivative on function (2013)
 
12 x1 t01 02 differentiating logs (2013)
12 x1 t01 02 differentiating logs (2013)12 x1 t01 02 differentiating logs (2013)
12 x1 t01 02 differentiating logs (2013)
 
12 x1 t01 01 log laws (2013)
12 x1 t01 01 log laws (2013)12 x1 t01 01 log laws (2013)
12 x1 t01 01 log laws (2013)
 
X2 t02 04 forming polynomials (2013)
X2 t02 04 forming polynomials (2013)X2 t02 04 forming polynomials (2013)
X2 t02 04 forming polynomials (2013)
 
X2 t02 03 roots & coefficients (2013)
X2 t02 03 roots & coefficients (2013)X2 t02 03 roots & coefficients (2013)
X2 t02 03 roots & coefficients (2013)
 
X2 t02 02 multiple roots (2013)
X2 t02 02 multiple roots (2013)X2 t02 02 multiple roots (2013)
X2 t02 02 multiple roots (2013)
 
X2 t02 01 factorising complex expressions (2013)
X2 t02 01 factorising complex expressions (2013)X2 t02 01 factorising complex expressions (2013)
X2 t02 01 factorising complex expressions (2013)
 
11 x1 t16 07 approximations (2013)
11 x1 t16 07 approximations (2013)11 x1 t16 07 approximations (2013)
11 x1 t16 07 approximations (2013)
 
11 x1 t16 06 derivative times function (2013)
11 x1 t16 06 derivative times function (2013)11 x1 t16 06 derivative times function (2013)
11 x1 t16 06 derivative times function (2013)
 
11 x1 t16 05 volumes (2013)
11 x1 t16 05 volumes (2013)11 x1 t16 05 volumes (2013)
11 x1 t16 05 volumes (2013)
 
11 x1 t16 04 areas (2013)
11 x1 t16 04 areas (2013)11 x1 t16 04 areas (2013)
11 x1 t16 04 areas (2013)
 
11 x1 t16 03 indefinite integral (2013)
11 x1 t16 03 indefinite integral (2013)11 x1 t16 03 indefinite integral (2013)
11 x1 t16 03 indefinite integral (2013)
 
11 x1 t16 02 definite integral (2013)
11 x1 t16 02 definite integral (2013)11 x1 t16 02 definite integral (2013)
11 x1 t16 02 definite integral (2013)
 

Recently uploaded

How to Configure Email Server in Odoo 17
How to Configure Email Server in Odoo 17How to Configure Email Server in Odoo 17
How to Configure Email Server in Odoo 17Celine George
 
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️9953056974 Low Rate Call Girls In Saket, Delhi NCR
 
DATA STRUCTURE AND ALGORITHM for beginners
DATA STRUCTURE AND ALGORITHM for beginnersDATA STRUCTURE AND ALGORITHM for beginners
DATA STRUCTURE AND ALGORITHM for beginnersSabitha Banu
 
Earth Day Presentation wow hello nice great
Earth Day Presentation wow hello nice greatEarth Day Presentation wow hello nice great
Earth Day Presentation wow hello nice greatYousafMalik24
 
Difference Between Search & Browse Methods in Odoo 17
Difference Between Search & Browse Methods in Odoo 17Difference Between Search & Browse Methods in Odoo 17
Difference Between Search & Browse Methods in Odoo 17Celine George
 
Field Attribute Index Feature in Odoo 17
Field Attribute Index Feature in Odoo 17Field Attribute Index Feature in Odoo 17
Field Attribute Index Feature in Odoo 17Celine George
 
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdf
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdfFraming an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdf
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdfUjwalaBharambe
 
EPANDING THE CONTENT OF AN OUTLINE using notes.pptx
EPANDING THE CONTENT OF AN OUTLINE using notes.pptxEPANDING THE CONTENT OF AN OUTLINE using notes.pptx
EPANDING THE CONTENT OF AN OUTLINE using notes.pptxRaymartEstabillo3
 
Procuring digital preservation CAN be quick and painless with our new dynamic...
Procuring digital preservation CAN be quick and painless with our new dynamic...Procuring digital preservation CAN be quick and painless with our new dynamic...
Procuring digital preservation CAN be quick and painless with our new dynamic...Jisc
 
Crayon Activity Handout For the Crayon A
Crayon Activity Handout For the Crayon ACrayon Activity Handout For the Crayon A
Crayon Activity Handout For the Crayon AUnboundStockton
 
How to do quick user assign in kanban in Odoo 17 ERP
How to do quick user assign in kanban in Odoo 17 ERPHow to do quick user assign in kanban in Odoo 17 ERP
How to do quick user assign in kanban in Odoo 17 ERPCeline George
 
Solving Puzzles Benefits Everyone (English).pptx
Solving Puzzles Benefits Everyone (English).pptxSolving Puzzles Benefits Everyone (English).pptx
Solving Puzzles Benefits Everyone (English).pptxOH TEIK BIN
 
Romantic Opera MUSIC FOR GRADE NINE pptx
Romantic Opera MUSIC FOR GRADE NINE pptxRomantic Opera MUSIC FOR GRADE NINE pptx
Romantic Opera MUSIC FOR GRADE NINE pptxsqpmdrvczh
 
ENGLISH6-Q4-W3.pptxqurter our high choom
ENGLISH6-Q4-W3.pptxqurter our high choomENGLISH6-Q4-W3.pptxqurter our high choom
ENGLISH6-Q4-W3.pptxqurter our high choomnelietumpap1
 
AmericanHighSchoolsprezentacijaoskolama.
AmericanHighSchoolsprezentacijaoskolama.AmericanHighSchoolsprezentacijaoskolama.
AmericanHighSchoolsprezentacijaoskolama.arsicmarija21
 
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdf
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdfAMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdf
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdfphamnguyenenglishnb
 

Recently uploaded (20)

How to Configure Email Server in Odoo 17
How to Configure Email Server in Odoo 17How to Configure Email Server in Odoo 17
How to Configure Email Server in Odoo 17
 
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️
call girls in Kamla Market (DELHI) 🔝 >༒9953330565🔝 genuine Escort Service 🔝✔️✔️
 
DATA STRUCTURE AND ALGORITHM for beginners
DATA STRUCTURE AND ALGORITHM for beginnersDATA STRUCTURE AND ALGORITHM for beginners
DATA STRUCTURE AND ALGORITHM for beginners
 
Earth Day Presentation wow hello nice great
Earth Day Presentation wow hello nice greatEarth Day Presentation wow hello nice great
Earth Day Presentation wow hello nice great
 
Difference Between Search & Browse Methods in Odoo 17
Difference Between Search & Browse Methods in Odoo 17Difference Between Search & Browse Methods in Odoo 17
Difference Between Search & Browse Methods in Odoo 17
 
Field Attribute Index Feature in Odoo 17
Field Attribute Index Feature in Odoo 17Field Attribute Index Feature in Odoo 17
Field Attribute Index Feature in Odoo 17
 
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdf
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdfFraming an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdf
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdf
 
Rapple "Scholarly Communications and the Sustainable Development Goals"
Rapple "Scholarly Communications and the Sustainable Development Goals"Rapple "Scholarly Communications and the Sustainable Development Goals"
Rapple "Scholarly Communications and the Sustainable Development Goals"
 
EPANDING THE CONTENT OF AN OUTLINE using notes.pptx
EPANDING THE CONTENT OF AN OUTLINE using notes.pptxEPANDING THE CONTENT OF AN OUTLINE using notes.pptx
EPANDING THE CONTENT OF AN OUTLINE using notes.pptx
 
Procuring digital preservation CAN be quick and painless with our new dynamic...
Procuring digital preservation CAN be quick and painless with our new dynamic...Procuring digital preservation CAN be quick and painless with our new dynamic...
Procuring digital preservation CAN be quick and painless with our new dynamic...
 
Model Call Girl in Bikash Puri Delhi reach out to us at 🔝9953056974🔝
Model Call Girl in Bikash Puri  Delhi reach out to us at 🔝9953056974🔝Model Call Girl in Bikash Puri  Delhi reach out to us at 🔝9953056974🔝
Model Call Girl in Bikash Puri Delhi reach out to us at 🔝9953056974🔝
 
Crayon Activity Handout For the Crayon A
Crayon Activity Handout For the Crayon ACrayon Activity Handout For the Crayon A
Crayon Activity Handout For the Crayon A
 
How to do quick user assign in kanban in Odoo 17 ERP
How to do quick user assign in kanban in Odoo 17 ERPHow to do quick user assign in kanban in Odoo 17 ERP
How to do quick user assign in kanban in Odoo 17 ERP
 
Solving Puzzles Benefits Everyone (English).pptx
Solving Puzzles Benefits Everyone (English).pptxSolving Puzzles Benefits Everyone (English).pptx
Solving Puzzles Benefits Everyone (English).pptx
 
Romantic Opera MUSIC FOR GRADE NINE pptx
Romantic Opera MUSIC FOR GRADE NINE pptxRomantic Opera MUSIC FOR GRADE NINE pptx
Romantic Opera MUSIC FOR GRADE NINE pptx
 
9953330565 Low Rate Call Girls In Rohini Delhi NCR
9953330565 Low Rate Call Girls In Rohini  Delhi NCR9953330565 Low Rate Call Girls In Rohini  Delhi NCR
9953330565 Low Rate Call Girls In Rohini Delhi NCR
 
ENGLISH6-Q4-W3.pptxqurter our high choom
ENGLISH6-Q4-W3.pptxqurter our high choomENGLISH6-Q4-W3.pptxqurter our high choom
ENGLISH6-Q4-W3.pptxqurter our high choom
 
Model Call Girl in Tilak Nagar Delhi reach out to us at 🔝9953056974🔝
Model Call Girl in Tilak Nagar Delhi reach out to us at 🔝9953056974🔝Model Call Girl in Tilak Nagar Delhi reach out to us at 🔝9953056974🔝
Model Call Girl in Tilak Nagar Delhi reach out to us at 🔝9953056974🔝
 
AmericanHighSchoolsprezentacijaoskolama.
AmericanHighSchoolsprezentacijaoskolama.AmericanHighSchoolsprezentacijaoskolama.
AmericanHighSchoolsprezentacijaoskolama.
 
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdf
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdfAMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdf
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdf
 

12 x1 t04 06 integrating functions of time (2013)

  • 1. Integrating Functions of Time  x 1 2 3 4 t
  • 2. Integrating Functions of Time  x 4 change in displacement   xdt  0 1 2 3 4 t
  • 3. Integrating Functions of Time  x 4 change in displacement   xdt  0 1 2 3 4 t 1 3 4 change in distance   xdt   xdt   xdt    0 1 3
  • 4. Integrating Functions of Time  x 4 change in displacement   xdt  0 1 2 3 4 t 1 3 4 change in distance   xdt   xdt   xdt    0 1 3  x 1 2 3 4 t
  • 5. Integrating Functions of Time  x 4 change in displacement   xdt  0 1 2 3 4 t 1 3 4 change in distance   xdt   xdt   xdt    0 1 3  x 4 change in velocity   dt x 0 1 2 3 4 t
  • 6. Integrating Functions of Time  x 4 change in displacement   xdt  0 1 2 3 4 t 1 3 4 change in distance   xdt   xdt   xdt    0 1 3  x 4 change in velocity   dt x 0 1 2 3 4 t 2 4 change in speed    dt   dt x x 0 2
  • 7. Derivative Graphs Function 1st derivative 2nd derivative displacement velocity acceleration
  • 8. Derivative Graphs Function 1st derivative 2nd derivative displacement velocity acceleration stationary point x intercept
  • 9. Derivative Graphs Function 1st derivative 2nd derivative displacement velocity acceleration stationary point x intercept inflection point stationary point x intercept
  • 10. Derivative Graphs Function 1st derivative 2nd derivative displacement velocity acceleration stationary point x intercept inflection point stationary point x intercept increasing positive
  • 11. Derivative Graphs Function 1st derivative 2nd derivative displacement velocity acceleration stationary point x intercept inflection point stationary point x intercept increasing positive decreasing negative
  • 12. Derivative Graphs Function 1st derivative 2nd derivative displacement velocity acceleration stationary point x intercept inflection point stationary point x intercept increasing positive decreasing negative concave up increasing positive
  • 13. Derivative Graphs Function 1st derivative 2nd derivative displacement velocity acceleration stationary point x intercept inflection point stationary point x intercept increasing positive decreasing negative concave up increasing positive concave down decreasing negative
  • 14. graph type integrate differentiate
  • 15. graph type integrate differentiate horizontal line oblique line x axis
  • 16. graph type integrate differentiate horizontal line oblique line x axis oblique line parabola horizontal line
  • 17. graph type integrate differentiate horizontal line oblique line x axis oblique line parabola horizontal line parabola cubic oblique line inflects at turning pt
  • 18. graph type integrate differentiate horizontal line oblique line x axis oblique line parabola horizontal line parabola cubic oblique line inflects at turning pt Remember: • integration = area
  • 19. graph type integrate differentiate horizontal line oblique line x axis oblique line parabola horizontal line parabola cubic oblique line inflects at turning pt Remember: • integration = area • on a velocity graph, total area = distance total integral = displacement
  • 20. graph type integrate differentiate horizontal line oblique line x axis oblique line parabola horizontal line parabola cubic oblique line inflects at turning pt Remember: • integration = area • on a velocity graph, total area = distance total integral = displacement • on an acceleration graph, total area = speed total integral = velocity
  • 21. (ii) 2003 HSC Question 7b) The velocity of a particle is given by v  2  4 cos t for 0  t  2 , where v is measured in metres per second and t is measured in seconds (i) At what times during this period is the particle at rest?
  • 22. (ii) 2003 HSC Question 7b) The velocity of a particle is given by v  2  4 cos t for 0  t  2 , where v is measured in metres per second and t is measured in seconds (i) At what times during this period is the particle at rest? v0 2  4cos t  0 1 cos t  2
  • 23. (ii) 2003 HSC Question 7b) The velocity of a particle is given by v  2  4 cos t for 0  t  2 , where v is measured in metres per second and t is measured in seconds (i) At what times during this period is the particle at rest? v0 Q1, 4 2  4cos t  0 1 1 cos   cos t  2 2   3
  • 24. (ii) 2003 HSC Question 7b) The velocity of a particle is given by v  2  4 cos t for 0  t  2 , where v is measured in metres per second and t is measured in seconds (i) At what times during this period is the particle at rest? v0 Q1, 4 t   , 2   2  4cos t  0 1  5 1 cos   t , cos t  2 3 3 2   3  5  particle is at rest after seconds and again after seconds 3 3
  • 25. (ii) 2003 HSC Question 7b) The velocity of a particle is given by v  2  4 cos t for 0  t  2 , where v is measured in metres per second and t is measured in seconds (i) At what times during this period is the particle at rest? v0 Q1, 4 t   , 2   2  4cos t  0 1  5 1 cos   t , cos t  2 3 3 2   3  5  particle is at rest after seconds and again after seconds 3 3 (ii) What is the maximum velocity of the particle during this period?
  • 26. (ii) 2003 HSC Question 7b) The velocity of a particle is given by v  2  4 cos t for 0  t  2 , where v is measured in metres per second and t is measured in seconds (i) At what times during this period is the particle at rest? v0 Q1, 4 t   , 2   2  4cos t  0 1  5 1 cos   t , cos t  2 3 3 2   3  5  particle is at rest after seconds and again after seconds 3 3 (ii) What is the maximum velocity of the particle during this period? 4  4 cos t  4 2  2  4 cos t  6  maximum velocity is 6 m/s
  • 27. (iii) Sketch the graph of v as a function of t for 0  t  2
  • 28. (iii) Sketch the graph of v as a function of t for 0  t  2 2 2 amplitude  4 units period  divisions  shift  2 units 1 4  2  flip upside down  2
  • 29. (iii) Sketch the graph of v as a function of t for 0  t  2 2 2 amplitude  4 units period  divisions  shift  2 units 1 4  2  flip upside down  2 v 6 5 4 3 2 1 -1   3 2 t -2 2 2
  • 30. (iii) Sketch the graph of v as a function of t for 0  t  2 2 2 amplitude  4 units period  divisions  shift  2 units 1 4  2  flip upside down  2 v 6 5 4 3 2 1 -1   3 2 t -2 2 2
  • 31. (iii) Sketch the graph of v as a function of t for 0  t  2 2 2 amplitude  4 units period  divisions  shift  2 units 1 4  2  flip upside down  2 v 6 5 4 3 2 1 -1   3 2 t -2 2 2
  • 32. (iii) Sketch the graph of v as a function of t for 0  t  2 2 2 amplitude  4 units period  divisions  shift  2 units 1 4  2  flip upside down  2 v 6 5 4 3 2 1 -1   3 2 t -2 2 2
  • 33. (iii) Sketch the graph of v as a function of t for 0  t  2 2 2 amplitude  4 units period  divisions  shift  2 units 1 4  2  flip upside down  2 v 6 5 v  2  4 cos t 4 3 2 1 -1   3 2 t -2 2 2
  • 34. (iv) Calculate the total distance travelled by the particle between t = 0 and t = 
  • 35. (iv) Calculate the total distance travelled by the particle between t = 0 and t =   3  distance =    2  4 cos t  dt    2  4 cos t  dt 0  3
  • 36. (iv) Calculate the total distance travelled by the particle between t = 0 and t =   3  distance =    2  4 cos t  dt    2  4 cos t  dt 0  =  2t  4sin t    2t 3 4sin t  0  3 3
  • 37. (iv) Calculate the total distance travelled by the particle between t = 0 and t =   3  distance =    2  4 cos t  dt    2  4 cos t  dt 0  =  2t  4sin t    2t 3 4sin t  0  3 3  2  4sin   =  0  0    2  4sin    2    3 3  2 4 3  =2  2     3 2  2 =4 3  metres 3
  • 38. (iii) 2004 HSC Question 9b) A particle moves along the x-axis. Initially it is at rest at the origin. The graph shows the acceleration, a, of the particle as a function of time t for 0  t  5 (i) Write down the time at which the velocity of the particle is a maximum
  • 39. (iii) 2004 HSC Question 9b) A particle moves along the x-axis. Initially it is at rest at the origin. The graph shows the acceleration, a, of the particle as a function of time t for 0  t  5 (i) Write down the time at which the velocity of the particle is a maximum v   adt  adt is a maximum when t  2
  • 40. (iii) 2004 HSC Question 9b) A particle moves along the x-axis. Initially it is at rest at the origin. The graph shows the acceleration, a, of the particle as a function of time t for 0  t  5 (i) Write down the time at which the velocity of the particle is a maximum dv v   adt OR v is a maximum when 0 dt  adt is a maximum when t  2
  • 41. (iii) 2004 HSC Question 9b) A particle moves along the x-axis. Initially it is at rest at the origin. The graph shows the acceleration, a, of the particle as a function of time t for 0  t  5 (i) Write down the time at which the velocity of the particle is a maximum dv v   adt OR v is a maximum when 0 dt  adt is a maximum when t  2  velocity is a maximum when t  2 seconds
  • 42. (ii) At what time during the interval 0  t  5 is the particle furthest from the origin? Give reasons for your answer.
  • 43. (ii) At what time during the interval 0  t  5 is the particle furthest from the origin? Give reasons for your answer. Question is asking, “when is displacement a maximum?” dx x is a maximum when 0 dt
  • 44. (ii) At what time during the interval 0  t  5 is the particle furthest from the origin? Give reasons for your answer. Question is asking, “when is displacement a maximum?” dx x is a maximum when 0 dt But v   adt  We must solve  adt  0
  • 45. (ii) At what time during the interval 0  t  5 is the particle furthest from the origin? Give reasons for your answer. Question is asking, “when is displacement a maximum?” dx x is a maximum when 0 dt But v   adt  We must solve  adt  0 i.e. when is area above the axis = area below By symmetry this would be at t = 4  particle is furthest from the origin at t  4 seconds
  • 46. (iv) 2007 HSC Question 10a) dx An object is moving on the x-axis. The graph shows the velocity, , dt of the object, as a function of t. The coordinates of the points shown on the graph are A(2,1), B(4,5), C(5,0) and D(6,–5). The velocity is constant for t  6 (i) Using Simpson’s rule, estimate the distance travelled between t = 0 and t = 4
  • 47. (iv) 2007 HSC Question 10a) dx An object is moving on the x-axis. The graph shows the velocity, , dt of the object, as a function of t. The coordinates of the points shown on the graph are A(2,1), B(4,5), C(5,0) and D(6,–5). The velocity is constant for t  6 (i) Using Simpson’s rule, estimate the distance travelled between t = 0 and t = 4 h distance   y0  4 yodd  2 yeven  yn  3
  • 48. (iv) 2007 HSC Question 10a) dx An object is moving on the x-axis. The graph shows the velocity, , dt of the object, as a function of t. The coordinates of the points shown on the graph are A(2,1), B(4,5), C(5,0) and D(6,–5). The velocity is constant for t  6 (i) Using Simpson’s rule, estimate the distance travelled between t = 0 and t = 4 h distance   y0  4 yodd  2 yeven  yn  3 t 0 2 4 v 0 1 5
  • 49. (iv) 2007 HSC Question 10a) dx An object is moving on the x-axis. The graph shows the velocity, , dt of the object, as a function of t. The coordinates of the points shown on the graph are A(2,1), B(4,5), C(5,0) and D(6,–5). The velocity is constant for t  6 (i) Using Simpson’s rule, estimate the distance travelled between t = 0 and t = 4 h distance   y0  4 yodd  2 yeven  yn  3 1 4 1 t 0 2 4 v 0 1 5
  • 50. (iv) 2007 HSC Question 10a) dx An object is moving on the x-axis. The graph shows the velocity, , dt of the object, as a function of t. The coordinates of the points shown on the graph are A(2,1), B(4,5), C(5,0) and D(6,–5). The velocity is constant for t  6 (i) Using Simpson’s rule, estimate the distance travelled between t = 0 and t = 4 h distance   y0  4 yodd  2 yeven  yn  3 1 4 1 2  0  4 1  5 t 0 2 4 3 v 0 1 5  6 metres
  • 51. (ii) The object is initially at the origin. During which time(s) is the displacement decreasing?
  • 52. (ii) The object is initially at the origin. During which time(s) is the displacement decreasing? dx x is decreasing when 0 dt  displacement is decreasing when t  5 seconds
  • 53. (ii) The object is initially at the origin. During which time(s) is the displacement decreasing? dx x is decreasing when 0 dt  displacement is decreasing when t  5 seconds (iii) Estimate the time at which the object returns to the origin. Justify your answer.
  • 54. (ii) The object is initially at the origin. During which time(s) is the displacement decreasing? dx x is decreasing when 0 dt  displacement is decreasing when t  5 seconds (iii) Estimate the time at which the object returns to the origin. Justify your answer. Question is asking, “when is displacement = 0?”
  • 55. (ii) The object is initially at the origin. During which time(s) is the displacement decreasing? dx x is decreasing when 0 dt  displacement is decreasing when t  5 seconds (iii) Estimate the time at which the object returns to the origin. Justify your answer. Question is asking, “when is displacement = 0?” But x   vdt  We must solve  vdt  0
  • 56. (ii) The object is initially at the origin. During which time(s) is the displacement decreasing? dx x is decreasing when 0 dt  displacement is decreasing when t  5 seconds (iii) Estimate the time at which the object returns to the origin. Justify your answer. Question is asking, “when is displacement = 0?” But x   vdt  We must solve  vdt  0 i.e. when is area above the axis = area below
  • 57. (ii) The object is initially at the origin. During which time(s) is the displacement decreasing? dx x is decreasing when 0 dt  displacement is decreasing when t  5 seconds (iii) Estimate the time at which the object returns to the origin. Justify your answer. Question is asking, “when is displacement = 0?” But x   vdt  We must solve  vdt  0 i.e. when is area above the axis = area below By symmetry, area from t = 4 to 5 equals area from t = 5 to 6
  • 58. (ii) The object is initially at the origin. During which time(s) is the displacement decreasing? dx x is decreasing when 0 dt  displacement is decreasing when t  5 seconds (iii) Estimate the time at which the object returns to the origin. Justify your answer. Question is asking, “when is displacement = 0?” But x   vdt  We must solve  vdt  0 i.e. when is area above the axis = area below By symmetry, area from t = 4 to 5 equals area from t = 5 to 6 In part (i) we estimated area from t = 0 to 4 to be 6,
  • 59. (ii) The object is initially at the origin. During which time(s) is the displacement decreasing? dx x is decreasing when 0 dt  displacement is decreasing when t  5 seconds (iii) Estimate the time at which the object returns to the origin. Justify your answer. Question is asking, “when is displacement = 0?” But x   vdt  We must solve  vdt  0 i.e. when is area above the axis = area below By symmetry, area from t = 4 to 5 equals area A4 from t = 5 to 6 In part (i) we estimated area from t = 0 to 4 to be 6,  A4  6
  • 60. (ii) The object is initially at the origin. During which time(s) is the displacement decreasing? dx x is decreasing when 0 dt  displacement is decreasing when t  5 seconds (iii) Estimate the time at which the object returns to the origin. Justify your answer. Question is asking, “when is displacement = 0?” But x   vdt  We must solve  vdt  0 a i.e. when is area above the axis = area below By symmetry, area from t = 4 to 5 equals area A4 5 from t = 5 to 6 In part (i) we estimated area from t = 0 to 4 to be 6,  A4  6 a  1.2 5a  6
  • 61. (ii) The object is initially at the origin. During which time(s) is the displacement decreasing? dx x is decreasing when 0 dt  displacement is decreasing when t  5 seconds (iii) Estimate the time at which the object returns to the origin. Justify your answer. Question is asking, “when is displacement = 0?” But x   vdt  We must solve  vdt  0 a i.e. when is area above the axis = area below By symmetry, area from t = 4 to 5 equals area A4 5 from t = 5 to 6 In part (i) we estimated area from t = 0 to 4 to be 6,  A4  6 a  1.2 5a  6  particle returns to the origin when t  7.2 seconds
  • 62. (iv) Sketch the displacement, x, as a function of time.
  • 63. (iv) Sketch the displacement, x, as a function of time. x 8.5 6 2 4 6 8 t
  • 64. (iv) Sketch the displacement, x, as a function of time. object is initially at the origin x 8.5 6 2 4 6 8 t
  • 65. (iv) Sketch the displacement, x, as a function of time. object is initially at the origin when t = 4, x = 6 x 8.5 6 2 4 6 8 t
  • 66. (iv) Sketch the displacement, x, as a function of time. object is initially at the origin when t = 4, x = 6 by symmetry of areas t = 6, x = 6 x 8.5 6 2 4 6 8 t
  • 67. (iv) Sketch the displacement, x, as a function of time. object is initially at the origin when t = 4, x = 6 by symmetry of areas t = 6, x = 6 Area of triangle = 2.5  when t  5, x  8.5 x 8.5 6 2 4 6 8 t
  • 68. (iv) Sketch the displacement, x, as a function of time. object is initially at the origin when t = 4, x = 6 by symmetry of areas t = 6, x = 6 Area of triangle = 2.5  when t  5, x  8.5 returns to x = 0 when t = 7.2 x 8.5 6 2 4 6 7.2 8 t
  • 69. (iv) Sketch the displacement, x, as a function of time. object is initially at the origin when t = 4, x = 6 by symmetry of areas t = 6, x = 6 Area of triangle = 2.5  when t  5, x  8.5 returns to x = 0 when t = 7.2 x v is steeper between t = 2 and 4 8.5 than between t = 0 and 2 6  particle covers more distance between t  2 and 4 2 4 6 7.2 8 t
  • 70. (iv) Sketch the displacement, x, as a function of time. object is initially at the origin when t = 4, x = 6 by symmetry of areas t = 6, x = 6 Area of triangle = 2.5  when t  5, x  8.5 returns to x = 0 when t = 7.2 x v is steeper between t = 2 and 4 8.5 than between t = 0 and 2 6  particle covers more distance between t  2 and 4 when t > 6, v is constant t  when t  6, x is a straight line 2 4 6 7.2 8
  • 71. (iv) Sketch the displacement, x, as a function of time. object is initially at the origin when t = 4, x = 6 by symmetry of areas t = 6, x = 6 Area of triangle = 2.5  when t  5, x  8.5 returns to x = 0 when t = 7.2 x v is steeper between t = 2 and 4 8.5 than between t = 0 and 2 6  particle covers more distance between t  2 and 4 when t > 6, v is constant t  when t  6, x is a straight line 2 4 6 7.2 8
  • 72. (v) 2005 HSC Question 7b) dx The graph shows the velocity, dt , of a particle as a function of time. Initially the particle is at the origin. (i) At what time is the displacement, x, from the origin a maximum?
  • 73. (v) 2005 HSC Question 7b) dx The graph shows the velocity, dt , of a particle as a function of time. Initially the particle is at the origin. (i) At what time is the displacement, x, from the origin a maximum? Displacement is a maximum when area is most positive, also when velocity is zero i.e. when t = 2
  • 74. (ii) At what time does the particle return to the origin? Justify your answer
  • 75. (ii) At what time does the particle return to the origin? Justify your answer Question is asking, “when is displacement = 0?” i.e. when is area above the axis = area below?
  • 76. (ii) At what time does the particle return to the origin? Justify your answer 2 a w a 2 Question is asking, “when is displacement = 0?” i.e. when is area above the axis = area below?
  • 77. (ii) At what time does the particle return to the origin? Justify your answer 2 a w a 2 Question is asking, “when is displacement = 0?” i.e. when is area above the axis = area below? 2w = 2 w=1
  • 78. (ii) At what time does the particle return to the origin? Justify your answer 2 a w a 2 Question is asking, “when is displacement = 0?” i.e. when is area above the axis = area below? 2w = 2 w=1 Returns to the origin after 4 seconds
  • 79. d 2x (iii) Draw a sketch of the acceleration, 2 , as afunction of dt time for 0  t  6 d 2x dt 2 1 2 3 5 6 t
  • 80. d 2x (iii) Draw a sketch of the acceleration, 2 , as afunction of dt time for 0  t  6 differentiate a horizontal line you get the xaxis d 2x dt 2 1 2 3 5 6 t
  • 81. d 2x (iii) Draw a sketch of the acceleration, 2 , as afunction of dt time for 0  t  6 differentiate a horizontal line you get the xaxis from 1 to 3 we have a cubic, inflects at 2, and is decreasing differentiate, you get a parabola, stationary at 2, it is below the x axis d 2x dt 2 1 2 3 5 6 t
  • 82. d 2x (iii) Draw a sketch of the acceleration, 2 , as afunction of dt time for 0  t  6 differentiate a horizontal line you get the xaxis from 1 to 3 we have a cubic, inflects at 2, and is decreasing differentiate, you get a parabola, stationary at 2, it is below the x axis d 2x dt 2 from 5 to 6 is a cubic, inflects at 6 and is increasing (using symmetry) differentiate, you get a parabola 1 2 3 5 6 t stationary at 6, it is above the x axis
  • 83. d 2x (iii) Draw a sketch of the acceleration, 2 , as afunction of dt time for 0  t  6 differentiate a horizontal line you get the xaxis from 1 to 3 we have a cubic, inflects at 2, and is decreasing differentiate, you get a parabola, stationary at 2, it is below the x axis d 2x dt 2 from 5 to 6 is a cubic, inflects at 6 and is increasing (using symmetry) differentiate, you get a parabola 1 2 3 5 6 t stationary at 6, it is above the x axis
  • 84. Exercise 3C; 1 ace etc, 2 ace etc, 4a, 7ab(i), 8, 9a, 10, 13, 15, 16, 18