SlideShare une entreprise Scribd logo
1  sur  55
Télécharger pour lire hors ligne
Applications of Calculus To
   The Physical World
Applications of Calculus To
   The Physical World
Displacement (x)
Distance from a point, with direction.
Applications of Calculus To
   The Physical World
Displacement (x)
Distance from a point, with direction.
          v, dx , x 
Velocity          
          dt 
The rate of change of displacement with respect to time i.e. speed
with direction.
Applications of Calculus To
   The Physical World
Displacement (x)
Distance from a point, with direction.
          v, dx , x 
Velocity          
          dt 
The rate of change of displacement with respect to time i.e. speed
with direction.
                dv d 2 x     
Acceleration  a, , 2 , , v 
                          x 
                dt dt        
The rate of change of velocity with respect to time
Applications of Calculus To
   The Physical World
Displacement (x)
Distance from a point, with direction.
          v, dx , x 
Velocity          
          dt 
The rate of change of displacement with respect to time i.e. speed
with direction.
                dv d 2 x     
Acceleration  a, , 2 , , v 
                          x 
                dt dt        
The rate of change of velocity with respect to time

 NOTE: “deceleration” or slowing down is when acceleration is in
        the opposite direction to velocity.
Displacement


differentiate    Velocity


                Acceleration
Displacement


differentiate    Velocity      integrate


                Acceleration
x
 2
 1

     1 2 3 4   t
-1
-2
x
 2   slope=instantaneous velocity
 1

     1 2 3 4       t
-1
-2
x
 2   slope=instantaneous velocity
 1

     1 2 3 4       t
-1
-2

x



     1 2 3 4       t
x
 2      slope=instantaneous velocity
 1

        1 2 3 4       t
-1
-2
     slope=instantaneous acceleration

x



        1 2 3 4       t
x
 2      slope=instantaneous velocity
 1

        1 2 3 4       t
-1
-2
     slope=instantaneous acceleration

x



        1 2 3 4       t



x



        1 2 3 4       t
x
 2      slope=instantaneous velocity
 1

        1 2 3 4       t
-1                                      e.g. (i) distance traveled  7 m
-2
     slope=instantaneous acceleration

x



        1 2 3 4       t



x



        1 2 3 4       t
x
 2      slope=instantaneous velocity
 1
        1 2 3 4       t
-1                                      e.g. (i) distance traveled  7 m
-2
     slope=instantaneous acceleration       (ii) total displacement  1m

x



        1 2 3 4       t



x



        1 2 3 4       t
x
 2      slope=instantaneous velocity
 1
        1 2 3 4       t
-1                                      e.g. (i) distance traveled  7 m
-2
     slope=instantaneous acceleration      (ii) total displacement  1m

x
                                                                 7
                                           (iii) average speed  m/s
                                                                 4

        1 2 3 4       t



x



        1 2 3 4       t
x
 2      slope=instantaneous velocity
 1
        1 2 3 4       t
-1                                      e.g. (i) distance traveled  7 m
-2
     slope=instantaneous acceleration      (ii) total displacement  1m

x
                                                                 7
                                           (iii) average speed  m/s
                                                                 4
                                                                   1
        1 2 3 4       t                    (iv) average velocity  m/s
                                                                    4


x



        1 2 3 4       t
e.g. (i) The displacement x from the origin at time t seconds, of a
          particle traveling in a straight line is given by the formula
          x  t 3  21t 2
a) Find the acceleration of the particle at time t.
e.g. (i) The displacement x from the origin at time t seconds, of a
          particle traveling in a straight line is given by the formula
          x  t 3  21t 2
a) Find the acceleration of the particle at time t.
                      x  t 3  21t 2
                      v  3t 2  42t
                      a  6t  42
e.g. (i) The displacement x from the origin at time t seconds, of a
          particle traveling in a straight line is given by the formula
          x  t 3  21t 2
a) Find the acceleration of the particle at time t.
                      x  t 3  21t 2
                      v  3t 2  42t
                      a  6t  42
b) Find the times when the particle is stationary.
e.g. (i) The displacement x from the origin at time t seconds, of a
          particle traveling in a straight line is given by the formula
          x  t 3  21t 2
a) Find the acceleration of the particle at time t.
                      x  t 3  21t 2
                      v  3t 2  42t
                      a  6t  42
b) Find the times when the particle is stationary.
                Particle is stationary when v = 0
                           i.e. 3t 2  42t  0
e.g. (i) The displacement x from the origin at time t seconds, of a
          particle traveling in a straight line is given by the formula
          x  t 3  21t 2
a) Find the acceleration of the particle at time t.
                      x  t 3  21t 2
                      v  3t 2  42t
                      a  6t  42
b) Find the times when the particle is stationary.
                Particle is stationary when v = 0
                           i.e. 3t 2  42t  0
                             3t t  14   0
                            t  0 or t  14
     Particle is stationary initially and again after 14 seconds
(ii) A particle is moving on the x axis. It started from rest at t = 0 from
     the point x = 7.
     If its acceleration at time t is 2 + 6t find the position of the particle
     when t = 3.
(ii) A particle is moving on the x axis. It started from rest at t = 0 from
     the point x = 7.
     If its acceleration at time t is 2 + 6t find the position of the particle
     when t = 3.
          a  2  6t
          v  2t  3t 2  c
(ii) A particle is moving on the x axis. It started from rest at t = 0 from
     the point x = 7.
     If its acceleration at time t is 2 + 6t find the position of the particle
     when t = 3.
          a  2  6t
          v  2t  3t 2  c
         when t  0, v  0
         i.e. 0  0  0  c
              c0
(ii) A particle is moving on the x axis. It started from rest at t = 0 from
     the point x = 7.
     If its acceleration at time t is 2 + 6t find the position of the particle
     when t = 3.
          a  2  6t
          v  2t  3t 2  c
         when t  0, v  0
         i.e. 0  0  0  c
              c0
            v  2t  3t 2
(ii) A particle is moving on the x axis. It started from rest at t = 0 from
     the point x = 7.
     If its acceleration at time t is 2 + 6t find the position of the particle
     when t = 3.
          a  2  6t
          v  2t  3t 2  c
         when t  0, v  0
         i.e. 0  0  0  c
              c0
            v  2t  3t 2
           x  t2  t3  c
(ii) A particle is moving on the x axis. It started from rest at t = 0 from
     the point x = 7.
     If its acceleration at time t is 2 + 6t find the position of the particle
     when t = 3.
          a  2  6t
           v  2t  3t 2  c
         when t  0, v  0
          i.e. 0  0  0  c
               c0
             v  2t  3t 2
            x  t2  t3  c
         when t  0, x  7
         i.e. 7  0  0  c
              c7
(ii) A particle is moving on the x axis. It started from rest at t = 0 from
     the point x = 7.
     If its acceleration at time t is 2 + 6t find the position of the particle
     when t = 3.
          a  2  6t
           v  2t  3t 2  c
         when t  0, v  0
          i.e. 0  0  0  c
               c0
             v  2t  3t 2
            x  t2  t3  c
         when t  0, x  7
         i.e. 7  0  0  c
              c7
          x  t2  t3  7
(ii) A particle is moving on the x axis. It started from rest at t = 0 from
     the point x = 7.
     If its acceleration at time t is 2 + 6t find the position of the particle
     when t = 3.
          a  2  6t                    when t  3, x  32  33  7
           v  2t  3t 2  c                           43
         when t  0, v  0
                                     after 3 seconds the particle is 43
          i.e. 0  0  0  c
                                     units to the right of O.
               c0
             v  2t  3t 2
            x  t2  t3  c
         when t  0, x  7
         i.e. 7  0  0  c
              c7
          x  t2  t3  7
e.g. 2001 HSC Question 7c)
     A particle moves in a straight line so that its displacement, in metres,
     is given by       t2
                    x
                       t2
     where t is measured in seconds.
 (i) What is the displacement when t = 0?
e.g. 2001 HSC Question 7c)
     A particle moves in a straight line so that its displacement, in metres,
     is given by        t2
                     x
                        t2
     where t is measured in seconds.
 (i) What is the displacement when t = 0?
                      02
      when t  0, x 
                      02
                    = 1
              the particle is 1 metre to the left of the origin
e.g. 2001 HSC Question 7c)
     A particle moves in a straight line so that its displacement, in metres,
     is given by        t2
                     x
                        t2
     where t is measured in seconds.
 (i) What is the displacement when t = 0?
                      02
      when t  0, x 
                      02
                    = 1
              the particle is 1 metre to the left of the origin
                         4
(ii) Show that x  1 
                       t2
Hence find expressions for the velocity and the acceleration in terms of t.
e.g. 2001 HSC Question 7c)
     A particle moves in a straight line so that its displacement, in metres,
     is given by         t2
                     x
                         t2
     where t is measured in seconds.
 (i) What is the displacement when t = 0?
                      02
      when t  0, x 
                      02
                    = 1
                the particle is 1 metre to the left of the origin
                          4
(ii) Show that x  1 
                        t2
Hence find expressions for the velocity and the acceleration in terms of t.
       4     t 24
1        
     t2        t2
              t2
                                4
              t  2  x  1
                               t2
e.g. 2001 HSC Question 7c)
     A particle moves in a straight line so that its displacement, in metres,
     is given by         t2
                     x
                         t2
     where t is measured in seconds.
 (i) What is the displacement when t = 0?
                      02
      when t  0, x 
                      02
                    = 1
                the particle is 1 metre to the left of the origin
                          4
(ii) Show that x  1 
                        t2
Hence find expressions for the velocity and the acceleration in terms of t.
       4     t 24                              4  1
1                                      v
     t2        t2                             t  2
                                                        2

              t2
                                4       v
                                                  4
              t  2  x  1                  t  2
                                                      2
                               t2
e.g. 2001 HSC Question 7c)
     A particle moves in a straight line so that its displacement, in metres,
     is given by         t2
                     x
                         t2
     where t is measured in seconds.
 (i) What is the displacement when t = 0?
                      02
      when t  0, x 
                      02
                    = 1
                the particle is 1 metre to the left of the origin
                          4
(ii) Show that x  1 
                        t2
Hence find expressions for the velocity and the acceleration in terms of t.
             t 24                              4  1       4  2  t  2  1
                                                                               1
       4
1                                      v               a
     t2        t2                             t  2              t  2
                                                        2                    4

              t2                                                       8
                                4       v
                                                  4
                                                                a
              t  2  x  1                  t  2
                                                      2
                                                                     t  2
                                                                             3
                               t2
(iii) Is the particle ever at rest? Give reasons for your answer.
(iii) Is the particle ever at rest? Give reasons for your answer.
                             4
                      v         2  0
                         t  2
                      the particle is never at rest
(iii) Is the particle ever at rest? Give reasons for your answer.
                              4
                       v         2  0
                          t  2
                       the particle is never at rest
(iv) What is the limiting velocity of the particle as t increases indefinitely?
(iii) Is the particle ever at rest? Give reasons for your answer.
                              4
                       v         2  0
                          t  2
                       the particle is never at rest
(iv) What is the limiting velocity of the particle as t increases indefinitely?
                     4
     lim v  lim
     t 
                      
             t  t  2 2
(iii) Is the particle ever at rest? Give reasons for your answer.
                              4
                       v         2  0
                          t  2
                       the particle is never at rest
(iv) What is the limiting velocity of the particle as t increases indefinitely?
                     4
     lim v  lim
     t 
                      
             t  t  2 2

           0
(iii) Is the particle ever at rest? Give reasons for your answer.
                              4
                       v         2  0
                          t  2
                       the particle is never at rest
(iv) What is the limiting velocity of the particle as t increases indefinitely?
                     4                      v
     lim v  lim               OR
     t 
                      
             t  t  2 2
                                                                   4
                                                            v
           0                              1                   t  2
                                                                       2




                                                                     t
(iii) Is the particle ever at rest? Give reasons for your answer.
                              4
                       v         2  0
                          t  2
                       the particle is never at rest
(iv) What is the limiting velocity of the particle as t increases indefinitely?
                     4                      v
     lim v  lim               OR
     t 
                      
             t  t  2 2
                                                                   4
                                                            v
           0                              1                   t  2
                                                                       2




                                                                     t

           the limiting velocity of the particle is 0 m/s
(ii) 2002 HSC Question 8b)
    A particle moves in a straight line. At time t seconds, its distance x
    metres from a fixed point O in the line is given by x  sin 2t  3

   (i) Sketch the graph of x as a function of t for 0  t  2
(ii) 2002 HSC Question 8b)
    A particle moves in a straight line. At time t seconds, its distance x
    metres from a fixed point O in the line is given by x  sin 2t  3

   (i) Sketch the graph of x as a function of t for 0  t  2
                                        2                     
       amplitude  1 unit     period             divisions 
                                         2                     4
      shift  3 units               
(ii) 2002 HSC Question 8b)
    A particle moves in a straight line. At time t seconds, its distance x
    metres from a fixed point O in the line is given by x  sin 2t  3

   (i) Sketch the graph of x as a function of t for 0  t  2
                                        2                     
       amplitude  1 unit     period             divisions 
                                         2                     4
      shift  3 units               
             x
             4
             3
             2
             1

                           3        5   3    7   2    t
                    4    2    4          4    2     4
(ii) 2002 HSC Question 8b)
    A particle moves in a straight line. At time t seconds, its distance x
    metres from a fixed point O in the line is given by x  sin 2t  3

   (i) Sketch the graph of x as a function of t for 0  t  2
                                        2                     
       amplitude  1 unit     period             divisions 
                                         2                     4
      shift  3 units               
             x
             4
             3
             2
             1

                           3        5   3    7   2    t
                    4    2    4          4    2     4
(ii) 2002 HSC Question 8b)
    A particle moves in a straight line. At time t seconds, its distance x
    metres from a fixed point O in the line is given by x  sin 2t  3

   (i) Sketch the graph of x as a function of t for 0  t  2
                                        2                     
       amplitude  1 unit     period             divisions 
                                         2                     4
      shift  3 units               
             x
             4
             3
             2
             1

                           3        5   3    7   2    t
                    4    2    4          4    2     4
(ii) 2002 HSC Question 8b)
    A particle moves in a straight line. At time t seconds, its distance x
    metres from a fixed point O in the line is given by x  sin 2t  3

   (i) Sketch the graph of x as a function of t for 0  t  2
                                        2                     
       amplitude  1 unit     period             divisions 
                                         2                     4
      shift  3 units               
             x
             4
             3
             2
             1

                           3        5   3    7   2    t
                    4    2    4          4    2     4
(ii) 2002 HSC Question 8b)
    A particle moves in a straight line. At time t seconds, its distance x
    metres from a fixed point O in the line is given by x  sin 2t  3

   (i) Sketch the graph of x as a function of t for 0  t  2
                                        2                     
       amplitude  1 unit     period             divisions 
                                         2                     4
      shift  3 units               
             x
             4                                          x  sin 2t  3
             3
             2
             1

                           3        5   3    7    2    t
                    4    2    4          4    2     4
(ii) Using your graph, or otherwise, find the times when the particle is at
     rest, and the position of the particle at those times.
(ii) Using your graph, or otherwise, find the times when the particle is at
     rest, and the position of the particle at those times.
   Particle is at rest when velocity = 0
        dx
             0 i.e. the stationary points
        dt
(ii) Using your graph, or otherwise, find the times when the particle is at
     rest, and the position of the particle at those times.
   Particle is at rest when velocity = 0
        dx
             0 i.e. the stationary points
        dt
                    
        when t  seconds, x  4 metres
                    4
                   3
               t      seconds, x  2 metres
                    4
                   5
               t      seconds, x  4 metres
                    4
                   7
               t      seconds, x  2 metres
                    4
(ii) Using your graph, or otherwise, find the times when the particle is at
     rest, and the position of the particle at those times.
   Particle is at rest when velocity = 0
        dx
             0 i.e. the stationary points
        dt
                    
        when t  seconds, x  4 metres
                    4
                   3
               t      seconds, x  2 metres
                    4
                   5
               t      seconds, x  4 metres
                    4
                   7
               t      seconds, x  2 metres
                    4
  (iii) Describe the motion completely.
(ii) Using your graph, or otherwise, find the times when the particle is at
     rest, and the position of the particle at those times.
   Particle is at rest when velocity = 0
        dx
             0 i.e. the stationary points
        dt
                    
        when t  seconds, x  4 metres
                    4
                   3
               t      seconds, x  2 metres
                    4
                   5
               t      seconds, x  4 metres
                    4
                   7
               t      seconds, x  2 metres
                    4
  (iii) Describe the motion completely.
        The particle oscillates between x=2 and x=4 with a period of
         seconds
Exercise 3B; 2, 4, 6, 8, 10, 12

Contenu connexe

Tendances

Linear equations in two variables- By- Pragyan
Linear equations in two variables- By- PragyanLinear equations in two variables- By- Pragyan
Linear equations in two variables- By- PragyanPragyan Poudyal
 
Kinematic equations of motion
Kinematic equations of motionKinematic equations of motion
Kinematic equations of motionmantlfin
 
Maxima & Minima of Calculus
Maxima & Minima of CalculusMaxima & Minima of Calculus
Maxima & Minima of CalculusArpit Modh
 
INTEGRATION BY PARTS PPT
INTEGRATION BY PARTS PPT INTEGRATION BY PARTS PPT
INTEGRATION BY PARTS PPT 03062679929
 
Solving systems of equations
Solving systems of equationsSolving systems of equations
Solving systems of equationsHind Al Awadi
 
04 kinematics in one dimension
04 kinematics in one dimension04 kinematics in one dimension
04 kinematics in one dimensionIZZUDIN IBRAHIM
 
30 surface integrals
30 surface integrals30 surface integrals
30 surface integralsmath267
 
Projectile motion 1
Projectile motion 1Projectile motion 1
Projectile motion 1Akash Deep
 
Higher Order Deriavatives
Higher Order DeriavativesHigher Order Deriavatives
Higher Order DeriavativesPadme Amidala
 
Area between curves
Area between curvesArea between curves
Area between curvesShaun Wilson
 
Introduction of Equation of pair of straight lines
Introduction of Equation of pair of straight lines Introduction of Equation of pair of straight lines
Introduction of Equation of pair of straight lines Janak Singh saud
 
Lesson 1 derivative of trigonometric functions
Lesson 1 derivative of trigonometric functionsLesson 1 derivative of trigonometric functions
Lesson 1 derivative of trigonometric functionsLawrence De Vera
 
Roots of polynomials
Roots of polynomialsRoots of polynomials
Roots of polynomialsDUBAN CASTRO
 
Taylor's and Maclaurin series
Taylor's and Maclaurin seriesTaylor's and Maclaurin series
Taylor's and Maclaurin seriesHarsh Parmar
 
Arc Length And Area of a Sector
Arc Length And Area of a SectorArc Length And Area of a Sector
Arc Length And Area of a SectorJosel Jalon
 
Trigonometric Limits
Trigonometric LimitsTrigonometric Limits
Trigonometric LimitsPablo Antuna
 
Projectile motion
Projectile motionProjectile motion
Projectile motiongngr0810
 

Tendances (20)

Linear equations in two variables- By- Pragyan
Linear equations in two variables- By- PragyanLinear equations in two variables- By- Pragyan
Linear equations in two variables- By- Pragyan
 
Kinematic equations of motion
Kinematic equations of motionKinematic equations of motion
Kinematic equations of motion
 
Trapezoidal rule
Trapezoidal ruleTrapezoidal rule
Trapezoidal rule
 
Maxima & Minima of Calculus
Maxima & Minima of CalculusMaxima & Minima of Calculus
Maxima & Minima of Calculus
 
INTEGRATION BY PARTS PPT
INTEGRATION BY PARTS PPT INTEGRATION BY PARTS PPT
INTEGRATION BY PARTS PPT
 
Solving systems of equations
Solving systems of equationsSolving systems of equations
Solving systems of equations
 
04 kinematics in one dimension
04 kinematics in one dimension04 kinematics in one dimension
04 kinematics in one dimension
 
30 surface integrals
30 surface integrals30 surface integrals
30 surface integrals
 
Projectile motion 1
Projectile motion 1Projectile motion 1
Projectile motion 1
 
Higher Order Deriavatives
Higher Order DeriavativesHigher Order Deriavatives
Higher Order Deriavatives
 
Area between curves
Area between curvesArea between curves
Area between curves
 
Application of derivative
Application of derivativeApplication of derivative
Application of derivative
 
Introduction of Equation of pair of straight lines
Introduction of Equation of pair of straight lines Introduction of Equation of pair of straight lines
Introduction of Equation of pair of straight lines
 
Lesson 1 derivative of trigonometric functions
Lesson 1 derivative of trigonometric functionsLesson 1 derivative of trigonometric functions
Lesson 1 derivative of trigonometric functions
 
Roots of polynomials
Roots of polynomialsRoots of polynomials
Roots of polynomials
 
Taylor's and Maclaurin series
Taylor's and Maclaurin seriesTaylor's and Maclaurin series
Taylor's and Maclaurin series
 
Volume of revolution
Volume of revolutionVolume of revolution
Volume of revolution
 
Arc Length And Area of a Sector
Arc Length And Area of a SectorArc Length And Area of a Sector
Arc Length And Area of a Sector
 
Trigonometric Limits
Trigonometric LimitsTrigonometric Limits
Trigonometric Limits
 
Projectile motion
Projectile motionProjectile motion
Projectile motion
 

En vedette

Velocity and stuff
Velocity and stuffVelocity and stuff
Velocity and stuffShaun Wilson
 
motion velocity accelaration and displacement
motion velocity accelaration and displacementmotion velocity accelaration and displacement
motion velocity accelaration and displacementjamesadam2001
 
Ppt Acceleration
Ppt AccelerationPpt Acceleration
Ppt Accelerationffiala
 
Velocity and acceleration
Velocity and accelerationVelocity and acceleration
Velocity and accelerationjtwining
 

En vedette (6)

Velocity and stuff
Velocity and stuffVelocity and stuff
Velocity and stuff
 
motion velocity accelaration and displacement
motion velocity accelaration and displacementmotion velocity accelaration and displacement
motion velocity accelaration and displacement
 
Ppt Acceleration
Ppt AccelerationPpt Acceleration
Ppt Acceleration
 
Chapter 1(3)DIMENSIONAL ANALYSIS
Chapter 1(3)DIMENSIONAL ANALYSISChapter 1(3)DIMENSIONAL ANALYSIS
Chapter 1(3)DIMENSIONAL ANALYSIS
 
Velocity and acceleration
Velocity and accelerationVelocity and acceleration
Velocity and acceleration
 
Speed,velocity,acceleration
Speed,velocity,accelerationSpeed,velocity,acceleration
Speed,velocity,acceleration
 

Similaire à 12 x1 t04 05 displacement, velocity, acceleration (2013)

12 x1 t07 02 v and a in terms of x (2013)
12 x1 t07 02 v and a in terms of x (2013)12 x1 t07 02 v and a in terms of x (2013)
12 x1 t07 02 v and a in terms of x (2013)Nigel Simmons
 
_lecture_03_curves_motion_in_3-space.pdf
_lecture_03_curves_motion_in_3-space.pdf_lecture_03_curves_motion_in_3-space.pdf
_lecture_03_curves_motion_in_3-space.pdfLeoIrsi
 
Lecture Dynamics Kinetics of Particles.pdf
Lecture Dynamics Kinetics of Particles.pdfLecture Dynamics Kinetics of Particles.pdf
Lecture Dynamics Kinetics of Particles.pdfCyberMohdSalahShoty
 
Lecture 13 applications - section 3.8
Lecture 13   applications - section 3.8Lecture 13   applications - section 3.8
Lecture 13 applications - section 3.8njit-ronbrown
 
Chapter 11_0 velocity, acceleration.pdf
Chapter 11_0 velocity, acceleration.pdfChapter 11_0 velocity, acceleration.pdf
Chapter 11_0 velocity, acceleration.pdfMrsTMDNMedagedara
 
Simple harmonic motion
Simple harmonic motionSimple harmonic motion
Simple harmonic motionAdarsh Ang
 
Lecture 02.pdf
Lecture 02.pdfLecture 02.pdf
Lecture 02.pdfjm_gecko
 
Theory of relativity
Theory of relativityTheory of relativity
Theory of relativityKumar
 
introduction-brownian-motion final
introduction-brownian-motion finalintroduction-brownian-motion final
introduction-brownian-motion finalK Thanh P Ng
 
Chapter3powerpoint 090825235704-phpapp02
Chapter3powerpoint 090825235704-phpapp02Chapter3powerpoint 090825235704-phpapp02
Chapter3powerpoint 090825235704-phpapp02Cleophas Rwemera
 

Similaire à 12 x1 t04 05 displacement, velocity, acceleration (2013) (14)

12 x1 t07 02 v and a in terms of x (2013)
12 x1 t07 02 v and a in terms of x (2013)12 x1 t07 02 v and a in terms of x (2013)
12 x1 t07 02 v and a in terms of x (2013)
 
_lecture_03_curves_motion_in_3-space.pdf
_lecture_03_curves_motion_in_3-space.pdf_lecture_03_curves_motion_in_3-space.pdf
_lecture_03_curves_motion_in_3-space.pdf
 
Lecture Dynamics Kinetics of Particles.pdf
Lecture Dynamics Kinetics of Particles.pdfLecture Dynamics Kinetics of Particles.pdf
Lecture Dynamics Kinetics of Particles.pdf
 
Lecture 13 applications - section 3.8
Lecture 13   applications - section 3.8Lecture 13   applications - section 3.8
Lecture 13 applications - section 3.8
 
Chapter 11_0 velocity, acceleration.pdf
Chapter 11_0 velocity, acceleration.pdfChapter 11_0 velocity, acceleration.pdf
Chapter 11_0 velocity, acceleration.pdf
 
Simple harmonic motion
Simple harmonic motionSimple harmonic motion
Simple harmonic motion
 
G11ex1
G11ex1G11ex1
G11ex1
 
Lecture 02.pdf
Lecture 02.pdfLecture 02.pdf
Lecture 02.pdf
 
Calc 2.2b
Calc 2.2bCalc 2.2b
Calc 2.2b
 
Gradient of a curve and equation of a
Gradient of a curve and equation of aGradient of a curve and equation of a
Gradient of a curve and equation of a
 
p02_007.pdf
p02_007.pdfp02_007.pdf
p02_007.pdf
 
Theory of relativity
Theory of relativityTheory of relativity
Theory of relativity
 
introduction-brownian-motion final
introduction-brownian-motion finalintroduction-brownian-motion final
introduction-brownian-motion final
 
Chapter3powerpoint 090825235704-phpapp02
Chapter3powerpoint 090825235704-phpapp02Chapter3powerpoint 090825235704-phpapp02
Chapter3powerpoint 090825235704-phpapp02
 

Plus de 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
 

Plus de 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)
 

Dernier

Analyzing and resolving a communication crisis in Dhaka textiles LTD.pptx
Analyzing and resolving a communication crisis in Dhaka textiles LTD.pptxAnalyzing and resolving a communication crisis in Dhaka textiles LTD.pptx
Analyzing and resolving a communication crisis in Dhaka textiles LTD.pptxLimon Prince
 
Stl Algorithms in C++ jjjjjjjjjjjjjjjjjj
Stl Algorithms in C++ jjjjjjjjjjjjjjjjjjStl Algorithms in C++ jjjjjjjjjjjjjjjjjj
Stl Algorithms in C++ jjjjjjjjjjjjjjjjjjMohammed Sikander
 
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...Nguyen Thanh Tu Collection
 
Personalisation of Education by AI and Big Data - Lourdes Guàrdia
Personalisation of Education by AI and Big Data - Lourdes GuàrdiaPersonalisation of Education by AI and Big Data - Lourdes Guàrdia
Personalisation of Education by AI and Big Data - Lourdes GuàrdiaEADTU
 
Contoh Aksi Nyata Refleksi Diri ( NUR ).pdf
Contoh Aksi Nyata Refleksi Diri ( NUR ).pdfContoh Aksi Nyata Refleksi Diri ( NUR ).pdf
Contoh Aksi Nyata Refleksi Diri ( NUR ).pdfcupulin
 
Major project report on Tata Motors and its marketing strategies
Major project report on Tata Motors and its marketing strategiesMajor project report on Tata Motors and its marketing strategies
Major project report on Tata Motors and its marketing strategiesAmanpreetKaur157993
 
When Quality Assurance Meets Innovation in Higher Education - Report launch w...
When Quality Assurance Meets Innovation in Higher Education - Report launch w...When Quality Assurance Meets Innovation in Higher Education - Report launch w...
When Quality Assurance Meets Innovation in Higher Education - Report launch w...Gary Wood
 
Observing-Correct-Grammar-in-Making-Definitions.pptx
Observing-Correct-Grammar-in-Making-Definitions.pptxObserving-Correct-Grammar-in-Making-Definitions.pptx
Observing-Correct-Grammar-in-Making-Definitions.pptxAdelaideRefugio
 
SPLICE Working Group: Reusable Code Examples
SPLICE Working Group:Reusable Code ExamplesSPLICE Working Group:Reusable Code Examples
SPLICE Working Group: Reusable Code ExamplesPeter Brusilovsky
 
8 Tips for Effective Working Capital Management
8 Tips for Effective Working Capital Management8 Tips for Effective Working Capital Management
8 Tips for Effective Working Capital ManagementMBA Assignment Experts
 
How to Send Pro Forma Invoice to Your Customers in Odoo 17
How to Send Pro Forma Invoice to Your Customers in Odoo 17How to Send Pro Forma Invoice to Your Customers in Odoo 17
How to Send Pro Forma Invoice to Your Customers in Odoo 17Celine George
 
OSCM Unit 2_Operations Processes & Systems
OSCM Unit 2_Operations Processes & SystemsOSCM Unit 2_Operations Processes & Systems
OSCM Unit 2_Operations Processes & SystemsSandeep D Chaudhary
 
What is 3 Way Matching Process in Odoo 17.pptx
What is 3 Way Matching Process in Odoo 17.pptxWhat is 3 Way Matching Process in Odoo 17.pptx
What is 3 Way Matching Process in Odoo 17.pptxCeline George
 
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...Nguyen Thanh Tu Collection
 
PS-Policies-on-Enrolment-Transfer-of-Docs-Checking-of-School-Forms-and-SF10-a...
PS-Policies-on-Enrolment-Transfer-of-Docs-Checking-of-School-Forms-and-SF10-a...PS-Policies-on-Enrolment-Transfer-of-Docs-Checking-of-School-Forms-and-SF10-a...
PS-Policies-on-Enrolment-Transfer-of-Docs-Checking-of-School-Forms-and-SF10-a...nhezmainit1
 
Model Attribute _rec_name in the Odoo 17
Model Attribute _rec_name in the Odoo 17Model Attribute _rec_name in the Odoo 17
Model Attribute _rec_name in the Odoo 17Celine George
 
Andreas Schleicher presents at the launch of What does child empowerment mean...
Andreas Schleicher presents at the launch of What does child empowerment mean...Andreas Schleicher presents at the launch of What does child empowerment mean...
Andreas Schleicher presents at the launch of What does child empowerment mean...EduSkills OECD
 

Dernier (20)

Analyzing and resolving a communication crisis in Dhaka textiles LTD.pptx
Analyzing and resolving a communication crisis in Dhaka textiles LTD.pptxAnalyzing and resolving a communication crisis in Dhaka textiles LTD.pptx
Analyzing and resolving a communication crisis in Dhaka textiles LTD.pptx
 
Stl Algorithms in C++ jjjjjjjjjjjjjjjjjj
Stl Algorithms in C++ jjjjjjjjjjjjjjjjjjStl Algorithms in C++ jjjjjjjjjjjjjjjjjj
Stl Algorithms in C++ jjjjjjjjjjjjjjjjjj
 
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...
 
OS-operating systems- ch05 (CPU Scheduling) ...
OS-operating systems- ch05 (CPU Scheduling) ...OS-operating systems- ch05 (CPU Scheduling) ...
OS-operating systems- ch05 (CPU Scheduling) ...
 
Personalisation of Education by AI and Big Data - Lourdes Guàrdia
Personalisation of Education by AI and Big Data - Lourdes GuàrdiaPersonalisation of Education by AI and Big Data - Lourdes Guàrdia
Personalisation of Education by AI and Big Data - Lourdes Guàrdia
 
Contoh Aksi Nyata Refleksi Diri ( NUR ).pdf
Contoh Aksi Nyata Refleksi Diri ( NUR ).pdfContoh Aksi Nyata Refleksi Diri ( NUR ).pdf
Contoh Aksi Nyata Refleksi Diri ( NUR ).pdf
 
Major project report on Tata Motors and its marketing strategies
Major project report on Tata Motors and its marketing strategiesMajor project report on Tata Motors and its marketing strategies
Major project report on Tata Motors and its marketing strategies
 
When Quality Assurance Meets Innovation in Higher Education - Report launch w...
When Quality Assurance Meets Innovation in Higher Education - Report launch w...When Quality Assurance Meets Innovation in Higher Education - Report launch w...
When Quality Assurance Meets Innovation in Higher Education - Report launch w...
 
Observing-Correct-Grammar-in-Making-Definitions.pptx
Observing-Correct-Grammar-in-Making-Definitions.pptxObserving-Correct-Grammar-in-Making-Definitions.pptx
Observing-Correct-Grammar-in-Making-Definitions.pptx
 
SPLICE Working Group: Reusable Code Examples
SPLICE Working Group:Reusable Code ExamplesSPLICE Working Group:Reusable Code Examples
SPLICE Working Group: Reusable Code Examples
 
8 Tips for Effective Working Capital Management
8 Tips for Effective Working Capital Management8 Tips for Effective Working Capital Management
8 Tips for Effective Working Capital Management
 
VAMOS CUIDAR DO NOSSO PLANETA! .
VAMOS CUIDAR DO NOSSO PLANETA!                    .VAMOS CUIDAR DO NOSSO PLANETA!                    .
VAMOS CUIDAR DO NOSSO PLANETA! .
 
How to Send Pro Forma Invoice to Your Customers in Odoo 17
How to Send Pro Forma Invoice to Your Customers in Odoo 17How to Send Pro Forma Invoice to Your Customers in Odoo 17
How to Send Pro Forma Invoice to Your Customers in Odoo 17
 
OSCM Unit 2_Operations Processes & Systems
OSCM Unit 2_Operations Processes & SystemsOSCM Unit 2_Operations Processes & Systems
OSCM Unit 2_Operations Processes & Systems
 
What is 3 Way Matching Process in Odoo 17.pptx
What is 3 Way Matching Process in Odoo 17.pptxWhat is 3 Way Matching Process in Odoo 17.pptx
What is 3 Way Matching Process in Odoo 17.pptx
 
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...
TỔNG HỢP HƠN 100 ĐỀ THI THỬ TỐT NGHIỆP THPT TOÁN 2024 - TỪ CÁC TRƯỜNG, TRƯỜNG...
 
PS-Policies-on-Enrolment-Transfer-of-Docs-Checking-of-School-Forms-and-SF10-a...
PS-Policies-on-Enrolment-Transfer-of-Docs-Checking-of-School-Forms-and-SF10-a...PS-Policies-on-Enrolment-Transfer-of-Docs-Checking-of-School-Forms-and-SF10-a...
PS-Policies-on-Enrolment-Transfer-of-Docs-Checking-of-School-Forms-and-SF10-a...
 
Model Attribute _rec_name in the Odoo 17
Model Attribute _rec_name in the Odoo 17Model Attribute _rec_name in the Odoo 17
Model Attribute _rec_name in the Odoo 17
 
Mattingly "AI and Prompt Design: LLMs with NER"
Mattingly "AI and Prompt Design: LLMs with NER"Mattingly "AI and Prompt Design: LLMs with NER"
Mattingly "AI and Prompt Design: LLMs with NER"
 
Andreas Schleicher presents at the launch of What does child empowerment mean...
Andreas Schleicher presents at the launch of What does child empowerment mean...Andreas Schleicher presents at the launch of What does child empowerment mean...
Andreas Schleicher presents at the launch of What does child empowerment mean...
 

12 x1 t04 05 displacement, velocity, acceleration (2013)

  • 1. Applications of Calculus To The Physical World
  • 2. Applications of Calculus To The Physical World Displacement (x) Distance from a point, with direction.
  • 3. Applications of Calculus To The Physical World Displacement (x) Distance from a point, with direction.  v, dx , x  Velocity    dt  The rate of change of displacement with respect to time i.e. speed with direction.
  • 4. Applications of Calculus To The Physical World Displacement (x) Distance from a point, with direction.  v, dx , x  Velocity    dt  The rate of change of displacement with respect to time i.e. speed with direction.  dv d 2 x  Acceleration  a, , 2 , , v  x   dt dt  The rate of change of velocity with respect to time
  • 5. Applications of Calculus To The Physical World Displacement (x) Distance from a point, with direction.  v, dx , x  Velocity    dt  The rate of change of displacement with respect to time i.e. speed with direction.  dv d 2 x  Acceleration  a, , 2 , , v  x   dt dt  The rate of change of velocity with respect to time NOTE: “deceleration” or slowing down is when acceleration is in the opposite direction to velocity.
  • 6. Displacement differentiate Velocity Acceleration
  • 7. Displacement differentiate Velocity integrate Acceleration
  • 8. x 2 1 1 2 3 4 t -1 -2
  • 9. x 2 slope=instantaneous velocity 1 1 2 3 4 t -1 -2
  • 10. x 2 slope=instantaneous velocity 1 1 2 3 4 t -1 -2  x 1 2 3 4 t
  • 11. x 2 slope=instantaneous velocity 1 1 2 3 4 t -1 -2 slope=instantaneous acceleration  x 1 2 3 4 t
  • 12. x 2 slope=instantaneous velocity 1 1 2 3 4 t -1 -2 slope=instantaneous acceleration  x 1 2 3 4 t  x 1 2 3 4 t
  • 13. x 2 slope=instantaneous velocity 1 1 2 3 4 t -1 e.g. (i) distance traveled  7 m -2 slope=instantaneous acceleration  x 1 2 3 4 t  x 1 2 3 4 t
  • 14. x 2 slope=instantaneous velocity 1 1 2 3 4 t -1 e.g. (i) distance traveled  7 m -2 slope=instantaneous acceleration (ii) total displacement  1m  x 1 2 3 4 t  x 1 2 3 4 t
  • 15. x 2 slope=instantaneous velocity 1 1 2 3 4 t -1 e.g. (i) distance traveled  7 m -2 slope=instantaneous acceleration (ii) total displacement  1m  x 7 (iii) average speed  m/s 4 1 2 3 4 t  x 1 2 3 4 t
  • 16. x 2 slope=instantaneous velocity 1 1 2 3 4 t -1 e.g. (i) distance traveled  7 m -2 slope=instantaneous acceleration (ii) total displacement  1m  x 7 (iii) average speed  m/s 4 1 1 2 3 4 t (iv) average velocity  m/s 4  x 1 2 3 4 t
  • 17. e.g. (i) The displacement x from the origin at time t seconds, of a particle traveling in a straight line is given by the formula x  t 3  21t 2 a) Find the acceleration of the particle at time t.
  • 18. e.g. (i) The displacement x from the origin at time t seconds, of a particle traveling in a straight line is given by the formula x  t 3  21t 2 a) Find the acceleration of the particle at time t. x  t 3  21t 2 v  3t 2  42t a  6t  42
  • 19. e.g. (i) The displacement x from the origin at time t seconds, of a particle traveling in a straight line is given by the formula x  t 3  21t 2 a) Find the acceleration of the particle at time t. x  t 3  21t 2 v  3t 2  42t a  6t  42 b) Find the times when the particle is stationary.
  • 20. e.g. (i) The displacement x from the origin at time t seconds, of a particle traveling in a straight line is given by the formula x  t 3  21t 2 a) Find the acceleration of the particle at time t. x  t 3  21t 2 v  3t 2  42t a  6t  42 b) Find the times when the particle is stationary. Particle is stationary when v = 0 i.e. 3t 2  42t  0
  • 21. e.g. (i) The displacement x from the origin at time t seconds, of a particle traveling in a straight line is given by the formula x  t 3  21t 2 a) Find the acceleration of the particle at time t. x  t 3  21t 2 v  3t 2  42t a  6t  42 b) Find the times when the particle is stationary. Particle is stationary when v = 0 i.e. 3t 2  42t  0 3t t  14   0 t  0 or t  14 Particle is stationary initially and again after 14 seconds
  • 22. (ii) A particle is moving on the x axis. It started from rest at t = 0 from the point x = 7. If its acceleration at time t is 2 + 6t find the position of the particle when t = 3.
  • 23. (ii) A particle is moving on the x axis. It started from rest at t = 0 from the point x = 7. If its acceleration at time t is 2 + 6t find the position of the particle when t = 3. a  2  6t v  2t  3t 2  c
  • 24. (ii) A particle is moving on the x axis. It started from rest at t = 0 from the point x = 7. If its acceleration at time t is 2 + 6t find the position of the particle when t = 3. a  2  6t v  2t  3t 2  c when t  0, v  0 i.e. 0  0  0  c c0
  • 25. (ii) A particle is moving on the x axis. It started from rest at t = 0 from the point x = 7. If its acceleration at time t is 2 + 6t find the position of the particle when t = 3. a  2  6t v  2t  3t 2  c when t  0, v  0 i.e. 0  0  0  c c0  v  2t  3t 2
  • 26. (ii) A particle is moving on the x axis. It started from rest at t = 0 from the point x = 7. If its acceleration at time t is 2 + 6t find the position of the particle when t = 3. a  2  6t v  2t  3t 2  c when t  0, v  0 i.e. 0  0  0  c c0  v  2t  3t 2 x  t2  t3  c
  • 27. (ii) A particle is moving on the x axis. It started from rest at t = 0 from the point x = 7. If its acceleration at time t is 2 + 6t find the position of the particle when t = 3. a  2  6t v  2t  3t 2  c when t  0, v  0 i.e. 0  0  0  c c0  v  2t  3t 2 x  t2  t3  c when t  0, x  7 i.e. 7  0  0  c c7
  • 28. (ii) A particle is moving on the x axis. It started from rest at t = 0 from the point x = 7. If its acceleration at time t is 2 + 6t find the position of the particle when t = 3. a  2  6t v  2t  3t 2  c when t  0, v  0 i.e. 0  0  0  c c0  v  2t  3t 2 x  t2  t3  c when t  0, x  7 i.e. 7  0  0  c c7  x  t2  t3  7
  • 29. (ii) A particle is moving on the x axis. It started from rest at t = 0 from the point x = 7. If its acceleration at time t is 2 + 6t find the position of the particle when t = 3. a  2  6t when t  3, x  32  33  7 v  2t  3t 2  c  43 when t  0, v  0 after 3 seconds the particle is 43 i.e. 0  0  0  c units to the right of O. c0  v  2t  3t 2 x  t2  t3  c when t  0, x  7 i.e. 7  0  0  c c7  x  t2  t3  7
  • 30. e.g. 2001 HSC Question 7c) A particle moves in a straight line so that its displacement, in metres, is given by t2 x t2 where t is measured in seconds. (i) What is the displacement when t = 0?
  • 31. e.g. 2001 HSC Question 7c) A particle moves in a straight line so that its displacement, in metres, is given by t2 x t2 where t is measured in seconds. (i) What is the displacement when t = 0? 02 when t  0, x  02 = 1  the particle is 1 metre to the left of the origin
  • 32. e.g. 2001 HSC Question 7c) A particle moves in a straight line so that its displacement, in metres, is given by t2 x t2 where t is measured in seconds. (i) What is the displacement when t = 0? 02 when t  0, x  02 = 1  the particle is 1 metre to the left of the origin 4 (ii) Show that x  1  t2 Hence find expressions for the velocity and the acceleration in terms of t.
  • 33. e.g. 2001 HSC Question 7c) A particle moves in a straight line so that its displacement, in metres, is given by t2 x t2 where t is measured in seconds. (i) What is the displacement when t = 0? 02 when t  0, x  02 = 1  the particle is 1 metre to the left of the origin 4 (ii) Show that x  1  t2 Hence find expressions for the velocity and the acceleration in terms of t. 4 t 24 1  t2 t2 t2  4 t  2  x  1 t2
  • 34. e.g. 2001 HSC Question 7c) A particle moves in a straight line so that its displacement, in metres, is given by t2 x t2 where t is measured in seconds. (i) What is the displacement when t = 0? 02 when t  0, x  02 = 1  the particle is 1 metre to the left of the origin 4 (ii) Show that x  1  t2 Hence find expressions for the velocity and the acceleration in terms of t. 4 t 24 4  1 1  v t2 t2 t  2 2 t2  4 v 4 t  2  x  1  t  2 2 t2
  • 35. e.g. 2001 HSC Question 7c) A particle moves in a straight line so that its displacement, in metres, is given by t2 x t2 where t is measured in seconds. (i) What is the displacement when t = 0? 02 when t  0, x  02 = 1  the particle is 1 metre to the left of the origin 4 (ii) Show that x  1  t2 Hence find expressions for the velocity and the acceleration in terms of t. t 24 4  1 4  2  t  2  1 1 4 1  v a t2 t2 t  2  t  2 2 4 t2 8  4 v 4 a t  2  x  1  t  2 2  t  2 3 t2
  • 36. (iii) Is the particle ever at rest? Give reasons for your answer.
  • 37. (iii) Is the particle ever at rest? Give reasons for your answer. 4 v 2  0 t  2  the particle is never at rest
  • 38. (iii) Is the particle ever at rest? Give reasons for your answer. 4 v 2  0 t  2  the particle is never at rest (iv) What is the limiting velocity of the particle as t increases indefinitely?
  • 39. (iii) Is the particle ever at rest? Give reasons for your answer. 4 v 2  0 t  2  the particle is never at rest (iv) What is the limiting velocity of the particle as t increases indefinitely? 4 lim v  lim t    t  t  2 2
  • 40. (iii) Is the particle ever at rest? Give reasons for your answer. 4 v 2  0 t  2  the particle is never at rest (iv) What is the limiting velocity of the particle as t increases indefinitely? 4 lim v  lim t    t  t  2 2 0
  • 41. (iii) Is the particle ever at rest? Give reasons for your answer. 4 v 2  0 t  2  the particle is never at rest (iv) What is the limiting velocity of the particle as t increases indefinitely? 4 v lim v  lim OR t    t  t  2 2 4 v 0 1 t  2 2 t
  • 42. (iii) Is the particle ever at rest? Give reasons for your answer. 4 v 2  0 t  2  the particle is never at rest (iv) What is the limiting velocity of the particle as t increases indefinitely? 4 v lim v  lim OR t    t  t  2 2 4 v 0 1 t  2 2 t  the limiting velocity of the particle is 0 m/s
  • 43. (ii) 2002 HSC Question 8b) A particle moves in a straight line. At time t seconds, its distance x metres from a fixed point O in the line is given by x  sin 2t  3 (i) Sketch the graph of x as a function of t for 0  t  2
  • 44. (ii) 2002 HSC Question 8b) A particle moves in a straight line. At time t seconds, its distance x metres from a fixed point O in the line is given by x  sin 2t  3 (i) Sketch the graph of x as a function of t for 0  t  2 2  amplitude  1 unit period  divisions  2 4 shift  3 units 
  • 45. (ii) 2002 HSC Question 8b) A particle moves in a straight line. At time t seconds, its distance x metres from a fixed point O in the line is given by x  sin 2t  3 (i) Sketch the graph of x as a function of t for 0  t  2 2  amplitude  1 unit period  divisions  2 4 shift  3 units  x 4 3 2 1   3  5 3 7 2 t 4 2 4 4 2 4
  • 46. (ii) 2002 HSC Question 8b) A particle moves in a straight line. At time t seconds, its distance x metres from a fixed point O in the line is given by x  sin 2t  3 (i) Sketch the graph of x as a function of t for 0  t  2 2  amplitude  1 unit period  divisions  2 4 shift  3 units  x 4 3 2 1   3  5 3 7 2 t 4 2 4 4 2 4
  • 47. (ii) 2002 HSC Question 8b) A particle moves in a straight line. At time t seconds, its distance x metres from a fixed point O in the line is given by x  sin 2t  3 (i) Sketch the graph of x as a function of t for 0  t  2 2  amplitude  1 unit period  divisions  2 4 shift  3 units  x 4 3 2 1   3  5 3 7 2 t 4 2 4 4 2 4
  • 48. (ii) 2002 HSC Question 8b) A particle moves in a straight line. At time t seconds, its distance x metres from a fixed point O in the line is given by x  sin 2t  3 (i) Sketch the graph of x as a function of t for 0  t  2 2  amplitude  1 unit period  divisions  2 4 shift  3 units  x 4 3 2 1   3  5 3 7 2 t 4 2 4 4 2 4
  • 49. (ii) 2002 HSC Question 8b) A particle moves in a straight line. At time t seconds, its distance x metres from a fixed point O in the line is given by x  sin 2t  3 (i) Sketch the graph of x as a function of t for 0  t  2 2  amplitude  1 unit period  divisions  2 4 shift  3 units  x 4 x  sin 2t  3 3 2 1   3  5 3 7 2 t 4 2 4 4 2 4
  • 50. (ii) Using your graph, or otherwise, find the times when the particle is at rest, and the position of the particle at those times.
  • 51. (ii) Using your graph, or otherwise, find the times when the particle is at rest, and the position of the particle at those times. Particle is at rest when velocity = 0 dx  0 i.e. the stationary points dt
  • 52. (ii) Using your graph, or otherwise, find the times when the particle is at rest, and the position of the particle at those times. Particle is at rest when velocity = 0 dx  0 i.e. the stationary points dt  when t  seconds, x  4 metres 4 3 t seconds, x  2 metres 4 5 t seconds, x  4 metres 4 7 t seconds, x  2 metres 4
  • 53. (ii) Using your graph, or otherwise, find the times when the particle is at rest, and the position of the particle at those times. Particle is at rest when velocity = 0 dx  0 i.e. the stationary points dt  when t  seconds, x  4 metres 4 3 t seconds, x  2 metres 4 5 t seconds, x  4 metres 4 7 t seconds, x  2 metres 4 (iii) Describe the motion completely.
  • 54. (ii) Using your graph, or otherwise, find the times when the particle is at rest, and the position of the particle at those times. Particle is at rest when velocity = 0 dx  0 i.e. the stationary points dt  when t  seconds, x  4 metres 4 3 t seconds, x  2 metres 4 5 t seconds, x  4 metres 4 7 t seconds, x  2 metres 4 (iii) Describe the motion completely. The particle oscillates between x=2 and x=4 with a period of  seconds
  • 55. Exercise 3B; 2, 4, 6, 8, 10, 12