SlideShare uma empresa Scribd logo
1 de 73
Stage 2 Physics

         Section 1
Motion in Two Dimensions
What is motion?
What types of motion are there?

What causes motion?

How to we describe motion in Physics?
What is a vector?
Vector quantities have magnitude (size) and
direction.

Scalar quantities have magnitude only.

Length represents the vectors magnitude.
Scalar         Vector
Distance      Displacement
Speed         Velocity
Mass          Acceleration
              Force
Time          weight
Velocity vector of an angry bird
Resultant of Two Vectors
The resultant is the sum or the combined addition of two vector
quantities

Vectors in the same direction:
       6N      4N      =          10 N




 Vectors in opposite directions:
        6m                 10 m          =
Vectors
• Vectors can be oriented to the gravitational
  field (up, down or some angle to the
  horizontal) or compass points (NESW).


             5 ms-1



                 5 ms-1 30o above the horizontal
Velocity Vectors
• Velocity can be resolved into its horizontal
  and vertical components at any instant.

                  v
                                vV



                   vH
SOHCAHTOA

       Hypotenuse
                       Opposite

            Adjacent
v
             vV = v sin



vH = v cos
Example 1
Resolve the following velocity vector into its
 horizontal and vertical components




               30o
Example 1
Resolve the following velocity vector into its
 horizontal and vertical components




               30o
This problem can be solved in two ways
(and you need to be able to do both)

1. Scale Diagram
2. Trigonometry
1. Scale diagram

By drawing a vector diagram (using a
protractor and a ruler) to scale we can
simply measure the size of the
components ideally the vector should be
10 cm or larger (for accuracy)
2. Trigonometry
            vvertical = v sin
                      = 40 sin 30o
                      = 20 m s-1

            vhorizontal = v cos
30o
                        = 40 cos 30o
                       = 34.6 m s-1
Example 2
Determine the velocity vector with initial
horizontal velocity component of 50 ms –1
and vertical 20 ms-1.
v=?
                    vv= 20 m s-1


      vh= 50 m s-
                1
1. Scale diagram
 Again we could accurately draw the figure
 and measure the resultant length and
 angle to find the direction of v.

(Note: You need to have a clear Perspex
  ruler and a protractor for EVERY test and
  exam)
2. Pythagoras & Trigonometry
  By Pythagoras theory:
v2 = vV2 + vH2
      v = v V 2 + vH 2
        = 202 + 502
        = 2900
        = 53.9 m s-1   v=?                     vv= 20 m s-1


                             vh= 50 m s-   1
tan     vV/vH
tan   = 20/50
        = 21.8o

ie. v = 53.9 m s-1 at 21.8o above the horizontal
Summary – Vectors in 2D
• Given any vector quantity in 2D it can be
  resolved into horizontal and vertical
  components
  eg displacement, force, fields etc
• Given the horizontal & vertical
  components you can determine magnitude
  and direction of the vector (formula)
Motion in a Uniform
Gravitational Field
In the absence of gravity objects move with
  constant velocity in a straight line.


  An object will remain at rest, or continue to move
  at a constant velocity, unless a net force acts on
  it.

Note: The following is all in the absence of air resistance.
When an object falls under the
influence of gravity, the vertical
force causes a constant
acceleration
vH

       The resultant motion is a
            combination of both
                 horizontal and
        vH
                        vertical
vV   vV            components
Horizontal Projection
                       While the vertical
                             component
                             undergoes
                               constant
If an object is            acceleration.
projected
horizontally, the
horizontal component
moves with constant
velocity.
Three equations of motion

Note that all the equations have “a” in them –
they only apply under CONSTANT acceleration
Constant vertical acceleration
                                  Vertical formulae
                                                 2
                                       v 2 v0         2as

                                                     1 2
Horizontal velocity is constant         s   vt         at
                                                     2
Horizontal formula
                                    v vo             at

                 s
        vH
             t
Three equations of motion
Learning Symbols in Physics
Quantity   Quantity Symbol   Units   Unit symbol
Example

A stone is dropped down a well and takes 3
seconds to hit the ground.
a) How fast does it hit the bottom?

b) How deep is the well?
A stone is dropped down a well at
takes 3 seconds to hit the ground.
a) How fast does it hit the bottom?
b) How deep is the well?
An arrow is fired upwards at 50ms-1.
a) How high does the arrow fly?
An arrow is fired upwards at 50ms-1.
b) How long does the arrow take to hit the
ground?
Projectile Motion Problems

Except for time, everything can be separated into horizontal and
  vertical components and treated separately.




                             sV = height
 V0




                         s H = range
                                       t = time of flight
Projectile Motion Problems
Horizontal projection: down is +ve
Uni-level projection: Up is considered positive, and down is
  negative.(Acceleration due to gravity aV = -9.8ms-2)




                             sV = height
 V0




                         s H = range
                                       t = time of flight
Projectile Motion Problems

At the top of the parabolic path, vV= 0 ms-1

                                               1
                                    vV   0ms                          2
                                                     aV
                                                              9.8ms



                          sV   height
 V0




                     sH   range
                                         t = time of flight
Projectile Motion Problems

Remember the time of flight is the time it takes to go up+ down.

                                               1
                                    vV   0ms                          2
                                                     aV
                                                              9.8ms



                          sV   height
 V0




                     sH   range
                                         t = time of flight
Example 1
Bi-level projection
• An object is projected at a height
Maximum Range

To get the maximum range sH max in a vacuum
(no air resistance) the launch angle must be 45o




                  sH max
For a projectile launched at ground level find
 by sample calculation the launch angle
 that results in a maximum range
Pairs of launch angles that yield the same
  range add up to 90o      α + θ = ranges
                           Projectile 90o
                               for various angles of launch
         500
         450
         400
         350
         300
height




         250
         200
         150
         100
         50
          0
               0   200   400     600      800      1000       1200
                               range
α + θ = 90o

Find the launch angle that yields the same
  range as 32o

θ = 32    α=?              α + θ = 90o
The Effect of Air Resistance
Air resistance acts in the opposite direction
  to motion.
      vertical             horizontal
The Effect of Air Resistance
       vertical                      horizontal




This decreases the
• height
• range
Slight decrease in time of flight of the projectile
The magnitude of Fair resistance


           Fair resistance
Speed
Shape
Aerodynamic

teardrop
Size
More surface area = more air resistance
Texture


Smooth




Rough
Air density
Low air density = less air resistance




High air density = high air resistance
Projectiles in Sport
Consider the effect of launch height on
 range
As the object has further to fall tflight is
increased.
As the object is in the air for longer it
travels farther.
45o

                 41o




  For objects at h=0 the optimal angle is 45o
For heights › 0
θ max height is less than 45o

Mais conteúdo relacionado

Mais procurados

Projectile
ProjectileProjectile
ProjectileAnjani
 
Introduction to Kinematics
Introduction to KinematicsIntroduction to Kinematics
Introduction to Kinematicsdryadav1300
 
Chapter 7 part 1 - conservation of momentum in 1 d
Chapter 7   part 1 - conservation of momentum in 1 dChapter 7   part 1 - conservation of momentum in 1 d
Chapter 7 part 1 - conservation of momentum in 1 dconquerer742
 
Displacement and Velocity
Displacement and VelocityDisplacement and Velocity
Displacement and Velocitymlong24
 
Kinematic equations of motion
Kinematic equations of motionKinematic equations of motion
Kinematic equations of motionmantlfin
 
Force and Acceleration
Force and AccelerationForce and Acceleration
Force and Accelerationrdk.rdk
 
Ch 2 One Dimensional Kinematics
Ch 2 One Dimensional KinematicsCh 2 One Dimensional Kinematics
Ch 2 One Dimensional KinematicsScott Thomas
 
Ch 3 Two Dimensional Kinematics
Ch 3 Two Dimensional KinematicsCh 3 Two Dimensional Kinematics
Ch 3 Two Dimensional KinematicsScott Thomas
 
Chapter : Force And Motion
Chapter : Force And MotionChapter : Force And Motion
Chapter : Force And Motiontehminafaizan
 
Nature and types of forces
Nature and types of forcesNature and types of forces
Nature and types of forcesmaryjane0116
 
Physics -vectors-projectile motion
Physics  -vectors-projectile motionPhysics  -vectors-projectile motion
Physics -vectors-projectile motionstephm32
 
Projecctile motion by sanjeev
Projecctile motion by sanjeev Projecctile motion by sanjeev
Projecctile motion by sanjeev sanjeev prajapati
 
Motion in two dimensions
Motion in two dimensionsMotion in two dimensions
Motion in two dimensionsmstf mstf
 
Momentum ppt physics grade 11
Momentum ppt physics grade 11Momentum ppt physics grade 11
Momentum ppt physics grade 11SaminaTariq5
 

Mais procurados (20)

Projectile
ProjectileProjectile
Projectile
 
Introduction to Kinematics
Introduction to KinematicsIntroduction to Kinematics
Introduction to Kinematics
 
Chapter 7 part 1 - conservation of momentum in 1 d
Chapter 7   part 1 - conservation of momentum in 1 dChapter 7   part 1 - conservation of momentum in 1 d
Chapter 7 part 1 - conservation of momentum in 1 d
 
Torque
TorqueTorque
Torque
 
Kinematics
KinematicsKinematics
Kinematics
 
Displacement and Velocity
Displacement and VelocityDisplacement and Velocity
Displacement and Velocity
 
Kinematic equations of motion
Kinematic equations of motionKinematic equations of motion
Kinematic equations of motion
 
Free fall
Free fallFree fall
Free fall
 
Force and Acceleration
Force and AccelerationForce and Acceleration
Force and Acceleration
 
Ch 2 One Dimensional Kinematics
Ch 2 One Dimensional KinematicsCh 2 One Dimensional Kinematics
Ch 2 One Dimensional Kinematics
 
Ch 3 Two Dimensional Kinematics
Ch 3 Two Dimensional KinematicsCh 3 Two Dimensional Kinematics
Ch 3 Two Dimensional Kinematics
 
Chapter : Force And Motion
Chapter : Force And MotionChapter : Force And Motion
Chapter : Force And Motion
 
Scalars and Vectors
Scalars and VectorsScalars and Vectors
Scalars and Vectors
 
Errors and uncertainties in physics
Errors and uncertainties in physicsErrors and uncertainties in physics
Errors and uncertainties in physics
 
Inertia
InertiaInertia
Inertia
 
Nature and types of forces
Nature and types of forcesNature and types of forces
Nature and types of forces
 
Physics -vectors-projectile motion
Physics  -vectors-projectile motionPhysics  -vectors-projectile motion
Physics -vectors-projectile motion
 
Projecctile motion by sanjeev
Projecctile motion by sanjeev Projecctile motion by sanjeev
Projecctile motion by sanjeev
 
Motion in two dimensions
Motion in two dimensionsMotion in two dimensions
Motion in two dimensions
 
Momentum ppt physics grade 11
Momentum ppt physics grade 11Momentum ppt physics grade 11
Momentum ppt physics grade 11
 

Destaque

Projectile motion
Projectile motionProjectile motion
Projectile motionmiss mitch
 
Presentation1
Presentation1Presentation1
Presentation1ghelhie
 
Projectile Motion
Projectile MotionProjectile Motion
Projectile MotionArlo Alegre
 
Physics 504 Chapter 11 The Motion of Projectiles
Physics 504 Chapter 11 The Motion of ProjectilesPhysics 504 Chapter 11 The Motion of Projectiles
Physics 504 Chapter 11 The Motion of ProjectilesNeil MacIntosh
 
Recent Developments on the Employer's Duty to Accommodate
Recent Developments on the Employer's Duty to AccommodateRecent Developments on the Employer's Duty to Accommodate
Recent Developments on the Employer's Duty to AccommodateDLA Piper (Canada) LLP
 
Science 9, Module 1: Cell Division
Science 9, Module 1: Cell DivisionScience 9, Module 1: Cell Division
Science 9, Module 1: Cell DivisionClaire Thompson
 
SCIENCE 9 MODULE
SCIENCE 9 MODULESCIENCE 9 MODULE
SCIENCE 9 MODULEGly Anao
 
Displacement, velocity, acceleration
Displacement, velocity, accelerationDisplacement, velocity, acceleration
Displacement, velocity, accelerationmiss mitch
 
Uri ng Panlapi Demoslides
Uri ng Panlapi DemoslidesUri ng Panlapi Demoslides
Uri ng Panlapi DemoslidesMJ1129
 
032616 week3 conservation of mechanical energy
032616 week3 conservation of mechanical energy032616 week3 conservation of mechanical energy
032616 week3 conservation of mechanical energySubas Nandy
 
Projectile motion Grade 9
Projectile motion Grade 9Projectile motion Grade 9
Projectile motion Grade 9Pearl Llagas
 

Destaque (20)

Vectors projectile motion
Vectors projectile motionVectors projectile motion
Vectors projectile motion
 
Projectile motion
Projectile motionProjectile motion
Projectile motion
 
Presentation1
Presentation1Presentation1
Presentation1
 
Projectile Motion
Projectile MotionProjectile Motion
Projectile Motion
 
1.2.1 projectile motion
1.2.1   projectile motion1.2.1   projectile motion
1.2.1 projectile motion
 
human rights
human rightshuman rights
human rights
 
Physics 504 Chapter 11 The Motion of Projectiles
Physics 504 Chapter 11 The Motion of ProjectilesPhysics 504 Chapter 11 The Motion of Projectiles
Physics 504 Chapter 11 The Motion of Projectiles
 
3 - Projectiles
3 - Projectiles3 - Projectiles
3 - Projectiles
 
Introduction to php
Introduction to phpIntroduction to php
Introduction to php
 
Chapter10
Chapter10Chapter10
Chapter10
 
Recent Developments on the Employer's Duty to Accommodate
Recent Developments on the Employer's Duty to AccommodateRecent Developments on the Employer's Duty to Accommodate
Recent Developments on the Employer's Duty to Accommodate
 
What causes motion
What causes motionWhat causes motion
What causes motion
 
Science 9, Module 1: Cell Division
Science 9, Module 1: Cell DivisionScience 9, Module 1: Cell Division
Science 9, Module 1: Cell Division
 
SCIENCE 9 MODULE
SCIENCE 9 MODULESCIENCE 9 MODULE
SCIENCE 9 MODULE
 
Forces
ForcesForces
Forces
 
Puva therapy
Puva therapyPuva therapy
Puva therapy
 
Displacement, velocity, acceleration
Displacement, velocity, accelerationDisplacement, velocity, acceleration
Displacement, velocity, acceleration
 
Uri ng Panlapi Demoslides
Uri ng Panlapi DemoslidesUri ng Panlapi Demoslides
Uri ng Panlapi Demoslides
 
032616 week3 conservation of mechanical energy
032616 week3 conservation of mechanical energy032616 week3 conservation of mechanical energy
032616 week3 conservation of mechanical energy
 
Projectile motion Grade 9
Projectile motion Grade 9Projectile motion Grade 9
Projectile motion Grade 9
 

Semelhante a Vectors and projectile motion and worked examples

Two Dimensional Motion and Vectors
Two Dimensional Motion and VectorsTwo Dimensional Motion and Vectors
Two Dimensional Motion and VectorsZBTHS
 
4. Motion in a Plane 1.pptx.pdf
4. Motion in a Plane 1.pptx.pdf4. Motion in a Plane 1.pptx.pdf
4. Motion in a Plane 1.pptx.pdfMKumarVarnana
 
Physics unit 1 kinematics.ppt
Physics unit 1 kinematics.pptPhysics unit 1 kinematics.ppt
Physics unit 1 kinematics.pptssuser5087b61
 
1 d chapter 2
1 d chapter 21 d chapter 2
1 d chapter 2mantlfin
 
Projectile motion ch 5 reg
Projectile motion ch 5 regProjectile motion ch 5 reg
Projectile motion ch 5 regZBTHS
 
Derivation of Kinematic Equations
Derivation of Kinematic EquationsDerivation of Kinematic Equations
Derivation of Kinematic Equationsomar_egypt
 
Chapter 3
Chapter 3Chapter 3
Chapter 3ZBTHS
 
Motion 2 d
Motion  2 dMotion  2 d
Motion 2 dwpchem81
 
Projectile motion
Projectile motionProjectile motion
Projectile motionstephm32
 
Projectile motionchemistory (4)
Projectile motionchemistory (4)Projectile motionchemistory (4)
Projectile motionchemistory (4)Sahil Raturi
 
Graphing Motion grade 7 powerpoint presentation
Graphing Motion grade 7 powerpoint presentationGraphing Motion grade 7 powerpoint presentation
Graphing Motion grade 7 powerpoint presentationGiaMacayPacaa
 
Projectile motionchemistory (4)
Projectile motionchemistory (4)Projectile motionchemistory (4)
Projectile motionchemistory (4)Sahil Raturi
 
Lecture Ch 03
Lecture Ch 03Lecture Ch 03
Lecture Ch 03rtrujill
 
Kinematics of Linear Motion​
Kinematics of Linear Motion​Kinematics of Linear Motion​
Kinematics of Linear Motion​Reema
 
Physics 504 Chapter 10 Uniformly Accelerated Rectilinear Motion
Physics 504 Chapter 10 Uniformly Accelerated Rectilinear MotionPhysics 504 Chapter 10 Uniformly Accelerated Rectilinear Motion
Physics 504 Chapter 10 Uniformly Accelerated Rectilinear MotionNeil MacIntosh
 
Motion in a plane chapter 3 converted
Motion in  a plane chapter 3 convertedMotion in  a plane chapter 3 converted
Motion in a plane chapter 3 convertedAbhirajAshokPV
 

Semelhante a Vectors and projectile motion and worked examples (20)

Two Dimensional Motion and Vectors
Two Dimensional Motion and VectorsTwo Dimensional Motion and Vectors
Two Dimensional Motion and Vectors
 
4. Motion in a Plane 1.pptx.pdf
4. Motion in a Plane 1.pptx.pdf4. Motion in a Plane 1.pptx.pdf
4. Motion in a Plane 1.pptx.pdf
 
Kinemetics
KinemeticsKinemetics
Kinemetics
 
Chap7
Chap7Chap7
Chap7
 
Physics unit 1 kinematics.ppt
Physics unit 1 kinematics.pptPhysics unit 1 kinematics.ppt
Physics unit 1 kinematics.ppt
 
1 d chapter 2
1 d chapter 21 d chapter 2
1 d chapter 2
 
Projectile motion ch 5 reg
Projectile motion ch 5 regProjectile motion ch 5 reg
Projectile motion ch 5 reg
 
Projectile Motion 2.ppt
Projectile Motion 2.pptProjectile Motion 2.ppt
Projectile Motion 2.ppt
 
Derivation of Kinematic Equations
Derivation of Kinematic EquationsDerivation of Kinematic Equations
Derivation of Kinematic Equations
 
Chapter 3
Chapter 3Chapter 3
Chapter 3
 
Motion 2 d
Motion  2 dMotion  2 d
Motion 2 d
 
Projectile motion
Projectile motionProjectile motion
Projectile motion
 
Projectile motionchemistory (4)
Projectile motionchemistory (4)Projectile motionchemistory (4)
Projectile motionchemistory (4)
 
Graphing Motion grade 7 powerpoint presentation
Graphing Motion grade 7 powerpoint presentationGraphing Motion grade 7 powerpoint presentation
Graphing Motion grade 7 powerpoint presentation
 
Projectile motionchemistory (4)
Projectile motionchemistory (4)Projectile motionchemistory (4)
Projectile motionchemistory (4)
 
Lecture Ch 03
Lecture Ch 03Lecture Ch 03
Lecture Ch 03
 
Kinematics of Linear Motion​
Kinematics of Linear Motion​Kinematics of Linear Motion​
Kinematics of Linear Motion​
 
Physics 504 Chapter 10 Uniformly Accelerated Rectilinear Motion
Physics 504 Chapter 10 Uniformly Accelerated Rectilinear MotionPhysics 504 Chapter 10 Uniformly Accelerated Rectilinear Motion
Physics 504 Chapter 10 Uniformly Accelerated Rectilinear Motion
 
Ch#4 MOTION IN 2 DIMENSIONS
Ch#4 MOTION IN 2 DIMENSIONSCh#4 MOTION IN 2 DIMENSIONS
Ch#4 MOTION IN 2 DIMENSIONS
 
Motion in a plane chapter 3 converted
Motion in  a plane chapter 3 convertedMotion in  a plane chapter 3 converted
Motion in a plane chapter 3 converted
 

Mais de cyberspaced educator

ACEC 2014 Google Search Your keys to the Googleverse
ACEC 2014 Google Search   Your keys to the GoogleverseACEC 2014 Google Search   Your keys to the Googleverse
ACEC 2014 Google Search Your keys to the Googleversecyberspaced educator
 
Uniform circular motion worked examples
Uniform circular motion worked examplesUniform circular motion worked examples
Uniform circular motion worked examplescyberspaced educator
 
Five things for teachers and students sl
Five things for teachers and students slFive things for teachers and students sl
Five things for teachers and students slcyberspaced educator
 
Google search and beyond sasta 25 11-2011
Google search and beyond sasta 25 11-2011Google search and beyond sasta 25 11-2011
Google search and beyond sasta 25 11-2011cyberspaced educator
 
2011 sasta psych conference presentation collins
2011 sasta psych conference presentation collins2011 sasta psych conference presentation collins
2011 sasta psych conference presentation collinscyberspaced educator
 
Year 10 psychology second semester
Year 10 psychology second semesterYear 10 psychology second semester
Year 10 psychology second semestercyberspaced educator
 

Mais de cyberspaced educator (20)

ACEC 2014 Google Search Your keys to the Googleverse
ACEC 2014 Google Search   Your keys to the GoogleverseACEC 2014 Google Search   Your keys to the Googleverse
ACEC 2014 Google Search Your keys to the Googleverse
 
Google Search
Google SearchGoogle Search
Google Search
 
Uniform circular motion worked examples
Uniform circular motion worked examplesUniform circular motion worked examples
Uniform circular motion worked examples
 
Five things for teachers and students sl
Five things for teachers and students slFive things for teachers and students sl
Five things for teachers and students sl
 
Digital imperative sl
Digital imperative slDigital imperative sl
Digital imperative sl
 
Google search and beyond sasta 25 11-2011
Google search and beyond sasta 25 11-2011Google search and beyond sasta 25 11-2011
Google search and beyond sasta 25 11-2011
 
2011 sasta psych conference presentation collins
2011 sasta psych conference presentation collins2011 sasta psych conference presentation collins
2011 sasta psych conference presentation collins
 
Year 10 psychology second semester
Year 10 psychology second semesterYear 10 psychology second semester
Year 10 psychology second semester
 
Respiration 2010
Respiration 2010Respiration 2010
Respiration 2010
 
Emotion annesley 2010
Emotion annesley 2010Emotion annesley 2010
Emotion annesley 2010
 
Memory 2010
Memory 2010Memory 2010
Memory 2010
 
Skeletal system 2010
Skeletal system 2010Skeletal system 2010
Skeletal system 2010
 
Circulatory system 2010
Circulatory system 2010Circulatory system 2010
Circulatory system 2010
 
Biomaterials 2010
Biomaterials 2010Biomaterials 2010
Biomaterials 2010
 
Particle physics 2010
Particle physics 2010Particle physics 2010
Particle physics 2010
 
Brain and behaviour 2010
Brain and behaviour 2010Brain and behaviour 2010
Brain and behaviour 2010
 
Post Mortem 09 Section A Final
Post Mortem 09  Section A FinalPost Mortem 09  Section A Final
Post Mortem 09 Section A Final
 
Post Mortem Investigations 2010
Post Mortem  Investigations 2010Post Mortem  Investigations 2010
Post Mortem Investigations 2010
 
Presenting Data
Presenting DataPresenting Data
Presenting Data
 
Collins Stage 1 Resources
Collins Stage 1 ResourcesCollins Stage 1 Resources
Collins Stage 1 Resources
 

Vectors and projectile motion and worked examples

  • 1. Stage 2 Physics Section 1 Motion in Two Dimensions
  • 2. What is motion? What types of motion are there? What causes motion? How to we describe motion in Physics?
  • 3. What is a vector? Vector quantities have magnitude (size) and direction. Scalar quantities have magnitude only. Length represents the vectors magnitude.
  • 4. Scalar Vector Distance Displacement Speed Velocity Mass Acceleration Force Time weight
  • 5. Velocity vector of an angry bird
  • 6. Resultant of Two Vectors The resultant is the sum or the combined addition of two vector quantities Vectors in the same direction: 6N 4N = 10 N Vectors in opposite directions: 6m 10 m =
  • 7. Vectors • Vectors can be oriented to the gravitational field (up, down or some angle to the horizontal) or compass points (NESW). 5 ms-1 5 ms-1 30o above the horizontal
  • 8. Velocity Vectors • Velocity can be resolved into its horizontal and vertical components at any instant. v vV vH
  • 9. SOHCAHTOA Hypotenuse Opposite Adjacent
  • 10. v vV = v sin vH = v cos
  • 11.
  • 12. Example 1 Resolve the following velocity vector into its horizontal and vertical components 30o
  • 13. Example 1 Resolve the following velocity vector into its horizontal and vertical components 30o
  • 14. This problem can be solved in two ways (and you need to be able to do both) 1. Scale Diagram 2. Trigonometry
  • 15. 1. Scale diagram By drawing a vector diagram (using a protractor and a ruler) to scale we can simply measure the size of the components ideally the vector should be 10 cm or larger (for accuracy)
  • 16. 2. Trigonometry vvertical = v sin = 40 sin 30o = 20 m s-1 vhorizontal = v cos 30o = 40 cos 30o = 34.6 m s-1
  • 17. Example 2 Determine the velocity vector with initial horizontal velocity component of 50 ms –1 and vertical 20 ms-1.
  • 18. v=? vv= 20 m s-1 vh= 50 m s- 1
  • 19. 1. Scale diagram Again we could accurately draw the figure and measure the resultant length and angle to find the direction of v. (Note: You need to have a clear Perspex ruler and a protractor for EVERY test and exam)
  • 20. 2. Pythagoras & Trigonometry By Pythagoras theory: v2 = vV2 + vH2 v = v V 2 + vH 2 = 202 + 502 = 2900 = 53.9 m s-1 v=? vv= 20 m s-1 vh= 50 m s- 1
  • 21. tan vV/vH tan = 20/50 = 21.8o ie. v = 53.9 m s-1 at 21.8o above the horizontal
  • 22. Summary – Vectors in 2D • Given any vector quantity in 2D it can be resolved into horizontal and vertical components eg displacement, force, fields etc • Given the horizontal & vertical components you can determine magnitude and direction of the vector (formula)
  • 23. Motion in a Uniform Gravitational Field
  • 24. In the absence of gravity objects move with constant velocity in a straight line. An object will remain at rest, or continue to move at a constant velocity, unless a net force acts on it. Note: The following is all in the absence of air resistance.
  • 25. When an object falls under the influence of gravity, the vertical force causes a constant acceleration
  • 26. vH The resultant motion is a combination of both horizontal and vH vertical vV vV components
  • 27. Horizontal Projection While the vertical component undergoes constant If an object is acceleration. projected horizontally, the horizontal component moves with constant velocity.
  • 28. Three equations of motion Note that all the equations have “a” in them – they only apply under CONSTANT acceleration
  • 29. Constant vertical acceleration Vertical formulae 2 v 2 v0 2as 1 2 Horizontal velocity is constant s vt at 2 Horizontal formula v vo at s vH t
  • 31. Learning Symbols in Physics Quantity Quantity Symbol Units Unit symbol
  • 32.
  • 33. Example A stone is dropped down a well and takes 3 seconds to hit the ground. a) How fast does it hit the bottom? b) How deep is the well?
  • 34. A stone is dropped down a well at takes 3 seconds to hit the ground. a) How fast does it hit the bottom?
  • 35. b) How deep is the well?
  • 36. An arrow is fired upwards at 50ms-1. a) How high does the arrow fly?
  • 37. An arrow is fired upwards at 50ms-1. b) How long does the arrow take to hit the ground?
  • 38.
  • 39.
  • 40. Projectile Motion Problems Except for time, everything can be separated into horizontal and vertical components and treated separately. sV = height V0 s H = range t = time of flight
  • 41. Projectile Motion Problems Horizontal projection: down is +ve Uni-level projection: Up is considered positive, and down is negative.(Acceleration due to gravity aV = -9.8ms-2) sV = height V0 s H = range t = time of flight
  • 42. Projectile Motion Problems At the top of the parabolic path, vV= 0 ms-1 1 vV 0ms 2 aV 9.8ms sV height V0 sH range t = time of flight
  • 43. Projectile Motion Problems Remember the time of flight is the time it takes to go up+ down. 1 vV 0ms 2 aV 9.8ms sV height V0 sH range t = time of flight
  • 45.
  • 46.
  • 47.
  • 48.
  • 49.
  • 50.
  • 51.
  • 52.
  • 53.
  • 54.
  • 55. Bi-level projection • An object is projected at a height
  • 56.
  • 57.
  • 58. Maximum Range To get the maximum range sH max in a vacuum (no air resistance) the launch angle must be 45o sH max
  • 59. For a projectile launched at ground level find by sample calculation the launch angle that results in a maximum range
  • 60. Pairs of launch angles that yield the same range add up to 90o α + θ = ranges Projectile 90o for various angles of launch 500 450 400 350 300 height 250 200 150 100 50 0 0 200 400 600 800 1000 1200 range
  • 61. α + θ = 90o Find the launch angle that yields the same range as 32o θ = 32 α=? α + θ = 90o
  • 62. The Effect of Air Resistance Air resistance acts in the opposite direction to motion. vertical horizontal
  • 63. The Effect of Air Resistance vertical horizontal This decreases the • height • range Slight decrease in time of flight of the projectile
  • 64.
  • 65. The magnitude of Fair resistance Fair resistance
  • 66. Speed
  • 68. Size More surface area = more air resistance
  • 70. Air density Low air density = less air resistance High air density = high air resistance
  • 71. Projectiles in Sport Consider the effect of launch height on range
  • 72. As the object has further to fall tflight is increased. As the object is in the air for longer it travels farther.
  • 73. 45o 41o For objects at h=0 the optimal angle is 45o For heights › 0 θ max height is less than 45o