SlideShare a Scribd company logo
1 of 22
Download to read offline
PROJECTILES
MUJUNGU HERBERT
(Mathematics Lecturer)
National Teachers College Kabale
May 25, 2020
Content
1 Definition of a projectile
Examples
2 Equations of motion for a projectile
3 Other general equations
Time at maximum height
Maximum Height Hmax
Time of flight T
Range R
Maximum range R
Equation of a trajectory
4 Summary
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 2 / 13
Definition of a projectile
Any Object that once thrown by some force continues in motion by its
own inertia.
Examples
Throwing/kicking a ball,
Throwing a stone,
A shell fired from a gun
etc
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 3 / 13
A particle projected at an angle θ to the horizontal
u
θ
u cos θ
u sin θ
g
X-axis
Y-axis
vx
vy
O
We shall investigate both the horizontal and vertical motions;
For horizontal motion, vx = ucosθ is constant since there are no
horizontal forces subject to the particle,
The vertical component of velocity, vy, is subject to acceleration due to
gravity, g.
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 4 / 13
Equations of motion for a projectile
The components of acceleration parallel to the axes at any instant are;
ax = 0 , ay = −g (1)
Integrating Equations 1 with respect to time, we have;
vx = constant , vy = −gt + constant
At t = 0, vx and vy are ucosθ and usinθ respectively, hence;
vx = ucosθ , vy = −gt + usinθ (2)
Integrating again with respect to time;
x = ucosθ · t , y = −1
2gt2 + usinθ · t (3)
Equations 2 and 3 give the velocity and coordinates respectively of a
projectile at any instant. Also; v2
y = u2
sin2
θ · −2gy, can be used.
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 5 / 13
Time at maximum height
Taking the fact that the particle is
momentarily at rest at maximum
height and by using Equation 2;
vy = −gt + usinθ
But vy = 0
0 = −gt + usinθ
t =
u sin θ
g
(4)
Maximum Height Hmax
Using the time at maximum height
and 3, i.e,
y = −
1
2
gt2
+ u sin θt
Hmax = −
1
2
g
u sin θ
g
2
+ u sin θ
u sin θ
g
Hmax =
u2
sin2
θ
2g
(5)
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 6 / 13
Time of flight T
For a complete flight, y = 0 and
t = T;
By using Eqn 3;
0 = −
1
2
gT2
+ u sin θT
T(u sin θ −
1
2
gT) = 0
T = 0 orT =
2u sin θ
g
Ignoring T = 0 then
T =
2u sin θ
g
(6)
Range R
R = T × u cos θ
R =
2u sin θ
g
u cos θ
R =
2u2 sin θ cos θ
g
R =
u2 sin 2θ
g
(7)
This is maximum when
sin 2θ = 1, i.e, is maximum;
Rmax =
u2
g
when θ = 45o (8)
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 7 / 13
Equation of a trajectory
From equation 3; x = ucosθ · t , y = −1
2gt2 + usinθt,
(a, b)
θ1
θ2
u
u
x1
x2
y y
(x1, y) (x1, y)
u
θ
1 Show that the
Equation of the trajectory is
y = x tan θ −
gx2
2u2
sec2
θ.
2 If the particle
passes through the point with
coordinates (a, b), show that
ga2
tan2
θ − 2u2
a tan θ + 2u2
b + ga2
= 0
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 8 / 13
Example 1
A particle is projected from a point on level ground such that its initial
velocity is 56 ms−1 at an angle of 30 o above the horizontal. Taking g as
9.8 ms−2, find the time taken for the particle to reach its maximum height.
Solution
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 9 / 13
Example 1
A particle is projected from a point on level ground such that its initial
velocity is 56 ms−1 at an angle of 30 o above the horizontal. Taking g as
9.8 ms−2, find the time taken for the particle to reach its maximum height.
Solution
Taking vertical motion and using the fact that the particle is momentarily
at rest vertically at the maximum height;
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 9 / 13
Example 1
A particle is projected from a point on level ground such that its initial
velocity is 56 ms−1 at an angle of 30 o above the horizontal. Taking g as
9.8 ms−2, find the time taken for the particle to reach its maximum height.
Solution
Taking vertical motion and using the fact that the particle is momentarily
at rest vertically at the maximum height;
Applying
˙y = 0, u = 56 ms−1, θ = 30 o and
g = 9.8 ms−2 in equation 2
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 9 / 13
Example 1
A particle is projected from a point on level ground such that its initial
velocity is 56 ms−1 at an angle of 30 o above the horizontal. Taking g as
9.8 ms−2, find the time taken for the particle to reach its maximum height.
Solution
Taking vertical motion and using the fact that the particle is momentarily
at rest vertically at the maximum height;
Applying
˙y = 0, u = 56 ms−1, θ = 30 o and
g = 9.8 ms−2 in equation 2 , i.e,
0 = −gt + u sin θ
0 = −9.8t + 56sin30o
t =
56sin30o
9.8
, ⇒ t = 2.86 s
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 9 / 13
Example 2
A bullet fired from a gun has a maximum horizontal range of 2000 m. Find
the muzzle velocity of the gun (i.e. the speed with which the bullet leaves
the gun).
Solution
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 10 / 13
Example 2
A bullet fired from a gun has a maximum horizontal range of 2000 m. Find
the muzzle velocity of the gun (i.e. the speed with which the bullet leaves
the gun).
Solution
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 10 / 13
Example 2
A bullet fired from a gun has a maximum horizontal range of 2000 m. Find
the muzzle velocity of the gun (i.e. the speed with which the bullet leaves
the gun).
Solution
So we have θ = 45o,
Rmax = 2000 m, u =? and
g = 9.8 ms−2
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 10 / 13
Example 2
A bullet fired from a gun has a maximum horizontal range of 2000 m. Find
the muzzle velocity of the gun (i.e. the speed with which the bullet leaves
the gun).
Solution
So we have θ = 45o,
Rmax = 2000 m, u =? and
g = 9.8 ms−2 By using in Eqn 8;
Rmax =
u2
g
2000 =
u2
9.8
u = (2000 ∗ 9.8), ⇒ u = 140 ms−1
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 10 / 13
Trial Questions
1 A particle is projected from a point on level ground such that its
initial velocity is 28 ms−1 at an angle of 45 o above the horizontal.
Taking g as 9.8 ms−2, find the time taken for the particle to reach its
maximum height.
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 11 / 13
Trial Questions
1 A particle is projected from a point on level ground such that its
initial velocity is 28 ms−1 at an angle of 45 o above the horizontal.
Taking g as 9.8 ms−2, find the time taken for the particle to reach its
maximum height.
2 A particle is projected from a point on a horizontal plane and has an
initial velocity u at an angle of θ above the plane. Show;
by using the equation; v2
y = u2
sin2
θ − 2gy, that the greatest height h
reached by the particle above the plane is given by h = u2 sin2 θ
2g .
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 11 / 13
Trial Questions
1 A particle is projected from a point on level ground such that its
initial velocity is 28 ms−1 at an angle of 45 o above the horizontal.
Taking g as 9.8 ms−2, find the time taken for the particle to reach its
maximum height.
2 A particle is projected from a point on a horizontal plane and has an
initial velocity u at an angle of θ above the plane. Show;
by using the equation; v2
y = u2
sin2
θ − 2gy, that the greatest height h
reached by the particle above the plane is given by h = u2 sin2 θ
2g .
3 A particle is projected from a point on a horizontal plane with an
initial velocity of 140 ms−1 at an angle of elevation of 30o. Find the
greatest height reached by the particle above the plane.
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 11 / 13
Trial Questions
1 A particle is projected from a point on level ground such that its
initial velocity is 28 ms−1 at an angle of 45 o above the horizontal.
Taking g as 9.8 ms−2, find the time taken for the particle to reach its
maximum height.
2 A particle is projected from a point on a horizontal plane and has an
initial velocity u at an angle of θ above the plane. Show;
by using the equation; v2
y = u2
sin2
θ − 2gy, that the greatest height h
reached by the particle above the plane is given by h = u2 sin2 θ
2g .
3 A particle is projected from a point on a horizontal plane with an
initial velocity of 140 ms−1 at an angle of elevation of 30o. Find the
greatest height reached by the particle above the plane.
For more questions; https://bit.ly/Projectile_questions
and for notes https://bit.ly/Projectile_notes .
All are reading materials are saved on https://bit.ly/padlet-DESII
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 11 / 13
Summary
A Projectile is any object that when thrown continues, continues in
motion under its own inertia.
Equations of motion
1 Horizontal Motion;
x = u cos θ · t
2 Vertical motion;
vy = u sin θ − gt
y = −
1
2
gt2
+ u sin θ · t and
v2
y = u2
sin2
θ − 2gy
1 Maximum Height;
Hmax =
u2 sin2
θ
2g
,
2 Time at Hmax; t = u sin θ
g ,
3 Time of Flight; T =
2u sin θ
g
,
4 Range;R =
u2 sin 2θ
g
,
Rmax =
u2
g
Equation of a Trajectory; y = x tan θ −
gx2
2u2
sec2
θ.
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 12 / 13
Thank You for Your Attention
For more information Contact me through; herbertmujungu@gmail.com
+256779547251
+256701310635
+256793854372
The class facebook account is; NTC-KABALE, MATHEMATICS YEAR II,
2019/2020
The class whatsapp account is;
NTC-KABALE, MTC2, 2019/20
MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 13 / 13

More Related Content

What's hot

01 20264 diminution of real power...
01 20264 diminution of real power...01 20264 diminution of real power...
01 20264 diminution of real power...IAESIJEECS
 
Statics and dynamics of nanoscale structures
Statics and dynamics of nanoscale structures Statics and dynamics of nanoscale structures
Statics and dynamics of nanoscale structures University of Glasgow
 
Work and energy part a
Work and energy part aWork and energy part a
Work and energy part aAngelo Aquino
 
Toward an Improved Computational Strategy for Vibration-Proof Structures Equi...
Toward an Improved Computational Strategy for Vibration-Proof Structures Equi...Toward an Improved Computational Strategy for Vibration-Proof Structures Equi...
Toward an Improved Computational Strategy for Vibration-Proof Structures Equi...Alessandro Palmeri
 
1 newton's laws notes
1 newton's laws notes1 newton's laws notes
1 newton's laws notescpphysics
 
Problem for the gravitational field
 Problem for the gravitational field Problem for the gravitational field
Problem for the gravitational fieldAlexander Decker
 
Lecture 5 castigliono's theorem
Lecture 5 castigliono's theoremLecture 5 castigliono's theorem
Lecture 5 castigliono's theoremDeepak Agarwal
 
Surface reconstruction from point clouds using optimal transportation
Surface reconstruction from point clouds using optimal transportationSurface reconstruction from point clouds using optimal transportation
Surface reconstruction from point clouds using optimal transportationGuillaume Matheron
 
Nonlinear transport phenomena: models, method of solving and unusual features...
Nonlinear transport phenomena: models, method of solving and unusual features...Nonlinear transport phenomena: models, method of solving and unusual features...
Nonlinear transport phenomena: models, method of solving and unusual features...SSA KPI
 
Stochastic Frank-Wolfe for Constrained Finite Sum Minimization @ Montreal Opt...
Stochastic Frank-Wolfe for Constrained Finite Sum Minimization @ Montreal Opt...Stochastic Frank-Wolfe for Constrained Finite Sum Minimization @ Montreal Opt...
Stochastic Frank-Wolfe for Constrained Finite Sum Minimization @ Montreal Opt...Geoffrey Négiar
 
CGI2018 keynote - fluids simulation
CGI2018 keynote - fluids simulationCGI2018 keynote - fluids simulation
CGI2018 keynote - fluids simulationBruno Levy
 
Using blurred images to assess damage in bridge structures?
Using blurred images to assess damage in bridge structures?Using blurred images to assess damage in bridge structures?
Using blurred images to assess damage in bridge structures? Alessandro Palmeri
 

What's hot (20)

01 20264 diminution of real power...
01 20264 diminution of real power...01 20264 diminution of real power...
01 20264 diminution of real power...
 
Statics and dynamics of nanoscale structures
Statics and dynamics of nanoscale structures Statics and dynamics of nanoscale structures
Statics and dynamics of nanoscale structures
 
Work and energy part a
Work and energy part aWork and energy part a
Work and energy part a
 
SDEE: Lecture 6
SDEE: Lecture 6SDEE: Lecture 6
SDEE: Lecture 6
 
Base excitation of dynamic systems
Base excitation of dynamic systemsBase excitation of dynamic systems
Base excitation of dynamic systems
 
Toward an Improved Computational Strategy for Vibration-Proof Structures Equi...
Toward an Improved Computational Strategy for Vibration-Proof Structures Equi...Toward an Improved Computational Strategy for Vibration-Proof Structures Equi...
Toward an Improved Computational Strategy for Vibration-Proof Structures Equi...
 
1 newton's laws notes
1 newton's laws notes1 newton's laws notes
1 newton's laws notes
 
Deflection energy
Deflection energyDeflection energy
Deflection energy
 
Gravitational Waves and Binary Systems (3) - Thibault Damour
Gravitational Waves and Binary Systems (3) - Thibault DamourGravitational Waves and Binary Systems (3) - Thibault Damour
Gravitational Waves and Binary Systems (3) - Thibault Damour
 
Problem for the gravitational field
 Problem for the gravitational field Problem for the gravitational field
Problem for the gravitational field
 
Lecture 5 castigliono's theorem
Lecture 5 castigliono's theoremLecture 5 castigliono's theorem
Lecture 5 castigliono's theorem
 
SDEE: Lectures 3 and 4
SDEE: Lectures 3 and 4SDEE: Lectures 3 and 4
SDEE: Lectures 3 and 4
 
Surface reconstruction from point clouds using optimal transportation
Surface reconstruction from point clouds using optimal transportationSurface reconstruction from point clouds using optimal transportation
Surface reconstruction from point clouds using optimal transportation
 
Nonlinear transport phenomena: models, method of solving and unusual features...
Nonlinear transport phenomena: models, method of solving and unusual features...Nonlinear transport phenomena: models, method of solving and unusual features...
Nonlinear transport phenomena: models, method of solving and unusual features...
 
Stochastic Frank-Wolfe for Constrained Finite Sum Minimization @ Montreal Opt...
Stochastic Frank-Wolfe for Constrained Finite Sum Minimization @ Montreal Opt...Stochastic Frank-Wolfe for Constrained Finite Sum Minimization @ Montreal Opt...
Stochastic Frank-Wolfe for Constrained Finite Sum Minimization @ Montreal Opt...
 
Centros de Masa
Centros de MasaCentros de Masa
Centros de Masa
 
CGI2018 keynote - fluids simulation
CGI2018 keynote - fluids simulationCGI2018 keynote - fluids simulation
CGI2018 keynote - fluids simulation
 
Ch07 ssm
Ch07 ssmCh07 ssm
Ch07 ssm
 
Using blurred images to assess damage in bridge structures?
Using blurred images to assess damage in bridge structures?Using blurred images to assess damage in bridge structures?
Using blurred images to assess damage in bridge structures?
 
Maquina de Movimiento Perpetuo
Maquina de Movimiento PerpetuoMaquina de Movimiento Perpetuo
Maquina de Movimiento Perpetuo
 

Similar to Projectile Motion Equations

Dinamika partikel Mata Kuliah Konsep Dasar IPA
Dinamika partikel Mata Kuliah Konsep Dasar IPADinamika partikel Mata Kuliah Konsep Dasar IPA
Dinamika partikel Mata Kuliah Konsep Dasar IPAlailam02
 
Motion under gravity By ghumare s m
Motion under gravity By ghumare s mMotion under gravity By ghumare s m
Motion under gravity By ghumare s msmghumare
 
Landing on a comet! The Rosetta project - Maria Eleftheriou - #OCCAthens
Landing on a comet! The Rosetta project - Maria Eleftheriou - #OCCAthensLanding on a comet! The Rosetta project - Maria Eleftheriou - #OCCAthens
Landing on a comet! The Rosetta project - Maria Eleftheriou - #OCCAthensEDEN Digital Learning Europe
 
Physics 2 LT3: Projectile Motion Solutions
Physics 2 LT3: Projectile Motion SolutionsPhysics 2 LT3: Projectile Motion Solutions
Physics 2 LT3: Projectile Motion SolutionsDarwin Quinsaat
 
Gravitational Fields
Gravitational FieldsGravitational Fields
Gravitational FieldsPaula Mills
 
Day 36 Ppt Batfink Angle Launched Projectile Motion
Day 36 Ppt Batfink Angle Launched Projectile MotionDay 36 Ppt Batfink Angle Launched Projectile Motion
Day 36 Ppt Batfink Angle Launched Projectile Motionffiala
 
5.50 ppt batfink angle launched projectile motion
5.50 ppt batfink angle launched projectile motion5.50 ppt batfink angle launched projectile motion
5.50 ppt batfink angle launched projectile motionffiala
 
_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
 
Chapter no. 7 projectile
Chapter no. 7 projectileChapter no. 7 projectile
Chapter no. 7 projectilePralhad Kore
 
Projectile-Motion_Process_Final.pdf
Projectile-Motion_Process_Final.pdfProjectile-Motion_Process_Final.pdf
Projectile-Motion_Process_Final.pdfPragyaPrakash29
 

Similar to Projectile Motion Equations (20)

Dinamika partikel Mata Kuliah Konsep Dasar IPA
Dinamika partikel Mata Kuliah Konsep Dasar IPADinamika partikel Mata Kuliah Konsep Dasar IPA
Dinamika partikel Mata Kuliah Konsep Dasar IPA
 
Motion under gravity By ghumare s m
Motion under gravity By ghumare s mMotion under gravity By ghumare s m
Motion under gravity By ghumare s m
 
lecture5
lecture5lecture5
lecture5
 
Projectile
ProjectileProjectile
Projectile
 
Landing on a comet! The Rosetta project - Maria Eleftheriou - #OCCAthens
Landing on a comet! The Rosetta project - Maria Eleftheriou - #OCCAthensLanding on a comet! The Rosetta project - Maria Eleftheriou - #OCCAthens
Landing on a comet! The Rosetta project - Maria Eleftheriou - #OCCAthens
 
motion
motionmotion
motion
 
Physics 2 LT3: Projectile Motion Solutions
Physics 2 LT3: Projectile Motion SolutionsPhysics 2 LT3: Projectile Motion Solutions
Physics 2 LT3: Projectile Motion Solutions
 
Gravitational Fields
Gravitational FieldsGravitational Fields
Gravitational Fields
 
Lecture10
Lecture10Lecture10
Lecture10
 
Lecture10
Lecture10Lecture10
Lecture10
 
Day 36 Ppt Batfink Angle Launched Projectile Motion
Day 36 Ppt Batfink Angle Launched Projectile MotionDay 36 Ppt Batfink Angle Launched Projectile Motion
Day 36 Ppt Batfink Angle Launched Projectile Motion
 
5.50 ppt batfink angle launched projectile motion
5.50 ppt batfink angle launched projectile motion5.50 ppt batfink angle launched projectile motion
5.50 ppt batfink angle launched projectile motion
 
_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
 
08 gravitation
08   gravitation08   gravitation
08 gravitation
 
Aieee Physics 2004
Aieee Physics  2004Aieee Physics  2004
Aieee Physics 2004
 
Projectiles
ProjectilesProjectiles
Projectiles
 
Physics 1
Physics 1Physics 1
Physics 1
 
9th std sci-gravitation_ppt.17-18
9th std sci-gravitation_ppt.17-189th std sci-gravitation_ppt.17-18
9th std sci-gravitation_ppt.17-18
 
Chapter no. 7 projectile
Chapter no. 7 projectileChapter no. 7 projectile
Chapter no. 7 projectile
 
Projectile-Motion_Process_Final.pdf
Projectile-Motion_Process_Final.pdfProjectile-Motion_Process_Final.pdf
Projectile-Motion_Process_Final.pdf
 

More from Herbert Mujungu

More from Herbert Mujungu (7)

Maclaurin series
Maclaurin seriesMaclaurin series
Maclaurin series
 
Maclaurins series
Maclaurins seriesMaclaurins series
Maclaurins series
 
Maclaurins series
Maclaurins seriesMaclaurins series
Maclaurins series
 
Notes on Equation of Plane
Notes on Equation of PlaneNotes on Equation of Plane
Notes on Equation of Plane
 
Maclaurin Series
Maclaurin SeriesMaclaurin Series
Maclaurin Series
 
Equation of a plane
Equation of a planeEquation of a plane
Equation of a plane
 
Taylor slides
Taylor slidesTaylor slides
Taylor slides
 

Recently uploaded

Analytical Profile of Coleus Forskohlii | Forskolin .pdf
Analytical Profile of Coleus Forskohlii | Forskolin .pdfAnalytical Profile of Coleus Forskohlii | Forskolin .pdf
Analytical Profile of Coleus Forskohlii | Forskolin .pdfSwapnil Therkar
 
Recombinant DNA technology( Transgenic plant and animal)
Recombinant DNA technology( Transgenic plant and animal)Recombinant DNA technology( Transgenic plant and animal)
Recombinant DNA technology( Transgenic plant and animal)DHURKADEVIBASKAR
 
Animal Communication- Auditory and Visual.pptx
Animal Communication- Auditory and Visual.pptxAnimal Communication- Auditory and Visual.pptx
Animal Communication- Auditory and Visual.pptxUmerFayaz5
 
TOPIC 8 Temperature and Heat.pdf physics
TOPIC 8 Temperature and Heat.pdf physicsTOPIC 8 Temperature and Heat.pdf physics
TOPIC 8 Temperature and Heat.pdf physicsssuserddc89b
 
Isotopic evidence of long-lived volcanism on Io
Isotopic evidence of long-lived volcanism on IoIsotopic evidence of long-lived volcanism on Io
Isotopic evidence of long-lived volcanism on IoSérgio Sacani
 
Call Girls in Mayapuri Delhi 💯Call Us 🔝9953322196🔝 💯Escort.
Call Girls in Mayapuri Delhi 💯Call Us 🔝9953322196🔝 💯Escort.Call Girls in Mayapuri Delhi 💯Call Us 🔝9953322196🔝 💯Escort.
Call Girls in Mayapuri Delhi 💯Call Us 🔝9953322196🔝 💯Escort.aasikanpl
 
Module 4: Mendelian Genetics and Punnett Square
Module 4:  Mendelian Genetics and Punnett SquareModule 4:  Mendelian Genetics and Punnett Square
Module 4: Mendelian Genetics and Punnett SquareIsiahStephanRadaza
 
Biopesticide (2).pptx .This slides helps to know the different types of biop...
Biopesticide (2).pptx  .This slides helps to know the different types of biop...Biopesticide (2).pptx  .This slides helps to know the different types of biop...
Biopesticide (2).pptx .This slides helps to know the different types of biop...RohitNehra6
 
A relative description on Sonoporation.pdf
A relative description on Sonoporation.pdfA relative description on Sonoporation.pdf
A relative description on Sonoporation.pdfnehabiju2046
 
Bentham & Hooker's Classification. along with the merits and demerits of the ...
Bentham & Hooker's Classification. along with the merits and demerits of the ...Bentham & Hooker's Classification. along with the merits and demerits of the ...
Bentham & Hooker's Classification. along with the merits and demerits of the ...Nistarini College, Purulia (W.B) India
 
Traditional Agroforestry System in India- Shifting Cultivation, Taungya, Home...
Traditional Agroforestry System in India- Shifting Cultivation, Taungya, Home...Traditional Agroforestry System in India- Shifting Cultivation, Taungya, Home...
Traditional Agroforestry System in India- Shifting Cultivation, Taungya, Home...jana861314
 
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.PraveenaKalaiselvan1
 
Recombination DNA Technology (Nucleic Acid Hybridization )
Recombination DNA Technology (Nucleic Acid Hybridization )Recombination DNA Technology (Nucleic Acid Hybridization )
Recombination DNA Technology (Nucleic Acid Hybridization )aarthirajkumar25
 
Genomic DNA And Complementary DNA Libraries construction.
Genomic DNA And Complementary DNA Libraries construction.Genomic DNA And Complementary DNA Libraries construction.
Genomic DNA And Complementary DNA Libraries construction.k64182334
 
Is RISC-V ready for HPC workload? Maybe?
Is RISC-V ready for HPC workload? Maybe?Is RISC-V ready for HPC workload? Maybe?
Is RISC-V ready for HPC workload? Maybe?Patrick Diehl
 
STERILITY TESTING OF PHARMACEUTICALS ppt by DR.C.P.PRINCE
STERILITY TESTING OF PHARMACEUTICALS ppt by DR.C.P.PRINCESTERILITY TESTING OF PHARMACEUTICALS ppt by DR.C.P.PRINCE
STERILITY TESTING OF PHARMACEUTICALS ppt by DR.C.P.PRINCEPRINCE C P
 
Analytical Profile of Coleus Forskohlii | Forskolin .pptx
Analytical Profile of Coleus Forskohlii | Forskolin .pptxAnalytical Profile of Coleus Forskohlii | Forskolin .pptx
Analytical Profile of Coleus Forskohlii | Forskolin .pptxSwapnil Therkar
 
GFP in rDNA Technology (Biotechnology).pptx
GFP in rDNA Technology (Biotechnology).pptxGFP in rDNA Technology (Biotechnology).pptx
GFP in rDNA Technology (Biotechnology).pptxAleenaTreesaSaji
 
Lucknow 💋 Russian Call Girls Lucknow Finest Escorts Service 8923113531 Availa...
Lucknow 💋 Russian Call Girls Lucknow Finest Escorts Service 8923113531 Availa...Lucknow 💋 Russian Call Girls Lucknow Finest Escorts Service 8923113531 Availa...
Lucknow 💋 Russian Call Girls Lucknow Finest Escorts Service 8923113531 Availa...anilsa9823
 

Recently uploaded (20)

Analytical Profile of Coleus Forskohlii | Forskolin .pdf
Analytical Profile of Coleus Forskohlii | Forskolin .pdfAnalytical Profile of Coleus Forskohlii | Forskolin .pdf
Analytical Profile of Coleus Forskohlii | Forskolin .pdf
 
Recombinant DNA technology( Transgenic plant and animal)
Recombinant DNA technology( Transgenic plant and animal)Recombinant DNA technology( Transgenic plant and animal)
Recombinant DNA technology( Transgenic plant and animal)
 
Animal Communication- Auditory and Visual.pptx
Animal Communication- Auditory and Visual.pptxAnimal Communication- Auditory and Visual.pptx
Animal Communication- Auditory and Visual.pptx
 
TOPIC 8 Temperature and Heat.pdf physics
TOPIC 8 Temperature and Heat.pdf physicsTOPIC 8 Temperature and Heat.pdf physics
TOPIC 8 Temperature and Heat.pdf physics
 
Isotopic evidence of long-lived volcanism on Io
Isotopic evidence of long-lived volcanism on IoIsotopic evidence of long-lived volcanism on Io
Isotopic evidence of long-lived volcanism on Io
 
Call Girls in Mayapuri Delhi 💯Call Us 🔝9953322196🔝 💯Escort.
Call Girls in Mayapuri Delhi 💯Call Us 🔝9953322196🔝 💯Escort.Call Girls in Mayapuri Delhi 💯Call Us 🔝9953322196🔝 💯Escort.
Call Girls in Mayapuri Delhi 💯Call Us 🔝9953322196🔝 💯Escort.
 
Module 4: Mendelian Genetics and Punnett Square
Module 4:  Mendelian Genetics and Punnett SquareModule 4:  Mendelian Genetics and Punnett Square
Module 4: Mendelian Genetics and Punnett Square
 
Biopesticide (2).pptx .This slides helps to know the different types of biop...
Biopesticide (2).pptx  .This slides helps to know the different types of biop...Biopesticide (2).pptx  .This slides helps to know the different types of biop...
Biopesticide (2).pptx .This slides helps to know the different types of biop...
 
Engler and Prantl system of classification in plant taxonomy
Engler and Prantl system of classification in plant taxonomyEngler and Prantl system of classification in plant taxonomy
Engler and Prantl system of classification in plant taxonomy
 
A relative description on Sonoporation.pdf
A relative description on Sonoporation.pdfA relative description on Sonoporation.pdf
A relative description on Sonoporation.pdf
 
Bentham & Hooker's Classification. along with the merits and demerits of the ...
Bentham & Hooker's Classification. along with the merits and demerits of the ...Bentham & Hooker's Classification. along with the merits and demerits of the ...
Bentham & Hooker's Classification. along with the merits and demerits of the ...
 
Traditional Agroforestry System in India- Shifting Cultivation, Taungya, Home...
Traditional Agroforestry System in India- Shifting Cultivation, Taungya, Home...Traditional Agroforestry System in India- Shifting Cultivation, Taungya, Home...
Traditional Agroforestry System in India- Shifting Cultivation, Taungya, Home...
 
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.
 
Recombination DNA Technology (Nucleic Acid Hybridization )
Recombination DNA Technology (Nucleic Acid Hybridization )Recombination DNA Technology (Nucleic Acid Hybridization )
Recombination DNA Technology (Nucleic Acid Hybridization )
 
Genomic DNA And Complementary DNA Libraries construction.
Genomic DNA And Complementary DNA Libraries construction.Genomic DNA And Complementary DNA Libraries construction.
Genomic DNA And Complementary DNA Libraries construction.
 
Is RISC-V ready for HPC workload? Maybe?
Is RISC-V ready for HPC workload? Maybe?Is RISC-V ready for HPC workload? Maybe?
Is RISC-V ready for HPC workload? Maybe?
 
STERILITY TESTING OF PHARMACEUTICALS ppt by DR.C.P.PRINCE
STERILITY TESTING OF PHARMACEUTICALS ppt by DR.C.P.PRINCESTERILITY TESTING OF PHARMACEUTICALS ppt by DR.C.P.PRINCE
STERILITY TESTING OF PHARMACEUTICALS ppt by DR.C.P.PRINCE
 
Analytical Profile of Coleus Forskohlii | Forskolin .pptx
Analytical Profile of Coleus Forskohlii | Forskolin .pptxAnalytical Profile of Coleus Forskohlii | Forskolin .pptx
Analytical Profile of Coleus Forskohlii | Forskolin .pptx
 
GFP in rDNA Technology (Biotechnology).pptx
GFP in rDNA Technology (Biotechnology).pptxGFP in rDNA Technology (Biotechnology).pptx
GFP in rDNA Technology (Biotechnology).pptx
 
Lucknow 💋 Russian Call Girls Lucknow Finest Escorts Service 8923113531 Availa...
Lucknow 💋 Russian Call Girls Lucknow Finest Escorts Service 8923113531 Availa...Lucknow 💋 Russian Call Girls Lucknow Finest Escorts Service 8923113531 Availa...
Lucknow 💋 Russian Call Girls Lucknow Finest Escorts Service 8923113531 Availa...
 

Projectile Motion Equations

  • 1. PROJECTILES MUJUNGU HERBERT (Mathematics Lecturer) National Teachers College Kabale May 25, 2020
  • 2. Content 1 Definition of a projectile Examples 2 Equations of motion for a projectile 3 Other general equations Time at maximum height Maximum Height Hmax Time of flight T Range R Maximum range R Equation of a trajectory 4 Summary MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 2 / 13
  • 3. Definition of a projectile Any Object that once thrown by some force continues in motion by its own inertia. Examples Throwing/kicking a ball, Throwing a stone, A shell fired from a gun etc MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 3 / 13
  • 4. A particle projected at an angle θ to the horizontal u θ u cos θ u sin θ g X-axis Y-axis vx vy O We shall investigate both the horizontal and vertical motions; For horizontal motion, vx = ucosθ is constant since there are no horizontal forces subject to the particle, The vertical component of velocity, vy, is subject to acceleration due to gravity, g. MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 4 / 13
  • 5. Equations of motion for a projectile The components of acceleration parallel to the axes at any instant are; ax = 0 , ay = −g (1) Integrating Equations 1 with respect to time, we have; vx = constant , vy = −gt + constant At t = 0, vx and vy are ucosθ and usinθ respectively, hence; vx = ucosθ , vy = −gt + usinθ (2) Integrating again with respect to time; x = ucosθ · t , y = −1 2gt2 + usinθ · t (3) Equations 2 and 3 give the velocity and coordinates respectively of a projectile at any instant. Also; v2 y = u2 sin2 θ · −2gy, can be used. MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 5 / 13
  • 6. Time at maximum height Taking the fact that the particle is momentarily at rest at maximum height and by using Equation 2; vy = −gt + usinθ But vy = 0 0 = −gt + usinθ t = u sin θ g (4) Maximum Height Hmax Using the time at maximum height and 3, i.e, y = − 1 2 gt2 + u sin θt Hmax = − 1 2 g u sin θ g 2 + u sin θ u sin θ g Hmax = u2 sin2 θ 2g (5) MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 6 / 13
  • 7. Time of flight T For a complete flight, y = 0 and t = T; By using Eqn 3; 0 = − 1 2 gT2 + u sin θT T(u sin θ − 1 2 gT) = 0 T = 0 orT = 2u sin θ g Ignoring T = 0 then T = 2u sin θ g (6) Range R R = T × u cos θ R = 2u sin θ g u cos θ R = 2u2 sin θ cos θ g R = u2 sin 2θ g (7) This is maximum when sin 2θ = 1, i.e, is maximum; Rmax = u2 g when θ = 45o (8) MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 7 / 13
  • 8. Equation of a trajectory From equation 3; x = ucosθ · t , y = −1 2gt2 + usinθt, (a, b) θ1 θ2 u u x1 x2 y y (x1, y) (x1, y) u θ 1 Show that the Equation of the trajectory is y = x tan θ − gx2 2u2 sec2 θ. 2 If the particle passes through the point with coordinates (a, b), show that ga2 tan2 θ − 2u2 a tan θ + 2u2 b + ga2 = 0 MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 8 / 13
  • 9. Example 1 A particle is projected from a point on level ground such that its initial velocity is 56 ms−1 at an angle of 30 o above the horizontal. Taking g as 9.8 ms−2, find the time taken for the particle to reach its maximum height. Solution MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 9 / 13
  • 10. Example 1 A particle is projected from a point on level ground such that its initial velocity is 56 ms−1 at an angle of 30 o above the horizontal. Taking g as 9.8 ms−2, find the time taken for the particle to reach its maximum height. Solution Taking vertical motion and using the fact that the particle is momentarily at rest vertically at the maximum height; MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 9 / 13
  • 11. Example 1 A particle is projected from a point on level ground such that its initial velocity is 56 ms−1 at an angle of 30 o above the horizontal. Taking g as 9.8 ms−2, find the time taken for the particle to reach its maximum height. Solution Taking vertical motion and using the fact that the particle is momentarily at rest vertically at the maximum height; Applying ˙y = 0, u = 56 ms−1, θ = 30 o and g = 9.8 ms−2 in equation 2 MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 9 / 13
  • 12. Example 1 A particle is projected from a point on level ground such that its initial velocity is 56 ms−1 at an angle of 30 o above the horizontal. Taking g as 9.8 ms−2, find the time taken for the particle to reach its maximum height. Solution Taking vertical motion and using the fact that the particle is momentarily at rest vertically at the maximum height; Applying ˙y = 0, u = 56 ms−1, θ = 30 o and g = 9.8 ms−2 in equation 2 , i.e, 0 = −gt + u sin θ 0 = −9.8t + 56sin30o t = 56sin30o 9.8 , ⇒ t = 2.86 s MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 9 / 13
  • 13. Example 2 A bullet fired from a gun has a maximum horizontal range of 2000 m. Find the muzzle velocity of the gun (i.e. the speed with which the bullet leaves the gun). Solution MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 10 / 13
  • 14. Example 2 A bullet fired from a gun has a maximum horizontal range of 2000 m. Find the muzzle velocity of the gun (i.e. the speed with which the bullet leaves the gun). Solution MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 10 / 13
  • 15. Example 2 A bullet fired from a gun has a maximum horizontal range of 2000 m. Find the muzzle velocity of the gun (i.e. the speed with which the bullet leaves the gun). Solution So we have θ = 45o, Rmax = 2000 m, u =? and g = 9.8 ms−2 MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 10 / 13
  • 16. Example 2 A bullet fired from a gun has a maximum horizontal range of 2000 m. Find the muzzle velocity of the gun (i.e. the speed with which the bullet leaves the gun). Solution So we have θ = 45o, Rmax = 2000 m, u =? and g = 9.8 ms−2 By using in Eqn 8; Rmax = u2 g 2000 = u2 9.8 u = (2000 ∗ 9.8), ⇒ u = 140 ms−1 MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 10 / 13
  • 17. Trial Questions 1 A particle is projected from a point on level ground such that its initial velocity is 28 ms−1 at an angle of 45 o above the horizontal. Taking g as 9.8 ms−2, find the time taken for the particle to reach its maximum height. MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 11 / 13
  • 18. Trial Questions 1 A particle is projected from a point on level ground such that its initial velocity is 28 ms−1 at an angle of 45 o above the horizontal. Taking g as 9.8 ms−2, find the time taken for the particle to reach its maximum height. 2 A particle is projected from a point on a horizontal plane and has an initial velocity u at an angle of θ above the plane. Show; by using the equation; v2 y = u2 sin2 θ − 2gy, that the greatest height h reached by the particle above the plane is given by h = u2 sin2 θ 2g . MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 11 / 13
  • 19. Trial Questions 1 A particle is projected from a point on level ground such that its initial velocity is 28 ms−1 at an angle of 45 o above the horizontal. Taking g as 9.8 ms−2, find the time taken for the particle to reach its maximum height. 2 A particle is projected from a point on a horizontal plane and has an initial velocity u at an angle of θ above the plane. Show; by using the equation; v2 y = u2 sin2 θ − 2gy, that the greatest height h reached by the particle above the plane is given by h = u2 sin2 θ 2g . 3 A particle is projected from a point on a horizontal plane with an initial velocity of 140 ms−1 at an angle of elevation of 30o. Find the greatest height reached by the particle above the plane. MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 11 / 13
  • 20. Trial Questions 1 A particle is projected from a point on level ground such that its initial velocity is 28 ms−1 at an angle of 45 o above the horizontal. Taking g as 9.8 ms−2, find the time taken for the particle to reach its maximum height. 2 A particle is projected from a point on a horizontal plane and has an initial velocity u at an angle of θ above the plane. Show; by using the equation; v2 y = u2 sin2 θ − 2gy, that the greatest height h reached by the particle above the plane is given by h = u2 sin2 θ 2g . 3 A particle is projected from a point on a horizontal plane with an initial velocity of 140 ms−1 at an angle of elevation of 30o. Find the greatest height reached by the particle above the plane. For more questions; https://bit.ly/Projectile_questions and for notes https://bit.ly/Projectile_notes . All are reading materials are saved on https://bit.ly/padlet-DESII MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 11 / 13
  • 21. Summary A Projectile is any object that when thrown continues, continues in motion under its own inertia. Equations of motion 1 Horizontal Motion; x = u cos θ · t 2 Vertical motion; vy = u sin θ − gt y = − 1 2 gt2 + u sin θ · t and v2 y = u2 sin2 θ − 2gy 1 Maximum Height; Hmax = u2 sin2 θ 2g , 2 Time at Hmax; t = u sin θ g , 3 Time of Flight; T = 2u sin θ g , 4 Range;R = u2 sin 2θ g , Rmax = u2 g Equation of a Trajectory; y = x tan θ − gx2 2u2 sec2 θ. MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 12 / 13
  • 22. Thank You for Your Attention For more information Contact me through; herbertmujungu@gmail.com +256779547251 +256701310635 +256793854372 The class facebook account is; NTC-KABALE, MATHEMATICS YEAR II, 2019/2020 The class whatsapp account is; NTC-KABALE, MTC2, 2019/20 MUJUNGU HERBERT (Mathematics Lecturer) (National Teachers College Kabale)PROJECTILES May 25, 2020 13 / 13