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PROJECTILE MOTION
▢ Definition:
Table 1: Projectile Motion
Term | Meaning |
|---|---|
Condition | Initial velocity and acceleration act at angle other than 0° or 180° |
Path | Parabolic |
Projectile motion | Motion of particle in plane under gravity alone |
Projectile | Particle thrown into space |
Acceleration | Constant = g downward |
Velocity | Changes in magnitude and direction |
▢ Types:
Table 1: Types of Projectile Motion
Type | Condition |
|---|---|
Horizontal projectile | Particle projected horizontally from height H with speed u |
Oblique projectile | Particle projected from ground with velocity u at angle heta with horizontal |
▢ Horizontal Projectile from Height H:
❖ Condition: Projected horizontally from height H with speed u
❖ Components:
Table 1: Horizontal Projection Components
Component | Value |
|---|---|
Horizontal velocity | u_x=u |
Vertical velocity initially | u_y=0 |
Horizontal acceleration | a_x=0 |
Vertical acceleration | a_y=-g |
❖ Motion Equations:
Table 1: Horizontal Projectile Formulae
Quantity | Formula |
|---|---|
Horizontal distance in time t | x=ut |
Vertical position in time t | y=H- rac{1}{2}gt^2 |
Trajectory | y=H- rac{1}{2}g eft( rac{x}{u} ight)^2 |
Time of flight | T= qrt{ rac{2H}{g}} |
Horizontal range | R=uT=u qrt{ rac{2H}{g}} |
Vertical range | H |
Final vertical velocity | v_y=gT= qrt{2gH} |
Final velocity | v_f= qrt{u^2+(gT)^2}= qrt{u^2+2gH} |
Angle with horizontal at striking point | an hi= rac{v_y}{v_x}= rac{gT}{u}= rac{ qrt{2gH}}{u} |
❖ Energy and Direction:
- •Velocity, speed, kinetic energy and momentum increase gradually
- •Potential energy gradually decreases
- •Mechanical energy remains constant
- •Acceleration remains constant
- •Angle between velocity and acceleration decreases gradually
▢ Oblique Projection:
❖ Condition: Projected from ground with initial velocity u at angle heta with horizontal
❖ Components:
Table 1: Oblique Projection Components
Component | Value |
|---|---|
Horizontal velocity | u_x=u os heta |
Vertical velocity | u_y=u in heta |
Horizontal acceleration | a_x=0 |
Vertical acceleration | a_y=-g |
❖ Motion Equations:
Table 1: Oblique Projectile Formulae
Quantity | Formula |
|---|---|
Horizontal distance in time t | x=u os heta t |
Vertical distance in time t | y=u in heta t- rac{1}{2}gt^2 |
Trajectory | y=x an heta- rac{g x^2}{2u^2 os^2 heta} |
Time of flight | T= rac{2u in heta}{g} |
Horizontal range | R= rac{u^2 in2 heta}{g} |
Maximum height | H= rac{u^2 in^2 heta}{2g} |
Useful relation | rac{1}{2}gT^2=R an heta=4H |
For R=H | heta= an^{-1}(4)=75.96^ irc |
❖ Velocity:
Table 1: Velocity During Oblique Motion
Point | Velocity |
|---|---|
At projection | u |
At highest point | u os heta |
At same level of projection | u |
At highest point vertical velocity | v_y=0 |
At highest point horizontal velocity | v_x=u os heta |
At ground, angle of velocity | heta below horizontal |
❖ Energy and Direction:
- •Speed, velocity, momentum and kinetic energy first decrease
- •At highest point, speed/KE/momentum become minimum
- •After highest point, speed/KE/momentum increase
- •Potential energy first increases, becomes maximum at highest point, then decreases
- •Mechanical energy remains constant
- •Acceleration remains constant
- •Angle between acceleration and velocity changes from (90^ irc+ heta) to (90^ irc- heta)
- •At highest point, velocity and acceleration are perpendicular
▢ At Highest Point of Oblique Projectile:
❖ Given: Mass m , initial velocity u , angle heta , initial KE E_0 , initial momentum p_0
Table 1: Quantities at Highest Point
Quantity | Formula |
|---|---|
Horizontal velocity | v_x=u os heta |
Vertical velocity | v_y=0 |
Net velocity | v=u os heta |
Momentum | P=mu os heta=p_0 os heta |
Kinetic energy | E_K= rac{1}{2}mv^2=E_0 os^2 heta |
Potential energy | E_P=mgH=E_0 in^2 heta |
Total mechanical energy | E_0 |
▢ Change in Quantities:
Table 1: Change from Projection
Quantity | From departure to highest point | From departure to arrival |
|---|---|---|
Speed | u-u os heta=u(1- os heta)=2u in^2 rac{ heta}{2} | 0 |
Velocity | elta u_x=0, elta u_y=u in heta, elta u=u in heta | 2u in heta |
Momentum | mu in heta | 2mu in heta=2p_0 in heta |
Kinetic energy | E_0-E_0 os^2 heta=E_0 in^2 heta | 0 |
Potential energy | E_0 in^2 heta | 0 |
Direction change | heta | 2 heta |
Average velocity | rac{u}{2} qrt{1+3 os^2 heta} | u os heta |
▢ Effect of Air Resistance:
- •Maximum height decreases
- •Horizontal range decreases
- •Speed at striking point decreases
- •Momentum at striking point decreases
- •Kinetic energy at striking point decreases
- •Time of flight is greater when air resistance is neglected
- •With air resistance, angle of striking is greater than angle of projection
▢ Read and Digest:
Table 1: Projectile Special Points
Case | Result |
|---|---|
To hit a target with rifle | Aim slightly higher than target |
Body dropped from uniformly moving vehicle | Path appears straight line to passenger |
Same dropped body seen from ground | Path appears parabolic |
One ball falls vertically and another is projected horizontally from same height | Both reach ground simultaneously |
Time to reach ground from height h | t= qrt{ rac{2h}{g}} |
One ball dropped and another thrown horizontally from same height | Horizontally thrown ball reaches ground with greater speed |
Javelin throw | Best practical angle is slightly less than 45° |
▢ High-Yield Recall:
Table 1: Projectile Motion One-Liners
Fact | Answer |
|---|---|
Path of projectile | Parabola |
Projectile acceleration | g downward |
Horizontal acceleration | 0 |
Vertical acceleration | -g |
Horizontal projectile time | T= qrt{ rac{2H}{g}} |
Horizontal projectile range | R=u qrt{ rac{2H}{g}} |
Horizontal projectile final velocity | v_f= qrt{u^2+2gH} |
Oblique projectile time of flight | T= rac{2u in heta}{g} |
Oblique projectile range | R= rac{u^2 in2 heta}{g} |
Maximum height | H= rac{u^2 in^2 heta}{2g} |
Range maximum angle | 45^ irc |
Velocity at highest point | u os heta |
Vertical velocity at highest point | 0 |
KE at highest point | E_0 os^2 heta |
PE at highest point | E_0 in^2 heta |
Momentum at highest point | p_0 os heta |
Mechanical energy | Constant |
If R=H | heta= an^{-1}4 |
Passenger view of dropped body | Straight line |
Ground observer view of dropped body | Parabola |
Javelin practical angle | Slightly less than 45° |
Q1.
A body is projected making angle 60° with vertical. What is the value of KE at the highest point?
📅CEE MBBS 2024B
Q2.
If the velocity of a body at maximum height is half of the initial velocity, find the range of the projectile if the initial velocity is u.
📅CEE MBBS 2024a
Q3.
Two bodies are projected at angles 45° and 60° respectively with the horizontal. If both attain the same maximum height, the ratio of their ranges is:
📅CEE MBBS 2021
Q4.
What is the ratio of the time of flight when a projectile is projected at an angle of θ and (90 − θ)?
📅CEE BDS 2024
Q5.
In a projectile motion, maximum horizontal range is obtained at the projection angle of ..... with horizontal:
📅CEE BDS 2024
Q6.
A plane is moving with 300 ms⁻¹ when it is just above the observer at a height of 2 km. At what angle with the vertical must he fire the gun with velocity 600 m/s directly to hit the aeroplane?
📅CEE BDS 2024
Q7.
The total time of flight for an object thrown upward with initial velocity u and g gravity of planet is:
📅CEE BDS 2023
Q8.
A fielder can throw a cricket ball to a maximum horizontal distance of 100 m. How high the fielder can throw the same ball?
📅CEE BDS 2021
Q9.
When air resistance is included, which property of a projectile generally increases relative to motion in vacuum?
📅BP 2014
Q10.
📅BP 2010
Q11.
Q12.
📅IOM 2014
Q13.
📅MOE 2012•MOE 2011
Q14.
📅MOE 2011
Q15.
📅IOM 2013
Q16.
Q17.
Q18.
Q19.
📅MOE 2013
Q20.
Q21.
Q22.
Q23.
Q24.
Q25.
Q26.
Q27.
Q28.
Q29.
Q30.
Q31.
Q32.
Q33.
Q34.
Q35.
📅MOE 2009
Q36.
📅IOM 2063 (source printed TOM 063)
Q37.
A ball is projected horizontally from a tower. Neglecting air resistance, its horizontal velocity component:
📅MOE 066
Q38.
Two bullets are fired horizontally from the same height at the same time, with different horizontal speeds. Which reaches the ground first?
📅MOE 2065
Q39.
📅MOE 2062
Q40.
📅MOE 2000
Q41.
📅MOE (year unspecified)
Q42.
📅IE 2002
Q43.
If both the mass and velocity magnitude of a projectile are doubled, its linear momentum magnitude becomes:
📅IE 2005
Q44.
📅IE 2007
Q45.
📅BPKIHS-09
Q46.
For a particular projectile, its horizontal range is four times its maximum height. What is its launch angle?
📅BPKIHS-07
Q47.
📅BPKIHS 02
Q48.
A passenger on a train moving at constant velocity drops a ball. What path does a stationary observer on the platform see, neglecting air resistance?
📅KU 2015
Q49.
📅KU 2017
Q50.
A stone is released from rest from a tower and experiences a constant horizontal force from wind throughout its fall. What is its trajectory if the net acceleration is constant?
📅IOM 2017