2. PROJECTILE MOTION:-
When a particle is thrown obliquely
near the earth’s surface it moves along
a curved path, such particle is called
projectile and it motion is said to be
projectile motion.
4. Terminology:-
Point of projection:- the point on the earth
from where particle is thrown .
Angle of projection (𝜽):- the angle made
by the velocity with x-axis is called as angle
of projection.
Trajectory:- the path followed by the
particle is called as the trajectory.
6. Sign convention:-
The vertically upward direction is
taken as the positive direction of
the y-axis.
The vertically downward motion
is taken as the negative direction
of the y- axis.
7. Terminology:-
u - initial velocity
𝜃 − 𝑎𝑛𝑔𝑙𝑒 𝑜𝑓 𝑝𝑟𝑜𝑗𝑒𝑐𝑡𝑖𝑜𝑛
ux - horizontal velocity(m/s)
uy - vertical velocity (m/s)
ax-acceleration in horizontal direction
ay – acceleration in vertical direction
t – time in second (s)
x – horizontal displacement
y- vertical displacement
8. Component of velocity and
acceleration:-
𝒖 𝒙= u cos 𝜽
𝒖 𝒚= u sin 𝜽
𝒂 𝒙= 0 m/s2
𝒂 𝒚= -g m/s2
9. Equation of motion for
horizontal direction:-
𝒂 𝒙= 0 m/s2
1. 𝒗 𝒙 = 𝒖 𝒙 + 𝒂 𝒙t
𝒗 𝒙 = 𝒖 𝒙=u cos 𝜽
2. x = 𝒖 𝒙t +
𝟏
𝟐
a𝒕 𝟐
x = u t cos 𝜽
t =
𝒙
𝒖𝒄𝒐𝒔𝜽
…………(1)
11. Time of flight:-
It is the total time taken for which the projectile
remains in its flight. (T)
y = 𝒖 𝒚 𝒕 -
𝟏
𝟐
g𝒕 𝟐
As we know that displacement along the y-axis is zero
( y = 0 ).
y = ut sin𝜽 −
𝟏
𝟐
g𝒕 𝟐
=> 0
=> usin𝜽 =
𝟏
𝟐
gt
…… (2)
T=
𝟐 𝒖 𝒔𝒊𝒏𝜽
𝒈
12. Horizontal Range:-
It is the horizontal distance travelled by the
particle during its time of flight.
So, range = horizontal velocity* time of flight
R = u cos𝜽 * T
From equation no (1) T=
𝟐 𝒖 𝒔𝒊𝒏𝜽
𝒈
R= u cos𝜽 *
𝟐 𝐮 𝐬𝐢𝐧𝛉
𝐠
….(3)
R =
𝒖 𝟐 𝐬𝐢𝐧𝟐𝜽
𝒈
13. Maximum height :-
It is the maximum vertical distance attained by the projectile
above the horizontal plane of projection.
Vertical velocity become zero at the maximum height.
𝑣 𝑦= 𝑢 𝑦- gt => 𝑣 𝑦= usin𝜃 – gt = 0
t =
usin 𝜃
𝑔
….(3)
Max height=
H = 𝑢 𝑦 𝑡 -
1
2
g𝑡2
Putting value of t from equation no (3)
H= usin𝜃 *
usin 𝜃
𝑔
-
1
2
g(
usin 𝜃
𝑔
∗
usin 𝜃
𝑔
)
….(4)
H =
𝐮 𝟐 𝐬𝐢𝐧 𝟐 𝛉
𝟐𝐠
14. Equation of trajectory:-
We know that displacement along y-axis is
Y = 𝒖 𝒚 𝒕 -
𝟏
𝟐
g𝒕 𝟐
=> u sin𝜽 t -
𝟏
𝟐
g𝒕 𝟐
From equation no 1 :- t =
𝒙
𝒖𝒄𝒐𝒔𝜽
Put the value of t in above equation we get,
y = u sin𝜽 ∗
𝒙
𝒖𝒄𝒐𝒔𝜽
-
𝟏
𝟐
g(
𝒙
𝒖𝒄𝒐𝒔𝜽
) 𝟐
On solving we get :-
y = x tan𝜽 −
𝟏
𝟐
(
𝒈
𝒖 𝟐𝒄𝒐𝒔 𝟐
𝜽
)𝒙 𝟐 ……..(5)
15. Velocity of the projectile at any
instant:-
In projectile motion, vertical component of velocity
changes but horizontal
component of velocity remains always constant.
Horizontal component of velocity=> 𝒖 𝒙= u cos 𝜽
Vertical component of velocity =>
. 𝒗 𝒚=usin𝜽 – gt
The resultant velocity will be:-
V= (u cos 𝜽) 𝟐+(usin𝜽 – gt ) 𝟐
Direction:-
tan𝜷 =
𝒗 𝒚
𝒗 𝒙
=
usin 𝜽 – gt
u cos 𝜽
16. Numerical:-
Q(1). A javelin thrower launches his javelin
with an initial velocity of 20 m/s at an angle
of 40 above the horizontal.
a) Calculate:
i. The initial horizontal velocity ii. The initial
vertical velocity
b) What is the maximum height the javelin
will reach?
c) What is the range of the javelin?
17. Solution:-
(a). Trigonometry is used to find the initial components of the velocity:
Horizontal:-
𝒖 𝒙= u cos 𝜽
𝒖 𝒙= 20 cos 𝟒𝟎 = 15.3m/s
Vertical :-
𝒖 𝒚= u sin 𝜽
𝒖 𝒚= 20 sin 40 = 12.9m/s
(b). The maximum height of the javelin depends on the vertical velocity so we use the
equations of motion:
𝒖 𝒚= 12.9 m/s
𝒗 𝒚 = 0 m/s
a = -9.8 m/s2
s = ?
t = X
𝒗 𝒚
𝟐
= 𝒖 𝒚
𝟐
- 2gy
𝟎 𝟐
=𝟏𝟐. 𝟗 𝟐
- 2*9.81*y
Y=8.5m
18. c) The range of a projectile will depend on the time of flight. The
time of flight is controlled by the vertical velocity:-
Y = 𝑢 𝑦 𝑡 -
1
2
g𝑡2
0=12.9t-
1
2
*9.81*𝑡2
t=2.6sec
The range of the projectile is then given by:
X=v*t
X=15.30*2.6
X=39.8m ….this will range of the projectile.
19. Question 2
The trajectory of a projectile is
represented by Y= 3𝑥 -
𝑔𝑥2
2
. then
the angle of projection is
(a) 30
(b) 45
(c) 60
(d) None of these
20. solution
By comparing the coefficient of x in given equation with standard
equation
y =x tan𝜃 −
1
2
(
𝑔
𝑢2𝑐𝑜𝑠2
𝜃
)𝑥2
tan𝜃 = 3
𝜃 = 60.
23. Trajectory of the projectile:-
The horizontal displacement x is governed by the equation
x = ut
t =
𝒙
𝒖
Vertical distance travelled by the body in time t :-
y = 𝒖 𝒚 𝒕 +
𝟏
𝟐
g𝒕 𝟐
𝒖 𝒚 =0 (only horizontal velocity will be given)
Y =
𝟏
𝟐
g𝒕 𝟐
=
𝟏
𝟐
g (
𝒙
𝒖
)
𝟐
Y=k𝒙 𝟐
……….this also equation of parabola
24. Time of flight:-
For vertical downward motion of the body
h = 𝒖 𝒚 𝒕 +
𝟏
𝟐
g𝒕 𝟐
𝒖 𝒚 = 0
Then ,
T = √
𝟐𝒉
𝒈
…… this is the time of flight.
26. Questions 3
A body is projected horizontally from the top of a
tower with initial velocity 18 ms–1. It hits the ground at
angle 45o. What is the vertical component of velocity
when it strikes the ground
(a) 9 m/s
(b) 9 √2 m/s
(c) 18 m/s
(d) 18√ 2 m/s
27. solution
When the body strikes the ground
tan45 =
𝑣 𝑦
𝑣 𝑥
=
𝑣 𝑦
18
𝑣 𝑦 = 18m/s
Correct answer :- (c)
28. Question 4
An aeroplane is flying at a height of 1960 m in
horizontal direction with a velocity of 360 km/hr. When
it is vertically above the point. A on the ground, it
drops a bomb. The bomb strikes a point B on the
ground, then the time taken by the bomb to reach the
ground is
(a) 2√20 sec
(b) 20 sec
(c) 2 √10 sec
(d) 10 sec
29. solution
We know that
Time of flight:-
T = √
2ℎ
𝑔
= T = √
2∗1960
9.8
T= 20sec
Correct answer :- (b)
30. Question 5
A bomb is dropped on an enemy post by an aeroplane flying with a
horizontal velocity of 60 km/hr and at a height of 490 m. How far
the aeroplane must be from the enemy post at time of dropping the
bomb, so that it may directly hit the target. (g = 9.8 m/s2)
(a)
100
3
m
(b)
500
3
m
(c)
200
3
m
(d)
400
3
m
31. solution
S= u*t
S=u*√
2ℎ
𝑔
S=60*
5
18
∗ √
2∗490
9.8
On solving we get,
S=
500
3
m
Correct answer :- (b)