Projectiles
When a body is projected from
a point in such a way that the only force assumed to be acting is gravity then
that body is classed as a projectile.
Parametric and Cartesian forms of equations of the trajectory (flight path)
The derivation of the following equations
is a little tricky but the process has appeared on an Edexcel
paper at M2.

Suppose a particle P is projected from O at angle α and is at the point (x,y) at time t after leaving O.
Equation of motion for P horizontally is F
= ma
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Therefore
and velocity parallel
to Ox is constant and equal to Vcosα.
For constant velocity x
= vel × time
x
= Vcosαt (1)
Equation of motion for P
vertically F = ma
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Using constant acceleration equations ![]()
With u = sinα and a = -g
(2)
1 and 2 are the parametric equations of trajectory.
Rearrange 1 to give:
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Substitute into equation 2
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(3)
Equation 3 is the Cartesian form of the trajectory of a
projectile. Assuming V, g and α are
constants for any particular case, this is the equation of a parabola.
Maximum height of a projectile.
At the maximum height the vertical
component of the velocity is zero.
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Time to maximum height and time of flight
Using v
= u + at
At maximum height v = 0
u = Vsinα 0 = Vsinα – gt
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For time of flight on the horizontal plane we use:
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There is zero displacement vertically hence s = 0.
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![]()
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and ![]()
By symmetry this time is twice the value to maximum height.
For sloping planes, (cliffs etc) use s as the vertical
displacement from the starting point to the landing point.
Range on the horizontal plane
Using equation 1 x
= Vcosαt
Time in flight is ![]()
Therefore range R is: - ![]()
![]()
2sinαcosα =
sin2α
![]()
Maximum range appears when sin2α = 1
Therefore
α = 45º
and
![]()
Examples
1. A particle is projected from a point O
with a speed of
at an angle of
elevation of arcsin
.
a) Find the greatest height above O
reached by the particle .
b) The particle strikes the horizontal through O at Q find the distance OQ.

a) Using the maximum height
formula
![]()

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You could also work out the answer by considering the vertical
component of the velocity and then use the constant acceleration equations.
Vertical component is given by
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At maximum height velocity equals zero.
Using:
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b) OQ is the horizontal range
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Which can be expressed as:
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2. A girl hits a ball at an
angle arctan
to the horizontal from a point O which is 0.5m
above level ground. The initial speed of the ball is
. The ball just clears a fence which is a
horizontal distance of 18m from the girl. By modelling
the ball as a particle find the time taken for the ball to reach the fence and
the height of the fence.

Horizontal component of the velocity is Vcosα.
Therefore time in flight is
given by:
![]()

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We must now consider the motion vertically to calculate the height of the
fence. The vertical component of the
velocity is:
and
by using ![]()

Fence
height = 12.9m
Questions A
1 A cricket ball is
hit from a point which is 0.9m above horizontal ground. It is given an initial
speed of
at an angle
of elevation of 27 º.
Find:
a) the time taken for the ball to reach
the ground.
b) the horizontal distance covered by the
ball.
2 A tennis ball is
served from a height of 2.6m at horizontal speed of
. The net is 0.9m high and 13m horizontally from the
server. Modelling
the ball as a particle, determine whether the ball clears the net and if so by
what distance.
3 A golfer hits a ball
with velocity
at an angle
θ above the horizontal, where
. Find the time for which the ball is at least 12m above the
ground.
4 A particle is
projected from a point O with speed
at an angle
above the horizontal.
Find
a) the time the particle takes to reach
the point P whose horizontal displacement is 96 metres,
b) the height of P above O,
c) the speed of the particle 2 seconds
after projection.
5 A cannon ball fired
at an angle of 10º has a range, on a horizontal plane, of 1.25km. Ignoring air
resistance, find the speed of projection.
6 A ball is projected
with velocity
. If the range on the horizontal plane is 60m, find the two
possible angles of projection.
7 At time t seconds,
where t≥0, the velocity v ms-1
of a particle Q moving in a straight line is given by
![]()
When t = 0, Q is at point O.
a) Find the acceleration of Q at time t.
b) Calculate the time at which Q returns to O.
Differentiating and
Integrating Vectors
The constant
acceleration equations were used extensively in M1 but in M2 displacement is a
function of time. It follows then that
velocity, which is the rate of change of displacement, can be found by
differentiating the displacement function.
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Displacement
Differentiate Velocity Integrate
(Remember
the constant)
Acceleration
If r is the position vector, and using dot
notation: -

Example 1
The position
vector of a particle Q at time t
is
(r measured in metres).
Find the initial
position vector and show that the acceleration is constant
Initial position
is when t=0
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Remembering that ![]()
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Since the
acceleration vector has no variable t it
is said to be constant.
Integrating Vectors
Since a vector has
both i and j components it will also
have two separate functions with respect to time.
Therefore if ![]()
We need to
integrate each function separately, remembering the constants.
Therefore ![]()
Where
are constants of integration.
R
is found by integrating the velocity function with respect to time.
Example 2
A particle moves
such that at time t
![]()
At
time t = 0 the particle has a position vector 5i – 6j
Find
the position vector at time t.
The
position vector is found by integrating the velocity vector.
At
time t = 0, r = 5i – 6j
,![]()
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Example
3
A
particle Q has position vector ( 25i – 40j )m
at time t = 0 relative to the origin. Q moves with constant acceleration and is
equal to
. When t = 0,
. Find:
a)
when
t = 4
b)
The distance of Q from O at this time.
a) By integrating the acceleration vector we can
find the velocity vector.

At
time t = 0,
![]()
![]()
When
t = 4 ![]()
b)
To find the distance OQ we need the position vector (r)
![]()

When
t = 0, r = 25i – 40j
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Substituting
t = 4 gives ![]()
Distance
OQ is the magnitude of r
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Example 4
A remote control
car is being tested in a horizontal playground. At time t seconds, the position
vector, r metres,
of the car relative to a fixed point O is given by
![]()
At the instant
when t = 4,
a) show that the car is moving with velocity ![]()
b) find the magnitude of the acceleration of the car.
A cyclist is
moving with constant velocity
. At the instant when t = 4, calculate
c) the velocity of the car relative to the cyclist;
d) the speed of the car relative to the cyclist;
e) the acute angle between the relative velocity and the
constant velocity of the cyclist.
a) ![]()

When t = 4 ![]()
b) ![]()
![]()
When t = 4 ![]()
So 
c) The velocity of
the car relative to the cyclist is given by:
![]()
d) the speed of the car relative to the cyclist is given by:

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e) The cyclist is
moving parallel to the vector j.
The car has
velocity
which can be represented diagrammatically as:

The required angle is θ, where

Example
5
A particle P of mass 5kg is acted on by a
constant force F. At time t seconds the position of the
particle, r metres,
is given by the equation
![]()
where k is a positive constant.
a) Find the acceleration of P in
in terms of
k
b) Given that the magnitude of F
is 50N, calculate the value of k.
The particle is moving in a direction parallel to j when t = T.
c) Find the value of T.
d) Hence find, to the nearest 0.1º, the angle that the position
vector makes with the direction of i when t = T
a) To find the acceleration we need to differentiate the position
vector twice.

b) F = 50N and by using F = ma

But K is positive, so K = 4
c) The particle is now traveling parallel
to j. Therefore the
i
component of the velocity must equate to zero.
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Therefore:

d) When
![]()
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The angle that the position vector makes
with the vector i
is given by:

Questions B
1 At time t=0 a particle Q is at the point
with position vector (6i + 10j)m relative
to a fixed origin O. The particle moves
with constant acceleration
where
. Given that when t=0,
find
a) the velocity,
, when t=3,
b) the distance of
Q from O at this time.
2 A
particle Q moves such that at time t seconds, t≥0, its position
vector, r metres,
relative to a fixed origin is given by
![]()
a) Find the velocity of Q when t = 3.
The velocity of Q is parallel to (3i – j) when t = T.
b) Find the value of T.
3 A
particle moves so that at time t seconds its position vector, rm, relative to
a fixed origin is given by:
![]()
where b is a constant.
a) Find an expression for the velocity of
the particle at time t seconds.
b) Given that the particle comes to
instantaneous rest, find the value of b.
4 A
ball of mass
0.1kg is hit by a bat which gives it an impulse of
( 3.5i + 3j)Ns.
The velocity of the ball immediately after being hit is
.
a) Find the
velocity of the ball immediately before it was hit.
In the subsequent motion the ball is
modeled as a particle moving freely under gravity. When it is hit the ball is 0.8m above the
ground.
b) Find the
greatest height of the ball above the ground.
The ball is caught when it is 0.8m above
the ground again.
c) Find the
distance from the point where the ball is hit to the point where it is caught.