The previous diagrams, tables, and discussion pertain to
how the horizontal and vertical components of the velocity vector change with
time during the course of projectile's trajectory. Now we will investigate the
manner in which the horizontal and vertical components of a projectile's
displacement vary with time.As has already been discussed, the vertical displacement (denoted by the symbol y in the
discussion below) of a projectile is dependent only upon the acceleration of
gravity and not dependent upon the horizontal velocity. Thus, the vertical
displacement (y) of a projectile
can be predicted using the same equation used to find the displacement of a
free-falling object undergoing one-dimensional motion. This equation was
discussed in Unit 1 of The Physics Classroom. The equation can be
written as follows.
y = 0.5 • g • t2
(equation for vertical
displacement for a horizontally launched projectile)
where g is -9.8
m/s/s and t is the time in seconds. The above equation pertains to a projectile with
no initial vertical velocity and as such predicts the vertical distance that a
projectile falls if dropped from rest. It was also discussed earlier, that the force
of gravity does not influence the horizontal motion of a projectile. The
horizontal displacement of a projectile is only influenced by the speed at
which it moves horizontally (vix) and the amount
of time (t) that it has
been moving horizontally. Thus, if the horizontal displacement (x) of a projectile were represented by an
equation, then that equation would be written as
x = vix • t
The diagram below shows the trajectory of a projectile (in
red), the path of a projectile released from rest with no horizontal velocity
(in blue) and the path of the same object when gravity is turned off (in
green). The position of the object at 1-second intervals is shown. In this
example, the initial horizontal velocity is 20 m/s and there is no initial
vertical velocity (i.e., a case of a horizontally launched projectile).
As can be seen in the diagram above, the vertical distance
fallen from rest during each consecutive second is increasing (i.e., there is a
vertical acceleration). It can also be seen that the vertical displacement
follows the equation above (y = 0.5 • g • t2). Furthermore, since
there is no horizontal acceleration, the horizontal distance traveled by the projectile each second is a constant
value - the projectile travels a horizontal distance of 20 meters each second.
This is consistent with the initial horizontal velocity of 20 m/s. Thus, the
horizontal displacement is 20 m at 1 second, 40 meters at 2 seconds, 60 meters
at 3 seconds, etc. This information is summarized in the table below.
|
Horizontal Displacement |
Vertical Displacement |
0 s |
0 m |
0 m |
1 s |
20 m |
-4.9 m |
2 s |
40 m |
-19.6 m |
3 s |
60 m |
-44.1 m |
4 s |
80m |
-78.4 m |
5 s |
100 m |
-122.5 m |
Now consider displacement values for a projectile launched at
an angle to the horizontal (i.e., a non-horizontally launched projectile). How
will the presence of an initial vertical component of velocity affect the
values for the displacement? The diagram below depicts the position of a
projectile launched at an angle to the horizontal. The projectile still falls
4.9 m, 19.6 m, 44.1 m, and 78.4 m below the straight-line, gravity-free path.
These distances are indicated on the diagram below.
The projectile still falls below its gravity-free path by a
vertical distance of 0.5*g*t^2. However, the gravity-free path is no longer a
horizontal line since the projectile is not launched horizontally. In the
absence of gravity, a projectile would rise a vertical distance equivalent to
the time multiplied by the vertical component of the initial velocity (viy• t). In the presence of gravity, it will
fall a distance of 0.5 • g • t2. Combining these two influences upon
the vertical displacement yields the following equation.
y = viy • t + 0.5 • g • t2
(Equation for vertical displacement for an angled-launched
projectile)
where viy is the initial vertical velocity in m/s, t is the
time in seconds, and g = -9.8 m/s/s (an approximate value of the acceleration of gravity). If a
projectile is launched with an initial vertical velocity of 19.6 m/s and an
initial horizontal velocity of 33.9 m/s, then the x- and y- displacements of
the projectile can be calculated using the equations above. A sample
calculation is shown below.
|
The following table lists the results of such calculations
for the first four seconds of the projectile's motion.
|
Horizontal Displacement |
Vertical Displacement |
0 s |
0 m |
0 m |
1 s |
33.9 m |
14.7 m |
2 s |
67.8 m |
19.6 m |
3 s |
101.7 m |
14.7 m |
4 s |
135.6 m |
0 m |
The data in the table above show the symmetrical nature of a
projectile's trajectory. The vertical displacement of a projectile t seconds
before reaching the peak is the same as the vertical displacement of a
projectile t seconds after reaching the peak. For
example, the projectile reaches its peak at a time of 2 seconds; the vertical
displacement is the same at 1 second (1 s before reaching the peak) is the same
as it is at 3 seconds (1 s after reaching its peak). Furthermore, the time to
reach the peak (2 seconds) is the same as the time to fall from its peak (2
seconds).
Use your understanding of projectiles to answer the following
questions. Then click the button to view the answers.
1. Anna Litical drops a
ball from rest from the top of 78.4-meter high cliff. How much time will it
take for the ball to reach the ground and at what height will the ball be after
each second of motion?
It will take 4 seconds to fall 78.4 meters
Use the equation y = 0.5 • g • t2 and substitute
-9.8 m/s/s for g. The vertical displacement must then be subtracted from the
initial height of 78. 4 m.
At t = 1 s, y = 4.9 m (down) so height is 73.5 m (78.4 m - 4.9 m )
At t = 2 s, y = 19.6 m (down) so height is 58.8 m (78.4 m -
19.6 m )
At t = 3 s, y = 44.1 m (down) so height is 34.3 m (78.4 m - 45 m)
At t = 4 s, y =
78.4 m (down) so height is 0 m (78.4 m - 78.4 m)
2. A cannonball is launched horizontally from the top
of an 78.4-meter high cliff. How much time
will it take for the ball to reach the ground and at what height will the ball
be after each second of travel?
It will still take 4 seconds to fall 78.4 meters
Use the equation y = 0.5 • g • t2 and substitute
-9.8 m/s/s for g. The vertical displacement must then be subtracted from the
initial height of 78. 4 m.
At t = 1 s, y =
4.9 m (down) so height is 73.5 m (78.4 m - 4.9 m )
At t = 2 s, y = 19.6 m (down) so height is 58.8 m (78.4 m - 19.6 m )
At t = 3 s, y = 44.1 m (down) so height is 34.3 m (78.4 m - 45 m)
At t = 4 s, y =
78.4 m (down) so height is 0 m (78.4 m - 78.4 m)
NOTE: the cannon
ball's horizontal speed does not affect the time to fall a vertical distance of
78.4 m.
3. Fill in the table below indicating the value of the
horizontal and vertical components of velocity and acceleration for a
projectile.
The vx values
will remain constant at 15.0 m/s for the entire 6 seconds; the ax values will be 0 m/s/s for the entire 6
seconds.
The vy values
will be changing by -9.8 m/s each second. Thus,
vy = 29.4 m/s (t = 0 s)
vy = 19.6 m/s (t = 1 s)
vy = 9.8 m/s (t = 2 s)
vy = 0 m/s (t = 3 s)
vy = -9.8 m/s (t = 4 s)
vy = -19.6 m/s (t = 5 s)
vy = -29.4 m/s (t = 6 s)
The ay values
will be -9.8 m/s/s for the entire 6 seconds.
4. The diagram below shows the trajectory for a projectile
launched non-horizontally from an elevated position on top of a cliff. The
initial horizontal and vertical components of the velocity are 8 m/s and 19.6
m/s respectively. Positions of the object at 1-second intervals are shown.
Determine the horizontal and vertical velocities at each instant shown in the
diagram.
The vx values
will remain 8 m/s for the entire 6 seconds.
The vy values
will be changing by 9.8 m/s each second. Thus,
vy =9.8 m/s (t = 1 s)
vy = 0 m/s (t = 2 s)
vy = -9.8 m/s (t = 3 s)
vy = -19.6 m/s (t = 4 s)
vy = -29.4 m/s (t = 5 s)
vy = -39.2 m/s (t = 6 s)
The following diagram pertains to questions #1
and #2 above. A scale is used where 1 cm = 5 meters. (Note that 1-cm may be a
different distance for different computer monitors; thus, a cm-ruler is given
in the diagram.)