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LEP
1.3.11
Projectile motion
R
PHYWE series of publications • Laboratory Experiments • Physics • PHYWE SYSTEME GMBH • 37070 Göttingen, Germany 21311 1
Related topics
Trajectory parabola, motion involving uniform acceleration,
ballistics.
Principle and task
A steel ball is fired by a spring at different velocities and at dif-
ferent angles to the horizontal. The relationships between the
range, the height of projection, the angle of inclination, and the
firing veolocity are determined.
Equipment
Ballistic pendulum 11229.00 1
Recording paper, 1 roll, 25 m 11221.01 1
Steel ball, d 19 mm 02502.01 2
Two-tier platform support 02076.03 1
Meter scale, demo, l = 1000 mm 03001.00 1
Barrel base 02006.10 1
Timer 4-4 13605.99 1
Speed measuring attachement 11229.30 1
Connecting cord, 750 mm, red 07362.01 1
Connecting cord, 750 mm, yellow 07362.02 2
Connecting cord, 750 mm, blue 07362.04 1
Problems
1. To determine the range as a function of the angle of incli-
nation.
2. To determine the maximum height of projection as a func-
tion of the angle of inclination.
3. To determine the (maximum) range as a function of the ini-
tial velocity.
Set-up and procedure
Tthe ballistics units is adjusted. The scale is set to read 90°
and a ball is fired upwards (setting 3) and is caught in the
hand. The support base adjusting screws are turned until a
vertical projection is obtained.
The initial velocities of the ball corresponding to the three ten-
sion stages of the firing spring can be determined using the
speed measuring attachment and timer (resolution 0.1 ms), or
from the maximum height for a vertical projection from the
expression v0 = . The inital velocities may vary greatly
from unit to unit.
͙2gh
Fig. 1: Experimental set-up for measuring the meximum range of a projectile with additional equipment to measure the initial
velocity.
LEP
1.3.11
Projectile motion
R
21311 PHYWE series of publications • Laboratory Experiments • Physics • PHYWE SYSTEME GMBH • 37070 Göttingen, Germany2
The 2-tier platform support (02076.01) is used for determining
th range. To mark the points of impact, the recording strip is
secured to the bench with adhesive tape. It is best to measure
the long ranges before the short ones (secondary impact
points!) and to mark the primary impact points with a felt pen.
The distance from the ballistics unit is frequently checked with
the metre scale during the test. An empty box can be placed
behind the bench to catch the balls.
To measure the height of projection the metre scale is clam-
ped in the barrel base and moved parallel to the plane of pro-
jection. The empty box is again used to catch the balls. The
heights of projection can be determined ballistically quite well
by eye.
Theory and evaluation
If a body of mass m moves in a constant gravitational field
(gravitational force mg
Ǟ
), the motion lies in a plane.
If the coordinate system is laid in this plane (x, y plane – see
fig. 2) and the equation of motion:
m r
Ǟ
(t) = mg
Ǟ
where:
r
Ǟ
= (x,y) ; g
Ǟ
= (o, –g)
is solved, then, with the initial conditions
r (o) = 0
v
Ǟ
(o) = (vo cos ␾, vo sin ␾)
we obtain the coordinates as a function of time t:
x (t) = vo · cos ␾ · t
y (t) = vo · sin ␾ · t – t2
:
From this, the maximum height of projection h is obtained as
a function of the angle of projection ␾:
h = sin2
␾
and the maximum range s is:
s = sin 2 ␾
From the regression line of the data of fig. 5, using the expres-
sion:
Y = A · XB
we obtain the exponent
B = 2.01 = 0.001 (see (1))
vo
2
g
vo
2
2 g
g
2
d2
dt2
Fig. 2: Movement of a mass point under the effect of gravita-
tional force.
Fig. 3: Maximum range as a function of the angle of inclination
␾ for different initial velocity vo:
Curve 1 vo 5.3 m/s
Curve 2 vo 4.1 m/s
Curve 3 vo 3.1 m/s
Fig. 4: Maximum height of projection h as a function of the
angle of inclination ␾ for the initial velocities as in Fig. 1:
LEP
1.3.11
Projectile motion
R
PHYWE series of publications • Laboratory Experiments • Physics • PHYWE SYSTEME GMBH • 37070 Göttingen, Germany 21311 3
Note
To ensure an accurate determination of the initial velocity with
the timer, the time taken for the ball to cover the measuring
distance must be taken into account. If vexp is the experimen-
tally determined inital velocity we obtain
vo =
where d is the distance between the point of rotation and the
centre between the light barriers.
͙v2
exp ϩ 2g d sin ␾
Fig. 5: Maximum range s as a function of the inital velocity vo
with a fixed angle of inclinination ␾ = 45°.

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1 3 11

  • 1. LEP 1.3.11 Projectile motion R PHYWE series of publications • Laboratory Experiments • Physics • PHYWE SYSTEME GMBH • 37070 Göttingen, Germany 21311 1 Related topics Trajectory parabola, motion involving uniform acceleration, ballistics. Principle and task A steel ball is fired by a spring at different velocities and at dif- ferent angles to the horizontal. The relationships between the range, the height of projection, the angle of inclination, and the firing veolocity are determined. Equipment Ballistic pendulum 11229.00 1 Recording paper, 1 roll, 25 m 11221.01 1 Steel ball, d 19 mm 02502.01 2 Two-tier platform support 02076.03 1 Meter scale, demo, l = 1000 mm 03001.00 1 Barrel base 02006.10 1 Timer 4-4 13605.99 1 Speed measuring attachement 11229.30 1 Connecting cord, 750 mm, red 07362.01 1 Connecting cord, 750 mm, yellow 07362.02 2 Connecting cord, 750 mm, blue 07362.04 1 Problems 1. To determine the range as a function of the angle of incli- nation. 2. To determine the maximum height of projection as a func- tion of the angle of inclination. 3. To determine the (maximum) range as a function of the ini- tial velocity. Set-up and procedure Tthe ballistics units is adjusted. The scale is set to read 90° and a ball is fired upwards (setting 3) and is caught in the hand. The support base adjusting screws are turned until a vertical projection is obtained. The initial velocities of the ball corresponding to the three ten- sion stages of the firing spring can be determined using the speed measuring attachment and timer (resolution 0.1 ms), or from the maximum height for a vertical projection from the expression v0 = . The inital velocities may vary greatly from unit to unit. ͙2gh Fig. 1: Experimental set-up for measuring the meximum range of a projectile with additional equipment to measure the initial velocity.
  • 2. LEP 1.3.11 Projectile motion R 21311 PHYWE series of publications • Laboratory Experiments • Physics • PHYWE SYSTEME GMBH • 37070 Göttingen, Germany2 The 2-tier platform support (02076.01) is used for determining th range. To mark the points of impact, the recording strip is secured to the bench with adhesive tape. It is best to measure the long ranges before the short ones (secondary impact points!) and to mark the primary impact points with a felt pen. The distance from the ballistics unit is frequently checked with the metre scale during the test. An empty box can be placed behind the bench to catch the balls. To measure the height of projection the metre scale is clam- ped in the barrel base and moved parallel to the plane of pro- jection. The empty box is again used to catch the balls. The heights of projection can be determined ballistically quite well by eye. Theory and evaluation If a body of mass m moves in a constant gravitational field (gravitational force mg Ǟ ), the motion lies in a plane. If the coordinate system is laid in this plane (x, y plane – see fig. 2) and the equation of motion: m r Ǟ (t) = mg Ǟ where: r Ǟ = (x,y) ; g Ǟ = (o, –g) is solved, then, with the initial conditions r (o) = 0 v Ǟ (o) = (vo cos ␾, vo sin ␾) we obtain the coordinates as a function of time t: x (t) = vo · cos ␾ · t y (t) = vo · sin ␾ · t – t2 : From this, the maximum height of projection h is obtained as a function of the angle of projection ␾: h = sin2 ␾ and the maximum range s is: s = sin 2 ␾ From the regression line of the data of fig. 5, using the expres- sion: Y = A · XB we obtain the exponent B = 2.01 = 0.001 (see (1)) vo 2 g vo 2 2 g g 2 d2 dt2 Fig. 2: Movement of a mass point under the effect of gravita- tional force. Fig. 3: Maximum range as a function of the angle of inclination ␾ for different initial velocity vo: Curve 1 vo 5.3 m/s Curve 2 vo 4.1 m/s Curve 3 vo 3.1 m/s Fig. 4: Maximum height of projection h as a function of the angle of inclination ␾ for the initial velocities as in Fig. 1:
  • 3. LEP 1.3.11 Projectile motion R PHYWE series of publications • Laboratory Experiments • Physics • PHYWE SYSTEME GMBH • 37070 Göttingen, Germany 21311 3 Note To ensure an accurate determination of the initial velocity with the timer, the time taken for the ball to cover the measuring distance must be taken into account. If vexp is the experimen- tally determined inital velocity we obtain vo = where d is the distance between the point of rotation and the centre between the light barriers. ͙v2 exp ϩ 2g d sin ␾ Fig. 5: Maximum range s as a function of the inital velocity vo with a fixed angle of inclinination ␾ = 45°.