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Instruction sheet

3B SCIENTIFIC

3B SCIENTIFIC

3B SCIENTIFIC

3B SCIENTIFIC

3B SCIENTIFIC

® 

PHYSICS

PHYSICS

PHYSICS

PHYSICS

PHYSICS

U10362 Ballistic pendulum

®

9/04 MH

1

Projectile launcher (U10360)

2

Back plate

3

Guide for swing pointer

4

Bearing screw

5

Counter bearing

6

Swing pointer

7

Angle scale

8

Pendulum

9

Projectile catcher

bl

Base plate

bm

Table clamp

bn

Knurled screw

bo

Ramrod (for U10360)

bp

Extra weights, 2 pcs.

1 2 3 4

5

6

7

8

9

bl

bm

bn

Fig. 1: Components

bp

bo

1. Safety instructions

This instruction sheet is concerned mainly with the
ballistic pendulum. You should also read the in-
structions for the projectile launcher U10360.

To check whether a projectile is located in the pro-
jectile launcher and the spring is cocked, only use
the observation holes at the sides. Do not look into
the barrel from the front. Risk of injury!

Never aim at people!

Protective goggles should be worn during the ex-
periments.

The projectile launcher should always be stored
with the spring loose and with no projectile in the
barrel.

2. Description

The ballistic pendulum is for experiment-based
determination of the launch velocity of a projec-
tile when it leaves the projectile launcher. It is also
possible to determine trajectories when the pro-
jectile is launched horizontally or at an angle.
Launch heights of 5, 10, 15, 20 or 30 cm can be
selected easily with the aid of the drilled holes.

Thanks to the extreme lightness of the pendulum,
the experiment can be performed using compara-

tively safe plastic projectiles instead of steel balls.
Experiments involving inelastic collisions (quanti-
tatively) and elastic collisions (qualitatively) can be
evaluated. The velocity of the projectiles deter-
mined from trajectory and pendulum experiments
typically agree to within about 3%.

Extra weights allow various pendulum travels to
be investigated for constant speeds.

3. Operation and maintenance

First the ballistic pendulum is screwed to a stable
bench by means of its clamp. The projectile
launcher is then screwed to the back plate 

2

 rom

behind either in a horizontal position in front of
the pendulum as in Fig. 1 or as shown in Fig 3.

Tip:

 if the workbench is not stable enough, it may

be that when the pendulum swings to its maximum
extent and then swings back, it may jog the appa-
ratus when striking the projectile launcher, caus-
ing the swing pointer to be shifted out of line. If
this happens, the pendulum should rather be
stopped by hand.

Projectiles should always be loaded when the sp-
ring is not under tension by placing the sphere in
loosely through the front of the plastic cylinder

Summary of Contents for U10362

Page 1: ...so possible to determine trajectories when the pro jectile is launched horizontally or at an angle Launch heights of 5 10 15 20 or 30 cm can be selected easily with the aid of the drilled holes Thanks to the extreme lightness of the pendulum the experiment can be performed using compara tively safe plastic projectiles instead of steel balls Experiments involving inelastic collisions quanti tativel...

Page 2: ...ision For experi ments on elastic collisions the pendulum should be turned round by 180 cf Section 3 Opera tion 4 1 2 Experiment procedure It is practical for these experiments to enter the experiment number the spring tension 1 2 or 3 the type of collision inelastic i or elastic e the number of extra weights used and the mea sured angle ϕ In order to obtain the most accu rate experiment results a...

Page 3: ...lues should be determined sepa rately for every pendulum since material and manufacturing tolerances mean that values may differ from one to another 4 1 3 2 Elastic collision For a swinging pendulum Eq 5 is still valid for the motion after a collision the only difference being that the moment of inertia IP is determined without the projectile but with any extra weights pendulum mass mP ω ϕ 2 1 cos...

Page 4: ... 0 62 3 15 5 2 0 90 5 15 6 3 0 120 7 15 4 1 3 Experiment evaluation It is practical to take as the origin of the coordi nate system the mid point of the projectile at the moment of launch Then the following applies vX v0 cos ϕ 17 vY v0 sin ϕ 18 y v t gt Y 1 2 2 19 x vX t 20 From Eq 20 t x vX whereby the time can be eliminated from Eq 19 If vX and vy are then eliminated from the resulting equation ...

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