| Spring-Mass
System
A
body of mass m attached to an ideal spring of stiffness k,
and free to move over a frictionless horizontal surface, is
an example of a simple harmonic oscillator (see Fig.1). Note
that there is a position (the equilibrium position: see Fig.1(a)
in which the spring exerts no force on the body. If the body
is displaced to the right (as in Fig.1(b)), the force exerted
by the spring on the body points to the left and is given
by
F
= -kx.
If
the body is displaced to the left (as in Fig.1(c)), the force
points to the right and is also given by
F=
-kx.
In
each case the force is a restoring force. The motion of the
oscillating mass is simple harmonic motion.

Figure
1
Experiment
1: Spring-Mass System
Supplies
1.
Several soft springs having different stiffnesses.
2. Objects of mass (for example, wood or metal blocks, or
any object weighing more than the spring).
3. Something to which the spring can be attached securely.
(Examples: a piece of plywood, ceiling, or metal frame, etc).
NOTE:
This experiment can be performed
either vertically or horizontally, but as shown in Figure
2, a vertical arrangement is easier to construct.
Procedure
(for vertical arrangements)
1.
Attach spring to the wood or metal frame and measure the total
length of the spring.
2. Hang a weight on the end of the spring.
3. Measure the distance that the end of the spring moves (x)
due to the weight (Force).
4. Repeat step 3 for each weight (F).
5. Plot Force vs. x (displacement) on graph paper or Excel
worksheet (more advanced student). The slope of the line (units
lb/in) gives the spring stiffness k.
6. Pull the weight downward and release. Count the number
of oscillations occurring over one minute. Divide the number
of oscillations by 60 seconds to get the frequency (f).
7. Compare the measured frequency to the predicted frequency:

where
,
and k has units lb/in.
8. Repeat steps 1-7 for different springs. Plot frequency
vs. spring stiffness and freqency vs. mass.
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