09 Spring Constant, Lecture notes of Law

In this experiment, values of x for a number of values of Fext are determined by changing M. Then a graph of M vs. x is plotted and k is determined from the ...

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Exp 9-1 P
Experiment 9. Spring Constant
-Is rubber more elastic than steel?
The answer lies in the concept of elasticity.
Objective:
To determine the spring constant of a spring by
(a) static method, and (b) dynamic method.
Apparatus:
A spring, a hanger with a light aluminium pointer, a small scale etched
on a plane mirror strip, weights, a timer.
Theory:
(a) Static method:
Consider a spring hanging from a rigid
support. When a load m is suspended from
the free end of the spring, an external, Fext,
acts on the spring in the downward direction.
The support applies an equal force in the
upward direction. Thus the spring has a Spring
balanced system of forces acting on it and it
is in equilibrium. . The length of the string
-increases and an internal (restoring) force
Fi nt is developed in the spring due to the
elasticity of the spring. This internal force
tends to bring the spring back to its original
length when the external forces are
withdrawn. Note that Fint and Fext are
equal in magnitude.
According to Hooke's law,
Fi nt is directly proportional to x, the
change in the length of the spring. Mirror
Thus Fint=-kx (1)
Here k is the constant of proportionality,
known as the spring constant or force
constant. The minus (-) sign indicates that
Fint and x are in opposite directions.
Obviously,
Fext=kx.
Eqs. (1) and (2) indicate that the sprin ,g constant k
to the force required to change the length of the spring
(2)
is numerically equal
by 1 unit.
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Exp 9-1 P

Experiment 9. Spring Constant

Is rubber more elastic than steel? The answer lies in the concept of elasticity.

Objective: To determine the spring constant of a spring by (a) static method, and (b) dynamic method. Apparatus: A spring, a hanger with a light aluminium pointer, a small scale etched on a plane mirror strip, weights, a timer. Theory: (a) Static method: Consider a spring hanging from a rigid support. When a load m is suspended from the free end of the spring, an external, Fext, acts on the spring in the downward direction. The support applies an equal force in the upward direction. Thus the spring has a Spring balanced system of forces acting on it and it

  • is^ in^ equilibrium.^.^ The^ length^ of^ the^ string increases and an internal (restoring) force Fi nt is developed in the spring due to the elasticity of the spring. This internal force tends to bring the spring back to its original length when the external forces are withdrawn. Note that Fint and Fext are equal in magnitude. According to Hooke's law, Fi nt is directly proportional to x, the change in the length of the spring. (^) Mirror

Thus Fint=-kx (1)

Here k is the constant of proportionality, known as the spring constant or force constant. The minus (-) sign indicates that Fint and x are in opposite directions. Obviously, Fext=kx. Eqs. (1) and (2) indicate that the sprin ,g constant k to the force required to change the length of the spring

is numerically equal by 1 unit.

Exp 9-2P

  • If the load on the spring is M and MP is the sum of the mass of the hanger and the effective mass of the spring, Fext = (M+Mp)g. In this experiment, values of x for a number of values of Fext are determined by changing M. Then a graph of M vs. x is plotted and k is determined from the slope of the graph. (b) Dynamic method: If a mass M is suspended from a spring of spring constant k and the system is made to oscillate, then for small amplitudes of oscillations· (that is, within elastic limit) along the length of the spring, the motion of the system is simple harmonic. In this case, the time period T of the system is given by T = 2 n,J M: rv'lp, (3) where Mp is the effective mass of the spring which is approximately equal to 1 /3 the mass of the spring (Reference: Vibrations and Waves by A. P. French, pages 60-61 ). In this experiment, Mp is eliminated in the following manner:
  • (^) 4n 2 4n 2 Eq. (3) gives T^2 = -- M + -· Mp. k k Thus if we plot T2 vs. M, then for a given spring (k and MP constant), the

graph will be a straight line. By choosing two points (M 1 , T 12 ) and (M 2 ,

T 2 2) on the graph, we get (^2) = 4n -·-M (^2)^ 4n 2 2 4n 2 4n 2 T (^1) k 1 + --Mpk and T 2 = --M2k + --Mp.k By subtracting one equation from the other, we get 2 2 4n 2 ( ) T 2 - T 1 = - M2 - M1 , k or k = 41t2 (M 2 - M1). (4) T2 -T2 2 1 Procedure: (a) Static method:

  1. Arrange the apparatus as shown in the figure. Make sure that the aluminum pointer is close to the mirror on which the scale is etched
  • (^) but it does not touch the mirror.

York College of The City University of New York

Physics I Name: Experiment No. 9: Pre-Lab Questionnaire

  1. A student finds the following values from a graph between M and x in the static method of determining the spring constant k: x 1 = 0.5 cm; x2 = 7.8 cm; M1 = 120 gm; M2 = 300 gm. Calculate the value of k.
  2. Consider the following data for an experiment to study the spring
  • constant by dynamic method: Number of oscillations, N = 25 Load M 1 = 120 gm; average time for N oscillations = 11.0 seconds Load M 2 = 280 gm; average time for N oscillations = 16.9 seconds Calculate the spring constant k. (Note that the mass of the hanger is not given.)

Experiment No. 9 ·

Name: Marks:

Partner: Rem9rks:

Section:

Date Submitted:

Title:

Objective:

Theory/Formulas:

Exp 9-7D

Experiment No. 9: Questions

  1. State Hooke's law.
  1. What is meant by the spring^ constant^ of^ a spring?I (RemE3n,ber, it is also (^) known as force conrant.)
  2. Under what conditions the period of oscillations of a mass on a spring is given by

T = 2rc~?

  1. Why is it not necessary to use the mass of the hanger in the calculations of the load on the spring?
  2. If the load M on the spring is made 4 times its previous value, will the time period then become exactly double its previous value? Explain your answer.

..JI 0