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To determine the rigidity modulus of the material of the given wire by dynamical method using a Torsional pendulum.

Apparatus Required:

:Torsional Pendulum, Stop Watch, Vertical Pointer, Screw Gauge and Vernier Calipers.

Description:

Torsional Pendulum consists of a uniform metal disc (or cylinder) suspended by a wire whose rigidity modulus is to be determined. The lower end of the wire is gripped in a chuck fixed at the center of the disc and the upper end is gripped in another chuck fixed to a wall bracket as shown in the fig.

Torisional pendulum

The disc is turned through a small angle in the horizontal plane to oscillations about the axis of the wire. The period of oscillations given by

T = 2π √I/C-------------------------------------------(1)

Where I is the moment of inertia of the disc about the axis of rotation and C is the couple per unit twist of the

But C = πna 4 /2L-------------------------------------------(2)

Where a is the radius of the wire L is its length and n is the rigidity modulus. From (I) and (II) we have

n = 8πI/a 4 L/T 2 -------------------------------------------(3)

In the case of a circular disc (or cylinder) whose geometric axis coincides with axis of rotation of the moment of inertia I is given by

Where M is the mass of the disc and R is the radius .On substituting the value of I in the Eqn. (III), we get

n = 8π/2 MR 2 /a 4 L/T 2 -------------------------------------------(4)

A meter wire whose ‘n’ is to be determined is taken without any kinks. The disc is suspended from one end of the wire .The other end of the wire is passed through the chuck fixed to the wall bracket and is rigidly fixed .The length ‘L’ of the wire between the chucks is adjusted to a convenient value (say 50 cms). A pin is fixed vertically on the edge of the disc and a vertical pointer is placed in front of the disc against the pin to serve as a reference to count the oscillations.

The disc is turned in the horizontal plane through a small angle, so as to twist the wire and released. There should not be any up and down and lateral movements of the disc. When it is executing Torsional oscillations, time for 20 oscillations is noted twice and the mean is taken. The period (T) is then calculated 1/T 2

The experiment is repeated for different values of ‘L’ and in each case the period is determined. The value of L/T 2 is calculated for each length. The observations are tabulated. From the observations mean the value of L/T 2 is calculated.

The mass ‘M’ of the disc is measured with a physical balance and its radius ‘R’ is calculated with Vernier calipers. The radius of the wire ‘a’ is determined very accurately with screw gauge at three of four different places and means value is taken since it occurs in fourth power.

Substituting these values in eqn (IV) ‘n’ is calculated. A graph is drawn taking the value of ‘L’ on the ‘x’ axis and the corresponding values of T 2 on the Y- axis. It is a straight line graph passing through origin. Slope can be calculated from the graph by inverting the slope we will get L/T2 Substituting this value ‘n’ is calculated.

The wire should be free from kinks.

The disc should not wobble.

Observations:-

Least count of vernier callipers

LC = 1 MSD / n; where, n= Total number of divisions in vernier scale

Least count of screw gauge

LC = 1 PSD / n; where, n= Total number of divisions on head scale

Tabular form:

Determination of Radius of disc

S.No. MSR(cm) VSR(cm) (D) TOTAL = MSR + VSR(LC)
1
2
3
4
5
6

Diameter of disc, D

Radius of disc R = D / 2

Determination of radius of wire (a)

S.No. PSR (mm) Corrected HSR (A) TOTAL = PSR + HSR(LC)
1
2
3
4
5
6

Diameter of Wire A =

Radius of Wire a = A/2 =

Least count of Vernier callipers(L.C) =----------------cms

Least count of Screw gauge (L.C) =----------------cms

Average radius of the wire (a) =----------------cms

Mass of the disc (M) =------------------------gms

Mean radius of the disc R =----------------cms

Table to find time period

Mean value of L/T 2 =

Calculations

m= (8π/2) (MR 2 /a 4 ) (L/T 2 )

m= (8π/2) (MR 2 /a 4 ) (1/slope)

Precautions:

  • The disc should be handled carefully.
  • The time for oscillations should be correctly noted.
  • Kinks should not be present along the length of the wire.

Rigidity modulus (n) of the wire dynes/cm 2 (By table)

Rigidity modulus (n) of the wire dynes/cm 2 (By Graph)

S.No. Length L Time for 20 oscillations/Trail I/Trail II/Mean time Time Period T=Meantime/20 T LT
1
2
3
4
5
6

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The photograph to the right shows the apparatus for the experiment.

The is mounted at the top, and hangs down into the chamber. We show a brass disc hanging from the wire. Its orientation is the same as in the .

You will measure different objects' period of oscillation with the supplied stopwatch.

Barely visible in the photograph is a plexiglas door, which is open in the picture. You will close it before taking data so that air currents do not disturb the motion of the object.

Do attempt to adjust the wire with the mount at the top. If you suspect the apparatus needs adjustment see your Demonstrator or one of the lab technologists.

You will measure the period of oscillation for 4 different moments of inertia. The above photograph shows the brass disc oriented for one of the moments of inertia you will measure. Here are the other 3 moments you will use:

The disc hanging from the wire in another orientation. This corresponds to above.

A hollow cylinder. Its moment of inertia is given by .

The same hollow cylinder and a solid brass rod. This corresponds to and , whose moment of inertia is given above.

A document on reading a vernier is available by clicking on the red button to the right. It will appear in a separate window, and has a file size of 56k. You should have your browser enabled for to effectively use this introduction.

A document on using a micrometer is available by clicking on the blue button to the right. It will appear in a separate window, and has a file size of 86k.

You will measure the period of oscillation for each moment of inertia with the stopwatch. A preparatory question below explores the best procedure to use for this measurement.

Although the data collection is simple and straightforward, the analysis of the your results and especially the calculation of the uncertainties in your determinations of the moments of inertia may seem at first to be a bit daunting. A preparatory question below, however, is intended to show you how to make these calculations much simpler than they seem.

We hope that the following questions will guide you in your preparation for the experiment you are about to perform. They are not meant to be particularly testing, nor do they contain any "tricks". Once you have answered them, you should be in a good position to begin the experiment.

Measured with a meter stick
Measured with a vernier caliper
Measured with a vernier caliper
Measured with a balance
  • Convert all the above values to SI units.
  • What is the percentage error in L ?
  • What is the value and error in p = L 2 /12?
  • What is the percentage error in p ? How does it compare to the percentage error in L ?
  • What is the value, error, and percentage error in a ?
  • What is the value and error in a 2 ?
  • How does the percentage error in a 2 compare to the percentage error in a ?
  • What is the value and error in b 2 ?
  • What is the value and error in q = ( a 2 + b 2 )/4?
  • For the previous calculation, is one of the errors negligible? If yes, which?
  • What is the percentage error in q ? Have you calculated any other percentage errors with this value?
  • What is the value and error in r = p + q ?
  • What is the value and error in the moment of inertia I = M r ?
  • What is the percentage error in I ? Have you calculated any other percentage errors with this value?

As promised, we have prepared a summary of the information presented above. It does not attempt to provide a full discussion, but just reviews the "high points" from above.

You may access the summary by clicking on the green button to the right. The summary is in pdf format, will appear in separate window, and has a file size of 47k. You may wish to print this document.

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Torsion pendulum test on metal wire.

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🕑 Reading time: 1 minute

Modulus of Rigidity is the coefficient of elasticity of wire for a shearing force. In simple words, rigidity modulus of a metal wire is a measurement of the capability of a material to resist deformation when external tangential (parallel to the surface) force is applied to the metal wire.

Torsion Pendulum Test Apparatus

Aim of the Test

To determine the rigidity modulus of the suspension wire using torsion pendulum.

Apparatus Required

  • Torsion Pendulum
  • Cylindrical wire
  • Vernier Caliper
  • Screw gauge
  • Meter scale
  • Test Specimens - Steel and Brass Wire.

Torsion Pendulum Principle

For small oscillations of the disc, it is in simple harmonic motion and the formula for simple pendulum holds good.

image

Where, T = period of oscillation in sec. I = Mass moment of inertia of the rotating system about the longitudinal axis of wire. L = Length of the wire between its grips. N = Modulus of rigidity (Shear modulus).

image

d = diameter of the given wire in the test

Equations 1 and 2 refer to conditions when no cylindrical weight is added on to the disc and when known cylindrical weights are added, We have,

image

From which it follows-

image

(I 2 -I 1 ) is the mass moment of inertia of the cylindrical weights about the axis of rotation of the disc. It is given by,

formula

Where, W = Total weight of cylinders added to the disc. g = Acceleration due to gravity. r = Radius of cylindrical weights. R = distance from center of the cylinder of the cylindrical weight to center of the wire.

Thus from equations (5) and (6)

image

Test Procedure

Part 1: Determination of Rigidity modulus using Torsion pendulum alone

  • The radius of the suspension wire is measured using a screw gauge.
  • The length of the suspension wire is adjusted to suitable values.
  • The wire for the test is tightened at its bottom to the disc and its top to the bracket.
  • The disc is turned and released without the cylindrical weights on it.
  • Time for a number oscillation (Say 20) is measured with a stopwatch and the mean period of oscillation ' T 0 ' is determined.

Part 2:  Determination of rigidity modulus and moment of inertia using torsion pendulum with identical masses

  • The two identical masses are placed symmetrically on either side of the suspension wire as close as possible to the center of the disc and and the distance d1 is measured which is the distance between the centers of the disc and one of the identical masses.
  • Find the time for 20 oscillations twice and determine the mean period of oscillation T 1 .
  • The two identical masses are placed symmetrically on either side of the suspension wire as far as possible to the center of the disc and measure d 2  which is the distance between the centers of the disc and one of the identical masses.
  • Find the time for 20 oscillations twice and determine the mean period of oscillation T 2 .
  • Find the moment of inertia of the disc and rigidity modulus of the suspension wire using the given formulae.

Observation and Calculation

For Part 1 -

observation table

Rigidity modulus of the suspension wire =

formula

For Part 2 -

observation table

Applications of Torsional Pendulum

  • The working of "Torsion pendulum clocks" (shortly torsion clocks or pendulum clocks), is based on torsional oscillation.
  • The freely decaying oscillation of  Torsion pendulum in medium(like polymers), helps to determine their characteristic properties.
  • New researches promising the determination of frictional forces between solid surfaces and flowing liquid environments using forced torsion pendulums.

Gopal Mishra

Gopal Mishra

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IMAGES

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  3. Torsional pendulum Rigidity Modulus Experiment Readings/Values

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  4. Measure rigidity modulus of suspension wire using Torsional Pendulum Theory & Simulation explained

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