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⚡ Physics / Mechanics / Experiment 07

Determination of the Modulus of Rigidity
of a Wire using Maxwell's Needle

Measure the torsional stiffness of a wire by comparing the periods of oscillation of Maxwell's needle in two mass configurations.

⌬  Level: Undergraduate◈  Topic: Elasticity↻  Method: Dynamic
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Objective

Section 01

Aim

To determine the modulus of rigidity η of the material of a given wire by the dynamic method using Maxwell's needle.

Learning objectives

After completing this experiment, students will be able to:

  1. Explain shear stress, shear strain, and modulus of rigidity.
  2. Describe the construction and working principle of Maxwell's needle.
  3. Measure the wire radius, needle length, masses, and oscillation time periods.
  4. Use two mass arrangements to eliminate the moment of inertia of the needle.
  5. Calculate G in pascals and estimate experimental uncertainty.
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Theory

Section 02

Modulus of rigidity

The modulus of rigidity (or shear modulus) of a material is defined as the ratio of shearing stress to shearing strain, within the elastic limit.

η = Shearing stressShearing strain

For a cylindrical wire of radius r and length L, the torsional constant k of the wire is:

k = πηr42L   (1)

Here, r is the radius of the suspension wire, L is its length, η is the modulus of rigidity, and k is the torsional constant.

Principle of Maxwell's needle

Maxwell's needle consists of a cylindrical body suspended horizontally by a thin wire. When the needle is slightly twisted about the axis of the wire and released, it performs torsional oscillations.

T = 2π√(I/k)   (2)
I = kT24π2   (3)

Combining this with Eq. (1),

η = 8πLIr4T2.

Experimental arrangement

The Maxwell's needle arrangement consists of a hollow cylindrical tube, two identical solid cylinders, and a suspension wire. The solid and hollow cylinders are placed symmetrically about the axis of suspension in two different configurations.

Configuration I: The solid cylinders are placed farther from the axis of suspension, while the hollow cylinders are placed closer to the axis. Let the moment of inertia and time period be I1 and T1, respectively.

Configuration II: The positions of the solid and hollow cylinders are interchanged. Let the moment of inertia and time period be I2 and T2, respectively.

This arrangement permits the difference I1 − I2 to be determined without requiring the moment of inertia of Maxwell's needle itself.

Determination of the difference in moments of inertia

Let ms be the mass of each solid cylinder, mh the mass of each hollow cylinder, and L the distance between the centres of the cylinders. The distances of the cylinders from the axis of suspension are 3L/8 and L/8.

I1 − I2 = 2(ms − mh) [(3L/8)2 − (L/8)2]
I1 − I2 = (ms − mh)L24   (5)

Relation between time period and moment of inertia

T1 = 2π√(I1/k)   and   T2 = 2π√(I2/k)

Therefore,

I1 = kT124π2   and   I2 = kT224π2.
k = 4π2(I1 − I2)T12 − T22   (6)
k = π2(ms − mh)L2T12 − T22   (7)

Formula for modulus of rigidity

From Eq. (1),

η = 2Lkπr4.

Substituting Eq. (7), we obtain the working formula:

η = 2πL3(ms − mh)r4(T12 − T22)

Final working formula

SymbolMeaning
ηModulus of rigidity of the suspension wire
LDistance between the centres of the cylinders
rRadius of the suspension wire
msMass of each solid cylinder
mhMass of each hollow cylinder
T1Time period with solid cylinders at the outer positions
T2Time period after interchanging the cylinders

SI unit of η: N m-2 (Pa).

Note: The final expression is written in the simplified and dimensionally consistent form:

η = 2πL3(ms − mh)r4(T12 − T22).
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Apparatus Required

Section 03

Equipment

  • Inertia table with suspension wire and torsional support
  • Rectangular test block or plane lamina
  • Three levelling screws and spirit level
  • Stopwatch or digital timer
Inertia table and rectangular test block
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Procedure

Section 04

Procedure — Verification of the Perpendicular Axis Theorem

Using an Inertia Table

  1. Level the apparatus: Place the inertia table on a stable horizontal surface and adjust its levelling screws until the table is properly level, using a spirit level.
  2. Determine the natural period of the unloaded inertia table: Place the circular inertia table on its support and ensure that it is properly balanced and free to rotate about the suspension wire. Give the table a small angular displacement and release it gently to produce torsional oscillations. Measure the time t0 required for 20 complete oscillations using a stopwatch. Repeat the measurement and determine the mean value. The period is T0 = t0/20.
  3. Measurement for rotation about the Z-axis: Place the rectangular block centrally on the inertia table with its base parallel to the XY-plane, so that its centre of mass lies on the axis of rotation. Give the table a small angular displacement and release it gently. Measure the time t1 for 20 complete oscillations and calculate T1 = t1/20.
  4. Measurement for rotation about the X-axis: Reorient the block so that its base is parallel to the YZ-plane, while keeping its centre of mass coincident with the axis of rotation. Give a small angular displacement and release the system. Measure the time t2 for 20 complete oscillations and calculate T2 = t2/20.
  5. Measurement for rotation about the Y-axis: Reorient the block so that its base is parallel to the ZX-plane, with its centre of mass still on the axis of rotation. Measure the time t3 for 20 complete oscillations and calculate T3 = t3/20.
  6. Repeat the measurements: Repeat the measurements of t0, t1, t2, and t3 at least three times and determine their mean values to reduce random errors.
  7. Verification: Use the measured values of T0, T1, T2, and T3 to test the relation T12 = T22 + T32 − T02. Agreement within the experimental uncertainty verifies the Perpendicular Axis Theorem of Moment of Inertia.

Important Experimental Precautions

  • Use only small angular displacements so that the torsional oscillations remain approximately simple harmonic.
  • Release the table gently without giving it an additional push.
  • Ensure that the block is centrally positioned and its centre of mass remains on the axis of rotation.
  • Count complete oscillations consistently and minimise timing errors while using the stopwatch.
  • Keep the apparatus free from unnecessary disturbances during measurement.
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Simulation

Interactive
Loading Maxwell's Needle simulation...
Modulus of Rigidity by Maxwell's Needle
ⓘ Interactive applet / Compare the two mass configurations↻ Record time for repeated oscillations
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Observation Table

Section 06
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Result and Analysis

Section 07

Calculation

Use the mean readings in the expression below. Since the period is squared, accurate wire-radius measurement is especially important.

η = 2πL3(ms − mh)r4(T12 − T22)

Record your calculation

MCQs: Verification of the Perpendicular Axis Theorem of Moment of Inertia

Level: Moderate · Select the most appropriate answer.

10 questions1 mark each
Question 1 The perpendicular axes theorem is applicable to which type of body?
Question 2 If Ix and Iy are the moments of inertia about two mutually perpendicular axes in the plane of a lamina, then Iz about the perpendicular axis is:
Question 3 For the theorem to be valid, the three axes must:
Question 4 A circular lamina has Ix = 0.020 kg m2 and Iy = 0.020 kg m2. The moment of inertia about the perpendicular axis is:
Question 5 If Ix = 0.012 and Iy = 0.018 kg m2, the expected value of Iz is:
Question 6 Why is the perpendicular axis generally associated with a larger moment of inertia than either in-plane axis?
Question 7 In a torsional oscillation method, the time period T is related to moment of inertia I by, where C is the torsional constant:
Question 8 If Ix = 25 g cm2, Iy = 35 g cm2, and Iz = 61 g cm2, the percentage deviation is approximately:
Question 9 Which observation provides the strongest evidence for successful verification?
Question 10 A student obtains Ix = 40 g cm2, Iy = 30 g cm2, and Iz = 68 g cm2. Which conclusion is most appropriate?