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Engineering Physics Experiments for BE and B.Tech., Prof. Praveen N. Vaidya, SDMCET Dharwad.
TORSIONAL PENDULUM
Aim: To determine the Rigidity modulus of the given Brass wire by using Torsional pendulum apparatus.
Apparatus: Brass wire, Circular disc with chuck nuts, Digital stop clock, Laboratory stand, and meter scale.
Principle: The torsional pendulum experiment is based on the principle of application of shearing stress to
the wire, hence it can show the shear strain, and therefore the ratio of shearing stress to shearing strain is
given the Modulus of rigidity.
Theory: A simple pendulum is a system of thread its one end is fixed to a ceiling and other end tied to a
mass and let free give periodic oscillations.
However, in case of torsional pendulum, one end of thread (normally metallic) tied to ceiling and other end
is tied to a mass in the form of disc at its center. If the disc is rotated through an angle โ€˜ฮธโ€™ from mean
position, so that the thread also twists and show resistance to rotate, if the disc is released now, the disc
starts giving to and fro rotations about its axis as shown in figure.
Since the mass is moving very quickly, it overshoots at the equilibrium
position and rotates through an angle โ€˜ฮธโ€™ in opposite direction.
The restoring force of metallic thread slows the mass down and causes
it to rotate the other way back. The restoring force is actually
proportional to the rotation angle โ€˜ฮธโ€™ of the disc.
During this time wire twists through angle ฯ†, so that l ฯ† = r ฮธ
Or or ๐œ‘ =
๐‘Ÿ๐œƒ
๐‘™
--------------------- 1
Where, l โ€“ length of the wire and r โ€“ radius of wire.
If n- modulus of rigidity, then Force per unit area on the wire is given by,
F = n ฯ† ------------------------------------------------2
From equation 1 and 2 we have, ๐น =
๐‘›๐‘Ÿ๐œƒ
๐‘™
For the whole perimeter 2ฯ€r, ๐น =
๐‘›๐‘Ÿ๐œƒ
๐‘™
2๐œ‹๐‘Ÿ๐‘‘๐‘ฅ =
2๐œ‹๐‘›๐‘Ÿ2๐œƒ
๐‘™
๐‘‘๐‘ฅ
๐ถ๐‘œ๐‘ข๐‘๐‘™๐‘’ = ๐น๐‘ฅ =
2๐œ‹๐‘›๐‘Ÿ3
๐œƒ
๐‘™
Total twisting couple for angle ๐œƒ,
2๐œ‹๐‘›๐œƒ
๐‘™
โˆซ ๐‘ฅ3
๐‘‘๐‘ฅ
๐‘…
0
where, R โ€“ Radius of wire
Therefore,๐œ๐จ๐ฎ๐ฉ๐ฅ๐ž ๐ฉ๐ž๐ซ ๐ญ๐ฐ๐ข๐ฌ๐ญ, ๐‚ ๐ญ =
๐‚
๐›‰
=
๐…๐’๐‘น๐Ÿ’
๐Ÿ๐’
, also
The time period of oscillation is given by equation ๐‘‡ =
2๐œ‹
๐œ”
and ๐‘‡2
=
4๐œ‹2
๐œ”2 or ๐œ”2
=
4๐œ‹2
๐‘‡2 โˆ’ โˆ’ โˆ’ โˆ’ โˆ’ โˆ’3
Engineering Physics Experiments for BE and B.Tech., Prof. Praveen N. Vaidya, SDMCET Dharwad.
and ฯ‰ = โˆšCt/I = โˆš
๐…๐’๐‘น๐Ÿ’
๐Ÿ๐’
/I or ฯ‰2
=
๐…๐’๐‘น๐Ÿ’
๐Ÿ๐’๐‘ฐ
----------------------------- 4
Where, I โ€“ Moment of Inertia of circular disc is given by, ๐ผ =
1
2
๐‘€๐‘…2
R โ€“ Radius of Disc and M โ€“ Mass of the disc
From 3 and 4 we have,
4๐œ‹2
๐‘‡2
=
๐œ‹๐‘›๐‘…4
2๐‘™๐ผ
, rearranging the term we get, ๐‘› =
8๐œ‹๐ผ
๐‘Ÿ4
ร—
๐‘™
๐‘‡2
Procedure:
๏‚ท Take the suitable length of brass wire and its one end is fixed at the center by means of chuck nut at the
center of circular disc and this set up is suspended by means of a rigid support as shown in figure.
๏‚ท Now rotate the circular disc about the axis of wire through some angle and leave, the disc is set to
oscillate about its mean position.
๏‚ท Note down the time taken to complete 10 oscillations using a stop clock. Now repeat the same
procedure for different length and tabulate the readings.
๏‚ท Determine the time period of oscillation and determine the value of L/T2
every time. Find out the mean
value of L/T2
๏‚ท Measure the mass of the circular disc (M), Radius of the circular disc (R), Radius of the Brass wire
using screw gauge (r).
๏‚ท Determine the Modulus of rigidity of brass wire is given by equation
๐‘› =
8๐œ‹๐ผ
๐‘Ÿ4 ร— ๐‘š๐‘’๐‘Ž๐‘› (
๐‘™
๐‘‡2),
Where I is moment of Inertia of circular disc is given by ๐ผ =
1
2
๐‘€๐‘…2
.
๏‚ท The graph is plotted taking T2
along Y-axis and L โ€“ along X โ€“ axis. Determine the slope.
Therefore the Modulus of rigidity by graphical method is given by
๏‚ท ๐‘› =
8๐œ‹๐ผ
๐‘Ÿ4 ร—
1
๐‘ ๐‘™๐‘œ๐‘๐‘’
Result: Modulus of rigidity of Brass wire is __________________ (By calculation)
Modulus of rigidity of Brass wire is __________________ (By Graph)
Experimental setup:
Observations:
Mass of the circular disc (M)______________ kg.
Radius of the circular disc (R)____________cm = _________m
Radius of the Brass wire (r)______________mm = _________m
Engineering Physics Experiments for BE and B.Tech., Prof. Praveen N. Vaidya, SDMCET Dharwad.
Tabular column:
Tr.
No.
Length
of wire,
L in m
Time taken for 10 oscillations
in seconds
Time
period,
T in sec
T2 L/T2
Trial -1 Trial -2 Trial -3
1 0.15
2 0.2
3 0.25
4 0.3
5 0.35
6 0.4
7 0.45
Calculation:

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torsinal pendulum.docx

  • 1. Engineering Physics Experiments for BE and B.Tech., Prof. Praveen N. Vaidya, SDMCET Dharwad. TORSIONAL PENDULUM Aim: To determine the Rigidity modulus of the given Brass wire by using Torsional pendulum apparatus. Apparatus: Brass wire, Circular disc with chuck nuts, Digital stop clock, Laboratory stand, and meter scale. Principle: The torsional pendulum experiment is based on the principle of application of shearing stress to the wire, hence it can show the shear strain, and therefore the ratio of shearing stress to shearing strain is given the Modulus of rigidity. Theory: A simple pendulum is a system of thread its one end is fixed to a ceiling and other end tied to a mass and let free give periodic oscillations. However, in case of torsional pendulum, one end of thread (normally metallic) tied to ceiling and other end is tied to a mass in the form of disc at its center. If the disc is rotated through an angle โ€˜ฮธโ€™ from mean position, so that the thread also twists and show resistance to rotate, if the disc is released now, the disc starts giving to and fro rotations about its axis as shown in figure. Since the mass is moving very quickly, it overshoots at the equilibrium position and rotates through an angle โ€˜ฮธโ€™ in opposite direction. The restoring force of metallic thread slows the mass down and causes it to rotate the other way back. The restoring force is actually proportional to the rotation angle โ€˜ฮธโ€™ of the disc. During this time wire twists through angle ฯ†, so that l ฯ† = r ฮธ Or or ๐œ‘ = ๐‘Ÿ๐œƒ ๐‘™ --------------------- 1 Where, l โ€“ length of the wire and r โ€“ radius of wire. If n- modulus of rigidity, then Force per unit area on the wire is given by, F = n ฯ† ------------------------------------------------2 From equation 1 and 2 we have, ๐น = ๐‘›๐‘Ÿ๐œƒ ๐‘™ For the whole perimeter 2ฯ€r, ๐น = ๐‘›๐‘Ÿ๐œƒ ๐‘™ 2๐œ‹๐‘Ÿ๐‘‘๐‘ฅ = 2๐œ‹๐‘›๐‘Ÿ2๐œƒ ๐‘™ ๐‘‘๐‘ฅ ๐ถ๐‘œ๐‘ข๐‘๐‘™๐‘’ = ๐น๐‘ฅ = 2๐œ‹๐‘›๐‘Ÿ3 ๐œƒ ๐‘™ Total twisting couple for angle ๐œƒ, 2๐œ‹๐‘›๐œƒ ๐‘™ โˆซ ๐‘ฅ3 ๐‘‘๐‘ฅ ๐‘… 0 where, R โ€“ Radius of wire Therefore,๐œ๐จ๐ฎ๐ฉ๐ฅ๐ž ๐ฉ๐ž๐ซ ๐ญ๐ฐ๐ข๐ฌ๐ญ, ๐‚ ๐ญ = ๐‚ ๐›‰ = ๐…๐’๐‘น๐Ÿ’ ๐Ÿ๐’ , also The time period of oscillation is given by equation ๐‘‡ = 2๐œ‹ ๐œ” and ๐‘‡2 = 4๐œ‹2 ๐œ”2 or ๐œ”2 = 4๐œ‹2 ๐‘‡2 โˆ’ โˆ’ โˆ’ โˆ’ โˆ’ โˆ’3
  • 2. Engineering Physics Experiments for BE and B.Tech., Prof. Praveen N. Vaidya, SDMCET Dharwad. and ฯ‰ = โˆšCt/I = โˆš ๐…๐’๐‘น๐Ÿ’ ๐Ÿ๐’ /I or ฯ‰2 = ๐…๐’๐‘น๐Ÿ’ ๐Ÿ๐’๐‘ฐ ----------------------------- 4 Where, I โ€“ Moment of Inertia of circular disc is given by, ๐ผ = 1 2 ๐‘€๐‘…2 R โ€“ Radius of Disc and M โ€“ Mass of the disc From 3 and 4 we have, 4๐œ‹2 ๐‘‡2 = ๐œ‹๐‘›๐‘…4 2๐‘™๐ผ , rearranging the term we get, ๐‘› = 8๐œ‹๐ผ ๐‘Ÿ4 ร— ๐‘™ ๐‘‡2 Procedure: ๏‚ท Take the suitable length of brass wire and its one end is fixed at the center by means of chuck nut at the center of circular disc and this set up is suspended by means of a rigid support as shown in figure. ๏‚ท Now rotate the circular disc about the axis of wire through some angle and leave, the disc is set to oscillate about its mean position. ๏‚ท Note down the time taken to complete 10 oscillations using a stop clock. Now repeat the same procedure for different length and tabulate the readings. ๏‚ท Determine the time period of oscillation and determine the value of L/T2 every time. Find out the mean value of L/T2 ๏‚ท Measure the mass of the circular disc (M), Radius of the circular disc (R), Radius of the Brass wire using screw gauge (r). ๏‚ท Determine the Modulus of rigidity of brass wire is given by equation ๐‘› = 8๐œ‹๐ผ ๐‘Ÿ4 ร— ๐‘š๐‘’๐‘Ž๐‘› ( ๐‘™ ๐‘‡2), Where I is moment of Inertia of circular disc is given by ๐ผ = 1 2 ๐‘€๐‘…2 . ๏‚ท The graph is plotted taking T2 along Y-axis and L โ€“ along X โ€“ axis. Determine the slope. Therefore the Modulus of rigidity by graphical method is given by ๏‚ท ๐‘› = 8๐œ‹๐ผ ๐‘Ÿ4 ร— 1 ๐‘ ๐‘™๐‘œ๐‘๐‘’ Result: Modulus of rigidity of Brass wire is __________________ (By calculation) Modulus of rigidity of Brass wire is __________________ (By Graph) Experimental setup: Observations: Mass of the circular disc (M)______________ kg. Radius of the circular disc (R)____________cm = _________m Radius of the Brass wire (r)______________mm = _________m
  • 3. Engineering Physics Experiments for BE and B.Tech., Prof. Praveen N. Vaidya, SDMCET Dharwad. Tabular column: Tr. No. Length of wire, L in m Time taken for 10 oscillations in seconds Time period, T in sec T2 L/T2 Trial -1 Trial -2 Trial -3 1 0.15 2 0.2 3 0.25 4 0.3 5 0.35 6 0.4 7 0.45 Calculation: