Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

13
Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU

Transcript of Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

Page 1: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

Shrieking Rod

Prof. Chih-Ta Chia

Dept. of Physics NTNU

Page 2: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

Problem # 13

Shrieking rodA metal rod is held between two fingers

and hit. Investigate how the sound produced depends on the position of holding and hitting the rod?  

Page 3: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

Vibration in rod? How did you create vibrations in the rod? Three type of vibrations are created simply by hitting

the rod: Longitudinal, torsional and flexural vibrations. Longitudinal and Flexural vibrations are most likely to

last longer, but not the torsional vibrations. What are the resonance conditions for these three

vibrations? What are the speeds of these three vibrations that

travel in the rod. How to determine the wave velocity?

Page 4: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

Vibration of Rod?

What is the damping effect on the longitudinal and vibrations? Hitting position dependence? Time dependence?

Longitudinal wave damping and flexural vibration damping? Which one is damped fast?

Page 5: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

Cylindrical Rod : Longitudinal and Torsional wave

E

Cl Longitudinal wave speedE: Young’s Modulus

Torsional wave speed: Shear Modulus

tC

Passion Ratio : 12

1 2

t

l

f

f

Page 6: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

Young’s Modulus

A

FS

Stress: S

Longitudinal Strain: Stl

lSt

Young’s Modulus: EtS

SY

Page 7: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

L

LStrain

A

FStress

Hook’s Law

L

LY

A

F

Stress is proportional to Strain.

Stress, Strain and Hook’s Law

Page 8: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

Shear Modulus The shear modulus is the elastic modulus we use for the deformation which takes place when a force is applied parallel to one face of the object while the opposite face is held fixed by another equal force.

L

L

A

F

Shear Modulus:

LxA

F

StrainShear

StressShear

Page 9: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

Resonance : When Clamped in the Middle

L

Cnf l

nl 212

L

Cnf t

nt 212

3, 2, 1, 0,n

Page 10: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

Speed of wave in Rod

Page 11: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.

Flexural VibrationsEquation of Motion : (Length L and radius a)

2

2

4

422

t

y

x

ycl

cl is the velocity of longitudinal waves in an infinitely long bar.

The radius of gyration is defined as above. For the circular rod, is half the bar’s radius. As for the square rod, is D/√12.

dAyA

22 1

Y

cl 2

Page 12: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.
Page 13: Shrieking Rod Prof. Chih-Ta Chia Dept. of Physics NTNU.