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Transverse waves

Storyboard

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Mechanisms

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Concept

Mechanisms

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Transverse wave

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A variant to the longitudinal wave, in which the deformation is in the same direction of propagation, is when the deformation is perpendicular to the direction of propagation:

This type of wave is called a transverse wave. Since there are two axes perpendicular to the direction of propagation, there will be two transverse modes.

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Transverse wave in a solid

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In the case of a solid, the transverse wave can be described as the lateral displacement of the atoms:

It should be noted that it is not a simple movement orthogonal to the translation, there is also a small displacement in the direction of propagation caused by the stresses of the 3D structure.

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Model

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Parameters

Symbol
Text
Variable
Value
Units
Calculate
MKS Value
MKS Units
E
E
Modulus of Elasticity
Pa
\nu
nu
Poisson coefficient
-
G
G
Shear module
Pa
c_t
c_t
Velocidad de la onda en el medio transmitido
m/s

Variables

Symbol
Text
Variable
Value
Units
Calculate
MKS Value
MKS Units
\rho
rho
Mean density
kg/m^3
\tau
tau
Torsion
Pa
\gamma
gamma
Twist angle
rad

Calculations


First, select the equation: to , then, select the variable: to
c_t ^2 = G / rho E =2* G *(1+ nu ) tau = G * gamma rhoEnuGtaugammac_t

Calculations

Symbol
Equation
Solved
Translated

Calculations

Symbol
Equation
Solved
Translated

Variable Given Calculate Target : Equation To be used
c_t ^2 = G / rho E =2* G *(1+ nu ) tau = G * gamma rhoEnuGtaugammac_t




Equations

#
Equation

c_t ^2 = \displaystyle\frac{ G }{ \rho }

c_t ^2 = G / rho


E =2 G (1+ \nu )

E =2* G *(1+ nu )


\tau = G \gamma

tau = G * gamma

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Hooke's Law for the Case Shear

Equation

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In the case of shear, the deformation is not associated with expanding or compressing, but with laterally offsetting the faces of a cube. The shear is therefore described by the angle \gamma with which it is possible to rotate the face perpendicular to the displaced surfaces. In analogy to Hook's law for compression and expansion, we have the relationship between torsion \tau and angle \gamma:

\tau = G \gamma

G
Shear module
Pa
5364
\tau
Torsion
Pa
5366
\gamma
Twist angle
rad
5367
tau = G * gamma E =2* G *(1+ nu ) c_t ^2 = G / rho rhoEnuGtaugammac_t

where G is the so-called shear modulus.

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Shear Modulus

Equation

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The shear modulus G is related to the modulus of elasticity E and Poisson's ratio
u
by

E =2 G (1+ \nu )

E
Modulus of Elasticity
Pa
5357
\nu
Poisson coefficient
-
5365
G
Shear module
Pa
5364
tau = G * gamma E =2* G *(1+ nu ) c_t ^2 = G / rho rhoEnuGtaugammac_t

where G is the so-called shear modulus.

ID:(3772, 0)



Transverse speed of sound

Equation

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If we compare the relationship of stress and strain

\sigma = E \epsilon



and the speed of sound (longitudinal)

c ^2 = \displaystyle\frac{ E }{ \rho }



with shear stress

\tau = G \gamma



so that a transverse speed of sound can be defined

c_t ^2 = \displaystyle\frac{ G }{ \rho }

\rho
Mean density
kg/m^3
5088
G
Shear module
Pa
5364
c_t
Velocidad de la onda en el medio transmitido
m/s
9657
tau = G * gamma E =2* G *(1+ nu ) c_t ^2 = G / rho rhoEnuGtaugammac_t

ID:(14181, 0)