Test sur les ondes mécaniques

Question

  • What is the definition of the phase velocity of a wave phenomenon ?

  • Give the definition of the group velocity of a wave phenomenon.

Solution

  • Phase velocity : \(v_{\varphi}=\frac {\omega}{k}\)

  • Group velocity : \(v_{g}=\frac {d\omega}{dk}\)

It was assumed here that \(k\) was real (no absorption).

Question

Provide part of the acoustic approximation.

Solution

The acoustic approximation is to consider that the magnitudes \(\vec v\), \(\mu\) (variation of density around the equilibrium value) andt \(p\) (change in pressure around the equilibrium value) are infinitesimal of the same order as their derivatives time and space.

In particular, the calculations will be made to order \(1\) in this infinitely small.

Magnitude :

Overpressure likely to be detected by the ear typically range from \(100 \;Pa\) (his painfull) to \(10^{-5}\; Pa\) (hearing threshold), covering \(7\) decades.

Question

Defining "acoustic Poynting vector".

Solution

The "Poynting vector" acoustics :

\(\vec \Pi = p\vec v\)

The conservation equation of energy of a sound wave is written :

\(\frac {\partial}{\partial t}(\frac{1}{2}\mu_0 v^2 + \frac{1}{2}\chi_Sp^2)=-div(\vec \Pi)\)

Question

Define the acoustic impedance.

Solution

That is the pressure \(p\), \(v\) the velocity of fluid particles and the volume flow rate\(D_v\).

We can define the acoustic impedance in two different ways : (\(S\) is the cross section of the studied acoustic pipe)

\(z_a=\frac {p}{v}\;\;\;\;\;or\;\;\;\;Z_a=\frac {p}{D_v}\)

We note that :

\(Z_a=\frac{z_a}{S}\)

Question

Define the sound intensity in decibels (\(dB\)).

Solution

We define the sound intensity (or acoustic) in decibels (\(dB\)) :

\({I_{dB}} = 10\log \left( {\frac{{\left\langle {\Pi (x,t)} \right\rangle }}{{{\Pi _{ref}}}}} \right)\;\;\;\;\;\;\;\left( {with {\kern 1pt} \;{\Pi _{ref}} = {{10}^{ - 12}}\;W.{m^{ - 2}}} \right)\)

Question

  • What is the expression of the speed of sound in air ?

  • What is its value at \(20 °C\) under \(1\; bar\) ?

Solution

  • The speed of sound in air is :

    \(c = \frac{1}{{\sqrt {{\mu _0}{\chi _S}} }} = \sqrt {\frac{{\gamma R{T_0}}}{M}}\)

  • At \( 20°C\) and \(1\;bar\) : \(c=340\;m.s^{-1}\)

Question

Why do we say that a wave is propagated even more harm than the nedium is softer and more inert ?

Solution

  • The sound propagation speed in the solids is :

    \(c = \sqrt {\frac{{k{d^2}}}{m}}\)

  • The speed of propagation of a wave in a string is :

    \(c=\sqrt {\frac {T}{\mu}}\)

We see that \(c\) is even smaller than the medium is "soft" (\(kd^2\) or \(T\) "weak") and inert (\(m\) and \(\mu\) "large").

Question

What is called the approximation of continuous medium ?

Solution

\(u_n(t)\) are the vibratory displacement at discrete points \(x_n\), small compared to the wavelength of the wave.

The approximation of continuous medium is to construct a continuous function \(u\) such that :

\(u(x_n,t)=u_n(t)\)

Question

Is a beam of rectangular cross section steel, height \( 10\; cm\), width \(5\;cm\) and \(10\;cm\) length, fitted at both ends.

Subjecting this beam to the rise of a temperature of \(50 \;K\).

The modulus of elasticity of the steel is \(200 \;GPa\) and its coefficient of expansion. \(12.10^{-6}\;K^{-1}\).

What is the compressive stress in the beam ?

Solution

The constraint (It's a pressure) is given by :

\(P=Y\frac{\Delta \ell}{\ell}\)

Where \(Y\) is the Young's modulus.

The coefficient of expansion is used to determine the relative change in length :

\(\alpha=\frac{1}{\ell}\frac{\Delta \ell}{\Delta T}\)

We deduce :

\(P=Y\alpha \Delta T=120\;MPa\)