Velocity of Longitudinal Wave Assignment Help

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Velocity of sound in any elastic medium

            It is given by   1864_Velocity of Longitudinal Wave.png

(i) In solids v = √(Υ/ρ) ; where Y ¾ Young's modulus of elasticity.

(ii) In a liquid and gaseous medium v = √(B/ρ) ; where B ¾ Bulk modulus of elasticity of liquid or gaseous medium.

(iii) As solids are most elastic while gases least EBksi > Enzo > EkSI i.e. . So the velocity of sound is maximum in solids and lowest in gases, hence vBksi > vnzo > vkSI

(iv) The speed of sound in  case of extended solid (crust of the earth) ; 428_Velocity of Longitudinal Wave1.png

B ¾ Bulk modulus ; η ¾ Modulus of rigidity; ρ ¾ Density.

 

Newton's Formula: He assumed that when sound propagates through air temperature remains fixed. i.e. the phenomena is isothermal.

            1484_Velocity of Longitudinal Wave2.png         k = Eθ = P [Eθ =Isothermal elasticity; P = Atmospheric pressure]

For air at N.T.P.  N/m2 and ρ ¾ 1.29 kg/m3.

           445_Velocity of Longitudinal Wave3.png = 279 m/s

However the experimental number of sound in air is 332 m/sec which is greater than that given by Newton's formula.

Laplace correction: He modified Newton's formula assuming that propagation of sound in gaseous medium is adiabatic process. For adiabatic method

                           2287_Velocity of Longitudinal Wave4.png   k = EΦ = γP  EΦ¾ Adiabatic elasticity γ =  Cp/Cv  = 1.41

For air,       212_Velocity of Longitudinal Wave5.png

 

Relation between velocity of sound and root mean square velocity : If sound travel in a gaseous medium then vsound=√(γRT)/M and r.m.s. velocity of gas vrms=√(3RT)/M

So vrms /vsound = √(3/γ)   or    vsound= [γ/3]1/2vrms          

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