دورية أكاديمية

Sound propagation in ionized gases and electroacoustic effect.

التفاصيل البيبلوغرافية
العنوان: Sound propagation in ionized gases and electroacoustic effect.
المؤلفون: Bhatnagar, V.P., Bhatnagar, D.P., Saxena, A.P.
المصدر: International Journal of Electronics. Aug72, Vol. 33 Issue 2, p193. 8p.
مصطلحات موضوعية: RADIO wave propagation, IONIZED gases, ELECTROACOUSTICS
مستخلص: Using hydrodynamical methods, the propagation of pressure waves in a non-isothermal fully ionized gas has been considered for a situation where collision between various particles cannot be ignored and the following pressure equation has been obtained: p/t + p/t - (V[SUB 3[SUP2]] + V[SUB l[SUP2]]) /tp + [SUB E[SUP2]] p/t - V[SUB l[SUP2]] /t p -[SUB e[SUP2]] V[SUB l[SUP2]]p + V[SUB i[SUP2]]V[SUB e[SUP2]]p = 0. where V[SUB i[SUP2]], V[SUB e[SUP2]] and V[SUB l[SUP2]] represent respectively kT/m, kT/m and k(T + T)/m and other symbols have their usual meaning.
This gives the following dispersion relation for a sinusoidal sound wave V[SUB i[SUP2]]V[SUB e[SUP2]]k - [ V[SUB e[SUP2]] - ([SUB e[SUP2]] - i) V[SUB l[SUP2]] ]k + [ - ([SUB e[SUP2]] - i)] = 0.
The phase velocity of propagation and attenuation of the sound waves have been discussed in the low frequency and high frequency region and it has been shown that low frequency sound waves travel with a velocity V, while high frequency sound waves are carried by ions and electrons with velocities V and V respectively.
Because of the difference in the masses of the ions and electrons, an electrostatic field of the same frequency as that of the sound is created during the propagation of sound waves. This field is given by: E = e/l/kTV/(V[SUB l[SUP2]]/V - 1) p and it is appreciable only at high frequencies where V < V. [ABSTRACT FROM AUTHOR]
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قاعدة البيانات: Business Source Index
الوصف
تدمد:00207217
DOI:10.1080/00207217208938355