HAL Id: jpa-00219546
https://hal.archives-ouvertes.fr/jpa-00219546
Submitted on 1 Jan 1979
HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.
L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.
NONLINEAR SOUND INTERACTION IN SUPERFLUID SOLUTIONS
R. Khokhlov, N. Pushkina
To cite this version:
R. Khokhlov, N. Pushkina. NONLINEAR SOUND INTERACTION IN SUPERFLUID SOLUTIONS.
Journal de Physique Colloques, 1979, 40 (C8), pp.C8-239-C8-240. �10.1051/jphyscol:1979841�. �jpa-
00219546�
N O N L I N E A R SOUND INTERACTION IN S U P E R F L U I D S O L U T I O N S R.V. Khokhlov, N.I. Pushkina
Moscow State University
Abstract - We present a thoretical analysis of nonlinear stimulated Raman-type of first sound by temperature waves in 3He - ''He superflind solutions. We show that the sound attenuation in 3He - "He solutions is lower that in pure ''He. The stimulated scattering of first sound by second sound in
3He - "He solutions could be the subject of investigations in experimental nonlinear acoustics.
In the report we present a theoretical analysis of nonlinar stimulated Raman-Type scattering of first sound by temperature waves in superfluid solutions 3 4 He - He /1,2/. Nonlinear Raman-type interactions of first sound with second sound (temperature waves) in superfluids were considered in Ref /3,4/
(in case of pure He and in Ref /5/ in case of He in anisotropic superfluid A-phase.
In solving the problem we start from the two- fluid-model hydrodynamic equations for superfluid solutions /&/. It is convenient to use normal coor- dinates Q, „, chosen in the form :
where
Here P is the pressure, T is the temperature, C is the concentration of He atoms in superfluid He, p , p are the normal and superfluid densities, p is the density, S is the entropy, IL and U„ are the first - and second- second velocities,
We assume plane-wave solutions of the equations for the incident and the scattered sound fields of
the form :
The amplitudes Q , „ are slowly varying functions
0,1,'-
of distance, Q is the pump first sound, Q. is the scattered first-sound wave and Q„ is the second- second wave.
The conditions oo = to^ + GO2, t = It. + t- are assumed to be fulfilled. We obtain the follo- wing equations for the amplitudes Q, 2 :
Q = const.
otj, a2 are the amplitude damping coefficients, JOURNAL DE PHYSIQUE Colloque C8, supplément au n° 11, tome 40, novembre 1979, page C8-239
Résumé.- Nous présentons une analyse théorique de la diffusion non linéaire de type Raman- stimulé du premier son par les ondes thermiques dans des solutions superfluides 3He - "He. Nous montrons que l'atténuation des ondes sonores dans les solutions 3He - ''He est plus faible que dans He pur. La diffusion stimulée du 1er son par le second son dans les solutions 3He - ""He devrait faire l'objet de développements expérimentaux en acoustique non linéaire.
Article published online by EDP Sciences and available at
Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:1979841
JOURNAL DE PHYSIQUE
I n d e r i v i n g the equations ( 1 ) we used t h e i n e q u a l i - t y
3
<< @ which i s t r u e i f t h e c o n c e n t r a t i o n C i s n o t t o o small. I n t h i s case t h e maxing o f pres- sure and temperature i n a mode i s due mainly t o t h e3 4
presence o f He i n s u p e r f l u i d He and n o t t o tem- p e r a t u r e expansion.
The equation ( 1 ) y i e l d t h e f o l l o w i n g expres- sion f o r t h e t h r e s h o l d i n t e n s i t y o f t h e pump sound a t which t h e s t i m u l a t e d s c a t t e r i n g becomes p o s s i b l e
The t h r e s h o l d i n t e n s i t y ( 2 ) i s s i g n i f i c a n t l y lower than t h a t i n pure 'he f o r t i l e two rezsons ;
i n case o f pure 4 ~ e i n debends on t h e q u a n t i t y
$
/2/ which i s lower than t h e q u a n t i t y @ e n t e r i n g the expression ( 2 ) ; besides, t h e sound a t t e n u a t i o n i n 3 ~ e-
4 He s o l u t i o n s i s lower than t h a t i n pure 4 ~ e . Thus t h e s t i m u l a t e d s c a t t e r i n g o f f i r s t sound by second sound i n 3 ~ e-
4 He s o l u t i o n s c o u l d be t h e s u b j e c t o f i n v e s t i g a t i o n s i n experimental n o n l i n e a r acoustics.References
/1/ N.I. Pushkina, R.V. Khokhlov, Proc. o f t h e I X Symposium on Acoustics, Moscow, June, 1977
/2/ V. Lebedev, JETP
3,
2224, 1977./3/ N . I . Pushkina, R.V. Khokhlov Pisma JETP 19, 672, 1974.
-
/4/ V . I . Pokrovsky, I . M . Khalatnikov, JETP - 71, 1974, 1976.
/5/ N . I . Pushkina, R.V. Khoklov, Pisma JETP
3,
N24, 1977.
/6/ i.M. Khalatnikov, "Theory o f S u p e r f l u i d i t y "
"Nauka", M., 1971.