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J O U R N a L O F P U R E a N D a P P L I ISSN 0256-4637 VOLUME 31 NUMBER 1 January-March, 2009 J o u r n a l o f P u r e a n d A p p l i e d Ultrasound techniques for characterizing liquids 1 I. broad-band spectrometers — UDO KAATZE Ultrasound techniques for characterizing liquids. 13 II. survey of single frequency methods — UDO KAATZE Ultrasonic internal rotary inspection system (IRIS) for heat 24 exchanger and steam generator tubes — A. JOSEPH, GOVIND K. SHARMA and T. JAYAKUMAR Nondestructive characterization of a lyotropic liquid crystalline system 31 — GIRIDHAR MISHRA, R.R. YADAV and S.K. KOR Report - NSU-XVII 36 Dr. T.K. Saksena - A Profile 38 Information for Authors 40 SOC S IET IC Y N O O F S A I N R D T I A L Website : www.ultrasonicsindia.com U Fo 4 u 97 nded 1 A Publication of — Ultrasonics Society of India A Quarterly Publication of Ultrasonics Society of India SOC S IET IC Y N J o u r n a l o f P u r e a n d A p p l i e d O O F S A I N R D T I A L U F ou 74 nded 19 Ultrasonics Society of India No. 1 Volume 31 Jan.-March, 2009 Ultrasonics Society of India established in 1974, is engaged in the promotion of research and diffusion of Chief Editor Dr. S.K. Jain knowledge concerning the field of ultrasonics and e-mail : [email protected] allied areas. Editorial Board Patrons : Dr. A. R. Verma Prof. S.S. Mathur Ex. Professor, Indian Institute of Technology, Dr. V. N. Bindal New Delhi Prof. E.S.R. Gopal Prof. V.P. Bhatnagar Ex. Professor, Delhi College of Engineering, Executive Board : New Delhi President Dr. Krishan Lal Mr. A.D. Prasad Ex. Chief Engineer, IDPL, Noida (U.P.) Vice Presidents Dr. Janardan Singh Dr. Klaus Beissner Physikalisch Technische- Bundesanstalt, Dr. P. Palanichamy Germany General Secretary Mr. S.K. Singhal Dr. J.N. Som Ex. Scientist, National Physical Laboratory, Treasurer Mr. G.K. Kohli New Delhi Publication Secretary Dr. Mukesh Chandra Publication Committee Joint Secretary Mr. N.K. Sharma Members Mr. Subhash Chandra Dr. Sanjay Yadav National Physical Laboratory, New Delhi Dr. J.N. Som Dr. A.K. Nain Dayal Singh College, New Delhi Dr. S.K. Shrivastava Mr. Subhash Chandra Ex. Technical Officer Mr. V.K. Ojha National Physical Laboratory, New Delhi Co-opted Members Dr. Raja Ram Yadav Mr. Gurmukh Singh Scientist F Mr. S.C. Dhawan E.R.T.L. (North), New Delhi SUBSCRIPTION (postage paid) Membership of the Society is open to individuals without distinction of sex, race or nationality and to Single Rs. 550/- US $ 50/- Annual Rs. 2200/- US $ 200/- bodies who subscribe to the aims and objectives of the USI Member Free Society. The membership fee is as follows : ADVERTISEMENT The Journal offers opportunity of wide and effective publicity for the Class of Membership Subscription manufacturers, suppliers of ultrasonic equipment, device and materials (one time) and also for other scientific instruments and components. Tariff is as follows : Honorary Fellow Nil Back Cover Rs. 2500/- US $ 100/- Fellow/Member Rs. 1200/- Inside Cover Rs. 1500/- US $ 75/- Associate Member Rs. 500/- Full Page Rs. 1000/- US $ 50/- (for 5 yrs.) Half Page Rs. 600/- US $ 30/- Corporate Member Rs. 6000/- Fellow/Member (Foreign) US $ 100/- Discount of 20% is admissible for 4 successive insertions. Corporate Member (Foreign) US $ 500/- Membership forms and the relevant information can The submission of papers and all other correspondence regarding the be downloaded from the website or obtained from : Journal may please be addressed to : Publication Secretary The General Secretary Journal of Pure and Applied Ultrasonics Ultrasonics Society of India C/o Ultrasonics Society of India National Physical Laboratory National Physical Laboratory Dr. K. S. Krishnan Marg Dr. K. S. Krishnan Marg New Delhi-110012 New Delhi-110012 e-mail : [email protected] J. Pure Appl. Ultrason. 31 (2009) pp. 1-12 Ultrasound techniques for characterizing liquids I. broad-band spectrometers† UDO KAATZE Drittes Physikalisches Institut, Georg-August-Universität, Friedrich-Hund-Platz 1, 37077 Göttingen, Germany e-mail : [email protected] This tutorial gives a short introduction into the broad-band ultrasonic spectroscopy of liquids. The fundamentals of acoustical methods are summarized. Preference is given to methods using continuous waves and pulse modulated signals. Related techniques, such as time-domain methods with step-like excitation of the sample and with optical monitoring of acoustical waves (Brillouin scattering), are briefly mentioned, too. Constructions of some types of sonic cells for liquids and electronic set-ups for spectral measurements are presented in detail. The merits and limitations of different techniques of measurements, covering the frequency range from almost 10 kHz up to nearly 10 GHz, are discussed. Together with applications in the relaxation properties of liquids, examples of broadband ultrasonic spectra are shown. Key words : Ultrasonic spectroscopy, liquids, relaxations, acoustical absorption coefficient, sound velocity INTRODUCTION The retarded energy transfer between different molecular states of a liquid results in a phase Acoustical signals couple to liquids via lag between pressure and density of a harmonic fundamental parameters, such as the density, acoustic wave. Therefore, acoustic energy is viscosity, and heat capacity1-11. By utilizing these absorbed and dissipated as heat. According to parameters acoustical measurements probe the the fluctuation - dissipation theorem and, by native systems; labels or markers, as required by analogy with the Kramers - Kronig relations12,13, many other measurement techniques for liquids, a characteristic velocity dispersion dc/dν > 0 is are not necessary. Variations in the relevant related with the absorption (c is the sound velocity liquid parameters may result from variations of the liquid). In a relaxing system the relative in the thermodynamic parameters, for example dispersion step [c(ν→0)-c(ν→∞)]/c(ν→∞) is small from changes in the hydrodynamic pressure, the and frequently does not exceed the experimental temperature, or the pH. Variations in the sample property following thereby are often investigated by single-frequency methods which will be the focus of part II of this review. Density, viscosity, and heat capacity of a liquid may also vary with the frequency ν of the sonic field. Such variations happen when an energy barrier exists that prevents molecules, ions, or mesoscopic structures of a liquid from instantaneously following the external field. Fig.1. Sound velocity spectrum of a 0.4 mol/l solution 14 of zinc chloride (ZnCl2) in water at 25°C. The †Invited talk presented at NSU-XVII, B.H.U., Varanasi, line shows the dispersion as calculated from the Dec. 4-6, 2008. J. Pure Appl. Ultrason. Vol. 31 No. 1 (2009) associated absorption spectra 1 errors. Fig. 1 displays already an extraordinarily large dispersion for aqueous systems. Because of the small dispersion amplitude of most liquid relaxations only a comparatively few broad- band sound velocity spectra exist presently. Outstanding exceptions are given, for instance 15 and 16. Because of the typically small dispersion, this part of the review is mainly restricted to ultrasonic absorption measurements. If small effects of thermal conductivity, which play a noticeable role only in liquid metals, are neglected, the laws of conservation of mass and momentum yield the following relation for the complex propagation constant γ =α+iβ of a 1 sinusoidal acoustic wave within a liquid Fig.2. Ultrasonic absorption spectra of a 0.5 mol/l solution of copper chloride (CuCl2) in water at 25°C14 Experimental total absorption-per-wavelength data are shown by points, the asymptotic high-frequency background absorption is represented by the dashed line, and the excess absorption-per-wavelength is (1) indicated by circles. The full line is the graph of a Debye-type relaxation term eq. 8 with the following 2 Here i =-1, α is the absorption coefficient, β = 2π/γ value for the parameters: A = 7. 6·10-3, τ = 0.35 ns where γ = c/ν is the wavelength, ω = 2πν is the angular frequency, ρ is the density, (6) (2) can be separated into two parts. Here is the adiabatic compressibility of the liquid, and ηs and ην are the shear and volume viscosity, respectively. The latter is related to the curl-free (7) part of the acoustic field. At small frequencies -1 is independent of ν if the compressibility does (ω«[κs(4ηs/3+ην] ) follows for the absorption along a wavelength not depend on ν. It is obvious from eq.(1) that a frequency dependent shear viscosity or volume viscosity leads also to a frequency dependent β and thus a frequency dependent cs. As, however, (3) briefly discussed above, the dispersion in the sound velocity of liquids is normally small. Strictly, κS with η and η referring to very low frequencies. s0 ν0 must be replaced by κS∞ in eq. (7). Because of molecular interactions, indicated by the internal energy barriers mentioned before, both Normally, in liquid spectroscopy we are the shear viscosity and the volume viscosity may interested in the excess absorption-per-wavelength be subject to relaxation and may thus depend on (αλ)exc(ν) only. Nevertheless the asymptotic high- frequency. If we write frequency term Bν in eq. (6) acts a considerable influence on the measurements. Due to its frequency ν (4) dependence, proportional to , it dominates the total absorption-per-wavelength αλ at high frequencies and and restricts measurements of liquids to frequencies below some GHz. An illustrative example, in which (αλ)exc ≈ 0.1·(αλ) only at 1 GHz, is given in Fig. 2. (5) It is the asymptotic high-frequency ("background") term Bν which necessitates different methods of with η = η (ν→∞) and η = η (ν→∞) denoting s∞ s ν∞ ν measurements at low and high frequencies.
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