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DOMNIKOV, L. The effect of ultrasonics on the phosphating process. Metal Finishing, 65, No. 2, p. 55 (1967). The use of ultrasonics in phosphating of ferrous metals pro- duces superior coating and obviates the necessity for pre- liminary sand blasting. The phosphate coatings produced in an ultrasonic bath at 16-22kHz for 40-60 min are less porous, have higher corrosion resistance, greater dielectric strength and a finer finish. Best results were obtained in solutions of 20-25g/lit phosphoric acid, 38-42g/lit zinc monophosphate, 56-62g/lit zinc nitrate at 70°C. (2 figures, 2 tables, 1 refer- ence) (Ultrasonics 1967, abstract 651) GARG, A. G. and TAYLOR, A. R. Effects of ultrasound--with special reference to the nervous system. Biomedical Engineering, 2, No. 5, p. 222 (1967). A review of an investigation to determine the effects of ultrasonics on the nervous system. Thermal, mechanical, chemical and electrochemical effects are summarized. Reference is made to biological changes and their thera- peutic applications, particularly on the central nervous sys- tems. (49 references) (Ultrasonics 1967, abstract 652) HEFFAN, H. et al Quality evaluation of missile structure spot welded joints. Materials Evaluation, 25, No. 1, p. 15 (1967). This research programme followed a number of structural failures in missiles during flight. A significant number of spot welds were found to be substandard to an extent that ranged from undersized nuggets to complete unbonds. In conjunction with radiographic and metallographic analysis new ultrasonic transducers have been developed, and special standards have been devised that are thought to give complete reliability in the grading of spot welds. (6 figures, 1 table) (Ultrasonics 1967, abstract 653) JACOBS, J. E. Performance of the ultrasonic microscope. Materials Evaluation, 25, No. 3, p. 41 (1967). The resolution of an ultrasonic camera is set by the thick- ness of the piezoelectric crystal and by the acoustic optics. Maximum resolution is obtained when the incident sound pattern does not deviate more than 2 ° from the beam axis. With present frequencies (up to approximately 15MHz) the smallest resolvable object is approximately 0.34mm. It is thought that with the advent of the depletion layer transducers frequencies of up to 3GHz will be able to be used but then the resolution will be determined by the electron beam diameter which is at present approximately 20~m. (8 figures, 6 refer- ences) (Ultrasonics 1967, abstract 654) KORDINA, K. et al Ultrasonic measurements on reinforced gravel-aggregate concrete. Materialprufung, 9, No. 3, p. 81 (1967). The usefulness of ultrasonic pulse velocity measuring methods in the building industry is investigated. The velo- city of ultrasonics in concrete depends on its composition, age, porosity and loading, the method of reinforcement, microcracks and other factors and by eliminating some of these variables the effects of others can be determined. Con- sistent and reproducible results have been derived for all the 27 different concretes investigated. Method of testing and the equipment used are described and it is concluded that this technique is suitable for on-site quality control applica- tions. (5 figures, 1 table, 1 reference) (Ultrasonics 1967, abstract 656) KORPEL, A. Visualization of the cross-echoes of a sound beam by Bragg diffraction of light. Applied Physics Letters, 9, No. 12, p. 425 (1966). A novel method of imaging the phase and amplitude of the cross-section of an ultrasonic beam is reported. Because the phase is retained in the acousto-optical conversion process an image of any chosen cross-section of the beam can be obtained by optical manipulations and reproduced on a screen or a photographic plate. The apparatus consists of a laser source, 22MHz ultrasound generator in a water-filled cell at right angles to the laser beam and a collection of cylindrical lenses. The ultrasound field behind various objects shows that at this frequency the smallest resolvable detail is about 0.8mm but at higher frequencies this technique might find application in sound microscopy. (4 figures, 4 references) (Ultrasonics 1967, abstract 657) IRVING, R. R. Are all weld defects harmful? Iron Age, 199, No. 14, p. 67, (1967). A comparison of the advantages and limitations in ultrasonic, radiographic, magnetic and penetrant techniques of non- destructive testing. Application to a given situation, ease of operation, relative cost and permanent records are also exami- ned. Emphasis is placed on the interpretation of the signifi- cance of flaws in ERW pipes destined for the power genera- tion industry. The author concludes that the multi-method approach is still the best. (8 figures, 3 tables (Ultrasonics 1967, abstract 658) LITTLEFORD, G. E. Welding electronic devices by ultrasonics. Industrial Electronics, 5, No. 3, p. 123 (1967). Ultrasonic welding of microelectronic devices is more effi- cient and precise than any other known method. Ultrasonics can weld many metal and alloy combinations in thicknesses of 100k upwards. A true solid state metallurgical bond is obtained without the application of heat or fluxes and the bonds are comparable in strength to the parent material. A number of examples are given that have found application in mass production. (2 tables, 3 figures) (Ultrasonics 1967, abstract 659) KELPIN, H. and WEIS, O. Sound energy receivers for the measurement of attenua- tion above 300MHz. Acustica, 18, No. 2, p. 105 (1967). To overcome the difficulties of measurements of high fre- quency ultrasound, temperature resistive elements were in- vestigated. These are thermocouple elements, the miniature NTC resistors and thin (BaSr)TiO 3 discs as PTC-resistors. These devices register the total energy dissipation and are not dependent on the parallelism, the surface finish or the homogeneity of the transducers and can be used in the giga- hertz frequency range. Results of some comparative experi- ments at approximately 312MHz in the 21°-42°C temperature range are given. (6 figures, 1 table, 8 references) (Ultra- sonics 1967, abstract 655) 194 ULTRASONICS July 1967 LOVELACE, J. F. Mathematical analysis of the effects of diameter and wall thickness on ultrasonic inspection of pipe butt welds. Materials Evaluation. Results of an investigation conducted to determine the feasi- bility of ultrasonic detection of internal defects in pipe butt welds are reported. The sizes and materials of interest were those used for critical circuits in the construction of sub- marines. A sensitivity standard was developed which uses a calibrated attenuator. It is thought that the reliability of ultrasonic testing is comparable to radiography. Some anoma- lous reflections from discontinuities in pipes below 0.5in (1.27cm) wall thickness have been observed and are analyzed theoretically. (8 figures, 1 table, 6 references) (Ultrasonics 1967, abstract 660)

Mathematical analysis of the effects of diameter and wall thickness on ultrasonic inspection of pipe butt welds

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Page 1: Mathematical analysis of the effects of diameter and wall thickness on ultrasonic inspection of pipe butt welds

DOMNIKOV, L. The effect of u l t r a s o n i c s on the phosphating p r o c e s s . Metal Finishing, 65, No. 2, p. 55 (1967).

The use of u l t r a s o n i c s in phosphat ing of f e r r o u s m e t a l s p ro - duces s u p e r i o r coat ing and obvia tes the neces s i t y for p r e - l im ina ry sand blast ing. The phosphate coat ings produced in an u l t r a son ic bath at 16-22kHz for 40-60 min a r e l e s s porous, have h igher c o r r o s i o n r e s i s t a n c e , g r e a t e r d i e l ec t r i c s t r eng th and a f i ne r f inish. Best r e s u l t s we re obta ined in so lu t ions of 20 -25g / l i t phosphor ic acid, 38 -42g / l i t zinc monophosphate , 56 -62g / l i t zinc n i t r a t e at 70°C. (2 f igures , 2 tables , 1 r e f e r - ence) (Ul t r a son ics 1967, a b s t r a c t 651)

GARG, A. G. and TAYLOR, A. R. Effec ts of u l t rasound--wi th spec ia l r e f e r e n c e to the ne rvous sys t em. Biomedica l Engineer ing , 2, No. 5, p. 222 (1967).

A review of an investigation to determine the effects of ultrasonics on the nervous system. Thermal, mechanical, chemical and electrochemical effects are summarized. Refe rence is made to biological changes and t h e i r t h e r a - peutic appl icat ions, p a r t i c u l a r l y on the cen t r a l ne rvous s y s - t ems . (49 r e f e r e n c e s ) (U l t r a son ic s 1967, a b s t r a c t 652)

HEFFAN, H. et al Quali ty evaluat ion of m i s s i l e s t r u c t u r e spot welded joints . M a t e r i a l s Evaluat ion, 25, No. 1, p. 15 (1967).

Th i s r e s e a r c h p r o g r a m m e followed a n u m b e r of s t r u c t u r a l f a i l u re s in m i s s i l e s dur ing flight. A s igni f icant n u m b e r of spot welds were found to be s u b s t a n d a r d to an extent that ranged f rom u n d e r s i z e d nuggets to comple te unbonds. In conjunct ion with r ad iograph ic and me ta l log raph ic ana ly s i s new u l t r a son ic t r a n s d u c e r s have been developed, and spec ia l s t anda rds have been devised that a r e thought to give comple te re l i ab i l i ty in the grad ing of spot welds. (6 f igures , 1 table) (Ul t r a son ics 1967, a b s t r a c t 653)

JACOBS, J. E. P e r f o r m a n c e of the u l t r a s o n i c m i c r o s cope . M a t e r i a l s Evaluation, 25, No. 3, p. 41 (1967).

The reso lu t ion of an u l t r a son ic c a m e r a is se t by the th ick- ness of the p i ezoe lec t r i c c r y s t a l and by the acous t ic opt ics . Maximum reso lu t ion is obtained when the incident sound pa t t e rn does not devia te m o r e than 2 ° f rom the beam axis . With p r e s e n t f r equenc i e s (up to approx imate ly 15MHz) the s m a l l e s t r e so lvab le object is approx imate ly 0 .34mm. It is thought that with the advent of the deplet ion l aye r t r a n s d u c e r s f r equenc ie s of up to 3GHz will be able to be used but then the reso lu t ion will be d e t e r m i n e d by the e l ec t ron beam d i a m e t e r which is at p r e s e n t approx imate ly 20~m. (8 f igures , 6 r e f e r - ences) (Ul t rason ics 1967, a b s t r a c t 654)

KORDINA, K. et a l Ultrasonic m e a s u r e m e n t s on r e i n f o r c e d g r a v e l - a g g r e g a t e concre te . Mater ia lp rufung , 9, No. 3, p. 81 (1967).

The u se fu lnes s of u l t r a son ic pulse ve loc i ty m e a s u r i n g methods in the bui lding indus t ry is inves t iga ted . The ve lo - ci ty of u l t r a s o n i c s in conc re t e depends on i t s composi t ion, age, po ros i ty and loading, the method of r e i n fo r cemen t , m i c r o c r a c k s and o ther f a c t o r s and by e l imina t ing some of these v a r i a b l e s the effects of o t h e r s can be de t e rmined . Con- s i s t en t and r ep roduc ib le r e s u l t s have been de r ived for a l l the 27 d i f fe rent c o n c r e t e s inves t iga ted . Method of t e s t ing and the equipment used a r e d e s c r i b e d and it is concluded that th is technique is su i tab le for o n - s i t e quali ty cont ro l app l ica - t ions. (5 f igures , 1 table, 1 r e f e r ence ) (Ul t r a son ic s 1967, a b s t r a c t 656)

KORPEL, A. Visua l i za t ion of the c r o s s - e c h o e s of a sound beam by Bragg d i f f rac t ion of l ight . Applied P h y s i c s Le t t e r s , 9, No. 12, p. 425 (1966).

A novel method of imaging the phase and ampl i tude of the c r o s s - s e c t i o n of an u l t r a s o n i c beam is r epor t ed . Because the phase is r e t a ined in the acous to -op t i ca l conve r s ion p r o c e s s an image of any chosen c r o s s - s e c t i o n of the beam can be obtained by opt ical manipu la t ions and r ep roduced on a s c r e e n or a photographic plate. The appa ra tu s c o n s i s t s of a l a s e r source , 22MHz u l t r a sound g e n e r a t o r in a wa t e r - f i l l ed cel l a t r igh t angles to the l a s e r beam and a col lec t ion of cy l indr ica l l enses . The u l t r a sound f ie ld behind va r ious objec ts shows that at th i s f requency the s m a l l e s t r e s o l v a b l e deta i l i s about 0 . 8 m m but at h igher f r equenc i e s th is technique might f ind appl ica t ion in sound microscopy . (4 f igures , 4 r e f e r e n c e s ) (Ul t r a son ics 1967, a b s t r a c t 657)

IRVING, R. R. Are a l l weld defec ts h a r m f u l ? I ron Age, 199, No. 14, p. 67, (1967).

A c o m p a r i s o n of the advantages and l imi ta t ions in u l t r ason ic , r ad iograph ic , magnet ic and pene t r an t t echniques of non- de s t ruc t i ve tes t ing. Applicat ion to a given s i tuat ion, ease of operat ion, r e l a t i ve cost and p e r m a n e n t r e c o r d s a r e a lso exami - ned. E m p h a s i s is p laced on the i n t e r p r e t a t i o n of the s ign i f i - cance of f laws in ERW pipes des t ined for the power g e n e r a - tion indus t ry . The author concludes that the m u l t i - m e t h o d approach is s t i l l the bes t . (8 f igures , 3 t ab les (Ul t r a son ic s 1967, a b s t r a c t 658)

LITTLEFORD, G. E. Welding e l ec t ron ic d e v i c e s by u l t rason ics . Indus t r i a l E lec t ron ics , 5, No. 3, p. 123 (1967).

U l t r a son ic welding of m i c r o e l e c t r o n i c dev ices is m o r e effi- c ient and p r e c i s e than any o the r known method. U l t r a son ic s can weld many meta l and al loy combina t ions in t h i c k n e s s e s of 100k upwards . A t rue sol id s t a t e me ta l l u rg i ca l bond i s obtained without the appl ica t ion of heat or f luxes and the bonds a r e c o m p a r a b l e in s t r eng th to the pa ren t ma te r i a l . A n u m b e r of examples a re given that have found appl ica t ion in m a s s product ion. (2 tables , 3 f igures ) (Ul t r a son ics 1967, a b s t r a c t 659)

KELPIN, H. and WEIS, O. Sound energy r e c e i v e r s for the m e a s u r e m e n t of a t t enua- t ion above 300MHz. Acust ica, 18, No. 2, p. 105 (1967).

To o v e r c o m e the dif f icul t ies of m e a s u r e m e n t s of high f r e - quency ul t rasound, t e m p e r a t u r e r e s i s t i v e e l emen t s were in- ves t iga ted . These a r e the rmocoup le e lements , the min i a tu r e NTC r e s i s t o r s and thin (BaSr)TiO 3 d i s c s as P T C - r e s i s t o r s . These devices r e g i s t e r the total energy d i ss ipa t ion and a r e not dependent on the pa ra l l e l i sm , the su r f ace f in ish or the homogenei ty of the t r a n s d u c e r s and can be used in the giga- he r t z f requency range. Resul t s of some com para t i ve expe r i - men t s at approximate ly 312MHz in the 21°-42°C t e m p e r a t u r e r ange a r e given. (6 f igures , 1 table, 8 r e f e r e n c e s ) (Ul t ra - sonics 1967, a b s t r a c t 655)

194 ULTRASONICS July 1967

LOVELACE, J. F. Mathemat ica l a n a l y s i s of the ef fec ts of d i a m e t e r and wal l th ickness on u l trasonic inspect ion of pipe but t welds. M a t e r i a l s Evaluat ion.

Resu l t s of an inves t iga t ion conducted to d e t e r m i n e the f e a s i - bi l i ty of u l t r a son ic detec t ion of in t e rna l defec ts in pipe butt welds a r e r epor t ed . The s i ze s and m a t e r i a l s of i n t e r e s t were those used for c r i t i ca l c i r cu i t s in the cons t ruc t ion of sub- m a r i n e s . A sens i t iv i ty s t anda rd was developed which u se s a c a l i b r a t e d a t tenua tor . It is thought tha t the r e l i ab i l i ty of u l t r a son ic t es t ing i s comparab l e to rad iography. Some a n o m a - lous r e f l ec t ions f rom d iscont inu i t i es in pipes below 0 .5 in (1 .27cm) wall th ickness have been o b s e r v e d and a r e ana lyzed theore t i ca l ly . (8 f igures , 1 table, 6 r e f e r e n c e s ) (Ul t rason ics 1967, a b s t r a c t 660)