TRANSDUCER AND BOND PHASE SHIFTS IN ULTRASONICS, AND THEIR EFFECTS ON MEASURED PRESSURE DERIVATIVES OF ELASTIC MODULI

Abstract Phase shifts introduced into ultrasonic signals by the presence of transducers and bonds at sample surfaces have been measured using an automated variable frequency ultrasonic interferometer. At zero pressure, phase shifts have been resolved due to transducers, bonds between transducers and samples, and bonds between buffer rods and samples. Observed transducer-bond-sample phase shifts are in good accord with theoretical estimates, and bond thicknesses of about 0.3 μ are inferred. Measurements to 7 kbar are consistent with theoretical estimates of the effect of pressure on transducer-bond-phase shifts. Providing the frequency of the ultrasonic signal is within a few percent of the resonance frequency of the transducer, and the effect of pressure on the transducer resonance frequency is accounted for (as recommended by McSkimin, [1961]), the effect of the bond phase shift on the measured pressure derivative of the elastic modulus should amount to less than about 0.02. If the frequency deviates substantially from the transducer resonance frequency, especially at zero pressure, errors of the order of 0.25 could be incurred in the pressure derivatives. The nonlinearity of transducer-bond phase shifts could cause significant errors in second-pressure derivatives, even under favorable conditions. For shear waves at zero pressure, the observed buffer-bond-sample phase shifts are consistent with those estimated theoretically for a bond of about 1 μ thickness. For compressional waves at zero pressure, phase shifts are very sensitive to the buffer-sample contact: large differences in phase are observed between dry lapped, “wetted” immersed, and resin-bonded contacts. The sources of these differences are not fully understood, but they may be due to variations in contact area produced by the ultrasonic wave. “Normal” buffer-sample bonds are estimated to be capable of affecting measured pressure derivatives by about 0.25. The behavior of the anomalous buffer-sample phase shifts under pressure is unknown, but the shifts could easily give rise to substantial errors in measured pressure derivatives.

[1]  H. Spetzler,et al.  Equation of State of Polycrystalline and Single‐Crystal MgO to 8 Kilobars and 800°K , 1970 .

[2]  I. J. Fritz Pressure and temperature dependences of the elastic properties of rutile (TiO2) , 1974 .

[3]  H. Spetzler,et al.  COUPLING OF ULTRASONIC ENERGY THROUGH LAPPED SURFACES AT HIGH TEMPERATURE AND PRESSURE , 1969 .

[4]  D. Schuele,et al.  Pressure derivatives of the elastic constants of NaCl and KCl at 295°K and 195°K , 1965 .

[5]  O. Anderson,et al.  Pressure Derivatives of Elastic Constants of Single‐Crystal MgO at 23° and ‐195.8°C , 1966 .

[6]  G. R. Barsch,et al.  Elastic constants of single‐crystal forsterite as a function of temperature and pressure , 1969 .

[7]  Mineo Kumazawa,et al.  Elastic moduli, pressure derivatives, and temperature derivatives of single‐crystal olivine and single‐crystal forsterite , 1969 .

[8]  Z. Chang,et al.  Pressure dependence of single‐crystal elastic constants and anharmonic properties of spinel , 1973 .

[9]  J. Drabble,et al.  The third-order elastic constants of potassium chloride, sodium chloride and lithium fluoride , 1967 .

[10]  Murli H. Manghnani,et al.  Elastic constants of single‐crystal rutile under pressures to 7.5 kilobars , 1969 .

[11]  M. Redwood,et al.  On the measurement of attenuation in ultrasonic delay lines , 1956 .

[12]  H. J. Mcskimin,et al.  Pulse Superposition Method for Measuring Ultrasonic Wave Velocities in Solids , 1961 .

[13]  H. J. Mcskimin,et al.  Analysis of the Pulse Superposition Method for Measuring Ultrasonic Wave Velocities as a Function of Temperature and Pressure , 1962 .

[14]  J. Williams,et al.  On the measurement of ultrasonic velocity in solids , 1958 .

[15]  H. Spetzler,et al.  COUPLING OF ULTRASONIC ENERGY THROUGH LAPPED SURFACES: APPLICATION TO HIGH TEMPERATURES , 1969 .

[16]  H.J. McSkimin,et al.  Use of High Frequency Ultrasound for Determining the Elastic Moduli of Small Specimens , 1957, IRE Transactions on Ultrasonic Engineering.

[17]  R. N. Thurston,et al.  Elastic Moduli of Quartz versus Hydrostatic Pressure at 25 and-195.8C , 1965 .

[18]  R. Meister,et al.  Pressure derivatives of elastic moduli of fused quartz to 10 kb , 1967 .

[19]  Z. Chang,et al.  Nonlinear Pressure Dependence of Elastic Constants and Fourth-Order Elastic Constants of Cesium Halides , 1967 .

[20]  Charles G. Sammis,et al.  Equation of state of NaCl: Ultrasonic measurements to 8 kbar and 800°C and static lattice theory , 1972 .

[21]  A. L. Frisillo,et al.  Measurement of single‐crystal elastic constants of bronzite as a function of pressure and temperature , 1972 .

[22]  K. D. Swartz Anharmonicity in Sodium Chloride , 1967 .

[23]  H. J. Mcskimin,et al.  Variations of the Ultrasonic Pulse‐Superposition Method for Increasing the Sensitivity of Delay‐Time Measurements , 1965 .

[24]  H. J. Mcskimin Ultrasonic Measurement Techniques Applicable to Small Solid Specimens , 1950 .

[25]  Z. Chang,et al.  Pressure dependence of the elastic constants of single-crystalline magnesium oxide , 1969 .