Temperature measurement in the tensile Hopkinson bar test

A thermal scanning camera has been used to measure the temperatures reached in a small tensile specimen of ductile Remco iron deformed at a strain rate of about 1600 s-1 in a split Hopkinson bar apparatus. True strains as high as 3.3 were reached in times of about 200 mu s, leading to a significant rise in temperature of the specimen. To estimate this rise in temperature from the scanner's signal, account had to be taken of (i) movement of the specimen with respect to the camera during the scanning period, (ii) changing orientation of the specimen surface with respect to the infrared detector due to strain localization in the neck and (iii) changing emissivity of the specimen surface as deformation proceeds. Errors in the first two stages are small whereas those in the last stage impose tolerances of approximately +40 degrees C and -30 degrees C on the maximum temperatures. The possibility of scanning away from the axis of the specimen increases the upper tolerance by as much as 25 degrees C, Finally, the detector's rise time may have prevented the scanner resolving the steep temperature gradients present, Together these factors give an overall tolerance of between +100-150 degrees C to -30 degrees C on an estimated temperature of about 300 degrees C. It is clear, therefore, that despite this large margin of error there is a significant rise in temperature within the specimen, sufficient to affect the observed mechanical response.

[1]  Frithiof I. Niordson,et al.  A unit for testing materials at high strain rates , 1965 .

[2]  Ares J. Rosakis,et al.  On the temperature distribution at the vicinity of dynamically propagating cracks in 4340 steel , 1991 .

[3]  R. Pond,et al.  Inhomogeneous thermal changes in copper during plastic elongation , 1975 .

[4]  Ehud Gartenberg,et al.  Influence of temperature gradients on the measurement accuracy of IR imaging systems , 1990, Defense, Security, and Sensing.

[5]  D. Dewitt,et al.  Theory and practice of radiation thermometry , 1988 .

[6]  Tjorbjohn Hamrelius Accurate temperature measurement in thermography: an overview of relevant features, parameters, and definitions , 1991, Defense, Security, and Sensing.

[7]  H. Kolsky An Investigation of the Mechanical Properties of Materials at very High Rates of Loading , 1949 .

[8]  Bo Wallin,et al.  Advanced real-time scanning concept for full dynamics recording, high image quality, and superior measurement accuracy , 1991, Defense, Security, and Sensing.

[9]  A. Rosakis,et al.  On the dependence of the dynamic crack tip temperature fields in metals upon crack tip velocity and material parameters , 1993 .

[10]  B. Hopkinson A method of measuring the pressure produced in the detonation of high explosives or by the impact of bullets , 1914 .

[11]  Geoffrey Ingram Taylor,et al.  The use of flat-ended projectiles for determining dynamic yield stress I. Theoretical considerations , 1948, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[12]  R. Davies A critical study of the Hopkinson pressure bar , 1948, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[13]  J. Duffy,et al.  Measurement of the temperature profile during shear band formation in steels deforming at high strain rates , 1987 .

[14]  J. Duffy,et al.  An experimental study of the formation process of adiabatic shear bands in a structural steel , 1988 .