Determination of the Constitutive Relation Parameters of a Metallic Material by Measurement of Temperature Increment in Compressive Dynamic Tests

The mechanical behaviour of a material can be established by an analytic expression called the constitutive relation that shows stress as a function of plastic strain, strain rate, temperature, and possibly other thermo-mechanical variables. The constitutive relation usually includes such parameters as coefficients or exponents that must be determined. At a high strain rate, the heat generated during the deformation process is directly related to the plastic deformation energy of the material. This energy can be calculated from the plastic work, resulting in an expression that includes the constitutive relation parameters as variables. The heat generated can also be estimated by measuring the temperature surface of the specimen during compressive tests using the technique of infrared thermography. The objective of this paper is to present a procedure for determining the constitutive relation parameters by measuring the temperature increase associated with plastic strain in compressive Hopkinson tests. The procedure was applied to estimate the parameters of the Johnson–Cook constitutive relation of an aluminium alloy (Al6082).

[1]  D. Macdougall,et al.  Determination of the plastic work converted to heat using radiometry , 2000 .

[2]  Ares J. Rosakis,et al.  Partition of plastic work into heat and stored energy in metals , 2000 .

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

[4]  A. Zehnder A model for the heating due to plastic work , 1991 .

[5]  Sia Nemat-Nasser,et al.  Determination of temperature rise during high strain rate deformation , 1998 .

[6]  J. Harding,et al.  The measurement of specimen surface temperature in high-speed tension and torsion tests , 1998 .

[7]  A. Rosakis,et al.  A thermodynamic internal variable model for the partition of plastic work into heat and stored energy in metals , 2000 .

[8]  F. Leckie,et al.  On the Calculations of the Stored Energy of Cold Work , 1990 .

[9]  J. Meléndez,et al.  Measurement of Temperature Increment in Compressive Quasi‐Static and Dynamic Tests Using Infrared Thermography , 2009 .

[10]  E. Pieczyska,et al.  Measurement of temperature during simple dynamic shear , 2002 .

[11]  J. Fernández-Sáez,et al.  An implicit consistent algorithm for the integration of thermoviscoplastic constitutive equations in adiabatic conditions and finite deformations , 2006 .

[12]  E. Pieczyska,et al.  Changes of temperature during the simple shear test of stainless steel , 1996 .

[13]  J. R. Klepaczko,et al.  Experiments on heat generated during plastic deformation and stored energy for TRIP steels , 2009 .

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

[15]  James J. Mason,et al.  On the strain and strain rate dependence of the fraction of plastic work converted to heat: an experimental study using high speed infrared detectors and the Kolsky bar☆ , 1992 .

[16]  J. Harding,et al.  An improved technique for the experimental measurement of specimen surface temperature during Hopkinson-bar tests , 1998 .