Determination of the fraction of plastic work converted into heat in metals

Abstract A new approach for measuring the fraction of plastic work that is converted into heat (also known as the Inelastic Heat Fraction, IHF or the Taylor–Quinney coefficient) during the plastic deformation of metals is proposed in this paper. The method is based on the uniaxial tension of a slender metal rod, with the lateral surface of the rod being under well-defined thermal boundary conditions. The corresponding one-dimensional model of heat transfer during the process is considered in the form that accounts for all major effects. The current approach is based on the fact that the unknown IHF enters this heat equation linearly and therefore can be found explicitly if all the other terms are accounted for experimentally. The experimental procedure developed is based on local measurements of temperature and its gradients and of strain and velocity with the aid of an infrared (IR) camera and a Digital Image Correlation (DIC) system, respectively. A vacuum tube that encloses the specimen was designed to provide control over the heat losses due to convection during the test. A fitting method based on Hermite splines allows us to deal with smooth functions instead of noisy data sets, improving the overall accuracy of the procedure. The IHF is obtained as a function of plastic strain for a set of strain rates for four materials: 303 and 316 stainless steels, commercially-pure titanium (CP Ti) and the alloy Ti–6Al–4V. The findings indicate that the IHF is not constant with the plastic strain and furthermore, it is also sensitive to the strain-rate. Our measurements revealed that depending on the material the IHF was generally between 0.55 and 0.8, but it could also be as low as 0.3.

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

[2]  T. Børvik,et al.  Heat sources, energy storage and dissipation in high-strength steels: Experiments and modelling , 2010 .

[3]  G. Taylor,et al.  The Heat Developed during Plastic Extension of Metals , 1925 .

[4]  F. Morel,et al.  Experimental and numerical study of the evolution of stored and dissipated energies in a medium carbon steel under cyclic loading , 2013 .

[5]  R. H. Wagoner,et al.  A simplified model of heat generation during the uniaxial tensile test , 1987 .

[6]  J. Rodríguez-Martínez,et al.  On the Taylor–Quinney coefficient in dynamically phase transforming materials. Application to 304 stainless steel , 2013 .

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

[8]  G. Cullen Ductility of 304 stainless steel under pulsed uniaxial loading , 2013 .

[9]  B. J. Pletka,et al.  Plastic deformation of hafnium under uniaxial compression , 1997 .

[10]  George C. Kirby,et al.  A HYBRID NUMERICAL/EXPERIMENTAL TECHNIQUE FOR DETERMINING THE HEAT DISSIPATED DURING LOW CYCLE FATIGUE , 1990 .

[11]  D. L. Holt,et al.  The stored energy of cold work , 1958 .

[12]  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 .

[13]  Daniel Rittel,et al.  On the conversion of plastic work to heat during high strain rate deformation of glassy polymers , 1999 .

[14]  M. Kamlah,et al.  On the Macroscopic Description of Stored Energy and Self Heating During Plastic Deformation , 1997 .

[15]  V. Shim,et al.  Determination of inelastic heat fraction of OFHC copper through dynamic compression , 2010 .

[16]  Geoffrey Ingram Taylor,et al.  The Latent Energy Remaining in a Metal after Cold Working , 1934 .

[17]  Xavier Maldague,et al.  Theory and Practice of Infrared Technology for Nondestructive Testing , 2001 .

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

[19]  R. H. Wagoner,et al.  An analytical investigation of deformation-induced heating in tensile testing , 1987 .

[20]  Muh-ren Lin,et al.  An experimental investigation of deformationinduced heating during tensile testing , 1987 .

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

[22]  Laurent Stainier,et al.  Study and validation of a variational theory of thermo-mechanical coupling in finite visco-plasticity , 2010 .

[23]  A. L. Titchener,et al.  The Stored Energy of Cold Work , 1973 .

[24]  A. N. Stroh A theoretical calculation of the stored energy in a work-hardened material , 1953, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[25]  Alan T. Zehnder,et al.  Hybrid method for determining the fraction of plastic work converted to heat , 1998 .

[26]  G. Pitarresi,et al.  A review of the general theory of thermoelastic stress analysis , 2003 .

[27]  François Hild,et al.  On the stored and dissipated energies in heterogeneous rate-independent systems: theory and simple examples , 2009 .

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

[29]  Patrice Longère,et al.  Evaluation of the inelastic heat fraction in the context of microstructure-supported dynamic plasticity modelling , 2008 .

[30]  Pierre Vacher,et al.  Inelastic heat fraction estimation from two successive mechanical and thermal analyses and full-field measurements , 2013 .

[31]  Patrice Longère,et al.  Plastic work induced heating evaluation under dynamic conditions : critical assessment , 2008 .

[32]  Y. Bréchet,et al.  The stored energy of cold work: Predictions from discrete dislocation plasticity , 2005 .

[33]  A. Chrysochoos,et al.  Plastic and dissipated work and stored energy , 1989 .