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Adiabatic shear fracture prediction in high-speed cutting at various negative rake angles and feeds

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Abstract

The critical characteristics of adiabatic shear fracture (ASF) that induce the formation of isolated segment chip in high-speed machining was further investigated. Based on the saturation limit theory, combining with the stress and deformation conditions and the modified Johnson-Cook constitutive relation, the theoretical prediction model of ASF was established. The predicted critical cutting speeds of ASF in high-speed machining of a hardened carbon steel and a stainless steel were verified through the chip morphology observations at various negative rake angles and feeds. The influences of the cutting parameters and thermal–mechanical variables on the occurrence of ASF were discussed. It was concluded that the critical cutting speed of ASF in the hardened carbon steel was higher than that in the stainless steel under a larger feed and a lower negative rake angle. The proposed prediction model of ASF could predict reasonable results in a wide cutting speed range, facilitating the engineering applications in high-speed cutting operations.

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Abbreviations

\(t\) :

Time (s)

\(v\) :

Cutting velocity (m·\({\text{s}}^{ - 1}\))

\(v_{\text{S}}\) :

Shear velocity (m·\({\text{s}}^{ - 1}\))

\(v\left( y \right)\) :

Velocity distribution (m·\({\text{s}}^{ - 1}\))

a :

Rate-related gradient factor

\(a_{\text{c}}\) :

Uncut thickness (m)

\(a_{\text{ch}}\) :

Chip thickness (m)

\(a_{\beta }\) :

Experimental coefficient

\(\phi\) :

Shear angle (\(^{ \circ }\))

\(\psi_{0}\) :

Section shrinkages (%)

\(\psi\) :

Angle between free surface plane and shear plane (\(^{ \circ }\))

\(p_{y}\) :

Momentum (kg·m/s)

\(U\) :

Upper side displacement of TP region (m)

\(W\) :

Boundary shear work of RP region (J·\({\text{m}}^{ - 2}\))

\(S\) :

Shear bandwidth (\(\upmu{\text{m}}\))

\(h_{\text{S}}\) :

Half thickness of primary shear zone (m)

\(\xi\) :

Location of thermo-plastic boundary (m)

\(\sigma\) :

Compressive stress (MPa)

\(\sigma_{\text{b}}\) :

Tensile strength (MPa)

\(\sigma_{\text{S}}\) :

Yield strength (MPa)

\(\delta\) :

Malleability (%)

\(\tau\) :

Shear stress (MPa)

\(\hat{\tau }\) :

Equivalent shear stress (MPa)

\(\tau_{\text{p}}\) :

Equivalent peak stress (MPa)

\(\tau \left( {\gamma ,\dot{\gamma },\theta } \right)\) :

Constitutive relation (MPa)

\(f_{1} \left( \varepsilon \right)\) :

Component of strain hardening effect

\(f_{2} \left( {\dot{\varepsilon }} \right)\) :

Component of strain rate hardening effect

\(f_{3} \left( {\theta^{*} } \right)\) :

Component of thermal softening effect

\(\varepsilon\) :

Strain

\(\dot{\varepsilon }\) :

Strain rate (\({\text{s}}^{ - 1}\))

\(\hat{\varepsilon }\) :

Effective strain

\(\hat{\dot{\varepsilon }}\) :

Effective strain rate (\({\text{s}}^{ - 1}\))

\(\gamma\) :

Shear strain

\(\dot{\gamma }\) :

Shear strain rate (\({\text{s}}^{ - 1}\))

\(\gamma_{0}\) :

Rake angle (\(^{ \circ }\))

\(\gamma_{\text{S}}\) :

Strain of RP region

\(L_{\text{P}}\) :

Teeth space (mm)

\(L_{\text{S}}\) :

Shear band space (mm)

\(\theta\) :

Temperature (K)

\(\theta_{0}\) :

Room temperature (K)

\(\theta_{\text{m}}\) :

Melt temperature (K)

\(\Delta \theta\) :

Temperature rise (K)

\(\rho\) :

Mass density (kg·\({\text{m}}^{ - 3}\))

\(c\) :

Thermal specific capacity (J·\({\text{kg}}^{ - 1}\)·\({\text{K}}^{ - 1}\))

\(\chi\) :

Thermal diffuse coefficient (m2·\({\text{s}}^{ - 1}\))

\(\beta\) :

Taylor and Quinney coefficient

\(\beta_{0}\) :

Incline angle of the free surface (\(^{ \circ }\))

\(G_{\text{ASB}}\) :

ASB energy (J·\({\text{m}}^{ - 2}\))

\(G_{\text{ASB}}^{\text{f}}\) :

Saturation limit (J·\({\text{m}}^{ - 2}\))

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Acknowledgements

This work is supported by the National Natural Science Foundation of China (Grant Nos. 51601155 & 51175063). Thanks for the language support from Ms. Nan Cui. Thanks for the support from School of Mechanical Engineering from Dalian University of Technology.

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Gu, LY., Wang, MJ. Adiabatic shear fracture prediction in high-speed cutting at various negative rake angles and feeds. Adv. Manuf. 6, 41–51 (2018). https://doi.org/10.1007/s40436-018-0212-2

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