The mechanism of shock-induced dynamic friction has been explored through an integrated programme of experiments and numerical simulations. A novel experimental technique has been developed for observing the sub-surface deformation in aluminium when sliding against a steel anvil at high velocity and pressure. The experimental observations suggest that slight differences in conditions at the interface between the metals affect frictional behaviour even at the very high-velocity, high-pressure regime studied here. However, a clear finding from the experimental work is the presence of two distinct modes of deformation termed deep and shallow. The deep deformation is observed in a region of the aluminium specimen where the interfacial velocity is relatively low and the shallow deformation is observed in a region where the interfacial velocity is higher. A 1D numerical treatment is presented which predicts the existence of two mechanisms for dynamic friction termed 'asymptotic melting' and 'slide-then-lock'. In both modes there is a warm-up phase in which the interface temperature is increased by frictional heating. For high initial sliding velocity, this is followed by the onset of the asymptotic melting state, in which the temperature is almost constant and melting is approached asymptotically. This mechanism produces low late-time frictional stress and shallow deformation. For lower initial sliding velocity, the warm-up terminates in a violent work hardening event that locks the interface and launches a strong plastic shear wave into the weaker material. This slide-then-lock mechanism is characterized by sustained high frictional stress and deep plastic deformation. These predicted mechanisms offer a plausible and consistent explanation for the abrupt transitions in the depth of sub-surface deformation observed in the experiments. A key conclusion arising from the current work is that the frictional stress does not vary smoothly with pressure or sliding velocity. Instead the pressure and sliding velocity determine whether the impulse will be very high or very low. The next generation of friction models for hydrocodes will need to account for these factors.
[1]
Dean L. Preston,et al.
Model of plastic deformation for extreme loading conditions
,
2003
.
[2]
Andrew Barlow,et al.
An adaptive multi-material Arbitrary Lagrangian Eulerian algorithm for computational shock hydrodynamics
,
2002
.
[3]
S. Szarzynski,et al.
Investigation of Dynamic Friction Induced by Shock Loading Conditions
,
2005
.
[4]
D. Steinberg,et al.
A constitutive model for metals applicable at high-strain rate
,
1980
.
[5]
Vikas Prakash,et al.
Frictional Response of Sliding Interfaces Subjected to Time Varying Normal Pressures
,
1998
.
[6]
R. Clifton,et al.
Finite Deformation Analysis of Pressure-Shear Plate Impact Experiments on an Elastohydrodynamic Lubricant
,
1992
.
[7]
A pressure-shear plate impact experiment for studying the rheology of lubricants at high pressures and high shearing rates
,
1987
.