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Non compact glide in face centered cubic metals

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HAL Id: jpa-00245827

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Submitted on 1 Jan 1988

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Non compact glide in face centered cubic metals

M. Carrard

To cite this version:

M. Carrard. Non compact glide in face centered cubic metals. Revue de Physique Appliquée, Société

française de physique / EDP, 1988, 23 (4), pp.678-678. �10.1051/rphysap:01988002304067800�. �jpa-

00245827�

(2)

678

NON COMPACT GLIDE IN FACE CENTERED CUBIC METALS M. Carrard

EPF Lausanne, Institut de Génie Atomique

1015 - Lausanne (Switzerland)

Revue Phys. Appl. 23 (1988) 678 AVRIL 1988,

The present knowledge and ideas on non compact glide in pure f.c.c. metals are reviewed, with special reference to Aluminium single crystals.

These glide systems, which were considered in past

as abnormal or exceptional, have in fact their own

Burgers vectors and well defined slip planes and

seem to obey the Schmid Law. Moreover, they become

easy at high temperatures, where they can replace completely the normal compact slip systems (see,

for example, [1-9]).

Several non compact slip planes have been ob- served, such as (001), (110), (112), (113) in single crystals and polycrystals for various

f.c.c. metals, such as Aluminium, Copper, Silver, Gold and Nickel. Although their study has been performed mainly by slip line observations, non compact glide activation affect also the deforma- tion curve shape, the dislocation substructure and the slip mode during in situ experiments.

The stress-strain curves present a sharp de-

crease in hardening when non-compact glide is acti- vated (see figure 1). The stress corresponding to

this decrease can be directly related to the cri- tical resolved shear stress for the corresponding non-compact glide. Figures 1 and 2 show that this

stress decreases rapidly with temperature. Non compact glide are therefore strongly thermally

activated with an apparent activation enthalpy

close to 1.7 eV for (001) glide and 1.4 eV for (110) glide.

Among the different models, the nucleation and propagation of kink pairs on screw dislocations

seems to be more appropriate to account for all these observations. The comparison of the differ-

ent apparent activation enthalpies measured in Aluminium show that non compact glide can be a

Figure 1. Stress-strain curves in [112] Al single

crystals for (001) glide [2]. The arrows correspond

to the critical stress for glide on the (001) plane. At 299 ° C1, only (111) glide is activated.

(y

=

12.10 sec ).

creep rate controlling mechanism at the beginning

of the high temperature domain. Besides, it can also explain the abnormally high values of apparent activation enthalpy found systematically

in high temperature creep of Copper.

This review shows that non compact glide takes

a prominent part in the deformation processes at

high temperatures. This importance was unsus- pected up to now and only two detailed studies exist. Consequently it appears urgent to undertake similar investigations with different single crystal orientations and various f.c.c. metals.

Figure 2. Critical resolved shear stress for (001) glide versus temperature for three different

strain rates (1 : 03B3 = 12.10-5 sec-1, 2 : 03B3

=

12.10-4 sec- 1, 3 : 03B3 = 12.10-3 sec-’). The curves

correspond to the kink pair model [2].

References :

[1] Carrard M. and Martin J.L., ICSMA 7, Montreal, 1985, p. 665.

[2] Carrard M., Doctorate Thesis, Lausanne, 1985.

[3] Bonneville J., Caillard D., Carrard M., Martin J.L., this conference.

[4] Carrard M. and Martin J.L., Phil. Mag.,

accepted for publication, 1987.

[5] Le Hazif R., Dorizzi P. and Poirier J.P., Acta Met., 21 (1973) 903.

[6] Le Hazif R. and Poirier J.P., Acta Met., 23

(1975) 865.

[7] Lacombe P. and Beaujard L., J. Inst. Met., 74 (1947) 1.

[8] Johnson R.D., Young A.P. and Schwope A.D.,

Proc. of a Symposium on the Creep and Fracture of Metals at high temperatures, London,1956,

p. 25.

[9] Cahn R.W., J. Inst. Metals, 79 (1951) 129.

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/rphysap:01988002304067800

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