Some observations of slip lines on deformed copper whiskers

Some observations of slip lines on deformed copper whiskers

SOME OBSERVATIONS OF SLIP LIhES WHISKERS P. ON DEFORMED COPPER * CHARSLEYt Observations on slip markings which are produced during the tensil...

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SOME

OBSERVATIONS

OF SLIP

LIhES

WHISKERS P.

ON DEFORMED

COPPER

*

CHARSLEYt

Observations on slip markings which are produced during the tensile deformation of copper whiskers indicate that visible cross-slip does not necessarily occur during the propagation of a Liiders band. A mechanism is proposed whereby such a band propagates as a result of the stress concentration between the slipped and unslipped regions of the whisker. QUELQUES

OBSERVATIONS

DE

LIGNES

CUIVRE

DE

GLISSEMENT

SUR

DES

BARBER

Les lignes de glissement qui apparaissent au tours de la d&formation par traction cuivre indiquent que le glissement croisb ne se produit pas n&zessairement pendant la bande de Liiders. L’auteur propose un m&anisme au tours duquel une telle bande se propager par suite d’une concentration de tensions & l’interface des regions de respectivement deformbes et non dbformhes. EINIGE

DE

DEFORMEES

GLEITLINIENBEOBACHTUNGEN

AN

AUS

VERFORMTEN

SUP des barbes de propagation d’une a la possibilite de la barbe qui sent’

FADENKRISTALLEN

KUPFER

Untersuchungen van Gleitspuren, die bei Zugversuchen auf Kupferwhiskern entstehen, zeigen, da0 sichtbare Quergleitung nicht notwendig bei der Ausbreitung eines Liidersbandes auftritt. Es wird ein Mechanismus vorgeschlagen, wodurch sich solch ein Band ausbreitet als Folge der Spannungskonzentration zwischen dem geglittenen und nicht geglittenen Gebiet des Whiskers.

The

plastic

deformation

of

copper

and

silver

Observations

were made with a low powered ( x 50)

whiskers has been reported in some detail by Brenner’l).

microscope

He found that after an initial yield point (usually at a

high powered

very

whisker had been removed

from the tensile machine.

In several

were removed

high stress) the whiskers

by the propagation

deformed

of one or more Liiders bands at

stresses of the order of one twentieth yield

stress.

It was proposed

Liiders

band

perfect

whisker

is propagated

of the initial

by Brenner through

by a double

multiple

propagation

that neither double slip mechanism

of

the

Liiders

before from

mechanism ;

slip on copper whiskers in some cases. which indicate

machine

that the

an essentially

cross-slip

this proposal was based on the observation

other

plastically

of multiple

are

stress-strain

whiskers with

of a number

(grown by the reduction

(loo),

measured

curves

in

(110) and

and (111)

observations

of

copper

of cuprous

iodide)

orientations made

some

systems

a varying

observed

was that,

slip

case of a (110) 2 per cent. band

it was assumed that

were also made

at a constant

on

orientation

slip on

stress and

slip was confined to several

systems

In

had

whisker

was

after a Liiders

at a stress constant

to within

Fig. 2 shows slip on two systems in the

between 2 and 4 kg/mm2.

the faces

although

but the slip was much more intense on one

best developed

between

but

conclusion

When the Liiders band propagated

stress,

band had propagated

of the slip lines

measurements

propagation

the

system than on any other. In Fig. 1 can be seen the slip which resulted in the

have been

the traces all resulted from slip on (111) planes.

from

the

in some cases, when the

had occurred,

case of a (100) orientation

some cases goniometric

band

when

The general

did occur

formed. By measuring the angles of the various slip traces it was found that for all three orientations the faces were {llO};

and under a

microscope

Liiders

these observations

several

at

this paper. The

after

any work-hardening.

only one system.

for the

reported

deformation

x800)

cases whiskers

no work-hardening

cross-slip nor any

band

plastic

(up to

Liiders band had propagated

Observations

is essential

during

propagated

whisker after the Liiders at

stresses

which

varied

In Fig. 2 it can be seen that

the “primary” slip extends along the whole length of the whisker and is intense in localized regions whilst

of the angles and these

were

slip also occurs

consistent with the indices of the faces deduced the slip trace angles.

from

patches. Some of the secondary slip is open to the interpretation that it is single cross-slip. Carbon replicas shadowed at tan-l & with goldpalladium were made of several deformed copper

*

Received June 25, 1959. t Research Laboratory, Associated Electrical Industries Limited, Aldermaston Court, Aldermaston, Berkshire. Present address: Battersea College of Technology, Physics Department, Battersea Park Road, London, S.W.ll. ACTA

METALLURGICA,

VOL.

8, JUNE

1960

whiskers.

on a secondary

system

These whiskers were deformed

in isolated

in tension in

a simple jig so that the Ltiders band had propagated 353

354

ACTA

FIG. 1. Slip

lines

on

along the whisker. about

a

(110) x 350

orientation

whisker.

were obtained

over a length of about

from

which

satisfactory

from two adjacent

0.1 mm.

faces

Slip was visible

VOL.

8,

FIG. 3. Carbon

In Fig. 3 is shown a whisker of

30 ,u mean diameter

micrographs

METALLURGICA,

on

1960

replica of whisker.

slip in strained x 8400

like the other whiskers, slip has given rise to only one slip trace some of the slip lines are of great depth. Several

slip lines, which

appeared

to be individual

slip steps, were about 0.8 ,u deep ; this is an appreciable

only one system for the whole area of both whisker

fraction

surfaces

between the lines was about 0.4 ,u.

investigated.

It was difficult

the step heights accurately slip lines were seen to end.

Replicas with

whiskers

were obtained

mean

diameters

Brenner

between

10 and 20 ,u; these showed slip on only one

mechanism.

The

can occur

spacings

between

the lines for

has

propagates

system.

mean

The mean spacing

DISCUSSION

300 A ; in some cases

from

other

of the whisker thickness.

on these replicas but they

were never more than about two

to determine

copper

proposed

that

the

Liiders

along the whisker by a double However, in copper,

cross-slip

band

cross-slip

is a process

at room-temperature,

which only

at

these three whiskers were 0.03, 0.1 and 0.3 ,u in order

high stresses such as can exist at the head of a piled up

of decreasing

group of dislocations

whisker diameter.

Some replicas were obtained

of a deformed

whisker

(see Schoeck and Seegerf2)).

11 ,u wide and 2 ,u thick and these present a strikingly

tions is necessary on the cross-slip system.

different

of whiskers

appearance

from

the

three

whiskers

of

larger mean diameter as is shown in Fig. 4. Although,

Fro. 2. Slip

lines

on

a (100) x 1050

orientation

whisker.

For

double cross-slip to occur, a further pile up of disloca-

resolvedshear

of (100)

orientation,

In the case

in particular,

the

stress factor is the same for the “cross-slip

FIG. 4. Carbon replica of a deformed diameter. x 8000

whisker of small

CHARSLEY:

system” the

SOME

as for the “primary

double

cross-slip

comparable

amounts

both slip systems. results indicate sarily

OBSERVATIONS

occur

slip system.”

mechanism

were

of slip would

SLIP

Thus

LINES

if

operative

be expected

In contrast to this the experimental

during

An alternative

the

Liiders

band

propagation.

mechanism,

more in agreement with

results,

the Liiders

as a result slipped

of the stress

between

the

whisker.

The observation

in zinc and cadmium

is that

and

unslipped

band

concentration regions

of the

of Liiders band propagation

whiskers

by Coleman

ON

DEFORMED

et &.t3)

COPPER

WHISKERS

355

supports this idea in so far as slip on any planes other than the basal planes is extremely

on

that visible cross-slip does not neces-

the experimental propagates

OF

unlikely.

ACKNOWLEDGMENTS

The author F.R.S.,

Director

wishes to thank

Dr. T. E. Allibone,

of this Laboratory,

for permission

to

publish this Paper. REFERENCES 1. S. S. BRENNER,J. Appl. Phys. 28, 1023 (1957). 2. G. SCHOECK and A. SEEGER in Rep. Bristol Conf. on Defects in Cqstalline Solids. p. 340. Physical Society, London (1955). 3. R.V. COLEMAN,B. PRICE and N. CABRERA, J. Appl. Phys. 28, 1361 (1957).