• Aucun résultat trouvé

MICROSCOPIC STRUCTURES OF METASTABLE PHASES IN Al-Ag BINARY ALLOYS

N/A
N/A
Protected

Academic year: 2021

Partager "MICROSCOPIC STRUCTURES OF METASTABLE PHASES IN Al-Ag BINARY ALLOYS"

Copied!
6
0
0

Texte intégral

(1)

HAL Id: jpa-00225659

https://hal.archives-ouvertes.fr/jpa-00225659

Submitted on 1 Jan 1986

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

MICROSCOPIC STRUCTURES OF METASTABLE PHASES IN Al-Ag BINARY ALLOYS

T. Sakurai, A. Jimbo, T. Hashizume, A. Sakai, K. Osamura, T. Nakamura

To cite this version:

T. Sakurai, A. Jimbo, T. Hashizume, A. Sakai, K. Osamura, et al.. MICROSCOPIC STRUCTURES

OF METASTABLE PHASES IN Al-Ag BINARY ALLOYS. Journal de Physique Colloques, 1986, 47

(C2), pp.C2-179-C2-183. �10.1051/jphyscol:1986226�. �jpa-00225659�

(2)

JOURNAL DE PHYSIQUE

Colloque C2, supplément au n03, Tome 47, mars 1986 page

c2-179

MICROSCOPIC STRUCTURES OF METASTABLE PHASES I N A l - A g BINARY ALLOYS

T. SAKURAI, A. JIMBO, T. HASHIZUME, A. SAKAI, K. OSAMURA' and T. NAKAMURA'

The Institute for Solid State Physics, The University of Tokyo, Tokyo, Japan

+

Department of Metallurgy, Kyoto University, Kyoto, Japan

Abstract - Morphology and chemical composition of metastable phases in an Al-5.72at% Ag alloy have been investigated by means of atom-probe field ion microscopy. The

ri

-G. P.

zone appears to have an ordered structure and its average solute concentration is 45.8at8 Ag at 413 K. The c-G. P.

zone is spherical in shape and its composition is 35.7at%

Ag. The

y'

metastable phase is plate-like precipitates lying on the { I l l 1 lattice planes, whose composition has been determined for the first time to be 33.3at% Ag.

1 - INTRODUCTION

Since the discovery of metastable coherent clusters by Guinier 1 the structures and growth proceses of G.P. zones have been extensively investigated in Al-Ag alloys / 2 / . The metastable phase diagram with respect to G.P. zones was given by Baur and Gerold /3/. The precipitation sequence is described as follows.

Depending on aging temperature, three types of G.P. zones precipitate. Below approximately 443 K, disordered

q

'-G.P. zones are formed and they are transformed to ordered

ri

-G.P. zones. Above 443K, disordered

E

- G. P. zones precipitate. At a later stage of aging, the metastable y ' phase appears. The equilibrium phase in this composition is Y phase.

Although the precipitation behaviors mentioned above have been generally accepted for long time, there exist still some uncertainties concerning the structures of these metastable phases.

In order to shed a light on these problems, direct observations on an atomic scale are most helpful. In the present study, the structures of both and

E

zones as well as

y '

metastable phase have been investigated by means of an AP-FIM and compared with the results obtained by other techniques, such as small-angle X-ray scattering.

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:1986226

(3)

C2-180

JOURNAL DE PHYSIQUE

II - EXPERIMENTAL PROCEDURE

An Al-5.72at% Ag binary alloy was solution-treated at 823 K for 6ks and then quenched into ice water. After the specimen was aged at 413 K or 463 K, it was electrochemically polished into a fine needle tip.

The details of the AP-FIM used in the present work were reported elsewhere/4/. The specimen tip is mounted on the manipulator and cooled down to approximately 30 K. After a good quality of hydrogen FI image is observed, the atom-probe analysis is performed using pulse ratio of 0.2 to 0.4 and repetition rate of 60 Hz.

III - RESULTS AND DISCUSSION

Fig. 1 shows the hydrogen FI images for the specimens aged at 413 K for 6 ks ( a ) and for 60 ks (b) and aged at 463 K for 60 ks (c).

Bright spots are Ag rich precipitates. Their size became larger and coarsened with increasing aging time as seen in the figure (a to b). Their shape appears to be spherical in those figures and we could not observe any facets or features characteristic to the octahedron. The present observation contradicts with the resluts by Alexander et a1./4/ who proposed the octahedral zones on a basis of the high resolution electron microscopy. This discrepancy may be attributed to the difference in particular particle sizes examined.

A typical result of the atom-probe analysis of these zones is shown in Fig. 2. The probe-hole was adjusted ont0 the (111) crystal plane. The layer-by-layer evaporation was realized and the number of atoms covered by a probe-hole was 51.4 per layer in average. The Ag concentration rises gradually at the edge of the zone £rom the matrix value (0.6 at% Ag) since the probe-hole covers both the matrix and the zone of Our interest at the interface. We note that the Ag concentration oscillates at the central part of the zone in the range of 25 to 50 at% Ag with an average of 37 at%. This may be due to the

O000

O 5 10 1 5 20 25

NUMBER OF LAYERS

Fig. 2. Ag concentration

profile of the zone

obtained upon aging at 413

K for 6 ks.

(4)

f act zone has an ordered structure along the < I l l > crystal orientation. Using a series of atom-probe data, the autocorrelation analysis was performed and the result is shown in Fig. 3. The correlation, G( rj , decreases rapidly as the distance between adjacent layers increases. After reaching a minimum at r u = 3.6nm, G( rj

)

increases again and shows a peak at = 6.3 nm. The first minimum of 9 r giveç the average cross-seclional dimension of the zone, 1, while the position of the maximum yields the average distance between the neighbouring zones, along the probing column.

The latter quantity is called the one-dimensional interparticle distance, Lu.

When the specimen was aged at 413 K for 60 ks, the size of the zone increased as shown in Fig. 1 (b). The solute concentration inside the zone is uniform and approximately 45.8at% Ag, slightly higher than that obtained by a shorter aging (Fig. 1 (a)). THe results on the structure of

ri

zones are summarized in Table 1 , along with the data of small-angle X-ray scattering measurements/5/.

0.8 0.6

n

L7

0.4

V

0.2-

O -0.2

Table 1. Summary of the size and interparticle distance of

ri

zones

O 2

4

6 8 1 0 1 2

' o i i i i ~ i i ~ i i ~

-

O

-

O

-

O

O o ~ O o ~ o

Fig. 3. Autocorrelation on

The average cross-sectional length,

9,

, is equal to 4 / 3 ~ for the identical spherical particles with radius R. In practice, however, the zones have a size distribution as its mean radius,

ii

, and the

standard deviation,

D

, and they are given in the table. Taking into account the size distribution, the present data of the length, , s qualitatively consistent with the SAXS result. The one-dimensional interparticle distance, Lu, may be different £rom the three dimensional distance, Lt! as determined by SAXS measurements. When the fine zones dlstribute homogeneously (the specimen aged for 6 ks), Lu obtained by AP-FIM is smaller than Lt. On the other hand, when the large zones are widely separated

(the specimen aged for 60 ks), Lu becomes larger than Lt.

For the specimen aged at 463 K for 60 ks, both spherical clusters and plate-like precipitates are observed as shown in Fig. 1 (c) and Fig. 4. The clusters are identified as

E

zone and the platelets as the metastable

y '

phase. The solute concentration of the spherical zone is found to be 35.7at% Ag. The concentration averaged over

O O O

O oo

O O

O O O00

-

O 0 O0 ~ o o o o o O

ooOf OO,OO

the fluctuation of the Ag concentration for an Al -

5.72 at% Ag aged at 413 K for 6 ks.

SAXS /17/

u Lt -

2.1 nm 1.4 8.3 nm 3.0 1.4 15.9 anneal ing

4 1 3 K 6 k s 413 60

- 0 . 4 - 1 " i " ' i ' i '

AP-FIM

v LI, - Rn

d

3.6 nm 6.3 nm 2.2 nm

5.3 30.9 3.2

(5)

~ 2 - 1 8 2

JOURNAL DE PHYSIQUE

f ive Y ' precipitates was determined to be 33,3at% Ag and the concentration profile inside the precipitate was found homogeneous.

This is the first time the composition of Y ' phase was determined.

From a series of FI images obtained sequentially during field evaporation, the relative positions and sizes of individual precipitates

( E

and

y

'

)

can be reconstructed

(

Fig. 5

)

. The

thickness of platelet Y ' phase is in the range of 2.3 to 7.9 nm and the size of

E

zone is approximately 30 nm. Recently Howe et al.

/8/ examined the thick

y

' layers and observed that there exist interfacial ledges whose height is more than two atomic layer high.

F i g .

4 . F i g . 5 .

Fig. 4. A series of H FI images of an Al- 5.72 at% Ag aged at 463 K for 60 ks, showing the evolution of the disk-shaped y ' precipitate (appeared as a ring).

Fig. 5. A schematic of the arrangement of disk-shape y ' precipitates appeared in Fig. 4.

However Our atom-probe work did not revealed any ledges in thin

y

'

layers examined so far.

An interesting observation as to the

Y

' precipitate is that the solute concentration becomes higher near the interface of the precipitate with thickness of one oe two layers as is shown in Fig.

5. It is suggested that this solute segregation may well be the initial stage of nucleation of the stabley phase.

Fig. 6. Concentration profile of Ag within the

y ' zone for an Al- 5.72

at% Ag aged at 463 K for

60 ks. The enrichment of

Ag is evident at the

boundar y.

(6)

IV - CONCLUSION

We have demonstrated that our focusing-type ToF atom-probe is capable of studying aging effects by analyzing the compositional profile of metastable phases in a small scale, using an Al-5.72at% Ag alloy aged at both 413 K and 463K.

REFERENCES

/1/ A. Guinier, J. Phys. Radium. Paris i3, 124 (1942).

/2/ G. W. Lorimer, "Precipitation in Aluminum Alloys", eds. K. C.

Russel amnd H. 1. Aaronson, (Meta1 Soc. AIME), 87 (1978).

/3/ R. Baur and V. Gerold, Acta Metal., u, 637 (1962).

/4/ K. B. Alexander, F. K. Legnoues, H.

1.

Aaronson and D. E.

Laughlin, Acta Metal., 32, 2241 (1984).

/5/ K. Osamura, M. Sakata and H. Okuda, Trans. JIM, submitted (1985).

/6/ R. B. Nicholson and J. Nutting, Acta Metal., 9 , 3323 (1961).

/7/ G. Ziegler, Z. Metallkde., 43, 213 (1952).

/8/ J. M. Howe, H. 1. Aaronson and R. Gronsky, Acta Metal., 33, 649

(1 985).

Références

Documents relatifs

4 Computer simulation of Nb3Sn FIM image in which the tin atoms appear brighter than the niobium atoms.. 6a Atom probe mass spectrum of grain boundary

Doi/3/ applied a Fourier analytical method to Toman's data and concluded that the zones are multi-layers and the zone center consists of 100% Cu and the adjacent layers only 50%

The conclusion is that the short range order in amorphous A1-V alloy and others, like AlMnSi is already similar to what it will be in the quasicrystalline phase which

Compositional depth profile of degree of order, to Li atoms in the brightly imaged region the 6 ' phase at of the Al-11.5 at% Li alloy aged at room the initial staae

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

Conventional microanalytical techniques (Optical Microscopy OM, Scanning Electron Microscopy SEM, Electron Probe Micro Analysis EPMA) were used in combination with new

The inltlal state of the alloys investigated was $he eta phase and by suitable heat treatments the different intermediate metastable phases can be produced and monitored using

The DSC analysis revealed that Ag addition modified the precipitation sequence in the investigated 6063 aluminium alloy through the formation of an additional metastable pre-?''