ternary and complex rhodium alloys - platinum metals review

13
Ternary and Complex Rhodium Alloys AN INVESTIGATION OF MECHANICAL PROPERTIES By J. R. Handley Johnson Matthey, Materials Technology Division A previous study on binary alloys of rhodium has shown that the addition of small quantities of suitable alloying elements produce useful com- mercial alloys (I). It was found that certain binary alloys did not colour liquid glass, had an acceptable creep life and could be fabricated in- to products used in the production of glass fibre. At high loading and high temperatures, some binary rhodium alloys had a superior creep life to zirconia grain stabilised (ZGS) 10 per cent rhodium-platinum. Binary alloys which contain hafnium, zirconium and niobium form a protec- tive surface oxide layer which prevents metal loss by the evaporation that is normally associated with the platinum group metals. This investigation of rhodium alloys was car- ried out to see if the useful properties of binary alloys could be enhanced by the addition of fur- ther alloying elements, and if the creep life could be improved by the addition of grain boundary strengthening elements, such as carbon, or by the formation of a gamma prime precipitate or an oxidation-resistant oxide spinel. The concentration of the alloying elements us- ed in this study was generally I weight per cent, which for most alloys is below the solid solubili- ty limit, thus preventing precipitation of a second intermetallic phase. The alloys were argon arc melted and fabricated into sheets, and their stress rupture properties were determined at loadings of I 10 to 345 bar at temperatures of 1200,1300, 1400 and I~xIOC. The addition of a further alloying element to the binary alloys only produced a small increase of up to 50 Hv in the as-cast hardness of the ter- nary alloys, as shown in Table I. In the previous paper it was shown that the binary alloys con- taining scandium, holmium, zirconium and lutetium had the longest stress rupture lives of 127,99, 94 and 73 hours, respectively, at a loading of 345 bar and at a temperature of 1200~C; but the rare earth alloys had poor workability (I). The addition of tantalum or rhenium to these alloys improved their workabili- ty. The addition of tantalum and rhenium to binary alloys of the other refractory group metals, and certain other elements, improved their cold formability, as shown in Table 11. The principal mode of oxidation in the binary alloys was by grain boundary diffusion and in- ternal oxidation. The addition of a spinel oxide former, such as chromium, was made to improve the oxidation resistance of these alloys. At the lower temperature of 120o0C chromium did im- prove the oxidation resistance of binary alloys. This improvement was similar to that found in stainless steels and nickel superalloys. At the higher temperature of 140ooC, chromium no longer formed a protective oxide spinel. The ox- idation resistance of the more complex alloys was similar to that found in the binary alloys where the addition of a strong oxide former prevented rhodium evaporation. Most of the alloys reveal- ed a weight gain after oxidation, as a result of the alloying element being converted to an ox- ide, Table 111. The most resistant oxide layers formed upon the ternary alloys containing tan- talum or niobium. Glass compatibility tests carried out on binary alloys revealed that the addition of a strong ox- ide former, such as chromium or hafnium, prevented rhodium from colouring liquid glass. The effect of small additions of these elements to those binary alloys which mildly coloured glass was to prevent them from colouring liquid glass (Table 111). The addition of a third or fourth ele- ment to most of the binary alloys did not reduce the contact angle of liquid glass. Only two of the Platinum Metals Rev., 1990, 34, (4), 192-204 192

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Ternary and Complex Rhodium Alloys AN INVESTIGATION OF MECHANICAL PROPERTIES

By J. R. Handley Johnson Matthey, Materials Technology Division

A previous study on binary alloys of rhodium has shown that the addition of small quantities of suitable alloying elements produce useful com- mercial alloys (I). It was found that certain binary alloys did not colour liquid glass, had an acceptable creep life and could be fabricated in- to products used in the production of glass fibre. At high loading and high temperatures, some binary rhodium alloys had a superior creep life to zirconia grain stabilised (ZGS) 10 per cent rhodium-platinum. Binary alloys which contain hafnium, zirconium and niobium form a protec- tive surface oxide layer which prevents metal loss by the evaporation that is normally associated with the platinum group metals.

This investigation of rhodium alloys was car- ried out to see if the useful properties of binary alloys could be enhanced by the addition of fur- ther alloying elements, and if the creep life could be improved by the addition of grain boundary strengthening elements, such as carbon, or by the formation of a gamma prime precipitate or an oxidation-resistant oxide spinel.

The concentration of the alloying elements us- ed in this study was generally I weight per cent, which for most alloys is below the solid solubili- ty limit, thus preventing precipitation of a second intermetallic phase. The alloys were argon arc melted and fabricated into sheets, and their stress rupture properties were determined at loadings of I 10 to 345 bar at temperatures of 1200,1300, 1400 and I~xIOC.

The addition of a further alloying element to the binary alloys only produced a small increase of up to 50 Hv in the as-cast hardness of the ter- nary alloys, as shown in Table I. In the previous paper it was shown that the binary alloys con- taining scandium, holmium, zirconium and lutetium had the longest stress rupture lives of

127, 99, 94 and 73 hours, respectively, at a loading of 345 bar and at a temperature of 1200~C; but the rare earth alloys had poor workability (I). The addition of tantalum or rhenium to these alloys improved their workabili- ty. The addition of tantalum and rhenium to binary alloys of the other refractory group metals, and certain other elements, improved their cold formability, as shown in Table 11.

The principal mode of oxidation in the binary alloys was by grain boundary diffusion and in- ternal oxidation. The addition of a spinel oxide former, such as chromium, was made to improve the oxidation resistance of these alloys. At the lower temperature of 120o0C chromium did im- prove the oxidation resistance of binary alloys. This improvement was similar to that found in stainless steels and nickel superalloys. At the higher temperature of 140ooC, chromium no longer formed a protective oxide spinel. The ox- idation resistance of the more complex alloys was similar to that found in the binary alloys where the addition of a strong oxide former prevented rhodium evaporation. Most of the alloys reveal- ed a weight gain after oxidation, as a result of the alloying element being converted to an ox- ide, Table 111. The most resistant oxide layers formed upon the ternary alloys containing tan- talum or niobium.

Glass compatibility tests carried out on binary alloys revealed that the addition of a strong ox- ide former, such as chromium or hafnium, prevented rhodium from colouring liquid glass. The effect of small additions of these elements to those binary alloys which mildly coloured glass was to prevent them from colouring liquid glass (Table 111). The addition of a third or fourth ele- ment to most of the binary alloys did not reduce the contact angle of liquid glass. Only two of the

Platinum Metals Rev., 1990, 34, (4), 192-204 192

T.Mo I

The As-Cast Hardness of Ternary Rhodium Alloys Containing 1 Weight Per Cent Each of the Second ~

and ~ Third ~~ Elements, Compared to the Basic Binary Alloy

hardness values, Hv

Element

Al Ag Au Ca co Cr DY " Er Fe Gd " Hf" Ho Ir La Lu Mg Mn Mo Nb Nd Ni 0s Pd Pt Re Ru sc Sm Ta Tb Ti Tm v W Y Yb Zr

Binary

176 98

128 152 130 117 158 174 117 157 179 156 94

151 162 108 134 121 131 160 134 111 109 110 102 98

189 156 126 168 118 167 164 116 187 146 151 -

Cr

117

169

163 158

152 209

167

163

143

128 129

206 -

Hf"

163

179 177

166

142 159

135

199

172

150

154

149 -

Nb

137

209

161

159 168 127

165

132 131

145 136 133 119 123 125 185

279

145

141 121

161 -

Mo

152

181

142 161

121 132

176

151

128

145 145

187 -

V

128

154 197

145 141

138

128

164 121

193 -

Ta

168 114 115 153 130 163 164 194 118 160 172 173 110 164 170 143 150 151 279 159 143 104 131 109 136 120 189 161 126 142

169 138 170 189 181 172 -

Ti

143

1 50

128 145

205

118

128 122

216 -

Zr

206

149

187 161

172

216

193 164

151 - O 0 . 5 wt.% dysprosium and gadolinium; 0.3 wt.% hafnium

more complex alloys, lutetium-tantalum- metals, rare earth metals and indium produced rhodium and hafnium-rhenium-scandium- the longest stress rupture lives. MOR a series rhodium, reduced the contact angle of liquid of ternary alloys was made to determine the ef- glass to below the 3 3 O angle that occurs with fect of additions of 0.75 weight per cent niobium rhodium to 2oo and 27O, respectively. and I weight per cent tantalum to binary alloys, In the previous study it was shown that binary and the results are given in Tables IV and V.

alloys formed by the addition of refractory group These results show that the most s ignif i i t

Platinum Me& REV., 1990,34, (4) 193

Erichsen

Element Binary

Al 1 1 Ag 41 Au 45 Ca 34 co 47 Cr 29 Er 28 Fe 46 Hf" 47 Ho 33 Ir 49 Lu 33 Mn 39 Mo 41 Nb" 38 Nd 19 Ni 52 0s 36 Pd 45 Pt 56 Re 54 Ru 53 sc 8 Sm 19 Ta 43 Tb 29 Ti 30 Tm 26 v 30 w 71 Y 21 Yb 35 Zr 42

0.3 wt.% hafnium, '0.75

improvement in creep life occurred in those alloys which contained either another refractory group metal, a rare earth metal, indium or another platinum group metal. The addition of I weight per cent of osmium or iridium to a 0.75 per cent niobium-rhodium alloy increased the stress rupture life from 56 to 105 hours. The effect of osmium concentration on the 0.75 per cent niobium-rhodium alloy is seen in Table VI, which shows the optimum osmium

number of turns of a 25 mm diameter disc, depth in O.Olmm per turn

Cr Hf' Nb Mo v Ta Ti Zr

41 57 54 29 54

29 33 36 50 37 59 40 29 32 29 19

57 33 55 47 38 29 100+ 32 54 18 22 29 21 34 28

60 55 29 24 30

48 50 38 40 41 26 38 34 19 36 47 38 40 48 75+ 43 40

31 33 55 50 51 48 57 53 61

102 59 64 42 54

25

39

32

20 29 26 18 26 14

59 100+ 75+ 38 54 43 56 46

40 32 43 56 38 28

37 29 48 26 30 54 29 100+ 48 31 34 27

31 29

54 4c 19 29 46 28 42

wt.% niobium

content to be I per cent. The ternary alloys of niobium-rhodium and tantalum-rhodium which had the longest creep life were zirconium-niobium-rhodium, molybdenum- niobium-rhodium and tungsten-tantalum- rhodium of 156, 151 and 106 hours, respective- ly, at 345 bar and 1200OC.

Therefore a further series of ternary alloys in- cluding refractory group metals was made to determine which combination would produce

Platinum Metals Rev., 1990, 34, (4) 194

Table II

Cuping Tests of Rhodium Alloys Containing 1 Weight Per Cent Each of the Second and Third Elements, Compared to the

Basic Binary Alloy Erichsen number of turns of a 25 mm diameter disc, depth in O.Olmm per turn

Table 111

Glass Compactibiity Tests and Oxidation of Complex Alloys of Rhodium I Glass test Oxidation

Weight loss or weight gain, mg/cm h Contact

angle, degrees

Alloying elements at 12OOOC

- 16.2 0.0

- 18.7 1.8

-4.7 8.1

20.2 6.6

- 3.0

at 140OOC Colour

v.v.1. brown clear v.v.1. green clear clear d.. blue d. blue I. brown v.v.1. brown

-

Ag-Ta AI-Ta Au-Ta Cr-Ta Cr-Mo Co-Ta Co-Ta-W Er-Ta Fe-Ta

64 68

46

6.0

Hf-Cr Hf-Cr-Mo

Hf-Re

Hf-Ta Hf-Ti

Hf-Lu

Hf-Sc

Hf-V Hf-W Hf-Re-Mo Hf-Re-Sc Hf-Re-Ta Hf-Ta-W Hf-Cr-Mo-Ta

47

45 54 49 62

50

27 58 46 51

v.1. brown clear brown I. brown I. brown clear clear clear clear

clear clear clear

- 4.6 13.1 12.6 9.4 0.5

16.2 2.5 4.6 7.6 2.5

5.6 1.3

11.1

- 5.6

17.5

60.0

15.7

17.4

Ho-Ta Lu-Ta Mn-Ta Mo-Ta

I. brown clear clear I. blue

5.0 5.6

- 2.4 -2.5

20

81

Nb-Cr Nb-Cr-Mo Nb-Lu Nb-Mo Nb-Ni Nb-Ni-Ti N b-Re-Sc

Nb-Ta Nb-Ta-lr Nb-Ti

Nb-Sc

Nb-V

47

68 34 55 38

I. blue I. blue I. brown blue d. brown I. brown v.v.1. brown I. brown clear clear v.v.1. brown I. blue

6.1 6.1 4.0

-1.0 0.0

18.2 2.5

20.7 11.0 6.8

- 3.0 1 .o

16.6 6.1

Pd-Ta Pt-Ta Re-Ta Ru-Ta Sc-Ta Ta-W Ta-Zr V-Ta Y-Ta Zr-6

brown v.1. brown v.1. brown

clear clear clear clear v.I. brown clear

5.6

- 4.4 - 6.4

1.8 3.1

12.3 0.0 6.1

- 7.5

47 64

57

57 68 56

39.2

- 125.0

Element Contact angle, O

Glass colour

. I . very light, v.v.1. very very lig

Cr Hf 62

CI cl

Nb Pt Re sc V Ta 47 62 53 47 55 cl v.l.br v.l.gr v.l.gr v.l.bl v.l.gr

d. dark, I. light, cI clear, k brown, gr green. bl blue

Platinum Metals Rev., 1990, 34, (4) 195

A 3

Ti

V C

r M

n

Fe

23.8

23

.7

39.4

2.

9 4.

2 5.

8

Zr N

b M

o T

c R

u 15

6.5

56.2

15

1.9

54.8

7.

3 9.

1 12

.6

3.7

Hf'

Ta

w

Re

0s

64

.2

98.6

76

.2

20.3

10

4.6

8.8

13.0

6.

3 0.

6 10

.0

Pr

Nd

Pm

Sm

Eu

Tab

le I

V

Stre

ss R

uptu

re L

ivea

of

Ter

nary

Allo

ys o

f R

hodi

um-0

.75

wt.%

, N

iobi

um C

onta

inin

g 1

Wei

ght P

er C

ent

of t

he

Thi

rd E

lem

ent a

t a

Loa

ding

of

345

bar

and

at T

empe

ratu

res o

f 12

0OO

C (

up

per

) and

140

0°C

(low

er)

time

to f

ailu

re, hours

co

N

i c

u

Zn

Ga

Ge

As

Se

50.7

39

.8

2.1

3.4

Rh

Pd

Ag

Cd

In

Sn

Sb

Te

56.2

22

.9

12.0

10

0 9.

1 4.

6 4.

9 10

.4

Ir P

t A

u H

g T

I Pb

B

i Po

10

5.6

48.8

38

.1

6.9

6.9

5.5

Gd

Tb

DV

Ho

Er

Tm

Y

b Lu

30

.1

31

.O

85.5

3.

7 2.

4 11

.2

103.

3 C

a 1 sc9.5

Mg

18

.5

2.4

Ca 27.5

Sr

Ba 92

.9

7.2

Ce

Al

Si

P

S

19.7

1.

8 sc

T

i V

C

r M

n

Fe

co

N

i c

u

Zn

Ga

Ge

As

Se

97.5

35

.9

100

35.9

20

.9

35.9

27

.4

32.0

17

.1

6.8

3.9

6.5

1.9

5.1

1.5

2.1

2.6

4.7

Y Zr

N

b'

Mo

Tc

Ru

Rh

Pd

Ag

Cd

In

Sn

Sb

Te

37.8

37

.5

98.6

57

.5

22.6

46

.5

24.0

26

.5

93.6

3.

7 1.

4 13

.0

7.1

9.3

6.2

1.6

3.6

82.9

46

.5

106.

6 55

.5

34.8

24

.3

20.9

9.

0 17

.2

6.2

7.5

6.7

0.7

4.3

2.2

0.7

La

Hf'

Ta

W

Re

0s

Ir P

t A

u H

g TI

Pb

B

i Po

Ce

Pr

Nd

Pm

Sm

Eu

G

d T

b DY

H

o Er

T

m

Yb

Lu

27.9

13

.0

42.6

32

.5

123.

8 15

.4

1.1

40.2

0.

2 0.

8 2.

3 5.

6 6.

5 0.

05

'0.3

wt.

% h

afni

um.

0.7

5 w

t.%

nio

bium

Table

V S

tres

s R

uptu

re Lives o

f T

erna

ry A

lloys

of Rhodium

Con

tain

ing

1 W

eigh

t P

er C

ent

Tan

talu

m a

nd 1

Wei

ght

Per

Cen

t of

the

Thi

rd E

lem

ent

at a L

oadi

ng o

f 34

5 bar and

at T

empe

rata

res

of 1

20O

OC

(up

per)

and

140

0OC

(low

er)

time

to f

ailu

re, h

ours

196 Pbtimcm Metals Rev., 1990, 34, (4) 196

the longest creep life, and the results are seen in Table VII. This shows that some of the strongest alloys are produced from combinations of elements on the same line of the Periodic Table (zirconium/niobium/molybdenum and haf- nium/tantalum/tungsten). Two of these alloys, 0.75 per cent niobium-1 per cent zirconium and 0.75 per cent niobium-1 per cent molybdenum, had a longer stress rupture life than a cobalt- based superalloy at a loading of 345 bar and at a temperature of 1z0o~C.

The effect of the addition of a refractory group metal on the stress rupture properties of the

Alloying elements, Temperature, Element weight per cent OC

binary alloys of scandium, holmium, erbium and lutetium is seen in Table VIII. This shows that most refractory group metals reduced the stress rupture life of these rare earth-containing alloys. However, the addition of hafnium to lutetium- rhodium, chromium to scandium-rhodium and tantalum to erbium-rhodium, increased the stress rupture life compared to that of the binary alloys, while only chromium improved the formability. The effect of the addition of osmium, iridium

. and rhenium upon the stress rupture properties of ternary alloys is given in Table IX. Of these elements, the addition of osmium and rhenium

Concentration, weight per cent

l % C r l % V

0.75% Nb 1% Ag

0.75% Nb 1% Er

0.75% Nb 1% 0 s

I

C 0.0 0.01

1200 32.4 27.7 1400 1.7 1.2

C 0.0 0.01

1200 12.0 48.2 1400 4.9 9.2

C 0.0 0.01

1200 31.0 29.6 1400 2.4

C 0.0 0.01

1200 104.6 35.6 1400 10.0 4.7

1% Ti 1% Mo

1% Ti 1% Zr

0.75% Nb

1% Ti 1% Cr

C 0.0 0.01

1200 43.5 33.8 1400 6.0 4.8

C 0.0 0.02

1200 83.4 27.9

0 s 0.0 0.5

1200 56.2 46.0 1400 16.6 10.6

1200 1400

1 .o 104.6

10.0

2.0

21.0 2.0 -

Platinum Metak Rev., 1990, 34, (4) 197

Table V I

Effect of Carbon and Osmium Concentrations on the Stress Rupture Properties of Ternary Alloys of Rhodium at a Loading of 345 bar

34.2 1.7

29.2 4.0

c I 0.0 1 0.01

~~~

Table VII

Stress Rupture Properties of Ternary Alloys of Rhodium and the Refractory Group Metals at a Loading of 345 bar

1% Ti

40.9 3.8

83.4 9.6

27.5 6.5

39.8 4.7

23.5 2.9

35.9 3.9

Element, weight per cent

1% 0.3% 1% Zr Hf V

83.4 27.5 39.8 9.6 6.5 4.7

94.4 58.7 52.2 4.1 4.6 5.8

58.7 49.8 53.8 4.6 3.9 10.5

52.2 53.8 47.2 5.8 10.5 5.7

153.5 62.4 23.7 7.3 8.8 4.2

37.5 82.9 100.0 1.4 17.2 6.5

1% Ti

1% Zr

0.3% Hf

1% v

0.75% Nb

1% Ta

1% Cr

1% Mo

1%W

Temper- ature,

O C

1200 1 400

1200 1400

1200 1400

1200 1400

1200 1400

1200 1400

1200 1400

1200 1400

1200 1400

Time to failure, hours '

34.2 46.9 50.7 32.6

2.41 fl 1 1.7 1 3.6

43.5 55.9 75.6 28.0 6.0 4.5 4.2

5.7 34.9 48.5 10.5 2.4 4.3 1.1

produced the most significant improvements in the stress rupture life of these ternary alloys.

The effects of the addition of non-metallic elements carbon, boron, phosphorus, sulphur and silicon on the creep lives of 0.75 per cent niobium-rhodium and I per cent zirconium- rhodium alloys are seen in Table X. This shows that even at low concentrations these elements can substantially reduce the stress rupture life achieved by the binary rhodium alloys. A similar result produced by small additions of carbon to other ternary alloys is given in Table VI. Very low concentrations of carbon in alloys which con- tain a strong carbide forming element, such as

niobium, improved the stress rupture life; but at higher concentrations the stress rupture life was decreased.

The effect of loading upon the creep life of complex alloys is seen in Table XI. The addi- tion of 0.75 per cent niobium to 0.1 per cent silicon-rhodium alloy at a loading of I 10 bar at 12m°C reduced the stress rupture life from 2147 to 2045 hours. Most of the alloy additions to the binary niobium-rhodium alloys substantially reduced the stress rupture life, at the loading of I IO bar at 12moC, from 1919 hours. Only one alloy, the 0.3 per cent hafnium-1 per cent zirconium-rhodium, produced a significant

Platinum Metah Rev., 1990, 34, (4) 198

Table VII

Stress Rupture Properties of Ternary Alloys of Rhodium and the Refractory Group Metals at a Loading of 345 bar

0.3% Hf

1% v

0.75% Nb

1% Ta

1% Cr

1% Mo

1 % W

1200 1400

1200 1400

1200 1400

1200 1400

1200 1400

1200 1400

1200 1400

Temper- ature,

Element, weight per cent

1% Ti

Time to failure, hours

1% Ti

1% Zr

0.3% Hf

1% V

).75% Nb

1% Ta

1% Cr

1% Mo

1% W

40.9 3.8

83.4 9.6

27.5 6.5

39.8 4.7

- 52.2

5.8

23.5 2.9

35.9 3.9

34.2 1.7

43.5 6.0

5.7 2.4 I 1400

I I

83.4 9.6

94.4 4.1

58.7 4.6

153.5 7.3

37.5 1.4

46.9 2.4

55.9 4.5

34.9 4.3

27.5 6.5

58.7 4.6

49.8 3.9

53.8 10.5

62.4 8.8

82.9 17.2

50.7 2.1

75.6 6.6

48.5 3.8

39.8 4.7

23.5 2.9

35.9 3.9

34.2 1.7

43.5 6.0

5.7 2.4

~

~

~

~

-

-

52.2 5.8

153.5 7.3

-

53.8 10.5

62.4 8.8

-

47.2 5.7

23.7 4.2

-

23.7 4.2

56.2 9.1

-

100.0 6.5

98.6 13.0

46.5 6.2

-

-

32.6 3.6

39.4 5.8

~

28.0 4.2

151.9 12.6

-

10.5 1.1

76.2 6.3

37.5 1.4

82.9 17.2

100.0 6.5

98.6 13.0

39.4 -

5.8

35.5 1.9

28.0 2.1

75.5 2.1

10.2 0.2

-

__

~

-

57.1 7.1

75.5 2.1

-

106.6 7.5

46.9 2.4

50.7 2.1

32.6 3.6

35.9 1.9

10.2 0.2

55.9 4.5

34.9 4.3

-

-

75.6 6.6

48.5 3.8

-

-

28.0 4.2

10.5 1.1

~

-

151.9 12.6

76.2 6.3

-

-

57.1 7.1

106.6 7.5

~

-

42.7 2.8

18.3 0.1

-

-

18.3 0.1

11.1 0.3 -

increase in the stress rupture life compared with that of the binary rhodium alloys containing haf- nium or zirconium, at a loading of I 10 bar and a temperature of 120oOC. Lives were increased from 869 and 677 hours to 1565 hours, respec- tively. The stress rupture results show that at high loadings the addition of a third element im- proves the creep life, but at lower loadings a fur- ther alloy addition makes no significant improvement. This lack of improvement in creep properties is due to the fact that the alloy addi- tion does not prevent the oxygen diffusion which produces large oxide particles, which then act as crack initiators.

It was found that the ternary alloy 0.75 per cent niobium-1 per cent of tantalum-rhodium could be used as a welding rod for rhodium alloys. Stress rupture results obtained from welded rhodium alloys of niobium-tantalum, hafnium- vanadium and hafnium-titanium at I 10 bar and a temperature of 120oOC gave lives of 792,1919 and 869 hours, respectively. This ternary alloy was used to weld fabricated rhodium spinner baskets.

Some alloys were made which contaiued a gam- ma prime precipitate, of either Ni,Ti or Nb,Ti, in order to determine their effect upon stress rup- ture properties. The results revealed that at 345 bar and a temperature of 120ooC, the gamma prime precipitates produced only a small increase in the stress rupture life of 51 hours for 3 per cent nickel-titanium-rhodium and 48 hours for 3 per cent niobium-titanium-rhodium, when compared to the values of 21 , 34, and 41 hours for the binary alloys of nickel-rhodium, niobium- rhodium and titanium-rhodium, respectively.

Other possible hardening ternary alloys were investigated. The addition of cobalt to a tungsten-rhodium alloy increased the stress rup- ture life from I I to 85 hours, at a loading of 345 bar and at 120ooC. The addition of gallium and indium, which are used to harden platinum, reduced the stress rupture life of indium- rhodium from 40 to 16 hours, at 345 bar and I200OC.

The formation of an oxide spinel used to pro- tect the low alloy steels of chromium, and molybdenum, together with the strong oxide

:? - 7

$ 6 ? t c c c

:: m

-I-

m 0 6

Platinum Metals Rev., 1990,34, (4) 199

Tem

pera

ture

, O

C

Ele

men

t, w

eigh

t pe

r ce

nt

1.0%

sc

1200

14

00

1.0%

Ho

1200

14

00

1.0%

Er

1200

14

00

1.0%

Lu

1 200

1400

Tim

e to

failu

re,

hour

s

1%

1%

1%

1%

1%

1%

0.3%

1%

0.

75%

1%

1%

1%

1%

S

c H

o Er

Lu

T

i Zr

H

f V

N

b Ta

C

r M

o W

127.

5 93

.8

66.1

10

3.3

97.5

13

6.8

72.0

5.

2 4.

1 5.

3 9.

5 6.

8 2.

7 9.

3

99.8

15

.2

24.8

30

.1

32.5

11

.7

17.0

2.

6 6.

1 1.

1 3.

7 2.

3 1.

4 1.

0

52.9

31

.0

123.

8 43

.6

16.2

2.

4 5.

6 1.

9 1.

4 4.

35

72.9

16

5.5

85.5

40

.2

1.5

0.6

11.8

Tabl

e V

lll

Str

ess

Rup

ture

Pro

per

ties

of

Ter

nary

Alloys

of Rhodium w

ith

Rar

e Earths a

nd R

efra

ctor

y M

etal

s at

a Loading o

f 34

5 ba

r

Ternary Alloy Complex Alloy

Table IX

Stress Rupture Lives of Complex Alloys of Rhodium at a Loading of 345 bar I Temperature, OC Alloying

elements Temperature, OC Alloying

elements

Cr Ho Cr Sc Cr Sc Co Ta Er Mo

Hf Ho Hf Ti Hf Ti Hf Nb Hf Mo Hf V Hf Zr Hf Sc Hf Ta Hf Ta

Ho Mo Ni Ta

Nb Cr Nb Ta Nb Ti Nb Lu Nb V

Mo Zr Mo Sc Mo V Sc Ti Y Ta Hf Cr Mo

1200 1400

31.1 48.0 1.4

85.1 22.9

1.7

2.4 4.4 1.8

136.8 2.7 27.4 16.2 1.3 Mo Re

46.3 92.0 26.3

137.6 99.9 32.2

135.8 87.7

163.7 50.7

15.2 27.5 27.5 62.4 75.6 53.8 58.7 66.1 82.9 82.9

6.1 6.5 6.5 8.8 6.6

10.5 4.6 5.2

17.2 17.2

Hf Ho Re Hf Ti Ir Hf Ti 0 s Hf Nb 0 s Hf Mo Re Hf V 0 s Hf Zr 0 s Hf Sc Re Hf Ta Re Hf Ta W

7.3 7.0

21.2 3.8 5.8

5.0 4.2

~~

39.2 51.4

22.0 92.4 15.0 40.6 43.7

1.1 3.0

17.0 32.0

1 .o 2.6

Ho Mo Re Ni" Ti Ta

Nb Cr 0 s Nb Ta Ir Nb Ni Ti Nb Lu 0 s Nb V 0 s

39.4 79.5 23.5 85.5 23.7

~

5.8 8.0 2.9

11.8 4.2

4.3 16.2 3.1 4.8 5.4

88.2 89.2

2.7 111.0 61.1

156.4

4.2 4.5 1.9

5.9

55.7 72.0 28.0 93.8 37.8 18.1

4.5 9.3 4.2 4.1 3.7 1.1

Mo Zr 0 s Mo Sc Re Mo V Re Sc Ti 0 s Y Ta Ir Hf Cr Mo Ta

'3 wt.% nickel-1 wt.% titanium and 0.75 wt.% niobium

formers, hafnium and tantalum, produced one of the longest lives of 156 hours, when tested at a loading of 345 bars and at 120o0C.

Discussion Studies of nickel and cobalt superalloys have

shown that the presence of low levels of non- metallic elements can significantly reduce the

stress rupture lives of these alloys (2). The pre- sent investigation has shown that small additions of boron, carbon, phosphorus, sulphur and silicon to a 0.75 weight per cent niobium- rhodium alloy all reduce the stress rupture life of the binary alloy, see Figure I. This effect was also found in a I weight per cent zirconium- rhodium alloy, and in other ternary alloys. At

Platinum Metals Rev., 1990, 34, (4) 200

Table IX

Stress Rupture Lives of Complex Alloys of Rhodium at a Loading of 345 bar I Stress rupture lives, hours I

Ternary Alloy Complex Alloy

Temperature, OC Alloying elements

~ ~~

Temperature, "C Alloying elements 1200

11.7 136.8 136.8 27.4 16.2

15.2 27.5 27.5 62.4 75.6 53.8 58.7 66.1 82.9 82.9

17.0 32.0

39.4 79.5 23.5 85.5 23.7

55.7 72.0 28.0 93.8 37.8 18.1 -

1400 1200 1400

Cr Ho Cr Sc Cr Sc Co Ta Er Mo

1.4 2.7 2.7 2.1 1.3

Cr Ho 0 s Cr Sc 0 s Cr Sc Re Co Ta W Er Mo Re

Hf Ho Re Hf Ti Ir Hf Ti 0 s Hf Nb 0 s Hf Mo Re Hf V 0 s Hf Zr 0 s Hf Sc Re Hf Ta Re Hf Ta W

31.1 48.0 1.4

85.1 22.9

46.3 92.0 26.3

137.6 99.9 32.2

135.8 87.7

163.7 50.7

1.7

2.4 4.4 1.8

Hf Ho Hf Ti Hf Ti Hf Nb Hf Mo Hf V Hf Zr Hf Sc Hf Ta Hf Ta

6.1 6.5 6.5 8.8 6.6

10.5 4.6 5.2

17.2 17.2

7.3 7.0

21.2 3.8 5.8

5.0 4.2

Ho Mo Ni Ta

1 .o 2.6

Ho Mo Re Ni" Ti Ta

39.2 51.4

1.1 3.0

Nb Cr Nb Ta Nb Ti Nb Lu Nb V

5.8 8.0 2.9

11.8 4.2

Nb Cr 0 s Nb Ta Ir Nb Ni Ti Nb Lu 0 s Nb V 0 s

22.0 92.4 15.0 40.6 43.7

4.3 16.2 3.1 4.8 5.4

Mo Zr Mo Sc Mo V Sc Ti Y Ta Hf Cr Mo

4.5 9.3 4.2 4.1 3.7 1.1

Mo Zr 0 s Mo Sc Re Mo V Re Sc Ti 0 s Y Ta Ir Hf Cr Mo Ta

88.2 89.2

2.7 111.0 61.1

156.4

4.2 4.5 1.9

5.9

ill alloy additions contain 1 wt.% of element, except 0.3 wt.% hafnium, '3 wt.% nickel-1 wt.% titanium and 0.75 wt.% niobium

very low levels of carbon, alloys which form very stable carbides, such as niobium, revealed an in- creased stress rupture life at 345 bar and at 1200OC. This improvement in stress rupture life may be due to the formation of fine particles of NbC which increased the grain boundary cohe-

sion. A similar improvement is found in the stress rupture properties of nickel supedoys with low carbon content. Studies of nickel superalloys have shown that the carbon increases the grain boundary adhesion, but at higher concentrations of carbon it forms large carbides at the grain

Temperature, OC

Effect of Non.

Element

0.75% Nb

1% Zr

Alloying Concentration of nonmetallic element, element weight per cent

Table x .metallic Element Concentration on the Stress of Binary Rhodium Alloys at a Loading of 345

B

Table x Effect of Non-metallic Element Concentration on the Stress

Element

0.75% Nb

1% Zr

Stress rupture life, hours

0.0 0.02 0.05 0.1 I I I

bar

1200 1400

56.2 21.2 9.1 0.8

1200 1400

56.2 69.3 21.5 7.9 9.1 6.3 4.3 1 .o

I C I 0.0 I 0.02 I 0.05 I 0.1

1200 1 400

I I I I I 1 I

P 0.0 0.02 0.05 0.1

56.2 38.0 11.6 9.1 4.8 2.1

Si 0.0 0.02 0.05 0.1

I S I 0.0 I 0.02 I 0.05 I 0.1

1200 1400

I I I I

56.2 48.3 9.1 5.0

0 0.0 0.1

1200 1400

1200 1400

1200 1400

94.4 39.9 4.1 5.4

C 0.0 0.01

94.4 47.1 4.1 . 6.3

Si 0.0 0.1

94.4 61.4 4.1 3.8

Plotinurn Metak Rev., 1990,34, (4) 201

Table x Effect of Non-metallic Element Concentration on the Stress

Rupture Properties of Binary Rhodium Alloys at a Loading of 345 bar

B

C

P

S

Element

0.0

56.2 9.1

0.0

56.2 9.1

0.0

56.2 9.1

0.0

56.2 9.1

0.75% Nb

1% Zr

0.02

0.02

69.3 6.3

0.02

0.02

Temperature, OC

0.05 0.1

21.2 0.8

0.05 0.1

21.5 7.9 4.3 1 .o

0.05 0.1

38.0 11.6 4.8 2.1

0.05 0.1

1200 1400

0.02

0.01

47.1 6.3

1200 1400

29.0 22.6 3.2 2.8

0.05 0.1

48.3 5.0

0.1

39.9 5.4

0.1

61.4 3.8

1200 1 400

0

C

Si

1200 1 400

0.0

94.4 4.1

0.0

94.4 4.1

0.0

94.4 4.1

1200 1400

1200 1400

1200 1400

1200 1400

Alloying Concentration of nonmetallic element, element weight per cent

Stress rupture life, hours

I 56.2 9.1

P P

0.3%

Hf

1%

Zr

12

00

15

65.5

5.

2 2

5

58.7

6.

5 3

0

13

00

24

2.3

6.5

45

0.

3% H

f 1

% Mo 1

% R

e 1

20

0

665.

1 2.

6 1

5

99.9

3.

9 8

0

14

00

44

.6

5.2

85

21

.2

9.2

50

15

00

18

.1

2.6

65

0.75

% N

b 1%

Cr

14

00

66

.3

1.3

35

5.

8 6.

6 8

0

0.75

% N

b 2.

0% 0

s

12

00

51

4.9

5.2

90

25

.1

5.2

15

5

0.75

% N

b 1%

Mo

~ 1

40

0

276.

4 1

.3

20

12

.6

9.2

11

0

0.75

% N

b 0.

1% S

i 12

00

2045

.0

3.9

2

5

48.3

6.

3 1

10

0.

75%

Nb

1%

Sc

12

00

86

.4

3.9

30

5.

2 9.

2 3

0

0.75

% N

b 1

% T

a 1

20

0

787.

6 9.

2 5

188.

6 11

.8

45

79.5

11

.8

10

5

1300

66

1 .O

7.

9 50

16

8.6

10.5

55

24

.6

13

.1

45

1

40

0

291.

8 3.

9 50

54

.6

6.6

1 00

8.0

11.8

1

40

1%

Mo 1

% T

i 1

20

0

901.

8 6.

5 4

5

43.5

2.

6 1

00

1%

V 1

% Z

r 1

20

0

829.

4 3.

9 3

5

52.2

2.

6 4

0

1% V

1%

Zr

0.01

% C

1

20

0

444.

3 6.

5 10

62

.1

7.8

20

. 15

00

103.

0 6.

6 7

0

Ben

d Te

st a

roun

d a

5mm

rad

ius

- W \o 0 y ,-.

v

P

N

0

N

Load

inq,

bar

Allo

ying

ele

men

ts

Tem

pera

ture

, OC

1%

Er

0.75% Nb

1200

1% Cr 1

% V

-1 200

~~ I

Tim

e to f

ailu

re,

hour

s 110

207

34

5

SR

L pe

r ce

nt

degr

ees

SRL

per

cen

t de

gree

s SR

L pe

r ce

nt

degr

ees

896.2

5.2

30

31 .O

7.8

5

462.4

6.5

20

32.6

7.8

130

Ben

d B

end

Ben

d E

long

atio

n,

angl

e,

Elo

ngat

ion,

an

gle,

E

long

atio

n,

angl

e,

Tab

le X

I

Str

ess

Rup

ture

Pro

per

ties

of

Rho

dium

Allo

ys a

t L

oadi

ngs

of 1

10, 2

07 a

nd 3

45 b

ar

Platinum Metals Reu., 1990, 34, (4)

-- I

0.02 0 6 4 0.06 0 08 0 . i O

CONCENTRATION, weight per cent

Fig. 1 Variations in the stress rupture life of 0.75 weight per cent niobium-rhodium alloys with various concentrations of the third, non-metallic constituent at a test temperature of 120OOC and a loading of 345 bar

boundaries which act as crack initiators pro- moting premature failure. In addition, at high temperature these elements are readily oxidised to volatile gases which form voids, which then cause rapid failure.

The results of th is investigation show that ad- ditions of non-metallic elements have a deleterious effect upon the high temperature pro- perties of rhodium, and this effect may occur in other platinum group metals or alloys. The use of electron beam melting makes it possible to produce alloys with a lower non-metallic content than can be achieved by conventional melting techniques. The use of such equipment for melting platinum group metals and their alloys for high temperature applications will reduce the concentration level of non-metallic elements, and hence may improve their high temperature pro- perties.

The superior stress rupture lives of binary and ternary rhodium alloys which contain additions of one or more refractory group metals can be explained by the Lewis acid based stabilisation theory. If this theory is applied to the formation of oxides (3) in rhodium alloys and those rhodium alloys which contain other platinum group metals, it can explain the improvement in the stress rupture properties of dilute solutions of refractory group metals in binary and ternary alloys. It shows that the improvement in creep

strength of ternary alloys of refractory group metals is produced by the large binding energies of the AB compounds between these metals. Metals from Groups I11 and IVY such as scan- dium and zirconium, produce the largest bindmg energies with rhodium, and also in ternary alloys containing these elements. The effect of the ad- dition of a second platinum group metal, such as iridium or osmium, is to promote the forma- tion of even more stable AB compounds, such as IrHf, and ZrIr 3 . Also the theory predicts ex- tremely strong bondmg of osmium with hafnium, niobium and zirconium; and in those ternary and quaternary alloys of rhodium which contain com- binations of two or more of these refractory group metals with osmium some of the longest lives at 345 bar at IZOO~C occurred.

At high loadings the creep properties of cer- tain rhodium alloys are superior to those of ZGS platinum, ZGS 10 per cent rhodium-platinum, nickel and cobalt superalloys. At loadings of 345 bar the principle mode of failure is by slip, which is easily made more difficult by internal oxida- tion of refractory group metals to a fine disper- sion of oxides. At a lower loading of IIO bar failure is initiated by grain boundary sliding and cavitation. Under these conditions the easy dif- fusion of oxygen along the grain boundaries of rhodium alloys promotes the formation of large oxide particles. These large oxides prevent dynamic recovery and act as crack initiators pro- moting rapid failure of the alloys. Under condi- tions of low stress this investigation could not find any rhodium alloys which had longer stress rupture lives than ZGS platinum or nickel and cobalt superalloys.

Conclusions The addition of one or more elements to binary

alloys of rhodium can improve the properties of the b i m q alloys. The formation of a stable pro- tective oxide coat can prevent liquid glass from being coloured. The inherent grain boundary weakness of rhodium will limit its usefulness as a high temperature material. The presence of small additions of non-metallic elements significantly reduced the stress rupture life of rhodium alloys. The longest creep lives in

Platinum Metals Rev., 1990, 34, (4) 203

rhodium based alloys were obtained from alloys containing mixtures of either refractory group metals, or rare earths and refractory group

tion of osmium or iridium.

References I J. R. Handley, Platinum Metals Rev. , 1989, 33,

2 J. J. debrbadillo, Trans. A I M E , 1983, 14A, 329 (’), ‘4

metal, or group l”letal with the addi- 3 J. K, Gibson, L. Brewer and K. A. Gingerich, Trans. AZME, 1984, 15A, 2075

A Review of Cathodically Modified Alloys The beneficial effects conferred on base

metals and their alloys by s m a l l additions of the platinum group metals have been reported here frequently. In recent issues, for example, the literature on the enhancement of corrosion resistance in stainless steels has been reviewed (I , 2); and that on amorphous chromium alloys (3) and surface-implanted titanium alloys has also been reported (4).

The platinum group metals enhance the cor- rosion resistance of such alloys in corrosive media by modifying the cathodic reaction, and this has led to the description “cathodically modified alloys”.

Now, an extensive review of the literature on base metals cathodically modified with noble metals has been published (5). This report surveys the literature on chromium, stainless steels and titanium. The author claims that it is the first comprehensive review of the subject which, he considers, has been neglected as a topic in recent years-the only active groups be- ing Professor Tomashov’s team in the U.S.S.R. Academy of Sciences, Moscow and Dr. Higgin- son and his co-workers at Mintek.

Several studies have been made on the effect of small additions of platinum group metals to chromium in both oxidising and reducing acids. In reducing conditions, platinum group metal modified alloys self passivate easily and their corrosion resistance is several orders of magnitude higher than that of pure chromium. The effectiveness of the platinum group metals is as follows: platinum>palladium>iridium >rutheniumhsmium. During the period of ac- tive dissolution that precedes the onset of passivation, an enrichment of the platinum group metals occurs at the alloy surface. The work carried out on stainless steels in

reducing acids shows that platinum group metal additions are more beneficial to ferritic steels than to austenitic steels, and that their ef- fect is enhanced with increasing chromium con- tent of the steel. When molybdenum is also present, there is a synergistic effect with the platinum group metal addition.

More economic use of the platinum group metals through surface alloying, rather than by

bulk alloying, favourably influences the com- mercial viability of cathodically alloyed steels.

In contrast, the alloying of titanium with platinum group metals has been shown to be beneficial in both oxidising and reducing media. Palladium has been the most studied ad- dition, and the research has led to the develop- ment of the widely used commercial titanium-0.2 per cent palladium alloy which is particularly suited to service in reducing condi- tions. Surface alloying by, for example, ion- implantation with palladium or platinum is also effective in conferring enhanced corrosion resistance as well as certain mechanical proper- ties, such as fatigue. C.W.C.

References I I. R. McGill, Platinum Metals Rev., 1 ~ , 3 4 , (z), 85 2 I. R. McGill, ibid., 1990, 34, (3), 14 3 C.W.C., Platinum Metals Rev., 1 9 , 34, f2), 84 4 IAnon.1 Platinum Metals Rev., 1990, 34, (z), 97 5 J. H. Potgieter, Report M397, Mintek, Randberg,

Oxidation-Resistant Alloys Tungsten and molybdenum possess high

melting points and good mechanical strengths at elevated temperatures, but even at moderate temperatures both oxidise rapidly. Previous studies have shown that tungsten-chromium- palladium alloys have remarkable oxidation resistance when heated in air, and different mechanisms have been proposed to explain the advantageous action of the palladium.

A recent investigation of the oxidation mechanism and of the characteristics of this alloy system, and of some quaternary alloys produced by substituting large amounts of molybdenum for some of the tungsten, has now been reported (D.-B. Lee and G. Simkovich, J. Less-Common Met., 1990, 163, (I), 51-62).

Between 1000 and 125ooC, the oxidation resistance of the alloys increases with temperature, the molybdenum-containing alloys being the more resistant. The palladium enhances the formation of a protective chromic oxide scale, acts as a reservoir for chromium, facilitates the outward movement of chromium and prevents oxygen diffusing inwards.

January 1990, 13pp, ISBN 0-86999-876-5

Platinum Metals Rev. , 1990, 34, (4) 204

rhodium based alloys were obtained from alloys containing mixtures of either refractory group metals, or rare earths and refractory group metal, or refractory group metal with the addi- tion of osmium or iridium.