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ORNL-TM-5781.txt
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ORNL/TM-5781
L1 /1074
Corrosion of Several Metals in
Supercritical Steam at 538°C
H. E. McCoy
B. McNabb
TR R T LW
Printed in the United States of America. Available from
National Technical Information Service
U.S. Department of Commerce
5285 Port Royal Road, Springfield, Virginia 22161
Price: Printed Copy $4,50; Microfiche $3.00
Lo
This report was prepared as an account of work sponsored by the United States
Government. Neither the United States nor the Energy Research and Development
Administration/United States Nuclear Reguiatory Commission, nor any of their
employees, nor any of their contractors, subcontractors, or their employees, makes
any warranty, express or implied, or assumes any legal liability or responsibility for the
accuracy, completeness or usefulness of any information, apparatus, product or
process disclosed, or represents that its use would not infringe privately owned rights.
"
ORNL/TM~5781
Distribution
Category UC-76
Contract No. W?7405—eng-26
METALS AND CERAMICS DIVISION
CORROSION OF SEVERAL METALS IN SUPERCRITICAL STEAM AT 538°C
H. E. McCoy and B. McNabb
Date Published: May 1977
NOTICE
was as an u:n:tmllt.ol“Ei -&:
nsored the United States Government.
|5 umaw States mor the United States Energy
Rescarch and Development Administration, mor any of
. { theit employees, mor any of their contiactors,
¥ subcontractors, or theit employees, makes any
warranty, express or implied, or sssumes any legal
Eability or responsibility for the accuracy, completenens
of usefulnes of any information, apparatus, product or
process disclosed, or represonts that its use would mot
. | infringe privately owned rights,
OAK RIDGE NATIONAL LABORATORY
Oak Ridge, Tennessee 37830
‘operated by
UNION CARBIDE CORPORATION
- for the =y | | {MASTER
ENERGY RESEARCH AND DEVELOPMENT ADMINISTRATION .
VISTRIBUTION OF THIS DOCUMENT IS UNLIMITED
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CONTENTS
ABSTRACT . « ¢« &+ ¢ ¢ « o« ¢ o o o
INTRODUCTION . . « & « o o o « &
EXPERIMENTAL DETAILS . . . . . .
Test Facility . . . . . . .
Test Materials . . . . . .
Evaluation . . . . . . . .
Errors . . « ¢« o o ¢ ¢ o &
Experimental Observations .
Low—-Alloy Ferritic Steels .
Hastelloy N . . . . . . . .
Stainless Steels . . . . .
Other Alloys . . . « « . &
Tube Burst Results — Hastelloy N
SUMMARY . . . & ¢« ¢ &+ o & & &
ACKNOWLEDGMENTS . . « « « ¢ ¢ ¢« ¢ o &
REFERENCES . . . « . + « « « « &
APPENDIX . . . . + . . . .
iii
o O N0 N
W NN NN N ke e
W & 00 g & O ~N O
i
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i
1
LY
CORROSION OF SEVERAL METALS IN SU?ERCRITICAL STEAM AT 538°C
H. E. McCoy and B. McNabb
ABSTRACT
The corrosion of several iron- and nickel-base
alloys in supercritical steam at 24.1 MPa (3500 psi)
and 538°C has been measured to 7.92 x 107 sec (22,000 hr).
The experiments were carried out in TVA's Bull Run Steam
‘Plant. Corrosion was measured almost entirely by weight
change and visual appearance; a few samples were evaluated
by more descriptive analytical techniques. The corrosion
rates of low-alloy ferritic steels containing from 1.1 to
8.7%2 Cr and 0.5 to 1.0%Z Mo differed by less than a factor
of 2 in steam. Several modified compositions of
Hastelloy N were evaluated and found to corrode at about
equivalent rates. Of the alloys studied, the lowest
weight gain in 3.6 X 107 sec (10,000 hr) ,vas 0.01 mg/cm®
for Inconel 718 and the highest 10 mg/cm® for the low-
alloy ferritic steels.
INTRODUCTION
This study was motivated by the need of the Molten-Salt Reactor
Program for a material for use in steam generators. Hastelloy N has
excellent compatibility with molten fluoride salts, but it failed
prematurely in a simulated superheated steam environment. ' Thus,
our program emphasized Hastelloy N, but included a total of over
80 alloys, mostly iron and nickel base. Because of our program to
modify the chemical composition of Hastelloy N to obtain better
resistance to embrittlement by irradiation and the fission product
tellurium, several alloys with compositions slightly different from
that of standard Hastelloy N were included in the study.
The tests were conducted in TVA's Bull Run Steam Plant in
supercritical steam at 24.1 MPa (3500 psi) and 538°C., One test period
included test times up to 5.4 x 107 sec (15,000 hr) and the data were
reported previously. A second test period covered an additional
2,52 x 107 sec (7000 hr) on many of the same test coupons and extended
the total exposure time to 7.92 X 107 sec (22,000 hr).. Since the
Molten Salt Reactor Program has again been discontinued, the results
of the total steam corrosion will be presented in this report.
Although the discussion will deal only with alloys selected to
illustrate several important characteristics of steam corrosion,
compositions and weight changes of all materials under investigation
will be listed.
EXPERIMENTAL DETAILS
Test Facility . -
The facility used in this study is located in TVA's Bull Run
Steam Plant.? This is a coal-fired plant with a supercritical steam
cycle and a power generation capability of 980 MW. The facility is
located about 5.49 m (18 ft) upstream from the turbine. The steam
is extremely clean at this location containing less than 1 ppb O2,
less than 5 ppb Cu, less than 3 ppb Na, less than 15 ppb Si02, and
less than 6 ppb Fe. Hydrazine is added to the feed water to scavenge
oxygen, and the pH was controlled at 9.40 to 9.45 with ammonia. The
electrical conductivity of the steam condensate is usually less than
3 x 1077 Qeem l.
Although the stream was generally very pure, during at least one
1.44 x 107 sec (4000 hr) period the level of impurities was significantly
higher. During this period all specimens gained very close to
0.5 mg/cm . Bull Run engineers pointed out that several condenser
tube leaks had occurred in the previous year of operation, whereas
in earlier years, few if any condenser leaks occurred. Since the
cooling water in the condensers is at higher pressure than the
condensing steam, untreated cooling water is introduced into the
steam system hot well when a leak occurs. After replacement of
condenser tubes, most of the specimens lost weight for a brief period.
Perturbations in the weight change data due to this phenomenon will
be pointed out as the data are presented.
- A schematic of the test facility is shown in Fig. 1 and a photo-
graph of the disassembled test assembly is shown in Fig. 2. The steam
entered the 4-in.-diam sched 160 type 316 stainless steel test chamber
at a flow rate of 0.12 to 0.13 kg/sec (16 to 17 1b/min). The initial
sample holder was a cube 50.8 mm (2 in.) on each side and would
accommodate 140 samples. A second sample holder was later added
that would hold 72 specimens. Most of the samples were 12.7 mm wide
X 50.8 mm long X 0.89 mm thick (1/2 in. wide X 2 in. long X 0.035 in.
thick). Alumina washers 0.51 mm (0.020 in.) thick were placed between
the specimens before they were bolted in place. Most of the space
between the holder and the vesgsel was baffled to force flow across
the samples at about 6.10 m/s (20 fps). Ten stressed instrumented
specimens were located at the front of the chamber and four uninstru-
mented stressed specimens were located in the filter basket. The
specimen geometry was chosen so that. the stress was provided by the
force of the steam on the inner wall. The wall thickness of the .
reduced section was varied from 0.25 to 0.75 mm (O. 010 to 0.030 in.) "
to provide stresses of 531 to 193 MPa (77 to 28 x. 103 psi). The
front ten specimens had small capillary tubes that were heated by
the steam when the tube specimen failed. A thermocouple attached to
each capillary was recorded by a multipoint recorder and indicated
when failure occurred. The steam passed through .a metal filter to
ORNL~DWG 68-3995R2
| r— ol
5. STEAM SUPPLY
*— 3500 psig, 1000 °F,
1617 Ibs/min
SAMPLE VESSEL
FILTER-
- Qe MULTIPOINT
i RECORDER
~SAMPLE HOLDER
FLOW RESTRICTER REDUCED WALL
THICKNESS
-CAPILLARY
TUBE
CONDENSER
TUBE BURST SPECIMEN (TYP 10)
WATER OUT " WATER iN
Fig. 1. Sch-emati'c of Test Facility Double~Walled Tube-Burst
Specimen.
~
. - 4% Photo 224475
9y
Fig. 2. Photograph of the Steam Corrosion Chamber After 19,000 hr of
Exposure. Features to note are the stressed but uninstrumented specimens
in the filter (foreground), the two groups of unstressed specimens, and
the 10 instrumented stressed specimens. The stressed specimens have an
outside diameter of 25 mm (1 in.) and a length of 76 mm (3 in.).
trap scale before it entered the small diameter flow restrictor. The
restrictor reduced the steam pressure to near atmospheric pressure
before reaching the condenser. The condensate was returned to
condensate storage.
Test Materials
Chemical analyses of the test materials are given in Table 1.
The first six alloys were commercial production materials. Alloys
LC, MC, and NC were small melts of 2 1/4 Cr-1 Mo steel with variations
in carbon content, and alloy 72768 is a commercial heat of 2 1/4 Cr-
1 Mo steel. The other alloys down to "Hastelloy N modifications"
were commercial production heats. Heats 185 through 237 were 2-1b
laboratory melts. Hastelloy N heats 21541 through 73008 were small
50- to 100-1b melts that were vacuum melted and fabricated by
commercial vendors. Hastelloy N heats 2477, 5065, 5067, 5085, 5095,
5101, and M1566 were large commercial heats of standard Hastelloy N.
All alloys were rolled to 0.89 m (0.035 in.) thick sheet. The
rolling was done cold with intermediate anneals for softening; the
finish of the exposed sample surface was generally typical of cold-
rolled sheet. Samples were sheared, cleaned in acetone and alcohol,
and annealed in argon for 1 hr at 927°C (the low-alloy ferritic steels),
1 hr at 1038°C (the stainless steels), or 1 hr at 1177°C (all other
alloys). :
Evaluation
Generally only weight change measurements were made. However,
the samples were also examined visually for evidence of spalling,
oxide color, etc. More extensive evaluation was carried out on a
few specimens, including metallography to determine depth of oxide
‘penetration and electron microprobe scans of oxide-metal interfaces
to determine the compositions of the oxide and the metal beneath the
oxide. '
The stressed specimens were removed every 1000 hr for examination.
Measurements were made of the inside diameter of each tube with a
die test gage. In this way several points were obtained on the
strain-time plot for each specimen. Any failed specimens were
replaced before the assembly was returned to Bull Run. Some of the
failed tubes were subjected to metallographic examination. '
)
Table 1. Chemical Analyses of Test Materials
Concentration, wt X
Alloy
Ni ¥o Cr Fe Mn c si P s Cu ’ Co v v Al T B Nb o ir Other
Armco Iron® Bal 0.017 0.012 0.005 0.025
Low=-Alloy Ferritic
1.1 ¢r 0.25 0.49 1.1 Bal 0.42° 0.64 <0.05 <0.02 <0.05 <0.05 <0.02
1.9 cr 0.20 0.5 1.9 Bal 0.46 0.17
2.0 ¢r 0.32 0.8 2.0 Bal 0.40 0.25
4.2 Cr 0.36 0.47 4.2 Bal 0.40 0.35
8.7 ¢r 0.35 0.97 8.7 Bal 0.44 0.50
e 0.05 0.98 2.3 Bal 0.51 0.009 0.58 0.002 0.009
M <0.05 1.14 2.4 Bal 0.38 0.030 0.27 0.019 0.025
§C 0.21 0.91 2.2 Bal 0.44 0.120 0.40 0,010 0.015
72768 0.16 0.95 2.2 Bal 0.44 0.09 0.38 0,011 0.011
12-5-3 Maraging 12.7 2.80 5.1 Bal 06.05 0.10 0.3
Stainless Steels
Type 502° 0.5 5.0 Bal 0.1
17-7 PR 7.10 17.0 Bal 0.07 1.15
Type 201 5.23 16.55 Bal 7.28 0.076 - 0.54 0.3 0.006 0.059 N
Type 304% 8.0 18.0 Bal 0.03
Type 309: 13.5 23.0 Bal 0.2
Type 310 20.5 25.0 Bal 0.25 1.5
Type 316, 13,01 - 2.8 17.0 Bal. L.74 0.027 0.65 0.016 0.017 0,10 0.15
Type 321 10.5 18.0 Bal 0.08 0.4
Type 347% 11.0 18.0 Bal 0.98 . 0.4 0.4 Ta
Type 406 13.0 Bal 0.15 4.0
Type 410% 12.5 Bal 0.15
Type 446% 25.0 Bal 0.20 0.25 N
N1-280 Bal . 0.0002 0.002 0.003 <0.0001 0.3% 0.005 <0,00t 0.00Z <0.000L <0.000L 0.3 <0.0001 <0.0001 <0.0001
Monel™ 60.0 1.5 3.5 0.5 23
Copper 0.02 9949
Inconel 600 78.0 14.5 7.0 0.05
Inconel 601 60.5 23.0 1l4.1 0.5 0.05 0.25 0.007 1.35
Inconel 718 53.0 3.0 18.0 0.05 0.50 1.0 5.0
Incoloy 800 3l1. 20.1 46.2 0.84 0.04 0.38 0.008 0,50 0.24 0.36
Hastelloy B Bal 27.0 <0.2 5.2 0.96 0.3 0.01 0.48 0.2 <0,05 <0.01 <0.05
Hastelloy C Bal 16.0 16.0 5.8 0.75 0.48 0.01 1.2 0.1 5.0 0.2 <0.01 <0.05
Hastelloy S Bal 14.7 14.5 0.90 0.04 0.007 <0.01 0.22 0.2 0.01 B
Hastelloy W 60.0 25.0 5.0 5.5 0.08 1.0 0.30
Hastelloy X 8.6 22.0 19.0 0.64 0.60 0.02 2.0 0.05 0.5 0.2 <0.01 <0,05
Haynes Alloy 25 10.0 0.5 20.0 1.4 1.0 0.1 0.7 0.015 0.01 0.02 Bal <0.02 15.2 0.1 0.02 <0.05
Haynes Alloy 188 22.0 22.0 3.0 1.25 0.15 Bal 15.0
Rene 62 Bal 9.0 15.0 22.0 0.25 0.05 0.25 1.25 2.5 2.25 0.01
Hastelloy N
Modificacions: - .
185 Bal 11.0 5.9 3.8 0.46 0.05 0.10 <0.03 <0.1 <0.05 0.91 <0.1 0.98
186 Bal 10.0 5.4 3.5 0.45 0.05 0.09 <0.03 <0.1 0.8 0.88 <0.1 <0.05
188 Bal 13.0 7.3 4.5 0.49 0.05 0.15 <0.03 <0.1 0.95 <0.02 1.1 <0.05
231 Bal 12.0 7.0 4,2 0.03 0.05 0.12 <0.03 <0.05 <0.02 <0.05 1.3 <0,05 1.2 ¥
232 Bal 13.0 8.0 4.5 ~<0,02 0.05 0,12 <0,03 <0.05 <0,02 <0.05 1.2 <0.05
234 Bal 16.0 7.2 4.0 <0.02 0.05. 0.13 <0.03 <0.05 <0.02 <0.05 <0.1 <0.05
236 Bal 11.0 7.0 4.0 0.5 0,05 0,13 <0.03 1.0 <0,02 <0.05 <0.05 0.5
237 Bal 12.0 6.7 4.3 0.49 0,05 0.13 <0,03 <0.05 0.04 1.03 <0.1 <0.05
2477 Bal 16,2 7.0 4.2 0.055 0.057 0.047 0,008 0,006 ©0.01 0.05 <0.,01 0.03 0.02 0.03 0.0002 <0.0005 <0.001 <0.001
5065 Bal 16,5 7.1 4.0 0.55 0,07 0.58 0.005 0.00&4 0.007 0.05 0,20 0.1 <0.03 <0,01 90.001 <0.05 <0.1 <0.1
5067 Bal 17.2 7.4 4.0 0.48 ~ 0.06 0.43 0,005 0.007 0.01: 0.09 0.30 - 0.6 0.01 001 0.004
5085 Bal 17.0 7.0 1.6 0.64 0.06 . 0.65 0.004 0.003 0.01 0.15 0,20 0.07 0.05 <u.01 0.004 <0.05 <0.002
N1 5095 Bal 16.39 7.2 3.87 ° 0.5 0.07 0.68° 0.001 0.007 0.01 0.15 : 0.02 0.002
N2 5101 Bal 16.39 6.92 3.91 0.44 0.05 0.63 0.001 0.009 0.01 0.09 0.02 0.007
21541 Bal 11.6 7.3 0.04 0.16 0.05 0.017 0.001 0.002 0.01 <0.10 <0.10 1.98 0.03 0.005 0.0007 <0.005
21542 Bal 12.1 7.21 - 0.041 0.16 0.06 0.016 0.001 0.004 0.01 <0.10 <0.10 2.05 <0.10 <0.10 ©0.0005 0.96 <0.005
21543 Bal 12.4 7.31 0.038 0.08 0.05 0.019 <0,001 0.004 0.01 <0.10 <0.10 <0.10 <D.02 <0.003 0.0002 0.70 <0.005
21544 Bal 12.6 7.3 <0.10 0.13 0.06 <0.03 <0.01 0.003 0.01 <0.10 <0.10 <0.10 <0.10 <0.10 0.0005 0.44
21545 Bal 12.0 7.18 0.03% 0.29 0.05 0.015 0.001 <0.002 0.01 <0.10 <010 <0.10 0.02 0.4% - 0.00007 0.01
21546 Bal 12.3 7.29 0.046 0.16 0.05 0.009 0.001 <0.002 0.01 <0.10 <0.10 <0.10 '0.02 0.10 0.0002 0.005
21554 Bal 12.4 7.39 0.097 - 0.16 0.065 0.01 0,004 <0,002 , 0.03 0,003 0.0002 0.35
21555 Bal 12,4 7.18 ©0.065 ©0.16 0.052 0.008 0,003 <0.002 - 0.02 0.003 0.0007 0.05
M1566 Bal 16.0 7.5 5.0 0.5 - 0.06 0.5 . - .
68688 Bal 13.8 7.9 498 0.52 0,079 0.38 0.042 <0.002 0.023 0.08 0.013 0.0002 <0.05 <0.05 = <0.05
68689 Bal 13.7 7.6 4.8 0.47 0.081 0.53 0.01 <0.002 0.02. 0.075 0.36 0.0002 <0.0S <0.05 = <0.05
69344 Bal 13.0 1.4 4.0 0.5 0.109 0.5 0.001 "0.004 0.03 0.06 <0.01 <0.01 0.24 0,77 0.00001 - 1.7 <0.01 0.001
69345 Bal 13.0 7.5 4.0 0.52 0.078 0.5 0.001 0.01 0.02 0.07 <001 0.03 0.27 1.05 0.00006 <0.01 0.92 0.3
69641 Bal 13.9 6.9 0.30 0.35 -0.06 0.02 0.001 0.003 0.01 <0.03 0.02 <0.03 1.30 . 0.0001 <0.05 0.70 0.0t
69648 Bal 12.8 6.9 0.30 0.24 0.06 0.05 0.001 0.003 0.02 <0.03 0.10 <0.05 0,92 0.00008 1.95 0.08 0.02
69714 Bal 12.4 . 8,0 0.10 0.35 0.012 <0.05 0.001 0.006 90.05 ° 0,05 <001 0.01 0.17 0.80 . 0.00001 1.6 - <0.01 <0.01
10727 Bal 1.7 1.5 0.05 0.37 0.04 <0.05 0,004 0.001 <0.01 <0.01 <0.01 0.01 <0.03 2,1 0.00006 <0.1 <0,01 <0.01
70785 Bal 12.2 7.0 0.16 - 0.27 0.057 0.09 0,002 0.004 .0.02 0.03 0.003 0.003 0.14 1,1 0.002 0.097 <0.003 0.01
70786 Bal 12,2 7.2 0.41 - 0.48 0.044 0.08 0,002 0.00 0.02 0.05 0.008 0,003 0.13 0,82 0.0005 0.62 0.003 0.06
70787 Bal 12.5. 7.0 0.18 0.43 0.041 0.09 0.002 0.004 0.02 .0.05 0.003 0.003 0.17 0.9 0.0005 . o.jf 0.77 0.07
70788 Bal 12.5 7.2 0.43 0.43 0.027 0.10 0.002 0.004 - 0.02 <0.02 0.008 0.003 0.18 = 1.36 0.0004 O. 0.30 0.01
10795 Bal 13.0 7.8 0.04 0.63 0.054 0.03 <0.005 0.005 0.003 0.005 0.001 <0.005 0.06 1,49 0.002 0.005 0.42 0.017
70796 Bal 12.4 7.3 . 0.05 0.64 0.043 0.02 <0.005 0.005 0.003 0.005 0.002 <0.005 0,10 -0.04 . 0.0005 0.04 0.75 0.024
70797 Bal 12.5 7.0 0.29 9.38 0.055 0.02 <0.005 0.003 0.003 0.005 0.002 <0.005 0.07 - 0.59 0.0002 0.98 0.75 0.035
70798 Bal 12.8 1.5 0.26 0¢.53 0.038 0.02 0.002 0.005 0.003 0.005 0.003 <0.005 0.07 0.71 ©0.0001 0.9% 0.32 0.011
70835 Bal 12,1 1.8 0.68 - 0.58 - 0.053 0.05 0.00L 0.004 - 0.005 0.10 <0.01 <0.01 0.10 -0.71 0.002 2.6 <0.01 <0.005
71114 ‘Bal 12.% 7.14 0.062 0.02 0.05 0.026 0.002 0.005 0.007. 0,07 0.07 1.75 0.002 <0.03
71583 Bal 12.4 7.35 0.13 0.03 0.05 0.055 0.002 0.004 0.015 .10 0.2 1.44 - <0.03
72118 Bal 11.9 7.03 0.07 0.07 0.091 0.09 0.003 0.002 <0.001 0.72 0.2
72503 Bal 12,9 6.79 0.32 0.01 0.066 0.01 0.0008 0.002 0.1 .1.94 <0.001
72604 Bal 11.5 6.69 0.07 0.07 0.09 0.09 0.003 0.003 <0.001 0.30 0.02
73008 Bal 12.4 7.63 0.18 0.45 0.078 0.06 0.03 . 2.1. <0.003 i
gouinal co-poaitién, all others are actual analyses.
Errors
The specimens were weighed on a standard four-place balance with
an accuracy of *0.0001 g. The specimens had surface areas of 12 to
14 cm?, so the uncertainty in weight corresponded to almost 0.01 mg/cm?. . et
This error does not include small pieces of loose material that may
have been adhering to the specimen or small amounts of oxide that may
have been knocked off during disassembly. Efforts were made to minimize
these sources of error, but they are likely still present.
The stresses imposed on the tube burst specimens were affected by
- uncertainties in tube dimensions. The uncertainty in the wall thickness
was about *#0,0127 mm (#0.0005 in.). When the nominal wall thickness
was 0.254 mm (0.010 in.), this uncertainty introduced an error in the
stress of *5%. When the wall thickness was 0.762 mm (0.030 in.), this
uncertainty was about *27.
Experimental Observations
Weight gain results on all materials tested in steam are given in
the Appendix.
Low-Alloy Ferritic Steels
Five alloys containing from 1.1 to 8.7% Cr and 0.5 to 1.0% Mo
(Table 1) were exposed to steam for 14,000 hr at 538°C and these results
were presented previously2 and are shown in Table Al. These specimens
were lost during the one year in which the program was inactive, and
it was necessary to begin testing with a new group of specimens. These
specimens were exposed 7000 hr, and the data for the second series are
shown in Fig. 3 along with the scatterband for the first series. The
extremes of the scatterband for the first series were defined by alloys
containing 1.1% Cr (lowest weight gain) and 1.9% Cr (highest weight
grain). These same alloys are near the extremes for the second series,
and the data from the two series generally agree very well.
The behavior in air was vastly different from that noted in
steam. After only 1000-hr exposure all alloys except the one containing
8.7% Cr had begun to spall, and after 13,000-hr exposure all alloys
had lost weight.2
Two samples from the steam series were examined metallographically
and typical photomicrographs are shown in Fig. 4. The microstructures
of the specimen containing 1.1 and 8.7% Cr were quite similar. The .
oxide, which consists of two distinct layers had a total thickness of
about 50 pm. The microstructure of the metal surface was altered to a
depth of about 10 um. Microprobe scans of these specimens showed that
the oxide layer nearest the metal contained detectable quantities of
ORNL-DWG 76-20796
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SERIES
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= 2 A 49 0.54 —
B 2.0 0.88
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. LI |
10> 2 5 10° 2
: TIME (hr) -
Fig. 3. Influence of Chromium Content on the Weight Change of
Annealed Low-Alloy Ferritic Steels in Supercritical Steam at 538°C and
24.1 MPa (3500 psi). .
Fe, Cr, Mo, and Si with Fe and Cr being the predominant constituents.
Only iron was detected in the outermost oxide. The two alloys chosen
for metallographic examination had very similar weight gains and
gained the least weight of the series. Note in Table 1 that these
alloys were the highest in silicon and that silicon was detectable
in the oxide film. In light of these observations and previous work
that showed silicon to reduce the oxidation rate of steel »5 it is
quite likely that the higher silicon content of these two alloys
resulted in their superior corrosion resistance.
The weight changes observed with several heats of 2 1/4 Cr-1 Mo
steel are shown in Fig. 5. The scatterbands from the observations
of steels containing from 1.1 to 8.7% Cr are shown and the data for
the four heats of 2 1/4 Cr-1 Mo steel fall within the scatterbands.
The low carbon heat had the lowest oxidation rate, but we do not
know a basis for attributing this to its low carbon content. These
same alloys were exposed in the 50% cold-worked condition. The data
from these specimens are presented in Fig. 6. A comparison of
Figs. 5 and 6 shows that cold working did not have a detectable
effect on corrosion. (These data are also tabulated in Table A2.)
| Y-141199
100 200 Ml‘%%OXNS 600 700
0.005 0.010 INCHES 0.020 0.025
.20 40 60 MICRONS 120 140
500 X-
0.001 INCHES 0.005
Fig. 4. Photomicrographs of Low-Alloy Ferritic Steel Exposed to Steam at 538°C and 24,1 MPa
(3500 psi) for 7000 hr. (a) and (b) Alloy containing 1.1% Cr. (c) and (d) Alloy containing 8.7% Cr.
All specimens as polished; however, specimen shown in (c) and (d) was etched slightly by moisture
in the ambient air. "
= »
- ORNL-DWG 76-20797
20
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SERIES
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— | SEconD
SERIES
oLC
A MC
O NC
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WEIGHT CHANGE (mg/cm?)
o
N
1 — .
10> 2 5 10 2
o | "TIME (hr) |
Fig. 5. Weight Changes of Several Heats of 2 1/4 Cr-1 Mo Steel in
Solution-Annealed Condition Exposed to Supercritical Steam at 538°C and
24.1 MPa (3500 psi).
ORNL-DWG 76-20798
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Fig. 6. Weight Changes of Several Heats of 2 1/4 Cr-1 Mo Steel in
the Cold-Worked Condition Exposed to Steam at 538°C and 24.1 MPa (3500 psi).
2
iy
10
Photomicrographs of three specimens of the 2 1/4 Cr-1 Mo steel
are shown in Fig. 7. The three specimens examined were (1) standard
alloy (heat 72768), annealed and air cooled, (2) standard alloy, “
cold worked 50%, and (3) normal carbon (NC) alloy, annealed and air '
cooled. The oxides on all three specimens were very similar to each
other and to the alloys shown in Fig. 4. The oxide consisted of
two layers and had an overall thickness of about 50 yum. The specimen
underneath the oxide was affected to a depth of 10 ym or less. Electron
microprobe spectral analysis showed that the oxide on each specimen
nearest the metal contained detectable quantities of Fe, Cr, Mo, and
Si with Fe and Cr being the major constituent. The outermost oxide
layer contained only iron in detectable concentrations.
Hastelloy N
The weight changes of four heats of Hastelloy N exposed in steam
are shown in Fig. 8. The variation among the four heats is about the
same as the variation noted for duplication specimens of heat 5065,
One of the heats, 2477, was vacuum melted, and the other three were
air melted. The vacuum-melted heat was much lower in silicon and
manganese than the air-melted heats, but this had no detectable
effect on the corrosion rate in steam. After the first 4000-hr
exposure, the weight change can be described by an equation of the
form :
AW = K£°-21 (1)
where AW is the weight gain in mg/cmz, t 1s the time in hr, and X is
a constant. The perturbation in rate after 15,000 hr is thought to
be due to the condenser leaks in the plant and the attendant higher
impurity levels in the steam. After the leaks were repaired, the
rate of corrosion decreased.
Some Hastelloy N specimens from heat 5065 were given various
surface treatments before exposure to steam. Six samples were solution
annealed. Two of these were tested in the as-rolled and solution-
treated condition, two others were electropolished, and two were
abraded with 400 grit paper before exposure. Figure 9 shows that
the weight changes were least for the electropolished material, inter-
mediate for the as-rolled samples, and greatest for the abraded
samples. Although the corrosion process may have been affected in
a more complex way, the weight changes are qualitatively proportional
to the "true" surface area. | i
© e
100 200 MICRONS 600 700
4 I oox 1 i L
{
0.005 0010 INCHES 0.020 0.025
Fig. 7. Photomicrographs of 2 1/4
538°C and 24.1 MPa (3500 psi). (a) and
(c) and (d) Heat 72768, cold worked 50%.
As polished.
20 40 €0 MICRONS 120 140
500X
0.001 INCHES 0.005
Cr-1 Mo Steel Exposed 7000 hr to Supercritical Steam
(b) Heat 72768, annealed at 927°C and air cooled.
at
(e) and (f) Heat NC annealed at 927°C and air cooled.
Tt
WEIGHT CHANGE (mg/cm2)
12
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(L)
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10° 2 5 40 2
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Fig. 8. Weight Changes of Several Heats of Annealed Hastelloy N
Exposed to Supercritical Steam at 538°C and 24.1 MPa (3500 psi).
0.5
0.2
0.4
-0.02
0.01
103
ORNL -DWG 73-4135R
Fig. 9. Effect of
Surface Finish on the Corro-
sion of Hastelloy N (Heat 5065)
in Steam at 538°C and 24.1 MPa