3.1. Pre-test in the lab
3.1.1. Chemical compositions
Table 4 lists the chemical compositions, requirements and the measured results of the tested
tubes. The concentrations of elements in the alloys of the three types of tubes were
consistent with code requirements. For T11 and T22, the concentrations of C, P, and
S were very close to the imported values, while Cr elements were slightly higher (0.2%),
with a very small amount of Nb and Al elements. There was a similar trend for the
T91 tubes, in which Cr was 0.36% high than in the imported tube.
3.1.2. Hardness and tensile strength
Table 5 lists the microhardness and tensile strength requirements, and the measurement results
for the test tubes. It can be seen that all of the hardness values of the locally
developed tubes were within the code requirements. T11 and T22 had a very similar
hardness, of 152~157 HV, and the locally developed tube was about 20 HV higher than
that of the imported tube. Moreover, the hardness of the locally developed T91 was
14 HV higher than the imported tube. The I/N ratio is also shown in the Table, and
it is clear that the hardness of the locally developed tube was the same level as
the imported one.
Room temperature (RT) and high temperature (HT) tensile properties were measured,
as shown in Table 5. The temperature for T11 and T22 was 500 °C, while for T91 it was 550 °C. For the
T11 tubes, the RT tensile properties were within the code requirements. At RT, the
yield strength (YS) and tensile strength (TS) of the ILJIN tubes were 20 MPa higher
and 18 MPa lower than those of the NSSMC tube, respectively. At 500 °C, the YS and
TS of the ILJIN tubes were 22 MPa lower and 22 MPa higher than that of the NSSMC tube,
respectively. The elongation (e) of the ILJIN and NSSMC tubes was almost the same
at both RT and HT. For the T22 tubes, the YS and TS of the ILJIN tubes were higher
than that of the NSSMC tube both at RT and HT, and the YS was as high as 91 MPa at
RT. This was probably due to the slightly higher Cr concentration and finer grain
size of the ILJIN tubes.
For the T91 tubes, the YS and TS of the ILJIN tubes were 12 MPa lower and 39 MPa higher
than those of the NSSMC tube at RT, respectively. The YS was 10 MPa lower than that
of the imported one at HT. The I/N ratio of the tubes’ tensile properties are also
given in the table. Most of the values were over 91%, which suggests that the locally
developed tubes had the same levels of tensile properties as the imported tube, and
in the case of T22, had even better properties than the imported tube.
3.1.3. Creep strength
Determining the creep strength of boiler tubes is a key way to evaluate the properties
of their material during high temperature service. Establishing the creep life data
of boiler tubes is necessary to determine their application in power plants. The tubes
manufacturers and a third institute were used to test the long-term creep rupture
properties of their products with different heat and different processes. The data
from third party testing is preferred for power plants.
Figure 3 shows the creep rupture life of the test tubes, compared with the data from the NIMS
creep data sheet [13]. The creep temperature of T11 and T22 was 500 °C, and for T91 it was 550 °C and
600 °C. NIMS had the same data points for the same grade tubes at the same test conditions
with different products, which are replotted with the lower and upper lines in Fig 3. Note that the variation in the time to rupture of the different products under the
same conditions was quite wide, in particular for the T22 tubes, where the upper line
was 10 times longer than the lower line.
As shown in Fig 3A, the time to rupture of the ILJIN T11 was within the range of the NIMS creep data
sheet. The T11 tube is to be demonstrated at the position of the W/W and to replace
the lower grade of the A213-A1 carbon steels, therefore, the creep properties are
supposed to qualify under the requirements. For the T22 tubes, the time to rupture
was between the lower and upper line of the NIMS data, as shown in Fig 4B.
More efforts were carried out on the T91 tubes, since they always need to be designed
for the higher temperature part of the boiler. The times to rupture of both the ILJIN
and NSSMC tubes at 550 °C and 600 °C are shown in Fig 3C. It can be seen that most of the test points obtained here were between the upper
and lower line of the NIMS data. In addition, the time to rupture of the ILJIN tube
was longer than that of the NSSMC tube at both test temperatures, suggesting that
the locally developed tubes have even better creep properties than the imported ones.
3.1.4. Microstructure
Figure 4 is a set of SEM and TEM images of the T11, T22 and T91 tubes used in the demonstration
test. It can be seen from the SEM images that the matrix of the T11 and T22 tubes
are ferrite and pearlite, while the T91 has a ferrite structure. The ferrite and pearlite
structures are respectively noted by F and P in the micrographs.
More grain boundaries can be easily found in the SEM micrographs of the ILJIN tubes,
which suggests that the prior austenite G.S. (PAGS) of the locally developed tubes
were finer than the imported one. In addition, tens of SEM images at lower magnification
were used to measure the average G.S. and the results are shown in Table 6.
The G.S. of the locally developed tubes of T11 and T22 were ~10 mm smaller. The G.S.
of T91 was similar to that of the imported tubes. In addition, a larger quantity of
white spots can be observed in the SEM micrographs, dispersed throughout the structure.
A closer observation is shown in the corresponding TEM images, in which the precipitates
are dispersed at the grain boundaries (G.B.) and grain interior (G.I.). These precipitates
may be the M2C and/or M3C in the G.B. and within the pearlite grains in the T11 steels, as suggested in the
literature [6,7]. The domain precipitates dispersed in the G.B. of T22 may be the M23C6, while M3C and M7C3 are in the pearlite grains, and the M2C is in the ferrite grain, as suggested by Yang [8].
In the T91 steels, the domain precipitates are supposed to be M23C6 [4,5,11], which is dispersed throughout the microstructures, as shown in Fig 4. The features of all the precipitates were measured in tens of TEM micrographs for
both the ILJIN and NSSMC tubes. The results are shown in Table 6. It can be seen that the average size of the precipitates in the locally developed
tube was finer than in the imported tube, and the area fraction of both types was
at the same level. These investigations confirmed that the microstructures of the
locally developed tubes were within the code requirements, and had the same level
as the imported ones.
3.2. Demonstration test
The demonstration operation began in July of 2017 at the coal-fired boiler of Youndong
unit #2. After about one year of safe operation, visible examinations were carried
out during the overhaul period in June of 2018. All areas of the bent and welded parts
were examined, from the lower to upper positions in the bundle. Typical images are
shown in Fig 5A. The test tubes are noted by red arrows. No failures or deformation were observed,
and the components look just as they were when originally installed. Safe operation
continued to the end of December 2018. At the beginning of 2019, re-construction of
the boiler began for fuel transformation from coal to biomass. During the construction
period, only parts of the tubes were cut from the test components, and most of the
parts were allowed to remain for long-term operation/testing with the biomass fuel.
Figure 5B shows the cut tubes of the demonstration test tubes after ~13,000 h; no cracks, failures,
or any other defects were found in the tubes.
3.3. Post-test after demonstration
Table 7 shows the evolution of tensile properties, and the thickness of scale in the tubes
after 13,000 h of the demonstration test. As shown in Table 7, the degradation ratio of the tensile strength of the locally developed T11 tubes
(ILJIN) was below 3% both at RT and HT. This suggests that the T11 tubes weren’t degraded
after the short-term demonstration test, which is most probably due to the low temperature
(382 °C) of the steam in the W/W.
The tensile properties of the T22 and T91 tubes decreased after the demonstration
test. For the T22 tubes, the tensile properties of the ILJIN and NSSMC tubes after
demonstration were almost the same at both RT and HT. However, the YS degradation
was as high as 38%, while the TS and e remained relatively stable (<7%) when tested
at RT. The degradation ratio of the ILJIN was 20% larger than that of the NSSMC tube,
probably due to the high YS of the locally developed tube. In the HT tensile test,
the YS and TS properties decreased with the e enhancement to almost the same level.
In the RT tensile test, the YS of the weld components was 25% away from the base tubes,
and the TS was as high as the base tubes. At HT, it is possible to say that the weld
components had the same level of tensile properties as the base one. The greatest
degradation in the weld components was the decrease in e (>64%). This is believed
to have occurred because the weld metal was not significantly deformed during the
tensile test. The position of the tensile fracture in the weld components appeared
in the heat affected zone (HAZ) in the ILJIN parts of the test specimens.
For the T91 tubes, the tensile strengths (YS and TS) of the locally developed and
imported tubes after the demonstration were almost the same at both RT and HT. However,
the ratios of the e of the ILJIN tubes with those of the imported one at RT and HT
were 75% and 87%, respectively. Degradation of the tensile properties (YS and TS)
of the ILJIN and NSSMC tubes were found to be at the same level, with ratios below
~18% and ~12% at RT and HT, respectively. In addition, the ε degradation in the ILJIN
tube was higher than that of the NSSMC tube.
For the weld components of the T91 tubes, the YS and TS of both the locally developed
and imported tubes were higher (~17%) than that of the base tubes at RT, while they
were lower than the base tubes (~18%) at HT. Obviously, the ε decreased as much as
39% in the weld components of the imported tubes. The position of the tensile fracture
in the weld components appeared in the HAZ in the imported parts of the test specimens.
Compared to the T22 tubes, the slight degradation in the T91 tubes is believed to
be the reason for the relatively low steam temperature of 541 °C.
Figure 6 is a set of SEM and TEM images of the T22 and T91 tubes after the demonstration test.
The SEM images show that the PAG size did not change too much compared to the new
one (Fig 4), in both the T22 and T91 tubes, while the fraction of precipitates within the pearlite,
as well as the pearlite content, decreased in the T22 tubes. Meanwhile, the dislocation
density decreased significantly in the demonstration tested tubes, as shown in Fig 6B. This indicates the grains recovered during the high temperature exposure. For the
T91 tubes, a number of independent precipitates can be observed in the grain boundaries
of the new tubes. They appeared continuously after the demonstration test (Fig 6A), indicating a slight coarsening of the precipitates.
It is known that the degradation of properties in the low alloyed T11 and T22 is related
to decomposition of the pearlite structure, complex carbide transformation, and grain
recovery during high temperature exposure [13]. Meanwhile, the formation of the Laves phase, the coarsening of domain precipitates,
and grain recovery are the main mechanisms found in the T91 tubes upon high temperature
exposure [4,5,11,14]. These factors may explain the decrease in the base tube tensile properties in T22
and T91 after the demonstration test, to a certain extent. A quantitative analysis
of the mentioned microstructure features is currently under study, and will be matched
with the properties, to finally determine the degradation mechanisms of the T22 and
T91 upon exposure in field conditions.
In addition, the scales formed on the steam side were measured in the cut tubes, and
the average thicknesses are shown in Table 7. A very thin oxide scale (~10 mm) was observed in the T11 tubes. For both the T22
and T91 tubes, the thickness of the scale formed on the ILJIN and NSSMC tubes after
TDM was almost the same. These results suggest that the oxidation resistance of the
locally developed tube was the same as the imported tube.
The creep properties of the test tubes, and in particular T22, decreased significantly
after the demonstration test. As of the writing of this paper, most of the creep test
samples had not ruptured. A further report will focus on the degradation mechanism
of creep life, and the corresponding microstructural evolution.