# Surface Hardening of Ti-15V-3Al-3Cr-3Sn Alloy after Cyclic Hydrogenation and Subsequent Solution Treatment

Authors: Chia-Po Hung; Tair-I Wu; Jiann-Kuo Wu
Journal: Advances in Materials Science and Engineering
 (2014)

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## Abstract

The as-received and preheated (1000°C-30 min. and 500°C-30 min.) sheets of Ti-15V-3Al-3Cr-3Sn alloy (Ti-153) were treated according to the predetermined process including a cyclic electrolytic hydrogenation (at 50 mA/cm2 for 1 hr and at 5 mA/cm2 for 10 hrs) combining a subsequent solution treatment to see the effects of various operating parameters on the evolution of microstructure and the variations of hardness. The hardening effect deriving from solid-solution strengthening of hydrogen eventually overrode that from precipitation hardening. The maximum hardness elevation was from 236.9 to 491.1 VHN.


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## Body

## 1. Introduction

Titanium alloys are traditionally divided into three categories,α, α + β, and β alloys, according to the stabilizing elements alloyed [1–3]. Commercial purity titanium (CP-Ti) and Ti-6Al-4V (Ti-64) are examples for α- and (α + β)-Ti alloys, respectively, while Ti-15V-3Al-3Cr-3Sn (Ti-153) alloy can be thought of as a typical β-Ti alloy.Hydrogen induced cracking inα- and (α + β)-Ti alloys were attributed to hydride precipitation. Fracture arising from hydride formation in the matrix has not been reported for β-Ti alloys. The hydrogen embrittlement problems in β-Ti alloys were concluded to result from decohesion [4–6].Microstructural modification and mechanical properties improvement ofα- and (α + β)-Ti alloys through thermohydrogen processing have been extensively studied by many investigators [7–12]. Ti-153, as a typical β-Ti alloy, was chosen in this study for investigating the variations in microstructure and mechanical properties after cyclic electrolytic hydrogenation and subsequent solution treatment.


## 2. Experiments

The specimens were grouped into three sets according to the preheating conditions (1) A0, machined from the as-received sheet; (2) B0, subjected A0 specimens to vacuum annealing at 1.33 × 10−4 Pa from room temperature to 1000°C, then held for 0.5 hr, and finally furnace cooled to room temperature; (3) C0, heated A0 specimens in a muffle furnace at 500°C for 0.5 hr and finally air cooled to room temperature. Chemical composition of the as-received sheet was listed in Table 1. The specimens were sheared to be 40 × 14 × 4 mm3, abraded with emery paper (up to grit 1200), and then lapped with alumina powder to minimize the interference of surface oxides on hydrogenation. The surface roughness was measured by employing surface roughness tester (MITUTOYO SV402) and listed in Table 2.Table 1
Analyzed composition of the as-received Ti-153 sheets (wt.%).
H
C
N
O
Fe
Al
Cr
Sn
V
Ti
0.015
0.05
0.05
0.13
0.25
2.5~3.5
2.5~3.5
2.5~3.5
14.0~16.0
balancedTable 2
The surface roughness of Ti-153 sheet specimens after various processing.
Processing
R
a (μm)
R
q (μm)
R
t (μm)
A0
0.073
0.090
0.61
B0
0.095
0.121
0.83
C0
0.084
0.104
0.76
R
a: The arithmetic mean of the departure of the profile from the mean line.
R
q: The root-mean-square parameter corresponding to R
a.
R
t: The maximum peak to valley height of the profile in the assessments.Electrolytic hydrogenation was performed at 50 mA/cm2 for 1 hr and 5 mA/cm2 for 10 hrs in 1 N H
2
SO
4
(
aq
) by adding 0.1 g/L As2O3, respectively. The subsequent solution treatments were operated in a muffle furnace at 300°C for 2 hrs. Processes were grouped and denoted by I
j
K
l according to the treating conditions (cathodic charging, heat treatment, and cycle time), where I and K correspond to the treatments (I or K
=
H means the specimen charged at 50 mA/cm2 for 1 hr; I or K
=
L means the specimen charged at 5 mA/cm2 for 10 hrs; I or K
=
T means the specimen heat treated in a muffle furnace at 300°C for 2 hrs, respectively, while j or l
=
1 means the first cycle, j or l
=
2 means the second cycle, j or l
=
3 means the third cycle, …, etc.). For instance, H2T2 means that the specimen was hydrogenated in the first cycle at 50 mA/cm2 for 1 hr, followed by a heat treatment at 300°C for 2 hrs, and then proceeded the same treatments in the second cycle. All the process designations and processing parameters were gathered in Table 3. The whole experimental procedure was schematically shown in Figure 1.Table 3
Process designations and the associated processing parameters.
Process designations
The associated processing parameters
T1
Heating for 2 hrs at 300°C and then air cooling to room temperature
Tn
Specimens heated forn times followed the T1 conditions (n
≧
2)
H1
Hydrogenated at 50 mA/cm2 for 1 hr in 1N H
2
SO
4(aq) + 0.1 g/L As2O3
L1
Hydrogenated at 5 mA/cm2 for 10 hrs in 1N H
2
SO
4(aq) + 0.1 g/L As2O3
H1T1
H1 treated specimens followed by a further T1 treatment
T1H2
H1T1 treated specimens followed by a further H1 treatment
HnTn
Tn-1Hn treated specimens followed by a further T1 treatment (n
≧
2)
TnHn + 1
HnTn treated specimens followed by a further H1 treatment (n
≧
2)
L1T1
L1 treated specimens followed by a further T1 treatment
T1L2
L1T1 treated specimens followed by a further L1 treatment
LnTn
Tn-1Ln treated specimens followed by a further T1 treatment (n
≧
2)
TnLn + 1
LnTn treated specimens followed by a further L1 treatment (n
≧
2)Schematic diagrams of the designed cyclic hydrogenation-solid solution treatment for (a) A0, (b) B0, and (c) C0 sheets.
(a)
(b)
(c)The effects of processing parameters on the microstructural changes and the electrolytic hydrogenation efficiency were evaluated qualitatively and quantitatively by utilizing X-ray diffractometry (XRD: X’Pert PRO MPD, PANalytical, Netherlands, 45 kV-40 mA), metallographic optical microscopy (MOM), glow discharge optical spectrometry (GDOS; LECO GDS-750), and elemental analysis (EA: elementar VarioEL-III), respectively. The hardness variation at the near surface was measured by utilizing Akashi Vickers hardness tester (MVK-H100).


## 3. Results and Discussion

### 3.1. Structural Variations

The microphotographs of surface and cross-sectional views of the as-received and processed sheets were shown in Figures2, 3, and 4, respectively. Figure 2(a) showed that the grain size of A0 specimens on the rolling surface is 30 μm. Figure 2(b) was the microstructure of long transverse side of A0 sheets. The rolled sheets did not show an exceedingly elongated grain structure. The microstructures in Figures 3(a) and 3(b) were relatively equiaxed. Having been subjected to vacuum annealing at 1000°C for 0.5 hr, the original small grains of A0 specimens grew to more than 300 μm in B0 specimens (Figures 3(a) and 3(b)). Heat treating A0 specimens at 500°C for 0.5 hr and air cooling to room temperature did not effectively alter the microstructure of A0 specimens. The microstructure of C0 specimens (Figures 4(a) and 4(b)) was similar to those of A0 ones.Metallographic microphotographs on (a) rolling surface and (b) long transverse side of A0 sheets.
(a)
(b)Metallographic microphotographs on (a) rolling surface and (b) long transverse side of B0 sheets.
(a)
(b)Metallographic microphotographs on (a) rolling surface and (b) long transverse side of C0 sheets.
(a)
(b)The XRD patterns of A0, B0, and C0 specimens were shown in Figure5. Annealing at β phase region for B0 treatment led to obvious variation in preferred orientation (from β(110) to β(200)) while no α precipitation and β peak shift were found. C0 treatment, however, annealing at α phase region resulted in slight α phase formation and β peaks shift without appreciable texture change [13]. Subsequent microstructural changes of A0, B0, and C0 specimens due to thermal annealing, hydrogen absorption, hydrogen evolution, and redistribution in the β-Ti substrate during cyclic hydrogenation and solution heat treatment were shown in Figures 6, 7, 8, and 9, respectively. The XRD patterns in Figures 6(a), 6(b), and 6(c) for T1, T2, T3, and T4 processes performed on A0, B0, and C0 sheets did not show significant phase transformation or texture change in comparison with those corresponding patterns of A0, B0, and C0 ones. The accumulated heating period up to 8 hours at 300°C did not bring about detectable α signal in the XRD patterns of AT4 and BT4 specimens. The C0 specimen, however, treated at 500°C for only 0.5 hour can lead to observable α peaks in Figure 5. Independent employment of solution heat treatment has minute effect on the microstructural changes of Ti-153 under the designed testing conditions while the subjection of cyclic hydrogenation combining post-solution heat treating to A0, B0, and C0 specimens resulted in appreciable microstructural evolutions.Figure 5
The respective XRD pattern for A0, B0, and C0 sheets.XRD patterns for specimens after cyclic annealing (a) ATl, (b) BTl, and (c) CTl series.
(a)
(b)
(c)XRD patterns for specimens after successive (a) AHjTl and (b) ALjTl treatments.
(a)
(b)XRD patterns for specimens after successive (a) BHjTl and (b) BLjTl treatments.
(a)
(b)XRD patterns for specimens after successive (a) CHjTl and (b) CLjTl treatments.
(a)
(b)The diffraction peaks ofβ phase presented in the XRD patterns of A0 and C0 sheets were gradually depressed and shifted to left while not significantly broadened after every hydrogenation process and would back shift to right slightly after the successive solution heating process. The variations of β diffraction peaks of B0 specimens, however, did not show the same tendency as that of A0 and C0 ones. The α peaks in C0 patterns diminished eventually after CH4T4 and CT2L3 treatments. The most pronounced angular discrepancy found in the XRD patterns of various series of specimens was to be of AT3L4, BT3L4, and CT3L4 ones (Figures 6 to 9). The differences of angular position (2
θ) of β(211) for AT3H4, BT3H4, and CT3H4 (in contrast to A0, B0 and C0 resp.) were 0.38°, 0.68°, and 0.78°, while those for AT3L4, BT3L4, and CT3L4 were 1.64°, 2.00°, and 2.48°, respectively. Since lower charging current densities would lead to higher hydrogenation efficiency [14–16], the discussion about the effects of hydrogen uptake on the angular shift and phase transformation was hereafter confined to the ATjLk, BTjLk,and CTjLk series.The magnitude of angular shift and the FWHM of peaksβ(110), β(200) and β(211) for A0, B0, C0, AT3, BT3, CT3, AT3L4, BT3L4 and CT3L4 specimens were listed in Table 4. T3 process was a blank test in contrast to the corresponding T3L4 process. According to the data grouped in Table 4, the crystallinity of cyclically hydrogenated specimens were superior to that of original and cyclic heat treated ones. T3 treatment was basically a cyclic precipitation process of α phase operated at 300°C. The absorbed hydrogen atoms occupying the interstitial sites during cathodic charging expanded the lattice, while the dissolved aluminum precipitated from the β matrix during heating relaxed the lattice expansion. The magnitude of angular shift of peaks β(110), β(200) and β(211) for AT3, BT3 and CT3 specimens are positive due to lattice relaxation in contrast to those correspondingly negative values for AT3L4, BT3L4 and CT3L4 ones due to lattice expansion.Table 4
The magnitude of angular shift and (/) the FWHM in degree of peaksβ
(
110
), β
(
200
), and β
(
211
) for some treated specimens corresponding to A0, B0, and C0 ones, respectively.
Specimen
β
(
110
)
β
(
200
)
β
(
211
)
A0
39.47 (—/0.19)
56.83 (—/0.30)
71.43 (—/0.23)
AT3
39.61 (0.14/0.20)
57.03 (0.20/0.32)
71.75 (0.32/0.32)
AT3L4
38.69 (−0.78/0.14)
55.73 (−1.10/0.30)
69.79 (−1.64/0.24)
B0
39.31 (—/0.29)
57.09 (—/0.23)
71.67 (—/0.21)
BT3
39.41 (0.10/0.16)
57.21 (0.12/0.27)
71.81 (0.14/0.29)
BT3L4
38.55 (−0.76/0.12)
55.77 (−1.32/0.23)
69.67 (−2.00/0.23)
C0
39.49 (—/0.22)
57.11 (—/0.34)
71.65 (—/0.25)
CT3
39.60 (0.11/0.14)
57.21 (0.10/0.20)
71.77 (0.12/0.19)
CT3L4
38.29 (−1.20/0.11)
55.39 (−1.82/0.14)
69.17 (−2.48/0.16)


### 3.2. Compositional Analyses

Figure10 shows the depth profiles of hydrogen distribution at the near surface of AT3L4, BT3L4 and CT3L4 specimens. After the A0 sheets had been vacuum annealed at 1000°C for half an hour and followed by a furnace cooling to room temperature, the defects density of B0 sheets were significantly reduced and all the solute atoms were dissolved into the matrix. There were limited defective regions for ingressive hydrogen so that the hydrogen depth profile for BT3L4 in Figure 10 located appreciably lower than those for AT3L4 and CT3L4. An annealing treatment at 500°C for half an hour and a following air cooling performed on A0 sheets also reduced defects density of C0 sheets but promoted aluminum to come out of the β matrix to form appreciable α phase (Figure 5). The larger amount of aluminum precipitation during heating, the higher extent of the lattice strain relaxed, thus, resulted in residential space to accommodate much more interstitial hydrogen.Figure 10
Hydrogen distribution depth profiles at the near surface after (a) AT3L4, (b) BT3L4, (c) CT3L4, and (d) AT3H4 treatments. The depth profiles for the treatments similar to AT3H4 and AT3L4 performed on (e) Ti-64 and (f) CP-Ti respectively were also attached for comparison.Positive difference between hydrogen absorption and evolution eventually caused structural changes. Hydrogen diffused intoβ structure induced dilatation of matrix and resulted in the enlargement of respective d-spacing, thus, decreased the diffraction angle 2
θ of corresponding β peaks. Since C0 sheets with lower defects density but far more relaxed interstitial sites than those of A0 ones, the hydrogen uptake for CT3L4 just slightly inferior to that for AT3L4 while with lower volume expansion (C0versus A0: −0.372%). The variations in lattice constant and volume expansion for typical treatments were analyzed by using Nelson-Riley approach [17] and listed in Table 5. After A0 sheets had been B0 and C0 treated, the volume contraction rate for B0 and C0 ones were 0.186% and 0.372%, respectively. T3 treatment led to further stress relaxation of A0, B0 and C0 sheets of which the volume contraction rate was all 0.031%, while T3L4 treatment resulted in evident volume expansion rate of A0 (3.90%), B0 (2.04%) and C0 (5.40%) ones, respectively.Table 5
Variations in lattice constant and volume expansion rate between typical treatments.
Treatment
Variation
Lattice constant (Å)
Lattice expansion
Volume expansion
A0
3.234
—
—
AT3 (versus A0)
3.233
−0.031%
−0.093%
AT3L4 (versus A0)
3.275
1.30%
3.90%
B0 (versus A0)
3.232
−0.062%
−0.186%
BT3 (versus B0)
3.231
−0.031%
−0.093%
BT3L4 (versus B0)
3.253
0.68%
2.04%
C0 (versus A0)
3.230
−0.124%
−0.372%
CT3 (versus C0)
3.229
−0.031%
−0.093%
CT3L4 (versus C0)
3.288
1.80%
5.40%The appreciable angular shifts in diffractedβ peaks for AT3L4, BT3L4 and CT3L4 leading to smaller FWHM means that the hydrogenated layer at the near surface of AT3L4, BT3L4 and CT3L4 specimens have long range order. This, in turn, implies that an almost homogeneously hydrogenated near surface was the prerequisite. It can be seen from Figure 10 that the linear section of the depth profiles are with slight gradient inclined from the surface into the interior for the AT3L4, BT3L4 and CT3L4 treatments. The steeply and mildly declined hydrogen depth profiles of CP-Ti and Ti-6Al-4V alloy processed with the similar parameters as applied to AT3L4 and AT3H4 specimens, respectively. The results had been published before [11, 18] and were partly extracted here for comparison. In [11], the appreciable concentration gradient for Ti-6Al-4V alloy at the near surface led to the broadened α and β diffraction peaks of Ti-6Al-4V specimens with A3H4 processing.The electrolytic hydrogenating parameters performed on the CP-Ti and Ti-6Al-4V specimens were 5 mA/cm2 for 30 hrs and 50 mA/cm2 for 3 hrs in 1 N H
2
SO
4
(
aq
) + 0.1 g/L As2O3, respectively. The total Faraday numbers for the two processes were three times as large as those applied to AT3L4 and AT3H4 ones. Comparison of the depth profiles between AT3L4 and AT3H4 ones quantitatively manifests that lower applied current density leading to higher charging efficiency. Compare the depth profiles of CP-Ti with AT3L4 and Ti-6Al-4V with AT3H4 to see the different hydrogenating behavior among α, α + β, and β titanium alloys. Obviously bcc structure of β phase offers a more open route and broader space for the diffusion and accommodation of hydrogen in titanium.


### 3.3. Hardness Measurements

There are various hydrogen accommodating microstructures such as interstitial sites, vacant sites, dislocation core, grain boundaries, and voids in the specimens. Shifts of diffraction peaks can arise from the occupation of interstitial sites only; besides, higher content of hydrogen absorption would result in higher dislocation density in the matrix [19]. This is the reason why shifts of β diffraction peaks cannot be served as a quantitative measurement of hydrogen absorption, even qualitative, of the processed specimens but can be directly related to lattice expansion and, thus, the hardness elevation. Zhao et al. [19] found that hydrogen atoms absorbed by titanium alloys would preferentially inhabit vacant sites and then dislocations rather the interstitial sites in the initial stage, which offers no solid-solution strengthening effect on the microstructure [20].A0 sheets had been rolled and process annealed to accumulate 50% in thickness reduction. Large amount of point and line defects were stored in A0 sheets during the processing. C0 sheets were obtained by subjecting A0 ones to an annealing treatment at 500°C for 30 min., which lowered the densities of point (vacancies and substitutional solute atoms) and line (dislocations) defects in the C0 sheets. Under the same charging condition, the amount of interstitial sites occupied by the ingressive hydrogen in the processed specimens determined the lattice dilatation, thus, angular shift of diffractedβ peaks, and finally the hardening effect on the specimens. In comparison with A0 specimens, C0 ones processed in the α-phase region (500°C) experienced precipitation hardening to compete against annealing softening. The softening arose from two sources (1) recovery of A0 specimens annealed at 500°C for half an hour and (2) the major α element in Ti-15333 alloy, aluminum, precipitated out of β matrix eliminated the effect of solid-solution strengthening. The angular shift and changes in preferred orientation of β phase (Table 4 and Figure 5) in contrast to that for A0 treatment are however not significant. Aluminum atoms diffusing away from β matrix also led to the latticeresuscitation (Table 5). In comparison with B0 specimens, precipitation of aluminum relaxed the lattice strain and elevated the accommodating capacity of hydrogen for C0 specimens during successive cathodic charging processes. Hardness elevation (491.1) and lattice dilatation (1.80%) of CT3L4 specimens were obviously higher than those of AT3L4 (409.3 and 1.30%) and BT3L4 ones (344.7 and 0.68%).Table6 showed Vickers hardness numbers (VHN) measured at different areas on the typical specimens, where H
S, H
N, and H
C were VHN obtained at surface and near surface at various depths, respectively. The core hardness H
C is the H
N measured at the depth of 500 μm. The correspondingly lowest hardness for specimens of series B arose from lower dislocation density, larger grain size (300 μm), and higher average aluminum content in the matrix (no precipitation hardening) of B0 sheets, while the correspondingly highest hardness for specimens of series C was from the controlled grain size (30 μm) and precipitation hardening.Table 6
H
S, H
N, and H
B for typical specimens (Vickers hardness measured at the load of 50 gw).
Process designation
H
S
H
N (μm)
H
C
50
100
150
200
250
300
350
400
450
H
N (500)
A0
236.9
241.2
226.3
230.4
231.7
234.6
AT3
264.5
AT3L4
409.3
376.2
387.6
378.6
371.4
380.0
356.6
346.5
336.9
345.6
346.1
AT4
301.1
257.2
260.5
250.3
254.2
253.1
B0
179.5
185.3
177.2
164.7
174.3
169.8
BT3
277.9
BT3L4
344.7
364.1
364.7
364.0
357.0
355.6
347.3
338.7
330.4
336.9
331.2
BT4
288.2
219.6
221.2
217.7
213.8
219.8
C0
314.7
318.6
317.4
310.6
317.9
318.2
CT3
330.7
CT3L4
491.1
476.3
467.2
436.8
443.1
438.7
436.5
429.8
432.7
427.3
423.8
CT4
348.1
327.9
322.6
317.4
338.1
326.7The hardening efficiencies (HE) for typical specimens were listed in Table7. Obviously, the differences of VHN between T0 and T3 specimens were derived from precipitation hardening, while those between T3 and T3L4 ones were derived from hydrogenation. The HE for CT3 and CT4 were the specimens correspondingly lowest ones among T3 and T4 because precipitating hardenability of C0 specimen was exhausted during 500°C pretreatment. H
S of A0 sheets increased from 236.9 to 264.5 (AT3), and then 302.3 (AT3H4) and 409.3 (AT3L4) finally dropped to 301.1 (AT4). The surface and core hardness variations for specimens of A, B, and C series were shown in Figure 11. It is reasonable to see that surface hardness is correspondingly higher than core hardness. The hardness variations of surface and core for A, B, and C series, however, follow the similar tendency. T3L4 is the optimal process for surface and core hardening for A, B, and C sheets. The maximum hardness elevation efficiencies of H
S and H
C for series A are 72.8% (H
S) and 47.5% (H
C). Those for B and C series are 92.0% (H
S), 95.1% (H
C) and 56.1% (H
S), 33.2% (H
C), respectively. Since the precipitating hardenability of specimens was gradually consumed while the hydrogen uptake of them increased with numbers of cyclic electrolytic hydrogenation, the hardening effect deriving from solid-solution strengthening of hydrogen eventually overrode that from precipitation hardening.Table 7
Hardening efficiency for typical specimens.
Process designation
H
S/HE
H
C/HE
A0
236.9
234.6
AT3
264.5/11.7%
—
AT3L4
409.3/72.8%
346.1/47.5%
AT4
301.1/27.1%
253.1/7.9%
B0
179.5
169.8
BT3
277.9/54.8%
—
BT3L4
344.7/92.0%
331.2/95.1%
BT4
288.2/60.6%
219.8/29.4%
C0
314.7
318.2
CT3
330.7/5.1%
—
CT3L4
491.1/56.1%
423.8/33.2%
CT4
348.1/10.6%
326.7/2.7%Variations of VHN for different treatments at (a) surface and (b) core.
(a)
(b)


## 3.1. Structural Variations

The microphotographs of surface and cross-sectional views of the as-received and processed sheets were shown in Figures2, 3, and 4, respectively. Figure 2(a) showed that the grain size of A0 specimens on the rolling surface is 30 μm. Figure 2(b) was the microstructure of long transverse side of A0 sheets. The rolled sheets did not show an exceedingly elongated grain structure. The microstructures in Figures 3(a) and 3(b) were relatively equiaxed. Having been subjected to vacuum annealing at 1000°C for 0.5 hr, the original small grains of A0 specimens grew to more than 300 μm in B0 specimens (Figures 3(a) and 3(b)). Heat treating A0 specimens at 500°C for 0.5 hr and air cooling to room temperature did not effectively alter the microstructure of A0 specimens. The microstructure of C0 specimens (Figures 4(a) and 4(b)) was similar to those of A0 ones.Metallographic microphotographs on (a) rolling surface and (b) long transverse side of A0 sheets.
(a)
(b)Metallographic microphotographs on (a) rolling surface and (b) long transverse side of B0 sheets.
(a)
(b)Metallographic microphotographs on (a) rolling surface and (b) long transverse side of C0 sheets.
(a)
(b)The XRD patterns of A0, B0, and C0 specimens were shown in Figure5. Annealing at β phase region for B0 treatment led to obvious variation in preferred orientation (from β(110) to β(200)) while no α precipitation and β peak shift were found. C0 treatment, however, annealing at α phase region resulted in slight α phase formation and β peaks shift without appreciable texture change [13]. Subsequent microstructural changes of A0, B0, and C0 specimens due to thermal annealing, hydrogen absorption, hydrogen evolution, and redistribution in the β-Ti substrate during cyclic hydrogenation and solution heat treatment were shown in Figures 6, 7, 8, and 9, respectively. The XRD patterns in Figures 6(a), 6(b), and 6(c) for T1, T2, T3, and T4 processes performed on A0, B0, and C0 sheets did not show significant phase transformation or texture change in comparison with those corresponding patterns of A0, B0, and C0 ones. The accumulated heating period up to 8 hours at 300°C did not bring about detectable α signal in the XRD patterns of AT4 and BT4 specimens. The C0 specimen, however, treated at 500°C for only 0.5 hour can lead to observable α peaks in Figure 5. Independent employment of solution heat treatment has minute effect on the microstructural changes of Ti-153 under the designed testing conditions while the subjection of cyclic hydrogenation combining post-solution heat treating to A0, B0, and C0 specimens resulted in appreciable microstructural evolutions.Figure 5
The respective XRD pattern for A0, B0, and C0 sheets.XRD patterns for specimens after cyclic annealing (a) ATl, (b) BTl, and (c) CTl series.
(a)
(b)
(c)XRD patterns for specimens after successive (a) AHjTl and (b) ALjTl treatments.
(a)
(b)XRD patterns for specimens after successive (a) BHjTl and (b) BLjTl treatments.
(a)
(b)XRD patterns for specimens after successive (a) CHjTl and (b) CLjTl treatments.
(a)
(b)The diffraction peaks ofβ phase presented in the XRD patterns of A0 and C0 sheets were gradually depressed and shifted to left while not significantly broadened after every hydrogenation process and would back shift to right slightly after the successive solution heating process. The variations of β diffraction peaks of B0 specimens, however, did not show the same tendency as that of A0 and C0 ones. The α peaks in C0 patterns diminished eventually after CH4T4 and CT2L3 treatments. The most pronounced angular discrepancy found in the XRD patterns of various series of specimens was to be of AT3L4, BT3L4, and CT3L4 ones (Figures 6 to 9). The differences of angular position (2
θ) of β(211) for AT3H4, BT3H4, and CT3H4 (in contrast to A0, B0 and C0 resp.) were 0.38°, 0.68°, and 0.78°, while those for AT3L4, BT3L4, and CT3L4 were 1.64°, 2.00°, and 2.48°, respectively. Since lower charging current densities would lead to higher hydrogenation efficiency [14–16], the discussion about the effects of hydrogen uptake on the angular shift and phase transformation was hereafter confined to the ATjLk, BTjLk,and CTjLk series.The magnitude of angular shift and the FWHM of peaksβ(110), β(200) and β(211) for A0, B0, C0, AT3, BT3, CT3, AT3L4, BT3L4 and CT3L4 specimens were listed in Table 4. T3 process was a blank test in contrast to the corresponding T3L4 process. According to the data grouped in Table 4, the crystallinity of cyclically hydrogenated specimens were superior to that of original and cyclic heat treated ones. T3 treatment was basically a cyclic precipitation process of α phase operated at 300°C. The absorbed hydrogen atoms occupying the interstitial sites during cathodic charging expanded the lattice, while the dissolved aluminum precipitated from the β matrix during heating relaxed the lattice expansion. The magnitude of angular shift of peaks β(110), β(200) and β(211) for AT3, BT3 and CT3 specimens are positive due to lattice relaxation in contrast to those correspondingly negative values for AT3L4, BT3L4 and CT3L4 ones due to lattice expansion.Table 4
The magnitude of angular shift and (/) the FWHM in degree of peaksβ
(
110
), β
(
200
), and β
(
211
) for some treated specimens corresponding to A0, B0, and C0 ones, respectively.
Specimen
β
(
110
)
β
(
200
)
β
(
211
)
A0
39.47 (—/0.19)
56.83 (—/0.30)
71.43 (—/0.23)
AT3
39.61 (0.14/0.20)
57.03 (0.20/0.32)
71.75 (0.32/0.32)
AT3L4
38.69 (−0.78/0.14)
55.73 (−1.10/0.30)
69.79 (−1.64/0.24)
B0
39.31 (—/0.29)
57.09 (—/0.23)
71.67 (—/0.21)
BT3
39.41 (0.10/0.16)
57.21 (0.12/0.27)
71.81 (0.14/0.29)
BT3L4
38.55 (−0.76/0.12)
55.77 (−1.32/0.23)
69.67 (−2.00/0.23)
C0
39.49 (—/0.22)
57.11 (—/0.34)
71.65 (—/0.25)
CT3
39.60 (0.11/0.14)
57.21 (0.10/0.20)
71.77 (0.12/0.19)
CT3L4
38.29 (−1.20/0.11)
55.39 (−1.82/0.14)
69.17 (−2.48/0.16)


## 3.2. Compositional Analyses

Figure10 shows the depth profiles of hydrogen distribution at the near surface of AT3L4, BT3L4 and CT3L4 specimens. After the A0 sheets had been vacuum annealed at 1000°C for half an hour and followed by a furnace cooling to room temperature, the defects density of B0 sheets were significantly reduced and all the solute atoms were dissolved into the matrix. There were limited defective regions for ingressive hydrogen so that the hydrogen depth profile for BT3L4 in Figure 10 located appreciably lower than those for AT3L4 and CT3L4. An annealing treatment at 500°C for half an hour and a following air cooling performed on A0 sheets also reduced defects density of C0 sheets but promoted aluminum to come out of the β matrix to form appreciable α phase (Figure 5). The larger amount of aluminum precipitation during heating, the higher extent of the lattice strain relaxed, thus, resulted in residential space to accommodate much more interstitial hydrogen.Figure 10
Hydrogen distribution depth profiles at the near surface after (a) AT3L4, (b) BT3L4, (c) CT3L4, and (d) AT3H4 treatments. The depth profiles for the treatments similar to AT3H4 and AT3L4 performed on (e) Ti-64 and (f) CP-Ti respectively were also attached for comparison.Positive difference between hydrogen absorption and evolution eventually caused structural changes. Hydrogen diffused intoβ structure induced dilatation of matrix and resulted in the enlargement of respective d-spacing, thus, decreased the diffraction angle 2
θ of corresponding β peaks. Since C0 sheets with lower defects density but far more relaxed interstitial sites than those of A0 ones, the hydrogen uptake for CT3L4 just slightly inferior to that for AT3L4 while with lower volume expansion (C0versus A0: −0.372%). The variations in lattice constant and volume expansion for typical treatments were analyzed by using Nelson-Riley approach [17] and listed in Table 5. After A0 sheets had been B0 and C0 treated, the volume contraction rate for B0 and C0 ones were 0.186% and 0.372%, respectively. T3 treatment led to further stress relaxation of A0, B0 and C0 sheets of which the volume contraction rate was all 0.031%, while T3L4 treatment resulted in evident volume expansion rate of A0 (3.90%), B0 (2.04%) and C0 (5.40%) ones, respectively.Table 5
Variations in lattice constant and volume expansion rate between typical treatments.
Treatment
Variation
Lattice constant (Å)
Lattice expansion
Volume expansion
A0
3.234
—
—
AT3 (versus A0)
3.233
−0.031%
−0.093%
AT3L4 (versus A0)
3.275
1.30%
3.90%
B0 (versus A0)
3.232
−0.062%
−0.186%
BT3 (versus B0)
3.231
−0.031%
−0.093%
BT3L4 (versus B0)
3.253
0.68%
2.04%
C0 (versus A0)
3.230
−0.124%
−0.372%
CT3 (versus C0)
3.229
−0.031%
−0.093%
CT3L4 (versus C0)
3.288
1.80%
5.40%The appreciable angular shifts in diffractedβ peaks for AT3L4, BT3L4 and CT3L4 leading to smaller FWHM means that the hydrogenated layer at the near surface of AT3L4, BT3L4 and CT3L4 specimens have long range order. This, in turn, implies that an almost homogeneously hydrogenated near surface was the prerequisite. It can be seen from Figure 10 that the linear section of the depth profiles are with slight gradient inclined from the surface into the interior for the AT3L4, BT3L4 and CT3L4 treatments. The steeply and mildly declined hydrogen depth profiles of CP-Ti and Ti-6Al-4V alloy processed with the similar parameters as applied to AT3L4 and AT3H4 specimens, respectively. The results had been published before [11, 18] and were partly extracted here for comparison. In [11], the appreciable concentration gradient for Ti-6Al-4V alloy at the near surface led to the broadened α and β diffraction peaks of Ti-6Al-4V specimens with A3H4 processing.The electrolytic hydrogenating parameters performed on the CP-Ti and Ti-6Al-4V specimens were 5 mA/cm2 for 30 hrs and 50 mA/cm2 for 3 hrs in 1 N H
2
SO
4
(
aq
) + 0.1 g/L As2O3, respectively. The total Faraday numbers for the two processes were three times as large as those applied to AT3L4 and AT3H4 ones. Comparison of the depth profiles between AT3L4 and AT3H4 ones quantitatively manifests that lower applied current density leading to higher charging efficiency. Compare the depth profiles of CP-Ti with AT3L4 and Ti-6Al-4V with AT3H4 to see the different hydrogenating behavior among α, α + β, and β titanium alloys. Obviously bcc structure of β phase offers a more open route and broader space for the diffusion and accommodation of hydrogen in titanium.


## 3.3. Hardness Measurements

There are various hydrogen accommodating microstructures such as interstitial sites, vacant sites, dislocation core, grain boundaries, and voids in the specimens. Shifts of diffraction peaks can arise from the occupation of interstitial sites only; besides, higher content of hydrogen absorption would result in higher dislocation density in the matrix [19]. This is the reason why shifts of β diffraction peaks cannot be served as a quantitative measurement of hydrogen absorption, even qualitative, of the processed specimens but can be directly related to lattice expansion and, thus, the hardness elevation. Zhao et al. [19] found that hydrogen atoms absorbed by titanium alloys would preferentially inhabit vacant sites and then dislocations rather the interstitial sites in the initial stage, which offers no solid-solution strengthening effect on the microstructure [20].A0 sheets had been rolled and process annealed to accumulate 50% in thickness reduction. Large amount of point and line defects were stored in A0 sheets during the processing. C0 sheets were obtained by subjecting A0 ones to an annealing treatment at 500°C for 30 min., which lowered the densities of point (vacancies and substitutional solute atoms) and line (dislocations) defects in the C0 sheets. Under the same charging condition, the amount of interstitial sites occupied by the ingressive hydrogen in the processed specimens determined the lattice dilatation, thus, angular shift of diffractedβ peaks, and finally the hardening effect on the specimens. In comparison with A0 specimens, C0 ones processed in the α-phase region (500°C) experienced precipitation hardening to compete against annealing softening. The softening arose from two sources (1) recovery of A0 specimens annealed at 500°C for half an hour and (2) the major α element in Ti-15333 alloy, aluminum, precipitated out of β matrix eliminated the effect of solid-solution strengthening. The angular shift and changes in preferred orientation of β phase (Table 4 and Figure 5) in contrast to that for A0 treatment are however not significant. Aluminum atoms diffusing away from β matrix also led to the latticeresuscitation (Table 5). In comparison with B0 specimens, precipitation of aluminum relaxed the lattice strain and elevated the accommodating capacity of hydrogen for C0 specimens during successive cathodic charging processes. Hardness elevation (491.1) and lattice dilatation (1.80%) of CT3L4 specimens were obviously higher than those of AT3L4 (409.3 and 1.30%) and BT3L4 ones (344.7 and 0.68%).Table6 showed Vickers hardness numbers (VHN) measured at different areas on the typical specimens, where H
S, H
N, and H
C were VHN obtained at surface and near surface at various depths, respectively. The core hardness H
C is the H
N measured at the depth of 500 μm. The correspondingly lowest hardness for specimens of series B arose from lower dislocation density, larger grain size (300 μm), and higher average aluminum content in the matrix (no precipitation hardening) of B0 sheets, while the correspondingly highest hardness for specimens of series C was from the controlled grain size (30 μm) and precipitation hardening.Table 6
H
S, H
N, and H
B for typical specimens (Vickers hardness measured at the load of 50 gw).
Process designation
H
S
H
N (μm)
H
C
50
100
150
200
250
300
350
400
450
H
N (500)
A0
236.9
241.2
226.3
230.4
231.7
234.6
AT3
264.5
AT3L4
409.3
376.2
387.6
378.6
371.4
380.0
356.6
346.5
336.9
345.6
346.1
AT4
301.1
257.2
260.5
250.3
254.2
253.1
B0
179.5
185.3
177.2
164.7
174.3
169.8
BT3
277.9
BT3L4
344.7
364.1
364.7
364.0
357.0
355.6
347.3
338.7
330.4
336.9
331.2
BT4
288.2
219.6
221.2
217.7
213.8
219.8
C0
314.7
318.6
317.4
310.6
317.9
318.2
CT3
330.7
CT3L4
491.1
476.3
467.2
436.8
443.1
438.7
436.5
429.8
432.7
427.3
423.8
CT4
348.1
327.9
322.6
317.4
338.1
326.7The hardening efficiencies (HE) for typical specimens were listed in Table7. Obviously, the differences of VHN between T0 and T3 specimens were derived from precipitation hardening, while those between T3 and T3L4 ones were derived from hydrogenation. The HE for CT3 and CT4 were the specimens correspondingly lowest ones among T3 and T4 because precipitating hardenability of C0 specimen was exhausted during 500°C pretreatment. H
S of A0 sheets increased from 236.9 to 264.5 (AT3), and then 302.3 (AT3H4) and 409.3 (AT3L4) finally dropped to 301.1 (AT4). The surface and core hardness variations for specimens of A, B, and C series were shown in Figure 11. It is reasonable to see that surface hardness is correspondingly higher than core hardness. The hardness variations of surface and core for A, B, and C series, however, follow the similar tendency. T3L4 is the optimal process for surface and core hardening for A, B, and C sheets. The maximum hardness elevation efficiencies of H
S and H
C for series A are 72.8% (H
S) and 47.5% (H
C). Those for B and C series are 92.0% (H
S), 95.1% (H
C) and 56.1% (H
S), 33.2% (H
C), respectively. Since the precipitating hardenability of specimens was gradually consumed while the hydrogen uptake of them increased with numbers of cyclic electrolytic hydrogenation, the hardening effect deriving from solid-solution strengthening of hydrogen eventually overrode that from precipitation hardening.Table 7
Hardening efficiency for typical specimens.
Process designation
H
S/HE
H
C/HE
A0
236.9
234.6
AT3
264.5/11.7%
—
AT3L4
409.3/72.8%
346.1/47.5%
AT4
301.1/27.1%
253.1/7.9%
B0
179.5
169.8
BT3
277.9/54.8%
—
BT3L4
344.7/92.0%
331.2/95.1%
BT4
288.2/60.6%
219.8/29.4%
C0
314.7
318.2
CT3
330.7/5.1%
—
CT3L4
491.1/56.1%
423.8/33.2%
CT4
348.1/10.6%
326.7/2.7%Variations of VHN for different treatments at (a) surface and (b) core.
(a)
(b)


## 4. Conclusions

(i)
No precipitates ofα phase were observed for Ti-153 alloy after vacuum annealed in the β-phase region (at 1000°C) by employing MOM and XRD but β grains grew significantly from 30 μm (A0) to 300 μm (B0) associated with evident annealing texture and softening. Aging at α-phase region (at 500°C) for 30 min led to almost no grain growth and texture change but appreciable hardness enhancement for C0 specimens.
(ii)
Application of cyclic heat treating at 300°C (lowerα-phase region) to A0, B0, and C0 specimens had nearly no influence on XRD patterns, while applying cyclic hydrogenation-solution treatment to those specimens led to significant hydrogen absorption and lattice dilatation. Hydrogen absorption from processing helped to increase the crystallinity of the specimens. The ascending order of hydrogen uptake was BT3L4, CT3L4, and AT3L4, while the volume expansion rates for AT3L4, BT3L4, and CT3L4 corresponding to A0, B0, and C0 ones were 3.90%, 2.04%, and 5.40%, respectively.
(iii)
A0, B0, and C0 sheets used in this study can be precipitation hardened by cyclic heat treating, however, with lower hardening efficiencies compared to those processed by employing cyclic hydrogenation-solution treatment. The process for the maximum HE ofH
S and H
C was BT3L4, while that for the maximum hardness was CT3L4. Since the precipitating hardenability of specimens was gradually consumed, the hardening effect deriving from solid-solution strengthening of hydrogen eventually overrode that from precipitation hardening. Process T3L4 is suitable for surface and core hardening for A, B, and C sheets.



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*Source: 160258-2014-03-12.xml*