This study suggests a new approach to diffusion bonding (DB) 316L stainless steel: a low-pressure procedure that includes a nickel interlayer. In this approach, relatively lower pressure is applied to the sample before the DB process, in contrast to the usual approach in which higher pressure is applied during the DB process. This new procedure was tested on mock-up 316L stainless steel tube-to-tubesheet joints, which simulated similar joints in coiled-tube heat-exchanger applications. This study confirms that the new procedure meets the overall success criteria, namely, a pull-out force exceeding the force required for tube rupture. It also shows that the DB joint is improved by the use of a Ni interlayer; the joint strength increased by approximately 33% for a 0.25 μm Ni interlayer and by approximately 18% for a 5 μm Ni interlayer. The joint cross sections were qualitatively examined using optical microscopy (OM) and scanning electron microscopy (SEM); the observations suggest that only portions of the interface were diffusion bonded, as a result of the low-pressure procedure and the surface roughness (due to the sample fabrication). The portions that were diffusion bonded, though, were sound, as characterized by the fact that the steel grains grew through the interface line to create a continuous metallographic structure.

Introduction

The Department of Nuclear Engineering at the University of California, Berkeley (UCB) is developing a coiled tube gas heater (CTGH) design, depicted in Fig. 1, that supports the use of Brayton-cycle power conversion for advanced nuclear reactors. UCB has developed an initial main design to transfer heat from a low-pressure 700 °C, fluoride-salt coolant (at approximately 0.1 MPa) to compressed air (at approximately 1.8 MPa), which is then expanded through a gas turbine to produce power [13]. UCB has also developed an alternative heat-exchanger design that uses supercritical carbon dioxide (S-CO2) instead of air, with low-pressure (0.1 MPa) liquid sodium metal as the primary coolant; this design requires operation at higher pressures (up to 20 MPa and 550 °C) [4]. Both of these designs thus require that the heat-exchanger tubes withstand the challenging combination of high-temperature and a high-pressure differential between the inside and the outside of the tubes. Furthermore, in contrast to pressurized-water-reactor steam-generator tubes that experience a net internal pressure and are loaded in radial tension, the tubes in a CTGH experience a net external pressure and are loaded in radial compression. This net external pressure works to weaken the tube-to-tubesheet joint. Due to these unusual conditions and concerns about conventional-fusion-welding defects [5] in the material, UCB has investigated diffusion-bonding (DB) technique for making the tube-to-tubesheet joints. UCB has focused specifically on joining tubes and tubesheets made out of 316L stainless steel (316L SS), because it is one of the candidate materials for service in the elevated temperatures, high-pressure differentials, and corrosive atmospheres of the CTGH.

Fig. 1
Schematic description of the CTGH (right) with enlarged area of the tubes connected to the hot inlet manifold (left) and picture of the tube-to-tubesheet joint sample (in the left corner)
Fig. 1
Schematic description of the CTGH (right) with enlarged area of the tubes connected to the hot inlet manifold (left) and picture of the tube-to-tubesheet joint sample (in the left corner)
Close modal

DB joints have been extensively investigated, and the main parameters are well known [6]: the roughness of the surfaces being joined and the temperature, time, atmosphere, and pressure of the heat-treatment process (i.e., the diffusion-bonding process). In conventional DB, the two pieces of the joint are pressed together with constant pressure during the heat treatment, but the geometric configuration of the tubes and tube manifold (tubesheet) in the CTGH (Fig. 1, left) makes it difficult to apply such pressure on those DB joints. Therefore, UCB has developed a novel joint procedure for low-pressure DB of these joints: Matching tapers are machined on the end of the tube and in the hole in the manifold, and the two components are press-fit together with low pressure prior to the DB heat treatment. The inset on the left part of Fig. 1 shows a mock-up of one of these tube-to-tubesheet joints, fabricated to simulate this specific area of the heat exchanger.

Several different DB procedures for making these DB joints have been investigated at UCB. Experiments with tapered interference fits, tube expansion, and hybrid friction diffusion bonding (HFDB) have been successfully conducted at UCB with thin-walled 316L SS tubes (OD: 6.35 mm (1/4 in.) and ID: 4.57 mm (0.18 in.)) [710]. This paper specifically describes the experiments on the procedure of using commercial plating techniques to apply a nickel (Ni) interlayer of various thicknesses onto the tubes to support the tube-to-tubesheet tapered interference fits. Such an interlayer, made from a “soft” material, was suggested as an improvement for the DB process of stainless steel by Kazakov [6] and Yeh and Chuang [11] and was described by many others [1216]. Ni was chosen here as the interlayer material since it is one of the major components of the 316L SS. The joint quality was evaluated quantitatively by pull-out testing as well as qualitatively by optical microscopy (OM) and scanning electron microscopy (SEM).

Setup and Experiment

In UCB's previous studies [710] of DB joining of thin-walled tubes to tubesheets, the pull-out force during testing was limited, by the small tube cross-sectional area, to approximately 8.7 kN. In the present study, rods were used instead of tubes to allow higher force to be developed on the joint. The tube was simulated by a rod (OD: 6.35 mm (1/4 in.)), and the tubesheet was simulated by a 12.7 mm (1/2 in.) thick collar. Figure 2 shows a drawing and a picture of a fabricated sample. Commercial 316L SS was used to fabricate the tube-to-tube sheet samples. The chemical composition of the 316L SS as provided by the vendor is given in Table 1. The composition was subsequently verified using SEM/energy dispersive X-ray spectroscopy (EDS).

Fig. 2
Technical drawing (in inches) and picture of the tube-to-tubesheet joint sample
Fig. 2
Technical drawing (in inches) and picture of the tube-to-tubesheet joint sample
Close modal
Table 1

Chemical composition (wt.%) of the 316L SS used in this study

CrNiCMnCuSiMoSPNTiFe
16–18.510–15<0.08<2<1<1<30.35<0.045<0.1<0.7Bal
CrNiCMnCuSiMoSPNTiFe
16–18.510–15<0.08<2<1<1<30.35<0.045<0.1<0.7Bal

The samples were fabricated on a computer numerical control machine or on a manual lathe, utilizing standard cutting tools. Three sample sets were fabricated (three samples in each group): group 1 samples with a 5 μm Ni interlayer, group 2 samples with a wood's nickel strike (WNS) interlayer, and group 3 reference samples without an interlayer. The 5 μm Ni interlayer was applied with a commercial electroless plating kit, following the manual instruction [17]. WNS is an electroplating process during which the protective oxide layer on the stainless steel is etched, while a thin Ni layer (approx. 0.25 μm [18]) is deposited at the same time. The literature contains several WNS procedures/parameters [1923], of which this study used the following:

  1. (1)

    24 g nickel chloride.

  2. (2)

    12.5 ml HCl.

  3. (3)

    Distilled water, to 100 ml solution.

  4. (4)

    Ni anode.

  5. (5)

    Cathodic process: The positive pole connects to the plating part; the negative pole connects to the Ni anode; current density of 5.4 × 10−4 A/mm2 for 2 min and then current density of 1.55 × 10−4 A/mm2 for an additional 2 min.

After fabrication, the samples were joined with 3 kN of assembly force, a value which was chosen with consideration to the final CTGH design (prevent tube buckling). The force was applied by using a tensile/compression testing machine or by using a manual press. When a manual press was used, the insertion depth of the rod (tube) into the tubesheet was measured, and the force was calculated by using Eq. (1) [24]. The contact pressure between the rod (tube) and the tubesheet was estimated using Eq. (2), and the procedure was presented by Buster et al. [7]. This process was termed “low-pressure DB,” since the assembly force that is used results in pressures much lower than those usually recommended for DB of stainless steel [6]
(1)
where Fp is the applied force, E is the Young's modulus, δ is the interference depth, Lc is the contact length, R is the collar outer radius, r is the collar bottom inner radius, and θ is the taper angle
(2)

where P is the interference pressure as a result of diametrical interference; Dt is the tube diameter, where o indicates the outer diameter and i the inner diameter; Δt+tol is the upper tolerance of the tube outer diameter; Ds is the tubesheet diameter, where o indicates the disk diameter and i the hole diameter; Δs−tol is the lower tolerance in the hole diameter; E is the Young's modulus, where t indicates the tube and s the tubesheet; and ν is the Poisson's ratio.

The heat treatment was conducted in a vacuum furnace at 1000 °C for 1000 min, as recommended by Haneklaus et al. [9]. A moderate vacuum (approx. 10−1 mBar) was chosen here to allow slight oxidation of the surfaces, which served to highlight the interfacing surfaces in the postmortem micrographs and thereby to make easier the evaluation of the DB quality.

The quality of the DB joint between the tapered tube-to-tubesheet fitting surfaces was determined primarily by measuring the load required to pull the rod out of the tubesheet. Quantitative pull-out testing was described by Massey and Jones [25] as an “established method” to determine the quality of heat-exchanger joints. Kikuchi et al. [26] used this criterion to determine the quality of the tube-to-tubesheet joints of the Japan sodium-cooled fast reactor (JSFR) heat-exchanger tubes, which have to withstand similar pressure differentials as the tubes in the UCB CTGH do. In contrast to the traditional configuration of pull-out testing [25,26] though, the pull-out testing in this study was conducted with a computer-controlled tensile/compression testing machine, made by MTS Systems Corporation, Eden Prairie, MN. The sample was mounted in an adaptor, and the test was run as a tensile test. Figure 3 depicts the adaptor apparatus and the sample setup in the MTS testing machine.

Fig. 3
Pictures of the sample and the adaptor (left) and the sample setup on the MTS testing machine (right) for the pull-out test
Fig. 3
Pictures of the sample and the adaptor (left) and the sample setup on the MTS testing machine (right) for the pull-out test
Close modal

Results

Table 2 summarizes the results of the different sample groups and the improvement (by percentage) for the different categories. The mean pull-out force was 9.07 kN (o′ = 3.8 kN) for the reference samples, 10.7 kN (o′ = 1.5 kN) for the samples with the 5 μm Ni interlayer, and 12.1 kN (o′ = 5.4 kN) for the samples with WNS. The mean pull-out force on these rods can be used to estimate the stress in a tubular cross section.

Table 2

Results summary of the three different groups: reference, 5 μm Ni interlayer, and WNS interlayer samples as well as results from the previous studies for 6.35 mm (1/4 in.) thin-walled tube samples

Thin wall tubeReference samples5 μm Ni interlayerWNS interlayer
Force (kN)8.7 ± 0.29.07 ± 3.810.7 ± 1.512.1 ± 5.4
Pressure on thin wall tube (MPa)570 ± 13594 ± 249701 ± 98793 ± 353
Equivalent ID (mm)4.57+0.054.48+0.864.05+0.403.65+1.39
−0.05−1.08−0.44−2.59
Equivalent wall thickness (mm)0.89 ± 0.020.94 + 0.541.15+0.221.35+1.27
−0.44−0.2−0.69
Load improvement (%)Ref.∼18∼33
Wall thickness improvement (%)Ref.∼22∼43
Thin wall tubeReference samples5 μm Ni interlayerWNS interlayer
Force (kN)8.7 ± 0.29.07 ± 3.810.7 ± 1.512.1 ± 5.4
Pressure on thin wall tube (MPa)570 ± 13594 ± 249701 ± 98793 ± 353
Equivalent ID (mm)4.57+0.054.48+0.864.05+0.403.65+1.39
−0.05−1.08−0.44−2.59
Equivalent wall thickness (mm)0.89 ± 0.020.94 + 0.541.15+0.221.35+1.27
−0.44−0.2−0.69
Load improvement (%)Ref.∼18∼33
Wall thickness improvement (%)Ref.∼22∼43

Figure 4 shows the representative, post-testing pictures of the rod surfaces on which DB occurred: a reference sample (left), a WNS sample (center), and 5 μm sample (right) are depicted. The improved DB on the WNS sample resulted in visible areas where base material is peeled off from the rod. Areas with such sound DB are smaller on the 5 μm sample and much smaller on the reference sample. The light oxidation of the surfaces, as shown in Fig. 4, suggests insufficient surface contact, since with ideal surface-matching, the touching areas should not have been exposed to the oxygen environment.

Fig. 4
Pictures of the rod pull-out areas of the reference sample (left), the WNS interlayer sample (center), and 5 μm sample (right). The 5 μm sample and the reference sample show smaller and much smaller areas of sound DB than the WNS interlayer sample shows, respectively.
Fig. 4
Pictures of the rod pull-out areas of the reference sample (left), the WNS interlayer sample (center), and 5 μm sample (right). The 5 μm sample and the reference sample show smaller and much smaller areas of sound DB than the WNS interlayer sample shows, respectively.
Close modal

In addition to quantitative pull-out testing, which was the success criterion of the study, qualitative analysis using OM and SEM was also conducted. Figure 5 shows representative SEM pictures of a reference sample (left) and a sample with 5 μm interlayer (right). The pictures show that the low pressure applied prior to DB was not sufficient to overcome the surface asperities induced by the cutting tool. Though the pressure was not sufficient to force the induced asperities to yield, partial DB could be observed with the OM and SEM.

Fig. 5
SEM pictures of the DB interface of a reference sample (left) and a 5 μm Ni interlayer sample (right) showing the result of surface roughness induced by the surface machining in cross section and partial DB on the matching interface
Fig. 5
SEM pictures of the DB interface of a reference sample (left) and a 5 μm Ni interlayer sample (right) showing the result of surface roughness induced by the surface machining in cross section and partial DB on the matching interface
Close modal

When the asperities yielded and the stainless steel's protective oxidation layer broke, sound DB was observed. In these areas, the material grains grow through the interface matching line (tube-to-tubesheet interface). Figures 6 and 7 (right) are micrographs of these areas, taken with OM and SEM/electron backscatter diffraction (EBSD), respectively. Figure 6 depicts the material grain growth through the tube-to-tubesheet interface line to create a continuous metallographic structure. Figure 7 compares the partial DB area (left picture) to the sound DB area (right picture); the sound DB is characterized by a continuous metallographic structure. The figure reveals that the tubesheet grains (bottom portion of pictures of Fig. 7) are twice the size of the rod (tube) grains (top portion), which is a consequence of the different manufacturing processes for the two components.

Fig. 6
OM picture where sound DB was observed; the material grains grow through the tube-to-tubesheet interface line to create a continuous metallographic structure
Fig. 6
OM picture where sound DB was observed; the material grains grow through the tube-to-tubesheet interface line to create a continuous metallographic structure
Close modal
Fig. 7
SEM/EBSD pictures; partial DB area (left) and sound DB area (right)
Fig. 7
SEM/EBSD pictures; partial DB area (left) and sound DB area (right)
Close modal

Conclusions

This study confirms that low-pressure DB of press-fit, 316 L stainless steel tube-to-tubesheet joints (with the tube simulated by a rod) meets the overall success criteria, namely, a pull-out force exceeding the force required for tube rupture. This study also suggests that the DB joint can be improved by using a Ni interlayer (Table 2; Fig. 4). The pull-out force increased by 18% when 5 μm, electroless-plated Ni interlayer was used and by 33% when an electroplated WNS interlayer (0.25 μm thick) was used. The SEM analysis and the visual observation of slight oxidation of the surfaces confirm the challenge of manufacturing perfectly matching surfaces. Imperfect matching of surfaces resulted in areas where the rod's surface could not be pressed against the tubesheet's surface with the necessary pressure, resulting in only partial DB of the two parts, as shown in Figs. 5 and 7 (left). The sound DB areas were characterized by the growth of material grains through the tube-to-tubesheet interface line to create a continuous metallographic structure (Figs. 6 and 7 right). The imperfection in surface matching may be resolved by using additional manufacturing techniques, such as grinding, to create smoother surfaces and thus better surface-matching.

Acknowledgment

The authors want to express their gratitude to the operators of the Mechanical Engineering Machine Shop at UCB, without whose guidance and assistance this work would have not been possible. This research was performed using funding received from the Nuclear Energy University Programs of the Office of Nuclear Energy in the U.S. Department of Energy (DOE).

Nomenclature

CTGH =

coiled tube gas heater

Dsi =

tubesheet hole diameter, mm

Dso =

tubesheet disk diameter, mm

Dti =

tube inner diameter, mm

Dto =

tube outer diameter, mm

DB =

diffusion bonding

E =

Young's modulus, Pa

Es =

Young's modulus of tubesheet material, Pa

Et =

Young's modulus of tube material, Pa

EBSD =

electron backscatter diffraction

EDS =

energy dispersive X-ray spectroscopy

Fp =

applied force, N

HFDB =

hybrid friction diffusion bonding

JSFR =

Japan sodium-cooled fast reactor

Lc =

contact length, mm

OM =

optic microscopy

P =

interference pressure as a result of diametrical interference, Pa

r =

collar bottom inner radius, mm

R =

collar outer radius, mm

SEM =

scanning electron microscopy

S-CO2 =

supercritical carbon dioxide

UCB =

University of California, Berkeley

νs =

Poisson's ratio of the tubesheet disk material

νt =

Poisson's ratio of the tube material

WNS =

wood's nickel strike

δ =

interference depth, mm

Δs−tol =

lower tolerance in the hole diameter, mm

Δt+tol =

upper tolerance in the tube outer diameter, mm

θ =

taper angle

μ =

static friction coefficient

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