Transcript Slide 1

Fabrication of Microchannel Devices Via Diffusion Bonding and Transient Liquid Phase Bonding Purpose:

To reduce the device size of microfluidic devices and heat exchanges to achieve higher efficiencies and better portability.

Previous Work: Present Diffusion Bonding

• • • • •

Materials:

Stainless Steel Shims 50 μm and 100 μm thick patterned with microchannels.

Pressure distribution plates Shims coated with nickel boron or nickel phosphorus Vacuum Hot Press Optical Microscope

Figure 1: schematic of vacuum hot press illustrating basic configuration of shims and microchannels to bond the device. Q is the heat delivered to the system and F is the force applied by the press.

Goals of diffusion bonding: 1. Minimize channel deformation.

2. Maximize the ratio of good channels to total channels.

3. Minimize bonding temperature and pressure, and therefore costs.

4. Maximize bonding efficiency.

Figure 3: Diffusion bonded stainless steel shims with channel deformation. Diffusion bonded shims at 1800 psi and 980 °C. The deformation is caused by too much pressure during bonding or cutting and polishing.

Present Work:

The present work is on un-coated shims. Each stack was arranged to maximize the vacuum hot press working time. Table 1 illustrates the parameters used for this experiment.

Method

:

Diffusion bonding and transient liquid phase bonding require pressure and heat Figures 1 and 2. The vacuum hot press can apply several tons force and up to 1200 °C to a stack of shims.

Vacuum Chamber and furnace Pressure Ram

• • Purpose of applying pressure and heat: Promote contact Increase diffusion speed

Figure 2: The vacuum hot press used to apply heat and pressure simultaneously to bond the shims.

The temperature must remain below the melting point of 316 stainless steel.

Special thanks to Steve Leith. Todd Miller, Jack Rundel, Danielle Clair, and Phillip Harding for all of their help and support.

Table 1: Diffusion bonding design of experiment used to maximize the information from each run. The two parameters varied per run are the temperature ramp rate and the shim span, which is the distance between channels on the shim.

Run 1 Run 2 Run 3 Run 4

Ramp up rate (

°

C/min)

2 8 8 2

Shim span (μm)

400 800 400 800

Dwell temperature (

°

C)

980 980 980 980

Dwell pressure (psi)

1000 1000 1000 1000

Dwell duration (minutes)

60 60 60 60

The shims are stacked to maximize information from each run. The stack is composed of four distribution plates and two thicknesses of shim, 50 μm and 100 μm as shown in Figure 4, which will be cut using a wire EDM and inspected.

10 shims 50 μm thick 5 shims 50 μm thick 5 shims 100 μm thick 10 shims 100 μm thick End blocks

Figure 4: An example of the shim stacks used to maximize data collected per run.

CBEE

Future Transient Liquid Phase Bonding

Transient liquid phase (TLP) bonding requires an interlayer between two parent metal shims. Using boron or phosphorus in a nickel interlayer will lower the melting point of the nickel hastening the bonding process, Figure 5.

1.

Interlayer melts 2. Melting point suppressant diffuses into the parent metal 3. The concentration of suppressant decreases 4. Interlayer solidifies 5. Bond homogenizes

Figure 5: The TLP bonding process. The interlayer melts, suppressant diffuses, and the bond solidifies

In preparation for future work on this project, modeling has been done for the interlayer thickness vs dwell time, Figure 6. 120

1065 °C

100

1100 °C

80

1150 °C

60 40

𝐶

𝛼𝐿

𝐶

𝑜

− 𝐶

𝑚

− 𝐶

𝑚

= 𝐸𝑅𝐹 𝑤 2 𝑡

𝑓

𝐷 𝐷 = 𝐷

𝑜

𝑒

−𝐸 𝑅𝑇 𝑎 20 0 0 20 40 60

Interlayer thickness (

μm)

80

Figure 6: Interlayer thickness vs dwell time in the vacuum hot press governed by the equations shown. D is the diffusion coefficient, t f concentration, C o is the dwell time, C is the initial concentration, and C m αL is the critical is the concentration at the interface of melting point suppressant in the interlayer. Thinner interlayers correspond to lower dwell times. Higher temperatures reduce dwell time due to the exponential effect of the temperature on diffusion coefficient.