Method of manufacturing hexagonal boron nitride laminates

Abstract

A method of manufacturing a hexagonal boron nitride laminate contains steps of: a) Dissolve dielectric polymers in solvent. b) Mixing h-BN powder to form a well-mixed h-BN coating slurry. c) Coating slurry on substrates and dried at 100-150° C. The substrates can directly be etched or processed to form electric circuits. Substrates can also be completely etched or detached to attain a free standing laminate. Thereby, a hexagonal boron nitride laminate exhibit thermal conductivity of 10 to 40 W/m.Math.K, which is significantly larger than that currently used in thermal management. In addition, thermal conductivity of hexagonal boron nitride laminates increases with the increasing mass density, which opens a way of fine tuning of its thermal properties. For heat dissipation application, hexagonal boron nitride laminate coating can significantly enhance the performance of LED light bulb.

Claims

1. A method of manufacturing a hexagonal boron nitride laminate according to a preferred embodiment of the present invention contains steps of: a) Dissolve 30 wt % to 80 wt % dielectric polymers in solvent. b) Mixing 20 wt % to 0 wt % h-BN powder to form a well-mixed h-BN coating slurry. c) Coating slurry on a substrate and dried at 100° C. to 150° C. A layer of h-BN laminates was obtained after this process.

2. The method of manufacturing a hexagonal boron nitride laminate as claimed in claim 1, wherein the dielectric polymer is flexible after curing with thickness of film ranging from 5 um to 200 um, and the dielectric polymer is selected from groups comprising polyethylene terephthalate (PETP), polyphenylene sulfide (PPS), polyetherimide (PEI), polyetherether ketone (PEEK), polyetherketone (PEK), polyimide (PI), Polyvinylidene fluoride (PVDF), phenol resin and acrylic resins.

3. The method of manufacturing a hexagonal boron nitride laminate as claimed in claim 1, the h-BN powder is flake powders with 2-D layer structure. The thickness of h-BN powder ranges from 0.34 nm to 500 nm, and the diameter is from 0.1 nm to 100 μm.

4. The method of manufacturing a hexagonal boron nitride laminate as claimed in claim 1, wherein the substrates are the backside of filament of LED light bulb.

5. The method of manufacturing a hexagonal boron nitride laminate as claimed in claim 4, wherein the filament substrate of LED light bulb is selected from the group of metals, ceramics, or polymer composites.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0015] FIG. 1(A) is a SEM micrograph of the surface of the hBN laminate, wherein vertical variations of contrast are due to the charging, and scale bar is 1 μm.

[0016] FIG. 1(B) is a cross-sectional SEM image of hBN laminate, wherein scale bar is 10 μm.

[0017] FIG. 2 shows thermal conductivity κ as a function of temperature T measured for different values of hBN laminates density ρ.

[0018] FIG. 3 shows thermal conductivity κ hBN laminates as a function of density measured at 80° C. (blue circles), wherein solid curves represent results of numerical simulations at different values of the thermal contact conductance.

[0019] FIG. 4 is a schematic view illustrating the laminate model used in numerical simulations for low (A) and high (B) density samples, wherein an individual hBN flake is modeled by a solid block with lateral dimensions 1 μm×1 μm and thickness 10 nm.

[0020] FIG. 5 is a schematic view illustrating a test of junction temperature of a chip on an LED filament with/without hBN-coating.

[0021] FIG. 6 is a schematic view illustrating a test result of the junction temperature of the chip on the LED filament with/without hBN-coating.

[0022] FIG. 7 is a schematic view illustrating luminous efficiency of the LED light bulb assembled by the LED filament with/without hBN-coating.

[0023] FIG. 8 shows aging test data of the non-coated LED metal filament fixed on the light bulb of 8 W.

[0024] FIG. 9 shows aging test data of the h-BN-coated LED metal filament fixed on the light bulb of 8 W.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0025] A method of manufacturing a hexagonal boron nitride laminate according to a preferred embodiment of the present invention contains steps of:

[0026] a) Dissolve 30 wt % to 80 wt % dielectric polymers in solvent.

[0027] Preferably, the dielectric polymer is selected from groups comprising polyethylene terephthalate (PETP), polyphenylene sulfide (PPS), polyetherimide (PEI), polyetherether ketone (PEEK), polyetherketone (PEK), polyimide (PI), Polyvinylidene fluoride (PVDF), phenol resin and acrylic resins.

[0028] Preferably, the dielectric polymer is flexible after curing with thickness of the film ranging from 5 um to 200 um.

[0029] b) Mixing 20 wt % to 70 wt % h-BN powder to form a well-mixed h-BN coating slurry.

[0030] Preferably, the thickness of h-BN powders ranges from 0.34 nm to 500 nm, and the diameter is from 0.1 μm to 100 μm.

[0031] c) Coating slurry on a substrate and dried at 100° C. to 150° C. A layer of h-BN laminate was obtained after this process.

[0032] Preferably, the substrates are electrically conductive layers such as Cu or Al foils.

[0033] Preferably, the thickness of the conductive layer ranges from 10 um to 100 um.

[0034] Preferably, the conductive layer can be further etched or processed to form electric circuit.

[0035] Preferably, the conductive layer can be thoroughly etched or detached to attain a free-standing laminate.

[0036] In FIG. 1, analysis of the top and cross-sectional SEM images of the laminate film reveal the dominant lateral dimensions of hBN laminate film are around 1 μm with average thickness of about 10 nm. The SEM figures also reveal how hBN powders construct heat dissipation channels to exhibit its high thermal conductivity. FIG. 1A shows the lateral contacts between hBN powders, while FIG. 1B illustrates an amorphous stacking of hBN powders in cross sectional view, which ensures the heat could be dissipated to all directions.

[0037] The thermal conductivity κ of the investigated laminate has been calculated using equation

κ=αρC.sub.p,   (1)

[0038] here α is the in-plane thermal diffusivity, ρ is the material density and C.sub.p is the specific heat. All three parameters were independently determined in experiment.

[0039] The thermal diffusivity α as a function of temperature T has been measured by the laser flash method using commercially available system (Netzsch LFA 457). To measure the in-plane thermal diffusivity the special sample holder has been used, which accommodates the free-standing hBN membrane samples cut into a round shape of 22 mm in diameter. A small spot of about 5 mm in diameter at the back side of the sample is flash heated by the laser beam. The heat diffusion as a function of time is registered by the infrared detector along the top circumference of the membrane at 5 mm to 6 mm from the centre of the sample. To avoid undesirable reflections the sample and sample holder have been spray coated with graphite paint. During the measurements the sample chamber of the laser flash system was continuously purged with nitrogen gas at the rate of 30 nal/min. The sample specific heat C.sub.p was measured by the differential scanning calorimeter (Netzsch DSC 404 F3) using sapphire as a reference sample. The mass density ρ was estimated by weighting the sample of the known dimensions with precision electronic balances.

[0040] To evaluate the effect of the membrane composition we measured the thermal conductivity κ as a function of temperature T for four hBN laminates with different mass density. As seen from FIG. 2, the thermal conductivity is weakly dependent on temperature and increases with the increasing density. The observed values of the thermal conductivity fall in the range between 10 W/m.Math.K to 20 W/m.Math.K, which is certainly an industrially relevant value.

[0041] To better understand the influence of the material density on the thermal conductivity we studied the dependence of κ on ρ at room temperature. The density of the laminate samples was controlled in two different ways: (i) by using hBN flakes of different thickness (only limited variations of ρ could be achieved in this way), and (ii) by variation of the additional roller compression applied during preparation of the laminates. Both methods had the same effect on the thermal conductivity. The combined results of this study are presented in FIG. 3. Similarly to the data shown in FIG. 2 the thermal conductivity tends to increase with the increasing density of the hBN laminate.

[0042] After systematic SEM examination of the laminates of different density, we concluded that the density variations are mostly due to the variation in the size of empty voids present between stacked hBN flakes. The schematic representation of two laminates with different density is given in FIG. 4. Thus we attribute the decreasing thermal conductivity to the discontinuity in the thermal path brought by the larger number of voids.

[0043] To confirm our suggestions, we carried out modeling of the thermal flow in laminates with voids. Our numerical simulation was done using ABAQUS 2011 finite element analysis software package. In order to explore the relation between the effective thermal conductivity and the density of hBN laminates we simulated the steady-state heat transfer governed by equation

[00001]$\begin{array}{cc}\rho .Math..Math.C_p.Math.\frac{\partial T}{\partial t}=\frac{\partial }{\partial x}.Math.\left(\frac{\kappa \left(T\right).Math.\partial T}{\partial x}\right)+\frac{\partial }{\partial y}.Math.\left(\frac{\kappa \left(T\right).Math.\partial T}{y}\right)+\frac{\partial }{\partial z}.Math.\left(\frac{\kappa \left(T\right).Math.\partial T}{\partial z}\right)+Q,& \left(2\right)\end{array}$

[0044] where Q is the heat flux and ∂T/∂t=0 (steady-state heat transfer). The modeled system was evaluated with the ABAQUS element type DC2D8 and represented by a strip of orderly stacked solid blocks of thermally conductive media with lateral size of 1 μm×1 μm and thickness of 10 nm, as show in FIG. 4. To mimic the hBN flakes the thermal conductivity of the solid blocks was chosen to be 390 W/m.Math.K at room temperature. To vary the effective density of the modeled laminates, we adjusted the overlap area of the adjacent blocks as illustrated in FIGS. 4(A) and 4(B). Also, to account for the imperfect thermal contact between the stacked flakes the finite thermal contact conductance has been introduced to the model. The final modeling results were matched to the experimental data by variation of the thermal contact conductance in the range of 10.sup.5 W/m.sup.2K to 10.sup.6 W/m.sup.2K. The resulting effective thermal conductivity κ.sub.eff of the hBN laminate was calculated using the Fourier law

[00002]$\begin{array}{cc}{\kappa }_{\mathrm{eff}}=q.Math.\frac{L}{\Delta .Math..Math.T}.& \left(3\right)\end{array}$

[0045] Here q is the total net heat flux through the cross section of the laminate, L is the total length of the laminate strip and ΔT is the temperature difference between hot and cold ends of the strip.

[0046] The result of the numerical simulation is shown by solid curves in FIG. 3. Each of the curves represents the effective thermal conductivity of the laminate with different thermal contact resistance between the stacked hBN flakes. The simulation shows only qualitative agreement with the experimental data because of simplicity of our model. A more accurate simulation would have to take into account size distribution of the flakes as well as the dependence of the contact conductance on the packing density. Nevertheless, our initial assumption that the thermal conductivity is restricted by the presence of the empty voids inside the laminate has been confirmed by this simple model. Also, it gave us a rough estimate of the thermal contact conductance to be of the order of 10.sup.6 W/m.sup.2.Math.K. There is no data on the thermal contact conductance is available for such a system, however experimental study of a rather similar graphene/hBN interface reveals the value of around 7.Math.10.sup.6 W/m.sup.2.Math.K, which is almost an order of magnitude higher than estimated in our simulation. The most probable explanation to this is the fact that the hBN flake surfaces are contaminated with solvent residues, which in turn reduces thermal conductivity across the flake-to-flake interface.

[0047] In conclusion, we demonstrated that hBN inks can be used to produce laminates with thermal conductivity as high as 20 W/m.Math.K in the above mentioned embodiment, which is significantly larger than that for materials currently used in thermal management. We also show that the effective thermal conductivity can be adjusted by varying the laminate packing density. We also identify a potential way for further increase in of thermal conductance by improving the quality of the flake-to-flake interface. Being electrically insulating, hBN laminates can potentially open a new avenue for using the advanced thermal management materials.

[0048] As shown in FIGS. 5-7, further comparisons of heat dissipation ability and light bulb performance between LED metal filaments with and without coating hBN material were carried out in order to exhibit our invention of hBN on LED heat dissipation application, thus obtaining a heat dissipation result of the LED light bulb assembled by the LED filament with and without hBN coating. Thereby, after the hBN coating material is coated on an LED metal filament of the LED light bulb, a junction temperature of a chip of the LED light bulb is lower that of non-coated LED light bulb. In high current condition, a difference of the junction temperature of the chip of the LED light bulb increases, hence the hBN coating material reduces the temperature of the chip of the LED light bulb and enhances luminous efficiency of the chip of the LED light bulb.

[0049] As illustrated in FIGS. 8 and 9, the junction temperature of the LED light bulb is reduced so as to lighting time of LED light bulb. According to the Energy Star test standards, compared with the non-coated LED bulbs, the LED light bulb on which the hBN coating material is coated, the light time of the LED light bulb is up to 20,000 hours, but the lighting time of the non-coated LED bulbs on which the hBN coating material is not coated, is 15,000 hours. While the preferred embodiments of the invention have been set forth for the purpose of disclosure, modifications of the disclosed embodiments of the invention as well as other embodiments thereof may occur to those skilled in the art. Accordingly, the appended claims are intended to cover all embodiments which do not depart from the spirit and scope of the invention.