CN102184902A - Porous alloy heat pipe radiator with gradient composite structure - Google Patents

Porous alloy heat pipe radiator with gradient composite structure Download PDF

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CN102184902A
CN102184902A CN 201110094194 CN201110094194A CN102184902A CN 102184902 A CN102184902 A CN 102184902A CN 201110094194 CN201110094194 CN 201110094194 CN 201110094194 A CN201110094194 A CN 201110094194A CN 102184902 A CN102184902 A CN 102184902A
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porous alloy
condensing zone
porous
zone
evaporating area
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CN102184902B (en
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陈岩
张树生
郭雷
常威
陈雅群
田帅
霍梦佳
位红燕
安保睿
陈婷婷
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Shandong University
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Abstract

The invention provides a porous alloy heat pipe radiator with a gradient composite structure, comprising a shell, wherein a working medium filling opening and an exhaust opening are arranged on the shell; the working medium filling opening is arranged at the bottom of the shell; the exhaust opening is arranged on the upper end face of the shell; an evaporation zone, an adiabatic zone and a condensing zone are arranged from bottom to top in the shell; and three zones are filled with porous alloys, the average pore size of the porous alloys in the evaporation zone is minimum, the average pore size of the porous alloys in the condensing zone is maximum and the average pore size of the porous alloys in the adiabatic zone is between the average pore size of the porous alloys in the evaporation zone and the average pore size of the porous alloys in the condensing zone. In the invention, the evaporation zone, the adiabatic zone and the condensing zone which are filled with the porous-alloys and arranged inside the radiator have different pore sizes and porosities; and therefore, the radiator has the characteristics of strong heat dissipation capability, good permeability and high heat conductivity and the heat dissipation effect can be effectively improved.

Description

A kind of porous alloy heat-pipe radiator with gradient composite construction
Technical field
The present invention relates to a kind of porous alloy heat-pipe radiator that is used for dissipation from electronic devices, belong to the dissipation from electronic devices technical field.
Background technology
Development along with digitlization and network informationization, demand to microelectronic component performance and speed is more and more higher, at present, semiconductor technology has entered nanometer scale, can on the IC chip, make more transistor, based on light and need the demand of integration function, also develop at present towards the system single chip direction.Among the IC during active device computing such as transistor, produce a large amount of heats, along with transistorized number in the chip is more and more, caloric value is also increasing, under the situation that chip area does not significantly increase thereupon, device heating density is more and more higher, problems of excessive heat has become the bottleneck of present restriction electronic device technical development, is example with CPU, and its caloric value increases gradually along with the raising of speed, reached at present more than the 115W, corresponding density of heat flow rate also increases considerably.Heat dissipation problem has become the biggest obstacle of restriction microelectronic component development, and has caused concern widely.
The microelectronic component caloric value improves constantly, and the heat dissipation technology that is complementary is not with it in time caught up with, and makes the development of CPU face great bottleneck gradually.Estimate according to ITRS, 2006 every DRAM (dynamic random access memory) caloric value will from about 1W, be increased to 2W.In order to enlarge the memory module capacity, present many companies begin to adopt 3D to pile up the encapsulation of form, though improved the application efficiency of chip, also make heat dissipation problem seem more and more important, according to statistics, account for over half that electronic device lost efficacy by the caused inefficacy of heat.Temperature is too high to cause the damage of semiconductor device except meeting, also can cause electronic reliability to reduce and decreased performance, for the solution of heat dissipation problem, must seek comprehensive technical solution scheme.In addition, heat dissipation problem also is one of key technology difficult problem that influences the LED life-span.
Common porous core heat exchanger generally comprises evaporating area, adiabatic region and condensing zone, each zone is to adopt compacted density, the aperture porous alloy heat pipe identical with porosity, in microstructure, when working medium undergoes phase transition, its internal pressure can sharply increase, cause poor permeability, thermal conductivity reduces, and influences radiating effect.
Summary of the invention
The present invention is directed to the problem that existing dissipation from electronic devices technology exists,, good penetrability strong according to heat-sinking capability that metal porous alloy had, the characteristics that thermal conductivity is high provide a kind of good heat dissipation effect, can satisfy the porous alloy heat-pipe radiator with gradient composite construction of the microminiaturized development of electronic product to the heat dissipation technology demand.
Porous alloy heat-pipe radiator with gradient composite construction of the present invention is by the following technical solutions:
This porous alloy heat-pipe radiator, comprise housing, housing is provided with working medium filling mouth and exhaust outlet, the bottom of housing is provided with working medium filling mouth, the upper surface is provided with exhaust outlet, be divided into evaporating area, adiabatic region and three zones of condensing zone in the housing from bottom to top, all fill full porous alloy in three zones, the average pore size minimum of porous alloy in the evaporating area, the average pore size maximum of porous alloy in the condensing zone, the average pore size of porous alloy is in evaporating area in porous alloy average pore size and the condensing zone between the porous alloy average pore size in the adiabatic region.Porous alloy can be the porous alloy of existing various structure types.
The evaporating area height H 1, the condensing zone height H 3With the adiabatic region height H 2Distribution be:
Figure BDA0000055392580000021
Figure BDA0000055392580000022
With
Figure BDA0000055392580000023
H wherein 1Be the height of evaporating area 7, H 2Be the height of adiabatic region 5, H 3Be the height of condensing zone, H is three region height sums; V lBe liquid phase topping up volume, φ 1Be the porosity of evaporating area porous alloy, V gBe gaseous phase volume, φ 3Be the porosity of condensing zone porous alloy, L is the length in arbitrary zone, and W is the width in arbitrary zone.
The mean pore size of porous alloy obtains by following formula in evaporating area, adiabatic region and the condensing zone: ln (p/p 0(the 2 γ V of)=- m/ rRT) cos θ, in the formula, in the formula, p 0Saturated vapour pressure when being the plane for the working media liquid level, p are the saturated vapour pressure of liquid-working-medium in the porous alloy, V mBe the molal volume of corresponding phase, γ is the surface tension of corresponding phase in each district, and R is a constant, and T is an absolute temperature, and θ is the contact angle of liquid-working-medium and porous alloy metal level wall; When correspondence is meant real work mutually, the situation of working media in radiator evaporating area, adiabatic region and the condensing zone, the evaporating area working media is a liquid phase, and the adiabatic region working media is the vapour-liquid two-phase, and the condensing zone working media is a vapour phase.
Porous alloy evaporating area, adiabatic region and the condensing zone of radiator of the present invention inside have different apertures and porosity, have that heat-sinking capability is strong, a good penetrability, characteristics that thermal conductivity is high, can effectively improve radiating effect.
Description of drawings
Accompanying drawing is a structural representation of the present invention.
Wherein, 1, housing, 2, exhaust outlet, 3, condensing zone, 4, adiabatic region and condensing zone critical surface, 5, adiabatic region; 6, evaporating area and adiabatic region critical surface, 7, evaporating area, 8, working medium filling mouth.
Embodiment
As shown in drawings, the porous alloy heat-pipe radiator with gradient composite construction of the present invention comprises housing 1, and the bottom of housing 1 is provided with working medium filling mouth 8, and the upper surface is provided with exhaust outlet 2.Be divided into evaporating area 7, adiabatic region 5 and 3 three zones of condensing zone in the housing 1 from bottom to top, be respectively evaporating area and adiabatic region critical surface 6 and adiabatic region and condensing zone critical surface 4 between the adjacent area.All filling full porous alloy in three zones steams.Send out the average pore size minimum of porous alloys in the district 7, the aperture of porous alloys is on average maximum in the condensing zone 3, and the average pore size of porous alloys is in evaporating area 7 in porous alloy average pore size and the condensing zone 3 between the porous alloy average pore size in the adiabatic region 5.
In evaporating area 7, fill liquid phase working fluid (liquid phase working fluid mainly is in evaporating area 7) by the working medium filling mouth 8 of housing 1 bottom.Radiator is when real work, and working medium mainly is liquid phase in the evaporating area 7, and working medium is the vapour-liquid two-phase in the adiabatic region 5, and working medium mainly is vapour phase in the condensing zone 3.
According to radiator caloric receptivity (Q 1) and heat dissipation capacity (Q 2), the size of determining the physical dimension of radiator of the present invention and rationally dividing evaporating area 7, adiabatic region 5 and condensing zone 3.According to the phase difference of working medium at evaporating area 7, adiabatic region 5 and condensing zone 3, each regional porous alloy is designed to the complex gradient structure, that is: the aperture minimum of porous alloys in the evaporating area 7, the aperture maximum of porous alloys in the condensing zone 3, the aperture of porous alloys is in evaporating area 7 in porous alloy aperture and the condensing zone 3 between the porous alloy aperture in the adiabatic region 5.
The heat dissipation environment of condensing zone 3 is generally relatively stable, and so, the heat that discharges at condensing zone also can keep relative stability.In design process, to consider:
1.Q 1, P, v 1Between logical relation;
When the heat of evaporating area 7 absorptions equaled the heat of condensing zone 3 releases, its internal pressure P changed little; And the heat that the heat that absorbs when evaporating area 7 discharges greater than condensing zone 3 constantly, and its internal pressure P must increase, and causes the medium elevation of boiling point, and phase transformation slows down, heat transfer rate v 1Descend, the heat sink temperature rises, until influencing its operate as normal.
2. the influence of aperture, porosity and pressure P;
Owing to do not consider the change in volume that Working fluid phase changing causes, the consequently increase of the heat that absorbs along with evaporating area 7, the ratio of its inner vapour phase and liquid phase changes, for keeping the relatively stable of P, and will appropriate design evaporating area 7, the height H of adiabatic region 5 and condensing zone 3 1, H 2And H 3Relative size.Detailed process is held as follows:
Utilize the continuity equation of saturated porous alloy, Darcy's law, the energy equation of consideration gravitational effect that trizonal working medium transport process is carried out mathematical modeling:
∂ ( φρ ) ∂ τ + ▿ · ( ρv ) = 0 - - - ( 1 )
In the formula, φ is the porosity of porous alloy, and ρ is the density of fluid, and v is the superficial velocity of fluid.
q V = - kA μL [ ( p 1 - p 2 ) + ρgL ] - - - ( 2 )
In the formula, q VBe volume flow, k is the permeability of porous alloy, and μ is the dynamic viscosity of fluid; A is that cell cross-section is long-pending, and L is a cell cube length.
( ρc ) m ∂ T ∂ τ + ( ρ c P ) f V · ▿ T = ▿ · ( λ m ▿ T ) + φ q m ′ ′ ′ - - - ( 3 )
Wherein (ρ c) m=(1-φ) (ρ c) s+ φ (ρ c p) fλ m=(1-φ) λ s+ φ λ fQ ' " m=(1-φ) q ' " s+ φ q ' " f
In the formula, subscript s and f represent that respectively solid phase and fluid are mutually; C is the specific heat of solid; c pSpecific heat at constant pressure for fluid; λ is a conductive coefficient; Q ' is " for the heat of the unit volume that endogenous pyrogen produced.
Use fractal theory then, set up the expression formula of porous alloy porosity and permeability:
φ = V p V b = ADπ 4 A 0 ( 3 - D - D T ) L 0 D T - 1 λ max 3 - D - D T ( 1 - τ 3 - D - D T ) - - - ( 4 )
k = μ L 0 Q Δp A 0 = π 128 A A 0 D 3 + D T - D L 0 1 - D T λ max 3 + D T - D - - - ( 5 )
In the formula, D is a porous alloy distribution of pores fractal dimension, D TBe the tortuous fractal dimension of porous alloy hole, Q then is the total flow by the unit section A.
The mean pore size that obtains pairing porous alloy in evaporating area, adiabatic region and the condensing zone according to the parameter expression of above acquisition is:
ln(p/p 0)=-(2γV m/rRT)cosθ (6)
In the formula, p 0Saturated vapour pressure when being the plane for the working media liquid level, p are the saturated vapour pressure of liquid-working-medium in the porous alloy, V mBe the molal volume of corresponding phase, γ is the surface tension of corresponding phase in each district, and R is a constant, and T is an absolute temperature, and θ is the contact angle of liquid-working-medium and porous alloy metal level wall; When correspondence is meant real work mutually, the situation of working media in radiator evaporating area, adiabatic region and the condensing zone, the evaporating area working media is a liquid phase, and the adiabatic region working media is the vapour-liquid two-phase, and the condensing zone working media is a vapour phase.
Porosity according to obtaining obtains evaporating area 7, condensing zone 3 and adiabatic region 5 and highly distributes:
Figure BDA0000055392580000042
Figure BDA0000055392580000043
With
Figure BDA0000055392580000044
H wherein 1Be the height of evaporating area 7, H 2Be the height of adiabatic region 5, H 3Be the height of condensing zone, H is three region height sums; V lBe liquid phase topping up volume, φ 1Be the porosity of evaporating area porous alloy, V gBe gaseous phase volume, φ 3Be the porosity of condensing zone porous alloy, L is the length in arbitrary zone, and W is the width in arbitrary zone.
The most important condition that the working medium of filling in the housing is selected is that working temperature should be between the solidifying point and critical point of working medium.According to universal experience, centering, Cryo Heat Tube, the general rule of screening working medium is under minimum operating temperature, interior pressure should be greater than 0.1 atmospheric pressure; Under maximum operating temperature, interior pressure should be less than 10~20 atmospheric pressure.Working temperature preferably is selected near the normal boiling point, is pressed in about an atmospheric pressure in promptly.The influence of working medium rerum natura opposite heat tube heat-transfer capability reduces a number group, and following form can be arranged:
N = σ · ρ l · h fg μ l - - - ( 7 )
In the formula, N is the transmission factor; σ is the surface tension coefficient of liquid; ρ lBe fluid density; h FgThe latent heat of vaporization for liquid; μ lDynamic viscosity for liquid.The transmission factor of working medium is high more, and then heat-transfer capability is strong more, and the working medium so as can be seen from formula should have high surface tension, the high latent heat of vaporization, characteristics such as wetability is good, and viscosity is little.
Working medium filling weight M should be:
M=ρ lV lvV v (8)
V in the formula l---evaporating area (V l) the volume V of receiving fluids 1=ε A wl
V v---vapor space volume V v=A vl
So
M V v = ( V l V v ρ l + ρ v ) = ( ϵ A w A v ρ l + ρ v ) - - - ( 9 )
Be full of full the working medium filling weight only with the structural parameters of heat pipe
Figure BDA0000055392580000052
And the working medium rerum natura is relevant.
The present invention has following technique effect and advantage:
1, be used for efficiently radiates heat to microelectronic components such as IC, LED, the porous alloy in its inner porous alloy evaporating area, adiabatic region and the condensing zone has different apertures and porosity, can effectively improve radiating effect.
2, utilize the notion of gradient composite construction porous alloy critical surface, and introduce analytic solutions fractal and numerical computations acquisition aperture, critical surface both sides and porosity.
3, distinguish clear and definite radiator overall height H and each region height H according to the phase difference and the physical parameter of working medium in the zones of different 1, H 2, H 3Between logical relation, calculated hole diameters and porosity size, and can application directs the type Design of for heat sinks.

Claims (3)

1. porous alloy heat-pipe radiator with gradient composite construction, comprise housing, it is characterized in that: housing is provided with working medium filling mouth and exhaust outlet, the bottom of housing is provided with working medium filling mouth, the upper surface is provided with exhaust outlet, be divided into evaporating area in the housing from bottom to top, three zones of adiabatic region and condensing zone, all fill full porous alloy in three zones, the average pore size minimum of porous alloy in the evaporating area, the average pore size maximum of porous alloy in the condensing zone, the average pore size of porous alloy is in evaporating area in porous alloy average pore size and the condensing zone between the porous alloy average pore size in the adiabatic region.
2. the porous alloy heat-pipe radiator with gradient composite construction according to claim 1 is characterized in that: described evaporating area height H 1, the condensing zone height H 3With the adiabatic region height H 2Distribution be:
Figure FDA0000055392570000011
Figure FDA0000055392570000012
With
Figure FDA0000055392570000013
H wherein 1Be the height of evaporating area 7, H 2Be the height of adiabatic region 5, H 3Be the height of condensing zone, H is three region height sums; V lBe liquid phase topping up volume, φ 1Be the porosity of evaporating area porous alloy, V gBe gaseous phase volume, φ 3Be the porosity of condensing zone porous alloy, L is the length in arbitrary zone, and W is the width in arbitrary zone.
3. the porous alloy heat-pipe radiator with gradient composite construction according to claim 1 is characterized in that: the mean pore size of porous alloy obtains by following formula in described evaporating area, adiabatic region and the condensing zone: ln (p/p 0(the 2 γ V of)=- m/ rRT) cos θ, in the formula, p 0Saturated vapour pressure when being the plane for the working media liquid level, p are the saturated vapour pressure of liquid-working-medium in the porous alloy, V mBe the molal volume of corresponding phase, γ is the surface tension of corresponding phase in each district, and R is a constant, and T is an absolute temperature, and θ is the contact angle of liquid-working-medium and porous alloy metal level wall; When correspondence is meant real work mutually, the situation of working media in radiator evaporating area, adiabatic region and the condensing zone, the evaporating area working media is a liquid phase, and the adiabatic region working media is the vapour-liquid two-phase, and the condensing zone working media is a vapour phase.
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109287104A (en) * 2018-11-21 2019-01-29 山东大学 A kind of bionical rising cooling adaptive radiator
CN113285138A (en) * 2021-04-16 2021-08-20 武汉理工大学 Automobile battery liquid cooling heat dissipation device based on steam cavity heat dissipation technology

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109287104A (en) * 2018-11-21 2019-01-29 山东大学 A kind of bionical rising cooling adaptive radiator
CN109287104B (en) * 2018-11-21 2019-09-17 山东大学 A kind of bionical rising cooling adaptive radiator
CN113285138A (en) * 2021-04-16 2021-08-20 武汉理工大学 Automobile battery liquid cooling heat dissipation device based on steam cavity heat dissipation technology

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