TWI760248B - Transient thermal diffusivity measurement method of heat dissipation module - Google Patents

Transient thermal diffusivity measurement method of heat dissipation module Download PDF

Info

Publication number
TWI760248B
TWI760248B TW110121510A TW110121510A TWI760248B TW I760248 B TWI760248 B TW I760248B TW 110121510 A TW110121510 A TW 110121510A TW 110121510 A TW110121510 A TW 110121510A TW I760248 B TWI760248 B TW I760248B
Authority
TW
Taiwan
Prior art keywords
heat
measurement point
heat dissipation
dissipation module
thermal diffusivity
Prior art date
Application number
TW110121510A
Other languages
Chinese (zh)
Other versions
TW202248876A (en
Inventor
馮建忠
Original Assignee
長聖儀器股份有限公司
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 長聖儀器股份有限公司 filed Critical 長聖儀器股份有限公司
Priority to TW110121510A priority Critical patent/TWI760248B/en
Application granted granted Critical
Publication of TWI760248B publication Critical patent/TWI760248B/en
Publication of TW202248876A publication Critical patent/TW202248876A/en

Links

Images

Landscapes

  • Investigating Or Analyzing Materials Using Thermal Means (AREA)

Abstract

一種散熱模組之暫態熱擴散性能量測方法,主要是於一散熱模組的表面選擇二量測點,並且使該二量測點位於熱中心點的同一側但不同距離,之後再分別量測該二量測點的溫度,並代入下列式(1),其中該式(1)係為對能量方程式求解析解; A method for measuring the transient thermal diffusivity of a heat dissipation module is mainly to select two measurement points on the surface of a heat dissipation module, and make the two measurement points located on the same side of a thermal center point but at different distances, and then separately Measure the temperature of the two measuring points, and substitute the following formula (1), wherein the formula (1) is an analytical solution to the energy equation;

Figure 110121510-A0101-11-0001-1
Figure 110121510-A0101-11-0001-1

在上述之代入式(1)運算之後,可得下列式(2)及式(3)來求得M; After substituting the above equation (1), the following equations (2) and (3) can be obtained to obtain M;

Figure 110121510-A0101-11-0001-2
Figure 110121510-A0101-11-0001-2

Figure 110121510-A0101-11-0001-3
Figure 110121510-A0101-11-0001-3

最後,將M與第一量測點的距離X1以及在暫態之某一時刻之溫度T1代入式(1),即可求得的熱擴散係數α的值,該熱擴散係數α的值即用來代表該散熱模組之暫態熱擴散性能。 Finally, the distance X1 between M and the first measurement point and the temperature T1 at a certain moment in the transient state are substituted into the formula (1), and the value of the thermal diffusivity α can be obtained. The value of the thermal diffusivity α is Used to represent the transient thermal diffusion performance of the cooling module.

Description

散熱模組之暫態熱擴散性能量測方法 Transient thermal diffusivity measurement method of heat dissipation module

本發明係與熱擴散性能的量測技術有關,特別是指一種散熱模組之暫態熱擴散性能量測方法。 The present invention is related to the measurement technology of thermal diffusivity, in particular to a method for measuring the transient thermal diffusivity of a heat dissipation module.

散熱模組是目前廣泛使用於電腦或發熱晶片模組(例如LED燈板)的裝置。目前已知的散熱模組,大多是以一金屬底板(鋁或銅)上方設置或一體成形複數散熱鰭片,並以該金屬底板貼置於一熱源,藉此對該熱源提供將熱能向側方傳導並向上傳導藉由該複數散熱鰭片進行散熱的效果。 The heat dissipation module is a device widely used in computers or heat-generating chip modules (such as LED light panels). Most of the known heat dissipation modules currently have a plurality of heat dissipation fins disposed on or integrally formed on a metal base plate (aluminum or copper), and the metal base plate is attached to a heat source, thereby providing heat energy to the heat source to the side. Square conduction and upward conduction through the plurality of heat dissipation fins to dissipate heat.

前述以金屬底板做為散熱模組來與熱源貼接的技術,在熱源的熱能不高時其金屬熱傳導的效果還可算得上堪用,但在現在電腦CPU(中央處理單元)或LED燈板愈來愈進步,而單位時間內所產生的熱能也愈來愈高的情況下,前述以金屬底板做為散熱模組的技術其藉由金屬熱傳導的速度顯已不敷使用。因此,有人提出使用均溫導熱板(蒸汽腔室,Vapor Chamber)設置於該金屬底板下方而貼接於熱源,而成為一種含有均溫導熱板的散熱模組,藉由該均溫導熱板的快速均溫的特性,達到將熱能快速分散至該均溫導熱板各個位置的效果,因此獲得了更好的散熱效果。 The aforementioned technology of using the metal base plate as a heat dissipation module to attach to the heat source, the effect of metal heat conduction can be considered acceptable when the heat energy of the heat source is not high, but in the current computer CPU (Central Processing Unit) or LED light board Under the situation that the heat energy generated per unit time is getting higher and higher, the above-mentioned technology of using the metal base plate as the heat dissipation module is obviously not enough to use the speed of metal heat conduction. Therefore, some people propose to use a vapor chamber (vapor chamber) to be placed under the metal bottom plate and attached to the heat source, so as to become a heat dissipation module including a vapor chamber. The characteristic of rapid temperature uniformity achieves the effect of quickly dispersing heat energy to various positions of the uniform temperature and heat conduction plate, thus obtaining a better heat dissipation effect.

然而,目前的技術雖已發展至使用均溫導熱板與散熱模組組合來增強散熱效果,然而,對於散熱模組的熱擴散性能,僅有概念上的快與慢或 好與差的區別而已,並沒有一個具體且有數據根據的量測技術,僅能依靠儀器長時間的量測以獲得觀察到的結果。 However, although the current technology has been developed to use a combination of a thermally conductive plate and a heat dissipation module to enhance the heat dissipation effect, however, for the heat dissipation performance of the heat dissipation module, there are only conceptual fast and slow or The difference between good and bad is just that, there is no specific and data-based measurement technology, and the observed results can only be obtained by measuring instruments for a long time.

本發明之主要目的即在於提出一種散熱模組之暫態熱擴散性能量測方法,其係為一種具體且有數據根據的量測技術。 The main purpose of the present invention is to provide a transient thermal diffusivity energy measurement method of a heat dissipation module, which is a specific and data-based measurement technology.

本發明之再一目的即在於提出一種散熱模組之暫態熱擴散性能量測方法,其可提供使用者具體的量測結果,供使用者判斷被量測的散熱模組之散熱效果的好壞。 Another object of the present invention is to provide a method for measuring the transient thermal diffusivity of a heat dissipation module, which can provide a user with specific measurement results, so that the user can judge whether the heat dissipation effect of the measured heat dissipation module is good. Bad.

為了達成上述目的,本發明提出一種散熱模組之暫態熱擴散性能量測方法,包含有下列步驟A)至步驟D):A)決定一第一量測點及一第二量測點:將該散熱模組用來與一熱源貼接的表面定義為一導熱面,該導熱面貼接該熱源的區域的中心點定義為一熱中心點,並且於該導熱面上以該熱中心點為中心定義一矩形,該矩形之長寬均不超出該導熱面之邊緣;於該導熱面上的該矩形一邊的外側與該導熱面邊緣之間,任意選擇一第一量測點以及一第二量測點,該第一量測點與該矩形之該邊或該邊之虛擬延長線的直線距離係大於該第二量測點與該矩形之該邊或該邊之虛擬延長線的直線距離;B)量測溫度:將該散熱模組貼置於該熱源,並在該熱源穩定發熱的狀態下,分別量測該第一量測點以及該第二量測點的溫度隨時間的變化,且該散熱模組的散熱狀態不再有所改變即進入穩態;C)代入計算式:將該第一量測點與該第二量測點的溫度及距離代入下列式(1)及計算:以該第一量測點的距離X1之穩態溫度T1及第二量測 點的距離X2之穩態溫度T2而言,代入下列式(1),其中該式(1)係為對能量方程式求解析解; In order to achieve the above object, the present invention provides a method for measuring the transient thermal diffusivity of a heat dissipation module, comprising the following steps A) to D): A) determining a first measurement point and a second measurement point: The surface used for the heat dissipation module to be attached to a heat source is defined as a heat conduction surface, the center point of the area where the heat conduction surface is attached to the heat source is defined as a heat center point, and the heat center point is defined as the heat center point on the heat conduction surface. A rectangle is defined as the center, and the length and width of the rectangle do not exceed the edge of the heat-conducting surface; a first measurement point and a first measuring point are arbitrarily selected between the outer side of the rectangle on the heat-conducting surface and the edge of the heat-conducting surface. Two measurement points, the straight line distance between the first measurement point and the side of the rectangle or the virtual extension of the side is greater than the straight line between the second measurement point and the side of the rectangle or the virtual extension of the side distance; B) measuring temperature: the heat dissipation module is attached to the heat source, and when the heat source is stably generating heat, the temperature of the first measurement point and the temperature of the second measurement point are respectively measured over time. change, and the heat dissipation state of the heat dissipation module no longer changes, that is, it enters a steady state; C) Substitute into the calculation formula: Substitute the temperature and distance of the first measurement point and the second measurement point into the following formula (1) And calculation: using the steady-state temperature T1 of the distance X1 of the first measurement point and the second measurement For the steady-state temperature T2 of the distance X2 from the point, substitute the following formula (1), where the formula (1) is an analytical solution to the energy equation;

Figure 110121510-A0101-12-0003-6
Figure 110121510-A0101-12-0003-6

其中,

Figure 110121510-A0101-12-0003-5
Figure 110121510-A0101-12-0003-7
Figure 110121510-A0101-12-0003-8
dX=X1-X2,
Figure 110121510-A0101-12-0003-9
Figure 110121510-A0101-12-0003-10
;其中,M為熱傳導與熱對流強度比,h為對流熱傳係數,K為熱傳導係數,D為特徵直徑,T為溫度,t為時間,X為位置,L為特徵長度,λ為特徵值,dx為第一量測點與第二量測點之間的距離,X1為該第一量測點與該矩形之該邊或該邊之虛擬延長線的直線距離;在上述之代入式(1)運算之後,可得下列式(2)及式(3); in,
Figure 110121510-A0101-12-0003-5
,
Figure 110121510-A0101-12-0003-7
,
Figure 110121510-A0101-12-0003-8
, dX = X 1 - X 2,
Figure 110121510-A0101-12-0003-9
,
Figure 110121510-A0101-12-0003-10
; where M is the ratio of heat conduction to heat convection intensity, h is the convective heat transfer coefficient, K is the heat transfer coefficient, D is the characteristic diameter, T is the temperature, t is the time, X is the position, L is the characteristic length, and λ is the characteristic value , dx is the distance between the first measurement point and the second measurement point, X1 is the straight-line distance between the first measurement point and the side of the rectangle or the virtual extension line of the side; in the above substitution formula ( 1) After the operation, the following formulas (2) and (3) can be obtained;

Figure 110121510-A0101-12-0003-11
Figure 110121510-A0101-12-0003-11

Figure 110121510-A0101-12-0003-12
Figure 110121510-A0101-12-0003-12

由上述之式(2)及式(3)可求得M;D)結果:將步驟C)中求得之M與該第一量測點的距離X1於暫態之某一時刻t1之溫度T1代入式(1),即可求得的熱擴散係數α的值,該熱擴散係數α的值即用來代表該散熱模組之暫態熱擴散性能。 M can be obtained from the above formulas (2) and (3); D) Result: the temperature of the distance X1 between the M obtained in step C) and the first measurement point at a certain moment t1 in the transient state Substitute T1 into Equation (1) to obtain the value of the thermal diffusivity α, which is used to represent the transient thermal diffusivity of the heat dissipation module.

藉此,本發明為一個具體且有數據根據的量測技術而可供業界使用,進而,本發明可提供使用者具體的量測結果,供使用者判斷被量測的散熱模組之散熱效果的好壞。 Therefore, the present invention is a specific and data-based measurement technology that can be used by the industry, and further, the present invention can provide the user with specific measurement results for the user to judge the heat dissipation effect of the measured heat dissipation module good or bad.

11:散熱模組 11: Cooling module

12:金屬底板 12: Metal bottom plate

14:散熱鰭片 14: cooling fins

15:均溫導熱板 15: Temperature and heat conduction plate

151:導熱面 151: Thermal surface

152:矩形 152: Rectangle

16:風扇 16: Fan

O:熱中心點 O: hot center point

O1:第一量測點 O1: The first measurement point

O2:第二量測點 O2: The second measuring point

X1:直線距離 X1: straight line distance

X2:直線距離 X2: Straight line distance

圖1係本發明一較佳實施例之流程圖。 FIG. 1 is a flow chart of a preferred embodiment of the present invention.

圖2係本發明一較佳實施例之散熱模組之組合示意圖。 FIG. 2 is a schematic diagram of a combination of a heat dissipation module according to a preferred embodiment of the present invention.

圖3係本發明一較佳實施例之散熱模組底面示意圖。 3 is a schematic diagram of the bottom surface of a heat dissipation module according to a preferred embodiment of the present invention.

圖4係本發明一較佳實施例之另一散熱模組之組合示意圖。 FIG. 4 is a schematic diagram of the assembly of another heat dissipation module according to a preferred embodiment of the present invention.

圖5係本發明一較佳實施例之另一散熱模組底面示意圖。 FIG. 5 is a schematic bottom view of another heat dissipation module according to a preferred embodiment of the present invention.

為了詳細說明本發明之技術特點所在,茲舉以下之較佳實施例並配合圖式說明如後,其中: In order to illustrate the technical features of the present invention in detail, the following preferred embodiments are given and described in conjunction with the drawings as follows, wherein:

如圖1至圖3所示,本發明一較佳實施例所提出之一種散熱模組之暫態熱擴散性能量測方法,主要是以下列步驟來進行量測: As shown in FIG. 1 to FIG. 3 , a method for measuring the transient thermal diffusivity of a heat dissipation module according to a preferred embodiment of the present invention is mainly performed by the following steps:

A)決定一第一量測點及一第二量測點:將一散熱模組11用來與一熱源(圖中未示)(例如電腦的中央處理單元CPU或LED晶片電路板)貼接的表面定義為一導熱面151,於本實施例中,該散熱模組11係具有一金屬底板12以及由該金屬底板12向上延伸的複數散熱鰭片14,以及具有一均溫導熱板15以其頂面貼設於該金屬底板12之底面,該均溫導熱板15之底面即做為該導熱面151,該散熱模組11還具有一風扇16設於該複數散熱鰭片14上;該導熱面151貼接該熱源的區域的中心點定義為一熱中心點O,並且於該導熱面151上以該熱中心點O為中心定義一矩形152,該矩形152之長寬均不超出該導熱面151之邊緣;於該導熱面151上的該矩形152一邊的外側與該導熱面151邊緣之間,選擇一第一量測點O1以及一第二量測點O2,該第一量測點O1與該矩形152之該邊的直線距離X1係大於該 第二量測點O2與該矩形152之該邊的直線距離X2。此外,於本實施例中,該第二量測點O2係位於該第一量測點O1與該矩形152之該邊的垂直連線上,亦即,該第二量測點O2與該第一量測點O1是沿著其與該矩形152之該邊的垂直線而呈現線性關係。另外,於本實施例中,是以該矩形152的大小與該熱源的大小一致為例說明,不過,該矩形152的大小也可以在長度及寬度上小於該熱源的長度及寬度,或大於該熱源的長度及寬度,在該矩形152極小的狀況下,其各邊即視為與該熱中心點O重疊。 A) Determine a first measurement point and a second measurement point: use a heat dissipation module 11 to attach to a heat source (not shown in the figure) (such as a computer's central processing unit CPU or an LED chip circuit board) The surface of the heat sink is defined as a heat conduction surface 151. In this embodiment, the heat dissipation module 11 has a metal base plate 12 and a plurality of heat dissipation fins 14 extending upward from the metal base plate 12. Its top surface is attached to the bottom surface of the metal base plate 12, and the bottom surface of the temperature-equalizing heat-conducting plate 15 is used as the heat-conducting surface 151. The heat dissipation module 11 also has a fan 16 disposed on the plurality of heat-dissipating fins 14; the The center point of the area where the thermally conductive surface 151 is attached to the heat source is defined as a thermal center point O, and a rectangle 152 is defined on the thermally conductive surface 151 with the thermal center point O as the center, and the length and width of the rectangle 152 do not exceed the thermal center point O. The edge of the heat-conducting surface 151; between the outer side of the rectangle 152 on the heat-conducting surface 151 and the edge of the heat-conducting surface 151, select a first measurement point O1 and a second measurement point O2, the first measurement The straight-line distance X1 between the point O1 and the side of the rectangle 152 is greater than the The linear distance X2 between the second measurement point O2 and the side of the rectangle 152 . In addition, in this embodiment, the second measurement point O2 is located on the vertical connection line between the first measurement point O1 and the side of the rectangle 152 , that is, the second measurement point O2 and the first measurement point O2 A measurement point O1 exhibits a linear relationship along its vertical line with the side of the rectangle 152 . In addition, in this embodiment, the size of the rectangle 152 and the size of the heat source are taken as an example for illustration. However, the size of the rectangle 152 may be smaller than the length and width of the heat source, or larger than the size of the heat source. The length and width of the heat source are considered to overlap with the heat center point O when the rectangle 152 is extremely small.

B)量測溫度:將該散熱模組11貼置於該熱源,並在該熱源穩定發熱的狀態下,分別量測該第一量測點O1以及該第二量測點O2的溫度隨時間的變化,且該散熱模組11的散熱狀態不再有所改變即進入穩態。 B) Measure temperature: place the heat dissipation module 11 on the heat source, and measure the temperature of the first measurement point O1 and the second measurement point O2 over time when the heat source is stably generating heat changes, and the heat dissipation state of the heat dissipation module 11 no longer changes, that is, it enters a steady state.

C)代入計算式:將該第一量測點O1與該第二量測點O2的溫度及距離代入下列式(1)計算: C) Substitute into calculation formula: Substitute the temperature and distance of the first measurement point O1 and the second measurement point O2 into the following formula (1) to calculate:

以該第一量測點O1的距離X1之穩態溫度T1及第二量測點O2的距離X2之穩態溫度T2而言,代入下列式(1),其中該式(1)係為對能量方程式求解析解; Taking the steady-state temperature T1 of the distance X1 of the first measurement point O1 and the steady-state temperature T2 of the distance X2 of the second measurement point O2, substitute the following formula (1), wherein the formula (1) is for Analytical solution of the energy equation;

Figure 110121510-A0101-12-0005-13
Figure 110121510-A0101-12-0005-13

其中,

Figure 110121510-A0101-12-0005-14
Figure 110121510-A0101-12-0005-15
Figure 110121510-A0101-12-0005-16
dX=X1-X2,
Figure 110121510-A0101-12-0005-17
Figure 110121510-A0101-12-0005-18
。 in,
Figure 110121510-A0101-12-0005-14
,
Figure 110121510-A0101-12-0005-15
,
Figure 110121510-A0101-12-0005-16
, dX = X 1 - X 2,
Figure 110121510-A0101-12-0005-17
,
Figure 110121510-A0101-12-0005-18
.

其中,M為熱傳導與熱對流強度比,h為對流熱傳係數,K為熱傳導係數,D為特徵直徑,T為溫度,t為時間,X為位置,L為特徵長度,λ為特徵 值,dx為第一量測點O1與第二量測點O2之間的距離,X1為該第一量測點O1與該矩形152之該邊的直線距離,X2為該第一量測點O2與該矩形152之該邊的直線距離。 Among them, M is the ratio of heat conduction to heat convection intensity, h is the convective heat transfer coefficient, K is the heat conduction coefficient, D is the characteristic diameter, T is the temperature, t is the time, X is the position, L is the characteristic length, and λ is the characteristic value, dx is the distance between the first measurement point O1 and the second measurement point O2, X1 is the straight-line distance between the first measurement point O1 and the side of the rectangle 152, and X2 is the first measurement point The linear distance between O2 and the side of the rectangle 152 .

在上述之代入式(1)運算之後,可得下列式(2)及式(3): After the above-mentioned substitution equation (1) operation, the following equations (2) and (3) can be obtained:

Figure 110121510-A0101-12-0006-19
Figure 110121510-A0101-12-0006-19

Figure 110121510-A0101-12-0006-20
Figure 110121510-A0101-12-0006-20

由上述之式(2)及式(3)可求得M。 M can be obtained from the above equations (2) and (3).

D)結果:將步驟C)中求得之M與該第一量測點O1的距離X1於暫態之某一時刻t1之溫度T1代入式(1),即可求得的熱擴散係數α的值,該熱擴散係數α的值即用來代表該散熱模組11之暫態熱擴散性能。 D) Result: Substitute the temperature T1 of the distance X1 between the M obtained in step C) and the first measurement point O1 at a certain moment t1 of the transient state into the formula (1), and the thermal diffusivity α can be obtained. The value of the thermal diffusivity α is used to represent the transient thermal diffusivity of the heat dissipation module 11 .

以上說明了本發明的量測方法的各個步驟,接下來以實際數據進行說明。 The steps of the measurement method of the present invention have been described above, and the actual data will be used to describe the following.

在該第一量測點O1與該矩形152之該邊的直線距離X1=0.16m(公尺)以及該第二量測點O2與該矩形152之該邊的直線距離X2=0.07m的條件下,在某一時刻(即穩態)時,該第一量測點O1的溫度t1=攝氏67.5℃,該第二量測點O2的溫度t2=攝氏71.5℃。依上述之公式代入後,即求得熱擴散係數α=1.187cm2/s。藉此,即可藉由該熱擴散係數α的數值大小來判斷該散熱模組11的散熱效果。 Under the condition that the linear distance between the first measurement point O1 and the side of the rectangle 152 is X1=0.16m (meters) and the linear distance between the second measurement point O2 and the side of the rectangle 152 is X2=0.07m At a certain moment (ie, steady state), the temperature t1 of the first measurement point O1 = 67.5°C, and the temperature t2 of the second measurement point O2 = 71.5°C. After substituting in the above formula, the thermal diffusivity α=1.187cm 2 /s can be obtained. In this way, the heat dissipation effect of the heat dissipation module 11 can be judged by the value of the thermal diffusivity α.

前述的散熱模組11,是以具有均溫導熱板15的散熱模組為例說明,然而,若是不含均溫導熱板15的散熱模組,亦即單純為具有一金屬底板12以及複數散熱鰭片14者,如圖4所示,亦可以對其底面使用本發明之方法來量測出該散熱模組11的熱擴散係數α之數值。 The above-mentioned heat dissipation module 11 is described by taking the heat dissipation module having the temperature uniformity and heat conduction plate 15 as an example. However, if the heat dissipation module does not include the temperature uniformity heat conduction plate 15, it simply has a metal base plate 12 and a plurality of heat dissipation modules. For the fins 14, as shown in FIG. 4, the method of the present invention can also be used on the bottom surface of the fins 14 to measure the value of the thermal diffusivity α of the heat dissipation module 11.

上述的說明中,是以該第二量測點O2係位於該第一量測點O1與該矩形152之該邊的垂直連線上的關係來說明的,然而,如圖5所示,事實上該第二量測點O2也可以不位於該第一量測點O1與該矩形152之該邊的垂直連線上,而呈現非線性關係。這是由於本案的技術主要是以該第一量測點O1及該第二量測點O2各自與該矩形152之該邊的直線距離來進行計算,因此即使是非線性關係,也可以進行運算。例如,如圖5所示,該第一量測點O1所處的位置超出該矩形152的該邊的範圍,則垂直連線即無法交接於該邊,此時則可以將該邊延長而得到一虛擬延伸線,供該第一量測點O1及該第二量測點O2與該虛擬延伸線之間得以構成垂直連線。 In the above description, the relationship between the second measurement point O2 and the vertical connection line between the first measurement point O1 and the side of the rectangle 152 is described. However, as shown in FIG. 5 , the fact is The second measurement point O2 may not be located on the vertical connection line between the first measurement point O1 and the side of the rectangle 152 , but presents a non-linear relationship. This is because the technique of the present application mainly calculates the straight-line distance between the first measurement point O1 and the second measurement point O2 and the side of the rectangle 152 , so even if the relationship is non-linear, the calculation can be performed. For example, as shown in FIG. 5 , if the position of the first measurement point O1 is beyond the range of the side of the rectangle 152 , the vertical connection line cannot be connected to the side. In this case, the side can be extended to obtain A virtual extension line for forming a vertical connection between the first measurement point O1 and the second measurement point O2 and the virtual extension line.

本案的技術重點在於該第一量測點O1及該第二量測點O2都位於該矩形152一邊的外側,也就是同一邊的外側,因此是屬於一維的熱擴散量測技術。本發明之技術並不包含該第一量測點O1位於該矩形152一邊的外側,而該第二量測點O2位於另一個邊的外側這樣的狀況。 The technical focus of this case is that the first measurement point O1 and the second measurement point O2 are both located outside of one side of the rectangle 152 , that is, outside of the same side, so they belong to one-dimensional thermal diffusion measurement technology. The technology of the present invention does not include the situation that the first measuring point O1 is located outside one side of the rectangle 152 and the second measuring point O2 is located outside the other side.

綜上可知,本發明乃是一種具體且有數據根據的量測技術,其可以提供使用者具體的量測結果,即熱擴散係數α,供使用者判斷被量測的散熱模組11之散熱效果的好壞。 To sum up, the present invention is a specific and data-based measurement technology, which can provide the user with a specific measurement result, that is, the thermal diffusivity α, for the user to judge the heat dissipation of the heat dissipation module 11 to be measured. The effect is good or bad.

11:散熱模組 11: Cooling module

15:均溫導熱板 15: Temperature and heat conduction plate

151:導熱面 151: Thermal surface

152:矩形 152: Rectangle

O:熱中心點 O: hot center point

O1:第一量測點 O1: The first measurement point

O2:第二量測點 O2: The second measuring point

X1:直線距離 X1: straight line distance

X2:直線距離 X2: Straight line distance

Claims (5)

一種散熱模組之暫態熱擴散性能量測方法,包含有下列步驟: A method for measuring transient thermal diffusivity of a heat dissipation module, comprising the following steps: A)決定一第一量測點及一第二量測點:將該散熱模組用來與一熱源貼接的表面定義為一導熱面,該導熱面貼接該熱源的區域的中心點定義為一熱中心點,並且於該導熱面上以該熱中心點為中心定義一矩形,該矩形之長寬均不超出該導熱面之邊緣;於該導熱面上的該矩形一邊的外側與該導熱面邊緣之間,任意選擇一第一量測點以及一第二量測點,該第一量測點與該矩形之該邊或該邊之虛擬延長線的直線距離係大於該第二量測點與該矩形之該邊或該邊之虛擬延長線的直線距離; A) Determining a first measurement point and a second measurement point: the surface of the heat dissipation module used to attach to a heat source is defined as a heat conduction surface, and the center point of the area where the heat conduction surface is attached to the heat source is defined is a thermal center point, and defines a rectangle with the thermal center point as the center on the heat-conducting surface, and the length and width of the rectangle do not exceed the edge of the heat-conducting surface; the outer side of the rectangle on the heat-conducting surface and the Between the edges of the heat-conducting surface, a first measurement point and a second measurement point are arbitrarily selected, and the linear distance between the first measurement point and the side of the rectangle or the virtual extension of the side is greater than the second measurement point The straight-line distance between the measuring point and the side of the rectangle or the virtual extension of the side; B)量測溫度:將該散熱模組貼置於該熱源,並在該熱源穩定發熱的狀態下,分別量測該第一量測點以及該第二量測點的溫度隨時間的變化,且該散熱模組的散熱狀態不再有所改變即進入穩態; B) Measurement of temperature: The heat dissipation module is attached to the heat source, and when the heat source is stably generating heat, the temperature of the first measurement point and the temperature of the second measurement point are respectively measured over time. And the heat dissipation state of the heat dissipation module no longer changes, that is, it enters a steady state; C)代入計算式:將該第一量測點與該第二量測點的溫度及距離代入下列式(1)及計算: C) Substitute into calculation formula: Substitute the temperature and distance of this first measurement point and this second measurement point into the following formula (1) and calculation: 以該第一量測點的距離X1之穩態溫度T1及第二量測點的距離X2之穩態溫度T2而言,代入下列式(1),其中該式(1)係為對能量方程式求解析解; Taking the steady-state temperature T1 of the distance X1 of the first measuring point and the steady-state temperature T2 of the distance X2 of the second measuring point, substitute the following equation (1), where the equation (1) is the equation for the energy seek analytical solution;
Figure 110121510-A0101-13-0001-21
Figure 110121510-A0101-13-0001-21
其中,
Figure 110121510-A0101-13-0001-22
Figure 110121510-A0101-13-0001-23
Figure 110121510-A0101-13-0001-24
dX=X1-X2,
Figure 110121510-A0101-13-0001-25
Figure 110121510-A0101-13-0001-26
in,
Figure 110121510-A0101-13-0001-22
,
Figure 110121510-A0101-13-0001-23
,
Figure 110121510-A0101-13-0001-24
, dX = X 1 - X 2,
Figure 110121510-A0101-13-0001-25
,
Figure 110121510-A0101-13-0001-26
;
其中,M為熱傳導與熱對流強度比,h為對流熱傳係數,K為熱傳導係數,D為特徵直徑,T為溫度,t為時間,X為位置,L為特徵長度,λ為特徵值,dx為第 一量測點與第二量測點之間的距離,X1為該第一量測點與該矩形之該邊或該邊之虛擬延長線的直線距離; Among them, M is the ratio of heat conduction to heat convection intensity, h is the convective heat transfer coefficient, K is the heat conduction coefficient, D is the characteristic diameter, T is the temperature, t is the time, X is the position, L is the characteristic length, and λ is the characteristic value, dx is the first The distance between a measurement point and the second measurement point, X1 is the straight-line distance between the first measurement point and the side of the rectangle or the virtual extension of the side; 在上述之代入式(1)運算之後,可得下列式(2)及式(3); After substituting the above-mentioned equation (1), the following equations (2) and (3) can be obtained;
Figure 110121510-A0101-13-0002-28
Figure 110121510-A0101-13-0002-28
Figure 110121510-A0101-13-0002-29
Figure 110121510-A0101-13-0002-29
由上述之式(2)及式(3)可求得M; M can be obtained from the above formulas (2) and (3); D)結果:將步驟C)中求得之M與該第一量測點的距離X1於暫態之某一時刻t1之溫度T1代入式(1),即可求得的熱擴散係數α的值,該熱擴散係數α的值即用來代表該散熱模組之暫態熱擴散性能。 D) Result: Substitute the temperature T1 of the distance X1 between the M obtained in step C) and the first measurement point at a certain moment t1 of the transient state into the formula (1), and the thermal diffusivity α can be obtained. The value of the thermal diffusivity α is used to represent the transient thermal diffusivity of the heat dissipation module.
依據請求項1所述之散熱模組之暫態熱擴散性能量測方法,其中:該第二量測點係位於該第一量測點與該矩形之該邊或該邊之虛擬延長線的垂直連線上。 The method for measuring transient thermal diffusivity of a heat dissipation module according to claim 1, wherein: the second measurement point is located between the first measurement point and the side of the rectangle or a virtual extension of the side connected vertically. 依據請求項1所述之散熱模組之暫態熱擴散性能量測方法,其中:該第二量測點係不位於該第一量測點與該矩形之該邊或該邊之虛擬延長線的垂直連線上。 The method for measuring transient thermal diffusivity of a heat dissipation module according to claim 1, wherein: the second measurement point is not located on the virtual extension line between the first measurement point and the side or the side of the rectangle on the vertical connection. 依據請求項1所述之散熱模組之暫態熱擴散性能量測方法,其中:該散熱模組係具有一金屬底板以及複數散熱鰭片,而以該金屬底板之底面做為該導熱面。 The method for measuring transient thermal diffusivity of a heat dissipation module according to claim 1, wherein: the heat dissipation module has a metal base plate and a plurality of heat dissipation fins, and the bottom surface of the metal base plate is used as the heat conduction surface. 依據請求項1所述之散熱模組之暫態熱擴散性能量測方法,其中:該散熱模組係具有一金屬底板以及複數散熱鰭片,以及具有一均溫導熱板以其頂面貼設於該金屬底板之底面,該均溫導熱板之底面係做為該導熱面。 The method for measuring the transient thermal diffusivity of a heat dissipation module according to claim 1, wherein: the heat dissipation module has a metal base plate and a plurality of heat dissipation fins, and has a heat-dissipating heat-dissipating plate on its top surface. On the bottom surface of the metal base plate, the bottom surface of the temperature uniform heat conduction plate is used as the heat conduction surface.
TW110121510A 2021-06-11 2021-06-11 Transient thermal diffusivity measurement method of heat dissipation module TWI760248B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
TW110121510A TWI760248B (en) 2021-06-11 2021-06-11 Transient thermal diffusivity measurement method of heat dissipation module

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
TW110121510A TWI760248B (en) 2021-06-11 2021-06-11 Transient thermal diffusivity measurement method of heat dissipation module

Publications (2)

Publication Number Publication Date
TWI760248B true TWI760248B (en) 2022-04-01
TW202248876A TW202248876A (en) 2022-12-16

Family

ID=82198743

Family Applications (1)

Application Number Title Priority Date Filing Date
TW110121510A TWI760248B (en) 2021-06-11 2021-06-11 Transient thermal diffusivity measurement method of heat dissipation module

Country Status (1)

Country Link
TW (1) TWI760248B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI833464B (en) * 2022-11-24 2024-02-21 長聖儀器股份有限公司 Thermal resistance measurement results consistency device for cooling modules

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TW201638706A (en) * 2015-04-24 2016-11-01 長聖儀器股份有限公司 Cooling device
TWI716240B (en) * 2019-12-27 2021-01-11 長聖儀器股份有限公司 Thermal diffusivity performance measuring system and method

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TW201638706A (en) * 2015-04-24 2016-11-01 長聖儀器股份有限公司 Cooling device
TWI716240B (en) * 2019-12-27 2021-01-11 長聖儀器股份有限公司 Thermal diffusivity performance measuring system and method

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI833464B (en) * 2022-11-24 2024-02-21 長聖儀器股份有限公司 Thermal resistance measurement results consistency device for cooling modules

Also Published As

Publication number Publication date
TW202248876A (en) 2022-12-16

Similar Documents

Publication Publication Date Title
Wang et al. Energy saving potential of using heat pipes for CPU cooling
Wang et al. Development of 30 Watt high-power LEDs vapor chamber-based plate
Xiang et al. Heat transfer performance and structural optimization of a novel micro-channel heat sink
US8029186B2 (en) Method for thermal characterization under non-uniform heat load
Kim et al. Heat pipe cooling technology for desktop PC CPU
Jang et al. Innovative analytic and experimental methods for thermal management of SMD-type LED chips
TWI760248B (en) Transient thermal diffusivity measurement method of heat dissipation module
US8315055B2 (en) Systems and methods for providing heat transfer
Habib et al. Characteristics of natural convection heat transfer in an array of discrete heat sources
Harahap et al. Measurements of heat dissipation from miniaturized vertical rectangular fin arrays under dominant natural convection conditions
Hashim Hussein et al. Investigation of free convection heat transfer from vertical cylinders with semicircular fins
Deshmukh et al. Experimental and numerical analysis of effect of combined drop-shape pin fins and plate fins type heat sink under natural convection
Wang L-and U-shaped heat pipes thermal modules with twin fans for cooling of electronic system under variable heat source areas
Huang et al. Experimental investigation of vapor chamber module applied to high-power light-emitting diodes
Wen et al. Natural convective performance of perforated heat sinks with circular pin fins
Zhang et al. An experimental investigation of a 100-W high-power light-emitting diode array using vapor chamber–based plate
Wang et al. Performance effects of heat transfer and geometry on heat pipe thermal modules under forced convection
TW201306726A (en) Heat sink assembly
Wang et al. Optimization of heat flow analysis for exceeding hundred watts in HI-LEDs projectors
US11835478B2 (en) Method for measuring the transient thermal diffusion performance of a heat dissipation module
Wang Novel thermal resistance network analysis of heat sink with embedded heat pipes
Lohan et al. Validation and application of different experimental techniques to measure electronic component operating junction temperature
Lin et al. Measurement of Performance Characterization of Ultra-Thin Vapor Chamber
Murthy et al. Orientation independent two-phase heat spreaders for space constrained applications
Wang A fitting, simple and versatile window program (HSHPTM) design using lumped parameters and one-dimensional thermal resistance models