CN110752130B - A composite heat dissipation method for instantaneous pulse ultra-high power electron collection stage - Google Patents

A composite heat dissipation method for instantaneous pulse ultra-high power electron collection stage Download PDF

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CN110752130B
CN110752130B CN201910985268.8A CN201910985268A CN110752130B CN 110752130 B CN110752130 B CN 110752130B CN 201910985268 A CN201910985268 A CN 201910985268A CN 110752130 B CN110752130 B CN 110752130B
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graphite layer
microchannel
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潘瑶
刘欣
巩萌萌
王思峰
张少华
周振君
王海英
王领华
余群
吕建伟
韩旭
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China Academy of Launch Vehicle Technology CALT
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/02Electrodes; Magnetic control means; Screens
    • H01J23/027Collectors
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/02Electrodes; Magnetic control means; Screens
    • H01J23/027Collectors
    • H01J23/033Collector cooling devices
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
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Abstract

本发明涉及一种瞬时脉冲超大功率电子收集级复合散热方法,属于瞬时脉冲超大功率散热领域;步骤一、将金属主体轴向竖直放置;步骤二、在金属主体的侧壁内加工双螺旋微通道;步骤三、在金属主体的内壁贴附石墨层;步骤四、调整金属主体位置,实现外部电子束射在石墨层内壁的电子束沉积加热区域;步骤五、双螺旋微通道中流动散热工质;步骤六、外部电子束沿金属主体轴向方向射向石墨层;热量通过石墨层的吸收以及通过石墨层向金属主体传递,最终通过双螺旋微通道流动的散热工质将热量带走,实现散热;本发明通过利用不同材料的特性,使收集极始终工作在正常的温度范围内,保证大功率调速管的可靠性和稳定性。

Figure 201910985268

The invention relates to a composite heat dissipation method of instantaneous pulse super-power electronic collection level, belonging to the field of instantaneous pulse super-power heat dissipation. channel; step 3, attaching a graphite layer to the inner wall of the metal body; step 4, adjusting the position of the metal body to realize the electron beam deposition heating area where the external electron beam is irradiated on the inner wall of the graphite layer; step 5, flow heat dissipation in the double-spiral microchannel Step 6: The external electron beam is directed to the graphite layer along the axial direction of the metal body; the heat is absorbed by the graphite layer and transferred to the metal body through the graphite layer, and finally the heat is taken away by the heat dissipation working medium flowing through the double helix microchannel, Realize heat dissipation; the present invention makes the collector always work within the normal temperature range by utilizing the characteristics of different materials, and ensures the reliability and stability of the high-power klystron.

Figure 201910985268

Description

一种瞬时脉冲超大功率电子收集级复合散热方法A composite heat dissipation method for instantaneous pulse ultra-high power electronic collection stage

技术领域technical field

本发明属于瞬时脉冲超大功率散热领域,涉及一种瞬时脉冲超大功率电子收集级复合散热方法。The invention belongs to the field of instantaneous pulse super-power heat dissipation, and relates to an instantaneous pulse super-power electronic collection-level composite heat dissipation method.

背景技术Background technique

大功率调速管是一种基于速度调制原理将电子束能量转换为微波能量的微波真空器件,它具有高功率、高增益等优点。但是调速管的转换效率较低,高能电子束在高频互作用段交出部分能量转换为微波后,仍具有较高的动能,收集极则用于收集这些高速电子束。收集极在调速管工作过程中用于收集瞬时脉冲轰击的电子束,瞬时脉冲高能电子束沉积在收集极上将能量转换为大量的热量,导致收集极上的温度升高,成为调速管中发热最严重的部分之一。如果其温度过高,将引起收集极材料表面的吸附气体解吸附甚至材料本身发生蒸发和汽化,不但会严重影响整个大功率调速管工作的可靠性和稳定性;更有甚者,若热量持续累积,收集极材料不断熔化将导致其熔穿,将破坏真空环境导致调速管失效。而且由于调速管的工作特性,收集极受到的电子束加热特性非常严酷,不仅平均加热功率高达几十kW,瞬时脉冲加热功率更是高达数GW,这对收集极的散热设计提出了非常严格的要求。目前并没有相关有效的解决方案。High-power klystron is a microwave vacuum device that converts electron beam energy into microwave energy based on the principle of velocity modulation. It has the advantages of high power and high gain. However, the conversion efficiency of the klystron is low. The high-energy electron beam still has high kinetic energy after the high-frequency interaction section surrenders part of the energy and converts it into microwave. The collector is used to collect these high-speed electron beams. The collector is used to collect the electron beam bombarded by the instantaneous pulse during the working process of the klystron. The high-energy electron beam of the instantaneous pulse is deposited on the collector to convert the energy into a large amount of heat, which causes the temperature on the collector to rise and becomes the klystron. One of the worst parts of the fever. If its temperature is too high, it will cause the desorption of the adsorbed gas on the surface of the collector material and even the evaporation and vaporization of the material itself, which will not only seriously affect the reliability and stability of the entire high-power klystron; Continued accumulation, the continuous melting of the collector material will cause it to melt through, which will destroy the vacuum environment and cause the failure of the klystron. Moreover, due to the working characteristics of the klystron, the electron beam heating characteristics of the collector are very harsh, not only the average heating power is as high as several tens of kW, but the instantaneous pulse heating power is as high as several GW, which puts forward very strict requirements for the heat dissipation design of the collector. requirements. There is currently no relevant effective solution.

发明内容SUMMARY OF THE INVENTION

本发明解决的技术问题是:克服现有技术的不足,提出一种瞬时脉冲超大功率电子收集级复合散热方法,通过利用不同材料的特性,使收集极始终工作在正常的温度范围内,保证大功率调速管的可靠性和稳定性。The technical problem solved by the present invention is: to overcome the deficiencies of the prior art, a composite heat dissipation method for instantaneous pulse ultra-high power electron collectors is proposed. Reliability and stability of power klystrons.

本发明解决技术的方案是:The technical solution of the present invention is:

一种瞬时脉冲超大功率电子收集级复合散热方法,包括如下步骤:A composite heat dissipation method for instantaneous pulse ultra-high power electron collection level, comprising the following steps:

步骤一、将金属主体轴向竖直放置;Step 1. Place the metal main body vertically in the axial direction;

步骤二、在金属主体的侧壁内加工双螺旋微通道;Step 2, processing double helix microchannels in the side wall of the metal body;

步骤三、在金属主体的内壁贴附石墨层;Step 3, attaching a graphite layer to the inner wall of the metal body;

步骤四、调整金属主体位置,实现外部电子束射在石墨层内壁的电子束沉积加热区域;Step 4: Adjust the position of the metal main body to realize the electron beam deposition heating area where the external electron beam is irradiated on the inner wall of the graphite layer;

步骤五、双螺旋微通道中流动散热工质;Step 5. Flow heat dissipation working medium in the double helix microchannel;

步骤六、外部电子束沿金属主体轴向方向射向石墨层;热量通过石墨层的吸收以及通过石墨层向金属主体传递,最终通过双螺旋微通道流动的散热工质将热量带走,实现散热。Step 6: The external electron beam is directed to the graphite layer along the axial direction of the metal body; the heat is absorbed by the graphite layer and transferred to the metal body through the graphite layer, and finally the heat is taken away by the heat dissipation working medium flowing through the double-spiral microchannel to realize heat dissipation. .

在上述的一种瞬时脉冲超大功率电子收集级复合散热方法,所述步骤一中,所述金属主体为圆环状结构;金属主体为不锈钢材料或钛材料;金属主体外壁直径为60~150mm,轴向长度为10-50mm;壁厚为3-5mm。In the above-mentioned composite heat dissipation method of instantaneous pulse ultra-high power electron collection level, in the first step, the metal main body is a circular structure; the metal main body is made of stainless steel or titanium material; the diameter of the outer wall of the metal main body is 60-150 mm, The axial length is 10-50mm; the wall thickness is 3-5mm.

在上述的一种瞬时脉冲超大功率电子收集级复合散热方法,所述步骤二中,所述双螺旋微通道包括第一螺旋微通道和第二螺旋微通道;第一螺旋微通道与第二螺旋微通道均为螺旋环状通道;且第一螺旋微通道与第二螺旋微通道交错设置;第一螺旋微通道的入口在金属主体轴向底端;出口在金属主体轴向顶端;第二螺旋微通道的入口在金属主体轴向顶端;出口在金属主体轴向底端;第一螺旋微通道与第二螺旋微通道的螺旋方向相反。In the above-mentioned composite heat dissipation method of instantaneous pulse super-power electron collection level, in the second step, the double-spiral microchannel includes a first spiral microchannel and a second spiral microchannel; the first spiral microchannel and the second spiral microchannel The microchannels are all spiral annular channels; and the first spiral microchannel and the second spiral microchannel are alternately arranged; the inlet of the first spiral microchannel is at the axial bottom end of the metal body; the outlet is at the axial top end of the metal body; the second spiral microchannel The inlet of the microchannel is at the axial top end of the metal body; the outlet is at the axial bottom end of the metal body; the helical directions of the first helical microchannel and the second helical microchannel are opposite.

在上述的一种瞬时脉冲超大功率电子收集级复合散热方法,所述第一螺旋微通道和第二螺旋微通道的管道截面为矩形结构;管道截面尺寸为3mm*1mm。In the above-mentioned composite heat dissipation method of instantaneous pulse ultra-high power electron collection stage, the pipe cross-sections of the first spiral microchannel and the second spiral microchannel are rectangular structures, and the pipe cross-section size is 3mm*1mm.

在上述的一种瞬时脉冲超大功率电子收集级复合散热方法,所述步骤三中,石墨层为环形层状结构;石墨层轴向长度为10-50mm;壁厚为1-2mm;熔点为3000℃。In the above-mentioned composite heat dissipation method of instantaneous pulse ultra-high power electron collection level, in the step 3, the graphite layer is an annular layered structure; the axial length of the graphite layer is 10-50mm; the wall thickness is 1-2mm; the melting point is 3000 °C.

在上述的一种瞬时脉冲超大功率电子收集级复合散热方法,所述步骤四中,所述电子束沉积加热区域设置在石墨层内壁的中部位置;电子束沉积加热区域为环形区域;轴向长度为5-25mm;电子束沉积加热区域的侧面积为石墨层内壁面积的一半。In the above-mentioned composite heat dissipation method of instantaneous pulse super-power electron collection level, in the step 4, the electron beam deposition heating area is arranged in the middle position of the inner wall of the graphite layer; the electron beam deposition heating area is an annular area; the axial length is It is 5-25mm; the side area of the electron beam deposition heating area is half of the inner wall area of the graphite layer.

在上述的一种瞬时脉冲超大功率电子收集级复合散热方法,所述金属主体与石墨层采用分子扩散焊焊接;实现金属主体与石墨层之间的接触热阻降低;接触传热系数为5000~10000W/(K·m2)。In the above-mentioned composite heat dissipation method of instantaneous pulse ultra-high power electron collection level, the metal body and the graphite layer are welded by molecular diffusion welding; the contact thermal resistance between the metal body and the graphite layer is reduced; the contact heat transfer coefficient is 5000~ 10000W/(K·m 2 ).

在上述的一种瞬时脉冲超大功率电子收集级复合散热方法,所述步骤五中,散热工质为离子水,导热系数为0.6W/(K·m),比热容为4183J/(kg·K)。In the above-mentioned composite heat dissipation method of instantaneous pulse super-power electron collection level, in the step 5, the heat dissipation working medium is ionized water, the thermal conductivity is 0.6W/(K·m), and the specific heat capacity is 4183J/(kg·K) .

在上述的一种瞬时脉冲超大功率电子收集级复合散热方法,所述步骤六中,外部电子束采用瞬时脉冲发射方式,单次脉冲发射功率为1~9GW;单次发射时间为100-500ns;发射频率为10~50Hz。In the above-mentioned composite heat dissipation method of instantaneous pulse super-power electron collection level, in the step 6, the external electron beam adopts the instantaneous pulse emission mode, the single pulse emission power is 1-9GW; the single emission time is 100-500ns; The emission frequency is 10 to 50 Hz.

在上述的一种瞬时脉冲超大功率电子收集级复合散热方法,整个散热机构实现了单次电子脉冲热流密度为1012-2×1012W/m2,平均热流密度为5×106-107W/m2的热量排散;石墨层最高温不超过2000℃;低于石墨层的熔点;金属主体的最高温由2600℃降低至650℃。In the above-mentioned composite heat dissipation method of instantaneous pulse ultra-high power electron collection stage, the whole heat dissipation mechanism achieves a single electron pulse heat flux density of 10 12 -2×10 12 W/m 2 , and an average heat flux density of 5×10 6 -10 The heat dissipation of 7 W/m 2 ; the maximum temperature of the graphite layer does not exceed 2000℃; lower than the melting point of the graphite layer; the maximum temperature of the metal body is reduced from 2600℃ to 650℃.

本发明与现有技术相比的有益效果是:The beneficial effects of the present invention compared with the prior art are:

(1)本发明将具有较大电子穿透深度和高熔点的石墨作为电子束的吸收材料,相比传统单一材料的收集极散热方法能够避免瞬时脉冲电子沉积过程中超大功率加载在有限区域使得收集极材料的熔化;(1) In the present invention, graphite with a large electron penetration depth and a high melting point is used as the absorbing material of the electron beam. Compared with the traditional single-material collector heat dissipation method, it can avoid the super power loading in the limited area during the instantaneous pulse electron deposition process. melting of collector material;

(2)本发明将具有高导热、易加工焊接的金属材料作为收集极主体,通过在金属主体中加工逆流螺旋冷却通道,通过工质不断流过两个螺旋冷却通道将电子束持续沉积带来的平均热量进行排散,保障收集极整体在长时间运行中温度一直处于许用范围;同时通过工质在两个螺旋通道中采用逆向流动的方式,控制通道出口附近电子沉积面温度升高,使得收集极温度分布更均匀。(2) In the present invention, a metal material with high thermal conductivity and easy processing and welding is used as the collector body, and the countercurrent spiral cooling channel is processed in the metal body, and the electron beam is continuously deposited by the continuous flow of the working medium through the two spiral cooling channels. The average heat is dissipated to ensure that the temperature of the collector as a whole is always within the allowable range during long-term operation; at the same time, the working fluid adopts the reverse flow method in the two spiral channels to control the temperature of the electron deposition surface near the outlet of the channel to increase, Make the collector temperature distribution more uniform.

附图说明Description of drawings

图1为本发明金属主体内双螺旋微通道示意图;Fig. 1 is the schematic diagram of the double helix microchannel in the metal main body of the present invention;

图2为本发明石墨层和电子束沉积加热区域示意图;Fig. 2 is the schematic diagram of graphite layer of the present invention and electron beam deposition heating area;

图3为本发明金属主体和石墨层截面示意图。3 is a schematic cross-sectional view of the metal body and the graphite layer of the present invention.

具体实施方式Detailed ways

下面结合实施例对本发明作进一步阐述。The present invention will be further elaborated below in conjunction with the examples.

本发明提供了一种瞬时脉冲超大功率电子收集级复合散热方法,提高了收集极吸收瞬时脉冲电子束的体积和热容,解决了电子收集极受瞬时脉冲超大功率加热后局部温度上升过高导致部分材料熔化;改进了收集极散热能力,解决了超高平均热流的排散难题;改善了收集极的温度均匀性,降低驱动工质流经散热器所需功耗。主要包括如下步骤:The invention provides a composite heat dissipation method of instantaneous pulse ultra-high power electron collection stage, which improves the volume and heat capacity of the collector to absorb the instantaneous pulse electron beam, and solves the problem that the local temperature rises too high after the electron collector is heated by the instantaneous pulse ultra-high power. Part of the material is melted; the heat dissipation capability of the collector is improved, and the problem of ultra-high average heat flow dissipation is solved; the temperature uniformity of the collector is improved, and the power consumption required to drive the working medium to flow through the radiator is reduced. It mainly includes the following steps:

步骤一、金属主体1为圆环状结构;金属主体1为不锈钢材料或钛材料;金属主体1外壁直径为60~150mm,轴向长度为10-50mm;壁厚为3-5mm。将金属主体1轴向竖直放置;如图1所示。Step 1: The metal main body 1 has a circular structure; the metal main body 1 is made of stainless steel or titanium; the outer wall diameter of the metal main body 1 is 60-150 mm, the axial length is 10-50 mm, and the wall thickness is 3-5 mm. Place the metal body 1 axially upright; as shown in Figure 1.

步骤二、在金属主体1的侧壁内加工双螺旋微通道;双螺旋微通道包括第一螺旋微通道2和第二螺旋微通道3;第一螺旋微通道2与第二螺旋微通道3均为螺旋环状通道;且第一螺旋微通道2与第二螺旋微通道3交错设置;第一螺旋微通道2的入口21在金属主体1轴向底端;出口22在金属主体1轴向顶端;第二螺旋微通道3的入口31在金属主体1轴向顶端;出口32在金属主体1轴向底端;第一螺旋微通道2与第二螺旋微通道3的螺旋方向相反。第一螺旋微通道2和第二螺旋微通道3的管道截面为矩形结构;管道截面尺寸为3mm*1mm。Step 2: Process a double helical microchannel in the side wall of the metal body 1; the double helical microchannel includes a first helical microchannel 2 and a second helical microchannel 3; It is a spiral annular channel; and the first spiral microchannel 2 and the second spiral microchannel 3 are alternately arranged; the inlet 21 of the first spiral microchannel 2 is at the axial bottom end of the metal body 1; the outlet 22 is at the axial top end of the metal body 1 The inlet 31 of the second spiral microchannel 3 is at the axial top end of the metal body 1; the outlet 32 is at the axial bottom end of the metal body 1; The pipe sections of the first helical microchannel 2 and the second helical microchannel 3 are rectangular structures; the size of the pipe section is 3mm*1mm.

步骤三、在金属主体1的内壁贴附石墨层4;石墨层4为环形层状结构;石墨层4轴向长度为10-50mm;壁厚为1-2mm;熔点为3000℃。如图2所示。在提高吸热体积热容方面,选用石墨作为收集极的电子束吸收层,电子束在石墨内的穿透深度是不锈钢的6倍,是钛的3倍,电子束进入石墨后动能转化为热能对穿透区域的石墨加热,由于石墨的电子穿透深度大,所以吸热体积大。而且石墨的熔点高达3000℃,远大于不锈钢的熔点1400℃和钛的熔点1660℃,所以受到电子束加热的石墨温度距离其熔点仍有较大空间。因此,利用石墨熔点高和电子穿透深度大的特点,可以解决瞬时超大功率电子沉积引发的局部温升所带来的收集极部分材料熔化的问题。金属主体1与石墨层4采用分子扩散焊焊接;实现金属主体1与石墨层4之间的接触热阻降低;接触传热系数为5000~10000W/(K·m2),如图3所示。Step 3, attaching a graphite layer 4 to the inner wall of the metal body 1; the graphite layer 4 is an annular layered structure; the axial length of the graphite layer 4 is 10-50 mm; the wall thickness is 1-2 mm; and the melting point is 3000°C. as shown in picture 2. In terms of improving the heat capacity of the endothermic volume, graphite is used as the electron beam absorption layer of the collector. The penetration depth of the electron beam in the graphite is 6 times that of stainless steel and 3 times that of titanium. The kinetic energy of the electron beam is converted into heat energy after entering the graphite. When the graphite in the penetration area is heated, the heat absorption volume is large due to the large electron penetration depth of the graphite. Moreover, the melting point of graphite is as high as 3000 ° C, which is much higher than the melting point of stainless steel of 1400 ° C and the melting point of titanium of 1660 ° C, so the temperature of graphite heated by the electron beam still has a large distance from its melting point. Therefore, by using the characteristics of graphite's high melting point and large electron penetration depth, the problem of melting of the collector part material caused by the local temperature rise caused by instantaneous ultra-high-power electron deposition can be solved. The metal body 1 and the graphite layer 4 are welded by molecular diffusion welding; the contact thermal resistance between the metal body 1 and the graphite layer 4 is reduced; the contact heat transfer coefficient is 5000-10000W/(K·m 2 ), as shown in Figure 3 .

步骤四、调整金属主体1位置,实现外部电子束射在石墨层4内壁的电子束沉积加热区域41;电子束沉积加热区域41设置在石墨层4内壁的中部位置;电子束沉积加热区域41为环形区域;轴向长度为5-25mm;电子束沉积加热区域41的侧面积为石墨层4内壁面积的一半。Step 4: Adjust the position of the metal body 1 to realize the electron beam deposition heating area 41 where the external electron beam is shot on the inner wall of the graphite layer 4; the electron beam deposition heating area 41 is arranged in the middle position of the inner wall of the graphite layer 4; the electron beam deposition heating area 41 is An annular area; the axial length is 5-25 mm; the side area of the electron beam deposition heating area 41 is half of the inner wall area of the graphite layer 4 .

步骤五、双螺旋微通道中流动散热工质;散热工质为离子水,导热系数为0.6W/(K·m),比热容为4183J/(kg·K)。Step 5: Flow a heat-dissipating working medium in the double-spiral microchannel; the heat-dissipating working medium is ionized water, the thermal conductivity is 0.6W/(K·m), and the specific heat capacity is 4183J/(kg·K).

步骤六、外部电子束沿金属主体1轴向方向射向石墨层4;外部电子束采用瞬时脉冲发射方式,单次脉冲发射功率为1~9GW;单次发射时间为100-500ns;发射频率为10~50Hz。热量通过石墨层(4)的吸收以及通过石墨层4向金属主体1传递,最终通过双螺旋微通道流动的散热工质将热量带走,实现散热。改进收集极散热能力和降低散热装置的流动阻力方面,主要是通过优化金属微通道结构的通道高度、通道宽度和肋片宽度等结构参数,平衡金属微通道内部换热过程中通过肋片导热和通过工质对流换热的比例,同时在提高金属微通道换热能力的同时降低工质在微通道中的流动阻力,减少驱动工质流动所需的泵功。整个散热机构实现了单次电子脉冲热流密度为1012-2×1012W/m2,平均热流密度为5×106-107W/m2的热量排散;石墨层4最高温不超过2000℃;低于石墨层4的熔点;金属主体1的最高温由2600℃降低至650℃。Step 6: The external electron beam is directed to the graphite layer 4 along the axial direction of the metal body 1; the external electron beam adopts the instantaneous pulse emission mode, and the single pulse emission power is 1-9GW; the single emission time is 100-500ns; the emission frequency is 10~50Hz. The heat is absorbed by the graphite layer (4) and transferred to the metal body 1 through the graphite layer 4, and finally the heat is taken away by the heat-dissipating working medium flowing through the double-spiral microchannel to realize heat dissipation. In terms of improving the heat dissipation capacity of the collector and reducing the flow resistance of the heat dissipation device, the structural parameters such as channel height, channel width and fin width of the metal microchannel structure are optimized to balance the thermal conductivity and thermal conductivity of the fins during the internal heat transfer process of the metal microchannel. Through the ratio of convective heat transfer of the working medium, the flow resistance of the working medium in the microchannel is reduced while the heat transfer capacity of the metal microchannel is improved, and the pump work required to drive the flow of the working medium is reduced. The whole heat dissipation mechanism realizes the heat dissipation with a single electron pulse heat flux density of 10 12 -2×10 12 W/m 2 and an average heat flux density of 5×10 6 -10 7 W/m 2 ; Over 2000°C; lower than the melting point of the graphite layer 4; the maximum temperature of the metal body 1 is reduced from 2600°C to 650°C.

瞬时脉冲发射的超大功率的电子束加载在石墨层上被石墨吸收,由于加热时间极短,热量在脉冲电子束加热时间内无法向外扩散,所以只有石墨中吸收电子束的区域温度立刻升高;之后在电子束脉冲加热间隔时间,热量逐步由石墨通过金属微通道向散热通道内的工质传递,石墨吸收电子束区域的温度迅速降低,使得石墨在受到超大功率瞬时脉冲加热下温度不超过石墨的许用温度,同时由于金属微通道与石墨之间存在接触热阻,金属微通道的温度远低于石墨的温度,最高温距离金属的熔点也较远。因此,石墨与金属微通道复合的收集极散热装置能够在受到超大功率电子束瞬时脉冲加热的情况下维持安全稳定的运行。The ultra-high-power electron beam emitted by the instantaneous pulse is loaded on the graphite layer and absorbed by the graphite. Due to the extremely short heating time, the heat cannot diffuse outward during the heating time of the pulsed electron beam, so only the area of the graphite that absorbs the electron beam increases in temperature immediately. After that, in the interval of electron beam pulse heating, the heat is gradually transferred from the graphite to the working medium in the heat dissipation channel through the metal microchannel, and the temperature of the graphite absorbing electron beam area decreases rapidly, so that the temperature of the graphite does not exceed the ultra-high power instantaneous pulse heating. The allowable temperature of graphite, and due to the contact thermal resistance between the metal microchannel and the graphite, the temperature of the metal microchannel is much lower than that of the graphite, and the maximum temperature is also far from the melting point of the metal. Therefore, the collector heat-sinking device of graphite and metal microchannels can maintain safe and stable operation under the condition of instantaneous pulse heating of ultra-high-power electron beams.

本发明虽然已以较佳实施例公开如上,但其并不是用来限定本发明,任何本领域技术人员在不脱离本发明的精神和范围内,都可以利用上述揭示的方法和技术内容对本发明技术方案做出可能的变动和修改,因此,凡是未脱离本发明技术方案的内容,依据本发明的技术实质对以上实施例所作的任何简单修改、等同变化及修饰,均属于本发明技术方案的保护范围。Although the present invention has been disclosed above with preferred embodiments, it is not intended to limit the present invention. Any person skilled in the art can use the methods and technical contents disclosed above to improve the present invention without departing from the spirit and scope of the present invention. The technical solutions are subject to possible changes and modifications. Therefore, any simple modifications, equivalent changes and modifications made to the above embodiments according to the technical essence of the present invention without departing from the content of the technical solutions of the present invention belong to the technical solutions of the present invention. protected range.

Claims (4)

1.一种瞬时脉冲超大功率电子收集级复合散热方法,其特征在于:包括如下步骤:1. an instantaneous pulse super-power electron collection-level composite heat dissipation method, is characterized in that: comprise the steps: 步骤一、将金属主体(1)轴向竖直放置;Step 1, place the metal body (1) vertically in the axial direction; 步骤二、在金属主体(1)的侧壁内加工双螺旋微通道;Step 2, processing double helical microchannels in the sidewall of the metal body (1); 步骤三、在金属主体(1)的内壁贴附石墨层(4);Step 3, attaching a graphite layer (4) to the inner wall of the metal body (1); 步骤四、调整金属主体(1)位置,实现外部电子束射在石墨层(4)内壁的电子束沉积加热区域(41);Step 4, adjusting the position of the metal body (1) to realize the electron beam deposition heating area (41) in which the external electron beam is irradiated on the inner wall of the graphite layer (4); 步骤五、双螺旋微通道中流动散热工质;Step 5. Flow heat dissipation working medium in the double helix microchannel; 步骤六、外部电子束沿金属主体(1)轴向方向射向石墨层(4);热量通过石墨层(4)的吸收以及通过石墨层(4)向金属主体(1)传递,最终通过双螺旋微通道流动的散热工质将热量带走,实现散热;Step 6: The external electron beam is directed towards the graphite layer (4) along the axial direction of the metal body (1); the heat is absorbed by the graphite layer (4) and transferred to the metal body (1) through the graphite layer (4), and finally passes through the double The heat dissipation working medium flowing in the spiral microchannel takes the heat away and realizes heat dissipation; 所述步骤一中,所述金属主体(1)为圆环状结构;金属主体(1)为不锈钢材料或钛材料;金属主体(1)外壁直径为60~150mm,轴向长度为10-50mm;壁厚为3-5mm;In the step 1, the metal main body (1) is an annular structure; the metal main body (1) is made of stainless steel or titanium material; the diameter of the outer wall of the metal main body (1) is 60-150 mm, and the axial length is 10-50 mm ;Wall thickness is 3-5mm; 所述步骤二中,所述双螺旋微通道包括第一螺旋微通道(2)和第二螺旋微通道(3);第一螺旋微通道(2)与第二螺旋微通道(3)均为螺旋环状通道;且第一螺旋微通道(2)与第二螺旋微通道(3)交错设置;第一螺旋微通道(2)的入口(21)在金属主体(1)轴向底端;出口(22)在金属主体(1)轴向顶端;第二螺旋微通道(3)的入口(31)在金属主体(1)轴向顶端;出口(32)在金属主体(1)轴向底端;第一螺旋微通道(2)与第二螺旋微通道(3)的螺旋方向相反;In the second step, the double helical microchannel includes a first helical microchannel (2) and a second helical microchannel (3); the first helical microchannel (2) and the second helical microchannel (3) are both. a spiral annular channel; and the first spiral microchannel (2) and the second spiral microchannel (3) are alternately arranged; the inlet (21) of the first spiral microchannel (2) is at the axial bottom end of the metal body (1); The outlet (22) is at the axial top of the metal body (1); the inlet (31) of the second helical microchannel (3) is at the axial top of the metal body (1); the outlet (32) is at the axial bottom of the metal body (1). end; the helical directions of the first helical microchannel (2) and the second helical microchannel (3) are opposite; 所述第一螺旋微通道(2)和第二螺旋微通道(3)的管道截面为矩形结构;管道截面尺寸为3mm*1mm;The pipe sections of the first helical microchannel (2) and the second helical microchannel (3) are rectangular structures; the size of the pipe section is 3mm*1mm; 所述步骤五中,散热工质为离子水,导热系数为0.6W/(K·m),比热容为4183J/(kg·K);In the step 5, the heat dissipation working medium is ionized water, the thermal conductivity is 0.6W/(K·m), and the specific heat capacity is 4183J/(kg·K); 石墨层(4)为环形层状结构;石墨层(4)轴向长度为10-50mm;壁厚为1-2mm;熔点为3000℃;The graphite layer (4) has an annular layered structure; the axial length of the graphite layer (4) is 10-50 mm; the wall thickness is 1-2 mm; the melting point is 3000° C.; 所述步骤四中,所述电子束沉积加热区域(41)设置在石墨层(4)内壁的中部位置;电子束沉积加热区域(41)为环形区域;轴向长度为5-25mm;电子束沉积加热区域(41)的侧面积为石墨层(4)内壁面积的一半。In the fourth step, the electron beam deposition heating area (41) is arranged in the middle position of the inner wall of the graphite layer (4); the electron beam deposition heating area (41) is an annular area; the axial length is 5-25 mm; the electron beam The lateral area of the deposition heating area (41) is half the area of the inner wall of the graphite layer (4). 2.根据权利要求1所述的一种瞬时脉冲超大功率电子收集级复合散热方法,其特征在于:所述金属主体(1)与石墨层(4)采用分子扩散焊焊接;实现金属主体(1)与石墨层(4)之间的接触热阻降低;接触传热系数为5000~10000W/(K·m2)。2. A kind of instantaneous pulse super-power electron collection-level composite heat dissipation method according to claim 1, characterized in that: the metal main body (1) and the graphite layer (4) are welded by molecular diffusion welding; ) and the graphite layer (4), the contact thermal resistance is reduced; the contact heat transfer coefficient is 5000-10000 W/(K·m 2 ). 3.根据权利要求2所述的一种瞬时脉冲超大功率电子收集级复合散热方法,其特征在于:所述步骤六中,外部电子束采用瞬时脉冲发射方式,单次脉冲发射功率为1~9GW;单次发射时间为100-500ns;发射频率为10~50Hz。3. A kind of instantaneous pulse ultra-high power electron collection-level composite heat dissipation method according to claim 2, characterized in that: in the step 6, the external electron beam adopts the instantaneous pulse emission mode, and the single pulse emission power is 1~9GW ;Single transmission time is 100-500ns; transmission frequency is 10~50Hz. 4.根据权利要求3所述的一种瞬时脉冲超大功率电子收集级复合散热方法,其特征在于:整个散热机构实现了单次电子脉冲热流密度为1012-2×1012W/m2,平均热流密度为5×106-107W/m2的热量排散;石墨层(4)最高温不超过2000℃;低于石墨层(4)的熔点;金属主体(1)的最高温由2600℃降低至650℃。4. A kind of instantaneous pulse super-power electron collection-level composite heat dissipation method according to claim 3, characterized in that: the whole heat dissipation mechanism realizes a single electron pulse heat flux density of 10 12 -2×10 12 W/m 2 , Heat dissipation with an average heat flux density of 5×10 6 -10 7 W/m 2 ; the maximum temperature of the graphite layer (4) does not exceed 2000°C; lower than the melting point of the graphite layer (4); the maximum temperature of the metal body (1) Decrease from 2600℃ to 650℃.
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