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CN110729525A - An air-cooled battery thermal management system cooling channel wind speed acquisition method - Google Patents

An air-cooled battery thermal management system cooling channel wind speed acquisition method Download PDF

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CN110729525A
CN110729525A CN201911023811.2A CN201911023811A CN110729525A CN 110729525 A CN110729525 A CN 110729525A CN 201911023811 A CN201911023811 A CN 201911023811A CN 110729525 A CN110729525 A CN 110729525A
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air
cooling channel
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武国良
李罡
李国强
祖光鑫
尚博宇
吕超
宋彦孔
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State Grid Corp of China SGCC
Electric Power Research Institute of State Grid Heilongjiang Electric Power Co Ltd
Harbin Institute of Technology Shenzhen
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Electric Power Research Institute of State Grid Heilongjiang Electric Power Co Ltd
Harbin Institute of Technology Shenzhen
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01MPROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
    • H01M10/00Secondary cells; Manufacture thereof
    • H01M10/60Heating or cooling; Temperature control
    • H01M10/61Types of temperature control
    • H01M10/613Cooling or keeping cold
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01MPROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
    • H01M10/00Secondary cells; Manufacture thereof
    • H01M10/60Heating or cooling; Temperature control
    • H01M10/63Control systems
    • H01M10/633Control systems characterised by algorithms, flow charts, software details or the like
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01MPROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
    • H01M10/00Secondary cells; Manufacture thereof
    • H01M10/60Heating or cooling; Temperature control
    • H01M10/65Means for temperature control structurally associated with the cells
    • H01M10/655Solid structures for heat exchange or heat conduction
    • H01M10/6556Solid parts with flow channel passages or pipes for heat exchange
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01MPROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
    • H01M10/00Secondary cells; Manufacture thereof
    • H01M10/60Heating or cooling; Temperature control
    • H01M10/65Means for temperature control structurally associated with the cells
    • H01M10/656Means for temperature control structurally associated with the cells characterised by the type of heat-exchange fluid
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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
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    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
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Abstract

一种风冷式电池热管理系统冷却流道风速获得方法,涉及锂离子电池散热领域。本发明是为了解决传统的获得电池热管理系统内风速分布的方式复杂、获得风速分布的效率低的问题。本申请建立风冷式锂离子电池热管理系统的流阻网络模型实现对各个流道内冷却空气流速的快速计算。它用于获得冷却通道的风速。

Figure 201911023811

A method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system relates to the field of heat dissipation of lithium ion batteries. The present invention aims to solve the problems that the traditional method of obtaining the wind speed distribution in the battery thermal management system is complicated and the efficiency of obtaining the wind speed distribution is low. The present application establishes a flow resistance network model of an air-cooled lithium-ion battery thermal management system to quickly calculate the cooling air flow rate in each flow channel. It is used to obtain the wind speed of the cooling channel.

Figure 201911023811

Description

一种风冷式电池热管理系统冷却通道风速获得方法An air-cooled battery thermal management system cooling channel wind speed acquisition method

技术领域technical field

本发明涉及风冷式电池热管理系统冷却流道风速获得方法。属于锂离子电池散热领域。The invention relates to a method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system. It belongs to the field of heat dissipation of lithium ion batteries.

背景技术Background technique

目前,能源紧缺、环境日益恶化,锂离子电池具有平均输出电压高、充放电效率高、环境友好等优点,使其在不同应用场合都得到了广泛关注。At present, energy is scarce and the environment is deteriorating day by day. Li-ion batteries have the advantages of high average output voltage, high charge and discharge efficiency, and environmental friendliness, making them widely concerned in different applications.

锂离子电池在实际应用过程中因为生热导致的安全和寿命问题十分突出。一方面,在 充放电过程中,电池内部热量不断累积,温度不断上升,如果不加以控制,有可能造成锂 电池的热失控,甚至会出现胀气、泄露、乃至爆炸等危险。另一方面,锂离子电池的老化 速度受到温度影响,当电池组内部各电池单体温度不均匀时,电池单体将逐渐出现性能差 异,根据短板原理,这将最终导致电池组的寿命缩短。因此对锂离子电池热管理系统进行 分析和设计是十分必要的。The safety and life problems of lithium-ion batteries due to heat generation in practical applications are very prominent. On the one hand, in the process of charging and discharging, the internal heat of the battery keeps accumulating and the temperature keeps rising. If it is not controlled, it may cause the thermal runaway of the lithium battery, and even the danger of flatulence, leakage, and even explosion. On the other hand, the aging speed of lithium-ion batteries is affected by temperature. When the temperature of each battery cell inside the battery pack is uneven, the battery cells will gradually have performance differences. According to the short board principle, this will eventually lead to a shortened battery pack life. . Therefore, it is necessary to analyze and design the thermal management system of lithium-ion battery.

空气强制对流冷却散热方式结构简单、成本低,广泛应用于电池热管理系统。在设计 风冷式电池热管理系统(BTMS)时,有限元仿真分析方法可以有效地获得气流分布。通常,BTMS的结构参数优化需要在优化过程中进行调整,并且应该进行成百上千次有限元 仿真计算以探索每个结构参数的热性能。传统的有限元仿真分析方法由于其计算效率低已不再适用,需要对BTMS的风速分布计算进行简化。The forced air convection cooling method is simple in structure and low in cost, and is widely used in battery thermal management systems. When designing an air-cooled battery thermal management system (BTMS), the finite element simulation analysis method can effectively obtain the airflow distribution. Typically, structural parameter optimization of BTMS requires adjustments during the optimization process, and hundreds or thousands of finite element simulation calculations should be performed to explore the thermal performance of each structural parameter. The traditional finite element simulation analysis method is no longer applicable due to its low computational efficiency, and it is necessary to simplify the wind speed distribution calculation of BTMS.

发明内容SUMMARY OF THE INVENTION

本发明是为了解决传统的获得电池热管理系统内风速分布的方式复杂、获得风速分布 的效率低的问题。现提供一种风冷式电池热管理系统冷却通道风速获得方法。The present invention is to solve the problems that the traditional way of obtaining the wind speed distribution in the battery thermal management system is complicated and the efficiency of obtaining the wind speed distribution is low. A method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system is provided.

一种风冷式电池热管理系统冷却通道风速获得方法,所述方法包括以下步骤:A method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system, the method comprising the following steps:

步骤一、在Z型风冷式电池热管理系统内部锂离子电池阵列的顶部和底部分别设置一 个出风口导流板和进风口导流板,出风口导流板与Z型风冷式电池热管理系统顶面之间的 夹角为θ2,进风口导流板与Z型风冷式电池热管理系统底面之间的夹角为θ1,使得每列锂 离子电池的顶部与出风口导流板之间形成一个汇流通道、每列锂离子电池的底部与进风口 导流板之间形成一个分流通道,每列锂离子电池的两侧为两个冷却通道;Step 1. Set an air outlet deflector and an air inlet deflector on the top and bottom of the lithium-ion battery array in the Z-type air-cooled battery thermal management system, respectively, and the air outlet deflector and the Z-type air-cooled battery thermal The included angle between the top surface of the management system is θ 2 , and the included angle between the air inlet deflector and the bottom surface of the Z-type air-cooled battery thermal management system is θ 1 , so that the top of each row of lithium-ion batteries is guided to the air outlet. A confluence channel is formed between the flow plates, a shunt channel is formed between the bottom of each column of lithium-ion batteries and the air inlet guide plate, and two cooling channels are formed on both sides of each column of lithium-ion batteries;

步骤二、将每列锂离子电池顶部的汇流通道、底部的分流通道和两侧冷却通道内的气 体压强求和获得压强和,利用空气流量守恒方程得到流阻网络模型,所述空气流量守恒方 程包括相互连通的分流通道与冷却通道内的空气流量守恒方程和相互连通的汇流通道与冷 却通道内的空气流量守恒方程;Step 2. The summation of the gas pressures in the confluence channel at the top of each row of lithium-ion batteries, the shunt channel at the bottom and the cooling channels on both sides to obtain the pressure sum, and the flow resistance network model is obtained by using the air flow conservation equation. The air flow conservation equation Including the air flow conservation equation in the interconnected shunt channel and the cooling channel and the air flow conservation equation in the interconnected confluence channel and the cooling channel;

根据锂离子电池阵列的总长度和总宽度、θ2、相邻的两列锂离子电池间的距离,得到 每个分流通道的横截面积;根据该横截面积,得到每个分流通道的直径和相邻两个分流通 道的流量比值;According to the total length and width of the lithium-ion battery array, θ 2 , and the distance between two adjacent rows of lithium-ion batteries, the cross-sectional area of each shunt channel is obtained; according to the cross-sectional area, the diameter of each shunt channel is obtained and the flow ratio of two adjacent shunt channels;

根据锂离子电池阵列的总长度和总宽度、相邻的两列锂离子电池间的距离和θ1,得到 每个汇流通道的横截面积;根据该横截面积,得到每个汇流通道的直径和相邻两个汇流通 道的流量比值;According to the total length and width of the lithium-ion battery array, the distance between two adjacent rows of lithium-ion batteries and θ 1 , the cross-sectional area of each bus channel is obtained; according to the cross-sectional area, the diameter of each bus channel is obtained and the flow ratio of two adjacent confluence channels;

根据锂离子电池阵列的总长度和总宽度、相邻的两列锂离子电池间的距离,得到每个 冷却通道的横截面积;根据该横截面积,得到每个冷却通道的直径;According to the total length and width of the lithium-ion battery array, and the distance between two adjacent rows of lithium-ion batteries, the cross-sectional area of each cooling channel is obtained; according to the cross-sectional area, the diameter of each cooling channel is obtained;

根据每个冷却通道的横截面积和每个分流通道的横截面积得到每个冷却通道与每个分 流通道的流量比值;According to the cross-sectional area of each cooling channel and the cross-sectional area of each shunt channel, the flow ratio of each cooling channel and each shunt channel is obtained;

根据每个冷却通道的横截面积和每个汇流通道的横截面积得到每个冷却通道与每个汇 流通道的流量比值;According to the cross-sectional area of each cooling channel and the cross-sectional area of each collecting channel, the flow ratio of each cooling channel and each collecting channel is obtained;

步骤三、根据流阻网络模型、每个分流通道的直径、相邻两个分流通道的流量比值、 每个汇流通道的直径、相邻两个汇流通道的流量比值、每个冷却通道的直径、每个冷却通 道与每个分流通道的流量比值、每个冷却通道与每个汇流通道的流量比值,得到每个冷却 通道的风速。Step 3: According to the flow resistance network model, the diameter of each shunt channel, the flow ratio of two adjacent shunt channels, the diameter of each confluence channel, the flow ratio of two adjacent confluence channels, the diameter of each cooling channel, The flow ratio of each cooling channel and each split channel, and the flow ratio of each cooling channel and each confluence channel, to obtain the wind speed of each cooling channel.

本发明的有益效果:Beneficial effects of the present invention:

本申请建立风冷式锂离子电池热管理系统的流阻网络模型实现对各个通道内冷却空气 流速的快速计算。当风冷式BTMS的形状固定后,每个部分空气的流速均可以通过流阻网 络模型得到。此申请不仅保证了较高的计算精度,也极大地提高了通道风速的计算速度, 为风冷式BTMS的结构优化设计奠定了基础。The present application establishes a flow resistance network model of an air-cooled lithium-ion battery thermal management system to achieve rapid calculation of the cooling air flow rate in each channel. When the shape of the air-cooled BTMS is fixed, the flow velocity of each part of the air can be obtained through the flow resistance network model. This application not only ensures high calculation accuracy, but also greatly improves the calculation speed of the channel wind speed, laying a foundation for the structural optimization design of the air-cooled BTMS.

附图说明Description of drawings

图1为多个锂离子电池单体放置在Z型风冷式电池热管理系统内的三维结构图;Figure 1 is a three-dimensional structural diagram of a plurality of lithium-ion battery cells placed in a Z-type air-cooled battery thermal management system;

图2为多个锂离子电池单体放置在Z型风冷式电池热管理系统内的二维结构图;Figure 2 is a two-dimensional structural diagram of a plurality of lithium-ion battery cells placed in a Z-type air-cooled battery thermal management system;

图3为流阻网络模型原理图;Figure 3 is a schematic diagram of the flow resistance network model;

图4(a)为进风口风速为3m/s时,采用流阻网络模型和有限元仿真软件分别获得冷却 通道内的风速的曲线对比图,图4(b)为进风口风速为5m/s时,采用流阻网络模型和有限元仿真软件分别获得冷却通道内的风速的曲线对比图;Figure 4(a) is the curve comparison of the air velocity in the cooling channel obtained by using the flow resistance network model and the finite element simulation software when the air velocity at the air inlet is 3m/s, and Figure 4(b) is the air velocity at the air inlet of 5m/s When the flow resistance network model and finite element simulation software are used to obtain the curve comparison diagram of the wind speed in the cooling channel;

图5(a)为进风口风速为3m/s时,采用流阻网络模型和有限元仿真软件分别获得冷却 通道内的风速的误差曲线图,图5(b)为为进风口风速为5m/s时,采用流阻网络模型和有限元仿真软件分别获得冷却通道内的风速的误差曲线图;Figure 5(a) is the error curve of the air velocity in the cooling channel obtained by using the flow resistance network model and the finite element simulation software when the air velocity at the air inlet is 3m/s. Figure 5(b) is the air velocity at the air inlet of 5m/s s, the flow resistance network model and the finite element simulation software are used to obtain the error curve of the wind speed in the cooling channel respectively;

图6(a)为进风口风速为3m/s时,采用流阻网络模型和实验分别获得冷却通道内的风 速的曲线对比图,图6(b)为进风口风速为5m/s时,采用流阻网络模型和实验分别获得冷却通道内的风速的曲线对比图;Figure 6(a) is a comparison diagram of the air velocity in the cooling channel obtained by using the flow resistance network model and experiment when the air velocity at the air inlet is 3m/s, and Figure 6(b) is when the air velocity at the air inlet is 5m/s, using The flow resistance network model and the experiment respectively obtain the curve comparison chart of the wind speed in the cooling channel;

图7(a)为为进风口风速为3m/s时,采用流阻网络模型和实验分别获得冷却通道内的 风速的误差曲线图,图7(b)为为进风口风速为5m/s时,采用流阻网络模型和实验分别获得冷却通道内的风速的误差曲线图。Figure 7(a) is the error curve of the air velocity in the cooling channel obtained by using the flow resistance network model and experiment when the air velocity at the air inlet is 3m/s, and Figure 7(b) is when the air velocity at the air inlet is 5m/s , using the flow resistance network model and the experiment to obtain the error curve of the wind speed in the cooling channel, respectively.

具体实施方式Detailed ways

具体实施方式一:参照图1至图3具体说明本实施方式,本实施方式所述的一种风冷 式电池热管理系统冷却通道风速获得方法,所述方法包括以下步骤:Embodiment 1: The present embodiment will be described in detail with reference to FIGS. 1 to 3. A method for obtaining the wind speed of the cooling channel of an air-cooled battery thermal management system described in the present embodiment includes the following steps:

步骤一、在Z型风冷式电池热管理系统内部锂离子电池阵列的顶部和底部分别设置一 个出风口导流板和进风口导流板,出风口导流板与Z型风冷式电池热管理系统顶面之间的 夹角为θ2,进风口导流板与Z型风冷式电池热管理系统底面之间的夹角为θ1,使得每列锂 离子电池的顶部与出风口导流板之间形成一个汇流通道、每列锂离子电池的底部与进风口 导流板之间形成一个分流通道,每列锂离子电池的两侧为两个冷却通道;Step 1. Set an air outlet deflector and an air inlet deflector on the top and bottom of the lithium-ion battery array in the Z-type air-cooled battery thermal management system, respectively, and the air outlet deflector and the Z-type air-cooled battery thermal The included angle between the top surface of the management system is θ 2 , and the included angle between the air inlet deflector and the bottom surface of the Z-type air-cooled battery thermal management system is θ 1 , so that the top of each row of lithium-ion batteries is guided to the air outlet. A confluence channel is formed between the flow plates, a shunt channel is formed between the bottom of each column of lithium-ion batteries and the air inlet guide plate, and two cooling channels are formed on both sides of each column of lithium-ion batteries;

步骤二、将每列锂离子电池顶部的汇流通道、底部的分流通道和两侧冷却通道内的气 体压强求和获得压强和,利用空气流量守恒方程得到流阻网络模型,所述空气流量守恒方 程包括相互连通的分流通道与冷却通道内的空气流量守恒方程和相互连通的汇流通道与冷 却通道内的空气流量守恒方程;Step 2. The summation of the gas pressures in the confluence channel at the top of each row of lithium-ion batteries, the shunt channel at the bottom and the cooling channels on both sides to obtain the pressure sum, and the flow resistance network model is obtained by using the air flow conservation equation. The air flow conservation equation Including the air flow conservation equation in the interconnected shunt channel and the cooling channel and the air flow conservation equation in the interconnected confluence channel and the cooling channel;

根据锂离子电池阵列的总长度和总宽度、θ2、相邻的两列锂离子电池间的距离,得到 每个分流通道的横截面积;根据该横截面积,得到每个分流通道的直径和相邻两个分流通 道的流量比值;According to the total length and width of the lithium-ion battery array, θ 2 , and the distance between two adjacent rows of lithium-ion batteries, the cross-sectional area of each shunt channel is obtained; according to the cross-sectional area, the diameter of each shunt channel is obtained and the flow ratio of two adjacent shunt channels;

根据锂离子电池阵列的总长度和总宽度、相邻的两列锂离子电池间的距离和θ1,得到 每个汇流通道的横截面积;根据该横截面积,得到每个汇流通道的直径和相邻两个汇流通 道的流量比值;According to the total length and width of the lithium-ion battery array, the distance between two adjacent rows of lithium-ion batteries and θ 1 , the cross-sectional area of each bus channel is obtained; according to the cross-sectional area, the diameter of each bus channel is obtained and the flow ratio of two adjacent confluence channels;

根据锂离子电池阵列的总长度和总宽度、相邻的两列锂离子电池间的距离,得到每个 冷却通道的横截面积;根据该横截面积,得到每个冷却通道的直径;According to the total length and width of the lithium-ion battery array, and the distance between two adjacent rows of lithium-ion batteries, the cross-sectional area of each cooling channel is obtained; according to the cross-sectional area, the diameter of each cooling channel is obtained;

根据每个冷却通道的横截面积和每个分流通道的横截面积得到每个冷却通道与每个分 流通道的流量比值;According to the cross-sectional area of each cooling channel and the cross-sectional area of each shunt channel, the flow ratio of each cooling channel and each shunt channel is obtained;

根据每个冷却通道的横截面积和每个汇流通道的横截面积得到每个冷却通道与每个汇 流通道的流量比值;According to the cross-sectional area of each cooling channel and the cross-sectional area of each collecting channel, the flow ratio of each cooling channel and each collecting channel is obtained;

步骤三、根据流阻网络模型、每个分流通道的直径、相邻两个分流通道的流量比值、 每个汇流通道的直径、相邻两个汇流通道的流量比值、每个冷却通道的直径、每个冷却通 道与每个分流通道的流量比值、每个冷却通道与每个汇流通道的流量比值,得到每个冷却 通道的风速。Step 3: According to the flow resistance network model, the diameter of each shunt channel, the flow ratio of two adjacent shunt channels, the diameter of each confluence channel, the flow ratio of two adjacent confluence channels, the diameter of each cooling channel, The flow ratio of each cooling channel and each split channel, and the flow ratio of each cooling channel and each confluence channel, to obtain the wind speed of each cooling channel.

本实施方式中,本申请以N×M方形铝壳动力锂离子电池组及其Z型槽电池热管理系统 为例,如图1所示。将该锂离子电池组放置在Z型风冷式电池热管理系统内,In this embodiment, the present application takes an N×M square aluminum shell power lithium-ion battery pack and its Z-slot battery thermal management system as an example, as shown in FIG. 1 . The lithium-ion battery pack is placed in the Z-type air-cooled battery thermal management system,

空气从进风口流入冷却系统并通过分流室(Divergence Plenum,简称为DP)进入冷却通 道。电池单元的热量被冷却通道(Cooling Channel,简称为CC)中的空气带走,然后空气在 汇流室(Convergence Plenum,简称为CP)汇集从出风口流出。Air flows into the cooling system from the air inlet and enters the cooling channel through the Divergence Plenum (DP for short). The heat of the battery cells is taken away by the air in the cooling channel (CC for short), and then the air is collected in the converging chamber (CP) and flows out from the air outlet.

考虑由Z型槽构成的锂离子电池热管理系统在理想条件下,进风口风速均一,Z型槽 内壁粗糙程度均匀,电池组各电池单体的极柱可以忽略不计,三维风冷式BTMS可以被等效成二维风冷式BTMS,如图2所示。Considering that the thermal management system of the lithium-ion battery composed of Z-shaped grooves is under ideal conditions, the air velocity at the air inlet is uniform, the inner wall of the Z-shaped groove is uniform, and the poles of each battery cell in the battery pack can be ignored. The three-dimensional air-cooled BTMS can It is equivalent to a two-dimensional air-cooled BTMS, as shown in Figure 2.

图3为流阻网络模型原理图,其中,每个方框区域代表因空气流动而产生该部分的压 差,称之为流阻。这种现象主要是由于当气流速度发生变化时空气在其动能和静压之间的 能量转换,以及由于能量损失,包括由于空气和粗糙通道壁之间摩擦引起的不可逆损失和 在某些特殊位置的空气分布和收敛引起的局部能量损失。根据相关流体力学理论,实际锂 离子电池组工作过程中风速远小于声速,所以空气被认为是不可压缩的牛顿流体,对于连 续流动过程,根据伯努利方程,得到公式1和公式2。Figure 3 is a schematic diagram of the flow resistance network model, in which each box area represents the pressure difference of this part due to air flow, which is called flow resistance. This phenomenon is mainly due to the energy conversion of the air between its kinetic energy and static pressure when the airflow velocity changes, and due to energy losses, including irreversible losses due to friction between the air and rough channel walls and at some special locations Local energy loss due to air distribution and convergence. According to the relevant fluid mechanics theory, the wind speed is much lower than the sound speed in the actual working process of the lithium-ion battery, so air is considered as an incompressible Newtonian fluid. For the continuous flow process, according to the Bernoulli equation, Equation 1 and Equation 2 are obtained.

锂离子电池阵列包括多个呈矩形阵列排布的多个单体。相邻两列电池之间的间距可以 相等也可以不相等。The lithium-ion battery array includes a plurality of cells arranged in a rectangular array. The spacing between two adjacent columns of cells may or may not be equal.

具体实施方式二:本实施方式是对具体实施方式一所述的一种风冷式电池热管理系统 冷却通道风速计算方法作进一步说明,本实施方式中,步骤二中,得到压强和的具体过程 为:Embodiment 2: This embodiment further describes the method for calculating the wind speed of the cooling channel of an air-cooled battery thermal management system described in Embodiment 1. In this embodiment, in step 2, the specific process of obtaining the sum of pressures for:

根据伯努利方程,得到第i个分流通道的压强PDP,i和第i个汇流通道的压强PCP,i分别为:According to Bernoulli's equation, the pressure P DP,i of the ith branch channel and the pressure P CP,i of the ith confluence channel are obtained as:

Figure BDA0002248056550000051
Figure BDA0002248056550000051

式中,PDP,1为第1个分流通道的压强,ρair为空气密度,vDP,i为第i个分流通道的风速, i=1至n,n为锂离子电池的列数,ΔPloss,DP,k为第k个分流通道的总压强差,PCP,1PCP,i为第1 个汇流通道的压强,vCP,i为第i个汇流通道的风速,vCP,1为第1个汇流通道的风速,ΔPloss,CP,k为第k个汇流通道的总压强差;In the formula, P DP,1 is the pressure of the first shunt channel, ρ air is the air density, v DP,i is the wind speed of the ith shunt channel, i=1 to n, n is the number of columns of lithium-ion batteries, ΔP loss,DP,k is the total pressure difference of the k-th shunt channel, P CP,1 P CP,i is the pressure of the first confluence channel, v CP,i is the wind speed of the i-th confluence channel, v CP, 1 is the wind speed of the first confluence channel, ΔP loss, CP,k is the total pressure difference of the k-th confluence channel;

风从第i-1个分流通道依次流向第i个冷却通道和第i个汇流通道,第i-1个分流通道、 第i个冷却通道和第i个汇流通道的压强关系为:The wind flows from the i-1th split channel to the i-th cooling channel and the i-th confluence channel in turn. The pressure relationship between the i-1th split channel, the i-th cooling channel and the i-th confluence channel is:

式中,ΔPloss,CC,i为第i个冷却通道的总压强差,vDP,i-1为第i-1个分流通道的风速,vDP,0为 Z型风冷式电池热管理系统进风口的风速;In the formula, ΔP loss,CC,i is the total pressure difference of the ith cooling channel, vDP,i-1 is the wind speed of the ith-1th shunt channel, and vDP,0 is the thermal management of the Z-type air-cooled battery The wind speed of the air inlet of the system;

根据公式1至公式3,得到每列锂离子电池顶部汇流通道、底部分流通道和两侧冷却 通道内的气体压强构成的压强和:According to Equation 1 to Equation 3, the sum of the pressures formed by the gas pressures in the top bus channel, bottom shunt channel and cooling channels on both sides of each column of lithium-ion batteries is obtained:

ΔPloss,DP,i+ΔPloss,CC,i+1-ΔPloss,CP,i-ΔPloss,CC,i=0 公式4,ΔP loss,DP,i +ΔP loss,CC,i+1 -ΔP loss,CP,i -ΔP loss,CC,i =0 Equation 4,

式中,ΔPloss,DP,i为第i个分流通道的总压强差,ΔPloss,CC,i+1为第i+1个冷却通道的总 压强差,ΔPloss,CP,i为第i个汇流通道的总压强差。In the formula, ΔP loss,DP,i is the total pressure difference of the ith shunt channel, ΔP loss,CC,i+1 is the total pressure difference of the ith+1 cooling channel, ΔP loss,CP,i is the ith The total pressure difference of the bus channels.

本实施方式中,公式4是形成流阻网络模型的主要控制方程,类似于电路中的基尔霍 夫电压定律。从公式4可以看出,图3中每个闭环的静态压差之和为零。In this embodiment, Equation 4 is the main governing equation for forming the flow resistance network model, which is similar to Kirchhoff's voltage law in the circuit. As can be seen from Equation 4, the sum of the static differential pressures for each closed loop in Figure 3 is zero.

具体实施方式三:本实施方式是对具体实施方式二所述的一种风冷式电池热管理系统 冷却通道风速计算方法作进一步说明,本实施方式中,第i个分流通道的总压强差 ΔPloss,DP,i、第i个冷却通道的总压强差ΔPloss,CC,i和第i个汇流通道的总压强差ΔPloss,CP,i均由 相应通道的局部压差ΔPlocal和沿程压差ΔPfriction组成,公式表示为:Embodiment 3: This embodiment further describes the method for calculating the wind speed of a cooling channel of an air-cooled battery thermal management system described in Embodiment 2. In this embodiment, the total pressure difference ΔP of the i-th shunt channel loss,DP,i , the total pressure difference ΔP loss,CC,i of the ith cooling channel and the total pressure difference ΔP loss,CP,i of the ith confluence channel are determined by the local pressure difference ΔP local and along the path of the corresponding channel. The pressure difference ΔP friction is composed, and the formula is expressed as:

ΔPloss=ΔPlocal+ΔPfriction 公式5,ΔP loss = ΔP local + ΔP friction Formula 5,

式中,

Figure BDA0002248056550000061
In the formula,
Figure BDA0002248056550000061

Figure BDA0002248056550000063
Figure BDA0002248056550000063

Figure BDA0002248056550000064
Figure BDA0002248056550000064

Figure BDA0002248056550000065
Figure BDA0002248056550000065

λDP,i为第i个分流通道的无量纲摩擦常数,λCP,i为第i个汇流通道的无量纲摩擦常数, λCC,i为第i个冷却通道的无量纲摩擦常数,lDP,i为第i个分流通道的长度,lCP,i第i个汇流通 道的长度,lCC,i为第i个冷却通道的长度,DDP,i为第i个分流通道横截面积等效为圆形分流 通道面积后的圆形分流通道的直径,DCP,i为第i个汇流通道横截面积等效为圆形汇流通道 面积后的圆形汇流通道的直径,DCC,i为第i个冷却通道横截面积等效为圆形冷却通道面积 后的圆形冷却通道的直径,ζDP,i为第i个分流通道与第i-1个分流通道的局部压差系数,ζCP,i为第i个汇流通道与第i-1个汇流通道的局部压差系数,ζDP,0→CC,1为Z型风冷式电池热管理 系统进风口与第1个冷却通道间的局部压差系数,ζDP,i-1→CC,i为第i-1个分流通道与第i个冷 却通道间的局部压差系数,ζCC,i→CP,i为第i个冷却通道与第i个汇流通道间的局部压差系数, vDP,i-1为第i-1个分流通道的风速,vDP,0为Z型风冷式电池热管理系统进风口的风速,vCP,i为 第i个汇流通道的风速,vDP,i为第i个分流通道的风速,vCC,i为第i个冷却通道的风速。λ DP,i is the dimensionless friction constant of the ith shunt channel, λ CP,i is the dimensionless friction constant of the ith confluence channel, λ CC,i is the dimensionless friction constant of the ith cooling channel, l DP ,i is the length of the i-th shunt channel, l CP,i is the length of the ith-th confluence channel, l CC,i is the length of the ith-th cooling channel, D DP,i is the cross-sectional area of the ith-th shunt channel, etc. Efficiency is the diameter of the circular shunt channel after the area of the circular shunt channel, D CP,i is the diameter of the circular shunt channel after the cross-sectional area of the i-th shunt channel is equivalent to the area of the circular shunt channel, D CC,i is the diameter of the circular cooling channel after the cross-sectional area of the ith cooling channel is equivalent to the area of the circular cooling channel, ζ DP,i is the local pressure difference coefficient between the ith branch channel and the i-1th branch channel, ζ CP,i is the local pressure difference coefficient between the ith bus channel and the i-1th bus channel, ζ DP,0→CC,1 is the air inlet of the Z-type air-cooled battery thermal management system and the first cooling channel The local pressure difference coefficient between the The coefficient of local pressure difference between the cooling channel and the i-th confluence channel, v DP,i-1 is the wind speed of the i-1th branch channel, v DP,0 is the wind speed of the air inlet of the Z-type air-cooled battery thermal management system , v CP,i is the wind speed of the ith confluence channel, v DP,i is the wind speed of the ith shunt channel, and v CC,i is the wind speed of the ith cooling channel.

具体实施方式四:本实施方式是对具体实施方式三所述的一种风冷式电池热管理系统 冷却通道风速计算方法作进一步说明,本实施方式中,第i个分流通道与第i-1个分流通道 的局部压差系数ζDP,i表示为:Embodiment 4: This embodiment further describes the method for calculating the wind speed of a cooling channel of an air-cooled battery thermal management system described in Embodiment 3. In this embodiment, the i-th shunt channel and the i-1th The local differential pressure coefficient ζ DP,i of each shunt channel is expressed as:

Figure BDA0002248056550000071
Figure BDA0002248056550000071

式中,pDP,i为第i个分流通道与第i-1个分流通道的流量比值;In the formula, p DP,i is the flow ratio of the i-th shunt channel to the i-1 th shunt channel;

第i-1个分流通道与第i个冷却通道间的局部压差系数ζDP,i-1→CC,i表示为:The local pressure difference coefficient ζ DP,i-1→CC,i between the i-1th shunt channel and the i-th cooling channel is expressed as:

Figure BDA0002248056550000072
Figure BDA0002248056550000072

式中,pDP,i-1→CC,i为第i-1个冷却通道与第i个分流通道流量的比值,ψDP,i-1→CC,i为第i-1 个分流通道与第i个冷却通道横截面积的比值,pDP,0→CC,1为Z型风冷式电池热管理系统进 风口与第1个分流通道流量的比值,ψDP,0→CC,1为Z型风冷式电池热管理系统进风口与第1个冷却通道横截面积的比值;In the formula, p DP,i-1→CC,i is the ratio of the flow rate of the i-1th cooling channel to the i-th split channel, ψ DP,i-1→CC,i is the i-1th split channel and The ratio of the cross-sectional area of the i-th cooling channel, p DP,0→CC,1 is the ratio of the air inlet of the Z-type air-cooled battery thermal management system to the flow rate of the first shunt channel, ψ DP,0→CC,1 is The ratio of the air inlet of the Z-type air-cooled battery thermal management system to the cross-sectional area of the first cooling channel;

第i个汇流通道与第i-1个汇流通道的局部压差系数ζCP,i表示为:The local pressure difference coefficient ζ CP,i of the ith confluence channel and the i-1 th confluence channel is expressed as:

ζCP,i=1-p2 CP,i 公式8,ζ CP,i =1-p 2 CP,i Formula 8,

式中,pCP,i为第i个汇流通道与第i-1个汇流通道的流量比值;In the formula, p CP,i is the flow ratio between the ith confluence channel and the i-1 th confluence channel;

第i个冷却通道与第i个汇流通道间的局部压差系数ζCC,i→CP,i表示为:The local pressure difference coefficient ζ CC,i→CP,i between the ith cooling channel and the ith confluence channel is expressed as:

ζCC,i→CP,i=p2 CC,i→CP,iψ2 CC,i→CP,i-2p2 CC,i→CP,i-1 公式9,ζ CC,i→CP,i =p 2 CC,i→CP,i ψ 2 CC,i→CP,i −2p 2 CC,i→CP,i −1 Equation 9,

式中,p2 CC,i→CP,i为第i个冷却通道与第i个汇流通道流量的比值,ψCC,i→CP,i为第i个汇 流通道与第i个冷却通道横截面积的比值。In the formula, p 2 CC,i→CP,i is the ratio of the flow of the ith cooling channel to the ith confluence channel, ψ CC,i→CP,i is the cross section of the ith confluence channel and the ith cooling channel area ratio.

具体实施方式五:本实施方式是对具体实施方式三所述的一种风冷式电池热管理系统 冷却通道风速计算方法作进一步说明,本实施方式中,第i个分流通道的无量纲摩擦常数 λDP,i、第i个汇流通道的无量纲摩擦常数λCP,i和第i个冷却通道的无量纲摩擦常数λCC,i均表 示为:Embodiment 5: This embodiment further describes a method for calculating the wind speed of a cooling channel of an air-cooled battery thermal management system described in Embodiment 3. In this embodiment, the dimensionless friction constant of the i-th shunt channel is λ DP,i , the dimensionless friction constant λ CP,i of the ith confluence channel and the dimensionless friction constant λ CC,i of the ith cooling channel are all expressed as:

Figure BDA0002248056550000073
Figure BDA0002248056550000073

式中,Re是局部雷诺数,Re=ρDU/μ,D为每个通道的直径,μ为空气的动力粘度, F为形状修正因子。where Re is the local Reynolds number, Re = ρDU/μ, D is the diameter of each channel, μ is the dynamic viscosity of air, and F is the shape correction factor.

具体实施方式六:本实施方式是对具体实施方式三所述的一种风冷式电池热管理系统 冷却通道风速计算方法作进一步说明,本实施方式中,根据公式11,得到相互连通的分流 通道与冷却通道内的空气流量守恒方程为:Embodiment 6: This embodiment further describes the method for calculating the wind speed of a cooling channel in an air-cooled battery thermal management system described in Embodiment 3. In this embodiment, according to formula 11, the shunt channels that communicate with each other are obtained. The conservation equation with the air flow in the cooling channel is:

vDP,iADP,i=vDP,i+1ADP,i+1+vCC,i+1ACC,i+1 公式11,v DP,i A DP,i =v DP,i+1 A DP,i+1 +v CC,i+1 A CC,i+1 Equation 11,

式中,Q0=vDP,1ADP,1,Q0为进风口空气的流量,ADP,i为第i个分流通道的截面积,ADP,i+1为第i+1个分流通道的截面积,vCC,i+1为第i+1个冷却通道的风速,vDP,i+1为第i+1个 分流通道的风速,In the formula, Q 0 =v DP,1 A DP,1 , Q 0 is the air flow at the air inlet, A DP,i is the cross-sectional area of the i-th shunt channel, A DP,i+1 is the i+1-th channel The cross-sectional area of the split channel, v CC,i+1 is the wind speed of the i+1th cooling channel, v DP,i+1 is the wind speed of the i+1th split channel,

根据公式12,得到相互连通的汇流通道与冷却通道内的空气流量守恒方程为:According to Equation 12, the air flow conservation equation in the interconnected confluence channel and cooling channel is obtained as:

vCP,iACP,i=vCP,i-1ACP,i-1+vCC,iACC,i 公式12,v CP,i A CP,i =v CP ,i -1 A CP ,i -1 +v CC,i A CC,i Equation 12,

式中,ACP,i为第i个汇流通道的截面积,ACP,i-1为第i-1个汇流通道的截面积,ACC,i为第i个冷却通道的截面积,ACP,i-1为第i-1个冷却通道的截面积,vCP,0=0,ACP,0=0。In the formula, A CP,i is the cross-sectional area of the ith confluence channel, A CP,i-1 is the cross-sectional area of the i-1 th confluence channel, A CC,i is the cross-sectional area of the ith cooling channel, A CP,i-1 is the cross-sectional area of the i-1th cooling channel, v CP,0 =0, A CP,0 =0.

本实施方式中,考虑到冷却的空气是不可压缩的,所以在每个空气分流点和汇集点空 气的流量是守恒的。因此,可以得到公式11和公式12。In this embodiment, considering that the cooled air is incompressible, the air flow rate is conserved at each air split point and collection point. Therefore, Equation 11 and Equation 12 can be obtained.

公式4~12提供了3×(N+1)个独立的方程。因此,当并行风冷式BTMS的形状固定后, 每部分空气的流速均可以通过流阻网络模型得到。局部压差系数ξ的大小取决于局部的几 何形状和流动状态。Equations 4-12 provide 3*(N+1) independent equations. Therefore, when the shape of the parallel air-cooled BTMS is fixed, the flow velocity of each part of the air can be obtained through the flow resistance network model. The magnitude of the local differential pressure coefficient ξ depends on the local geometry and flow state.

具体实施方式七:本实施方式是对具体实施方式一所述的一种风冷式电池热管理系统 冷却通道风速计算方法作进一步说明,本实施方式中,步骤三中,锂离子电池阵列的总长 度Wx表示为:Embodiment 7: This embodiment further describes the method for calculating the wind speed of the cooling channel of the air-cooled battery thermal management system described in Embodiment 1. In this embodiment, in step 3, the total amount of the lithium-ion battery array is The length W x is expressed as:

Figure BDA0002248056550000081
Figure BDA0002248056550000081

式中,N为锂离子电池的列数,lx为每列锂离子电池中的每个锂离子电池单体的长,di为相邻的两列锂离子电池间的距离;In the formula, N is the number of columns of lithium-ion batteries, lx is the length of each lithium-ion battery cell in each column of lithium-ion batteries, and d i is the distance between two adjacent columns of lithium-ion batteries;

锂离子电池阵列的总长度的总宽度Wy表示为:The total width W y of the total length of the lithium-ion battery array is expressed as:

Wy=M×ly+(M+1)×dy 公式14,W y =M× ly +(M+1)× dy Equation 14,

式中,M为每列锂离子电池中锂离子电池单体的数量,ly为每个锂离子电池单体的宽, dy为相邻的两列锂离子电池间的距离。In the formula, M is the number of lithium-ion battery cells in each column of lithium-ion batteries, ly is the width of each lithium-ion battery cell, and dy is the distance between two adjacent columns of lithium-ion batteries.

本实施方式中,设锂离子电池单体的长、宽和高分别为lx、ly、lz,其电池横向排布的 数量为N,电池纵向排布的数量为M,电池组横向间距分别为d1,d2,…,di,…,dN,dN+1, 电池组纵向间距为dy,则锂离子电池组的总长度Wx和总宽度Wy的表达式分别如公式13 和14所示。In this embodiment, the length, width, and height of the lithium-ion battery cells are set as lx, ly , and lz , respectively, the number of the horizontal arrangement of the batteries is N, the number of the vertical arrangement of the batteries is M, and the horizontal arrangement of the battery pack is The spacings are d 1 , d 2 , ..., d i , ..., d N , d N+1 , and the longitudinal spacing of the battery pack is dy , then the expressions of the total length W x and the total width W y of the lithium ion battery pack as shown in Equations 13 and 14, respectively.

具体实施方式八:本实施方式是对具体实施方式七所述的一种风冷式电池热管理系统 冷却通道风速计算方法作进一步说明,本实施方式中,步骤二中,每个分流通道的横截面 积获得过程为:Embodiment 8: This embodiment further describes the method for calculating the wind speed of a cooling channel of an air-cooled battery thermal management system described in Embodiment 7. In this embodiment, in step 2, the transverse direction of each shunt channel is The process of obtaining the cross-sectional area is:

进风口导流板与Z型风冷式电池热管理系统底面之间的角度θ1表示为:The angle θ1 between the air inlet deflector and the bottom surface of the Z-type air-cooled battery thermal management system is expressed as:

Figure BDA0002248056550000091
Figure BDA0002248056550000091

式中,w1为进风口导流板的角度调整参数;In the formula, w 1 is the angle adjustment parameter of the air inlet deflector;

将公式15带入公式16中,得到分流通道的横截面积ADP,i为:Bringing Equation 15 into Equation 16, the cross-sectional area A DP,i of the shunt channel is obtained as:

Figure BDA0002248056550000092
Figure BDA0002248056550000092

每个汇流通道的横截面积获得过程为:The process of obtaining the cross-sectional area of each bus channel is:

出风口导流板与Z型风冷式电池热管理系统顶面之间的角度θ2表示为:The angle θ2 between the air outlet baffle and the top surface of the Z-type air - cooled battery thermal management system is expressed as:

Figure BDA0002248056550000093
Figure BDA0002248056550000093

式中,w2为汇流通道角度调整参数;In the formula, w 2 is the adjustment parameter of the angle of the confluence channel;

汇流通道的横截面积ACP,i表示为:The cross-sectional area A CP,i of the bus channel is expressed as:

冷却通道的横截面积ACC,i表示为:The cross-sectional area A CC,i of the cooling channel is expressed as:

ACC,i=Wy·di 公式19。A CC,i = W y ·di Equation 19.

本实施方式中,进风口和出风口处均设置有一个导流板,进风口和出风口导流板的角 度分别为θ1和θ2,进风口和出风口导流板角度调整参数分别为w1和w2In this embodiment, both the air inlet and the air outlet are provided with a deflector, the angles of the air inlet and the air outlet deflector are θ 1 and θ 2 respectively, and the angle adjustment parameters of the air inlet and the air outlet deflector are respectively w 1 and w 2 .

具体实施方式九:本实施方式是对具体实施方式八所述的一种风冷式电池热管理系统 冷却通道风速计算方法作进一步说明,本实施方式中,将第i个分流通道横截面积ADP,i等 效为圆形分流通道的面积,等效后的圆形分流通道的直径DDP,i表示为:Embodiment 9: This embodiment further describes the method for calculating the wind speed of a cooling channel of an air-cooled battery thermal management system described in Embodiment 8. In this embodiment, the cross-sectional area A of the i-th shunt channel is DP,i is equivalent to the area of the circular shunt channel, and the diameter D DP,i of the equivalent circular shunt channel is expressed as:

将第i个汇流通道的横截面积ACP,i等效为圆形分流通道的面积,等效后的圆形分流通道 的直径DCP,i表示为:The cross-sectional area A CP,i of the ith confluence channel is equivalent to the area of the circular shunt channel, and the diameter D CP,i of the equivalent circular shunt channel is expressed as:

将第i个冷却通道的横截面积ACC,i等效为圆形分流通道的面积,等效后的圆形分流通 道的直径DCC,i表示为:The cross-sectional area A CC,i of the i-th cooling channel is equivalent to the area of the circular shunt channel, and the diameter D CC,i of the equivalent circular shunt channel is expressed as:

Figure BDA0002248056550000103
Figure BDA0002248056550000103

具体实施方式十:本实施方式是对具体实施方式九所述的一种风冷式电池热管理系统 冷却通道风速计算方法作进一步说明,本实施方式中,根据每个冷却通道的横截面积和每 个分流通道的横截面积得到每个冷却通道与每个分流通道的流量比值pDP,i-1→CC,iEmbodiment 10: This embodiment further describes the method for calculating the wind speed of a cooling channel of an air-cooled battery thermal management system described in Embodiment 9. In this embodiment, according to the cross-sectional area of each cooling channel and the The cross-sectional area of each shunt channel yields the flow ratio p DP,i-1→CC,i of each cooling channel and each shunt channel:

第i个冷却通道与第i-1个分流通道流量的比值表示为:The ratio of the flow rate of the i-th cooling channel to the i-1-th split channel flow is expressed as:

Figure BDA0002248056550000104
Figure BDA0002248056550000104

式中,pDP,i-1→CC,i为第i个冷却通道与第i-1个分流通道流量的比值;In the formula, p DP,i-1→CC,i is the ratio of the flow rate of the i-th cooling channel to the i-1th split channel;

根据每个冷却通道的横截面积和每个汇流通道的横截面积得到每个冷却通道与每个汇 流通道的流量比值pCC,i→CP,iAccording to the cross-sectional area of each cooling channel and the cross-sectional area of each collecting channel, the flow ratio p CC,i→CP,i of each cooling channel and each collecting channel is obtained:

Figure BDA0002248056550000105
Figure BDA0002248056550000105

式中,pCC,i→CP,i为第i个冷却通道与第i个汇流通道流量的比值;In the formula, p CC,i→CP,i is the ratio of the flow rate of the ith cooling channel to the ith confluence channel;

第i个分流通道与第i-1个分流通道的流量比值pDP,i表示为:The flow ratio p DP,i of the ith branch channel and the i-1th branch channel is expressed as:

Figure BDA0002248056550000111
Figure BDA0002248056550000111

式中,当i=1时,ADP,0表示进风口的横截面积。In the formula, when i=1, A DP,0 represents the cross-sectional area of the air inlet.

第i个汇流通道与第i-1个汇流通道的流量比值pCP,i表示为:The flow ratio p CP,i of the ith confluence channel and the i-1 th confluence channel is expressed as:

Figure BDA0002248056550000112
Figure BDA0002248056550000112

实验验证:Experimental verification:

本申请从有限元仿真和实验两个角度对采用流阻网络模型计算风冷式锂离子电池热管 理系统冷却通道风速的有效性和可靠性进行验证。This application verifies the validity and reliability of using the flow resistance network model to calculate the cooling channel wind speed of the air-cooled lithium-ion battery thermal management system from the perspectives of finite element simulation and experiment.

本申请采用由8×3方形铝壳动力锂离子电池单体组成的电池组构成的风冷式BTMS结 构装置,具体参数如表1所示。This application adopts an air-cooled BTMS structure device composed of a battery pack composed of 8 × 3 square aluminum shell power lithium-ion battery cells, and the specific parameters are shown in Table 1.

表1风冷式BTMS结构装置参数Table 1 Parameters of air-cooled BTMS structure device

Figure BDA0002248056550000113
Figure BDA0002248056550000113

方形铝壳三元(材料为镍,钴,锰)锂离子电池单体的相关参数如表3-2所示。The relevant parameters of the square aluminum shell ternary (materials are nickel, cobalt, manganese) lithium-ion battery cells are shown in Table 3-2.

表2电池基本参数Table 2 Basic battery parameters

风冷式电池热管理系统的流动域空气材料属性如表3所示。The material properties of the air in the flow domain of the air-cooled battery thermal management system are shown in Table 3.

表3空气材料属性Table 3 Air material properties

Figure BDA0002248056550000115
Figure BDA0002248056550000115

Figure BDA0002248056550000121
Figure BDA0002248056550000121

用仿真软件验证流阻网络模型的准确性:Use simulation software to verify the accuracy of the flow resistance network model:

本节通过在COMSOL Multiphysics仿真软件中建立风冷式锂离子电池热管理系统的仿 真模型以验证所建立的流阻网络模型的准确性与可靠性。In this section, a simulation model of an air-cooled lithium-ion battery thermal management system is established in the COMSOL Multiphysics simulation software to verify the accuracy and reliability of the established flow resistance network model.

利用COMSOL Multiphysics仿真软件建立的电池组几何模型,其中忽略了电池单体极 柱和焊接座对有限元仿真计算结果的影响。The geometric model of the battery pack established by the COMSOL Multiphysics simulation software ignores the influence of the battery cell pole and welding seat on the finite element simulation results.

考虑本申请所建立的风冷式锂离子电池热管理系统的流体部分相对复杂,因此采用结 构化网格划分方式,使用自由四面体网格单元,选用细化的网格单元大小。电池单体部分 采用自由三角形网格与扫掠结合的方式,选用常规的网格单元大小。对锂离子电池组以及 流体部分的网格剖分。Considering that the fluid part of the air-cooled lithium-ion battery thermal management system established in this application is relatively complex, a structured mesh division method is adopted, a free tetrahedral mesh element is used, and a refined mesh element size is selected. The battery cell part adopts the combination of free triangular mesh and sweep, and selects the conventional mesh unit size. Mesh the Li-Ion battery pack and the fluid section.

在风冷式BTMS装置具有导流板,且进风口和出风口导流板角度调整参数w1和w2均为10mm,各锂离子电池单体排布间距为20mm的情况下进行对比,进风口风速vin分别为 3m/s和5m/s的流阻网络模型与有限元仿真软件对冷却通道内风速的计算,对比图如图4 所示。The comparison is made under the condition that the air-cooled BTMS device has a deflector, and the angle adjustment parameters w 1 and w 2 of the air inlet and air outlet deflector are both 10mm, and the arrangement spacing of each lithium-ion battery cell is 20mm. Figure 4 shows the comparison between the flow resistance network model and the finite element simulation software for the air velocity v in of the tuyere, which are 3m/s and 5m/s respectively.

COMSOL Multiphysics仿真与流阻网络模型的误差曲线如图5所示。The error curves of the COMSOL Multiphysics simulation and the flow resistance network model are shown in Figure 5.

从图中可以看出,在误差允许的范围内,流阻网络模型对冷却通道内风速的计算是较 为准确的。It can be seen from the figure that within the allowable error range, the flow resistance network model is relatively accurate in calculating the wind speed in the cooling channel.

用实验装置验证流阻网络模型的准确性:Verify the accuracy of the flow resistance network model with an experimental setup:

最后从实验的角度验证流阻网络模型的准确性。用Z型风冷式电池热管理系统、进风 装置、风速测试仪、单相风机调速器和冷却通道风速测试圆孔组成的实验装置验证流阻网 络模型的准确性。Finally, the accuracy of the flow resistance network model is verified from the experimental point of view. The accuracy of the flow resistance network model is verified by an experimental device consisting of a Z-type air-cooled battery thermal management system, an air inlet device, an air speed tester, a single-phase fan speed regulator and a cooling channel air speed test hole.

风冷式BTMS为Z型槽,电池组采用8×3的排布方式,且为8串3并,布线时尽量贴 近壁面以减少其对风冷式BTMS冷却通道风速分布的影响。进风口的冷却空气由风扇提供, 且由单相风速调节器控制风扇的速度,冷却通道的风速由热敏式风速测试仪获得。The air-cooled BTMS has a Z-shaped slot, and the battery packs are arranged in an 8×3 arrangement with 8 strings and 3 parallels. The wiring should be as close to the wall as possible to reduce its influence on the air velocity distribution of the air-cooled BTMS cooling channel. The cooling air at the air inlet is provided by a fan, and the speed of the fan is controlled by a single-phase anemometer, and the air speed of the cooling channel is obtained by a thermal anemometer.

在风冷式BTMS装置具有导流板,且进风口和出风口导流板角度调整参数w1和w2均为10mm,各锂离子电池单体排布间距为20mm的情况下,进风口风速vin分别为3m/s和 5m/s的实验与流阻网络模型对冷却通道内风速的获取结果,对比图如图6所示。When the air-cooled BTMS device has a baffle, and the angle adjustment parameters w 1 and w 2 of the air inlet and outlet baffles are both 10 mm, and the arrangement spacing of each lithium-ion battery cell is 20 mm, the air velocity at the air inlet is The results obtained from the experiment and the flow resistance network model with v in being 3m/s and 5m/s respectively for the wind speed in the cooling channel are shown in Figure 6 for comparison.

第二组实验验证与流阻网络模型的误差曲线如图7所示。从图中可以看出,流阻网络 模型对冷却通道内风速的计算是较为准确的。The error curve of the second set of experimental verification and the flow resistance network model is shown in Figure 7. It can be seen from the figure that the flow resistance network model is more accurate in calculating the wind speed in the cooling channel.

本申请通过建立流阻网络模型实现了对风冷式电池热管理系统冷却通道内风速的快速 计算。根据风冷式BTMS的装置结构建立了其有限元仿真的流体模型并进行了仿真分析, 单次有限元仿真软件计算时间在3h以上,而单次流阻网络模型计算时间在1s以内,说明 了相较于传统的有限元仿真分析方法,在保证计算精度的前提下,流阻网络模型对风冷式 BTMS冷却通道内风速计算的快速性。最后搭建了实验装置平台,验证了基于流阻网络模 型的风冷式BTMS冷却流道风速计算方法具有较强的可行性和准确度。This application realizes the rapid calculation of the wind speed in the cooling channel of the air-cooled battery thermal management system by establishing a flow resistance network model. According to the device structure of the air-cooled BTMS, the finite element simulation fluid model of the air-cooled BTMS was established and the simulation analysis was carried out. The calculation time of the single finite element simulation software is more than 3h, while the calculation time of the single flow resistance network model is less than 1s. Compared with the traditional finite element simulation analysis method, under the premise of ensuring the calculation accuracy, the flow resistance network model can quickly calculate the wind speed in the air-cooled BTMS cooling channel. Finally, an experimental device platform was built to verify the feasibility and accuracy of the air-cooled BTMS cooling channel wind speed calculation method based on the flow resistance network model.

Claims (10)

1.一种风冷式电池热管理系统冷却通道风速获得方法,其特征在于,所述方法包括以下步骤:1. A method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system, wherein the method comprises the following steps: 步骤一、在Z型风冷式电池热管理系统内部锂离子电池阵列的顶部和底部分别设置一个出风口导流板和进风口导流板,出风口导流板与Z型风冷式电池热管理系统顶面之间的夹角为θ2,进风口导流板与Z型风冷式电池热管理系统底面之间的夹角为θ1,使得每列锂离子电池的顶部与出风口导流板之间形成一个汇流通道、每列锂离子电池的底部与进风口导流板之间形成一个分流通道,每列锂离子电池的两侧为两个冷却通道;Step 1. Set an air outlet deflector and an air inlet deflector on the top and bottom of the lithium-ion battery array in the Z-type air-cooled battery thermal management system, respectively, and the air outlet deflector and the Z-type air-cooled battery thermal The included angle between the top surface of the management system is θ 2 , and the included angle between the air inlet deflector and the bottom surface of the Z-type air-cooled battery thermal management system is θ 1 , so that the top of each row of lithium-ion batteries is guided to the air outlet. A confluence channel is formed between the flow plates, a shunt channel is formed between the bottom of each column of lithium-ion batteries and the air inlet guide plate, and two cooling channels are formed on both sides of each column of lithium-ion batteries; 步骤二、将每列锂离子电池顶部的汇流通道、底部的分流通道和两侧冷却通道内的气体压强求和获得压强和,利用空气流量守恒方程得到流阻网络模型,所述空气流量守恒方程包括相互连通的分流通道与冷却通道内的空气流量守恒方程和相互连通的汇流通道与冷却通道内的空气流量守恒方程;Step 2. The summation of the gas pressures in the confluence channel at the top of each row of lithium-ion batteries, the shunt channel at the bottom and the cooling channels on both sides to obtain the pressure sum, and the flow resistance network model is obtained by using the air flow conservation equation. The air flow conservation equation Including the air flow conservation equation in the interconnected shunt channel and the cooling channel and the air flow conservation equation in the interconnected confluence channel and the cooling channel; 根据锂离子电池阵列的总长度和总宽度、θ2、相邻的两列锂离子电池间的距离,得到每个分流通道的横截面积;根据该横截面积,得到每个分流通道的直径和相邻两个分流通道的流量比值;According to the total length and width of the lithium-ion battery array, θ 2 , and the distance between two adjacent rows of lithium-ion batteries, the cross-sectional area of each shunt channel is obtained; according to the cross-sectional area, the diameter of each shunt channel is obtained and the flow ratio of two adjacent shunt channels; 根据锂离子电池阵列的总长度和总宽度、相邻的两列锂离子电池间的距离和θ1,得到每个汇流通道的横截面积;根据该横截面积,得到每个汇流通道的直径和相邻两个汇流通道的流量比值;According to the total length and width of the lithium-ion battery array, the distance between two adjacent rows of lithium-ion batteries and θ 1 , the cross-sectional area of each bus channel is obtained; according to the cross-sectional area, the diameter of each bus channel is obtained and the flow ratio of two adjacent confluence channels; 根据锂离子电池阵列的总长度和总宽度、相邻的两列锂离子电池间的距离,得到每个冷却通道的横截面积;根据该横截面积,得到每个冷却通道的直径;According to the total length and width of the lithium-ion battery array and the distance between two adjacent rows of lithium-ion batteries, the cross-sectional area of each cooling channel is obtained; according to the cross-sectional area, the diameter of each cooling channel is obtained; 根据每个冷却通道的横截面积和每个分流通道的横截面积得到每个冷却通道与每个分流通道的流量比值;According to the cross-sectional area of each cooling channel and the cross-sectional area of each shunt channel, the flow ratio of each cooling channel and each shunt channel is obtained; 根据每个冷却通道的横截面积和每个汇流通道的横截面积得到每个冷却通道与每个汇流通道的流量比值;According to the cross-sectional area of each cooling channel and the cross-sectional area of each collecting channel, the flow ratio of each cooling channel and each collecting channel is obtained; 步骤三、根据流阻网络模型、每个分流通道的直径、相邻两个分流通道的流量比值、每个汇流通道的直径、相邻两个汇流通道的流量比值、每个冷却通道的直径、每个冷却通道与每个分流通道的流量比值、每个冷却通道与每个汇流通道的流量比值,得到每个冷却通道的风速。Step 3: According to the flow resistance network model, the diameter of each shunt channel, the flow ratio of two adjacent shunt channels, the diameter of each confluence channel, the flow ratio of two adjacent confluence channels, the diameter of each cooling channel, The flow ratio of each cooling channel and each split channel, and the flow ratio of each cooling channel and each confluence channel, to obtain the wind speed of each cooling channel. 2.根据权利要求1所述一种风冷式电池热管理系统冷却通道风速获得方法,其特征在于,步骤二中,得到压强和的具体过程为:2. A method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system according to claim 1, wherein in step 2, the specific process for obtaining the sum of pressures is: 根据伯努利方程,得到第i个分流通道的压强PDP,i和第i个汇流通道的压强PCP,i分别为:According to Bernoulli's equation, the pressure P DP,i of the ith branch channel and the pressure P CP,i of the ith confluence channel are obtained as:
Figure FDA0002248056540000021
Figure FDA0002248056540000021
Figure FDA0002248056540000022
Figure FDA0002248056540000022
式中,PDP,1为第1个分流通道的压强,ρair为空气密度,vDP,i为第i个分流通道的风速,i=1至n,n为锂离子电池的列数,ΔPloss,DP,k为第k个分流通道的总压强差,PCP,1PCP,i为第1个汇流通道的压强,vCP,i为第i个汇流通道的风速,vCP,1为第1个汇流通道的风速,ΔPloss,CP,k为第k个汇流通道的总压强差;In the formula, P DP,1 is the pressure of the first shunt channel, ρ air is the air density, v DP,i is the wind speed of the ith shunt channel, i=1 to n, n is the number of columns of lithium-ion batteries, ΔP loss,DP,k is the total pressure difference of the k-th shunt channel, P CP,1 P CP,i is the pressure of the first confluence channel, v CP,i is the wind speed of the i-th confluence channel, v CP, 1 is the wind speed of the first confluence channel, ΔP loss, CP,k is the total pressure difference of the k-th confluence channel; 风从第i-1个分流通道依次流向第i个冷却通道和第i个汇流通道,第i-1个分流通道、第i个冷却通道和第i个汇流通道的压强关系为:The wind flows from the i-1th split channel to the i-th cooling channel and the i-th confluence channel in turn. The pressure relationship between the i-1th split channel, the i-th cooling channel and the i-th confluence channel is:
Figure FDA0002248056540000023
Figure FDA0002248056540000023
式中,ΔPloss,CC,i为第i个冷却通道的总压强差,vDP,i-1为第i-1个分流通道的风速,vDP,0为Z型风冷式电池热管理系统进风口的风速;In the formula, ΔP loss,CC,i is the total pressure difference of the ith cooling channel, vDP,i-1 is the wind speed of the ith-1th shunt channel, and vDP,0 is the thermal management of the Z-type air-cooled battery The wind speed at the air inlet of the system; 根据公式1至公式3,得到每列锂离子电池顶部汇流通道、底部分流通道和两侧冷却通道内的气体压强构成的压强和:According to Equation 1 to Equation 3, the sum of the pressures formed by the gas pressures in the top bus channel, bottom shunt channel and cooling channels on both sides of each column of lithium-ion batteries is obtained: ΔPloss,DP,i+ΔPloss,CC,i+1-ΔPloss,CP,i-ΔPloss,CC,i=0 公式4,ΔP loss,DP,i +ΔP loss,CC,i+1 -ΔP loss,CP,i -ΔP loss,CC,i =0 Equation 4, 式中,ΔPloss,DP,i为第i个分流通道的总压强差,ΔPloss,CC,i+1为第i+1个冷却通道的总压强差,ΔPloss,CP,i为第i个汇流通道的总压强差。In the formula, ΔP loss,DP,i is the total pressure difference of the ith shunt channel, ΔP l oss,CC ,i+1 is the total pressure difference of the i+1th cooling channel, ΔP loss,CP,i is the ith The total pressure difference of the i bus channels.
3.根据权利要求2所述一种风冷式电池热管理系统冷却通道风速获得方法,其特征在于,第i个分流通道的总压强差ΔPloss,DP,i、第i个冷却通道的总压强差ΔPloss,CC,i和第i个汇流通道的总压强差ΔPloss,CP,i均由相应通道的局部压差ΔPlocal和沿程压差ΔPfriction组成,公式表示为:3. The method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system according to claim 2, wherein the total pressure difference ΔP loss,DP,i of the i-th shunt channel and the total pressure of the i-th cooling channel The pressure difference ΔP loss,CC,i and the total pressure difference ΔP loss,CP,i of the ith confluence channel are both composed of the local pressure difference ΔP local and the pressure difference ΔP friction along the path of the corresponding channel, and the formula is expressed as: ΔPloss=ΔPlocal+ΔPfriction 公式5,ΔP loss = ΔP local + ΔP friction Formula 5, 式中,
Figure FDA0002248056540000031
In the formula,
Figure FDA0002248056540000031
Figure FDA0002248056540000032
Figure FDA0002248056540000032
Figure FDA0002248056540000033
Figure FDA0002248056540000033
Figure FDA0002248056540000035
Figure FDA0002248056540000035
Figure FDA0002248056540000036
Figure FDA0002248056540000036
λDP,i为第i个分流通道的无量纲摩擦常数,λCP,i为第i个汇流通道的无量纲摩擦常数,λCC,i为第i个冷却通道的无量纲摩擦常数,lDP,i为第i个分流通道的长度,lCP,i第i个汇流通道的长度,lCC,i为第i个冷却通道的长度,DDP,i为第i个分流通道横截面积等效为圆形分流通道面积后的圆形分流通道的直径,DCP,i为第i个汇流通道横截面积等效为圆形汇流通道面积后的圆形汇流通道的直径,DCC,i为第i个冷却通道横截面积等效为圆形冷却通道面积后的圆形冷却通道的直径,ζDP,i为第i个分流通道与第i-1个分流通道的局部压差系数,ζCP,i为第i个汇流通道与第i-1个汇流通道的局部压差系数,ζDP,0→CC,1为Z型风冷式电池热管理系统进风口与第1个冷却通道间的局部压差系数,ζDP,i-1→CC,i为第i-1个分流通道与第i个冷却通道间的局部压差系数,ζCC,i→CP,i为第i个冷却通道与第i个汇流通道间的局部压差系数,vDP,i-1为第i-1个分流通道的风速,vDP,0为Z型风冷式电池热管理系统进风口的风速,vCP,i为第i个汇流通道的风速,vDP,i为第i个分流通道的风速,vCC,i为第i个冷却通道的风速。λ DP,i is the dimensionless friction constant of the ith shunt channel, λ CP,i is the dimensionless friction constant of the ith confluence channel, λ CC,i is the dimensionless friction constant of the ith cooling channel, l DP ,i is the length of the i-th shunt channel, l CP,i is the length of the ith-th confluence channel, l CC,i is the length of the ith-th cooling channel, D DP,i is the cross-sectional area of the ith-th shunt channel, etc. Efficiency is the diameter of the circular shunt channel after the area of the circular shunt channel, D CP,i is the diameter of the circular shunt channel after the cross-sectional area of the i-th shunt channel is equivalent to the area of the circular shunt channel, D CC,i is the diameter of the circular cooling channel after the cross-sectional area of the ith cooling channel is equivalent to the area of the circular cooling channel, ζ DP,i is the local pressure difference coefficient between the ith branch channel and the i-1th branch channel, ζ CP,i is the local pressure difference coefficient between the ith bus channel and the i-1th bus channel, ζ DP,0→CC,1 is the air inlet of the Z-type air-cooled battery thermal management system and the first cooling channel The local pressure difference coefficient between , ζ DP,i-1→CC,i is the local pressure difference coefficient between the i-1th branch channel and the ith cooling channel, ζ CC,i→CP,i is the ith The coefficient of local pressure difference between the cooling channel and the i-th confluence channel, v DP,i-1 is the wind speed of the i-1th branch channel, v DP,0 is the wind speed of the air inlet of the Z-type air-cooled battery thermal management system , v CP,i is the wind speed of the i-th confluence channel, v DP,i is the wind speed of the i-th split channel, and v CC,i is the wind speed of the i-th cooling channel.
4.根据权利要求3所述一种风冷式电池热管理系统冷却通道风速获得方法,其特征在于,第i个分流通道与第i-1个分流通道的局部压差系数ζDP,i表示为:4. The method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system according to claim 3, wherein the local pressure difference coefficient ζ DP of the i-th split channel and the i-1th split channel is represented by for: 式中,pDP,i为第i个分流通道与第i-1个分流通道的流量比值;In the formula, p DP,i is the flow ratio of the i-th shunt channel to the i-1 th shunt channel; 第i-1个分流通道与第i个冷却通道间的局部压差系数ζDP,i-1→CC,i表示为:The local pressure difference coefficient ζ DP,i-1→CC,i between the i-1th shunt channel and the i-th cooling channel is expressed as:
Figure FDA0002248056540000042
Figure FDA0002248056540000042
式中,pDP,i-1→CC,i为第i-1个冷却通道与第i个分流通道流量的比值,ψDP,i-1→CC,i为第i-1个分流通道与第i个冷却通道横截面积的比值,pDP,0→CC,1为Z型风冷式电池热管理系统进风口与第1个分流通道流量的比值,ψDP,0→CC,1为Z型风冷式电池热管理系统进风口与第1个冷却通道横截面积的比值;In the formula, p DP,i-1→CC,i is the ratio of the flow rate of the i-1th cooling channel to the i-th split channel, ψ DP,i-1→CC,i is the i-1th split channel and The ratio of the cross-sectional area of the i-th cooling channel, p DP,0→CC,1 is the ratio of the air inlet of the Z-type air-cooled battery thermal management system to the flow rate of the first shunt channel, ψ DP,0→CC,1 is The ratio of the air inlet of the Z-type air-cooled battery thermal management system to the cross-sectional area of the first cooling channel; 第i个汇流通道与第i-1个汇流通道的局部压差系数ζCP,i表示为:The local pressure difference coefficient ζ CP,i of the ith confluence channel and the i-1 th confluence channel is expressed as: ζCP,i=1-p2 CP,i 公式8,ζ CP,i =1-p 2 CP,i Formula 8, 式中,pCP,i为第i个汇流通道与第i-1个汇流通道的流量比值;In the formula, p CP,i is the flow ratio between the ith confluence channel and the i-1 th confluence channel; 第i个冷却通道与第i个汇流通道间的局部压差系数ζCC,i→CP,i表示为:The local pressure difference coefficient ζ CC,i→CP,i between the ith cooling channel and the ith confluence channel is expressed as: ζCC,i→CP,i=p2 CC,i→CP,iψ2 CC,i→CP,i-2p2 CC,i→CP,i-1 公式9,ζ CC,i→CP,i =p 2 CC,i→CP,i ψ 2 CC,i→CP,i −2p 2 CC,i→CP,i −1 Equation 9, 式中,p2 CC,i→CP,i为第i个冷却通道与第i个汇流通道流量的比值,ψCC,i→CP,i为第i个汇流通道与第i个冷却通道横截面积的比值。In the formula, p 2 CC,i→CP,i is the ratio of the flow of the ith cooling channel to the ith confluence channel, ψ CC,i→CP,i is the cross section of the ith confluence channel and the ith cooling channel area ratio.
5.根据权利要求3所述一种风冷式电池热管理系统冷却通道风速获得方法,其特征在于,第i个分流通道的无量纲摩擦常数λDP,i、第i个汇流通道的无量纲摩擦常数λCP,i和第i个冷却通道的无量纲摩擦常数λCC,i均表示为:5. The method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system according to claim 3, wherein the dimensionless friction constant λ DP,i of the i-th shunt channel and the dimensionless of the i-th confluence channel The friction constant λ CP,i and the dimensionless friction constant λ CC,i of the ith cooling channel are both expressed as:
Figure FDA0002248056540000043
Figure FDA0002248056540000043
式中,Re是局部雷诺数,Re=ρDU/μ,D为每个通道的直径,μ为空气的动力粘度,F为形状修正因子。where Re is the local Reynolds number, Re = ρDU/μ, D is the diameter of each channel, μ is the dynamic viscosity of air, and F is the shape correction factor.
6.根据权利要求3所述一种风冷式电池热管理系统冷却通道风速获得方法,其特征在于,根据公式11,得到相互连通的分流通道与冷却通道内的空气流量守恒方程为:6. The method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system according to claim 3, wherein, according to formula 11, the air flow conservation equation in the interconnected shunt channel and the cooling channel is obtained as: vDP,iADP,i=vDP,i+1ADP,i+1+vCC,i+1ACC,i+1 公式11,v DP,i A DP,i =v DP,i+1 A DP,i+1 +v CC,i+1 A CC,i+1 Equation 11, 式中,Q0=vDP,1ADP,1,Q0为进风口空气的流量,ADP,i为第i个分流通道的截面积,ADP,i+1为第i+1个分流通道的截面积,vCC,i+1为第i+1个冷却通道的风速,vDP,i+1为第i+1个分流通道的风速,In the formula, Q 0 =v DP,1 A DP,1 , Q 0 is the air flow at the air inlet, A DP,i is the cross-sectional area of the i-th shunt channel, A DP,i+1 is the i+1-th channel The cross-sectional area of the split channel, v CC,i+1 is the wind speed of the i+1th cooling channel, v DP,i+1 is the wind speed of the i+1th split channel, 根据公式12,得到相互连通的汇流通道与冷却通道内的空气流量守恒方程为:According to Equation 12, the air flow conservation equation in the interconnected confluence channel and cooling channel is obtained as: vCP,iACP,i=vCP,i-1ACP,i-1+vCC,iACC,i 公式12,v CP,i A CP,i =v CP,i-1 A CP,i-1 +v CC,i A CC,i Equation 12, 式中,ACP,i为第i个汇流通道的截面积,ACP,i-1为第i-1个汇流通道的截面积,ACC,i为第i个冷却通道的截面积,ACP,i-1为第i-1个冷却通道的截面积,vCP,0=0,ACP,0=0。In the formula, A CP,i is the cross-sectional area of the ith confluence channel, A CP,i-1 is the cross-sectional area of the i-1 th confluence channel, A CC,i is the cross-sectional area of the ith cooling channel, A CP,i-1 is the cross-sectional area of the i-1th cooling channel, v CP,0 =0, A CP,0 =0. 7.根据权利要求1所述一种风冷式电池热管理系统冷却通道风速获得方法,其特征在于,步骤三中,锂离子电池阵列的总长度Wx表示为:7. The method for obtaining the wind speed of the cooling channel of an air-cooled battery thermal management system according to claim 1, wherein in step 3, the total length W x of the lithium-ion battery array is expressed as:
Figure FDA0002248056540000051
Figure FDA0002248056540000051
式中,N为锂离子电池的列数,lx为每列锂离子电池中的每个锂离子电池单体的长,di为相邻的两列锂离子电池间的距离;In the formula, N is the number of columns of lithium-ion batteries, lx is the length of each lithium-ion battery cell in each column of lithium-ion batteries, and d i is the distance between two adjacent columns of lithium-ion batteries; 锂离子电池阵列的总长度的总宽度Wy表示为:The total width W y of the total length of the lithium-ion battery array is expressed as: Wy=M×ly+(M+1)×dy 公式14,W y =M× ly +(M+1)× dy Equation 14, 式中,M为每列锂离子电池中锂离子电池单体的数量,ly为每个锂离子电池单体的宽,dy为相邻的两列锂离子电池间的距离。In the formula, M is the number of lithium-ion battery cells in each column of lithium-ion batteries, ly is the width of each lithium-ion battery cell, and dy is the distance between two adjacent columns of lithium-ion batteries.
8.根据权利要求7所述一种风冷式电池热管理系统冷却通道风速获得方法,其特征在于,步骤二中,每个分流通道的横截面积获得过程为:8. The method for obtaining the wind speed of the cooling channel of an air-cooled battery thermal management system according to claim 7, wherein in step 2, the process of obtaining the cross-sectional area of each shunt channel is: 进风口导流板与Z型风冷式电池热管理系统底面之间的角度θ1表示为:The angle θ1 between the air inlet deflector and the bottom surface of the Z-type air-cooled battery thermal management system is expressed as: 式中,w1为进风口导流板的角度调整参数;In the formula, w 1 is the angle adjustment parameter of the air inlet deflector; 将公式15带入公式16中,得到分流通道的横截面积ADP,i为:Bringing Equation 15 into Equation 16, the cross-sectional area A DP,i of the shunt channel is obtained as:
Figure FDA0002248056540000061
Figure FDA0002248056540000061
每个汇流通道的横截面积获得过程为:The process of obtaining the cross-sectional area of each bus channel is: 出风口导流板与Z型风冷式电池热管理系统顶面之间的角度θ2表示为:The angle θ2 between the air outlet baffle and the top surface of the Z-type air - cooled battery thermal management system is expressed as:
Figure FDA0002248056540000062
Figure FDA0002248056540000062
式中,w2为汇流通道角度调整参数;In the formula, w 2 is the adjustment parameter of the angle of the confluence channel; 汇流通道的横截面积ACP,i表示为:The cross-sectional area A CP,i of the bus channel is expressed as:
Figure FDA0002248056540000063
Figure FDA0002248056540000063
冷却通道的横截面积ACC,i表示为:The cross-sectional area A CC,i of the cooling channel is expressed as: ACC,i=Wy·di 公式19。A CC,i =W y ·d i Formula 19.
9.根据权利要求8所述一种风冷式电池热管理系统冷却通道风速获得方法,其特征在于,将第i个分流通道横截面积ADP,i等效为圆形分流通道的面积,等效后的圆形分流通道的直径DDP,i表示为:9. The method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system according to claim 8, wherein the cross-sectional area A DP,i of the i-th shunt channel is equivalent to the area of a circular shunt channel, The diameter D DP,i of the equivalent circular shunt channel is expressed as:
Figure FDA0002248056540000064
Figure FDA0002248056540000064
将第i个汇流通道的横截面积ACP,i等效为圆形分流通道的面积,等效后的圆形分流通道的直径DCP,i表示为:The cross-sectional area A CP,i of the ith confluence channel is equivalent to the area of the circular shunt channel, and the diameter D CP,i of the equivalent circular shunt channel is expressed as:
Figure FDA0002248056540000065
Figure FDA0002248056540000065
将第i个冷却通道的横截面积ACC,i等效为圆形分流通道的面积,等效后的圆形分流通道的直径DCC,i表示为:The cross-sectional area A CC,i of the i-th cooling channel is equivalent to the area of the circular shunt channel, and the diameter D CC,i of the equivalent circular shunt channel is expressed as:
10.根据权利要求9所述一种风冷式电池热管理系统冷却通道风速获得方法,其特征在于,根据每个冷却通道的横截面积和每个分流通道的横截面积得到每个冷却通道与每个分流通道的流量比值pDP,i-1→CC,i10 . The method for obtaining the wind speed of a cooling channel of an air-cooled battery thermal management system according to claim 9 , wherein each cooling channel is obtained according to the cross-sectional area of each cooling channel and the cross-sectional area of each branch channel. 11 . With the flow ratio p DP,i-1→CC,i of each branch channel: 第i个冷却通道与第i-1个分流通道流量的比值表示为:The ratio of the flow rate of the i-th cooling channel to the i-1-th split channel flow is expressed as:
Figure FDA0002248056540000071
Figure FDA0002248056540000071
式中,pDP,i-1→CC,i为第i个冷却通道与第i-1个分流通道流量的比值;In the formula, p DP,i-1→CC,i is the ratio of the flow rate of the i-th cooling channel to the i-1th split channel; 根据每个冷却通道的横截面积和每个汇流通道的横截面积得到每个冷却通道与每个汇流通道的流量比值pCC,i→CP,iAccording to the cross-sectional area of each cooling channel and the cross-sectional area of each collecting channel, the flow ratio p CC,i→CP,i of each cooling channel and each collecting channel is obtained:
Figure FDA0002248056540000072
Figure FDA0002248056540000072
式中,pCC,i→CP,i为第i个冷却通道与第i个汇流通道流量的比值;In the formula, p CC,i→CP,i is the ratio of the flow rate of the ith cooling channel to the ith confluence channel; 第i个分流通道与第i-1个分流通道的流量比值pDP,i表示为:The flow ratio p DP,i of the ith branch channel and the i-1th branch channel is expressed as:
Figure FDA0002248056540000073
Figure FDA0002248056540000073
式中,当i=1时,ADP,0表示进风口的横截面积。In the formula, when i=1, A DP,0 represents the cross-sectional area of the air inlet. 第i个汇流通道与第i-1个汇流通道的流量比值pCP,i表示为:The flow ratio p CP,i of the ith confluence channel and the i-1 th confluence channel is expressed as:
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