CN109033619A - A kind of transient temperature model modelling approach of 18650 type lithium battery discharge cycles - Google Patents

A kind of transient temperature model modelling approach of 18650 type lithium battery discharge cycles Download PDF

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CN109033619A
CN109033619A CN201810816701.0A CN201810816701A CN109033619A CN 109033619 A CN109033619 A CN 109033619A CN 201810816701 A CN201810816701 A CN 201810816701A CN 109033619 A CN109033619 A CN 109033619A
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汪秋婷
戚伟
肖铎
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Hangzhou City University
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Abstract

The present invention relates to a kind of transient temperature model modelling approach of 18650 type lithium battery discharge cycles, comprising steps of 1) the foundation rule of lithium battery monomer discharge cycles thermal model;2) governing equation of transient state thermal behavior is established;3) boundary condition of transient state thermal behavior is established.The beneficial effects of the present invention are: the present invention is based on the pseudo- two dimensional models of Newman to establish transient temperature model of the lithium battery monomer under different discharge-rate operating conditions, designed, designed constant current charge-discharge experimental provision, acquisition calculates and emulates single battery thermal behavior data, and transient temperature parameter and voltage distribution curves are subjected to interpretation of result, transient temperature model proposed by the present invention has good reliability and validity;New model and new algorithm calculating speed proposed by the present invention is fast simultaneously, and computational solution precision is higher.

Description

一种18650型锂电池放电循环的瞬态温度模型建模方法A transient temperature model modeling method for 18650 type lithium battery discharge cycle

技术领域technical field

本发明涉及一种18650型锂电池放电循环工况下的瞬态温度模型和电压分布模拟曲线,更具体地说,它涉及一种恒流放电工况下的锂电池瞬态温度模型建立,以及温度与放电电压之间的函数关系曲线。The present invention relates to a transient temperature model and a voltage distribution simulation curve of a 18650 lithium battery discharge cycle working condition, more specifically, it relates to the establishment of a lithium battery transient temperature model under a constant current discharge working condition, and The function relationship curve between temperature and discharge voltage.

背景技术Background technique

锂电池因能量密度高、寿命长、自放电率低等优点受到了行业的青睐,目前占据着动力电池的主要市场。锂电池也有较大的局限性,主要是需要在适宜的环境温度下工作,温度过高或过低都会对其性能、循环寿命以及安全性产生较大影响。国内外众多学者致力于锂电池温度模型的研究,提出不同的建模方法,如人工神经网络、有限元模型(FEM)或集总参数模型(LPM)、线性参数变化(LPV)模型或偏微分方程(PDE)模型、CFD模型。基于电化学方程的模型对电池内部物理和化学过程进行精确描述,在设计电池单体时电化学模型实用可靠。但是,该模型的计算时间较长,不适用于高动态的锂电池工作环境。Newman和Tie首次提出一种具有锂电池动态应用的多孔电极电化学建模方法。在多孔电极理论中,电极被视为电解质溶液与固体基质之间的叠加。基质本身被建模为微观的球形颗粒,其中锂离子扩散并在球体表面上反应。Full等将该方法进行推广,设计包括两个复合模型和分离器的温度模型,该模型同时适用于锂电池和MH-Ni电池。Lithium batteries are favored by the industry due to their advantages such as high energy density, long life, and low self-discharge rate, and currently occupy the main market for power batteries. Lithium batteries also have relatively large limitations, mainly because they need to work at a suitable ambient temperature. Too high or too low a temperature will have a great impact on its performance, cycle life and safety. Many scholars at home and abroad are committed to the research of lithium battery temperature model, and propose different modeling methods, such as artificial neural network, finite element model (FEM) or lumped parameter model (LPM), linear parameter variation (LPV) model or partial differential Equation (PDE) model, CFD model. The model based on electrochemical equations accurately describes the internal physical and chemical processes of the battery, and the electrochemical model is practical and reliable when designing battery cells. However, the calculation time of this model is long and it is not suitable for the highly dynamic lithium battery working environment. Newman and Tie proposed for the first time a method for electrochemical modeling of porous electrodes with dynamic applications in lithium batteries. In porous electrode theory, the electrode is considered as a superposition between the electrolyte solution and the solid matrix. The matrix itself is modeled as microscopic spherical particles in which lithium ions diffuse and react on the surface of the spheres. The method was promoted by Full et al., and the design included two composite models and a temperature model of the separator. This model is suitable for both lithium batteries and MH-Ni batteries.

根据锂电池充放电内部机制,电化学反应中的正极、负极和总反应公式为:According to the internal mechanism of lithium battery charge and discharge, the positive electrode, negative electrode and total reaction formula in the electrochemical reaction are:

正极 positive electrode

负极 negative electrode

总公式 total formula

发明内容Contents of the invention

本发明的目的是克服现有技术中的不足,提供一种18650型锂电池放电循环的瞬态温度模型建模方法。The purpose of the present invention is to overcome the deficiencies in the prior art, and provide a transient temperature model modeling method of a 18650 type lithium battery discharge cycle.

这种18650型锂电池放电循环的瞬态温度模型建模方法,包括如下步骤:The transient temperature model modeling method of this 18650 type lithium battery discharge cycle includes the following steps:

步骤1):锂电池单体放电循环热模型的建立规则;将基于物理特征的二维电化学模型与反映锂电池性能的电荷守恒和热扩散方程相结合,从而计算温度分布值;Step 1): The rules for establishing the thermal model of the lithium battery cell discharge cycle; the two-dimensional electrochemical model based on physical characteristics is combined with the charge conservation and thermal diffusion equations reflecting the performance of lithium batteries to calculate the temperature distribution value;

步骤2):建立瞬态热行为的控制方程;方程描述固相电荷守恒、电解质相电荷守恒、固相锂离子守恒、电解质相锂离子守恒;Step 2): establish the governing equation of transient thermal behavior; the equation describes the conservation of charge in the solid phase, the conservation of charge in the electrolyte phase, the conservation of lithium ions in the solid phase, and the conservation of lithium ions in the electrolyte phase;

步骤2-1):建立固相电荷守恒方程如下:Step 2-1): Establish the solid-phase charge conservation equation as follows:

▽(ρeff▽φs)-iLi=0 (4)▽(ρ eff ▽φ s )-i Li =0 (4)

另一种表示方式为:Another representation is:

AndAnd

AndAnd

其中,ρeff为固相有效电导率,ρ+和ρ-分别为正负极的有效电导率,φ+和φ-分别为相电势正负极,ln为负极长度,ls为分离器长度,lp为正极长度,L=ln+ls+lp为总长度;Among them, ρ eff is the effective conductivity of the solid phase, ρ + and ρ - are the effective conductivity of the positive and negative electrodes respectively, φ + and φ - are the phase potential positive and negative electrodes respectively, l n is the length of the negative electrode, and l s is the separator Length, l p is the length of the positive pole, L=l n +l s +l p is the total length;

步骤2-2):建立电解质相电荷守恒方程如下:Step 2-2): Establish the electrolyte phase charge conservation equation as follows:

AndAnd

其中,κeff为有效扩散电导率,满足β为Burggeman孔隙度指数;为有效离子电导率,计算公式为:where κ eff is the effective diffusion conductivity, which satisfies β is the Burggeman porosity index; For the effective ionic conductivity, the calculation formula is:

其中,f±为电解质的分子活度系或电解质活度系数,ξe为电极中电解质相的体积分数,R为通用气体常数,F为法拉第常数,为锂离子转移数,Ce为电解液中的锂浓度;Among them, f ± is the molecular activity system or the electrolyte activity coefficient of the electrolyte, ξe is the volume fraction of the electrolyte phase in the electrode, R is the universal gas constant, F is the Faraday constant, Is the transfer number of lithium ions, and Ce is the lithium concentration in the electrolyte;

步骤2-3):建立固相锂离子守恒方程;活性固体材料中锂离子的物质平衡粒子在球面坐标系下方程为:Step 2-3): establish the solid-phase lithium ion conservation equation; the mass balance particle of lithium ion in the active solid material is in the spherical coordinate system and the equation is:

结合边界条件如下,Combined with the boundary conditions as follows,

AndAnd

其中,Cs为锂离子在固相中的浓度,Ds为锂离子在电解质中的质量扩散系数,r为沿活性物质颗粒的径向坐标,Rs为固体活性物质颗粒的半径;设as为电流分配系数,锂离子在插入和脱嵌过程中分别表示为as,a和as,c,则电极/电解质界面上锂离子插入和脱嵌引起的转移电流iLi表示为:Among them, C s is the concentration of lithium ions in the solid phase, D s is the mass diffusion coefficient of lithium ions in the electrolyte, r is the radial coordinate along the active material particles, R s is the radius of the solid active material particles; let a s is the current distribution coefficient, and lithium ions are expressed as a s,a and a s,c during the insertion and deintercalation process, respectively, then the transfer current i Li caused by the insertion and deintercalation of lithium ions on the electrode/electrolyte interface is expressed as:

步骤2-4):建立电解液锂离子守恒方程:Step 2-4): Establish the electrolyte lithium ion conservation equation:

或者表示为:or expressed as:

其中,ξe为电解质的体积分数/孔隙率,为有效扩散系数,满足 为基于溶剂流速的锂离子转移速度;where ξe is the volume fraction/porosity of the electrolyte, is the effective diffusion coefficient, satisfying is the lithium ion transfer rate based on the solvent flow rate;

步骤3):建立瞬态热行为的边界条件;Step 3): Establish boundary conditions for transient thermal behavior;

步骤3-1):建立反应速率方程;将其转化为耦合电荷系的控制方程:Step 3-1): Establish the reaction rate equation; transform it into the governing equation of the coupled charge system:

其中,局部表面超电势表示为:where the local surface overpotential is expressed as:

η=φse-U (19)η=φ se -U (19)

交换电流密度表示为:The exchange current density is expressed as:

其中,i0为交换电流密度,αa和αc分别为阳极和阴极的传递系数,T为温度值,η为过电位,U为热力学OCV,Cs,max为固相锂的最大浓度,Cs,e为锂在固体颗粒表面的浓度,φs和φe分别为固相和电解质相的电势;Among them, i 0 is the exchange current density, α a and α c are the transfer coefficients of the anode and cathode, respectively, T is the temperature value, η is the overpotential, U is the thermodynamic OCV, C s,max is the maximum concentration of solid-phase lithium, C s,e is the concentration of lithium on the surface of solid particles, φ s and φ e are the potentials of the solid phase and the electrolyte phase, respectively;

将模型进行耦合,引入基于温度的物理化学参数,如电解质扩散系数Ds和锂离子导电性参数km,两个参数表示为:The model is coupled to introduce temperature-based physical and chemical parameters, such as the electrolyte diffusion coefficient D s and the lithium ion conductivity parameter k m , the two parameters are expressed as:

同时,电解质相扩散系数计算公式为:At the same time, the formula for calculating the phase diffusion coefficient of the electrolyte is:

其中,Ds为固相扩散系数,Ds.ref为参考固体扩散系数,km.ref为参考反应速率系数,De为电解质相的扩散系数,Ed为控制Ds温度敏感性的活化能,Er为控制km温度灵敏度的活化能,Tref为温度参考系数;where Ds is the solid-phase diffusion coefficient, Ds.ref is the reference solid diffusion coefficient, km.ref is the reference reaction rate coefficient, De is the diffusion coefficient of the electrolyte phase , Ed is the activation controlling the temperature sensitivity of Ds energy, E r is the activation energy controlling the temperature sensitivity of km, and T ref is the temperature reference coefficient;

步骤3-2):建立能量守恒公式:Step 3-2): Establish the energy conservation formula:

或者表示为:or expressed as:

上述公式进一步修改为:The above formula is further modified as:

其中,公式(26)和公式(27)中的各参数计算公式如下:Wherein, the calculation formulas of each parameter in formula (26) and formula (27) are as follows:

▽(ρ+φ+)=-i (28)▽(ρ +φ+ )=-i (28)

▽(ρ-φ-)=+i (29)▽(ρ -φ - )=+i (29)

其中,为电化学热,满足公式(31):in, is the electrochemical heat, which satisfies formula (31):

其中,ip为长度为lp范围内锂离子转移电流,满足公式 Among them, ip is the lithium ion transfer current within the range of length l p , which satisfies the formula

作为优选:所述步骤1)包括以下步骤:As preferably: described step 1) comprises the following steps:

步骤1-1):新模型给出控制方程和边界条件,并计算用于模型建立的材料特性参数;Step 1-1): The new model gives the governing equations and boundary conditions, and calculates the material characteristic parameters used for model establishment;

步骤1-2):新模型特征如下:利用基于物理特征的二维模型准确估计正极和负极的动态行为;考虑活性电极颗粒内部的材料相变状况;利用扫描电子显微镜得到电极内部的颗粒尺寸分布。Step 1-2): The features of the new model are as follows: use a two-dimensional model based on physical characteristics to accurately estimate the dynamic behavior of the positive and negative electrodes; consider the material phase transition inside the active electrode particles; use the scanning electron microscope to obtain the particle size distribution inside the electrode .

本发明的有益效果是:本发明基于Newman的伪二维模型(P2D)建立锂电池单体在不同放电倍率工况下的瞬态温度模型,自行设计恒流充放电实验装置,采集、计算和仿真单体电池热行为数据,并将瞬态温度参数与电压分布曲线进行结果分析,本发明提出的瞬态温度模型具有很好的可靠性和有效性。同时本发明提出的新模型和新算法计算速度快,计算结果精度较高。The beneficial effect of the present invention is: the present invention is based on Newman's pseudo-two-dimensional model (P2D) and establishes the transient temperature model of lithium battery monomer under different discharge rate working conditions, designs constant current charging and discharging experiment device by oneself, collects, calculates and By simulating the thermal behavior data of a single battery, and analyzing the results of the transient temperature parameters and the voltage distribution curve, the transient temperature model proposed by the present invention has good reliability and effectiveness. Simultaneously, the new model and the new algorithm proposed by the invention have fast calculation speed and high calculation result precision.

附图说明Description of drawings

图1为18650型锂电池实验测试装置结构框图;Figure 1 is a structural block diagram of the 18650 lithium battery experimental test device;

图2为1C放电倍率下实验温度和模拟温度的比较结果图;Figure 2 is a comparison result diagram of the experimental temperature and the simulated temperature at a discharge rate of 1C;

图3为4C放电倍率下实验温度和模拟温度的比较结果图;Fig. 3 is the comparison result figure of experimental temperature and simulated temperature under 4C discharge rate;

图4为1C放电倍率下实验电压和模拟电压的比较结果图;Fig. 4 is the comparison result diagram of experimental voltage and simulated voltage under 1C discharge rate;

图5为4C放电倍率下实验电压和模拟电压的比较结果图。Fig. 5 is a comparison result graph of the experimental voltage and the simulated voltage at a discharge rate of 4C.

具体实施方式Detailed ways

下面结合实施例对本发明做进一步描述。下述实施例的说明只是用于帮助理解本发明。应当指出,对于本技术领域的普通技术人员来说,在不脱离本发明原理的前提下,还可以对本发明进行若干改进和修饰,这些改进和修饰也落入本发明权利要求的保护范围内。The present invention will be further described below in conjunction with the examples. The description of the following examples is provided only to aid the understanding of the present invention. It should be pointed out that for those skilled in the art, without departing from the principle of the present invention, some improvements and modifications can be made to the present invention, and these improvements and modifications also fall within the protection scope of the claims of the present invention.

所述的18650型锂电池放电循环的瞬态温度模型建模方法,包括以下步骤:The transient temperature model modeling method of described 18650 type lithium battery discharge cycle, comprises the following steps:

步骤1):锂电池单体放电循环热模型的建立规则。将基于物理特征的二维电化学模型与反映锂电池性能的电荷守恒和热扩散方程相结合,从而计算温度分布值。Step 1): Establishment rules for the thermal model of the lithium battery cell discharge cycle. A two-dimensional electrochemical model based on physical characteristics is combined with the charge conservation and thermal diffusion equations reflecting the lithium battery performance to calculate the temperature distribution value.

步骤1-1):新模型给出控制方程和边界条件,并计算用于模型建立的材料特性参数。Step 1-1): The new model gives the governing equations and boundary conditions, and calculates the material property parameters for model building.

步骤1-2):新模型特征如下:利用基于物理特征的二维模型准确估计正极和负极的动态行为;考虑活性电极颗粒内部的材料相变状况;利用扫描电子显微镜(SEM)得到电极内部的颗粒尺寸分布。Step 1-2): The features of the new model are as follows: use a two-dimensional model based on physical characteristics to accurately estimate the dynamic behavior of the positive and negative electrodes; consider the phase transition of the material inside the active electrode particles; use a scanning electron microscope (SEM) to obtain the internal state of the electrode. Particle size distribution.

步骤2):建立瞬态热行为的控制方程。方程描述固相电荷守恒、电解质相电荷守恒、固相锂离子守恒、电解质相锂离子守恒。Step 2): Establish the governing equations for the transient thermal behavior. The equations describe the conservation of charge in the solid phase, the conservation of charge in the electrolyte phase, the conservation of lithium ions in the solid phase, and the conservation of lithium ions in the electrolyte phase.

步骤2-1):建立固相电荷守恒方程。基于欧姆法则建立固相电荷守恒方程如下:Step 2-1): Establish solid phase charge conservation equation. Based on Ohm's law, the solid-phase charge conservation equation is established as follows:

▽(ρeff▽φs)-iLi=0 (4)▽(ρ eff ▽φ s )-i Li =0 (4)

另一种表示方式为:Another representation is:

AndAnd

AndAnd

其中,ρeff为固相有效电导率,ρ+和ρ-分别为正负极的有效电导率,φ+和φ-分别为相电势正负极,ln为负极长度,ls为分离器长度,lp为正极长度。L=ln+ls+lp为总长度。Among them, ρ eff is the effective conductivity of the solid phase, ρ + and ρ - are the effective conductivity of the positive and negative electrodes respectively, φ + and φ - are the phase potential positive and negative electrodes respectively, l n is the length of the negative electrode, and l s is the separator length, l p is the length of the positive electrode. L=l n +l s +l p is the total length.

步骤2-2):建立电解质相电荷守恒方程如下:Step 2-2): Establish the electrolyte phase charge conservation equation as follows:

AndAnd

其中,κeff为有效扩散电导率,满足β为Burggeman孔隙度指数。为有效离子电导率,计算公式为:where κ eff is the effective diffusion conductivity, which satisfies β is the Burggeman porosity index. For the effective ionic conductivity, the calculation formula is:

其中,f±为电解质的分子活度系或电解质活度系数,ξe为电极中电解质相的体积分数,R为通用气体常数,取值8.3143kJ/kg.摩尔.K,F为法拉第常数,取值96485Columb/mole,为锂离子转移数,Ce为电解液中的锂浓度。Among them, f ± is the molecular activity system of the electrolyte or the electrolyte activity coefficient, ξ e is the volume fraction of the electrolyte phase in the electrode, R is the universal gas constant, the value is 8.3143kJ/kg.mol.K, F is the Faraday constant, The value is 96485Columb/mole, is the transfer number of lithium ions, and Ce is the lithium concentration in the electrolyte.

步骤2-3):建立固相锂离子守恒方程。根据Fick第二定律,活性固体材料中锂离子的物质平衡粒子在球面坐标系下方程为:Step 2-3): establishing a solid-phase lithium ion conservation equation. According to Fick's second law, the mass balance particles of lithium ions in active solid materials have the following equation in the spherical coordinate system:

结合边界条件如下,Combined with the boundary conditions as follows,

AndAnd

其中,Cs为锂离子在固相中的浓度,Ds为锂离子在电解质中的质量扩散系数,r为沿活性物质颗粒的径向坐标,Rs为固体活性物质颗粒的半径。假设as为电流分配系数,锂离子在插入和脱嵌过程中分别表示为as,a和as,c,则电极/电解质界面上锂离子插入和脱嵌引起的转移电流iLi表示为:Among them, C s is the concentration of lithium ions in the solid phase, D s is the mass diffusion coefficient of lithium ions in the electrolyte, r is the radial coordinate along the active material particle, and R s is the radius of the solid active material particle. Assuming that a s is the current distribution coefficient, and lithium ions are denoted as a s,a and a s,c during the insertion and deintercalation process, respectively, the transfer current i Li caused by the insertion and deintercalation of lithium ions on the electrode/electrolyte interface is expressed as :

步骤2-4):建立电解液锂离子守恒方程:Step 2-4): Establish the electrolyte lithium ion conservation equation:

或者表示为:or expressed as:

其中,ξe为电解质的体积分数/孔隙率,为有效扩散系数,满足 为基于溶剂流速的锂离子转移速度。where ξe is the volume fraction/porosity of the electrolyte, is the effective diffusion coefficient, satisfying is the lithium ion transfer rate based on the solvent flow rate.

步骤3):建立瞬态热行为的边界条件。Step 3): Establish boundary conditions for transient thermal behavior.

步骤3-1):建立反应速率方程。电极表面电化学反应速率通常由Butler Volmer方程描述,本发明将其转化为耦合电荷系的控制方程:Step 3-1): Establish a reaction rate equation. The electrode surface electrochemical reaction rate is usually described by the Butler Volmer equation, which is transformed into the governing equation of the coupled charge system in the present invention:

其中,局部表面超电势表示为:where the local surface overpotential is expressed as:

η=φse-U (19)η=φ se -U (19)

交换电流密度表示为:The exchange current density is expressed as:

其中,i0为交换电流密度(电解质和固体活性材料中锂浓度的函数),αa和αc分别为阳极和阴极的传递系数,T为温度值(K),η为过电位(V),U为热力学OCV,Cs,max为固相锂的最大浓度,Cs,e为锂在固体颗粒表面的浓度,φs和φe分别为固相和电解质相的电势。where i0 is the exchange current density ( a function of the lithium concentration in the electrolyte and the solid active material), α and α are the transfer coefficients of the anode and cathode, respectively, T is the temperature value ( K ), and η is the overpotential (V) , U is the thermodynamic OCV, C s,max is the maximum concentration of lithium in the solid phase, C s,e is the concentration of lithium on the surface of solid particles, φ s and φ e are the potentials of the solid phase and the electrolyte phase, respectively.

将模型进行耦合,引入基于温度的物理化学参数,如电解质扩散系数Ds和锂离子导电性参数km(K),根据Arrhenius方程两个参数表示为:The model is coupled and temperature-based physicochemical parameters are introduced, such as the electrolyte diffusion coefficient D s and the lithium ion conductivity parameter k m (K). According to the Arrhenius equation, the two parameters are expressed as:

同时,电解质相扩散系数计算公式为,At the same time, the formula for calculating the phase diffusion coefficient of the electrolyte is,

其中,Ds为固相扩散系数,Ds.ref为参考固体扩散系数,km.ref为参考反应速率系数,De为电解质相的扩散系数,Ed为控制Ds温度敏感性的活化能,Er为控制km温度灵敏度的活化能,Tref为温度参考系数,取值为298K。where Ds is the solid-phase diffusion coefficient, Ds.ref is the reference solid diffusion coefficient, km.ref is the reference reaction rate coefficient, De is the diffusion coefficient of the electrolyte phase , Ed is the activation controlling the temperature sensitivity of Ds Energy, E r is the activation energy to control the temperature sensitivity of km, T ref is the temperature reference coefficient, the value is 298K .

步骤3-2):建立能量守恒公式:Step 3-2): Establish the energy conservation formula:

或者表示为:or expressed as:

上述公式进一步修改为:The above formula is further modified as:

其中,公式(26)和公式(27)中的各参数计算公式如下:Wherein, the calculation formulas of each parameter in formula (26) and formula (27) are as follows:

▽(ρ+φ+)=-i (28)▽(ρ +φ+ )=-i (28)

▽(ρ-φ-)=+i (29)▽(ρ -φ - )=+i (29)

其中,为电化学热,满足公式(31):in, is the electrochemical heat, which satisfies formula (31):

其中,ip为长度为lp范围内锂离子转移电流,满足公式 Among them, ip is the lithium ion transfer current within the range of length l p , which satisfies the formula

算法效果algorithm effect

本发明提出一种18650型锂电池单体放电循环工况下的瞬态温度模型和电压分布模拟曲线。在1C(小电流)和4C(大电流)放电倍率两种情况下,对电池单体的温度分布和电压分布进行仿真和实验研究,得出以下算法效果:The invention proposes a transient temperature model and a voltage distribution simulation curve under the single discharge cycle working condition of a 18650 type lithium battery. Under the two conditions of 1C (small current) and 4C (high current) discharge rate, the temperature distribution and voltage distribution of the battery cell are simulated and experimentally studied, and the following algorithm effects are obtained:

(1)随着放电倍率的增加,单体电池表面的温度分布值增大,靠近电极的热电偶测量值比中心线热电偶测量值大;(1) As the discharge rate increases, the temperature distribution on the surface of the single battery increases, and the measured value of the thermocouple near the electrode is larger than the measured value of the centerline thermocouple;

(2)锂电池单体内部产热现象,导致温度与放电时间的变化;(2) The internal heat generation phenomenon of lithium battery cells, resulting in changes in temperature and discharge time;

(3)新模型仿真得到的模拟温度值高于实验值,特别是高倍率放电工况,低倍率放电工况的模拟值更接近实验值;(3) The simulated temperature value obtained by the simulation of the new model is higher than the experimental value, especially the high-rate discharge condition, and the simulated value of the low-rate discharge condition is closer to the experimental value;

(4)4C放电倍率的模拟温度值为46.86℃,1C放电倍率的模拟值为29.6℃;(4) The simulated temperature value of 4C discharge rate is 46.86°C, and the simulated value of 1C discharge rate is 29.6°C;

(5)本发明建立的瞬态温度模型和电压分布模型的实验和仿真结果,实现锂电池的设计和热优化过程,并提供重要的物理化学模型基础。(5) The experimental and simulation results of the transient temperature model and the voltage distribution model established by the present invention realize the design and thermal optimization process of the lithium battery, and provide an important physical and chemical model basis.

如图1所示,选取18650型锂电池用于测量单体电池充放电电压、电流和温度参数,表1列出单体电池充放电实验放电倍率和充放电电流值。该装置主要由五部分组成:Arbin电池测试仪,国家仪器(NI)温度测量装置,带有热电偶的锂电池单元,计算机界面PC-1和PC-2。Arbin电池测试仪(BITRODE)最大电压为20V和最大电流为1200A。通过Visual C软件,PC-1控制单体电池装循环充放电过程,并记录充放电电压和电流数据,PC-2控制热数据采集。As shown in Figure 1, the 18650 lithium battery is selected to measure the charging and discharging voltage, current and temperature parameters of the single battery. Table 1 lists the discharge rate and the charging and discharging current value of the single battery charging and discharging experiment. The device mainly consists of five parts: Arbin battery tester, National Instruments (NI) temperature measuring device, lithium battery unit with thermocouple, computer interface PC-1 and PC-2. The Arbin battery tester (BITRODE) has a maximum voltage of 20V and a maximum current of 1200A. Through the Visual C software, PC-1 controls the charging and discharging process of the single battery cycle, and records the charging and discharging voltage and current data, and PC-2 controls the thermal data collection.

表1恒流放电实验参数设定Table 1 Constant current discharge experiment parameter settings

放电倍率Discharge rate 恒流电流值Constant current value 1C1C 1.5A1.5A 2C2C 3.0A3.0A 3C3C 4.5A4.5A 4C4C 6.0A6.0A

如图2和图3所示,为1C和4C放电倍率工况下实验温度和模拟温度分布之间的比较结果。放电实验的初始温度设定为22℃。As shown in Figure 2 and Figure 3, it is the comparison result between the experimental temperature and the simulated temperature distribution under the discharge rate conditions of 1C and 4C. The initial temperature of the discharge experiment was set at 22 °C.

(1)1C和4C放电倍率工况下,平均表面温度升高到29.25℃和42.16℃;(1) Under the discharge rate conditions of 1C and 4C, the average surface temperature rises to 29.25°C and 42.16°C;

(2)新算法仿真得到的模拟温度值高于实验值,特别是高倍率放电工况,4C放电倍率的模拟温度值为46.86℃,1C放电倍率的模拟值为29.6℃,更接近实验值;(2) The simulated temperature value obtained by the new algorithm simulation is higher than the experimental value, especially in the high-rate discharge condition. The simulated temperature value of the 4C discharge rate is 46.86°C, and the simulated value of the 1C discharge rate is 29.6°C, which is closer to the experimental value;

(3)放电倍率越高,表面温度增加越快,温度与放电时间的变化可能由于内部产热导致的。由此可知,本发明提出的新模型和新算法的优点为计算速度快,计算结果精度较高。(3) The higher the discharge rate, the faster the surface temperature increases, and the change of temperature and discharge time may be caused by internal heat generation. It can be seen that the advantages of the new model and new algorithm proposed by the present invention are fast calculation speed and high calculation result accuracy.

如图4和图5所示,为1C和4C放电倍率工况下实验电压和模拟电压分布曲线之间的比较结果。As shown in Figure 4 and Figure 5, it is the comparison result between the experimental voltage and the simulated voltage distribution curve under the discharge rate conditions of 1C and 4C.

(1)充放电实验为恒流电流,放电循环设置为1C充电、2小时静置、1C放电、2小时静置;(1) The charge and discharge experiment is a constant current, and the discharge cycle is set to charge at 1C, rest for 2 hours, discharge at 1C, and rest for 2 hours;

(2)电压值上下限设置在2.0V和3.6V之间;(2) The upper and lower limits of the voltage value are set between 2.0V and 3.6V;

(3)电压分布模型的模拟值和实验值之间具有较好的一致性。(3) There is good agreement between the simulated and experimental values of the voltage distribution model.

Claims (2)

1. A18650 type lithium battery discharge cycle transient temperature model modeling method is characterized by comprising the following steps:
step 1): establishing rules of a lithium battery monomer discharge cycle thermal model; combining a two-dimensional electrochemical model based on physical characteristics with a charge conservation and thermal diffusion equation reflecting the performance of the lithium battery, thereby calculating a temperature distribution value;
step 2): establishing a control equation of the transient thermal behavior; the equation describes the conservation of solid phase charge, the conservation of electrolyte phase charge, the conservation of solid phase lithium ions and the conservation of electrolyte phase lithium ions;
step 2-1): the solid phase charge conservation equation is established as follows:
▽(ρeff▽φs)-iLi=0 (4)
the other expression mode is as follows:
And
And
where ρ iseffIs the effective conductivity of the solid phase, p+And p-is the effective conductivity, phi, of the positive and negative electrodes, respectively+And phi-are positive and negative poles of phase potential, respectively, lnIs the length of the negative electrode, /)sFor the length of the separator, /)pFor positive electrode length, L ═ Ln+ls+lpThe total length is shown;
step 2-2): the electrolyte phase charge conservation equation was established as follows:
And
wherein, κeffFor effective diffusion of conductivity, satisfyβ is the Burrgeman porosity index;for effective ionic conductivity, the calculation formula is:
wherein f is±is the molecular activity system of the electrolyte or the activity coefficient of the electrolyte, ξeIs the volume fraction of the electrolyte phase in the electrode, R is the universal gas constant, F is the Faraday constant,is the number of lithium ion transfers, CeIs the lithium concentration in the electrolyte;
step 2-3): establishing a solid-phase lithium ion conservation equation; the equation of the material balance particle of lithium ion in the active solid material under a spherical coordinate system is as follows:
the binding boundary conditions are as follows,
And
wherein, CsConcentration of lithium ions in the solid phase, DsIs the mass diffusion coefficient of lithium ions in the electrolyte, R is the radial coordinate along the active material particle, RsRadius of the solid active substance particles; let asFor the current distribution coefficient, lithium ions are denoted as a during insertion and extraction, respectivelys,aAnd as,cTransfer current i caused by insertion and extraction of lithium ions at the electrode/electrolyte interfaceLiExpressed as:
step 2-4): establishing an electrolyte lithium ion conservation equation:
or as:
wherein ξeIs the volume fraction/porosity of the electrolyte,is an effective diffusion coefficient, satisfies Is the lithium ion transfer rate based on the solvent flow rate;
step 3): establishing boundary conditions of transient thermal behavior;
step 3-1): establishing a reaction rate equation; converting the charge into a control equation of a coupled charge system:
wherein the local surface overpotential is represented as:
η=φse-U (19)
the exchange current density is expressed as:
wherein i0to exchange the current density, αaand alphacthe transmission coefficients of the anode and the cathode are respectively, T is a temperature value, η is an overpotential, U is thermodynamic OCV, Cs,maxIs the maximum concentration of solid-phase lithium, Cs,eIs the concentration of lithium on the surface of the solid particlessAnd phiePotentials of the solid phase and the electrolyte phase, respectively;
coupling the model to introduce a temperature-based physicochemical parameter, such as the electrolyte diffusion coefficient DsAnd lithium ion conductivity parameter kmTwo parameters are expressed as:
meanwhile, the electrolyte phase diffusion coefficient calculation formula is as follows:
wherein D issIs the solid phase diffusion coefficient, Ds.refFor reference to the solid diffusion coefficient, km.refFor reference to the reaction rate coefficient, DeIs the diffusion coefficient of the electrolyte phase, EdTo control DsActivation energy of temperature sensitivity, ErTo control kmActivation energy of temperature sensitivity, TrefIs a temperature reference coefficient;
step 3-2): establishing an energy conservation formula:
or as:
the above formula is further modified as:
wherein, the calculation formula of each parameter in the formula (26) and the formula (27) is as follows:
wherein,satisfies formula (31) for electrochemical heating:
wherein ipIs of length lpThe lithium ion transfer current in the range satisfies the formulaAnd i ═ aip
2. The modeling method for the transient temperature model of 18650 lithium battery discharge cycle of claim 1, wherein step 1) comprises the steps of:
step 1-1): giving a control equation and boundary conditions by the new model, and calculating material characteristic parameters for establishing the model;
step 1-2): the new model features are as follows: accurately estimating the dynamic behaviors of the anode and the cathode by using a two-dimensional model based on physical characteristics; considering the phase change condition of the material inside the active electrode particles; the particle size distribution inside the electrode was obtained using a scanning electron microscope.
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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110457742A (en) * 2019-06-26 2019-11-15 北京航空航天大学 A lithium-ion battery electrochemical-thermo-mechanical coupling model and modeling method
CN111952685A (en) * 2019-05-15 2020-11-17 重庆金康新能源汽车有限公司 Continuous derating fast charging method based on multi-particle reduced-order model
CN112487735A (en) * 2020-12-02 2021-03-12 浙大城市学院 Power balance model algorithm for fluid lithium-oxygen battery
CN114398792A (en) * 2022-01-11 2022-04-26 浙江蓝盒子航空科技有限公司 Lithium ion battery pack thermal performance analysis method based on liquid-vapor cooling system
CN114757026A (en) * 2022-04-08 2022-07-15 昆明理工大学 Full-working-condition multi-scale power lithium battery electrochemical coupling modeling method

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6534954B1 (en) * 2002-01-10 2003-03-18 Compact Power Inc. Method and apparatus for a battery state of charge estimator
US20130119921A1 (en) * 2011-11-14 2013-05-16 Auburn University Rapid battery charging method and system
CN103941196A (en) * 2014-05-07 2014-07-23 吉林大学 Lithium ion battery state-of-charge estimation method
CN104991980A (en) * 2014-10-31 2015-10-21 吉林大学 Electrochemical mechanism modeling method for lithium-ion battery
CN107145628A (en) * 2017-03-31 2017-09-08 中南大学 The method of prediction lithium battery cycle life based on electrochemical heat coupling model

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6534954B1 (en) * 2002-01-10 2003-03-18 Compact Power Inc. Method and apparatus for a battery state of charge estimator
US20130119921A1 (en) * 2011-11-14 2013-05-16 Auburn University Rapid battery charging method and system
CN103941196A (en) * 2014-05-07 2014-07-23 吉林大学 Lithium ion battery state-of-charge estimation method
CN104991980A (en) * 2014-10-31 2015-10-21 吉林大学 Electrochemical mechanism modeling method for lithium-ion battery
CN107145628A (en) * 2017-03-31 2017-09-08 中南大学 The method of prediction lithium battery cycle life based on electrochemical heat coupling model

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
朱聪等: "方形锂离子电池组热模型", 《汽车工程》 *

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111952685A (en) * 2019-05-15 2020-11-17 重庆金康新能源汽车有限公司 Continuous derating fast charging method based on multi-particle reduced-order model
CN111952685B (en) * 2019-05-15 2021-11-26 重庆金康新能源汽车有限公司 Method and system for adjusting charging current based on modeled battery cells, and non-transitory computer-readable storage medium
CN110457742A (en) * 2019-06-26 2019-11-15 北京航空航天大学 A lithium-ion battery electrochemical-thermo-mechanical coupling model and modeling method
CN112487735A (en) * 2020-12-02 2021-03-12 浙大城市学院 Power balance model algorithm for fluid lithium-oxygen battery
CN112487735B (en) * 2020-12-02 2024-03-15 浙大城市学院 Power balance model method for fluid lithium-oxygen battery
CN114398792A (en) * 2022-01-11 2022-04-26 浙江蓝盒子航空科技有限公司 Lithium ion battery pack thermal performance analysis method based on liquid-vapor cooling system
CN114398792B (en) * 2022-01-11 2022-12-16 浙江蓝盒子航空科技有限公司 Lithium ion battery pack thermal performance analysis method based on liquid-vapor cooling system
CN114757026A (en) * 2022-04-08 2022-07-15 昆明理工大学 Full-working-condition multi-scale power lithium battery electrochemical coupling modeling method
CN114757026B (en) * 2022-04-08 2024-06-07 昆明理工大学 A multi-scale electrochemical coupling modeling method for power lithium batteries under full operating conditions

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