PEMFC阳极扩散层表面温度和热流密度联测

质子交换膜燃料电池内部温度及热流密度对电池性能和寿命等有重要影响。为实时监测电池内部的温度和热流密度,本文利用真空蒸发镀膜技术自制了薄膜传感器,并将传感器置于质子交换膜燃料电池阳极侧,同步在线测量了燃料电池在不同气体流量下温度及热流密度随电流密度变化规律。结果表明,燃料电池运行过程中,内部温度和热流密度随电流密度增大而升高,高电流密度工作时温升更明显。电流密度较小时,加热棒对电池内部温度影响显著。随着电流密度增加,电化学反应产热作为主要热源,对电池内部温度影响逐渐占据主导作用。     

质子交换膜燃料电池动态响应性能实验研究

本文实验研究了质子交换膜燃料电池负载变化时的动态性能,分析了氧气计量比流量和流场板结构的影响。结果表明,在本文的操作条件下,燃料电池动态响应能力的控制因素为质子交换膜水含量及液态水传递过程。随着氧气计量比流量的增加,电池性能及动态响应能力提高。采用不同流场板结构时,在输出电流较小的运行区间,平行流场板电池性能较好,随着平行流道数目减少,电池性能逐渐变差。     

流道结构和几何尺寸对燃料电池性能影响的实验研究

流场板是质子交换膜燃料电池重要部件之一。本文对以氢气和氧气作为反应气体的质子交换膜电池的极化曲线进行了实验测定,研究了不同流场板结构、流场板深度和宽度对电池性能的影响．研究发现采用组合流道的电池性能最佳．     

PEM燃料电池内液态水和温度分布特性

水和热的管理对PEM燃料电池的性能具有决定性的作用.本文建立了一个两相流模型,对PEM燃料电池换质子交换膜和阴极中的水分和温度进行了模拟,分析了燃料电池阴极中液态水和质子交换膜中水分,以及阴极催化剂层和质子交换膜中温度的分布状态.模拟结果显示:升高加湿温度,电池阴极中的液态水和质子交换膜中的含水量显著增加;沿着气体流动方向,燃料电池内的温度降低,水分含量升高;从质子交换膜阳极侧到阴极催化剂层中,温度先升高,达到最大值后,渐渐降低.     

质子交换膜燃料电流道淹没与传质强化

在地面常重力环境下,采用透明电池可视化方法研究了质子交换膜燃料电池阳极和阴极的流道淹没现象。分别研究了阳极和阴极反应物流量对电池内部传质和电池性能的影响。结果表明,电池阴极的淹没区域比阳极大,由电极淹没引起的气体传质受限和电化学反应受限主要发生在阴极。提高反应物流量能够强化气体传质并提高电池性能,并且提高电池阴极侧反应物流量比提高阳极侧反应物流量对提高电池性能更有效。本文工作为进一步开展微重力环境中的燃料电池实验提供了比较依据。     

质子交换膜燃料电池电流分布的动态响应

动态特性是理解质子交换膜燃料电池性能的重要参数之一.运用燃料电池测试系统、恒电流/恒电压多通道测试仪和燃料电池电流密度分布测试装置,试验测量了质子交换膜燃料电池在不同加湿温度、电池温度和压力下的电流分布动态响应和动态特性.研究发现:不同区域的局部电流达到新的平衡所需的时间不同;加湿温度变化时,不同区域的局部电流的变化趋...     

质子交换膜燃料电池短时微重力性能实验研究

利用落塔开展了不同重力情况下质子交换膜燃料电池性能的实验研究.对常重力和微重力条件下质子交换膜燃料电池发电时其阴极蛇形流场内部的两相流动开展了可视化现场观测.对重力因素对质子交换膜燃料电池内部传质过程的影响进行了分析和讨论.实验结果表明:在常重力环境中,液态水堆积在竖置流道的底部,无法有效排出.聚集在流道内的液态水与反应气体在流道内形成气/液两相流动.在微重力环境中,液态水在气体推动力的作用下从流道的底部上升并沿流道向出口流动.聚集在流道内的液态水排除后,减小了反应气体(氧气)从流道向催化层的传递阻力,从而使质子交换膜燃料电池的性能得到提高.     

质子交换膜燃料电池动态特性仿真

建立了质子交换膜燃料电池数学模型,并进行了仿真实现,计算分析了质子交换膜燃料电池典型动态特性和温度对其工作状况的影响.结果表明PEMFC内气体传质速度是影响电压响应时间的决定因素,扩散层内液态水的积累需要较长的时间,数量级在102～103,温度升高会降低PEMFC的动态响应时间并提高电池的输出功率,温度超过80°C后会降低电池的输出性能.     

直流道PEMFC两相流数学模型

建立直流道质子交换膜燃料电池(PEMFC)三维非等温两相流数学模型,基于质子交换膜与气体之间的水分传递特征,综合考虑电渗、浓度扩散及电化学反应作用的影响,发展了膜电极水分传递的非平衡扩散模型.并自主开发程序代码对电池内复杂的多物理场耦合传递过程进行数值模拟,研究PEMFC电极内气态水、液态水分布、质子膜含水量分布和水迁移特性等,分析单电池内部的温度分布特征,并获得电池极化性能曲线.     

不同流场下进气对质子交换膜燃料电池性能的影响

流场的结构对于质子交换膜燃料电池(PEMFC)的水管理和气体的传递具有十分重要的影响,相关研究一直是燃料电池的研究热点与重点。本文以纯氧气和空气作为阴极氧化剂,通过电池的性能测试、极化曲线和电化学阻抗分析等原位实验,分析了气体的流动与传输、不同流场下的电流密度、入口反应气体浓度等条件对电池性能的影响。实验结果表明,提高氧气浓度可以获得更好的质子交换膜燃料电池性能和最小化活化损失,纯氧气、波状流场的使用效果随进气量的变化而有明显的变化。     

Direct conversion of solid hydrocarbons in a molten carbonate fuel cell

Electrical characteristics of a molten carbonate fuel cell allowing direct electrochemical oxidation of dispersed hydrocarbons have been examined. As the fuel, graphite, anthracite, and cannel coal samples were used. Data illustrating the effect of electrolyte temperature, fuel type and dispersion, and also reactant gas mixture composition on the performance characteristics of the fuel cell, were obtained. Correlation between the specific characteristics of the fuel cell and the hydrogen content of fuel material was established. The maximum current-density values were achieved with hydrogen-rich cannel coal. For dispersed fuel samples, interparticle contact losses were found to have influence on the cell-generated voltage. The maximum cell opencircuit voltage was reached with stoichiometric oxygen-carbon dioxide mixture blown into the cathode. Yet, the largest current-density values were obtained when carbon dioxide lean mixtures were used. Even at zero carbon dioxide concentration the range of cathode polarizations was less than that observed with stoichiometric mixture. The processes proceeding in the cathode and anode packs of the fuel cell are believed to be interrelated processes. In a model fuel cell fueled with dispersed coal, current densities up to 140 mA/cm² and specific powers up to 70 mW/cm² were achieved.     

Effect of addition of a non-equidiffusional reactant to an equidiffusional diffusion flame

A Burke–Schumann (flame-sheet) formulation is developed for diffusion flames between a fuel and oxidiser with Lewis numbers of unity, subject to addition to the fuel and/or oxidiser stream of a different reactant for which the Lewis number differs from unity. This formulation is applied to laminar counterflow diffusion-flame experiments, reported here, in which hydrogen was added to either methane–nitrogen mixtures or oxygen–nitrogen mixtures at normal atmospheric pressure, with both feed streams at normal room temperature. Experimental conditions were adjusted to fix selected values of the stoichiometric mixture fraction and the adiabatic flame temperature, and the strain rate was increased gradually, maintaining the momentum balance of the two streams, until extinction occurred. At the selected sets of values, the strain rate at extinction was measured as a function of the hydrogen concentration in the fuel or oxidiser stream. The ratio of the fraction of the oxidiser flux that consumes hydrogen to the fraction that consumes fuel was calculated from the new Burke–Schumann formulation, and it was found that, within experimental uncertainty, the ratio of the extinction strain rate with hydrogen addition to that without was the same at any given value of this oxygen flux ratio, irrespective of whether the hydrogen was added on the fuel or oxidiser side. This experimental result was also in close agreement with computational predictions employing detailed chemistry. These results imply that differences in detailed hydrogen concentration profiles within the reaction zone have little or no influence on the chemical kinetics of extinction when the stoichiometric mixture fraction, the adiabatic flame temperature, and the proportion of oxygen that consumes the added fuel are fixed. This same correspondence may be expected to apply for other fuels and additives.     

Dilution effects on laminar jet diffusion flame lengths

Many studies have examined the stoichiometric lengths of laminar gas jet diffusion flames. However, these have emphasized normal flames of undiluted fuel burning in air. Many questions remain about the effects of fuel dilution, oxygen-enhanced combustion, and inverse flames. Thus, the stoichiometric lengths of 287 normal and inverse gas jet flames are measured for a broad range of nitrogen dilution. The fuels are methane and propane and the ambient pressure is atmospheric. Nitrogen addition to the fuel and/or oxidizer is found to increase the stoichiometric lengths of both normal and inverse diffusion flames, but this effect is small at high reactant mole fraction. This counters previous assertions that inert addition to the fuel stream has a negligible effect on the lengths of normal diffusion flames. The analytical model of Roper is extended to these conditions by specifying the characteristic diffusivity to be the mean diffusivity of the fuel and oxidizer into stoichiometric products and a characteristic temperature that scales with the adiabatic flame temperature and the ambient temperature. The extended model correlates the measured lengths of normal and inverse flames with coefficients of determination of 0.87 for methane and 0.97 for propane.     

温度对直接甲醇燃料电池动态性能的影响

利用可计算机控制的电子负载单元,本文实验研究了电池温度对液态进料直接甲醇燃料电池单体电池的稳态和动态性能的影响,并考察了该电池对电池温度变化的动态响应。实验结果表明:电池稳态性能随着电池温度的升高而提升,电池对动态负载的响应随着电池的温度的升高而变得更快和更稳定,升温过程中电池对电池温度变化的响应值要高于降温过程中对应的响应值。     

热物理参数对燃料电池内传质过程的影响

本文利用自行设计的实验系统,对自制的镀金不锈钢极板液态进料直接甲醇燃料电池的性能进行了测试。实验结果表明,较高的氧气压力和流量、较大的甲醇溶液流量、较高的电池温度均有助于强化燃料电池内部的传质过程。另外,在甲醇溶液浓度不超过2.0kmol/m~3的范围内,提高浓度有助于缓解催化层反应物不足的问题,从而改善燃料电池的性能。本文从机理上对这些实验结果进行了分析。     

质子交换膜燃料电池动态启动特性的实验研究

实际应用时燃料电池的运行条件会随时间不断地变化,因此是一个非稳态过程.本文研究了在不同的加湿条件以及反应气流量下电池的启动特性.结果表明:随着气体流量的增大,电池启动速度加快;对电池加湿有利于提高电池的启动性能.     

Effect of injection dynamics on detonation wave propagation in a linear detonation combustor

The effect of reactant injection and mixing on detonation wave propagation is studied in a self-excited, optically-accessible linear detonation combustor operated with natural gas and oxygen. Fuel injection and mixing processes are captured with 100 kHz planar laser induced fluorescence (PLIF) measurements of acetone tracer injected into the fuel stream. Measurements are acquired at multiple orthogonal planes downstream of the reactant injection site to investigate the three-dimensional mixing field in the chamber. The fuel distribution field is correlated with simultaneously acquired OH${}^{*}$ chemiluminescence measurements that provide a qualitative indication of heat release in the combustor. These measurements are used to provide quantitative information of the fuel injector recovery process and its impact on detonation wave structure across a range of equivalence ratios. While significant differences in the detonation wavefront are observed with change in equivalence ratio, the characterization of the fuel refill process into the chamber after the passage of the detonation wave highlights some key generalizable features. The time available for fuel recovery is consistently between 12 – 19% of the detonation wave period across an equivalence ratio range of 0.83 – 1.48. A linear correlation between injector recovery times and the ratio of the average detonation wave pressure amplitude relative to the pressure drop across the fuel injector is observed. Instantaneous and phase-averaged measurements of acetone-PLIF with the time-coincident OH${}^{*}$ chemiluminescence images provide qualitative information of wave structure and injection dynamics along with quantification of fuel injector recovery, a key metric that drives combustor operation and performance. These measurements significantly enhance the ability to obtain detailed information on the intra- and inter-cycle spatiotemporal evolution of the reactant refill process and its coupled effects on the detonation wave structure and propagation.     

EXPERIMENTAL INVESTIGATION OF THE PERFORMANCE OF A SINGLE PROTON EXCHANGE MEMBRANE FUEL CELL USING DRY FUEL

Recently, the requirements for cellular phones, portable computers, and digital cameras have increased dramatically. A portable electric power supply with long duration and high performance is needed for these products. A proton exchange membrane fuel cell (PEMFC) can meet these requirements and becomes one of the best candidates for a portable power source. It is impossible to install an extra humidifier into small-scale portable electric products for PEMFC water management. This article presents a series of experiments to investigate the performance of a single PEMFC. The effects of different operating conditions on cell performance, including the temperature, pressure, and inlet fuel/oxidant flow rate, are discussed. The test results confirm the positive effect of these parameters on cell performance and power output. The interaction effect of temperature--flow rate is related to the cell humidity, and is important for cell performance. The dry-out problem for a PEMFC is also significantly revealed in the experiments for higher cell temperature and flow rate. Current experimental results can provide useful information for investigating the cell performance and its operating effects under dry fuel/oxidant flow conditions and as a benchmark for simulation work in future studies.