SCR脱硝超低排放工程改造流场优化

采用CFD数值模拟方法对某电厂400 MW机组烟气脱硝装置流场进行了诊断,分析了导致效率低、烟道积灰以及空预器磨损等问题的具体原因,之后对此脱硝装置流场进行优化。优化结果表明:在省煤器出口水平扩张段烟道增设导流板,消除了该区域的大范围涡流,有利于减轻烟道积灰,并使喷氨区域烟气速度分布均匀;将喷氨混合装置改成喷氨格栅+圆盘混合器型式,强化了氨氮混合,使首层催化剂入口氨浓度分布均匀性得到显著改善,有利于提高脱硝效率、降低氨逃逸率;在空预器上游烟道增设导流装置,提高了空预器烟气速度分布均匀性,有利于解决空预器磨损问题。通过流场优化后,提高了此脱硝装置脱硝效率,减轻和消除了烟道积灰及空预器磨损。     

三维数值模拟在水力澄清池中的应用

采用了标准的κ-ε紊流模型方程组及有限体积法，对某工厂水力澄清池的流速场和压强场进行了三维数值模拟．并用实际运行情况对数学模型和计算方法进行了验证，计算结果与实际情况吻合良好，说明用数学模型模拟水力澄清池的流速场和压强场是确实有效可行的。     

烟道喷射石灰(石)烟气脱硫技术综述

本文介绍了近几年发展起来的一种简单、中效、适合燃烧中低硫煤的工业锅炉的烟气脱硫技术———烟道喷射石灰 (石 )烟气脱硫技术。从湿法、干法、半干法 3种工艺对烟道喷射烟气脱硫进行了介绍 ,并提出新型脱硫吸收剂是提高烟道脱硫效率的可行方法。最后指出烟道脱硫今后的研究方向     

SCR系统超洁净排放调整与出口NO_x均匀性分析

针对典型SCR系统普遍存在的出口烟道与烟囱处NOx在线监测值不一致的问题与超洁净排放要求,选择2台流场与喷氨格栅结构不同的SCR系统进行性能与优化调整实验。通过对喷氨格栅区域烟气分布与喷氨调整前后出口烟道内NOx分布的测试,分析了导致问题的原因与调整方案的有效性以及不同喷氨格栅结构的优劣性。结果表明:喷氨格栅区域烟气流场分布与区域喷氨量的不一致性是导致不同点位NOx浓度在线监测值不一致的原因;依据调整方案能有效实现SCR出口烟道内NOx浓度均匀分布与超洁净排放的要求;改造后,能针对烟道宽度方向上烟气不均现象进行区域喷氨量调整的喷氨格栅结构Ⅱ与更均匀的烟气分布,促使调整后的2号机组A、B两侧出口NOx浓度分布相对标准偏差明显优于1号机组。     

脱硝系统烟气流场的性能与优化

选择性催化还原(SCR)系统均匀喷氨后,空气预热器易出现堵塞,并且出口在线检测位置不具代表性。为此,根据国内典型SCR系统建立等尺寸的物理结构模型,利用计算流体力学(CFD)技术对烟道与装置内烟气分布、烟气与NH3的混合、压降分布及其原因进行分析,并对导流板的结构进行优化。同时,通过与现场实测入口速度、压降值的对比,论证了数值模型的准确性。结果表明,烟道缩放区域导流板促使烟气均匀分布的同时也使烟气产生倾斜的流动惯性,这使得喷氨格栅(AIG)区域的速度偏差过大,导致了烟气与NH3混和的不均匀,是氨逃逸率高与出口NOx不均匀的首要原因;优化的导流板结构消除了烟气倾斜的流动惯性,进一步促进了AIG区域与催化剂上层烟气的均匀分布以及烟气与NH3的均匀性混合。     

SCR脱硝反应器烟道内部流场的数值模拟与优化

为优化无锡某电厂选择性催化还原脱硝反应器烟道内部流场,研究导流板和整流器对流场的影响,基于FLUENT软件和SIMPLE算法,采用RNG k-ε湍流模型和离散相模型数值模拟导流装置安装前、安装后和优化后3种情况下的烟道内部气流流动和固体颗粒流动.研究表明,导流板可以改善烟道内气流分布,同时保证气流进入催化剂层前的速度小于6 m/s,速度不均匀系数小于15％;整流器对改善气流流动、避免涡流存在具有重要作用,且对压降影响较小;合理的导流板结构和布置可以有效减小压降,导流板优化后压降降低至109.9 Pa.     

磁场作用下烟气流速对静电旋风除尘器收集微粒影响的模拟研究

为了提高静电旋风除尘器(ECP)中微粒的除尘效率,利用磁场能有效抑制微粒逃逸的机理,将磁场引入ECP中,建立多场耦合作用下的微粒运动数学模型,利用Fluent软件数值模拟了有无磁场环境下烟气流速对微粒逃逸率的影响。结果表明:磁场的引入有效降低了ECP中微粒的逃逸率;低烟气流速更有利于微粒在ECP内的捕集;微粒的除尘效率随着磁感应强度的增加而增大,但这一过程中磁场的贡献量逐步减小。研究结果可为新型ECP的设计提供技术参考。     

循环流化床垃圾焚烧炉助燃配风改造对降低CO排放效果的数值模拟

循环流化床(CFB)是垃圾焚烧主要炉型之一,中国生活垃圾具有水分高和挥发分高等特性导致现阶段CFB垃圾焚烧炉CO排放偏高,对其正常运转造成较大影响。对锅炉实体进行助燃配风改造,结合计算流体动力学技术对改造前后炉膛流体场进行模拟,并分析第一烟道内的流场分布情况。结果表明:助燃配风率为40%时,CO的排放均值可降低至80mg/Nm3,烟气含氧量保持在9.5%(体积分数)左右,炉膛中上部温度的平均增幅达到41.3℃。可视化数值模拟结果表明,助燃配风明显提高了烟气旋流和回流,使得烟气轴向速度降幅达37.69%,烟气在第一烟道内停留时间延长;改造后炉膛中上部局部区域内的颗粒质量浓度均值在2.287kg/m3左右,优化了助燃配风参与炉内燃烧的能力。     

SCR脱硝系统烟道内流场优化

为了改善选择性催化还原法(SCR)催化剂上游烟气的流场、温度场和浓度场分布,基于CFD仿真分析技术,建立了整个脱硝系统三维模型,并通过优化导流板及整流格栅,使得速度标准偏差、浓度标准偏差、温度偏差、速度偏转角以及压降等性能指标都满足设计要求,在满足脱硝效率和氨逃逸率前提下,大大降低了烟气对催化剂层的冲刷,保证催化剂的使用寿命。最后,为了合理布置吹灰器,对优化结构下粉尘颗粒在烟道内的运动情况进行了仿真分析研究,为设计提供了依据。     

电除尘器进口矩形烟道气流分布改进的CFD模拟

应用CFD软件对某电厂电除尘器进口矩形烟道内气流分布进行数值模拟.结果表明:电除尘器原进口矩形烟道监测截面的气流分布极其不均匀,数值模拟结果与实验结果速度分布趋势比较吻合.基于此,通过多次改变电除尘器进口矩形烟道内导流板的数量、位置、尺寸等结构参数,使得改造后烟道监测截面风量偏差降到了±2.2%,气流分布相对均方根值均...     

废水液滴在低温烟气中的蒸发特性数值研究

建立了液滴在低温低速烟气中运动和蒸发的数学模型,数值研究了液滴在不同的烟气速度和烟气温度环境中的蒸发特性,获得了液滴速度、温度和直径随时间的变化规律,以及烟气速度和温度对液滴蒸发特性的影响。计算结果表明：气相速度越大,液滴初速度对液滴运动速度的影响越小,液滴速度越容易达到烟气速度。对于初始直径和速度一定的液滴,气液初始相对速度越大,液滴达到临界蒸发温度所需的时间越短,完全蒸发时间也越短。在文中研究的烟气速度范围内,整体上气相速度的改变对液滴完全蒸发时间的影响很小。气相温度的改变对液滴达到临界蒸发温度的时间以及完全蒸发时间的影响很大。烟气从较高温度和较低温度分别下降相同幅度的温度时,液滴在烟气中的完全蒸发时间按不同的倍数在增加,烟气温度越低,液滴完全蒸发时间增加的越多。对于文中研究的液滴,无量纲完全蒸发时间随烟气温度变化呈指数递减规律。     

半干法烟气脱硫除尘多级功能处理装置技术与应用

文中介绍了一种炉窑烟气调质、烟气除尘、烟气脱硫在一个单体结构中的一体化装置和在烟气除尘脱硫技术上的应用,并对该脱硫除尘装置与传统的半干法烟气脱硫除尘装置进行了比较。     

脱硫后净烟气携带浆液量监测的实验研究

在WFGD系统中,净烟气携带的浆液液滴引起后续设备的腐蚀堵塞,带来的景观污染问题影响周围居民的正常生活.为了精确量化脱硫后净烟气携带浆液量,提出了适用于环境监测专业的测试取样分析方法,并对该方法进行了讨论分析.实验结果表明:该方法的适用范围为净烟气浆液液滴含量在1.1 mg/Nm3以上,通过对取样分析关键环节的讨论分析...     

新型离心式脱硫塔气液两相流数值模拟

利用FLUENT软件和SIMPLE算法对新型旋流脱硫塔的气液两相流场进行了数值模拟。计算中气相采用了RSM湍流模型,颗粒相采用了Lagrange坐标系下的随机轨道模型。分析结果表明,气相流场具有强旋流特性;喷射液滴的直径、喷淋量和烟气流速影响其在塔内的分布:喷射液滴粒径越大、喷射量越小、烟气流速越大,入口段降温越少;塔体上方截面平均浓度随液滴粒径的增加而降低,随液气比的增加而增加,随烟气流速的增加会先增加至最高值然后降低。喷淋液滴在其他运行参数不变时,平均粒径范围为0.5～1 mm,会对进口烟气起到较好的净化与降温的作用,并使塔体上方喷淋液滴在截面z=4.15 m处浓度分布均匀且覆盖率高;在保证液滴粒径较小时,通过降低烟气流速或增加喷淋量可提高液滴喷淋覆盖率,使得烟气与喷淋充分接触。计算得到的气相流场分布与实测值吻合较好,证明了数学模型的合理性,为进一步优化分离器结构提供了可靠依据。     

Population Exposure to Toxic Substances: Use of 1970 Census Data

A particulate sampling train has been constructed which satisfies the conflicting requirements of isokinetic sample extraction and constant flow rate through an inertial sizing device. Its design allows a variable fraction of the filtered emission gas to be added to the sample upstream of the inertial sizing device in order to maintain a preselected flow rate through this device while the gas flow rate into the sampling nozzle is adjusted to remain isokinetic with the local duct velocity. The prototype emission gas recycle (EGR) train was constructed by relatively simple modifications of a commercially available Method 5 sampling system, and much of the sampling technique is identical with Method 5 protocol. The train was tested by comparison of parallel runs in the EPA/SRI wind tunnel using redispersed fly ash. In one series of runs performed without inertial sizing devices, the EGR train and a colocated non- EGR train sampled 3-point traverses. The differences of the average mass concentrations measured by the two trains was 3.3 percent, with a standard deviation of 4.7 percent. In the next series of runs, identical cyclone inertial sizing devices were added to each train. The difference of the average mass concentration for these runs was 1.2 percent, with a standard deviation of 5.7 percent.     

尿素/三乙醇胺吸收烟气NO_x的实验研究

以尿素作为吸收液,与NOx反应生成N2和CO2,脱除烟气中的氮氧化物。以一套双级串连的填料塔为主体反应器,分别对气速、液气比、反应物浓度、添加剂浓度和反应温度等参数对尿素溶液吸收NOx反应的影响进行了实验研究,获得了优化实验工况,研究结果显示,在气速为0.1 m/s、液气比为16 L/m3、三乙醇胺为0.01%（质量比）、尿素浓度为13%（质量比）工况下,反应温度为30~70℃,脱硝总效率可达50%以上,且随着NOx体积分数增加而提高。     

双循环多级水幕吸收塔烟气除尘脱硫性能研究

以改进后的双循环多级水幕塔对烟气进行除尘脱硫性能的研究，利用双循环不同pH值控制的优点和多级水幕的效果，增加气液接触面积和传质动力，提高SO₂吸收效果。在正交实验的最佳运行工况基础上，实验从烟气流量、上下两段pH、L/G和SO₂进气浓度等方面进行单因素研究。结果表明，除尘效率维持在98%以上，进气SO₂浓度在5 000 mg/m³以下时，脱硫率在93%以上。上段pH值为6、下段pH值为5、L/G在15左右的脱硫效率和运行工况最佳，无结垢现象发生。改进后的吸收塔具有良好的应用前景，实验结果对于现场脱硫设备的调试和运行有很好的参考价值。     

Precipitator Gas Flow Distribution

An electrostatic precipitator, furnished on a 500-Mw tan-gentially-fired steam generator burning coal, was to collect 99.6% of the fly ash being generated in the furnace of this unit. Preliminary measurements indicated that the installation was not meeting its collection guarantee. Precipitator outlet flue dust distribution indicated that poor gas flow distribution might be one of the causes of the low performance. When observation ports were installed in the outlet flue to permit a direct visual evaluation of the problem, it was found that high velocity jets were present in the collecting electrodes, and that hopper sweepage was present. A model study along with velocity distribution measurements of the installation were authorized. Flow analysis indicated that the field and model correlated well. Extensive changes were made in the model, which eliminated or minimized the high velocity jets and hopper sweepage. After these changes were made in the field installation, it was able to achieve the required dust collection efficiency.     

Turbulent Plume in a Turbulent Cross Flow: Comparison of Wind Tunnel Tests with Field Observations

Plume rise downwind of a large stationary gas turbine was measured in the field and the conditions were then scaled in the laboratory. For the laboratory, the plume exit conditions, wind velocity and temperature profiles, and wind direction were matched. It was found that for high temperature exhaust, the buoyancy is best matched by calculating a dimensionless density difference. With properly calculated buoyancy length scales, the plume trajectories were compared and were found to agree quite well. The probability distributions of the entrainment constant and the average values of the entrapment constant with downwind distance were compared. The field data showed about 15% greater plume rise. The median entrainment constant was about 10% greater for the lab test and the shape of the probability distribution matched very closely.     

Gas-phase mercury reduction to measure total mercury in the flue gas of a coal-fired boiler

Gaseous elemental and total (elemental + oxidized) mercury (Hg) in the flue gas from a coal-fired boiler was measured by a modified ultraviolet (UV) spectrometer. Challenges to Hg measurement were the spectral interferences from other flue gas components and that UV measures only elemental Hg. To eliminate interference from flue gas components, a cartridge filled with gold-coated sand removed elemental Hg from a flue gas sample. The Hg-free flue gas was the reference gas, eliminating the spectral interferences. To measure total Hg by UV, oxidized Hg underwent a gas-phase, thermal-reduction in a quartz cell heated to 750 degrees C. Simultaneously, hydrogen was added to flash react with the oxygen present forming water vapor and preventing Hg re-oxidation as it exits the cell. Hg concentration results are in parts per billion by volume Hg at the flue gas oxygen concentration. The modified Hg analyzer and the Ontario Hydro method concurrently measured Hg at a field test site. Measurements were made at a 700-MW steam turbine plant with scrubber units and selective catalytic reduction. The flue gas sampled downstream of the selective catalytic reduction contained 2100 ppm SO2 and 75 ppm NOx. Total Hg measured by the Hg analyzer was within 20% of the Ontario Hydro results.