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南华大学机械工程学院毕业设计(论文)外文翻译英文原文: A SCREENING METHOD FOR THE OPTIMAL SELECTION OF PLATE HEAT EXCHANGER CONFIGURATIONSJ.M.Pinto and J.A.W.GutDepartment of Chemical Engineering,University of So Paulo, USPAbstract - An optimization method for determining the best configuration(s) of gasketed plate heat exchangers is presented. The objective is to select the configuration(s) with the minimum heat transfer area that still satisfies constraints on the number of channels, the pressure drop of both fluids, the channel flow velocities and the exchanger thermal effectiveness. The configuration of the exchanger is defined by six parameters, which are as follows: the number of channels, the numbers of passes on each side, the fluid locations, the feed positions and the type of flow in the channels. The resulting configuration optimization problem is formulated as the minimization of the exchanger heat transfer area and a screening procedure is proposed for its solution. In this procedure, subsets of constraints are successively applied to eliminate infeasible and nonoptimal solutions. Examples show that the optimization method is able to successfully determine a set of optimal configurations with a minimum number of exchanger evaluations. Approximately 5 % of the pressure drop and channel velocity calculations and 1 % of the thermal simulations are required for the solution. Keywords: plate heat exchanger, heat exchanger configuration, optimization, screening method.INTRODUCTIONThe plate heat exchanger (PHE) consists of a pack of gasketed corrugated metal plates, pressed together in a frame. The fluids flow through a series of parallel flow channels and exchange heat through the thin corrugated metal plates. The gasket design and the closed ports of the plates determine the fluid flow arrangement, which can be parallel, in series or one of several possible combinations of the two. The flow distribution, number of plates, type of gaskets and feed locations characterize the exchanger configuration.CONFIGURATION CHARACTERIZATIONTo characterize the PHE configuration, six distinct parameters are used: NC, PI, PII, f , Yh and Yf, which are described as follows:NC : Number of ChannelsPI and PII : Number of Passes on Sides I and IIf : Feed Connection Relative LocationYh : Hot Fluid LocationYf : Type of Flow in Channels.This binary parameter defines the type of flow inside the channels, which can be straight or crossed depending on the gasket type (Fig. 1). The crossed flow avoids the formation of stagnation areas, but the straight flow type is easier to assemble. It is not possible to use both types together. If Yf = 1, then the flow is crossed in all channels. If Yf = 0, the flow is straight in all channels.The six parameters can represent any regular configuration and an example of configurations for a nine-plate PHE is shown in Fig. (2). For any given number of channels, NC, the five remaining parameters have a finite set of allowable values, which limits the number of possible configurations, as shown in Fig. (3). The disperse pattern is due to the variation in the number of integer factors of NCI and NCII. For the range of number of channels between 2 and 500 there are 284,976 different configurations.Equivalent ConfigurationsFor a given value of number of channels and a fixed type of flow, the existence of equivalent configurations (that have the same thermal effectiveness and pressure drops) is possible. Identification of equivalent configurations is important to avoid unnecessary exchanger evaluations. The equivalence of two or more configurations occurs due to the property of flow reversibility (Pignotti & Tamborenea, 1988), to the presence of single pass or to geometrical similarity (the configuration can be freely rotated or mirrored).A methodology to detect equivalent configurations is shown in Tab. (1). For each set of NC, PI, PII and Yf there are groups of values for parameter f that result in equivalent configurations. In the case of even-numbered NC, there may be equivalency between Yh = 0 and Yh = 1 because sides I and II have the same number of channels and therefore can have the same numbers of passes. Consider for instance the exchanger shown in Fig. (2), which is arranged for f = 1 and Yh = 1; according to Tab. (1), changing the sides of the fluids (Yh = 1 Yh = 0) will yield a different although equivalent configuration.CONFIGURATION OPTIMIZATIONThe configuration optimization problem is formulated as the minimization of the number of channels, NC, which is equivalent to minimizing the exchanger heat transfer area or its fixed cost (Eq. 1). There are constraints on the number of channels (NC), fluid pressure drops (DPhot, DPcold), channel flow velocities (vhot, vcold) and exchanger effectiveness (E), as shown in Constraints (2a) to (2f). The optimization model is also subject to the PHE model, necessary for calculation of the aforementioned variables (Constraint 3).subject toConstraint (2a) on the number of channels is related to the available number of plates and exchanger capacity. The minimum values for fluid pressure drop avoid large variations between the average fluid pressures that can bend the plates. Lower bounds on channel flow velocities avoid the formation of preferential paths or stagnation areas inside the channels.The thermal and hydraulic modeling of the PHE (Constraint 3) was developed by Gut and Pinto (2001). The rigorous thermal model accounts for the variation in the overall heat transfer coefficient in the exchanger and consists of a system of differential and algebraic nonlinear equations, which can be solved by numerical methods. Assuming the heat transfer coefficient invariable, the rigorous model can be reduced to the so-called simplified thermal model, which consists of a system of linear ordinary differential equations and has an analytical solution. Since there is little difference between the main simulation results achieved by rigorous and simplified thermal models, the latter will be used for the optimization, keeping the former for final verification of the results.The Screening MethodThe proposed optimization procedure is based on the screening method, also employed by Daichendt and Grossmann (1994) for heat exchanger network optimization. In this procedure, constraints are successively used to remove infeasible and nonoptimal solutions of a MINLP problem, thus reducing its size and complexity.In the optimization of a PHE configuration, the Constraint on the number of channels (2a) defines the initial set, IS, of possible configurations, formed by combinations of the five remaining parameters. An exhaustive enumeration procedure could be used to obtain the optimal configurations within this set; however, this procedure requires a large computational effort due to the large number of thermal simulations needed.Since it is possible to calculate (DP, v) prior to the thermal simulation using average values for the fluid temperatures, the constraints on pressure drops and channel velocities (Constraints 2b to 2e) can be used to eliminate all infeasible elements in set IS. Therefore, a reduced set of configurations, RS, is generated. It is important to note that to obtain set RS it is not necessary to calculate (DP, v) for all the configurations in IS because of the following:A1) parameter f has no influence over (DP, v), A2) (DP, v) is independent for sides I and II. Thus, for a given NC, the calculations are made only once for each allowable number of passes, A3) for a given NC, DP is proportional to the number of passes; therefore, if DP DPmax is verified, any configuration with a larger number of passes also results in an infeasible solution, A4) for an even-numbered NC, sides I and II have the same number of channels and therefore the same allowable numbers of passes. In this case, (DP, v) will have the same value for Yh = 1 and Yh = 0. Once set RS is obtained, the effectiveness Constraint (2f) is used to select the optimal set of configurations, OS. However, it is not necessary to thermally simulate all elements in RS because of the following:B1) there are equivalent configurations with the same effectiveness; thus only one needs to be simulated, B2) if a search is conducted in increasing order of NC, when the optimal set is found, all remaining configurations with higher values of NC can be neglected. Since the influence of parameter Yf on the convective coefficients and friction factor is usually unknown, this parameter may be fixed prior to optimization, thus reducing the number of possible configurations by 50 %. Moreover, it is not possible to change the type of flow in an existing exchanger.Based on these principles, a screening algorithm is developed for the solution of the PHE configuration problem. The steps of the screening algorithm are as follows. For this algorithm, Yf must have a given value (Yf = 0 or 1). If there is available data on the influence of Yf on the heat exchange and friction correlations, this algorithm can be used once for each case and the results compared.1. The required data for plate (corrugation pattern, dimensions, area enlargement factor and thermal conductivity), hot and cold fluids (flow rate, inlet temperature, fouling factor and correlations for friction factor, convective heat transfer coefficients and physical properties) and constraints (lower and upper bounds for Constraints (2a) to (2f) are read. 2. Initialization: RS = , NC(k) = NCmin , k = 1. 3. All allowable numbers of passes for sides I and II (PIi, PIIj) are obtained for NCk. 4. Verification of constraints on pressure drop and channel flow velocities: 4.1 The (DP, v) pair is calculated for the cold fluid located on side I for each one of the numbers of passes PIi (in increasing order). If the constraints of (DP, v) are satisfied, the cold-fluid/sideI-pass pair is selected. If DPmax is exceeded, there is no need to evaluate larger numbers of passes. This procedure is applied to the cold fluid located on side II for all the numbers of passes, PIIj, thereby selecting the cold-fluid/sideII-pass pairs. 4.2 The same procedure as that in step 4.1 is applied to the hot fluid, obtaining the hot-fluid/sideI-pass and hot-fluid/sideII-pass pairs. 5. The selected pairs of cold-fluid/sideI-pass and hot-fluid/sideII-pass are combined to generate all possible configurations with Yh = 0. Each combination results in four configurations since f has four values equivalent to (DP, v). The same procedure is applied to the selected hot-fluid/sideI-pass and cold-fluid/sideII-pass pairs, yielding configurations with Yh = 1. All generated configurations are stored in RS. 6. If NC(k) = NCmax, then proceed to step 7. Otherwise, NC(k+1) = NC(k) + 1, k = k + 1 and return to step 3. 7. Set RS is now complete. It contains all the configurations that satisfy the constraints on pressure drop and channel velocity for both sides. Now the optimal set, OS, must be obtained. 8. The configurations in RS with the minimum value of NC are selected. 9. The equivalent configurations are detected and grouped using the methodology shown in Tab. (1). 10. The simplified thermal model (the overall heat transfer coefficient is constant) is used to simulate one of the configurations in each group, obtaining the corresponding thermal effectiveness. 11. If one or more groups of equivalent configurations satisfy the effectiveness constraint, they are stored in set OS and there is no need to simulate other elements of RS. Otherwise, proceed to the next value of NC in set RS and return to step 9. 12. The rigorous thermal model is used to simulate the nonequivalent elements in OS to verify the effectiveness results. In case of discrepancy (|Esimplified Erigorous| / Erigorous e ), the rigorous model should be used in the previous simulations after step 8. Otherwise, the optimal solution is achieved. OPTIMIZATION RESULTSIt was verified that the number of channels per pass has a strong effect on the pressure drop, and consequently, about 98 % of the elements in IS are eliminated in the first part of the screening (steps 1 through 8). Compared to an exhaustive enumeration procedure, the screening method demands approximately 5 % of the required evaluations of (DP, v). Further, to obtain set OS only a few elements are thermally simulated (approximately 1 % of the elements in IS or 20 % of the elements in RS).As an example to show the efficiency of the screening method, consider the selection of a configuration for a process-water (26.0 kg/s, 67 C) / cooling-water (62.5 kg/s, 22 C) PHE with 1.4 m chevron plates with crossed channel flow (Yf = 1). The constraint bounds are shown in Constraints (4a) to (4f).In this problem, IS has 26,240 elements and only 1.8 % of the (DP, v) calculations and 0.06 % of the simulations were necessary for the solution of the problem by the screening method. The comparative performance of the screening and enumeration methods is shown in Fig. (4). The set RS obtained contains 84 configurations, ranging from NC = 43 to NC = 144, with pass arrangements of 1/2, 2/3 and 2/4 for hot fluid/cold fluid. The problem solution consists of two pairs of equivalent configurations, all with 120 channels, two passes for the hot fluid and three passes for the cold fluid, as shown in Tab. (2). The required CPU time in a DEC-Unix workstation for the simulations of the simplified model was under 1 min, and 5 min were necessary to validate the results using the rigorous model (the deviations in E were under 1 %).CONCLUSIONSThe configuration of a gasketed plate heat exchanger (PHE) was represented by a set of six distinct parameters and a methodology to detect equivalent configurations was presented. The problem of optimizing the PHE configuration was formulated as the minimization of the heat transfer area, subject to constraints on the number of channels, the pressure drop and channel flow velocities for hot and cold fluids and the exchanger thermal effectiveness as well as the PHE simulation model. Since it is not possible to derive a mathematical model of the PHE that is explicitly a function of the configuration parameters, a mixed-integer nonlinear programming (MINLP) approach could not be used. A screening procedure was then proposed to solve the optimization problem. In this procedure, subsets of the constraints were successively used to eliminate infeasible and nonoptimal elements from the set defined by the bounds on the number of channels. An algorithm was developed to perform the screening with minimum computational effort. Examples show that this algorithm can successfully select a group of optimal configurations (rather than a single solution) for a given application using a very reduced number of thermal simulations.中文翻译:板式换热器构型的最佳选择的筛选方法J.M.Pinto和J.A.W.GutUSP圣保罗大学化学工程系摘要:一种确定垫片式板式换热器的最佳配置的优化方法。目标是选择仍然满足约束条件的信道数目的最小传热面积的配置,两种流体的压力降,该通道的流速和换热器的热效率。热交换器的结构由6个参数,如下定义的信道数目,通行证的每一侧的流体的位置,进给位置和不同的流中的信道的数目。生成的配置优化问题转化为尽量减少换热面积,并提出了其解决方案的筛选程序。在此过程中,依次施加约束的子集,以消除不可行的和非最佳的解决方案。实施例表明,该优化方法能够成功地确定一组最优的配置与最小数量的热交换器评估。约5的压力降和信道的速度计算和1的热模拟所需的解决方案。关键词:板式热交换器,热交换器的配置,优化,筛选方法。 简介板式换热器(PHE)由一包垫圈的金属波纹板,在一个框架中压合在一起。通过一系列的平行流动通道进行热交换,通过薄金属波纹板构成的流体。板的垫圈设计和关闭的端口确定的流体流动装置,它可以是平行的,串联或几种可能的组合的两个。流板,分布,数量型垫片和进料位置交换配置的特点。 构型表征为了表征的PHE配置,六个不同的参数用于NC,PI,PII,F,YH,YF,描述如下:NC:通道数PI和PII:两侧的传球数I和IIF:进给连接的相对位置YH:热流体地点YF:通道中的流量类型。这个二进制参数定义了不同的内部流动通道,它可以是直链或划线根据对垫片的类型(图1)。交叉流可避免形成的停滞区,但直路的流类型是更容易组装。一起使用这两种类型,这是不可能的。如果Yf的=1,则流程的所有通道中的交叉。如果Yf的=0时,流程是直链的所有通道中。6个参数可以表示任何常规配置和九板的板式换热器的配置的一个例子示于图。 (2)。对于任何给定的信道数,NC,五个其它参数允许值的有限集合,这限制了可能的配置数,在图所示。 (3)。分散模式是由于NCI和NCII数量的整数因子的变化。如果在2和500之间的信道数的范围内,有284976个不同的组态。图3:通道数可能出现的常规组态的函数等效配置对于一个给定的信道和一个固定的不同的流数的值,等效的构型(即具有相同的热效率和压力下降)的存在是可能的。相当于配置的识别是很重要的,以避免不必要的热交换器评价。两个或两个以上的配置等价的发生是由于流量可逆性的财产(Pignotti Tamborenea,1988),单通的存在或几何相似(构型可以自由旋转或镜像)。一种方法来检测同等构型标签。 (1)。对于每一组的NC,PI,PII和Yf各组的值,结果在相当于构型参数f。在偶数NC的情况下,有可能是YH= 0和YH=1之间的适合的,因为I和II两侧具有相同的信道数,因此可以有相同的遍数。考虑例如图中所示的热交换器。 (2),它被设置为f= 1,YH= 1;为制表。 (1),改变流体的两侧(YH= 1(R)YH= 0)将产生不同虽然等效的构型。 构型优化配制成的信道的数目,NC,这相当于最小化的换热面积或者其固定费用(式1)的最小化的构型的最优化问题。通道(NC),流体压力的的下降(DPhot DPcold),通道的流速(vhot,vcold)和换热效率(E)的数量上有限制,如图以约束(2A)(2F)。优化模型也受到PHE模型,计算上述变量(约束3)所必需的。得到(2a)中的信道数目的约束有关的可利用的数字板和交换容量。流体压力降的最低值,避免了大的变化,可以弯曲板之间的平均流体压力。下界通道的流速避免的优先路径或通道内的停滞区的形成。筛选方法建议优化程序是基于的筛选方法,Daichendt之外,格罗斯曼(1994)也采用换热网络优化。在此过程中,依次使用约束除去不可行的和非最佳的MINLP问题的解决方案,从而降低了它的大小和复杂性。在板式换热器的构型的最优化,约束的数量的信道(2a)中定义的初始设置,IS,可能的构型,形成的5个其它参数组合。穷举程序,可以被用来获得该组合内的最佳构型,但是,此过程需要一个大的计算工作量,由于需要大量的热模拟。因为它是可以计算(DP,v)的前热模拟使用的流体温度的平均值,压力下降,信道速度(2b中的约束到2e)上的约束可以被用来消除所有不可行元素在套IS。因此,一组简化的构型,RS,生成的。重要的是要注意,要获得设置的RS(DP,v)的计算中的所有构型为由于下述原因,这是没有必要的:A1)参数f有没有影响(DP,V),A2)(DP,v)的独立的I和II两侧。因此,对于一个给定的NC,是由计算只有一次,每个允许的遍数,A3)对于一个给定NC,DP是遍数成比例,因此,如果DP DPMAX验证,也通过与更大数量的任何构型的查询结果在一个不可行的解决方案,A4)的偶数NC,侧面I和II具有相同数量的信道,因此,相同的允许的遍数。在这种情况下,(DP,v)的YH = 1和YH = 0具有相同的值。一旦设置RS获得的有效性约束(2f)的用于选择最佳的一组构型,操作系统。然而,这是没有必要的热模拟RS因为下列因素中的所有元素:B1)是等价的配置具有相同的有效性,因此只有一个需要被模拟B2),如果搜索进行数值越高,数控数控递增的顺序,找到最优集时,所有剩余的构型可以忽略不计。由于参数Yf的对流系数和摩擦系数的影响通常是未知的,是固定的,这个参数可能在优化之前,从而减少了50,可能的构型。此外,它是不可能改变现有的热交换器中的流动不同的。基于这些原则,筛选算法开发的解决方案,的PHE构型问题。筛选算法的步骤如下所示。对于此算法,Yf的必须有一个给定的值(Yf的
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