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http://www.spinellis.gr/pubs/jrnl/1999-IJPR-Optim/html/bap.html This is an HTML rendering of a working paper draft that led to a publication. The publication should always be cited in preference to this draft using the following reference:
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Diomidis Spinellis
Department of Information and Communication Systems
University of the Aegean
83200 Karlovasi
Samos, Greece.
email: dspin@aegean.gr
Chrissoleon Papadopoulos
Department of Business Administration
University of the Aegean
82100 Chios, Greece
email: hpap@aegean.gr
J. MacGregor Smith
Department of Mechanical and Industrial
Engineering
University of Massachusetts
Amherst Massachusetts 01003, USA
email: jmsmith@ecs.umaecs.edu
Keywords: Buffer Allocation, Nonlinear, Stochastic, Integer, Network Design, Simulated Annealing
A large amount of research has been devoted to the analysis and design of production lines. A lot of this research concerns the design of manufacturing systems with considerable inherent variability in the processing times at the various stations, a common situation with human operators/assemblers. The literature on the modelling and optimization of production lines is vast, allowing us to review only the most directly relevant studies. For a systematic classification of the relevant works on the stochastic modelling of these and other types of manufacturing systems (e.g., transfer lines, flexible manufacturing systems (FMS) and flexible assembly systems (FAS)), the interested reader is referred to a review paper by Papadopoulos and Heavey [63] and some recently published books, such as those by Askin and Standridge [5], Buzacott and Shanthikumar [9], Gershwin [25], Papadopoulos et al. [64], Viswanadham and Narahari [81] and Altiok [2].
Two are the basic problem classes:
the optimization of the decision variables of these lines.
Examples of decision variables that have been considered are:
The corresponding optimization problems are named, respectively, (1) the buffer allocation problem, (2) the server allocation problem and (3) the workload allocation problem, in a production line.
In Papadopoulos et al. [64] both evaluative and generative (optimization) models are given for modelling the various types of manufacturing systems. This work falls into the second category. Evaluative and optimization models can be combined by closing the loop between them; that is, one can use feedback from an evaluative model to modify the decisions taken by the optimization model.
One of the key questions that the designers face in a serial production line is the buffer allocation problem (BAP), i.e., how much buffer storage to allow and where to place it within the line. This is an important question because buffers can have a great impact on the efficiency of the production line. They compensate for the blocking and the starving of the line's stations. For this reason, the buffer allocation problem has received a lot more attention than the other two design problems. Buffer storage is expensive due both to its direct cost, and to the increase of the work-in-process (WIP) inventories. In addition, the requirement to limit the buffer storage can also be a result of space limitations in the shop floor. The literature on the BAP is extensive. A systematic classification of the research work in this area is given in Singh and MacGregor Smith [71] and Papadopoulos et al. [64]. The works are split according to:
Apart of the buffer allocation problem, the other two interesting design problems have been also considered by some researchers, e.g., the work allocation problem (Hillier and Boling [37], [34], [36], Ding and Greenberg [19], Huang and Weiss [45], Shanthikumar et al. [70], Wan and Wolff [82] and Yamazaki et al. [84], among others) and the server allocation problem (Magazine and Stecke [60] and Hillier and So [38]). Hillier and So [41] studied various combinations of these three design problems. Other references may be found therein (Buzacott and Shanthikumar [8], [9], among others).
The present work deals with the same design problems (buffer allocation, server allocation and workload allocation) but for long production lines with multi-machine stations.
As the problem being investigated is combinatorial in nature, traditional Operations Researh techniques as not practical for obtaining optimal solutions for long production lines. We propose a simulated annealing (SA) approach as the search method in conjunction with the expansion method developed by Kerbache and MacGregor Smith [50] as the evaluative tool. Simulated annealing is an adaptation of the simulation of physical thermodynamic annealing principles described by Metropolis et al. [61] to the combinatorial optimization problems [53,11]. Similar to genetic algorithms [44,28] and tabu search techniques [27] it follows the ``local improvement'' paradigm for harnessing the exponential complexity of the solution space.
The algorithm is based on randomization techniques. An overview of algorithms based on such techniques can be found in the survey by Gupta et al. [31]. A complete presentation of the method and its applications is described by Van Laarhoven and Aarts [58] and accessible algorithms for its implementation are presented by Corana et al. [15] and Press et al. [67]. A critical evaluation of different approaches to annealing schedules and other method optimizations are given by Ingber [46]. As a tool for operational research SA is presented by Eglese [20], while Koulamas et al. [55] provide a complete survey of SA applications to operations research problems.
The use of the Simulated Annealing algorithm appears to be a promissing approach. We believe that this algorithm could be applied in conjunction with a fast decomposition algorithm to solve efficiently and accurately the aforementioned optimization problems in much longer production lines.
The remainder of the paper is organized as follows: we first describe the production line model and the problem of our interest followed by the methodology of our approach namely: the performance model, the expansion method used for evaluating the line performance, an overview of the combinatorial optimization methods, the simulated annealing optimization method, and the complete enumeration method; we then we describe our experimental methodology and present an overview of the numerical and performance results for short and long production lines. In the Appendix following the concluding section, we provide a full tabulated set of the experimental results.

A N-station line consists of N workstations in series, labelled M1, M2, ¼, MN and N-1 locations for buffers, labelled B2, B3, ¼, BN, is illustrated in Figure 1. Each station i has si servers operating in parallel. The buffer capacities of the intermediate buffers Bi, i = 2,¼,N, are denoted by qi, whereas the mean service times of the i stations (i = 1,¼,N) are denoted by wi.
The main performance measure of the production line is the mean throughput, denoted by R(q,s,w), where q = (q2,q3,¼,qN), s = (s1,s2,¼,sN) and w = (w1,w2,¼,wN).
If Q denotes the total number of available buffer slots to be allocated to the N-1 buffers and S the total number of available servers (machines) to allocated to the N stations then the general version of the optimization model (first reported by Hillier and So, 1995) is:
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The objective function of throughput, R(q,s,w), is not the only performance measure of interest. The average WIP, the flow time, the cycle time, the system utilization, the average queue lengths and other measures are equally important performance measures. However, throughput is the most commonly used performance measure in the international literature.
The queueing model M/M/C/K that we use refers to a queueing system where:
While our focus in this paper is on M/M/C/K approximations for open queueing networks of series-parallel topologies, we also briefly discuss some of the available approaches used for modelling M/M/1/K systems since most of the literature has focused on M/M/1/K systems.
Both open and closed systems have been studied by exact analysis although results have been limited. Exact analyses of open two, three, and four node-server models with exponential service are limited by the explosive growth of the Markov chain models for analyzing these systems. The analysis of very large Markov chain models has led to effective aggregation techniques for these models [68,77] but the computation time and power required for these exact results leaves open the need for approximation techniques.
Van Dijk and his co-authors [79,80] have developed some bounding methodologies for both M/M/1/K and M/M/C/K systems and have demonstrated their usefulness in the design of small queueing networks. Of course, when doing optimization of medium and long queueing networks, bounds can be far off the optimum, so robust approximation techniques close to the optimal performance measures are most desireable.
Most approximation techniques appearing in the literature rely on decomposition/aggregation methods to approximate performance measures. One and two node decompositions of the network have been carried out, all with varying degree of success.
The few approximation approaches available in the literature can be classified as follows: Isolation methods, Repeated Trials, Node-by-node decomposition, and Expansion methods. In the Isolation method, the network is subdivided into smaller subnetworks and then studied in isolation [59,6]. This method was used by Kuehn [57,23] but they failed to consider networks with finite capacity.
Closely related to the Isolation method is the Repeated Trials Method, a class of techniques based upon repeatedly attempting to send blocked customers to a queue causing the blocking [10,22,21].
In Node-by-node decomposition, the network is broken down into single, pairs, and triplets of nodes with augmented service and arrival parameters which are then studied separately [35,78,1,3,65,7]. More general service time approximations appear in [30]. The Expansion method is the approach argued for in this paper for computing the performance measures of M/M/C/K finite queueing networks [49,51,52]. It can be characterized conceptually as a combination of Repeated Trials and Node-by-Node Decomposition where the key difference is that a ``holding'' node is added to the network to register blocked customers. The addition of the holding node ``expands'' the network. This approach transforms the queueing network into an equivalent Jackson network which is then decomposed allowing for each node to be solved independently. We have successfully used the Expansion Method to model M/M/1/K[52], M/M/C/K[48,32], M/G/1/K[51], and most recently M/G/C/C [12,72,73] queues and queueing networks. In addition, we have also used our Expansion Methodology to model routing [18,17,29] and optimal resource allocation problems [75,72,74,71].
The Expansion Method is a robust and effective approximation technique developed by Kerbache and Smith [51]. As described in previous papers, this method is characterized as a combination of Repeated Trials and Node-by-node Decomposition solution procedures. Methodologies for computing performance measures for a finite queueing network use primarily the following two kinds of blocking:
The Expansion Method uses Type I blocking, which is prevalent in most production and manufacturing, transportation and other similar systems.
Consider a single node with finite capacity K (including service). This node essentially oscillates between two states - the saturated phase and the unsaturated phase. In the unsaturated phase, node j has at most K- 1 customers (in service or in the queue). On the other hand, when the node is saturated no more customers can join the queue. Refer to Figure 2 for a graphical representation of the two scenarios.

The Expansion Method consists of the following three stages :
The following notation defined by Kerbache and Smith [51,52] shall be used in further discussion regarding this methodology :
Using the concept of two phases at node j, an artificial node h is added for each finite node in the network to register blocked customers. Figure 2 shows the additional delay, caused to customers trying to join the queue at node j when it is full, with probability pK. The customers successfully join queue j with a probability (1 - pK). Introduction of an artificial node also dictates the addition of new arcs with pK and (1 - pK) as the routing probabilities.
The blocked customer proceeds to the finite queue with probability (1- pK¢) once again after incurring a delay at the artificial node. If the queue is still full, it is rerouted with probability pK¢ to the artificial node where it incurs another delay. This process continues till it finds a space in the finite queue. A feedback arc is used to model the repeated delays. The artificial node is modeled as an M/M/¥ queue. The infinite number of servers is used simply to serve the blocked customer a delay time without queueing.
This stage essentially estimates the parameters pK, pK¢ and mh utilizing known results for the M/M/C/K model.
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where for (l/cm\not = 1)
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and for (l/cm = 1),
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where r1 and r2 are the roots to the polynomial:
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while, l = lj - lh(1 - pK¢) and lj and lh are the actual arrival rates to the finite and artificial holding nodes respectively.
In fact, lj the arrival rate to the finite node is given by:
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Let us examine the following argument to determine the service time at the artificial node. If an arriving customer is blocked, the queue is full and thus a customer is being serviced, so the arriving customer to the holding node has to remain in service at the artificial holding node for the remaining service time interval of the customer in service. The delay distribution of a blocked customer at the holding node has the same distribution as the remaining service time of the customer being serviced at the node doing the blocking. Using renewal theory, one can show that the remaining service time distribution has the following rate mh:
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where, s2 is the service time variance given by Kleinrock [54]. Notice that if the service time distribution at the finite queue doing the blocking is exponential with rate mj, then:
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Due to the feedback loop around the holding node, there are strong dependencies in the arrival processes. Elimination of these dependencies requires reconfiguration of the holding node which is accomplished by recomputing the service time at the node and removing the feedback arc. The new service rate is given by:
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The probabilities of being in any of the two phases (saturated or unsaturated) are pK and (1 - pK) . The mean service time at a node i preceding the finite node is mi-1 when in the unsaturated phase and (mi-1 + mh¢-1) in the saturated phase. Thus, on an average, the mean service time at the node i preceding a finite node is given by:
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Similar equations can be established with respect to each of the finite nodes. Ultimately, we have simultaneous non-linear equations in variables pK, pK¢, mh-1 along with auxiliary variables such as mj and [(li)\tilde] . Solving these equations simultaneously we can compute all the performance measures of the network.
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Equations 14 to 17 are related to the arrivals and feedback in the holding node. The equations 18 to 20 are used for solving equation 17 with z used as a dummy parameter for simplicity of the solution. Lastly, equation 21 gives the approximation to the blocking probability derived from the exact model for the M/M/C/K queue. Hence, we essentially have five equations to solve, viz. 14 to 17 and 21. To recapitulate, we first expand the network with an artifical holding node; this stage is then followed by the approximation of the routing probabilities, due to blocking, and the service delay in the holding node; and, finally, the feedback arc at the holding node is eliminated. Once these three stages are complete, we have an expanded network which can then be used to compute the performance measures for the original network. As a decomposition technique this approach allows successive addition of a holding node for every finite node, estimation of the parameters and subsequent elimination of the holding node.
Exact approaches are appropriate for solving small problem instances or for problems with special structure e.g. the Travelling Salesman Problem, which admit optimal solutions. Classical approaches for achieveing an optimal solution include Branch-and-Bound, Branch-and-Cut, Dynamic Programming, Exhaustive Search, and related implicit and explicit enumeration methods. The difficulty with utilizing these exact approaches for the BAP such as Branch-and-Bound is that the subproblems for which one seeks to compute upper and lower bounds on the objective function are stochastic, nonlinear programming problems which are as difficult as the original problem so little is gained by these exact problem decomposition methods.
This dilemma implies that heuristic approaches are the only reasonable methodology for large scale problem instances of the BAP problem. Heuristic approaches can be classified as either classical Nonlinear Programming search methods or Metaheuristics.
Nonlinear Programming (derivative-free) search [42] methods such as Hooke-Jeeves, Nelder-Mead simplex methods, PARTAN, Powell's Conjugate Direction metods, Flexible Tolerance, the Complex Method of Box, and other related techniques to name a few have met with varied levels of success in the BAP literature and are viable means of dealing with the BAP because of the non-closed form nature of the nonlinear objective function. While many researchers feel that the objective function is concave or pseudo-concave in the decision variables, the discrete nature of the decision variables makes the problem discontinuous and so no derivative information is available.
Metaheuristic methods such as Simulated Annealing, Tabu Search, Genetic Algorithms, and related techniques have not historically been utilized to solve the BAP, and we shall explore the use of Simulated Annealing in this paper.

Physical matter can be brought into a low-temperature ground state by careful annealing. First the substance is melted, then it is gradually cooled with a lot of time spent at temperatures near the freezing point. If this procedure is not followed the resulting substance may form a glass with not crystalline order and only metastable, consisting of locally optimal structures [53]. During the cooling process the system can escape local minima by moving to a thermal equilibrium of a higher energy potential based on the probabilistic distribution w of entropy S:
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| (23) |
| (24) |
The application of the annealing optimization method to other processes works by repeatedly changing the problem configuration and gradually lowering the temperature until a minimum is reached.
The correspondence between annealing in the physical world and simulated annealing as used for production line optimization is outlined in Table 1.
| Physical World | Production Line Optimization |
| Atom placement | Line configuration |
| Random atom movements | Buffer space, server, service rate movement |
| Energy E | Throughput R |
| Energy differential DE | Configuration throughput differential DR |
| Energy state probability distribution | Changes according to the Metropolis criterion, exp([(-DE)/ T]) > rand (0 ¼1), implementing the Boltzmann probability distribution |
| Temperature | Variable for establishing configuration acceptance termination |
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All buffer and server combinations can be methodically enumerated by considering a vector p denoting the position within the production line of each buffer or server. Given the vector p we can then easily map p to q or s using the following equation (for the case of q):
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| (27) |
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Essentially, g maps the vector of positions to a new one representing another line configuration. When the position pi of buffer or server resource i, as it is incremented, reaches the last place in the line N (pi + 1 = N) g is recursively applied to the buffer or server in position pi+1 setting pi-pQ to the new value of pi+1. The complete enumeration terminates when all buffers or servers reach the line position N. To enumerate all buffer and server combinations one complete server enumeration is performed for each line buffer configuration.
The generalized queueing network throughput evaluation algorithm was initially ported from a VAX VMS operating system, to a PC-based Intel architecture. Most changes involved the adjustment of numerical constants according to the IEEE 488 floating point representation used on the Intel platforms. Subsequently, the algorithm was rewritten in a pure subroutine form so that it could be repeatedly called from within a program and semi-automatically converted from FORTRAN to ANSI C.
The simulated annealing algorithm used for distributing Q buffer space, S servers, and N service rate in an N-station line is given below:
The SA procedure was run with the following characteristics based on the number of stations N:
The following facts clarify the use of the evaluation algorithm:
the line topology graph is a linear series of stations allowing for parallel servers, and
the initial and the effective arrival rate at the first server are set to 1.5.
Three batches of tests were planned and executed. One, presented in Tables 2-13, was planned in order to compare the results of our approach with those of Hillier and So [41]. A second set, presented in Tables 14-17, was planned in order to compare the approach to the results obtained using a different evaluative procedure [76]. Finally, the third batch of tests, presented in Tables 18-27, aimed at establishing our method's efficacy in determining optimal configurations of large production lines. Tables 14-27 contain an additional column, T, presenting the program execution time (s).
The bowl phenomenon occurs when for j = 1,2,¼,N,
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Correspondingly, the L-phenomenon is the allocation of extra servers to the first station of the production line. This leads to almost the maximum throughput of the line, which is attained when the extra servers are allocated to the last station of the line, having the advantage that it leads to less work-in-process inventory.
Concerning the behaviour of SA compared to CE the results of the two methods are as follows:
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Having demonstrated the viability of using an algorithm based on randomization techniques for optimizing large production lines we now plan to explore other optimization methods based on similar principles such as genetic algorithms to find how they compare to our approach. The simulated annealing algorithm can be fine-tuned in a number of ways. Results for long production lines from different approaches will allow us to tune the algorithm for optimal performance in terms of execution time and derivation of optimal results and propose prescriptive guidelines for implementing production line optimization systems.
N S Q w R
3 3 3 (1.04 1.01 0.951) 0.5478
4 4 4 (1.06 1.01 0.976 0.95) 0.4913
5 5 5 (1.06 1.02 0.99 0.975 0.947) 0.4493
6 6 6 (1.07 1.03 1.01 0.975 0.962 0.955) 0.4164
7 7 7 (1.08 1.05 1.01 0.966 0.968 0.969 0.965) 0.3898
8 8 8 (1.09 1.04 0.98 0.998 0.973 0.983 0.97 0.962) 0.3675
9 9 9 (1.07 1.06 0.995 0.989 0.994 0.98 0.976 0.964 0.978) 0.3487
N S Q q R
8 9 8 ( 1 1 1 1 1 1 1 2 ) 0.3809
8 10 8 ( 1 1 1 1 1 1 2 2 ) 0.3961
8 11 8 ( 1 1 1 1 1 2 2 2 ) 0.4122
8 12 8 ( 1 1 1 1 2 2 2 2 ) 0.4292
8 13 8 ( 1 1 1 2 2 2 2 2 ) 0.4469
8 14 8 ( 1 1 2 2 2 2 2 2 ) 0.4648
8 15 8 ( 1 2 2 2 2 2 2 2 ) 0.4831
6 12 6 ( 2 2 2 2 2 2 ) 0.5429
6 13 6 ( 2 2 2 2 2 3 ) 0.5578
4 25 4 ( 5 6 7 7 ) 0.8246
4 28 4 ( 5 7 8 8 ) 0.8415
4 29 4 ( 5 8 8 8 ) 0.8462
4 30 4 ( 5 8 8 9 ) 0.8509
N S Q s R
7 7 8 ( 1 2 1 1 1 1 1 ) 0.421
7 7 9 ( 1 2 1 1 1 2 1 ) 0.4614
7 7 10 ( 1 2 1 2 1 2 1 ) 0.5132
7 7 11 ( 2 2 1 2 1 2 1 ) 0.5753
5 5 6 ( 1 2 1 1 1 ) 0.4992
5 5 7 ( 1 2 1 2 1 ) 0.5683
5 5 8 ( 2 2 1 2 1 ) 0.6594
5 5 9 ( 2 2 2 2 1 ) 0.7573
3 3 5 ( 2 2 1 ) 0.8051
3 3 47 ( 27 8 12 ) 1
3 3 92 ( 89 1 2 ) 1
N S Q s w R
5 5 6 ( 1 1 1 2 1 ) (1.16 1.11 1.05 0.795 0.878) 0.512
5 5 8 ( 2 2 1 2 1 ) (0.995 0.789 1.16 0.948 1.11) 0.678
5 5 10 ( 2 2 2 2 2 ) (1.31 0.917 0.934 0.923 0.918) 0.8651
N S Q q w R
3 4 3 ( 1 1 2 ) (1.08 1.04 0.885) 0.5928
3 5 3 ( 1 2 2 ) (1.08 0.972 0.943) 0.6371
3 6 3 ( 2 2 2 ) (1.04 0.998 0.959) 0.6685
3 7 3 ( 2 2 3 ) (1.07 1 0.931) 0.6986
3 8 3 ( 2 3 3 ) (1.07 0.978 0.953) 0.7258
4 5 4 ( 1 1 1 2 ) (1.09 1.04 1 0.862) 0.5258
4 6 4 ( 1 1 2 2 ) (1.12 1.06 0.912 0.908) 0.5598
4 7 4 ( 1 2 2 2 ) (1.09 0.988 0.957 0.961) 0.5926
4 8 4 ( 2 2 2 2 ) (1.06 1 0.977 0.966) 0.6157
4 9 4 ( 2 2 2 3 ) (1.07 1.02 0.998 0.914) 0.6397
4 10 4 ( 2 2 3 3 ) (1.09 1.02 0.945 0.938) 0.6621
5 6 5 ( 1 1 1 1 2 ) (1.1 1.06 1.02 0.986 0.834) 0.477
5 7 5 ( 1 1 1 2 2 ) (1.12 1.08 1.02 0.895 0.877) 0.5049
5 8 5 ( 1 1 2 2 2 ) (1.14 1.07 0.944 0.925 0.917) 0.5319
5 9 5 ( 1 2 2 2 2 ) (1.12 1 0.965 0.968 0.944) 0.5577
5 10 5 ( 1 2 2 2 3 ) (1.14 1.01 0.991 0.97 0.889) 0.5764
5 11 5 ( 2 2 2 2 3 ) (1.08 1.03 1.01 0.985 0.899) 0.5956
5 12 5 ( 2 2 2 3 3 ) (1.09 1.03 1.01 0.932 0.927) 0.6147
5 13 5 ( 2 2 3 3 3 ) (1.1 1.04 0.956 0.962 0.947) 0.6324
N S Q q s R
3 3 4 ( 1 1 1 ) ( 1 2 1 ) 0.6487
3 4 4 ( 2 1 1 ) ( 1 2 1 ) 0.6918
3 5 4 ( 2 2 1 ) ( 1 2 1 ) 0.7329
3 6 4 ( 2 2 2 ) ( 1 2 1 ) 0.7647
3 7 4 ( 3 2 2 ) ( 1 2 1 ) 0.7906
3 3 5 ( 1 1 1 ) ( 2 2 1 ) 0.8051
3 4 5 ( 1 1 2 ) ( 2 2 1 ) 0.8447
3 5 5 ( 1 1 3 ) ( 2 2 1 ) 0.8698
3 6 5 ( 1 1 4 ) ( 2 2 1 ) 0.8872
3 7 5 ( 1 1 5 ) ( 2 2 1 ) 0.8999
3 4 6 ( 2 1 1 ) ( 2 2 2 ) 1.037
3 5 6 ( 3 1 1 ) ( 2 2 2 ) 1.09
3 6 6 ( 3 1 2 ) ( 2 2 2 ) 1.134
3 7 6 ( 3 2 2 ) ( 2 2 2 ) 1.181
4 5 5 ( 1 1 1 2 ) ( 1 2 1 1 ) 0.6008
4 6 5 ( 2 1 1 2 ) ( 1 2 1 1 ) 0.6323
4 7 5 ( 2 2 1 2 ) ( 1 2 1 1 ) 0.6607
4 8 5 ( 2 2 1 3 ) ( 1 2 1 1 ) 0.687
4 5 6 ( 1 1 1 2 ) ( 2 2 1 1 ) 0.7065
4 6 6 ( 1 1 1 3 ) ( 2 2 1 1 ) 0.7385
4 7 6 ( 1 1 2 3 ) ( 2 2 1 1 ) 0.7648
4 8 6 ( 1 1 2 4 ) ( 2 2 1 1 ) 0.786
4 5 7 ( 1 1 1 2 ) ( 2 2 2 1 ) 0.817
4 6 7 ( 1 1 1 3 ) ( 2 2 2 1 ) 0.8403
4 7 7 ( 1 1 2 3 ) ( 2 2 2 1 ) 0.8569
4 8 7 ( 1 2 2 3 ) ( 2 2 2 1 ) 0.8737
4 5 8 ( 2 1 1 1 ) ( 2 2 2 2 ) 0.9762
4 6 8 ( 3 1 1 1 ) ( 2 2 2 2 ) 1.019
4 7 8 ( 3 1 1 2 ) ( 2 2 2 2 ) 1.055
4 8 8 ( 3 1 2 2 ) ( 2 2 2 2 ) 1.093
N S Q q s R
5 6 6 ( 1 1 1 1 2 ) ( 1 2 1 1 1 ) 0.5304
5 7 6 ( 1 2 1 1 2 ) ( 1 1 2 1 1 ) 0.5603
5 8 6 ( 2 1 1 2 2 ) ( 1 2 1 1 1 ) 0.5884
5 9 6 ( 2 2 1 2 2 ) ( 1 2 1 1 1 ) 0.6097
5 6 7 ( 1 1 1 1 2 ) ( 2 2 1 1 1 ) 0.5984
5 7 7 ( 1 1 1 2 2 ) ( 2 2 1 1 1 ) 0.6426
5 8 7 ( 1 1 1 2 3 ) ( 2 2 1 1 1 ) 0.6669
5 9 7 ( 1 1 1 3 3 ) ( 2 2 1 1 1 ) 0.6913
5 6 8 ( 1 1 1 2 1 ) ( 2 2 1 2 1 ) 0.6939
5 7 8 ( 1 1 1 1 3 ) ( 2 2 2 1 1 ) 0.7213
5 8 8 ( 1 1 1 2 3 ) ( 2 2 2 1 1 ) 0.7468
5 9 8 ( 1 1 2 2 3 ) ( 2 2 1 2 1 ) 0.7649
5 6 9 ( 2 1 1 1 1 ) ( 2 2 2 2 1 ) 0.8065
5 7 9 ( 2 1 1 1 2 ) ( 2 2 2 2 1 ) 0.8463
5 8 9 ( 2 1 1 1 3 ) ( 2 2 2 2 1 ) 0.8716
5 9 9 ( 2 1 1 1 4 ) ( 2 2 2 2 1 ) 0.889
5 6 10 ( 2 1 1 1 1 ) ( 2 2 2 2 2 ) 0.9262
5 7 10 ( 3 1 1 1 1 ) ( 2 2 2 2 2 ) 0.9611
5 8 10 ( 3 1 1 1 2 ) ( 2 2 2 2 2 ) 0.9916
5 9 10 ( 3 1 1 2 2 ) ( 2 2 2 2 2 ) 1.024
N S Q q s w R
3 4 4 ( 1 2 1 ) ( 1 2 1 ) (1.2 0.778 1.02) 0.7228
3 5 4 ( 2 2 1 ) ( 1 2 1 ) (1.16 0.789 1.05) 0.7686
3 6 4 ( 2 2 2 ) ( 1 2 1 ) (1.2 0.767 1.04) 0.8052
3 7 4 ( 2 3 2 ) ( 1 2 1 ) (1.19 0.773 1.04) 0.8317
3 4 5 ( 2 1 1 ) ( 2 2 1 ) (0.913 0.823 1.26) 0.9071
3 5 5 ( 2 1 2 ) ( 2 2 1 ) (0.93 0.836 1.23) 0.9481
3 6 5 ( 3 1 2 ) ( 2 2 1 ) (0.874 0.859 1.27) 0.9881
3 7 5 ( 3 2 2 ) ( 2 2 1 ) (0.883 0.802 1.31) 1.027
3 4 6 ( 2 1 1 ) ( 2 2 2 ) (1.09 0.964 0.948) 1.041
3 5 6 ( 3 1 1 ) ( 2 2 2 ) (1.02 0.994 0.987) 1.091
3 6 6 ( 3 1 2 ) ( 2 2 2 ) (1.06 1.03 0.914) 1.139
3 7 6 ( 3 2 2 ) ( 2 2 2 ) (1.09 0.96 0.954) 1.185
4 5 5 ( 1 1 1 2 ) ( 1 2 1 1 ) (1.22 0.804 0.989 0.983) 0.6161
4 6 5 ( 1 2 2 1 ) ( 1 1 2 1 ) (1.19 1.04 0.778 0.99) 0.6515
4 7 5 ( 2 2 2 1 ) ( 1 1 2 1 ) (1.15 1.07 0.767 1.02) 0.6833
4 8 5 ( 2 2 2 2 ) ( 1 1 2 1 ) (1.16 1.09 0.772 0.971) 0.7103
4 5 6 ( 1 1 2 1 ) ( 2 1 2 1 ) (0.95 1.15 0.797 1.11) 0.7299
4 6 6 ( 2 2 1 1 ) ( 1 2 2 1 ) (1.27 0.794 0.797 1.14) 0.7681
4 7 6 ( 2 2 1 2 ) ( 1 2 2 1 ) (1.31 0.798 0.791 1.1) 0.7997
4 8 6 ( 2 1 3 2 ) ( 2 1 2 1 ) (0.86 1.21 0.798 1.13) 0.8367
4 5 7 ( 2 1 1 1 ) ( 2 2 2 1 ) (0.965 0.853 0.862 1.32) 0.8766
4 6 7 ( 2 1 1 2 ) ( 2 2 2 1 ) (0.988 0.883 0.869 1.26) 0.9121
4 7 7 ( 3 1 1 2 ) ( 2 2 2 1 ) (0.923 0.897 0.894 1.29) 0.9449
4 8 7 ( 2 1 3 2 ) ( 2 1 2 2 ) (1.01 1.39 0.803 0.801) 0.9404
5 6 6 ( 1 1 1 1 2 ) ( 1 1 2 1 1 ) (1.19 1.14 0.796 0.932 0.94) 0.5438
5 7 6 ( 1 1 1 2 2 ) ( 1 2 1 1 1 ) (1.23 0.809 0.986 0.99 0.983) 0.5759
5 6 7 ( 1 1 2 1 1 ) ( 1 1 2 2 1 ) (1.3 1.19 0.743 0.748 1.02) 0.6226
5 7 7 ( 1 2 2 1 1 ) ( 1 1 2 2 1 ) (1.27 1.1 0.788 0.786 1.06) 0.6556
5 6 8 ( 1 2 1 1 1 ) ( 1 2 2 2 1 ) (1.43 0.803 0.796 0.8 1.17) 0.7202
5 7 8 ( 2 1 1 1 2 ) ( 2 2 2 1 1 ) (0.908 0.809 0.801 1.24 1.24) 0.769
N S Q q R
8 9 8 ( 1 1 1 1 1 1 1 2 ) 0.3809
8 10 8 ( 1 1 1 1 1 1 2 2 ) 0.3961
8 11 8 ( 1 1 1 1 1 2 2 2 ) 0.4122
8 12 8 ( 1 1 1 1 2 2 2 2 ) 0.4292
8 13 8 ( 1 1 1 2 2 2 2 2 ) 0.4469
8 14 8 ( 1 1 2 2 2 2 2 2 ) 0.4648
8 15 8 ( 1 2 2 2 2 2 2 2 ) 0.4831
6 12 6 ( 2 2 2 2 2 2 ) 0.5429
6 13 6 ( 2 2 2 2 2 3 ) 0.5578
4 25 4 ( 5 6 7 7 ) 0.8246
4 28 4 ( 5 7 8 8 ) 0.8415
4 29 4 ( 5 8 8 8 ) 0.8462
4 30 4 ( 5 8 8 9 ) 0.8509
N S Q s R
7 7 8 ( 1 2 1 1 1 1 1 ) 0.421
7 7 9 ( 1 2 1 1 1 2 1 ) 0.4614
7 7 10 ( 1 2 1 2 1 2 1 ) 0.5132
7 7 11 ( 2 2 1 2 1 2 1 ) 0.5753
5 5 6 ( 1 2 1 1 1 ) 0.4992
5 5 7 ( 1 2 1 2 1 ) 0.5683
5 5 8 ( 2 2 1 2 1 ) 0.6594
5 5 9 ( 2 2 2 2 1 ) 0.7573
3 3 5 ( 2 2 1 ) 0.8051
3 3 47 ( 15 15 17 ) 4.109e+004
3 3 92 ( 29 32 31 ) 41.89
N S Q q s R
3 4 4 ( 2 1 1 ) ( 1 2 1 ) 0.6918
3 5 4 ( 2 2 1 ) ( 1 2 1 ) 0.7329
3 6 4 ( 2 2 2 ) ( 1 2 1 ) 0.7647
3 7 4 ( 3 2 2 ) ( 1 2 1 ) 0.7906
3 4 5 ( 1 1 2 ) ( 2 2 1 ) 0.8447
3 5 5 ( 1 1 3 ) ( 2 2 1 ) 0.8698
3 6 5 ( 1 1 4 ) ( 2 2 1 ) 0.8872
3 7 5 ( 1 1 5 ) ( 2 2 1 ) 0.8999
3 4 6 ( 2 1 1 ) ( 2 2 2 ) 1.037
3 5 6 ( 3 1 1 ) ( 2 2 2 ) 1.09
3 6 6 ( 3 1 2 ) ( 2 2 2 ) 1.134
3 7 6 ( 3 2 2 ) ( 2 2 2 ) 1.181
4 5 5 ( 1 1 1 2 ) ( 1 2 1 1 ) 0.6008
4 6 5 ( 2 1 1 2 ) ( 1 2 1 1 ) 0.6323
4 7 5 ( 2 2 1 2 ) ( 1 2 1 1 ) 0.6607
4 8 5 ( 2 2 1 3 ) ( 1 2 1 1 ) 0.687
4 5 6 ( 1 1 1 2 ) ( 2 2 1 1 ) 0.7065
4 6 6 ( 1 1 1 3 ) ( 2 2 1 1 ) 0.7385
4 7 6 ( 1 1 2 3 ) ( 2 2 1 1 ) 0.7648
4 8 6 ( 1 1 2 4 ) ( 2 2 1 1 ) 0.786
4 5 7 ( 1 1 1 2 ) ( 2 2 2 1 ) 0.817
4 6 7 ( 1 1 1 3 ) ( 2 2 2 1 ) 0.8403
4 7 7 ( 1 1 2 3 ) ( 2 2 2 1 ) 0.8569
4 8 7 ( 1 2 2 3 ) ( 2 2 2 1 ) 0.8737
4 5 8 ( 2 1 1 1 ) ( 2 2 2 2 ) 0.9762
4 6 8 ( 3 1 1 1 ) ( 2 2 2 2 ) 1.019
4 7 8 ( 3 1 1 2 ) ( 2 2 2 2 ) 1.055
4 8 8 ( 3 1 2 2 ) ( 2 2 2 2 ) 1.093
N S Q q s R
5 6 6 ( 1 1 1 1 2 ) ( 1 2 1 1 1 ) 0.5304
5 7 6 ( 1 1 1 2 2 ) ( 1 2 1 1 1 ) 0.5639
5 8 6 ( 2 1 1 2 2 ) ( 1 2 1 1 1 ) 0.5884
5 9 6 ( 2 2 1 2 2 ) ( 1 2 1 1 1 ) 0.6097
5 6 7 ( 1 1 1 1 2 ) ( 2 2 1 1 1 ) 0.5984
5 7 7 ( 1 1 1 2 2 ) ( 2 2 1 1 1 ) 0.6426
5 8 7 ( 1 1 1 2 3 ) ( 2 2 1 1 1 ) 0.6669
5 9 7 ( 1 1 1 3 3 ) ( 2 2 1 1 1 ) 0.6913
5 6 8 ( 1 1 1 2 1 ) ( 2 2 1 2 1 ) 0.6939
5 7 8 ( 1 1 1 2 2 ) ( 2 2 1 2 1 ) 0.7218
5 8 8 ( 1 1 1 2 3 ) ( 2 2 2 1 1 ) 0.7468
5 9 8 ( 1 1 1 2 4 ) ( 2 2 2 1 1 ) 0.7665
5 6 9 ( 2 1 1 1 1 ) ( 2 2 2 2 1 ) 0.8065
5 7 9 ( 2 1 1 1 2 ) ( 2 2 2 2 1 ) 0.8463
5 8 9 ( 2 1 1 1 3 ) ( 2 2 2 2 1 ) 0.8716
5 9 9 ( 2 1 1 1 4 ) ( 2 2 2 2 1 ) 0.889
5 6 10 ( 2 1 1 1 1 ) ( 2 2 2 2 2 ) 0.9262
5 7 10 ( 3 1 1 1 1 ) ( 2 2 2 2 2 ) 0.9611
5 8 10 ( 3 1 1 1 2 ) ( 2 2 2 2 2 ) 0.9916
5 9 10 ( 3 1 1 2 2 ) ( 2 2 2 2 2 ) 1.024
Q q R T
11 1 1 1 1 1 1 1 2 2 0.3735 311
12 1 1 1 1 1 1 2 2 2 0.3876 299
13 1 1 1 1 1 2 2 2 2 0.4024 282
14 1 1 1 1 2 2 2 2 2 0.4179 291
15 1 1 1 2 2 2 2 2 2 0.4337 287
16 1 1 2 2 2 2 2 2 2 0.4496 491
17 1 2 2 2 2 2 2 2 2 0.4658 135
18 2 2 2 2 2 2 2 2 2 0.4761 338
19 2 2 2 2 2 2 2 2 3 0.4861 429
20 2 2 2 2 2 2 2 3 3 0.4964 374
21 2 2 2 2 2 2 3 3 3 0.5071 342
Q q R T
11 1 1 1 1 1 1 1 2 2 0.3735 1
12 1 1 1 1 1 1 2 2 2 0.3876 2
13 1 1 1 1 1 2 2 2 2 0.4024 6
14 1 1 1 1 2 2 2 2 2 0.4179 15
15 1 1 1 2 2 2 2 2 2 0.4337 37
16 1 1 2 2 2 2 2 2 2 0.4496 78
17 1 2 2 2 2 2 2 2 2 0.4658 155
18 2 2 2 2 2 2 2 2 2 0.4761 294
Q q R T
16 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 0.281 843
17 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 0.288 817
18 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 0.2954 880
19 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 0.3031 849
20 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 0.3113 870
21 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 0.3198 836
22 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 0.3287 705
23 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 0.338 748
24 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 0.3475 763
25 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 0.3572 862
26 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 0.3669 819
27 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 0.3765 740
28 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 0.3858 1326
29 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.3947 425
30 1 2 2 2 2 2 2 2 2 2 2 2 2 2 3 0.4003 1290
31 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 0.406 1442
32 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 0.412 1196
33 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 0.4182 1155
34 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 0.4246 1059
35 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 0.4311 1000
36 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 0.4378 1009
37 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 0.4446 881
38 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 0.4514 869
39 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 0.4582 815
40 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 0.465 785
41 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 0.4716 830
42 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 0.4779 852
43 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 0.4837 748
44 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 0.489 803
45 2 3 3 3 3 3 3 3 3 3 3 3 3 3 4 0.4937 1051
Q q R T
16 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 0.281 0
17 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 0.288 2
18 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 0.2954 12
19 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 0.3031 54
20 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 0.3113 208
N q R T
4 3 1 2 2 1.093 55
5 3 1 2 2 2 1.057 100
6 3 1 2 2 2 2 1.025 132
7 3 1 2 2 2 2 2 0.9976 170
8 3 1 2 2 2 2 2 2 0.9728 235
10 3 1 2 2 2 2 2 2 2 2 0.93 347
20 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.7932 1315
30 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.7152 2313
40 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.6626 4174
50 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.6237 6495
60 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.5933 10075
N q R T
4 2 2 2 2 1.077 1
5 2 2 2 2 2 1.043 1
N w R T
4 1.2 0.933 0.943 0.926 1.09 103
5 1.21 0.943 0.942 0.946 0.959 1.056 148
6 1.23 0.958 0.958 0.963 0.946 0.947 1.025 193
7 1.23 0.961 0.957 0.968 0.957 0.962 0.966 0.9974 255
8 1.23 0.951 0.967 0.962 0.965 0.976 0.972 0.974 0.9727 316
10 1.24 0.978 0.982 0.972 0.964 0.983 0.97 0.968 0.967 0.974 0.9301 465
20 1.26 1 0.996 0.988 0.981 0.982 0.975 0.981 0.973 0.991 0.987 1 0.983 0.995 0.985 0.987 0.979 0.987 0.984 0.984 0.7933 1501
30 1.27 0.971 0.974 0.989 0.985 0.978 0.992 0.974 1 0.986 0.996 0.983 0.976 0.983 0.981 0.984 0.99 0.998 1.01 1.02 0.988 0.986 1 0.982 1.01 0.984 0.984 1.01 1.01 1 0.7153 2822
40 1.26 0.977 1 0.994 0.995 0.968 0.976 1.02 1 1.01 0.984 0.988 1 0.985 1.01 0.982 0.988 0.984 1.01 0.98 0.991 0.991 0.994 1 0.98 0.991 0.998 0.997 0.985 1.02 1.01 0.987 1.01 0.987 1.01 0.997 1.02 0.982 0.981 0.973 0.6625 4501
50 1.26 1 0.988 0.985 0.994 0.998 0.964 0.975 0.998 1 0.986 0.956 0.97 1 0.977 1.03 0.993 0.982 0.969 0.98 1.01 0.988 0.997 0.996 0.998 0.994 1 1 1.01 0.994 1.01 0.979 0.99 0.997 1.01 0.995 0.981 0.98 0.982 1.02 0.973 1.01 1.03 1.01 1.01 1.01 1.01 0.986 1.01 0.991 0.6235 6389
60 1.28 0.972 0.964 0.966 0.968 0.972 1.02 0.973 1.02 1 0.983 0.98 0.989 0.997 0.977 0.992 0.982 0.98 1.02 0.948 1 0.968 0.989 1.06 1.01 0.994 1.03 0.96 0.995 1.01 1 1.08 0.981 0.967 0.995 1.03 1.01 0.998 1.02 0.991 0.975 0.988 0.986 0.961 1.01 1.02 1.01 0.99 0.976 0.984 1.01 0.997 1.01 0.994 1 1 1 0.983 1.01 1.02 0.5928 11659
N s R T
4 2 2 2 2 1.077 21
5 2 2 2 2 2 1.043 25
6 2 2 2 2 2 2 1.013 32
7 2 2 2 2 2 2 2 0.9866 44
8 2 2 2 2 2 2 2 2 0.9629 60
10 2 2 2 2 2 2 2 2 2 2 0.9218 124
20 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.789 460
30 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.7126 920
40 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.6607 1867
50 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.6223 2788
60 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.5921 4915
N s R T
4 2 2 2 2 1.077 1
5 2 2 2 2 2 1.043 26
N q, w R T
4 q: 3 1 2 2 1.098 126
" w: 1.08 1.05 0.936 0.935 " "
5 q: 3 1 2 2 2 1.062 181
" w: 1.08 1.07 0.949 0.959 0.938 " "
6 q: 3 1 2 2 2 2 1.031 244
" w: 1.1 1.07 0.96 0.943 0.965 0.961 " "
7 q: 3 1 2 2 2 2 2 1.003 319
" w: 1.11 1.07 0.965 0.958 0.957 0.967 0.964 " "
8 q: 3 1 2 2 2 2 2 2 0.9773 401
" w: 1.12 1.07 0.979 0.972 0.963 0.958 0.972 0.969 " "
10 q: 3 1 2 2 2 2 2 2 2 2 0.9339 597
" w: 1.12 1.09 0.969 0.982 0.979 0.983 0.958 0.982 0.968 0.974 " "
20 q: 3 2 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.7945 1937
" w: 1.11 0.975 1.09 0.984 1 0.997 0.976 0.988 1 0.974 0.992 0.988 0.997 0.979 1 0.982 0.978 0.987 0.995 0.993 " "
30 q: 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.7164 3871
" w: 1.14 1.09 0.984 0.973 0.973 0.982 0.998 1 1 0.981 0.976 0.99 0.994 1 0.999 1.02 0.983 0.986 0.98 0.988 1 0.991 0.986 1 1.01 0.981 1.01 1.02 0.977 0.98 " "
50 q: 3 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 2 2 0.6241 9290
" w: 1.15 1.13 1.11 0.992 0.982 0.981 0.942 1.01 0.997 0.986 0.991 0.987 0.995 0.975 0.977 0.976 0.978 0.952 1 1.03 1 1.02 1.02 0.987 0.996 1.01 1 0.968 1.01 1.01 0.984 1.01 1.02 1.02 1.01 0.988 0.993 1 1.01 0.985 1 0.999 1.03 0.995 0.962 1.02 0.99 0.833 1.01 0.991 " "
60 q: 3 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.5934 12742
" w: 1.13 1.06 1.08 0.971 0.987 0.985 0.97 0.978 1.01 0.977 0.983 0.982 0.991 1 1 1.02 0.992 0.981 0.985 0.994 1.01 1.01 1.02 1 0.984 1.01 1.01 0.981 0.996 0.975 0.994 1.02 0.99 0.992 0.826 1.01 0.987 1.04 1 1.02 0.99 1.02 0.985 0.99 1 0.958 1.01 1.01 1.02 1.01 1 1.04 0.999 0.987 1.02 1.02 1.02 0.991 1.01 0.998 " "
N q, s R T
4 q: 3 1 2 2 1.093 83
" s: 2 2 2 2 " "
5 q: 3 1 2 2 2 1.057 117
" s: 2 2 2 2 2 " "
6 q: 3 1 2 2 2 2 1.025 144
" s: 2 2 2 2 2 2 " "
7 q: 3 1 2 2 2 2 2 0.9976 201
" s: 2 2 2 2 2 2 2 " "
8 q: 3 1 2 2 2 2 2 2 0.9728 279
" s: 2 2 2 2 2 2 2 2 " "
10 q: 3 1 2 2 2 2 2 2 2 2 0.93 360
" s: 2 2 2 2 2 2 2 2 2 2 " "
20 q: 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.7932 1152
" s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 " "
30 q: 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.7152 2434
" s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 " "
40 q: 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.6626 4713
" s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 " "
50 q: 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.6237 7244
" s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 " "
60 q: 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.5933 12114
" s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 " "
N q, s R T
4 q: 3 1 2 2 1.093 25
" s: 2 2 2 2 " "
5 q: 3 1 2 2 2 1.057 828
" s: 2 2 2 2 2 " "
N s, w R T
4 s: 2 2 2 2 1.091 151
" w: 1.19 0.935 0.94 0.938 " "
5 s: 2 2 2 2 2 1.056 215
" w: 1.21 0.94 0.946 0.959 0.944 " "
6 s: 2 2 2 2 2 2 1.025 288
" w: 1.22 0.943 0.954 0.961 0.965 0.956 " "
7 s: 2 2 2 2 2 2 2 0.9974 362
" w: 1.22 0.948 0.977 0.958 0.969 0.959 0.966 " "
8 s: 2 2 2 2 2 2 2 2 0.9727 453
" w: 1.24 0.96 0.966 0.962 0.966 0.958 0.975 0.969 " "
10 s: 2 2 2 2 2 2 2 2 2 2 0.9301 746
" w: 1.25 0.961 0.964 0.972 0.964 0.969 0.989 0.976 0.975 0.982 " "
20 s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.7933 2120
" w: 1.26 0.987 0.972 0.977 0.98 0.987 0.975 0.99 0.968 0.994 0.989 0.985 0.981 0.986 1 1 0.98 0.997 0.988 1 " "
30 s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.7152 4326
" w: 1.28 0.983 0.981 0.99 0.97 0.999 0.991 0.993 0.991 1 1 0.965 0.995 0.977 0.98 0.991 0.98 1 0.984 0.977 1.01 0.988 0.991 0.994 0.993 0.96 1.03 1.01 0.994 0.997 " "
50 s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.6235 10130
" w: 1.26 0.981 0.986 0.972 0.963 0.981 0.939 0.996 0.97 0.982 0.968 0.994 0.989 0.976 0.991 0.993 1.01 1.02 1.02 0.988 0.974 1 0.987 0.978 0.979 1 1.01 1.02 1.02 0.999 0.994 0.994 0.997 0.986 1.02 1.03 1.02 1.01 1.02 1 0.988 0.982 1 0.997 1.01 1.01 0.996 0.991 0.991 1.02 " "
60 s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.593 13943
" w: 1.28 0.99 0.988 0.972 0.949 0.984 0.952 0.955 0.973 0.978 0.997 1.03 0.975 0.992 1.01 0.971 0.965 1.03 0.994 0.982 0.965 0.997 0.967 1.01 0.995 0.983 0.974 1.01 0.996 1.03 0.998 1.01 1.02 1 0.98 0.978 0.996 0.983 0.967 1 1.01 1 1 1.01 0.987 0.979 1.03 1 0.987 1 1.01 1.03 1.02 1.01 1.02 1.03 1.03 0.99 1 1.02 " "
N q, s, w R T
4 q: 3 1 2 2 1.098 151
" s: 2 2 2 2 " "
" w: 1.07 1.05 0.934 0.945 " "
5 q: 3 1 2 2 2 1.062 218
" s: 2 2 2 2 2 " "
" w: 1.1 1.06 0.951 0.95 0.941 " "
6 q: 3 1 2 2 2 2 1.031 293
" s: 2 2 2 2 2 2 " "
" w: 1.1 1.06 0.955 0.958 0.962 0.958 " "
7 q: 3 1 2 2 2 2 2 1.003 376
" s: 2 2 2 2 2 2 2 " "
" w: 1.11 1.07 0.966 0.962 0.963 0.964 0.961 " "
8 q: 3 1 2 2 2 2 2 2 0.9774 480
" s: 2 2 2 2 2 2 2 2 " "
" w: 1.11 1.08 0.97 0.965 0.968 0.961 0.973 0.975 " "
10 q: 3 1 2 2 2 2 2 2 2 2 0.9339 709
" s: 2 2 2 2 2 2 2 2 2 2 " "
" w: 1.11 1.08 0.977 0.98 0.955 0.975 0.984 0.973 0.98 0.982 " "
20 q: 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 1 3 0.7867 2332
" s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 2 1 " "
" w: 1.12 1.09 0.97 0.975 0.956 0.984 0.972 0.965 0.964 0.97 0.976 0.983 0.972 0.969 0.983 0.963 0.974 0.794 0.989 1.43 " "
30 q: 3 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 0.7164 4866
" s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 " "
" w: 1.13 1.09 0.975 0.998 0.978 0.98 0.998 1.01 0.975 0.998 0.996 1.01 0.974 0.988 1.02 0.975 0.993 0.992 0.978 1.01 0.985 0.99 1 0.991 0.967 1.01 0.993 0.996 1 1.01 " "
50 q: 3 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 1 2 2 2 2 3 2 3 0.6219 11680
" s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 2 2 2 2 2 2 2 1 " "
" w: 1.16 1.12 1.11 0.994 0.971 0.973 0.946 0.995 0.952 0.975 0.965 0.969 0.988 0.975 0.997 0.979 0.952 1.01 1.01 0.995 0.979 1.02 0.997 0.993 1 1.01 0.988 0.999 0.99 0.977 1.03 1.01 1.02 0.985 0.981 0.998 0.988 0.986 1.03 0.981 0.983 0.816 1.02 0.992 0.974 1.01 0.996 0.818 1 1.4 " "
60 q: 3 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 2 2 2 2 2 2 2 2 2 3 0.5919 16632
" s: 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 1 " "
" w: 1.15 1.13 1.09 0.963 0.952 0.983 0.993 0.995 1 0.997 0.984 0.996 1.02 0.958 0.999 1.01 0.975 0.97 0.974 1.02 0.967 0.987 1.01 0.806 1.01 0.998 0.977 0.986 1 0.969 0.968 0.999 0.983 1.03 1.04 0.996 0.985 0.981 1.05 0.999 1.01 0.996 0.969 1.04 0.98 0.989 0.988 1.01 0.988 0.806 0.997 1.03 0.997 1.02 0.955 1.02 0.983 1 0.968 1.39 " "