January 9, 2006 1527 WSPCTrim Size 11in x 8.5in for Proceedings linnemann SOFTWARE FOR STAT
On the Frame Fixing in Quantum Gravity

a r Xiv:g r-qc/41127v 13Jan24February 4,20081:40WSPC/Trim Size:9.75in x 6.5in for Proceedings main ON THE FRAME FIXING IN QUANTUM GRA VITY S.MERCURI ICRA —International Center for Relativistic Astrophysics G.MONTANI ICRA —International Center for Relativistic Astrophysics Dipartimento di Fisica,Universit`a di Roma “La Sapienza”,Piazzale Aldo Moro 5,I-00185,Roma,Italy We provide a discussion about the necessity to fix the reference frame before quantizing the gravitational field.Our presentation is based on stressing how the 3+1-slicing of the space time becomes an ambiguous procedure as referred to a quantum 4-metric.In the Wheeler-DeWitt (WDW)approach 3,the quantization of gravity is per-formed in the canonical way,starting from the Arnowitt-Deser-Misner (ADM)ac-tion.The use of the ADM formalism 1is justified by the necessity to obtain Hamil-tonian constraints,but the straightforward quantization of such (3+1)-picture con-tains some relevant ambiguities.In fact,the aim of the WDW approach is to quantize the gravitational field in a particular representation and its outcoming provides essentially information on the quantum dynamics of the 3-metric tensordefined on spatial hypersurfaces.To use the ADM splitting is equivalent to a kind of “gauge fixing”,because it is pre-served only under restricted coordinates transformations (time displacements and 3-diffeomorphisms);the point here is that the “gauge fixing”depends on the field we are quantizing and therefore the canonical approach seems to be an ambiguous procedure.Since in the ADM action the conjugate momenta,πand πi ,respectively to the lapse function N and to the shift vector N i are constrained to vanish,then,on a quantum level,the wave functional of the system does not depend on the lapse function and on the shift vector.The ambiguity relies on regarding as equivalent the fully covariant approach and the “gauge fixed”ADM one,in fact passing from g µνto ADM variables involves a metric dependent procedure,in the sense that we must be able to define a unit time-like normal field n µ(g µνn µn ν=−1),which ensures the space-like nature of h ij (in this respect we recall that h ij≡g µν∂i y µ∂j y νcorresponds to the spatial components of the 4-tensor h µν=g µν+n µn ν).Now the following question arises:how is it possible to speak of a unit time-like normal field1February4,20081:40WSPC/Trim Size:9.75in x6.5in for Proceedings main2for a quantum space-time?Indeed such a notion can be recognized,in quantum regime,at most in the sense of expectation values;therefore assuming the existence of nµbefore quantizing the system dynamics makes the WDW approach physically ill defined.Our point of view is that the canonical quantization of the gravitationalfield can be performed in a(3+1)-picture only if we add,to such a scheme,some information about the existence of the time-like normalfield,as shown in7,5,this result can be achieved by including in the dynamics the kinematical action4,already adopted to quantize“matter”fields on afixed background4.The physical interpretation of such new term either on a classical as well as on a quantum level leads to recognize the existence of a referencefluid and in this sense the analysis of7,5,6converges with the literature on the framefixing problem(see2and references therein).We observe that to include the kinematical action can be regarded as a consequence of fixing in the gravity action the lapse function and the shift vector and,therefore, to choose four independent components of the gravitationalfield,which is just the outcoming of the framefixing.A more physical manner to ensure the existence of a time-like vector consistsoffilling the space time with afluid which plays the role of real reference frame.Here we discuss on a phenomenological ground,the canonical quantization of the gravitationalfield plus a dust referencefluid,outlining some relevant differences between the classical and quantum behavior of this system.The Einstein equations and the conservation law,for the coupled gravity-fluid sys-tem,take the formGµν=χεuµuν,uν∇νuµ=0,∇ν(εuν)=0,(1) where Gµνandχdenotes respectively the Einstein tensor and constant.Remembering a well-known result,it is easy to show that the following relations take place8Gµνuµuν=−H(h ij,p ij)h=χε,Gµνuµhνi=H i(h ij,p ij)h=0.(2)Here h ij(ij=1,2,3)denotes the3-metric of the spatial hypersurfaces orthogo-nal to uµand p ij its conjugate momenta,while H and H i refer respectively to the super-Hamiltonian and to the super-momentum of the gravitationalfield.The above relations hold if we make reasonable assumption that the conjugate momen-tum p ij is not affected by the matter variables(i.e.thefluid term in ADM formalism should not contain the time derivative of the3-metric tensor).Only the Hamilto-nian constraints are relevant for the quantization procedure and,in the comoving frame,when the4-velocity becomes uµ={1,0}(N=1N i=0),we have to retain also the conservation lawε√February4,20081:40WSPC/Trim Size:9.75in x6.5in for Proceedings main3 Thus,when the coordinates system becomes a real physical frame,the Hamiltonianconstraints readH=ω(x i)H i=0.(3) Now,to assign a Cauchy problem for such a system,for which equations(3)play therole of constraints on the Cauchy data,corresponds to provide on a(non-singular)space-like hypersurface,sayΣ(0),the values{h(0)ij,p(0)ij,ε(0)};from these values ω(0)can be calculated by(3).It follows that,by specifying a suitable initial condition,the value ofω(0)can bemade arbitrarily small;from the constraints point of view,a very small value ofω(0)means,if h(0)is not so,that thefluid becomes a test one(beingωa constant ofthe motion);we emphasize that forfinite values ofω,h should not vanish to avoidunphysical diverging energy density of thefluid.The canonical quantization of this system is achieved as soon as we implementthe canonical variables into quantum operators and annihilate the state functionalΨvia the Hamiltonian operator constraints.Thus the quantum dynamics obeysthe following eigenvalue problem:HΨ({hij},ω)=ωΨ({h ij},ω),(4) where{h ij}refers to a whole class of3-geometries,so that the super-momentum constraint holds automatically.We stress how the above result is equivalent to the eigenvalues problem obtainedin7.In the above equation(4),the spatial functionωplays the role of the super-Hamiltonian eigenvalue;in this respect,we observe how its values can no longerbe assigned by the initial values,but they have to be determined via the spectrumof H.We conclude that,in the quantum regime,a real dust referencefluid never approaches a test system.Moreover the presence of non zero eigenvalues for the super-Hamiltonian removesthe so called“frozen formalism”of the WDW equation and confirms the idea thatintroducing a physical unit time like vector provides a consistent and evolutivecanonical quantum gravity dynamics.References1.R.Arnowitt,S.Deser,C.Misner,(1959),Phys.Rev.116,1322.2.J.Bicak,K.Kuchaˇr,(1997),Phys.Rev.D56,4878.3. B.S.DeWitt,(1967),Phys.Rev.160,1113.4.K.Kuchaˇr,Canonical Methods of Quantization,(1981),‘Quantum Gravity2:A Sec-ond Oxford Symposium’,Clarendon Press,Oxford,pp.329-374.5.S.Mercuri,G.Montani,(2003),to appear on Int.Jour.Mod.Phys.D,available ong r-qc/0310077.6.S.Mercuri,G.Montani,(2003),submitted to Class.Quant.Grav.,available on g r-qc/0312077.7.G.Montani,(2002),Nucl.Phys.B634,370.8.T.Thiemann,(2001),available gr-qc/0110034.。
DYNAMICAL SYSTEMS, STABILITY, AND CHAOS

In this expository and resources chapter we review selected aspects of the mathematics of dynamical systems, stability, and chaos, within a historical framework that draws together two threads of its early development: celestial mechanics and control theory, and focussing on qualitative theory. From this perspective we show how concepts of stability enable us to classify dynamical equations and their solutions and connect the key issues of nonlinearity, bifurcation, control, and uncertainty that are common to time-dependent problems in natural and engineered systems. We discuss stability and bifurcations in three simple model problems, and conclude with a survey of recent extensions of stability theory to complex networks.
a The
Greek word for governor is kubernetes, from which the mathematician Norbert Wiener (1894–1964) coined the term cybernetics as a name for the collective field of automated control and information theory.
ISO16750-1-2006

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6.1 General................................................................................................................................................... 4
6.4 Class C ................................................................................................................................................... 5
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_计算机应用基础_网上考试系统的设计

收稿日期:2006-02-10作者简介:张 巍(1979—),男,洛阳工业高等专科学校教师。
《计算机应用基础》网上考试系统的设计张 巍,赵震伟(洛阳工业高等专科学校,河南洛阳471003) 摘要:介绍《计算机应用基础》网上考试系统的设计方案。
该系统利用ASP 技术实现了题库管理、题目的自动生成、考生成绩查询等功能。
关键词:计算机应用基础;ASP ;考试系统中图分类号:TP311 文献标识码:A 文章编号:1671-7864(2006)04-0019-03 《计算机应用基础》课程网上考试能够使教师提高阅卷速度和工作效率。
该考试系统由计算机随机抽题、组题,增强了试卷的保密性、客观性和公平性。
1 《计算机应用基础》考试系统模块设计本系统分为四个子系统:用户登录与注册、学生子系统、教师子系统和管理员子系统。
1.1 用户登陆与注册模块本模块在考试之前收集考生信息———姓名、性别、身份证号、考号和考试时间等,用于验证考生身份,将数据存入考生数据库作为考试原始记录。
如图1所示。
图1 用户登录与注册模块1.2 学生子系统主要功能是实现学生网上考试和成绩查询。
本系统功能如图2所示。
图2 学生子系统1.2.1 考试模块(1)登录考试在登录界面(图3)输入考生考号、姓名和班级,检查无误后可进入抽题界面(图4)。
图3 登录界面图4 抽题界面 (2)取得不同试卷根据不同IP 地址,系统自动抽取不同试卷,使相邻N 个同学的试卷各异,防止考试作弊行为。
(3)计时功能当学生开始考试时,计时器由预先设定的考试第5卷 第4期漯河职业技术学院学报(综合版)V ol.5N o 14 2006年10月Journal of Luohe V ocational and T echnical C ollege (C omprehensive )Oct 12006时间(60分钟)开始倒计时,试卷上显示剩余时间。
(4)保存答案选择题、判断题和汉字录入题通过点击按钮存盘;Windows 操作题和W ord 、Excel 通过文件菜单的保存命令存盘(注意:默认路径存盘)。
2006年11月5日

KPMG - Invitation for Aptitude Test - UESTC 时间: 2006年11月5日 (星期日) 上午10:30
算器及身份证或学生证。
所有在网上递交申请的同学请届时带上成绩单复印件、简历(附照片)。
KPMG - Invitation for Aptitude Test - UESTC
时间: 2006年11月5日 (星期日) 下午12:30
算器及身份证或学生证。
所有在网上递交申请的同学请届时带上成绩单复印件、简历(附照片)。
KPMG - Invitation for Aptitude Test - UESTC
时间: 2006年11月5日 (星期日) 下午12:30
算器及身份证或学生证。
所有在网上递交申请的同学请届时带上成绩单复印件、简历(附照片)。
成绩单复印件、简历(附照
成绩单复印件、简历(附照
成绩单复印件、简历(附照。
天气预报的业务技术进展

天气预报的业务技术进展矫梅燕龚建东周兵赵声蓉(国家气象中心,北京100081)摘要该文总结回顾了中央气象台近年来的天气预报业务技术进展。
天气预报质量的历史演变显示了预报业务水平的提高,这种业务能力的提高既反映了预报技术的发展,也带来了天气预报业务的变化。
对业务天气预报中各种预报技术应用进展的分析表明:数值预报在天气预报业务能力提高中发挥着重要的基础性作用;同时,基于对不同尺度天气影响系统发展演变过程深入认识的基础上,天气学的预报方法依然是预报业务中的重要技术方法;动力诊断预报已成为灾害性天气预报中的重要手段之一,数值预报产品的解释应用是实现气象要素精细定量预报的技术途径。
关键词:预报业务技术进展;数值预报;天气学预报;动力诊断引言近年来,在谈到天气预报业务技术发展时,人们几乎把主要的关注点放在了数值预报的发展方面。
正如全球大气研究计划中的TH ORPEX科学计划的报告中一句令人印象深刻的话/数值预报的成功是20世纪最重大的科技和社会进步之一0[1]。
数值天气预报已经成为现代天气预报的基础和天气预报业务发展的主流方向,正是由于数值预报的发展,使天气形势预报的可用时效超过了7d。
但是还应该看到,目前的数值预报能力不能完全解决天气预报业务中的各种需求,因此,天气预报业务中在强调以数值预报为基础的同时,也提出要综合应用多种资料和多种技术方法的预报技术路线。
在目前的天气预报业务中,在数值预报基础上的天气学预报方法,无时无刻不通过预报员体现在其预报业务实践中,特别是在重大灾害性天气预报中发挥着重要作用;基于数值预报的解释应用技术、集合预报技术以及动力诊断预报技术在灾害性天气预报中正越来越受到重视。
本文拟结合中央气象台的预报业务实际,对近年来天气预报业务能力和各种预报技术的应用进展作一个简要回顾总结。
1天气预报的业务水平分析1.1降水的业务预报水平降水预报是天气预报业务的重点内容之一。
评估降水预报水平,一是对降水的总体预报水平,即不论降雨量的大小,有降水发生的预报能力;二是对小雨、中雨、大雨、暴雨等的分级降水的预报水平,即定量降水的预报能力。
2004 improvement and validation of a model for photovoltaic array performance
Improvement and validation of a model for photovoltaic array performanceW.De Soto,S.A.Klein *,W.A.BeckmanSolar Energy Laboratory,University of Wisconsin-Madison,1500Engineering Drive,Madison,WI 53706,USAReceived 20December 2004;received in revised form 21June 2005;accepted 21June 2005Available online 16August 2005Communicated by:Associate Editor Arturo Morales-AcevedoAbstractManufacturers of photovoltaic panels typically provide electrical parameters at only one operating condition.Pho-tovoltaic panels operate over a large range of conditions so the manufacturer Õs information is not sufficient to determine their overall performance.Designers need a reliable tool to predict energy production from a photovoltaic panel under all conditions in order to make a sound decision on whether or not to incorporate this technology.A model to predict energy production has been developed by Sandia National Laboratory,but it requires input data that are normally not available from the manufacturer.The five-parameter model described in this paper uses data provided by the manufac-turer,absorbed solar radiation and cell temperature together with semi-empirical equations,to predict the current–volt-age curve.This paper indicates how the parameters of the five-parameter model are determined and compares predicted current–voltage curves with experimental data from a building integrated photovoltaic facility at the National Institute of Standards and Technology (NIST)for four different cell technologies (single crystalline,poly crystalline,silicon thin film,and triple-junction amorphous).The results obtained with the Sandia model are also shown.The predictions from the five-parameter model are shown to agree well with both the Sandia model results and the NIST measurements for all four cell types over a range of operating conditions.The five-parameter model is of interest because it requires only a small amount of input data available from the manufacturer and therefore it provides a valuable tool for energy predic-tion.The predictive capability could be improved if manufacturer Õs data included information at two radiation levels.Ó2005Elsevier Ltd.All rights reserved.Keywords:Photovoltaic cells;PV cells;Performance;I –V curves;Prediction;Solar energy1.IntroductionThe electrical power output from a photovoltaic panel depends on the incident solar radiation,the celltemperature,the solar incidence angle and the load resis-tance.Manufacturers typically provide only limited operational data for photovoltaic panels,such as the open circuit voltage (V oc ),the short circuit current (I sc ),the maximum power current (I mp )and voltage (V mp ),the temperature coefficients at open circuit volt-age and short circuit current (b V oc and a I sc ,respectively),and the nominal operating cell temperature (NOCT).These data are available only at standard rating0038-092X/$-see front matter Ó2005Elsevier Ltd.All rights reserved.doi:10.1016/j.solener.2005.06.010*Corresponding author.Tel.:+16082635626;fax:+16082628464/9.E-mail address:klein@ (S.A.Klein).Solar Energy 80(2006)78–88conditions(SRC),for which the irradiance is1000W/m2 and the cell temperature(T c)is25°C(except for the NOCT which is determined at800W/m2and an ambi-ent temperature of20°C).These conditions produce high power output,but are rarely encountered in actual operation.The results of this study were obtained using panel performance at SRC.Accurate,reliable,and easy to apply methods for predicting the energy production of photovoltaic panels are needed to identify optimum photovoltaic systems.The model developed by King (2000)and King et al.(1998,2004)accurately predicts energy production with an algebraically simple model, but it requires parameters that are normally not avail-able from the manufacturer.A database of the model parameters for many different array types is provided by Sandia National Laboratories(2002).A model that uses the only data provided by manufacturers to predict energy production is presented in this paper.2.The current–voltage relationship for a photovoltaic deviceThe electrical power available from a photovoltaic (PV)device can be modeled with the well known equiv-alent circuit shown in Fig.1(Duffie and Beckman,1991; Nelson,2003).This circuit includes a series resistance and a diode in parallel with a shunt resistance.ThisNomenclaturea ideality factor parameter defined asa N s n I kT c/q(eV)a0–4coefficients for air mass modifier in Eq.(17) a ref ideality factor parameter at SRC(eV)AM air massb0–5coefficients for incidence angle modifier in Eq.(13)E g energy bandgap(eV)E g;Tref energy bandgap at reference temperature (1.121eV for silicon)(eV)G total irradiance on horizontal surface(W/m2)G b beam component of total irradiance on hor-izontal surface(W/m2)G d diffuse component of total irradiance onhorizontal surface(W/m2)G ref irradiance at SRC(1000W/m2)(W/m2)I current(A)I L light current(A)I L,ref light current at SRC(A)I mp current at maximum power point(A)I mp,ref current at maximum power point at SRC(A)I o diode reverse saturation current(A)I o,ref diode reverse saturation current at SRC(A) I sc,ref short circuit current at SRC(A)k BoltzmannÕs constant(1.38066E–23J/K)K glazing extinction coefficient(1/m)K sa incidence angle modifier at beam incidence angle hK sa,d incidence angle modifier for diffuse compo-nentK sa,g incidence angle modifier for ground reflected componentL thickness of transparent cover(m)M air mass modifier M ref air mass modifier at SRC and air mass1.5 NOCT nominal operating cell temperature(K)n refractive indexn I ideality factorn D diode factor(in KingÕs model)N s number of cells in seriesP predicted power(W)P mp maximum power(W)q electron charge(1.60218E–19Coulomb)R beam ratio of beam radiation on tilted surface to that on a horizontal surfaceR s series resistance(X)R s,ref series resistance at SRC(X)R sh shunt resistance(X)R sh,ref shunt resistance at SRC(X)S total absorbed irradiance(W/m2)S ref total absorbed irradiance at SRC(W/m2) T c cell temperature(K)T c,ref cell temperature at SRC(K)V voltage(V)V mp voltage at maximum power point(V)V mp,ref voltage at maximum power point at SRC (V)V oc,ref open circuit voltage at SRC(V)a Imptemperature coefficient for maximum powercurrent(A/K)a Isctemperature coefficient for short circuit cur-rent(A/K)b slope of the panel(°)b Vocopen voltage temperature coefficient(V/K) e material band gap energy(eV)h incidence angle,angle between the beam oflight and the normal to the panel surface(°) h r angle of refraction(°)q ground reflectances(h)transmittance of glazing system at angle hW.De Soto et al./Solar Energy80(2006)78–8879circuit can be used either for an individual cell,for a module consisting of several cells,or for an array con-sisting of several modules (Duffie and Beckman,1991).The current–voltage relationship at a fixed cell perature and solar radiation for the circuit in Fig.1is expressed in Eq.(1).Five parameters must be known in order to determine the current and voltage,and thus the power delivered to the load.These are:the light cur-rent I L ,the diode reverse saturation current I o ,the series resistance R s ,the shunt resistance R sh ,and the modified ideality factor a defined in Eq.(2).I ¼I L ÀI o eV þIR s a À1h i ÀV þIRsR sh ð1Þwhere aN s n I kT c qð2ÞThe electron charge q ,and Boltzmann Õs constant k are known,n I is the usual ideality factor,N s is the number of cells in series and T c is the cell temperature.The power produced by the PV device is the product of the current and voltage.Ideally,a PV panel would always operate at a voltage that produces maximum power.Such operation is possi-ble,approximately,by using a maximum power point tracker (MPPT).Without an MPPT the PV panel oper-ates at a point on the cell I –V curve that coincides with the I –V characteristic of the load.It is this second situ-ation (i.e.,no MPPT)that is the focus of this investigation.2.1.The reference parametersTo evaluate the five parameters in Eq.(1),five inde-pendent pieces of information are needed.In general,these five parameters are functions of the solar radiation incident on the cell and cell temperature.Reference val-ues of these parameters are determined for a specified operating condition such as SRC.Three current–voltage pairs are normally available from the manufacturer at SRC:the short circuit current,the open circuit voltage and the current and voltage at the maximum power point.A fourth piece of information results from recog-nizing that the derivative of the power at the maximum power point is zero.Although both the temperature coefficient of the open circuit voltage (b V oc )and the tem-perature coefficient of the short circuit current (a I sc )are known,only b V oc is used to find the five reference param-eters.a I sc is used when the cell is operating at conditions other than reference conditions.The five parameters appearing in Eq.(1)correspond-ing to operation at SRC are designated:a ref ,I o,ref ,I L,ref ,R s,ref ,and R sh,ref .To determine the values of these parameters,the three known I –V pairs at SRC are substituted into Eq.(1)resulting in Eqs.(3)–(5).For short circuit current:I =I sc,ref ,V =0I sc ;ref ¼I L ;ref ÀI o ;ref e I sc ;ref R s ;ref a ref À1 ÀI sc ;ref R s ;refR sh ;ref ð3ÞFor open circuit voltage:I =0,V =V oc,ref0¼I L ;ref ÀI o ;ref e V oc ;ref a ref À1 ÀV oc ;refsh ;refð4ÞAt the maximum power point:I =I mp,ref ,V =V mp,refI mp ;ref ¼I L ;ref ÀI o ;ref e V mp ;ref þI mp ;ref R s ;refa refÀ1ÀV mp ;ref þI mp ;ref R s ;refR sh ;refð5ÞThe derivative with respect to power at the maximum power point is zero.d ðIV Þd V mp ¼I mp ÀV mp d I d Vmp ¼0ð6a Þwhere d I /d V j mp is given byd I d V mp ¼ÀI oe V mp þI mp R s a À1sh 1þI o R s a e V mp þI mp R s aþR s Rshð6b ÞThe temperature coefficient of open circuit voltage isgiven byl V oc ¼o V o T I ¼0%V oc ;ref ÀV oc ;T cT ref ÀT c ð7ÞTo evaluate l V oc numerically,it is necessary to know V oc ;T c ,the open circuit voltage at some cell temperature near the reference temperature.The cell temperature used for this purpose is not critical since values of T c ranging from 1to 10K above or below T ref provide essentially the same result.V oc ;T c can be found from Eq.(4)if the temperature dependencies for parameters I o ,I L ,and a ,are known.The shunt resistance,R sh was assumed to be independent of temperature.Therefore,in order to apply Eq.(7),it is necessary to obtain expres-sions for the temperature dependence of the three parameters a ,I o and,I L .The dependence of all of the parameters in the model on the operating conditions is considered in the following section.Fig. 1.Equivalent circuit representing the five-parameter model.80W.De Soto et al./Solar Energy 80(2006)78–882.2.Dependence of the parameters on operating conditionsFrom the definition of a ,the modified ideality factor is a linear function of cell temperature (assuming n I is independent of temperature)so that:a ref ¼T cc ;refð8Þwhere T c,ref and a ref are the cell temperature and modi-fied ideality factor for reference conditions,while T c and a are the cell temperature and modified ideality fac-tor parameter for the new operating conditions.Messenger and Ventre (2004)present an equation from diode theory for the diode reverse saturation current,I o .The ratio of their equation at the new oper-ating temperature to that at the reference temperature yields:I o I o ;ref ¼T c T c ;ref 3exp 1k E g T T ref ÀE g T T c !"#ð9Þwhere k is Boltzmann Õs constant and E g is the materialband gap.The values of the material band gap energies at 25°C for the four cell types investigated in this study can be found in Table A.1.E g exhibits a small tempera-ture dependence (Van Zeghbroeck,2004)which,for sil-icon,can be represented as indicated in Eq.(10)whereE g ;T ref ¼1:121eV for silicon cells.Eq.(10)was used for all of the cells considered in this study.The value of E g ;T ref used for the triple junction amorphous cell type was 1.6eV.E g g ;T ref¼1À0:0002677ðT ÀT ref Þð10ÞThe light current,(I L ),is nearly a linear function of inci-dent solar radiation.Some pyranometers in fact use the short circuit current of a solar cell as a measure of the incident solar radiation.The light current (I L )is ob-served to depend on the absorbed solar irradiance (S ),the cell temperature (T c ),the short circuit current tem-perature coefficient (a I sc ),and the air mass modifier (M ).The light current I L for any operating conditions is assumed to be related to the light current at reference conditions by I L ¼S S ref MM ref½I L ;ref þa I sc ðT c ÀT c ;ref Þð11Þwhere S ref ,M ref ,I L,ref ,T c,ref are the parameters at refer-ence conditions,while S ,M ,I L ,and T c are the values for specified operating conditions.When using Eq.(11)to find the reference parameters,S =S ref and M =M ref .The air mass modifier is assumed to be a function of the local zenith angle and is discussed below.The information needed to determine the reference parameters is now complete.Eqs.(3)–(7)relate themodel to the known reference conditions.To evaluate Eq.(7)it is necessary to include the temperature depen-dence of a ,I o and I L as given by Eqs.(8)–(11).The simultaneous solution of these equations is facilitated with a non-linear equation solver,such as EES (Klein,2005).The final task to complete the model is to investigate the operating condition dependence of the series resis-tance R s ,and the shunt resistance,R sh .The series resis-tance impacts the shape of current and voltage curve near the maximum power point.This effect is seen in Fig.2in which the current–voltage curves for the single-crystalline cell at SRC conditions have been plot-ted for series resistance values that are 20%greater and 20%lower than the value determined at reference condi-tions using Eqs.(1)–(11).The effect on the I –V curve is small and,although methods of adjusting R s as a func-tion of operating conditions have been investigated (De Soto,2004),R s is assumed constant at its reference value,R s,ref in this study.The shunt resistance (R sh )controls the slope of the I –V curve at the short circuit condition;large shunt resis-tances result in a horizontal slope.Fig.3shows the effect of halving and doubling the shunt resistance determined using Eqs.(1)–(11)for the single-crystalline cell at stan-dard radiation conditions.The shunt resistance appears to change with absorbed solar radiation for all of the cells although the effect is most noticeable for cell types that have a relatively small shunt resistance at SRC,such as the triple junction amorphous cell.If experimen-tal data were generally available at more than one solar radiation value,it would be possible to develop a rela-tion between the shunt resistance and absorbed radia-tion.However,this information is not normally available.Schroder (1998)indicates that the shunt resis-tance is approximately inversely proportional to theshort-circuit current (and thus radiation)at very low light intensities.An observation apparent from an exam-ination of the slopes of the I –V curves at short circuit conditions based on the experimental data from NIST is that the effective shunt resistance increases (and the slope thus decreases)as absorbed radiation is reduced.This behavior is observed for all cell types but it is most observable for the triple-junction amorphous cell type.Eq.(12),in which the shunt resistance is inversely pro-portional to absorbed radiation,is empirically proposed to describe this effect.The model specification is now complete.R sh R sh ;ref ¼S refSð12Þ3.The incidence angle modifier,K saThe incidence angle h is the angle between the beam solar radiation and the normal to the panel surface.The incidence angle is directly involved in the determination of the radiation incident on the surface of the PV device.In addition,the incidence angle affects the amount of solar radiation transmitted through the protective cover and converted to electricity by the cell.As the incidence angle increases,the amount of radiation reflected from the cover increases.Significant effects of inclination occur at incidence angles greater than 65°.The effect of reflection and absorption as a function of incidence angle is expressed in terms of the incidence angle modifier,K sa (h )defined as the ratio of the radia-tion absorbed by the cell at some incidence angle h di-vided by the radiation absorbed by the cell at normal incidence.The short circuit current is linearly dependent on the absorbed radiation.The incidence angle is depen-dent on the panel slope,location and on time.Panels that are mounted on a vertical surface,for example,exacerbate the incidence angle effects because much of the annual beam solar radiation strikes the panel sur-face at angles greater than 65°.Nevertheless,vertically mounted panels are of interest because of the applicabil-ity of this orientation to installation on building fac ¸ades.The experimental data that are available to validate the model presented in this paper were taken on a vertical surface.King et al.(1998)provides a cell-specific correlation for the incidence angle modifier in the form shown in Eq.(13).Coefficients for many cell types have been determined by Sandia National Laboratories (2002).Coefficients for the PV modules tested by NIST were determined by Fanney et al.(2002b)and these coeffi-cients are provided in Table A.1.However,an alterna-tive form for K sa (h )was developed for use with the five-parameter model that does not require specific experimental information.K sa ðh Þ¼X 5i ¼0b i h ið13ÞThe incidence angle modifier for a PV panel differssomewhat from that of a flat-plate solar collector in that the glazing is bonded to the cell surface,thereby elimi-nating one air–glazing interface and the glazing surface may be treated so as to reduce reflection losses.Sjerps-Koomen et al.(1996)have shown that the transmission of this cover system can be well-represented by a simple air–glass model.Eqs.(14)and (15),based on Snell Õs and Bougher Õs laws as reported in Duffie and Beckman (1991),are used to calculate the incidence angle modifier for one glass–air interface.The angle of refraction (h r )is determined from Snell Õs law h r ¼arc sin ðn sin h Þð14Þwhere h is the incidence angle and n is an effective index of refraction of the cell cover.A good approximation of the transmittance of the cover system considering both reflective losses at the interface and absorption within the glazing iss ðh Þ¼e ÀðKL =cos h r Þ1À12sin 2ðh r Àh Þsin ðh r þh Þþtan 2ðh rÀh Þtan ðh r þh Þ!"#ð15Þwhere K is the glazing extinction coefficient and L is the glazing thickness.In this study the value of K is assumed to be 4m À1,the value for ‘‘water white’’glass and the glazing thickness is assumed to be 2mm,a reasonable value for most PV cell panels.The refractive index is set to 1.526,the value for glass.To obtain the incidence angle modifier (K sa ),Eq.(15)needs be evaluated for incidence angles of 0°and h .Theratio of these two transmittances yields the incidence an-gle modifier:K saðhÞ¼sðhÞsð0Þð16ÞSeparate incidence angle modifiers are needed for beam, diffuse,and ground-reflected radiation,but each can be calculated in the same way.Average angles for isotropic diffuse and ground-reflected radiation are provided as a function of the slope of the panel in Fig.5.4.1of Duffie and Beckman(1991).Although these average angles for diffuse radiation were obtained for thermal collectors, they were found to yield reasonable results for PV systems.A plot of the incidence angle modifier calculated using Eqs.(14)–(16)as a function of incidence angle is shown in Fig.4.The incidence angle modifiers deter-mined from Eq.(13)for the four cell types with the coef-ficients provided by Fanney et al.(2002b)are also shown in Fig.4with dotted lines.The plots are all similar.Dif-ferences are apparent at high incidence angles,but the incident radiation is normally low at these high angles and the uncertainty in the experimental values of the incidence angle modifier is larger at these conditions. The triple-junction amorphous cell type uses a thin poly-mer cover while the other three cell types employ a glass cover.The parameters for K,L and n used for glass are likely not appropriate for the polymer cover,but the cal-culated cell performance for the conditions investigated was not found to be sensitive to these parameter values. The advantage of Eqs.(14)–(16)is that it eliminates the need for specific incidence angle modifier constants which are not generally available from the manufac-turer.This method of estimating the incidence angle modifier is used in all of the following results for the five-parameter model.4.The air mass modifier,MAir mass is the ratio of the mass of air that the beam radiation has to traverse at any given time and location to the mass of air that the beam radiation would traverse if the sun were directly overhead.Selective absorption by species in the atmosphere causes the spectral content of irradiance to change,altering the spectral distribution of the radiation incident on the PV panel.King et al.(1998) developed an empirical relation to account for air mass: MM ref¼X4a iðAMÞið17Þwhere AM is the air mass and is approximately given by King et al.(1998).AM¼1cosðh ZÞþ0:5057ð96:080Àh zÞð18ÞIn Eq.(17)a0,a1,a2,a3,and a4are constants for differ-ent PV materials which are available for many cell types from Sandia National Laboratories(2002).These con-stants were also determined for the cells tested by NIST as reported by Fanney et al.(2002b).The NIST coeffi-cients are listed for the four different cell types in Table A.1and used to plot the air mass modifier as a function of zenith angle for the four cell types in Fig.5.The air mass modifiers for all cell types except the triple junction cell type are nearly the same for zenith angles between0°and75°.Zenith angles greater than75°are generally associated with low solar radiation values and thus the differences observed in the air mass modifiers for large angles are not important.It was found that if one set of air mass constants is chosen and used for all cell types there is little difference in the results compared to using a different air mass modifier relation for each cell type. Consequently,the air mass modifier for thepoly-crystalline cell was used for all following results obtained with thefive-parameter model.5.Absorbed radiation,SThe major factor affecting the power output from a PV device is the solar radiation absorbed on the cell sur-face,S,which is a function of the incident radiation and the incidence angle.Radiation data are not normally known on the plane of the PV panel,so it is necessary to estimate the absorbed solar radiation using horizontal data and incidence angle information.The total ab-sorbed irradiance S consists of beam,diffuse,and ground reflected components.Eq.(19)provides an approximate method of estimating the absorbed radia-tion,S,assuming that both diffuse and ground-reflected radiation are isotropic(Duffie and Beckman,1991):S¼ðsaÞnG b R beam K sa;bþG d K sa;dð1þcos bÞ2þG q K sa;g ð1Àcos bÞ2ð19ÞIn Eq.(19),q is the ground reflectance,b is the slope of the panel,K sa,b is the incidence angle modifier at the beam incidence angle,K sa,d and K sa,g are the incidence angle modifiers at effective incidence angles for isotropic diffuse and ground-reflected radiation,and R beam is the ratio of beam radiation on a tilted surface to that on a horizontal surface.The NIST data that were used to test the validity of the model included measurements of G T,the solar radiation incident on the vertical PV array surface. However,the beam,diffuse and ground-reflected com-ponents were not measured so it was necessary to estimate these radiation components in order to determine the incidence angle modifiers in Eq.(19). Employing the same assumptions used for Eq.(19), the solar radiation on the array surface can be expressed as:G T¼G b R beamþG d ð1þcos bÞ2þG qð1Àcos bÞ2ð20ÞValues of G T were available from the measurements on the vertical(b=90°)surface.R beam is a time dependent geometric factor provided in Duffie and Beckman (1991).The ground reflectance,q,was assumed to be0.2.The only unknown in Eq.(19)is the diffuse fraction,G d/G since G b=GÀG d.The ErbÕs hourly diffuse frac-tion correlation(Duffie and Beckman,1991)was used to estimate G d/G as a function of the clearness index. Eq.(19)was solved to determine the clearness index and thus the total radiation and beam and diffuse components on a horizontal surface corresponding to the measured value of the radiation on the vertical surface.Since the ratio of S/S ref is needed for further calcula-tions,Eq.(19)is more conveniently represented as:SS ref¼G bG refR beam K sa;bþG dG refK sa;dð1þcos bÞ2þGG refq K sa;gð1Àcos bÞ2ð21Þwhere G ref is the radiation at SRC conditions(1000 W/m2)at normal incidence so that(sa)n cancels out.6.Validation of thefive-parameter modelThe data used for this study were provided by Fan-ney et al.(2002a)from a building integrated photovol-taic facility at the National Institute of Standards and Technology(NIST)in Gaithersburg,Maryland.The experimental data provide,atfive-minute intervals,one year(1January2000–31December2000)of meteorolog-ical data,and measured cell temperatures along with current and voltage values for four different photovol-taic cell technology types installed on a vertical surface. The four different cell technologies are:single-crystal-line,poly-crystalline,silicon thinfilm,and triple-junction amorphous.The solid lines in Fig.6show typical results at4dif-ferent operating conditions calculated for the single-crystalline cells with thefive-parameter model presented in this paper.Also shown in Fig.6are the NIST exper-imental data(open circles)and the results obtained with the King model(closed circles).A summary of the King model is provided in the Appendix.The maximum power values measured by NIST and determinedbythe King andfive-parameter models at SRC conditions and at the4operating conditions are shown in Table 1.Figs.7–9and Tables2–4show similar information for the other three cell types.Note that the reference parameters for all four cell types were determined at the SRC operating condition,1000W/m2and25°C. Differences between the experimental data and the calcu-lated values occur as a result of limitations in the cell model itself,as well as in the methods used to calculate absorbed radiation,incidence angle modifier and air mass modifier.In addition,there are uncertainties inher-ent in the experimental data.Figs.6–8show excellent agreement between the cur-rent–voltages points determined by thefive-parameter model and NIST data.The King model shows slightly better agreement with the data but this behavior is ex-pected since the model requires many measurements over a wide range of conditions to determine the model parameters.It is interesting to note that,at points where Table1Maximum power values from NIST measurements and the King andfive-parameter models for the single-crystalline cell typeSolar [W/m2]Temperature[°C]Maximum power[W/m2]NIST King Five-parameter1000.025.0133.4133.4133.4 882.639.5109.5111.4110.6 696.047.080.182.082.4 465.732.262.761.161.0 189.836.523.822.522.3Table2Maximum power values from NIST measurements and theKing andfive-parameter models for the poly-crystalline celltypeSolar [W/m2]Temperature[°C]Maximum power[W/m2]NIST King Five-parameter1000.025.0125.8125.8125.8882.639.5106.8109.3105.6696.047.077.479.178.1465.732.256.656.955.8189.836.521.218.520.6W.De Soto et al./Solar Energy80(2006)78–8885。
GMW-14171-2006
Heavy Layer Sound Barriers and Decoupler Assemblies© Copyright 2006 General Motors Corporation All Rights ReservedFebruary 2006 Originating Department: North American Engineering StandardsPage 1 of 21 Introduction1.1 Scope. This specification identifies all types of heavy layer or sound barrier materials and their usage with sound absorbing or dissipative materials for noise decoupling assemblies.1.2 Mission/Theme. Products qualified to this specification shall be identified in two parts. The first part shall identify heavy layer sound barriers by class according to density ranges These heavy layer materials will be further identified, in sections 1.4.1 and 1.4.2, as decoupler assemblies and/or dashmats when used in conjunction with sound absorbing materials identified in GMW14194 “Fibrous Sound Absorption Materials”, and GMW14196, “Polyurethane Foams for General Applications”.1.3 Classification.1.3.1 All heavy layer sound materials qualified to this specification shall be listed by class. 1.3.1.1 Class 1 (2.5 ± 0.250 kg/m²). 1.3.1.2 Class 2 (3.5 ± 0.350 kg/m²). 1.3.1.3 Class 3 (4.5 ± 0.450 kg/m²). 1.3.1.4 Class 4 (5.5 ± 0.550 kg/m²). 1.3.1.5 Class 5 (TBD).1.3.2 All decoupler assemblies shall be identified by the proper class of heavy layer and the specific type of sound absorbing material as identified in GMW14194 or GMW14196. 1.4 Decoupler Identifications.1.4.1 Fibrous Noise Decoupler Combinations. Material is designated by “A”; Type refers to only those fibrous materials outlined in GMW14194. See Table 1. Example designation: GMW14171 Class 2 Type A41.4.2 PU Foam Noise Decoupler Combinations. Material is designated by “B”; Types refers to only those materials referenced in GMW14196. See Table 1. Example designation: GMW14171 Class 5 Type B6Table 1: Material Code CombinationsClass Material Material Type123 4 5 12 3 4 5A B6 Note 1Note 1: Material Type 6 is only for Type B materials.2 ReferencesNote: Only the latest approved standards are applicable unless otherwise specified. 2.1 External Standards/Specifications. ASTM 2240 ISO 34-1 FMVSS 3022.2 GM Standards/Specifications.GME 60252 GMW3232GMW3001 GMW3235 GMW3059 GMW3259 GMW3154 GMW4217 GMW3205 GMW14194 GMW3221 GMW141963 Requirements3.1 All materials tested to this specification shall be conditioned for 24 hours according to GMW3221 Code A.3.1.1 Tear Strength (ISO 34-1 Method B, Procedure a. This method requires an angle test piece without a nick. Data for both initial tear and tear propagation shall be required.3.1.2 Hardness (GME 60252 or ASTM 2240). Hardness shall be 80 ± 5 Shore A.3.1.3 Dimensional Stability (GMW4217). Use dry method. !.5% maximum change.3.1.4 Low Temperature Flexibility (GMW3154). The backing shall not break crack or deteriorate in any fashion after the mandrel test.GMW14171 GM WORLDWIDE ENGINEERING STANDARDS© Copyright 2006 General Motors Corporation All Rights ReservedPage 2 of 2 February 20063.1.5 Odor (GMW3205). Report both wet and dry results. Rating of 6 minimum.3.1.6 Flammability (GMW3232). Must comply to FMVSS 302. Test to GMW3232.Note : If the material is a composite or is to be used in a composite, the composite must meet this requirement.3.1.7 Mildew (GMW3259). Required only if natural fibers are present in the construction. There shall be no visible growth or odor of mildew.3.1.8 Fogging (GMW3235). Method A, code T1. Report the average of the 5 reflectance values . A Reflectance value of 90 minimum with either a dry uniform or non-uniform film is required. Specimens that form crystals, an oily film, or discernable droplets ≥ 0.05 mm in diameter at 40X magnification do not meet this requirement.3.2 Performance Requirements. Some products may be highly sound absorbing but not meet chemical resistant requirements for underhood applications.4 ValidationNot applicable.5 Provisions for ShippingNot applicable.6 Notes6.1 Glossary. Not applicable. 6.2 Acronyms, Abbreviations, and Symbols. Not applicable.7 Additional Paragraphs7.1 All materials supplied to this specification must comply with the requirements of GMW3001, Rules and Regulations for Materials Specifications. 7.2 All materials supplied to this specification must comply with the requirements of GMW3059, Restricted and Reportable Substances for Parts.8 Coding SystemThis specification shall be referenced in other documents, drawings, VTS, CTS, etc. as follows: GMW14171 Class X, Type YZ Where:X refers to sound barrier material referred to in section 1.3,Y refers to the sound absorption materials referred to in sections 1.4.1.1 and 1.4.2.1.Z refers to type of sound absorption materials referred to in sections 1.4.1.1 and 1.4.2.1.9 Release and Revisions9.1 Release. This general specification originated in June 2005, replacing TM 374100, TM 373800, TM 374200, TM 373300, TM 605800, GM2212M, GM6045M, and GM2211M. It was first approved by the Global Acoustics Committee in February 2006. It was first published in February 2006.。
SSP_892503_The 2006 new GTI Introduction
3ELF 3TUDY 0ROGRAM#OURSE .UMBER4HE NEW '4))NTRODUCTIONT able of Contentsiii1The newVolkswagen GTIThe new GTI is a fifth generation total redesign of the original “pocket rocket.”Always an incredibly fun car to drive, mating low vehicle weight and precise handlingcharacteristics to a powerful engine package,the new GTI redefines its class.A new chassis, body and electrical system complement the 2.0L turbocharged 200 hp engine. Best of all, 207 lbs-ft of torque give the new GTI remarkable grunt from the line and in all gears. The optional Direct Shift Gearbox (DSG) is a perfect match to the new GTI drivetrain.To ensure optimum handling and driving characteristics, the new GTI’s static body rigidity is up 80 percent. This increasedstiffness results in more direct use of power,greater stability, and enviable handling through corners.Red painted brake calipers, black honeycomb grille, and a well-appointed interior make this new GTI stand out, not only against thecompetition, but alongside the GTI legacy of nearly three decades.Introduction892503_001Brief OverviewThe new GTIThe new GTI sets new standards for itsclass in many areas, including:•Design•Handling dynamics•Drivetrain technology•Spaciousness•Safety•Quality•High-end radio and sound system •Variable intermittent windshield wipers•Electro-mechanical power steering• 2.0T FSI, 200 hp engine2Brief Overview3Dimensions and Weights 4SpecificationsWeights and Exterior Dimensions101.5 in (2578 mm)165.5 in (4210 mm)59.8 in (1518 mm)60.6 in (1540 mm)69.3 in (1759 mm)58.2 i n (1479 m m )Brief OverviewFour-door new GTI shown here will be launched in North America later in2006.892503_003Brief Overview5BodyChassis ConstructionStatic and Dynamic RigidityThe new GTI sets new standards in its classfor static and dynamic rigidity usinglightweight design principles.Fenders, doors, and side panels are all madeof high strength steel.The new GTI has 23 feet of laser-weldedseams compared to 16 feet in the previousGTI. This increase in laser welds hasresulted in significant improvements inchassis strength and rigidity.Laser weld technology improves chassisquality by strengthening the welded surfacewhile reducing sheet metal deformationtypically caused by the heat and pressure ofother welding methods.Key:Green= Side impact zoneY ellow= Occupant cellBlue= Frame structure6892503_005 Hot FormedPanels892503_007Exterior PartsFront BumperAn impact-absorbing foam element is integrated into the front bumper, reducing the risk of injury to pedestrians. This foam element allows compression of the front bumper during impact.HeadlightsStandard:•Xenon headlights•Halogen foglights•Headlight washer system featuring polycarbonate lenses that are:– Clear– Lightweight– Chip resistantThe turn signals are located below the low and high beam headlights to improve their visibility to other drivers.WindowsThe windows on the new GTI are blue-tinted heat insulated glass. Thickness of window glass depends on its location:•Windshield glass is 0.17 in (4.4 mm)•Front side windows are 0.14 in (3.5 mm)•All other windows are 0.12 in (3.15 mm)All fixed windows are bonded to the body.Always place the windshield on its side. Other placement may damage the sash at the bottom or the sealinglip at the top.AreaLabel Drip MoldingAreaChamber CoverHood Latch CableThe hood latch cable (bowden cable) for releasing the hood latch from inside the passenger compartment is located in a protected area in the engine compartment.The hood latch cable disconnect point is located under the hood behind the driver side headlight assembly. This allows front end service without removing the cable from the vehicle’s interior.Disconnect Point OpenSeat Design FeaturesFront SeatsThe standard seat has the followingfeatures:•8-way manual adjustment•Full recline•Adjustable, lockable head restraints•Easy Entry System (illustrated below)•Adjustable lumbar supportThe optional seat adds:•Leather sport trim•Electrically adjustable lumbar support• Adjustable heated seating surfaces892503_019Optional Seat with Lumbar Support892503_020Easty Entry SystemStorage AreasThe new GTI features numerous convenient storage areas.Overhead StorageThere is a standard open storage compartment in the overhead console of the new GTI.Front StorageThe spacious, lockable glovebox features an adjustable temperature outlet, so contents can be kept cool.Door StorageStorage compartments, and a cup holder for 1.6 quart (1.5 liter) bottles are located in the door panels.TemperatureOutletBody 892503_029IntroductionThe new GTI provides the following protection systems and devices.Standard protection equipment includes:•Driver and front passenger airbags •Driver and front passenger side thorax airbags •Front to rear Side Curtain Protection airbags •Three-point seatbelts with retractors on all seats •Front seatbelt pre-tensioners with seatbelt guides and belt force limiters ••Driver and Passenger Side controls airbag deploymentTwo Longitudinal Acceleration Sensors (Early Crash Sensors)G251, located in front of vehicle, detect impact and impact intensityDriver’s and Front Passenger’s Side Airbag Crash Sensors G179and G180 in front doors Occupant SafetyOccupant Safety 892503_030Side Airbag Crash SensorsDriver Side Airbag Crash Sensor G179 and Front Passenger Side Airbag Crash SensorG180 replace the conventional acceleration sensors for side impact detection.These new pressure sensors provide faster detection of side impacts in the door area. Sensor FunctionThe side airbag crash sensors are located in the front doors between the inner and outer body panels. These sensors react to changes in air pressure in the door cavity. Air is directed through an inflow duct to a plate. The components on the plate react to rapid changes in air pressure that occur during a crash.Sensor SignalThe sensor continuously monitors air pressure in the door cavity. If the sensor detects a rise in air pressure above a predetermined value, it sends a signal to the airbag control module.Sensor FailureIf the sensor fails, the airbag warning lamp, located in the instrument cluster, will come ON.SealingOccupant SafetyPowertrainPowertrain6-Speed Manual T ransmission 02QThe 02M transmission, previously used inthe Golf, Jetta and New Beetle was used asa base for the 6-speed manual transmission02Q.This transmission has the following changesin comparison to the 02M:•Selector switch modifications•Stops in the housing to provide additionalsupport for selector forks892503_036PowertrainFor additional information on the DSG, please refer to SSP 841403“Volkswagen 02E Direct Shift Gearbox.”Oil CoolerMulti-Plate ClutchesMechatronics Control ModulePowertrainNotesRunning GearSuspension FeaturesA front axle strut suspension provides thenew GTI with state of the art handlingcharacteristics. The new balanced four-linkrear axle suspension complements the frontsuspension with its own superiorperformance characteristics.•Floor-mounted accelerator pedal assemblywith redundant position sensors•Optimized MacPherson strutsuspension•Direct 1 to 1 anti-roll barconnection•Electro-mechanicalpower steering•Dual rate brake servo•Continental/Teves MK 60 ElectronicStabilization Program (ESP)Running Gear •Four link rear suspensionFront AxleThe new GTI is equipped with a MacPherson strut front suspension with a double wishbone design. This design optimizes comfort while maintaining stability.Wishbone SuspensionAnti-Roll BarSubframeStrutCoupling RodWheelBearingWheelBearingRunning GearRunning Gear Rear AxleThe rear axle suspension of the new GTI is acompact four-link design. Each side consistsof four suspension links: lower link, track rodand upper link, and a trailing arm. This designgreatly enhances stability and ride.This suspension develops a slight understeerduring cornering.Steel SpringUpper Link DamperAnti-Roll Bar BearingBracketSubframeTrack RodTrailing Arm 892503_040Steering SystemThe electro-mechanical power steering system enhances the vehicle’s driving response by maintaining the driver’s precise feel of the road. As speed changes, steering assist adapts. Road surface factors such as bumps and grooves in the road are minimized as much as possible.For additional information on electro-mechanical power steering, pleaserefer to SSP 892403 “Electro-mechanical Power Steering Designand Function.”SteeringColumnSteeringWheelIntermediateShaftElectro-MechanicalPower Steering Running GearNotesBrake SystemThe newly designed braking system on the new GTI presents the driver with the latest generation ABS/ESP combined with its state-of-the-art power brake assist system.Brake ServoABS/ESP ModuleHand BrakeRear CaliperBrake CableBrake LinesBolted Swivel MountingBrake SystemBrake SystemBrake SystemABS Control Module J104 withSpring ContactsBrake System magnesium. This resulted in a weightsavings of more than half of the steel892503_049892503_050892503_051Pedal Assembly892503_052Mechanical ComponentsSmall Metal PlateCoverPedal AssemblyElectrical SystemFuse and relay center underhood on driver side SBElectrical SystemElectrical SystemE l ec t ric a l S y s t emElectrical SystemDrivetrain CAN Control ModulesControl Module Locationsis transferred through the CAN high wire(orange/black) and CAN low wire(orange/brown). To ensure reliablecommunication without conflict orinterference, the CAN wires aretwisted together.Airbag Control Module J234,beneath center console, infront of tunnelABS Control Module J104,on right side of bulkhead,in engine compartmentElectrical System Steering Column ElectronicSystems Control Module J527beneath steering column switchElectrical SystemComfort System Central ControlModule J393, on right side,beneath instrument cluster,behind glove compartmentin center consoleElectrical System Vehicle Electrical SystemControl Module J519,under instrument cluster,on relay carrierInfotainment CAN Control ModulesControl Module LocationsThe Infotainment CAN-bus transfer rate is 100 kbit/s. The data is transferred through the CAN-bus high wire (orange/purple) and the CAN-bus low wire (orange/brown). To ensure reliable communication without conflict or interference, the CAN-bus wires are twisted together.Electrical System。
pvb054
resistance as the interface. As the characteristic dimensions of a system approach h, the interfacial thermal conductance plays an increasingly important role in thermal transport [16]. In our previous studies on G of solid-liquid interfaces, we employed colloidal dispersions of hydrophilic Au nanoparticles in aqueous solution [17,18]. The Au nanoparticles ranged in diameter from 3 to 24 nm and were functionalized with a wide variety of hydrophilic molecules; we determined G by modeling the cooling curves measured by transient absorption in an optical pump-probe experiment. In aqueous solution, despite the variety of surface chemistries we investigated, G was surprisingly constant, 150 < G < 250 MW mÿ2 Kÿ1 [17], indicating that thermal coupling between hydrophilic surfaces and water is relatively strong regardless of the detailed chemistry. Because it is impossible to reliably suspend hydrophobic metal nanoparticles in aqueous solution—hydrophobic particles will rapidly aggregate —we could not answer an obvious next question: how do these values of G for hydrophilic interfaces compare with G for hydrophobic interfaces? Recently, we developed a means to measure G at planar interfaces by time-domain thermoreflectance [19,20], thereby enabling the study of interfaces between water and hydrophobic surfaces. Two sample configurations were prepared as illustrated in Fig. 1 for studying Al and Au based interfaces. First, a 130 nm thick film of SiO2 was deposited by e-beam evaporation on the bottom of a sapphire substrate. This layer serves as an antireflection optical coating at 770 nm, the laser wavelength used in the pump-probe measurements. A polyimide precursor was spin coated on the top of the sapphire substrate and cured at 250 C in air, resulting in a 20 –30 nm thick layer with low thermal conductivity; this layer ensures that most of the heat deposited in the overlying metal film flows into the liquid at short time scales, maximizing the sensitivity of our experiment to the thermal conductance of the solid-liquid interface. Different © 2006 The American Physical Society
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1 SOFTW ARE FOR STATISTICS FOR PHYSICSJAMES T.LINNEMANNMichigan State University,Department of Physics&Astronomy,nsing,MI48824,USAE-mail:linnemann@I discuss two workshops held in2004and2005relevant to the software environment for statistical analysis in physicsand astrophysics.Thefirst largely explored the R environment used by statisticians and the Root environment widelyused in particle physics and relatedfields.The second was a step towards starting a repository for software useful in statistical analyses for thesefields.I also discuss some of the statistical software resources on the web of relevance to physicists.1.IntroductionThe work behind this talk grew out of the PHYS-TAT2003conference,where Louis Lyons invited pro-posals for focused PHYSTAT workshops.After my interactions with statisticians at PHYSTAT2003,the first thing I wanted was to improve the environment for doing particle and cosmic ray physics analysis using statistical tools.I particularly wanted to en-hance what I already had available in Root1,which is our everyday working environment.I clearly suffered from R envy.The R language and environment2 is heavily used by statisticians.The second thing I missed was a web page for physicists of pointers to implementations of statistical methods.And the third thing I felt we lacked was a web site to col-lect new statistical software oriented to the needs of physics.Thefirst and the third of these were sub-jects of workshops,and the second I started work on myself.I’ll discuss each in turn.I must apologize if I didn’t invite you personally to these workshops.Each workshop had a limited goal:to try to do work in a day or two(or at least to start).To me,the right way to do that is to get at least some of the right people in a room.Thus, the workshops were designed with small attendance, to concentrate on discussion rather than hearing a parade of presentations.I’ll leave you to judge how successful we were.2.R and RootIn2004I organized a PHYSTAT workshop3at MSU on statistical software,concentrating mainly,be-cause of those able to attend,on Root and R.Two developers of major software systems attended:Luc Tierney of the R core development team(thanks to valuable contacts by Jerry Friedman,Nancy Reid), and Rene Brun,lead developer of the Root sys-tem.Astronomers also attended:Eric Feigelson, who developed the StatCodes4web site and who is working on the virtual observatory statistics project VOStat5,and Tim Beers who developed the Rostat6 robust statistics package.Physicist/developers in-cluded Harrison Prosper,Scott Snyder,Sherry Tow-ers(TerraFerMa7),and three physicist R users from Fermilab:Adam Lyon,Jim Kowalkowski,and Marc Paterno.For those not familiar with Root,I would de-scribe its key features as follows.It provides a GUI for publication-quality graphics and for making the cuts(data sub-region selections)we physicists are so fond of.It also provides I/O which scales to petabytes data sets consisting of collections offiles containing event data(with each event individu-ally tree-structured).Root uses a histogram as its base metaphor.Its primary interface is a command prompt,which accepts C++as a language for in-terpreted and compiled macros.Root is extensible, though most might not say“easily.”Root contains sophisticated nonlinearfitting and reporting of mul-tidimensional parameter errors.Its collection of sta-tistical algorithms is small,but growing.For exam-ple,robust(to outliers)curvefitting was recently added.Anna Kreshuk’s talk at this conference gives more information on recent developments in Root.For those not familiar with R,it is an elegant data manipulation language(R is a gnu implemen-tation of the S language8),embedded in an environ-ment rich in statistical functionality.The user sees a command prompt.Macros in R are interpreted, but heading toward byte-compilation.R is not GUI-2oriented,though hooks are being built:most users are satisfied with the command line.However,S+,a commercial9implementation of the S language,does provide a rich GUI interface.Most S or S+code runs happily in the R environment.R is described by statisticians as a quick and easy interactive analysis tool,and is indeed the stan-dard tool of professional research statisticians.So if a statistician suggests a method to you(for example bootstrapping,the lasso,bagging,boosting,cross-validation etc.),its probably implemented in R.The R environment has as built in functions a large range of sophisticated statistical tests and graphics,many of which are not in common physics usage.R has links to further multidimensional graph-ics(Ggobi),and a broad package library10,with trivial download mechanism.R allows straight-forward extensibility to new packages in R or C code.Functions and packages are often very fast if they are R-wrapped C code.R keeps data in virtual memory Data Frames,and uses vectors as its basic metaphor.R has interfaces to postgres, mysql,and other databases,and has parallel com-putation under development.While both Root and R are used outside their home communities,R and S documentation2,8is commercially published and available at Amazon.Susan Holmes’talk at this conference discusses data visualization largely using R tools,and Marc Paterno’s talk provides further detail on R use from a physicist’s perspective.Also useful is Adam Lyon’s talk11at the MSU workshop.There were three main results of the workshop. Eric Feigelson was confirmed in his initial inclination to use R for the basis of the VOStat project.Adam Lyon,encouraged by discussions with Luc Tierney, wrote a fairly general Root Tree reader for R.Rene Brun was perhaps further interested in R,encour-aged on his existing path of adding statistical func-tionality to Root,and,I hope,inspired by R’s elegant package mechanism10.Rene and I at this conference celebrated(?)a quarter century of my encouraging Rene to do even better than he has in providing an everyday environment for particle physicists.3.Statistical Resources on the Web forPhysicistsMy second topic grew out of preparation for the software workshop just described.I wanted to sur-vey what statistical resources were available on the web for physicists.Having a few lazy bones in my body,I wanted to know where I mightfind useful statistical software without having to write it all from scratch.In the process I developed a page of links at /people/ linnemann/stat_resources.html.I definitely don’t want to claim there had been no effort in particle physics before mine.But to my shock,this is now the largest such page I know of. Others who had preceded me in HEP included Glen Cowan,and the CDF statistics committee.But the reason for the lack of pointer pages is,I believe,the lack of actual web statistics-oriented resources spe-cific to physics.Here again I suffer envy of otherfields.In par-ticular,astrophysicist Eric Feigelson has done an ex-cellent job of surveying statistical resources at his StatCodes site4.Its point of view is quite gen-eral in fact–physicists should most certainly look there–though of course he is particularly interested in items relevant to astronomy and astrophysics,a few of which have found less application in particle physics.Tom Loredo12also has a very useful collec-tion of links.Not surprisingly,there are many useful sites from statistics,particularly StatLib13.There are also quite a number of useful resources on mul-tidimensional analysis which I included on my page. I’m sure many of you have your own favorite links to software,and I would be delighted for you to send them to me.I have avoided most references to com-mercial software,mainly because I have seldom seen my physicist colleagues use(i.e.pay for)commer-cial analysis software.Astrophysicists,however,find their productivity gains well worth the cost of the commercial IDL14package for analysis,interpola-tion and manipulation of2and3D image data;it contains substantial statistical functionality as well.4.Towards a Repository for StatisticalSoftware for PhysicistsOne conclusion I drew after searching for physics-oriented statistical resources was that I was also suf-fering from a serious case of repository envy.As-3tronomy has a number of user-contributed reposito-ries under way for analysis and statistical codes,for example those maintained by the Astronomical Soft-ware Directory Service15and NASA’s HEASARC16. Even biology has bioconductor17,a large collection of R software for bioinformatics.There are a few HEP repositories18,but there is little physics-oriented analysis or statistical software on the web at present. In some ways this is surprising,as the web was in-vented for HEP.Assessing user interest in such a repository was the motivation for a2005workshop19 Mark Fishler and I organized at Fermilab.Behind the archive is Mark Twain’s notion that if you make it sufficiently attractive for someone to write statistical code,they might actually do it for you20.Louis Lyons advised me that in giving this talk,I was coming to the right place tofind software writers.And when I asked who in the audience had written statistical software of use to someone else,a goodly majority indeed raised their hands.I know I wouldfind it useful to have access to the programs used to produce results for many of the talks at this conference.The basic motivation for a software repository is sharing:don’t reinvent the wheel;improve it.A repository requires some implied longevity which seems best met by having an organization rather than an individual as sponsor.Fermilab is poten-tially interested in such a role.Clearly a web inter-face is needed for upload,search,retrieval.One can envision a hierarchy of purposes,ranging from an archive for source code of software associated with physics or conference papers,through a download-able package library(either of stand-alone packages, or packages adapted to particular frameworks),to a component library with various language or web interfaces,possibly with distribution of binaries for various platforms.A Statistical Software Archive.The sim-plest repository function discussed at the work-shop was an open archive(roughly analogous to ).If you publish a statistical calculation in refereed physics papers or at statistical confer-ences such as this one,you could put the code in the archive,and reference it.With an archival reposi-tory available,one could hope that this becomes as much a part of the culture as submitting preprints to has become.Archiving offers the potential of substantial benefit for a modest effort.The“guarantee”for users would be intention-ally weak:once,the code compiled and ran on some machine and produced useful results.To allow reuse of code with credit to authors,the minimal infor-mation supplied would be the author,title,and a one-line explanation of purpose.Keywords and pos-sibly the experiment to which it was relevant would make it easier to locate.Your grad student could start a project here,rather than from scratch,and possibly compare methods used by different exper-iments.Documentation would be encouraged(but not quite required).Version tracking would need to be supported by the system even at this basic level.There are many candidates for software in such an archive:calculations of significance,limit setting programs,and goodness offit tests come to mind,as does software for studying the behavior of statistical methods.In these areas,competing procedures exist: some are published,some not.Actual programs are very hard tofind:you have to know of the method, and ask its author personally;at best,you mightfind some such code in your physics collaboration’s CVS repository.Only a few such programs have public web interfaces(D0or Babar have some).A Package Download Site.A more sophis-ticated use of a repository would be software writ-ten explicitly for re-use(rather than archived for the historical record).Packages of this kind might be stand-alone programs,or packages for frameworks such as R or Root.Here there is a real need for well-designed conventions to support portability and simplify building and upload.Documentation now also becomes a vital issue,including of course any published references for the methods used.In this context,R’s package mechanism is particularly ad-mirable.Attaining the same level of simplicity for user and author for Root add-ons would be a real achievement.A repository sponsor can add real value by providing proper repository design to help authors reach users simply and effectively.Further value could be added by choosing packages(possibly even those originally submitted only for archiving) which are of sufficient interest to maintain for reuse at this level,and by providing assistance to authors on issues of portability,numerical techniques,base library choice,or other coding practices.Candidates for packages of this type also spring readily to mind:multidimensional analysis pack-ages such as Sherry Towers’TerraFerMa7and Ilya4Narsky’s StatPatternRecognition(described at this conference).Both are currently stand-alone pro-grams rather than framework packages.A Linkable Toolkit.An even higher level of functionality is also conceivable,by working from the basis of such a repository.One could imagine pro-viding a toolkit library.One might aim to support writing“toy Monte Carlo”or ensemble test writing by providing a coherent library,perhaps building on the gsl(Gnu Scientific Library),or on the mathcore or mathmore libraries envisioned within Root.This would involve interacting with users to assess exist-ing tools and designing and supplying missing ones. One might repackage existing programs as frame-work packages to enhance usability.Quality control (robustness,accuracy,etc)become critical at this level of ambition.Personnel for design,coding,and maintenance would be required.One might also pro-vide a computation service for some of the simpler algorithms,with web data entry via forms or ASCII datafiles.Plans.The main outcome of this workshop was a consensus statement(included here as an Ap-pendix).Based on this consensus,we had further negotiations with the Fermilab computing division and carried forward discussion to this conference. Marc Paterno of Fermilab attended this conference in large part to assess the interest of a wider com-munity in the repository.At this PHYSTAT2005 conference,Marc Paterno,Louis Lyons,and I have discussed these ideas with many people.These con-sultations uncovered potentially interesting synergies with Root and the Cedar physics archive in the UK. We also found that considerable interest was ex-pressed for the archive,and were strongly encouraged to get started and see how things evolve once contri-butions begin arriving.Thus,we are in the process of preparing a proposal to the Fermilab Computing Di-vision to support some version of an archive.Let us know if you think its worthwhile,and pass along any advice you might have.We are currently thinking about the level of manpower required to get started, and working through computer security,copyright, and license issues associated with such a venture.In the end,it is hardly our vision of the repos-itory and how it might be used that matter.What counts is how the community chooses to use it,and our main motivation is to provide a forum for un-leashing the creativity of that community.Whether it houses mathematica,mathcad,or matlab software for producing statisticalfigures for conference pa-pers;C++or Fortran routines used in Physical Re-view or Physics Letters or NIM articles;massfitters, deconvolvers,goodness offit or significance or limit calculators,or cunning ways of telling signal from background;whether submissions are programs or packages for R or Root;whether written in java,C, C++,perl,ruby,or python;or entirely other things, depends on what the communityfinds most useful.5.The Reproducible Research Ideal Reproducible Research21is an interesting concept in some ways related to the repository.The ideal is that when you write a paper,you save(in a tar archive, say)the entire environment necessary for creating the paper through scripts,and the whole paper and itsfigures and tables are generated by executing a single high-level script.This tar archive would of course be an excellent submission to the software repository we have discussed.We all know the kind of problems that led to these thoughts:you ask a graduate student to pick up a project and suggest one of your papers as a starting point,but the studentfinds it remarkably difficult to actually reproduce the plot you suggested. To do so requires having the same data set you used several years ago,and to use the programs with all the same settings.To achieve a reasonable approxi-mation to this ideal requires as a minimum a power-ful script-oriented method of producingfigures and tables(such as R or Root)and all the data used in the paper.It also implicitly implies a data set of rather modest size,and a stable set of tools.Other-wise you’d have to save the entire contents of your computer each time.More is required,however:directory conven-tions,makefiles,and many other details should be conventional and provides a subset of such an environment:you know that you will be able to rebuild a pdffile from the latex source and epsfiles if you meet arxiv’s requirements.This ideal is achievable for most(not all)plots shown at this conference,and for most significance and limit cal-culations in our physics papers.It is problematic for large HEP data sets,which are not publicly avail-able and not necessarily permanently archived with full version control.It is also problematic for analy-5ses which are long in duration(months to years,not hours to days).This is exacerbated when multiple analyses are combined into a single publication,as is often the case in large physics collaborations.Still,the reproducible research ideal is well worth striving toward.Those who have created a research environment fully supporting the ideal describe it as a discipline with more benefits to authors than to readers wishing to build on the published research.6.ConclusionsTo summarize,I’d like you to take away three main points.First,R has many intrinsic attractions,and is a window to the statistics community.It should be better known in physics and astrophysics,and it is now possible to read Root trees in R.I would person-ally be delighted if everything in R appeared in Root, my everyday environment.Second,I started a page of web links to statistical software resources relevant to physicists and astrophysicists.If youfind it useful, tell your colleagues,link to it,and more importantly, help me improve it.Third,we are trying to start a repository for statistics-oriented software of use to physicists and astrophysicists.I’d appreciate your discussing this repository within your collaboration, and encourage us(and the Fermilab Computing Di-vision)if you think it should be pursued.And we hope you will also contribute software to the reposi-tory.Appendix:Consensus Statement fromthe2005Fermilab WorkshopFollowing is a slightly abbreviated version of the con-sensus statement resulting from the workshop: Currently,statistical tools are in use by individ-ual physicists,and within collaborations.Their ulti-mate purpose is to make the best use of the data col-lected by collaborations.However,their effectiveness is limited by the lack of a straightforward mechanism for the community to share software on a wider ba-sis,learn best practice from one another,and avoid unnecessary re-development of similar tools.Some tools are of general use(for example event classi-fiers,or limit calculation programs).These codes often embody standard practices within a collabo-ration,recent progress of understanding within our field,or implementation of important ideas devel-oped by statisticians or within the machine learn-ing communities.Other programs encode hard-won expertise in handing particular situations.Sharing such codes across research groups and collaborations contributes directly to the diffusion of such knowl-edge,and indirectly to improvement of our under-standing of our data and the training of students by facilitating comparison of methods.A repository could provide,as objects of study and understanding, working codes which have been tested under realistic conditions.Such codes would also provide a point of departure for improvements,rather than having to first re-implement present ideas for lack of publicly-accessible code.What sort of repository would support such ef-forts?We suggest a phased approach.Thefirst and perhaps most important step would be a very open archival repository,where essentially anyone could upload code felt to be useful for statisti-cal tasks in physics experiments.The repository should make it straightforward to store software used to perform calculations for a paper,and refer to those calculations in the publications:“we calcu-lated the upper limit using a Bayesian technique as-suming aflat prior in the cross section[17]”,and reference[17]might read“C.Calvin&H.Hobbes, /05/07/23/0013/,version3”.The repository would provide some basic expectations on what a submitting author should provide,but the absolute requirements would be purposely minimal, in order to encourage submission.A submission should minimally include authors, an email contact address,a tar archive with code and a brief text description of what the submission does. There would be a possibility to provide keywords and an experiment of origin,but not a requirement.A read-mefile would be encouraged to include docu-mentation and the platform(s)on which the code had run.Overall,the effort required for submission should be less than or comparable to submitting a paper to .Downloading code from the archive should be similarly straightforward.Search facilities from the web might start with a simple web listing of entries with a one line description,but could become more sophisticated as more entries became available.At-taching user feedback is another possible evolution path.Fermilab would be a natural sponsor of such a repository,assuming that it could provide the desired6degree of openness.The lab hosts experiments which are currently producing much innovative statistical software,and the lab intends to be a center for on-going research in particle and astro-particle physics. This is an important activity supporting data analy-sis,which does not require proximity to the physical location of the experiment.And there are members of the computing division with professional interests in this area.A longer term vision of the repository goes be-yond passively archiving code.One value-added ac-tivity would be to classify the submissions to distin-guish archival entries from actively maintained pack-ages.Capture of user assessment of such packages might be particularly useful.Packages could also benefit from expertise by improving the efficiency or portability of the submitted code.Design expertise might provide standards for packages which would make them more readily usable.A particular ex-ample of interest is the elegant R package mecha-nism:it would be a real achievement to have de-sign standards which would allow a similar ease of package creation and import within the Root frame-work.Standards might include naming conventions, package directory structure,allowed base libraries, or build tools.Other activities might include mining the submissions for likely contributions to a linkable library(for example mathmore packages),identify-ing and writing code for missing functionality,inte-grating related packages,soliciting and supporting extensions of existing code(justifiable by a broader use base than a single experiment),or actively look-ing for interesting software produced by the statisti-cal software community and providing web interfaces or language translation wrappers to support use by the physics community.Another possibility is main-tenance of a list of such software,perhaps building on the software link web site developed by Jim Linne-mann.Such value-added activities would best evolve over time as the use of the repository grows.We intend to submit soon a more formal request to Fermilab management,and to approach large col-laborations to solicit their support for such an en-deavor.AcknowledgmentsThanks to Tom Loredo for many astronomy links, and reminding me of Reproducible Research,and to Bob Nichol for useful comments on this manuscript.A word on referencesI have omitted the initial http://in all the web references.Many more links are available at:/people/linnemann/ stat_resources.html.References1.root.cern.ch.This site contains links to sourcecode,online documentation and tutorials.;Venables and Smith,An In-troduction to R,Network Theory Limited(2001);Dalgaard,Introductory Statistics with R,Springer (2002);Everitt,An R and S-Plus Companion to Mul-tivariate Analysis,Springer(2005);zoonek2.free.fr/UNIX/48_R/all.html(R tutorial)./linnemann/public/workshop/statcodes/vostat6.Beers,T.C.,Flynn,K.,Gebhardt,K.,“Measuresof Location and Scale in Clusters of Galaxies.I.A Robust Approach,”1990,Astronomical Journal,100,32;see also Hoaglin,Mosteller,Tukey,Un-derstanding Robust and Exploratory Data Analysis, Wiley(2000).There is no Rostat web site./$\sim$smjt/multiv.html8.Becker,Chambers,and Wilks,The New S Language,Chapman and Hall(1988);Chambers and Hastie, Statistical Models in S,Chapman and Hall(1992);Venables and Ripley,S Programming,Spring(2000);Chambers,Programming with Data:A Guide to the S Language,Springer(2004)./linnemann/public/workshop/rInHep.ppt/staff/loredo/statpy/idl//packages.html/docs/software.html18.ph-sft.web.cern.ch/ph-sft,,/CPD,www.cedar.,/computing/top_ pages/software.htm/PHYSTATworkshop,/linnemann/public/workshop/Fermi_Program.htm20.Mark Twain,Adventures of Tom Sawyer(1876);seehow Tom handles the chore of painting the fence around his house./jaw/jaw.research.reproducible.html。