The Concrete Centre. Dynamic Thermal Properties Calculator

Size: px
Start display at page:

Download "The Concrete Centre. Dynamic Thermal Properties Calculator"

Transcription

1 The Concrete Centre Dynamc Thermal Propertes Calculator The Concrete Centre Dynamc Thermal Propertes Calculator

2 Page 2

3 The Concrete Centre Dynamc Thermal Propertes Calculator Contents Page 1 Introducton 1 2 User gude Software requrements 3 3 Theory Admttance parameters (ISO 13786) Internal heat capactes, and 30 (ISO 13790) 5 4 References and Further Informaton 6

4

5 The Concrete Centre Dynamc Thermal Propertes Calculator 1 Introducton Ths gudance note descrbes The Concrete Centre s Dynamc Thermal Property Calculator tool (developed for TCC by Arup). The tool s an Excel spreadsheet that calculates parameters relatng to the dynamc thermal storage of constructon elements. Two groups of parameters are calculated: 1) thermal admttance, Y, and related quanttes, as specfed n EN ISO 13786:2007 and 2) surface heat capactes, (or Cm ), as specfed n EN ISO 13790:2004, whch are used n the SAP(2009 draft) and SBEM calculaton tools supportng Part L of the Buldng Regulatons. The specfc parameters calculated are: Thermal admttance parameters: Surface heat capactes - Thermal admttance, Y [W/m²K]. Ths s the amount of energy leavng the nternal surface of the element nto the room per unt degree of temperature swng. Ths s under theoretcal condtons where the nternal envronmental temperature undergoes perodc oscllaton and the external envronmental temperature s constant. - Tme lead for thermal admttance [hours]. Ths s the tme dfference between the tmng of the peak heat flow at the nternal surface and tmng of the peak nternal temperature. - Decrement factor [dmensonless]. Ths s the rato of the peak heat flow out of the external surface of the element per unt degree of external temperature swng to the steady state heat flow through the element per unt degree of temperature dfference between the nternal and external envronmental temperatures. - Decrement delay [n hours]. Ths s the tme lag between the tmng of the nternal temperature peak and the peak heat flow out of the external surface. - Surface factor [dmensonless]. Ths s the rato of the swng n heat flow from the nternal surface of the element to the swng n heat flow receved at the nternal surface of the element (such as solar gan from a sun patch). - Tme lag for the surface factor [n hours]. Ths s the tme lag between the tmng of the peak heat flow enterng the surface and peak heat flow leavng the surface nto the room. - Areal heat capacty [kj/m²k]. Ths s the amount of energy stored n the element over the frst half perod of the heat flow swng per unt area of element per unt degree of temperature swng. The same amount of heat s released n the followng half perod. - U-value [W/m²K]. Ths s the steady state heat flow through the element per unt degree of temperature dfference between the nternal and external envronmental temperatures per unt area. Note that ths quantty may dffer from other U-values quoted as t does not take account of thermal brdgng and s senstve to the values of surface thermal resstances used. - [kj/m²k]. Ths s the volumetrc heat capacty of the thermally actve part of the constructon up to a maxmum thckness of 100mm [kj/m²k]. Ths s the equvalent of but for a maxmum thckness of 30mm 2 User gude The spreadsheet contans three sheets: Input, Full Results and Reference Data. Error! Reference source not found. shows a screen shot of the Input sheet. On ths sheet the user specfes the constructon buld up and can alter (optonal) the tme perod, the nteror and exteror heat transfer coeffcents and the locaton of the element (external or nternal). The user can also enter project detals. Further detals on data entry are gven below. Page 1

6 On the Input sheet some key output results are also shown for convenence. These are admttance, decrement factor, decrement delay and value (note that decrement factor and decrement delay are not calculated for nternal elements). A graph showng the ampltude and phase of the swngs n nternal and external heat flows and nternal temperature s also dsplayed. The Full results sheet contans the full set of calculated parameters, lsted n Secton 1 together wth a summary of the constructon buld up and other assumptons on whch the calculaton s based. The Reference Data sheet contans a lst of thermal propertes of common constructon materals, taken from CISBE Gude A. The followng nstructons explan how to use the spreadsheet. 1) Fll n the calculaton settngs. a. Enter the perod of oscllaton of the nternal envronmental temperature. b. Enter the nternal surface resstance for the element. (Refer to Table 1 for typcal values). c. Enter the external surface resstance. d. Select whether the element s an external element (.e. separatng a condtoned space from the outsde) or an nternal element (.e. separatng two condtoned spaces). 2) Fll n the Element constructon. a. Select the layer type for each layer before enterng any other detals for the layer. Select Sold Layer f the layer s a layer of buldng materal. Select Cavty Unlned f the layer s a cavty wthout a fol lnng. Select Cavty Fol-lned f the layer s a cavty wth a low emssvty fol lnng. If these automatcally calculated cavty resstances are not approprate, select the Cavty User defned thermal resstance. b. Once the layer types have been selected, the parameters requred for each layer wll be hghlghted. All of the hghlghted felds must receve entres for the calculaton to be carred out. c. Enter a layer name to dentfy each layer. d. Enter the thckness of each layer. e. Enter the densty, specfc heat capacty and thermal conductvty of each sold layer. Values of these propertes for common materals are provded n the Reference data sheet. These may be coped and pasted nto the nput felds. f. Enter the thermal resstance of each cavty wth a user defned thermal resstance. The layers do not need to be n consecutve rows n the Element Constructon table. Empty rows wll be gnored by the calculaton. Once all the requred parameters for a layer have been entered, the layer may be coped and pasted nto other locatons wthn the Element Constructon table. To delete a layer, delete the layer type for the layer. 3) Clck the calculate button to calculate the result for the element. The results wll be presented n three formats. a. Key. Ths shows the most commonly used results. b. Heat flow plot. The plot shows a unt perodc swng n the nternal envronmental temperature. The plot also shows the surface heat flows nto the nternal surface and out of the external surface resultng from the plotted swng n nternal temperature and a constant external temperature. Ths s a graphcal nterpretaton of the admttance and the decrement factor, respectvely. Page 2

7 The Concrete Centre Dynamc Thermal Propertes Calculator c. Full Results sheet. Vew ths by clckng on the tab at the bottom of the wndow. Ths shows all the nput parameters that have been used n the calculaton and the thermal resstance used n the calculaton for each cavty layer. The Full Results sheet also gves a full lst of the dynamc thermal propertes calculated. If any error messages are produced whlst usng the calculator, follow the nstructons to check the nput parameters are vald. The programme checks that the user nputs are adequate to perform the calculaton. There are no restrctons, however, on whether the nput values are realstc. If the error message perssts when there seems to be no problem wth the entered data, open an empty verson of the calculator and re-enter the data. 2.1 Software requrements The tool was developed on the 2003 Servce Pack 3 verson of Excel and has also been tested on Excel Theory 3.1 Admttance parameters (ISO 13786) Thermal admttance s a framework to quantfy how a constructon element responds to perodc (snusodal) cycles n temperature and heat gan. Ths framework s descrbed fully n EN ISO 13786:2007. The admttance framework also provdes the bass for the CIBSE Smple Dynamc Model for calculatng coolng loads and summertme space temperatures (CIBSE (2005) Gude A: Envronmental desgn). The admttance framework calculates parameters descrbng the dynamc thermal propertes of constructon buld ups composed of homogeneous, planar elements, from the thermal propertes (thermal conductvty, specfc heat capacty and densty) of the materal layers and cavtes that make up the constructon. The two prncpal admttance parameters are admttance and decrement factor. These descrbe the response of the constructon element to a perodc (snusodal) thermal forcng consstng of a heat flow nto the surface from the room (by radatve and conductve heat transfer processes). The admttance descrbes the rate of heat flow nto the nteror surface of the element and decrement descrbes the rate of heat flow from the exteror surface of the element. In both calculatons t s assumed that the room ar temperature s varyng and the outsde ar temperature s constant (smlar concepts can be defned reversng these assumptons). Each parameter descrbes the ampltude of the response and also has an assocated tme lead or lag between the tmng of the response and of the forcng. The tme perod for the thermal forcng s usually taken to be 24-hours, but any tme perod can be used and the tool enables the tme perod to be used to be specfed by the user. Although admttance s sometmes taken to be a measure of thermal storage, ths s not strctly true, snce Y only descrbes the heat flow nto the surface, whereas t s the dfference between the heat flow nto the nteror surface of the element and that leavng the exteror surface that relates to the heat storage acheved. To calculate the effectve thermal storage, therefore, requres both Y and decrement factor to be used and the assocated tme delays. Ths s done n the calculaton of the areal heat capacty whch descrbes the effectve heat storage acheved over one half cycle. The thrd parameter calculated s the surface factor. Ths s not ncluded n ISO but s used n the CIBSE smple dynamc model. It relates to the ablty of a surface element to absorb ncdent radatve heat gan, e.g. from a sun patch on the surface. Ths parameter also has an ampltude and a tme lag. The theoretcal scenaros formng the bass of these three parameters are shown schematcally n Fgure 1. Page 3

8 Tˆ Admttance, Y Tˆ Tˆ e Decrement factor, f Tˆ U e absorb Surface factor, F absorb Fgure 1: Schematc of the scenaros under whch the dynamc thermal characterstcs are calculated. s the swng n heat leavng the nternal surface of the element nto the room, Tˆ s the swng n nternal envronmental temperature, Tˆ e s the swng n external envronmental temperature, U s the U-value of the element and absorb s the heat absorbed by the surface (heat flows are shown n orange and temperatures n green). To calculate the admttance parameters, the tool follows the methodology set out n ISO 13786:2007 Thermal performance of buldng components Dynamc thermal characterstcs Calculaton methods. Two mportant features of the calculaton requrng clarfcaton are the values used for the surface heat transfer coeffcents and the thermal resstance of any nternal cavtes n the constructon Surface heat transfer coeffcents The surface heat transfer coeffcents used n the default calculaton are those for horzontal heat transfer. Ths s obvously approprate for a vertcal wall. For a horzontal slab, typcally the drecton of heat transfer alternates between upwards and downwards over the durnal cycle. It s therefore approprate to use these ntermedate values for the surface heat transfer coeffcent. In cases where the heat transfer s ether always upwards or always downwards the user may alter the surface heat transfer coeffcents to the conventonal surface resstances gven n BS EN ISO 6946:2007 Buldng components and buldng elements Thermal resstance and thermal transmttance Calculaton method and shown n Table 1. Page 4

9 The Concrete Centre Dynamc Thermal Propertes Calculator Surface Resstance m 2 K/W Drecton of Heat Flow Upwards Horzontal Downwards Rs Rse Table 1: Conventonal heat transfer coeffcents gven n ISO Cavty thermal resstance In stuatons where the constructon buld up has cavtes the thermal resstance of these cavtes needs to specfed or calculated. The tool allows the user to ether nput a cavty thermal resstance based on an offlne calculaton or can calculate the thermal resstance from a specfcaton of cavty thckness. The calculated values based on thckness are taken from the tabulated values gven n the CIBSE Gude A (2005). Two types of cavty can be specfed: unlned or fol-lned (low-e). To mprove the nterpolaton of ntermedate values between these tabulate values the methodology set out n BS EN ISO 6946 was used. To use ths methodology to reproduce the values gven n the CIBSE Gude A requred a number of assumptons to be made, n lne wth the standard. For a fol lned cavty, the convectve heat transfer coeffcent could not be less than 1.39 W/m 2 K as the cavty got wder; the black-body radatve coeffcent was 5.7 W/m 2 K; the emssvty of the fol-lned surface was 0.16; and the emssvty of the unlned surface was 0.9. The drecton of heat transfer through the cavty s assumed to be horzontal for the same reasons as the heat transfer from the nternal and external surfaces s assumed to be horzontal. If ths s not approprate the user may set the thermal resstance of the cavty by selectng the Cavty - user defned thermal resstance layer type. 3.2 Internal heat capactes, and 30 (ISO 13790) The tool calculates two surface heat capactes, and 30. These quanttes are not drectly related to the admttance framework but to a smpler framework for calculatng thedynamc thermal response of buldng elements used n ISO 13790:2004 Thermal performance of buldngs Calculaton of energy use for space heatng. 1 These quanttes relate smply to the volumetrc heat capacty of dfferent parts of the constructon element. The way n whch they are calculated s descrbed below. s used n SAP (2009, draft) and the SBEM calculaton tools supportng Part L of the Buldng Regulatons. It s calculated (n unts of kj/k per m² of surface area) from: 10 6 c d where: s the densty of layer n the constructon (kg/m³) c s the specfc heat capacty of layer (J/kg K) d s the thckness of layer (mm). 1 Note that ISO uses the notaton rather than and n SBEM was formerly referred to as Cm. Page 5

10 The summaton s done over all layers n the element, startng at the nsde surface and stoppng at whchever of these condtons occurs frst (whch may mean part way through the layer) half way through the constructon an nsulatng layer a maxmum thckness of 100mm An nsulatng layer s defned here as an element havng a thermal conductvty of less than 0.08 W/mK. Ths threshold s taken from the User Gude to SBEM verson 3.3.b (Note: ISO and SAP(2009) do not specfcally defne a crtera for an nsulatng layer). In the case of cavtes, an effectve thermal conductvty for the layer s calculated by dvdng the cavty thckness by the cavty thermal resstance. The surface heat capacty, 30, s calculated n a smlar way to but the maxmum thckness for the summaton s 30mm. Ths quantty s used n ISO to model thermal storage effects where heatng s ntermttent. It s not used n SAP or SBEM. Note: s a relatvely smplstc way of charactersng the thermal mass of a constructon element as, n addton to the assumptons made regardng the thermally actve layer thckness, t does not take account of the effect of thermal conductvty n determnng the tmescale for heat to enter and leave the element. The areal heat capacty defned n ISO provdes a more accurate measure of the effectve heat capacty of a constructon element. 4 References and Further Informaton Envronmental Desgn CIBSE Gude A Chartered Insttute of Buldng Servces Engneers 2006 EN ISO 13786:2007 Thermal performance of buldng components Dynamc thermal characterstcs Calculaton methods Internatonal Organzaton for Standardzaton 2007 EN ISO 13790:2004 Thermal performance of buldngs Calculaton of energy use for space heatng Internatonal Organzaton for Standardzaton 2004 EN ISO 6946:2007 Buldng components and buldng elements Thermal resstance and thermal transmttance Calculaton method Internatonal Organzaton for Standardzaton 2007 Harrngton-Lynn, J. The Admttance Procedure: Intermttent Plant Operaton Buldng Servce Engneerng Volume 42 pg Mlbank, N. O. Harrngton-Lynn, J. Thermal Response and the Admttance Procedure Buldng Servce Engneerng Volume 42 pg Loudon, A.G. Summertme Temperature n Buldngs Wthout Ar-condtonng IHVE/BRS Symposum 1968 Daves, M.G. Hourly Estmaton of Temperature Usng Wall Transfer Coeffcents School of Archtecture and Buldng Engneerng, Unversty of Lverpool 1995 Thermal Mass Explaned - The Concrete Centre 2009 Publshed by MPA The Concrete Centre Gllngham House, Gllngham Street, London SW1V 1HU Tel: +44 (0) All advce or nformaton from MPA The Concrete Centre s ntended only for use n the UK by those who wll evaluate the sgnfcance and lmtatons of ts contents and take responsblty for ts use and applcaton. No lablty (ncludng that for neglgence) for any loss resultng from such advce or nformaton s accepted by MPA The Concrete Centre or ts subcontractors, supplers or advsors. Readers should note that publcatons from MPA The Concrete Centre are subject to revson from tme to tme and they should therefore ensure that they are n possesson of the latest verson. Page 6

SPANC -- SPlitpole ANalysis Code User Manual

SPANC -- SPlitpole ANalysis Code User Manual Functonal Descrpton of Code SPANC -- SPltpole ANalyss Code User Manual Author: Dale Vsser Date: 14 January 00 Spanc s a code created by Dale Vsser for easer calbratons of poston spectra from magnetc spectrometer

More information

Structure and Drive Paul A. Jensen Copyright July 20, 2003

Structure and Drive Paul A. Jensen Copyright July 20, 2003 Structure and Drve Paul A. Jensen Copyrght July 20, 2003 A system s made up of several operatons wth flow passng between them. The structure of the system descrbes the flow paths from nputs to outputs.

More information

ORIGIN 1. PTC_CE_BSD_3.2_us_mp.mcdx. Mathcad Enabled Content 2011 Knovel Corp.

ORIGIN 1. PTC_CE_BSD_3.2_us_mp.mcdx. Mathcad Enabled Content 2011 Knovel Corp. Clck to Vew Mathcad Document 2011 Knovel Corp. Buldng Structural Desgn. homas P. Magner, P.E. 2011 Parametrc echnology Corp. Chapter 3: Renforced Concrete Slabs and Beams 3.2 Renforced Concrete Beams -

More information

Problem Set 9 Solutions

Problem Set 9 Solutions Desgn and Analyss of Algorthms May 4, 2015 Massachusetts Insttute of Technology 6.046J/18.410J Profs. Erk Demane, Srn Devadas, and Nancy Lynch Problem Set 9 Solutons Problem Set 9 Solutons Ths problem

More information

APPENDIX 2 FITTING A STRAIGHT LINE TO OBSERVATIONS

APPENDIX 2 FITTING A STRAIGHT LINE TO OBSERVATIONS Unversty of Oulu Student Laboratory n Physcs Laboratory Exercses n Physcs 1 1 APPEDIX FITTIG A STRAIGHT LIE TO OBSERVATIOS In the physcal measurements we often make a seres of measurements of the dependent

More information

Comparison of Regression Lines

Comparison of Regression Lines STATGRAPHICS Rev. 9/13/2013 Comparson of Regresson Lnes Summary... 1 Data Input... 3 Analyss Summary... 4 Plot of Ftted Model... 6 Condtonal Sums of Squares... 6 Analyss Optons... 7 Forecasts... 8 Confdence

More information

Negative Binomial Regression

Negative Binomial Regression STATGRAPHICS Rev. 9/16/2013 Negatve Bnomal Regresson Summary... 1 Data Input... 3 Statstcal Model... 3 Analyss Summary... 4 Analyss Optons... 7 Plot of Ftted Model... 8 Observed Versus Predcted... 10 Predctons...

More information

Thermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850)

Thermal-Fluids I. Chapter 18 Transient heat conduction. Dr. Primal Fernando Ph: (850) hermal-fluds I Chapter 18 ransent heat conducton Dr. Prmal Fernando prmal@eng.fsu.edu Ph: (850) 410-6323 1 ransent heat conducton In general, he temperature of a body vares wth tme as well as poston. In

More information

Uncertainty in measurements of power and energy on power networks

Uncertainty in measurements of power and energy on power networks Uncertanty n measurements of power and energy on power networks E. Manov, N. Kolev Department of Measurement and Instrumentaton, Techncal Unversty Sofa, bul. Klment Ohrdsk No8, bl., 000 Sofa, Bulgara Tel./fax:

More information

9.2 Seismic Loads Using ASCE Standard 7-93

9.2 Seismic Loads Using ASCE Standard 7-93 CHAPER 9: Wnd and Sesmc Loads on Buldngs 9.2 Sesmc Loads Usng ASCE Standard 7-93 Descrpton A major porton of the Unted States s beleved to be subject to sesmc actvty suffcent to cause sgnfcant structural

More information

Chapter 3. Estimation of Earthquake Load Effects

Chapter 3. Estimation of Earthquake Load Effects Chapter 3. Estmaton of Earthquake Load Effects 3.1 Introducton Sesmc acton on chmneys forms an addtonal source of natural loads on the chmney. Sesmc acton or the earthquake s a short and strong upheaval

More information

This column is a continuation of our previous column

This column is a continuation of our previous column Comparson of Goodness of Ft Statstcs for Lnear Regresson, Part II The authors contnue ther dscusson of the correlaton coeffcent n developng a calbraton for quanttatve analyss. Jerome Workman Jr. and Howard

More information

Experience with Automatic Generation Control (AGC) Dynamic Simulation in PSS E

Experience with Automatic Generation Control (AGC) Dynamic Simulation in PSS E Semens Industry, Inc. Power Technology Issue 113 Experence wth Automatc Generaton Control (AGC) Dynamc Smulaton n PSS E Lu Wang, Ph.D. Staff Software Engneer lu_wang@semens.com Dngguo Chen, Ph.D. Staff

More information

Numerical Transient Heat Conduction Experiment

Numerical Transient Heat Conduction Experiment Numercal ransent Heat Conducton Experment OBJECIVE 1. o demonstrate the basc prncples of conducton heat transfer.. o show how the thermal conductvty of a sold can be measured. 3. o demonstrate the use

More information

UNIFAC. Documentation. DDBSP Dortmund Data Bank Software Package

UNIFAC. Documentation. DDBSP Dortmund Data Bank Software Package UNIFAC Documentaton DDBSP Dortmund Data Ban Software Pacage DDBST Dortmund Data Ban Software & Separaton Technology GmbH Mare-Cure-Straße 10 D-26129 Oldenburg Tel.: +49 441 361819 0 Fax: +49 441 361819

More information

November 5, 2002 SE 180: Earthquake Engineering SE 180. Final Project

November 5, 2002 SE 180: Earthquake Engineering SE 180. Final Project SE 8 Fnal Project Story Shear Frame u m Gven: u m L L m L L EI ω ω Solve for m Story Bendng Beam u u m L m L Gven: m L L EI ω ω Solve for m 3 3 Story Shear Frame u 3 m 3 Gven: L 3 m m L L L 3 EI ω ω ω

More information

( ) = ( ) + ( 0) ) ( )

( ) = ( ) + ( 0) ) ( ) EETOMAGNETI OMPATIBIITY HANDBOOK 1 hapter 9: Transent Behavor n the Tme Doman 9.1 Desgn a crcut usng reasonable values for the components that s capable of provdng a tme delay of 100 ms to a dgtal sgnal.

More information

On the correction of the h-index for career length

On the correction of the h-index for career length 1 On the correcton of the h-ndex for career length by L. Egghe Unverstet Hasselt (UHasselt), Campus Depenbeek, Agoralaan, B-3590 Depenbeek, Belgum 1 and Unverstet Antwerpen (UA), IBW, Stadscampus, Venusstraat

More information

Analytical Chemistry Calibration Curve Handout

Analytical Chemistry Calibration Curve Handout I. Quck-and Drty Excel Tutoral Analytcal Chemstry Calbraton Curve Handout For those of you wth lttle experence wth Excel, I ve provded some key technques that should help you use the program both for problem

More information

Lab 2e Thermal System Response and Effective Heat Transfer Coefficient

Lab 2e Thermal System Response and Effective Heat Transfer Coefficient 58:080 Expermental Engneerng 1 OBJECTIVE Lab 2e Thermal System Response and Effectve Heat Transfer Coeffcent Warnng: though the experment has educatonal objectves (to learn about bolng heat transfer, etc.),

More information

AGC Introduction

AGC Introduction . Introducton AGC 3 The prmary controller response to a load/generaton mbalance results n generaton adjustment so as to mantan load/generaton balance. However, due to droop, t also results n a non-zero

More information

DUE: WEDS FEB 21ST 2018

DUE: WEDS FEB 21ST 2018 HOMEWORK # 1: FINITE DIFFERENCES IN ONE DIMENSION DUE: WEDS FEB 21ST 2018 1. Theory Beam bendng s a classcal engneerng analyss. The tradtonal soluton technque makes smplfyng assumptons such as a constant

More information

EN40: Dynamics and Vibrations. Homework 4: Work, Energy and Linear Momentum Due Friday March 1 st

EN40: Dynamics and Vibrations. Homework 4: Work, Energy and Linear Momentum Due Friday March 1 st EN40: Dynamcs and bratons Homework 4: Work, Energy and Lnear Momentum Due Frday March 1 st School of Engneerng Brown Unversty 1. The fgure (from ths publcaton) shows the energy per unt area requred to

More information

Modal Strain Energy Decomposition Method for Damage Detection of an Offshore Structure Using Modal Testing Information

Modal Strain Energy Decomposition Method for Damage Detection of an Offshore Structure Using Modal Testing Information Thrd Chnese-German Jont Symposum on Coastal and Ocean Engneerng Natonal Cheng Kung Unversty, Tanan November 8-16, 2006 Modal Stran Energy Decomposton Method for Damage Detecton of an Offshore Structure

More information

Process Modeling. Improving or understanding chemical process operation is a major objective for developing a dynamic process model

Process Modeling. Improving or understanding chemical process operation is a major objective for developing a dynamic process model Process Modelng Improvng or understandng chemcal process operaton s a major objectve for developng a dynamc process model Balance equatons Steady-state balance equatons mass or energy mass or energy enterng

More information

ONE DIMENSIONAL TRIANGULAR FIN EXPERIMENT. Technical Advisor: Dr. D.C. Look, Jr. Version: 11/03/00

ONE DIMENSIONAL TRIANGULAR FIN EXPERIMENT. Technical Advisor: Dr. D.C. Look, Jr. Version: 11/03/00 ONE IMENSIONAL TRIANGULAR FIN EXPERIMENT Techncal Advsor: r..c. Look, Jr. Verson: /3/ 7. GENERAL OJECTIVES a) To understand a one-dmensonal epermental appromaton. b) To understand the art of epermental

More information

Module 3: The Whole-Process Perspective for Thermochemical Hydrogen

Module 3: The Whole-Process Perspective for Thermochemical Hydrogen "Thermodynamc Analyss of Processes for Hydrogen Generaton by Decomposton of Water" by John P. O'Connell Department of Chemcal Engneerng Unversty of Vrgna Charlottesvlle, VA 2294-4741 A Set of Energy Educaton

More information

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS Avalable onlne at http://sck.org J. Math. Comput. Sc. 3 (3), No., 6-3 ISSN: 97-537 COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

More information

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X Statstcs 1: Probablty Theory II 37 3 EPECTATION OF SEVERAL RANDOM VARIABLES As n Probablty Theory I, the nterest n most stuatons les not on the actual dstrbuton of a random vector, but rather on a number

More information

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng

More information

Chapter 11: Simple Linear Regression and Correlation

Chapter 11: Simple Linear Regression and Correlation Chapter 11: Smple Lnear Regresson and Correlaton 11-1 Emprcal Models 11-2 Smple Lnear Regresson 11-3 Propertes of the Least Squares Estmators 11-4 Hypothess Test n Smple Lnear Regresson 11-4.1 Use of t-tests

More information

Operating conditions of a mine fan under conditions of variable resistance

Operating conditions of a mine fan under conditions of variable resistance Paper No. 11 ISMS 216 Operatng condtons of a mne fan under condtons of varable resstance Zhang Ynghua a, Chen L a, b, Huang Zhan a, *, Gao Yukun a a State Key Laboratory of Hgh-Effcent Mnng and Safety

More information

Workshop: Approximating energies and wave functions Quantum aspects of physical chemistry

Workshop: Approximating energies and wave functions Quantum aspects of physical chemistry Workshop: Approxmatng energes and wave functons Quantum aspects of physcal chemstry http://quantum.bu.edu/pltl/6/6.pdf Last updated Thursday, November 7, 25 7:9:5-5: Copyrght 25 Dan Dll (dan@bu.edu) Department

More information

Department of Electrical & Electronic Engineeing Imperial College London. E4.20 Digital IC Design. Median Filter Project Specification

Department of Electrical & Electronic Engineeing Imperial College London. E4.20 Digital IC Design. Median Filter Project Specification Desgn Project Specfcaton Medan Flter Department of Electrcal & Electronc Engneeng Imperal College London E4.20 Dgtal IC Desgn Medan Flter Project Specfcaton A medan flter s used to remove nose from a sampled

More information

Measurement Uncertainties Reference

Measurement Uncertainties Reference Measurement Uncertantes Reference Introducton We all ntutvely now that no epermental measurement can be perfect. It s possble to mae ths dea quanttatve. It can be stated ths way: the result of an ndvdual

More information

Solution Thermodynamics

Solution Thermodynamics Soluton hermodynamcs usng Wagner Notaton by Stanley. Howard Department of aterals and etallurgcal Engneerng South Dakota School of nes and echnology Rapd Cty, SD 57701 January 7, 001 Soluton hermodynamcs

More information

Chapter 13: Multiple Regression

Chapter 13: Multiple Regression Chapter 13: Multple Regresson 13.1 Developng the multple-regresson Model The general model can be descrbed as: It smplfes for two ndependent varables: The sample ft parameter b 0, b 1, and b are used to

More information

Department of Statistics University of Toronto STA305H1S / 1004 HS Design and Analysis of Experiments Term Test - Winter Solution

Department of Statistics University of Toronto STA305H1S / 1004 HS Design and Analysis of Experiments Term Test - Winter Solution Department of Statstcs Unversty of Toronto STA35HS / HS Desgn and Analyss of Experments Term Test - Wnter - Soluton February, Last Name: Frst Name: Student Number: Instructons: Tme: hours. Ads: a non-programmable

More information

Strength Requirements for Fore Deck Fittings and Equipment

Strength Requirements for Fore Deck Fittings and Equipment (Nov 2002) (Rev.1 March 2003) (Corr.1 July 2003) (Rev.2 Nov 2003) (Rev.3 July 2004) (Rev.4 Nov 2004) (Rev.5 May 2010) Strength Requrements for Fore Deck Fttngs and Equpment 1. General 1.1 Ths UR S 27 provdes

More information

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look

More information

x = , so that calculated

x = , so that calculated Stat 4, secton Sngle Factor ANOVA notes by Tm Plachowsk n chapter 8 we conducted hypothess tests n whch we compared a sngle sample s mean or proporton to some hypotheszed value Chapter 9 expanded ths to

More information

The optimal delay of the second test is therefore approximately 210 hours earlier than =2.

The optimal delay of the second test is therefore approximately 210 hours earlier than =2. THE IEC 61508 FORMULAS 223 The optmal delay of the second test s therefore approxmately 210 hours earler than =2. 8.4 The IEC 61508 Formulas IEC 61508-6 provdes approxmaton formulas for the PF for smple

More information

Chapter 6 Electrical Systems and Electromechanical Systems

Chapter 6 Electrical Systems and Electromechanical Systems ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems Chapter 6 Electrcal Systems and Electromechancal Systems 6. INTODUCTION A. Bazoune The majorty of engneerng systems

More information

EURAMET.M.D-S2 Final Report Final report

EURAMET.M.D-S2 Final Report Final report Fnal report on ERAMET blateral comparson on volume of mass standards Project number: 1356 (ERAMET.M.D-S2) Volume of mass standards of 10g, 20 g, 200 g, 1 kg Zoltan Zelenka 1 ; Stuart Davdson 2 ; Cslla

More information

Principles of Food and Bioprocess Engineering (FS 231) Solutions to Example Problems on Heat Transfer

Principles of Food and Bioprocess Engineering (FS 231) Solutions to Example Problems on Heat Transfer Prncples of Food and Boprocess Engneerng (FS 31) Solutons to Example Problems on Heat Transfer 1. We start wth Fourer s law of heat conducton: Q = k A ( T/ x) Rearrangng, we get: Q/A = k ( T/ x) Here,

More information

Analysis of the Magnetomotive Force of a Three-Phase Winding with Concentrated Coils and Different Symmetry Features

Analysis of the Magnetomotive Force of a Three-Phase Winding with Concentrated Coils and Different Symmetry Features Analyss of the Magnetomotve Force of a Three-Phase Wndng wth Concentrated Cols and Dfferent Symmetry Features Deter Gerlng Unversty of Federal Defense Munch, Neubberg, 85579, Germany Emal: Deter.Gerlng@unbw.de

More information

Winter 2008 CS567 Stochastic Linear/Integer Programming Guest Lecturer: Xu, Huan

Winter 2008 CS567 Stochastic Linear/Integer Programming Guest Lecturer: Xu, Huan Wnter 2008 CS567 Stochastc Lnear/Integer Programmng Guest Lecturer: Xu, Huan Class 2: More Modelng Examples 1 Capacty Expanson Capacty expanson models optmal choces of the tmng and levels of nvestments

More information

Module 9. Lecture 6. Duality in Assignment Problems

Module 9. Lecture 6. Duality in Assignment Problems Module 9 1 Lecture 6 Dualty n Assgnment Problems In ths lecture we attempt to answer few other mportant questons posed n earler lecture for (AP) and see how some of them can be explaned through the concept

More information

Topic 23 - Randomized Complete Block Designs (RCBD)

Topic 23 - Randomized Complete Block Designs (RCBD) Topc 3 ANOVA (III) 3-1 Topc 3 - Randomzed Complete Block Desgns (RCBD) Defn: A Randomzed Complete Block Desgn s a varant of the completely randomzed desgn (CRD) that we recently learned. In ths desgn,

More information

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law:

Introduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law: CE304, Sprng 2004 Lecture 4 Introducton to Vapor/Lqud Equlbrum, part 2 Raoult s Law: The smplest model that allows us do VLE calculatons s obtaned when we assume that the vapor phase s an deal gas, and

More information

Chapter 4. Velocity analysis

Chapter 4. Velocity analysis 1 Chapter 4 Velocty analyss Introducton The objectve of velocty analyss s to determne the sesmc veloctes of layers n the subsurface. Sesmc veloctes are used n many processng and nterpretaton stages such

More information

Difference Equations

Difference Equations Dfference Equatons c Jan Vrbk 1 Bascs Suppose a sequence of numbers, say a 0,a 1,a,a 3,... s defned by a certan general relatonshp between, say, three consecutve values of the sequence, e.g. a + +3a +1

More information

Constitutive Modelling of Superplastic AA-5083

Constitutive Modelling of Superplastic AA-5083 TECHNISCHE MECHANIK, 3, -5, (01, 1-6 submtted: September 19, 011 Consttutve Modellng of Superplastc AA-5083 G. Gulano In ths study a fast procedure for determnng the constants of superplastc 5083 Al alloy

More information

8 Derivation of Network Rate Equations from Single- Cell Conductance Equations

8 Derivation of Network Rate Equations from Single- Cell Conductance Equations Physcs 178/278 - Davd Klenfeld - Wnter 2015 8 Dervaton of Network Rate Equatons from Sngle- Cell Conductance Equatons We consder a network of many neurons, each of whch obeys a set of conductancebased,

More information

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD Ákos Jósef Lengyel, István Ecsed Assstant Lecturer, Professor of Mechancs, Insttute of Appled Mechancs, Unversty of Mskolc, Mskolc-Egyetemváros,

More information

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle

More information

Chapter - 2. Distribution System Power Flow Analysis

Chapter - 2. Distribution System Power Flow Analysis Chapter - 2 Dstrbuton System Power Flow Analyss CHAPTER - 2 Radal Dstrbuton System Load Flow 2.1 Introducton Load flow s an mportant tool [66] for analyzng electrcal power system network performance. Load

More information

9 Derivation of Rate Equations from Single-Cell Conductance (Hodgkin-Huxley-like) Equations

9 Derivation of Rate Equations from Single-Cell Conductance (Hodgkin-Huxley-like) Equations Physcs 171/271 - Chapter 9R -Davd Klenfeld - Fall 2005 9 Dervaton of Rate Equatons from Sngle-Cell Conductance (Hodgkn-Huxley-lke) Equatons We consder a network of many neurons, each of whch obeys a set

More information

Chapter 5 Multilevel Models

Chapter 5 Multilevel Models Chapter 5 Multlevel Models 5.1 Cross-sectonal multlevel models 5.1.1 Two-level models 5.1.2 Multple level models 5.1.3 Multple level modelng n other felds 5.2 Longtudnal multlevel models 5.2.1 Two-level

More information

An Interactive Optimisation Tool for Allocation Problems

An Interactive Optimisation Tool for Allocation Problems An Interactve Optmsaton ool for Allocaton Problems Fredr Bonäs, Joam Westerlund and apo Westerlund Process Desgn Laboratory, Faculty of echnology, Åbo Aadem Unversty, uru 20500, Fnland hs paper presents

More information

Inductance Calculation for Conductors of Arbitrary Shape

Inductance Calculation for Conductors of Arbitrary Shape CRYO/02/028 Aprl 5, 2002 Inductance Calculaton for Conductors of Arbtrary Shape L. Bottura Dstrbuton: Internal Summary In ths note we descrbe a method for the numercal calculaton of nductances among conductors

More information

ECE559VV Project Report

ECE559VV Project Report ECE559VV Project Report (Supplementary Notes Loc Xuan Bu I. MAX SUM-RATE SCHEDULING: THE UPLINK CASE We have seen (n the presentaton that, for downlnk (broadcast channels, the strategy maxmzng the sum-rate

More information

Norm Bounds for a Transformed Activity Level. Vector in Sraffian Systems: A Dual Exercise

Norm Bounds for a Transformed Activity Level. Vector in Sraffian Systems: A Dual Exercise ppled Mathematcal Scences, Vol. 4, 200, no. 60, 2955-296 Norm Bounds for a ransformed ctvty Level Vector n Sraffan Systems: Dual Exercse Nkolaos Rodousaks Department of Publc dmnstraton, Panteon Unversty

More information

8 Derivation of Network Rate Equations from Single- Cell Conductance Equations

8 Derivation of Network Rate Equations from Single- Cell Conductance Equations Physcs 178/278 - Davd Klenfeld - Wnter 2019 8 Dervaton of Network Rate Equatons from Sngle- Cell Conductance Equatons Our goal to derve the form of the abstract quanttes n rate equatons, such as synaptc

More information

For now, let us focus on a specific model of neurons. These are simplified from reality but can achieve remarkable results.

For now, let us focus on a specific model of neurons. These are simplified from reality but can achieve remarkable results. Neural Networks : Dervaton compled by Alvn Wan from Professor Jtendra Malk s lecture Ths type of computaton s called deep learnng and s the most popular method for many problems, such as computer vson

More information

Fundamental loop-current method using virtual voltage sources technique for special cases

Fundamental loop-current method using virtual voltage sources technique for special cases Fundamental loop-current method usng vrtual voltage sources technque for specal cases George E. Chatzaraks, 1 Marna D. Tortorel 1 and Anastasos D. Tzolas 1 Electrcal and Electroncs Engneerng Departments,

More information

LNG CARGO TRANSFER CALCULATION METHODS AND ROUNDING-OFFS

LNG CARGO TRANSFER CALCULATION METHODS AND ROUNDING-OFFS CARGO TRANSFER CALCULATION METHODS AND ROUNDING-OFFS CONTENTS 1. Method for determnng transferred energy durng cargo transfer. Calculatng the transferred energy.1 Calculatng the gross transferred energy.1.1

More information

MA 323 Geometric Modelling Course Notes: Day 13 Bezier Curves & Bernstein Polynomials

MA 323 Geometric Modelling Course Notes: Day 13 Bezier Curves & Bernstein Polynomials MA 323 Geometrc Modellng Course Notes: Day 13 Bezer Curves & Bernsten Polynomals Davd L. Fnn Over the past few days, we have looked at de Casteljau s algorthm for generatng a polynomal curve, and we have

More information

Study on Non-Linear Dynamic Characteristic of Vehicle. Suspension Rubber Component

Study on Non-Linear Dynamic Characteristic of Vehicle. Suspension Rubber Component Study on Non-Lnear Dynamc Characterstc of Vehcle Suspenson Rubber Component Zhan Wenzhang Ln Y Sh GuobaoJln Unversty of TechnologyChangchun, Chna Wang Lgong (MDI, Chna [Abstract] The dynamc characterstc

More information

Chapter 3 Describing Data Using Numerical Measures

Chapter 3 Describing Data Using Numerical Measures Chapter 3 Student Lecture Notes 3-1 Chapter 3 Descrbng Data Usng Numercal Measures Fall 2006 Fundamentals of Busness Statstcs 1 Chapter Goals To establsh the usefulness of summary measures of data. The

More information

Numerical Heat and Mass Transfer

Numerical Heat and Mass Transfer Master degree n Mechancal Engneerng Numercal Heat and Mass Transfer 06-Fnte-Dfference Method (One-dmensonal, steady state heat conducton) Fausto Arpno f.arpno@uncas.t Introducton Why we use models and

More information

ASSOCIATION POUR LA CERTIFICATION DES MATERIAUX ISOLANTS

ASSOCIATION POUR LA CERTIFICATION DES MATERIAUX ISOLANTS Revson ndex Date of mplementaton C 15/03/017 Techncal Specfcaton E ASSOCIATIO POUR LA CERTIFICATIO DES MATERIAUX ISOLATS 4, avenue du Recteur-Poncaré, 7578 Pars Cedex 16 Tel. 33.(0)1.64.68.84.97 Fax. 33.(0)1.64.68.83.45

More information

Statistical Evaluation of WATFLOOD

Statistical Evaluation of WATFLOOD tatstcal Evaluaton of WATFLD By: Angela MacLean, Dept. of Cvl & Envronmental Engneerng, Unversty of Waterloo, n. ctober, 005 The statstcs program assocated wth WATFLD uses spl.csv fle that s produced wth

More information

Indeterminate pin-jointed frames (trusses)

Indeterminate pin-jointed frames (trusses) Indetermnate pn-jonted frames (trusses) Calculaton of member forces usng force method I. Statcal determnacy. The degree of freedom of any truss can be derved as: w= k d a =, where k s the number of all

More information

Pressure Measurements Laboratory

Pressure Measurements Laboratory Lab # Pressure Measurements Laboratory Objectves:. To get hands-on experences on how to make pressure (surface pressure, statc pressure and total pressure nsde flow) measurements usng conventonal pressuremeasurng

More information

A Mathematical Model for Infiltration Heat Recovery

A Mathematical Model for Infiltration Heat Recovery A Mathematcal Model for Infltraton Heat Recovery C. R. Buchanan and M. H. Sherman 1 Energy Performance of Buldngs Group Indoor Envronment Department Envronmental Energy Technologes Dvson Lawrence Berkeley

More information

Supplementary Notes for Chapter 9 Mixture Thermodynamics

Supplementary Notes for Chapter 9 Mixture Thermodynamics Supplementary Notes for Chapter 9 Mxture Thermodynamcs Key ponts Nne major topcs of Chapter 9 are revewed below: 1. Notaton and operatonal equatons for mxtures 2. PVTN EOSs for mxtures 3. General effects

More information

Foundations of Arithmetic

Foundations of Arithmetic Foundatons of Arthmetc Notaton We shall denote the sum and product of numbers n the usual notaton as a 2 + a 2 + a 3 + + a = a, a 1 a 2 a 3 a = a The notaton a b means a dvdes b,.e. ac = b where c s an

More information

The Analysis of Convection Experiment

The Analysis of Convection Experiment Internatonal Conference on Appled Scence and Engneerng Innovaton (ASEI 5) The Analyss of Convecton Experment Zlong Zhang School of North Chna Electrc Power Unversty, Baodng 7, Chna 469567@qq.com Keywords:

More information

Copyright 2017 by Taylor Enterprises, Inc., All Rights Reserved. Adjusted Control Limits for P Charts. Dr. Wayne A. Taylor

Copyright 2017 by Taylor Enterprises, Inc., All Rights Reserved. Adjusted Control Limits for P Charts. Dr. Wayne A. Taylor Taylor Enterprses, Inc. Control Lmts for P Charts Copyrght 2017 by Taylor Enterprses, Inc., All Rghts Reserved. Control Lmts for P Charts Dr. Wayne A. Taylor Abstract: P charts are used for count data

More information

N- and P-Channel 20-V (D-S) MOSFET

N- and P-Channel 20-V (D-S) MOSFET S45DY N- and P-Channel -V (D-S) MOSFET PRODUCT SUMMARY V DS (V) R DS(on) (Ω) (A).45 at V GS = V 9.6 N-Channel.7 at V GS = 4.5 V.6 FEATURES Halogen-free Accordng to IEC 649-- Defnton TrenchFET Power MOSFET

More information

Statistical Energy Analysis for High Frequency Acoustic Analysis with LS-DYNA

Statistical Energy Analysis for High Frequency Acoustic Analysis with LS-DYNA 14 th Internatonal Users Conference Sesson: ALE-FSI Statstcal Energy Analyss for Hgh Frequency Acoustc Analyss wth Zhe Cu 1, Yun Huang 1, Mhamed Soul 2, Tayeb Zeguar 3 1 Lvermore Software Technology Corporaton

More information

Adiabatic Sorption of Ammonia-Water System and Depicting in p-t-x Diagram

Adiabatic Sorption of Ammonia-Water System and Depicting in p-t-x Diagram Adabatc Sorpton of Ammona-Water System and Depctng n p-t-x Dagram J. POSPISIL, Z. SKALA Faculty of Mechancal Engneerng Brno Unversty of Technology Techncka 2, Brno 61669 CZECH REPUBLIC Abstract: - Absorpton

More information

Frequency dependence of the permittivity

Frequency dependence of the permittivity Frequency dependence of the permttvty February 7, 016 In materals, the delectrc constant and permeablty are actually frequency dependent. Ths does not affect our results for sngle frequency modes, but

More information

829. An adaptive method for inertia force identification in cantilever under moving mass

829. An adaptive method for inertia force identification in cantilever under moving mass 89. An adaptve method for nerta force dentfcaton n cantlever under movng mass Qang Chen 1, Mnzhuo Wang, Hao Yan 3, Haonan Ye 4, Guola Yang 5 1,, 3, 4 Department of Control and System Engneerng, Nanng Unversty,

More information

Infiltration Heat Recovery in Building Walls: Computational Fluid Dynamics Investigations Results

Infiltration Heat Recovery in Building Walls: Computational Fluid Dynamics Investigations Results LBNL-534 Infltraton Heat Recovery n Buldng Walls: Computatonal Flud Dynamcs Investgatons Results Marc O. Abade, Elzabeth U. Fnlayson and Ashok J. Gadgl Lawrence Berkeley Natonal Laboratory Envronmental

More information

A PROCEDURE FOR SIMULATING THE NONLINEAR CONDUCTION HEAT TRANSFER IN A BODY WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY.

A PROCEDURE FOR SIMULATING THE NONLINEAR CONDUCTION HEAT TRANSFER IN A BODY WITH TEMPERATURE DEPENDENT THERMAL CONDUCTIVITY. Proceedngs of the th Brazlan Congress of Thermal Scences and Engneerng -- ENCIT 006 Braz. Soc. of Mechancal Scences and Engneerng -- ABCM, Curtba, Brazl,- Dec. 5-8, 006 A PROCEDURE FOR SIMULATING THE NONLINEAR

More information

LINEAR REGRESSION ANALYSIS. MODULE IX Lecture Multicollinearity

LINEAR REGRESSION ANALYSIS. MODULE IX Lecture Multicollinearity LINEAR REGRESSION ANALYSIS MODULE IX Lecture - 30 Multcollnearty Dr. Shalabh Department of Mathematcs and Statstcs Indan Insttute of Technology Kanpur 2 Remedes for multcollnearty Varous technques have

More information

ENERGY SAVING SOLAR FACADE FOR NON-RESIDENTIAL BUILDINGS FOR CLIMATIC CONDITION IN THE CZECH REPUBLIC

ENERGY SAVING SOLAR FACADE FOR NON-RESIDENTIAL BUILDINGS FOR CLIMATIC CONDITION IN THE CZECH REPUBLIC ENERGY SAVING SOLAR FACADE FOR NON-RESIDENTIAL BUILDINGS FOR CLIMATIC CONDITION IN THE CZECH REPUBLIC Jr Sedlak and Mlos Kalousek Department of Buldng Desgn Engneerng, Faculty of Cvl Engneerng, Techncal

More information

Section 8.3 Polar Form of Complex Numbers

Section 8.3 Polar Form of Complex Numbers 80 Chapter 8 Secton 8 Polar Form of Complex Numbers From prevous classes, you may have encountered magnary numbers the square roots of negatve numbers and, more generally, complex numbers whch are the

More information

One-sided finite-difference approximations suitable for use with Richardson extrapolation

One-sided finite-difference approximations suitable for use with Richardson extrapolation Journal of Computatonal Physcs 219 (2006) 13 20 Short note One-sded fnte-dfference approxmatons sutable for use wth Rchardson extrapolaton Kumar Rahul, S.N. Bhattacharyya * Department of Mechancal Engneerng,

More information

Multiple Contrasts (Simulation)

Multiple Contrasts (Simulation) Chapter 590 Multple Contrasts (Smulaton) Introducton Ths procedure uses smulaton to analyze the power and sgnfcance level of two multple-comparson procedures that perform two-sded hypothess tests of contrasts

More information

The equation of motion of a dynamical system is given by a set of differential equations. That is (1)

The equation of motion of a dynamical system is given by a set of differential equations. That is (1) Dynamcal Systems Many engneerng and natural systems are dynamcal systems. For example a pendulum s a dynamcal system. State l The state of the dynamcal system specfes t condtons. For a pendulum n the absence

More information

Second Order Analysis

Second Order Analysis Second Order Analyss In the prevous classes we looked at a method that determnes the load correspondng to a state of bfurcaton equlbrum of a perfect frame by egenvalye analyss The system was assumed to

More information

since [1-( 0+ 1x1i+ 2x2 i)] [ 0+ 1x1i+ assumed to be a reasonable approximation

since [1-( 0+ 1x1i+ 2x2 i)] [ 0+ 1x1i+ assumed to be a reasonable approximation Econ 388 R. Butler 204 revsons Lecture 4 Dummy Dependent Varables I. Lnear Probablty Model: the Regresson model wth a dummy varables as the dependent varable assumpton, mplcaton regular multple regresson

More information

International Power, Electronics and Materials Engineering Conference (IPEMEC 2015)

International Power, Electronics and Materials Engineering Conference (IPEMEC 2015) Internatonal Power, Electroncs and Materals Engneerng Conference (IPEMEC 2015) Dynamc Model of Wnd Speed Dstrbuton n Wnd Farm Consderng the Impact of Wnd Drecton and Interference Effects Zhe Dong 1, a,

More information

Lecture 8 Modal Analysis

Lecture 8 Modal Analysis Lecture 8 Modal Analyss 16.0 Release Introducton to ANSYS Mechancal 1 2015 ANSYS, Inc. February 27, 2015 Chapter Overvew In ths chapter free vbraton as well as pre-stressed vbraton analyses n Mechancal

More information

= = = (a) Use the MATLAB command rref to solve the system. (b) Let A be the coefficient matrix and B be the right-hand side of the system.

= = = (a) Use the MATLAB command rref to solve the system. (b) Let A be the coefficient matrix and B be the right-hand side of the system. Chapter Matlab Exercses Chapter Matlab Exercses. Consder the lnear system of Example n Secton.. x x x y z y y z (a) Use the MATLAB command rref to solve the system. (b) Let A be the coeffcent matrx and

More information

ESCI Cloud Physics and Precipitation Processes Lesson 4 - Convection Dr. DeCaria

ESCI Cloud Physics and Precipitation Processes Lesson 4 - Convection Dr. DeCaria References: ESCI 340 - Cloud Physcs and Precptaton Processes Lesson 4 - Convecton Dr. DeCara Glossary of Meteorology, 2nd ed., Amercan Meteorologcal Socety A Short Course n Cloud Physcs, 3rd ed., Rogers

More information

Resource Allocation with a Budget Constraint for Computing Independent Tasks in the Cloud

Resource Allocation with a Budget Constraint for Computing Independent Tasks in the Cloud Resource Allocaton wth a Budget Constrant for Computng Independent Tasks n the Cloud Wemng Sh and Bo Hong School of Electrcal and Computer Engneerng Georga Insttute of Technology, USA 2nd IEEE Internatonal

More information