APPLICATION OF WATER EQUIVALENTS METHOD TO CALCULATION OF CERAMIC HEAT EXCHANGERS

Size: px
Start display at page:

Download "APPLICATION OF WATER EQUIVALENTS METHOD TO CALCULATION OF CERAMIC HEAT EXCHANGERS"

Transcription

1 METALLURGY AND FOUNDRY ENGINEERING Vol. 35, 2009, No. 2 Krzysztof Krczewski* APPLICATION OF WATER EQUIVALENTS METHOD TO CALCULATION OF CERAMIC HEAT EXCHANGERS Nottion: c het cpcity of ir, kj/(m 3 K), c g het cpcity of furnce gs, kj/(m 3 K), D, d dimeter, m, ε het effectiveness, F heting surfce re, m 2, k over-ll het-trnsfer coefficient, W/(m 2 K), N Number of Het Trnsfer Units, T, t temperture, K, o C, V volumetric rte of fluid flow, m 3 /h, m 3 /s, W wter equivlent of ir, W/K, W g wter equivlent of furnce gs, W/K. 1. INTRODUCTION Cermic recupertors re used for the recovery of het from wste gses with industril het furnces nd glss tnks [1, 2, 3, 5]. In ZM Ropczyce [10] production of new genertion mgnesi shpes to cermic recupertors ws developed nd included to glss furnces. On ccount of mteril costs the cermic recupertor re clculted by mthemticl * Ph.D.: Fculty of Metls Engineering nd Industril Computer Sciences, AGH University of Science nd Technology, Krków, Polnd; e-mil: ztc@gh.edu.pl 137

2 method to chieve required construction nd service chrcteristic for miniml number of shpes. For clcultion of cermic recupertor mde of new genertion shpes the blnce method were elborted [5]. In clcultion of het exchngers the wter equivlents method is very importnt [7, 8, 9]. This method is more universl thn blnce method. The im of this pper is presenttion of mthemtic model nd clcultion lgorithm by wter equivlents method the cermic recupertor mde of mgnesi shpes. 2. SIMILARITY FUNCTION USED TO CALCULATE THE HEATING SURFACE OF CROSS-FLOW CERAMIC HEAT EXCHANGERS Cermic recupertors belong to cross-flow het exchngers group. The wter equivlent method enbles to clculte the construction prmeters of het exchngers. In recupertors recovered furnce gs from industril furnces wter equivlent of furnce gs is: W g = V g c g V g volumetric rte of furnce gs flow, het cpcity of furnce gs. c g (1) Wter equivlent of ir is: W = V c V volumetric rte of ir, het cpcity of ir. c (2) Wter equivlent of furnce gs is bigger thn ir wter equivlent: W g > W (3) The similrity function (Fig. 1) used in cross-flow het exchngers is [4, 9] expressed by eqution: Wg ε= f,n (4) W t t ε= tg t t ir preheted temperture outlet, t ir temperture inlet to recupertor, t g furnce gs temperture inlet to recupertor, N Number of Het Trnsfer Units. (5) 138

3 ) b) Wg Fig. 1. Similrity function ε= f,n used in cross-flow exchngers [9]: W ) prllel flow; b) counter flow The Number of Het Trnsfer Units is the mesure of het surfce re nd is expressed by eqution: kf N = W k over-ll het trnsfer coefficient, F het trnsfer surfce re, W wter equivlent of ir. (6) 139

4 3. THE CALCULATION OF CERAMIC HEAT EXCHANGERS BY WATER EQUIVALENT METHOD The proposed lgorithm of clcultion of cermic recupertor consists eqution. The volumetric rte of ir outlet from recupertor is = 1 n where n untight of ir chnnel. (7) The rithmetic men of volumetric rte of ir + = 2 The bsolute untight of ir equls Δ = The volumetric rte of furnce gs outlet from recupertor is V = V +ΔV g g (8) (9) (10) The ir wter equivlent is W = c where c het cpcity of ir. (11) The rithmetic men of volumetric rte of furnce gs is V g Vg + Vg = 2 The furnce gs wter equivlent equls (12) Wg = Vgcg (13) where c g het cpcity of furnce gs. The microfinned surfce re of cermic recupertor is NW F = k N Number of Het Trnsfer Units, W wter equivlent of ir, k over-ll het trnsfer coefficient. (14) 140

5 4. THE CALCULATIONS OF CERAMIC RECUPERATOR TO GLASS TANK The cermic recupertor uses het of wste gs from glss tnk. Preheting in recupertor ir is used directly in combustion of fuel. The recupertor works in cross-flow nd hs the following prmeters: volumetric rte of ir V = 1000 m 3 /h (0.278 m 3 /s), inlet ir temperture t C, outlet ir temperture t C, volumetric rte of furnce gs inlet to recupertor V g = 1200 m 3 /h (0.33 m 3 /s), inlet furnce gs to recupertor t g = 1300 o C. The recupertor mde of mgnesi shpes illustrtes Figure 2 with the following dimensions: outer dimeter of tube D = m, inner dimeter of tube d = m, thickness of tube wll s = m, totl height h = m, height of het element h 1 = m, pitch of shpes p = 0.11 m. Fig. 2. Mgnesi M98G recupertor shpe 141

6 The volumetric rte of ir inlet to recupertor is: = = = 1176 m /h (0.327 m /s), 1 n where n untight of ir chnnel. The rithmetic men of volumetric rte of ir is: = = = m /s. 2 2 The bsolute untight of ir equls: 3 Δ = = = 176 m /h. The volumetric rte of furnce gs outlet from recupertor is: 3 3 V = V +Δ V = = 1376 m /h = m /s. g g The ir wter equivlent is: W = V c = = W/K, where het cpcity of ir c = 1350 J/(m 3 K). The rithmetic men of volumetric rte of furnce gs equls: V g Vg + Vg = = = m /s. 2 2 The furnce gs wter equivlent is: Wg = Vg cg = = W/K, where het cpcity of furnce gs c g = 1640 J/(m 3 K). The simplex of wter equivlent is: Wg W = = 142

7 The het effectiveness of recupertor is expressed by eqution: t t ε= = = t t g The Number of Het Trnsfer Units by Figure 1b is N = 0.8. The over-ll het-trnsfer coefficient is k = 7.5 W/(m 2 K). The surfce re of recupertor is NW F = = = 43.6 /m. k 7.5 The number of shpes in recupertor equls: F 43.6 L = = = 321, dmitted 336. f The het surfce re [10] of cermic shpe is f 1 = m 2. The recupertor row of shpes in lger is: x y = 8 7 = 56. The number of rows on height of recupertor equls: L 336 z = = = The cermic het exchnger chmbers over-ll dimensions re the following: length = 2.4 m, width = 2.1 m, height = 2.4 m. The het surfce res clculted by blnce method [6] is 45.3 m 2. The het surfce re clculted by wter equivlents method is 43.6 m 2. The differences of surfce is: Δ= 100% = 3.8% The cermic recupertor to glss tnk using Glsmg M98G mterils illustrtes Figure

8 Fig. 3. Cermic recupertor to tnk furnce 5. INFERENCES Cermic exchngers using energy of flue gses from glss melting furnces on ccount of high-temperture, dust, nd therml shocks work in very difficult conditions. The service life of glss melting tnks is determined by effectiveness of het exchngers. Therefore new models of cermic recupertors mde of mgnesi or luminmullite-zircon shpes re introduce into service. By wter equivlents method mthemtic model nd lgorithm of clcultions the recupertors mde of mgnesi shpes were elborted. This model mkes possible to define recupertor s design: over ll dimensions, het surfce re nd lttice work of shpes. By the model cermic recupertor to glss melting tnk were clculted. The difference of het surfce res clculted by blnce method nd wter equivlents method is 3.8%. REFERENCES [1] Krczewski K.: Metllic Recupertors to Glss Tnks, Technicl University of Kosice, Kosice, 1998 [2] Krczewski K.: Wp³yw mikrou ebrowni powierzchni równoleg³opr¹dowych rekupertorów metlowych n ich cechy konstrukcyjne i eksplotcyjne, UWND AGH, Krków,

9 [3] Krczewski K.: Foundry nd Metllurgy Engineering, 29 (2003) [4] Krczewski K.: Obliczeni cieplne rekupertorów metlowych dl pieców przemys³owych, UWND AGH, Krków, 2004, SU 1667 [5] Krczewski K.: Metllurgy nd Foundry Engineering, 32 (2006) [6] Krczewski K.: Metllurgy nd Foundry Engineering, 34 (2008) [7] Mikheyev M.: Fundmentls of Het Trnsfer. Mir Publishers, Moscow, 1968 [8] Senkr T.: Obliczeni pieców grzewczych w hutnictwie elz, Wyd. Œl¹sk, Ktowice, 1983 [9] Tjc N.: Rszczety ngrewtielnych pieczej. Miet³³urgij, Moscow, 1969 [10] Ctlog: Glss-Mking Industry, ZM Ropczyce, 2004 Received November

APPLICATION OF WATER EQUIVALENTS METHOD TO CALCULATION OF RADIATION RECUPERATORS WITH MICROFINNED SURFACE

APPLICATION OF WATER EQUIVALENTS METHOD TO CALCULATION OF RADIATION RECUPERATORS WITH MICROFINNED SURFACE METALLURGY AND FOUNDRY ENGINEERING Vol. 34, 008, No. 1 Krzysztof Krczewski APPLICATION OF WATER EQUIVALENTS METHOD TO CALCULATION OF RADIATION RECUPERATORS WITH MICROFINNED SURFACE NOTATION: α c convection

More information

HIGH-EFFICIENCY CERAMIC RECUPERATORS TO GLASS FURNACES

HIGH-EFFICIENCY CERAMIC RECUPERATORS TO GLASS FURNACES METALLURGY AND FOUNDRY ENGINEERING Vol. 3, 006, No. 1 Krzysztof Karczewski * HIGH-EFFICIENCY CERAMIC RECUPERATORS TO GLASS FURNACES Notation: α convection heat-transfer coefficient to air, W/(m K) α g

More information

G. MATEESCU 1 A. MATEESCU 1 C. SAMOILĂ 2 D. URSUŢIU 2

G. MATEESCU 1 A. MATEESCU 1 C. SAMOILĂ 2 D. URSUŢIU 2 PRELIMINARY EXPERIMENTS OF THE NEW FACILITY AND TECHNOLOGY FOR VACUUM DRYING AND THERMAL POLIMERIZATION OF THE TURBOGENERATORS STATOR BARS INSULATION (INTEPOL) G. MATEESCU 1 A. MATEESCU 1 C. SAMOILĂ 2

More information

THE INTERVAL LATTICE BOLTZMANN METHOD FOR TRANSIENT HEAT TRANSFER IN A SILICON THIN FILM

THE INTERVAL LATTICE BOLTZMANN METHOD FOR TRANSIENT HEAT TRANSFER IN A SILICON THIN FILM ROMAI J., v.9, no.2(2013), 173 179 THE INTERVAL LATTICE BOLTZMANN METHOD FOR TRANSIENT HEAT TRANSFER IN A SILICON THIN FILM Alicj Piseck-Belkhyt, Ann Korczk Institute of Computtionl Mechnics nd Engineering,

More information

Simulated Performance of Packed Bed Solar Energy Storage System having Storage Material Elements of Large Size - Part I

Simulated Performance of Packed Bed Solar Energy Storage System having Storage Material Elements of Large Size - Part I The Open Fuels & Energy Science Journl, 2008, 1, 91-96 91 Open Access Simulted Performnce of Pcked Bed Solr Energy Storge System hving Storge Mteril Elements of Lrge Size - Prt I Rnjit Singh *,1, R.P.

More information

Thermal Performance of Electrocaloric Refrigeration using Thermal Switches of Fluid Motion and Changing Contact Conductance

Thermal Performance of Electrocaloric Refrigeration using Thermal Switches of Fluid Motion and Changing Contact Conductance Americn Journl of Physics nd Applictions 2016; 4(5): 134-139 http://www.sciencepublishinggroup.com/j/jp doi:.11648/j.jp.20160405.12 ISSN: 2330-4286 (Print); ISSN: 2330-4308 (Online) Therml Performnce of

More information

Estimation of the particle concentration in hydraulic liquid by the in-line automatic particle counter based on the CMOS image sensor

Estimation of the particle concentration in hydraulic liquid by the in-line automatic particle counter based on the CMOS image sensor Glyndŵr University Reserch Online Conference Presenttion Estimtion of the prticle concentrtion in hydrulic liquid by the in-line utomtic prticle counter bsed on the CMOS imge sensor Kornilin, D.V., Kudryvtsev,

More information

Freely propagating jet

Freely propagating jet Freely propgting jet Introduction Gseous rectnts re frequently introduced into combustion chmbers s jets. Chemicl, therml nd flow processes tht re tking plce in the jets re so complex tht nlyticl description

More information

Applications of Bernoulli s theorem. Lecture - 7

Applications of Bernoulli s theorem. Lecture - 7 Applictions of Bernoulli s theorem Lecture - 7 Prcticl Applictions of Bernoulli s Theorem The Bernoulli eqution cn be pplied to gret mny situtions not just the pipe flow we hve been considering up to now.

More information

Measuring Electron Work Function in Metal

Measuring Electron Work Function in Metal n experiment of the Electron topic Mesuring Electron Work Function in Metl Instructor: 梁生 Office: 7-318 Emil: shling@bjtu.edu.cn Purposes 1. To understnd the concept of electron work function in metl nd

More information

19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, 2-7 SEPTEMBER 2007 A NON-CONTACT SYSTEM FOR TRANSPORTING OBJECTS USING ULTRASONIC LEVITATION

19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, 2-7 SEPTEMBER 2007 A NON-CONTACT SYSTEM FOR TRANSPORTING OBJECTS USING ULTRASONIC LEVITATION 19 th INTERNATIONAL CONGRESS ON ACOUSTICS MADRID, -7 SEPTEMBER 007 A NON-CONTACT SYSTEM FOR TRANSPORTING OBJECTS USING ULTRASONIC LEVITATION PACS: 3.5.Uv Gudr, Tdeusz 1 ; Perkowski, Dniel ; Opielinski,

More information

Energy Consideration

Energy Consideration Energy Considertion It hs been noted tht the most common brkes employ friction to trnsform the brked system's mechnicl energy, irreversibly into het which is then trnsferred to the surrounding environment

More information

Determining thermal contact resistance of the fin-to-tube attachment in plate fin-and-tube heat exchanger

Determining thermal contact resistance of the fin-to-tube attachment in plate fin-and-tube heat exchanger 2 nd Interntionl Conference on Engineering Optimiztion September 6-9, 2010, Lisbon, Portugl Determining therml contct resistnce of the fin-to-tube ttchment in plte fin-nd-tube het exchnger Did Tler 1,

More information

Optimum Design of a Horizontal Condenser

Optimum Design of a Horizontal Condenser Fourth Interntionl Wter echnology Conference IWC 99, Alexndri, Egypt 9 Abstrct Optimum esign of Horizontl Condenser A.M. Abdllh nd Aly Krmeldin Atomic Energy Authority-Nucler eserch Center ectors eprtment

More information

Thermal Diffusivity. Paul Hughes. Department of Physics and Astronomy The University of Manchester Manchester M13 9PL. Second Year Laboratory Report

Thermal Diffusivity. Paul Hughes. Department of Physics and Astronomy The University of Manchester Manchester M13 9PL. Second Year Laboratory Report Therml iffusivity Pul Hughes eprtment of Physics nd Astronomy The University of nchester nchester 3 9PL Second Yer Lbortory Report Nov 4 Abstrct We investigted the therml diffusivity of cylindricl block

More information

Physics 1402: Lecture 7 Today s Agenda

Physics 1402: Lecture 7 Today s Agenda 1 Physics 1402: Lecture 7 Tody s gend nnouncements: Lectures posted on: www.phys.uconn.edu/~rcote/ HW ssignments, solutions etc. Homework #2: On Msterphysics tody: due Fridy Go to msteringphysics.com Ls:

More information

DETERMINATION OF MECHANICAL PROPERTIES OF NANOSTRUCTURES WITH COMPLEX CRYSTAL LATTICE USING MOMENT INTERACTION AT MICROSCALE

DETERMINATION OF MECHANICAL PROPERTIES OF NANOSTRUCTURES WITH COMPLEX CRYSTAL LATTICE USING MOMENT INTERACTION AT MICROSCALE Determintion RevAdvMterSci of mechnicl 0(009) -7 properties of nnostructures with complex crystl lttice using DETERMINATION OF MECHANICAL PROPERTIES OF NANOSTRUCTURES WITH COMPLEX CRYSTAL LATTICE USING

More information

Physics Lecture 14: MON 29 SEP

Physics Lecture 14: MON 29 SEP Physics 2113 Physics 2113 Lecture 14: MON 29 SEP CH25: Cpcitnce Von Kleist ws le to store electricity in the jr. Unknowingly, he h ctully invente novel evice to store potentil ifference. The wter in the

More information

Conservation Law. Chapter Goal. 5.2 Theory

Conservation Law. Chapter Goal. 5.2 Theory Chpter 5 Conservtion Lw 5.1 Gol Our long term gol is to understnd how mny mthemticl models re derived. We study how certin quntity chnges with time in given region (sptil domin). We first derive the very

More information

HT Module 2 Paper solution. Module 2. Q6.Discuss Electrical analogy of combined heat conduction and convection in a composite wall.

HT Module 2 Paper solution. Module 2. Q6.Discuss Electrical analogy of combined heat conduction and convection in a composite wall. HT Module 2 Pper solution Qulity Solutions wwwqulitytutorilin Module 2 Q6Discuss Electricl nlogy of combined het conduction nd convection in composite wll M-16-Q1(c)-5m Ans: It is frequently convient to

More information

KINEMATICS OF RIGID BODIES

KINEMATICS OF RIGID BODIES KINEMTICS OF RIGID ODIES Introduction In rigid body kinemtics, e use the reltionships governing the displcement, velocity nd ccelertion, but must lso ccount for the rottionl motion of the body. Description

More information

A formula sheet and table of physical constants is attached to this paper. Linear graph paper is available.

A formula sheet and table of physical constants is attached to this paper. Linear graph paper is available. DEPARTMENT OF PHYSICS AND ASTRONOMY Dt Provided: A formul sheet nd tble of physicl constnts is ttched to this pper. Liner grph pper is vilble. Spring Semester 2015-2016 PHYSICS 1 HOUR Answer questions

More information

What s in Chapter 13?

What s in Chapter 13? Are nd volume 13 Wht s in Chpter 13? 13 01 re 13 0 Are of circle 13 03 res of trpeziums, kites nd rhomuses 13 04 surfce re of rectngulr prism 13 05 surfce re of tringulr prism 13 06 surfce re of cylinder

More information

CONTRIBUTION TO THE EXTENDED DYNAMIC PLANE SOURCE METHOD

CONTRIBUTION TO THE EXTENDED DYNAMIC PLANE SOURCE METHOD CONTRIBUTION TO THE EXTENDED DYNAMIC PLANE SOURCE METHOD Svetozár Mlinrič Deprtment of Physics, Fculty of Nturl Sciences, Constntine the Philosopher University, Tr. A. Hlinku, SK-949 74 Nitr, Slovki Emil:

More information

Properties of Integrals, Indefinite Integrals. Goals: Definition of the Definite Integral Integral Calculations using Antiderivatives

Properties of Integrals, Indefinite Integrals. Goals: Definition of the Definite Integral Integral Calculations using Antiderivatives Block #6: Properties of Integrls, Indefinite Integrls Gols: Definition of the Definite Integrl Integrl Clcultions using Antiderivtives Properties of Integrls The Indefinite Integrl 1 Riemnn Sums - 1 Riemnn

More information

CBE 291b - Computation And Optimization For Engineers

CBE 291b - Computation And Optimization For Engineers The University of Western Ontrio Fculty of Engineering Science Deprtment of Chemicl nd Biochemicl Engineering CBE 9b - Computtion And Optimiztion For Engineers Mtlb Project Introduction Prof. A. Jutn Jn

More information

Name Class Date. Match each phrase with the correct term or terms. Terms may be used more than once.

Name Class Date. Match each phrase with the correct term or terms. Terms may be used more than once. Exercises 341 Flow of Chrge (pge 681) potentil difference 1 Chrge flows when there is between the ends of conductor 2 Explin wht would hppen if Vn de Grff genertor chrged to high potentil ws connected

More information

A study of fluid flow simulation in convergentdivergent

A study of fluid flow simulation in convergentdivergent IOP Conference Series: Mterils Science nd Engineering PAPER OPEN ACCESS A study of fluid flow simultion in convergentdivergent nozzles To cite this rticle: I Olru 2015 IOP Conf. Ser.: Mter. Sci. Eng. 95

More information

MATH SS124 Sec 39 Concepts summary with examples

MATH SS124 Sec 39 Concepts summary with examples This note is mde for students in MTH124 Section 39 to review most(not ll) topics I think we covered in this semester, nd there s exmples fter these concepts, go over this note nd try to solve those exmples

More information

CHAPTER 20: Second Law of Thermodynamics

CHAPTER 20: Second Law of Thermodynamics CHAER 0: Second Lw of hermodynmics Responses to Questions 3. kg of liquid iron will hve greter entropy, since it is less ordered thn solid iron nd its molecules hve more therml motion. In ddition, het

More information

Hints for Exercise 1 on: Current and Resistance

Hints for Exercise 1 on: Current and Resistance Hints for Exercise 1 on: Current nd Resistnce Review the concepts of: electric current, conventionl current flow direction, current density, crrier drift velocity, crrier numer density, Ohm s lw, electric

More information

Studies on Nuclear Fuel Rod Thermal Performance

Studies on Nuclear Fuel Rod Thermal Performance Avilble online t www.sciencedirect.com Energy Procedi 1 (1) 1 17 Studies on Nucler Fuel od herml Performnce Eskndri, M.1; Bvndi, A ; Mihndoost, A3* 1 Deprtment of Physics, Islmic Azd University, Shirz

More information

PROFESSIONAL ENGINEERS OF ONTARIO. ANNUAL EXAMINATIONS May Mec-B2 Environmental Control in Buildings. 3 hours duration

PROFESSIONAL ENGINEERS OF ONTARIO. ANNUAL EXAMINATIONS May Mec-B2 Environmental Control in Buildings. 3 hours duration ANNUAL EXAMINATIONS My 201 S Pge 1 of 7 07-MEC-B2 Environmentl Control in Buildings PROFESSIONAL ENGINEERS OF ONTARIO ANNUAL EXAMINATIONS My 2015 07-Mec-B2 Environmentl Control in Buildings 3 hours durtion

More information

An inverse steady state thermal stresses in a thin clamped circular plate with internal heat generation

An inverse steady state thermal stresses in a thin clamped circular plate with internal heat generation Americn Journl of Engineering Reserch (AJER) e-issn : 2320-0847 p-issn : 2320-0936 Volume-02, Issue-10, pp-276-281 www.jer.org Reserch Pper Open Access An inverse stedy stte therml stresses in thin clmped

More information

A Brief Note on Quasi Static Thermal Stresses In A Thin Rectangular Plate With Internal Heat Generation

A Brief Note on Quasi Static Thermal Stresses In A Thin Rectangular Plate With Internal Heat Generation Americn Journl of Engineering Reserch (AJER) 13 Americn Journl of Engineering Reserch (AJER) e-issn : 3-847 p-issn : 3-936 Volume-, Issue-1, pp-388-393 www.jer.org Reserch Pper Open Access A Brief Note

More information

Thin and Thick Cylinders and Spheres

Thin and Thick Cylinders and Spheres CHAPTR 8 Thin nd Thick Cylinders nd Spheres Prolem. A shell.5 m long nd m dimeter, is sujected to n internl pressure of. N/mm. If the thickness of the shell is 0 mm find the circumferentil nd longitudinl

More information

THERMAL EXPANSION COEFFICIENT OF WATER FOR VOLUMETRIC CALIBRATION

THERMAL EXPANSION COEFFICIENT OF WATER FOR VOLUMETRIC CALIBRATION XX IMEKO World Congress Metrology for Green Growth September 9,, Busn, Republic of Kore THERMAL EXPANSION COEFFICIENT OF WATER FOR OLUMETRIC CALIBRATION Nieves Medin Hed of Mss Division, CEM, Spin, mnmedin@mityc.es

More information

CHAPTER 08: MONOPROTIC ACID-BASE EQUILIBRIA

CHAPTER 08: MONOPROTIC ACID-BASE EQUILIBRIA Hrris: Quntittive Chemicl Anlysis, Eight Edition CHAPTER 08: MONOPROTIC ACIDBASE EQUILIBRIA CHAPTER 08: Opener A CHAPTER 08: Opener B CHAPTER 08: Opener C CHAPTER 08: Opener D CHAPTER 08: Opener E Chpter

More information

The heat budget of the atmosphere and the greenhouse effect

The heat budget of the atmosphere and the greenhouse effect The het budget of the tmosphere nd the greenhouse effect 1. Solr rdition 1.1 Solr constnt The rdition coming from the sun is clled solr rdition (shortwve rdition). Most of the solr rdition is visible light

More information

Exam 1 Solutions (1) C, D, A, B (2) C, A, D, B (3) C, B, D, A (4) A, C, D, B (5) D, C, A, B

Exam 1 Solutions (1) C, D, A, B (2) C, A, D, B (3) C, B, D, A (4) A, C, D, B (5) D, C, A, B PHY 249, Fll 216 Exm 1 Solutions nswer 1 is correct for ll problems. 1. Two uniformly chrged spheres, nd B, re plced t lrge distnce from ech other, with their centers on the x xis. The chrge on sphere

More information

AN IMPROVED SMALL CLOSED DRIFT THRUSTER WITH BOTH CONDUCTING AND DIELECT RIC CHANNELS

AN IMPROVED SMALL CLOSED DRIFT THRUSTER WITH BOTH CONDUCTING AND DIELECT RIC CHANNELS AN IMPROVED SMALL CLOSED DRIFT THRUSTER WITH BOTH CONDUCTING AND DIELECT RIC CHANNELS A.I.Bugrov, A.D.Desitskov, H.R.Kufmn, V.K.Khrchevnikov, A.I.Morozov c, V.V.Zhurin d Moscow Institute of Rdioelectronics,

More information

Thermodynamic analysis of geothermal heat pump during the cold season

Thermodynamic analysis of geothermal heat pump during the cold season IOP onference eries: Mterils cience nd ngineering PAPR OPN A hermodynmic nlysis of geotherml het pump during the cold seson o cite this rticle: G Dumitrcu et l 2016 IOP onf. er.: Mter. ci. ng. 147 012137

More information

ENERGY-BASED METHOD FOR GAS TURBINE ENGINE DISK BURST SPEED CALCULATION

ENERGY-BASED METHOD FOR GAS TURBINE ENGINE DISK BURST SPEED CALCULATION 28 TH INTERNATIONAL CONGRESS OF THE AERONAUTICAL SCIENCES ENERGY-BASED METHOD FOR GAS TURBINE ENGINE DISK BURST SPEED CALCULATION Anton N. Servetnik Centrl Institute of Avition Motors, Moscow, Russi servetnik@cim.ru

More information

CML: Series Low Resistance Chip Resistor Specification

CML: Series Low Resistance Chip Resistor Specification CML: Series Low Resistnce Chip Resistor Specifiction 1. Scope This specifiction pplies to CML**** Series Low Resistnce Chip Resistor for use in electric equipment. *****METAL FOIL***** 2. Prt number CML

More information

13: Diffusion in 2 Energy Groups

13: Diffusion in 2 Energy Groups 3: Diffusion in Energy Groups B. Rouben McMster University Course EP 4D3/6D3 Nucler Rector Anlysis (Rector Physics) 5 Sept.-Dec. 5 September Contents We study the diffusion eqution in two energy groups

More information

Partial Derivatives. Limits. For a single variable function f (x), the limit lim

Partial Derivatives. Limits. For a single variable function f (x), the limit lim Limits Prtil Derivtives For single vrible function f (x), the limit lim x f (x) exists only if the right-hnd side limit equls to the left-hnd side limit, i.e., lim f (x) = lim f (x). x x + For two vribles

More information

ANALYSIS OF FAST REACTORS SYSTEMS

ANALYSIS OF FAST REACTORS SYSTEMS ANALYSIS OF FAST REACTORS SYSTEMS M. Rghe 4/7/006 INTRODUCTION Fst rectors differ from therml rectors in severl spects nd require specil tretment. The prsitic cpture cross sections in the fuel, coolnt

More information

Math 124A October 04, 2011

Math 124A October 04, 2011 Mth 4A October 04, 0 Viktor Grigoryn 4 Vibrtions nd het flow In this lecture we will derive the wve nd het equtions from physicl principles. These re second order constnt coefficient liner PEs, which model

More information

Physics 2135 Exam 1 September 23, 2014

Physics 2135 Exam 1 September 23, 2014 Exm Totl Physics 2135 Exm 1 September 23, 2014 Key Printe Nme: 200 / 200 N/A Rec. Sec. Letter: Five multiple choice questions, 8 points ech. Choose the best or most nerly correct nswer. B 1. Object A hs

More information

Chapter 13 Lyes KADEM [Thermodynamics II] 2007

Chapter 13 Lyes KADEM [Thermodynamics II] 2007 Gs-Vpor Mixtures Air is mixture of nitrogen nd oxygen nd rgon plus trces of some other gses. When wtervpor is not included, we refer to it s dry ir. If wter-vpor is included, we must properly ccount for

More information

NSW Syllabus references: 5.2 M&G Area and surface area, 5.2 M&G Volume Outcomes: MA5.2-1WM, MA5.2-2WM, MA5.2-11MG, MA5.2-12MG

NSW Syllabus references: 5.2 M&G Area and surface area, 5.2 M&G Volume Outcomes: MA5.2-1WM, MA5.2-2WM, MA5.2-11MG, MA5.2-12MG SA M PL E 2 Surfce re nd volume This chpter dels with clculting the surfce res nd volumes of right prisms nd cylinders. After completing this chpter you should e le to: solve prolems involving the surfce

More information

Math 1B, lecture 4: Error bounds for numerical methods

Math 1B, lecture 4: Error bounds for numerical methods Mth B, lecture 4: Error bounds for numericl methods Nthn Pflueger 4 September 0 Introduction The five numericl methods descried in the previous lecture ll operte by the sme principle: they pproximte the

More information

Sample Exam 5 - Skip Problems 1-3

Sample Exam 5 - Skip Problems 1-3 Smple Exm 5 - Skip Problems 1-3 Physics 121 Common Exm 2: Fll 2010 Nme (Print): 4 igit I: Section: Honors Code Pledge: As n NJIT student I, pledge to comply with the provisions of the NJIT Acdemic Honor

More information

Numerical Study Of Coated Electrical Contacts

Numerical Study Of Coated Electrical Contacts Excerpt from the Proceedings of the COMSOL Conference 21 Pris Numericl Study Of Coted Electricl Contcts Per Lindholm Mchine Design KTH Brinellvägen 83 SE-144 Stockholm per@md.kth.se Abstrct: Electricl

More information

Lesson 8. Thermomechanical Measurements for Energy Systems (MENR) Measurements for Mechanical Systems and Production (MMER)

Lesson 8. Thermomechanical Measurements for Energy Systems (MENR) Measurements for Mechanical Systems and Production (MMER) Lesson 8 Thermomechnicl Mesurements for Energy Systems (MEN) Mesurements for Mechnicl Systems nd Production (MME) A.Y. 205-6 Zccri (ino ) Del Prete Mesurement of Mechnicl STAIN Strin mesurements re perhps

More information

Estimation of Global Solar Radiation at Onitsha with Regression Analysis and Artificial Neural Network Models

Estimation of Global Solar Radiation at Onitsha with Regression Analysis and Artificial Neural Network Models eserch Journl of ecent Sciences ISSN 77-5 es.j.ecent Sci. Estimtion of Globl Solr dition t Onitsh with egression Anlysis nd Artificil Neurl Network Models Abstrct Agbo G.A., Ibeh G.F. *nd Ekpe J.E. Fculty

More information

Designing Information Devices and Systems I Discussion 8B

Designing Information Devices and Systems I Discussion 8B Lst Updted: 2018-10-17 19:40 1 EECS 16A Fll 2018 Designing Informtion Devices nd Systems I Discussion 8B 1. Why Bother With Thévenin Anywy? () Find Thévenin eqiuvlent for the circuit shown elow. 2kΩ 5V

More information

NUMERICAL SIMULATION OF FRONTAL MIXED CLOUD SYSTEMS AND CLOUD MICROSTRUCTURE EFFECT ON SATELLITE SIGNAL

NUMERICAL SIMULATION OF FRONTAL MIXED CLOUD SYSTEMS AND CLOUD MICROSTRUCTURE EFFECT ON SATELLITE SIGNAL NUMERICAL SIMULATION OF FRONTAL MIXED CLOUD SYSTEMS AND CLOUD MICROSTRUCTURE EFFECT ON SATELLITE SIGNAL V. Bkhnov, O. Kryvook, B. Dormn Ukrinin Hydrometeorologicl Reserch Institute, Avenue of Science 37,

More information

An approximation to the arithmetic-geometric mean. G.J.O. Jameson, Math. Gazette 98 (2014), 85 95

An approximation to the arithmetic-geometric mean. G.J.O. Jameson, Math. Gazette 98 (2014), 85 95 An pproximtion to the rithmetic-geometric men G.J.O. Jmeson, Mth. Gzette 98 (4), 85 95 Given positive numbers > b, consider the itertion given by =, b = b nd n+ = ( n + b n ), b n+ = ( n b n ) /. At ech

More information

13.4 Work done by Constant Forces

13.4 Work done by Constant Forces 13.4 Work done by Constnt Forces We will begin our discussion of the concept of work by nlyzing the motion of n object in one dimension cted on by constnt forces. Let s consider the following exmple: push

More information

The missing ingredient in effective-medium theories: Standard deviations USA. University Park, PA 16802, USA

The missing ingredient in effective-medium theories: Standard deviations USA. University Park, PA 16802, USA The missing ingredient in effective-medium theories: Stndrd devitions Crig F. Bohren 1,*, Xuerong Xio 2, nd Akhlesh Lkhtki 2 1 Deprtment of Meteorology, Pennsylvni Stte University, University Prk, PA 16802,

More information

Department of Mechanical Engineering ME 322 Mechanical Engineering Thermodynamics. Lecture 33. Psychrometric Properties of Moist Air

Department of Mechanical Engineering ME 322 Mechanical Engineering Thermodynamics. Lecture 33. Psychrometric Properties of Moist Air Deprtment of Mechnicl Engineering ME 3 Mechnicl Engineering hermodynmics Lecture 33 sychrometric roperties of Moist Air Air-Wter Vpor Mixtures Atmospheric ir A binry mixture of dry ir () + ter vpor ()

More information

CHM Physical Chemistry I Chapter 1 - Supplementary Material

CHM Physical Chemistry I Chapter 1 - Supplementary Material CHM 3410 - Physicl Chemistry I Chpter 1 - Supplementry Mteril For review of some bsic concepts in mth, see Atkins "Mthemticl Bckground 1 (pp 59-6), nd "Mthemticl Bckground " (pp 109-111). 1. Derivtion

More information

HYDROTHERMAL ANALYSIS OF THE ABSORBER TUBES USED IN LINEAR FRESNEL REFLECTOR SOLAR THERMAL SYSTEM

HYDROTHERMAL ANALYSIS OF THE ABSORBER TUBES USED IN LINEAR FRESNEL REFLECTOR SOLAR THERMAL SYSTEM Proceedings of the 21 st Ntionl & 10 th ISHMT-ASME Het nd Mss Trnsfer Conference Decemer 27-30, 2011, IIT Mdrs, Indi Pper ID: ISHMT_IND_17_034 HYDROTHERMAL ANALYSIS OF THE ABSORBER TUBES USED IN LINEAR

More information

Numerical simulation of ohmic heating in idealized thin-layer electrodeposition cells

Numerical simulation of ohmic heating in idealized thin-layer electrodeposition cells JOURNAL OF OPTOELECTRONICS AND ADVANCED MATERIALS Vol. 8, No. 1, Ferury 2006, p. 271-279 Numericl simultion of ohmic heting in idelized thin-lyer electrodeposition cells P. BARVINSCHI West University of

More information

NUCLEAR SYSTEMS I (2 nd Printing): THERMAL HYDRAULIC FUNDAMENTALS ERRATA

NUCLEAR SYSTEMS I (2 nd Printing): THERMAL HYDRAULIC FUNDAMENTALS ERRATA NUCLEAR SYSTEMS I ( nd Printing): THERMAL HYDRAULIC FUNDAMENTALS Neil E. Todres nd Mujid S. Kzimi ERRATA /10/04 48 (Eq. 3-0)... = q S n... = q n S n 69 (Fig. 3-11, Cption)... for irrdition time of 10 13

More information

COURSE OUTLINE. Introduction Signals and Noise Filtering Sensors: PD1 PhotoDetector Fundamentals. Sensors, Signals and Noise 1

COURSE OUTLINE. Introduction Signals and Noise Filtering Sensors: PD1 PhotoDetector Fundamentals. Sensors, Signals and Noise 1 Sensors, Signls nd Noise 1 COURSE OUTLINE Introduction Signls nd Noise Filtering Sensors: PD1 PhotoDetector Fundmentls Photons nd photodetector principles 2 Photons nd Spectrl rnges Reflection nd Absorption

More information

Experimental and theoretical study of a humidification dehumidification water desalination system using solar energy

Experimental and theoretical study of a humidification dehumidification water desalination system using solar energy Deslintion 168 (2004) 151 159 Experimentl nd theoreticl study of humidifiction dehumidifiction wter deslintion system using solr energy J. Orfi *, M. Lplnte b, H. Mrmouch, N. Glnis b, B. Benhmou c, S.

More information

Materials Analysis MATSCI 162/172 Laboratory Exercise No. 1 Crystal Structure Determination Pattern Indexing

Materials Analysis MATSCI 162/172 Laboratory Exercise No. 1 Crystal Structure Determination Pattern Indexing Mterils Anlysis MATSCI 16/17 Lbortory Exercise No. 1 Crystl Structure Determintion Pttern Inexing Objectives: To inex the x-ry iffrction pttern, ientify the Brvis lttice, n clculte the precise lttice prmeters.

More information

Design Data 1M. Highway Live Loads on Concrete Pipe

Design Data 1M. Highway Live Loads on Concrete Pipe Design Dt 1M Highwy Live Lods on Concrete Pipe Foreword Thick, high-strength pvements designed for hevy truck trffic substntilly reduce the pressure trnsmitted through wheel to the subgrde nd consequently,

More information

Non-Linear & Logistic Regression

Non-Linear & Logistic Regression Non-Liner & Logistic Regression If the sttistics re boring, then you've got the wrong numbers. Edwrd R. Tufte (Sttistics Professor, Yle University) Regression Anlyses When do we use these? PART 1: find

More information

Summary of equations chapters 7. To make current flow you have to push on the charges. For most materials:

Summary of equations chapters 7. To make current flow you have to push on the charges. For most materials: Summry of equtions chpters 7. To mke current flow you hve to push on the chrges. For most mterils: J E E [] The resistivity is prmeter tht vries more thn 4 orders of mgnitude between silver (.6E-8 Ohm.m)

More information

Generalized Fano and non-fano networks

Generalized Fano and non-fano networks Generlized Fno nd non-fno networks Nildri Ds nd Brijesh Kumr Ri Deprtment of Electronics nd Electricl Engineering Indin Institute of Technology Guwhti, Guwhti, Assm, Indi Emil: {d.nildri, bkri}@iitg.ernet.in

More information

Factors affecting the phonation threshold pressure and frequency

Factors affecting the phonation threshold pressure and frequency 3SC Fctors ffecting the phontion threshold pressure nd frequency Zhoyn Zhng School of Medicine, University of Cliforni Los Angeles, CA, USA My, 9 57 th ASA Meeting, Portlnd, Oregon Acknowledgment: Reserch

More information

Neuro-Fuzzy Modeling of Superheating System. of a Steam Power Plant

Neuro-Fuzzy Modeling of Superheating System. of a Steam Power Plant Applied Mthemticl Sciences, Vol. 1, 2007, no. 42, 2091-2099 Neuro-Fuzzy Modeling of Superheting System of Stem Power Plnt Mortez Mohmmdzheri, Ali Mirsephi, Orng Asef-fshr nd Hmidrez Koohi The University

More information

Week 10: Line Integrals

Week 10: Line Integrals Week 10: Line Integrls Introduction In this finl week we return to prmetrised curves nd consider integrtion long such curves. We lredy sw this in Week 2 when we integrted long curve to find its length.

More information

Modelling Heat and Mass Transfer in a Cooling Tower under Hot and Humid Conditions

Modelling Heat and Mass Transfer in a Cooling Tower under Hot and Humid Conditions Journl of Advnced Engineering Reserch ISSN: 2393-8447 Volume 2, Issue 1, 2015, pp.1-10 Modelling Het nd Mss Trnsfer in Cooling Toer under Hot nd Humid Conditions Dng Trn Tho* nd Dng Quoc Phu School of

More information

A Thermal Model of a Forced-Cooled Heat Sink for Transient Temperature Calculations Employing a Circuit Simulator

A Thermal Model of a Forced-Cooled Heat Sink for Transient Temperature Calculations Employing a Circuit Simulator A Therml Model of Forced-Cooled Het Sink for Trnsient Temperture Clcultions Employing Circuit Simultor Uwe DROFENIK * Johnn W. KOLAR * Astrct. Power semiconductors cn e modeled s therml network of resistors

More information

Consequently, the temperature must be the same at each point in the cross section at x. Let:

Consequently, the temperature must be the same at each point in the cross section at x. Let: HW 2 Comments: L1-3. Derive the het eqution for n inhomogeneous rod where the therml coefficients used in the derivtion of the het eqution for homogeneous rod now become functions of position x in the

More information

Entropy ISSN

Entropy ISSN Entropy 006, 8[], 50-6 50 Entropy ISSN 099-4300 www.mdpi.org/entropy/ ENTROPY GENERATION IN PRESSURE GRADIENT ASSISTED COUETTE FLOW WITH DIFFERENT THERMAL BOUNDARY CONDITIONS Abdul Aziz Deprtment of Mechnicl

More information

Chapter 6 Electrostatic Boundary Value Problems. Dr. Talal Skaik

Chapter 6 Electrostatic Boundary Value Problems. Dr. Talal Skaik Chpter 6 Electrosttic Boundry lue Problems Dr. Tll Skik 1 1 Introduction In previous chpters, E ws determined by coulombs lw or Guss lw when chrge distribution is known, or potentil is known throughout

More information

Lect-23. In this lecture... Tutorial on axial flow turbines. Prof. Bhaskar Roy, Prof. A M Pradeep, Department of Aerospace, IIT Bombay

Lect-23. In this lecture... Tutorial on axial flow turbines. Prof. Bhaskar Roy, Prof. A M Pradeep, Department of Aerospace, IIT Bombay Lect- In this lecture... Lect- utoril on xil flow turbines Prof. Bhskr Roy, Prof. A M Prdeep, Deprtment of Aerospce, II Bomby Problem # Lect- A single stge gs turbine opertes t its design condition with

More information

P 3 (x) = f(0) + f (0)x + f (0) 2. x 2 + f (0) . In the problem set, you are asked to show, in general, the n th order term is a n = f (n) (0)

P 3 (x) = f(0) + f (0)x + f (0) 2. x 2 + f (0) . In the problem set, you are asked to show, in general, the n th order term is a n = f (n) (0) 1 Tylor polynomils In Section 3.5, we discussed how to pproximte function f(x) round point in terms of its first derivtive f (x) evluted t, tht is using the liner pproximtion f() + f ()(x ). We clled this

More information

Acceptance Sampling by Attributes

Acceptance Sampling by Attributes Introduction Acceptnce Smpling by Attributes Acceptnce smpling is concerned with inspection nd decision mking regrding products. Three spects of smpling re importnt: o Involves rndom smpling of n entire

More information

4.5 THE FUNDAMENTAL THEOREM OF CALCULUS

4.5 THE FUNDAMENTAL THEOREM OF CALCULUS 4.5 The Funmentl Theorem of Clculus Contemporry Clculus 4.5 THE FUNDAMENTAL THEOREM OF CALCULUS This section contins the most importnt n most use theorem of clculus, THE Funmentl Theorem of Clculus. Discovere

More information

First Law of Thermodynamics. Control Mass (Closed System) Conservation of Mass. Conservation of Energy

First Law of Thermodynamics. Control Mass (Closed System) Conservation of Mass. Conservation of Energy First w of hermodynmics Reding Problems 3-3-7 3-0, 3-5, 3-05 5-5- 5-8, 5-5, 5-9, 5-37, 5-0, 5-, 5-63, 5-7, 5-8, 5-09 6-6-5 6-, 6-5, 6-60, 6-80, 6-9, 6-, 6-68, 6-73 Control Mss (Closed System) In this section

More information

MATHEMATICAL SIMULATION OF GEOTHERMAL HEAT TRANSFER IN HOT DRY ROCK UNDERGROUND HEAT EXCHANGERS

MATHEMATICAL SIMULATION OF GEOTHERMAL HEAT TRANSFER IN HOT DRY ROCK UNDERGROUND HEAT EXCHANGERS SCIENIFIC PROCEEDINGS 009, Fculty of Mechnicl Engineering, SU in Brtislv MAHEMAICAL SIMULAION OF GEOHERMAL HEA RANSFER IN HO DRY ROCK UNDERGROUND HEA EXCHANGERS Kristín KÁZMÉROVÁ, Michl MASARYK Slovk University

More information

An Improved Model for Predicting Fluid Temperature in Deep Wells

An Improved Model for Predicting Fluid Temperature in Deep Wells Mthemticl Modelling nd Applictions 016; 1(1): 0-5 http://www.sciencepublishinggroup.com/j/mm doi: 10.11648/j.mm.0160101.14 An Improved Model for Predicting Fluid Temperture in Deep Wells Boyun Guo, Jinze

More information

Development and Evaluation of a Solar Thermal Collector Designed for Drying Grain

Development and Evaluation of a Solar Thermal Collector Designed for Drying Grain Irnic Journl of Energy & Environment 3 (4): 380-384, 0 ISSN 079-5 IJEE n Officil Peer Reviewed Journl of Bbol Noshirvni University of Technology DOI: 0.589/idosi.ijee.0.03.04.3 BUT Development nd Evlution

More information

dy ky, dt where proportionality constant k may be positive or negative

dy ky, dt where proportionality constant k may be positive or negative Section 1.2 Autonomous DEs of the form 0 The DE y is mthemticl model for wide vriety of pplictions. Some of the pplictions re descried y sying the rte of chnge of y(t) is proportionl to the mount present.

More information

Energy (kcal mol -1 ) Force (kcal mol -1 Å -1 ) Pore axis (Å) Mixed Mo-only S-only Graphene

Energy (kcal mol -1 ) Force (kcal mol -1 Å -1 ) Pore axis (Å) Mixed Mo-only S-only Graphene Force (kcl mol -1 Å -1 ) Energy (kcl mol -1 ) 3 1-1 - -3 Mixed Mo-only S-only Grphene 6 5 3 1 Mixed Mo-only S-only Grphene - -1-1 1 Pore xis (Å) -1 1 Pore xis (Å) Supplementry Figure 1 Energy Brriers.

More information

Casimir-Polder interaction in the presence of parallel walls

Casimir-Polder interaction in the presence of parallel walls Csimir-Polder interction in the presence of prllel wlls rxiv:qunt-ph/2v 6 Nov 2 F C Sntos, J. J. Pssos Sobrinho nd A. C. Tort Instituto de Físic Universidde Federl do Rio de Jneiro Cidde Universitári -

More information

Period #2 Notes: Electronic Structure of Atoms

Period #2 Notes: Electronic Structure of Atoms Period # Notes: Electronic Structure of Atoms The logicl plce (for civil engineers) to begin in describing mterils is t the tomic scle. The bsic elements of the tom re the proton, the neutron, nd the electron:

More information

Set up Invariable Axiom of Force Equilibrium and Solve Problems about Transformation of Force and Gravitational Mass

Set up Invariable Axiom of Force Equilibrium and Solve Problems about Transformation of Force and Gravitational Mass Applied Physics Reserch; Vol. 5, No. 1; 013 ISSN 1916-9639 E-ISSN 1916-9647 Published by Cndin Center of Science nd Eduction Set up Invrible Axiom of orce Equilibrium nd Solve Problems bout Trnsformtion

More information

The Islamic University of Gaza Faculty of Engineering Civil Engineering Department. Numerical Analysis ECIV Chapter 11

The Islamic University of Gaza Faculty of Engineering Civil Engineering Department. Numerical Analysis ECIV Chapter 11 The Islmic University of Gz Fculty of Engineering Civil Engineering Deprtment Numericl Anlysis ECIV 6 Chpter Specil Mtrices nd Guss-Siedel Associte Prof Mzen Abultyef Civil Engineering Deprtment, The Islmic

More information

Joule-Thomson effect TEP

Joule-Thomson effect TEP Joule-homson effect EP elted oics el gs; intrinsic energy; Gy-Lussc theory; throttling; n der Wls eqution; n der Wls force; inverse Joule- homson effect; inversion temerture. Princile A strem of gs is

More information

Lecture 13 - Linking E, ϕ, and ρ

Lecture 13 - Linking E, ϕ, and ρ Lecture 13 - Linking E, ϕ, nd ρ A Puzzle... Inner-Surfce Chrge Density A positive point chrge q is locted off-center inside neutrl conducting sphericl shell. We know from Guss s lw tht the totl chrge on

More information

Some parameters of varicaps with gradient base area based on Shottky barrier

Some parameters of varicaps with gradient base area based on Shottky barrier ISSN: 35-38 Vol. 4, Issue, December 7 Some prmeters of vricps with grdient bse re bsed on Shottky brrier Mmtkrimov O.O., KuchkrovB.Kh. Rector, Nmngn engineering-technology institute, Kosonsoy str.,7, Nmngn,

More information

Physics 24 Exam 1 February 18, 2014

Physics 24 Exam 1 February 18, 2014 Exm Totl / 200 Physics 24 Exm 1 Februry 18, 2014 Printed Nme: Rec. Sec. Letter: Five multiple choice questions, 8 points ech. Choose the best or most nerly correct nswer. 1. The totl electric flux pssing

More information

Final Exam - Review MATH Spring 2017

Final Exam - Review MATH Spring 2017 Finl Exm - Review MATH 5 - Spring 7 Chpter, 3, nd Sections 5.-5.5, 5.7 Finl Exm: Tuesdy 5/9, :3-7:pm The following is list of importnt concepts from the sections which were not covered by Midterm Exm or.

More information