SIMPLE ONE LINE DIAGRAM FAULT IMPEDANCE INPUT DATA
|
|
- Ατρεύς Ασπάσιος
- 7 χρόνια πριν
- Προβολές:
Transcript
1 Exam June Heidi Krohns Student number: nnnnnn SIMPLE ONE LINE DIAGRAM FAULT IMPEDANCE INPUT DATA δ :=. Voltage Phase Angle er := es := 7 e j δ Source S Voltage es = i er := 7 Source R Voltage ZS := j.76 Source S Positive Sequence Impedance ZS := j Source S Zero Sequence Impedance ZR :=.58 + j.93 Source R Positive Sequence Impedance ZR := 3 ZR Source S Zero Sequence Impedance ZL :=.35 + j Positive Sequence Line Impedance Fault Indicator Charles Kim /5
2 ZL := 3 ZL Zero Sequence Line Impedance Fault Location m :=.5 Fault Impedances (for AG fault case) INF := Fault Resistance ZFA := + j ZFB := INF + j ZFC := INF + j ZFG :=.85 + j ZFG :=. ZFG :=.4 + j ZFG :=.57 + j ZFG := + j CONSTANTS rad := Operator := π 8 rad a := e j a = i BAL := a one := a Three phase voltages at S and R zero := i ES := es BAL ES = i i ER := er BAL ER = i i CIRCUIT EQUATION In 3-phase matrix form, the equation loos lie this: Fault Indicator Charles Kim /5
3 How do we form the soure impedance ZS and ZR? Let us consider the lin between 3-phase circuit and symmetrical components Coversion of positive sequence and zero sequence impedances to Self and Mutual impedances zs( z, z) := Conversion Matrix Format z + 3 z zm( z, z) := z z 3 Zzz (, ) := zs( z, z) zm( z, z) zm( z, z) zm( z, z) zs( z, z) zm( z, z) zm( z, z) zm( z, z) zs( z, z) Now Conversion ZS := Z( ZS, ZS) ZL := Z( ZL, ZL) ZR := Z( ZR, ZR) ZS = i i i i i i i i i Source and Line Impedances to the Fault ZSS := ZS + m ZL ZSS = ZRR := ZR + ( m) ZL ZRR = i i i i i i i i i i i i i i i i i i Fault Indicator Charles Kim 3/5
4 Build System Part of the Impedance Matrix ZTOP := augment( augment( ZSS, zero), one) ZTOP = i i i i i i i i i ZMID := augment( augment( zero, ZRR), one) ZMID = i i i i i i i i i ZSYS := stac( ZTOP, ZMID) ZSYS = i i i i i i i i i i i i i i i i i i Pre-fault conditions: ZPRE := ZS + ZL + ZR ZPRE = i i i i i i i i i ISPRE := ZPRE ( ES ER) ISPRE =.7 +.4i.4.73i i Fault Indicator Charles Kim 4/5
5 IRPRE := ZPRE ( ER ES) IRPRE =.7.4i i.56.49i Pre_fault voltage at S end VSP := ES ZS ISPRE VRP := ZS IRPRE ER VSP = VRP = i i i i i i ES = i i i Build the voltage Vector null := ( ) ( ) E := stac stac( ES, ER), null T TS := augment( augment( one, zero), zero) TR := augment( augment( zero, one), zero) Building Fault Part of the Impedance Matrix: E = i i i i i TS = TR = Fault Indicator Charles Kim 5/5
6 ZFAG := ZFA + ZFG ZFBG := ZFB + ZFG ZFCG := ZFC + ZFG ZFAG =.57 ZFBG = ZF := ZFAG ZFG ZFG ZFG ZFBG ZFG ZFG ZFG ZFCG ZF = FABCG := augment( augment( ZF, ZF), one) FABCG = FINAL Z MATRIX Fault Indicator Charles Kim 6/5
7 ZABCG := stac( ZSYS, FABCG) ZABCG = i i i i i i i i i i i i i i i i i i YABCG := ZABCG Fault Currents: IABCG := YABCG E E = i i i i i IABCG = i i i i.5.69i.66.9i i i i Fault Indicator Charles Kim 7/5
8 S - End Fault Currents: IS := TS IABCG IS = i i i R - End Fault Currents: IR := TR IABCG IR = i.5.69i.66.9i S - End Voltages i VS := ES ZS IS VSP = VS = i i R End Voltages * Additional Component for FI VR := ( ZR IR ER) VR = i VRP = i Line Prefault Load Currents from S Bus i i i i i i i Ia := ISPRE Ia =.75 Ib := ISPRE Ib =.75 Ic := ISPRE Ic =.75 arg( Ia) arg( Ib) arg( Ic) = = =.7 = ISPRE = IRPRE =.7 +.4i.4.73i i.7.4i i.56.49i Fault Indicator Charles Kim 8/5
9 Line Prefault Voltages at S Bus Va := VSP Va = Vb := VSP Vb = arg( Va) arg( Vb) =.366 = VSP = i i i Vc := VSP Vc = arg( Vc) =.366 Line Fault Currents from S Bus Iasf := IS Iasf =.35 Ibsf := IS Ibsf =. arg( Iasf) arg( Ibsf ) = 5.97 = IS = i i i Icsf := IS Icsf =.336 arg( Icsf) = 9.75 Line Fault Currents from R Bus Iarf := IR Iarf = 9.88 Ibrf := IR Ibrf =. arg( Iarf ) arg( Ibrf) = = IR = i.5.69i.66.9i Icrf := IR Icrf =.336 Line Fault Voltages at S Bus arg( Icrf ) = 6.95 VSP = i i i Fault Indicator Charles Kim 9/5
10 Vasf := VS Vasf =.56 arg( Vasf) = 39.9 Vbsf := VS Vbsf = Vcsf := VS Vcsf = 8.66 Line Fault Voltage at R Bus arg( Vbsf ) arg( Vcsf) = 3.6 = VS = i i i Varf := VR Vbrf := VR Vcrf := VR Varf = arg( Varf ) Vbrf = arg( Vbrf ) Vcrf = arg( Vcrf ) = = 53.5 = Residual Current and Voltage Vsr, Vrr, Isr, Irr Isrf := IS =.3.387i Irrf := IR = j j j = j = Vsrf := VS = i Vrrf := VR = j j j = j = arg( Isrf ) =.899 IRPREr := j = IRPRE = j arg( Irrf ) =.58 ISPREr := j = i ISPRE = j i IS = arg( Vsrf ) = i i i IR = VS = arg( Vrrf) =.5 VR i.5.69i.66.9i = i i i i i i Fault Indicator Charles Kim /5
11 VRPr VRP i 4 := = VSPr := j j = j = VSP = i 4 j Vsrf Zs := = i Zr := Isrf Vrrf Irrf = i Wattmeteric Method???? SS := Vsrf Isrf SR := Vrrf Irrf Re( SS) = Re( SR) = So How do we generate digital signals of Voltage and Current of the Simulation 4 Cycles with 768 samples per second (8 samples per cycle in 6HZ system)? For S side :=.. 5 delt :=.3 Van := VSP sin π 6 delt + arg VSP T := delt delt = = 8 T := 5 delt + delt T3 := 4 delt + delt Vbn := VSP sin π 6 delt + arg VSP ( 6 delt + arg( VS )) Vcn := VSP sin π 6 delt + arg VSP Vaf := VS sin π Vbf := VS sin π 6 delt + arg VS Vcf := VS sin π 6 delt + arg VS T = Fault Indicator Charles Kim /5
12 Ian := ISPRE sin π 6 delt + arg ISPRE Ibn := ISPRE sin π 6 delt + arg ISPRE Icn := ISPRE sin π 6 delt + arg ISPRE Iaf := IS sin π 6 delt + arg IS Ibf := IS sin π 6 delt + arg IS Icf := IS sin π 6 delt + arg IS Van Vbn Vaf 5 Vbf Ian Ibn Iaf Ibf Fault Indicator Charles Kim /5
13 Let us mae Normal (4 cycle)+ Fault (4 cycle) +Normal (4 cycle) Seg := augment( T, Ian, Ibn, Icn, Van, Vbn, Vcn) Seg := augment( T, Iaf, Ibf, Icf, Vaf, Vbf, Vcf) Seg3 := augment( T3, Ian, Ibn, Icn, Van, Vbn, Vcn) Final := stac( Seg, Seg, Seg3) T := Final IaS := Final IrS := IaS + IbS + IcS VrS := VaS + VbS + VcS IbS := Final IcS := Final 3 VaS := Final 4 VbS := Final 5 VcS := Final 6 3 IaS IbS IcS IrS T Fault Indicator Charles Kim 3/5
14 VaS VbS VcS VrS T VrS IrS.6.8. T VrS = IrS = dt :=.38 ω := π 6 ω = mm := 536 window := 8 wind := window Now for all the calculations Fault Indicator Charles Kim 4/5
15 dd := mm.. window :=.. mm window mm window :=.. 8 UrS := submatrix( VrS, 8, 8 + wind,, ) ArS := submatrix( IrS, 8, 8 + wind,, ) UaS := submatrix( VaS, 8, 8 + wind,, ) AaS := submatrix( IaS, 8, 8 + wind,, ) UbS := submatrix( VbS, 8, 8 + wind,, ) AbS := submatrix( IbS, 8, 8 + wind,, ) UcS := submatrix( VcS, 8, 8 + wind,, ) AcS := submatrix( IcS, 8, 8 + wind,, ) PrS := FrS := FFT( UrS ) FFT( ArS ) CompS := PrS ( ) FrS, ( ) CompS = i CompS = i, WattS := Re( CompS ) Real Current Component Method Fault Indicator Charles Kim 5/5
16 ( ) ( ) ( ) ( ) ( ) ( ) PaS := FFT UaS PbS := FFT UbS PcS := FFT UcS FaS := FFT AaS FbS := FFT AbS FcS := FFT AcS CaS := ( PaS ) FaS, ( ), Re( CaS ) RaS := RbS := Re CbS CbS := PbS ( ) FbS, ( ) CcS := PcS, ( ) RcS := Re( CcS ) ( ) FcS, ( ), 5 RaS RbS RcS Phase a: Ima := ( FaS ), ( FbS ), ( FcS ), ZL = i ZL = i αa:= e i π 3 Fault Indicator Charles Kim 6/5
17 Am := 3 αa ( αa) ( αa) αa Phase a: Iaseq := Am Ima Ia := Iaseq ( ) Ia := Iaseq ( ) Yang method: K := ZL ZL ZL Compensated current: Phase a: Ia := FaS + K Ia αa := arg Ia ( ) arg( Ia ) Resistance and Reactance: X := R := Im( ZL) Re( ZL) X = R =.35 Phase Impedance: Phase a: Fault Indicator Charles Kim 7/5
18 Za := PaS ( Ia ), ( ), ( ), Xa := Im Za Ra := Re Za Fault Distance: ma := ( Xa ) + Ra ( ) tan ( αa ), ( ), X + R tan αa m =.5 Fault Indicator Charles Kim 8/5
19 ma ma =.95 6 ma = ma =.44 7 ma =.43 ma =.44 Results and Discussion Part: When changing the m value (place of the fault) at start of the file ma is changing in same relation. However, ma values seem to come more exact when m is bigger. m=.5 m=.45 m=.5 m=.75 m=.9 ma=.7 ma=.4 ma=.459 ma=.695 ma=.83 Fault resistance ZFG was changed and fault place m was constant (m=.5). If the change of resistance is minor, algorithm wors. If value of ZFG increase much, algorithm stops woring. m=.5 ZFG=.4+j ZFG=.85+j ZFG=.57+j ZFG= +j ma=.48 ma=.458 ma=.43 ma=7.378*^-3 Fault Indicator Charles Kim 9/5
Matrices and Determinants
Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z
Διαβάστε περισσότερα3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β
3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle
Διαβάστε περισσότεραSection 8.3 Trigonometric Equations
99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.
Διαβάστε περισσότεραCHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS
CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =
Διαβάστε περισσότεραHomework 8 Model Solution Section
MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx
Διαβάστε περισσότερα10.7 Performance of Second-Order System (Unit Step Response)
Lecture Notes on Control Systems/D. Ghose/0 57 0.7 Performance of Second-Order System (Unit Step Response) Consider the second order system a ÿ + a ẏ + a 0 y = b 0 r So, Y (s) R(s) = b 0 a s + a s + a
Διαβάστε περισσότεραEE101: Resonance in RLC circuits
EE11: Resonance in RLC circuits M. B. Patil mbatil@ee.iitb.ac.in www.ee.iitb.ac.in/~sequel Deartment of Electrical Engineering Indian Institute of Technology Bombay I V R V L V C I = I m = R + jωl + 1/jωC
Διαβάστε περισσότεραPotential Dividers. 46 minutes. 46 marks. Page 1 of 11
Potential Dividers 46 minutes 46 marks Page 1 of 11 Q1. In the circuit shown in the figure below, the battery, of negligible internal resistance, has an emf of 30 V. The pd across the lamp is 6.0 V and
Διαβάστε περισσότερα6.1. Dirac Equation. Hamiltonian. Dirac Eq.
6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2
Διαβάστε περισσότεραExercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.
Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given
Διαβάστε περισσότεραSecond Order RLC Filters
ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor
Διαβάστε περισσότεραMock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =
Mock Eam 7 Mock Eam 7 Section A. Reference: HKDSE Math M 0 Q (a) ( + k) n nn ( )( k) + nk ( ) + + nn ( ) k + nk + + + A nk... () nn ( ) k... () From (), k...() n Substituting () into (), nn ( ) n 76n 76n
Διαβάστε περισσότεραCable Systems - Postive/Negative Seq Impedance
Cable Systems - Postive/Negative Seq Impedance Nomenclature: GMD GMR - geometrical mead distance between conductors; depends on construction of the T-line or cable feeder - geometric mean raduius of conductor
Διαβάστε περισσότεραDESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.
DESIGN OF MACHINERY SOLUTION MANUAL -7-1! PROBLEM -7 Statement: Design a double-dwell cam to move a follower from to 25 6, dwell for 12, fall 25 and dwell for the remader The total cycle must take 4 sec
Διαβάστε περισσότεραSCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions
SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)
Διαβάστε περισσότεραSampling Basics (1B) Young Won Lim 9/21/13
Sampling Basics (1B) Copyright (c) 2009-2013 Young W. Lim. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version 1.2 or any
Διαβάστε περισσότεραNPI Unshielded Power Inductors
FEATURES NON-SHIELDED MAGNETIC CIRCUIT DESIGN SMALL SIZE WITH CURRENT RATINGS TO 16.5 AMPS SURFACE MOUNTABLE CONSTRUCTION TAKES UP LESS PCB REAL ESTATE AND SAVES MORE POWER TAPED AND REELED FOR AUTOMATIC
Διαβάστε περισσότεραDifferential equations
Differential equations Differential equations: An equation inoling one dependent ariable and its deriaties w. r. t one or more independent ariables is called a differential equation. Order of differential
Διαβάστε περισσότεραInverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------
Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin
Διαβάστε περισσότεραPg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is
Pg. 9. The perimeter is P = The area of a triangle is A = bh where b is the base, h is the height 0 h= btan 60 = b = b In our case b =, then the area is A = = 0. By Pythagorean theorem a + a = d a a =
Διαβάστε περισσότεραSurface Mount Aluminum Electrolytic Capacitors
FEATURES CYLINDRICAL V-CHIP CONSTRUCTION LOW COST, GENERAL PURPOSE, 2000 HOURS AT 85 O C NEW EXPANDED CV RANGE (up to 6800µF) ANTI-SOLVENT (2 MINUTES) DESIGNED FOR AUTOMATIC MOUNTING AND REFLOW SOLDERING
Διαβάστε περισσότερα= 0.927rad, t = 1.16ms
P 9. [a] ω = 2πf = 800rad/s, f = ω 2π = 27.32Hz [b] T = /f = 7.85ms [c] I m = 25mA [d] i(0) = 25cos(36.87 ) = 00mA [e] φ = 36.87 ; φ = 36.87 (2π) = 0.6435 rad 360 [f] i = 0 when 800t + 36.87 = 90. Now
Διαβάστε περισσότεραSection 7.6 Double and Half Angle Formulas
09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)
Διαβάστε περισσότεραMINIATURE ALUMINUM ELECTROLYTIC CAPACITORS. Characteristics. Leakage Current(MAX) I=Leakage Current(µA) C=Nominal Capacitance(µF) V=Rated Voltage(V)
SERIES 5 C Long Life. Low impedance. (Rated Voltage 6.3~V.DC) FEATURES Load Life : 5 C 4~hours. Low impedance at khz with selected materials. SPECIFICATIONS Items Operating Temperature Range Rated Voltage
Διαβάστε περισσότεραPhys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)
Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts
Διαβάστε περισσότεραQueensland University of Technology Transport Data Analysis and Modeling Methodologies
Queensland University of Technology Transport Data Analysis and Modeling Methodologies Lab Session #7 Example 5.2 (with 3SLS Extensions) Seemingly Unrelated Regression Estimation and 3SLS A survey of 206
Διαβάστε περισσότεραHOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:
HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying
Διαβάστε περισσότεραIXBH42N170 IXBT42N170
High Voltage, High Gain BIMOSFET TM Monolithic Bipolar MOS Transistor IXBH42N17 IXBT42N17 S 9 = 1 = 42A (sat) 2.8V Symbol Test Conditions Maximum Ratings TO-247 (IXBH) S = 25 C to 15 C 17 V V CGR = 25
Διαβάστε περισσότεραCHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS
CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS EXERCISE 01 Page 545 1. Use matrices to solve: 3x + 4y x + 5y + 7 3x + 4y x + 5y 7 Hence, 3 4 x 0 5 y 7 The inverse of 3 4 5 is: 1 5 4 1 5 4 15 8 3
Διαβάστε περισσότεραOther Test Constructions: Likelihood Ratio & Bayes Tests
Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :
Διαβάστε περισσότεραJesse Maassen and Mark Lundstrom Purdue University November 25, 2013
Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering
Διαβάστε περισσότεραΤΕΧΝΟΛΟΓΙΚΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΥΠΡΟΥ ΣΧΟΛΗ ΜΗΧΑΝΙΚΗΣ ΚΑΙ ΤΕΧΝΟΛΟΓΙΑΣ. Πτυχιακή εργασία
ΤΕΧΝΟΛΟΓΙΚΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΥΠΡΟΥ ΣΧΟΛΗ ΜΗΧΑΝΙΚΗΣ ΚΑΙ ΤΕΧΝΟΛΟΓΙΑΣ Πτυχιακή εργασία ΕΝΕΡΓΟ ΦΙΛΤΡΟ ΔΙΑΚΟΠΤΙΚΟΥ ΠΗΝΙΟΥ ( Switched Inductor Variable Filter ) Ευτυχία Ιωσήφ Λεμεσός, Μάιος 2016 ΤΕΧΝΟΛΟΓΙΚΟ ΠΑΝΕΠΙΣΤΗΜΙΟ
Διαβάστε περισσότεραExample Sheet 3 Solutions
Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note
Διαβάστε περισσότεραECE 308 SIGNALS AND SYSTEMS FALL 2017 Answers to selected problems on prior years examinations
ECE 308 SIGNALS AND SYSTEMS FALL 07 Answers to selected problems on prior years examinations Answers to problems on Midterm Examination #, Spring 009. x(t) = r(t + ) r(t ) u(t ) r(t ) + r(t 3) + u(t +
Διαβάστε περισσότερα+85 C Snap-Mount Aluminum Electrolytic Capacitors. High Voltage Lead free Leads Rugged Design. -40 C to +85 C
+85 C Snap-Mount Capacitors FEATURES High ripple Current Ratings Large Case Size Selection Extended Life High Voltage Lead free Leads Rugged Design SPECIFICATIONS Tolerance ±20% at 120Hz, 20 C Operating
Διαβάστε περισσότεραThe ε-pseudospectrum of a Matrix
The ε-pseudospectrum of a Matrix Feb 16, 2015 () The ε-pseudospectrum of a Matrix Feb 16, 2015 1 / 18 1 Preliminaries 2 Definitions 3 Basic Properties 4 Computation of Pseudospectrum of 2 2 5 Problems
Διαβάστε περισσότεραHomework 3 Solutions
Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For
Διαβάστε περισσότερα0.5W SMD Zener Diodes TLZJ2.0A TLZJ W SMD Zener Diodes. Features. MiniMelf. Mechanical Data
Features Planar Die Construction 0.5W Power Dissipation Zener Voltage: 2.0V to 56V Ideally Suited for Automated Assembly Processes RoHS Compliant MiniMelf Mechanical Data Case: Molded Glass MiniMelf Terminals:
Διαβάστε περισσότεραΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 24/3/2007
Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Όλοι οι αριθμοί που αναφέρονται σε όλα τα ερωτήματα μικρότεροι του 10000 εκτός αν ορίζεται διαφορετικά στη διατύπωση του προβλήματος. Αν κάπου κάνετε κάποιες υποθέσεις
Διαβάστε περισσότεραChapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
Διαβάστε περισσότεραHigh Frequency Chip Inductor / CF TYPE
High Frequency Chip Inductor / CF TYPE.Features: 1.Closed magnetic circuit avoids crosstalk. 2.S.M.T. type. 3.Excellent solderability and heat resistance. 4.High realiability. 5.The products contain no
Διαβάστε περισσότεραNumerical Analysis FMN011
Numerical Analysis FMN011 Carmen Arévalo Lund University carmen@maths.lth.se Lecture 12 Periodic data A function g has period P if g(x + P ) = g(x) Model: Trigonometric polynomial of order M T M (x) =
Διαβάστε περισσότεραLecture 23. Impedance, Resonance in R-C-L Circuits. Preparation for the Final Exam
Lecture 3. Impedance, Resonance in R-C-L Circuits (a) Start earlier! Preparation for the Final Exam (b) Review the concepts (lectures + textbook) and prepare your equation sheet. Think how you can use
Διαβάστε περισσότεραΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007
Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Αν κάπου κάνετε κάποιες υποθέσεις να αναφερθούν στη σχετική ερώτηση. Όλα τα αρχεία που αναφέρονται στα προβλήματα βρίσκονται στον ίδιο φάκελο με το εκτελέσιμο
Διαβάστε περισσότεραPartial Differential Equations in Biology The boundary element method. March 26, 2013
The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet
Διαβάστε περισσότεραΑΝΙΧΝΕΥΣΗ ΓΕΓΟΝΟΤΩΝ ΒΗΜΑΤΙΣΜΟΥ ΜΕ ΧΡΗΣΗ ΕΠΙΤΑΧΥΝΣΙΟΜΕΤΡΩΝ ΔΙΠΛΩΜΑΤΙΚΗ ΕΡΓΑΣΙΑ
ΕΘΝΙΚΟ ΜΕΤΣΟΒΙΟ ΠΟΛΥΤΕΧΝΕΙΟ ΣΧΟΛΗ ΗΛΕΚΤΡΟΛΟΓΩΝ ΜΗΧΑΝΙΚΩΝ ΚΑΙ ΜΗΧΑΝΙΚΩΝ ΥΠΟΛΟΓΙΣΤΩΝ ΤΟΜΕΑΣ ΕΠΙΚΟΙΝΩΝΙΩΝ ΗΛΕΚΤΡΟΝΙΚΗΣ ΚΑΙ ΣΥΣΤΗΜΑΤΩΝ ΠΛΗΡΟΦΟΡΙΚΗΣ ΑΝΙΧΝΕΥΣΗ ΓΕΓΟΝΟΤΩΝ ΒΗΜΑΤΙΣΜΟΥ ΜΕ ΧΡΗΣΗ ΕΠΙΤΑΧΥΝΣΙΟΜΕΤΡΩΝ
Διαβάστε περισσότεραΜηχανική Μάθηση Hypothesis Testing
ΕΛΛΗΝΙΚΗ ΔΗΜΟΚΡΑΤΙΑ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ Μηχανική Μάθηση Hypothesis Testing Γιώργος Μπορμπουδάκης Τμήμα Επιστήμης Υπολογιστών Procedure 1. Form the null (H 0 ) and alternative (H 1 ) hypothesis 2. Consider
Διαβάστε περισσότεραAccu-Guard II. SMD Thin-Film Fuse ELECTRICAL SPECIFICATIONS
Accu-Guard II is a version of Accu-Guard fuses for a wider range of current and voltage ratings. Con struct ed on alumina substrates, Accu-Guard II fuses display superior electrical, mechanical and en
Διαβάστε περισσότεραMultilayer Ceramic Chip Capacitors
FEATURES X7R, X6S, X5R AND Y5V DIELECTRICS HIGH CAPACITANCE DENSITY ULTRA LOW ESR & ESL EXCELLENT MECHANICAL STRENGTH NICKEL BARRIER TERMINATIONS RoHS COMPLIANT SAC SOLDER COMPATIBLE* PART NUMBER SYSTEM
Διαβάστε περισσότεραCapacitors - Capacitance, Charge and Potential Difference
Capacitors - Capacitance, Charge and Potential Difference Capacitors store electric charge. This ability to store electric charge is known as capacitance. A simple capacitor consists of 2 parallel metal
Διαβάστε περισσότεραConcrete Mathematics Exercises from 30 September 2016
Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)
Διαβάστε περισσότεραdepartment listing department name αχχουντσ ϕανε βαλικτ δδσϕηασδδη σδηφγ ασκϕηλκ τεχηνιχαλ αλαν ϕουν διξ τεχηνιχαλ ϕοην µαριανι
She selects the option. Jenny starts with the al listing. This has employees listed within She drills down through the employee. The inferred ER sttricture relates this to the redcords in the databasee
Διαβάστε περισσότεραTHICK FILM LEAD FREE CHIP RESISTORS
Features Suitable for lead free soldering. Compatible with flow and reflow soldering Applications Consumer Electronics Automotive industry Computer Measurement instrument Electronic watch and camera Configuration
Διαβάστε περισσότεραSurface Mount Multilayer Chip Capacitors for Commodity Solutions
Surface Mount Multilayer Chip Capacitors for Commodity Solutions Below tables are test procedures and requirements unless specified in detail datasheet. 1) Visual and mechanical 2) Capacitance 3) Q/DF
Διαβάστε περισσότεραBreaking capacity: ~200kA Rated voltage: ~690V, 550V. Operating I 2 t-value (A 2 s) Power
SYSTEM NV-NH NV/NH SERIES TYPES gr UQ M M, M-striker pin ~ 5V ~9V Technical data on page 8 Technical data: Application: MCUQ/5A/9V Standards: IEC 9- Breaking capacity: ~ka Rated voltage: ~9V, 55V For battery
Διαβάστε περισσότεραAluminum Electrolytic Capacitors
Aluminum Electrolytic Capacitors Snap-In, Mini., 105 C, High Ripple APS TS-NH ECE-S (G) Series: TS-NH Features Long life: 105 C 2,000 hours; high ripple current handling ability Wide CV value range (47
Διαβάστε περισσότεραIES LM Report. Form. No. GLW-0001-F / 21 P.2 P.2 P.3 P.5 P.6 P.7
IES LM-80-08 Report ~ Copy ~ Description of LED Light Sources Tested Applicable Product Series IES LM-80-08 Report Requirement IES TM-21-11 Prediction IES LM-80-08 Test Summary IES LM-80-08 Test Result
Διαβάστε περισσότεραMultilayer Ceramic Chip Capacitors
FEATURES X7R, X6S, X5R AND Y5V DIELECTRICS HIGH CAPACITANCE DENSITY ULTRA LOW ESR & ESL EXCELLENT MECHANICAL STRENGTH NICKEL BARRIER TERMINATIONS RoHS COMPLIANT SAC SOLDER COMPATIBLE* Temperature Coefficient
Διαβάστε περισσότεραAluminum Electrolytic Capacitors (Large Can Type)
Aluminum Electrolytic Capacitors (Large Can Type) Snap-In, 85 C TS-U ECE-S (U) Series: TS-U Features General purpose Wide CV value range (33 ~ 47,000 µf/16 4V) Various case sizes Top vent construction
Διαβάστε περισσότερα2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.
EAMCET-. THEORY OF EQUATIONS PREVIOUS EAMCET Bits. Each of the roots of the equation x 6x + 6x 5= are increased by k so that the new transformed equation does not contain term. Then k =... - 4. - Sol.
Διαβάστε περισσότεραTechnical Data Catalog
42 to 65 khz-a (Broadband) Transformed to 100 ohms minimum (B1) 42 to 65 khz 1 kw 25 W Power Rating: 1 kw @ 1% duty cycle CW (4) : 25W in B265, PM265 15W in M265, TM265 7 x 28.6 mm (1.13 in) PZT Active
Διαβάστε περισσότεραParametrized Surfaces
Parametrized Surfaces Recall from our unit on vector-valued functions at the beginning of the semester that an R 3 -valued function c(t) in one parameter is a mapping of the form c : I R 3 where I is some
Διαβάστε περισσότεραANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?
Teko Classes IITJEE/AIEEE Maths by SUHAAG SIR, Bhopal, Ph (0755) 3 00 000 www.tekoclasses.com ANSWERSHEET (TOPIC DIFFERENTIAL CALCULUS) COLLECTION # Question Type A.Single Correct Type Q. (A) Sol least
Διαβάστε περισσότεραSummary of Specifications
Snap Mount Large High CV High Ripple 85 C Temperature The series capacitors are the standard 85 C, large capacitance, snap-in capacitors from United Chemi-Con. The load life for the series is 2,000 hours
Διαβάστε περισσότεραPolymer PTC Resettable Fuse: KMC Series
Features 1. RoHS & Halogen-Free (HF) compliant 2. IA size: 0603, 0805, 1206, 1812 3. Hold current ratings from 0.05 to 3A 4. Voltage ratings from 6V computer and electronic applications to 60V 5. Small
Διαβάστε περισσότεραSecond Order Partial Differential Equations
Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y
Διαβάστε περισσότεραThin Film Chip Resistors
FEATURES PRECISE TOLERANCE AND TEMPERATURE COEFFICIENT EIA STANDARD CASE SIZES (0201 ~ 2512) LOW NOISE, THIN FILM (NiCr) CONSTRUCTION REFLOW SOLDERABLE (Pb FREE TERMINATION FINISH) Type Size EIA PowerRating
Διαβάστε περισσότεραDETERMINATION OF DYNAMIC CHARACTERISTICS OF A 2DOF SYSTEM. by Zoran VARGA, Ms.C.E.
DETERMINATION OF DYNAMIC CHARACTERISTICS OF A 2DOF SYSTEM by Zoran VARGA, Ms.C.E. Euro-Apex B.V. 1990-2012 All Rights Reserved. The 2 DOF System Symbols m 1 =3m [kg] m 2 =8m m=10 [kg] l=2 [m] E=210000
Διαβάστε περισσότεραSrednicki Chapter 55
Srednicki Chapter 55 QFT Problems & Solutions A. George August 3, 03 Srednicki 55.. Use equations 55.3-55.0 and A i, A j ] = Π i, Π j ] = 0 (at equal times) to verify equations 55.-55.3. This is our third
Διαβάστε περισσότεραWritten Examination. Antennas and Propagation (AA ) April 26, 2017.
Written Examination Antennas and Propagation (AA. 6-7) April 6, 7. Problem ( points) Let us consider a wire antenna as in Fig. characterized by a z-oriented linear filamentary current I(z) = I cos(kz)ẑ
Διαβάστε περισσότεραΕΛΛΗΝΙΚΗ ΔΗΜΟΚΡΑΤΙΑ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ. Ψηφιακή Οικονομία. Διάλεξη 7η: Consumer Behavior Mαρίνα Μπιτσάκη Τμήμα Επιστήμης Υπολογιστών
ΕΛΛΗΝΙΚΗ ΔΗΜΟΚΡΑΤΙΑ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ Ψηφιακή Οικονομία Διάλεξη 7η: Consumer Behavior Mαρίνα Μπιτσάκη Τμήμα Επιστήμης Υπολογιστών Τέλος Ενότητας Χρηματοδότηση Το παρόν εκπαιδευτικό υλικό έχει αναπτυχθεί
Διαβάστε περισσότεραthe total number of electrons passing through the lamp.
1. A 12 V 36 W lamp is lit to normal brightness using a 12 V car battery of negligible internal resistance. The lamp is switched on for one hour (3600 s). For the time of 1 hour, calculate (i) the energy
Διαβάστε περισσότεραC (3) (4) R 3 R 4 (2)
Πανεπιστήμιο Θεσσαλίας Βόλος, 29/03/2016 Τμήμα: Μηχανολόγων Μηχανικών Συντελεστής Βαρύτητας: 40%/ Χρόνος Εξέτασης: 3 Ώρες Γραπτή Ενδιάμεση Εξέταση στο Μάθημα: «ΜΜ604, Ηλεκτροτεχνία Ηλεκτρικές Μηχανές»
Διαβάστε περισσότεραderivation of the Laplacian from rectangular to spherical coordinates
derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used
Διαβάστε περισσότεραTridiagonal matrices. Gérard MEURANT. October, 2008
Tridiagonal matrices Gérard MEURANT October, 2008 1 Similarity 2 Cholesy factorizations 3 Eigenvalues 4 Inverse Similarity Let α 1 ω 1 β 1 α 2 ω 2 T =......... β 2 α 1 ω 1 β 1 α and β i ω i, i = 1,...,
Διαβάστε περισσότερα( )( ) ( ) ( )( ) ( )( ) β = Chapter 5 Exercise Problems EX α So 49 β 199 EX EX EX5.4 EX5.5. (a)
hapter 5 xercise Problems X5. α β α 0.980 For α 0.980, β 49 0.980 0.995 For α 0.995, β 99 0.995 So 49 β 99 X5. O 00 O or n 3 O 40.5 β 0 X5.3 6.5 μ A 00 β ( 0)( 6.5 μa) 8 ma 5 ( 8)( 4 ) or.88 P on + 0.0065
Διαβάστε περισσότερα6.4 Superposition of Linear Plane Progressive Waves
.0 - Marine Hydrodynamics, Spring 005 Lecture.0 - Marine Hydrodynamics Lecture 6.4 Superposition of Linear Plane Progressive Waves. Oblique Plane Waves z v k k k z v k = ( k, k z ) θ (Looking up the y-ais
Διαβάστε περισσότεραw o = R 1 p. (1) R = p =. = 1
Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 205 ιδάσκων : Α. Μουχτάρης Τριτη Σειρά Ασκήσεων Λύσεις Ασκηση 3. 5.2 (a) From the Wiener-Hopf equation we have:
Διαβάστε περισσότερα500mW Zener Diodes TZXJ2.0A TZXJ mW Zener Diodes. Features. Mechanical Data. Maximum Ratings (T Ambient=25ºC unless noted otherwise)
Features Planar Die Construction 500mW Power Dissipation Zener Voltage: 2.0V to 56V Ideally Suited for Automated Assembly Processes RoHS compliant and Halogen Free DO-35 Mechanical Data Case: Molded glass
Διαβάστε περισσότερα[1] P Q. Fig. 3.1
1 (a) Define resistance....... [1] (b) The smallest conductor within a computer processing chip can be represented as a rectangular block that is one atom high, four atoms wide and twenty atoms long. One
Διαβάστε περισσότερα38 Te(OH) 6 2NH 4 H 2 PO 4 (NH 4 ) 2 HPO 4
Fig. A-1-1. Te(OH) NH H PO (NH ) HPO (TAAP). Projection of the crystal structure along the b direction [Ave]. 9 1. 7.5 ( a a )/ a [1 ] ( b b )/ b [1 ] 5..5 1.5 1 1.5 ( c c )/ c [1 ].5 1. 1.5. Angle β 1.
Διαβάστε περισσότεραThermistor (NTC /PTC)
ISO/TS16949 ISO 9001 ISO14001 2015 Thermistor (NTC /PTC) GNTC (Chip in Glass Thermistor) SMD NTC Thermistor SMD PTC Thermistor Radial type Thermistor Bare Chip Thermistor (Gold & silver Electrode) 9B-51L,
Διαβάστε περισσότεραMetal Oxide Varistors (MOV) Data Sheet
Φ SERIES Metal Oxide Varistors (MOV) Data Sheet Features Wide operating voltage (V ma ) range from 8V to 0V Fast responding to transient over-voltage Large absorbing transient energy capability Low clamping
Διαβάστε περισσότεραDaewoo Technopark A-403, Dodang-dong, Wonmi-gu, Bucheon-city, Gyeonggido, Korea LM-80 Test Report
LM-80 Test Report Approved Method: Measuring Lumen Maintenance of LED Light Sources Project Number: KILT1212-U00216 Date: September 17 th, 2013 Requested by: Dongbu LED Co., Ltd 90-1, Bongmyeong-Ri, Namsa-Myeon,
Διαβάστε περισσότεραGraded Refractive-Index
Graded Refractive-Index Common Devices Methodologies for Graded Refractive Index Methodologies: Ray Optics WKB Multilayer Modelling Solution requires: some knowledge of index profile n 2 x Ray Optics for
Διαβάστε περισσότερα+85 C General Purpose Radial Lead Aluminum Electrolytic Capacitors
+85 C General Purpose Radial Lead Aluminum Electrolytic acitors Applications Filtering Coupling Bypass Features Standard case sizes RoHS compliant Multiple case sizes Lead free Operating Temperature Range
Διαβάστε περισσότεραReminders: linear functions
Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U
Διαβάστε περισσότεραwave energy Superposition of linear plane progressive waves Marine Hydrodynamics Lecture Oblique Plane Waves:
3.0 Marine Hydrodynamics, Fall 004 Lecture 0 Copyriht c 004 MIT - Department of Ocean Enineerin, All rihts reserved. 3.0 - Marine Hydrodynamics Lecture 0 Free-surface waves: wave enery linear superposition,
Διαβάστε περισσότεραSOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM
SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr T t N n) Pr max X 1,..., X N ) t N n) Pr max
Διαβάστε περισσότεραModel: MTZ22. Data. Cylinder count: 1 Displacement [m³/h]: 6,63 Cylinder capacity [cm³]: 38,1 RPM [min -1 ]: 2900 Weight [kg]: 21 Oil charge [dm³]: 1
Technical data Data Cylinder count: 1 Displacement [m³/h]: 6,63 Cylinder capacity [cm³]: 38,1 RPM [min -1 ]: 2900 Weight [kg]: 21 Oil charge [dm³]: 1 Oil type: 160PZ Crankcase heater type: PTC 35 W Maximum
Διαβάστε περισσότεραb. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!
MTH U341 urface Integrals, tokes theorem, the divergence theorem To be turned in Wed., Dec. 1. 1. Let be the sphere of radius a, x 2 + y 2 + z 2 a 2. a. Use spherical coordinates (with ρ a) to parametrize.
Διαβάστε περισσότερα65W PWM Output LED Driver. IDLV-65 series. File Name:IDLV-65-SPEC
~ A File Name:IDLV65SPEC 07050 SPECIFICATION MODEL OUTPUT OTHERS NOTE DC VOLTAGE RATED CURRENT RATED POWER DIMMING RANGE VOLTAGE TOLERANCE PWM FREQUENCY (Typ.) SETUP TIME Note. AUXILIARY DC OUTPUT Note.
Διαβάστε περισσότεραPrepolarized Microphones-Free Field
Prepolarized Microphones-Free Field MP0 / MP3 / MP / MP / MP / MP / MP8 MP0 MP3 MP MP MP MP MP8 Standards (IEC7) I I I.3 ~ 0k 3 ~ 0k 0 ~.k 0 ~.k 0 ~ 70k 0 ~ k 0 ~ k Open-circuit Sensitivity (mv/pa) (±db)
Διαβάστε περισσότεραTechnical Report. General Design Data of a Three Phase Induction Machine 90kW Squirrel Cage Rotor
Technical Report General Design Data of a Three Phase Induction Machine 90kW Squirrel Cage Rotor Tasos Lazaridis Electrical Engineer CAD/CAE Engineer tasoslazaridis13@gmail.com Three-Phase Induction Machine
Διαβάστε περισσότεραMathCity.org Merging man and maths
MathCity.org Merging man and maths Exercise 10. (s) Page Textbook of Algebra and Trigonometry for Class XI Available online @, Version:.0 Question # 1 Find the values of sin, and tan when: 1 π (i) (ii)
Διαβάστε περισσότεραF19MC2 Solutions 9 Complex Analysis
F9MC Solutions 9 Complex Analysis. (i) Let f(z) = eaz +z. Then f is ifferentiable except at z = ±i an so by Cauchy s Resiue Theorem e az z = πi[res(f,i)+res(f, i)]. +z C(,) Since + has zeros of orer at
Διαβάστε περισσότερα( ) 2 and compare to M.
Problems and Solutions for Section 4.2 4.9 through 4.33) 4.9 Calculate the square root of the matrix 3!0 M!0 8 Hint: Let M / 2 a!b ; calculate M / 2!b c ) 2 and compare to M. Solution: Given: 3!0 M!0 8
Διαβάστε περισσότεραSAW FILTER - RF RF SAW FILTER
FEATURES - Frequencies from 0MHz to 700MHz - Custom specifications available - Industry standard package configurations - Low-loss saw component - Low amplitude ripple - RoHS compliance - Electrostatic
Διαβάστε περισσότεραΔΙΠΛΩΜΑΤΙΚΗ ΕΡΓΑΣΙΑ. του φοιτητή του Τμήματος Ηλεκτρολόγων Μηχανικών και. Τεχνολογίας Υπολογιστών της Πολυτεχνικής Σχολής του. Πανεπιστημίου Πατρών
ΠΑΝΕΠΙΣΤΗΜΙΟ ΠΑΤΡΩΝ ΤΜΗΜΑ ΗΛΕΚΤΡΟΛΟΓΩΝ ΜΗΧΑΝΙΚΩΝ ΚΑΙ ΤΕΧΝΟΛΟΓΙΑΣ ΥΠΟΛΟΓΙΣΤΩΝ ΤΟΜΕΑΣ ΣΥΣΤΗΜΑΤΩΝ ΗΛΕΚΤΡΙΚΗΣ ΕΝΕΡΓΕΙΑΣ ΕΡΓΑΣΤΗΡΙΟ ΗΛΕΚΤΡΟΜΗΧΑΝΙΚΗΣ ΜΕΤΑΤΡΟΠΗΣ ΕΝΕΡΓΕΙΑΣ ΔΙΠΛΩΜΑΤΙΚΗ ΕΡΓΑΣΙΑ του φοιτητή του
Διαβάστε περισσότεραΙ ΑΚΤΟΡΙΚΗ ΙΑΤΡΙΒΗ. Χρήστος Αθ. Χριστοδούλου. Επιβλέπων: Καθηγητής Ιωάννης Αθ. Σταθόπουλος
ΕΘΝΙΚΟ ΜΕΤΣΟΒΙΟ ΠΟΛΥΤΕΧΝΕΙΟ ΣΧΟΛΗ ΗΛΕΚΤΡΟΛΟΓΩΝ ΜΗΧΑΝΙΚΩΝ ΚΑΙ ΜΗΧΑΝΙΚΩΝ ΥΠΟΛΟΓΙΣΤΩΝ ΤΟΜΕΑΣ ΗΛΕΚΤΡΙΚΗΣ ΙΣΧΥΟΣ ΕΡΓΑΣΤΗΡΙΟ ΥΨΗΛΩΝ ΤΑΣΕΩΝ ΣΥΜΒΟΛΗ ΣΤΗ ΜΕΛΕΤΗ TΩΝ ΚΑΘΟ ΙΚΩΝ ΑΛΕΞΙΚΕΡΑΥΝΩΝ Ι ΑΚΤΟΡΙΚΗ ΙΑΤΡΙΒΗ Χρήστος
Διαβάστε περισσότερα