2 Definitions and parameters of the impulse-technics
|
|
- Jason Fowler
- 5 years ago
- Views:
Transcription
1 efiniions and parameers of he impulse-echnics igial logic-circuis are driven wih signals, which only represen wo levels: he levels LOW and HIGH or he variables wih he values "" and ". These levels are for specific imes a he inpus of he logical circui. The logical circui processes he inpu levels and delivers oupu levels, ha have a funcional coherence o he inpu levels. A a digial circui he oupu values appear afer an inernal delay ime. In circuis wih memory-behavior (sequenial sysems) he previous hisory is included ino he logical combinaion. Because here are only wo saes, ideally occure square pulse signals. A many digial circuis iself he influence of inducors and capaciors canno be negleced. These energy-memories lead o falsificaions of he shape of he square pulses. A paricular circuis hese energy-memories are used for pulse shaping. This leads o pulses, ha have riangular, rapezium or exponenial shapes. In he following par-secions he parameers of impulses and he impulse-behavior of simple passive neworks are reaed. A more exac descripion of impulse echnics is given in he references.. hapes and parameers of impulses In he sandard IN 5488 he elecric impulse is described as process wih any emporal course, whose momenary value in definie areas of ime is differen from zero. An I M P L E is a process wih any course in ime of a physical quaniy, whose momenary value has wihin a definie space of ime values, which are no zero. niversiy of EFINITION OF AN IMPLE (IN 5488) IPT- An impulse consequenly is a signal wih seady saring and final value. In final imeinervals signal-aleraions beween hese values appear
2 A pulsed quaniy is a periodical process of a series of equal impulses. There are possible many courses in ime: - one sided impulses wih no change of polariy during he pulse duraion () a b c a) square pulse b) riangular pulse c) rapezium pulse niversiy of OE OF PLE AOING TO IN 5488 IPT-3 - square pulse (only wo values, ransiions from hese values in infinie shor ime) - real square-pulses in pracice are always rapezium pulses wih finie ransiion imes - if he duraion of a rapezium signal is shorened, i originaes a riangular signal, if he impulse-op vanishes and he edges ouch iself Because of processes of charging and uncharging a capaciors and inducors appear exponenial impulses. Figure IPT-4 shows his ypical impulses. quare pulse (IPT-3 a), riangular pulse (IPT-3 b), rapezium pulse (IPT-3 c), impulse wih riangle-increase and exponenial fall (IPT-4 a), square pulse wih exponenial fall (IPT-4 b) Two sided pulses have a change of polariy (alernaing pulse)
3 () a b a) unequal rising and falling pulse b) exponenial pulse niversiy of OE OF PLE AOING TO IN 5488 IPT-4 quare pulses wih exremely shor impulse-duraion are named as "needle-impulses" or "spike pulse" (IPT-7). () T niversiy of PIKE PLE IPT-7 aring from an impulse-duraion T and an impuls ampliude an impulse is defined, ha for a consan impulse-area T * a he border crossing-poin T agains zero shows an infiniely high ampliude. This impulse is called "irac-impulse"
4 An impulse is characerized by he following parameers: () % 9 % O 5 % T P T % T T F niversiy of EFINITION IPT- IPT- shows a real square-pulse wih he definiions: - rise ime T, - fall ime T F, - duraion ime T (pulse duraion, pulse widh), - pulse ampliude MAX - MIN, - pulse op MAX, - pulse boom MIN, - ramp off d / and - overshoo O O / A periodical impulses is addiionally given: - pause ime T P (pause duraion, puls pause), - periode T T T P, - repeiion frequency f / T and - duy cycle v T T / T (pulse duy facor). The definiion of he ramp off is only a he signals meaningful, ha have a nearly linear ramp off or increase of he ampliude. The rise- and fall-imes are measured beween he % and 9% values (,*( MAX - MIN ) and.9*( MAX - MIN )). The duraion-ime and he pause-duraion are measured a.5*( MAX - MIN ) or a he swiching hreshold of a logic circui (a TTL is.5 V). The values of MIN and MAX are averages of he minimum- and maximum-ampliudes, ha means, ha shor-ime appearing over- and under-shoos are no considered
5 eal square-pulses in pracice are always rapezium impulses wih clear visible rise- and fallimes. The ransiions of MIN o MAX, i.e. of LOW o HIGH, or of HIGH o LOW are named as "posiive" respecively as "negaive edges". If he duraion of a rapezium signal is shorened, i originaes a riangular signal, if he impulse-op vanishes and he edges ouch iself. The edge-seepness a he posiive and he negaive edge are in his case consan d / d / cons. (.) Triangular impulses appear, if energy-memories are charged or uncharged. The volage a a capacior raises a a consan charging curren linear in ime. The impulse is riangular, if he capacior is uncharged again by a consan curren. Because of processes of charging and uncharging a capaciors and inducors appear exponenial impulses (see figure IPT-4). A he employmen of elecronic swiches appear because of nonlinear effecs differen charging- and uncharging processes. o follows a he charging of a capacior by a volagesource wih consan swich-resisor an exponenial increase, a he uncharging he volage sinks linear, because he swich a his ransiion shows a curren-source-behavior. There are possible all mixed forms of impulses. For he calculaion of impulse-parameers he characerisic signal-parameerss of he signaland nework-heory are used for impulses oo. I is valid (exemplary for he volage): The linear average-value as he inegral of he volage relaive on a ime-inerval: i T () d (.) T and he roo mean square ( M ): i T / M () d (.3) T T / The quoien ou of impulse-op-value MAX and he roo mean square-value M is called peak-value or cresfacor. I is valid MAX F (.4) M - 8 -
6 . Impulse-funcions () A ( - ) A () () niversiy of ELEMENTAY PLE FNTION IPT-3 For he mahemaical descripion of a square pulse he sep-funcion and he sep-funcion wih ime lag are used. These funcions are defined as für < () (.5a) A für für < ( ) (.5b) A für Through superposiion of uni-sep-funcions wih ime lag follows: () () ( ) { [ ( T )]} f (.6) The irac-impulse and he uni-irac-impulse: für () (.7a) für für () (.7b) für The ramp-funcion: für () (.8) für > - 9 -
7 .3 Impulse-behavior of passive wo-pors The wo-por, in he pas named as "quadrupole", is a circui wih wo inpu-connecions and wo oupu-connecions. The wo-pors, ha we calculae, only have resisors, capaciors and inducors. They are ime-invariable and linear. Wih he aid of he nework-heory for wo-pors he linear behavior of neworks can be calculaed. The impulse-behavior of high- and low-passes for he half-t-circui or volage divider circui wih one energy-memory is invesigaed. The high-pass wih an energy-memory can be a -circui or a L-circui. I() niversiy of () () () HIGH-PA I() () () L L () IPT- The -high-pass is driven a he ime by a volage sep wih he ampliude. Ideally exiss no rise-ime (T ) and he consan volage is valid for imes >. The mesh of he circui yields (d by d): Wih follows () () () I() (.) I () d (.) d d () (.) d - -
8 This is a differenial equaion of he firs order. In consideraion of he condiions ( ) and ( ) follows he soluion () exp (.3) and I () A (.4) () () exp () () exp (.5) wih he ime-consan (.6) The courses of he volages (), (), () and he curren I() shows figure IPT-. () () () I() niversiy of TEP-EPONE -HIGH-PA IPT- A he ime he volage () has he value.37, () has raised on,63. A he ime 4.6 () has he value, and ( ),99. The capacior is nearly charged compleely. The volage a he oupu () shows a differenial behavior. o he circui is named differeniaing circui. For he L-high-pass is valid: () () I ( ) ( ) (.7) L L L - -
9 Wih L () di L L (.8) d follows I L di L L() (.9) d nder consideraion of he condiions I L ( ) and I L ( ) / follows he soluion I L () exp (.) and A (.) () exp () L () I () exp L (.) wih he ime-consan L. (.3) Are high-passes driven by a square pulse-volage a he inpu, so appears a he falling edge a negaive oupu-volage. This can be calculaed wih he superposiion, because he squarepulse consiss ou of wo overlaid emporal posponed sep-funcions. niversiy of E () A () () A () E - square pulse HIGH-PA AN QAE PLE T / IPT-5 - -
10 For a square pulse a a high-pass i is valid: A () exp (.6) 3 K K K.! 3! Wih erminaion of he series afer he linear erm and wih T and >> T follows he approximaion T A ( T ), (.7) he decrease of he volage by he ramp off A ( T ) (.8) and T. (.9) I follows he relaive ramp off T d. (.3) A T E () has a negaive edge (sep o zero). This sep effecs a volage sep of a he resisor (he volage a a capacior never can jump!!) and one ges a negaive value of A ()
11 Is a high-pass driven by a periodical square pulse one ges in he seady sae he following exreme-values of he oupu-volage in: E () A () A T T P A niversiy of HIGH-PA AN QAE PLE PEIO IPT-6 and TP exp AMAX (.4) T exp T exp AMIN (.5) T exp wih and T T T. P The calculaion of hese values: (for he seady sae is valid ) Firs inerval ( < T ): ( dash) A ' ' ( ) AMAX exp - 4 -
12 A T : T ( T ) exp A AMAX AMIN econd inerval (T < T T P ): A A T T P : A ( ' ) AMIN exp ' T P ( T T ) exp P AMIN T AMAX These are wo equaions wih wo unknown values. o one can calculae he exreme-values
13 A low-pass is as - or L-circui: I() niversiy of () () () LOW-PA I() L () L () () IPT- One ges for he volages and he curren a a -low-pass: () exp A (), (.3) () () exp, (.3) I () () exp (.33) and he ime-consan For a L-low-pass is valid: wih he ime-consan. (.34) A (.35) () exp () L. (.36) - 6 -
14 In he echnology of digial circuis one ofen finds wo-pors wih only one ime-consan. A hese circuis one can ake direcly he general soluion of he differenial-equaion of. order for deermine he course of he exponenial funcion. If one knows he sar-value ( ), he final value ( ) and he ime-consan he following soluion is valid: E () Z Z () A niversiy of () E () E - sep-funcion IIT WITH IMPEANE IPT-5 ( ) ( ) [ ( ) ( ) ] exp. (.39) or in oher forms () ( ) ( exp ) wih ( ) ( ) () ( ) exp. Pus one for T*, so one ges for his ime a definie volage ( T*). In his case one can calculae by knowledge (e.g. hrough measuremen) of ( T*) he belonging ime T*. Ou of (.39) follows ( ) ( ) * ( ) ( ) T ln. (.4) * T For he deerminaion of any ime-inervals T T - T a an exponenial course (wihou inermission and only wih one ime-consan) i is valid, if he volage has changed in he ime T abou (T ) - (T ): - 7 -
15 ( ) ( ) T ln. (.4) T For he deerminaion of he rise-ime and fall-ime one ses,9 -,,8. Then follows T T T,. The overview-figure IPT-5 shows all combinaions wih sep-answers of simple circuis, ha can be realized by he volage divider circui. The sar- and final-values of he sep-answers and he ime-consans are in he able. Z Z a b c d e f g h i j k l m n () niversiy of -IIT WITH ONE TIME ONTANT IPT-5-8 -
16 - 9 - a: b: c: d: ) ( e: f: g: h: ) ( i: j: k: more han one ime consan ) ( ) ( l: m: n: more han one ime consan ) ( ) (
17 .4 ircuis for producing impulses.4. omparaors The comparaor-funcion can be realized by an operaional amplifier, if he invering inpu is conneced wih a reference-volage and he noninvering is he inpu of he circui. OMP niversiy of OMPAATO EBE-36 The ransfer-characerisic shows figure EBE-36: niversiy of TANFE HAATEITI OF A OMPAATO EBE-36 The levels can be adaped o he level-range of a circui-family (e.g. TTL). - -
18 .4. chmi-trigger A level-conrolled rigger-circui wih wo differen hreshold-volages is called chmirigger. The difference of he swich-on-hreshold IE and he swich-off-hreshold IA is he hyseresis H. Figure T-4 shows he symbol and he ransfer-characerisic of a chmi-rigger. niversiy of I Q Q QY YMBOL AN HAATE- ITI OF THE HMITT- TIGGE QX IA IE I T-4 The mode of operaion shows figure T-4. I niversiy of IE IA Q QY MOE OF OPEATION OF THE HMITT- TIGGE QX T-4 - -
19 One can see, ha a disurbed inpu-signal is regeneraed by a chmi-rigger. Forbidden levels do no lead o a swiching of he oupu of he chmi-rigger. o his circui can be used as signal-regeneraor..4.3 Timer Asable and monosable circuis wih logic-circuis (NAN or NO) show deviaions ino he emporal course, because of unsable hreshold-volage and because of deviaions of he inpuand oupu-resisors. To he avoidance of hese disadvanages inegraed imer-circuis were developped, ha include a precision chmi-rigger and a -flipflop. An in he ONcondiion very low resisive swiching-ransisor serves for a fas discharging of a imecapacior. By exernal resisors and he ime-capacior is generaed he required impulsewidh. The figure T-6 shows he srucure of he precision-chmi-rigger. OMP G A IA > Q I K A I OMP > I IB K B G B Q I B I A I niversiy of PEIION HMITT TIGGE T-6 The hreshold-volages are derived from reference-volages, ha are a he inpus of wo comparaors K A and K B. A -flipflop is cleared (Q L), if he inpu-volage I crosses he level IA, and se, if I falls under he level IB. I IB :, : se IB I IA :, : sore (hold) IA I :, : rese (clear) IB I IA :, : sore (hold) I IB :, : se This circui is used a he "sandard" imer 555 and 7555 (in TTL- respecively MOechnology). The simplified circui of he imer wih he applicaion as asable rigger-circui (mulivibraor) shows figure T-6: - -
20 K A G A OMP > Q Y OMP > KB G B T niversiy of MLTIVIBATO WITH TIME 555 T-6 By he volage-divider consising ou of he hree same resisors from he supply-volage are derived he reference-volages A and B. Through he high relaive accuracy of he resisors wih deviaions of maximum % (yp. 5%) a he 555 and maximum 6% (yp. %) a he 7555 only a low ime-error appears. The hresholds B and A are / 3 and / 3. A he asable circui he -flipflop is cleared if he volage a he capacior is higher han he upper hreshold A, i.e. he oupu Y has LOW-level. The oupu of he flipflop has HIGH-level, he ransisor T is conducing and he capacior is discharged over he resisor, unil he lower hreshold B is reached. Then he oupu of comparaor K B has HIGHlevel, ses he -flipflop and closes he ransisor T. Over he resisors of and he capacior is charged again. o he capacior-volage in he seady sae changes wih exponenial course beween A and B. Inerval T : Inerval T P : /3,, ( ) * /3,, * The impulse-duraion follows o T ( ) * * ln[( B ) / ( A )] T ( ) * * ln and he impulse-pause o T P * * ln[ A / B ] T P * * ln - 3 -
21 niversiy of 3 3 Y T T P IMPLE- IAGAM OF THE MLTI- VIBATO WITH TIME 555 T-6 I follows he frequency f / (T T P ),44 / [(! ) * ] A symmerical recangle-vibraion wih a pulse-duy-facor v T,5 (T T P ) can be generaed, if parallel o he resisor a diode is swiched, whose caode is conneced wih he capacior. The resisors and mus have he same value. A he charging of he capacior hrough he conducing-resisor F of he diode is bridged. For >> F one ges approximaely he same ime-consans for charging and discharging. I is possible o change he values for he hreshold-volages by changing he volage-divider or he supply-volage. The change of he supply-volage enables he employmen of he imer as a volage conrolled oscillaor (VO) or as frequency-modulaor. Wih a simple circui-aleraion he imer operaes as monosable rigger-circui (T-6). Ino he sable sae he capacior is shorened consanly by he conducing ransisor T. A LOW-acive rigger-impulse a he comparaor K B ses he -flipflop and he ransisor T is blocked. The capacior is charged over he resisor from nearly V unil A / 3. The -FF is cleared, he oupu has he LOW-level. Now he capacior is discharged over he ransisor T in a very shor ime (T-6). Inerval T : V,, * The impulse-duraion follows o T * * ln[( V) / ( A )] T * * ln 3-4 -
22 K A OMP G A > Q Y OMP > X K B G B T niversiy of MONOFLOP WITH TIME 555 T-6 X niversiy of 3 T IMPLE- IAGAM OF THE MONOFLOP WITH TIME 555 Y T-6 Wih help of an exernal ransisor T* he monoflop can be expanded as a reriggerable monosable rigger-circui. The circui and he courses of he impulses are shown in he figures T-65 and T-66. The rigger-impulse discharges in his HIGH-phase he capacior and ses he oupu Y o HIGH. If he rigger-impulse reaches he LOW-level he exernal ransisor T* is blocked, and could be charged over he resisor. If during his phase a new rigger-impulse appears, he capacior is discharged over T*. The oupu Y remains all he ime on HIGH, unil he - 5 -
23 capacior-volage reaches he hreshold A. The pulse-duraion T is beween he falling edge of he las rigger-impulse and he falling edge of he oupu-signal Y. This circui can be used for deecing missing-pulses, e. g. clock-impulses of a microprocessor (wachdog). K A OMP G A > Q Y T * OMP > I K B G B T niversiy of ETIGGEABLE MONOFLOP WITH TIME 555 T-65 I niversiy of 3 T IMPLE- IAGAM OF THE MONOFLOP WITH TIME 555 Y T
U(t) (t) -U T 1. (t) (t)
Prof. Dr.-ng. F. Schuber Digial ircuis Exercise. () () A () - T T The highpass is driven by he square pulse (). alculae and skech A (). = µf, = KΩ, = 5 V, T = T = ms. Exercise. () () A () T T The highpass
More informationChapter 7 Response of First-order RL and RC Circuits
Chaper 7 Response of Firs-order RL and RC Circuis 7.- The Naural Response of RL and RC Circuis 7.3 The Sep Response of RL and RC Circuis 7.4 A General Soluion for Sep and Naural Responses 7.5 Sequenial
More informationUniversity of Cyprus Biomedical Imaging and Applied Optics. Appendix. DC Circuits Capacitors and Inductors AC Circuits Operational Amplifiers
Universiy of Cyprus Biomedical Imaging and Applied Opics Appendix DC Circuis Capaciors and Inducors AC Circuis Operaional Amplifiers Circui Elemens An elecrical circui consiss of circui elemens such as
More informationnon-linear oscillators
non-linear oscillaors The invering comparaor operaion can be summarized as When he inpu is low, he oupu is high. When he inpu is high, he oupu is low. R b V REF R a and are given by he expressions derived
More informationNon Linear Op Amp Circuits.
Non Linear Op Amp ircuis. omparaors wih 0 and non zero reference volage. omparaors wih hyseresis. The Schmid Trigger. Window comparaors. The inegraor. Waveform conversion. Sine o ecangular. ecangular o
More information( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is
UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires
More informationChapter 8 The Complete Response of RL and RC Circuits
Chaper 8 The Complee Response of RL and RC Circuis Seoul Naional Universiy Deparmen of Elecrical and Compuer Engineering Wha is Firs Order Circuis? Circuis ha conain only one inducor or only one capacior
More informationEECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits
EEE25 ircui Analysis I Se 4: apaciors, Inducors, and Firs-Order inear ircuis Shahriar Mirabbasi Deparmen of Elecrical and ompuer Engineering Universiy of Briish olumbia shahriar@ece.ubc.ca Overview Passive
More informationBasic Principles of Sinusoidal Oscillators
Basic Principles of Sinusoidal Oscillaors Linear oscillaor Linear region of circui : linear oscillaion Nonlinear region of circui : ampliudes sabilizaion Barkhausen crierion X S Amplifier A X O X f Frequency-selecive
More informationCHAPTER 6: FIRST-ORDER CIRCUITS
EEE5: CI CUI T THEOY CHAPTE 6: FIST-ODE CICUITS 6. Inroducion This chaper considers L and C circuis. Applying he Kirshoff s law o C and L circuis produces differenial equaions. The differenial equaions
More informationTopic Astable Circuits. Recall that an astable circuit has two unstable states;
Topic 2.2. Asable Circuis. Learning Objecives: A he end o his opic you will be able o; Recall ha an asable circui has wo unsable saes; Explain he operaion o a circui based on a Schmi inverer, and esimae
More informationL1, L2, N1 N2. + Vout. C out. Figure 2.1.1: Flyback converter
page 11 Flyback converer The Flyback converer belongs o he primary swiched converer family, which means here is isolaion beween in and oupu. Flyback converers are used in nearly all mains supplied elecronic
More informationEEEB113 CIRCUIT ANALYSIS I
9/14/29 1 EEEB113 CICUIT ANALYSIS I Chaper 7 Firs-Order Circuis Maerials from Fundamenals of Elecric Circuis 4e, Alexander Sadiku, McGraw-Hill Companies, Inc. 2 Firs-Order Circuis -Chaper 7 7.2 The Source-Free
More informationRC, RL and RLC circuits
Name Dae Time o Complee h m Parner Course/ Secion / Grade RC, RL and RLC circuis Inroducion In his experimen we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors.
More informationHomework-8(1) P8.3-1, 3, 8, 10, 17, 21, 24, 28,29 P8.4-1, 2, 5
Homework-8() P8.3-, 3, 8, 0, 7, 2, 24, 28,29 P8.4-, 2, 5 Secion 8.3: The Response of a Firs Order Circui o a Consan Inpu P 8.3- The circui shown in Figure P 8.3- is a seady sae before he swich closes a
More informationLab 10: RC, RL, and RLC Circuits
Lab 10: RC, RL, and RLC Circuis In his experimen, we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors. We will sudy he way volages and currens change in
More informationBasic Circuit Elements Professor J R Lucas November 2001
Basic Circui Elemens - J ucas An elecrical circui is an inerconnecion of circui elemens. These circui elemens can be caegorised ino wo ypes, namely acive and passive elemens. Some Definiions/explanaions
More information8. Basic RL and RC Circuits
8. Basic L and C Circuis This chaper deals wih he soluions of he responses of L and C circuis The analysis of C and L circuis leads o a linear differenial equaion This chaper covers he following opics
More informationPulse Generators. Any of the following calculations may be asked in the midterms/exam.
ulse Generaors ny of he following calculaions may be asked in he miderms/exam.. a) capacior of wha capaciance forms an RC circui of s ime consan wih a 0 MΩ resisor? b) Wha percenage of he iniial volage
More informationi L = VT L (16.34) 918a i D v OUT i L v C V - S 1 FIGURE A switched power supply circuit with diode and a switch.
16.4.3 A SWITHED POWER SUPPY USINGA DIODE In his example, we will analyze he behavior of he diodebased swiched power supply circui shown in Figure 16.15. Noice ha his circui is similar o ha in Figure 12.41,
More informationReading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.
PHY1 Elecriciy Topic 7 (Lecures 1 & 11) Elecric Circuis n his opic, we will cover: 1) Elecromoive Force (EMF) ) Series and parallel resisor combinaions 3) Kirchhoff s rules for circuis 4) Time dependence
More informationDesigning Information Devices and Systems I Spring 2019 Lecture Notes Note 17
EES 16A Designing Informaion Devices and Sysems I Spring 019 Lecure Noes Noe 17 17.1 apaciive ouchscreen In he las noe, we saw ha a capacior consiss of wo pieces on conducive maerial separaed by a nonconducive
More informationPhysical Limitations of Logic Gates Week 10a
Physical Limiaions of Logic Gaes Week 10a In a compuer we ll have circuis of logic gaes o perform specific funcions Compuer Daapah: Boolean algebraic funcions using binary variables Symbolic represenaion
More informationTimer 555. Digital Electronics
Timer 555 Digial Elecronics This presenaion will Inroduce he 555 Timer. 555 Timer Derive he characerisic equaions for he charging and discharging of a capacior. Presen he equaions for period, frequency,
More informationV L. DT s D T s t. Figure 1: Buck-boost converter: inductor current i(t) in the continuous conduction mode.
ECE 445 Analysis and Design of Power Elecronic Circuis Problem Se 7 Soluions Problem PS7.1 Erickson, Problem 5.1 Soluion (a) Firs, recall he operaion of he buck-boos converer in he coninuous conducion
More informationES 250 Practice Final Exam
ES 50 Pracice Final Exam. Given ha v 8 V, a Deermine he values of v o : 0 Ω, v o. V 0 Firs, v o 8. V 0 + 0 Nex, 8 40 40 0 40 0 400 400 ib i 0 40 + 40 + 40 40 40 + + ( ) 480 + 5 + 40 + 8 400 400( 0) 000
More informationSilicon Controlled Rectifiers UNIT-1
Silicon Conrolled Recifiers UNIT-1 Silicon Conrolled Recifier A Silicon Conrolled Recifier (or Semiconducor Conrolled Recifier) is a four layer solid sae device ha conrols curren flow The name silicon
More informationChapter 4 DC converter and DC switch
haper 4 D converer and D swich 4.1 Applicaion - Assumpion Applicaion: D swich: Replace mechanic swiches D converer: in racion drives Assumions: Ideal D sources Ideal Power emiconducor Devices 4.2 D swich
More informationCHAPTER 12 DIRECT CURRENT CIRCUITS
CHAPTER 12 DIRECT CURRENT CIUITS DIRECT CURRENT CIUITS 257 12.1 RESISTORS IN SERIES AND IN PARALLEL When wo resisors are conneced ogeher as shown in Figure 12.1 we said ha hey are conneced in series. As
More informationR.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder#
.#W.#Erickson# Deparmen#of#Elecrical,#Compuer,#and#Energy#Engineering# Universiy#of#Colorado,#Boulder# Chaper 2 Principles of Seady-Sae Converer Analysis 2.1. Inroducion 2.2. Inducor vol-second balance,
More information2.4 Cuk converter example
2.4 Cuk converer example C 1 Cuk converer, wih ideal swich i 1 i v 1 2 1 2 C 2 v 2 Cuk converer: pracical realizaion using MOSFET and diode C 1 i 1 i v 1 2 Q 1 D 1 C 2 v 2 28 Analysis sraegy This converer
More informationSequential Logic. Digital Integrated Circuits A Design Perspective. Latch versus Register. Naming Conventions. Designing Sequential Logic Circuits
esigning Sequenial Logic Circuis Adaped from Chaper 7 of igial egraed Circuis A esign Perspecive Jan M. Rabaey e al. Copyrigh 23 Prenice Hall/Pearson Sequenial Logic pus Curren Sae COMBINATIONAL LOGIC
More informationEE100 Lab 3 Experiment Guide: RC Circuits
I. Inroducion EE100 Lab 3 Experimen Guide: A. apaciors A capacior is a passive elecronic componen ha sores energy in he form of an elecrosaic field. The uni of capaciance is he farad (coulomb/vol). Pracical
More informationh[n] is the impulse response of the discrete-time system:
Definiion Examples Properies Memory Inveribiliy Causaliy Sabiliy Time Invariance Lineariy Sysems Fundamenals Overview Definiion of a Sysem x() h() y() x[n] h[n] Sysem: a process in which inpu signals are
More informationThe problem with linear regulators
he problem wih linear regulaors i in P in = i in V REF R a i ref i q i C v CE P o = i o i B ie P = v i o o in R 1 R 2 i o i f η = P o P in iref is small ( 0). iq (quiescen curren) is small (probably).
More information2.9 Modeling: Electric Circuits
SE. 2.9 Modeling: Elecric ircuis 93 2.9 Modeling: Elecric ircuis Designing good models is a ask he compuer canno do. Hence seing up models has become an imporan ask in modern applied mahemaics. The bes
More informationDirect Current Circuits. February 19, 2014 Physics for Scientists & Engineers 2, Chapter 26 1
Direc Curren Circuis February 19, 2014 Physics for Scieniss & Engineers 2, Chaper 26 1 Ammeers and Volmeers! A device used o measure curren is called an ammeer! A device used o measure poenial difference
More informationINDEX. Transient analysis 1 Initial Conditions 1
INDEX Secion Page Transien analysis 1 Iniial Condiions 1 Please inform me of your opinion of he relaive emphasis of he review maerial by simply making commens on his page and sending i o me a: Frank Mera
More informationEE202 Circuit Theory II , Spring. Dr. Yılmaz KALKAN & Dr. Atilla DÖNÜK
EE202 Circui Theory II 2018 2019, Spring Dr. Yılmaz KALKAN & Dr. Ailla DÖNÜK 1. Basic Conceps (Chaper 1 of Nilsson - 3 Hrs.) Inroducion, Curren and Volage, Power and Energy 2. Basic Laws (Chaper 2&3 of
More informationLecture 13 RC/RL Circuits, Time Dependent Op Amp Circuits
Lecure 13 RC/RL Circuis, Time Dependen Op Amp Circuis RL Circuis The seps involved in solving simple circuis conaining dc sources, resisances, and one energy-sorage elemen (inducance or capaciance) are:
More information555 Timer. Digital Electronics
555 Timer Digial Elecronics This presenaion will Inroduce he 555 Timer. 555 Timer Derive he characerisic equaions for he charging and discharging of a capacior. Presen he equaions for period, frequency,
More informationSignal and System (Chapter 3. Continuous-Time Systems)
Signal and Sysem (Chaper 3. Coninuous-Time Sysems) Prof. Kwang-Chun Ho kwangho@hansung.ac.kr Tel: 0-760-453 Fax:0-760-4435 1 Dep. Elecronics and Informaion Eng. 1 Nodes, Branches, Loops A nework wih b
More information(b) (a) (d) (c) (e) Figure 10-N1. (f) Solution:
Example: The inpu o each of he circuis shown in Figure 10-N1 is he volage source volage. The oupu of each circui is he curren i( ). Deermine he oupu of each of he circuis. (a) (b) (c) (d) (e) Figure 10-N1
More informationChapter 2: Principles of steady-state converter analysis
Chaper 2 Principles of Seady-Sae Converer Analysis 2.1. Inroducion 2.2. Inducor vol-second balance, capacior charge balance, and he small ripple approximaion 2.3. Boos converer example 2.4. Cuk converer
More informationUniversità degli Studi di Roma Tor Vergata Dipartimento di Ingegneria Elettronica. Analogue Electronics. Paolo Colantonio A.A.
Universià degli Sudi di Roma Tor Vergaa Diparimeno di Ingegneria Eleronica Analogue Elecronics Paolo Colanonio A.A. 2015-16 Diode circui analysis The non linearbehaviorofdiodesmakesanalysisdifficul consider
More informationElectrical Circuits. 1. Circuit Laws. Tools Used in Lab 13 Series Circuits Damped Vibrations: Energy Van der Pol Circuit
V() R L C 513 Elecrical Circuis Tools Used in Lab 13 Series Circuis Damped Vibraions: Energy Van der Pol Circui A series circui wih an inducor, resisor, and capacior can be represened by Lq + Rq + 1, a
More informationChapter 9 Sinusoidal Steady State Analysis
Chaper 9 Sinusoidal Seady Sae Analysis 9.-9. The Sinusoidal Source and Response 9.3 The Phasor 9.4 pedances of Passive Eleens 9.5-9.9 Circui Analysis Techniques in he Frequency Doain 9.0-9. The Transforer
More informationECE 2100 Circuit Analysis
ECE 1 Circui Analysis Lesson 35 Chaper 8: Second Order Circuis Daniel M. Liynski, Ph.D. ECE 1 Circui Analysis Lesson 3-34 Chaper 7: Firs Order Circuis (Naural response RC & RL circuis, Singulariy funcions,
More information( ) = Q 0. ( ) R = R dq. ( t) = I t
ircuis onceps The addiion of a simple capacior o a circui of resisors allows wo relaed phenomena o occur The observaion ha he ime-dependence of a complex waveform is alered by he circui is referred o as
More informationLAPLACE TRANSFORM AND TRANSFER FUNCTION
CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions
More information6.01: Introduction to EECS I Lecture 8 March 29, 2011
6.01: Inroducion o EES I Lecure 8 March 29, 2011 6.01: Inroducion o EES I Op-Amps Las Time: The ircui Absracion ircuis represen sysems as connecions of elemens hrough which currens (hrough variables) flow
More informationd 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3
and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or
More informationExperimental Buck Converter
Experimenal Buck Converer Inpu Filer Cap MOSFET Schoky Diode Inducor Conroller Block Proecion Conroller ASIC Experimenal Synchronous Buck Converer SoC Buck Converer Basic Sysem S 1 u D 1 r r C C R R X
More informationEECS 141: FALL 00 MIDTERM 2
Universiy of California College of Engineering Deparmen of Elecrical Engineering and Compuer Science J. M. Rabaey TuTh9:30-11am ee141@eecs EECS 141: FALL 00 MIDTERM 2 For all problems, you can assume he
More information9. Alternating currents
WS 9. Alernaing currens 9.1 nroducion Besides ohmic resisors, capaciors and inducions play an imporan role in alernaing curren (AC circuis as well. n his experimen, one shall invesigae heir behaviour in
More informationElectrical and current self-induction
Elecrical and curren self-inducion F. F. Mende hp://fmnauka.narod.ru/works.hml mende_fedor@mail.ru Absrac The aricle considers he self-inducance of reacive elemens. Elecrical self-inducion To he laws of
More informationContinuous Time. Time-Domain System Analysis. Impulse Response. Impulse Response. Impulse Response. Impulse Response. ( t) + b 0.
Time-Domain Sysem Analysis Coninuous Time. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 1. J. Robers - All Righs Reserved. Edied by Dr. Rober Akl 2 Le a sysem be described by a 2 y ( ) + a 1
More informationADDITIONAL PROBLEMS (a) Find the Fourier transform of the half-cosine pulse shown in Fig. 2.40(a). Additional Problems 91
ddiional Problems 9 n inverse relaionship exiss beween he ime-domain and freuency-domain descripions of a signal. Whenever an operaion is performed on he waveform of a signal in he ime domain, a corresponding
More informationSome Basic Information about M-S-D Systems
Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,
More information10. State Space Methods
. Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he
More informationUnified Control Strategy Covering CCM and DCM for a Synchronous Buck Converter
Unified Conrol Sraegy Covering CCM and DCM for a Synchronous Buck Converer Dirk Hirschmann, Sebasian Richer, Chrisian Dick, Rik W. De Doncker Insiue for Power Elecronics and Elecrical Drives RWTH Aachen
More informationdv 7. Voltage-current relationship can be obtained by integrating both sides of i = C :
EECE202 NETWORK ANALYSIS I Dr. Charles J. Kim Class Noe 22: Capaciors, Inducors, and Op Amp Circuis A. Capaciors. A capacior is a passive elemen designed o sored energy in is elecric field. 2. A capacior
More informationAC Circuits AC Circuit with only R AC circuit with only L AC circuit with only C AC circuit with LRC phasors Resonance Transformers
A ircuis A ircui wih only A circui wih only A circui wih only A circui wih phasors esonance Transformers Phys 435: hap 31, Pg 1 A ircuis New Topic Phys : hap. 6, Pg Physics Moivaion as ime we discovered
More informationLecture -14: Chopper fed DC Drives
Lecure -14: Chopper fed DC Drives Chopper fed DC drives o A chopper is a saic device ha convers fixed DC inpu volage o a variable dc oupu volage direcly o A chopper is a high speed on/off semiconducor
More informationLearning Objectives: Practice designing and simulating digital circuits including flip flops Experience state machine design procedure
Lab 4: Synchronous Sae Machine Design Summary: Design and implemen synchronous sae machine circuis and es hem wih simulaions in Cadence Viruoso. Learning Objecives: Pracice designing and simulaing digial
More informationUNIVERSITY OF CALIFORNIA AT BERKELEY
Homework #10 Soluions EECS 40, Fall 2006 Prof. Chang-Hasnain Due a 6 pm in 240 Cory on Wednesday, 04/18/07 oal Poins: 100 Pu (1) your name and (2) discussion secion number on your homework. You need o
More informationSOLUTIONS TO ECE 3084
SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no
More informationECE 2100 Circuit Analysis
ECE 1 Circui Analysis Lesson 37 Chaper 8: Second Order Circuis Discuss Exam Daniel M. Liynski, Ph.D. Exam CH 1-4: On Exam 1; Basis for work CH 5: Operaional Amplifiers CH 6: Capaciors and Inducor CH 7-8:
More informationChapter 10 INDUCTANCE Recommended Problems:
Chaper 0 NDUCTANCE Recommended Problems: 3,5,7,9,5,6,7,8,9,,,3,6,7,9,3,35,47,48,5,5,69, 7,7. Self nducance Consider he circui shown in he Figure. When he swich is closed, he curren, and so he magneic field,
More informationFirst Order RC and RL Transient Circuits
Firs Order R and RL Transien ircuis Objecives To inroduce he ransiens phenomena. To analyze sep and naural responses of firs order R circuis. To analyze sep and naural responses of firs order RL circuis.
More informationVoltage/current relationship Stored Energy. RL / RC circuits Steady State / Transient response Natural / Step response
Review Capaciors/Inducors Volage/curren relaionship Sored Energy s Order Circuis RL / RC circuis Seady Sae / Transien response Naural / Sep response EE4 Summer 5: Lecure 5 Insrucor: Ocavian Florescu Lecure
More informationMath 333 Problem Set #2 Solution 14 February 2003
Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial
More informationApplication Note AN Software release of SemiSel version 3.1. New semiconductor available. Temperature ripple at low inverter output frequencies
Applicaion Noe AN-8004 Revision: Issue Dae: Prepared by: 00 2008-05-21 Dr. Arend Winrich Ke y Words: SemiSel, Semiconducor Selecion, Loss Calculaion Sofware release of SemiSel version 3.1 New semiconducor
More informationVehicle Arrival Models : Headway
Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where
More informationSub Module 2.6. Measurement of transient temperature
Mechanical Measuremens Prof. S.P.Venkaeshan Sub Module 2.6 Measuremen of ransien emperaure Many processes of engineering relevance involve variaions wih respec o ime. The sysem properies like emperaure,
More informationContinuous Time Linear Time Invariant (LTI) Systems. Dr. Ali Hussein Muqaibel. Introduction
/9/ Coninuous Time Linear Time Invarian (LTI) Sysems Why LTI? Inroducion Many physical sysems. Easy o solve mahemaically Available informaion abou analysis and design. We can apply superposiion LTI Sysem
More informationSimulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010
Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid
More informationLabQuest 24. Capacitors
Capaciors LabQues 24 The charge q on a capacior s plae is proporional o he poenial difference V across he capacior. We express his wih q V = C where C is a proporionaliy consan known as he capaciance.
More informationChapter 3 Boundary Value Problem
Chaper 3 Boundary Value Problem A boundary value problem (BVP) is a problem, ypically an ODE or a PDE, which has values assigned on he physical boundary of he domain in which he problem is specified. Le
More informationV AK (t) I T (t) I TRM. V AK( full area) (t) t t 1 Axial turn-on. Switching losses for Phase Control and Bi- Directionally Controlled Thyristors
Applicaion Noe Swiching losses for Phase Conrol and Bi- Direcionally Conrolled Thyrisors V AK () I T () Causing W on I TRM V AK( full area) () 1 Axial urn-on Plasma spread 2 Swiching losses for Phase Conrol
More informationChapter 5: Discontinuous conduction mode. Introduction to Discontinuous Conduction Mode (DCM)
haper 5. The isconinuous onducion Mode 5.. Origin of he disconinuous conducion mode, and mode boundary 5.. Analysis of he conversion raio M(,K) 5.3. Boos converer example 5.4. Summary of resuls and key
More informationStructural Dynamics and Earthquake Engineering
Srucural Dynamics and Earhquae Engineering Course 1 Inroducion. Single degree of freedom sysems: Equaions of moion, problem saemen, soluion mehods. Course noes are available for download a hp://www.c.up.ro/users/aurelsraan/
More information- If one knows that a magnetic field has a symmetry, one may calculate the magnitude of B by use of Ampere s law: The integral of scalar product
11.1 APPCATON OF AMPEE S AW N SYMMETC MAGNETC FEDS - f one knows ha a magneic field has a symmery, one may calculae he magniude of by use of Ampere s law: The inegral of scalar produc Closed _ pah * d
More informationFundamentals of Power Electronics Second edition. Robert W. Erickson Dragan Maksimovic University of Colorado, Boulder
Fundamenals of Power Elecronics Second ediion Rober W. Erickson Dragan Maksimovic Universiy of Colorado, Boulder Chaper 1: Inroducion 1.1. Inroducion o power processing 1.2. Some applicaions of power elecronics
More informationCHAPTER 2 Signals And Spectra
CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par
More informationGuest Lectures for Dr. MacFarlane s EE3350 Part Deux
Gues Lecures for Dr. MacFarlane s EE3350 Par Deux Michael Plane Mon., 08-30-2010 Wrie name in corner. Poin ou his is a review, so I will go faser. Remind hem o go lisen o online lecure abou geing an A
More information04. Kinetics of a second order reaction
4. Kineics of a second order reacion Imporan conceps Reacion rae, reacion exen, reacion rae equaion, order of a reacion, firs-order reacions, second-order reacions, differenial and inegraed rae laws, Arrhenius
More informationSmart Highside Power Switch PROFET
Smar ighside Power Swich PROFET BTS 410E2 Feaures TO220AB/ Overload proecion Curren limiaion Shor circui proecion Thermal shudown 1 1 Overvolage proecion (including Sandard Sraigh leads SMD load dump)
More informationAnalytic Model and Bilateral Approximation for Clocked Comparator
Analyic Model and Bilaeral Approximaion for Clocked Comparaor M. Greians, E. Hermanis, G.Supols Insiue of, Riga, Lavia, e-mail: gais.supols@edi.lv Research is suppored by: 1) ESF projec Nr.1DP/1.1.1.2.0/09/APIA/VIAA/020,
More informationChapter 4 AC Network Analysis
haper 4 A Nework Analysis Jaesung Jang apaciance Inducance and Inducion Time-Varying Signals Sinusoidal Signals Reference: David K. heng, Field and Wave Elecromagneics. Energy Sorage ircui Elemens Energy
More informationChapter 5-4 Operational amplifier Department of Mechanical Engineering
MEMS08 Chaper 5-4 Operaional amplifier Deparmen of Mechanical Engineering Insrumenaion amplifier Very high inpu impedance Large common mode rejecion raio (CMRR) Capabiliy o amplify low leel signals Consisen
More informationChapter 5 Digital PID control algorithm. Hesheng Wang Department of Automation,SJTU 2016,03
Chaper 5 Digial PID conrol algorihm Hesheng Wang Deparmen of Auomaion,SJTU 216,3 Ouline Absrac Quasi-coninuous PID conrol algorihm Improvemen of sandard PID algorihm Choosing parameer of PID regulaor Brief
More informationMEMS 0031 Electric Circuits
MEMS 0031 Elecric Circuis Chaper 1 Circui variables Chaper/Lecure Learning Objecives A he end of his lecure and chaper, you should able o: Represen he curren and volage of an elecric circui elemen, paying
More information8.022 (E&M) Lecture 9
8.0 (E&M) Lecure 9 Topics: circuis Thevenin s heorem Las ime Elecromoive force: How does a baery work and is inernal resisance How o solve simple circuis: Kirchhoff s firs rule: a any node, sum of he currens
More information3. Alternating Current
3. Alernaing Curren TOPCS Definiion and nroducion AC Generaor Componens of AC Circuis Series LRC Circuis Power in AC Circuis Transformers & AC Transmission nroducion o AC The elecric power ou of a home
More informationDual Current-Mode Control for Single-Switch Two-Output Switching Power Converters
Dual Curren-Mode Conrol for Single-Swich Two-Oupu Swiching Power Converers S. C. Wong, C. K. Tse and K. C. Tang Deparmen of Elecronic and Informaion Engineering Hong Kong Polyechnic Universiy, Hunghom,
More informationLAB 5: Computer Simulation of RLC Circuit Response using PSpice
--3LabManualLab5.doc LAB 5: ompuer imulaion of RL ircui Response using Ppice PURPOE To use a compuer simulaion program (Ppice) o invesigae he response of an RL series circui o: (a) a sinusoidal exciaion.
More informationPT8A A-F/67A/68A NTC Heating Controller with Multi LEDs
PTA-A-F/A/A Feaures / seps hea emperaure seings wih EDs or EDs indicaor Auo emperaure conrol wih TC TC open proecion Pulse rigger for high curren / TRIAC (up o ma) Auo power off afer exac Hour heaing(i
More informationECE-205 Dynamical Systems
ECE-5 Dynamical Sysems Course Noes Spring Bob Throne Copyrigh Rober D. Throne Copyrigh Rober D. Throne . Elecrical Sysems The ypes of dynamical sysems we will be sudying can be modeled in erms of algebraic
More information23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes
Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals
More information