قسم: العلوم. This test includes three mandatory exercises. The use of non-programmable calculators is allowed.

Size: px
Start display at page:

Download "قسم: العلوم. This test includes three mandatory exercises. The use of non-programmable calculators is allowed."

Transcription

1 الهيئة األكاديمي ة المشتركة قسم: العلوم نموذج مسابقة )يراعي تعليق الدروس والتوصيف المعد ل للعام الدراسي المادة: الفيزياء الشهادة: الثانوية العام ة الفرع: علوم الحياة نموذج رقم 1 المد ة: ساعتان وحتى صدور المناهج المطو رة( This es includes hree andaory exercises. The use of non-prograable calculaors is allowed. xercise 1 (6 poins) Young s slis onsider he Young s slis device (Doc 1) ade up of wo very hin and horizonal slis S1 and S separaed by a disance a = 1, a screen () parallel o he plane conaining S1 and S and a onochroaic ligh source S. The screen () is a a disance D = fro he idpoin I of [S1S]. The ligh source (S) is on he perpendicular bisecor of [S1S]. This bisecor ees he screen () a a poin O. The wavelengh in air of he onochroaic ligh is = 650 n. (Doc 1) (P) 1) A paern is observed on he screen (). Indicae he nae of he corresponden phenoenon. ) Sae he condiions ensured by S1 and S in order o obain his paern. 3) onsider a poin M of he paern observed on he screen () such as OM x. Tae d1 = S1M and d = SM. Wrie he relaion ha gives he opical pah difference = d d1 a M in ers of a, D and x. 4) Define he inerfringe disance i. 5) Give he expression of i in ers of, D and a, hen calculae is value. 6) The poin O coincides wih he cenre of a fringe called cenral fringe. 6-1) alculae he opical pah difference a O. 6-) Specify wheher his fringe is brigh or dar. 7) Le N be he cenre of a fringe where =,75. Specify wheher his fringe is brigh or dar. 8) S is a a disance d = 10 c fro I. We displace S verically of a disance y = 1 c o he side of ax ay S1. The new opical pah difference is hen: '. Specify he direcion of he displaceen D d of he cenre of he cenral fringe (o he side of S1 or S) and calculae he displaceen. xercise (6 poins) () series circui The elecric circui of he docuen (Doc ) is fored of: A generaor delivering across is erinals a consan volage = 8 V; A resisor of unnown resisance ; A capacior of capaciance = 100 µf, iniially discharged; A swich K. K (Doc ) A B q -q 1/3

2 A he insan 0 = 0, we close he swich K. A an insan, he capacior is charged by q and he circui carries a curren i. 1) edraw he figure of he docuen (Doc ) and show he connecions of an oscilloscope ha allows o display he volage ug = across he generaor and he volage u = uab across he capacior. ) Wrie he expression of he curren i in ers of q. 3) Deduce he expression of i in ers of he capaciance and he volage u. 4) Deerine he differenial equaion ha describes he variaion of u as a funcion of ie. 5) The soluion of his differenial equaion is: u D 1 e. Deerine he expressions of he consans D and in ers of, and. 6) Deerine, a he insan =, he expression of he volage u in ers of. 7) eferring o he graph of u = f() of he docuen (Doc 3) below: 7-1) Deerine he value of. 7-) Deduce he value of he resisance. 8) Deerine he expression of he curren i as a funcion of ie. 9) Deduce he value of he curren i in seady sae. xercise 3 (7 poins) Horizonal elasic pendulu An air puc (S) of ass = 709 g is aached o he free end of a spring () of un-joined urns, of negligible ass and of siffness = 7 N. -l. This puc, of cenre of ass G, ay slide wihou fricion on a horizonal rail (Doc 4). The docuen (Doc 4) shows a horizonal axis Ox of origin O. A equilibriu, G coincides wih O. (S) is shifed 3 c fro O ( OG 0 = x 0 i = 3 i) in he posiive direcion and released wihou velociy a he insan 0 = 0. A an insan, x is he abscissa of G and dx v is he algebraic easure of is velociy. d /3

3 1) The echanical energy of he syse ((S), (), arh) is conserved. 1-1) Deerine he second order differenial equaion in x. 1-) Verify ha x x cos is he soluion of his differenial equaion. 1-3) alculae he values of he consans x and. ) Wrie down he expression of he naural period T0 of he oion in ers of and hen calculae is value. 3) The docuen (Doc 5) below shows he curves giving he variaions of he ineic energy K of (S), of he elasic poenial energy Pe of () and of he echanical energy M of he syse ((S), (), arh). Idenify he curves K, Pe and M of he docuen (Doc 5). 4) ach of he curves A and is sinusoidal of a period T. eferring o he graph of docuen (Doc 5) : 4-1) Pic up he value of he period T; 4-) opare is value o he naural period T0 of he oion. 3/3

4 الهيئة األكاديمي ة المشتركة قسم: العلوم أسس التصحيح )تراعي تعليق الدروس والتوصيف المعد ل للعام الدراسي المادة: الفيزياء الشهادة: الثانوية العام ة الفرع: علوم الحياة نموذج رقم 1 المد ة: ساعتان وحتى صدور المناهج المطو رة( xercise 1 (6 poins) Young s slis Quesion Answer Mar 1 Inerference. The ligh sources us be synchronous (hey us have he sae frequency) and coheren (hey us eep a consan phase difference). 3 ax D 4 The inerfringe disance is he disance beween he ceners of wo consecuive fringes of he sae naure. 5 D i a i i d = d1 = d d1 = 0 or x = 0 ax 0 D 6- = 0 so = wih = 0 Z The inerference is consrucive and he fringe is brigh so wih = 1 Z The inerference is desrucive and he fringe is dar. ax O' ay y.d 0 x O' D d d 10 xo' The cenral fringe oves 0. owards S 1/3

5 xercise (6 poins) () series circui Quesion Answer Mar 1 K P M A B dq i d 3 du q u so i d 4 Law of addiion of volages: 5 upm = upa +uab +ubm upa = u ; uab = u and ubm = 0 So : u u Ɐ Oh s law: u i u du d The differenial equaion in ers of u is hen: u D 1 e u D De du d u du 1 D D e e d du eplace u and by heir expressions in he differenial equaion. d We ge: D e D De Ɐ D( 1)e D 0 Ɐ Idenifying, we ge: D-=0 D= 1 0 τ = 6 1 A = ; u 1 e 1 e 0, A = ; u = 0.63 = 0.63 x 8 = 5.04 V 5 V fro he graph we ge : = s /3

6 8 9 du i e e e d Peranen regie: = ; i e 0 0 A xercise 3 (7 poins) Horizonal elasic pendulu Quesion Answer Mar 1-1 dp g P g consan because he rail is horizonal 0 d M K P e P g The echanical energy of he syse (puc, spring, arh) is conserved M = v + x dm + Pg = consan Ɐ 0 Ɐ d x x xx 0 0 Ɐ x x x 0 Ɐ The produc of he wo quaniies is always nil. Bu x' is no always nil, we ge: x x 0 Ɐ 1- x x cos x' x sin x" x cos x eplace x" by is expression in he differenial equaion: The relaion x x 0 is rue. A 0 = 0 s ; v0 = x' 0 x sin 0 sin 0 0 or rd A = 0 s ; x0 x cos 0 For 0 rd : x x 3c (accepable because x 0) 0 For rd : x0 x 3c x 3 c (rejeced because x is always posiive) T T 0 π s 7 1 The curve A corresponds o Pe because a 0 = 0 s, x0 0 bu P e x so Pe(0) 0 J The curve B corresponds o M because i has a consan value 1 The curve corresponds o K because a = 0 s, v = 0 /s bu K v so K(0) = 0 J 4-1 Fro he graph we ge : T = 1 s 4- T = T0/ 3/3

Determination of the focal length of a converging lens

Determination of the focal length of a converging lens الهيئة األكاديمي ة المشتركة قسم: العلوم المادة: الفيزياء الشهادة: المتوسطة نموذج رقم 4 المد ة: ساعة واحدة نموذج مسابقة )يراعي تعليق الدروس والتوصيف المعد ل للعام الدراسي 207-206 وحتى صدور المناهج المطو

More information

This exam is formed of four exercises in four pages. The use of non-programmable calculator is allowed.

This exam is formed of four exercises in four pages. The use of non-programmable calculator is allowed. وزارة التربية والتعلين العالي الوديرية العاهة للتربية دائرة االهتحانات اهتحانات الشهادة الثانىية العاهة الفرع : علىم عاهة مسابقة في مادة الفيزياء المدة ثالث ساعات االسن: الرقن: الدورة اإلستثنائية للعام

More information

قسم : العلوم. This exam includes three exercises. It is inscribed on 4 pages numbered from 1 to 4. The use of a nonprogrammable

قسم : العلوم. This exam includes three exercises. It is inscribed on 4 pages numbered from 1 to 4. The use of a nonprogrammable نموذج مسابقة الهيئة األكاديمي ة المشتركة قسم : العلوم المادة: الكيمياء الشهادة: الثانوية العامة فرعا: علوم الحياة / العلوم العامة نموذج رقم -٢- المد ة : ساعتان )يراعي تعليق الدروس والتوصيف المعد ل للعام

More information

CHAPTER 12 DIRECT CURRENT CIRCUITS

CHAPTER 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 information

Lecture 23 Damped Motion

Lecture 23 Damped Motion Differenial Equaions (MTH40) Lecure Daped Moion In he previous lecure, we discussed he free haronic oion ha assues no rearding forces acing on he oving ass. However No rearding forces acing on he oving

More information

Reading 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.

Reading 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 information

Chapter 7 Response of First-order RL and RC Circuits

Chapter 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 information

This exam is formed of 4 obligatory exercises in four pages numbered from 1 to 4 The use of non-programmable calculators is allowed

This exam is formed of 4 obligatory exercises in four pages numbered from 1 to 4 The use of non-programmable calculators is allowed وزارةالتربیةوالتعلیمالعالي المدیریةالعامةللتربیة داي رةالامتحانات امتحاناتشھادةالثانویةالعامة فرع العلومالعامة مسابقةفي ال فیزیاء المدة:ثلاثساعات دورةسنة الاسم : الرقم : 005 ا لعادیة This exam is formed

More information

( ) = Q 0. ( ) R = R dq. ( t) = I t

( ) = 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 information

Exercise 1 (7 points) Kinetic Study of the Reaction of Ethyl Ethanoate with Sodium Hydroxide

Exercise 1 (7 points) Kinetic Study of the Reaction of Ethyl Ethanoate with Sodium Hydroxide الھیي ة الا كادیمی ة المشتركة المادة: الكیمیاء الشھادة: الثانویة العامة الفرع: علوم حیاة وعلوم عامة نموذج رقم -۱- المد ة :.ساعتان قسم : العلوم نموذج مسابقة (یراعي تعلیق الدروس والتوصیف المعد ل للعام الدراسي

More information

Homework-8(1) P8.3-1, 3, 8, 10, 17, 21, 24, 28,29 P8.4-1, 2, 5

Homework-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 information

Lab 10: RC, RL, and RLC Circuits

Lab 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 information

RC, RL and RLC circuits

RC, 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 information

This exam is formed of three exercises in three pages numbered from 1 to 3 The use of non-programmable calculators is recommended.

This exam is formed of three exercises in three pages numbered from 1 to 3 The use of non-programmable calculators is recommended. 009 وزارة التربية والتعلين العالي الوديرية العاهة للتربية دائرة االهتحانات اهتحانات الشهادة الثانىية العاهة الفرع : علىم الحياة مسابقة في مادة الفيزياء المدة ساعتان االسن: الرقن: الدورة العادية للعام This

More information

Chapter 9 Sinusoidal Steady State Analysis

Chapter 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 information

EE100 Lab 3 Experiment Guide: RC Circuits

EE100 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 information

Basic Circuit Elements Professor J R Lucas November 2001

Basic 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 information

AC Circuits AC Circuit with only R AC circuit with only L AC circuit with only C AC circuit with LRC phasors Resonance Transformers

AC 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 information

LabQuest 24. Capacitors

LabQuest 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 information

Direct Current Circuits. February 19, 2014 Physics for Scientists & Engineers 2, Chapter 26 1

Direct 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 information

Chapter 10 INDUCTANCE Recommended Problems:

Chapter 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 information

Phys1112: DC and RC circuits

Phys1112: DC and RC circuits Name: Group Members: Dae: TA s Name: Phys1112: DC and RC circuis Objecives: 1. To undersand curren and volage characerisics of a DC RC discharging circui. 2. To undersand he effec of he RC ime consan.

More information

Name: Total Points: Multiple choice questions [120 points]

Name: Total Points: Multiple choice questions [120 points] Name: Toal Poins: (Las) (Firs) Muliple choice quesions [1 poins] Answer all of he following quesions. Read each quesion carefully. Fill he correc bubble on your scanron shee. Each correc answer is worh

More information

Section 3.8, Mechanical and Electrical Vibrations

Section 3.8, Mechanical and Electrical Vibrations Secion 3.8, Mechanical and Elecrical Vibraions Mechanical Unis in he U.S. Cusomary and Meric Sysems Disance Mass Time Force g (Earh) Uni U.S. Cusomary MKS Sysem CGS Sysem fee f slugs seconds sec pounds

More information

Lecture 13 RC/RL Circuits, Time Dependent Op Amp Circuits

Lecture 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 information

This exam is formed of three exercises in three pages. The Use of non-programmable calculators is allowed.

This exam is formed of three exercises in three pages. The Use of non-programmable calculators is allowed. 008 وزارة التربية والتعليم العالي المديرية العامة للتربية دائرة االمتحانات امتحانات الشهادة الثانوية العامة الفرع : علوم الحياة مسابقة في مادة الفيزياء المدة ساعتان االسم: الرقم: الدورة اإلستثنائية للعام

More information

copper ring magnetic field

copper ring magnetic field IB PHYSICS: Magneic Fields, lecromagneic Inducion, Alernaing Curren 1. This quesion is abou elecromagneic inducion. In 1831 Michael Faraday demonsraed hree ways of inducing an elecric curren in a ring

More information

Thus the force is proportional but opposite to the displacement away from equilibrium.

Thus the force is proportional but opposite to the displacement away from equilibrium. Chaper 3 : Siple Haronic Moion Hooe s law saes ha he force (F) eered by an ideal spring is proporional o is elongaion l F= l where is he spring consan. Consider a ass hanging on a he spring. In equilibriu

More information

الھیي ة الا كادیمی ة المشتركة قسم : العلوم

الھیي ة الا كادیمی ة المشتركة قسم : العلوم الھیي ة الا كادیمی ة المشتركة قسم : العلوم المادة: الكیمیاء الشھادة: الثانویة العامة الفرع: علوم الحیاة نموذج رقم -٢ - المد ة : ساعتان نموذج مسابقة (یراعي تعلیق الدروس والتوصیف المعد ل للعام الدراسي ٢٠١٦-٢٠١٧

More information

MEI STRUCTURED MATHEMATICS 4758

MEI STRUCTURED MATHEMATICS 4758 OXFORD CAMBRIDGE AND RSA EXAMINATIONS Advanced Subsidiary General Cerificae of Educaion Advanced General Cerificae of Educaion MEI STRUCTURED MATHEMATICS 4758 Differenial Equaions Thursday 5 JUNE 006 Afernoon

More information

EEEB113 CIRCUIT ANALYSIS I

EEEB113 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 information

المادة: الریاضیات الشھادة: المتوسطة نموذج رقم -۱- قسم : الریاضیات

المادة: الریاضیات الشھادة: المتوسطة نموذج رقم -۱- قسم : الریاضیات الھیي ة الا كادیمی ة المشتركة قسم : الریاضیات المادة: الریاضیات الشھادة: المتوسطة نموذج رقم -۱- المد ة : ساعتان I - ( points) نموذج مسابقة (یراعي تعلیق الدروس والتوصیف المعد ل للعام الدراسي ۲۰۱۷-۲۰۱٦ وحتى

More information

Pulse Generators. Any of the following calculations may be asked in the midterms/exam.

Pulse 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 information

Some Basic Information about M-S-D Systems

Some 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 information

(b) (a) (d) (c) (e) Figure 10-N1. (f) Solution:

(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 information

Inductor Energy Storage

Inductor Energy Storage School of Compuer Science and Elecrical Engineering 5/5/ nducor Energy Sorage Boh capaciors and inducors are energy sorage devices They do no dissipae energy like a resisor, bu sore and reurn i o he circui

More information

University of Cyprus Biomedical Imaging and Applied Optics. Appendix. DC Circuits Capacitors and Inductors AC Circuits Operational Amplifiers

University 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 information

IB Physics Kinematics Worksheet

IB Physics Kinematics Worksheet IB Physics Kinemaics Workshee Wrie full soluions and noes for muliple choice answers. Do no use a calculaor for muliple choice answers. 1. Which of he following is a correc definiion of average acceleraion?

More information

9. Alternating currents

9. 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 information

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits

EECE251. 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 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

- 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 information

Electrical Circuits. 1. Circuit Laws. Tools Used in Lab 13 Series Circuits Damped Vibrations: Energy Van der Pol Circuit

Electrical 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 information

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8.

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8. Kinemaics Vocabulary Kinemaics and One Dimensional Moion 8.1 WD1 Kinema means movemen Mahemaical descripion of moion Posiion Time Inerval Displacemen Velociy; absolue value: speed Acceleraion Averages

More information

Chapter 8 The Complete Response of RL and RC Circuits

Chapter 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 information

Physics for Scientists & Engineers 2

Physics for Scientists & Engineers 2 Direc Curren Physics for Scieniss & Engineers 2 Spring Semeser 2005 Lecure 16 This week we will sudy charges in moion Elecric charge moving from one region o anoher is called elecric curren Curren is all

More information

Exam #2 PHYSICS 211 Monday July 6 th, 2009 Please write down your name also on the back page of this exam

Exam #2 PHYSICS 211 Monday July 6 th, 2009 Please write down your name also on the back page of this exam Exa #2 PHYSICS 211 Monday July 6 h, 29 NME Please wrie down your nae also on he back pae of his exa 1. The fiure ives how he force varies as a funcion of he posiion. Such force is acin on a paricle, which

More information

INDEX. Transient analysis 1 Initial Conditions 1

INDEX. 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 information

ECE 2100 Circuit Analysis

ECE 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

MEMS 0031 Electric Circuits

MEMS 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 information

ES 250 Practice Final Exam

ES 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 information

3. Alternating Current

3. 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 information

5.2. The Natural Logarithm. Solution

5.2. The Natural Logarithm. Solution 5.2 The Naural Logarihm The number e is an irraional number, similar in naure o π. Is non-erminaing, non-repeaing value is e 2.718 281 828 59. Like π, e also occurs frequenly in naural phenomena. In fac,

More information

2. The following diagram shows a circular loop of wire in a uniform magnetic field that points out of the page.

2. The following diagram shows a circular loop of wire in a uniform magnetic field that points out of the page. 1. Two elecromagneic waves ravel hrough emp space. Wave A as a wavelengh of 700 nm (red ligh), while Wave B has a wavelengh of 400 nm (blue ligh). Which saemen is rue? A) Wave A ravels faser because i

More information

R.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder#

R.#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 information

BEng (Hons) Telecommunications. Examinations for / Semester 2

BEng (Hons) Telecommunications. Examinations for / Semester 2 BEng (Hons) Telecommunicaions Cohor: BTEL/14/FT Examinaions for 2015-2016 / Semeser 2 MODULE: ELECTROMAGNETIC THEORY MODULE CODE: ASE2103 Duraion: 2 ½ Hours Insrucions o Candidaes: 1. Answer ALL 4 (FOUR)

More information

1. VELOCITY AND ACCELERATION

1. VELOCITY AND ACCELERATION 1. VELOCITY AND ACCELERATION 1.1 Kinemaics Equaions s = u + 1 a and s = v 1 a s = 1 (u + v) v = u + as 1. Displacemen-Time Graph Gradien = speed 1.3 Velociy-Time Graph Gradien = acceleraion Area under

More information

Chapter 1 Fundamental Concepts

Chapter 1 Fundamental Concepts Chaper 1 Fundamenal Conceps 1 Signals A signal is a paern of variaion of a physical quaniy, ofen as a funcion of ime (bu also space, disance, posiion, ec). These quaniies are usually he independen variables

More information

Chapter 16: Summary. Instructor: Jean-François MILLITHALER.

Chapter 16: Summary. Instructor: Jean-François MILLITHALER. Chaper 16: Summary Insrucor: Jean-François MILLITHALER hp://faculy.uml.edu/jeanfrancois_millihaler/funelec/spring2017 Slide 1 Curren & Charge Elecric curren is he ime rae of change of charge, measured

More information

6.01: Introduction to EECS I Lecture 8 March 29, 2011

6.01: 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 information

Oscillations. Periodic Motion. Sinusoidal Motion. PHY oscillations - J. Hedberg

Oscillations. Periodic Motion. Sinusoidal Motion. PHY oscillations - J. Hedberg Oscillaions PHY 207 - oscillaions - J. Hedberg - 2017 1. Periodic Moion 2. Sinusoidal Moion 3. How do we ge his kind of moion? 4. Posiion - Velociy - cceleraion 5. spring wih vecors 6. he reference circle

More information

First Order RC and RL Transient Circuits

First 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 information

Q.1 Define work and its unit?

Q.1 Define work and its unit? CHP # 6 ORK AND ENERGY Q.1 Define work and is uni? A. ORK I can be define as when we applied a force on a body and he body covers a disance in he direcion of force, hen we say ha work is done. I is a scalar

More information

ECE 2100 Circuit Analysis

ECE 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 information

8. Basic RL and RC Circuits

8. 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 information

2.4 Cuk converter example

2.4 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 information

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x WEEK-3 Reciaion PHYS 131 Ch. 3: FOC 1, 3, 4, 6, 14. Problems 9, 37, 41 & 71 and Ch. 4: FOC 1, 3, 5, 8. Problems 3, 5 & 16. Feb 8, 018 Ch. 3: FOC 1, 3, 4, 6, 14. 1. (a) The horizonal componen of he projecile

More information

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes Some common engineering funcions 2.7 Inroducion This secion provides a caalogue of some common funcions ofen used in Science and Engineering. These include polynomials, raional funcions, he modulus funcion

More information

Introduction to Mechanical Vibrations and Structural Dynamics

Introduction to Mechanical Vibrations and Structural Dynamics Inroducion o Mechanical Viraions and Srucural Dynaics The one seeser schedule :. Viraion - classificaion. ree undaped single DO iraion, equaion of oion, soluion, inegraional consans, iniial condiions..

More information

8.022 (E&M) Lecture 9

8.022 (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 information

امتحانات الشهادة الثانوية العامة الفرع : العلوم العامة مسابقة في مادة الفيزياء الرقم:

امتحانات الشهادة الثانوية العامة الفرع : العلوم العامة مسابقة في مادة الفيزياء الرقم: وزارة التربية والتعليم العالي المديرية العامة للتربية دائرة االمتحانات امتحانات الشهادة الثانوية العامة الفرع : العلوم العامة دورة العام 5 االستثنائية الخميس اب 5 االسم: مسابقة في مادة الفيزياء الرقم:

More information

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17

Designing 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 information

Topic Astable Circuits. Recall that an astable circuit has two unstable states;

Topic 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 information

CLASS XI SET A PHYSICS. 1. If and Let. The correct order of % error in. (a) (b) x = y > z (c) x < z < y (d) x > z < y

CLASS XI SET A PHYSICS. 1. If and Let. The correct order of % error in. (a) (b) x = y > z (c) x < z < y (d) x > z < y PHYSICS 1. If and Le. The correc order of % error in (a) (b) x = y > z x < z < y x > z < y. A hollow verical cylinder of radius r and heigh h has a smooh inernal surface. A small paricle is placed in conac

More information

4. Electric field lines with respect to equipotential surfaces are

4. Electric field lines with respect to equipotential surfaces are Pre-es Quasi-saic elecromagneism. The field produced by primary charge Q and by an uncharged conducing plane disanced from Q by disance d is equal o he field produced wihou conducing plane by wo following

More information

Homework: See website. Table of Contents

Homework: See website. Table of Contents Dr. Friz Wilhelm page of 4 C:\physics\3 lecure\ch3 Inducance C circuis.docx; P /5/8 S: 5/4/9 9:39: AM Homework: See websie. Table of Conens: 3. Self-inducance in a circui, 3. -Circuis, 4 3.a Charging he

More information

Voltage/current relationship Stored Energy. RL / RC circuits Steady State / Transient response Natural / Step response

Voltage/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 information

Chapter 4 AC Network Analysis

Chapter 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 information

Parametrics and Vectors (BC Only)

Parametrics and Vectors (BC Only) Paramerics and Vecors (BC Only) The following relaionships should be learned and memorized. The paricle s posiion vecor is r() x(), y(). The velociy vecor is v(),. The speed is he magniude of he velociy

More information

AP Calculus BC Chapter 10 Part 1 AP Exam Problems

AP Calculus BC Chapter 10 Part 1 AP Exam Problems AP Calculus BC Chaper Par AP Eam Problems All problems are NO CALCULATOR unless oherwise indicaed Parameric Curves and Derivaives In he y plane, he graph of he parameric equaions = 5 + and y= for, is a

More information

Traveling Waves. Chapter Introduction

Traveling Waves. Chapter Introduction Chaper 4 Traveling Waves 4.1 Inroducion To dae, we have considered oscillaions, i.e., periodic, ofen harmonic, variaions of a physical characerisic of a sysem. The sysem a one ime is indisinguishable from

More information

SHM SHM. T is the period or time it takes to complete 1 cycle. T = = 2π. f is the frequency or the number of cycles completed per unit time.

SHM SHM. T is the period or time it takes to complete 1 cycle. T = = 2π. f is the frequency or the number of cycles completed per unit time. SHM A ω = k d x x = Acos ( ω +) dx v = = ω Asin( ω + ) vax = ± ωa dv a = = ω Acos + k + x Apliude ( ω ) = 0 a ax = ± ω A SHM x = Acos is he period or ie i akes o coplee cycle. ω = π ( ω +) π = = π ω k

More information

This exam is formed of three exercises in three pages numbered from 1 to 3. The use of a non-programmable calculator is recommended.

This exam is formed of three exercises in three pages numbered from 1 to 3. The use of a non-programmable calculator is recommended. 0 وزارة التربية والتعليم العالي المديرية العامة للتربية دائرة االمتحانات امتحانات الشهادة الثانوية العامة الفرع : علوم الحياة الدورة العادية للعام مسابقة في مادة الفيزياء المدة ساعتان االسم: الرقم: This

More information

The equation to any straight line can be expressed in the form:

The equation to any straight line can be expressed in the form: Sring Graphs Par 1 Answers 1 TI-Nspire Invesigaion Suden min Aims Deermine a series of equaions of sraigh lines o form a paern similar o ha formed by he cables on he Jerusalem Chords Bridge. Deermine he

More information

non-linear oscillators

non-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 information

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions MA 14 Calculus IV (Spring 016) Secion Homework Assignmen 1 Soluions 1 Boyce and DiPrima, p 40, Problem 10 (c) Soluion: In sandard form he given firs-order linear ODE is: An inegraing facor is given by

More information

Electrical and current self-induction

Electrical 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 information

Elementary Differential Equations and Boundary Value Problems

Elementary Differential Equations and Boundary Value Problems Elemenar Differenial Equaions and Boundar Value Problems Boce. & DiPrima 9 h Ediion Chaper 1: Inroducion 1006003 คณ ตศาสตร ว ศวกรรม 3 สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา 1/2555 ผศ.ดร.อร ญญา ผศ.ดร.สมศ

More information

4.5 Constant Acceleration

4.5 Constant Acceleration 4.5 Consan Acceleraion v() v() = v 0 + a a() a a() = a v 0 Area = a (a) (b) Figure 4.8 Consan acceleraion: (a) velociy, (b) acceleraion When he x -componen of he velociy is a linear funcion (Figure 4.8(a)),

More information

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still. Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in

More information

!!"#"$%&#'()!"#&'(*%)+,&',-)./0)1-*23)

!!#$%&#'()!#&'(*%)+,&',-)./0)1-*23) "#"$%&#'()"#&'(*%)+,&',-)./)1-*) #$%&'()*+,&',-.%,/)*+,-&1*#$)()5*6$+$%*,7&*-'-&1*(,-&*6&,7.$%$+*&%'(*8$&',-,%'-&1*(,-&*6&,79*(&,%: ;..,*&1$&$.$%&'()*1$$.,'&',-9*(&,%)?%*,('&5

More information

y = (y 1)*(y 3) t

y = (y 1)*(y 3) t MATH 66 SPR REVIEW DEFINITION OF SOLUTION A funcion = () is a soluion of he differenial equaion d=d = f(; ) on he inerval ff < < fi if (d=d)() =f(; ()) for each so ha ff

More information

Viscous Damping Summary Sheet No Damping Case: Damped behaviour depends on the relative size of ω o and b/2m 3 Cases: 1.

Viscous Damping Summary Sheet No Damping Case: Damped behaviour depends on the relative size of ω o and b/2m 3 Cases: 1. Viscous Daping: && + & + ω Viscous Daping Suary Shee No Daping Case: & + ω solve A ( ω + α ) Daped ehaviour depends on he relaive size of ω o and / 3 Cases:. Criical Daping Wee 5 Lecure solve sae BC s

More information

Solution: b All the terms must have the dimension of acceleration. We see that, indeed, each term has the units of acceleration

Solution: b All the terms must have the dimension of acceleration. We see that, indeed, each term has the units of acceleration PHYS 54 Tes Pracice Soluions Spring 8 Q: [4] Knowing ha in he ne epression a is acceleraion, v is speed, is posiion and is ime, from a dimensional v poin of view, he equaion a is a) incorrec b) correc

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

( ) ( ) 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 information

Electromagnetic Induction: The creation of an electric current by a changing magnetic field.

Electromagnetic Induction: The creation of an electric current by a changing magnetic field. Inducion 1. Inducion 1. Observaions 2. Flux 1. Inducion Elecromagneic Inducion: The creaion of an elecric curren by a changing magneic field. M. Faraday was he firs o really invesigae his phenomenon o

More information

Experiment 123 Determination of the sound wave velocity with the method of Lissajous figures

Experiment 123 Determination of the sound wave velocity with the method of Lissajous figures perimen 3 Deerminaion of he sound wave veloci wih he mehod of Lissajous figures The aim of he eercise To sud acousic wave propagaion in he air To deermine of he sound wave veloci in he air Mehodolog of

More information

Introduction to Numerical Analysis. In this lesson you will be taken through a pair of techniques that will be used to solve the equations of.

Introduction to Numerical Analysis. In this lesson you will be taken through a pair of techniques that will be used to solve the equations of. Inroducion o Nuerical Analysis oion In his lesson you will be aen hrough a pair of echniques ha will be used o solve he equaions of and v dx d a F d for siuaions in which F is well nown, and he iniial

More information

LINEAR MODELS: INITIAL-VALUE PROBLEMS

LINEAR MODELS: INITIAL-VALUE PROBLEMS 5 LINEAR MODELS: INITIAL-VALUE PROBLEMS 9 5 LINEAR MODELS: INITIAL-VALUE PROBLEMS REVIEW MATERIAL Secions 4, 4, and 44 Problems 9 6 in Eercises 4 Problems 7 6 in Eercises 44 INTRODUCTION In his secion

More information

15. Vector Valued Functions

15. Vector Valued Functions 1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,

More information

5.1 - Logarithms and Their Properties

5.1 - Logarithms and Their Properties Chaper 5 Logarihmic Funcions 5.1 - Logarihms and Their Properies Suppose ha a populaion grows according o he formula P 10, where P is he colony size a ime, in hours. When will he populaion be 2500? We

More information