LTI Systems with Feedback, IIR Filter Design
|
|
- Janel Watson
- 5 years ago
- Views:
Transcription
1 Lectue 27 Outine: LTI Systems with Feedbac, IIR Fite Design Announcements: Last HW wi be posted, due Thu June 7, no ate HWs Pactice fina wi be posted today Fina exam announcements on next side Feedbac in discete LTI Systems IIR fite design
2 Fina Exam Detais Time/Location: Monday June, 3:36:3 in this oom. Food aftewads. Open boo and notes you can bing any witten mateia you wish to the exam. Cacuatos not aowed. PDF bowsing devices aowed. Coves a cass mateia; emphasis on postmt mateia (ectues 4 on) See ectue ppt sides fo mateia in the eade that you ae esponsibe fo Pactice fina wi be posted today, 25 EC pts fo taing it (not gaded). Can be tuned in any time up unti exam, Sons given when you tun in you answes if done by pm June, so we have time to emai them to you Fina exam fom 26 did not incude IIR fite design My fina eview on W 6/6 in cass. Geogia Th 6/7 46pm (eview + OHs) OHs befoe fina: Me: today afte cass, 6/6, Wed, 2:3 (hee); 6/8, Fi, by appt. (equest by Thu 5pm) Regua Tuesday section and TA OHs this wee pus Th 6/7 ~56pm (Geogia) Sun, 6/, 22pm (John), Mon 6/, 22pm (Maavia)
3 Review of Last Lectue DT systems impemented with deay/ampifie eements A system with output feedbac geneay has infinite impuse esponse Can compute impuse esponse by hand ; had to do LTI Systems descibed by diffeentia equations Exampe: 2 nd ode feedbac system [ ] [ ] M N n x b n y a ( ) ( ) X b Y a M N ø ö ç ç è æ ø ö ç ç è æ ( ) ( ) ( ) A B a b H N M ( ) ( )( ) e e H j j > +, cos q q q ( ) W W W cos 2 j j j e e e H q ( ) ( ) 2 H [ ] ( ) [ ] [ ] u n n h n n + q:
4 Review Continued Diect Fom IIR Fite Impementation This ectue wi discuss IIR fite design Appoximates continuous time fites with owe compexity than FIR designs
5 Feedbac in discete LTI Systems + e[n] g[n] x [n] S y[n] G() ± G( ) x ( t) y( t ( ) ( ) )! G H h[n] H () Motivation fo Feedbac Can mae an unstabe system stabe; mae a system ess sensitive to distubances; mae it cose to idea Can have negative effect: mae a stabe system unstabe Tansfe Function T() of Feedbac System: Y()G()E(); E()X()±Y()H() Exampe: Popuation Gowth: y[n]2y[n]+x[n][n] Poe at 22b, Stabe fo.5<b<.5 Equivaent System ( ) ( ) Y G T ( ) X! G T ( ) ( ) H ( ) 2( b ) ( )
6 IIR Fite Design x(t) H c (s) y c (t) Discussed FIR fite design of h w [n] fo desied IIR noncausa fite H c (jw) befoe MT ADC Sampe time T x[n] y H() DAC y d [n] d(t) Convet H c (jw) to DT IIR fite as H c (jw)þh d (e jw ) fo WwT Now conside design of IIR H() to appoximate H c (s) Have moe toos at ou disposa fo this design (tansfoms) Low compexity impementation of IIR fites vs FIR (via feedbac) Two methods: tempoa and fequency esponse matching Tempoa (not on HW/exam): Design H() so that fo a given x(t) (impuse, step), y d [n]y c (nt); intoduces aiasing if T>p/W
7 Fequency Response (FR) Matching FR Matching: Biatea Tansfom (BLT) Noninea invetibe mapping between spane and pane Can use moe genea mapping fo any ea C, <C Discete time fite design of H() unde BLT: Ensues that if H c (s) stabe, H() aso stabe with no aiasing Thee is waping due to noninea mapping, esp. at high fequencies Mapping between s and pane: s yieds jw axis in spane Þ unit cice in pane eft/ight haf of spane Þ inside/outside unit cice Lefthaf poes of spane map inside cice Stabiity peseved in the mapping to H()
8 s/ pane mapping Phase: fo w <<p/t <w< p<w<p So entie jw axis of spane mapped to one evoution of the pane aong unit cice No aiasing of the fequency esponse, but waps
9 Exampe: 2 nd ode Buttewoth BLT: IR
10
11 Main Points Feedbac stabiies unstabe systems; obtains desied tansfe function; can mae stabe system unstabe Easy to anaye systems with feedbac using tansfoms IIR fite design using biinea tansfom entais a noninea mapping fom s to pane Fo desied CT fite tabe, ensue DT fite is aso stabe Avoids aiasing Cosey matches CT fite fo ow fequencies Waps high fequencies
Zero-Order Hold Sampling, Upsampling and Downsampling
Lecture 5 Outine: Zero-Order Hod Samping, Upsamping and Downsamping Announcements: Updated OHs: Me: MWF after cass & by appt. (made by emai or before/after cass, ate MWF ok) Wed 4PM-5PM (Maavika), 6PM-7PM
More informationAnalog-to-Digital and Back
Lecture 2 Outine: Anaog-to-Digita and Back Bridging the anaog and digita divide Announcements: Po for discussion section and OHs: pease respond First HW posted tonight Lectures going forward: PPides and
More informationEEO 401 Digital Signal Processing Prof. Mark Fowler
EEO 41 Digital Signal Pocessing Pof. Mak Fowle Note Set #31 Linea Phase FIR Design Optimum Equiipple (Paks-McClellan) Reading: Sect. 1.2.4 1.2.6 of Poakis & Manolakis 1/2 Motivation The window method and
More informationMechanics Physics 151
Mechanics Physics 5 Lectue 5 Centa Foce Pobem (Chapte 3) What We Did Last Time Intoduced Hamiton s Pincipe Action intega is stationay fo the actua path Deived Lagange s Equations Used cacuus of vaiation
More informationMechanics Physics 151
Mechanics Physics 5 Lectue 5 Centa Foce Pobem (Chapte 3) What We Did Last Time Intoduced Hamiton s Pincipe Action intega is stationay fo the actua path Deived Lagange s Equations Used cacuus of vaiation
More informationQuantum Fourier Transform
Chapte 5 Quantum Fouie Tansfom Many poblems in physics and mathematics ae solved by tansfoming a poblem into some othe poblem with a known solution. Some notable examples ae Laplace tansfom, Legende tansfom,
More informationAbsolute Specifications: A typical absolute specification of a lowpass filter is shown in figure 1 where:
FIR FILTER DESIGN The design of an digital filte is caied out in thee steps: ) Specification: Befoe we can design a filte we must have some specifications. These ae detemined by the application. ) Appoximations
More informationDIGITAL FILTER DESIGN OF IIR FILTERS USING REAL VALUED GENETIC ALGORITHM
DIGITAL FILTER DESIGN OF IIR FILTERS USING REAL VALUED GENETIC ALGORITHM MIKAEL NILSSON, MATTIAS DAHL AND INGVAR CLAESSON Bekinge Institute of Technoogy Department of Teecommunications and Signa Processing
More informationMechanics Physics 151
Mechanics Physics 151 Lectue 6 Kepe Pobem (Chapte 3) What We Did Last Time Discussed enegy consevation Defined enegy function h Conseved if Conditions fo h = E Stated discussing Centa Foce Pobems Reduced
More informationLecture 13. Rotational motion Moment of inertia
Lectue 13 Rotational motion Moment of inetia EXAM 2 Tuesday Mach 6, 2018 8:15 PM 9:45 PM Today s Topics: Rotational Motion and Angula Displacement Angula Velocity and Acceleation Rotational Kinematics
More informationDYNAMICS OF UNIFORM CIRCULAR MOTION
Chapte 5 Dynamics of Unifom Cicula Motion Chapte 5 DYNAMICS OF UNIFOM CICULA MOTION PEVIEW An object which is moing in a cicula path with a constant speed is said to be in unifom cicula motion. Fo an object
More informationLaplace Examples, Inverse, Rational Form
Lecture 20 Outine: Lapace Eampe, Invere, Rationa Form Announcement: HW 5 poted, due Friday ore Lapace Tranform Eampe Invere Lapace Tranform Rationa Lapace Tranform ROC for Right/Left/Toided Signa agnitude/phae
More informationLectures on Multivariable Feedback Control
Lectues on Mutivaiabe Feedback onto i Kaimpou epatment of Eectica Engineeing, Facuty of Engineeing, Fedowsi Univesity of Mashhad (Septembe 9 hapte 4: Stabiity of Mutivaiabe Feedback onto Systems 4- We-Posedness
More informationQuantum Lyapunov Control Based on the Average Value of an Imaginary Mechanical Quantity
Quantum Lyapunov Conto Based on the Aveage Vaue o an Imaginay Mechanica Quantity Shuang Cong, Fangang Meng, and Sen Kuang Abstact The convegence o cosed quantum systems in the degeneate cases to the desied
More informationPhysics 221 Lecture 41 Nonlinear Absorption and Refraction
Physics 221 Lectue 41 Nonlinea Absoption and Refaction Refeences Meye-Aendt, pp. 97-98. Boyd, Nonlinea Optics, 1.4 Yaiv, Optical Waves in Cystals, p. 22 (Table of cystal symmeties) 1. Intoductoy Remaks.
More informationProbability Estimation with Maximum Entropy Principle
Pape 0,CCG Annua Repot, 00 ( c 00) Pobabiity Estimation with Maximum Entopy Pincipe Yupeng Li and Cayton V. Deutsch The pincipe of Maximum Entopy is a powefu and vesatie too fo infeing a pobabiity distibution
More informationPhysics 1502: Lecture 4 Today s Agenda
1 Physics 1502: Today s genda nnouncements: Lectues posted on: www.phys.uconn.edu/~cote/ HW assignments, solutions etc. Homewok #1: On Mastephysics today: due next Fiday Go to masteingphysics.com and egiste
More informationMerging to ordered sequences. Efficient (Parallel) Sorting. Merging (cont.)
Efficient (Paae) Soting One of the most fequent opeations pefomed by computes is oganising (soting) data The access to soted data is moe convenient/faste Thee is a constant need fo good soting agoithms
More informationSeidel s Trapezoidal Partitioning Algorithm
CS68: Geometic Agoithms Handout #6 Design and Anaysis Oigina Handout #6 Stanfod Univesity Tuesday, 5 Febuay 99 Oigina Lectue #7: 30 Januay 99 Topics: Seide s Tapezoida Patitioning Agoithm Scibe: Michae
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.
More informationIntroduction to Simulation - Lecture 14. Multistep Methods II. Jacob White. Thanks to Deepak Ramaswamy, Michal Rewienski, and Karen Veroy
Introduction to Simuation - Lecture 14 Mutistep Methods II Jacob White Thans to Deepa Ramaswamy, Micha Rewiensi, and Karen Veroy Outine Sma Timestep issues for Mutistep Methods Reminder about LTE minimization
More information= ρ. Since this equation is applied to an arbitrary point in space, we can use it to determine the charge density once we know the field.
Gauss s Law In diffeentia fom D = ρ. ince this equation is appied to an abita point in space, we can use it to detemine the chage densit once we know the fied. (We can use this equation to ve fo the fied
More informationObjectives. We will also get to know about the wavefunction and its use in developing the concept of the structure of atoms.
Modue "Atomic physics and atomic stuctue" Lectue 7 Quantum Mechanica teatment of One-eecton atoms Page 1 Objectives In this ectue, we wi appy the Schodinge Equation to the simpe system Hydogen and compae
More informationA Tutorial on Multiple Integrals (for Natural Sciences / Computer Sciences Tripos Part IA Maths)
A Tutoial on Multiple Integals (fo Natual Sciences / Compute Sciences Tipos Pat IA Maths) Coections to D Ian Rud (http://people.ds.cam.ac.uk/ia/contact.html) please. This tutoial gives some bief eamples
More informationExam 1. Exam 1 is on Tuesday, February 14, from 5:00-6:00 PM.
Exam 1 Exam 1 is on Tuesday, Febuay 14, fom 5:00-6:00 PM. Testing Cente povides accommodations fo students with special needs I must set up appointments one week befoe exam Deadline fo submitting accommodation
More informationPHYS 705: Classical Mechanics. Central Force Problems II
PHYS 75: Cassica Mechanics Centa Foce Pobems II Obits in Centa Foce Pobem Sppose we e inteested moe in the shape of the obit, (not necessay the time evotion) Then, a sotion fo = () o = () wod be moe sef!
More informationCourse Outline. ECE 178: Image Processing REVIEW. Relationship between pixels. Connected components. Distance Measures. Linear systems-review
ECE 78: Image Pocessing REVIEW Lectue #2 Mach 3, 23 Couse Outline! Intoduction! Digital Images! Image Tansfoms! Sampling and Quantization! Image Enhancement! Image/Video Coding JPEG MPEG Mach 3, 23 Mach
More informationCompactly Supported Radial Basis Functions
Chapte 4 Compactly Suppoted Radial Basis Functions As we saw ealie, compactly suppoted functions Φ that ae tuly stictly conditionally positive definite of ode m > do not exist The compact suppot automatically
More informationMutual Inductance. If current i 1 is time varying, then the Φ B2 flux is varying and this induces an emf ε 2 in coil 2, the emf is
Mutua Inductance If we have a constant cuent i in coi, a constant magnetic fied is ceated and this poduces a constant magnetic fux in coi. Since the Φ B is constant, thee O induced cuent in coi. If cuent
More informationLecture 22. PE = GMm r TE = GMm 2a. T 2 = 4π 2 GM. Main points of today s lecture: Gravitational potential energy: Total energy of orbit:
Lectue Main points of today s lectue: Gavitational potential enegy: Total enegy of obit: PE = GMm TE = GMm a Keple s laws and the elation between the obital peiod and obital adius. T = 4π GM a3 Midtem
More informationSection 8.2 Polar Coordinates
Section 8. Pola Coodinates 467 Section 8. Pola Coodinates The coodinate system we ae most familia with is called the Catesian coodinate system, a ectangula plane divided into fou quadants by the hoizontal
More informationTUTORIAL 9. Static magnetic field
TUTOIAL 9 Static magnetic field Vecto magnetic potential Null Identity % & %$ A # Fist postulation # " B such that: Vecto magnetic potential Vecto Poisson s equation The solution is: " Substitute it into
More informationQualifying Examination Electricity and Magnetism Solutions January 12, 2006
1 Qualifying Examination Electicity and Magnetism Solutions Januay 12, 2006 PROBLEM EA. a. Fist, we conside a unit length of cylinde to find the elationship between the total chage pe unit length λ and
More informationCourse Updates. Reminders: 1) Assignment #10 due next Wednesday. 2) Midterm #2 take-home Friday. 3) Quiz # 5 next week. 4) Inductance, Inductors, RLC
Couse Updates http://www.phys.hawaii.edu/~vane/phys7-sp10/physics7.htm Remindes: 1) Assignment #10 due next Wednesday ) Midtem # take-home Fiday 3) Quiz # 5 next week 4) Inductance, Inductos, RLC Mutua
More informationPhysics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009
Physics 111 Lectue 5 (Walke: 3.3-6) Vectos & Vecto Math Motion Vectos Sept. 11, 2009 Quiz Monday - Chap. 2 1 Resolving a vecto into x-component & y- component: Pola Coodinates Catesian Coodinates x y =
More informationF O R SOCI AL WORK RESE ARCH
7 TH EUROPE AN CONFERENCE F O R SOCI AL WORK RESE ARCH C h a l l e n g e s i n s o c i a l w o r k r e s e a r c h c o n f l i c t s, b a r r i e r s a n d p o s s i b i l i t i e s i n r e l a t i o n
More informationIn the previous section we considered problems where the
5.4 Hydodynamically Fully Developed and Themally Developing Lamina Flow In the pevious section we consideed poblems whee the velocity and tempeatue pofile wee fully developed, so that the heat tansfe coefficient
More informationPhysics 161 Fall 2011 Extra Credit 2 Investigating Black Holes - Solutions The Following is Worth 50 Points!!!
Physics 161 Fall 011 Exta Cedit Investigating Black Holes - olutions The Following is Woth 50 Points!!! This exta cedit assignment will investigate vaious popeties of black holes that we didn t have time
More information! Frequency Response of LTI Systems. " Magnitude Response. " Phase Response. " Example: Zero on Real Axis. ! We can define a magnitude response
Lectue Outline ESE 53: Digital Signal Pocessing Lec 3: Febuay 23st, 207 Fequency Response of LTI Systems! Fequency Response of LTI Systems " agnitude Response " Simple Filtes " Phase Response " Goup Delay
More informationr cos, and y r sin with the origin of coordinate system located at
Lectue 3-3 Kinematics of Rotation Duing ou peious lectues we hae consideed diffeent examples of motion in one and seeal dimensions. But in each case the moing object was consideed as a paticle-like object,
More informationBasic Gray Level Transformations (2) Negative
Gonzalez & Woods, 22 Basic Gay Level Tansfomations (2) Negative 23 Basic Gay Level Tansfomations (3) Log Tansfomation (Example fo Fouie Tansfom) Fouie spectum values ~1 6 bightest pixels dominant display
More informationLecture 1. time, say t=0, to find the wavefunction at any subsequent time t. This can be carried out by
Lectue The Schödinge equation In quantum mechanics, the fundamenta quantity that descibes both the patice-ike and waveike chaacteistics of patices is wavefunction, Ψ(. The pobabiity of finding a patice
More informationPHYS 1444 Section 501 Lecture #7
PHYS 1444 Section 51 Lectue #7 Wednesday, Feb. 8, 26 Equi-potential Lines and Sufaces Electic Potential Due to Electic Dipole E detemined fom V Electostatic Potential Enegy of a System of Chages Capacitos
More informationStanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012
Stanfod Univesity CS59Q: Quantum Computing Handout 8 Luca Tevisan Octobe 8, 0 Lectue 8 In which we use the quantum Fouie tansfom to solve the peiod-finding poblem. The Peiod Finding Poblem Let f : {0,...,
More information4/18/2005. Statistical Learning Theory
Statistical Leaning Theoy Statistical Leaning Theoy A model of supevised leaning consists of: a Envionment - Supplying a vecto x with a fixed but unknown pdf F x (x b Teache. It povides a desied esponse
More informationPhysics 201, Lecture 6
Physics 201, Lectue 6 Today s Topics q Unifom Cicula Motion (Section 4.4, 4.5) n Cicula Motion n Centipetal Acceleation n Tangential and Centipetal Acceleation q Relatie Motion and Refeence Fame (Sec.
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electical and Compute Engineeing, Conell Univesity ECE 33: Electomagnetic Fields and Waves Fall 7 Homewok 6 Due on Oct. 5, 7 by 5: PM Reading Assignments: i) Review the lectue notes. ii) Review
More informationChapter 2: Basic Physics and Math Supplements
Chapte 2: Basic Physics and Math Supplements Decembe 1, 215 1 Supplement 2.1: Centipetal Acceleation This supplement expands on a topic addessed on page 19 of the textbook. Ou task hee is to calculate
More informationPractice Integration Math 120 Calculus I Fall 2015
Pactice Integation Math 0 Calculus I Fall 05 Hee s a list of pactice eecises. Thee s a hint fo each one as well as an answe with intemediate steps... ( + d. Hint. Answe. ( 8 t + t + This fist set of indefinite
More informationLecture 04: HFK Propagation Physical Optics II (Optical Sciences 330) (Updated: Friday, April 29, 2005, 8:05 PM) W.J. Dallas
C:\Dallas\0_Couses\0_OpSci_330\0 Lectue Notes\04 HfkPopagation.doc: Page of 9 Lectue 04: HFK Popagation Physical Optics II (Optical Sciences 330) (Updated: Fiday, Apil 9, 005, 8:05 PM) W.J. Dallas The
More informationCurrent Balance Warm Up
PHYSICS EXPERIMENTS 133 Cuent Balance-1 Cuent Balance Wam Up 1. Foce between cuent-caying wies Wie 1 has a length L (whee L is "long") and caies a cuent I 0. What is the magnitude of the magnetic field
More informationPHYS 705: Classical Mechanics. Central Force Problems I
1 PHYS 705: Cassica Mechanics Centa Foce Pobems I Two-Body Centa Foce Pobem Histoica Backgound: Kepe s Laws on ceestia bodies (~1605) - Based his 3 aws on obsevationa data fom Tycho Bahe - Fomuate his
More informationJackson 4.7 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell
Jackson 4.7 Homewok obem Soution D. Chistophe S. Baid Univesity of Massachusetts Lowe ROBLEM: A ocaized distibution of chage has a chage density ρ()= 6 e sin θ (a) Make a mutipoe expansion of the potentia
More informationPractice Integration Math 120 Calculus I D Joyce, Fall 2013
Pactice Integation Math 0 Calculus I D Joyce, Fall 0 This fist set of indefinite integals, that is, antideivatives, only depends on a few pinciples of integation, the fist being that integation is invese
More informationPHYS 1441 Section 002. Lecture #3
PHYS 1441 Section 00 Chapte 1 Lectue #3 Wednesday, Sept. 6, 017 Coulomb s Law The Electic Field & Field Lines Electic Fields and Conductos Motion of a Chaged Paticle in an Electic Field Electic Dipoles
More informationME 3600 Control Systems Frequency Domain Analysis
ME 3600 Contol Systems Fequency Domain Analysis The fequency esponse of a system is defined as the steady-state esponse of the system to a sinusoidal (hamonic) input. Fo linea systems, the esulting steady-state
More informationF-IF Logistic Growth Model, Abstract Version
F-IF Logistic Gowth Model, Abstact Vesion Alignments to Content Standads: F-IFB4 Task An impotant example of a model often used in biology o ecology to model population gowth is called the logistic gowth
More informationMethod for Approximating Irrational Numbers
Method fo Appoximating Iational Numbes Eic Reichwein Depatment of Physics Univesity of Califonia, Santa Cuz June 6, 0 Abstact I will put foth an algoithm fo poducing inceasingly accuate ational appoximations
More informationPAPER 39 STOCHASTIC NETWORKS
MATHEMATICAL TRIPOS Pat III Tuesday, 2 June, 2015 1:30 pm to 4:30 pm PAPER 39 STOCHASTIC NETWORKS Attempt no moe than FOUR questions. Thee ae FIVE questions in total. The questions cay equal weight. STATIONERY
More information( ) John A. Quinn Lecture. ESE 531: Digital Signal Processing. Lecture Outline. Frequency Response of LTI System. Example: Zero on Real Axis
John A. Quinn Lecture ESE 531: Digital Signal Processing Lec 15: March 21, 2017 Review, Generalized Linear Phase Systems Penn ESE 531 Spring 2017 Khanna Lecture Outline!!! 2 Frequency Response of LTI System
More informationThe Z transform (2) 1
The Z transform (2) 1 Today Properties of the region of convergence (3.2) Read examples 3.7, 3.8 Announcements: ELEC 310 FINAL EXAM: April 14 2010, 14:00 pm ECS 123 Assignment 2 due tomorrow by 4:00 pm
More informationPHYS 172: Modern Mechanics. Summer Lecture 4 The Momentum Principle & Predicting Motion Read
PHYS 172: Moden Mechanics Summe 2010 Δp sys = F net Δt ΔE = W + Q sys su su ΔL sys = τ net Δt Lectue 4 The Momentum Pinciple & Pedicting Motion Read 2.6-2.9 READING QUESTION #1 Reading Question Which of
More informationON THE ASYMPTOTIC BEHAVIO R OF SOLUTIONS OF LINEAR DIFFERENCE EQUATION S
Publicacions Matemàtiques, Vol 38 (1994), 3-9. ON THE ASYMPTOTIC BEHAVIO R OF SOLUTIONS OF LINEAR DIFFERENCE EQUATION S JERZY POPENDA AND EWA SCHMEIDE L Abstact In the pape sufficient conditions fo the
More informationPhysics 401. Electromagnetic Theory (Electrodynamics)
Physics 401 Electomagnetic Theoy (Electodynamics) Please ead handouts and see couse webpages fo moe info Class: Monday, Wednesday & Fiday 9:00-10:00 Henn 302 Pofesso: Janis McKenna Office: Hennings-Physics
More informationEQUATIONS OF MOTION LUCA GUIDO MOLINARI
EQUATIONS OF MOTION LUCA GUIDO MOLINARI 1. Equation of motion of destuction opeatos Conside a system of bosons o femions descibed by a Hamiltonian H = H 1 + H 2, whee H 1 and H 2 ae espectively the one
More informationA new force Magnetic force. Today. Force Fields: A disturbance of space. The correspondence of a loop of current and magnet.
Today A new foce Magnetic foce Announcements HW#6 and HW#7 ae both due Wednesday Mach 18th. Thanks to my being WAY behind schedule, you 2nd exam will be a take-home exam! Stay tuned fo details Even if
More informationCHAPTER 3. Section 1. Modeling Population Growth
CHAPTER 3 Section 1. Modeling Population Gowth 1.1. The equation of the Malthusian model is Pt) = Ce t. Apply the initial condition P) = 1. Then 1 = Ce,oC = 1. Next apply the condition P1) = 3. Then 3
More informationModule 9: Electromagnetic Waves-I Lecture 9: Electromagnetic Waves-I
Module 9: Electomagnetic Waves-I Lectue 9: Electomagnetic Waves-I What is light, paticle o wave? Much of ou daily expeience with light, paticulaly the fact that light ays move in staight lines tells us
More informationOH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9
OH BOY! O h Boy!, was or igin a lly cr eat ed in F r en ch an d was a m a jor s u cc ess on t h e Fr en ch st a ge f or young au di enc es. It h a s b een s een by ap pr ox i ma t ely 175,000 sp ect at
More informationLecture 21 Helioseismology
ASTR 7500: Sola & Stella Magnetism Hale CGEP Sola & Space Physics Pofs. Bad Hindman & Jui Toome Lectue 1 Tues 9 Ap 013 zeus.coloado.edu/ast7500-toome Lectue 1 Helioseismology Obsevations of Sola Oscillations
More informationMath 1525 Excel Lab 3 Exponential and Logarithmic Functions Spring, 2001
Math 1525 Excel Lab 3 Exponential and Logaithmic Functions 1 Math 1525 Excel Lab 3 Exponential and Logaithmic Functions Sping, 21 Goal: The goals of Lab 3 ae to illustate exponential, logaithmic, and logistic
More informationHomework 1 Solutions CSE 101 Summer 2017
Homewok 1 Soutions CSE 101 Summe 2017 1 Waming Up 1.1 Pobem and Pobem Instance Find the smaest numbe in an aay of n integes a 1, a 2,..., a n. What is the input? What is the output? Is this a pobem o a
More informationb) (5) What is the magnitude of the force on the 6.0-kg block due to the contact with the 12.0-kg block?
Geneal Physics I Exam 2 - Chs. 4,5,6 - Foces, Cicula Motion, Enegy Oct. 13, 2010 Name Rec. Inst. Rec. Time Fo full cedit, make you wok clea to the gade. Show fomulas used, essential steps, and esults with
More informationPY208 Matter & Interactions Final Exam S2005
PY Matte & Inteactions Final Exam S2005 Name (pint) Please cicle you lectue section below: 003 (Ramakishnan 11:20 AM) 004 (Clake 1:30 PM) 005 (Chabay 2:35 PM) When you tun in the test, including the fomula
More informationCircular motion. Objectives. Physics terms. Assessment. Equations 5/22/14. Describe the accelerated motion of objects moving in circles.
Cicula motion Objectives Descibe the acceleated motion of objects moving in cicles. Use equations to analyze the acceleated motion of objects moving in cicles.. Descibe in you own wods what this equation
More informationSolution to HW 3, Ma 1a Fall 2016
Solution to HW 3, Ma a Fall 206 Section 2. Execise 2: Let C be a subset of the eal numbes consisting of those eal numbes x having the popety that evey digit in the decimal expansion of x is, 3, 5, o 7.
More informationGEORGIA INSTITUTE OF TECHNOLOGY SCHOOL OF ELECTRICAL AND COMPUTER ENGINEERING
GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL OF ELECTRICAL AND COMPUTER ENGINEERING ECE 06 Summer 08 Final Exam July 7, 08 NAME: Important Notes: Do not unstaple the test. Closed book and notes, except for three
More informationPhysics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 18: System of Particles II. Slide 18-1
Physics 1501 Fall 2008 Mechanics, Themodynamics, Waves, Fluids Lectue 18: System of Paticles II Slide 18-1 Recap: cente of mass The cente of mass of a composite object o system of paticles is the point
More informationCompletion. is dense in H. If V is complete, then U(V) = H.
Competion Theorem 1 (Competion) If ( V V ) is any inner product space then there exists a Hibert space ( H H ) and a map U : V H such that (i) U is 1 1 (ii) U is inear (iii) UxUy H xy V for a xy V (iv)
More informationarxiv: v1 [physics.pop-ph] 3 Jun 2013
A note on the electostatic enegy of two point chages axiv:1306.0401v1 [physics.pop-ph] 3 Jun 013 A C Tot Instituto de Física Univesidade Fedeal do io de Janeio Caixa Postal 68.58; CEP 1941-97 io de Janeio,
More informationCoordinate Geometry. = k2 e 2. 1 e + x. 1 e. ke ) 2. We now write = a, and shift the origin to the point (a, 0). Referred to
Coodinate Geomet Conic sections These ae pane cuves which can be descibed as the intesection of a cone with panes oiented in vaious diections. It can be demonstated that the ocus of a point which moves
More informationLINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE
LINEAR AND NONLINEAR ANALYSES O A WIND-TUNNEL INTRODUCTION BALANCE R. Kakehabadi and R. D. Rhew NASA LaRC, Hampton, VA The NASA Langley Reseach Cente (LaRC) has been designing stain-gauge balances fo utilization
More informationThe Solutions of the Classical Relativistic Two-Body Equation
T. J. of Physics (998), 07 4. c TÜBİTAK The Soutions of the Cassica Reativistic Two-Body Equation Coşkun ÖNEM Eciyes Univesity, Physics Depatment, 38039, Kaysei - TURKEY Received 3.08.996 Abstact With
More informationEach problem is worth 25 points, and you may solve the problems in any order.
EE 120: Signals & Systems Department of Electrical Engineering and Computer Sciences University of California, Berkeley Midterm Exam #2 April 11, 2016, 2:10-4:00pm Instructions: There are four questions
More informationand Slater Sum Rule Method * M L = 0, M S = 0 block: L L+ L 2
5.7 Lectue #4 e / ij and Sate Sum Rue Method 4 - LAST TIME:. L,S method fo setting up NLM L SM S many-eecton basis states in tems of inea combination of Sate deteminants * M L = 0, M S = 0 boc: L L+ L
More informationThe Strain Compatibility Equations in Polar Coordinates RAWB, Last Update 27/12/07
The Stain Compatibility Equations in Pola Coodinates RAWB Last Update 7//7 In D thee is just one compatibility equation. In D polas it is (Equ.) whee denotes the enineein shea (twice the tensoial shea)
More informationLecture 8 - Gauss s Law
Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.
More informationEnd of Semester Details: Final Exam
End of Semeste Details: Poject: By midnight Tuesday! - empty you bin Repot (MUST be pdf fomat) Pictues: device, team PDF of poste Web fom completed Team membe contibution Homewok Semeste homewok due Tuesday
More informationUniform Circular Motion
Unifom Cicula Motion Intoduction Ealie we defined acceleation as being the change in velocity with time: a = v t Until now we have only talked about changes in the magnitude of the acceleation: the speeding
More informationSolution 7 August 2015 ECE301 Signals and Systems: Final Exam. Cover Sheet
Solution 7 August 2015 ECE301 Signals and Systems: Final Exam Cover Sheet Test Duration: 120 minutes Coverage: Chap. 1, 2, 3, 4, 5, 7 One 8.5" x 11" crib sheet is allowed. Calculators, textbooks, notes
More informationL6 Energy Conversion. EIEN20 Design of Electrical Machines, IEA, Previous lecture. L6: Energy conversion. Today s goal
L: Enegy convesion a potentia fo causing a change R Ω u i L σ e R μ N i Pevious ectue R δ N i e L σ R Ω u i E x(y), i eectomagnetism eecto- and magnetomotive foce Induction action tansfomed o motiona votage
More informationConservative Averaging Method and its Application for One Heat Conduction Problem
Poceedings of the 4th WSEAS Int. Conf. on HEAT TRANSFER THERMAL ENGINEERING and ENVIRONMENT Elounda Geece August - 6 (pp6-) Consevative Aveaging Method and its Application fo One Heat Conduction Poblem
More informationMATHEMATICS GRADE 12 SESSION 38 (LEARNER NOTES)
EXAM PREPARATION PAPER (A) Leane Note: In this session you will be given the oppotunity to wok on a past examination pape (Feb/Ma 010 DoE Pape ). The pape consists of 1 questions. Question 1, and will
More informationMacro Theory B. The Permanent Income Hypothesis
Maco Theoy B The Pemanent Income Hypothesis Ofe Setty The Eitan Beglas School of Economics - Tel Aviv Univesity May 15, 2015 1 1 Motivation 1.1 An econometic check We want to build an empiical model with
More informationTo Feel a Force Chapter 7 Static equilibrium - torque and friction
To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on
More informationPHYS 172: Modern Mechanics. Fall Lecture 6 Fundamental Forces, Reciprocity Read
PHYS 172: Moden Mechanics Fall 2009 Lectue 6 Fundamental Foces, Recipocity Read 3.9 3.14 Exam 1 - Tuesday Septembe 15, 8:00-10:00 PM Elliott Hall of Music 1. The exam will be witten as a standad 1 hou
More informationThe physics of induction stoves
The physics of uction stoves This is an aticle fom my home page: www.olewitthansen.dk Contents 1. What is an uction stove...1. Including self-uctance...4 3. The contibution fom the magnetic moments...6
More informationECE503: Digital Signal Processing Lecture 6
ECE503: Digital Signal Processing Lecture 6 D. Richard Brown III WPI 20-February-2012 WPI D. Richard Brown III 20-February-2012 1 / 28 Lecture 6 Topics 1. Filter structures overview 2. FIR filter structures
More informationF 12. = G m m 1 2 F 21 = F 12. = G m 1m 2. Review. Physics 201, Lecture 22. Newton s Law Of Universal Gravitation
Physics 201, Lectue 22 Review Today s Topics n Univesal Gavitation (Chapte 13.1-13.3) n Newton s Law of Univesal Gavitation n Popeties of Gavitational Foce n Planet Obits; Keple s Laws by Newton s Law
More informationToday. Homework Problem Traveling Car. Announcements:
nnouncements: Today HW#3 due by 8:00 am Wednesday Exam #1 on Thusday /11 No class on Thusday /4 Taveling a Poblem fom HW# Gavity The Newtonian Woldview Vectos (Hints fo the boat poblem) ISP09s10 Lectue
More information