AP Physics - Electric Current

Size: px
Start display at page:

Download "AP Physics - Electric Current"

Transcription

1 AP Physics - Elecric Curren Did you ever imagine wha your paheic life, grim as i already is, would be like wihou hose lile wall socke hingees you have mouned on he wall jus above he deck of your house? Know wha he Physics Teacher is alking abou? Well, he s alking abou your basic elecriciy! People have only had elecriciy for he pas hundred years or so. Wha a difference i makes in how we live. Jus abou everyhing in he modern home works off elecriciy we make ligh, wash dishes, clean he deck, drill holes, cook food, freeze pork chops, sew clohes, cu wood, lisen o music, cool food, wach moving images, mash poaoes, dry our hair, ape T shows for laer viewing, hea air and waer, manipulae bis of informaion... he lis goes on and on. When we sudied elecric fields, we mainly deal wih charges ha weren doing much. You ginned up a bi of charge by rubbing a balloon wih a rabbi fur, and hen had fun waving he hing around, aracing bis of paper. Grea spor, bu wha good is i? Can really do any proper work wih i, can you? Well, ruh be old, saic elecriciy was no erribly useful (even hough he Physics Teacher loves i) - aside from a physics lab (where i was explored wih grea ineres) i was mainly used o enerain people during lecures or as oys. Sill, saic elecriciy, while cool and ineresing in and of iself, was no erribly useful. For one hing i was a lo of rouble. You had o rub hings or roae hings his enailed a lo of work and he payoff was raher piiful you ge a lousy spark or arac a bi of fluff o a charged up rubber sick. Big deal. Elecriciy didn really ake off and become he huge, dynamic engine of change ha ransformed he plane unil a way was found o have a coninuous flow of charge hrough a conducor. Wha was needed was a volage source. The firs volage source was wha we now call he baery. Baery Business: In he 1790 s Luigi Galvani found ha he could remove he leg of a frog (from he frog), place i on his lab able, and make i wich by ouching i wih a scalpel. This acually happened by acciden. Kind of scary don you hink? A dead leg suddenly wiching? Well, i quie caugh he fancy of Galvani. How could his be? Afer a series of experimens, he found ha he cause of he wich was a flow of charge generaed by wo dissimilar meals he scalpel and he meal lab ableop. The word galvanized remains as a ribue o Mr. Galvani. One is galvanized when he muscles suddenly conrac. Alessandro ola was inspired by his and learned o manufacure he firs we cells (he hing ha led o he modern baery). He used bis of dissimilar meals o generae elecriciy placed ino a sequence of elecrolye bearing bowls. The bowls were placed in a line and he conneced hem ogeher wih srips of meal ha were half copper and half zinc. He called his device he crown of cups. 340

2 The device produced elecriciy coninuously! As fas as you drew he elecrons off hey were replaced wih new ones. Amazing! Allesandro also developed an even beer mehod his one involved a sack of discs ha alernaed beween wo differen meals. Beween he meal discs was a cardboard disc ha had been soaked in sal waer. If he op meal disc was conneced o he boom disc wih a conducor, a coninuous flow of elecrons hrough he wire and he discs resuled. The device is called ola's pile. The uni for poenial difference, he vol, was named for ola. These primiive devices evolved ino he baeries ha we use oday dry cells (your basic alkaline energy cell ype hing) and rechargeable baeries (nickel cadmium and lead acid baeries). Properly speaking a baery is a collecion of cells. A single AA Duracell hingee is, o be correc abou he hing, called a cell, no a baery. A French physicis named George Leclanche ( ) invened he dry cell over a hundred years ago. These cells were made up from a zinc can he zinc acs as he cahode - and a carbon rod ha serves as he anode. The elecrolye is a pase made up of manganese oxide (MnO 4 ), ammonium chloride (NH 4 Cl), and powdered carbon. Modern dry cells include he alkaline ype dry cells. These are consruced much he same as he older (and cheaper) zinc carbon ypes. The main difference is he elecrolye. Boh use carbon rods and zinc cans. The elecrolye in he alkaline baery is basic raher han acidic. I urns ou ha he zinc can lass longer in a basic soluion. In his ype, he NH 4 Cl is replaced wih poassium hydroxide (KOH) or sodium hydroxide (NaOH). Boh of hese cells produce approximaely 1.5. The amoun of charge ha can be provided depends upon he size of he cell. A large D cell can produce a greaer amoun of charge han can a small AAA cell. All of hese ypes of cells or baeries are called primary cells. They produce elecriciy as long as he chemical reacions ake place. When hey cease, he baery is dead. A which poin you go ou and buy a + - anode cahode carbon rod pase of MnO 4, NH Cl, and carbon 4 zinc case 341

3 new one. You use hem and hen hrow hem away. A second major ype of cell or baery is also in use, hese are called secondary cells or sorage cells. These baeries, once hey've been drained of curren, can be recharged. Examples would be your old auomobile lead acid baery and nickel cadmium baeries used in porable elecric devices. Baeries work because of a chemical reacion ha akes place wihin he hing. These are known as oxidaion/reducion reacions. You will learn all abou hem in advanced or AP chemisry. The name is ofen shorened o redox reacions. In a redox reacion, elecrons are ransferred from one reacan o he oher. The reacan ha gains elecrons is "reduced", and he reacan ha loses elecrons is "oxidized". This causes elecrons o move from one chemical subsance o anoher. Any movemen of elecrons is called an elecric curren. Elecric Curren: Elecric curren is simply he flow of elecrons hrough a conducor. Two hings are needed for curren o flow: 1. A volage source (a dry cell will do nicely).. A complee pah hrough wich he elecrons may move. The carrier of charge in a solid conducor is he elecron. Posiive charge canno move as i is ied up in he proons of he aoms, which are essenially fixed in posiion. There are wo differen kinds of elecric curren; dc and ac. dc sands for direc curren. This is where he elecrons all flow in he same direcion. ac sands for alernaing curren. In an ac circui he direcion of he curren changes. We will deal mainly wih dc curren. To mainain he flow of elecrons - he elecric curren - a consan poenial difference mus be mainained. Such poenial differences are produced by volage sources. Common volage sources are: dry cells, baeries, generaors, magneos, solar cells, fuel cells, and alernaors jus o name a few. The symbol for elecric curren is I. (This doesn make a whole bunch of sense. You have o undersand, however, ha his convenion comes from France, so wha did you expec?) The uni for curren is he ampere, which is abbreviaed as A or amps. 1A1amp 1 C s Elecric curren is defined as he rae a which he charge flows hrough he conducor. The equaion for curren is: Q I Equaion for curren. 34

4 I is he curren in amperes, Q is he charge in Coulombs, and is he ime in seconds. Q The equaion given on he AP Physics Tes is: I Avg Q Bu we ll use I because i s easier o wrie. The ampere is a fairly large quaniy, so i is very common o use he ma. 1 ma = 10-3 A 3.5 x e - flow pas a poin in 0.35 s. Wha is he curren? We firs have o conver he number of elecrons o he charge ha hey have in Coulombs. 17 1C x 10 e 0.50 x10 C C x10 e I Q C 0.35 s 0.1 A Direcion of Curren Flow: This is an area of conroversy. Doesn seem logical ha people would argue abou his, bu hey do. The convenion ha we will use is his one. The direcion of curren flow is he direcion ha a posiive charge carrier would ravel in he circui. Now his makes no sense a all, and wise people don use i. The U.S. Navy does no use his convenion; ha s how bad i is. Anyway for us: elecriciy flows in he same direcion as posiive charge. The reason his is so supid is ha here is no posiive charge carrier. Only a negaive charge carrier, he ubiquious elecron. Acually, he only reason we use his supid convenion is ha i is he one used on he AP Physics es. So se your mind o using his supid convenion. Curren Flow Basics: The pah ha he elecrons use as hey flow around and around is called a circui. The simples possible circui would have a volage source and a conducor ha connecs he posiive and negaive side of he volage source. 343

5 As he elecrons move hrough he conducor, heir moion is blocked somewha by he aoms in he conducor, so he curren encouners a kind of opposiion o is flow. We define his as resisance. The uni for resisance is he Ohm. The symbol you ask? Okay i is his;. The hing ha uses up he elecriciy and provides he resisance is called he load. A load could be a ligh bulb, an elecric moor, a solenoid, a heaing coil, &c. The resisance of a conducor is very small, so elecrons ravel hrough i very easily. If i had a lo of resisance i would be called an insulaor. Many circuis have componens placed in hem o deliberaely add resisance. These are called resisors. For curren o flow hrough a resisor here mus be a poenial difference across i one side is a one poenial and he oher side is a anoher poenial, he elecrons flow hrough he hing aemping o equalize he poenial. We call his volage difference he volage drop. Circui Symbols: There are a number of sandard symbols ha are used when a drawing is made of a circui. These drawings are called schemaics. In old imey days elecronic devices would come wih a schemaic showing how he circui worked. You don see his much hese days, mainly because he circuiry oday is usually shrunk down and pu on a microchip. Can do much o repair a broken microchip. The symbol for a resisor is: The symbol for a baery is: + or The large line is he posiive side of he baery and he small line is he negaive side of he baery. Where you have only a large line and a small one, you have a cell. Conducors are simply sraigh lines. The symbol for a swich is: Le s look a a simple circui. I is shown in an open posiion. Which means ha i has creaed a gap in he circui so ha curren canno flow. The circui has a baery, a swich, and a resisor. The resisor represens he load on he circui. The load is he hing in a circui ha uses up he elecriciy. The load for a power plan is all he various places on he nework ha use he curren ha is produced. The load in a flashligh for example is he ligh bulb. The direcion of curren is he direcion of a posiive charge carrier. This would be from he posiive side of he baery o he negaive side of he baery. So he curren goes up (when he 344

6 swich is closed, making a complee circui), makes a righ urn, goes hrough he swich, hen urns righ, goes down, hen urns lef, ravels righ o lef hrough he resisor, hen urns righ, hen goes up and back ino he baery. Ohm s Law: We now have hree quaniies we can measure in a simple circui: volage (poenial difference), curren, and resisance. These hree quaniies are relaed o each oher by a simple formula known as Ohm s Law. I Ohm' s Law A poenial difference across a conducor causes curren o flow. The flow of he curren is opposed by he resisance of he circui. The resisance uses up some of he energy in he curren and convers i o hea. A waffle iron draws 7.1 A when plugged ino a 10 circui. Wha is is resisance? 10 I 17 I 7.1 A esisiviy: We consider shor lenghs of conducors o have essenially zero resisance, bu his is no rue for long lenghs. The resisance of a conducor is given by his equaion: l A is he resisance, is he resisiviy of he conducor, l is he lengh of he conducor, and A is he cross secional area of he conducor. This equaion is only good for wires ha have a consan cross-secion. The resisiviy depends on he meal, each meal has i own value. Generally you look he hing up when you wan o do a problem. The longer he wire, he greaer is resisance will be. Wha abou he size of he wire; is diameer? You can see from he equaion ha as he cross secional area of he wire increases, he resisance will decrease. So a hick fa wire will have less resisance han a very hin one will. Ineresing. Think of i his way, in a big fa wire here are esisiviies of Common Maerials Maerial esisiviy (m) Silver Copper Gold Aluminum Tungsen Iron Plainum Lead Nichrome Carbon Germanium Silicon Glass Hard ubber Sulfur Quarz 1.59 x x x x x x x x x x x

7 los of pahs for he elecrons o go hrough. In a skinny wire, here aren as many pahs and he elecrons are sor of scrunched ogeher rying o ge hrough, so hey ge held up more. This means more resisance. If you look a he able of resisiviy values, you see ha he bes conducor is silver wih copper coming in a close second. Silver, grea conducor ha i is, is quie expensive, so copper is he conducor of choice when wiring hings ogeher. Gold is someimes used, no because i is he bes conducor, which, from he able, you can see, bu raher because i is prey iner suff and doesn reac wih is surroundings or corrode. Copper is quie happy o corrode. So elecrical connecions wih copper wire ha is exposed o he elemens can corrode. Tha wouldn happen wih gold. Here is a lovely model of elecriciy flowing hrough a circui. We have a coal mine which pus 100 ons of coal ino each car ha goes hrough. The cars come in empy, hey leave wih coal. The mine represens he volage source. Each car receives 100 ons of poenial energy. This is equivalen of he energy provided by a baery. The rain ravels along he rack, which represens he conducor in a circui. As he cars ravel along hey pass hrough a car rae meer which measures he number of cars ha pass in a minue. This represens he curren, which is he number of Coulombs of charge per second. Here we have a rae of 5 cars/minue. each car begins wih 100 ons A Mass Difference is 100 ons Coal Mine adds 100 ons o each car 5 cars/minue each car reurns wih no coal A Car rae Meer The nex hing he rain mus ravel hrough is a coal deecor. This is he gizmo represened by This device measures Power Plan 500 ons/min he amoun of coal in each car going in and ou and measures he difference. For he firs one, he ons of coal in each car is he same going in as coming ou. This meer represens he vol meer which measures poenial difference across a componen. There is no poenial difference in a shor piece Mass Difference of conducor jus as here is no is 100 ons difference in he amoun of coal in each car raveling along he sraigh rack. No mass Difference 346

8 The coal arrives a a power plan. This, he power plan, represens he load. Each car dumps he 100 ons of coal i began wih. There is a coal mass difference across he plan of 100 ons per car. This represens he volage drop of he load. Afer he power plan, once again here is no mass difference beween he cars. Also he car rae is sill he same, 5 cars/minue. Back a he mine, here is a mass difference as he cars go ino he mine and leave he mine of 100 ons per car. This represens he volage drop across he baery. Wha a lovely lile model. Is everyhing clear? Wha if here were power plans? Wha is he resisance of a copper wire, which has a diameer of 1.00 mm and a lengh of 5 m? The resisiviy of copper is 1.7 x 10-8 m. All we have o do is plug and chug. l x10 m l A A 6.4 x m 1.00 x10 3 m Elecrical Energy & Power: A baery conains poenial energy which, when i is discharged, is convered ino he kineic energy of he elecrons. The resisance of he circui convers he kineic energy of he elecrons o hermal energy. Ever noice how warm a ligh bulb ges afer is been swiched on for a few minues? Toy ovens ha lile girls play wih acually use he hea produced by a ligh bulb o bake cookies. The circui uses up he energy provided by he volage source. We know ha elecrical poenial energy is: U q The rae a which he poenial energy is provided is he power: W U P becomes P q Bu q is he curren, I. so q q P I This gives us a simple equaion for power: 347

9 P I P is power, I is curren, and is he poenial difference. This equaion will be provided o you on he AP Physics Tes. If we apply Ohm s law o he power equaion, we can develop a few oher power equaions as well. Bu you won have hese for he es, alhough you can easily develop hem yourself. You will have Ohm s law o play around wih, so his is a useful hing. Here is he power equaion: P I Using Ohm s law, I we can plug I ino he power equaion for. P I I P I Also, from Ohm s law I So P P This gives us 3 equaions for Power: P I P I P When elecrons flow hrough a conducor, he power loss due o he resisance of he conducor is equal o I. This is called he I Loss or joule heaing. I can be very significan in long conducors. For example, power lines can have very large losses of energy o he I loss. When you buy elecriciy from he power company, you are no buying power. You are acually buying work, i.e. hey sell you energy which you do work wih. The uni ha he friendly power company sells heir energy in is no he joule. They sell i by he kilowa hour. Bu wha is a kilowa hour? 348

10 Power is he rae a which work is done: W P so W P We can ake a kilowa hour and conver i o joules. This should convince you ha i is in fac a uni of energy s10 3W J kw h s 3.6 x 10 1 h 1kW s J An elecric heaer provides 50.0 o a nichrome wire of resisance 8.0. Find he (a) curren hrough he wire and (b) power of he device. (a) We can easily find he curren in he wire using Ohm s law: I 50.0 I A (b) Find he power: 50.0 P I and I so P 310W 8.00 You have a 75 W ligh bulb. I goes ino a 10 circui. So wha is (a) he resisance of he bulb and (b) he curren ha flows hrough i? (a) esisance: (b) Curren: 10 P 190 P 75W 10 I I 0.63 A 190 You wach T for.8 hours. The T is raed a 3.8 kw. If elecriciy coss 9.5 cens per kwh, how much did your lile T program cos you o wach? All we need figure ou is he number of kilowa hours used up, hen aply he 9.5 cens per kilowa hour conversion facor. W P W P 3.8 kw.8 h 10.6 kwh 9.5 cens 10.6 kwh cens $ kwh 349

11 We didn round i off o wo significan figures. This is because you jus know ha he power company would never round anyhing off (excep o round i up), he greedy blighers! An oven operaes drawing 4.0 A on a 10 household circui. If you run i for 5.0 hours, how much does i cos (a 8.0 cens a kwh)? P I 4 A W.88 kw.88 kw 5.0 h 14.4 kwh Cos: $0.08 Cos 14.4 kwh $ kwh When a coffee seed is planed, i akes five years o yield consumable frui. Our eyes are always he same size from birh, bu our nose and ears never sop growing. The whie par of your fingernail is called he lunula. A wo-bi moon is in he firs quarer. Oak rees do no have acorns unil hey are fify years old or older. Ocober 10 is Naional Meric Day. The permanen eeh ha erup o replace heir primary predecessors (baby eeh) are called succedaneous eeh. Assuming udolph was in fron, here are 4030 ways o arrange he oher eigh reindeer. If you can see a rainbow you mus have your back o he sun. If you don', you can' see i. Drinking waer afer eaing reduces he acid in your mouh by 61 percen. Source: Denianne Bland The wo mos common surgeries are biopsies and cesarean secions. Naional Pi Day is March 14, a 1:59. (3/14 1:59) The digis of pi are , he greaes sum of 7 consequive digis in he firs 1,000,000 or so digis. If you need o remember pi, jus coun he leers in each word in he senence: "May I have a large conainer of coffee?" If you ge he coffee and are polie and say "Thank you," you ge wo more decimal places. [ ] Plaser of Paris is naurally fire reardan. A abou 600 degrees Farenhei he chemical waer ha is sored in i is released. This is also why walls are ofen "sweay" afer a fire. Mos of he iamin C in fruis is in he pih (skin). 350

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

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

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 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

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

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

Hall effect. Formulae :- 1) Hall coefficient RH = cm / Coulumb. 2) Magnetic induction BY 2

Hall effect. Formulae :- 1) Hall coefficient RH = cm / Coulumb. 2) Magnetic induction BY 2 Page of 6 all effec Aim :- ) To deermine he all coefficien (R ) ) To measure he unknown magneic field (B ) and o compare i wih ha measured by he Gaussmeer (B ). Apparaus :- ) Gauss meer wih probe ) Elecromagne

More information

Introduction to AC Power, RMS RMS. ECE 2210 AC Power p1. Use RMS in power calculations. AC Power P =? DC Power P =. V I = R =. I 2 R. V p.

Introduction to AC Power, RMS RMS. ECE 2210 AC Power p1. Use RMS in power calculations. AC Power P =? DC Power P =. V I = R =. I 2 R. V p. ECE MS I DC Power P I = Inroducion o AC Power, MS I AC Power P =? A Solp //9, // // correced p4 '4 v( ) = p cos( ω ) v( ) p( ) Couldn' we define an "effecive" volage ha would allow us o use he same relaionships

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

KINEMATICS IN ONE DIMENSION

KINEMATICS IN ONE DIMENSION KINEMATICS IN ONE DIMENSION PREVIEW Kinemaics is he sudy of how hings move how far (disance and displacemen), how fas (speed and velociy), and how fas ha how fas changes (acceleraion). We say ha an objec

More information

Chapter 28 - Circuits

Chapter 28 - Circuits Physics 4B Lecure Noes Chaper 28 - Circuis Problem Se #7 - due: Ch 28 -, 9, 4, 7, 23, 38, 47, 53, 57, 66, 70, 75 Lecure Ouline. Kirchoff's ules 2. esisors in Series 3. esisors in Parallel 4. More Complex

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

Chapter 1 Electric Circuit Variables

Chapter 1 Electric Circuit Variables Chaper 1 Elecric Circui Variables Exercises Exercise 1.2-1 Find he charge ha has enered an elemen by ime when i = 8 2 4 A, 0. Assume q() = 0 for < 0. 8 3 2 Answer: q () = 2 C 3 () 2 i = 8 4 A 2 8 3 2 8

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

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

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

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

Biol. 356 Lab 8. Mortality, Recruitment, and Migration Rates

Biol. 356 Lab 8. Mortality, Recruitment, and Migration Rates Biol. 356 Lab 8. Moraliy, Recruimen, and Migraion Raes (modified from Cox, 00, General Ecology Lab Manual, McGraw Hill) Las week we esimaed populaion size hrough several mehods. One assumpion of all hese

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

Activity 4 Solutions: Transfer of Thermal Energy

Activity 4 Solutions: Transfer of Thermal Energy Aciviy 4 Soluions: Transfer of Thermal nergy 4.1 How Does Temperaure Differ from Thermal nergy? a) Temperaure Your insrucor will demonsrae molecular moion a differen emperaures. 1) Wha happens o molecular

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

The problem with linear regulators

The 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 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

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

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

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

a 10.0 (m/s 2 ) 5.0 Name: Date: 1. The graph below describes the motion of a fly that starts out going right V(m/s)

a 10.0 (m/s 2 ) 5.0 Name: Date: 1. The graph below describes the motion of a fly that starts out going right V(m/s) Name: Dae: Kinemaics Review (Honors. Physics) Complee he following on a separae shee of paper o be urned in on he day of he es. ALL WORK MUST BE SHOWN TO RECEIVE CREDIT. 1. The graph below describes he

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

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

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

dv 7. Voltage-current relationship can be obtained by integrating both sides of i = C :

dv 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 information

3.6 Derivatives as Rates of Change

3.6 Derivatives as Rates of Change 3.6 Derivaives as Raes of Change Problem 1 John is walking along a sraigh pah. His posiion a he ime >0 is given by s = f(). He sars a =0from his house (f(0) = 0) and he graph of f is given below. (a) Describe

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

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

MOMENTUM CONSERVATION LAW

MOMENTUM CONSERVATION LAW 1 AAST/AEDT AP PHYSICS B: Impulse and Momenum Le us run an experimen: The ball is moving wih a velociy of V o and a force of F is applied on i for he ime inerval of. As he resul he ball s velociy changes

More information

Math 333 Problem Set #2 Solution 14 February 2003

Math 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 information

Conceptual Physics Review (Chapters 2 & 3)

Conceptual Physics Review (Chapters 2 & 3) Concepual Physics Review (Chapers 2 & 3) Soluions Sample Calculaions 1. My friend and I decide o race down a sraigh srech of road. We boh ge in our cars and sar from res. I hold he seering wheel seady,

More information

Of all of the intellectual hurdles which the human mind has confronted and has overcome in the last fifteen hundred years, the one which seems to me

Of all of the intellectual hurdles which the human mind has confronted and has overcome in the last fifteen hundred years, the one which seems to me Of all of he inellecual hurdles which he human mind has confroned and has overcome in he las fifeen hundred years, he one which seems o me o have been he mos amazing in characer and he mos supendous in

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

Constant Acceleration

Constant Acceleration Objecive Consan Acceleraion To deermine he acceleraion of objecs moving along a sraigh line wih consan acceleraion. Inroducion The posiion y of a paricle moving along a sraigh line wih a consan acceleraion

More information

PHYS 1401 General Physics I Test 3 Review Questions

PHYS 1401 General Physics I Test 3 Review Questions PHYS 1401 General Physics I Tes 3 Review Quesions Ch. 7 1. A 6500 kg railroad car moving a 4.0 m/s couples wih a second 7500 kg car iniially a res. a) Skech before and afer picures of he siuaion. b) Wha

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

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

Welcome Back to Physics 215!

Welcome Back to Physics 215! Welcome Back o Physics 215! (General Physics I) Thurs. Jan 19 h, 2017 Lecure01-2 1 Las ime: Syllabus Unis and dimensional analysis Today: Displacemen, velociy, acceleraion graphs Nex ime: More acceleraion

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

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs.

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs. Physics 180A Fall 2008 Tes 1-120 poins Name Provide he bes answer o he following quesions and problems. Wach your sig figs. 1) The number of meaningful digis in a number is called he number of. When numbers

More information

Chapter Floating Point Representation

Chapter Floating Point Representation Chaper 01.05 Floaing Poin Represenaion Afer reading his chaper, you should be able o: 1. conver a base- number o a binary floaing poin represenaion,. conver a binary floaing poin number o is equivalen

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

2) Of the following questions, which ones are thermodynamic, rather than kinetic concepts?

2) Of the following questions, which ones are thermodynamic, rather than kinetic concepts? AP Chemisry Tes (Chaper 12) Muliple Choice (40%) 1) Which of he following is a kineic quaniy? A) Enhalpy B) Inernal Energy C) Gibb s free energy D) Enropy E) Rae of reacion 2) Of he following quesions,

More information

Physics 1502: Lecture 20 Today s Agenda

Physics 1502: Lecture 20 Today s Agenda Physics 152: Lecure 2 Today s Agenda Announcemens: Chap.27 & 28 Homework 6: Friday nducion Faraday's Law ds N S v S N v 1 A Loop Moving Through a Magneic Field ε() =? F() =? Φ() =? Schemaic Diagram of

More information

04. Kinetics of a second order reaction

04. 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 information

72 Calculus and Structures

72 Calculus and Structures 72 Calculus and Srucures CHAPTER 5 DISTANCE AND ACCUMULATED CHANGE Calculus and Srucures 73 Copyrigh Chaper 5 DISTANCE AND ACCUMULATED CHANGE 5. DISTANCE a. Consan velociy Le s ake anoher look a Mary s

More information

Circuit Variables. AP 1.1 Use a product of ratios to convert two-thirds the speed of light from meters per second to miles per second: 1 ft 12 in

Circuit Variables. AP 1.1 Use a product of ratios to convert two-thirds the speed of light from meters per second to miles per second: 1 ft 12 in Circui Variables 1 Assessmen Problems AP 1.1 Use a produc of raios o conver wo-hirds he speed of ligh from meers per second o miles per second: ( ) 2 3 1 8 m 3 1 s 1 cm 1 m 1 in 2.54 cm 1 f 12 in 1 mile

More information

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws Chaper 5: Phenomena Phenomena: The reacion (aq) + B(aq) C(aq) was sudied a wo differen emperaures (98 K and 35 K). For each emperaure he reacion was sared by puing differen concenraions of he 3 species

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

Displacement ( x) x x x

Displacement ( x) x x x Kinemaics Kinemaics is he branch of mechanics ha describes he moion of objecs wihou necessarily discussing wha causes he moion. 1-Dimensional Kinemaics (or 1- Dimensional moion) refers o moion in a sraigh

More information

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan Ground Rules PC11 Fundamenals of Physics I Lecures 3 and 4 Moion in One Dimension A/Prof Tay Seng Chuan 1 Swich off your handphone and pager Swich off your lapop compuer and keep i No alking while lecure

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

SPH3U: Projectiles. Recorder: Manager: Speaker:

SPH3U: Projectiles. Recorder: Manager: Speaker: SPH3U: Projeciles Now i s ime o use our new skills o analyze he moion of a golf ball ha was ossed hrough he air. Le s find ou wha is special abou he moion of a projecile. Recorder: Manager: Speaker: 0

More information

In this chapter the model of free motion under gravity is extended to objects projected at an angle. When you have completed it, you should

In this chapter the model of free motion under gravity is extended to objects projected at an angle. When you have completed it, you should Cambridge Universiy Press 978--36-60033-7 Cambridge Inernaional AS and A Level Mahemaics: Mechanics Coursebook Excerp More Informaion Chaper The moion of projeciles In his chaper he model of free moion

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

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

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

Section 2.2 Charge and Current 2.6 b) The current direction is designated as the direction of the movement of positive charges.

Section 2.2 Charge and Current 2.6 b) The current direction is designated as the direction of the movement of positive charges. Chaper Soluions Secion. Inroducion. Curren source. Volage source. esisor.4 Capacior.5 Inducor Secion. Charge and Curren.6 b) The curren direcion is designaed as he direcion of he movemen of posiive charges..7

More information

i 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.

i 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 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

Seminar 4: Hotelling 2

Seminar 4: Hotelling 2 Seminar 4: Hoelling 2 November 3, 211 1 Exercise Par 1 Iso-elasic demand A non renewable resource of a known sock S can be exraced a zero cos. Demand for he resource is of he form: D(p ) = p ε ε > A a

More information

Predator - Prey Model Trajectories and the nonlinear conservation law

Predator - Prey Model Trajectories and the nonlinear conservation law Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories

More information

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a Kinemaics Paper 1 1. The graph below shows he ariaion wih ime of he acceleraion a of an objec from = o = T. a T The shaded area under he graph represens change in A. displacemen. B. elociy. C. momenum.

More information

IE1206 Embedded Electronics

IE1206 Embedded Electronics E06 Embedded Elecronics Le Le3 Le4 Le Ex Ex P-block Documenaion, Seriecom Pulse sensors,, R, P, serial and parallel K LAB Pulse sensors, Menu program Sar of programing ask Kirchhoffs laws Node analysis

More information

dv i= C. dt 1. Assuming the passive sign convention, (a) i = 0 (dc) (b) (220)( 9)(16.2) t t Engineering Circuit Analysis 8 th Edition

dv i= C. dt 1. Assuming the passive sign convention, (a) i = 0 (dc) (b) (220)( 9)(16.2) t t Engineering Circuit Analysis 8 th Edition . Assuming he passive sign convenion, dv i= C. d (a) i = (dc) 9 9 (b) (22)( 9)(6.2) i= e = 32.8e A 9 3 (c) i (22 = )(8 )(.) sin. = 7.6sin. pa 9 (d) i= (22 )(9)(.8) cos.8 = 58.4 cos.8 na 2. (a) C = 3 pf,

More information

Suggested Practice Problems (set #2) for the Physics Placement Test

Suggested Practice Problems (set #2) for the Physics Placement Test Deparmen of Physics College of Ars and Sciences American Universiy of Sharjah (AUS) Fall 014 Suggesed Pracice Problems (se #) for he Physics Placemen Tes This documen conains 5 suggesed problems ha are

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

The average rate of change between two points on a function is d t

The average rate of change between two points on a function is d t SM Dae: Secion: Objecive: The average rae of change beween wo poins on a funcion is d. For example, if he funcion ( ) represens he disance in miles ha a car has raveled afer hours, hen finding he slope

More information

Chapter 2 The Derivative Applied Calculus 107. We ll need a rule for finding the derivative of a product so we don t have to multiply everything out.

Chapter 2 The Derivative Applied Calculus 107. We ll need a rule for finding the derivative of a product so we don t have to multiply everything out. Chaper The Derivaive Applie Calculus 107 Secion 4: Prouc an Quoien Rules The basic rules will le us ackle simple funcions. Bu wha happens if we nee he erivaive of a combinaion of hese funcions? Eample

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

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

Instructor: Barry McQuarrie Page 1 of 5

Instructor: Barry McQuarrie Page 1 of 5 Procedure for Solving radical equaions 1. Algebraically isolae one radical by iself on one side of equal sign. 2. Raise each side of he equaion o an appropriae power o remove he radical. 3. Simplify. 4.

More information

Decimal moved after first digit = 4.6 x Decimal moves five places left SCIENTIFIC > POSITIONAL. a) g) 5.31 x b) 0.

Decimal moved after first digit = 4.6 x Decimal moves five places left SCIENTIFIC > POSITIONAL. a) g) 5.31 x b) 0. PHYSICS 20 UNIT 1 SCIENCE MATH WORKSHEET NAME: A. Sandard Noaion Very large and very small numbers are easily wrien using scienific (or sandard) noaion, raher han decimal (or posiional) noaion. Sandard

More information

Learning Objectives: Practice designing and simulating digital circuits including flip flops Experience state machine design procedure

Learning 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 information

By the end of this chapter, you will have covered the following key knowledge and skills:

By the end of this chapter, you will have covered the following key knowledge and skills: Chaper 2 Elecriciy Key knowledge and skills By he end of his chaper, you will have covered he following key knowledge and skills: \\\\\\\\\\\\\\\\\\\\\\ \\\\\\\\\\\\\\\\\\ \\\\\\\\\\\\\\\\\\\\\\\ \\\\\\\\

More information

Lab #2: Kinematics in 1-Dimension

Lab #2: Kinematics in 1-Dimension Reading Assignmen: Chaper 2, Secions 2-1 hrough 2-8 Lab #2: Kinemaics in 1-Dimension Inroducion: The sudy of moion is broken ino wo main areas of sudy kinemaics and dynamics. Kinemaics is he descripion

More information

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively:

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively: XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of

More information

1. Kinematics I: Position and Velocity

1. Kinematics I: Position and Velocity 1. Kinemaics I: Posiion and Velociy Inroducion The purpose of his eperimen is o undersand and describe moion. We describe he moion of an objec by specifying is posiion, velociy, and acceleraion. In his

More information

Two Coupled Oscillators / Normal Modes

Two Coupled Oscillators / Normal Modes Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own

More information

15. Bicycle Wheel. Graph of height y (cm) above the axle against time t (s) over a 6-second interval. 15 bike wheel

15. Bicycle Wheel. Graph of height y (cm) above the axle against time t (s) over a 6-second interval. 15 bike wheel 15. Biccle Wheel The graph We moun a biccle wheel so ha i is free o roae in a verical plane. In fac, wha works easil is o pu an exension on one of he axles, and ge a suden o sand on one side and hold he

More information

Today: Falling. v, a

Today: Falling. v, a Today: Falling. v, a Did you ge my es email? If no, make sure i s no in your junk box, and add sbs0016@mix.wvu.edu o your address book! Also please email me o le me know. I will be emailing ou pracice

More information

x i v x t a dx dt t x

x i v x t a dx dt t x Physics 3A: Basic Physics I Shoup - Miderm Useful Equaions A y A sin A A A y an A y A A = A i + A y j + A z k A * B = A B cos(θ) A B = A B sin(θ) A * B = A B + A y B y + A z B z A B = (A y B z A z B y

More information

A First Course on Kinetics and Reaction Engineering. Class 19 on Unit 18

A First Course on Kinetics and Reaction Engineering. Class 19 on Unit 18 A Firs ourse on Kineics and Reacion Engineering lass 19 on Uni 18 Par I - hemical Reacions Par II - hemical Reacion Kineics Where We re Going Par III - hemical Reacion Engineering A. Ideal Reacors B. Perfecly

More information

Key points. Unit 7. Kinetic Energy -E K orke. Energy Storage 2/4/2016. Describing the Interaction between energy and matter continued

Key points. Unit 7. Kinetic Energy -E K orke. Energy Storage 2/4/2016. Describing the Interaction between energy and matter continued Key poins Uni 7 Energy Sorage and Transfer Model Energy-a conserved, subsance-like quaniy wih he capabiliy o produce change in physical sysems I does no come in differen forms i s jus energy. I s sored

More information

Math 116 Practice for Exam 2

Math 116 Practice for Exam 2 Mah 6 Pracice for Exam Generaed Ocober 3, 7 Name: SOLUTIONS Insrucor: Secion Number:. This exam has 5 quesions. Noe ha he problems are no of equal difficuly, so you may wan o skip over and reurn o a problem

More information

Physics 1402: Lecture 22 Today s Agenda

Physics 1402: Lecture 22 Today s Agenda Physics 142: ecure 22 Today s Agenda Announcemens: R - RV - R circuis Homework 6: due nex Wednesday Inducion / A curren Inducion Self-Inducance, R ircuis X X X X X X X X X long solenoid Energy and energy

More information

PHYSICS 220 Lecture 02 Motion, Forces, and Newton s Laws Textbook Sections

PHYSICS 220 Lecture 02 Motion, Forces, and Newton s Laws Textbook Sections PHYSICS 220 Lecure 02 Moion, Forces, and Newon s Laws Texbook Secions 2.2-2.4 Lecure 2 Purdue Universiy, Physics 220 1 Overview Las Lecure Unis Scienific Noaion Significan Figures Moion Displacemen: Δx

More information

Chapter 7: Solving Trig Equations

Chapter 7: Solving Trig Equations Haberman MTH Secion I: The Trigonomeric Funcions Chaper 7: Solving Trig Equaions Le s sar by solving a couple of equaions ha involve he sine funcion EXAMPLE a: Solve he equaion sin( ) The inverse funcions

More information

Lecture -14: Chopper fed DC Drives

Lecture -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 information

x(m) t(sec ) Homework #2. Ph 231 Introductory Physics, Sp-03 Page 1 of 4

x(m) t(sec ) Homework #2. Ph 231 Introductory Physics, Sp-03 Page 1 of 4 Homework #2. Ph 231 Inroducory Physics, Sp-03 Page 1 of 4 2-1A. A person walks 2 miles Eas (E) in 40 minues and hen back 1 mile Wes (W) in 20 minues. Wha are her average speed and average velociy (in ha

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

Position, Velocity, and Acceleration

Position, Velocity, and Acceleration rev 06/2017 Posiion, Velociy, and Acceleraion Equipmen Qy Equipmen Par Number 1 Dynamic Track ME-9493 1 Car ME-9454 1 Fan Accessory ME-9491 1 Moion Sensor II CI-6742A 1 Track Barrier Purpose The purpose

More information

Physical Limitations of Logic Gates Week 10a

Physical 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 information