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letcure01_06_21_2010

Course: EE 40 40, Summer 2010
School: Berkeley
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to Introduction Microelectronic Circuits EE40 Lecture 1 Josh Hug 6/21/2010 EE40 Summer 2010 Hug 1 A Story EE40 Summer 2010 Hug 2 Integrated Circuit (Core i7 processor) EE40 Summer 2010 Courtesy of Intel Hug 3 Integrated Circuits (Core i7 processor) Almost 1,000,000,000 transistors Features as small as a nanometer EE40 Summer 2010 Hug 4 Then (C64, 1983) and Now (iPhone, 2010) 5000 nanometer...

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to Introduction Microelectronic Circuits EE40 Lecture 1 Josh Hug 6/21/2010 EE40 Summer 2010 Hug 1 A Story EE40 Summer 2010 Hug 2 Integrated Circuit (Core i7 processor) EE40 Summer 2010 Courtesy of Intel Hug 3 Integrated Circuits (Core i7 processor) Almost 1,000,000,000 transistors Features as small as a nanometer EE40 Summer 2010 Hug 4 Then (C64, 1983) and Now (iPhone, 2010) 5000 nanometer process 1.023 MHz (CPU) 10,000s of transistors 160 x 200 x 16 color display $1300 dollars at release (adjusted for inflation) EE40 Summer 2010 45 nanometer process 1,000 MHz 100,000,000 transistors 320 x 480 x 262,144 color display $600 dollars at release Hug 5 Moores Law EE40 Summer 2010 Hug 6 Electron Microscope view of MOS Transistor Insulating Layer (gate oxide) now just 1.2 nm thick For reference: Human hair: 100,000 nm Silicon atom: 0.1 nm 35 nm wide In 10 years, we will hit a wall. EE40 Summer 2010 Courtesy: Toms Hardware, June 11 2006 (65 nm process) Hug 7 Theres (still) Plenty of Room at the Bottom Theres more than one way to build a nanoscale information processing unit Folklore E coli is a 2000 nm by 500 nm device by area (in 3D, 500 nm tall) Self-replicating, self-powered system 1 million interconnected subdevices of 4000 types Stores 1 megabyte of genomic data Humans are capable of building only a 10 bit SRAM in the same area EE40 Summer 2010 Painting of E. Coli courtesy of shardcore.org Hug 8 Even if we switch from MOS transistors Integrated Circuits will be an important technology for a long time Designing and building these circuits requires knowledge in many fields Circuit analysis Semiconductor physics Chemistry Computer microarchitecture Signal processing And many many more EE40 Summer 2010 Hug 9 EE 40 Course Overview EECS 40: One of five EECS core courses (with 20, 61A, 61B, and 61C) introduces hardware side of EECS prerequisite for EE105, EE130, EE141, EE150 Prerequisites: Math 1B, Physics 7B Course content: Electronic circuits Some very basic semiconductor physics Integrated-circuit devices and technology EE40 Summer 2010 Hug 10 EE40 Circuit Input/Output Response Silicon EE40 Circuit Modeling EE105, EE130 Device Modeling Copper Device Response Other Materials EE40 Summer 2010 Hug 11 Core EECS Courses (Computer Centric View) Computer Programs CS61C 61A/B EE40 Computers Integrated Circuits Circuit models Combinational and Sequential Logic State machines EE40 CS61C Transistors and other devices Buildable Artifacts EE40 Summer 2010 Silicon and other materials CS61C EE20 Network Models Hug 12 Course Logistics EE40 Summer 2010 Hug 13 Important Dates Two or three in-class midterms July 9th (18 days from now) July 28th August 11th (if you guys vote to do this) One comprehensive final August 13th July 2 must be registered for course June 25th last day to drop for a refund July 30th last day to drop for no refund EE40 Summer 2010 Hug 14 Grades Reading Assignments (5%) HW (20%) Lowest HW dropped One late homework allowed Midterm and Final (20%, 20%, 20%) If we do 3 midterms, lowest dropped Labs (15%) Six labs Two lab projects 2nd project is open ended, get started early if you want to do something crazy EE40 Summer 2010 Hug 15 Reading Assignments Reading assignments due before class Easy problems to make sure you got at least something out of the reading Credit/No Credit grading No late submissions allowed Lowest two dropped Submit on bspace (bspace.berkeley.edu) EE40 Summer 2010 Hug 16 Homeworks Homeworks due on either Tuesdays or Fridays Must be in the HW box, 240 Cory by 5 PM Problems graded on a 0,1,2,3 basis You do not get 1 point for writing the problem down Will be returned in lecture Also available during my office hours On the top page, right top corner, write your name (in the form: Last Name, First Name) Fine to discuss problems with others but ALL WORK SHOULD BE YOUR OWN EE40 Summer 2010 Hug 17 Homework Philosophy Homework is where the real learning happens, similar to practicing a musical instrument My homeworks are for a grade so that if you perform poorly on midterms, it is evidence of what youve accomplished outside of a testing environment Copying homework answers is tempting, but: It is an unfair representation of your accomplishments You will be unprepared for midterms EE40 Summer 2010 Hug 18 Labs Labs start NEXT week 2 labs per week, 3 hours each Labs 50% on Prelab and 50% on Report Do prelabs BEFORE the lab You must complete the prelab section before going to the lab. The prelabs are checked by the GSIs at the beginning of each session. If prelabs are completed during the lab sessions, it is considered late and 50% will be deducted Lab reports are due exactly one week after your lab is completed Some make up labs will be scheduled EE40 Summer 2010 Hug 19 Discussion Sections and Office Hours Note that discussion section times have changed, now only one hour: Tuesday: 1-2 PM Friday: 2-3 PM Held in 293 Cory Office Hours will be posted later today EE40 Summer 2010 Hug 20 Textbook and i>Clicker Our textbook is Foundations of Analog and Digital Electronic Circuits, 1st edition by Anant Agarwal and Jeffrey Lang Also required is an i>Clicker For submitting answers in class Available at ASUC bookstore or online ASUC will buy them for $30 (as of last semester) Will register them by serial # to your name online (details on website soon) EE40 Summer 2010 Hug 21 Lectures We have a 2 hour lecture Nobody on this earth is that entertaining End of each hour peer instruction Work on small problem in groups Submit answer via i>Clicker Go over problem Take a break Attendance isnt required, but reading assignments for lecture ARE required Lectures will be posted online EE40 Summer 2010 Hug 22 i>Clicker Test Lets test those i>Clickers Question: Does your i>Clicker work? A. Yes B. No EE40 Summer 2010 Hug 23 Course Website Course website is at http://wwwinst.eecs.berkeley.edu/~ee40/su10/ Homeworks, midterm solutions, labs, and anything else we want you to know will be posted there Bspace will be used for Submitting reading assignments Discussion board EE40 Summer 2010 Hug 24 HW0 Mini-biography assignment Due Wednesday May submit either: Online on bSpace (due at midnight) In class (at beginning of class) Our HW0 is available on the web under our pictures EE40 Summer 2010 Hug 25 Study Groups Learning or working in a team works better than alone Reduces chance that you get stuck on something minor Helping someone else requires very deep well organized knowledge of a topic You learn best by teaching Provides a chance to learn how to solve problems more efficiently and with higher accuracy Gives immediate feedback on how you stand on coursework comprehension EE40 Summer 2010 Hug 26 Study Groups In my obscenely difficult Graduate Probability and Statistics Class, wed: Start the homework early (like the day it came out), and attempt all of the problems alone. Meet a day or two before it was due Go over every homework problem Discuss our approach to each Different person led on each problem This is fine, but ALL WORK MUST BE YOUR OWN. Do not copy. EE40 Summer 2010 Hug 27 Extra Credit: EPA! Effort Attending office hours, completing all assignments, turning in HW0 Participation Attending lecture and voting using i>Clickers Asking great questions in discussion, lab, and lecture and making things generally more interactive Altruism Helping others in lab or on the discussion board EPA! extra credit points have the potential to bump students up to the next grade level! (but actual EPA! scores are internal) EE40 Summer 2010 Hug 28 Course ProblemsCheating What is cheating? Studying together in groups is encouraged. Turned-in work must be completely your own. Common examples of cheating: running out of time on a assignment and then copying an answer from a friend, taking homework from box and copying, asking to borrow a solution just to take a look, copying an exam question, Both giver and receiver are equally culpable Cheating points: 0 EPA, negative points for that assignment / lab / exam (e.g., if its worth 10 pts, you get -10) In most cases, F in the course. Every offense will be referred to the Office of Student Judicial Affairs. www.eecs.berkeley.edu/Policies/acad.dis.shtml EE40 Summer 2010 Hug 29 About Me (Josh Hug) 6th year graduate student Research on Biological Systems How Bacillus subtilis makes decisions Math is the same as well use in this class One day, maybe a Teaching Professor My HW0 is available online! EE40 Summer 2010 Hug 30 My Goal as an Instructor To make your time in EE40 as fun and informative as I can Make lectures interesting and timely Bring out the beauty and make clear the usefulness of the material Give secrets to getting good grades To get a 7.0 with HKN This is my first class, be gentle Ill need your feedback as much as possible EE40 Summer 2010 Hug 31 Friday Lunch Every Friday after class Email me at least a day in advance so that I am not overbooked EE40 Summer 2010 Hug 32 Teaching Staff GSI/TAs: Onur Ergen Cooper Levy Readers/Lab Assistants: Jonathan Lin Tony Dear EE40 Summer 2010 Hug 33 Topic 1 Fundamentals of Electronic Circuits EE40 Summer 2010 Hug 34 Topic 1 Outline Electrical quantities Charge, Current, Voltage, Power The ideal basic circuit element Circuit schematics Sign conventions Mostly a review of Physics 7B EE40 Summer 2010 Hug 35 Etymology The word electric is derived from the Greek elektron (Latin electrum) denoting amber. It was discovered in ancient times that when amber is rubbed it attracts feathers, dried leaves, etc. This is due to the amber becoming charged (discovered much later). These are the roots of our subject. EE40 Summer 2010 Hug 36 Common Sense If we take a AA battery and a paperclip and connect the two terminals, it heats up If we stick the same paperclip into the wall outlet and get it to actually stay there, it will heat up much more (and then melt) This heat is due to the flow of electrical current driven by the voltage provided by the source As electrons bump into neighboring electrons, they get jostled around. This is exactly what heat is EE40 Summer 2010 Hug 37 Intuition Test and a break We decide to stick a piece of wire in a nearby electrical outlet to heat our room. We have a choice of many different thicknesses of wire to use. Assume that resistance scales inversely with diameter of the wire, i.e. Rwire=constant/diameter Assuming our wire wont melt, if we wish to maximize the amount of heat generated, which wire should we choose: A. The thinnest wire B. The thickest wire C. Some medium wire EE40 Summer 2010 Hug 38 The Universe Electric charges exert forces on other electric charges, according to Coulombs Law: The part of the universe we care about is made up of atoms composed of these charges Negative charges (electrons) orbiting a positively charged nucleus in discrete (i.e. quantum) orbits EE40 Summer 2010 Hug 39 Atomic Structure Electrons are organized into orbitals, basically a nested set of shells If you rememeber high school chemistry: Neons electronic subshells: 1s22s22p6 The existence of these shells plays a key role in conductivity. It is hard to give an electron to someone with no room to hold it. EE40 Summer 2010 http://www.iq.poquoson.org/6sci/atoms/neonA.gif Hug 40 Matter Atoms agglomerate into solids, liquids, and gases Typically, most objects in the world are neutrally charged Exceptions: clouds in a thunderstorm, people on carpets in dry weather, rubbed amber, plates of a charged capacitor, etc. When there is an imbalance of charge, there are forces (Coulombs Law) Static cling Current through a wire EE40 Summer 2010 Hug 41 Classification of Materials: Insulators Solids in which all electrons are tightly bound to atoms are insulators. e.g. Neon: applying an electric field will tend to do little, because it is hard for an electron to move in to your neighbors valence shell. EE40 Summer 2010 Hug 42 CoM : Metals and Semiconductors Solids in which the outermost atomic electrons are free to move around are metals Metals typically have ~1 free electron per atom ~5 1022 free electrons per cubic cm Electrons in semiconductors are not tightly bound, nor are they free, but can be easily promoted to a free state insulators semiconductors metals Quartz, SiO2 Si, GaAs Al, Cu poor conductors EE40 Summer 2010 excellent conductors Hug 43 Abstraction Though a detailed quantum mechanical formulation would be the most accurate choice, it would be hard to use Thinking of 1023+ atoms composed of charged subatomic particles each with their own individual state is too much Well instead lump large objects like a battery into more abstract Likewise, pieces we will treat current as a bulk flow of charges EE40 Summer 2010 Hug 44 Current Electrical Current is simply a measure of the net amount of positive charge that passes a plane in space per second in a reference direction For convenience, the base unit is 1 Ampere, which is 1.6x1019 charges/sec or 1 Coulomb/sec EE40 Summer 2010 Hug 45 A Plane in Space? Net amount of positive charge passing a plane in space in a reference direction Analogous to measuring river flow Dont care how much total water is moving throughout the entire length of a river Do care about how much water is passing a given point on the shore per second Current = speed of water * cross section of river Cross section is the plane in space We care about the plane perpendicular to flow ? EE40 Summer 2010 Hug 46 Electric Current Examples 1. 105 positively charged hydrogen ions (each with charge 1.610-19 C) pass the perpendicular plane in space to the right (+x direction) every nanosecond. What is the current to the right? 2. 105 electrons (each with charge -1.610-19 C) pass the perpendicular plane in space to the right (+x direction) every nanosecond. What is the current to the right? Current is net positive charges to the right, so EE40 Summer 2010 Hug 47 Electric Current Summary Definition: Rate of positive charge flow in a reference direction Symbol: I Units: Ampere (A) = 1 Coulomb/second Simply the net amount of charge/second passing through a plane perpendicular to the direction of flow EE40 Summer 2010 Hug 48 Current Density Definition: rate of positive charge flow per unit area Symbol: J Units: A / cm2 Example 1: Wire attached to end Suppose we force a electron current of 1 A to flow from C1 to C2, what is the current density: Electron flow is in -x direction through 2cm2 cross section: -0.5 A/cm2 EE40 Summer 2010 Hug 49 Voltage The voltage between two points in space is simply the amount of energy (in Joules) that it would take to move 1 Coulomb of charge between those two points Example: There is a uniform electric field pulling electrons to the left at 9.8 Newtons/Coulomb. How much energy would it take to move this charge 2 meters to the right? Energy=Force*Distance EE40 Summer 2010 Hug 50 Analogy to Gravity Example: There is a uniform gravitational field pulling some matter downwards at 9.8 Newtons/kg. How much energy/kg would it take to move this matter 2 meters upwards? EE40 Summer 2010 Hug 51 Electric Potential (Voltage) Definition: energy per unit charge Symbol: v Units: Joules/Coulomb Volts (V) v = dw/dq Alessandro Volta (17451827) where w = energy (in Joules), q = charge (in Coulombs) Note: Potential is always referenced to some point. a b EE40 Summer 2010 Subscript convention: vab means the potential at a minus the potential at b. vab va - vb Hug 52 Electric Power Definition: transfer of energy per unit time Symbol: p Units: Joules per second Watts (W) p = dw/dt = (dw/dq)(dq/dt) = vi Concept: As a positive charge q moves through a drop in voltage v, it loses potential energy Voltage is Joules/Coulomb Current is Coulombs/second Power is the product of these EE40 Summer 2010 Hug 53 Summary So far: Current: Number of positive charges per second passing a plane in a particular direction Current density: Current per unit area Voltage: Amount of energy per Coulomb to move a charge between two points Power: Amount of energy per second Where do these quantities arise? When we build networks of electrical components EE40 Summer 2010 Hug 54 Power Sources We want to get charges moving in a controlled fashion Generate heat Turn motors Perform computation Store entire corpus of written human work in easily transmittable format It is easier to build a source which provides an almost constant voltage as opposed to an almost constant current (more on this later) EE40 Summer 2010 Hug 55 Voltage Sources One of the fundamental devices in electrical engineering is the voltage source Batteries Generators Provide a consistent voltage difference between two points in space If a charge is at the top of the voltage, a force will try to move it towards the bottom EE40 Summer 2010 Hug 56 Voltage Sources Positive and negative charges will move in opposite directions given the same voltage Positive terminal of a voltage source High potential for a positive charge Low potential for a negative charge EE40 Summer 2010 Hug 57 Our First Circuit Imagine that we have an ideal voltage source connected to a piece of metal. What happens? Electrons at the negative terminal travel towards the positive terminal These electrons will encounter some resistance as they travel generating heat The current of the electrons will be a function of this resistance and the original voltage EE40 Summer 2010 Hug 58 Ohms Law Ohm* discovered in 1825 that for many materials, voltage and current are related by a simple linear relationship: V=IR Here the resistance is a bulk property of the object connecting the two terminals of a voltage source and is empirically derived Measured in Ohms Any material which obeys Ohms Law is called a resistor *: Cavendish was first in 1781, but didnt publish. Take note. EE40 Summer 2010 Hug 59 Ohms Law Ohms law doesnt always work Consider your wall outlet with terminals connected by a gaseous mixture of mostly nitrogen and oxygen There is no current flow With a high enough voltage, called the breakdown voltage, current will eventually flow (via a spark, a.k.a. lightning) Such phenomena are beyond the scope of this course EE40 Summer 2010 Hug 60 Circuit Schematics Ohms law paved the way for simple circuit schematics We can model circuits as a series of interconnected discrete components or ideal basic circuit elements For now, each component can be characterized with a single physical parameter EE40 Summer 2010 Hug 61 The Ideal Basic Circuit Element i + v _ Polarity reference for voltage can be indicated by plus and minus signs Reference direction for the current is indicated by an arrow Attributes: Two terminals (points of connection) Device model gives us current/voltage relationship (I-V Characteristic) Cannot be subdivided into other elements EE40 Summer 2010 Hug 62 Example Circuit Element: Resistor Resistor: Circuit element where the voltage across the element is linearly proportional to the amount of current flowing through the device i + v _ v i The slope must be positive and the characteristic must go through the origin. EE40 Summer 2010 Hug 63 Example Circuit Element: Voltage Source Voltage Source: Circuit element that maintains a prescribed voltage across its terminals, regardless of the current flowing in those terminals Voltage is known, but current is determined by the circuit to which the source is connected A battery can be approximated by a voltage source EE40 Summer 2010 Hug 64 I-V Characteristic of Ideal Voltage Source a + Vab _ i i + _ vs i=0 v b Vs>0 Voltage is known, but current is determined by the circuit to which the source is connected EE40 Summer 2010 Hug 65 Circuit Schematics Combinations of ideal basic circuit elements A (high resistance) paperclip connecting the terminals of a 10 volt battery can be schematically represented as shown below EE40 Summer 2010 Hug 66 Larger Circuit Schematics We can compose these components into an arbitrary network For much of the semester we will discuss how to convert these networks into a system of algebraic (and later differential) equations The solution will give us the current and voltage between any two terminals in an arbitrary network EE40 Summer 2010 Hug 67 Example Problem Structure Find the voltage V1 and current I2 Note that the problem statement assumes a certain reference direction for currents and voltages If you find that the reference direction is wrong, just note your answer as negative EE40 Summer 2010 Hug 68 Reference Example Find the current I1 I1 Magnitude of the current is obviously 10V/100 or 0.1 Amps. Current flows from positive to negative, so reference current is wrong. Answer is -0.1 Amps EE40 Summer 2010 Hug 69 Reference Directions and Sign Conventions The minus sign is just shorthand for its going the other way than the one you asked for Like asking how fast is your plane moving in the direction of New York? when youre flying away from New York Could say 500 mph, but the other direction Or just minus 500 mph If you get confused on sign conventions at any point in the course, just step back and think about what is reasonable EE40 Summer 2010 Hug 70 Sign Convention Example Suppose you have an unlabelled battery and you measure its voltage with a digital voltmeter (DVM). It will tell you the magnitude and sign of the voltage. With this circuit, you are measuring vab. The DVM indicates 1.401, so va is lower than vb by 1.401 V. + EE40 Summer 2010 Which is the positive battery terminal? Hug 71 Sign Convention for Power If P > 0 for a circuit element Consuming power (as heat, light, motion, etc) If P < 0 for a circuit element Providing power Resistors always consume power Voltage sources may consume or provide power EE40 Summer 2010 Hug 72 Sign Convention for Power Remember earlier that we said P=VI This can be problematic depending on the chosen reference directions + V1 I1 P=VI=10 V * (-0.1 Amps) = -1 Watt EE40 Summer 2010 Resistor providing power?? Hug 73 Sign Convention for Power Well have to revise P=VI to take into account this reference direction problem + V1 I1 EE40 Summer 2010 Hug 74 Sign Convention for Power Passive sign convention p = vi p = -vi i + v _ i _ v + Current from + to i + v _ i _ v + Current from to + If p > 0, power is being delivered to the box. If p < 0, power is being extracted from the box. EE40 Summer 2010 Hug 75 Sign Convention for Power For this circuit, since reference current is in the opposite direction of reference voltage in the resistor, then P=-VI + V1 I1 P=VI=-10 V * (-0.1 Amps) = 1 Watt EE40 Summer 2010 All is well Hug 76 Summary Current = rate of charge flow Voltage = energy per unit charge created by charge separation Power = energy per unit time Ideal Basic Circuit Element 2-terminal component that cannot be sub-divided Described mathematically in terms of its terminal voltage and current Circuit Schematics Networks of ideal basic circuit elements Equivalent to a set of algebraic equations Solution provides voltage and current through all elements of the circuit EE40 Summer 2010 Hug 77 iClickers Once More We decide to stick a piece of wire in a nearby electrical outlet to heat our room. We have a choice of many different thicknesses of wire to use. Assume that resistance scales inversely with diameter of the wire, i.e. Rwire=constant/diameter Assuming our wire wont melt, if we wish to maximize the amount of heat generated, which wire should we choose: A. The thinnest wire B. The thickest wire C. Some medium wire EE40 Summer 2010 Hug 78 Acknowledgements Dan Garcia, Babak Ayazifar, Mike Clancy for help in CS302 (a course in course design) Slides and Course Organization: Tsu Jae King Connie Chang-Hasnain Octavian Florescu Brian Gawalt Bernhard Boser Labs Bernhard Boser EE40 Summer 2010 Hug 79 Extra Slides Extra slides youre responsible for knowing about, but which I wont talk about in class for lack of time EE40 Summer 2010 Hug 80 EE40 Content (Detailed Version) Fundamental Circuit Concepts and Analysis Techniques Networks of power sources and resistors Op-amps Signal amplification Conversion of circuit schematics into algebraic equations Circuits with Energy Storage Elements Capacitors Inductors Filtering Conversion of circuit schematics into differential equations Semiconductors and Integrated Circuits Basic semiconductor devices Diodes Transistors Logic gates Textbook Foundation of Analog and Digital Electronic Circuits, Anant Agarwal and Jeffrey Lang, Morgan Kaufman, 1st Edition EE40 Summer 2010 Hug 81 Final Grade Distribution subject to change before first midterm Grading: 800 pts total 120pts = 15% Labs 160pts = 20% Homework 320pts = 40% Two midterms (each 20%) 160 pts= 20% Final 40 pts = 5% Reading Assignments + Extra credit for EPA. Whats EPA? Grade distributions Pseudo-Absolute Scale Perfect score is 1000 points. 25-60-25 for A+, A, ASimilar for Bs and Cs (110 pts per letter-grade) C+, C, C-, D, F (No D+ or D- distinction) Exception: No F will be given if all but one hw and labs are completed and all exams taken Well ooch grades up but never down EE40 Summer 2010 Hug 82 Weekly Calendar EE40 Summer 2010 Hug 83 Core EE Courses Input Signals Systems Modeling System Architecture Circuit Input/Output Response Silicon EE20 EE40 Circuit Modeling Device Modeling Copper EE40 Summer 2010 Output Signals Other Materials Device Response Hug 84
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Berkeley - EE 40 - 40
Getting Started Announcements, instructions, and coursedocuments onhttp:/inst.eecs.berkeley.edu/~ee40/ Also linked with Bspacehttps:/bspace.berkeley.edu Discussion sections, lab sections, andoffice hours will begin next week. Readprelab instructio
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Lab 20Jia jie huo(10780081)Result and Discussion:In part 1, we prepared 250ml of 0.1M KHP by transferring 5.334g KHP into a250ml flask and adding water into it until full. We got the actual molarity of KHPsolution is 0.1045mol/L. In part 2, we added
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Lab2Motion with Constant AccelerationInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Tran, TranTrum NguyenSean CloughAnhuang HerncnlzDana Feuiez2. introduction.In this experiment, we are generally focusing on measuring themoving of the metal rou
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Lab3Projectile MotionInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Tran, TranTrum NguyenSean CloughAnhuang HerncnlzDana Feuiez2. introduction.In this experiment, we are generally focusing on measuring themoving of the metal projected from the
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Lab5Force of FrictionInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Tran, TranTrum NguyenSean CloughAnhuang HerncnlzDana Feuiez2. introduction.In this experiment, we are generally focusing on exploring thefriction of the object by trying to pul
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Lab6VectorsInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Tran, TranTrum NguyenSean CloughAnhuang HerncnlzDana Feuiez2. introduction.In this experiment, we are generally focusing on exploring thecombination or separation of the vectors and tryi
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Lab7Work and EnergyInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Tran, TranTrum NguyenSean CloughAnhuang HerncnlzDana Feuiez2. introduction.In this experiment, we are generally focusing onconfirming the work-energy theorem, by comparing the wo
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Lab12EquilibriumInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Tran, TranTram NguyenAnhuang HerncnlzDana Feuiez2. introduction.In this experiment, we are generally focusing on measuring theperiod ofa pendulum and comparing the results with theor
Laney College - PHYSICS - 1A+1B
Lab12EquilibriumInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Tran, TranTram NguyenAnhuang HerncnlzDana Feuiez2. introduction.In this experiment, we are generally focusing on measuring theperiod ofa pendulum and comparing the results with theor
Laney College - PHYSICS - 1A+1B
Lab2Specific HeatInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Ruihong XiaoTEJ ShiwakotiAnthony HernandezDana SaiezRneiang Ye2. introduction.In this experiment, we are generally focusing on finding specificheat and molar specific heat for Al,
Laney College - PHYSICS - 1A+1B
Lab3Latent HeatInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Ruihong XiaoTEJ ShiwakotiAnthony HernandezDana SaiezRneiang YeWAJIH RAHMAN2. introduction.In this experiment, we are generally focusing on Measuring thelatent heat of fusion for wat
Laney College - PHYSICS - 1A+1B
Lab4Static Electric ChargeInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Ruihong XiaoTEJ ShiwakotiAnthony HernandezDana SaiezRneiang YeWAJIH RAHMAN2. introduction.In this experiment, we are generally focusing on determining therelatice effecti
Laney College - PHYSICS - 1A+1B
Lab6CapacitanceInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Ruihong XiaoTEJ ShiwakotiAnthony HernandezDana SaiezRneiang YeWAJIH RAHMAN2. introduction.In this experiment, we are generally focusing on definingcapacitance and learning to measur
Laney College - PHYSICS - 1A+1B
Lab6CapacitanceInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Ruihong XiaoTEJ ShiwakotiAnthony HernandezDana SaiezRneiang YeWAJIH RAHMAN2. introduction.In this experiment, we are generally focusing on definingcapacitance and learning to measur
Laney College - PHYSICS - 1A+1B
Lab7ResistenceInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Ruihong XiaoTEJ ShiwakotiAnthony HernandezDana SaiezRneiang YeWAJIH RAHMAN2. introduction.In this experiment, we are generally focusing on measuring theresistance of four objects usi
Laney College - PHYSICS - 1A+1B
Lab8Electric CurrentInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Ruihong XiaoTEJ ShiwakotiAnthony HernandezDana SaiezRneiang YeWAJIH RAHMAN2. introductionIn this experiment, we are generally focusing on investatingOhms Law and Kirchhoffs rul
Laney College - PHYSICS - 1A+1B
Lab9Magnetic fieldInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Ruihong XiaoTEJ ShiwakotiAnthony HernandezDana SaiezRneiang YeWAJIH RAHMAN2. introductionIn this experiment, we are generally focusing on having someexperimental information abou
Laney College - PHYSICS - 1A+1B
Lab12Measuring the Inductance of an InductorInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Ruihong XiaoTEJ ShiwakotiAnthony HernandezDana SaiezRneiang YeWAJIH RAHMAN2. introductionIn this experiment, we are generally focusing on measuring thei
Laney College - PHYSICS - 1A+1B
Lab4Diffraction GratingsInstructor:Pro. TsaiJiajie Huo(Jacky)Member:Yao Bin YuZeyuan (Seth) Guan1. introduction.In this experiment, we are generally focusing on informationabout inference and diffraction.2. Procedure.a. In section 1, we align
Laney College - PHYSICS - 1A+1B
Lab3PolarizationInstructor:Pro. TsaiJiajie Huo(Jacky)Member:Yao Bin YuZeyuan (Seth) Guan1. introduction.In this experiment, we are generally focusing on learning thecharacteristics of polarization2. Procedure.In section 1, we aligned the lamp
Laney College - PHYSICS - 1A+1B
Lab4Diffraction GratingsInstructor:Pro. TsaiJiajie Huo(Jacky)Member:Yao Bin YuZeyuan (Seth) Guan1. introduction.In this experiment, we are generally focusing on informationabout inference and diffraction.2. Procedure.a. In section 1, we align
Laney College - PHYSICS - 1A+1B
Lab7Speed of lightInstructor:Pro. TsaiJiajie Huo(Jacky)Member:Yao Bin YuZeyuan (Seth) Guan1. introduction.In this experiment, we are generally focusing on using the mirrorreflection and deflation to measure to speed of light.2. Procedure.a. Fi
Laney College - PHYSICS - 1A+1B
Lab10ElectromagnetInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Ruihong XiaoTEJ ShiwakotiAnthony HernandezDana SaiezRneiang YeWAJIH RAHMAN1. introductionIn this experiment, we are generally focusing on measuring thevalue of permeability of fr
Laney College - PHYSICS - 1A+1B
Lab1Absolute ZeroInstructor:Dr. MohebiJiajie Huo(Jacky)Member:Ruihong XiaoTEJ ShiwakotiAnthony HernandezDana SaiezRneiang Ye2. introduction.In this experiment, we are generally focusing on finding specificheat and molar specific heat for Al,
Laney College - PHYSICS - 1A+1B
Section2Angle(relative)Max=540lm 2rd one is at 59 degreeIntensity(lm)0540154603040345345602727522290212105222120274135316150389165424180448Section 3 1st=0degree2nd =90degree3rd=10 degree max=165lmAngle(relative) Intensity(
Laney College - PHYSICS - 1A+1B
RodrobberplasticrobberplasticglassplasticMeasured DateCalculationMaterialD(cm) m(g) L(m) angle(o) Q(c)NeMicrother0 0.1 0.1930silk1.6 0.1 0.1934.8 1.10E-09 6.88E+09silk0 0.1 0.1930silk1.2 0.1 0.1933.6 7.00E-10 4.38E+09microther0 0.
Laney College - PHYSICS - 1A+1B
Seperation(page)2368101214Seperation,d(m)1.04E-032.08E-033.12E-034.16E-035.20E-036.24E-037.28E-031/d(m-1)9.62E+024.81E+023.21E+022.40E+021.92E+021.60E+021.37E+02Capacitance1.37E-085.10E-092.76E-092.40E-092.34E-091.85E-091.63
Laney College - PHYSICS - 1A+1B
current(ma)Poten diff(V)10.60.00422.50.01637.20.047439.60.26559.20.39695.20.6287127.90.8378170.71.086V vs I1.2Current (ma)Pot Dif (V)Current (ma)4.410.313.119.322.32533.34651102.4117.1122.5132.6140.3153.2162.3
Berkeley - EE 105 - EE105
Lecture 2OUTLINE Semiconductor BasicsReading: Chapter 2EE105 Fall 2011Lecture 2, Slide 1Prof. Salahuddin, UC BerkeleyAnnouncement Office Hours for tomorrow is cancelled(ONLY for this week)There will be office hours on Friday (2P-3P)(ONLY for th
Berkeley - EE 105 - EE105
Lecture 4OUTLINE PN Junction Diodes Electrostatics Capacitance I/V Reverse Breakdown Large and Small signalmodelsReading: Chapter 2.2-2.3,3.2-3.4EE105 Fall 2010Lecture 4, Slide 1Prof. Salahuddin, UC BerkeleyEnergy Band DescriptionEE105 Fall
Berkeley - EE 105 - EE105
Lecture 5OUTLINE PN Junction Diodes I/V Capacitance Reverse Breakdown Large and Small signalmodelsReading: Chapter 2.2-2.3,3.2-3.4EE105 Fall 2011Lecture 5, Slide 1Prof. Salahuddin, UC BerkeleyRecap: Law of the JunctionLaw of the junction:n(a
Berkeley - EE 105 - EE105
EE105Microelectronic Devices andCircuitshttp:/wwwinst.eecs.berkeley.edu/~ee105Prof. Sayeef Salahuddinsayeef@eecs.berkeley.edu515 Sutardja Dai HallTeaching StaffSayeef SalahuddinProfessor@ Berkeley since Fall 2008Courses: EE 230, EE105Office Hou
Berkeley - EE 105 - EE105
EE-105-Fall-2011COURSE SYLLABUS AND TENTATIVE SCHEDULE FALL 2010WeekDayLectureDate1118/25Introduction. Basic Semiconductor Physics: charge carriers, doping,1, 2.12228/302.2339/1carrier drift &amp; diffusion.pn Junction Diodes: electrostat
The Chinese University of Hong Kong - MATHEMATIC - MAT2310
THE DIHEDRAL GROUPS DnSome authors use D2n to denote the n-th dihedral group. An excellent referencefor dihedral groups is the textbook Algebra by Michael Artin, Chapter 5.Let n 3. Let Dn be the set of all symmetries of a regular n-gon. More precisely,
The Chinese University of Hong Kong - MATHEMATIC - MAT2310
The Chinese University of Hong Kong - MATHEMATIC - MAT2310
The Chinese University of Hong Kong - MATHEMATIC - MAT2310
The Chinese University of Hong Kong - MATHEMATIC - MAT2310
The Chinese University of Hong Kong - MATHEMATIC - MAT2310
The Chinese University of Hong Kong - MATHEMATIC - MAT2310
The Chinese University of Hong Kong - MATHEMATIC - MAT2310
The Chinese University of Hong Kong - MATHEMATIC - MAT2310
The Chinese University of Hong Kong - MATHEMATIC - MAT2310
The Chinese University of Hong Kong - MATHEMATIC - MAT2310