CIRCUITS AND ELECTRONICS. Introduction and Lumped Circuit Abstraction

Transcription

1 6.002 CIRCUITS AND ELECTRONICS Introduction and Lumped Circuit Abstraction

2 ADMINISTRIVIA Lecturer: Prof. Anant Agarwal Textbook: Agarwal and Lang (A&L) Readings are important! Handout no. 3 Web site Assignments Homework exercises Labs Quizzes Final exam

3 Two homework assignments can be missed (except HW11). Collaboration policy Homework You may collaborate with others, but do your own write-up. Lab You may work in a team of two, but do you own write-up. Info handout Reading for today Chapter 1 of the book

4 What is engineering? Purposeful use of science What is about? Gainful employment of Maxwell s equations From electrons to digital gates and op-amps

5 Nature as observed in experiments V 3 6 I Physics laws or abstractions Maxwell s abstraction for Ohm s tables of data V = R I Lumped circuit abstraction + R V C L M S Simple amplifier abstraction Operational amplifier abstraction abstraction + - Filters Digital abstraction Combinational logic Clocked digital abstraction f Analog system components: Modulators, oscillators, RF amps, power supplies Instruction set abstraction Pentium, MIPS Programming languages Java, C++, Matlab Software systems Operating systems, Browsers Mice, toasters, sonar, stereos, doom, space shuttle

6 Lumped Circuit Abstraction Consider I The Big Jump from physics to EECS V? Suppose we wish to answer this question: What is the current through the bulb?

7 We could do it the Hard Way Apply Maxwell s Differential form Integral form Faraday s Continuity Others E J E B = t ρ = t = ε ρ 0 φb E dl = t q J ds = t q E ds = ε 0

8 Instead, there is an Easy Way First, let us build some insight: Analogy F a? I ask you: What is the acceleration? You quickly ask me: What is the mass? I tell you: You respond: m a = F m Done!!!

9 Instead, there is an Easy Way First, let us build some insight: Analogy F a? In doing so, you ignored the object s shape its temperature its color point of force application Point-mass discretization

10 The Easy Way Consider the filament of the light bulb. A B We do not care about how current flows inside the filament its temperature, shape, orientation, etc. Then, we can replace the bulb with a discrete resistor for the purpose of calculating the current.

11 The Easy Way A B Replace the bulb with a discrete resistor for the purpose of calculating the current. A I + V R and I = V R B In EE, we do things the easy way R represents the only property of interest! Like with point-mass: replace objects F with their mass m to find a = m

12 The Easy Way A + V I R and V I = R B In EE, we do things the easy way R represents the only property of interest! R relates element v and i V I = R called element v-i relationship

13 R is a lumped element abstraction for the bulb.

14 R is a lumped element abstraction for the bulb. Not so fast, though I A + V S A B S B black box Although we will take the easy way using lumped abstractions for the rest of this course, we must make sure (at least the first time) that our abstraction is reasonable. In this case, ensuring that V I are defined for the element

15 A B I + V S A S B V I must be defined for the element black box

16 I must be defined. True when I into S = I out of A SB True only when q = 0 t in the filament! J ds S A from Maxwell J ds S B J ds q I A = I B only if = 0 t So let s assume this A B J ds q = t S S I A I B

17 V Must also be defined. see A & L So let s assume this too So φ VAB defined when B = 0 t VAB = E dl outside elements AB

18 Lumped Matter Discipline (LMD) Or self imposed constraints: More in Chapter 1 of A & L φ B t q t = 0 = 0 outside inside elements bulb, wire, battery Lumped circuit abstraction applies when elements adhere to the lumped matter discipline.

19 Demo only for the sorts of questions we as EEs would like to ask! Lumped element examples whose behavior is completely captured by their V I relationship. Demo Exploding resistor demo can t predict that! Pickle demo can t predict light, smell

20 So, what does this buy us? Replace the differential equations with simple algebra using lumped circuit abstraction (LCA). For example a V R1 + b R 3 d R 4 R 2 R 5 c What can we say about voltages in a loop under the lumped matter discipline?

21 What can we say about voltages in a loop under LMD? a V R1 + b R 3 d R 4 R 2 R 5 c φb E dl = under DMD t 0 E dl + E dl + E dl = 0 ca ab bc + ca + Vab + Vbc V = 0 Kirchhoff s Voltage Law (KVL): The sum of the voltages in a loop is 0.

22 What can we say about currents? Consider Ica S a Ida I ba

23 What can we say about currents? Ica S a Ida I ba I ca S J ds + Ida + Iba q = t = 0 under LMD 0 Kirchhoff s Current Law (KCL): The sum of the currents into a node is 0. simply conservation of charge

24 KVL and KCL Summary KVL: j ν loop j = 0 KCL: j i j = 0 node