Celso José Faria de Araújo, M.Sc.

Similar documents
9/12/2013. Microelectronics Circuit Analysis and Design. Modes of Operation. Cross Section of Integrated Circuit npn Transistor

(8) Gain Stage and Simple Output Stage

6. Introduction to Transistor Amplifiers: Concepts and Small-Signal Model

Physics Exam II Chapters 25-29

CHAPTER 3 DIODES. NTUEE Electronics L. H. Lu 3-1

CHAPTER 13. Exercises. E13.1 The emitter current is given by the Shockley equation:

Chapter 13 - Universal Gravitation

Amplifier Constant Gain and Noise

III. Electromechanical Energy Conversion

TEST-03 TOPIC: MAGNETISM AND MAGNETIC EFFECT OF CURRENT Q.1 Find the magnetic field intensity due to a thin wire carrying current I in the Fig.

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M

Dynamics of Rigid Bodies

Driving your LED s. LED Driver. The question then is: how do we use this square wave to turn on and turn off the LED?

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o?

Chapter 8. Linear Momentum, Impulse, and Collisions

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1

Scalars and Vectors Scalar

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. "Flux": = da i. "Force": = -Â g a ik k = X i. Â J i X i (7.

rectangle, triangle, saw tooth, pulse, etc.

24-2: Electric Potential Energy. 24-1: What is physics

CIRCUITS 1 DEVELOP TOOLS FOR THE ANALYSIS AND DESIGN OF BASIC LINEAR ELECTRIC CIRCUITS

Physics Exam 3

Physics 1501 Lecture 19

UNIT # 08 CURRENT ELECTRICITY

THE EQUIVALENCE OF GRAM-SCHMIDT AND QR FACTORIZATION (page 227) Gram-Schmidt provides another way to compute a QR decomposition: n

Unconventional double-current circuit accuracy measures and application in twoparameter

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints.

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering

6. CURRENT ELECTRICITY

CSJM University Class: B.Sc.-II Sub:Physics Paper-II Title: Electromagnetics Unit-1: Electrostatics Lecture: 1 to 4

ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.

Event Shape Update. T. Doyle S. Hanlon I. Skillicorn. A. Everett A. Savin. Event Shapes, A. Everett, U. Wisconsin ZEUS Meeting, October 15,

3. A Review of Some Existing AW (BT, CT) Algorithms

Chapter 6. Operational Amplifier. inputs can be defined as the average of the sum of the two signals.

Physics 2A Chapter 11 - Universal Gravitation Fall 2017

Rotating Disk Electrode -a hydrodynamic method

Chapter I Matrices, Vectors, & Vector Calculus 1-1, 1-9, 1-10, 1-11, 1-17, 1-18, 1-25, 1-27, 1-36, 1-37, 1-41.

Remember: When an object falls due to gravity its potential energy decreases.

19 The Born-Oppenheimer Approximation

PHYS Week 5. Reading Journals today from tables. WebAssign due Wed nite

EE 5337 Computational Electromagnetics (CEM)

Week 11: Differential Amplifiers

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in

P 365. r r r )...(1 365

Phys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Lesson 8: Work, Energy, Power (Sections ) Chapter 6 Conservation of Energy

3.5 Rectifier Circuits

A. Thicknesses and Densities

I = α I I. Bipolar Junction Transistors (BJTs) 2.15 The Emitter-Coupled Pair. By using KVL: V

COMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS

UNIT10 PLANE OF REGRESSION

Objectives. Chapter 6. Learning Outcome. Newton's Laws in Action. Reflection: Reflection: 6.2 Gravitational Field

55:041 Electronic Circuits

Graphical Analysis of a BJT Amplifier

Contact, information, consultations

Chapter Fifiteen. Surfaces Revisited

2 dependence in the electrostatic force means that it is also

Physics 207 Lecture 16

1. A body will remain in a state of rest, or of uniform motion in a straight line unless it

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

3.1 Electrostatic Potential Energy and Potential Difference

Stellar Astrophysics. dt dr. GM r. The current model for treating convection in stellar interiors is called mixing length theory:

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems

Faraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law

BASIC ELECTRICAL CIRCUITS AND ANALYSIS. Ref: Horowitz, P, & W. Hill, The Art of Electronics, 2nd. ed., Cambridge (1989).

Chapter 12 Equilibrium and Elasticity

Chapter 2 ONE DIMENSIONAL STEADY STATE CONDUCTION. Chapter 2 Chee 318 1

1.4 Small-signal models of BJT

Physics 202, Lecture 2. Announcements

T-model: - + v o. v i. i o. v e. R i

Multipole Radiation. March 17, 2014

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution

Density Functional Theory I

Chapter 2 Problem Solutions 2.1 R v = Peak diode current i d (max) = R 1 K 0.6 I 0 I 0

Electrical Circuits II (ECE233b)

MECHANICAL PULPING REFINER MECHANICAL PULPS

Copyright 2004 by Oxford University Press, Inc.

Linearity. If kx is applied to the element, the output must be ky. kx ky. 2. additivity property. x 1 y 1, x 2 y 2

Part V: Velocity and Acceleration Analysis of Mechanisms

4 Recursive Linear Predictor

CSU ATS601 Fall Other reading: Vallis 2.1, 2.2; Marshall and Plumb Ch. 6; Holton Ch. 2; Schubert Ch r or v i = v r + r (3.

Transistors. Lesson #10 Chapter 4. BME 372 Electronics I J.Schesser

Energy in Closed Systems

Diode. Current HmAL Voltage HVL Simplified equivalent circuit. V γ. Reverse bias. Forward bias. Designation: Symbol:

Insulated Bearings MEGAOHM TM Series

5-99C The Taylor series expansion of the temperature at a specified nodal point m about time t i is

Rigid Bodies: Equivalent Systems of Forces

Power efficiency and optimum load formulas on RF rectifiers featuring flow-angle equations

Design of CMOS Analog Integrated Circuits. Basic Building Block

Boise State University Department of Electrical and Computer Engineering ECE 212L Circuit Analysis and Design Lab

V V. This calculation is repeated now for each current I.

KIRCHHOFF CURRENT LAW

The geometric construction of Ewald sphere and Bragg condition:

iclicker Quiz a) True b) False Theoretical physics: the eternal quest for a missing minus sign and/or a factor of two. Which will be an issue today?

A new force Magnetic force. Today. Force Fields: A disturbance of space. The correspondence of a loop of current and magnet.

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other

EKT 356 MICROWAVE COMMUNICATIONS CHAPTER 2: PLANAR TRANSMISSION LINES

Experiment I Voltage Variation and Control

Active Load. Reading S&S (5ed): Sec. 7.2 S&S (6ed): Sec. 8.2

Transcription:

Celso José Faa de Aaújo, M.c.

he deal dode: (a) dode ccut symbol; (b) - chaactestc; (c) equalent ccut n the eese decton; (d) equalent ccut n the fowad decton. odes

(a) Rectfe ccut. (b) nput waefom. (c) Equalent ccut when (d) Equalent ccut when 1 0 (e) Output waefom. odes

odes Examples (deal ode) OE LOGC GAE BAERY-LOA CRCU ( snusodal) he cuent flew to battey though dode at 20% of nput sgnal peod whose mean alue s 100mA. (a) pp =? (b)r=? (c) (Peak) =?

odes mplfed physcal stuctue of the juncton dode.

(a) he pn juncton wth no appled oltage (open-ccuted temnals). (b) he potental dstbuton along an axs pependcula to the juncton. odes

(a) (b) (a) he pn juncton excted by a constant-cuent souce n the eese decton. o aod beakdown, s kept smalle than s. Note that the depleton laye wdens and the bae oltage nceases by olts, whch appeas between the temnals as a eese oltage. (b) he pn juncton excted by a constant-cuent souce supplyng a cuent n the fowad decton. he depleton laye naows and the bae oltage deceases by olts, whch appeas as an extenal oltage n the fowad decton. odes

odes he dode - elatonshp wth some scales expanded and othes compessed n ode to eeal detals.

n s e 1 s n e fo = hemal oltage he Fowad-Bas Regon = atuaton Cuent s a constant fo a gen dode at a gen tempeatue. t s also called cale n 0.5 ln k Cuent due to fact that s dectly popotonal to the coss-sectonal aea of de dode. s of the ode of 10 15 A. q 2.3 n log k = Boltzmann s constant = 1.38x10 23 Joules/Keln = the absolute tempeatue n Keln q = the magntude of electonc chage = 1.60x10 19 Coulomb (20 o )=25.2m 25m 1 n 2 n=1 standad ntegated-ccut and n=2 dscete twotemnal components. odes

40 35 30 25 20 15 10 5 4.5 n s e 1 5 4 0-5 -0.1 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 odes 3.5 2.5 1.5 0.5-0.5 0.5 0.525 0.55 0.575 0.6 0.625 0.65 0.675 0.7 0.725 0.75 Gaph of - chaactestc of a p-n juncton dode =1x10-15 A, n=1 and =25m 3 2 ode Cuent (ma) 12 11 10 9 8 7 6 5 4 3 2 1 0-1 -2-0.2-0.15-0.1-0.05 0 0.05 0.1 ode oltage () 1 ode Cuent (x10 15 A) ode Cuent (ma) ode oltage () 0 ode oltage ()

10 1 10 0 10-1 10-2 10-3 10-4 10-5 10-6 60m/ecade of Cuent n=1 ode Cuent (A) 10-7 10-8 10-9 10-10 120m/ecade of Cuent n=2 10-11 0.46 0.52 0.58 0.64 0.7 0.76 0.82 0.88 0.94 1 ode oltage () = 1x10-15 A = 25m ode - chaactestc on semlog scale odes ln 2 n 2.3 log 2 n 2.3 2.3 n n 25m; 25m; n n 1 2 0.0575 0.115 60m 120m 2 1 n ln 2 1 2.3 n log 2 1 2 1

n n e e n 1 ode 1(0.7 1mA) ode 2 1 2(0.7 1A) 1000 1 2 10 1 e 3 e 0.7 0.7 25m 25m 6.9x10 6.9x10 Aea( ode2) 1000 x Aea( ode 1 ) 12 x 10-13 13 A 16 A 1 10 8 0.8 6 4 ode 2 2 0 ode Cuent (A) 0.6 0.4 ode Cuent (A) 0.2-2 0-4 ode 1-0.2 0.5 0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9 ode oltage () n = 1 = 25m -6-0.2-0.15-0.1-0.05 0 0.05 0.1 0.15 0.2 ode oltage () n = 1 = 25m odes Example: Aea x cale Cuent

Fowad Bas Regon 1.6 x 10-3 ode (0.7 -- 1mA; n = 1 and =20 o ) 1.5 1.4 1.3 1.2 =21 o 1.1 1 0.9 =20 o ode Cuent (A) 0.8 0.7 0.6 0.69 0.692 0.694 0.696 0.698 0.7 0.702 0.704 0.706 0.708 0.71 ode oltage () Geneal ode 2m o C empeatue Effect odes Reese Bas Regon doubles fo eey 10 o C n tempeatue.

Execses (1) 1. Consde a slcon wth n=1.5. Fnd the change n oltage f cuent changes fom 0.1mA to 10mA. Ans. 172.5m 2. A slcon juncton dode wth n=1 has =0.7 at =1mA. Fnd the oltage dop at =0.1mA and =10mA. Ans. 0.64; 0.76 3. Usng the fact that a slcon dode has =10-14 A at 25 o C and that nceases by 15% pe o C se n tempeatue, fnd the alue of at 125 o C. Ans. 1.17x10-8 A 4. he dode n the ccut of fgue below s a lage, hgh-cuent dece whose eese leakage s easonably ndependent of oltage. f =1 at 20 o C, fnd the alue of at 40 o C and at 0 o C. Ans. 4; 0.25 odes

Execses (2) 1. Fo the ccut shown below, both dodes ae dentcal, conductng 10mA at 0,7 and 100mA at 0,8. Fnd the alue of R, fo whch =50m. 2. n the ccut shown below, both dodes hae n = 1, but 1 has ten tmes the juncton aea of 2. What alue of esults fo 1 of 1mA? o obtan a alue fo of 50m, what cuent 1 s needed? 3. A juncton ode s opeated n a ccut n whch t s suppled wth a constant cuent. What s the effect on the fowad oltage of the dode f an dentcal dode s connected n paallel? Assume n= 1. odes

odes Gaphcal Analyss

teate Analyss etemne the cuent and the dode oltage fo the ccut below wth =5 and R=1k. Assume that the dode has a cuent of 1mA at a oltage of 0.7 and that ts oltage dop changes by 0.1 fo eey decade change n cuent. Recuent Equaton: 2 0.7 0.1 log 1m o begn the teaton, we assume that =0.7 5 0.7 ' 4.3mA ' 0.7 0.1 log 1k 0.763 1k 4.3m 1m 5 '' 4.237mA '' 0.7 0.1 log ''' 5 0.7627 1k 0.7627 4.2373mA 4.2373mA ''' 0.7 0.1 log 0.763 4.237m 1m m 4.2373 1m 0.7627 0.7627 odes

Pecewse-lnea Model of the dode fowad chaactestc and ts equalent ccut epesentaton. odes

Example of Pecewse-lnea model of the dode fowad chaactestc. etemne the cuent and the dode oltage fo the ccut below wth =5 and R=1k, utlzng the pecewse-lnea model whose paametes ae gen n fgue below. O = 0.65 =20 5 1k O 0.65 20 4.26mA 0.65 4.26m 20 0.735 odes

he constant-oltage-dop model of the dode fowad chaactestc and ts equalent ccut epesentaton. etemne the cuent and the dode oltage fo the ccut below wth =5 and R=1k, utlzng the constant-oltage-dop model ( O = 0.7). 5 0.7 1k 4.3mA odes

Execses (3) 1. Fo the ccuts n Fg. below fnd and fo the case =5 and R=10K. Assume that the dode has a oltage of 0.7 at 1mA cuent that oltage changes by 0.1/decade of cuent change. Use (a) teaton (b) the pecewse-lnea model wth =20 and (c) the constant-oltage-dop model wth =0.7. Ans. (a) 0.434mA, 0.63; (b) 0.431mA, 0.689; (c) 0.43mA, 0.7. 2. Consde a dode that s 100 tmes as lage (n juncton aea) as a dode whose chaactestcs ae O =0.65 and =20 how would the model paametes O and change? Ans. O does not change; deceases by a facto of 100 to 0.2. 3. esgn the ccut n fgue below to pode an output oltage of 2.4. Assume that the dodes aalable hae 0.7 dop at 1mA and that =0.1/decade change n cuent. Ans. 760. odes

eelopment of the dode small-sgnal model. Note that the numecal alues shown ae fo a dode wth n = 2. d s a small-sgnal esstance o ncemental esstance d 1 e d d d n d n e e d n d n n n odes d e d d d n 1 d n d e d n Equalent ccut model fo the dode fo small changes aound bas pont Q. he ncemental esstance d s the nese of the slope of the tangent at Q, and 0 s the ntecept of the tangent on the axs.

(a) (b) (c) (d) he analyss of the ccut n (a), whch contans both dc and sgnal quanttes, can be pefomed by eplacng the dode wth the model of Fg. (a), as shown n (b). hs allows sepaatng the dc analyss [the ccut n (c)] fom the sgnal analyss [the ccut n (d)]. odes

Example of usng small-sgnal model (1) Consde the ccut shown n fg. below fo the case R=10K. he powe supply + has a C alue of 10 on whch s supemposed a 60Hz snusod of 1 peak ampltude (powe supply pple). Calculate both the C oltage of the dode and the ampltude of the sne-wae sgnal appeang acoss t. Assume the dode to hae a 0.7 dop at 1mA cuent and n=2. C analyss (we assume 10 0.7 0.93mA 10K 53.8Ω d AC analyss d d n (peak (peak) model s to 2 25m 0.93m peak) 5.35m p justfed. 2 d d R,snce d 0.7 2 ) 53.8 53.8 10k n the 10.7m small pp sgnal odes

odes Example of usng small-sgnal model (2) Consde the ccut shown n fg. below. A stng of thee dodes s used to pode a constant oltage of about 2.1. We want to calculate the pecentage change n ths egulated oltage caused by (a) 10% change n the powe-supply oltage and (b) connecton of a 1K load esstance. Assume n = 2. (a) C analyss 10 2.1 7.9mA 1K n 2 25m d 6.3Ω 7.9m 3 d 18.9Ω AC analyss 18.9 o 2 2 R 18.9 1k 18.5m o 0.9% o snce the d small p 6.2 m p sgnalmodel n 37.1m s pp justfed. O O (b) Fo all thee dodes the small-sgnal model we can use the paametes O =1.95 and d = 18.9 obtaned fom (a) analyss. 1 1 k //18.9 k //18.9 1 k 2.061 o 10 2.1 1k//1k 1k//1k 18.9 39m 1.95 2.061

Execses (4) 1. Fnd the alue of the dode small-sgnal esstance at bas cuent of 0.1, 1, and 10mA. Assume n=1. Ans. 250; 25; 2.5. 2. Fo a dode that conducts 1mA at a fowad oltage dop of 0.7 and whose n=1, fnd the equaton of the staght-lne tangent at =1mA. Ans. = (1/25)( -0.675). 3. Consde a dode wth n=2 based at 1mA. Fnd the change n cuent as a esult of changng the oltage by (a) 20m; (b) 10m; (c) -5m (d) +5m (e)+10m; (f) +20m. n each case, do the calculatons () usng the small-sgnal model and () usng the exponental model. Ans. (a) 0.40, -0.33mA; (b) 0.20, -0.18mA; (c) 0.10, -0.10mA; (d) +0.10, +0.11mA; (e) +0.20, +0.22mA; (f) +0.40, +0.49mA. 4. esgn the ccut of fg. below so that O =3 when L = 0, and O changes by 40m pe 1mA of load cuent. Fnd the alue of R and the juncton aea of each dode (assume all fou dodes ae dentcal) elate to a dode wth 0.7 dop at 1mA cuent. Assume n=1. Ans. R= 4.8k; 0.34. odes

Opeaton n the Reese Beakdown Regon-Zene odes. Model fo the zene dode. Ccut symbol fo a zene dode. he dode - chaactestc wth the beakdown egon shown n some detal. odes

Lne Load R mn Z mn ZO L z max odes esgn of the hunt Regulato egulaton egulaton O O L un un m/ m/ma Z mn O R R z ZO Lne Regulaton Load Regulaton z z R z z R ( //R) z ( //R) z L

Zeneode -Example he 6.8 zene dode n the ccut of fg. below s specfed to hae Z = 6.8 at Z = 5mA, z = 20, and ZK = 0.2mA. he supply oltage + s nomnally 10 but can ay by 1. (a) Fnd O wth no load and wth + at ts nomnal alue. (b) Fnd the change n O esultng fom the 1 change n +. (c) Fnd the change n O esultng fom connectng a load esstance R L = 2k. (d) Fnd the alue of O when R L = 0.5k. (e) What s the mnmum alue of R L fo whch the dode stll opeates n the beakdown egon? ZO O (a) (b) O O 6.8 20 5m 6.7 z z z O z // R 10 R R 6.83 O // R R L L R 10 R R // 6.76 (c) z z z R 6.7 O 38.5mA (d) // R R L L z 6.7 R 68m (e) L mn R O L 0.5k 0.5k 0.5k ( ZO ZK z ZO R ZK z ) ZK 1526 10 5 odes

odes Block agam of a C Powe upply.

o (C) ( o max ( O 1/π )/R ) O /2 ω t o (a) Half-wae ectfe. (b) Equalent ccut of the half-wae ectfe wth the dode eplaced wth ts battey-plus-esstance model. (c) tansfe chaactestc of the ectfe ccut. (d) nput and output waefoms, assumng that << R. max ( π 2θ O ) whee P θ ωt o sen 1 O odes

o (C) o max ( ( O 2/π ) )/R O ω t o max ( π 2θ O ) whee P θ 2 ωt o sen O 1 O Full-wae ectfe utlzng a tansfome wth a cente-tapped seconday wndng. (a) Ccut. (b) ansfe chaactestc assumng a constant-oltage-dop model fo the dodes. (c) nput and output waefoms. odes

o (C) o max ( ( 2/π ) 2 O )/R 2 O ω t ( π 2θ ) whee θ ωt o sen odes 2 P o max O he bdge ectfe: (a) ccut and (b) nput and output waefoms. O 1 2 O

L o (C) C max a f L L L p CR o 1 1 π p p 2π 1 2 2 p 1 2 2 p /R ω t 2 P 2 p p oltage and cuent waefoms n the peak ectfe ccut wth CR >>. he dode s assumed deal. (Half Wae) odes

L o (C) C max a 2f L L L p CR o 1 1 π p p 2π 1 2 2 p 1 2 p 2 2 /R ω t P P 2 2 p p p (Cente ap) (Bdge) oltage and cuent waefoms n the peak ectfe ccut wth CR >>. he dode s assumed deal. (Full Wae Rectfe) odes

Execses (5) 1. Consde a bdge-ectfe ccut wth a flte capacto C placed acoss the load essto R, fo the case n whch the tansfome seconday deles a snusod of 12 ms hang 60Hz fequency, and assumng O = 0,8 and a load esstance R= 100. Fnd the alue of C that esults n a pple oltage no lage than 1 pp. What s the C oltage at the output? Fnd the load cuent. Fnd de dodes conducton angle. What s the aeage dode cuent? What s the peak eese oltage acoss each dode? pecfy the dode n tems of ts peak cuent and ts P. Ans. 1281F; 15.4 o (a bette estmate) 14.9; 0.15A; 0.36 ad; 1.45A; 2.74A; 16.2. hus select a dode wth 3.5 to 4 A peak cuent and a 25 P atng (50%). 2. t s equed to use a peak ectfe to desgn a C powe supply that podes an aeage C output oltage of 15 on whch a maxmum of 1 pple s allowed. he ectfe feeds a load of 150. he ectfe s fed fom the lne oltage (120 ms 60Hz) though a tansfome. he dodes aalable hae 0.7 dop when conductng. f the desgne opts fo the half-wae ccut: (a) pecfy the ms oltage that must appea acoss the tansfome seconday. (b) Fnd the equed alue of the flte capacto. (c) Fnd the maxmum eese oltage that wll appea acoss the dode, and specfy the P atng of the dode. (d) Calculate the aeage cuent though the dode dung conducton. (e) Calculate the peak dode cuent. Ans. (a) 11.8 ms ; (b) 889F; (c) 32.7; (d) 2.61A; (e) 1.36 A. odes

odes A AREY OF BAC LMNG CRCU.

Execses (6) 1. Assumng the dodes to be deal, descbe the tansfe chaactestc of the ccuts shown n Fgue below. o=(3/4)+5/4 5 o 6 3-6 o o=(4/7)+15/7 5-6 o= o=(4/5)+3/5 o=(2/3)-2 3 o= 2. Assumng the dodes has a 0.7 dop when conductng and the zene specfed oltage s 8.2 (deal), descbe the tansfe chaactestc of the ccuts shown n Fgue below. 6.75 o=(1/6)+8 9.6 o -9.6 9.6-9.6 o= o=(1/6)-8 odes

he Clamped Capacto o C Restoe O 10 10 4 10-6 t t 10 4 O t t -10-6 10 etemne X to hae an aeage oltage of output A fo the ccut shown n fgue below. Consde the dode deal and the nput sgnal s that shown n fgue below. Ans.: X = -(1/2)A odes

1 -P -2P odes he oltage ouble 1 P t -P O t -2P t

PECAL OE YPE he chottky-bae ode (B) aactos Photododes Lght-Emttng odes (LEs) odes

Photonc eces Lght-emttng dodes (LE) ecombnaton electon (+) hole (-) enegy = E G / h h: Planck s constant h=6.63x10-34 Jsec - heat - lght (E=h) Mateals: 10 GaAs ( nfaed ) GaAs 1-x P x GaAs 0.6 P 0.4 ed lght ( E G 1.8 e ) (ma) 20 1.0 2.0 () B.G. teetman, old tate Electonc eces, 2nd edton, Pentce-Hall, 1980 odes

Photododes (1/2) h > E G p n E R gop G op : optcal geneaton ate Relate numbe of MNORY caes ncease by a lage amount dft cuent nceases. odes dak cuent

Photododes (2/2) PH a,c p = x > 0 b p = x < 0 the dode s a powe souce. No llumnaton a OC Model fo optcally llumnated dode. PH epesents the cuent geneated by absopton of photons n the cnty of the pn juncton. c C b 1 C 0 PH PH n s e OC 0 n ln PH s odes

Photo detecto Optosolato + B + B R R O O PH (a) (b) Basc photo-detecto ccut (a) and model (b) No llumnaton: O = B llumnaton: O = B -R ph LE photodode Lght-to-oltage conete R ph O = Rph odes

ola cells 1.5 1.0 0.5 0.0-0.5 sc Pmax oc Cell Cuent c (A) 3 n = m, = m fo P = P max m m < oc sc Aeage sola enegy (zenth): 100mW/cm 2 Maxmum powe 300 mw -1.0-1 Cell oltage () C emnal chaactestcs fo a pn juncton sola cell 0 1 Effcency of sola cells ange between 10% and 20% odes