Lecture1-Introduction to Electronics(20!3!11)

download Lecture1-Introduction to Electronics(20!3!11)

of 7

Transcript of Lecture1-Introduction to Electronics(20!3!11)

  • 7/27/2019 Lecture1-Introduction to Electronics(20!3!11)

    1/7

    EE 332

    DEVICES AND CIRCUITS II

    Lecture 1Introduction to Electronics(1)

    The Start of the Modern Electronics Era

    Bardeen, Shockley, and Brattain at Bell The first germanium bipolar transistor.

    Labs - Brattain and Bardeen invented

    the bipolar transistor in 1947.

    Roughly 50 years later, electronics

    account for 10% (4 trillion dollars) of

    Electronics Milestones

    1874 Braun invents the solid-staterectifier.

    1906 DeForest invents triode vacuumtube.

    1907-1927

    First radio circuits de-veloped fromdiodes and triodes.

    1925 Lilienfeld field-effect device patentfiled.

    1947 Bardeen and Brattain at BellLaboratories invent bipolartransistors.

    1952 Commercial bipolar transistorproduction at Texas Instruments.

    1956 Bardeen, Brattain, and Shockleyreceive Nobel prize.

    1958 Integrated circuit developed byKilby and Noyce

    1961 First commercial IC from FairchildSemiconductor

    1963 IEEE formed from merger or IRE

    and AIEE1968 First commercial IC opamp

    1970 One transistor DRAM cell inventedby Dennard at IBM.

    1971 4004 Intel microprocessorintroduced.

    1978 First commercial 1-kilobit memory.

    1974 8080 microprocessor introduced.

    1984 Megabit memory chip introduced.

    2000 Alferov, Kilby, and Kromer shareNobel prize

    Goals of Lecture 1-2

    Explore the history of electronics.

    Quantify the impact of integrated circuit

    technologies.

    Describe classification of electronic signals.

    Review circuit notation and theory. Introduce tolerance impacts and analysis.

    Describe problem solving approach

    1

  • 7/27/2019 Lecture1-Introduction to Electronics(20!3!11)

    2/7

    Evolution of Electronic Devices

    Vacuum

    Tubes

    Discrete

    Transistors

    SSI and MSI

    Integrated

    Circuits

    VLSI

    Surface-Mount

    Circuits

    Device Feature Size

    Feature size reductions

    enabled by process

    innovations.

    Smaller features lead to

    more transistors per unit

    area and therefore higher

    density.

    Rapid Increase in Density ofMicroelectronics

    Memory chip density

    versus time.

    Microprocessor complexity

    versus time.

    Microelectronics Proliferation

    The integrated circuit was invented in 1958.

    World transistor production has more than doubled every

    year for the past twenty years.

    Every year, more transistors are produced than in all

    previous years combined.

    Approximately 109 transistors were produced in a recent

    year. Roughly 50 transistors for every ant in the world .

    *Source: Gordon Moores Plenary address at the 2003 International Solid

    State Circuits Conference.

    2

  • 7/27/2019 Lecture1-Introduction to Electronics(20!3!11)

    3/7

    Signal Types

    Analog signals take oncontinuous values -typically current orvoltage.

    Digital signals appear atdiscrete levels. Usuallywe use binary signalswhich utilize only twolevels.

    One level is referred to aslogical 1 and logical 0 isassigned to the other level.

    Digital-to-Analog (D/A) Conversion

    For an n-bit D/A converter, the output voltage is expressed

    as:

    The smallest possible voltage change is known as the least

    significant bit or LSB.

    VLSB = 2n

    VFS

    VO = (b121 + b2 2

    2 + ... + bn 2n )VFS

    Analog-to-Digital (A/D) Conversion

    Analog input voltage vx is converted to the nearest n-bit number.

    For a four bit converter, 0 -> vx input yields a 0000 -> 1111 digitaloutput.

    Output is approximation of input due to the limited resolution of the n-bit output. Error is expressed as:

    1 2 nV = vx (b1 2 + b2 2 + ... + bn 2 )VFS

    Analog and Digital Signals

    Analog signals arecontinuous in time and

    voltage or current.

    (Charge can also be used

    as a signal conveyor.)

    After digitization, thecontinuous analog signal

    becomes a set of discrete

    values, typically separated

    by fixed time intervals.

    3

  • 7/27/2019 Lecture1-Introduction to Electronics(20!3!11)

    4/7

    A/D Converter Transfer Characteristic

    V = vx (b121 + b2 2

    2 + ... + bn 2n )VFS

    Problem-Solving Approach

    Make a clear problem statement.

    List known information and given data.

    Define the unknowns required to solve the problem.

    List assumptions. Develop an approach to the solution.

    Perform the analysis based on the approach.

    Check the results.

    Has the problem been solved? Have all the unknowns been found?

    Is the math correct?

    Evaluate the solution.

    Do the results satisfy reasonableness constraints?

    Are the values realizable?

    Use computer-aided analysis to verify hand analysis

    What are Reasonable Numbers?

    If the power suppy is +-10 V, a calculated DC bias value of 15 V (not

    within the range of the power supply voltages) is unreasonable.

    Generally, our bias current levels will be between 1 uA and a few

    hundred milliamps.

    A calculated bias current of 3.2 amps is probably unreasonable and

    should be reexamined.

    Peak-to-peak ac voltages should be within the power supply voltage

    range.

    A calculated component value that is unrealistic should be rechecked.

    For example, a resistance equal to 0.013 ohms.

    Given the inherent variations in most electronic components, three

    significant digits are adequate for representation of results. Three

    significant digits are used throughout the text.

    Notational Conventions

    Total signal = DC bias + time varying signal

    Resistance and conductance - R and G with same

    subscripts will denote reciprocal quantities. Mostconvenient form will be used within expressions.

    vT = VDC + Vsig

    iT = IDC + isig

    Gx =1

    Rx and g =

    1

    r

    4

  • 7/27/2019 Lecture1-Introduction to Electronics(20!3!11)

    5/7

    Circuit Theory Review: Voltage

    Division

    v1 = isR1 v2 = isR2

    and

    vs = v1 + v2 = is (R1 +R2)

    is =vs

    R1 +R2

    v1 = vsR1

    R1 +R2v2 = vs

    R2

    R1 +R2

    Applying KVL to the loop,

    Combining these yields the basic voltage division formula:

    and

    Circuit Theory Review: Current Division

    is = i1 + i2

    i = i1 sR2

    R1 +R2

    Combining and solving for vs,

    Combining these yields the basic current division formula:

    where i2 =vs

    R2i1 =

    vs

    R1and

    vs = is1

    1

    R1+

    1

    R2

    = isR1R2

    R1 +R2= isR1 || R2

    =i2 isR1

    R1 +R2

    Circuit Theory Review: CurrentDivision (cont.)

    i1 = 5 ma3 k

    2 k + 3 k= 3.00 mA

    Using the derived equations

    with the indicated values,

    Design Note: Current division only applies when the same

    i2 = 5 ma2 k

    voltage appears across both resistors.

    2 k + 3 k= 2.00 mA

    v1 = 10 V8 k

    8 k + 2 k= 8.00 V

    Using the derived equations

    with the indicated values,

    v2 = 10 V2 k

    8 k + 2 k = 2.00 V

    Design Note: Voltage division only applies when both

    resistors are carrying the same current.

    Division (cont.)

    Circuit Theory Review: Voltage

    5

  • 7/27/2019 Lecture1-Introduction to Electronics(20!3!11)

    6/7

    Circuit Theory Review: Thevenin and

    Norton Equivalent Circuits

    Circuit Theory Review: Find theThevenin Equivalent Voltage

    i1 =vo vs

    R1+vo

    RS= G1 vo vs( )+ GSvo

    i1 = G1 vo vs( )

    G1 + 1( )vs = G1 + 1( )+ GS[ ]vo

    v =G1

    o

    + 1( )G1 + 1( )+ GS

    v R1RS

    sR1RS

    =+ 1( )RS

    + 1( )RS + R1v

    Applying KCL at the output node,

    Current i1 can be written as:

    Combining the previous equations

    s

    Circuit Theory Review: Find theThevenin Equivalent Voltage (cont.)

    vo

    =+ 1( )RS

    + 1( )RS + R1vs

    =50 + 1( )1 k

    50 + 1( )1 k + 1 kvs

    = 0.718vs

    Using the given component values:

    and

    vTH = 0.718vs

    Circuit Theory Review: Find the

    Thevenin Equivalent VoltageProblem: Find the Thevenin

    equivalent voltage at the output.

    Solution:

    Known Information and

    Given Data: Circuit topology

    and values in figure.

    Unknowns: Thevenin

    equivalent voltage vTH.

    Approach: Voltage source vTHis defined as the output voltage

    with no load.

    Assumptions:None.

    Analysis:Next slide

    6

  • 7/27/2019 Lecture1-Introduction to Electronics(20!3!11)

    7/7

    Circuit Theory Review: Find the

    Thevenin Equivalent ResistanceProblem: Find the Thevenin

    equivalent resistance.

    Solution:

    Known Information and

    Given Data: Circuit topology

    and values in figure.

    Unknowns: Thevenin

    equivalent voltage vTH

    .

    Approach: Voltage source

    vTH is defined as the output

    voltage with no load.

    Assumptions: None.

    Analysis: Next slide

    Test voltage vx has been added to the

    previous circuit. Applying vx andsolving for ix allows us to find the

    Thevenin resistance as vx/ix.

    End of Lecture 1

    Circuit Theory Review: Find the

    Thevenin Equivalent Resistance (cont.)

    ix = i1 i1 +GSvx

    = G1vx +G1vx +GSvx

    = G1 +1( )+GS[ ]vx

    Rth =vxix

    =1

    G1 + 1( )+GS= RS

    R1

    + 1

    Applying KCL,

    Rth = RSR1

    +1= 1 k

    20 k

    50 +1= 1 k 392 = 282

    7