Handouts 6002 L2 Oei12 Gaps

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    Basic Circuit Analysis Methods

    (KVL and KCL method, Node method)

    6.002xCIRCUITS ANDELECTRONICS

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    Remember, our EECS playgroun

    Review

    Observe the lumpedmatter discipline LMD

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    Lumped circuit element+

    -

    power consumed by element =

    Review

    i

    v

    vi

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    LMD allows us to create thelumped circuit abstraction

    Review

    +!! R1

    R3R2

    V

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    KVL:

    For all loops

    KCL:

    For all nodes

    0=j j

    0=j ji

    ReviewReview

    Maxwells equations simplify toalgebraic KVL and KCL under LMD!

    dlE =

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    DE

    +!!

    Review

    R1 R4R3

    R2 R5

    d

    c

    b

    a

    V0

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    Lets Begin by Building aToolchest ofAnalysis Techniques

    +!!

    R1 R4

    R3

    R2 R5

    Analyzingcircuit me

    Find allelemenand is

    V0

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    Method 1: Basic KVL, KCL method ofCircuit analysis

    Goal: Find all element vs and is

    1. write element v-i relationships(from lumped circuit abstraction)

    2. write KCL for all nodes

    3. write KVL for all loopslots of unknownslots of equationslots of fun

    solve

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    !

    i+

    -

    Element e

    Current is taken to bepositive going into thepositive voltage terminal

    Method 1: Basic KVL, KCL method of Circuit analy

    Then powerconsumedby element e

    is = vi

    This

    convecalledAssocvaria

    discip

    Goal: Find all element vs and isLabeling element vs and is

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    Method 1: Basic KVL, KCL method ofCircuit analysis

    For R

    For voltage source

    For current source

    You will need this for step 1: Element Relations

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    Lets Apply KVL, KCL Method to this

    The Demo Circuit

    +!!

    R1 R4

    R3

    R2 R5

    V0

    Goal: Find all element vs and is

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    KVL, KCL Example

    a

    d

    c

    +!!

    Note the use of associated var

    R4

    R5R2

    R1

    R3bV0

    Label all vs and is

    0

    12 u

    a

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    Step 1 of KVL, KCL Method12 unknowns

    1. Element relationshipsiv,

    c

    1

    +

    2

    +

    0i

    +!!V00+

    a

    5050, ii

    L1

    a

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    Step 2 of KVL, KCL Method

    12 unknowns

    2. KCL at the nodes

    (use conventiosum currents the node)

    5050, ii

    c

    1

    +

    2

    +

    0i

    +!!V00+

    a

    L1

    a

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    Step 3 of KVL, KCL Method12 unknowns

    3. KVL for loops

    (use conventyou go arounassign first sign to each

    5050, ii

    c

    1

    +

    2

    +

    0i

    +!!V00+

    a

    L1

    KVL KCL M th d

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    KVL, KCL Method1. Element v, i relationships

    v0 = V0v1 = i1R1

    v2 = i2R2

    v3 = i3R3v4 = i4R4

    v5 = i5R5

    2. KCL at the nodes

    redundant

    0410=++ iii

    0132=+ iii

    0435=

    iii

    0520= iii

    a:

    b:

    d:

    c:

    3. KVL for loops

    431=+ vvv

    210=++ vvv

    253

    =+ vvv

    540=++ vvv

    L1:

    L2:

    L3:

    L4:

    Method 3 the node method will be much better!

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    Other Analysis MethodsMethod 2 Apply element combination rules

    A R1 R2 R3 RN

    B G2G1 GN

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    Method 2 Apply element combination ru

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    Method 2 Apply element combination ru

    +!!

    Example

    R1

    R3R2

    V

    Method 3 Node analysis

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    1.

    2.

    3.

    4.

    5.

    Select reference node ( ground) fromwhich voltages are measured.

    Label voltages of remaining nodes withrespect to ground. These are theprimary unknowns.

    Write KCL for all but the ground node,substituting device laws and KVL.

    Solve for node voltages.

    Back solve for branch voltages andcurrents (i.e., the secondary unknowns).

    ParticularapplicatioKVL, KCLmethod

    Method 3 Node analysis

    6.002xworkhorse

    Method 3 Node analysis

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    Example: Old Faithful, plus current source

    +!!

    R1 R4R3

    R2R5

    V0

    Method 3 Node analysis

    1. Select rground n

    2. Label nowith resground.

    g

    I1

    St 3 f N d M th dV0

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    Step 3 of Node Method

    For convenience, writei

    iR

    G1

    =

    To avoid mistakes, use convention

    E.g., always sum the currents leaving a node

    +!! e1

    R

    V0

    V0

    3. Writnodes

    devic

    Step 4 of Node Method

    V0

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    Step 4 of Node Method

    Move constant terms to RHS & collect unknowns

    2 equations, 2 unknowns Solve for es

    (compare units)

    0)()()( 21321101 =++ GeGeeGVe

    0)()()( 152402312 =++ IGeGVeGee

    KCL at e1

    KCL at e2

    4. Solvvolt

    +!! e1

    R

    V0

    0

    Step 5 of Node Method

    V0

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    Step 5 of Node Method

    5. Bacbran

    curr

    +!! e1

    R

    V0

    0

    e1 e2Once you have solved for and ,easy to find branch vs and is

    For example:

    i+

    v1

    Revisit Step 4 of Node Method for Cultural Intere

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    In matrix form:

    =

    ++

    ++

    04

    1

    2

    1

    5433

    3321

    VG

    VG

    e

    e

    GGGG

    GGGG

    conductivitymatrix

    unknownnode

    voltages

    Revisit Step 4 of Node Method for Cultural Intere

    )()()( 10323211 GVGeGGGe =+++

    140543231 )()()( IGVGGGeGe +=+++

    4. Solve for no

    Step 4 of Node Method 4 S l f

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    +

    =

    ++

    ++

    104

    01

    2

    1

    5433

    3321

    IVG

    VG

    e

    e

    GGGG

    GGGG

    ( )( ) 23543321

    104

    01

    3213

    3543

    2

    1

    GGGGGGG

    IVG

    VG

    GGGG

    GGGG

    e

    e

    ++++

    +

    ++

    ++

    =

    Solve

    5G

    3G

    4G

    3G

    2

    3G

    5G

    2G

    4G

    2G

    3G

    2G

    5G1

    G4

    G1

    G3

    G1

    G

    1I0V4G3G0V1G5G4G3G

    1e

    ++++++++

    ++++

    =

    ( )( ) ( )( )

    5343

    2

    3524232514131

    104321013

    2

    GGGGGGGGGGGGGGGGG

    IVGGGGVGGe

    ++++++++

    ++++

    =

    (same denominator)

    Nin

    nein th

    Step 4 of Node Method 4. Solve for no

    Step 4 of Node Method V0

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    E.g., solve for , given

    K2.8

    1

    G

    G

    5

    1=

    K9.3

    1

    G

    G

    4

    2=

    K5.1

    1G

    3= 0

    1=I

    026.0 Ve =

    If , thenVV 30= 02

    8.1 Ve =

    Step 4 of Node Method

    +!! e1

    R

    V0

    e2